diff --git a/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/2301.01240v1.pdf.txt b/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/2301.01240v1.pdf.txt new file mode 100644 index 0000000000000000000000000000000000000000..794b5e16b06bd383c4dbb02af3cd4c29fa3a76d5 --- /dev/null +++ b/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/2301.01240v1.pdf.txt @@ -0,0 +1,1300 @@ +1 +Modeling Effective Lifespan of Payment +Channels +Soheil Zibakhsh Shabgahi, Seyed Mahdi Hosseini, Seyed Pooya Shariatpanahi, Behnam Bahrak +Abstract—While being decentralized, secure, and reliable, Bitcoin and many other blockchain-based cryptocurrencies suffer from +scalability issues. One of the promising proposals to address this problem is off-chain payment channels. Since, not all nodes are +connected directly to each other, they can use a payment network to route their payments. Each node allocates a balance that is frozen +during the channel’s lifespan. Spending and receiving transactions will shift the balance to one side of the channel. A channel becomes +unbalanced when there is not sufficient balance in one direction. In this case, we say the effective lifespan of the channel has ended. +In this paper, we develop a mathematical model to predict the expected effective lifespan of a channel based on the network’s topology. +We investigate the impact of channel unbalancing on the payment network and individual channels. We also discuss the effect of +certain characteristics of payment channels on their lifespan. Our case study on a snapshot of the Lightning Network shows how the +effective lifespan is distributed, and how it is correlated with other network characteristics. Our results show that central unbalanced +channels have a drastic effect on the network performance. +Index Terms—Bitcoin, Lightning Network, Payment Channel, Lifespan, Random Walk. +! +1 +INTRODUCTION +B +ITCOIN is the first decentralized cryptocurrency, in- +troduced in 2008 which provides security, anonymity, +transparency, and democracy without any trusted third +party [1]. Most of these properties are achieved by using +a blockchain as a distributed ledger. An inherent problem +with using a blockchain over a network is that it sacrifices +scalability [2], [3]. The reason is that all nodes, potentially +tens of thousands, must exchange, store, and verify each +and every transaction in the system [4]. Furthermore, each +block has a limited size and blocks get generated at regular +intervals (approximately every 10 minutes). This means that +with the current blocksize of 1 MB the throughput of Bitcoin +is about 4.6 transactions per second, which is much slower +than centralized systems like Visa, WeChatPay, and PayPal +[5]; making the use of Bitcoin in everyday transactions +impractical. +Another trade-off the Bitcoin consensus makes is that it +ensures security by waiting for other miners to confirm a +transaction by extending the block holding that transaction, +which reduces the throughput. This way it makes sure that +the double spending attack is highly improbable. Currently, +the standard waiting time for a block to be confirmed is 6 +blocks, which is almost one hour [6]. +Bitcoin’s capacity limitations are being felt by users in +the form of increased transaction fees and latency. With +an increasing demand for making transactions, users need +to pay more transaction fees in order to make sure that +their transaction is more profitable for the miners; hence +have a higher chance of making it into a block. Queuing of +transactions and network bandwidth will lead to a longer +delay time for a transaction to appear in the blockchain. +There are many different proposals to solve the scala- +bility problem. Most of the proposals fall into three cate- +gories: Layer0, Layer1, and Layer2 solutions [7]. Layer0 +solutions try to enhance the infrastructure, like the network +that connects the nodes. Layer1 solutions try to enhance +the blockchain’s shortcomings by changing the consensus +mechanism and protocols [8], [9]. Layer2 solutions propose +ways to move away from the blockchain, and for this reason, +they are also called off-chain solutions [10]. +In 2016 the idea of Lightning Network (LN) was pro- +posed to move the transactions to the second layer (off- +chain) [4]. The Lightning Network consists of payment +channels in a P2P fashion. Payment channels allow two +parties to exchange payments with negligible time and cost, +but both parties must freeze an initial fund in the channel +so no one can spend more money than they own and no +double spending occurs. It is important to note that the sum +of funds in each channel remains constant throughout the +channel’s lifespan and only the channel’s balance changes. +When two parties that do not have a direct channel want to +exchange payments they can use other parties to route their +payments. So a network of nodes is constructed and all the +connected nodes can send each other payments. +This system moves the cost of submitting a transaction +off the blockchain. Only the final states between two nodes +will eventually make it into the blockchain, which signifi- +cantly increases throughput. Furthermore, no time is needed +for the transaction to be confirmed and all transactions in a +channel happen almost instantly. +After several transactions through a channel, the channel +starts to get unbalanced; meaning all of its funds have gone +to one of the parties and the other node cannot route any +more payments through the channel. In this case, it is best +to close the unbalanced channel or open a new one. +In this paper, we investigate the expected effective lifes- +pan of a channel in a payment network. Our contributions +can be summarized as follows: +• +We provide simulation evidence of how channel +unbalancing impacts its throughput. Moreover, we +show how the performance of the payment network +arXiv:2301.01240v1 [cs.DC] 11 Sep 2022 + +2 +can be affected if a number of channels become +unbalanced. +• +We present a mathematical model of payment chan- +nels to predict the expected time for a channel to get +unbalanced considering the channel’s position in the +network and its initial balance. We call this time the +Effective Lifespan of the channel. +• +We evaluate our model through simulation, and +observe how the Effective Lifespan of a channel is +affected if we change any of its characteristics. +• +By analyzing a recent snapshot of the Lightning Net- +work, we find the distribution of real-world chan- +nel lifespans and its correlation with the network’s +topological parameters. We also investigate the rela- +tionship between the centrality of a channel in the +network and its effective lifespan. +2 +RELATED WORK +While the LN white paper [4] does not discuss channel re- +balancing, there exists some research on channel balances +and their significance. +The importance of channel balances is mainly discussed +in four major areas; re-balancing, security, performance, and +financial. +Re-balancing: [11] proposes a method for re-balancing +payment channels. This work allows arbitrary sets of users +to securely re-balance their channels. However, this paper +does not discuss the application of re-balancing, and how +frequently it should be performed. [12] also proposes meth- +ods for rebalancing LN channels, but does not discuss the +frequency of rebalancing. +Performance: In [13] the authors discuss why it is in +the best interest of the network to have balanced channels. +They propose a method to re-balance some channels to +improve the network’s performance. [14] presents a method +in which a node can make its channels balanced through +circular subgraphs. It also develops a method for measuring +imbalance in a payment network. +Security: There has been some research on the security +aspects of channel unbalancing. In [14], [15], and [16] the +authors describe a method in which it is possible for an +adversary to uncover channel balances. Having unbalanced +channels poses the threat of griefing attacks. The incentive +for honest behavior in the LN channels is the penalty for +misbehavior. If a node cheats by publishing an old contract, +it will be penalized and all of the channel funds can be +claimed by the victim. When channels are unbalanced the +penalty is less so there is less incentive for honest behav- +ior. In [17] the authors discuss some countermeasures like +watchtowers to keep the misbehaving nodes from closing +the channel. +Financial: Routing payments through a channel can +make revenue for the owner. So payment channels can be +looked at as investments. In [18] the authors do an in-depth +financial analysis on how much should payment channels +charge for routing payments. One of the key factors in this +analysis is the lifespan of payment channels. In order to +analyze investing in a payment channel, nodes should be +able to have an estimate on how long the investment stays +profitable and what is the impact of channel unbalancing on +the profits of a channel. Branzei et al. [18] assume an equal +probability of having a payment from each side in a channel +and use the lifetime of channels for financial analyses. We +will show how the lifespan of a channel could be affected +by this probability. +In this paper we focus on the details of estimating chan- +nel lifespans; considering parameters such as the placement +of the channel in the topology and payment rates between +each pair and explain the importance of estimating channel +lifespans. This gives us a better and more realistic estimation +of the channel’s lifespan compared to existing work. More- +over, we measure the impact of imbalanced channels on the +network. +Despite the importance of payment channel’s lifespan, to +the best of our knowledge, the expected lifespan of channels +in the payment network has not been discussed in detail. +3 +TECHNICAL BACKGROUND +In this section, we provide a technical background to under- +stand the remainder of this paper thoroughly. +Payment Channels +Payment channel is a financial contract between two parties +in a cryptocurrency like Bitcoin. The contract allocates a +balance of funds from both parties. The contract is estab- +lished by a 2-of-2 multisignature address which requires the +cooperation of both parties to spend the funds. +Payments are made off the blockchain by passing on +a new version of the contract with a different balance of +allocated funds on the spending transaction; which both +parties have to sign. The channel is closed when one of +the parties publishes the latest version of the contract to +the blockchain. We define the payment direction to be the +direction in which funds are moving during a transaction. +In this paper, we call the sum of locked funds in a +channel the channel’s capacity. When all of the funds of +a channel are allocated to one of the parties, the channel +becomes unbalanced. In this case payments can only be made +from one side of the channel. A channel’s effective lifespan is +the time from creation of a channel until the first imbalance +occurs. A channel’s success probability is defined as the +number of successful payments made through the channel +divided by the total number of payment attempts. +Several connected payment channels can form a pay- +ment network, in the case of Bitcoin, this network is called +the Lightning Network [4]. This network is used to route +payments through intermediate channels between nodes +who do not have a direct channel between them. We de- +fine a network’s success probability as the total number of +successful payments made on the network divided by the +total attempts to route payments through the network [19]. +Random Walk +The random walk model has been used in a wide variety +of contexts to model the movement of objects in different +spaces. This paper uses one-dimensional random walk to +model the liquidity balance in a payment channel. Two +endpoints on the left and right sides of the random walk +are assumed to represent the channel imbalance condition. + +3 +Fig. 1. Relation of network success rate with percentage of unbalanced +channels in the network. +In our model, each payment corresponds to one step of +the random walk model, and the direction of the payment +determines the direction of that step. Suppose we take prob- +abilities p and 1 − p as the probability of payment direction +(i.e., step direction). We can find the expected number of +payments (steps) needed for the channel (the random walk +model)to get unbalanced (to reach one of the endpoints). +Betweenness Centrality +Betweenness centrality is a measure based on shortest paths +for the importance of the location of a node or an edge +in a graph. Betweenness centrality for an edge(a, b) in the +network is defined as follows: � +s,t∈V +s̸=t +σ(s,t|edge(a,b)) +σ(s,t) +, where +σ(s, t) is the total number of shortest paths between nodes +s and t and σ(s, t|edge(a, b)) is the total number of shortest +paths between s and t that pass through edge(a, b). +4 +MOTIVATION +One of the important characteristics of a payment network +is reliability. Reliability can be defined as the probability of +payment success [19]. +In this section, we analyze the payment routing failure +probability of a singular channel after unbalancing, and the +network’s success probability of routing a payment when +some channels are unbalanced. +4.1 +Singular Channel +We ran a simulator of a single payment channel to see how +much the failure rate increases after the first time that the +channel becomes unbalanced. Fig. 2 shows the failure rate +after the first time a channel becomes unbalanced. During +the simulation, 5000 payments were being routed through +an initially balanced channel. Then the simulator calculates +the failure rate after the first time the channel becomes un- +balanced. As Fig. 2 suggests, the probability of the direction +of payments (p) is a key factor in determining how much +the probability of payment success degrades after the first +imbalance occurs. Channels capacity has little to no impact +on how well it performs after unbalancing. +These results show that the probability of payment di- +rection (p), which depends on the network topology and +Fig. 2. Failure rate after unbalancing. +the network’s transaction flow, is one of the most impor- +tant parameters in determining the channel’s lifespan; more +importantly, shows the impact of unbalancing on channel +success probability after the channel becomes unbalanced. +4.2 +Network Performance +Using the CLoTH simulator [19] we simulate and measure +the performance of Lightning Network. In each iteration we +take channels from the given LN snapshot and make them +unbalanced, we then measure the success probability after +attempting 5000 payments. Choosing more central channels +as unbalanced channels is more reasonable, because they +route more payments and thus have a higher probability +of becoming unbalanced in the real world. We considered +two scenarios for selecting channels to unbalance: choos- +ing channels randomly and choosing channels that have +a higher betweenness centrality. As illustrated in Fig. 1, +as the percentage of unbalanced channels increases, the +routing success rate decreases dramatically for both channel +selection scenarios. In the random selection scenario, it is +noticeable that the first 10 percent of unbalanced channels +have less effect on the network performance than the last +10 percent of unbalanced channels. We see that unbalancing +channels with a higher betweenness centrality has a higher +impact on the network performance in contrast with the +random selection scenarios. Therefore, per any percentage of +unbalanced channels, selection with betweenness centrality +is more effective. +Seres et al. [20] suggest that in the Lightning Network, +the top 14% central channels will have the most significant +impact on the network. In a different experiment we made +15% of the network’s channels unbalanced, we first sort the +channels by betweenness centrality and take a window of +15% of the channels per experiment. We start with the 15% +most central channels and move all the way up to 15% +least central channels. It can be inferred from the results +in Fig. 3 that more central channels have more impact on +the network success rate when they become unbalanced. As +we can see in Fig. 3, the top 15% central channels have the +most significant effect on the success rate when they become +unbalanced. This confirms the result from Fig. 1. + +100 +Random +90 +Most central +80 +rate +70 +Success +60 +50 +40 +30 +20 +20 +40 +60 +80 +100 +Percentage of initialy unbalanced channels0.40 +Capacity: 1.2 Msat +Capacity: 1.8 Msat. +0.35 +Capacity: 2.4 Msat. +Capacity: 3.0 Msat. +0.30 +Capacity: 3.6 Msat. +0.20 +Fal +0.15 +0.10 +0.05 +0.300 +0.325 +0.3500.3750.400 +0.425 +0.450 +0.475 +0.500 +probability of payment direction4 +Fig. 3. Per each data point the i-th to (i+4500)-th most central channels +are unbalanced and the success rate of the network is measured. The +total number of channels is 30457. +5 +THE MODEL +As we discussed in Section 4 channel balances have a sig- +nificant effect on both channel, and network performance. +In this section, we introduce a mathematical model to deter- +mine the expected time for a channel to get unbalanced; +we call this the channel’s expected lifespan. We model +the dynamics of a payment channel with a random walk +problem. Each payment passing through the channel will +represent a step the random walker takes. We will first +discuss our assumptions and describe the model in detail. +We then discuss how to find the model parameters. We +proceed by doing an analysis on how the expected lifespan +is affected by changing channel’s characteristics. +5.1 +Random Walk Model +Take a payment channel between two nodes A and B, and +take their initial balance allocated for the channel to be FA +and FB, respectively. The goal is to determine the expected +time it will take for this payment channel to become unbal- +anced for the first time. We make the following assumptions: +• +All the payments have the same amount denoted +with ω (PaymentSize). +• +The payments from each node come with a Poisson +distribution. +Since the number of nodes is large and the probability +of sending a transaction for a given time is small, we can +assume that transaction arrival for each channel is a Poisson +process for moderate time windows [21]. Although the +dynamics of the network will change over time, we make +the assumption of having a fixed topology. +We model the dynamics of a payment channel with a +random walk problem. Each payment is simulated by a step +the random walk takes. To simulate a payment channel, take +the liquidity of node A as the distance of the random walk +from the endpoint on the right hand side and the liquidity +of node B as the distance from the endpoint on the left hand +side. +The payment direction determines the direction of that +step. So the payment direction probability is the probability +of going to the right or left for the random walk in each step. +Fig. 4. Distribution of expected lifespan with 10000 random walk simula- +tions with p = 1 +2 and a = b = 1.2 Msat. +Let the random walk start at the origin of the number +line. The two endpoints a and −b are ⌊ FA +ω ⌋ and ⌊ FB +ω ⌋, +respectively. +Since we assume that the payments from each side are +made independently with a Poisson process, and the sum +of two independent Poisson processes is itself a Poisson +process, we can say that payments come to the channel with +a Poisson distribution having: +λpayment = λA,B + λB,A, +(1) +thus the relation between expected time and expected num- +ber of random walk steps is: +Etime = +Esteps +λpayment +, +(2) +where Etime is the expected time until unbalancing and +Esteps is the expected number of steps until unbalancing +occurs. +The expected number of payments until unbalancing +occurs, can be a better metric depending on the application; +when multiplied by average fee per payment, it gives the +expected routing income, and when divided by λ it gives +the expected lifespan. +The objective is to determine the time it takes for a +channel to become unbalanced. We first try to find the +expected number of steps needed for the random walker +to reach +a or −b for the first time. +Lemma 1. The expected number of steps to reach +a or −b +for the first time starting from zero considering the probability p +for the positive direction and q = 1 − p for the negative direction +is: +Esteps = +� apa(pb−qb)+bqb(qa−pa) +(p−q)(pa+b−qa+b) +p ̸= 1/2 +ab +p = 1/2 +(3) +. +We provide the proof of Lemma 1 in Appendix A. +We simulated a Random Walk which starts from point +zero with the same probability of going to each side (p = 1 +2). +The simulation ran 10000 times to find the distribution of the +number of steps needed to reach +a or −b. Fig. 4 illustrates +the result of the simulation. We can observe that most of +the times the random walk reaches one of the bounds in +less than 400 steps, but there are not many situations where + +98 +96 +Success rate +94 +92 +90 +88 +86 +0 +5000 +10000 +15000 +20000 +25000350 +300 +250 +count +200 +150 +100 +50 +0 +0 +500 +1000 +1500 +2000 +2500 +3000 +number of steps5 +it takes a huge number of steps to reach these bounds. +However, the average number of steps needed to reach these +bounds is 400.5 confirming 11. +5.2 +Finding p +In Section 5.1 we modeled the payment channel dynamics +with a random walk and a parametric formula was con- +structed according to Lemma 1. +A payment network can be formally expressed by an +unweighted directed graph. V +represents the set of all +nodes, and the set of edges is denoted by E. Each channel +is represented using two edges from E each for one of the +directions. +We define MRates to be the matrix of payment rates +between each two nodes. The rate of payments (i.e., number +of payments per day) from node i to node j is denoted by +MRatesij. +λa,b represents the rate of payments transmitted over +the edge(a, b). λa,b consists of the sum of portions of the +payment rate between each pair of nodes that pass through +edge(a, b). So we have: +λa,b = +� +s,t∈V +s̸=t +σ(s, t|edge(a, b)) +σ(s, t) +MRatesst, +(4) +where σ(s, t) is the number of shortest paths from node s +to node t and σ(s, t|edge(a, b)) is the number of shortest +paths from node s to node t passing through edge(a, b) in +the directed graph G. +Lemma 2. p +q = λ(a,b) +λ(b,a). +According to Lemma 2: +p = +λ(a, b) +λ(a, b) + λ(b, a) +(5) +Therefore we can find p based on the network topology. +Lemma 3. If ∀s, t ∈ V +: MRatesst = MRatests then +p = 0.5. +We provide the proofs of Lemmas 2 and 3 in Appendix A. If +we assume that MRates is a symmetric matrix, according +to Lemma 3, p is independent of MRates matrix and the +network topology. +5.3 +Model Analysis +In this section we analyze the effect of channel parameters +on the channel’s expected lifespan and perform a financial +analysis for channel lifespan. +For more realistic parameter values we used a recent +snapshot of the Lightning Network taken on Feb2019 as +a reference point. The average payment size is considered +to be 60000 sat1 [22] and the average channel capacity is +considered 2.4 Msat2 according to the snapshot. +For simplicity we use ”lifespan” and ”expected number +of payments until channel is unbalanced”, interchangeably. +1. satoshi +2. million satoshi +Fig. 5. Effect of payment direction probability on balanced channels, +according to different channel capacities. +Fig. 6. The effect of payment direction probability on expected number +of payments, according to different initial balance ratios. The channel +capacity is considered 2.4 Msat. +We first answer the question of how sensitive is a +channel’s lifespan to the changes in p. As demonstrated in +Fig. +5; if the channel is initially balanced, the maximum +lifespan happens on p = 1 +2. Also, lifespan is more sensitive +to changes in p when the capacity is higher. From this +result we can infer that it is an important consideration +for a node to make sure the channel is placed in a way +that p is close to +1 +2, otherwise the channel’s lifespan is +affected dramatically. A reasonable proposal for nodes who +want to keep their channels active as long as possible is to +charge routing fees in a way that encourages other nodes to +route their payments through the node in order to achieve +p = 0.5. Fig. 6 shows that if a channel is initially unbalanced, +its maximum possible lifespan takes a hit. Although the +maximum lifespan does not occur at exact p = 1 +2, it occurs at +a point close to this value. So even if a channel is somewhat +unbalanced, the nodes must try to keep p as close as possible +to 50%. +We now answer the question of how the lifespan is +affected by the channel capacity. As Fig. 7 suggests, the +channel lifespan increases with increasing its capacity. It is +noteworthy that the slope of this graph is increasing. So if +a node doubles its channel capacity, the channel’s lifespan +will be more than doubled. Moreover, Fig. 7 shows the effect +of a channel’s initial imbalance on its lifespan. +Usually when a node wants to create a new channel + +Capacity: 1.80 Msat. +600 +Capacity: 2.40 Msat. +Capacity: 3.00 Msat. +500 +400 +300 +200 +100 +0 +0.0 +0.2 +0.4 +0.6 +0.8 +1.0 +Probability (p)400 +a/b: 1 +a/b: 5 +350 +a/b: 50 +300 +250 +200 +150 +100 +50 +0 +0.0 +0.2 +0.4 +0.6 +0.8 +1.0 +Probability (p)6 +Fig. 7. Effect of channel capacity on the expected number of payments, +according to initial balance ratios +Fig. 8. For a fixed a = 1.2 Msat, the effect of channel b’s capacity on the +maximum possible lifespan in any p. +with another node in the network, the only parameter it has +control over is the amount of funds it wants to put in the +channel, not the funds its partner puts in the channel. This +brings up the question: how will the channel’s lifespan be +affected with the amount the other node wants to put in the +channel if our fund stays at a fixed value. Figures (8) and (9) +illustrate this effect. Fig. 8 shows the maximum achievable +lifespan considering any p value and how it is affected by +the fund that the other node commits to the channel. The +maximum lifespan grows with the initial fund of the other +edge in a linear fashion. Fig. 9 illustrates the effect of our +edge capacity if the peer node’s capacity is fixed. Figure +(9) shows that if p is in favor of payments in the direction +of our edge (p ≥ 1 +2), the lifespan increases almost linearly; +otherwise (p < 1 +2), the other edge becomes the bottleneck +and the fund we put towards the channel will have little +to no effect on the expected lifespan of the channel. If the +funds we put towards the channel do not have an effect on +the channel’s lifespan, we have wasted cost opportunities. +6 +IMPLEMENTATION AND EVALUATION +We provided a simulation proof of concept on a constructed +Lightning Network to show the accuracy of the model +discussed in Section 5. In this section we describe our +methodology for creating data and calculating accuracy of +Fig. 9. Having a fixed initial balance from peer node (b) analyzing the +effect of our initial balance fund (a), according to different payment +direction probabilities (p). +our model. We later analyze the results to see under which +conditions the model performs better. +6.1 +Methodology +The testing pipeline shown in Fig. 10 uses the following +modules: +6.1.1 +Network Generator +For each test, a random network was generated using Net- +workX’s [23] gnp random graph with the number of nodes +being 50 and the channel existence probability being 20% +(245 edges on average). +6.1.2 +Mrates Generator +As discussed in previous sections the Mrates matrix holds +the rates in which each two nodes send payments to one +another. The Mrates generator takes two main parameters: +SC and SK. SC determines the sparseness of the Mrates +matrix and SK determines the matrix skewness in relation to +its main diagonal. Per each test, a new matrix is generated. +In table (1) the sparse coefficient and the skew were changed +to test how the model will perform in each scenario. +6.1.3 +Lifespan Predictor +The lifespan predictor takes the network and the Mrates +matrix and using the model discussed in 5 gives the ex- +pected time for each channel to become unbalanced. +6.1.4 +Payment Generator +Payment generator creates random payments in CLoTH +simulator’s input format [19]. These payments follow the +Mrates generator values on average. +6.1.5 +Simulator +We used a modified version of the CLoTH simulator [19]. +We modified CLoTH such that the simulator logs the un- +balancing of channels and chooses paths randomly in cases +where more than one shortest path exists. +The payment generator and simulator run 100 iterations +per test. + +10000 +a/b: 1 +f Payments +a/b: 5 +a/b: 50 +8000 +6000 +4000 +2000 +0 +0.0 +0.2 +0.4 +0.6 +0.8 +1.0 +1.2 +Capacity (sat.) +1e7Maximum Expected Number of Payments +5000 +4000 +3000 +2000 +1000 +0 +0.0 +0.2 +0.4 +0.6 +0.8 +1.0 +1.2 +Other Edge Capacity (sat.) +1e7800 +p: 0.40 +p: 0.45 +700 +p: 0.50 +600 +p: 0.55 +p: 0.60 +500 +400 +300 +200 +100 +0 +0.5 +1.0 +1.5 +2.0 +2.5 +Edge Capacity (sat.) +1e67 +Fig. 10. Model evaluation pipeline. +TABLE 1 +error of prediction and real lifetime +SK +1 +4 +6 +10 +0.9 +0.15 +0.10 +0.09 +0.10 +SC +0.5 +0.11 +0.10 +0.08 +0.07 +0.3 +0.09 +0.07 +0.05 +0.06 +0 +0.11 +0.07 +0.07 +0.07 +6.1.6 +Lifespan Calculator +This module aggregates the results of 100 iterations of the +previous step and calculates the average lifespan and its +error. This data will be used to determine the accuracy of +the model. +6.1.7 +Model Evaluation +The error of each channel is calculated as |real−prediction| +real +. +Because some channels are positioned in a way that almost +no payments pass through them, only after a long while that +most channels are unbalanced, some payments pass through +them, we count these channels as abnormalities and do not +consider them in the error calculations. These are usually +the channels that are estimated to have a very long lifespan. +The means of calculated errors are given in Table (1) +considering different SC and SK values. +As we see, better results are obtained with smaller SCs +(meaning a busier Lightning Network). It is also notable that +SK value has little to no effect on the model performance. +This means that the model performs well in either case that +p is close to 0.5 and p is far from 0.5. +7 +LIGHTNING NETWORK ANALYSIS +In this section we will provide an analysis on channel +lifespans of a recent snapshot of the Lightning Network. +The simulation is constituted by nodes and channels taken +from a snapshot of the Lightning Network Mainnet [24] on +Feb 2019. +In Section 5, we proposed a model for a payment channel +using a random walk and we derived a formula to predict +expected channel lifespans. Moreover, the expected lifespan +of a payment channel can be found if the rate of payments +are known by using 2. Lemma 3 shows that if we have the +same rate for every pair of nodes, the probability of going +to each side is equal to 0.5. +Because payment rates and channel balances usually are +not public in the Lightning Network, we have to make +assumptions on the distribution, the amount of payments, +and channel balances. We assume that all payment rates +have the same value r, which means that the rates matrix +(MRates) is symmetric. Thus according to Lemma 3, p = 1 +2 +for every channel in the network. According to 11 the +expected number of payments is equal to a × b, where +a = ⌊ FA +ω ⌋ and b = ⌊ FB +ω ⌋ for a bidirectional channel between +A and B. We assume that all channels are initially balanced, +meaning a = b = C +2ω , where C is the channel’s capacity. +According to previous results in Section 5 (equations (1) +and (4)) we have: +λpayment = ( +� +s,t∈V +s̸=t +σ(s, t|edge(a, b)) +σ(s, t) ++ σ(s, t|edge(b, a)) +σ(s, t) +)r +(6) +We also know that � +s,t∈V +s̸=t +σ(s,t|edge(a,b)) +σ(s,t) +is equal to the +edge betweenness centrality of edge(a, b) (EBC(a, b)) in +directed graph G [25]. +Because all channels are bidirectional: ∀edge(j, i) −→ +∃edge(i, j), thus ∀s, t ∈ V : +σ(s, t|edge(a, b)) +σ(s, t) += σ(t, s|edge(b, a)) +σ(t, s) +. +(7) +Assuming G +′ as an undirected graph that is derived +from G we have: +EBCG(a, b) = EBCG′ (a, b), +(8) +thus +λpayment = 2 × EBCG′ (a, b) × r. +(9) +If we put all results in (2), we have: +Etime = +( C +ω )2 +4 × 2 × EBCG′ (a, b) × r +(10) +In what follows, we first calculate all payment channels’ +lifespans in the LN snapshot using equation (10). Then we +focus on the relation between edge betweenness centrality +and lifespan of the channels. +7.1 +Distribution of Channels Effective Lifespan +Equation (10) shows that the lifespan of a channel can be +calculated based on its edge betweenness centrality and +initial fund. We assume that r = 0.0022 transactions per day +[26] and ω = 60000 sat [22]. The distribution of channels +lifespans in our snapshot is shown in Fig. 11. Much like the +distribution of channel capacities that resemble the Power +Law distribution, Fig. 11 shows that there are a lot of +channels with a low lifespan and very few channels with +a very high lifespan. +According to Seres et.al. [20] the most effective channels +are the channels with the highest betweenness centrality. +This paper suggests that the top 14% of the channels have +the most significant effect on the network’s performance. +Table (2) gives average, standard deviation, and median, +for all channels in the network and the top 14% central +channels. + +network generation +MRates generation +payment generation +loop for 100 run +lifespan prediction +simulation +lifespan calculation +model evaluation8 +Fig. 11. Histogram of expected lifespan for the LN snapshot in Feb 2019. +TABLE 2 +Lifespan statistics of the LN snapshot (day). +All Channels +Central Channels +average +1833.2 +172.3 +STD +7086.9 +587.2 +median +27.0 +1.6 +7.2 +Betweenness-Lifespan Correlation +As Seres et.al. [20] suggests, the most central channels have +the most impact on the network. As Fig. 12 shows, more +central channels have a shorter lifespan because they route +more payments per unit of time. In Fig. 12 we took batches +of the most central edges and calculated the average cen- +trality and the average lifespan per batch. The result shows +that in general the more central a channel is, the sooner it +will get unbalanced. We see an exception to this statement +in the middle of the plot, where betweenness has a positive +correlation with the average lifespan. This is due to the fact +that some very central edges have a large capacity so they +can route more payment considering that lifespan increases +with capacity quadratically. +In Section 7 A we showed that channels with larger +edge betweenness centrality values have a higher impact +on the performance of the network. In this section, we have +shown these central channels will have shorter lifespans. +Therefore, the network success rate will decrease quickly +Fig. 12. The relation between expected lifespan and betweenness cen- +trality of channels in the LN snapshot. +due to unbalancing. +8 +CONCLUSION +In this paper we modeled payment channel liquidity with +a random walk to estimate how long it takes for a channel +to become unbalanced and the effect of being unbalanced +on a channel’s probability of successful routing. We also +analyzed how unbalanced channels degrade the network’s +performance, and the relation between a channel’s centrality +and its lifespan. We showed that the network’s success +probability is sensitive to the channels’ unbalancing. +We also introduced a method to estimate the lifespan +of a channel in a payment network which can be used for +determining a good placement in the network. We provided +a proof of concept for our model and showed the results are +95% accurate. +This work shows that just allocating more funds towards +a channel does not lead to having a more successful channel. +The results show the channel’s success in the network +depends greatly on the network topology, transaction flow, +and the amount of funds the peer node puts in the channel. +We suggested the amount a node should invest in a +channel to get the longest channel lifespan and maximize its +return on investment. These results show that a misplaced +channel can have a very short lifespan and lose up to 40% +of its efficiency, so nodes could potentially create a market +based on these criteria to sell each other good connections +in the network. +APPENDIX A +PROOFS +A.1 +Lemma 1. The expected number of steps to reach ++a or −b for the first time starting from zero is +Esteps = +� apa(pb−qb)+bqb(qa−pa) +(p−q)(pa+b−qa+b) +p ̸= 1/2 +ab +p = 1/2 +(11) +Consider Sx as the expected number of steps to reach +a or +−b for the first time starting from x. Let p be the probability +of going to the positive direction and q the probability of +going in the negative direction (p + q = 1). Then we can say +that if the Random Walk starts from x, he will go to x + 1 +with probability of p and x − 1 with probability of q. so we +can infer this recurrence equation: sx = 1 + qsx−1 + psx+1 +where sx is the expected number of steps until reaching the +end point starting from point x. For the boundary conditions +we have: sa = s−b = 0 implying that the expected number +of steps needed to reach +a or −b starting from +a or −b is +zero. +so: +sx = 1 +psx−1 − q +psx−2 − 1 +p +(12) +The characteristic equation of (12) is: +(z2 − 1 +pz + q +p)(z − 1) = 0 +(13) + +104 +103 +Count +102 +101 +100 +0 +25000 +50000 +75000100000125000150000175000 +Lifespan (day)1750 +1500 +1250 +1000 +750 +500 +250 +0 +5000 +10000 +15000 +20000 +Average Edge Betweenness Centrality of Batch9 +if p = q = 1/2 we have ∆ = 0 therefore z1 = z2 = z3 = +1 so the expected number of steps needed to reach +a or −b +starting from x is: +sx = (a − x)(b − x) +(14) +if p ̸= 1/2 we have +√ +∆ = | 1−2p +p +| therefore z1 = z2 = +1, z3 = q +p and for the number of steps we have: +sx = +apa+b + bqa+b +(2p − 1)(pa+b − qa+b) + +1 +1 − 2p x+ +(a + b)paqb +(2p − 1)(qa+b − pa+b) ( q +p )x +(15) +we take x = 0 as this gives the expected number of steps to +reach +a or −b starting from zero. so we have: +S0 = +� apa(pb−qb)+bqb(qa−pa) +(p−q)(pa+b−qa+b) +p ̸= 1/2 +ab +p = 1/2 +(16) +A.2 +Lemma 2. p +q = λ(A,B) +λ(B,A) +In assumptions of Section 5 it is assumed that each node +sends its payments to other nodes with a Poisson distri- +bution. The parameter of the distribution for edge(a, b) is +λ(a, b), which is the payment rate between nodes a and b. +Assume the random variable of payments from a to b as X +and the random variable of payments from b to a as Y .Thus +we have: +P(X = n) = e−λ(A,B)(λ(A, B))n +n! +(17) +The total payment rate in each channel is the sum of rates of +its two edges. It is known that the distribution of a random +variable which is the sum of two random variables with a +Poisson process is a Poisson process; the rate of this process +equals the sum of rates. +When we have a payment from two Poisson distribu- +tions sending payments to the same channel; The probabil- +ity for the payment to be a payment from node a to node b +(p) is: +p = P(X = 1|X + Y = 1) = +e−λx(λx)1 +1! +× e−λy (λy)0 +0! +e−(λx+λy)(λx+λy)1 +1! +(18) +Thus: +p = +λx +λx + λy += +λ(a, b) +λ(a, b) + λ(b, a) +(19) +A.3 +Lemma 3. If ∀s, t ∈ V : MRatesst = MRatests then +p = 0.5. +We know from lemma 2 that: p +q = λ(a,b) +λ(b,a) so we have: +p +q = +� σ(s,t|edge(a,b)) +σ(s,t) +MRatesst +� σ(t,s|edge(b,a)) +σ(t,s) +MRatests +(20) +Because +all +channels +are +bidirectional(∀edge(a, b) +: +∃edge(b, a)) we have ∀s, t ∈ V : +σ(s, t|edge(a, b)) +σ(s, t) += σ(t, s|edge(b, a)) +σ(t, s) +(21) +In the other hand if we have ∀s, t ∈ V : MRatesst = +MRatests, we can say: +σ(s, t|edge(a, b)) +σ(s, t) +×MRatesst = σ(T, S|edge(b, a)) +σ(t, s) +×MRatests (22) +then finally we have: +λ(a, b) = λ(b, a) +(23) +so +p = 1 +2 +(24) +REFERENCES +[1] +S. Nakamoto, “Bitcoin: A peer-to-peer electronic cash system,” +Decentralized Business Review, p. 21260, 2008. +[2] +A. Chauhan, O. P. Malviya, M. Verma, and T. S. 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Le Cam, “The poisson approximation to +the poisson binomial distribution,” The Annals of Mathematical +Statistics, vol. 31, no. 3, pp. 737–740, 1960. +[22] F. B´eres, I. A. Seres, and A. A. Bencz´ur, “A cryptoeconomic +traffic analysis of bitcoin’s lightning network,” arXiv preprint +arXiv:1911.09432, 2019. +[23] A. A. Hagberg, D. A. Schult, and P. J. Swart, “Exploring network +structure, dynamics, and function using networkx,” in Proceedings +of the 7th Python in Science Conference, G. Varoquaux, T. Vaught, +and J. Millman, Eds., Pasadena, CA USA, 2008, pp. 11 – 15. +[24] E. Rohrer, J. Malliaris, and F. Tschorsch, “Discharged pay- +ment channels: Quantifying the lightning network’s resilience to +topology-based attacks,” in SandB ’19: Proceedings of IEEE Security +& Privacy on the Blockchain, jun 2019. +[25] U. Brandes, “On variants of shortest-path betweenness centrality +and their generic computation,” Social Networks, vol. 30, no. 2, pp. +136–145, 2008. +[26] A. +Research, +“The +growth +of +the +Lightning +Network,” +https://www.research.arcane.no/blog/ +the-growth-of-the-lightning-network, +2021, +[Online; +accessed +11-Nov-2021]. +Soheil Zibakhsh Shabgahi received his bach- +elor’s degree in Computer Engineering from +the Department of Electrical and Computer En- +gineering, University of Tehran, Tehran, Iran. +He is currently a research assistant at the +Data lab under the supervision of professor +Behnam Bahrak. His research interest are in +blockchain systems, Theoretical Computer Sci- +ence,distributed systems, and Machine Learn- +ing. +Seyed Mahdi Hosseini is currently an under- +graduate student majoring in computer engi- +neering at the School of Electrical and Computer +Engineering at the College of Engineering of +the University of Tehran. His research interest +consists of blockchain, system networks, and +distributed systems. +Seyed +Pooya +Shariatpanahi +received +the +B.Sc., M.Sc., and Ph.D. degrees from the De- +partment of Electrical Engineering, Sharif Uni- +versity of Technology, Tehran, Iran, in 2006, +2008, and 2013, respectively. He is currently an +Assistant Professor with the School of Electri- +cal and Computer Engineering, College of En- +gineering, University of Tehran. Before joining +the University of Tehran, he was a Researcher +with the Institute for Research in Fundamental +Sciences (IPM), Tehran. His research interests +include information theory, network science, wireless communications, +and complex systems. He was a recipient of the Gold Medal at the +National Physics Olympiad in 2001. +Behnam Bahrak received his bachelor’s and +master’s degrees, both in electrical engineering, +from Sharif University of Technology, Tehran, +Iran, in 2006 and 2008, respectively. He received +the Ph.D. degree from the Bradley Department +of Electrical and Computer Engineering at Vir- +ginia Tech in 2013. He is currently an Assistant +Professor of Electrical and Computer Engineer- +ing at University of Tehran. + diff --git a/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/load_file.txt b/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..a11a7881adeaa7e48f58e6874be3e25dfd299bc0 --- /dev/null +++ b/-9AzT4oBgHgl3EQfS_sw/content/tmp_files/load_file.txt @@ -0,0 +1,765 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf,len=764 +page_content='1 Modeling Effective Lifespan of Payment Channels Soheil Zibakhsh Shabgahi, Seyed Mahdi Hosseini, Seyed Pooya Shariatpanahi, Behnam Bahrak Abstract—While being decentralized, secure, and reliable, Bitcoin and many other blockchain-based cryptocurrencies suffer from scalability issues.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' One of the promising proposals to address this problem is off-chain payment channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Since, not all nodes are connected directly to each other, they can use a payment network to route their payments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Each node allocates a balance that is frozen during the channel’s lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Spending and receiving transactions will shift the balance to one side of the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' A channel becomes unbalanced when there is not sufficient balance in one direction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this case, we say the effective lifespan of the channel has ended.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this paper, we develop a mathematical model to predict the expected effective lifespan of a channel based on the network’s topology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We investigate the impact of channel unbalancing on the payment network and individual channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We also discuss the effect of certain characteristics of payment channels on their lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Our case study on a snapshot of the Lightning Network shows how the effective lifespan is distributed, and how it is correlated with other network characteristics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Our results show that central unbalanced channels have a drastic effect on the network performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Index Terms—Bitcoin, Lightning Network, Payment Channel, Lifespan, Random Walk.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' !' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 1 INTRODUCTION B ITCOIN is the first decentralized cryptocurrency, in- troduced in 2008 which provides security, anonymity, transparency, and democracy without any trusted third party [1].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Most of these properties are achieved by using a blockchain as a distributed ledger.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' An inherent problem with using a blockchain over a network is that it sacrifices scalability [2], [3].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The reason is that all nodes, potentially tens of thousands, must exchange, store, and verify each and every transaction in the system [4].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Furthermore, each block has a limited size and blocks get generated at regular intervals (approximately every 10 minutes).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This means that with the current blocksize of 1 MB the throughput of Bitcoin is about 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 transactions per second, which is much slower than centralized systems like Visa, WeChatPay, and PayPal [5];' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' making the use of Bitcoin in everyday transactions impractical.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Another trade-off the Bitcoin consensus makes is that it ensures security by waiting for other miners to confirm a transaction by extending the block holding that transaction, which reduces the throughput.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This way it makes sure that the double spending attack is highly improbable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Currently, the standard waiting time for a block to be confirmed is 6 blocks, which is almost one hour [6].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Bitcoin’s capacity limitations are being felt by users in the form of increased transaction fees and latency.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' With an increasing demand for making transactions, users need to pay more transaction fees in order to make sure that their transaction is more profitable for the miners;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' hence have a higher chance of making it into a block.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Queuing of transactions and network bandwidth will lead to a longer delay time for a transaction to appear in the blockchain.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' There are many different proposals to solve the scala- bility problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Most of the proposals fall into three cate- gories: Layer0, Layer1, and Layer2 solutions [7].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Layer0 solutions try to enhance the infrastructure, like the network that connects the nodes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Layer1 solutions try to enhance the blockchain’s shortcomings by changing the consensus mechanism and protocols [8], [9].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Layer2 solutions propose ways to move away from the blockchain, and for this reason, they are also called off-chain solutions [10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In 2016 the idea of Lightning Network (LN) was pro- posed to move the transactions to the second layer (off- chain) [4].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The Lightning Network consists of payment channels in a P2P fashion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Payment channels allow two parties to exchange payments with negligible time and cost, but both parties must freeze an initial fund in the channel so no one can spend more money than they own and no double spending occurs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It is important to note that the sum of funds in each channel remains constant throughout the channel’s lifespan and only the channel’s balance changes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' When two parties that do not have a direct channel want to exchange payments they can use other parties to route their payments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So a network of nodes is constructed and all the connected nodes can send each other payments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This system moves the cost of submitting a transaction off the blockchain.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Only the final states between two nodes will eventually make it into the blockchain, which signifi- cantly increases throughput.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Furthermore, no time is needed for the transaction to be confirmed and all transactions in a channel happen almost instantly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' After several transactions through a channel, the channel starts to get unbalanced;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' meaning all of its funds have gone to one of the parties and the other node cannot route any more payments through the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this case, it is best to close the unbalanced channel or open a new one.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this paper, we investigate the expected effective lifes- pan of a channel in a payment network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Our contributions can be summarized as follows: We provide simulation evidence of how channel unbalancing impacts its throughput.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Moreover, we show how the performance of the payment network arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='01240v1 [cs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='DC] 11 Sep 2022 2 can be affected if a number of channels become unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We present a mathematical model of payment chan- nels to predict the expected time for a channel to get unbalanced considering the channel’s position in the network and its initial balance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We call this time the Effective Lifespan of the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We evaluate our model through simulation, and observe how the Effective Lifespan of a channel is affected if we change any of its characteristics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' By analyzing a recent snapshot of the Lightning Net- work, we find the distribution of real-world chan- nel lifespans and its correlation with the network’s topological parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We also investigate the rela- tionship between the centrality of a channel in the network and its effective lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 2 RELATED WORK While the LN white paper [4] does not discuss channel re- balancing, there exists some research on channel balances and their significance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The importance of channel balances is mainly discussed in four major areas;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' re-balancing, security, performance, and financial.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Re-balancing: [11] proposes a method for re-balancing payment channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This work allows arbitrary sets of users to securely re-balance their channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' However, this paper does not discuss the application of re-balancing, and how frequently it should be performed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [12] also proposes meth- ods for rebalancing LN channels, but does not discuss the frequency of rebalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Performance: In [13] the authors discuss why it is in the best interest of the network to have balanced channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' They propose a method to re-balance some channels to improve the network’s performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [14] presents a method in which a node can make its channels balanced through circular subgraphs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It also develops a method for measuring imbalance in a payment network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Security: There has been some research on the security aspects of channel unbalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In [14], [15], and [16] the authors describe a method in which it is possible for an adversary to uncover channel balances.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Having unbalanced channels poses the threat of griefing attacks.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The incentive for honest behavior in the LN channels is the penalty for misbehavior.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' If a node cheats by publishing an old contract, it will be penalized and all of the channel funds can be claimed by the victim.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' When channels are unbalanced the penalty is less so there is less incentive for honest behav- ior.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In [17] the authors discuss some countermeasures like watchtowers to keep the misbehaving nodes from closing the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Financial: Routing payments through a channel can make revenue for the owner.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So payment channels can be looked at as investments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In [18] the authors do an in-depth financial analysis on how much should payment channels charge for routing payments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' One of the key factors in this analysis is the lifespan of payment channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In order to analyze investing in a payment channel, nodes should be able to have an estimate on how long the investment stays profitable and what is the impact of channel unbalancing on the profits of a channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Branzei et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [18] assume an equal probability of having a payment from each side in a channel and use the lifetime of channels for financial analyses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We will show how the lifespan of a channel could be affected by this probability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this paper we focus on the details of estimating chan- nel lifespans;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' considering parameters such as the placement of the channel in the topology and payment rates between each pair and explain the importance of estimating channel lifespans.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This gives us a better and more realistic estimation of the channel’s lifespan compared to existing work.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' More- over, we measure the impact of imbalanced channels on the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Despite the importance of payment channel’s lifespan, to the best of our knowledge, the expected lifespan of channels in the payment network has not been discussed in detail.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 3 TECHNICAL BACKGROUND In this section, we provide a technical background to under- stand the remainder of this paper thoroughly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Payment Channels Payment channel is a financial contract between two parties in a cryptocurrency like Bitcoin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The contract allocates a balance of funds from both parties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The contract is estab- lished by a 2-of-2 multisignature address which requires the cooperation of both parties to spend the funds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Payments are made off the blockchain by passing on a new version of the contract with a different balance of allocated funds on the spending transaction;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' which both parties have to sign.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The channel is closed when one of the parties publishes the latest version of the contract to the blockchain.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We define the payment direction to be the direction in which funds are moving during a transaction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this paper, we call the sum of locked funds in a channel the channel’s capacity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' When all of the funds of a channel are allocated to one of the parties, the channel becomes unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this case payments can only be made from one side of the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' A channel’s effective lifespan is the time from creation of a channel until the first imbalance occurs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' A channel’s success probability is defined as the number of successful payments made through the channel divided by the total number of payment attempts.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Several connected payment channels can form a pay- ment network, in the case of Bitcoin, this network is called the Lightning Network [4].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This network is used to route payments through intermediate channels between nodes who do not have a direct channel between them.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We de- fine a network’s success probability as the total number of successful payments made on the network divided by the total attempts to route payments through the network [19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Random Walk The random walk model has been used in a wide variety of contexts to model the movement of objects in different spaces.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This paper uses one-dimensional random walk to model the liquidity balance in a payment channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Two endpoints on the left and right sides of the random walk are assumed to represent the channel imbalance condition.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 3 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Relation of network success rate with percentage of unbalanced channels in the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In our model, each payment corresponds to one step of the random walk model, and the direction of the payment determines the direction of that step.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Suppose we take prob- abilities p and 1 − p as the probability of payment direction (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=', step direction).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We can find the expected number of payments (steps) needed for the channel (the random walk model)to get unbalanced (to reach one of the endpoints).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Betweenness Centrality Betweenness centrality is a measure based on shortest paths for the importance of the location of a node or an edge in a graph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Betweenness centrality for an edge(a, b) in the network is defined as follows: � s,t∈V s̸=t σ(s,t|edge(a,b)) σ(s,t) , where σ(s, t) is the total number of shortest paths between nodes s and t and σ(s, t|edge(a, b)) is the total number of shortest paths between s and t that pass through edge(a, b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 4 MOTIVATION One of the important characteristics of a payment network is reliability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Reliability can be defined as the probability of payment success [19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this section, we analyze the payment routing failure probability of a singular channel after unbalancing, and the network’s success probability of routing a payment when some channels are unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Singular Channel We ran a simulator of a single payment channel to see how much the failure rate increases after the first time that the channel becomes unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 2 shows the failure rate after the first time a channel becomes unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' During the simulation, 5000 payments were being routed through an initially balanced channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Then the simulator calculates the failure rate after the first time the channel becomes un- balanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 2 suggests, the probability of the direction of payments (p) is a key factor in determining how much the probability of payment success degrades after the first imbalance occurs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Channels capacity has little to no impact on how well it performs after unbalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' These results show that the probability of payment di- rection (p), which depends on the network topology and Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Failure rate after unbalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' the network’s transaction flow, is one of the most impor- tant parameters in determining the channel’s lifespan;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' more importantly, shows the impact of unbalancing on channel success probability after the channel becomes unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Network Performance Using the CLoTH simulator [19] we simulate and measure the performance of Lightning Network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In each iteration we take channels from the given LN snapshot and make them unbalanced, we then measure the success probability after attempting 5000 payments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Choosing more central channels as unbalanced channels is more reasonable, because they route more payments and thus have a higher probability of becoming unbalanced in the real world.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We considered two scenarios for selecting channels to unbalance: choos- ing channels randomly and choosing channels that have a higher betweenness centrality.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As illustrated in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 1, as the percentage of unbalanced channels increases, the routing success rate decreases dramatically for both channel selection scenarios.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In the random selection scenario, it is noticeable that the first 10 percent of unbalanced channels have less effect on the network performance than the last 10 percent of unbalanced channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We see that unbalancing channels with a higher betweenness centrality has a higher impact on the network performance in contrast with the random selection scenarios.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Therefore, per any percentage of unbalanced channels, selection with betweenness centrality is more effective.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Seres et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [20] suggest that in the Lightning Network, the top 14% central channels will have the most significant impact on the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In a different experiment we made 15% of the network’s channels unbalanced, we first sort the channels by betweenness centrality and take a window of 15% of the channels per experiment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We start with the 15% most central channels and move all the way up to 15% least central channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It can be inferred from the results in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 3 that more central channels have more impact on the network success rate when they become unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As we can see in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 3, the top 15% central channels have the most significant effect on the success rate when they become unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This confirms the result from Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 100 Random 90 Most central 80 rate 70 Success 60 50 40 30 20 20 40 60 80 100 Percentage of initialy unbalanced channels0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='40 Capacity: 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Msat Capacity: 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='8 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='35 Capacity: 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Capacity: 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='30 Capacity: 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='20 Fal 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='15 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='10 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='05 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='300 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='325 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3500.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3750.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='400 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='425 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='450 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='475 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='500 probability of payment direction4 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Per each data point the i-th to (i+4500)-th most central channels are unbalanced and the success rate of the network is measured.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The total number of channels is 30457.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5 THE MODEL As we discussed in Section 4 channel balances have a sig- nificant effect on both channel, and network performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this section, we introduce a mathematical model to deter- mine the expected time for a channel to get unbalanced;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' we call this the channel’s expected lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We model the dynamics of a payment channel with a random walk problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Each payment passing through the channel will represent a step the random walker takes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We will first discuss our assumptions and describe the model in detail.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We then discuss how to find the model parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We proceed by doing an analysis on how the expected lifespan is affected by changing channel’s characteristics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Random Walk Model Take a payment channel between two nodes A and B, and take their initial balance allocated for the channel to be FA and FB, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The goal is to determine the expected time it will take for this payment channel to become unbal- anced for the first time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We make the following assumptions: All the payments have the same amount denoted with ω (PaymentSize).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The payments from each node come with a Poisson distribution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Since the number of nodes is large and the probability of sending a transaction for a given time is small, we can assume that transaction arrival for each channel is a Poisson process for moderate time windows [21].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Although the dynamics of the network will change over time, we make the assumption of having a fixed topology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We model the dynamics of a payment channel with a random walk problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Each payment is simulated by a step the random walk takes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' To simulate a payment channel, take the liquidity of node A as the distance of the random walk from the endpoint on the right hand side and the liquidity of node B as the distance from the endpoint on the left hand side.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The payment direction determines the direction of that step.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So the payment direction probability is the probability of going to the right or left for the random walk in each step.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Distribution of expected lifespan with 10000 random walk simula- tions with p = 1 2 and a = b = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Let the random walk start at the origin of the number line.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The two endpoints a and −b are ⌊ FA ω ⌋ and ⌊ FB ω ⌋, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Since we assume that the payments from each side are made independently with a Poisson process,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' and the sum of two independent Poisson processes is itself a Poisson process,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' we can say that payments come to the channel with a Poisson distribution having: λpayment = λA,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='B + λB,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='A,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (1) thus the relation between expected time and expected num- ber of random walk steps is: Etime = Esteps λpayment ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (2) where Etime is the expected time until unbalancing and Esteps is the expected number of steps until unbalancing occurs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The expected number of payments until unbalancing occurs, can be a better metric depending on the application;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' when multiplied by average fee per payment, it gives the expected routing income, and when divided by λ it gives the expected lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The objective is to determine the time it takes for a channel to become unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We first try to find the expected number of steps needed for the random walker to reach +a or −b for the first time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Lemma 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The expected number of steps to reach +a or −b for the first time starting from zero considering the probability p for the positive direction and q = 1 − p for the negative direction is: Esteps = � apa(pb−qb)+bqb(qa−pa) (p−q)(pa+b−qa+b) p ̸= 1/2 ab p = 1/2 (3) .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We provide the proof of Lemma 1 in Appendix A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We simulated a Random Walk which starts from point zero with the same probability of going to each side (p = 1 2).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The simulation ran 10000 times to find the distribution of the number of steps needed to reach +a or −b.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 4 illustrates the result of the simulation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We can observe that most of the times the random walk reaches one of the bounds in less than 400 steps, but there are not many situations where 98 96 Success rate 94 92 90 88 86 0 5000 10000 15000 20000 25000350 300 250 count 200 150 100 50 0 0 500 1000 1500 2000 2500 3000 number of steps5 it takes a huge number of steps to reach these bounds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' However, the average number of steps needed to reach these bounds is 400.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 confirming 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Finding p In Section 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 we modeled the payment channel dynamics with a random walk and a parametric formula was con- structed according to Lemma 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' A payment network can be formally expressed by an unweighted directed graph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' V represents the set of all nodes, and the set of edges is denoted by E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Each channel is represented using two edges from E each for one of the directions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We define MRates to be the matrix of payment rates between each two nodes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The rate of payments (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=', number of payments per day) from node i to node j is denoted by MRatesij.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' λa,b represents the rate of payments transmitted over the edge(a, b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' λa,b consists of the sum of portions of the payment rate between each pair of nodes that pass through edge(a, b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So we have: λa,b = � s,t∈V s̸=t σ(s, t|edge(a, b)) σ(s, t) MRatesst, (4) where σ(s, t) is the number of shortest paths from node s to node t and σ(s, t|edge(a, b)) is the number of shortest paths from node s to node t passing through edge(a, b) in the directed graph G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' p q = λ(a,b) λ(b,a).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' According to Lemma 2: p = λ(a, b) λ(a, b) + λ(b, a) (5) Therefore we can find p based on the network topology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Lemma 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' If ∀s, t ∈ V : MRatesst = MRatests then p = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We provide the proofs of Lemmas 2 and 3 in Appendix A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' If we assume that MRates is a symmetric matrix, according to Lemma 3, p is independent of MRates matrix and the network topology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3 Model Analysis In this section we analyze the effect of channel parameters on the channel’s expected lifespan and perform a financial analysis for channel lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' For more realistic parameter values we used a recent snapshot of the Lightning Network taken on Feb2019 as a reference point.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The average payment size is considered to be 60000 sat1 [22] and the average channel capacity is considered 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 Msat2 according to the snapshot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' For simplicity we use ”lifespan” and ”expected number of payments until channel is unbalanced”, interchangeably.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' satoshi 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' million satoshi Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Effect of payment direction probability on balanced channels, according to different channel capacities.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The effect of payment direction probability on expected number of payments, according to different initial balance ratios.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The channel capacity is considered 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We first answer the question of how sensitive is a channel’s lifespan to the changes in p.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As demonstrated in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 5;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' if the channel is initially balanced, the maximum lifespan happens on p = 1 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Also, lifespan is more sensitive to changes in p when the capacity is higher.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' From this result we can infer that it is an important consideration for a node to make sure the channel is placed in a way that p is close to 1 2, otherwise the channel’s lifespan is affected dramatically.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' A reasonable proposal for nodes who want to keep their channels active as long as possible is to charge routing fees in a way that encourages other nodes to route their payments through the node in order to achieve p = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6 shows that if a channel is initially unbalanced, its maximum possible lifespan takes a hit.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Although the maximum lifespan does not occur at exact p = 1 2, it occurs at a point close to this value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So even if a channel is somewhat unbalanced, the nodes must try to keep p as close as possible to 50%.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We now answer the question of how the lifespan is affected by the channel capacity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 7 suggests, the channel lifespan increases with increasing its capacity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It is noteworthy that the slope of this graph is increasing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' So if a node doubles its channel capacity, the channel’s lifespan will be more than doubled.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Moreover, Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 7 shows the effect of a channel’s initial imbalance on its lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Usually when a node wants to create a new channel Capacity: 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='80 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 600 Capacity: 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='40 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Capacity: 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='00 Msat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 500 400 300 200 100 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='8 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 Probability (p)400 a/b: 1 a/b: 5 350 a/b: 50 300 250 200 150 100 50 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='8 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 Probability (p)6 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Effect of channel capacity on the expected number of payments, according to initial balance ratios Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' For a fixed a = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Msat, the effect of channel b’s capacity on the maximum possible lifespan in any p.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' with another node in the network, the only parameter it has control over is the amount of funds it wants to put in the channel, not the funds its partner puts in the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This brings up the question: how will the channel’s lifespan be affected with the amount the other node wants to put in the channel if our fund stays at a fixed value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Figures (8) and (9) illustrate this effect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 8 shows the maximum achievable lifespan considering any p value and how it is affected by the fund that the other node commits to the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The maximum lifespan grows with the initial fund of the other edge in a linear fashion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 9 illustrates the effect of our edge capacity if the peer node’s capacity is fixed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Figure (9) shows that if p is in favor of payments in the direction of our edge (p ≥ 1 2), the lifespan increases almost linearly;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' otherwise (p < 1 2), the other edge becomes the bottleneck and the fund we put towards the channel will have little to no effect on the expected lifespan of the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' If the funds we put towards the channel do not have an effect on the channel’s lifespan, we have wasted cost opportunities.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6 IMPLEMENTATION AND EVALUATION We provided a simulation proof of concept on a constructed Lightning Network to show the accuracy of the model discussed in Section 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this section we describe our methodology for creating data and calculating accuracy of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Having a fixed initial balance from peer node (b) analyzing the effect of our initial balance fund (a), according to different payment direction probabilities (p).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' our model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We later analyze the results to see under which conditions the model performs better.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Methodology The testing pipeline shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 10 uses the following modules: 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Network Generator For each test, a random network was generated using Net- workX’s [23] gnp random graph with the number of nodes being 50 and the channel existence probability being 20% (245 edges on average).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Mrates Generator As discussed in previous sections the Mrates matrix holds the rates in which each two nodes send payments to one another.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The Mrates generator takes two main parameters: SC and SK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' SC determines the sparseness of the Mrates matrix and SK determines the matrix skewness in relation to its main diagonal.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Per each test, a new matrix is generated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In table (1) the sparse coefficient and the skew were changed to test how the model will perform in each scenario.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3 Lifespan Predictor The lifespan predictor takes the network and the Mrates matrix and using the model discussed in 5 gives the ex- pected time for each channel to become unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 Payment Generator Payment generator creates random payments in CLoTH simulator’s input format [19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' These payments follow the Mrates generator values on average.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 Simulator We used a modified version of the CLoTH simulator [19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We modified CLoTH such that the simulator logs the un- balancing of channels and chooses paths randomly in cases where more than one shortest path exists.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The payment generator and simulator run 100 iterations per test.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 10000 a/b: 1 f Payments a/b: 5 a/b: 50 8000 6000 4000 2000 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='8 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Capacity (sat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=') 1e7Maximum Expected Number of Payments 5000 4000 3000 2000 1000 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='8 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Other Edge Capacity (sat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=') 1e7800 p: 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='40 p: 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='45 700 p: 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='50 600 p: 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='55 p: 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='60 500 400 300 200 100 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 Edge Capacity (sat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=') 1e67 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Model evaluation pipeline.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' TABLE 1 error of prediction and real lifetime SK 1 4 6 10 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='9 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='15 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='10 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='09 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='10 SC 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='11 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='10 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='08 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='07 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='09 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='07 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='05 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='06 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='11 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='07 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='07 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='07 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 Lifespan Calculator This module aggregates the results of 100 iterations of the previous step and calculates the average lifespan and its error.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This data will be used to determine the accuracy of the model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='7 Model Evaluation The error of each channel is calculated as |real−prediction| real .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Because some channels are positioned in a way that almost no payments pass through them, only after a long while that most channels are unbalanced, some payments pass through them, we count these channels as abnormalities and do not consider them in the error calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' These are usually the channels that are estimated to have a very long lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The means of calculated errors are given in Table (1) considering different SC and SK values.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As we see, better results are obtained with smaller SCs (meaning a busier Lightning Network).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It is also notable that SK value has little to no effect on the model performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This means that the model performs well in either case that p is close to 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5 and p is far from 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 7 LIGHTNING NETWORK ANALYSIS In this section we will provide an analysis on channel lifespans of a recent snapshot of the Lightning Network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The simulation is constituted by nodes and channels taken from a snapshot of the Lightning Network Mainnet [24] on Feb 2019.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In Section 5, we proposed a model for a payment channel using a random walk and we derived a formula to predict expected channel lifespans.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Moreover, the expected lifespan of a payment channel can be found if the rate of payments are known by using 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Lemma 3 shows that if we have the same rate for every pair of nodes, the probability of going to each side is equal to 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Because payment rates and channel balances usually are not public in the Lightning Network, we have to make assumptions on the distribution, the amount of payments, and channel balances.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We assume that all payment rates have the same value r, which means that the rates matrix (MRates) is symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Thus according to Lemma 3, p = 1 2 for every channel in the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' According to 11 the expected number of payments is equal to a × b, where a = ⌊ FA ω ⌋ and b = ⌊ FB ω ⌋ for a bidirectional channel between A and B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We assume that all channels are initially balanced, meaning a = b = C 2ω , where C is the channel’s capacity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' According to previous results in Section 5 (equations (1) and (4)) we have: λpayment = ( � s,t∈V s̸=t σ(s, t|edge(a, b)) σ(s, t) + σ(s, t|edge(b, a)) σ(s, t) )r (6) We also know that � s,t∈V s̸=t σ(s,t|edge(a,b)) σ(s,t) is equal to the edge betweenness centrality of edge(a, b) (EBC(a, b)) in directed graph G [25].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Because all channels are bidirectional: ∀edge(j, i) −→ ∃edge(i, j), thus ∀s, t ∈ V : σ(s, t|edge(a, b)) σ(s, t) = σ(t, s|edge(b, a)) σ(t, s) .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (7) Assuming G ′ as an undirected graph that is derived from G we have: EBCG(a, b) = EBCG′ (a, b), (8) thus λpayment = 2 × EBCG′ (a, b) × r.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (9) If we put all results in (2), we have: Etime = ( C ω )2 4 × 2 × EBCG′ (a, b) × r (10) In what follows, we first calculate all payment channels’ lifespans in the LN snapshot using equation (10).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Then we focus on the relation between edge betweenness centrality and lifespan of the channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Distribution of Channels Effective Lifespan Equation (10) shows that the lifespan of a channel can be calculated based on its edge betweenness centrality and initial fund.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We assume that r = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0022 transactions per day [26] and ω = 60000 sat [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The distribution of channels lifespans in our snapshot is shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Much like the distribution of channel capacities that resemble the Power Law distribution, Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 11 shows that there are a lot of channels with a low lifespan and very few channels with a very high lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' According to Seres et.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [20] the most effective channels are the channels with the highest betweenness centrality.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This paper suggests that the top 14% of the channels have the most significant effect on the network’s performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Table (2) gives average, standard deviation, and median, for all channels in the network and the top 14% central channels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' network generation MRates generation payment generation loop for 100 run lifespan prediction simulation lifespan calculation model evaluation8 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Histogram of expected lifespan for the LN snapshot in Feb 2019.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' TABLE 2 Lifespan statistics of the LN snapshot (day).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' All Channels Central Channels average 1833.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 172.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3 STD 7086.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='9 587.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 median 27.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='6 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Betweenness-Lifespan Correlation As Seres et.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' [20] suggests, the most central channels have the most impact on the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' As Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 12 shows, more central channels have a shorter lifespan because they route more payments per unit of time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 12 we took batches of the most central edges and calculated the average cen- trality and the average lifespan per batch.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The result shows that in general the more central a channel is, the sooner it will get unbalanced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We see an exception to this statement in the middle of the plot, where betweenness has a positive correlation with the average lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This is due to the fact that some very central edges have a large capacity so they can route more payment considering that lifespan increases with capacity quadratically.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In Section 7 A we showed that channels with larger edge betweenness centrality values have a higher impact on the performance of the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' In this section, we have shown these central channels will have shorter lifespans.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Therefore, the network success rate will decrease quickly Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The relation between expected lifespan and betweenness cen- trality of channels in the LN snapshot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' due to unbalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' 8 CONCLUSION In this paper we modeled payment channel liquidity with a random walk to estimate how long it takes for a channel to become unbalanced and the effect of being unbalanced on a channel’s probability of successful routing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We also analyzed how unbalanced channels degrade the network’s performance, and the relation between a channel’s centrality and its lifespan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We showed that the network’s success probability is sensitive to the channels’ unbalancing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We also introduced a method to estimate the lifespan of a channel in a payment network which can be used for determining a good placement in the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We provided a proof of concept for our model and showed the results are 95% accurate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' This work shows that just allocating more funds towards a channel does not lead to having a more successful channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The results show the channel’s success in the network depends greatly on the network topology, transaction flow, and the amount of funds the peer node puts in the channel.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We suggested the amount a node should invest in a channel to get the longest channel lifespan and maximize its return on investment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' These results show that a misplaced channel can have a very short lifespan and lose up to 40% of its efficiency, so nodes could potentially create a market based on these criteria to sell each other good connections in the network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' APPENDIX A PROOFS A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 Lemma 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The expected number of steps to reach +a or −b for the first time starting from zero is Esteps = � apa(pb−qb)+bqb(qa−pa) (p−q)(pa+b−qa+b) p ̸= 1/2 ab p = 1/2 (11) Consider Sx as the expected number of steps to reach +a or −b for the first time starting from x.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Let p be the probability of going to the positive direction and q the probability of going in the negative direction (p + q = 1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Then we can say that if the Random Walk starts from x, he will go to x + 1 with probability of p and x − 1 with probability of q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' so we can infer this recurrence equation: sx = 1 + qsx−1 + psx+1 where sx is the expected number of steps until reaching the end point starting from point x.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' For the boundary conditions we have: sa = s−b = 0 implying that the expected number of steps needed to reach +a or −b starting from +a or −b is zero.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='so: ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='sx = 1 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='psx−1 − q ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='psx−2 − 1 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='p ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='(12) ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='The characteristic equation of (12) is: ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='(z2 − 1 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='pz + q ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='p)(z − 1) = 0 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='(13) ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='104 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='103 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Count ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='102 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='101 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='100 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='25000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='50000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='75000100000125000150000175000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Lifespan (day)1750 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1500 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1250 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='750 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='500 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='250 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='0 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='10000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='15000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='20000 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Average Edge Betweenness Centrality of Batch9 ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='if p = q = 1/2 we have ∆ = 0 therefore z1 = z2 = z3 = ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1 so the expected number of steps needed to reach +a or −b ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='starting from x is: ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='sx = (a − x)(b − x) ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='(14) ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='if p ̸= 1/2 we have ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='√ ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='∆ = | 1−2p ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='p ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='| therefore z1 = z2 = ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' z3 = q p and for the number of steps we have: sx = apa+b + bqa+b (2p − 1)(pa+b − qa+b) + 1 1 − 2p x+ (a + b)paqb (2p − 1)(qa+b − pa+b) ( q p )x (15) we take x = 0 as this gives the expected number of steps to reach +a or −b starting from zero.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' so we have: S0 = � apa(pb−qb)+bqb(qa−pa) (p−q)(pa+b−qa+b) p ̸= 1/2 ab p = 1/2 (16) A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='2 Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' p q = λ(A,B) λ(B,A) In assumptions of Section 5 it is assumed that each node sends its payments to other nodes with a Poisson distri- bution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The parameter of the distribution for edge(a, b) is λ(a, b), which is the payment rate between nodes a and b.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Assume the random variable of payments from a to b as X and the random variable of payments from b to a as Y .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Thus we have: P(X = n) = e−λ(A,B)(λ(A, B))n n!' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (17) The total payment rate in each channel is the sum of rates of its two edges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' It is known that the distribution of a random variable which is the sum of two random variables with a Poisson process is a Poisson process;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' the rate of this process equals the sum of rates.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' When we have a payment from two Poisson distribu- tions sending payments to the same channel;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' The probabil- ity for the payment to be a payment from node a to node b (p) is: p = P(X = 1|X + Y = 1) = e−λx(λx)1 1!' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' × e−λy (λy)0 0!' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' e−(λx+λy)(λx+λy)1 1!' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' (18) Thus: p = λx λx + λy = λ(a, b) λ(a, b) + λ(b, a) (19) A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='3 Lemma 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' If ∀s, t ∈ V : MRatesst = MRatests then p = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' We know from lemma 2 that: p q = λ(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='b) λ(b,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='a) so we have: p q = � σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='t|edge(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='b)) σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='t) MRatesst � σ(t,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='s|edge(b,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='a)) σ(t,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='s) MRatests (20) Because all channels are bidirectional(∀edge(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' b) : ∃edge(b,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' a)) we have ∀s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t ∈ V : σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t|edge(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' b)) σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t) = σ(t,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' s|edge(b,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' a)) σ(t,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' s) (21) In the other hand if we have ∀s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t ∈ V : MRatesst = MRatests,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' we can say: σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t|edge(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' b)) σ(s,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' t) ×MRatesst = σ(T,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' S|edge(b,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' a)) σ(t,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' s) ×MRatests (22) then finally we have: λ(a,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' b) = λ(b,' metadata={'source': 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'/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Research, “The growth of the Lightning Network,” https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='research.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='arcane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='no/blog/ the-growth-of-the-lightning-network, 2021, [Online;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' accessed 11-Nov-2021].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Soheil Zibakhsh Shabgahi received his bach- elor’s degree in Computer Engineering from the Department of Electrical and Computer En- gineering, University of Tehran, Tehran, Iran.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' He is currently a research assistant at the Data lab under the supervision of professor Behnam Bahrak.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' His research interest are in blockchain systems, Theoretical Computer Sci- ence,distributed systems, and Machine Learn- ing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Seyed Mahdi Hosseini is currently an under- graduate student majoring in computer engi- neering at the School of Electrical and Computer Engineering at the College of Engineering of the University of Tehran.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' His research interest consists of blockchain, system networks, and distributed systems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Seyed Pooya Shariatpanahi received the B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Sc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=', M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='Sc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=', and Ph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' degrees from the De- partment of Electrical Engineering, Sharif Uni- versity of Technology, Tehran, Iran, in 2006, 2008, and 2013, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' He is currently an Assistant Professor with the School of Electri- cal and Computer Engineering, College of En- gineering, University of Tehran.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Before joining the University of Tehran, he was a Researcher with the Institute for Research in Fundamental Sciences (IPM), Tehran.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' His research interests include information theory, network science, wireless communications, and complex systems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' He was a recipient of the Gold Medal at the National Physics Olympiad in 2001.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' Behnam Bahrak received his bachelor’s and master’s degrees, both in electrical engineering, from Sharif University of Technology, Tehran, Iran, in 2006 and 2008, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' He received the Ph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content='D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' degree from the Bradley Department of Electrical and Computer Engineering at Vir- ginia Tech in 2013.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} +page_content=' He is currently an Assistant Professor of Electrical and Computer Engineer- ing at University of Tehran.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/-9AzT4oBgHgl3EQfS_sw/content/2301.01240v1.pdf'} diff --git a/-NFRT4oBgHgl3EQfrTfI/content/2301.13620v1.pdf b/-NFRT4oBgHgl3EQfrTfI/content/2301.13620v1.pdf new file mode 100644 index 0000000000000000000000000000000000000000..a516d20c3ee24cf95ed473a134ff05d535030cb6 --- /dev/null +++ b/-NFRT4oBgHgl3EQfrTfI/content/2301.13620v1.pdf @@ -0,0 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SEMIDEFINITE MATRIX POLYNOMIALS +SARAH GIFT AND HUGO J. WOERDEMAN +Abstract. A real symmetric positive semidefinite matrix polynomial Q(x) with square determinant that +is not identically zero can be factored as +Q(x) = G(x)T G(x) +where G(x) is itself a real square matrix polynomial with degree half that of Q(x). We provide a constructive +proof of this fact, rooted in finding a skew-symmetric solution to a modified algebraic Riccati equation +XSX − XR + RT X + P = 0, +where P, R, S are real n × n matrices with P and S real symmetric. +Keywords Positive semidefinite matrix polynomial, Algebraic Riccati equation, Matrix factorization +MSCcodes 47A68 (Primary), 46C20, 15A48, 93B05 +1. Introduction +The Fej´er-Riesz factorization was first shown for matrix polynomials by Rosenblatt [19] and Helson [14]. In +particular, given a matrix polynomial Q(x) = �2m +i=0 Qixi with Qi Hermitian and Q(x) positive semidefinite +for all x ∈ R, we can factorize it as +Q(x) = G(x)∗G(x) +where G(x) = �m +i=0 Gixi. In 1964, Gohberg generalized this factorization to certain operator-valued poly- +nomials [8]. +Later it was further generalized to operator-valued polynomials in general form [20]. +The +multivariable case has also been studied, e.g. in [17]. For an overview of the work done with the operator- +valued Fej´er-Riesz theorem, see [5]. +In this paper, we provide a constructive proof of the real analog of the Fej´er-Riesz factorization of matrix- +valued polynomials. +In particular, we show that a matrix polynomial Q(x) = �2m +i=0 Qixi with Qi real +symmetric, Q(x) positive semidefinite for all x ∈ R, and det(Q(x)) equal to a nonzero square, admits the +factorization +Q(x) = G(x)T G(x) +where G(x) is itself a real square matrix polynomial with degree half that of Q(x). This result was first +shown by Hanselka and Sinn [13] using methods from projective algebraic geometry and number theory. We +provide an alternative, linear algebraic proof, inspired by the proof of the Fej´er-Riesz factorization presented +in Section 2.7 of [1]. That proof in turn, was taken from [6, 12]. For earlier work on factorizations of real +symmetric matrix polynomials (not necessarily positive semidefinite) see e.g. [18]. +A key part of the Fej´er-Riesz factorization proof we follow requires finding a Hermitian solution to an +algebraic Riccati equation +(∗) +XDX + XA + A∗X − C = 0, +where D and C are Hermitian. Reducing a factorization problem to solving a Riccati equation is a technique +that has been used in many other papers as well (see, e.g., [2], [7], [15, Chapter 19] and references therein). +This technique is useful because Riccati equations have been studied extensively. Early work was done by +Willems [21] and Coppel [3] in analyzing properties of solutions of continuous algebraic Riccati equations. +Another key paper was [4] where Riccati equations were used to solve H∞-control problems. For an in depth +analysis of algebraic Riccati equations, please see the book by Lancaster and Rodman [15]. +Both authors were supported by National Science Foundation grant DMS 2000037 . +1 + +2 +SARAH GIFT AND HUGO J. WOERDEMAN +For the current real factorization problem, we end up needing to find a real skew-symmetric solution to +an equation of the form +(∗∗) +XSX − XR + RT X + P = 0, +where P and S are real symmetric. This is not quite an algebraic Riccati equation of the form eq. (∗) and +thus we call it a modified algebraic Riccati equation. In general, to find a skew-Hermitian solution X, one +often considers instead iX, which is Hermitian; however, we want real solutions and thus this method is +not applicable here. Thus we instead follow the same steps presented in [15] for finding a real symmetric +solution to the real algebraic Riccati equation and amend them to our current situation. This is the topic +of Section 2, which culminates in giving sufficient conditions for a skew-symmetric solution of our modified +Riccati equation eq. (∗∗). In Section 3 we provide additional background on matrix polynomials necessary +for our main result, the real factorization of a symmetric positive semidefinite matrix polynomial, presented +in Section 4. The major advantage of our proof compared to that by Hanselka and Sinn [13] is that ours is +constructive. We end this paper with a couple examples illustrating the construction. +2. A Modified Algebraic Riccati Equation +The goal of this section is to provide necessary and sufficient conditions for which there is a real skew- +symmetric solution X to the modified algebraic Riccati equation +(1) +XSX − XR + RT X + P = 0, +where P, R, S are real n × n matrices with P and S real symmetric. In the book Algebraic Riccati Equations +[15], Lancaster and Rodman show conditions for which there is a real symmetric solution X to the CARE +equation +XDX + XA + AT X − C = 0, +where A, C, D are real n × n matrices with C and D real symmetric. We amend these results to the present +situation. Define the 2n × 2n real matrices +(2) +Mr = +�R +−S +P +RT +� +, +ˆHr = +�0 +I +I +0 +� +, +Hr = +� +P +RT +R +−S +� +. +Then both ˆHr and Hr are real symmetric. Also +ˆHrMr = M T +r ˆHr +and +HrMr = M T +r Hr. +Using terminology from [15], we say Mr is both Hr-symmetric and ˆHr-symmetric. +We can now give a +condition for a real solution of eq. (1) to exist. +Proposition 2.1. X is a real solution of eq. (1) if and only if +G(X) := Im +� +I +X +� +is Mr-invariant. +Proof. If G(X) is Mr-invariant, then +(3) +�R +−S +P +RT +� � I +X +� += +� I +X +� +Z +for some n × n matrix Z. The first block row gives Z = R − SX and the second gives P + RT X = XZ. +Combining the two gives +P + RT X = X(R − SX). +Thus X solves eq. (1). Conversely, if X solves eq. (1), then eq. (3) holds for Z = R − SX and ths G(X) is +Mr-invariant. +□ +More than just a real solution, though, we want a skew-symmetric solution. Thus we next strive to give a +condition for such a solution. For this we first need a definition (see [15]). +Definition 2.1. Let H be a real invertible n × n matrix. A subspace M is called +(1) H-nonnegative if ⟨Hx, x⟩ ≥ 0 for all x ∈ M +(2) H-nonpositive if ⟨Hx, x⟩ ≤ 0 for all x ∈ M + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +3 +(3) H-neutral if ⟨Hx, x⟩ = 0 for all x ∈ M +Proposition 2.2. Let X be a real solution of eq. (1). Then, +(1) X is skew-symmetric if and only if G(X) is ˆHr-neutral. +(2) G(X) is Hr-nonpositive if and only if (XT + X)(R − SX) ≤ 0. +Proof. +(1) Assume X is skew-symmetric. Let y ∈ G(X), so y = +� I +X +� +z for some z ∈ Rn. Then +⟨Hry, y⟩ = zT �I +XT � ˆHr +� I +X +� +z = zT (X + XT )z = 0. +Thus G(X) is ˆHr-neutral. On the other hand, suppose G(X) is ˆHr-neutral. Then for all z ∈ Rn, +zT(X + XT )z = 0, so X + XT = 0. Thus X is skew-symmetric. +(2) G(X) is Hr-nonpositive if and only if for all z ∈ Rn, +� +Hr +� +I +X +� +z, +� +I +X +� +z +� +≤ 0 +zT �I +XT � �P +RT +R +−S +� � I +X +� +z ≤ 0 +zT[P + RT X + XT R − XT SX]z ≤ 0 +zT [XR − XSX + XT R − XT SX]z ≤ 0 +by eq. (1) +zT (XT + X)(R − SX)z ≤ 0 +Thus G(X) is Hr-nonpositive if and only if (XT + X)(R − SX) ≤ 0. +□ +proposition 2.2 shows that in order to get a real skew-symmetric solution X to the equation eq. (1), we need +an ˆHr-neutral subspace G(X) of dimension n. We consider now conditions for such a subspace to exist. For +this we first state a few known results (see [15]). +Definition 2.2. Let A be a square matrix and λi be an eigenvalue of A. We call the sizes of the Jordan +blocks of λi the partial multiplicities of λi. +Theorem 2.1. [15, Part of Theorem 2.6.3] +Let A be a real n × n H-symmetric matrix and the partial +multiplicities of A corresponding to the real eigenvalues are all even. Then there exists an A-invariant H- +neutral subspace of dimension k − p where k is the number of positive eigenvalues of H (counting algebraic +multiplicities) and p is the number of distinct pairs of non-real complex conjugate eigenvalues of A with odd +algebraic multiplicity. +Lemma 2.1. [15, p. 56] Let H be a real symmetric matrix. A real subspace M is H-neutral if and only if +⟨Hx, y⟩ = 0 for all x, y ∈ M. +Proof. This follows from the relation +⟨Hx, y⟩ = 1 +2 (⟨H(x + y), x + y⟩ − ⟨Hx, x⟩ − ⟨Hy, y⟩) . +□ +Now we are ready for the new result. +Lemma 2.2. Let eq. (2) hold with P and S real symmetric. Among the following statements, (iii) =⇒ +(ii) =⇒ (i) +(i) There exists an n-dimensional Mr-invariant Hr-neutral subspace +(ii) There exists an n-dimensional Mr-invariant ˆHr-neutral subspace +(iii) All real eigenvalues of Mr have even partial multiplicities and all imaginary eigenvalues of Mr have +even algebraic multiplicity. +If in addition Mr is invertible, then we also have (i) =⇒ (ii). + +4 +SARAH GIFT AND HUGO J. WOERDEMAN +Proof. By theorem 2.1, if every imaginary eigenvalue of Mr has even algebraic multiplicity (i.e. p = 0), +then an n-dimensional Mr-invariant ˆHr-neutral subspace exists (since ˆHr has n positive and n negative +eigenvalues so k = n here). Thus (iii) =⇒ (ii). Next, since Hr = ˆ +HrMr, it follows by lemma 2.1 that (ii) +implies (i). Finally, if Mr is invertible, ˆ +Hr = HrM −1 +r +and thus (i) implies (ii). +□ +We need one more result before the main theorem of this section. For this result, we first recall a definition +(see, e.g., [15]). +Definition 2.3. Let A ∈ Rn×n and B ∈ Rn×m. The pair (A, B) is said to be controllable if +rank +�B +AB +A2B +· · · +An−1B� += n. +Lemma 2.3. Assume that S ≥ 0 (positive semidefinite) and the pair (R, S) is controllable. Let L be an +n-dimensional Mr-invariant Hr-nonnegative subspace of R2n. Then L is a graph subspace, i.e. +L = Im +� I +X +� +for some real n × n matrix X. +Proof. For L as defined in the statement, write +L = Im +� +X1 +X2 +� +for some real n × n matrices X1 and X2. We shall show that X1 is invertible. First, since L is Mr-invariant, +� +R +−S +P +RT +� � +X1 +X2 +� += +� +X1 +X2 +� +T +for some n × n matrix T . Thus, +RX1 − SX2 = X1T +(4) +PX1 + RT X2 = X2T +(5) +Next, since L is Hr-nonnegative, we know +(6) +�XT +1 +XT +2 +� � +P +RT +R +−S +� � +X1 +X2 +� += XT +1 PX1 + XT +1 RT X2 + XT +2 RX1 − XT +2 SX2 +is positive semidefinite. Let K = ker X1. Since eq. (6) is positive semidefinite, for every x ∈ K, +0 ≤ xT XT +1 PX1x + xT XT +1 RT X2x + xT XT +2 RX1x − xT XT +2 SX2x = −xT XT +2 SX2x. +Since S ≥ 0, X2x ∈ ker S, so +X2K ⊂ ker S. +Then, equation eq. (4) implies +T K ⊂ K. +Consequently, equation eq. (5) gives +RT X2K ⊂ X2K. +All together, we have +RT X2K ⊂ ker S. +By induction, we get +(RT )rX2K ⊂ ker S, +r = 0, 1, 2, . . . +Now for every x ∈ K, + + +S +SRT +... +S(RT )n−1 + + (X2x) = 0 + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +5 +Since (R, S) is controllable, we must have X2x = 0. The only n-dimensional vector x for which X1x = +X2x = 0 is the zero vector (otherwise dim L < n). Thus K = {0} and X1 is invertible. Hence +L = Im +� +I +X +� +, +where X = X2X−1 +1 +and so L is a graph subspace. +□ +Now we put everything together to get sufficient conditions for a real skew-symmetric solution of eq. (1): +Theorem 2.2. Let eq. (2) hold with P and S real symmetric. Assume that S ≥ 0 and the pair (R, S) is +controllable. Then the conditions (i) - (ii) are equivalent and (iii) implies (ii) +(i) The equation eq. (1) has a real skew-symmetric solution. +(ii) There exists an n-dimensional Mr-invariant ˆ +Hr-neutral subspace. +(iii) All real eigenvalues of Mr have even partial multiplicities and all imaginary eigenvalues of Mr have +even algebraic multiplicity. +Proof. The (iii) =⇒ (ii) was part of lemma 2.2. By proposition 2.1 and proposition 2.2, we know that +if X is a real skew-symmetric solution to eq. (1), then G(X) is an n-dimensional Mr-invariant ˆHr-neutral +subspace. +Thus (i) +=⇒ +(ii). +Finally, assume there exists an n-dimensional Mr-invariant ˆHr-neutral +subspace, say L. Since Hr = ˆHrMr, L is also an n-dimensional Mr-invariant Hr-neutral subspace. Clearly +L is an Hr-nonnegative subspace, so by lemma 2.3, L is a graph subspace. Since L = G(X) is Mr-invariant, +X is a real solution of eq. (1) by proposition 2.1. Since L = G(X) is also ˆHr-neutral, by proposition 2.2 X +is skew-symmetric. Thus (ii) =⇒ (i). +□ +3. Matrix Polynomials +Building toward our goal of factorizing a real symmetric positive semidefinite matrix polynomial, we next +state a few relevant results on matrix polynomials (see [11]). +Definition 3.1. For n × n matrices Pi, we define an n × n matrix polynomial P(x) of degree m by +P(x) = +m +� +i=0 +Pixi. +• The matrix polynomial is called real if all Pi are real matrices. +• The matrix polynomial is called monic if Pm = In. +• The matrix polynomial is called self-adjoint if Pi = P ∗ +i , its conjugate transpose, for all i. +• The matrix polynomial is called symmetric if Pi = P T +i +for all i. +• The matrix polynomial is called positive semidefinite (also nonnegative) if for all x ∈ R, P(x) is +positive semidefinite. +• The matrix polynomial is called regular if det(P(x)) is not identically zero. +As in [16], we define the spectrum and Jordan canonical form of a matrix polynomial in the following +ways.1 +Definition 3.2. Let P(x) be a regular matrix polynomial. Then the set of eigenvalues of P, i.e. the spectrum, +is +σ(P) := {λ ∈ C : det(P(λ)) = 0}. +Definition 3.3. Let P(x) be a monic matrix polynomial, i.e. +P(x) = Inxm + +m−1 +� +i=0 +Pixi. +1Note that the partial multiplicities of an eigenvalue of a matrix polynomial are often defined as powers of the elementary +divisors; however, these partial multiplicities are the same as the sizes of the Jordan blocks of our companion matrix. See the +Appendix of [10] for a more in depth understanding of matrix polynomial equivalences, linearizations, partial multiplicities and +elementary divisors. + +6 +SARAH GIFT AND HUGO J. WOERDEMAN +The Jordan canonical form for P(x) is defined to be that of the companion matrix +Cp := + + +0 +In +0 +· · · +0 +0 +0 +In +· · · +0 +... +... +... +... +... +0 +0 +· · · +0 +In +−P0 +−P1 +· · · +−Pm−2 +−Pm−1 + + +Theorem 3.1. [11, part of Theorem 12.8] For a monic self-adjoint matrix polynomial P(x), the following +statements are equivalent: +(i) P(x) is nonnegative. +(ii) The partial multiplicities of P(x) for real points of the spectrum are all even. +In the previous section, we found that if all real eigenvalues of Mr have even partial multiplicities and all +imaginary eigenvalues of Mr have even algebraic multiplicity, then our equation eq. (1) has the desired real +skew-symmetric solution. Thus we now want to connect the eigenvalues of Mr and their partial multiplicities +with the eigenvalues of a monic nonnegative matrix polynomial P(x). For this, we begin with a few definitions +from [11]. +Definition 3.4. Two matrix polynomials M1(x) and M2(x) of size n × n are called equivalent if +M1(x) = E(x)M2(x)F(x) +for some n × n matrix polynomials E(x) and F(x) with constant nonzero determinants. +Definition 3.5. Let P(x) be an n × n monic matrix polynomial of degree m. A linear matrix polynomial +λI − A is called a linearization of P(x) if +(7) +λI − A ∼ +� +P(x) +0 +0 +In(m−1) +� +where ∼ means equivalence of matrix polynomials. +Note that Cp, the companion matrix, is a linearization of P(x). For any linearization λI − A, the partial +multiplicities in every eigenvalue of A and P(x) are the same. Thus to gain results about the multiplicities +of the eigenvalues of Mr, it suffices to show λI − Mr is a linearization of a matrix polynomial P(x). +Lemma 3.1. Let Q(x) = �2m +j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with +Q0 = In. Then for +Mr = + + +− 1 +2Q1 +−In +In +0 +0 +... +... +... +In +0 +0 +Q2 − 1 +4Q2 +1 +1 +2Q3 +− 1 +2Q1 +In +1 +2Q3 +Q4 +... +0 +... +... +... +1 +2Q2m−1 +... +In +1 +2Q2m−1 +Q2m +0 + + +, +we have +λI − Mr ∼ +� +rev Q(λ) +0 +0 +I +� +where +rev Q(x) := +2m +� +i=0 +Q2m−ixi = x2mIn + +2m−1 +� +i=1 +Q2m−ixi. + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +7 +Proof. First permute the rows and columns as follows: +M1:= + + +0 +0 +· · · +0 +In +0 +In +... +0 +0 +... +... +... +... +0 +In +0 +· · · +0 +In +0 +· · · +0 +0 +0 +0 +... +In +0 +... +... +0 +... +... +0 +· · · +0 +In +0 + + +(λI − Mr) + + +In +... +In +0 +0 +In +... +In + + +, += + + +−Q2m +− 1 +2Q2m−1 +0 +λIn +λIn +−In +0 +... +... +... +... +... +λIn +−In +0 +λIn + 1 +2Q1 +In +− 1 +2Q3 +1 +4Q2 +1 − Q2 +λIn + 1 +2Q1 +−In +... +−Q4 +− 1 +2Q3 +λIn +... +... +... +... +... +... +− 1 +2Q2m−1 +−Q2m−2 +− 1 +2Q2m−3 +λIn +−In + + +Define V1, . . . , Vm by +V1 = −Q2m − 1 +2λQ2m−1 +V2 = −1 +2Q2m−1 − λQ2m−2 − 1 +2λ2Q2m−3 +V3 = −1 +2λQ2m−3 − λ2Q2m−4 − 1 +2λ3Q2m−5 +... +Vm−1 = −1 +2λm−3Q5 − λm−2Q4 − 1 +2λm−1Q3 +Vm = −1 +2λm−2Q3 − λm−1Q2 − λmQ1 − λm+1In +Then, multiply M1 on the left by + + +In +�m +i=2 λi−2Vi +�m +i=3 λi−3Vi +· · · +Vm−1 + λVm +Vm +−λm−1(λIn + 1 +2Q1) +λm−1In +· · · +λ2In +λIn +0 +In(m−1) +0 +0 +0 +Inm + +. +Noting that +−Q2m − 1 +2λQ2m−1 + λ +m +� +i=2 +λi−2Vi = − rev Q(λ), + +8 +SARAH GIFT AND HUGO J. WOERDEMAN +we get +λI − Mr ∼ + + +− rev Q(λ) +−In +0 +∗ +... +−In +0 +∗ +In +−In +0 +∗ +... +−In + + +Thus it is evident now that +λI − Mr ∼ +� +rev Q(λ) +0 +0 +I +� +. +□ +4. Real Factorization of Non-negative Matrix Polynomial +We are now ready for the main result. While the following theorem was previously proven by Hanselka +and Sinn [13], we provide a new constructive proof following that of the complex analogue presented in the +monograph by Bakonyi and Woerdeman [1]. +Theorem 4.1. Let Q(x) = �2m +j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with +Q(x) ≥ 0 for all x ∈ R and Q0 > 0. Then det(Q(x)) is a square if and only if there exists an n × n real +matrix polynomial G(x) = �m +j=0 Gjxj of degree m such that +Q(x) = G(x)T G(x). +Proof. First, assume Q(x) = G(x)T G(x). Then det(Q(x)) = det(G(x))2. +On the other hand, assume +det(Q(x)) is a square. Without loss of generality, assume Q0 = In (otherwise, take ˜Q(x) := Q−1/2 +0 +Q(x)Q−1/2 +0 +). +Consider the (m + 1)n × (m + 1)n real symmetric matrix +F0 = + + +In +1 +2Q1 +1 +2Q1 +Q2 +... +... +... +1 +2Q2m−1 +1 +2Q2m−1 +Q2m + + +. +Given an nm × nm real skew-symmetric matrix +X = + + +X1,1 +· · · +X1,m +... +... +Xm,1 +· · · +Xm,m + + , +let +FX = F0 + +� 0 +X +0n +0 +� +− +� 0 +0n +X +0 +� +. +It should be noted that in the above line, the matrix decompositions are different; e.g. the X block and the +−X block overlap in general. We want to solve +Xopt = arg min +rank(FX) +such that FX ≥ 0. +Let +A = + + +0 +In +0 +... +... +In +0 + + ∈ Rnm×nm +and +B = + + +In +0 +... +0 + + ∈ Rnm×n. + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +9 +Then (A, B) is controllable, +� +0 +0 +X +0 +� += +� +0 +0 +XB +XA +� +, +and +� +0 +X +0 +0 +� += +� +0 +BT X +0 +AT X +� +. +Split F0 into four blocks as follows, +F0 = +� In +Γ12 +Γ21 +Γ22 +� +. +Noting ΓT +12 = Γ21 and Γ22 is real symmetric, we can recast the condition FX ≥ 0 as +� +In +Γ12 + BT X +ΓT +12 − XB +Γ22 + AT X − XA +� +≥ 0 +Consider the Schur complement with respect to In, +Γ22 + AT X − XA − (ΓT +12 − XB)I−1 +n (Γ12 + BT X). +Setting this equal to zero, we get the modified algebraic Riccati equation +(8) +P + RT X − XR + XSX = 0 +where +P = Γ22 − ΓT +12Γ12 +R = A − BΓ12 +S = BBT . +Note P = P T and S = ST with S ≥ 0. In this case, the associated Mr matrix is as follows: +Mr = +� A − BΓ12 +−BBT +Γ22 − ΓT +12Γ12 +AT − ΓT +12BT +� += + + +− 1 +2Q1 +−In +In +0 +0 +... +... +... +In +0 +0 +Q2 − 1 +4Q2 +1 +1 +2Q3 +− 1 +2Q1 +In +1 +2Q3 +Q4 +... +0 +... +... +... +1 +2Q2m−1 +... +In +1 +2Q2m−1 +Q2m +0 + + +By lemma 3.1, Mr is a linearization of rev Q(x). Since Q(x) ≥ 0 for all x ∈ R, rev Q(x) = x2mQ +� 1 +x +� +≥ 0 +for all nonzero x ∈ R. By continuity, then rev Q(x) ≥ 0 for all x ∈ R. Then by theorem 3.1, the partial +multiplicities of every real eigenvalue of rev Q(λ) are all even. Since Mr is a linearization of rev Q(x), all +the partial multiplicities of every eigenvalue of Mr and rev Q(λ) are the same, so the partial multiplicities +of every real eigenvalue of Mr are all even. Further, by the non-negativity of rev Q(x), +det(λI − Mr) = det(rev Q(x)) +has all roots of even algebraic multiplicity. In particular, all non-real eigenvalues of Mr have even algebraic +multiplicity. Hence by theorem 2.2, there is a skew-symmetric solution, ˜X of eq. (8). Then since the Schur +complement with respect to In is zero, we know +F ˜ +X = +� +In +Γ12 + BT ˜X +ΓT +12 − ˜XB +Γ22 + AT ˜X − ˜XA +� +≥ 0 + +10 +SARAH GIFT AND HUGO J. WOERDEMAN +and +rank(F ˜ +X) = rank +�� +In +Γ12 + BT ˜X +ΓT +12 − ˜XB +Γ22 + AT ˜X − ˜XA +�� += rank In = n. +If we factorize +F ˜ +X = +� +In +Γ12 + BT ˜X +ΓT +12 − ˜XB +Γ22 + AT ˜X − ˜XA +� += + + +GT +0 +... +GT +m + + +� +G0 +· · · +Gm +� +with G0 = In and Gi, i = 1, 2, . . . , m, real n × n matrices, we have +Q(x) = +�In +xIn +· · · +xmIn +� +F ˜ +X + + +In +xIn +... +xmIn + + += +�In +xIn +· · · +xmIn +� + + +GT +0 +... +GT +m + + +�G0 +· · · +Gm +� + + +In +xIn +... +xmIn + + . +Thus for G(x) = �m +j=0 Gjxj, Q(x) = G(x)T G(x). +□ +theorem 4.1 required Q0 > 0. We can relax this condition as follows. +Corollary 4.1. Let Q(x) = �2m +j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with +Q(x) ≥ 0 for all x ∈ R and Q(x0) > 0 for some x0 ∈ R. Then det(Q(x)) is a square if and only if there +exists an n × n real matrix polynomial G(x) = �m +j=0 Gjxj of degree m such that +Q(x) = G(x)T G(x). +Proof. First, assume Q(x) = G(x)T G(x). Then det(Q(x)) = det(G(x))2. +On the other hand, assume +det(Q(x)) = f(x)2 for some polynomial f of degree m. Consider +P(x) := Q(x0 − x). +Then P(x) is an n × n real symmetric matrix polynomial of degree 2m such that +P(0) = Q(x0) > 0 +and +det(P(x)) = det(Q(x0 − x)) = f(x0 − x)2. +Thus by theorem 4.1, there is an n × n real matrix polynomial H(x) = �m +j=0 Hjxj of degree m such that +P(x) = H(x)T H(x). +Define +G(x) := H(x0 − x). +Then G(x) = �m +j=0 Gjxj is an n × n real matrix polynomial such that +Q(x) = P(x0 − x) = H(x0 − x)T H(x0 − x) = G(x)T G(x). +□ +The proof of theorem 4.1 is constructive. It hinges on finding the real skew-symmetric solution X to the +modified algebraic Riccati equation. Back in Section 2, we found such a solution by constructing an mn- +dimensional Mr-invariant Hr-neutral subspace. Following the proof of Theorem 2.6.2, found in [15], also to +be found in Gohberg, Lancaster, and Rodman’s later book Indefinite Linear Algebra and Applications [9], +we first convert Mr to its real Jordan form +Mr = SJS−1, +where +J = Jr1(λ1) ⊕ · · · ⊕ Jrk(λk) ⊕ J2rk+1(λk+1 ± iµk+1) ⊕ · · · ⊕ J2rk+ℓ(λk+ℓ ± iµk+ℓ). + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +11 +For real eigenvalues λj, where 1 ≤ j ≤ α, we take the first rj/2 columns of S corresponding to the block +Jrj (note we know each rj is even). For any imaginary eigenvalues λj ± iµj with rj even, we do the same. +Finally, we must consider the imaginary eigenvalues λj ± iµj with rj odd. For such an eigenvalues, there +must be an even number of Jordan blocks of odd size (since we know every imaginary eigenvalue has even +algebraic multiplicity). Collect the Jordan blocks together in pairs +Kj = J2rj(λj ± iµj) ⊕ J2rj+1(λj+1 ± iµj+1). +Then take the first rj − 1 columns of S corresponding to J2rj(λj ± iµj), the first rj+1 − 1 columns of S +corresponding to J2rj+1(λj+1 ± iµj+1), along with the following two vectors +(1) The rjth column of S corresponding to J2rj(λj ± iµj) plus the rj+1 + 1st column of S corresponding +to J2rj+1(λj+1 ± iµj+1). +(2) The rj +1st column of S corresponding to J2rj(λj ±iµj) minus the rj+1st column of S corresponding +to J2rj+1(λj+1 ± iµj+1). +Let us illustrate the above ideas in a few examples. The first example is the real eigenvalue case. The second +example is the imaginary eigenvalue case with odd rj. +Example 4.1. Take +Q(x) = +�2x2 + 2x + 1 +−4x2 − 3x +−4x2 − 3x +8x2 + 4x + 1 +� += +�1 +0 +0 +1 +� ++ x +� 2 +−3 +−3 +4 +� ++ x2 +� 2 +−4 +−4 +8 +� +. +Then Mr(x) = SJS−1 for +J = + + +−3 +1 +0 +0 +0 +−3 +0 +0 +0 +0 +0 +1 +0 +0 +0 +0 + + , S ≈ + + +−0.2778 +0.3148 +0.2222 +0.6852 +0.2778 +−0.3704 +0.1111 +0.3704 +−0.1389 +0.3519 +−0.0556 +−0.3519 +−0.1389 +−0.1759 +0.1111 +0.1759 + + . +We have J = J2 (−3) ⊕ J2 (0), so r1 = r2 = 2. Thus we take the 1st column corresponding to the first block +as well as the 1st column corresponding to the second block. + + +−0.2778 +0.2222 +0.2778 +0.1111 +−0.1389 +−0.0556 +0.1389 +0.1111 + + =: +� +X1 +X2 +� +Our invariant subspace is thus +Im +� +X1 +X2 +� += Im +� +I +X2X−1 +1 +� +. +Here we have then +X = X2X−1 +1 += +� +0 +−0.5 +0.5 +0 +� +. +Thus +Fopt = F0 + +� +0 +X +0 +0 +� +− +� +0 +0 +X +0 +� += + + +1 +0 +1 +−2 +0 +1 +−1 +2 +1 +−1 +2 +−4 +−2 +2 +−4 +8 + + . +We factorize as +F = + + +1 +0 +0 +1 +1 +−1 +−2 +2 + + +�1 +0 +1 +−2 +0 +1 +−1 +2 +� +. +Thus +G0 = +�1 +0 +0 +1 +� +, +G1 = +� 1 +−2 +−1 +2 +� +, +G(x) = G0 + xG1. +We can verify Q(x) = G(x)T G(x). + +12 +SARAH GIFT AND HUGO J. WOERDEMAN +Example 4.2. Take now +Q(x) = +�2x2 + 2x + 1 +x2 + 2x +x2 + 2x +13x2 + 4x + 1 +� += +�1 +0 +0 +1 +� ++ x +�2 +2 +2 +4 +� ++ x2 +�2 +1 +1 +13 +� +. +Then Mr(x) = SJS−1 for +J = 1 +2 + + +−3 +√ +11 +0 +0 +− +√ +11 +−3 +0 +0 +0 +0 +−3 +√ +11 +0 +0 +− +√ +11 +−3 + + , S ≈ + + +0.5477 +0 +−0.5477 +0 +0.0913 +−0.3028 +−0.0913 +0.3028 +0.1826 +−0.6055 +−0.1826 +0.6055 +−1.0954 +0 +1.0954 +0 + + . +We have J = J2 +� +3±i +√ +11 +2 +� +⊕ J2 +� +3±i +√ +11 +2 +� +, so r1 = r2 = 1. Thus we take the 1st column corresponding to the +first block plus the 2nd column corresponding to the second block as well as the 2nd column corresponding +to the first block minus the first column corresponding to the second block. + + +0.5477 + 0 +0 − (−0.5477) +0.0913 + 0.3028 +−0.3028 − (−0.0913) +0.1826 + 0.6055 +−0.6055 − (−0.1826) +−1.0954 + 0 +0 − 1.0954 + + =: +�X1 +X2 +� +Our invariant subspace is thus +Im +� +X1 +X2 +� += Im +� +I +X2X−1 +1 +� +. +Here we have then +X = X2X−1 +1 += +� 0 +2 +−2 +0 +� +. +Thus +Fopt = F0 + +�0 +X +0 +0 +� +− +� 0 +0 +X +0 +� += + + +1 +0 +1 +3 +0 +1 +−1 +2 +1 +−1 +2 +1 +3 +2 +1 +13 + + . +We factorize as +F = + + +1 +0 +0 +1 +1 +−1 +3 +2 + + +�1 +0 +1 +3 +0 +1 +−1 +2 +� +. +Thus +G0 = +�1 +0 +0 +1 +� +, +G1 = +� 1 +3 +−1 +2 +� +, +G(x) = G0 + xG1. +We can verify Q(x) = G(x)T G(x). +References +[1] M. Bakonyi and H. J. Woerdeman, Matrix Completions, Moments, and Sums of Hermitian Squares, Princeton Series +in Applied Mathematics, Princeton University Press, 2011, http://www.jstor.org/stable/j.ctt7rp1d. +[2] T. Chen and B. A. Francis, Spectral and inner-outer factorizations of rational matrices, SIAM Journal on Matrix +Analysis and Applications, 10 (1989), pp. 1–17, https://doi.org/10.1137/0610001. +[3] W. A. Coppel, Matrix quadratic equations, Bulletin of the Australian Mathematical Society, 10 (1974), pp. 377 – 401, +https://doi.org/10.1017/S0004972700041071. +[4] J. Doyle, K. Glover, P. Khargonekar, and B. Francis, State space solution to standard H2 and H∞ control problem, +IEEE Transactions on Automatic Control, 34 (1989), pp. 831 – 847, https://doi.org/10.1109/9.29425. +[5] M. A. Dritschel and J. Rovnyak, The operator fej´er-riesz theorem, in A Glimpse at Hilbert Space Operators: Paul +R. Halmos in Memoriam, S. Axler, P. Rosenthal, and D. Sarason, eds., Springer Basel, Basel, 2010, pp. 223–254, https: +//doi.org/10.1007/978-3-0346-0347-8_14. +[6] M. A. Dritschel and H. J. Woerdeman, Outer factorizations in one and several variables, Transactions of the American +Mathematical Society, 357 (2005), pp. 4661–4679, http://www.jstor.org/stable/3845206. +[7] B. A. Francis, A course in H∞ control theory, vol. 88 of Lecture Notes in Control and Information Sciences, Springer- +Verlag, Berlin, 1987, https://doi.org/10.1007/BFb0007371. +[8] I. Gohberg, The factorization problem for operator functions, Izvestiya Akademii Nauk SSSR Seriya Matematicheskaya, +28 (1964), pp. 1055–1082. + +REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS +13 +[9] I. Gohberg, P. Lancaster, and L. Rodman, Indefinite Linear Algebra and Applications, Birkh¨auser, 2005, https: +//doi.org/10.1007/b137517. +[10] I. Gohberg, P. Lancaster, and L. Rodman, Invariant Subspaces of Matrices with Applications, SIAM, 2006, https: +//doi.org/10.1137/1.9780898719093. +[11] I. Gohberg, +P. Lancaster, +and L. Rodman, +Matrix Polynomials, +SIAM, 2009, +https://doi.org/10.1137/1. +9780898719024. +[12] Y. Hachez and H. J. Woerdeman, The fischer-frobenius transformation and outer factorization, in Operator theory, +structured matrices, and dilations, vol. 10 of Theta Series in Advanced Mathematics, Theta, Bucharest, 2007, pp. 181–203. +[13] C. Hanselka and R. Sinn, Positive semidefinite univariate matrix polynomials, Mathematische Zeitschrift, 292 (2019), +pp. 83–101, https://doi.org/10.1007/s00209-018-2137-7. +[14] H. Helson, Lectures on invariant subspaces, Academic Press, 1964, https://doi.org/10.1016/C2013-0-12454-3. +[15] P. Lancaster and L. Rodman, Algebraic Riccati Equations, Oxford University Press, 1995. +[16] P. Lancaster and I. Zaballa, Spectral theory for self-adjoint auadratic eigenvalue problems - a review, ILAS, 37 (2021), +pp. 211–246, https://doi.org/10.13001/ela.2021.5361. +[17] J. W. McLean and H. J. Woerdeman, Spectral factorizations and sums of squares representations via semidefinite +programming, SIAM J. Matrix Anal. Appl., 23 (2001/02), pp. 646–655, https://doi.org/10.1137/S0895479800371177. +[18] A. C. M. Ran and L. Rodman, Factorization of matrix polynomials with symmetries, SIAM Journal on Matrix Analysis +and Applications, 15 (1994), pp. 845–864, https://doi.org/10.1137/S0895479892235502. +[19] M. Rosenblatt, A multi-dimensional prediction problem, Arkiv f¨or Matematik, 3 (1958), pp. 407–424, https://doi.org/ +10.1007/BF02589495. +[20] M. Rosenblum, Vectorial teoplitz operators and the fej´er-riesz theorem, Journal of Mathematical Analysis and Applica- +tions, 23 (1968), pp. 139–147. +[21] J. Willems, Least squares stationary optimal control and the algebraic riccati equation, IEEE Transactions on Automatic +Control, 16 (1971), pp. 621–634, https://doi.org/10.1109/TAC.1971.1099831. + diff --git a/0NFST4oBgHgl3EQfVTgy/content/tmp_files/load_file.txt b/0NFST4oBgHgl3EQfVTgy/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..019abacba89109de0d46a5d767984d79297ef1d0 --- /dev/null +++ b/0NFST4oBgHgl3EQfVTgy/content/tmp_files/load_file.txt @@ -0,0 +1,665 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf,len=664 +page_content='arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='13776v1 [math.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='OC] 31 Jan 2023 REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN Abstract.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A real symmetric positive semidefinite matrix polynomial Q(x) with square determinant that is not identically zero can be factored as Q(x) = G(x)T G(x) where G(x) is itself a real square matrix polynomial with degree half that of Q(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We provide a constructive proof of this fact, rooted in finding a skew-symmetric solution to a modified algebraic Riccati equation XSX − XR + RT X + P = 0, where P, R, S are real n × n matrices with P and S real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Keywords Positive semidefinite matrix polynomial, Algebraic Riccati equation, Matrix factorization MSCcodes 47A68 (Primary), 46C20, 15A48, 93B05 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Introduction The Fej´er-Riesz factorization was first shown for matrix polynomials by Rosenblatt [19] and Helson [14].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In particular, given a matrix polynomial Q(x) = �2m i=0 Qixi with Qi Hermitian and Q(x) positive semidefinite for all x ∈ R, we can factorize it as Q(x) = G(x)∗G(x) where G(x) = �m i=0 Gixi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 1964, Gohberg generalized this factorization to certain operator-valued poly- nomials [8].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Later it was further generalized to operator-valued polynomials in general form [20].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The multivariable case has also been studied, e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' in [17].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For an overview of the work done with the operator- valued Fej´er-Riesz theorem, see [5].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In this paper, we provide a constructive proof of the real analog of the Fej´er-Riesz factorization of matrix- valued polynomials.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In particular, we show that a matrix polynomial Q(x) = �2m i=0 Qixi with Qi real symmetric, Q(x) positive semidefinite for all x ∈ R, and det(Q(x)) equal to a nonzero square, admits the factorization Q(x) = G(x)T G(x) where G(x) is itself a real square matrix polynomial with degree half that of Q(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' This result was first shown by Hanselka and Sinn [13] using methods from projective algebraic geometry and number theory.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We provide an alternative, linear algebraic proof, inspired by the proof of the Fej´er-Riesz factorization presented in Section 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='7 of [1].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' That proof in turn, was taken from [6, 12].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For earlier work on factorizations of real symmetric matrix polynomials (not necessarily positive semidefinite) see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' [18].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A key part of the Fej´er-Riesz factorization proof we follow requires finding a Hermitian solution to an algebraic Riccati equation (∗) XDX + XA + A∗X − C = 0, where D and C are Hermitian.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Reducing a factorization problem to solving a Riccati equation is a technique that has been used in many other papers as well (see, e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=', [2], [7], [15, Chapter 19] and references therein).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' This technique is useful because Riccati equations have been studied extensively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Early work was done by Willems [21] and Coppel [3] in analyzing properties of solutions of continuous algebraic Riccati equations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Another key paper was [4] where Riccati equations were used to solve H∞-control problems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For an in depth analysis of algebraic Riccati equations, please see the book by Lancaster and Rodman [15].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Both authors were supported by National Science Foundation grant DMS 2000037 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 1 2 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN For the current real factorization problem, we end up needing to find a real skew-symmetric solution to an equation of the form (∗∗) XSX − XR + RT X + P = 0, where P and S are real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' This is not quite an algebraic Riccati equation of the form eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (∗) and thus we call it a modified algebraic Riccati equation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In general, to find a skew-Hermitian solution X, one often considers instead iX, which is Hermitian;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' however, we want real solutions and thus this method is not applicable here.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus we instead follow the same steps presented in [15] for finding a real symmetric solution to the real algebraic Riccati equation and amend them to our current situation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' This is the topic of Section 2, which culminates in giving sufficient conditions for a skew-symmetric solution of our modified Riccati equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (∗∗).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In Section 3 we provide additional background on matrix polynomials necessary for our main result, the real factorization of a symmetric positive semidefinite matrix polynomial, presented in Section 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The major advantage of our proof compared to that by Hanselka and Sinn [13] is that ours is constructive.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We end this paper with a couple examples illustrating the construction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A Modified Algebraic Riccati Equation The goal of this section is to provide necessary and sufficient conditions for which there is a real skew- symmetric solution X to the modified algebraic Riccati equation (1) XSX − XR + RT X + P = 0, where P, R, S are real n × n matrices with P and S real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In the book Algebraic Riccati Equations [15], Lancaster and Rodman show conditions for which there is a real symmetric solution X to the CARE equation XDX + XA + AT X − C = 0, where A, C, D are real n × n matrices with C and D real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We amend these results to the present situation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Define the 2n × 2n real matrices (2) Mr = �R −S P RT � , ˆHr = �0 I I 0 � , Hr = � P RT R −S � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then both ˆHr and Hr are real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Also ˆHrMr = M T r ˆHr and HrMr = M T r Hr.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Using terminology from [15], we say Mr is both Hr-symmetric and ˆHr-symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We can now give a condition for a real solution of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) to exist.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' X is a real solution of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) if and only if G(X) := Im � I X � is Mr-invariant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' If G(X) is Mr-invariant, then (3) �R −S P RT � � I X � = � I X � Z for some n × n matrix Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The first block row gives Z = R − SX and the second gives P + RT X = XZ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Combining the two gives P + RT X = X(R − SX).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus X solves eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Conversely, if X solves eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1), then eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (3) holds for Z = R − SX and ths G(X) is Mr-invariant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ More than just a real solution, though, we want a skew-symmetric solution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus we next strive to give a condition for such a solution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For this we first need a definition (see [15]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let H be a real invertible n × n matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A subspace M is called (1) H-nonnegative if ⟨Hx, x⟩ ≥ 0 for all x ∈ M (2) H-nonpositive if ⟨Hx, x⟩ ≤ 0 for all x ∈ M REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS 3 (3) H-neutral if ⟨Hx, x⟩ = 0 for all x ∈ M Proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let X be a real solution of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then, (1) X is skew-symmetric if and only if G(X) is ˆHr-neutral.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (2) G(X) is Hr-nonpositive if and only if (XT + X)(R − SX) ≤ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) Assume X is skew-symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let y ∈ G(X), so y = � I X � z for some z ∈ Rn.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then ⟨Hry, y⟩ = zT �I XT � ˆHr � I X � z = zT (X + XT )z = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus G(X) is ˆHr-neutral.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' On the other hand, suppose G(X) is ˆHr-neutral.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then for all z ∈ Rn, zT(X + XT )z = 0, so X + XT = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus X is skew-symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (2) G(X) is Hr-nonpositive if and only if for all z ∈ Rn, � Hr � I X � z, � I X � z � ≤ 0 zT �I XT � �P RT R −S � � I X � z ≤ 0 zT[P + RT X + XT R − XT SX]z ≤ 0 zT [XR − XSX + XT R − XT SX]z ≤ 0 by eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) zT (XT + X)(R − SX)z ≤ 0 Thus G(X) is Hr-nonpositive if and only if (XT + X)(R − SX) ≤ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2 shows that in order to get a real skew-symmetric solution X to the equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1), we need an ˆHr-neutral subspace G(X) of dimension n.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We consider now conditions for such a subspace to exist.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For this we first state a few known results (see [15]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let A be a square matrix and λi be an eigenvalue of A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We call the sizes of the Jordan blocks of λi the partial multiplicities of λi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' [15, Part of Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3] Let A be a real n × n H-symmetric matrix and the partial multiplicities of A corresponding to the real eigenvalues are all even.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then there exists an A-invariant H- neutral subspace of dimension k − p where k is the number of positive eigenvalues of H (counting algebraic multiplicities) and p is the number of distinct pairs of non-real complex conjugate eigenvalues of A with odd algebraic multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' [15, p.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 56] Let H be a real symmetric matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A real subspace M is H-neutral if and only if ⟨Hx, y⟩ = 0 for all x, y ∈ M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' This follows from the relation ⟨Hx, y⟩ = 1 2 (⟨H(x + y), x + y⟩ − ⟨Hx, x⟩ − ⟨Hy, y⟩) .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ Now we are ready for the new result.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (2) hold with P and S real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Among the following statements, (iii) =⇒ (ii) =⇒ (i) (i) There exists an n-dimensional Mr-invariant Hr-neutral subspace (ii) There exists an n-dimensional Mr-invariant ˆHr-neutral subspace (iii) All real eigenvalues of Mr have even partial multiplicities and all imaginary eigenvalues of Mr have even algebraic multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' If in addition Mr is invertible, then we also have (i) =⇒ (ii).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 4 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' By theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1, if every imaginary eigenvalue of Mr has even algebraic multiplicity (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' p = 0), then an n-dimensional Mr-invariant ˆHr-neutral subspace exists (since ˆHr has n positive and n negative eigenvalues so k = n here).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus (iii) =⇒ (ii).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Next, since Hr = ˆ HrMr, it follows by lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1 that (ii) implies (i).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Finally, if Mr is invertible, ˆ Hr = HrM −1 r and thus (i) implies (ii).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ We need one more result before the main theorem of this section.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For this result, we first recall a definition (see, e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=', [15]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let A ∈ Rn×n and B ∈ Rn×m.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The pair (A, B) is said to be controllable if rank �B AB A2B · · An−1B� = n.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Assume that S ≥ 0 (positive semidefinite) and the pair (R, S) is controllable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let L be an n-dimensional Mr-invariant Hr-nonnegative subspace of R2n.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then L is a graph subspace, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' L = Im � I X � for some real n × n matrix X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For L as defined in the statement, write L = Im � X1 X2 � for some real n × n matrices X1 and X2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We shall show that X1 is invertible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' First, since L is Mr-invariant, � R −S P RT � � X1 X2 � = � X1 X2 � T for some n × n matrix T .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus, RX1 − SX2 = X1T (4) PX1 + RT X2 = X2T (5) Next, since L is Hr-nonnegative, we know (6) �XT 1 XT 2 � � P RT R −S � � X1 X2 � = XT 1 PX1 + XT 1 RT X2 + XT 2 RX1 − XT 2 SX2 is positive semidefinite.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let K = ker X1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (6) is positive semidefinite, for every x ∈ K, 0 ≤ xT XT 1 PX1x + xT XT 1 RT X2x + xT XT 2 RX1x − xT XT 2 SX2x = −xT XT 2 SX2x.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since S ≥ 0, X2x ∈ ker S, so X2K ⊂ ker S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then, equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (4) implies T K ⊂ K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Consequently, equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (5) gives RT X2K ⊂ X2K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' All together, we have RT X2K ⊂ ker S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' By induction, we get (RT )rX2K ⊂ ker S, r = 0, 1, 2, .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Now for every x ∈ K, \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 S SRT .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' S(RT )n−1 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb (X2x) = 0 REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS 5 Since (R, S) is controllable, we must have X2x = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The only n-dimensional vector x for which X1x = X2x = 0 is the zero vector (otherwise dim L < n).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus K = {0} and X1 is invertible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Hence L = Im � I X � , where X = X2X−1 1 and so L is a graph subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ Now we put everything together to get sufficient conditions for a real skew-symmetric solution of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1): Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (2) hold with P and S real symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Assume that S ≥ 0 and the pair (R, S) is controllable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then the conditions (i) - (ii) are equivalent and (iii) implies (ii) (i) The equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) has a real skew-symmetric solution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (ii) There exists an n-dimensional Mr-invariant ˆ Hr-neutral subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (iii) All real eigenvalues of Mr have even partial multiplicities and all imaginary eigenvalues of Mr have even algebraic multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The (iii) =⇒ (ii) was part of lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' By proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1 and proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2, we know that if X is a real skew-symmetric solution to eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1), then G(X) is an n-dimensional Mr-invariant ˆHr-neutral subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus (i) =⇒ (ii).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Finally, assume there exists an n-dimensional Mr-invariant ˆHr-neutral subspace, say L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since Hr = ˆHrMr, L is also an n-dimensional Mr-invariant Hr-neutral subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Clearly L is an Hr-nonnegative subspace, so by lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3, L is a graph subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since L = G(X) is Mr-invariant, X is a real solution of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) by proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since L = G(X) is also ˆHr-neutral, by proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2 X is skew-symmetric.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus (ii) =⇒ (i).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Matrix Polynomials Building toward our goal of factorizing a real symmetric positive semidefinite matrix polynomial, we next state a few relevant results on matrix polynomials (see [11]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For n × n matrices Pi, we define an n × n matrix polynomial P(x) of degree m by P(x) = m � i=0 Pixi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called real if all Pi are real matrices.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called monic if Pm = In.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called self-adjoint if Pi = P ∗ i , its conjugate transpose, for all i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called symmetric if Pi = P T i for all i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called positive semidefinite (also nonnegative) if for all x ∈ R, P(x) is positive semidefinite.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The matrix polynomial is called regular if det(P(x)) is not identically zero.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' As in [16], we define the spectrum and Jordan canonical form of a matrix polynomial in the following ways.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1 Definition 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let P(x) be a regular matrix polynomial.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then the set of eigenvalues of P, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' the spectrum, is σ(P) := {λ ∈ C : det(P(λ)) = 0}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let P(x) be a monic matrix polynomial, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' P(x) = Inxm + m−1 � i=0 Pixi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 1Note that the partial multiplicities of an eigenvalue of a matrix polynomial are often defined as powers of the elementary divisors;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' however, these partial multiplicities are the same as the sizes of the Jordan blocks of our companion matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' See the Appendix of [10] for a more in depth understanding of matrix polynomial equivalences, linearizations, partial multiplicities and elementary divisors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 6 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN The Jordan canonical form for P(x) is defined to be that of the companion matrix Cp := \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 0 In 0 · · 0 0 0 In · · 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 0 · · 0 In −P0 −P1 · · −Pm−2 −Pm−1 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb Theorem 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' [11, part of Theorem 12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='8] For a monic self-adjoint matrix polynomial P(x), the following statements are equivalent: (i) P(x) is nonnegative.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (ii) The partial multiplicities of P(x) for real points of the spectrum are all even.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In the previous section, we found that if all real eigenvalues of Mr have even partial multiplicities and all imaginary eigenvalues of Mr have even algebraic multiplicity, then our equation eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (1) has the desired real skew-symmetric solution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus we now want to connect the eigenvalues of Mr and their partial multiplicities with the eigenvalues of a monic nonnegative matrix polynomial P(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For this, we begin with a few definitions from [11].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Two matrix polynomials M1(x) and M2(x) of size n × n are called equivalent if M1(x) = E(x)M2(x)F(x) for some n × n matrix polynomials E(x) and F(x) with constant nonzero determinants.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Definition 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let P(x) be an n × n monic matrix polynomial of degree m.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' A linear matrix polynomial λI − A is called a linearization of P(x) if (7) λI − A ∼ � P(x) 0 0 In(m−1) � where ∼ means equivalence of matrix polynomials.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Note that Cp, the companion matrix, is a linearization of P(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For any linearization λI − A, the partial multiplicities in every eigenvalue of A and P(x) are the same.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus to gain results about the multiplicities of the eigenvalues of Mr, it suffices to show λI − Mr is a linearization of a matrix polynomial P(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Lemma 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let Q(x) = �2m j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with Q0 = In.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then for Mr = \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 − 1 2Q1 −In In 0 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 0 0 Q2 − 1 4Q2 1 1 2Q3 − 1 2Q1 In 1 2Q3 Q4 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 1 2Q2m−1 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 1 2Q2m−1 Q2m 0 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb , we have λI − Mr ∼ � rev Q(λ) 0 0 I � where rev Q(x) := 2m � i=0 Q2m−ixi = x2mIn + 2m−1 � i=1 Q2m−ixi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS 7 Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' First permute the rows and columns as follows: M1:= \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 0 0 · · 0 In 0 In .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 In 0 · · 0 In 0 · · 0 0 0 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 · · 0 In 0 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb (λI − Mr) \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 In .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 0 0 In .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb , = \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 −Q2m − 1 2Q2m−1 0 λIn λIn −In 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' λIn −In 0 λIn + 1 2Q1 In − 1 2Q3 1 4Q2 1 − Q2 λIn + 1 2Q1 −In .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' −Q4 − 1 2Q3 λIn .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' − 1 2Q2m−1 −Q2m−2 − 1 2Q2m−3 λIn −In \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb Define V1, .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' , Vm by V1 = −Q2m − 1 2λQ2m−1 V2 = −1 2Q2m−1 − λQ2m−2 − 1 2λ2Q2m−3 V3 = −1 2λQ2m−3 − λ2Q2m−4 − 1 2λ3Q2m−5 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Vm−1 = −1 2λm−3Q5 − λm−2Q4 − 1 2λm−1Q3 Vm = −1 2λm−2Q3 − λm−1Q2 − λmQ1 − λm+1In Then, multiply M1 on the left by \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 In �m i=2 λi−2Vi �m i=3 λi−3Vi · · Vm−1 + λVm Vm −λm−1(λIn + 1 2Q1) λm−1In · · λ2In λIn 0 In(m−1) 0 0 0 Inm \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Noting that −Q2m − 1 2λQ2m−1 + λ m � i=2 λi−2Vi = − rev Q(λ), 8 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN we get λI − Mr ∼ \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 − rev Q(λ) −In 0 ∗ .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' −In 0 ∗ In −In 0 ∗ .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' −In \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb Thus it is evident now that λI − Mr ∼ � rev Q(λ) 0 0 I � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Real Factorization of Non-negative Matrix Polynomial We are now ready for the main result.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' While the following theorem was previously proven by Hanselka and Sinn [13], we provide a new constructive proof following that of the complex analogue presented in the monograph by Bakonyi and Woerdeman [1].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let Q(x) = �2m j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with Q(x) ≥ 0 for all x ∈ R and Q0 > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then det(Q(x)) is a square if and only if there exists an n × n real matrix polynomial G(x) = �m j=0 Gjxj of degree m such that Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' First, assume Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then det(Q(x)) = det(G(x))2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' On the other hand, assume det(Q(x)) is a square.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Without loss of generality, assume Q0 = In (otherwise, take ˜Q(x) := Q−1/2 0 Q(x)Q−1/2 0 ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Consider the (m + 1)n × (m + 1)n real symmetric matrix F0 = \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 In 1 2Q1 1 2Q1 Q2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 1 2Q2m−1 1 2Q2m−1 Q2m \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Given an nm × nm real skew-symmetric matrix X = \uf8ee \uf8ef\uf8f0 X1,1 · · X1,m .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Xm,1 · · Xm,m \uf8f9 \uf8fa\uf8fb , let FX = F0 + � 0 X 0n 0 � − � 0 0n X 0 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' It should be noted that in the above line, the matrix decompositions are different;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' the X block and the −X block overlap in general.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We want to solve Xopt = arg min rank(FX) such that FX ≥ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let A = \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 0 In 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 0 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb ∈ Rnm×nm and B = \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 In 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb ∈ Rnm×n.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS 9 Then (A, B) is controllable, � 0 0 X 0 � = � 0 0 XB XA � , and � 0 X 0 0 � = � 0 BT X 0 AT X � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Split F0 into four blocks as follows, F0 = � In Γ12 Γ21 Γ22 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Noting ΓT 12 = Γ21 and Γ22 is real symmetric, we can recast the condition FX ≥ 0 as � In Γ12 + BT X ΓT 12 − XB Γ22 + AT X − XA � ≥ 0 Consider the Schur complement with respect to In, Γ22 + AT X − XA − (ΓT 12 − XB)I−1 n (Γ12 + BT X).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Setting this equal to zero, we get the modified algebraic Riccati equation (8) P + RT X − XR + XSX = 0 where P = Γ22 − ΓT 12Γ12 R = A − BΓ12 S = BBT .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Note P = P T and S = ST with S ≥ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In this case, the associated Mr matrix is as follows: Mr = � A − BΓ12 −BBT Γ22 − ΓT 12Γ12 AT − ΓT 12BT � = \uf8ee \uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8ef\uf8f0 − 1 2Q1 −In In 0 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 0 0 Q2 − 1 4Q2 1 1 2Q3 − 1 2Q1 In 1 2Q3 Q4 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 1 2Q2m−1 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In 1 2Q2m−1 Q2m 0 \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fa\uf8fb By lemma 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1, Mr is a linearization of rev Q(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since Q(x) ≥ 0 for all x ∈ R, rev Q(x) = x2mQ � 1 x � ≥ 0 for all nonzero x ∈ R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' By continuity, then rev Q(x) ≥ 0 for all x ∈ R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then by theorem 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1, the partial multiplicities of every real eigenvalue of rev Q(λ) are all even.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Since Mr is a linearization of rev Q(x), all the partial multiplicities of every eigenvalue of Mr and rev Q(λ) are the same, so the partial multiplicities of every real eigenvalue of Mr are all even.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Further, by the non-negativity of rev Q(x), det(λI − Mr) = det(rev Q(x)) has all roots of even algebraic multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' In particular, all non-real eigenvalues of Mr have even algebraic multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Hence by theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2, there is a skew-symmetric solution, ˜X of eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (8).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then since the Schur complement with respect to In is zero, we know F ˜ X = � In Γ12 + BT ˜X ΓT 12 − ˜XB Γ22 + AT ˜X − ˜XA � ≥ 0 10 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN and rank(F ˜ X) = rank �� In Γ12 + BT ˜X ΓT 12 − ˜XB Γ22 + AT ˜X − ˜XA �� = rank In = n.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' If we factorize F ˜ X = � In Γ12 + BT ˜X ΓT 12 − ˜XB Γ22 + AT ˜X − ˜XA � = \uf8ee \uf8ef\uf8f0 GT 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' GT m \uf8f9 \uf8fa\uf8fb � G0 · · Gm � with G0 = In and Gi, i = 1, 2, .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' , m, real n × n matrices, we have Q(x) = �In xIn · · xmIn � F ˜ X \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 In xIn .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' xmIn \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb = �In xIn · · xmIn � \uf8ee \uf8ef\uf8f0 GT 0 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' GT m \uf8f9 \uf8fa\uf8fb �G0 · · Gm � \uf8ee \uf8ef\uf8ef\uf8ef\uf8f0 In xIn .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' xmIn \uf8f9 \uf8fa\uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus for G(x) = �m j=0 Gjxj, Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1 required Q0 > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We can relax this condition as follows.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Corollary 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let Q(x) = �2m j=0 Qjxj be an n × n real symmetric matrix polynomial of degree 2m with Q(x) ≥ 0 for all x ∈ R and Q(x0) > 0 for some x0 ∈ R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then det(Q(x)) is a square if and only if there exists an n × n real matrix polynomial G(x) = �m j=0 Gjxj of degree m such that Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' First, assume Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then det(Q(x)) = det(G(x))2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' On the other hand, assume det(Q(x)) = f(x)2 for some polynomial f of degree m.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Consider P(x) := Q(x0 − x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then P(x) is an n × n real symmetric matrix polynomial of degree 2m such that P(0) = Q(x0) > 0 and det(P(x)) = det(Q(x0 − x)) = f(x0 − x)2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus by theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1, there is an n × n real matrix polynomial H(x) = �m j=0 Hjxj of degree m such that P(x) = H(x)T H(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Define G(x) := H(x0 − x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then G(x) = �m j=0 Gjxj is an n × n real matrix polynomial such that Q(x) = P(x0 − x) = H(x0 − x)T H(x0 − x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' □ The proof of theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1 is constructive.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' It hinges on finding the real skew-symmetric solution X to the modified algebraic Riccati equation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Back in Section 2, we found such a solution by constructing an mn- dimensional Mr-invariant Hr-neutral subspace.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Following the proof of Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2, found in [15], also to be found in Gohberg, Lancaster, and Rodman’s later book Indefinite Linear Algebra and Applications [9], we first convert Mr to its real Jordan form Mr = SJS−1, where J = Jr1(λ1) ⊕ · · · ⊕ Jrk(λk) ⊕ J2rk+1(λk+1 ± iµk+1) ⊕ · · · ⊕ J2rk+ℓ(λk+ℓ ± iµk+ℓ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' REAL FACTORIZATION OF POSITIVE SEMIDEFINITE MATRIX POLYNOMIALS 11 For real eigenvalues λj, where 1 ≤ j ≤ α, we take the first rj/2 columns of S corresponding to the block Jrj (note we know each rj is even).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For any imaginary eigenvalues λj ± iµj with rj even, we do the same.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Finally, we must consider the imaginary eigenvalues λj ± iµj with rj odd.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' For such an eigenvalues, there must be an even number of Jordan blocks of odd size (since we know every imaginary eigenvalue has even algebraic multiplicity).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Collect the Jordan blocks together in pairs Kj = J2rj(λj ± iµj) ⊕ J2rj+1(λj+1 ± iµj+1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then take the first rj − 1 columns of S corresponding to J2rj(λj ± iµj), the first rj+1 − 1 columns of S corresponding to J2rj+1(λj+1 ± iµj+1), along with the following two vectors (1) The rjth column of S corresponding to J2rj(λj ± iµj) plus the rj+1 + 1st column of S corresponding to J2rj+1(λj+1 ± iµj+1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' (2) The rj +1st column of S corresponding to J2rj(λj ±iµj) minus the rj+1st column of S corresponding to J2rj+1(λj+1 ± iµj+1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Let us illustrate the above ideas in a few examples.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The first example is the real eigenvalue case.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' The second example is the imaginary eigenvalue case with odd rj.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Example 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Take Q(x) = �2x2 + 2x + 1 −4x2 − 3x −4x2 − 3x 8x2 + 4x + 1 � = �1 0 0 1 � + x � 2 −3 −3 4 � + x2 � 2 −4 −4 8 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then Mr(x) = SJS−1 for J = \uf8ee \uf8ef\uf8ef\uf8f0 −3 1 0 0 0 −3 0 0 0 0 0 1 0 0 0 0 \uf8f9 \uf8fa\uf8fa\uf8fb , S ≈ \uf8ee \uf8ef\uf8ef\uf8f0 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2778 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3148 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2222 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6852 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2778 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3704 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1111 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3704 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1389 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3519 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0556 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3519 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1389 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1759 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1111 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1759 \uf8f9 \uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We have J = J2 (−3) ⊕ J2 (0), so r1 = r2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus we take the 1st column corresponding to the first block as well as the 1st column corresponding to the second block.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' \uf8ee \uf8ef\uf8ef\uf8f0 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2778 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2222 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2778 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1111 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1389 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0556 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1389 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1111 \uf8f9 \uf8fa\uf8fa\uf8fb =: � X1 X2 � Our invariant subspace is thus Im � X1 X2 � = Im � I X2X−1 1 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Here we have then X = X2X−1 1 = � 0 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5 0 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus Fopt = F0 + � 0 X 0 0 � − � 0 0 X 0 � = \uf8ee \uf8ef\uf8ef\uf8f0 1 0 1 −2 0 1 −1 2 1 −1 2 −4 −2 2 −4 8 \uf8f9 \uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We factorize as F = \uf8ee \uf8ef\uf8ef\uf8f0 1 0 0 1 1 −1 −2 2 \uf8f9 \uf8fa\uf8fa\uf8fb �1 0 1 −2 0 1 −1 2 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus G0 = �1 0 0 1 � , G1 = � 1 −2 −1 2 � , G(x) = G0 + xG1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We can verify Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' 12 SARAH GIFT AND HUGO J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' WOERDEMAN Example 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Take now Q(x) = �2x2 + 2x + 1 x2 + 2x x2 + 2x 13x2 + 4x + 1 � = �1 0 0 1 � + x �2 2 2 4 � + x2 �2 1 1 13 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Then Mr(x) = SJS−1 for J = 1 2 \uf8ee \uf8ef\uf8ef\uf8f0 −3 √ 11 0 0 − √ 11 −3 0 0 0 0 −3 √ 11 0 0 − √ 11 −3 \uf8f9 \uf8fa\uf8fa\uf8fb , S ≈ \uf8ee \uf8ef\uf8ef\uf8f0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5477 0 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5477 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0913 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3028 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0913 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3028 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1826 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6055 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1826 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6055 −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0954 0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0954 0 \uf8f9 \uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We have J = J2 � 3±i √ 11 2 � ⊕ J2 � 3±i √ 11 2 � , so r1 = r2 = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus we take the 1st column corresponding to the first block plus the 2nd column corresponding to the second block as well as the 2nd column corresponding to the first block minus the first column corresponding to the second block.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' \uf8ee \uf8ef\uf8ef\uf8f0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5477 + 0 0 − (−0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='5477) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0913 + 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3028 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='3028 − (−0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0913) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1826 + 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6055 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='6055 − (−0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='1826) −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0954 + 0 0 − 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content='0954 \uf8f9 \uf8fa\uf8fa\uf8fb =: �X1 X2 � Our invariant subspace is thus Im � X1 X2 � = Im � I X2X−1 1 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Here we have then X = X2X−1 1 = � 0 2 −2 0 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus Fopt = F0 + �0 X 0 0 � − � 0 0 X 0 � = \uf8ee \uf8ef\uf8ef\uf8f0 1 0 1 3 0 1 −1 2 1 −1 2 1 3 2 1 13 \uf8f9 \uf8fa\uf8fa\uf8fb .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We factorize as F = \uf8ee \uf8ef\uf8ef\uf8f0 1 0 0 1 1 −1 3 2 \uf8f9 \uf8fa\uf8fa\uf8fb �1 0 1 3 0 1 −1 2 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' Thus G0 = �1 0 0 1 � , G1 = � 1 3 −1 2 � , G(x) = G0 + xG1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' We can verify Q(x) = G(x)T G(x).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/0NFST4oBgHgl3EQfVTgy/content/2301.13776v1.pdf'} +page_content=' References [1] 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Stefan Tautz1, 2, 5 +1Peter Gr¨unberg Institute (PGI-3), Forschungszentrum J¨ulich, 52425 J¨ulich, Germany +2J¨ulich Aachen Research Alliance (JARA), Fundamentals of Future Information Technology, 52425 J¨ulich, Germany +3Institute of Physics II B, RWTH Aachen University, 52074 Aachen, Germany +4Institute of Physics II, University of Cologne, 50937 Cologne, Germany +5Experimental Physics IV A, RWTH Aachen University, 52074 Aachen, Germany +(Dated: January 30, 2023) +Artificial nanostructures, fabricated by placing building blocks such as atoms or molecules in well- +defined positions, are a powerful platform in which quantum effects can be studied and exploited on +the atomic scale. Here, we report a strategy to significantly reduce the electron-electron coupling +between a large planar aromatic molecule and the underlying metallic substrate. To this end, we +use the manipulation capabilities of a scanning tunneling microscope (STM) and lift the molecule +into a metastable upright geometry on a pedestal of two metal atoms. Measurements at millikelvin +temperatures and magnetic fields reveal that the bottom-up assembled standing metal-molecule +nanostructure has an S = 1/2 spin which is screened by the substrate electrons, resulting in a Kondo +temperature of only 291 ± 13 mK. We extract the Land´e g-factor of the molecule and the exchange +coupling Jρ to the substrate by modeling the differential conductance spectra using a third-order +perturbation theory in the weak coupling and high-field regimes. Furthermore, we show that the +interaction between the STM tip and the molecule can tune the exchange coupling to the substrate, +which suggests that the bond between the standing metal-molecule nanostructure and the surface +is mechanically soft. +On the way to spin qubits based on single atoms or +molecules, it is essential to minimize the interaction with +the environment, since the latter leads to decoherence +[1]. The scanning tunneling microscope (STM) is an ideal +tool to study quantum properties of nanoscale structures, +because it not only allows the magnetic states of individ- +ual atoms and molecules to be read out [2] and coher- +ently controlled [3–5], but also enables the environment +to be changed directly. +The ability to arrange atoms +and molecules on surfaces with atomic precision allows +for the fabrication and study of unprecedented artificial +nanostructures [6, 7]. Moreover, the STM can be used +to fabricate multiple absolutely identical qubits [8] from +individual atoms and molecules, which can also be ar- +ranged and coupled with each other as desired. Com- +pared to mesoscopic qubits, the structural control down +to the atomic level may offer advantages. +Magnetic atoms and molecules with degenerate ground +states on metallic surfaces typically show the Kondo ef- +fect: the spin degree of freedom is quenched at temper- +atures below a characteristic Kondo temperature TK by +the formation of a many-electron singlet state with the +electrons of the bath [9, 10]. Because TK depends di- +rectly on the coupling with the metal, the Kondo effect +itself can be used as a gauge of the interaction with the +environment. The strong hybridization of the d-orbitals +of magnetic atoms with states of the metal substrate +leads to TK of typically 40 - 300 K [11]. For magnetic +molecules, on the other hand, Kondo temperatures of +only a few Kelvin have been observed on metal surfaces +[12–14], which can be explained by the weaker hybridiza- +tion of the molecular orbitals with the substrate, or the +shielding of the magnetic atoms by the surrounding lig- +ands of the molecule. However, long relaxation times T1 +of several hundred nanoseconds up to days [15, 16] and +dephasing times T2 in the nanosecond range [3–5] were so +far only achieved for atoms and molecules that were de- +coupled from the metallic surface by an atomically thin +insulating layer. +The presence of the decoupling layer +has also resulted in a significant reduction of TK to a few +Kelvin for magnetic atoms [17, 18]. +In this work, we show that exploiting the third +dimension for the bottom-up assembly of standing +metal-molecule nanostructures offers an alternative ap- +proach to tune the coupling with the metallic sub- +strate. Specifically, we show that for a single 3,4,9,10- +perylenetetracarboxylic dianhydride (PTCDA) in the +standing configuration on a pedestal of two Ag adatoms +(Fig. 1a), both the interaction with the Ag(111) sub- +strate is drastically reduced compared to the flat-lying +PTCDA and the coupling with the metal substrate can +be tuned by stretching the bond between the molecule +and surface, utilizing the attraction between the STM +tip and the molecule. We report the fabrication of an +S = 1/2 spin nanostructure based on this strategy, with a +very weak coupling to the underlying substrate, resulting +in a TK of only 291 ± 13 mK — to our knowledge, the +smallest TK ever measured on a metallic substrate using +STM. Comparably low TK have so far only been found +in mesoscopic quantum dots [19, 20]. +The Ag(111) surface was prepared in ultra-high vac- +uum (UHV) by repeated Ar+ sputtering and heating at +800 K. A small coverage of PTCDA molecules was evap- +orated onto the clean Ag(111) surface at room temper- +arXiv:2301.11762v1 [cond-mat.mes-hall] 27 Jan 2023 + +2 +(a) +(b) +(c) +10 Å +Ag(111) +~17.5 Å +STM tip +−6 +−4 +−2 +0 +Current (pA) ++ +−0.6 +−0.4 +−0.2 +0.0 +0.2 +0.4 +0.6 +Bias voltage (mV) +5.5 +6.0 +6.5 +7.0 +7.5 +dI/dV (10-4 G0) +FIG. 1. +(a) Schematic view of a standing PTCDA + 2Ag +nanostructure on the Ag(111) surface, including the STM +tip above the molecule. +The bar shows the tunneling cur- +rent IT measured above the standing nanostructure at con- +stant height. The white, grey and red spheres indicate hy- +drogen, carbon and oxygen atoms, respectively, of PTCDA. +(b) Constant-height STM image above a standing nanostruc- +ture recorded at a tip height of z ≃ 17.5 ˚A above the surface. +The bias voltage was V = −50 mV. The white cross marks +the location where the dI/dV conductance spectra were mea- +sured. The molecular plane is indicated by the dashed orange +line. (c) dI/dV conductance spectrum (blue) on a standing +metal-molecule nanostructure measured at T = 30 mK and +B = 0 T (Vmod = 50 µV). The tip was stabilized at IT = 45 pA +and V = −1 mV. The red curve shows the fit based on the +Frota function (see text for details). The spectrum is shown +in units of the conductance quantum G0 = 2e +h . +ature from a custom-built Knudsen cell. After evapora- +tion, the sample was flashed at 480 K for 2 min and then +cooled down to 100 K and transferred to the STM. All ex- +periments were performed in the J¨ulich Quantum Micro- +scope [21], a millikelvin scanning tunneling microscope +which uses the adiabatic demagnetization of electronic +magnetic moments in a magnetocaloric material to reach +temperatures in the range between 30 mK and 1 K. In +this instrument, B fields of up to 8 T perpendicular to the +sample surface can also be applied. Differential conduc- +tance (dI/dV ) spectra were measured using conventional +lock-in techniques with the STM feedback loop switched +off and an AC modulation amplitude Vmod = 20−100 µV +and frequency fmod = 187 Hz. The PtIr tip was treated +in-situ by applying controlled voltage pulses and indenta- +tions into the clean silver surface until the spectroscopic +signature of the Ag(111) surface state appeared. +The standing PTCDA + 2Ag nanostructure was fabri- +cated on the Ag(111) surface in three steps by controlled +manipulation with the tip of the STM as described in +Ref. [22]. First, two single Ag atoms were attached to +the two carboxylic oxygens on one side of the flat-lying +molecule by lateral manipulation with the tip. +Then, +one of the carboxylic oxygens on the opposite side was +contacted and the PTCDA molecule was pulled up on a +curved trajectory until it stood upright. The tip was then +moved straight up until the bond between the molecule +and the tip broke, leaving the molecule in the standing +position on the two Ag adatoms [22]. The stability of +the standing metal-molecule nanostructure arises from +the balance between local covalent interactions and non- +local long-range van der Waals forces [23, 24]. +In constant-height STM images, the standing metal- +molecule nanostructure can be recognized by two fea- +tures that are distributed symmetrically around the plane +of the molecule (dashed orange line in Fig. 1b) and +separated by a nodal plane perpendicular to the latter +(Fig. 1b). It is interesting to note that the node of the π- +orbital in the plane of the molecule could not be resolved. +The two features coincide with the positions where the +interaction with the tip is most pronounced [22]. In the +standing configuration, there is only a weak overlap be- +tween the wave functions of the metallic surface and the +lowest unoccupied molecular orbital (LUMO) of PTCDA, +because the lobes of the molecular π-orbital are oriented +perpendicular to the plane of the molecule. This allows +the standing nanostructure to function as a quantum dot +and coherent field emitter [22]. +At mK temperatures, a peak at zero bias is evident +in the dI/dV spectrum measured on a standing metal- +molecule nanostructure (Fig. 1c). In fact, at these low +temperatures we additionally observe a dip at zero bias +due to the dynamical Coulomb blockade (DCB) [25]. We +have thus corrected all dI/dV spectra on the standing +nanostructure for the DCB dip (see Supplementary Ma- +terial). Previous studies have hinted that the LUMO of +the standing metal-molecule nanostructure must contain +a single unpaired electron [22, 26]. Therefore, it is plausi- +ble to assume that the zero-bias peak originates from the +Kondo effect, in which the spin of this localized electron is +screened by itinerant substrate electrons. To verify this, +we measured dI/dV spectra at different B fields. Already +at B ≈ 100 − 120 mT a Zeeman splitting of the zero-bias +peak is discernable (Fig. 2a). +At higher B fields, the +Kondo effect is completely quenched and the spectrum is +dominated by the symmetric steps arising from inelastic +spin-flip excitations (Fig. 2b). +To extract the precise energy of the Zeeman splitting +∆, we calculated the numerical derivative of the dI/dV +spectra and fitted the peak positions with a Gaussian (see +Supplementary Material). As shown in Figs. 2c and d, +the energies of the spin-flip excitations scale linearly with +the external B field. Only close to the critical field BC, +which is required to initially split the Kondo resonance, + +3 +−1 +0 +1 +Bias voltage (mV) +1 +2 +3 +4 +dI/dV (10-4 G0) +0 +0.1 +0.2 +B field (T) +0.00 +0.01 +0.02 +0.03 +Δ (mV) +(a) +(b) +(c) +(d) +1 T +3 T +5 T +7 T +2Δ +−0.25 +0 +0.25 +Bias voltage (mV) +15 +20 +25 +30 +35 +dI/dV (10-4 G0) +0.08 T +0.20 T +0 +2.5 +5.0 +B field (T) +0.0 +0.2 +0.4 +0.6 +0.8 +Δ (mV) +g = 2.006 ± 0.007 +FIG. 2. (a)-(b) dI/dV spectra (blue) on a standing metal- +molecule nanostructure, measured at different B fields at +T +≃ 50 mK (setpoints in panel (a) were IT += 100 pA, +V = −10 mV, Vmod = 100 µV and IT = 100 pA, V = −1 mV, +Vmod = 20 µV in panel(b)). +In panel (a), the B field was +changed in steps of 20 mT. The orange curves in panel (b) +show the fits based on perturbation theory (see text for de- +tails). The spectra are vertically displaced for clarity. (c)-(d) +The Zeeman splitting ∆ extracted from the dI/dV spectra as +a function of B. The gray dashed line in panel (c) serves as a +guide for the eye. The red curve in panel (d) shows the linear +fit for the Zeeman splitting. +the Zeeman energy rises noticeably faster with increas- +ing B field. To extract the Land´e factor g, we consider +only the data points at B fields ≥ 1 T (Fig. 2b) since +the Kondo effect in the strong coupling regime leads to +renormalization of the g-factor. A linear fit of the form +∆ = gµBB for the Zeeman effect, where µB is the Bohr +magneton, yields a Land´e factor g = 2.006 ± 0.007. By +interpolating the data points at low B fields, we obtain +BC = 108±5 mT for the critical field. Using the relation +[27] +BC = 1 +2 +kBTK +gµB +, +(1) +valid for temperatures T < 0.25 TK, this gives an esti- +mate of 291 ± 13 mK for the Kondo temperature TK. +An independent estimate of the Kondo temperature +TK can be obtained from the width of the Kondo reso- +nance (Fig. 1c). However, it should be noted that this is +only a rough estimate, since the width of the Kondo reso- +nance is related to TK by a non-universal scaling constant +[28]. To extract its width, we fitted the Kondo resonance +with a Frota line shape [29] +ρ(E)Frota = ℜ +� +iΓK +E − E0 + iΓK +. +(2) +Additional broadening effects due to the Fermi distri- +bution and the modulation amplitude were taken into +account. +The best fit then yields a width of ΓK ≃ +43 µV and thus a TK = ΓK(2π × 0.103)/kB ≃ 320 mK +[29], in good agreement with the above estimate from +the B field dependence. +We attribute the features in +the dI/dV spectrum at approximately ±0.25 mV and +±0.55 mV (Fig. 1c and Supplementary Material) to ei- +ther molecular vibrations or frustrated translations of the +standing metal-molecule nanostructure [23]. Note that a +strong electron-vibrational coupling can also lead to a +further decrease of TK [30]. +The low Kondo temperature of the standing nanostruc- +ture in conjunction with the low base temperature and +high energy resolution of our mK STM enable us to quan- +titatively describe the interaction of the localized spin +with its environment, also as a function of temperature. +For this purpose, we employ the Anderson-Appelbaum +model [31–33] and calculate the tunneling conductance +from the Kondo Hamiltonian in a perturbative approach +that includes processes up to third order in the exchange +interaction J [34]. The model allows tunneling electrons +to interact with the localized spin via spin-spin (tT S ˆσt·ˆS) +or potential scattering (tT S U). Here tT S is the matrix +element for a transition from the tip to the molecule or +vice versa, and ˆσt and ˆS are the spin operators of the +tunneling and localized electrons, respectively. In addi- +tion, the model takes into account the spin-spin exchange +scattering between the electrons of the substrate and the +localized spin (Jρ ˆσs · ˆS), where ρ denotes the substrate’s +electron density at the Fermi energy and ˆσs the spin oper- +ator of itinerant electrons in the substrate. This approach +provides the correct description under the following con- +ditions: the magnetic impurity is predominantly coupled +to one of the electrodes (here the substrate), the system +is in equilibrium (limit of small bias voltages), and the +system is in the weak coupling limit (T >∼ TK) or high- +field regime (B >∼ kBTK). +We performed least-square +fits and extracted the dimensionless coupling strength +Jρ between the substrate and the localized electron and +its Land´e factor g. +Before we focus on the temperature dependence, we +first examine the influence of the B field on Jρ at 50 mK +(Fig. 2b). +As the B field increases, we see a decrease +in the height of the peak structure on top of the steps +originating from spin-flip excitations. Since those peak +heights are proportional to Jρ [34], this indicates that +|Jρ| decreases with increasing B field. +This is clearly +seen in Fig. 3a, where the fitted Jρ is plotted versus B +field. It may at first sight seem surprising that we still +observe a coupling between the localized and itinerant +spins at high B fields. +This behaviour is, however, in + +4 +−1 +0 +1 +Bias voltage (mV) +1 +2 +3 +4 +5 +dI/dV (10-4 G0) +(a) +(b) +(c) +(d) +1009 mK +751 mK +275 mK +70 mK +41 mK +0 +2.5 +5.0 +B field (T) +−0.10 +−0.09 +−0.08 +−0.07 +−0.06 +Jρ +0 +500 +1000 +Temperature (mK) +−0.06 +−0.05 +−0.04 +Jρ +~TK +0 +500 +1000 +Temperature (mK) +1.90 +1.95 +2.00 +2.05 +g-factor +FIG. 3. (a) Coupling strength Jρ as extracted from the fits in +Fig. 2b as a function of B field. (b) dI/dV spectra (blue) on +a standing metal-molecule nanostructure, measured at differ- +ent temperatures in an external field B = 7 T (IT = 100 pA, +V += −10 mV, Vmod = 100 µV). The orange curves show +the fits based on perturbation theory (see text for details). +The spectra are vertically displaced for clarity. (c) Coupling +strength Jρ as extracted from the fits as a function of tem- +perature. The dashed blue line indicates the Kondo energy +scale TK as determined from the B-field data of Fig. 2. (d) +Land´e g-factor estimated from the fits in panel (b) (black) +and the effective g-factor geff after taking into account renor- +malization effects due to the exchange interaction (red). The +red line illustrates a linear fit and the red shaded area the +corresponding confidence interval. +good agreement with numerical renormalization group +(NRG) calculations for an S = 1/2 Kondo impurity at +finite temperatures and B fields [27], in which it was +shown that the intensity of the split Kondo resonance +varies even if µBB/kBTK ≫ 1, which corresponds to the +present situation. In other words, we have even at high +B fields access to bias driven Kondo correlations whose +gradual emergence at decreasing temperatures drives |Jρ| +up. This behavior can be readily observed by looking at +the temperature-dependent data for constant B = 7 T +(Fig. 3b). The fits reveal that |Jρ| increases with decreas- +ing temperature (Fig. 3c). For B = 0, such an increase +of |Jρ| would signal the progressive breakdown of the +perturbation approach, yielding a divergence of Jρ and +the crossover into the Kondo singlet as a new ground +state [9, 10]. +However, here we are in the high-field +regime and therefore will not reach the Kondo ground +state even in the limit T → 0. We note that the tem- +perature range in which the perturbation theory starts to +0.5 +1.0 +1.5 +2.0 +Setpoint conductance (10-4 G0) +−0.075 +−0.070 +−0.065 +−0.060 +Jρ +zB,eq +zB,st +FIG. 4. Coupling strength Jρ as extracted from the fits of +dI/dV spectra on a standing metal-molecule nanostructure +that were measured for different setpoint conductances at T ≃ +45 mK and an external field of B = 7 T. The tip was initially +stabilized at IT = 100 pA and V = −6 mV and then moved +up by 1 ˚A in steps of 0.1 ˚A. The gray dashed line serves as a +guide for the eye. Insets show schematically how the PTCDA +molecule is pulled up by the tip. +collapse (Fig. 3b) agrees very well with the Kondo energy +scale of 291 ± 13 mK which was derived from the B-field +behaviour at low temperatures T < TK. +For the fitted Land´e factor g in Fig. 3d we also see a +strong decrease with increasing temperature. This can +be attributed to the energy renormalization [34]. Taking +this into account, we obtain an effective gyromagnetic +factor of geff = g(T)×(1+Jρ(T)) ≈ 1.91±0.01, which has +no temperature dependence. Note that the deviation of +the obtained g-factors from the B-field-dependent mea- +surements and from the perturbative approach is <∼ 6%. +Having demonstrated the sensitivity to changes of Jρ, +we now explore the possibility to tune the exchange cou- +pling mechanically. It was shown before that the standing +metal-molecule nanostructure is susceptible to attractive +forces from the tip, enabling controlled tilts, translations +and rotations [22]. If it was possible to tune the verti- +cal distance of the standing nanostructure from the sub- +strate with attractive forces from the STM tip, it might +also be possible to tune the exchange coupling Jρ. To +explore this possibility, we measured dI/dV spectra on +the standing metal-molecule nanostructure at B = 7 T +and T ≃ 45 mK for different setpoint conductances, cor- +responding to different distances between the tip and the +molecule. In Fig. 4 the fitted Jρ are plotted as a function +of setpoint conductances G. For G ≤ 0.6 · 10−4G0, the +coupling is constant at (Jρ)eq ≃ −0.075. With increasing +G, corresponding to decreasing tip-molecule distances, +|Jρ| decreases and reaches (Jρ)st ≃ −0.060 for the high- +est G. Measurements at even smaller distances (higher +setpoints) are not feasible, because the resulting larger +tunnel currents frequently induce sudden 30◦ rotations +of the standing nanostructure around its vertical axis. +Since we know that there are attractive forces acting be- + +5 +tween the molecule and the tip [22, 23], we interpret the +decreasing |Jρ| as the result of an increased distance of +the standing metal-molecule nanostructure from the sur- +face. Under the assumption that the exchange interac- +tion scales exponentially with the bond distance zB [35], +J(zB) ∝ exp(−zB/dex), the vertical relaxation ∆zB of +the bond between the standing molecule and substrate +surface can be estimated. For a typical decay length of +the exchange interaction, dex ≃ 0.4 ˚A [35], we obtain +∆zB = dex ln(Jeq/Jst) ≃ 0.09 ˚A between the smallest +and the largest G in Fig. 4. +In conclusion, we have shown that in the standing +configuration the exchange coupling between PTCDA +within the assembled nanostructure and the Ag(111) sub- +strate is strongly reduced, if compared to the flat-lying +molecule. +At B = 0 we observed a Kondo resonance +with a width of only ΓK ≃ 43 µV at an experimental +temperature of T = 30 mK. B-field-dependent measure- +ments showed that the standing metal-molecule nanos- +tructure is an S = +1/2 system with a critical field of +BC = 108 ± 5 mT. This corresponds to a Kondo tem- +perature of only TK = 291 ± 13 mK. Furthermore, we +demonstrated that, using attractive forces exerted by the +STM tip, it is possible to tune the exchange coupling be- +tween the localized spin in the nanostructure and the +substrate. The combination of the small exchange cou- +pling and the softness of the surface bond against verti- +cal distortions makes the standing metal-molecule nanos- +tructure an interesting candidate for STM-based electron +spin resonance (STM-ESR) experiments. For STM-ESR +experiments on individual atoms and molecules [1, 3– +5, 7, 16, 18, 35–40], two important requirements have to +be met [37, 41]: first, a sufficiently small coupling be- +tween the object to be investigated and the substrate, +in order to reach long relaxation and dephasing times, +and second, the possibility to drive with a high-frequency +electric field applied to the STM tip mechanical oscilla- +tions of the object in the inhomogeneous B field of the +tip, the latter being produced by a magnetic atom at +the tip apex. +Although a significant reduction of the +interaction between the atomic or molecular object of +interest with the metal substrate has been achieved on +different atomically thin insulating layers [15, 42], ESR +signals in the STM have been observed, somewhat sur- +prisingly, mainly on a bilayer of magnesium oxide (MgO) +film on Ag(001) surfaces [1, 3–5, 7, 16, 18, 35–40] and +recently for the first time on two-monolayer NaCl films +on Cu(100) [43]. In this situation, the standing metal- +molecule nanostructure may be a promising specimen: its +spin is more weakly coupled to the substrate than that +of Cu atoms on MgO/Ag(001), which are ESR active +[18], and the tip-induced displacement is about an order +of magnitude larger than the displacements required for +ESR-STM [37, 41]. It should be noted, however, that for +ESR-STM a dynamic displacement driven by the high- +frequency electric field is required, whereas in the present +experiment we so far only tested the response to static +forces between the molecule and the tip. But due to the +strong molecular polarizability of PTCDA [26], we an- +ticipate that the high-frequency electric field may have +a similar effect. In upcoming experiments we will there- +fore determine whether the dynamic displacement is suf- +ficiently large, and whether relaxation times are suffi- +ciently long for STM-ESR experiments. Finally, we note +that standing metal-molecule nanostructure can also be +prepared on the tip [26, 44, 45]. If it was indeed STM- +ESR capable, the standing nanostructure could therefore +be employed as a magnetic field sensor on the atomic +scale [13, 46], in addition to being a sensor of electric sur- +face potentials, as which it has already been used [44, 45]. +We thank Frithjof B. Anders (TU Dortmund) for +fruitful discussions. The authors acknowledge financial +support from the German Federal Ministry of Educa- +tion and Research through the funding program ’quan- +tum technologies - from basic research to market’, un- +der Q-NL (project number 13N16032). M.T. acknowl- +edges funding by the Heisenberg Program (TE 833/2- +1) of the Deutsche Forschungsgemeinschaft (DFG). +F.S.T. acknowledges funding by the DFG through SFB +1083 ”Structure and Dynamics of Internal Interfaces” +(223848855-SFB 1083). +∗ Corresponding author: t.esat@fz-juelich.de +[1] P. Willke, W. Paul, F. D. 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Limot, Atomic-scale spin sensing with a single +molecule at the apex of a scanning tunneling microscope, +Science 366, 623 (2019). + diff --git a/19FKT4oBgHgl3EQfPS1l/content/tmp_files/load_file.txt b/19FKT4oBgHgl3EQfPS1l/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..940c2b17fb2283b94c1da4c86f1edb66c93326f5 --- /dev/null +++ b/19FKT4oBgHgl3EQfPS1l/content/tmp_files/load_file.txt @@ -0,0 +1,713 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf,len=712 +page_content='Electron spin secluded inside a bottom-up assembled standing metal-molecule nanostructure Taner Esat,1, 2, ∗ Markus Ternes,1, 2, 3 Ruslan Temirov,1, 2, 4 and F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Stefan Tautz1,' metadata={'source': 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'/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 50937 Cologne,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Germany 5Experimental Physics IV A,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' RWTH Aachen University,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 52074 Aachen,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Germany (Dated: January 30,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2023) Artificial nanostructures,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' fabricated by placing building blocks such as atoms or molecules in well- defined positions,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' are a powerful platform in which quantum effects can be studied and exploited on the atomic scale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Here, we report a strategy to significantly reduce the electron-electron coupling between a large planar aromatic molecule and the underlying metallic substrate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To this end, we use the manipulation capabilities of a scanning tunneling microscope (STM) and lift the molecule into a metastable upright geometry on a pedestal of two metal atoms.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Measurements at millikelvin temperatures and magnetic fields reveal that the bottom-up assembled standing metal-molecule nanostructure has an S = 1/2 spin which is screened by the substrate electrons, resulting in a Kondo temperature of only 291 ± 13 mK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We extract the Land´e g-factor of the molecule and the exchange coupling Jρ to the substrate by modeling the differential conductance spectra using a third-order perturbation theory in the weak coupling and high-field regimes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Furthermore, we show that the interaction between the STM tip and the molecule can tune the exchange coupling to the substrate, which suggests that the bond between the standing metal-molecule nanostructure and the surface is mechanically soft.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' On the way to spin qubits based on single atoms or molecules, it is essential to minimize the interaction with the environment, since the latter leads to decoherence [1].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The scanning tunneling microscope (STM) is an ideal tool to study quantum properties of nanoscale structures, because it not only allows the magnetic states of individ- ual atoms and molecules to be read out [2] and coher- ently controlled [3–5], but also enables the environment to be changed directly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The ability to arrange atoms and molecules on surfaces with atomic precision allows for the fabrication and study of unprecedented artificial nanostructures [6, 7].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Moreover, the STM can be used to fabricate multiple absolutely identical qubits [8] from individual atoms and molecules, which can also be ar- ranged and coupled with each other as desired.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Com- pared to mesoscopic qubits, the structural control down to the atomic level may offer advantages.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Magnetic atoms and molecules with degenerate ground states on metallic surfaces typically show the Kondo ef- fect: the spin degree of freedom is quenched at temper- atures below a characteristic Kondo temperature TK by the formation of a many-electron singlet state with the electrons of the bath [9, 10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Because TK depends di- rectly on the coupling with the metal, the Kondo effect itself can be used as a gauge of the interaction with the environment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The strong hybridization of the d-orbitals of magnetic atoms with states of the metal substrate leads to TK of typically 40 - 300 K [11].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For magnetic molecules, on the other hand, Kondo temperatures of only a few Kelvin have been observed on metal surfaces [12–14], which can be explained by the weaker hybridiza- tion of the molecular orbitals with the substrate, or the shielding of the magnetic atoms by the surrounding lig- ands of the molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' However, long relaxation times T1 of several hundred nanoseconds up to days [15, 16] and dephasing times T2 in the nanosecond range [3–5] were so far only achieved for atoms and molecules that were de- coupled from the metallic surface by an atomically thin insulating layer.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The presence of the decoupling layer has also resulted in a significant reduction of TK to a few Kelvin for magnetic atoms [17, 18].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In this work, we show that exploiting the third dimension for the bottom-up assembly of standing metal-molecule nanostructures offers an alternative ap- proach to tune the coupling with the metallic sub- strate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Specifically, we show that for a single 3,4,9,10- perylenetetracarboxylic dianhydride (PTCDA) in the standing configuration on a pedestal of two Ag adatoms (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1a), both the interaction with the Ag(111) sub- strate is drastically reduced compared to the flat-lying PTCDA and the coupling with the metal substrate can be tuned by stretching the bond between the molecule and surface, utilizing the attraction between the STM tip and the molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We report the fabrication of an S = 1/2 spin nanostructure based on this strategy, with a very weak coupling to the underlying substrate, resulting in a TK of only 291 ± 13 mK — to our knowledge, the smallest TK ever measured on a metallic substrate using STM.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Comparably low TK have so far only been found in mesoscopic quantum dots [19, 20].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The Ag(111) surface was prepared in ultra-high vac- uum (UHV) by repeated Ar+ sputtering and heating at 800 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' A small coverage of PTCDA molecules was evap- orated onto the clean Ag(111) surface at room temper- arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='11762v1 [cond-mat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='mes-hall] 27 Jan 2023 2 (a) (b) (c) 10 Å Ag(111) ~17.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 Å STM tip −6 −4 −2 0 Current (pA) + −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='6 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='4 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='6 Bias voltage (mV) 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 dI/dV (10-4 G0) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (a) Schematic view of a standing PTCDA + 2Ag nanostructure on the Ag(111) surface, including the STM tip above the molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The bar shows the tunneling cur- rent IT measured above the standing nanostructure at con- stant height.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The white, grey and red spheres indicate hy- drogen, carbon and oxygen atoms, respectively, of PTCDA.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (b) Constant-height STM image above a standing nanostruc- ture recorded at a tip height of z ≃ 17.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 ˚A above the surface.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The bias voltage was V = −50 mV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The white cross marks the location where the dI/dV conductance spectra were mea- sured.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The molecular plane is indicated by the dashed orange line.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (c) dI/dV conductance spectrum (blue) on a standing metal-molecule nanostructure measured at T = 30 mK and B = 0 T (Vmod = 50 µV).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The tip was stabilized at IT = 45 pA and V = −1 mV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The red curve shows the fit based on the Frota function (see text for details).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The spectrum is shown in units of the conductance quantum G0 = 2e h .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' ature from a custom-built Knudsen cell.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' After evapora- tion, the sample was flashed at 480 K for 2 min and then cooled down to 100 K and transferred to the STM.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' All ex- periments were performed in the J¨ulich Quantum Micro- scope [21], a millikelvin scanning tunneling microscope which uses the adiabatic demagnetization of electronic magnetic moments in a magnetocaloric material to reach temperatures in the range between 30 mK and 1 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In this instrument, B fields of up to 8 T perpendicular to the sample surface can also be applied.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Differential conduc- tance (dI/dV ) spectra were measured using conventional lock-in techniques with the STM feedback loop switched off and an AC modulation amplitude Vmod = 20−100 µV and frequency fmod = 187 Hz.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The PtIr tip was treated in-situ by applying controlled voltage pulses and indenta- tions into the clean silver surface until the spectroscopic signature of the Ag(111) surface state appeared.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The standing PTCDA + 2Ag nanostructure was fabri- cated on the Ag(111) surface in three steps by controlled manipulation with the tip of the STM as described in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' First, two single Ag atoms were attached to the two carboxylic oxygens on one side of the flat-lying molecule by lateral manipulation with the tip.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Then, one of the carboxylic oxygens on the opposite side was contacted and the PTCDA molecule was pulled up on a curved trajectory until it stood upright.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The tip was then moved straight up until the bond between the molecule and the tip broke, leaving the molecule in the standing position on the two Ag adatoms [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The stability of the standing metal-molecule nanostructure arises from the balance between local covalent interactions and non- local long-range van der Waals forces [23, 24].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In constant-height STM images, the standing metal- molecule nanostructure can be recognized by two fea- tures that are distributed symmetrically around the plane of the molecule (dashed orange line in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1b) and separated by a nodal plane perpendicular to the latter (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' It is interesting to note that the node of the π- orbital in the plane of the molecule could not be resolved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The two features coincide with the positions where the interaction with the tip is most pronounced [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In the standing configuration, there is only a weak overlap be- tween the wave functions of the metallic surface and the lowest unoccupied molecular orbital (LUMO) of PTCDA, because the lobes of the molecular π-orbital are oriented perpendicular to the plane of the molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This allows the standing nanostructure to function as a quantum dot and coherent field emitter [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' At mK temperatures, a peak at zero bias is evident in the dI/dV spectrum measured on a standing metal- molecule nanostructure (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1c).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In fact, at these low temperatures we additionally observe a dip at zero bias due to the dynamical Coulomb blockade (DCB) [25].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We have thus corrected all dI/dV spectra on the standing nanostructure for the DCB dip (see Supplementary Ma- terial).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Previous studies have hinted that the LUMO of the standing metal-molecule nanostructure must contain a single unpaired electron [22, 26].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Therefore, it is plausi- ble to assume that the zero-bias peak originates from the Kondo effect, in which the spin of this localized electron is screened by itinerant substrate electrons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To verify this, we measured dI/dV spectra at different B fields.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Already at B ≈ 100 − 120 mT a Zeeman splitting of the zero-bias peak is discernable (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2a).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' At higher B fields, the Kondo effect is completely quenched and the spectrum is dominated by the symmetric steps arising from inelastic spin-flip excitations (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To extract the precise energy of the Zeeman splitting ∆, we calculated the numerical derivative of the dI/dV spectra and fitted the peak positions with a Gaussian (see Supplementary Material).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' As shown in Figs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2c and d, the energies of the spin-flip excitations scale linearly with the external B field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Only close to the critical field BC, which is required to initially split the Kondo resonance, 3 −1 0 1 Bias voltage (mV) 1 2 3 4 dI/dV (10-4 G0) 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='2 B field (T) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='00 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='01 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='02 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='03 Δ (mV) (a) (b) (c) (d) 1 T 3 T 5 T 7 T 2Δ −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='25 0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='25 Bias voltage (mV) 15 20 25 30 35 dI/dV (10-4 G0) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='08 T 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='20 T 0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 B field (T) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='6 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='8 Δ (mV) g = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='006 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='007 FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (a)-(b) dI/dV spectra (blue) on a standing metal- molecule nanostructure, measured at different B fields at T ≃ 50 mK (setpoints in panel (a) were IT = 100 pA, V = −10 mV, Vmod = 100 µV and IT = 100 pA, V = −1 mV, Vmod = 20 µV in panel(b)).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In panel (a), the B field was changed in steps of 20 mT.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The orange curves in panel (b) show the fits based on perturbation theory (see text for de- tails).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The spectra are vertically displaced for clarity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (c)-(d) The Zeeman splitting ∆ extracted from the dI/dV spectra as a function of B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The gray dashed line in panel (c) serves as a guide for the eye.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The red curve in panel (d) shows the linear fit for the Zeeman splitting.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' the Zeeman energy rises noticeably faster with increas- ing B field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To extract the Land´e factor g, we consider only the data points at B fields ≥ 1 T (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2b) since the Kondo effect in the strong coupling regime leads to renormalization of the g-factor.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' A linear fit of the form ∆ = gµBB for the Zeeman effect, where µB is the Bohr magneton, yields a Land´e factor g = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='006 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='007.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' By interpolating the data points at low B fields, we obtain BC = 108±5 mT for the critical field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Using the relation [27] BC = 1 2 kBTK gµB , (1) valid for temperatures T < 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='25 TK, this gives an esti- mate of 291 ± 13 mK for the Kondo temperature TK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' An independent estimate of the Kondo temperature TK can be obtained from the width of the Kondo reso- nance (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1c).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' However, it should be noted that this is only a rough estimate, since the width of the Kondo reso- nance is related to TK by a non-universal scaling constant [28].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To extract its width, we fitted the Kondo resonance with a Frota line shape [29] ρ(E)Frota = ℜ � iΓK E − E0 + iΓK .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (2) Additional broadening effects due to the Fermi distri- bution and the modulation amplitude were taken into account.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The best fit then yields a width of ΓK ≃ 43 µV and thus a TK = ΓK(2π × 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='103)/kB ≃ 320 mK [29], in good agreement with the above estimate from the B field dependence.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We attribute the features in the dI/dV spectrum at approximately ±0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='25 mV and ±0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='55 mV (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 1c and Supplementary Material) to ei- ther molecular vibrations or frustrated translations of the standing metal-molecule nanostructure [23].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Note that a strong electron-vibrational coupling can also lead to a further decrease of TK [30].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The low Kondo temperature of the standing nanostruc- ture in conjunction with the low base temperature and high energy resolution of our mK STM enable us to quan- titatively describe the interaction of the localized spin with its environment, also as a function of temperature.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For this purpose, we employ the Anderson-Appelbaum model [31–33] and calculate the tunneling conductance from the Kondo Hamiltonian in a perturbative approach that includes processes up to third order in the exchange interaction J [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The model allows tunneling electrons to interact with the localized spin via spin-spin (tT S ˆσt·ˆS) or potential scattering (tT S U).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Here tT S is the matrix element for a transition from the tip to the molecule or vice versa, and ˆσt and ˆS are the spin operators of the tunneling and localized electrons, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In addi- tion, the model takes into account the spin-spin exchange scattering between the electrons of the substrate and the localized spin (Jρ ˆσs · ˆS), where ρ denotes the substrate’s electron density at the Fermi energy and ˆσs the spin oper- ator of itinerant electrons in the substrate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This approach provides the correct description under the following con- ditions: the magnetic impurity is predominantly coupled to one of the electrodes (here the substrate), the system is in equilibrium (limit of small bias voltages), and the system is in the weak coupling limit (T >∼ TK) or high- field regime (B >∼ kBTK).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We performed least-square fits and extracted the dimensionless coupling strength Jρ between the substrate and the localized electron and its Land´e factor g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Before we focus on the temperature dependence, we first examine the influence of the B field on Jρ at 50 mK (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' As the B field increases, we see a decrease in the height of the peak structure on top of the steps originating from spin-flip excitations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Since those peak heights are proportional to Jρ [34], this indicates that |Jρ| decreases with increasing B field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This is clearly seen in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3a, where the fitted Jρ is plotted versus B field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' It may at first sight seem surprising that we still observe a coupling between the localized and itinerant spins at high B fields.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This behaviour is, however, in 4 −1 0 1 Bias voltage (mV) 1 2 3 4 5 dI/dV (10-4 G0) (a) (b) (c) (d) 1009 mK 751 mK 275 mK 70 mK 41 mK 0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 B field (T) −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='10 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='09 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='08 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='07 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='06 Jρ 0 500 1000 Temperature (mK) −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='06 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='05 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='04 Jρ ~TK 0 500 1000 Temperature (mK) 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='90 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='95 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='00 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='05 g-factor FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (a) Coupling strength Jρ as extracted from the fits in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2b as a function of B field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (b) dI/dV spectra (blue) on a standing metal-molecule nanostructure, measured at differ- ent temperatures in an external field B = 7 T (IT = 100 pA, V = −10 mV, Vmod = 100 µV).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The orange curves show the fits based on perturbation theory (see text for details).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The spectra are vertically displaced for clarity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (c) Coupling strength Jρ as extracted from the fits as a function of tem- perature.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The dashed blue line indicates the Kondo energy scale TK as determined from the B-field data of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' (d) Land´e g-factor estimated from the fits in panel (b) (black) and the effective g-factor geff after taking into account renor- malization effects due to the exchange interaction (red).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The red line illustrates a linear fit and the red shaded area the corresponding confidence interval.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' good agreement with numerical renormalization group (NRG) calculations for an S = 1/2 Kondo impurity at finite temperatures and B fields [27], in which it was shown that the intensity of the split Kondo resonance varies even if µBB/kBTK ≫ 1, which corresponds to the present situation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In other words, we have even at high B fields access to bias driven Kondo correlations whose gradual emergence at decreasing temperatures drives |Jρ| up.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This behavior can be readily observed by looking at the temperature-dependent data for constant B = 7 T (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The fits reveal that |Jρ| increases with decreas- ing temperature (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3c).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For B = 0, such an increase of |Jρ| would signal the progressive breakdown of the perturbation approach, yielding a divergence of Jρ and the crossover into the Kondo singlet as a new ground state [9, 10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' However, here we are in the high-field regime and therefore will not reach the Kondo ground state even in the limit T → 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We note that the tem- perature range in which the perturbation theory starts to 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='0 Setpoint conductance (10-4 G0) −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='075 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='070 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='065 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='060 Jρ zB,eq zB,st FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Coupling strength Jρ as extracted from the fits of dI/dV spectra on a standing metal-molecule nanostructure that were measured for different setpoint conductances at T ≃ 45 mK and an external field of B = 7 T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The tip was initially stabilized at IT = 100 pA and V = −6 mV and then moved up by 1 ˚A in steps of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='1 ˚A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The gray dashed line serves as a guide for the eye.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Insets show schematically how the PTCDA molecule is pulled up by the tip.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' collapse (Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3b) agrees very well with the Kondo energy scale of 291 ± 13 mK which was derived from the B-field behaviour at low temperatures T < TK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For the fitted Land´e factor g in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3d we also see a strong decrease with increasing temperature.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This can be attributed to the energy renormalization [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Taking this into account, we obtain an effective gyromagnetic factor of geff = g(T)×(1+Jρ(T)) ≈ 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='91±0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='01, which has no temperature dependence.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Note that the deviation of the obtained g-factors from the B-field-dependent mea- surements and from the perturbative approach is <∼ 6%.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Having demonstrated the sensitivity to changes of Jρ, we now explore the possibility to tune the exchange cou- pling mechanically.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' It was shown before that the standing metal-molecule nanostructure is susceptible to attractive forces from the tip, enabling controlled tilts, translations and rotations [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' If it was possible to tune the verti- cal distance of the standing nanostructure from the sub- strate with attractive forces from the STM tip, it might also be possible to tune the exchange coupling Jρ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' To explore this possibility, we measured dI/dV spectra on the standing metal-molecule nanostructure at B = 7 T and T ≃ 45 mK for different setpoint conductances, cor- responding to different distances between the tip and the molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 4 the fitted Jρ are plotted as a function of setpoint conductances G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For G ≤ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='6 · 10−4G0, the coupling is constant at (Jρ)eq ≃ −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='075.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' With increasing G, corresponding to decreasing tip-molecule distances, |Jρ| decreases and reaches (Jρ)st ≃ −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='060 for the high- est G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Measurements at even smaller distances (higher setpoints) are not feasible, because the resulting larger tunnel currents frequently induce sudden 30◦ rotations of the standing nanostructure around its vertical axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Since we know that there are attractive forces acting be- 5 tween the molecule and the tip [22, 23], we interpret the decreasing |Jρ| as the result of an increased distance of the standing metal-molecule nanostructure from the sur- face.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Under the assumption that the exchange interac- tion scales exponentially with the bond distance zB [35], J(zB) ∝ exp(−zB/dex), the vertical relaxation ∆zB of the bond between the standing molecule and substrate surface can be estimated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For a typical decay length of the exchange interaction, dex ≃ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='4 ˚A [35], we obtain ∆zB = dex ln(Jeq/Jst) ≃ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='09 ˚A between the smallest and the largest G in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In conclusion, we have shown that in the standing configuration the exchange coupling between PTCDA within the assembled nanostructure and the Ag(111) sub- strate is strongly reduced, if compared to the flat-lying molecule.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' At B = 0 we observed a Kondo resonance with a width of only ΓK ≃ 43 µV at an experimental temperature of T = 30 mK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' B-field-dependent measure- ments showed that the standing metal-molecule nanos- tructure is an S = 1/2 system with a critical field of BC = 108 ± 5 mT.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' This corresponds to a Kondo tem- perature of only TK = 291 ± 13 mK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Furthermore, we demonstrated that, using attractive forces exerted by the STM tip, it is possible to tune the exchange coupling be- tween the localized spin in the nanostructure and the substrate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The combination of the small exchange cou- pling and the softness of the surface bond against verti- cal distortions makes the standing metal-molecule nanos- tructure an interesting candidate for STM-based electron spin resonance (STM-ESR) experiments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' For STM-ESR experiments on individual atoms and molecules [1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 3– 5,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 7,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 16,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 18,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 35–40],' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' two important requirements have to be met [37,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' 41]: first,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' a sufficiently small coupling be- tween the object to be investigated and the substrate,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' in order to reach long relaxation and dephasing times,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' and second,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' the possibility to drive with a high-frequency electric field applied to the STM tip mechanical oscilla- tions of the object in the inhomogeneous B field of the tip,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' the latter being produced by a magnetic atom at the tip apex.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Although a significant reduction of the interaction between the atomic or molecular object of interest with the metal substrate has been achieved on different atomically thin insulating layers [15, 42], ESR signals in the STM have been observed, somewhat sur- prisingly, mainly on a bilayer of magnesium oxide (MgO) film on Ag(001) surfaces [1, 3–5, 7, 16, 18, 35–40] and recently for the first time on two-monolayer NaCl films on Cu(100) [43].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In this situation, the standing metal- molecule nanostructure may be a promising specimen: its spin is more weakly coupled to the substrate than that of Cu atoms on MgO/Ag(001), which are ESR active [18], and the tip-induced displacement is about an order of magnitude larger than the displacements required for ESR-STM [37, 41].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' It should be noted, however, that for ESR-STM a dynamic displacement driven by the high- frequency electric field is required, whereas in the present experiment we so far only tested the response to static forces between the molecule and the tip.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' But due to the strong molecular polarizability of PTCDA [26], we an- ticipate that the high-frequency electric field may have a similar effect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' In upcoming experiments we will there- fore determine whether the dynamic displacement is suf- ficiently large, and whether relaxation times are suffi- ciently long for STM-ESR experiments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Finally, we note that standing metal-molecule nanostructure can also be prepared on the tip [26, 44, 45].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' If it was indeed STM- ESR capable, the standing nanostructure could therefore be employed as a magnetic field sensor on the atomic scale [13, 46], in addition to being a sensor of electric sur- face potentials, as which it has already been used [44, 45].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' We thank Frithjof B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Anders (TU Dortmund) for fruitful discussions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' The authors acknowledge financial support from the German Federal Ministry of Educa- tion and Research through the funding program ’quan- tum technologies - from basic research to market’, un- der Q-NL (project number 13N16032).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' acknowl- edges funding by the Heisenberg Program (TE 833/2- 1) of the Deutsche Forschungsgemeinschaft (DFG).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' acknowledges funding by the DFG through SFB 1083 ”Structure and Dynamics of Internal Interfaces” (223848855-SFB 1083).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' ∗ Corresponding author: t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='esat@fz-juelich.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content='de [1] P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Willke, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Paul, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Natterer, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Yang, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Bae, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Choi, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Fern´andez-Rossier, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/19FKT4oBgHgl3EQfPS1l/content/2301.11762v1.pdf'} +page_content=' Heinrich, , and C.' metadata={'source': 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REWARD +DAMIAN JELITO∗,† AND �LUKASZ STETTNER∗ +Abstract. We consider a long-run impulse control problem for a generic +Markov process with a multiplicative reward functional. We construct a solu- +tion to the associated Bellman equation and provide a verification result. The +argument is based on the probabilistic properties of the underlying process +combined with the Krein-Rutman theorem applied to the specific non-linear +operator. Also, it utilises the approximation of the problem in the bounded +domain and with the help of the dyadic time-grid. +Keywords: impulse control, Bellman equation, risk-sensitive criterion, Markov +process +MSC2020 subject classifications: 93E20, 49J21, 49K21, 60J25 +1. Introduction +Impulse control constitutes a versatile framework for controlling real-life stochas- +tic systems. In this type of control, a decision-maker determines intervention times +and instantaneous after-intervention states of the controlled process. By doing so, +one can affect a continuous time phenomenon in a discrete time manner. Conse- +quently, impulse control attracted considerable attention in the mathematical liter- +ature; see e.g. [4, 9, 26] for classic contributions and [3, 10, 19, 21] for more recent +results. In addition to generic mathematical properties, impulse control problems +were studied with reference to specific applications including i.a. controlling ex- +change rates, epidemics, and portfolios with transaction costs; see e.g. [18, 25, 27] +and references therein. +When looking for an optimal impulse control strategy, one must decide on the +optimality criterion. +Recently, considerable attention was paid to the so-called +risk-sensitive functional given, for any γ ∈ R, by +µγ(Z) := +� +1 +γ ln E[exp(γZ)], +γ ̸= 0, +E[Z], +γ = 0, +(1.1) +where Z is a (random) payoff corresponding to a chosen control strategy; see [14] for +a seminal contribution. This functional with γ = 0 corresponds to the usual linear +criterion and the case γ < 0 is associated with risk-averse preferences; see [5] for +a comprehensive overview. Also, the functional with γ > 0 could be linked to the +asymptotics of the power utility function; see [31] for details. Recent comprehensive +discussion on the long-run version with µγ could be found in [6]. We refer also +∗Institute of Mathematics, Polish Academy of Sciences, Warsaw, Poland +E-mail addresses: djelito@impan.pl, l.stettner@impan.pl. +†Corresponding author. +1 + +2 +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +to [23] and references therein for a discussion on the connection between (1.1) and +the duality of the large deviations-based criteria. +In this paper we focus on the use of the functional µγ with γ > 0. More specif- +ically, we consider the impulse control problem for some continuous time Markov +process and construct a solution to the associated Bellman equation which char- +acterises an optimal impulse control strategy. To do this, we study the family of +impulse control problems in bounded domains and then extend the analysis to the +generic locally compact state space. This idea was used in [1], where PDEs tech- +niques were applied to obtain the characterisation of the controlled diffusions in the +risks-sensitive setting. A similar approximation for the the average cost per unit +time problem was considered in [32]. +The main contribution of this paper is a construction of a solution to the Bell- +man equation associated with the problem, see Theorem 5.1 for details. It should +be noted that we get a bounded solution even though the state space could be +unbounded and we assume virtually no ergodicity conditions for the uncontrolled +process. Also, note that present results for γ > 0 complement our recent findings +on the impulse control with the risk-averse preferences; see [24] for the dyadic case +and [15] for the continuous time framework. Nevertheless, it should be noted that +the techniques for γ < 0 and γ > 0 are substantially different and it is not possible +to directly transform the results in one framework to the other; see e.g. [16, 20] for +further discussion. +The structure of this paper is as follows. In Section 2 we formally introduce +the problem, discuss the assumptions and, in Theorem 2.3, provide a verification +argument. Next, in Section 3 we consider an auxiliary dyadic problem in a bounded +domain and in Theorem 3.1 we construct a solution to the corresponding Bellman +equation. This is used in Section 4 where we extend our analysis to the unbounded +domain with the dyadic time-grid; see Theorem 4.2. Next, in Section 5 we finally +construct a solution to the Bellman equation for the original problem; see Theo- +rem 5.1. Finally, in Appendix A we discuss some properties of the optimal stopping +problems that are used in this paper. +2. Preliminaries +Let X = (Xt)t≥0 be a continuous time standard Feller–Markov process on a +filtered probability space (Ω, F, (Ft), P). The process X takes values in a locally +compact separable metric space E endowed with a metric ρ and the Borel σ-field +E. With any x ∈ E we associate a probability measure Px describing the evolution +of the process X starting in x; see Section 1.4 in [28] for details. Also, we use Ex, +x ∈ E, and Pt(x, A) := Px[Xt ∈ A], t ≥ 0, x ∈ E, A ∈ E, for the corresponding +expectation operator and the transition probability, respectively. +By Cb(E) we +denote the family of continuous bounded real-valued functions on E. +Also, to +ease the notation, by T , Tx, and Tx,b we denote the families of stopping times, +Px a.s. finite stopping times, and Px a.s. bounded stopping times, respectively. +Also, for any δ > 0, by T δ ⊂ T , T δ +x ⊂ Tx, and T δ +x,b ⊂ Tx,b, we denote the +respective subfamilies of dyadic stopping times, i.e. +those taking values in the +set {0, δ, 2δ, . . .} ∪ {∞}. +Throughout this paper we fix some compact U ⊆ E and we assume that a +decision-maker is allowed to shift the controlled process to U. This is done with +the help of an impulse control strategy, i.e. a sequence V := (τi, ξi)∞ +i=1, where (τi) + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +3 +is an increasing sequence of stopping times and (ξi) is a sequence of Fτi-measurable +after-impulse states with values in U. With any starting point x ∈ E and a strategy +V we associate a probability measure P(x,V ) for the controlled process Y . Under this +measure, the process starts at x and follows its usual (uncontrolled) dynamics up +to the time τ1. Then, it is immediately shifted to ξ1 and starts its evolution again, +etc. More formally, we consider a countable product of filtered spaces (Ω, F, (Ft)) +and a coordinate process (X1 +t , X2 +t , . . .). Then, we define the controlled process Y +as Yt := Xi +t, t ∈ [τi−1, τi) with the convention τ0 ≡ 0. Under the measure P(x,V ) +we get Yτi = ξi; we refer to Chapter V in [26] for the construction details; see +also Appendix in [8] and Section 2 in [29]. A strategy V = (τi, ξi)∞ +i=1 is called +admissible if for any x ∈ E we get P(x,V )[limn→∞ τn = ∞] = 1. The family of +admissible impulse control strategies is denoted by V. Also, note that, to simplify +the notation, by Yτ − +i := Xi +τi, i ∈ N∗, we denote the state of the process right before +the ith impulse (yet, possibly, after the jump). +In this paper we study the asymptotics of the impulse control problem given by +sup +V ∈V +J(x, V ), +x ∈ E, +(2.1) +where, for any x ∈ E and V ∈ V, we set +J(x, V ) := lim inf +T →∞ +1 +T ln E(x,V ) +� +e +� T +0 f(Ys)ds+�∞ +i=1 1{τi≤T }c(Yτ− +i +,ξi)� +, +(2.2) +with f denoting the running cost function and c being the shift-cost function, +respectively. Note that this could be seen as a long-run standardised version of +the functional (1.1) with γ > 0 applied to the impulse control framework. Here, +the standardisation refers to the fact that we do not use directly the parameter γ +(apart from its sign). Also, the problem is of the long-run type, i.e. the utility is +averaged over time which improves the stability of the results. +The analysis in this paper is based on the approximation of the problem in a +bounded domain. +Thus, we fix a sequence (Bm)m∈N of compact sets satisfying +Bm ⊂ Bm+1 and E = �∞ +m=0 Bm. Also, we assume that U ⊂ B0. Next, we assume +the following conditions. +(A1) (Cost functions). The map f : E �→ R− is a continuous and bounded. Also, +the map c : E × U �→ R− is continuous, bounded, and strictly non-positive, +and satisfies the triangle inequality, i.e. for some c0 < 0, we have +0 > c0 ≥ c(x, ξ) ≥ c(x, η) + c(η, ξ), +x ∈ E, ξ, η ∈ U. +Also, we assume that c satisfies the uniform limit at infinity condition +lim +∥x∥,∥y∥→∞ sup +ξ∈U +|c(x, ξ) − c(y, ξ)| = 0. +(2.3) +(A2) (Transition probability continuity). For any t, the transition probability Pt +is continuous with respect to the total variation norm, i.e. for any sequence +(xn) ⊂ E converging to x ∈ E, we get +lim +n→∞ sup +A∈E +|Pt(xn, A) − Pt(x, A)| = 0. +(A3) (Distance control). For any compact set Γ ⊂ E, t0 > 0, and r0 > 0, we +have +lim +r→∞ MΓ(t0, r) = 0, +lim +t→0 MΓ(t, r0) = 0, +(2.4) + +4 +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +where MΓ(t, r) := supx∈Γ Px[sups∈[0,t] ρ(Xs, x) ≥ r], t, r > 0. +(A4) (Process irreducibility). For any m ∈ N, x ∈ Bm, δ > 0, and any open set +O ⊂ Bm, we have +Px [∪∞ +i=1{Xiδ ∈ O}] = 1. +Also, we assume that for any x ∈ E, δ > 0, and m ∈ N, we have +Px[τBm < ∞] = 1 +(2.5) +where τBm := δ inf{k ∈ N: Xkδ /∈ Bm}. +Before we proceed, let us comment on these assumptions. First, note that (A1) +states typical cost-functions conditions. In particular, the non-positivity assump- +tion for f is merely a technical normalisation. Indeed, for a generic ˜f ∈ Cb(E) we +may set f(·) := ˜f(·) − ∥ ˜f∥ ≤ 0 to get +Jf(x, V ) = J +˜f(x, V ) − ∥ ˜f∥, +x ∈ E, V ∈ V, +where Jf denotes the version of the functional J from (2.2) corresponding to the +running cost function f. +Second, Assumption (A2) states that the transition probabilities Pt(x, ·) are +continuous with respect to the total variation norm. Note that this directly implies +that the transition semigroup associated to X is strong Feller, i.e. for any t > 0 +and a bounded measurable map h: E �→ R, the map x �→ Ex[h(Xt)] is continuous +and bounded. +Third, Assumption (A3) quantifies distance control properties of the underlying +process. It states that, for a fixed time horizon, the process with a high probability +stays close to its starting point and, with a fixed radius, with a high probability it +does not leave the corresponding ball with a sufficiently short time horizon. Note +that these properties are automatically satisfied if the transition semigroup is C0- +Feller; see Proposition 2.1 in [21] and Proposition 6.4 in [2] for details. +Finally, Assumption (A4) states a form of the irreducibility of the process X. It +requires that the process visits a sufficiently rich family of sets with unit probability. +To solve (2.1), we show the existence of a solution to the impulse control Bellman +equation, i.e. a function w ∈ Cb(E) and a constant λ ∈ R satisfying +w(x) = sup +τ∈Tx,b +ln Ex +� +exp +�� τ +0 +(f(Xs) − λ)ds + Mw(Xτ) +�� +, +x ∈ E, +(2.6) +where the operator M is given by +Mh(x) := sup +ξ∈U +(c(x, ξ) + h(ξ)), +h ∈ Cb(E), x ∈ E. +We start with a simple observation giving a lower bound for the constant λ +from (2.6). To do this, we define the semi-group type by +r(f) := lim +t→∞ +1 +t ln sup +x∈E +Ex +� +e +� t +0 f(Xs)ds� +; +(2.7) +see e.g. Proposition 1 in [30] for a discussion on the properties of r(f). +Lemma 2.1. Let (w, λ) be a solution to (2.6). Then, we get λ ≥ r(f). +Proof. From (2.6), for any T ≥ 0, we get +w(x) ≥ ln Ex +� +e +� T +0 (f(Xs)−λ)ds+Mw(XT )� +. + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +5 +Thus, using the boundedness of w and Mw, we get +∥w∥ ≥ sup +x∈E +ln Ex +� +e +� T +0 (f(Xs)−λ)ds� +− ∥Mw∥. +Consequently, dividing both hand-sides by T and letting T → ∞, we get 0 ≥ +r(f − λ), which concludes the proof. +□ +Let us now link a solution to (2.6) with the optimal value and an optimal strategy +for (2.1). To ease the notation, we recursively define the strategy ˆV := (ˆτi, ˆξi)∞ +i=1 +for i ∈ N \ {0} by +� +ˆτi +:= inf{t ≥ ˆτi−1 : w(Xi +t) = Mw(Xi +t)}, +ˆξi +:= arg maxξ∈U +� +c(Xi +ˆτi, ξ) + w(ξ) +� +1{ˆτi<∞} + ξ01{ˆτi=∞}, +(2.8) +where ˆτ0 := 0 and ξ0 ∈ U is some fixed point. First, we show that ˆV is a proper +strategy. +Proposition 2.2. The strategy ˆV given by (2.8) is admissible. +Proof. To ease the notation, we define N(0, T ) := �∞ +i=1 1{ˆτi≤T }, T ≥ 0. We fix +some T > 0 and x ∈ E, and show that we get +P(x, ˆV )[N(0, T ) = ∞] = 0. +(2.9) +Recalling (2.8), on the event A := {limi→∞ ˆτi < +∞}, for any n ∈ N, n ≥ 1, +we get w(Xn +ˆτn) = Mw(Xn +ˆτn) = c(Xn +ˆτn, Xn+1 +ˆτn +) + w(Xn+1 +ˆτn +). +Also, recalling that +c(x, ξ) ≤ c0 < 0, x ∈ E, ξ ∈ U, for any n ∈ N, n ≥ 1, we have w(Xn+1 +ˆτn +)−w(Xn +ˆτn) = +−c(Xn +ˆτn, Xn+1 +ˆτn +) ≥ −c0 > 0. Using this observation and Assumption (A3), we esti- +mate the distance between consecutive impulses which will be used to prove (2.9). +More specifically, for any k, m ∈ N, k, m ≥ 1, we get +k+m−2 +� +n=k +(w(Xn+1 +ˆτn +) − w(Xn+1 +ˆτn+1)) + (w(Xk+m +ˆτk+m−1) − w(Xk+1 +ˆτk +)) += w(Xk+1 +ˆτk +) + +k+m−1 +� +n=k+1 +(w(Xn+1 +ˆτn +) − w(Xn +ˆτn)) − w(Xk+1 +ˆτk +) += +k+m−1 +� +n=k+1 +(w(Xn+1 +ˆτn +) − w(Xn +ˆτn)) ≥ −(m − 1)c0; +(2.10) +it should be noted that the specific values for k and m will be determined later. +Using the continuity of w we may find K > 0 such that supx,y∈U(w(x) − w(y)) ≤ +K. +Let m ∈ N be big enough to get −(m − 1) c0 +2 +> K. +Thus, noting that +Xk+m +ˆτk+m−1, Xk+1 +ˆτk +∈ U, we have (w(Xk+m +ˆτk+m−1) − w(Xk+1 +ˆτk +)) ≤ K < −(m − 1) c0 +2 . Con- +sequently, recalling (2.10), on A, we get +k+m−2 +� +n=k +(w(Xn+1 +ˆτn +) − w(Xn+1 +ˆτn+1)) ≥ −(m − 1)c0 +2 . +(2.11) +Recalling the compactness of U and the continuity of w we may find r > 0 such +that for any x ∈ U and y ∈ E satisfying ρ(x, y) < r we get |w(x) − w(y)| < − c0 +2 . + +6 +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +Let us now consider the family of events +Bk := +k+m−2 +� +n=k +{ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+1) < r}, +k ∈ N, k ≥ 1, +(2.12) +and note that, for any k ∈ N, k ≥ 1, on Bk ∩ A we have �k+m−2 +n=k +(w(Xn+1 +ˆτn +) − +w(Xn+1 +ˆτn+1)) < −(m − 1) c0 +2 . Thus, recalling (2.11), for any k ∈ N, k ≥ 1, we get +P(x0, ˆV )[Bk ∩ A] = 0 and, in particular, we have +P(x0, ˆV )[Bk ∩ {N(0, T ) = ∞}] = 0. +(2.13) +Let us now show that lim supk→∞ P(x0, ˆV )[Bc +k ∩{N(0, T ) = ∞}] = 0. Noting that +{N(0, T ) = ∞} = {limi→∞ ˆτi ≤ T }, for any t0 > 0 and k ∈ N, k ≥ 1, we get +P(x0, ˆV ) [Bc +k ∩ {N(0, T ) = ∞}] +≤ P(x0, ˆV ) +��k+m−2 +� +n=k +{ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+1) ≥ r} ∩ {ˆτn+1 − ˆτn ≤ t0} +� +∩ { lim +i→∞ ˆτi ≤ T } +� ++ P(x0, ˆV ) +��k+m−2 +� +n=k +{ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+1) ≥ r} ∩ {ˆτn+1 − ˆτn > t0} +� +∩ { lim +i→∞ ˆτi ≤ T } +� +≤ P(x0, ˆV ) +�k+m−2 +� +n=k +{ sup +t∈[0,t0] +ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+t) ≥ r} ∩ { lim +i→∞ ˆτi ≤ T } +� ++ P(x0, ˆV ) +�k+m−2 +� +n=k +{ˆτn+1 − ˆτn > t0} ∩ { lim +i→∞ ˆτi ≤ T } +� +. +(2.14) +Using Assumption (A3), for any ε > 0, we may find t0 > 0, such that +sup +x∈U +Px +� +sup +t∈[0,t0] +ρ(X0, Xt) ≥ r +� +≤ +ε +m − 1. +(2.15) +Thus, using the strong Markov property and noting that Xn+1 +ˆτn +∈ U, for any k ∈ N, +k ≥ 1, we get +P(x0, ˆV ) +�k+m−2 +� +n=k +{ sup +t∈[0,t0] +ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+t) ≥ r} ∩ { lim +i→∞ ˆτi ≤ T } +� +≤ +k+m−2 +� +n=k +P(x0, ˆV ) +� +{ sup +t∈[0,t0] +ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+t) ≥ r} ∩ {ˆτn ≤ T } +� += +k+m−2 +� +n=k +P(x0, ˆV ) +� +{ˆτn ≤ T }PXn+1 +ˆτn +� +sup +t∈[0,t0] +ρ(X0, Xt) ≥ r +�� +≤ ε. +(2.16) +Recalling that ε > 0 was arbitrary, for any k ∈ N, k ≥ 1, we get +P(x0, ˆV ) +�k+m−2 +� +n=k +{ sup +t∈[0,t0] +ρ(Xn+1 +ˆτn +, Xn+1 +ˆτn+t) ≥ r} ∩ { lim +i→∞ ˆτi ≤ T } +� += 0. +(2.17) + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +7 +Now, to ease the notation, let Ck := �∞ +n=k{ˆτn+1 − ˆτn > t0} ∩ {limi→∞ ˆτi ≤ T }, +k ∈ N, k ≥ 1, and note that Ck+1 ⊂ Ck, k ∈ N, k ≥ 1. We show that +lim +k→∞ P(x0, ˆV ) [Ck] = 0. +For the contradiction, assume that limk→∞ P(x0, ˆV ) [Ck] > 0. Consequently, we get +P(x0, ˆV ) [�∞ +k=1 Ck] > 0. Note that for any ω ∈ �∞ +k=1 Ck we have limi→∞ ˆτi(ω) ≤ T . +In particular, we may find i0 ∈ N such that for any n ≥ i0 we get ˆτn+1(ω)− ˆτn(ω) ≤ +t0 +2 . This leads to the contradiction as from the fact that ω ∈ �∞ +k=1 Ck we also get +ω ∈ +∞ +� +k=1 +∞ +� +n=k +{ˆτn+1 − ˆτn > t0} ⊂ +∞ +� +n=i0 +{ˆτn+1 − ˆτn > t0}. +Consequently, we get limk→∞ P(x0, ˆV ) [Ck] = 0 and, in particular, we get +lim sup +k→∞ +P(x0, ˆV ) +�k+m−2 +� +n=k +{ˆτn+1 − ˆτn > t0} ∩ { lim +i→∞ ˆτi ≤ T } +� +≤ lim +k→∞ P(x0, ˆV ) [Ck] = 0. +Hence, recalling (2.14) and (2.17), we get +lim sup +k→∞ +P(x0, ˆV ) [Bc +k ∩ {N(0, T ) = ∞}] = 0. +Thus, recalling (2.13), for any k ∈ N, k ≥ 1, we obtain +P(x0, ˆV ) [N(0, T ) = ∞] = P(x0, ˆV ) [Bc +k ∩ {N(0, T ) = ∞}] , +and letting k → ∞, we conclude the proof of (2.9). +□ +Now, we show the verification result linking (2.6) with the optimal value and an +optimal strategy for (2.1). +Theorem 2.3. Let (w, λ) be a solution to (2.6) with λ > r(f). Then, we get +λ = sup +V ∈V +J(x, V ) = J(x, ˆV ), +x ∈ E, +where the strategy ˆV is given by (2.8). +Proof. The proof is based on the argument from Theorem 4.4 in [15] thus we show +only an outline. First, we show that λ = J(x, ˆV ), x ∈ E, where the strategy ˆV is +given by (2.8). Let us fix x ∈ E. Then, combining the argument used in Lemma +7.1 in [2] and Proposition A.3, we get that the process +e +� ˆτ1∧T +0 +(f(X1 +s )−λ)ds+w(X1 +ˆτ1∧T ), +T ≥ 0, +is a P(x, ˆV )-martingale. Noting that on the event {ˆτk+1 < T } we get w(Xk+1 +ˆτk+1) = +Mw(Xk+1 +ˆτk+1) = c(Xk+1 +ˆτk+1, ˆξk+1) + w(ˆξk+1), k ∈ N, for any n ∈ N we recursively get +ew(x) = E(x, ˆV ) +� +e +� ˆτ1∧T +0 +(f(Ys)−λ)ds+w(X1 +ˆτ1∧T )� += E(x, ˆV ) +� +e +� ˆτ1∧T +0 +(f(Ys)−λ)ds+1{ˆτ1 0 and m ∈ N. We show the existence of a map wm +δ ∈ Cb(Bm) +and a constant λm +δ ∈ R satisfying +wm +δ (x) = sup +τ∈T δ +x,b +ln Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +δ )ds+Mwm +δ (Xτ∧τBm ) +� +, +x ∈ Bm. +(3.1) + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +9 +In fact, we start with the analysis of an associated one-step equation. More specif- +ically, we show the existence of a constant λm +δ +∈ R and a map wm +δ +∈ Cb(Bm) +satisfying +wm +δ (x) = max +� +ln Ex +� +e +� δ +0 (f(Xs)−λm +δ )ds+1{Xδ∈Bm}wm +δ (Xδ)+1{Xδ / +∈Bm}Mwm +δ (Xδ)� +, +Mwm +δ (x) +� +, +x ∈ Bm, +wm +δ (x) = Mwm +δ (x), +x /∈ Bm; +(3.2) +see Theorem 3.1 for details. Also, note that we link (3.2) with (3.1) in Theorem 3.4. +Theorem 3.1. There exists a constant λm +δ +> 0 and a map wm +δ +∈ Cb(Bm) such +that (3.2) is satisfied and we get supξ∈U wm +δ (ξ) = 0. +Proof. The idea of the proof is to use the Krein-Rutman theorem to get a pos- +itive eigenvalue with a non-negative eigenvector of the suitable operator. +More +specifically, we consider a cone of non-negative continuous and bounded functions +C+ +b (Bm) ⊂ Cb(Bm) and, for any h ∈ C+ +b (Bm), we define the operators +˜ +Mh(x) := sup +ξ∈U +ec(x,ξ)h(ξ), +x ∈ E, +˜P m +δ h(x) := Ex +� +e +� δ +0 f(Xs)ds � +1{Xδ∈Bm}h(Xδ) + 1{Xδ /∈Bm} ˜ +Mh(Xδ) +�� +, +x ∈ Bm, +˜T m +δ h(x) := max +� +˜P m +δ h(x), ˜ +M ˜P m +δ h(x) +� +, +x ∈ Bm. +Now, we use the Krein-Rutman theorem to show that ˜T m +δ +admits a positive eigen- +value and a non-negative eigenfunction; see Theorem 4.3 in [7] for details. We start +with verifying the assumptions. First, note that ˜T m +δ +is positively homogeneous, +monotonic increasing, and we have +˜T m +δ +1(x) ≥ e−δ∥f∥−∥c∥ +1(x), +x ∈ Bm, +where +1 denotes the function identically equal to 1 on Bm. Also, using Assump- +tion (A2), we get that ˜T m +δ +transforms C+ +b (Bm) into itself and it is continuous with +respect to the supremum norm. Let us now show that ˜T m +δ +is in fact completely +continuous. To see this, let (hn)n∈N ⊂ C+ +b (Bm) be a bounded (by some constant +K > 0) sequence; using Arzel`a-Ascoli Theorem we show that it is possible to find +a convergent subsequence of ( ˜T m +δ hn)n∈N. Note that, for any n ∈ N, we get +∥ ˜T m +δ hn∥ ≤ eδ∥f∥K, +hence ( ˜T m +δ hn) is uniformly bounded. Next, let us fix some ε > 0, x ∈ Bm, and +(xk) ⊂ Bm such that xk → x as k → ∞. Also, to ease the notation, for any n ∈ N, +we set Hn(x) := 1{x∈Bm}hn(x) + 1{x/∈Bm} ˜ +Mhn(x), x ∈ E and note that Hn are +measurable functions bounded by 2K uniformly in n ∈ N. Then, for any n, k ∈ N, +we get +| ˜T m +δ hn(x) − ˜T m +δ hn(xk)| ≤ +���Ex +� +e +� δ +0 f(Xs)dsHn(Xδ) +� +− Exk +� +e +� δ +0 f(Xs)dsHn(Xδ) +���� ++ | ˜ +M ˜P m +δ hn(x) − ˜ +M ˜P m +δ hn(xk)|. +(3.3) +Also, using Assumption (A1), we may find k ∈ N big enough such that, for any +n ∈ N, we obtain +| ˜ +M ˜P m +δ hn(x) − ˜ +M ˜P m +δ hn(xk)| ≤ eδ∥f∥K sup +ξ∈U +|ec(x,ξ) − ec(xk,ξ)| ≤ ε +2. +(3.4) + +10 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +Next, note that for any u ∈ (0, δ) and n, k ∈ N, we get +���Ex +� +e +� δ +0 f(Xs)dsHn(Xδ) +� +− Exk +� +e +� δ +0 f(Xs)dsHn(Xδ) +���� +≤ +���Ex +�� +e +� δ +0 f(Xs)ds − e +� δ +u f(Xs)ds� +Hn(Xδ) +���� ++ +���Exk +�� +e +� δ +0 f(Xs)ds − e +� δ +u f(Xs)ds� +Hn(Xδ) +���� ++ +���Exk +� +e +� δ +u f(Xs)dsHn(Xδ) +� +− Ex +� +e +� δ +u f(Xs)dsHn(Xδ) +���� . +(3.5) +Also, using the inequality |ey − ez| ≤ emax(y,z)|y − z|, y, z ∈ R, we may find u > 0 +small enough such that, for any n, k ∈ N, we get +���Exk +�� +e +� δ +0 f(Xs)ds − e +� δ +u f(Xs)ds� +Hn(Xδ) +���� ≤ 2Keδ∥f∥u∥f∥ ≤ ε +6. +(3.6) +Next, setting F u +n (x) := Ex +� +e +� δ−u +0 +f(Xs)dsHn(Xδ−u) +� +, n ∈ N, x ∈ E, and using the +Markov property combined with Assumption (A2), we may find k ∈ N big enough +such that for any n ∈ N, we get +���Exk +� +e +� δ +u f(Xs)dsHn(Xδ) +� +− Ex +� +e +� δ +u f(Xs)dsHn(Xδ) +���� += |Exk[F u +n (Xu)] − Ex[F u +n (Xu)]| +≤ 2Keδ∥f∥ sup +A∈E +|Pu(xk, A) − Pu(x, A)| ≤ ε +6. +Thus, recalling (3.5)–(3.6), we get that for k ∈ N big enough and any n ∈ N, +we get +���Ex +� +e +� δ +0 f(Xs)dsHn(Xδ) +� +− Exk +� +e +� δ +0 f(Xs)dsHn(Xδ) +���� ≤ +ε +2. This combined +with (3.3)–(3.4) shows | ˜T m +δ hn(x) − ˜T m +δ hn(xk)| ≤ ε for k ∈ N big enough and any +n ∈ N, which proves the equicontinuity of the family ( ˜T m +δ hn)n∈N. Consequently, +using Arzel`a-Ascoli, we may find a uniformly (in x ∈ Bm) convergent subsequence +of ( ˜T m +δ hn)n∈N and the operator ˜T m +δ +is completely continuous. +Thus, using the +Krein-Rutman theorem we conclude that there exists a constant ˜λm +δ +> 0 and a +non-zero map hm +δ ∈ C+ +b (Bm) such that +˜T m +δ hm +δ (x) = ˜λm +δ hm +δ (x), +x ∈ Bm. +(3.7) +After a possible normalisation, we assume that supξ∈U hm +δ (ξ) = 1. +Let us now show that hm +δ (x) > 0, x ∈ Bm. To see this, let us define D := +e−δ∥f∥ 1 +˜λm +δ +and let Oh ⊂ Bm be an open set such that +inf +x∈Oh hm +δ (x) > 0; +(3.8) +note that this set exists thanks to the continuity of hm +δ +and the fact that hm +δ +is +non-zero. Next, using (3.7), we have +hm +δ (x) ≥ DEx +� +1{Xδ∈Oh}hm +δ (Xδ) + 1{Xδ∈Bm\Oh}hm +δ (Xδ) +� +, +x ∈ Bm. + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 11 +Then, for any n ∈ N, we inductively get +hm +δ (x) ≥ DEx[1{Xδ∈Oh}hm +δ (Xδ)] ++ +n +� +i=2 +DiEx +� +1{Xδ∈Bm\Oh,X2δ∈Bm\Oh,...,X(i−1)δ∈Bm\Oh,Xiδ∈Oh}hm +δ (Xiδ) +� ++ DnEx +� +1{Xδ∈Bm\Oh,X2δ∈Bm\Oh,...,Xiδ∈Bm\Oh}hm +δ (Xnδ) +� +, x ∈ Bm. +Thus, letting n → ∞ and using Assumption (A4) combined with (3.8), we show +hm +δ (x) > 0 for any x ∈ Bm. +Next, we define wm +δ (x) := ln hm +δ (x), x ∈ Bm, and λm +δ +:= +1 +δ ln ˜λm +δ . +Thus, +from (3.7), we get that the pair (wm +δ , λm +δ ) satisfies +˜T m +δ ewm +δ (x) = eδλm +δ ewm +δ (x), +x ∈ Bm, +and +sup +ξ∈U +wm +δ (ξ) = 0. +In fact, using Assumption (A1) and the argument from Theorem 3.1 in [15], we +have +wm +δ (x) = max +� +ln Ex +� +e +� δ +0 (f(Xs)−λm +δ )ds+1{Xδ∈Bm}wm +δ (Xδ)+1{Xδ / +∈Bm}Mwm +δ (Xδ)� +, +Mwm +δ (x) +� +, +x ∈ Bm. +Finally, we extend the definition of wm +δ to the full space E by setting +wm +δ (x) := Mwm +δ (x), +x /∈ Bm; +note that the definition is correct since, at the right-hand side, we need to evaluate +wm +δ only at the points from U ⊂ B0 ⊂ Bm and this map is already defined there. +□ +As we show now, Equation (3.2) may be linked to a specific martingale charac- +terisation. +Proposition 3.2. Let (wm +δ , λm +δ ) be a solution to (3.2). Then, for any x ∈ Bm, we +get that the process +zm +δ (n) := e +� (nδ)∧τBm +0 +(f(Xs)−λm +δ )ds+wm +δ (X(nδ)∧τBm ), +n ≥ 0, +is a Px-supermartingale. Also, the process +zm +δ (n ∧ (ˆτ m +δ /δ)), +n ∈ N, +is a Px-martingale, where ˆτ m +δ := δ inf{k ∈ N: wm +δ (Xkδ) = Mwm +δ (Xkδ)}. +Proof. To ease the notation, we show the proof only for δ = 1; the general case +follows the same logic. Let us fix m, n ∈ N and x ∈ Bm. Then, using the fact +wm +1 (y) = Mwm +1 (y), x /∈ Bm, and the inequality +ewm +1 (y) ≥ Ey +� +e +� 1 +0 (f(Xs)−λm +1 )ds+1{X1∈Bm}wm +1 (X1)+1{X1 / +∈Bm}Mwm +1 (X1)� +, +y ∈ Bm, + +12 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +we have +Ex[zm +1 (n + 1)|Fn] += 1{τBm≤n}e +� τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (XτBm ) ++ 1{τBm>n}e +� n +0 (f(Xs)−λm +1 )ds× +× EXn[e +� n+1 +n +(f(Xs)−λm +1 )ds+1{X1∈Bm}wm +1 (X1)+1{X1 / +∈Bm}wm +1 (X1)|Fn] += 1{τBm≤n}e +� n∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xn∧τBm ) ++ 1{τBm>n}e +� n∧τBm +0 +(f(Xs)−λm +1 )ds× +× EXn[e +� n+1 +n +(f(Xs)−λm +1 )ds+1{X1∈Bm}wm +1 (X1)+1{X1 / +∈Bm}Mwm +1 (X1)|Fn] +≤ e +� n∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xn∧τBm ) = zm +1 (n), +which shows the supermartingale property of (zm +1 (n)). Next, note that on the set +{τBm ∧ ˆτ m +1 > n} we get +ewm +1 (Xn) = EXn +� +e +� 1 +0 (f(Xs)−λm +1 )ds+1{X1∈Bm}wm +1 (X1)+1{X1 / +∈Bm}Mwm +1 (X1)� +. +Thus, we have +Ex[zm +1 ((n + 1) ∧ ˆτ m +1 )|Fn] += 1{τBm∧ˆτ m +1 ≤n}e +� τBm ∧ˆτm +1 +0 +(f(Xs)−λm +1 )ds+wm +1 (XτBm ∧ˆτm +1 ) ++ 1{τBm∧ˆτ m +1 >n}e +� n +0 (f(Xs)−λm +1 )ds× +× EXn[e +� n+1 +n +(f(Xs)−λm +1 )ds+1{X1∈Bm}wm +1 (X1)+1{X1 / +∈Bm}Mwm +1 (X1)|Fn] += e +� n∧τBm ∧ˆτm +1 +0 +(f(Xs)−λm +1 )ds+wm +1 (Xn∧τBm ∧ˆτm +1 ) = zm +1 (n ∧ ˆτ m +1 ), +which concludes the proof. +□ +Let us denote by Vδ,m the family of impulse control strategies with impulse times +in the time-grid {0, δ, 2δ, . . .} and obligatory impulses when the controlled process +exits the set Bm at some multiple of δ. Using a martingale characterisation of (3.2), +we get that λm +δ is the optimal value of the impulse control problem with impulse +strategies from Vδ,m. To show this result, we introduce a strategy ˆV := (ˆτi, ˆξi)∞ +i=1 ∈ +Vδ,m defined recursively, for i = 1, 2, . . ., by +ˆτi := ˆσi ∧ τ i +Bm, +ˆσi := δ inf{n ≥ ˆτi−1/δ: n ∈ N, wm +δ (Xi +nδ) = Mwm +δ (Xi +nδ)}, +τ i +Bm := δ inf{n ≥ ˆτi−1/δ: n ∈ N, Xi +nδ /∈ Bm}, +ˆξi := arg max +ξ∈U +(c(Xi +ˆτi, ξ) + wm +δ (ξ))1{ˆτi<∞} + ξ01{ˆτi=∞}, +(3.9) +where ˆτ0 := 0 and ξ0 ∈ U is some fixed point. +Theorem 3.3. Let (wm +δ , λm +δ ) be a solution to (3.2). Then, for any x ∈ Bm, we get +λm +δ = +sup +V ∈Vδ,m +lim inf +n→∞ +1 +nδ ln E(x,V ) +� +e +� nδ +0 +f(Ys)ds+�∞ +i=1 1{τi≤nδ}c(Yτ− +i +,ξi)� +. +Also, the strategy ˆV defined in (3.9) is optimal. + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 13 +Proof. The proof follows the lines of the proof of Theorem 2.3 and is omitted for +brevity. +□ +Next, we link (3.2) with an infinite horizon optimal stopping problem under the +non-degeneracy assumption. +Theorem 3.4. Let (wm +δ , λm +δ ) be a solution to (3.2) with λm +δ > r(f). Then, we get +that (wm +δ , λm +δ ) satisfies (3.1). +Proof. As in the proof of Proposition 3.2, we consider only δ = 1; the general case +follows the same logic. +First, note that for any x ∈ Bm, n ∈ N, and τ ∈ T δ +x , using Proposition 3.2 and +Doob’s optional stopping theorem, we have +ewm +1 (x) ≥ Ex +� +e +� n∧τ∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xn∧τ∧τBm ) +� +. +Also, recalling the boundedness of wm +1 and Proposition A.2, and letting n → ∞, +we get +ewm +1 (x) ≥ Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xτ∧τBm ) +� +. +Next, noting that wm +1 (Xτ∧τBm) ≥ Mwm +1 (Xτ∧τBm), and taking the supremum over +τ ∈ T δ +x , we get +ewm +1 (x) ≥ sup +τ∈T δ +x +Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +1 )ds+Mwm +1 (Xτ∧τBm ) +� +. +Second, using again Proposition 3.2, for any x ∈ Bm and n ∈ N, we get +wm +1 (x) = ln Ex +� +e +� n∧ˆτm +δ ∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xn∧ˆτm +δ +∧τBm ) +� +. +Using again the boundedness of wm +1 and Proposition A.2, and letting n → ∞, we +get +wm +1 (x) = ln Ex +� +e +� ˆτm +δ ∧τBm +0 +(f(Xs)−λm +1 )ds+wm +1 (Xˆτm +δ +∧τBm ) +� +. +In fact, noting that wm +1 (Xˆτ m +δ ∧τBm) = Mwm +1 (Xˆτ m +δ ∧τBm), we obtain +wm +1 (x) = ln Ex +� +e +� ˆτm +δ ∧τBm +0 +(f(Xs)−λm +1 )ds+Mwm +1 (Xˆτm +δ +∧τBm ) +� +, +thus we get +ewm +1 (x) = sup +τ∈T δ +x +Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +1 )ds+Mwm +1 (Xτ∧τBm ) +� +. +Finally, using Proposition A.4, we have +ewm +1 (x) = sup +τ∈T δ +x,b +Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +1 )ds+Mwm +1 (Xτ∧τBm ) +� +, +which concludes the proof. +□ +Remark 3.5. In Theorem 3.4 we showed that, if λm +δ +> r(f), a solution to the +one-step equation (3.2) is uniquely characterised by the optimal stopping value +function (3.1). +If λm +δ +≤ r(f), the problem is degenerate and, in particular, we +cannot use the uniform integrability result from Proposition A.2. In fact, in this + +14 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +case it is even possible that the one-step Bellman equation admits multiple solutions +and the optimal stopping characterisation does not hold; see e.g. Theorem 1.13 +in [22] for details. +4. Dyadic impulse control +In this section we consider a dyadic full-domain version of (2.1). We construct +a solution to the associated Bellman equation which will be later used to find +a solution to (2.6). +The argument uses a bounded domain approximation from +Section 3. More specifically, throughout this section we fix some δ > 0 and show +the existence of a function wδ ∈ Cb(E) and a constant λδ ∈ R, which are a solution +to the dyadic Bellman equation of the form +wδ(x) = sup +τ∈T δ +x,b +ln Ex +� +e +� τ +0 (f(Xs)−λδ)ds+Mwδ(Xτ )� +, +x ∈ E. +(4.1) +In fact, we set +λδ := lim +m→∞ λm +δ ; +(4.2) +note that this constant is well-defined as, from Theorem 3.3, recalling that Bm ⊂ +Bm+1, we get λm +δ ≤ λm+1 +δ +, m ∈ N. +First, we state the lower bound for λδ. +Lemma 4.1. Let (wδ, λδ) be a solution to (4.1). Then, we get λδ ≥ r(f). +Proof. The proof follows the lines of the proof of Lemma 2.1 and is omitted for +brevity. +□ +Next, we show the existence of a solution to (4.1) under the non-degeneracy +assumption λδ > r(f). +Theorem 4.2. Let λδ be given by (4.2) and assume that λδ > r(f). Then, there +exists wδ ∈ Cb(E) such that (4.1) is satisfied and we get supξ∈U wδ(ξ) = 0. +Proof. We start with some general comments and an outline of the argument. First, +note that from Theorem 3.1, for any m ∈ N, we get a solution (wm +δ , λm +δ ) to (3.2) +satisfying supξ∈U wm +δ (ξ) = 0. Also, from the assumption λδ > r(f) we get λm +δ > +r(f) for m ∈ N sufficiently big (for simplicity, we assume that λ0 +δ > r(f)). Thus, +using Theorem 3.4, we get that, for any m ∈ N, the pair (wm +δ , λm +δ ) satisfies (3.1). +Second, to construct a function wδ, we use Arzel`a-Ascoli Theorem. More specif- +ically, recalling that supξ∈U wm +δ (ξ) = 0 and using the fact that −∥c∥ ≤ c(x, ξ) ≤ 0, +x ∈ E, ξ ∈ U, for any m ∈ N and x ∈ E, we get +−∥c∥ ≤ Mwm +δ (x) ≤ 0. +Also, note that, for any m ∈ N and x, y ∈ E, we have +|Mwm +δ (x) − Mwm +δ (y)| ≤ sup +ξ∈U +|c(x, ξ) − c(y, ξ)|. +Consequently, the sequence (Mwm +δ )m∈N is uniformly bounded and equicontinuous. +Thus, using Arzel`a-Ascoli Theorem combined with a diagonal argument, we may +find a subsequence (for brevity still denoted by (Mwm +δ )m∈N) and a map φδ ∈ Cb(E) +such that Mwm +δ (x) converges to φδ(x) as m → ∞ uniformly in x from any compact +set. In fact, using Assumption (A1) and the argument from the first step of the + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 15 +proof of Theorem 4.1 in [15], we get that the convergence is uniform in x ∈ E. +Then, we define +wδ(x) := sup +τ∈T δ +x,b +ln Ex +� +e +� τ +0 (f(Xs)−λδ)ds+φδ(Xτ )� +, +x ∈ E. +(4.3) +To complete the construction, we show that wm +δ +converges to wδ uniformly on +compact sets. Indeed, in this case we have +|Mwm +δ (x) − Mwδ(x)| ≤ sup +ξ∈U +|wm +δ (ξ) − wδ(ξ)| → 0, +m → ∞, +thus φδ ≡ Mwδ and from (4.3) we get that (4.1) is satisfied. Also, recalling that +from Theorem 3.1 we get supξ∈U wm +δ (ξ) = 0, m ∈ N, we also get supξ∈U wδ(ξ) = 0. +Finally, to show the convergence, we define the auxiliary functions +wm,1 +δ +(x) := sup +τ∈T δ +x,b +ln Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +δ )ds+φδ(Xτ∧τBm ) +� +, +x ∈ E, +(4.4) +wm,2 +δ +(x) := sup +τ∈T δ +x,b +ln Ex +� +e +� τ∧τBm +0 +(f(Xs)−λδ)ds+φδ(Xτ∧τBm ) +� +, +x ∈ E. +(4.5) +We split the rest of the proof into three steps: (1) proof that |wm +δ (x)−wm,1 +δ +(x)| → 0 +as m → ∞ uniformly in x ∈ E; (2) proof that |wm,1 +δ +(x) − wm,2 +δ +(x)| → 0 as m → ∞ +uniformly in x ∈ E; (3) proof that |wm,2 +δ +(x) − wδ(x)| → 0 as m → ∞ uniformly in +x from compact sets. +Step 1. We show |wm +δ (x) − wm,1 +δ +(x)| → 0 as m → ∞ uniformly in x ∈ E. Note +that, for any x ∈ E and m ∈ N, we have +wm,1 +δ +(x) ≤ sup +τ∈T δ +x,b +ln +� +Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +δ )ds+Mwm +δ (Xτ∧τBm ) +� +e∥φδ−Mwm +δ ∥ +� += wm +δ (x) + ∥φδ − Mwm +δ ∥. +Similarly, we get wm +δ (x) ≤ wm,1 +δ +(x) + ∥φδ − Mwm +δ ∥, thus +sup +x∈E +|wm +δ (x) − wm,1 +δ +(x)| ≤ ∥φδ − Mwm +δ ∥. +Recalling the fact that φδ is a uniform limit of Mwm +δ as m → ∞, we conclude the +proof of this step. +Step 2. We show that |wm,1 +δ +(x) − wm,2 +δ +(x)| → 0 as m → ∞ uniformly in x ∈ E. +Recalling that λm +δ ↑ λδ, we get wm,1 +δ +(x) ≥ wm,2 +δ +(x) ≥ −∥φδ∥, x ∈ E. Thus, using +the inequality | ln y − ln z| ≤ +1 +min(y,z)|y − z|, y, z > 0, we get +0 ≤ wm,1 +δ +(x) − wm,2 +δ +(x) ≤ e∥φδ∥(ewm,1 +δ +(x) − ewm,2 +δ +(x)), +x ∈ E. +(4.6) +Then, noting that φδ(·) ≤ 0, for any m ∈ N and x ∈ E, we obtain +0 ≤ ewm,1 +δ +(x) − ewm,2 +δ +(x) ≤ sup +τ∈T δ +x,b +� +Ex +� +e +� τ∧τBm +0 +(f(Xs)−λm +δ )ds+φδ(Xτ∧τBm ) +� +− Ex +� +e +� τ∧τBm +0 +(f(Xs)−λδ)ds+φδ(Xτ∧τBm ) +�� +≤ sup +τ∈T δ +x,b +Ex +� +e +� τ +0 f(Xs)ds � +e−λm +δ τ − e−λδτ�� +. +(4.7) + +16 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +Also, recalling that λ0 +δ ≤ λm +δ ≤ λδ, m ∈ N, for any x ∈ E and T ≥ 0, we get +0 ≤ sup +τ∈Tx,b +Ex +� +e +� τ +0 f(Xs)ds � +e−λm +δ τ − eλδτ�� +≤ sup +τ∈Tx,b +Ex +�� +1{τ≤T } + 1{τ>T } +� +e +� τ +0 f(Xs)ds � +e−λm +δ τ − e−λδτ�� +≤ sup +τ r(f) and using Lemma A.1, for any ε > 0, we may find T ≥ 0, such +that +0 ≤ sup +x∈E +sup +τ≥T +τ∈Tx,b +Ex +� +e +� τ +0 (f(Xs)−λ0 +δ)ds� +≤ ε. +Also, using the inequality |ex − ey| ≤ emax(x,y)|x − y|, x, y ≥ 0, we obtain +sup +τ 0 was arbitrary, we conclude the proof of this step. +Step 3. We show that |wm,2 +δ +(x) − wδ(x)| → 0 as m → ∞ uniformly in x from +compact sets. First, we show that wm,2 +δ +(x) ≤ wδ(x) for any m ∈ N and x ∈ E. Let +ε > 0 and τ ε +m ∈ T δ +x,b be an ε-optimal stopping time for wm,2 +δ +(x). Then, we get +wδ(x) ≥ ln Ex +� +e +� τεm∧τBm +0 +(f(Xs)−λδ)ds+φδ(Xτεm∧τBm ) +� +≥ wm,2 +δ +(x) − ε. +As ε > 0 was arbitrary, we get wm,2 +δ +(x) ≤ wδ(x), m ∈ N, x ∈ E. In fact, using +a similar argument, for any x ∈ E, we may show that the map m �→ wm,2 +δ +(x) is +non-decreasing. +Second, let ε > 0 and τε ∈ T δ +x,b be an ε-optimal stopping time for wδ(x). Then, +we obtain +0 ≤ wδ(x) − wm,2 +δ +(x) ≤ ln Ex +� +e +� τε +0 +(f(Xs)−λδ)ds+φδ(Xτε )� ++ ε +− ln Ex +� +e +� τε∧τBm +0 +(f(Xs)−λδ)ds+φδ(Xτε∧τBm ) +� +. +(4.10) +Noting that τBm ↑ +∞ as m → ∞ and using the quasi left-continuity of X combined +with Lemma A.2 and the boundedness of φδ, we get +lim +m→∞ Ex +� +e +� τε∧τBm +0 +(f(Xs)−λδ)ds+φδ(Xτε∧τBm ) +� += Ex +� +e +� τε +0 +(f(Xs)−λδ)ds+φδ(Xτε )� +. +Thus, using (4.10) and recalling that ε > 0 was arbitrary, we get limm→∞ wm,2 +δ +(x) = +wδ(x). Also, noting that by Proposition A.3 and Proposition A.4, the maps x �→ + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 17 +wδ(x) and x �→ wm,2 +δ +(x) are continuous, and using the monotonicity of m �→ +wm,2 +δ +(x), from Dini’s Theorem we get that wm,2 +δ +(x) converges to wδ(x) uniformly +in x from compact sets, which concludes the proof. +□ +We conclude this section with a verification result related to (4.1). +Theorem 4.3. Let (wδ, λδ) be a solution to (4.1) with λδ > r(f). Then, we get +λδ := sup +V ∈Vδ lim inf +n→∞ +1 +n ln E(x,V ) +� +e +� nδ +0 +f(Ys)ds+�∞ +i=1 1{τi≤nδ}c(Yτ− +i +,ξi)� +, +where Vδ is a family of impulse control strategies with impulse times on the dyadic +time-grid {0, δ, 2δ, . . .}. +Proof. The proof follows the lines of the proof of Theorem 2.3 and is omitted for +brevity. +□ +5. Existence of a solution to the Bellman equation +In this section we construct a solution (w, λ) to (2.6), which together with The- +orem 2.3 provides a solution to (2.1). The argument uses a dyadic approximation +and the results from Section 4. More specifically, we consider a family of dyadic +time steps δk := +1 +2k , k ∈ N. First, we specify the value of λ. In fact, we define +λ := lim inf +k→∞ λδk, +(5.1) +where λδk is a constant given by (4.2), corresponding to δk. Note that, if for some +k0 ∈ N we get λδk0 > r(f), then using Theorem 4.3, we get that λδk ≤ λδk+1, +k ≥ k0, and the limit inferior could be replaced by the usual limit. +Theorem 5.1. Let λ be given by (5.1) and assume that λ > r(f). Then, there +exists w ∈ Cb(E) such that (2.6) is satisfied. +Proof. The argument is partially based on the one used in Theorem 4.2 thus we +discuss only the main points. From the fact that λ > r(f) we get λδk > r(f) for +sufficiently big k ∈ N; to simplify the notation, we assume λδ0 > r(f). Thus, using +Theorem 4.2, for any k ∈ N, we get the existence of a map wδk ∈ Cb(E) satisfying +wδk(x) = sup +τ∈T +δk +x,b +ln Ex +� +e +� τ +0 (f(Xs)−λδk )ds+Mwδk (Xτ )� +, +x ∈ E +and such that supξ∈U wδk(ξ) = 0. Thus, we get +−∥c∥ ≤ Mwδk(x) ≤ 0, +k ∈ N, x ∈ E, +and the family (Mwδk)k∈N is uniformly bounded. Also, it is equicontinuous as we +have +|Mwδk(x) − Mwδk(y)| ≤ sup +x∈U +|c(x, ξ) − c(y, ξ)|, +x, y ∈ E. +Thus, using Arzel`a-Ascoli theorem, we may choose a subsequence (for brevity still +denoted by (Mwδk)), such that (Mwδk) converges uniformly on compact sets to +some map φ. In fact, using Assumption (A1) and the argument from the first step +of the proof of Theorem 4.1 from [15], we get that Mwδk(x) converges to φ(x) as +k → ∞ uniformly in x ∈ E. Next, let us define +w(x) := sup +τ∈Tx,b +ln Ex +� +e +� τ +0 (f(Xs)−λ)ds+φ(Xτ )� +, +x ∈ E. +(5.2) + +18 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +In the following, we show that wδk converges to w uniformly in compact sets as +k → ∞. Then, we get that Mwδk converges to Mw, hence Mw ≡ φ and (2.6) is +satisfied. +To show the convergence, we define +w1 +δk(x) := sup +τ∈T +δk +x,b +ln Ex +� +e +� τ +0 (f(Xs)−λδk)ds+φ(Xτ )� +, +k ∈ N, x ∈ E. +In the following, we show that |w(x) − w1 +δk(x)| → 0 and |w1 +δk(x) − wδk(x)| → 0 as +k → ∞ uniformly in x from compact sets. In fact, to show the first convergence, +we note that +w0 +δk(x) ≤ w1 +δk(x) ≤ w2 +δk(x), +k ∈ N, x ∈ E, +where +w0 +δk(x) := sup +τ∈T +δk +x,b +ln Ex +� +e +� τ +0 (f(Xs)−λ)ds+φ(Xτ )� +, +k ∈ N, x ∈ E, +w2 +δk(x) := sup +τ∈Tx,b +ln Ex +� +e +� τ +0 (f(Xs)−λδk )ds+φ(Xτ )� +, +k ∈ N, x ∈ E. +Thus, to prove |w(x) − w1 +δk(x)| → 0 it is enough to show |w(x) − w0 +δk(x)| → 0 and +|w(x) − w2 +δk(x)| → 0 as k → ∞. +For transparency, we split the rest of the proof into three parts: (1) proof that +|w(x) − w0 +δk(x)| → 0 as k → ∞ uniformly in x from compact sets; (2) proof that +|w(x) − w2 +δk(x)| → 0 as k → ∞ uniformly in x ∈ E; (3) proof that |w1 +δk(x) − +wδk(x)| → 0 as k → ∞ uniformly in x ∈ E. +Step 1. We show that |w(x) − w0 +δk(x)| → 0 as k → ∞ as k → ∞ uniformly in x +from compact sets. First, note that we have w0 +δk(x) ≤ w(x), k ∈ N, x ∈ E. Next, +for any x ∈ E and ε > 0, let τε ∈ Tx,b be an ε-optimal stopping time for w(x) and +let τ k +ε be its T δk +x,b approximation given by +τ k +ε := inf +� +τ ∈ T δk +x,b : τ ≥ τε +� += +∞ +� +j=1 +1{ j−1 +2k <τε≤ +j +2m } +j +2k . +Then, we get +0 ≤ w(x) − w0 +δk(x) +≤ Ex +� +e +� τε +0 +(f(Xs)−λ)ds+φ(Xτε )� +− Ex +� +e +� τk +ε +0 +(f(Xs)−λ)ds+φ(Xτk +ε ) +� ++ ε. +Also, using Proposition A.2 and letting k → ∞, we have +lim +k→∞ Ex +� +e +� τk +ε +0 +(f(Xs)−λ)ds+φ(Xτk +ε ) +� += Ex +� +e +� τε +0 +(f(Xs)−λ)ds+φ(Xτε )� +. +Consequently, recalling that ε > 0 was arbitrary, we obtain limk→∞ w0 +δk(x) = +w(x) for any x ∈ E. +In fact, using the monotonicity of the sequence (w0 +δk)k∈N +combined with Proposition A.3, Proposition A.4, and Dini’s theorem, we get that +the convergence is uniform on compact sets, which concludes the proof of this step. + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 19 +Step 2. We show that |w(x) − w2 +δk(x)| → 0 as k → ∞ uniformly in x ∈ E. +First, note that −∥φ∥ ≤ w(x) ≤ w2 +δk(x), k ∈ N, x ∈ E. Thus, using the inequality +| ln y − ln z| ≤ +1 +min(y,z)|y − z|, y, z > 0, we get +0 ≤ w2 +δk(x) − w(x) ≤ e∥φ∥(ew2 +δk (x) − ew(x)), +k ∈ N, x ∈ E. +Also, recalling that φ(·) ≤ 0, for any k ∈ N and x ∈ E, we obtain +0 ≤ ew2 +δk (x) − ew(x) ≤ sup +τ∈Tx,b +Ex +� +e +� τ +0 f(Xs)ds � +e−λδkτ − e−λτ�� +. +Thus, repeating the argument from the second step of the proof of Theorem 4.2, +we get w2 +δk(x) → w(x) as k → ∞ uniformly in x ∈ E, which concludes the proof of +this step. +Step 3. We show that |w1 +δk(x) − wδk(x)| → 0 as k → ∞ uniformly in x ∈ E. +In fact, recalling that ∥Mwδk − φ∥ → 0 as k → ∞, the argument follows the lines +of the one used in the first step of the proof of Theorem 4.2. This concludes the +proof. +□ +Appendix A. Properties of optimal stopping problems +In this section we discuss some properties of the optimal stopping problems that +are used in this paper. +Throughout this section we consider g, G ∈ Cb(E) and +assume G(·) ≤ 0 and r(g) < 0, where r(g) is the type of the semigroup given +by (2.7) corresponding to the map g. We start with a useful result related to the +asymptotic behaviour of the running cost function g. +Lemma A.1. Let a be such that r(g) < a < 0. Then, +(1) The map x �→ U g−a +0 +1(x) := Ex +�� ∞ +0 +e +� t +0 (g(Xs)−a)dsdt +� +is continuous and +bounded. +(2) We get +lim +T →∞ sup +x∈E +sup +τ≥T +τ∈Tx +Ex +� +e +� τ +0 g(Xs)ds� += 0. +Proof. For transparency, we prove the claims point by point. +Proof of (1). First, we show the boundedness of x �→ U g−a +0 +1(x). Let ε < +a − r(g). +Using the definition of r(g − a) we may find t0 ≥ 0, such that for +any t ≥ t0 we get supx∈E Ex +� +e +� t +0 (g(Xs)−a)ds� +≤ et(r(g)−a+ε). Then, using Fubini’s +theorem and noting that r(g) − a + ε < 0, for any x0 ∈ E, we get +0 ≤ U g−a +0 +1(x0) ≤ +� ∞ +0 +sup +x∈E +Ex +� +e +� t +0 (g(Xs)−a)ds� +dt += +� t0 +0 +sup +x∈E +Ex +� +e +� t +0 (g(Xs)−a)ds� +dt + +� ∞ +t0 +sup +x∈E +Ex +� +e +� t +0 (g(Xs)−a)ds� +dt +≤ +� t0 +0 +et(∥g∥−a)dt + +� ∞ +t0 +et(r(g)−a+ε)dt < ∞, +which concludes the proof of the boundedness of x �→ U g−a +0 +1(x). + +20 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +For the continuity, note that using Assumption (A2) and repeating the argument +used in Lemma 4 in Section II.5 of [13], we get that x �→ Ex +� +e +� t +0 (g(Xs)−a)dsdt +� +is +continuous for any t ≥ 0. Also, as in the proof of the boundedness, we may show +0 ≤ sup +x∈E +Ex +� +e +� t +0 (g(Xs)−a)ds� +≤ et(∥g∥−a)1{t∈[0,t0]} + et(r(g)−a+ε)1{t>t0} +and the upper bound is integrable (with respect to t). +Thus, using Lebesgue’s +dominated convergence theorem, we get the continuity of the map x �→ U g−a +0 +1(x) = +� ∞ +0 +Ex +� +e +� t +0 (g(Xs)−a)ds� +dt, which concludes the proof of this step. +Proof of (2). Noting that U g−a +0 +1(x) ≥ +� 1 +0 e−t(∥g∥−a)dt, x ∈ E, we may find +d > 0, such that U g−a +0 +1(x) ≥ d > 0, x ∈ E. Thus, recalling that a < 0, we get +0 ≤ sup +τ≥T +τ∈Tx +Ex +� +e +� τ +0 g(Xs)ds� +≤ sup +τ≥T +τ∈Tx +Ex +� +e +� τ +0 (g(Xs)−a)dseaτU g−a +0 +1(Xτ)1 +d +� +≤ eaT +d +sup +τ≥T +τ∈Tx +Ex +� +e +� τ +0 (g(Xs)−a)dsU g−a +0 +1(Xτ) +� += eaT +d +sup +τ≥T +τ∈Tx +Ex +�� ∞ +0 +e +� t+τ +0 +(g(Xs)−a)dsdt +� += eaT +d +sup +τ≥T +τ∈Tx +Ex +�� ∞ +τ +e +� t +0 (g(Xs)−a)dsdt +� +≤ eaT +d Ex +�� ∞ +0 +e +� t +0 (g(Xs)−a)dsdt +� +≤ eaT +d ∥U g−a +0 +1∥ → 0, +T → ∞, +which concludes the proof. +□ +Using Lemma A.1 we get the uniform integrability of a suitable family of random +variables. +This result is extensively used throughout the paper as it simplifies +numerous limiting arguments. +Proposition A.2. For any x ∈ E, the family {e +� τ +0 g(Xs)ds}τ∈Tx is Px-uniformly +integrable. +Proof. Let us fix some x ∈ E and, for any τ ∈ Tx and n ∈ N, define the event +Aτ +n := {� τ +0 g(Xs)ds ≥ n}. Note that for any T ≥ 0, we get +sup +τ∈Tx +Ex[1Aτne +� τ +0 g(Xs)ds] ≤ sup +τ≤T +τ∈Tx +Ex[1Aτne +� τ +0 g(Xs)ds] + sup +τ>T +τ∈Tx +Ex[1Aτne +� τ +0 g(Xs)ds] +≤ sup +τ≤T +τ∈Tx +eT ∥g∥Px[Aτ +n] + sup +τ>T +τ∈Tx +Ex[e +� τ +0 g(Xs)ds]. +Next, for any ε > 0, using Lemma A.1, we may find T > 0 big enough to get +sup +τ>T +τ∈Tx +Ex[e +� τ +0 g(Xs)ds] < ε. + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 21 +Also, noting that for τ ≤ T , we get Aτ +n ⊂ {T ∥g∥ ≥ n}, for any n > T ∥g∥, we also +get +sup +τ≤T +τ∈Tx +Px[Aτ +n] = 0. +Consequently, recalling that ε > 0 was arbitrary, we obtain +lim +n→∞ sup +τ∈Tx +Ex[Aτ +ne +� τ +0 g(Xs)ds] = 0, +which concludes the proof. +□ +Next, we consider an optimal stopping problem of the form +u(x) := sup +τ∈Tx,b +ln Ex +� +exp +�� τ +0 +g(Xs)ds + G(Xτ) +�� +, +x ∈ E; +(A.1) +note that here the non-positivity assumption for G is only a normalisation as for a +generic ˜G we may set G(·) = ˜G(·) − ∥ ˜G∥ to get G(·) ≤ 0. +The properties of the map (A.1) are summarised in the following proposition. +Proposition A.3. Let the map u be given by (A.1). Then, x �→ u(x) is continuous +and bounded. Also, we get +u(x) = sup +τ∈Tx +ln Ex +� +exp +�� τ +0 +g(Xs)ds + G(Xτ) +�� +, +x ∈ E. +(A.2) +Moreover, the process +z(t) := e +� t +0 g(Xs)+u(Xt), +t ≥ 0, +is a supermartingale and the process z(t ∧ ˆτ), t ≥ 0, is a martingale, where +ˆτ := inf{t ≥ 0 : u(Xt) ≤ G(Xt)}. +(A.3) +Proof. For transparency, we split the proof into two steps: (1) proof of the conti- +nuity of x �→ u(x) and identity (A.2); (2) proof of the martingale properties of the +process z. +Step 1. We show that the map x �→ u(x) is continuous and the identity (A.2) +holds. For any T ≥ 0 and x ∈ E, let us define +ˆu(x) := sup +τ∈Tx +ln Ex +� +exp +�� τ +0 +g(Xs)ds + G(Xτ) +�� +; +(A.4) +uT (x) := sup +τ≤T +ln Ex +� +exp +�� τ +0 +g(Xs)ds + G(Xτ) +�� +. +(A.5) +Using Assumption (A3) and following the proof of Proposition 10 and Proposition +11 in [16], we get that the map (T, x) �→ uT (x) is jointly continuous and bounded; +see also Remark 12 therein. We show that uT (x) → ˆu(x) as T → ∞ uniformly in +x ∈ E. Noting that +−∥G∥ ≤ uT (x) ≤ u(x), +T ≥ 0, x ∈ E, +and using the inequality | ln y−lnz| ≤ +1 +min(y,z)|y−z|, y, z > 0, to show uT (x) → ˆu(x) +as T → ∞ uniformly in x ∈ E it is enough to show euT (x) → eˆu(x) as T → ∞ + +22 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +uniformly in x ∈ E. Then, using Lemma A.1, for any ε > 0, we may find T ≥ 0 +such that for any x ∈ E, we obtain +0 ≤ eˆu(x) − euT (x) ≤ sup +τ∈Tx +Ex +� +e +� τ +0 g(Xs)ds+G(Xτ ) − e +� τ∧T +0 +g(Xs)ds+G(Xτ∧T )� +≤ sup +τ∈Tx +Ex +� +1{τ≥T } +� +e +� τ +0 g(Xs)ds+G(Xτ ) − e +� T +0 g(Xs)ds+G(XT )�� +≤ sup +τ∈Tx +Ex +� +1{τ≥T }e +� τ +0 g(Xs)ds+G(Xτ )� +≤ sup +τ≥T +τ∈Tx +Ex +� +e +� τ +0 g(Xs)ds� +≤ ε. +Thus, letting ε → 0, we get euT (x) → eˆu(x) as T → ∞ uniformly in x ∈ E and +consequently uT (x) → ˆu(x) as T → ∞ uniformly in x ∈ E. +Thus, from the +continuity of x �→ uT (x), T ≥ 0, we get that the map x �→ ˆu(x) is continuous. +Now, we show that u ≡ ˆu. First, we show that limT →∞ uT (x) = ˜u(x), where +˜u(x) := supτ∈Tx lim infT →∞ ln Ex +� +e +� τ∧T +0 +g(Xs)ds+G(Xτ∧T )� +, x ∈ E. For any T ≥ 0 +and x ∈ E, we get +uT (x) = sup +τ≤T +lim inf +S→∞ ln Ex +� +e +� τ∧S +0 +g(Xs)ds+G(Xτ∧S)� +≤ ˜u(x), +thus we get limT →∞ uT (x) ≤ ˜u(x). Also, for any x ∈ E, ˜τ ∈ Tx, and T ≥ 0, we get +ln Ex +� +e +� ˜τ∧T +0 +g(Xs)ds+G(X˜τ∧T )� +≤ uT(x). +Thus, letting T → ∞ and taking supremum over ˜τ ∈ Tx we get limT →∞ uT (x) = +˜u(x), x ∈ E. Also, using the argument from Lemma 2.2 from [17] we get ˜u ≡ u. +Thus, we get u(x) = limT →∞ uT (x) = ˆu(x), x ∈ E, hence the map x �→ u(x) is +continuous. Also, we get (A.2). +Step 2. We show the martingale properties of z. First, we focus on the stopping +time ˆτ. Let us define +τT := inf{t ≥ 0 : uT −t(Xt) ≤ G(Xt)}. +Using the argument from Proposition 11 in [16] we get that τT is an optimal stopping +time for uT . Also, noting that the map T �→ uT (x), x ∈ E, is increasing, we get +that T �→ τT is also increasing, thus we may define ˜τ := limT →∞ τT . We show that +˜τ ≡ ˆτ. +Let A := {˜τ < ∞}. First, we show that ˜τ ≡ ˆτ on A. On the event A, we get +uT −τT (XτT ) = G(XτT ). Thus, letting T → ∞, we get u(X˜τ) = G(X˜τ), hence we +get ˆτ ≤ ˜τ. Also, noting that uS(x) ≤ u(x), x ∈ E, S ≥ 0, on the set {ˆτ ≤ T } we +get uT −ˆτ(Xˆτ) ≤ u(Xˆτ) ≤ G(Xˆτ), hence +τT ≤ ˆτ. +(A.6) +Thus, recalling that ˆτ ≤ ˜τ < ∞ and letting T → ∞ in (A.6), we get ˜τ ≤ ˆτ, which +shows ˜τ ≡ ˆτ on A. +Now, we show that ˜τ ≡ ˆτ on Ac. Let ω ∈ Ac and suppose that ˆτ(ω) < ∞. Then, +we may find T ≥ 0 such that ˆτ(ω) < T . Also, for any S ≥ T we get +uS−ˆτ(ω)(Xˆτ(ω)(ω)) ≤ u(Xˆτ(ω)(ω)) ≤ G(Xˆτ(ω)(ω)). + +ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 23 +Thus, we get τS(ω) ≤ ˆτ(ω) for any S ≥ T . Consequently, letting S → ∞ we get +˜τ(ω) < ∞, which contradicts the choice of ω ∈ Ac. Consequently, on Ac we have +˜τ = ∞ = ˆτ. +Finally, we show the martingale properties. Let us define the processes +zT (t) := e +� t∧T +0 +g(Xs)ds+uT −t∧T (Xt∧T ), +T, t ≥ 0, +z(t) := e +� t +0 g(Xs)ds+u(Xt), +t ≥ 0. +Using standard argument we get that for any T ≥ 0, the process zT (t), t ≥ 0, is a +supermartingale and zT (t ∧ τT ), t ≥ 0, is a martingale; see e.g. [11, 12] for details. +Also, recalling that from the first step we get uT (x) → u(x) as T → ∞ uniformly +in x ∈ E, for any t ≥ 0, we get that zT (t) → z(t) and zT (t ∧ τT ) → z(t ∧ ˆτ) as +T → ∞. Consequently, using Lebesgue’s dominated convergence theorem, we get +that the process z(t) is a supermartingale and z(t∧ ˆτ), t ≥ 0, is a martingale, which +concludes the proof. +□ +Next, we consider an optimal stopping problem in a compact set and dyadic +time-grid. More specifically, let δ > 0, let B ⊂ E be compact and assume that +Px[τB < ∞] = 1, x ∈ B, where τB := δ inf{n ∈ N: Xnδ /∈ B}. +Within this +framework, we consider an optimal stopping problem of the form +uB(x) := sup +τ∈T δ ln Ex +� +exp +�� τ∧τB +0 +g(Xs)ds + G(Xτ∧τB) +�� +, +x ∈ E. +(A.7) +The properties of (A.7) are summarised in the following proposition. +Proposition A.4. Let uB be given by (A.7). Then, we get +uB(x) = sup +τ∈T δ +x,b +ln Ex +� +exp +�� τ∧τB +0 +g(Xs)ds + G(Xτ∧τB) +�� +, +x ∈ E. +(A.8) +Also, the map x �→ uB(x) is continuous and bounded. Moreover, the process +zδ(n) := e +� nδ +0 +g(Xs)+u(Xnδ), +n ∈ N, +is a supermartingale and the process z(n ∧ ˆτ/δ), n ∈ N, is a martingale, where +ˆτ := δ inf{n ∈ N: uB(Xnδ) ≤ G(Xnδ)}. +(A.9) +Proof. To ease the notation, let us define +ˆuB(x) := sup +τ∈T δ +x,b +ln Ex +� +exp +�� τ∧τB +0 +g(Xs)ds + G(Xτ∧τB) +�� +, +x ∈ E, +un +B(x) := sup +τ∈T δ +τ≤nδ +ln Ex +� +exp +�� τ∧τB +0 +g(Xs)ds + G(Xτ∧τB) +�� +, +n ∈ N, x ∈ E, +and note that we get un +B(x) ≤ ˆuB(x) ≤ uB(x), +x ∈ E. Next, note that using +the boundedness of G and Proposition A.2, by Lebesgue’s dominated convergence +theorem, we obtain +uB(x) = sup +τ∈T +lim +n→∞ ln Ex +� +exp +�� τ∧(nδ)∧τB +0 +g(Xs)ds + G(Xτ∧(nδ)∧τB) +�� +, +x ∈ E. + +24 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +Also, for any n ∈ N, x ∈ E, and τ ∈ T δ, we get +un +B(x) ≥ ln Ex +� +exp +�� τ∧(nδ)∧τB +0 +g(Xs)ds + G(Xτ∧(nδ)∧τB) +�� +, +x ∈ E. +Thus, letting n → ∞ and taking the supremum with respect to τ ∈ T δ, we get +limn→∞ un +B(x) ≥ uB(x), x ∈ E. Consequently, we have +lim +n→∞ un +B(x) = ˆuB(x) = uB(x), +x ∈ E, +which concludes the proof of (A.8). +Let us now show the continuity of the map x �→ uB(x) and the martingale +characterisation. To see this, note that using a standard argument one may show +that, for any n ∈ N and x ∈ B, we get +u0 +B(x) = G(x), x ∈ B, +eun+1 +B +(x) = max(eG(x), Ex +� +1{Xδ∈B}e +� δ +0 g(Xs)ds+un +B(Xδ) + 1{Xδ /∈B}e +� δ +0 g(Xs)ds+G(Xδ)� +, +and, for any n ∈ N and x /∈ B, we get un +B(x) = G(x); see e.g. Section 2.2 in [28] +for details. Thus, letting n → ∞, for x ∈ B, we have +euB(x) = max(eG(x), Ex +� +1{Xδ∈B}e +� δ +0 g(Xs)ds+uB(Xδ) + 1{Xδ /∈B}e +� δ +0 g(Xs)ds+G(Xδ)� +, +while for x /∈ B, we get uB(x) = G(x). Also, using Assumption (A2), we get that +the process X is strong Feller. Thus, repeating the argument used in Lemma 4 +from Chapter II.5 in [13], we get that, for any bounded and measurable function +h: E �→ R, the map +E ∋ x �→ Ex +� +e +� δ +0 g(Xs)dsh(Xt) +� +is continuous and bounded. Applying this observation to h(x) := 1{x∈B}euB(x) and +h(x) := 1{x/∈B}eG(x), x ∈ E, we get the continuity of x �→ uB(x). Also, using the +argument from Proposition 3.2 we get that zδ(n), n ∈ N is a supermartingale and +z(n ∧ ˆτ/δ), n ∈ N, is a martingale, which concludes the proof. +□ +References +[1] A. Arapostathis and A. Biswas. Infinite horizon risk-sensitive control of dif- +fusions without any blanket stability assumptions. Stochastic Processes and +their Applications, 128:1485–1524, 2018. +[2] A. Basu and �L. Stettner. Zero-sum Markov games with impulse controls. SIAM +Journal on Control and Optimization, 58(1):580–604, 2020. +[3] E. Bayraktar, T. Emmerling, and J. Menaldi. On the impulse control of jump +diffusions. SIAM Journal on Control and Optimization, 51(3):2612–2637, 2013. +[4] A. Bensoussan and J.-L. Lions. Impulse Control And Quasi-Variational In- +equalities. Gauthier-Villars, Montrouge, 1984. +[5] T. R. Bielecki and S. R. 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Springer International Publishing. +[24] M. Pitera and �L. Stettner. +Long-run risk sensitive dyadic impulse control. +Applied Mathematics & Optimization, 84(1):19–47, 2021. +[25] A. Piunovskiy, A. Plakhov, and M. Tumanov. Optimal impulse control of a SIR +epidemic. Optimal Control Applications and Methods, 41(2):448–468, 2020. +[26] M. +Robin. +Contrˆole +impulsionnel +des +processus +de +Markov. +th`ese +d’´etat, +Universit´e +Paris +Dauphine, +1978. +Available +at +https://tel.archives-ouvertes.fr/tel-00735779. +[27] W. J. Runggaldier and K. Yasuda. Classical and restricted impulse control +for the exchange rate under a stochastic trend model. Journal of Economic +Dynamics and Control, 91:369–390, 2018. + +26 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD +[28] A. Shiryaev. Optimal Stopping Rules. Springer, 1978. +[29] �L. Stettner. On impulsive control with long run average cost criterion. In +Stochastic Differential Systems, pages 354–360. 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SIAM Journal on Control and Optimization, 60(4):2115– +2131, 2022. +Statements and Declarations +Damian Jelito and �Lukasz Stettner acknowledge research support by Polish Na- +tional Science Centre grant no. 2020/37/B/ST1/00463. +The authors have no relevant financial or non-financial interests to disclose. +The authors contributed equally to this work. + diff --git a/3NE2T4oBgHgl3EQf5wjH/content/tmp_files/load_file.txt b/3NE2T4oBgHgl3EQf5wjH/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..82a70a6b28b7af38b48ed269c96c40551715956a --- /dev/null +++ b/3NE2T4oBgHgl3EQf5wjH/content/tmp_files/load_file.txt @@ -0,0 +1,981 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf,len=980 +page_content='arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='04194v1 [math.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='OC] 10 Jan 2023 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD DAMIAN JELITO∗,† AND �LUKASZ STETTNER∗ Abstract.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We consider a long-run impulse control problem for a generic Markov process with a multiplicative reward functional.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We construct a solu- tion to the associated Bellman equation and provide a verification result.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The argument is based on the probabilistic properties of the underlying process combined with the Krein-Rutman theorem applied to the specific non-linear operator.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, it utilises the approximation of the problem in the bounded domain and with the help of the dyadic time-grid.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Keywords: impulse control, Bellman equation, risk-sensitive criterion, Markov process MSC2020 subject classifications: 93E20, 49J21, 49K21, 60J25 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Introduction Impulse control constitutes a versatile framework for controlling real-life stochas- tic systems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In this type of control, a decision-maker determines intervention times and instantaneous after-intervention states of the controlled process.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' By doing so, one can affect a continuous time phenomenon in a discrete time manner.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Conse- quently, impulse control attracted considerable attention in the mathematical liter- ature;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' [4, 9, 26] for classic contributions and [3, 10, 19, 21] for more recent results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In addition to generic mathematical properties, impulse control problems were studied with reference to specific applications including i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='a.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' controlling ex- change rates, epidemics, and portfolios with transaction costs;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' [18, 25, 27] and references therein.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' When looking for an optimal impulse control strategy, one must decide on the optimality criterion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Recently, considerable attention was paid to the so-called risk-sensitive functional given, for any γ ∈ R, by µγ(Z) := � 1 γ ln E[exp(γZ)], γ ̸= 0, E[Z], γ = 0, (1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1) where Z is a (random) payoff corresponding to a chosen control strategy;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see [14] for a seminal contribution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' This functional with γ = 0 corresponds to the usual linear criterion and the case γ < 0 is associated with risk-averse preferences;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see [5] for a comprehensive overview.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, the functional with γ > 0 could be linked to the asymptotics of the power utility function;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see [31] for details.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Recent comprehensive discussion on the long-run version with µγ could be found in [6].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We refer also ∗Institute of Mathematics, Polish Academy of Sciences, Warsaw, Poland E-mail addresses: djelito@impan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='pl, l.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='stettner@impan.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='pl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' †Corresponding author.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' 1 2 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD to [23] and references therein for a discussion on the connection between (1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1) and the duality of the large deviations-based criteria.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In this paper we focus on the use of the functional µγ with γ > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' More specif- ically, we consider the impulse control problem for some continuous time Markov process and construct a solution to the associated Bellman equation which char- acterises an optimal impulse control strategy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' To do this, we study the family of impulse control problems in bounded domains and then extend the analysis to the generic locally compact state space.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' This idea was used in [1], where PDEs tech- niques were applied to obtain the characterisation of the controlled diffusions in the risks-sensitive setting.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' A similar approximation for the the average cost per unit time problem was considered in [32].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The main contribution of this paper is a construction of a solution to the Bell- man equation associated with the problem, see Theorem 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1 for details.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' It should be noted that we get a bounded solution even though the state space could be unbounded and we assume virtually no ergodicity conditions for the uncontrolled process.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, note that present results for γ > 0 complement our recent findings on the impulse control with the risk-averse preferences;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see [24] for the dyadic case and [15] for the continuous time framework.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Nevertheless, it should be noted that the techniques for γ < 0 and γ > 0 are substantially different and it is not possible to directly transform the results in one framework to the other;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' [16, 20] for further discussion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The structure of this paper is as follows.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In Section 2 we formally introduce the problem, discuss the assumptions and, in Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='3, provide a verification argument.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Next, in Section 3 we consider an auxiliary dyadic problem in a bounded domain and in Theorem 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1 we construct a solution to the corresponding Bellman equation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' This is used in Section 4 where we extend our analysis to the unbounded domain with the dyadic time-grid;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see Theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Next, in Section 5 we finally construct a solution to the Bellman equation for the original problem;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see Theo- rem 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Finally, in Appendix A we discuss some properties of the optimal stopping problems that are used in this paper.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Preliminaries Let X = (Xt)t≥0 be a continuous time standard Feller–Markov process on a filtered probability space (Ω, F, (Ft), P).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The process X takes values in a locally compact separable metric space E endowed with a metric ρ and the Borel σ-field E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' With any x ∈ E we associate a probability measure Px describing the evolution of the process X starting in x;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see Section 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='4 in [28] for details.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, we use Ex, x ∈ E, and Pt(x, A) := Px[Xt ∈ A], t ≥ 0, x ∈ E, A ∈ E, for the corresponding expectation operator and the transition probability, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' By Cb(E) we denote the family of continuous bounded real-valued functions on E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, to ease the notation, by T , Tx, and Tx,b we denote the families of stopping times, Px a.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' finite stopping times, and Px a.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' bounded stopping times, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, for any δ > 0, by T δ ⊂ T , T δ x ⊂ Tx, and T δ x,b ⊂ Tx,b, we denote the respective subfamilies of dyadic stopping times, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' those taking values in the set {0, δ, 2δ, .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='} ∪ {∞}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Throughout this paper we fix some compact U ⊆ E and we assume that a decision-maker is allowed to shift the controlled process to U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' This is done with the help of an impulse control strategy, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' a sequence V := (τi, ξi)∞ i=1, where (τi) ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 3 is an increasing sequence of stopping times and (ξi) is a sequence of Fτi-measurable after-impulse states with values in U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' With any starting point x ∈ E and a strategy V we associate a probability measure P(x,V ) for the controlled process Y .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Under this measure, the process starts at x and follows its usual (uncontrolled) dynamics up to the time τ1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Then, it is immediately shifted to ξ1 and starts its evolution again, etc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' More formally, we consider a countable product of filtered spaces (Ω, F, (Ft)) and a coordinate process (X1 t , X2 t , .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Then, we define the controlled process Y as Yt := Xi t, t ∈ [τi−1, τi) with the convention τ0 ≡ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Under the measure P(x,V ) we get Yτi = ξi;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' we refer to Chapter V in [26] for the construction details;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see also Appendix in [8] and Section 2 in [29].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' A strategy V = (τi, ξi)∞ i=1 is called admissible if for any x ∈ E we get P(x,V )[limn→∞ τn = ∞] = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The family of admissible impulse control strategies is denoted by V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, note that, to simplify the notation, by Yτ − i := Xi τi, i ∈ N∗, we denote the state of the process right before the ith impulse (yet, possibly, after the jump).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In this paper we study the asymptotics of the impulse control problem given by sup V ∈V J(x, V ), x ∈ E, (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1) where, for any x ∈ E and V ∈ V, we set J(x, V ) := lim inf T →∞ 1 T ln E(x,V ) � e � T 0 f(Ys)ds+�∞ i=1 1{τi≤T }c(Yτ− i ,ξi)� , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='2) with f denoting the running cost function and c being the shift-cost function, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Note that this could be seen as a long-run standardised version of the functional (1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1) with γ > 0 applied to the impulse control framework.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Here, the standardisation refers to the fact that we do not use directly the parameter γ (apart from its sign).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, the problem is of the long-run type, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' the utility is averaged over time which improves the stability of the results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The analysis in this paper is based on the approximation of the problem in a bounded domain.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Thus, we fix a sequence (Bm)m∈N of compact sets satisfying Bm ⊂ Bm+1 and E = �∞ m=0 Bm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, we assume that U ⊂ B0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Next, we assume the following conditions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (A1) (Cost functions).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The map f : E �→ R− is a continuous and bounded.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, the map c : E × U �→ R− is continuous, bounded, and strictly non-positive, and satisfies the triangle inequality, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' for some c0 < 0, we have 0 > c0 ≥ c(x, ξ) ≥ c(x, η) + c(η, ξ), x ∈ E, ξ, η ∈ U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, we assume that c satisfies the uniform limit at infinity condition lim ∥x∥,∥y∥→∞ sup ξ∈U |c(x, ξ) − c(y, ξ)| = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='3) (A2) (Transition probability continuity).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' For any t, the transition probability Pt is continuous with respect to the total variation norm, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' for any sequence (xn) ⊂ E converging to x ∈ E, we get lim n→∞ sup A∈E |Pt(xn, A) − Pt(x, A)| = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (A3) (Distance control).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' For any compact set Γ ⊂ E, t0 > 0, and r0 > 0, we have lim r→∞ MΓ(t0, r) = 0, lim t→0 MΓ(t, r0) = 0, (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='4) 4 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD where MΓ(t, r) := supx∈Γ Px[sups∈[0,t] ρ(Xs, x) ≥ r], t, r > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (A4) (Process irreducibility).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' For any m ∈ N, x ∈ Bm, δ > 0, and any open set O ⊂ Bm, we have Px [∪∞ i=1{Xiδ ∈ O}] = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, we assume that for any x ∈ E, δ > 0, and m ∈ N, we have Px[τBm < ∞] = 1 (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='5) where τBm := δ inf{k ∈ N: Xkδ /∈ Bm}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Before we proceed, let us comment on these assumptions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' First, note that (A1) states typical cost-functions conditions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In particular, the non-positivity assump- tion for f is merely a technical normalisation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Indeed, for a generic ˜f ∈ Cb(E) we may set f(·) := ˜f(·) − ∥ ˜f∥ ≤ 0 to get Jf(x, V ) = J ˜f(x, V ) − ∥ ˜f∥, x ∈ E, V ∈ V, where Jf denotes the version of the functional J from (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='2) corresponding to the running cost function f.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Second, Assumption (A2) states that the transition probabilities Pt(x, ·) are continuous with respect to the total variation norm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Note that this directly implies that the transition semigroup associated to X is strong Feller, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' for any t > 0 and a bounded measurable map h: E �→ R, the map x �→ Ex[h(Xt)] is continuous and bounded.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Third, Assumption (A3) quantifies distance control properties of the underlying process.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' It states that, for a fixed time horizon, the process with a high probability stays close to its starting point and, with a fixed radius, with a high probability it does not leave the corresponding ball with a sufficiently short time horizon.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Note that these properties are automatically satisfied if the transition semigroup is C0- Feller;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' see Proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1 in [21] and Proposition 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='4 in [2] for details.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Finally, Assumption (A4) states a form of the irreducibility of the process X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' It requires that the process visits a sufficiently rich family of sets with unit probability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' To solve (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1), we show the existence of a solution to the impulse control Bellman equation, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' a function w ∈ Cb(E) and a constant λ ∈ R satisfying w(x) = sup τ∈Tx,b ln Ex � exp �� τ 0 (f(Xs) − λ)ds + Mw(Xτ) �� , x ∈ E, (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6) where the operator M is given by Mh(x) := sup ξ∈U (c(x, ξ) + h(ξ)), h ∈ Cb(E), x ∈ E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We start with a simple observation giving a lower bound for the constant λ from (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' To do this, we define the semi-group type by r(f) := lim t→∞ 1 t ln sup x∈E Ex � e � t 0 f(Xs)ds� ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='7) see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Proposition 1 in [30] for a discussion on the properties of r(f).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Lemma 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Let (w, λ) be a solution to (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Then, we get λ ≥ r(f).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' From (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6), for any T ≥ 0, we get w(x) ≥ ln Ex � e � T 0 (f(Xs)−λ)ds+Mw(XT )� .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 5 Thus, using the boundedness of w and Mw, we get ∥w∥ ≥ sup x∈E ln Ex � e � T 0 (f(Xs)−λ)ds� − ∥Mw∥.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Consequently, dividing both hand-sides by T and letting T → ∞, we get 0 ≥ r(f − λ), which concludes the proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' □ Let us now link a solution to (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6) with the optimal value and an optimal strategy for (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' To ease the notation, we recursively define the strategy ˆV := (ˆτi, ˆξi)∞ i=1 for i ∈ N \\ {0} by � ˆτi := inf{t ≥ ˆτi−1 : w(Xi t) = Mw(Xi t)}, ˆξi := arg maxξ∈U � c(Xi ˆτi, ξ) + w(ξ) � 1{ˆτi<∞} + ξ01{ˆτi=∞}, (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='8) where ˆτ0 := 0 and ξ0 ∈ U is some fixed point.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' First, we show that ˆV is a proper strategy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Proposition 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The strategy ˆV given by (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='8) is admissible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' To ease the notation, we define N(0, T ) := �∞ i=1 1{ˆτi≤T }, T ≥ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We fix some T > 0 and x ∈ E, and show that we get P(x, ˆV )[N(0, T ) = ∞] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='9) Recalling (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='8), on the event A := {limi→∞ ˆτi < +∞}, for any n ∈ N, n ≥ 1, we get w(Xn ˆτn) = Mw(Xn ˆτn) = c(Xn ˆτn, Xn+1 ˆτn ) + w(Xn+1 ˆτn ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Also, recalling that c(x, ξ) ≤ c0 < 0, x ∈ E, ξ ∈ U, for any n ∈ N, n ≥ 1, we have w(Xn+1 ˆτn )−w(Xn ˆτn) = −c(Xn ˆτn, Xn+1 ˆτn ) ≥ −c0 > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Using this observation and Assumption (A3), we esti- mate the distance between consecutive impulses which will be used to prove (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='9).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' More specifically, for any k, m ∈ N, k, m ≥ 1, we get k+m−2 � n=k (w(Xn+1 ˆτn ) − w(Xn+1 ˆτn+1)) + (w(Xk+m ˆτk+m−1) − w(Xk+1 ˆτk )) = w(Xk+1 ˆτk ) + k+m−1 � n=k+1 (w(Xn+1 ˆτn ) − w(Xn ˆτn)) − w(Xk+1 ˆτk ) = k+m−1 � n=k+1 (w(Xn+1 ˆτn ) − w(Xn ˆτn)) ≥ −(m − 1)c0;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='10) it should be noted that the specific values for k and m will be determined later.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Using the continuity of w we may find K > 0 such that supx,y∈U(w(x) − w(y)) ≤ K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Let m ∈ N be big enough to get −(m − 1) c0 2 > K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Thus, noting that Xk+m ˆτk+m−1, Xk+1 ˆτk ∈ U, we have (w(Xk+m ˆτk+m−1) − w(Xk+1 ˆτk )) ≤ K < −(m − 1) c0 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Con- sequently, recalling (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='10), on A, we get k+m−2 � n=k (w(Xn+1 ˆτn ) − w(Xn+1 ˆτn+1)) ≥ −(m − 1)c0 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='11) Recalling the compactness of U and the continuity of w we may find r > 0 such that for any x ∈ U and y ∈ E satisfying ρ(x, y) < r we get |w(x) − w(y)| < − c0 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' 6 ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD Let us now consider the family of events Bk := k+m−2 � n=k {ρ(Xn+1 ˆτn , Xn+1 ˆτn+1) < r}, k ∈ N, k ≥ 1, (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='12) and note that, for any k ∈ N, k ≥ 1, on Bk ∩ A we have �k+m−2 n=k (w(Xn+1 ˆτn ) − w(Xn+1 ˆτn+1)) < −(m − 1) c0 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Thus, recalling (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='11), for any k ∈ N, k ≥ 1, we get P(x0, ˆV )[Bk ∩ A] = 0 and, in particular, we have P(x0, ˆV )[Bk ∩ {N(0, T ) = ∞}] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='13) Let us now show that lim supk→∞ P(x0, ˆV )[Bc k ∩{N(0, T ) = ∞}] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Noting that {N(0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' T ) = ∞} = {limi→∞ ˆτi ≤ T },' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' for any t0 > 0 and k ∈ N,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' k ≥ 1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' we get P(x0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ˆV ) [Bc k ∩ {N(0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' T ) = ∞}] ≤ P(x0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ˆV ) ��k+m−2 � n=k {ρ(Xn+1 ˆτn ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Xn+1 ˆτn+1) ≥ r} ∩ {ˆτn+1 − ˆτn ≤ t0} � ∩ { lim i→∞ ˆτi ≤ T } � + P(x0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ˆV ) ��k+m−2 � n=k {ρ(Xn+1 ˆτn ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Xn+1 ˆτn+1) ≥ r} ∩ {ˆτn+1 − ˆτn > t0} � ∩ { lim i→∞ ˆτi ≤ T } � ≤ P(x0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ˆV ) �k+m−2 � n=k { sup t∈[0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='t0] ρ(Xn+1 ˆτn ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Xn+1 ˆτn+t) ≥ r} ∩ { lim i→∞ ˆτi ≤ T } � + P(x0,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' ˆV ) �k+m−2 � n=k {ˆτn+1 − ˆτn > t0} ∩ { lim i→∞ ˆτi ≤ T } � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='14) Using Assumption (A3), for any ε > 0, we may find t0 > 0, such that sup x∈U Px � sup t∈[0,t0] ρ(X0, Xt) ≥ r � ≤ ε m − 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='15) Thus, using the strong Markov property and noting that Xn+1 ˆτn ∈ U, for any k ∈ N, k ≥ 1, we get P(x0, ˆV ) �k+m−2 � n=k { sup t∈[0,t0] ρ(Xn+1 ˆτn , Xn+1 ˆτn+t) ≥ r} ∩ { lim i→∞ ˆτi ≤ T } � ≤ k+m−2 � n=k P(x0, ˆV ) � { sup t∈[0,t0] ρ(Xn+1 ˆτn , Xn+1 ˆτn+t) ≥ r} ∩ {ˆτn ≤ T } � = k+m−2 � n=k P(x0, ˆV ) � {ˆτn ≤ T }PXn+1 ˆτn � sup t∈[0,t0] ρ(X0, Xt) ≥ r �� ≤ ε.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='16) Recalling that ε > 0 was arbitrary, for any k ∈ N, k ≥ 1, we get P(x0, ˆV ) �k+m−2 � n=k { sup t∈[0,t0] ρ(Xn+1 ˆτn , Xn+1 ˆτn+t) ≥ r} ∩ { lim i→∞ ˆτi ≤ T } � = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='17) ASYMPTOTICS OF IMPULSE CONTROL PROBLEM WITH MULTIPLICATIVE REWARD 7 Now, to ease the notation, let Ck := �∞ n=k{ˆτn+1 − ˆτn > t0} ∩ {limi→∞ ˆτi ≤ T }, k ∈ N, k ≥ 1, and note that Ck+1 ⊂ Ck, k ∈ N, k ≥ 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' We show that lim k→∞ P(x0, ˆV ) [Ck] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' For the contradiction, assume that limk→∞ P(x0, ˆV ) [Ck] > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Consequently, we get P(x0, ˆV ) [�∞ k=1 Ck] > 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Note that for any ω ∈ �∞ k=1 Ck we have limi→∞ ˆτi(ω) ≤ T .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' In particular, we may find i0 ∈ N such that for any n ≥ i0 we get ˆτn+1(ω)− ˆτn(ω) ≤ t0 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' This leads to the contradiction as from the fact that ω ∈ �∞ k=1 Ck we also get ω ∈ ∞ � k=1 ∞ � n=k {ˆτn+1 − ˆτn > t0} ⊂ ∞ � n=i0 {ˆτn+1 − ˆτn > t0}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Consequently, we get limk→∞ P(x0, ˆV ) [Ck] = 0 and, in particular, we get lim sup k→∞ P(x0, ˆV ) �k+m−2 � n=k {ˆτn+1 − ˆτn > t0} ∩ { lim i→∞ ˆτi ≤ T } � ≤ lim k→∞ P(x0, ˆV ) [Ck] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Hence, recalling (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='14) and (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='17), we get lim sup k→∞ P(x0, ˆV ) [Bc k ∩ {N(0, T ) = ∞}] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Thus, recalling (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='13), for any k ∈ N, k ≥ 1, we obtain P(x0, ˆV ) [N(0, T ) = ∞] = P(x0, ˆV ) [Bc k ∩ {N(0, T ) = ∞}] , and letting k → ∞, we conclude the proof of (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='9).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' □ Now, we show the verification result linking (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6) with the optimal value and an optimal strategy for (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Theorem 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Let (w, λ) be a solution to (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='6) with λ > r(f).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Then, we get λ = sup V ∈V J(x, V ) = J(x, ˆV ), x ∈ E, where the strategy ˆV is given by (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='8).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Proof.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' The proof is based on the argument from Theorem 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='4 in [15] thus we show only an outline.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' First, we show that λ = J(x, ˆV ), x ∈ E, where the strategy ˆV is given by (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='8).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Let us fix x ∈ E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Then, combining the argument used in Lemma 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='1 in [2] and Proposition A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content='3, we get that the process e � ˆτ1∧T 0 (f(X1 s )−λ)ds+w(X1 ˆτ1∧T ), T ≥ 0, is a P(x, ˆV )-martingale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/3NE2T4oBgHgl3EQf5wjH/content/2301.04194v1.pdf'} +page_content=' Noting that on the event {ˆτk+1 < T } we get w(Xk+1 ˆτk+1) = Mw(Xk+1 ˆτk+1) = c(Xk+1 ˆτk+1, ˆξk+1) + w(ˆξk+1), k ∈ N, for any n ∈ N we recursively get ew(x) = E(x, ˆV ) � e � ˆτ1∧T 0 (f(Ys)−λ)ds+w(X1 ˆτ1∧T )� = E(x, ˆV ) � e � ˆτ1∧T 0 (f(Ys)−λ)ds+1{ˆτ1 Second time slot +Passive element +H +nid +H +:Hir +Hir +Destination +(S) +(D) +H +nrd +AF relay4 +SNR = +γs|(hH +rd + hH +idΘ2HH +ir)A(hsr + HirΘ1hsi)|2 +∥(hH +rd + hH +idΘ2HH +ir)AHirEKΘ1∥2 + ∥(hH +rd + hH +idΘ2HH +ir)A∥2 + ∥hH +idEKΘ2∥2 + 1. +(10) +where HH +ir ∈ CN×M is the channel from AF relay to IRS. +n2i ∼ CN(0, σ2 +2iEKIN) is the noise. The received signal at +D is as follows +yd = (hH +rd + hH +idΘ2HH +ir)yt + hH +idEKΘ2n2i + nd, +(7) +where hH +rd ∈ C1×M and hH +id ∈ C1×N are the channels from +AF relay to D and IRS to D. Θ2 = diag(α21, · · · , α2N) and +Φ2 = diag(φ21, · · · , φ2N) are the reflecting coefficient matri- +ces of EN and EK in the second time slot. nd ∼ CN(0, σ2 +d) is +the AWGN at D. Substituting (4) and (5) into (7) yields +yd = +� +Ps(hH +rd + hH +idΘ2HH +ir)A(hsr + HirΘ1hsi)x ++ (hH +rd + hH +idΘ2HH +ir)A(HirEKΘ1n1i + nr) ++ hH +idEKΘ2n2i + nd. +(8) +It is assumed that σ2 +1i = σ2 +2i = σ2 +r = σ2 +d = σ2 and γs = Ps +σ2 , +the achievable system rate can be defined as +R = 1 +2 log2(1 + SNR), +(9) +where SNR can be formulated as (10), as shown at the top of +next page. +B. Problem Formulation +To enhance the system rate performance, it is necessary +to maximize system rate. Maximizing rate is equivalent to +maximize SNR due to the fact that the log function is +a monotone increasing function of SNR. The optimization +problem is casted as +max +Θ1,Θ2,A SNR +(11a) +s.t. |Θ1(i, i)| = 1, |Θ2(i, i)| = 1, for i ∈ EL, +(11b) +γs∥EKΘ1hsi∥2 + ∥EKΘ1∥2 +F ≤ γi, +(11c) +γs∥A(hsr + HirΘ1hsi)∥2 ++ ∥AHirEKΘ1∥2 +F + ∥A∥2 +F ≤ γr, +(11d) +γs∥EKΘ2HH +irA(hsr + HirΘ1hsi)∥2 ++ ∥EKΘ2HH +irAHirEKΘ1∥2 +F ++ ∥EKΘ2HH +irA∥2 +F + ∥EKΘ2∥2 +F ≤ γi, (11e) +where γi = Pi +σ2 and γr = Pr +σ2 , Pi and Pr respectively denote +the transmit power budgets at IRS and AF relay. Since the +IRS is hybrid consisting of active and passive elements, it +is difficult to solve the optimization problem. To enhance the +rate performance, three efficient beamforming methods: 1) HP- +SDR-FP; 2) LC-SCA-FP; and 3) WF-GPI-GRR, are proposed +to optimize AF relay beamforming matrix A, IRS reflecting +coefficient matrices Θ1 and Θ2. +III. PROPOSED A HIGH-PERFORMANCE SDR-FP-BASED +MAX-SNR METHOD +In this section, a HP-SDR-FP method is proposed to solve +problem (11). To facilitate processing, problem (11) is de- +coupled into three subproblems by optimizing one and fixing +the other two. For each subproblem, we relax it as an SDR +problem, and combine Charnes-Cooper transformation of FP +algorithm to transform the SDR problem into an semidefinite +programming (SDP) problem. Furthermore, Gaussian random- +ization method is applied to recover the rank-1 solution. +A. Optimization of A Given Θ1 and Θ2 +Given Θ1 and Θ2, the optimization problem is reduced to +max +A +SNR +s.t. +(11d), +(11e). +(12) +Let us define a = vec(A) ∈ CM2×1, SNR can be translated +to +SNR = +γsaHB1a +aH(B2 + B3)a + ∥hH +idEKΘ2∥2 + 1, +(13) +where +B1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] +⊗ [(hH +rd + hH +idΘ2HH +ir)H(hH +rd + hH +idΘ2HH +ir)], (14a) +B2 = [(HirEKΘ1)∗(HirEKΘ1)T ] +⊗ [(hH +rd + hH +idΘ2HH +ir)H(hH +rd + hH +idΘ2HH +ir)], (14b) +B3 = IM ⊗ [(hH +rd + hH +idΘ2HH +ir)H(hH +rd + hH +idΘ2HH +ir)]. (14c) +In the same manner, the constraints (11d) and (11e) can be +respectively converted to +aH(γsC1 + C2 + IM2)a ≤ γr, +(15a) +aH(γsD1 + D2 + D3)a + ∥EKΘ2∥2 +F ≤ γi, +(15b) +where +C1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] ⊗ IM, (16a) +C2 = [(HirEKΘ1)∗(HirEKΘ1)T ] ⊗ IM, +(16b) +D1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] +⊗ [(EKΘ2HH +ir)H(EKΘ2HH +ir)], +(16c) +D2 = [(HirEKΘ1)∗(HirEKΘ1)T ] +⊗ [(EKΘ2HH +ir)H(EKΘ2HH +ir)], +(16d) +D3 = IM ⊗ [(EKΘ2HH +ir)H(EKΘ2HH +ir)]. +(16e) +Let us define �A = aaH ∈ CM2×M2, in accordance with the +rank inequality: rank P ≤ min{m, n}, where P ∈ Cm×n, we + +5 +can get rank(�A) ≤ rank(a) = 1. The optimization problem +can be recast as +max +�A +γstr(B1�A) +tr{(B2 + B3)�A} + ∥hH +idEKΘ2∥2 + 1 +(17a) +s.t. +tr{(γsC1 + C2 + IM2)�A} ≤ γr, +(17b) +tr{(γsD1 + D2 + D3)�A} + ∥EKΘ2∥2 +F ≤ γi, +(17c) +�A ⪰ 0, +rank(�A) = 1, +(17d) +which is a non-convex problem because of rank-one constraint. +After removing rank(�A) = 1 constraint, we have the SDR +problem of (17) as follows +max +�A +γstr(B1�A) +tr{(B2 + B3)�A} + ∥hH +idEKΘ2∥2 + 1 +(18a) +s.t. +(17b), +(17c), +�A ⪰ 0. +(18b) +The objective function (18a) is a linear fractional function with +respect to �A, which is a quasi-convex function with the denom- +inator > 0, so problem (18) is a quasi-convex problem with +convex constraints. It is necessary to apply Charnes-Cooper +transformation, which helps convert the optimization problem +from quasi-convex to convex. Introducing a slack variable m +and defining m = (tr{(B2 + B3)�A} + ∥hH +idEKΘ2∥2 + 1)−1, +the above problem (18) is further rewritten as follows +max +�A,m +γstr{B1�A} +(19a) +s.t. tr{(γsC1 + C2 + IM2)�A} ≤ mγr, +(19b) +tr{(γsD1 + D2 + D3)�A} + m∥EKΘ2∥2 +F ≤ mγi, (19c) +tr{(B2 + B3)�A} + m∥hH +idEKΘ2∥2 + m = 1, +(19d) +�A ⪰ 0, m > 0, +(19e) +where �A = m�A. Clearly, the above optimization problem has +become a SDP problem, which is directly solved by CVX. +The solution to problem (18) is �A = �A/m. However, the +rank-one constraint rank(�A) = 1 is not considered in the SDR +problem. Since the obtained solution �A is not generally rank- +one matrix, the Gaussian randomization method is applied to +achieve a rank-one solution �A, thereby, AF relay beamforming +matrix A is achieved. +B. Optimization of Θ1 Given A and Θ2 +Given that A and Θ2 are fixed, the optimization problem +can be represented by as follows +max +Θ1 +γs|hH +rid(hsr + HirΘ1hsi)|2 +∥hH +ridHirEKΘ1∥2 + ∥hH +rid∥2 + ∥hH +idEKΘ2∥2 + 1 +(20a) +s.t. +|Θ1(i, i)| = 1, +for i ∈ EL, +(20b) +(11c), +(11d), +(11e), +(20c) +where +hrid += +[(hH +rd + hH +idΘ2HH +ir)A]H. +In +order +to +further +simplify +the +objective +function +and +constraints +of +the +optimization +problem, +let +us +define +u1 += +[α11, · · · , α1N]T , we have hsr + HirΘ1hsi = Hsirv1 and +hH +ridHirEKΘ1 = uT +1 diag{hH +ridHirEK}, where v1 = [u1; 1] +and Hsir += +[Hirdiag{hsi}, hsr]. Substituting these for- +mulas into (20a), and due to ∥uT +1 diag{hH +ridHirEK}∥2 += +∥diag{hH +ridHirEK}u1∥2, the object function can be further +rewritten as +vH +1 F1v1 +vH +1 F2v1 +, +(21) +where F1 = γsHH +sirhridhH +ridHsir and F2 is written as (22) at +the top of next page. The constraint (20b) for passive elements +EL can be rewritten as +|v1(i)|2 = 1, +for i ∈ EL. +(23) +Obviously, ∥EKΘ1∥2 +F = ∥EKu1∥2, and the constraint (11c) +can be translated to +vH +1 G1v1 ≤ γi, +(24) +where +G1 = +� +γsdiag{hH +si}EKdiag{hsi} + EK +0N×1 +01×N +0 +� +. +(25) +Then for constraint (11d), according to the property of +Hadamard product: tr(X(Y ⊙ Z)) = tr((X ⊙ YT )Z), where +X ∈ Cm×n, Y ∈ Cn×m and Z ∈ Cn×m, we have +∥AHirEKΘ1∥2 +F = ∥AHirEKdiag{u1}∥2 +F += tr{EKHH +irAHAHirEKdiag{u1}diag{uH +1 }} += tr{EKHH +irAHAHir[EK ⊙ (u1uH +1 )]} += uH +1 [(EKHH +irAHAHir) ⊙ EK]u1 += uH +1 [(HH +irAHAHir) ⊙ EK]u1 +(26) +Inserting hsr + HirΘ1hsi = Hsirv1 and (26) back into the +constraint (11d), which can be rewritten as +vH +1 G2v1 ≤ γr, +(27) +where +G2 =γsHH +sirAHAHsir + +� +(HH +irAHAHir) ⊙ EK +0N×1 +01×N +∥A∥2 +F +� +. +(28) +Similarly, (11e) can be written in the following form +vH +1 G3v1 ≤ γi, +(29) +where G3 is written as (30), as shown at the top of the page. +Substituting the simplified objective function and constraints +into (20), the optimization problem can be equivalently trans- +formed into +max +v1 +(21) +(31a) +s.t. +(23), (24), (27), (29), v1(N + 1) = 1. +(31b) +Aiming at further transforming the optimization problem, and +defining V1 = v1vH +1 , problem (31) can be equivalently given +by +max +V1 +tr(F1V1) +tr(F2V1) +(32a) +s.t. +V1(i, i) = 1, +for i ∈ EL, +(32b) +V1(N + 1, N + 1) = 1, +(32c) +tr(G1V1) ≤ γi, tr(G2V1) ≤ γr, +(32d) +tr(G3V1) ≤ γi, rank(V1) = 1, V1 ⪰ 0. +(32e) + +6 +F2 = +� diag{EKHH +irhrid}diag{hH +ridHirEK} +0N×1 +01×N +∥hH +rid∥2 + ∥hH +idEKΘ2∥2 + 1 +� +, +(22) +G3 =γsHH +sirAHHirΘH +2 EKΘ2HH +irAHsir ++ +� +(HH +irAHHirΘH +2 EKΘ2HH +irAHir) ⊙ EK +0N×1 +01×N +∥EKΘ2HH +irA∥2 +F + ∥EKΘ2∥2 +F +� +. +(30) +Due to the fact that the object function is quasi-convex +and constraint rank(V1) = 1 is non-convex, (32) is still +a non-convex problem. Relaxing the rank-1 constraint, the +problem is transformed into a SDR problem, which can also be +solved by applying Charnes-Cooper transformation. Moreover, +introducing a slack variable τ, then defining τ = tr(F2V1)−1 +and �V1 = τV1, the SDR problem of (32) can be translated to +a SDP problem, i.e., +max +�V1,τ +tr(F1�V1) +(33a) +s.t. +�V1(i, i) = τ, +for i ∈ EL, +(33b) +�V1(N + 1, N + 1) = τ, τ > 0, +(33c) +tr(G1�V1) ≤ τγi, tr(G2�V1) ≤ τγr, +(33d) +tr(G3�V1) ≤ τγi, tr(F2�V1) = 1, �V1 ⪰ 0, +(33e) +which can be directly solved by CVX, thereby the solution V1 +of SDR problem of (32) is achieved, and Gaussian randomiza- +tion method is used to recover a rank-one solution V1. Then +the solution v1 is extracted from the eigenvalue decomposition +of V1, subsequently, IRS reflecting coefficient matrix Θ1 can +be obtained. +C. Optimization of Θ2 Given A and Θ1 +In the subsection, defining u2 = [α21, · · · , α2N]H, we have +hH +rd +hH +idΘ2HH +ir = vH +2 Hrid and Θ2HH +irA(hsr +HirΘ1hsi) = +diag{HH +irA(hsr + HirΘ1hsi)}u∗ +2, where v2 = [u2; 1] and +Hrid = [diag{hH +id}HH +ir; hH +rd]. Similarly, when A and Θ1 are +fixed, the SDP problem to optimize �V2 can be expressed as +max +�V2,ρ +tr(H1�V2) +(34a) +s.t. +�V2(i, i) = ρ, +for i ∈ EL, +(34b) +�V2(N + 1, N + 1) = ρ, ρ > 0, +(34c) +tr(J�V2) ≤ ργi, tr(H2�V2) = 1, �V2 ⪰ 0, +(34d) +where ρ = tr(H2v2vH +2 )−1 is a slack variable, �V2 = ρv2vH +2 , +H1 = γsHridA(hsr + HirΘ1hsi)[HridA(hsr + HirΘ1hsi)]H, +H2 =HridA(HirEKΘ1ΘH +1 EKHH +ir + IM)AHHH +rid ++ +� +diag{hH +idEK}diag{EKhid} +0N×1 +01×N +1 +� +, +(35) +and J is written as (36) at the top of next page, where +H3 += +EKdiag{HT +irA∗(hsr + HirΘ1hsi)∗} and H4 += +HH +irAHirEKΘ1. It is observed that (34) is similar to (33), +thus (34) can be solved in the same way as (33). Finally the +solutions v2 and Θ2 are obtained, and the details are omitted +here for brevity. +D. Overall Algorithm and Complexity Analysis +Since the objective function of problem (11) is non- +decreasing and the transmit powers of S, AF relay and IRS +active elements are limited, the objective function has an +upper bound. Therefore, the convergence of the proposed HP- +SDR-FP algorithm can be guaranteed. Our idea is alternative +iteration, that is, the alternative iteration process are performed +among A, Θ1 and Θ2 until the convergence criterion is +satisfied, while the system rate is maximum. The proposed +HP-SDR-FP method is summarized in Algorithm 1. +Algorithm 1 Proposed HP-SDR-FP Method +1. Initialize A0, Θ0 +1 and Θ0 +2. According to (9), R0 can be +obtained. +2. +set the convergence error δ and the iteration number +t = 0. +3. repeat +4. Given Θt +1 and Θt +2, solve problem (19) for �A +t+1, recover +rank-1 solution �A +t+1 via Gaussian randomization, obtain +At+1. +5. Given At+1 and Θt +2, solve problem (33) for �V +t+1 +1 +, +recover rank-1 solution Vt+1 +1 +via Gaussian randomization, +obtain Θt+1 +1 +. +6. Given At+1 and Θt+1 +1 +, solve problem (34) for �V +t+1 +2 +, +recover rank-1 solution Vt+1 +2 +via Gaussian randomization, +obtain Θt+1 +2 +. +7. Calculate Rt+1 by using At+1, Θt+1 +1 +and Θt+1 +2 +. +8. Update t = t + 1. +9. until +��Rt+1 − Rt�� ≤ δ. +After that, the complexity of Algorithm 1 is calculated +and analyzed according to problems (19), (33) and (34). +Problem (19) has 4 linear constraints with dimension 1, one +linear matrix inequality (LMI) constraint of size M 2 and +M 4+1 decision variables. Hence, the computational complex- +ity of problem (19) is denoted as O{nA +√ +M 2 + 4(M 6 + 4 + +nA(M 4 + 4) + n2 +A)ln(1/ε)} float-point operations (FLOPs), +where nA = M 4 + 1 and ε represents the computation +accuracy. For problem (33), there exit L + 6 linear constraints +with dimension 1, one LMI constraint of size N + 1 and +(N +1)2+1 decision variables, so the computational complex- +ity of problem (33) is written as O{nV1 +√ +N + L + 7((N + + +7 +J = +� +γsHH +3 H3 + (H4HH +4 + HH +irAAHHir + IN) ⊙ EK +0N×1 +01×N +0 +� +. +(36) +1)3 + L + 6 + nV1((N + 1)2 + L + 6) + n2 +V1)ln(1/ε)} FLOPs, +where nV1 = (N + 1)2 + 1. For problem (34), there are L + 4 +linear constraints with dimension 1, one LMI constraint of +size N + 1 and (N + 1)2 + 1 decision variables. Thus, the +computational complexity of problem (34) is expressed as +O{nV2 +√ +N + L + 5((N + 1)3 + L + 4 + nV2((N + 1)2 + +L + 4) + n2 +V2)ln(1/ε)} FLOPs, where nV2 = (N + 1)2 + 1. +Therefore, the total computational complexity of Algorithm 1 +is written by +O{D1[nA +� +M 2 + 4(M 6 + 4 + nA(M 4 + 4) + n2 +A) ++ nV1 +√ +N + L + 7((N + 1)3 + L + 6 + nV1((N + 1)2 ++ L + 6) + n2 +V1) + nV2 +√ +N + L + 5((N + 1)3 + L + 4 ++ nV2((N + 1)2 + L + 4) + n2 +V2)]ln(1/ε)} +(37) +FLOPs, where D1 is the maximum number of alternating +iterations needed for convergence in Algorithm 1. It is obvious +that the highest order of computational complexity is M 13 and +N 6.5 FLOPs. +IV. PROPOSED A LOW-COMPLEXITY SCA-FP-BASED +MAX-SNR METHOD +In the previous section, HP-SDR-FP method is proposed +to obtain AF relay beamforming matrix A, IRS reflecting +coefficient matrices Θ1 and Θ2. However, its computational +complexity is very high because of SDR algorithm with lots of +FLOPs. To reduce the high computational complexity of HP- +SDR-FP method, a low-complexity SCA-FP-based Max-SNR +method is proposed in this section. +A. Optimize A With Fixed Θ1 and Θ2 +For given Θ1 and Θ2, the optimization problem based on +(13) is given by +max +a +γsaHB1a +aH(B2 + B3)a + ∥hH +idEKΘ2∥2 + 1 +(38a) +s.t. +(15a), (15b). +(38b) +Observing the above objective function, it is seen that (38) +is also a fractional optimization problem. In the subsection, +Dinkelbachs transformation is introduced to solve problem +(38). Here, introducing a slack variables µ, the problem (38) +is reformulated as +max +a,µ +γsaHB1a − µ[aH(B2 + B3)a + ∥hH +idEKΘ2∥2 + 1] +(39a) +s.t. +(15a), (15b), +(39b) +where µ is iteratively updated by +µ(t + 1) = +γsaH(t)B1a(t) +aH(t)(B2 + B3)a(t) + ∥hH +idEKΘ2∥2 + 1, (40) +where t is the iteration number. µ is nondecreasing after each +iteration, which guarantees the convergence of the objective +function (39a). Note that the above problem is still non- +convex due to the first term of the objective function is non- +concave, which can be solved by using SCA method. We +approximate the first term by using a linear function, i.e., +its first-order Taylor expansion at feasible vector �a, which +is γsaHB1a ≥ 2γsℜ{aHB1�a} − γs�aHB1�a, where �a is the +solution of previous iteration. Inserting the low bound of +γsaHB1a back into problem (39) yields +max +a +2γsℜ{aHB1�a} − γs�aHB1�a +− µ[aH(B2 + B3)a + ∥hH +idEKΘ2∥2 + 1] +(41a) +s.t. +(15a), (15b). +(41b) +It is known that the above optimization problem consists of +a concave objective function and several convex constraints. +Therefore, problem (41) is a convex optimization problem. +When �a and µ are fixed, a can be directly achieved by CVX. +Correspondingly, A can be obtained. +B. Optimize Θ1 With Fixed A and Θ2 +It is assumed that AF relay beamforming matrix A and Θ2 +are given. The constraint (11b) can be re-expressed as +|u1(i)|2 = 1, +for i ∈ EL, +(42) +which can be relaxed as +uH +1 (i)u1(i) ≤ 1, +for i ∈ EL. +(43) +Problem (11) with respect to u1 can be rearranged as +max +u1 +γs|hH +1 u1 + a|2 +∥diag{hH +ridHirEK}u1∥2 + b +(44a) +s.t. +uH +1 (i)u1(i) ≤ 1, +for i ∈ EL, +(44b) +γs∥EKdiag{hsi}u1∥2 + ∥EKu1∥2 ≤ γi, +(44c) +γs∥Ahsr + P1u1∥2 + ∥AHirEKdiag{u1}∥2 +F ++ ∥A∥2 +F ≤ γr, +(44d) +γs∥h2 + P2u1∥2 + ∥P3EKdiag{u1}∥2 +F ≤ �γi, +(44e) +where +h1 = [(hH +rd + hH +idΘ2HH +ir)AHirdiag{hsi}]H, +(45a) +h2 = EKΘ2HH +irAhsr, P1 = AHirdiag{hsi}, +(45b) +P2 = EKΘ2HH +irAHirdiag{hsi}, +(45c) +P3 = EKΘ2HH +irAHir, a = (hH +rd + hH +idΘ2HH +ir)Ahsr, (45d) +b = ∥(hH +rd + hH +idΘ2HH +ir)A∥2 + ∥hH +idEKΘ2∥2 + 1, +(45e) +�γi = γi − ∥EKΘ2HH +irA∥2 +F − ∥EKΘ2∥2 +F . +(45f) + +8 +Problem (44) can be further converted to +max +u1 +γs|hH +1 u1 + a|2 +∥diag{hH +ridHirEK}u1∥2 + b +(46a) +s.t. +uH +1 (i)u1(i) ≤ 1, +for i ∈ EL, +(46b) +uH +1 (γsdiag{hH +si}EKdiag{hsi} + EK)u1 ≤ γi, +(46c) +uH +1 [γsPH +1 P1 + (HH +irAHAHir) ⊙ EK]u1 + ∥A∥2 +F ++ 2γsℜ{uH +1 PH +1 Ahsr} + γshH +srAHAhsr ≤ γr, +(46d) +uH +1 [γsPH +2 P2 + (PH +3 P3) ⊙ EK]u1 ++ 2γsℜ{uH +1 PH +2 h2} + γshH +2 h2 ≤ �γi. +(46e) +In the same manner, Dinkelbach’s transformation is also +introduced to problem (46). Problem (46) can be rewritten +as +max +u1 +γs|hH +1 u1 + a|2 − ωb +− ωuH +1 diag{EKHH +irhrid}diag{hH +ridHirEK}u1 (47a) +s.t. +(46b), (46c), (46d), (46e), +(47b) +where ω is a variable scalar, which is defined as +ω(t + 1) = +γs|hH +1 u1(t) + a|2 +∥diag{hH +ridHirEK}u1(t)∥2 + b. +(48) +Similarly, aiming at converting the objective function (47a) +to convex, the first-order Taylor expansion at the point �u1 is +employed to γs|hH +1 u1 + a|2 and transform it into the linear +function, i.e., |hH +1 u1 + a|2 ≥ 2ℜ{uH +1 h1(hH +1 �u1 + a)} + a∗a − +�uH +1 h1hH +1 �u1. Inserting the low bound of +��hH +1 u1 + a +��2 back into +problem (47) yields the following optimization problem +max +u1 +2γsℜ{uH +1 h1(hH +1 �u1 + a)} + γsa∗a − γs�uH +1 h1hH +1 �u1− +ω(b + uH +1 diag{EKHH +irhrid}diag{hH +ridHirEK}u1) (49a) +s.t. +(46b), (46c), (46d), (46e), +(49b) +where the object function is concave and the constraints are +convex, thus problem (49) is convex. For a given feasible +vector �u1 and ω, problem (49) can be solved by CVX directly, +thereby u1 is achieved. +C. Optimize Θ2 With Fixed A and Θ1 +Similarly, given AF relay beamforming matrix A and Θ1, +the optimization problem with respect to u2 is modeled as +max +u2 +2γsℜ{uH +2 h3(hH +3 �u2 + c∗)} + γscc∗ − γs�uH +2 h3hH +3 �u2 +− λ(uH +2 Q1QH +1 u2 + 2ℜ{uH +2 Q1h4} + hH +4 h4) +− λ(uH +2 Q2QH +2 u2 + 2ℜ{uH +2 Q2AHhrd}) +− λhH +rdAAHhrd − λuH +2 Q3QH +3 u2 − λ +(50a) +s.t. +uH +2 (i)u2(i) ≤ 1, for i ∈ EL, +(50b) +uH +2 [γsHH +3 H3 + (H4HH +4 + HH +irAAHHir + IN) ⊙ EK]u2 +≤ γi, +(50c) +where λ is a variable, �u2 is a feasible vector, and +h3 = diag{hH +id}HH +irA(hsr + HirΘ1hsi), +(51a) +h4 = (hH +rdAHirEKΘ1)H, +(51b) +Q1 = diag{hH +id}HH +irAHirEKΘ1, +(51c) +Q2 = diag{hH +id}HH +irA, Q3 = diag{hH +idEK}, +(51d) +c = hH +rdA(hsr + HirΘ1hsi), +(51e) +λ(t + 1) = +γs|uH +2 (t)h3 + c|2 +∥uH +2 (t)Q1 + hH +4 ∥2 + ∥uH +2 (t)Q2 + hH +rdA∥2 + ∥uH +2 (t)Q3∥2 + 1. +(51f) +It is clear that problem (50) is a convex optimization problem +with concave objective function and convex constraints. Given +�u2 and λ, u2 can be effectively obtained by CVX. +D. Overall Algorithm and Complexity Analysis +In the same manner, the proposed LC-SCA-FP method +is convergent with an upper bound. The alternate iteration +idea is roughly as follows: for given Θ1 and Θ2, first- +order Taylor expansion is applied in problem (39), AF relay +beamforming vector a can be calculated by solving problem +(41) iteratively; similarly, for given A and Θ2, reflecting +coefficient vector u1 can be obtained by solving problem (49) +iteratively; for given A and Θ1, reflecting coefficient vector +u2 can be achieved by solving problem (50) iteratively. Then +the alternative iteration process are operated among A, Θ1 +and Θ2 until the convergence criterion is satisfied, while the +system rate is maximum. The proposed LC-SCA-FP method +is summarized in Algorithm 2. +Furthermore, we calculate and analyze the complexity of +Algorithm 2 in accordance with problems (41), (49) and (50). +It is observed that problem (41) consists of one SOC constraint +of dimension M 2 and one SOC constraint of dimension +M 2 + 1. The number of decision variables na = M 2. The +computational complexity corresponding to problem (41) is +represented as O{2na(M 4+(M 2+1)2+n2 +a)ln(1/ε)} FLOPs. +Problem (49) includes L SOC constraints of dimension 1, +one SOC constraint of dimension N, one SOC constraint of +dimension N +1 and one SOC constraint of dimension N +2. +The number of decision variables nu1 = N. The computa- +tional complexity corresponding to problem (49) is written as +O{nu1 +√ +2L + 6(L+N 2+(N +1)2+(N +2)2+n2 +u1)ln(1/ε)} +FLOPs. Problem (50) is composed of L SOC constraints of +dimension 1 and one SOC constraint of dimension N. The +number of decision variables nu2 = N. The computational +complexity corresponding to problem (50) is expressed as +O{nu2 +√2L + 2(L+N 2+n2 +u2)ln(1/ε)} FLOPs. Consequently, +the total computational complexity of Algorithm 2 is denoted +as +O{D2[2na(M 4 + (M 2 + 1)2 + n2 +a) + nu1 +√ +2L + 6 +· (L + N 2 + (N + 1)2 + (N + 2)2 + n2 +u1) ++ nu2 +√ +2L + 2(L + N 2 + n2 +u2)]ln(1/ε)} +(52) +FLOPs, where D2 is the maximum number of alternating +iterations to obtain a, u1 and u2. For Algorithm 2, its highest + +9 +Algorithm 2 Proposed LC-SCA-FP Method +1. Initialize A0, Θ0 +1 and Θ0 +2. According to (9), R0 can be +obtained. +2. set the convergence error δ and the iteration number +t = 0. +3. repeat +4. Fix Θt +1 and Θt +2, initialize �a0, set δ and t1 = 0. +5. +repeat +6. +Update solution at1+1 with (�at1, µt1) by solving +problem (41), t1 = t1 + 1. +7. +Set �at1+1 = at1+1 and update µt1+1. +8. +until (41a) converges, update at+1 = at1+1 and +obtain At+1. +9. Fix At+1 and Θt +2, initialize �u0 +1, set δ and t2 = 0. +10. +repeat +11. +Update solution ut2+1 +1 +with (�ut2 +1 , wt2) by solving +problem (49), t2 = t2 + 1. +12. +Set �ut2+1 +1 += ut2+1 +1 +and update wt2+1. +13. +until (49a) converges, update ut+1 +1 += ut2+1 +1 +and +obtain Θt+1 +1 +. +14. Fix At+1 and Θt+1 +1 +, initialize �u0 +2, set δ and t3 = 0. +15. +repeat +16. +Update solution ut3+1 +2 +with (�ut3 +2 , λt3) by solving +problem (50), t3 = t3 + 1. +17. +Set �ut3+1 +2 += ut3+1 +2 +and update λt3+1. +18. +until (50a) converges, update ut+1 +2 += ut3+1 +2 +and +obtain Θt+1 +2 +. +19. Calculate R by using At+1, Θt+1 +1 +and Θt+1 +2 +, t = t+1. +20. until +��Rt+1 − Rt�� ≤ δ. +order of computational complexity is M 6 and N 3 FLOPS, +which is greatly reduced compared to the complexity of HP- +SDR-FP method. +V. PROPOSED A LOWER-COMPLEXITY +WF-GPI-GRR-BASED MAX-SNR METHOD +In what follows, to further reduce the computational com- +plexity, a lower-complexity WF-GPI-GRR-based Max-SNR +method is put forward. For gaining rate enhancement, we ap- +ply WF operation to exploit the colored property of noise and +present the related system model. Here, active IRS reflecting +coefficient matrix is split into amplifying coefficient and IRS +phase-shift matrix. The details of derivation on the amplifying +coefficients, AF relay beamforming matrix and IRS phase-shift +matrices are described as below. +A. System Model +For brevity, it is assumed that the amplifying coefficients of +each IRS active element in the first time slot and the second +time slot are |β1| and |β2|, respectively. Let us define +Ψ1 = EK �Θ1, Φ1 = |β1|EK �Θ1, +(53a) +Ψ2 = EK �Θ2, Φ2 = |β2|EK �Θ2, +(53b) +where the phase-shift matrix �Θ1 = diag(ejθ1i, · · · , ejθ1N ), +�Θ2 = diag(ejθ2i, · · · , ejθ2N), | �Θ1(i, i)| = 1 and | �Θ2(i, i)| = +1. Thus we have +Θ1 = (EK + |β1|EK) �Θ1, Θ2 = (EK + |β2|EK) �Θ2. (54) +In the first time slot, the received signal at AF relay can be +redescribed as +yr = +� +Ps[hsr + Hir(EK + |β1|EK) �Θ1hsi]x ++ (|β1|HirEK �Θ1n1i + nr) +� +�� +� +n1r +. +(55) +As matter of fact, n1r is color, not white. It is necessary for +us to whiten the color noise n1r by using covariance matrix +Cn. The covariance W1r of n1r is given by +W1r = β2 +1∥HirEK �Θ1∥2 +F σ2 + σ2. +(56) +While n1i and nr are the independent and identically dis- +tributed random vectors, n1r has a mean vector of all-zeros +and covariance matrix +C1r = β2 +1σ2HirEK �Θ1 �ΘH +1 EKHH +ir + σ2IM, +(57) +where obviously C1r is a positive definite matrix. Defining the +WF matrix W1r with W1rWH +1r = C−1 +1r , which yields +W1r = C +− 1 +2 +1r = (Q1rΛ1rQH +1r)− 1 +2 = Q1rΛ +− 1 +2 +1r QH +1r, +(58) +where Q1r is an unitary matrix, and Λ1r is a diagonal matrix +consisting of eigenvalues. Performing the WF operation to (55) +yields +yr = +� +PsW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]x ++ W1r(|β1|HirEK �Θ1n1i + nr) +� +�� +� +n1r +, +(59) +where n1r is the standard white noise with covariance matrix +IM. The transmit signal at AF relay is yt = Ayr. In the second +time slot, the received signal at D is denoted as +yd = +� +Ps[hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir]AW1r +· [hsr + Hir(EK + |β1|EK) �Θ1hsi]x ++ [hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir]An1r ++ |β2|hH +idEK �Θ2n2i + nd. +(60) +The corresponding SNR can be represented as (61), as shown +at the top of next page. It is assumed that the power budgets +Ps, Pr and Pi are respectively fully used to transmit signals +at S, AF relay and IRS. Therefore, the optimization problem +can be converted to +max +|β1|,|β2|, � +Θ1, � +Θ2,A +(61) +(62a) +s.t. +| �Θ1(i, i)| = 1, +| �Θ2(i, i)| = 1. +(62b) +It is necessary to solve the above problem for optimal |β1|, +|β2|, �Θ1, �Θ2 and A. + +10 +SNR = +γs|[hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir]AW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]|2 +β2 +1∥[hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir]AW1rHirEK �Θ1∥2 + ∥[hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir]AW1r∥2 + β2 +2∥hH +idEK �Θ2∥2 + 1 +. +(61) +B. Solve |β1| and |β2| +In the first time slot, the reflected signal at IRS is written +by +yt +1i = +� +PsΘ1hsix + Φ1n1i, += +� +PsEK �Θ1hsix +� +�� +� +ypt +1i ++ +� +Ps|β1|EK �Θ1hsix + |β1|EK �Θ1n1i +� +�� +� +yat +1i +, +(63) +where ypt +1i and yat +1i are respectively the signals reflected by +passive elements EL and active elements EK. Additionally, the +power consumed by the active elements is Pi. We have +Pi = Psβ2 +1∥EK �Θ1hsi∥2 + β2 +1∥EK �Θ1∥2 +F σ2 +1i += β2 +1Ps +K +� +k=1 +|ejθ1khk +si|2 + β2 +1 +K +� +k=1 +|ejθ1k|2σ2 +1i += β2 +1Ps +K +� +k=1 +|hk +si|2 + Kβ2 +1σ2, +(64) +where θ1k is the phase shift of the kth IRS active element +in the first time slot, hk +si is the channel between S and the +kth IRS active element and follows Rayleigh distribution with +the expression hk +si = +� +PLk +sigk +sie−jϕsk, where PLk +si, gk +si and +ϕsk denote the path loss, the channel gain and the channel +phase from S to the kth IRS active element, respectively. |gk +si|2 +follows Exponential distribution [41], and the corresponding +probability density function is given by +f|gk +si|2(x) = + + + +1 +λsi +e− +x +λsi +x ∈ [0, +∞), +(65a) +0 +otherwise, +(65b) +where λsi is the Exponential distribution parameter. Let us +define PLk +si is equal to the path loss from S to IRS (i.e., +PLsi). Using the weak law of large numbers, (64) can be +further written as +Pi = β2 +1Ps +K +� +k=1 +| +� +PLsigk +sie−jϕsk|2 + Kβ2 +1σ2 += β2 +1PsPLsi +K +� +k=1 +|gk +si|2 + Kβ2 +1σ2 +≈ Kβ2 +1PsPLsi · E(|gk +si|2) + Kβ2 +1σ2 += Kβ2 +1PsPLsiλsi + Kβ2 +1σ2, +(66) +β1 can be achieved as +|β1| = +� +Pi +KPsPLsiλsi + Kσ2 . +(67) +Similarly, the received signal of the kth active IRS element in +the second time slot is +yrk +2i = hH +rkAyr + n2i,k = hH +rkyt + n2i,k, +(68) +where hH +rk ∈ C1×M represents the channel between AF relay +and the kth active IRS element, +hH +rk = [ +� +PL1k +ri g1k +ri e−jϕ1k, · · · , +� +PLMk +ri gMk +ri e−jϕMk], (69) +where PLmk +ri , gmk +ri +and ϕmk are the path loss, the channel gain +and the channel phase between the mth antenna at AF relay +and the kth active IRS element. Defining PLmk +ri += PLri, +PLri is the path loss from AF relay to IRS. The reflected +signal of the kth active IRS element is +ytk +2i = |β2|ejθ2khH +rkyt + |β2|ejθ2kn2i,k += |β2||hH +rk||yt|ej(θ2k+ϕrkt) + |β2|ejθ2kn2i,k, +(70) +where θ2k is the phase shift of the kth IRS active element in +the second time slot, ϕrkt is the phase of hH +rkyt. It is assumed +that the transmit power of AF relay is Pr, the corresponding +power of the reflected signal of the kth active IRS element is +P tk +2i = β2 +2|hH +rk|2|yt|2 + β2 +2σ2 +2i,k += β2 +2PrPLri +M +� +m=1 +|gmk +ri |2 + β2 +2σ2 +K += Mβ2 +2PrPLriλri + β2 +2σ2 +K , +(71) +where σ2 +2i,k = σ2 +2i/K = σ2/K, λri is the Exponential +distribution parameter of channel from AF relay to IRS. Thus +the power of the reflected signal of K active IRS elements is +Pi = +K +� +k=1 +P tk +2i = KMβ2 +2PrPLriλri + β2 +2σ2, +(72) +which yields +|β2| = +� +Pi +KMPrPLriλri + σ2 . +(73) +C. Optimize A Given �Θ1 and �Θ2 +Aiming at maximizing the received signal power, MRC- +MRT method are applied to solve A as follows +A = A [hrd + Hir �ΘH +2 (EK + |β2|EK)hid] +∥hH +rd + hH +id(EK + |β2|EK) �Θ2HH +ir∥ +· [hsr + Hir(EK + |β1|EK) �Θ1hsi]HWH +1r +∥W1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]∥ += AΥ, +(74) +where A is the amplify factor of AF relay. Since the transmit +power of AF relay is Pr, we have A as shown in (75) at the top +of next page. Inserting A back into (74), A can be obtained. + +11 +A = +� +γr +γs∥ΥW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]∥2 + β2 +1∥ΥW1rHirEK �Θ1∥2 +F + ∥ΥW1r∥2 +F +, +(75) +�F2 = +� +β2 +1diag{EKHH +ir�hrid}diag{�h +H +ridHirEK} +0N×1 +01×N +∥�h +H +rid∥2 + β2 +2∥hH +idEK �Θ2∥2 + 1 +� +. +(77) +D. Optimize �Θ1 Given A and �Θ2 +By defining �u1 = [ejθ1i, · · · , ejθ1N ]T , �v1 = [�u1; 1] and +�Hsir = [Hir(EK + |β1|EK)diag{hsi}, hsr]. Given A and �Θ2, +the optimization problem is equivalent to +max +�v1 +�vH +1 �F1�v1 +�vH +1 �F2�v1 +(76a) +s.t. +|�v1(i)| = 1, ∀i = 1, 2, · · · , N, +(76b) +�v1(N + 1) = 1, +(76c) +where �F1 and �F2 are Hermitian matrices, and �F2 is positive +semi-definite. �F1 = γs �H +H +sir�hrid�h +H +rid �Hsir, �hrid = [(hH +rd + +hH +id(EK +|β2|EK) �Θ2HH +ir)AW1r]H, and �F2 is denoted as (77) +at the top of next page. The above problem can be relaxed to +max +�v1 +�vH +1 �F1�v1 +�vH +1 �F2�v1 +s.t. +∥�v1∥2 = N + 1, +(78) +which can be constructed as +max +�v1 +�vH +1 �F1�v1 +�vH +1 �F2�v1 +· �vH +1 IN+1�v1 +�vH +1 IN+1�v1 +s.t. +∥�v1∥2 = N + 1. (79) +�v1 can be solved by using GPI algorithm, the details of +GPI procedure is presented in Algorithm 3, where we define +Ω(�vt +1) = (�vH +1 �F1�v1)IN+1 + (�vH +1 IN+1�v1)�F1 and Ξ1(�vt +1) = +(�vH +1 �F2�v1)IN+1 + (�vH +1 IN+1�v1)�F2. +Algorithm 3 GPI Algorithm to Compute Phase-Shift +Vector �v1 with Given A and �Θ2 +1. Given A and �Θ2, and initialize �v0 +1. +2. Set the tolerance factor ξ and the iteration number t = 0. +3. repeat +4. +Compute the function matrix Ω(�vt +1) and Ξ1(�vt +1). +5. +Calculate yt = Ξ1(�vt +1)†Ω(�vt +1)�vt +1. +6. +Update �vt+1 +1 += +yt +∥yt∥. +7. +Update t = t + 1. +8. until +∥�vt+1 +1 +− �vt +1∥ ≤ ξ. +E. Optimize �Θ2 Given A and �Θ1 +If +A +and +�Θ1 +are +fixed, +let +us +define +�u2 += +[ejθ2i, · · · , ejθ2N ]H, �v2 = [�u2; 1], �Hrid = [diag{hH +id(EK + +|β2|EK)}HH +ir; hH +rd]. Accordingly, the optimization problem is +reduced to +max +�v2 +�vH +2 �H1�v2 +�vH +2 �H2�v2 +(80a) +s.t. +|�v2(i)| = 1, ∀i = 1, 2, · · · , N, +(80b) +�v2(N + 1) = 1, +(80c) +where �H1 and �H2 are Hermitian matrices, and �H2 is positive +definite. �H1 = γs �HridAW1r[hsr +Hir(EK +|β1|EK) �Θ1hsi]· +{�HridAW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]}H, and +�H2 = �HridAW1r(β2 +1HirEK �Θ1 �ΘH +1 EKHH +ir + IM)WH +1rAH· +�H +H +rid + +� +β2 +2diag{hH +idEK}diag{EKhid} +0N×1 +01×N +1 +� +. +(81) +We have the following relaxed transformation +max +�v2 +�vH +2 �H1�v2 +�vH +2 �H2�v2 +s.t. +�vH +2 �v2 = 1 +(82) +where �v2 = +�v2 +√N+1. Moreover, in line with the GRR theorem, +the optimal �v2 is obtained as the eigenvector corresponding +to the largest eigenvalue of �H +−1 +2 �H1. Thereby �v2 and �Θ2 is +achieved. +F. Overall Algorithm and Complexity Analysis +The proposed lower-complexity WF-GPI-GRR method is +summarized in Algorithm 4. The main idea consists of two +parts: the amplifying coefficient of active element and the +iterative idea. The analytic solutions of amplifying coefficients +of IRS active elements in the first time slot and the second time +slot, i.e., β1 and β2, are determined by the transmit power +of S, AF relay, IRS. Furthermore, β1 and β2 are denoted as +(67) and (73). The iterative idea can be described as follows: +for given �Θ1 and �Θ2, the closed-form expression of A are +represented as (74) by utilizing MRC-MRT; for given A and +�Θ2, GPI is applied to achieve �Θ1; for given A and �Θ1, �Θ2 is +obtained in a closed-form expression by using GRR theorem. +The alternative iteration process are performed among A, �Θ1 +and �Θ2 until the stop criterion is satisfied, while the system +rate is maximum. +In the following, the total computational complexity of +Algorithm 4 is calculated as +O{D3(N 3 + 4M 3 + 4M 2N + 2MN 2 + 2M 2K+ +8M 2 + 6N 2 + 9MN + 5MK + 5M + 11N+ +3 + D4(7N 3 + 27N 2 + 43N + 18))} +(83) + +12 +Algorithm 4 Proposed WF-GPI-GRR Method +1. +Calculate β1 and β2 through (67) and (73). +2. +Initialize A0, �Θ0 +1 and �Θ0 +2. According to (9) and (61), +R0 can be obtained. +3. +set the convergence error δ and the iteration number +t = 0. +4. repeat +5. +Fix �Θt +1 and �Θt +2, compute At+1 through (74). +6. +Fix At+1 and �Θt +2, solve problem (79) to achieve +�vt+1 +1 +based on GPI presented in Algorithm 3, �Θt+1 +1 += +diag{�vt+1 +1 +(1 : N)}. +7. +Fix At+1 and �Θt+1 +1 +, solve problem (82) to achieve +�vt+1 +2 +based on GRR theorem, �Θt+1 +2 += diag{�vt+1 +2 +(1 : N)}. +8. +Update Rt+1 by using β1, β2, At+1, �Θt+1 +1 +and �Θt+1 +2 +. +9. +Update t = t + 1. +10. until +��Rt+1 − Rt�� ≤ δ. +FLOPs, where D3 is the maximum number of alternating +iterations for Algorithm 4 and D4 is the number of iteration in +GPI algorithm. Its highest order of computational complexity +is M 3 and N 3 FLOPs, which is lower than the complexity of +Algorithm 1 and Algorithm 2. +VI. SIMULATION AND NUMERICAL RESULTS +In this section, in order to evaluate the rate performance +among the proposed three methods, numerical simulations are +performed. Moreover, it is assumed that S, D, hybrid IRS +and AF relay are located in three-dimensional (3D) space, the +related coordinate simulation setup is shown in Fig. 2, where +S, D, hybrid IRS and AF relay are located at (0, 0, 0), (0, 100, +0), (−10, 50, 20) and (10, 50, 10) in meter (m), respectively. +The path loss is modeled as PL(d) = PL0 − 10αlog10( d +d0 ), +where PL0 = −30dB is the path loss at the reference distance +d0 = 1m, d is the distance between transmitter and receiver, +and α is the path loss exponent, respectively. Here, the path +loss exponents of each channel link associated with IRS, i.e., +S-IRS, IRS-AF relay and IRS-D, are set as 2.0, and those of +S-AF relay and AF relay-D links are considered as 3.0. The +remaining system parameters are set as follow: σ2 = −80dBm +and EK is randomly generated. +Fig. 2. Simulation setup. +Additionally, to demonstrate the proposed three methods, +the following three benchmark schemes are taken into account. +1) AF relay+passive IRS: A passive IRS-aided AF relay +network is considered, where IRS only reflects the signal +without amplifying the reflected signal, and the reflecting +coefficient of each IRS element is set as 1; +2) AF relay+passive IRS with random phase: With ran- +dom phase of each reflection element uniformly and indepen- +dently generated from the interval (0, 2π], the beamforming +matrix A at AF relay is optimized. +3) Only AF relay: A AF relay network without IRS +is considered, while the AF relay beamforming matrix A +can be achieved by MRC-MRT, which is given by A = +� +Pr +Ps∥Γhsr∥2+σ2∥Γ∥2 +F Γ, where Γ = +hrdhH +sr +∥hH +rd∥∥hsr∥. +Towards a fair comparison between a hybrid IRS-aided +AF relay wireless network and the above three benchmark +schemes, let us define that the total transmit power budgets +of S and AF relay in the three benchmark schemes are the +same as that of S, AF relay and IRS in the hybrid IRS-aided +AF relay network. For instance, the AF relay transmit power +budget PR in the three benchmark schemes is equal to Pi+Pr. +4 +5 +6 +7 +8 +9 +10 +11 +12 +log2N +105 +1010 +1015 +1020 +1025 +1030 +Computational Complexity (FLOPs) +Proposed HP-SDR-FP +Proposed LC-SCA-FP +Proposed WF-GPI-GRR +Fig. 3. Computational complexity versus N with (M, K, D1, D2, D3, D4) = +(2, 4, 6, 10, 5, 2). +Fig. 3 plots the computational complexity of the proposed +three methods. By suppressing ln(1/ε) [42], the computational +complexities of the proposed three methods, 1) HP-SDR- +FP; 2) LC-SCA-FP; and 3) WF-GPI-GRR, increase as N +increases. It is clear that the first method has the highest +computational complexity, which is much higher than those +of the other two methods. In addition, the third method has +the lowest computational complexity. +Fig. 4 demonstrates the proposed three methods are con- +vergent under different Ps, respectively. Obviously, for Ps = +10dBm, the proposed HP-SDR-FP, LC-SCA-FP and WF-GPI- +GRR methods require about only four iterations to achieve the +rate ceil. While for Ps = 30dBm, it takes ten iterations for the +proposed three methods to converge to the rate ceil. From the +above two cases, we conclude that the proposed three methods +are feasible. +Fig. 5 shows the achievable rate versus Ps with (M, N, K) += (2, 32, 4). It can be seen that the proposed HP-SDR- +FP, LC-SCA-FP and WF-GPI-GRR methods with (Pi, Pr) = +(30dBm, 30dBm) perform better than AF relay+passive IRS, + +Hybrid IRS (-10, 50, 20) +y +AF relay (10, 50, 10) +S +(0, 0, 0) +(0, 100, 0) +X13 +0 +3 +6 +9 +12 +15 +18 +Number of iterations +4 +5 +6 +7 +8 +9 +10 +Achivable Rate(bits/s/Hz) +Proposed HP-SDR-FP +Proposed LC-SCA-FP +Proposed WF-GPI-GRR +30dBm +10dBm +Fig. 4. Convergence of proposed methods with (M, N, K, Pi, Pr) = (2, 32, +4, 30dBm, 30dBm). +0 +5 +10 +15 +20 +25 +30 + Ps (dBm) +0 +1 +2 +3 +4 +5 +6 +7 +8 +9 +Achivable Rate (bits/s/Hz) +Proposed HP-SDR-FP +Proposed LC-SCA-FP +Proposed WF-GPI-GRR +AF relay+passive IRS +AF relay+passive IRS with random phase +Only AF relay +Fig. 5. Achievable rate versus Ps with (M, N, K) = (2, 32, 4). +AF relay+passive IRS with random phase and only AF relay +with PR = 33dBm. Furthermore, the rate performance of LC- +SCA-FP method is the most closest to that of HP-SDR-FP +method in the low and medium power Ps region. For instance, +when power Ps is equal to 15dBm, the rate performance gaps +between the method LC-SCA-FP, the worst method WF-GPI- +GRR and the best method HP-SDR-FP method are respectively +0.037bits/s/Hz and 0.245bits/s/Hz. +Fig. 6 illustrates the achievable rate versus Pi +with +(M, N, K, Ps) = (2, 32, 4, 30dBm). It is particularly noted +that the proposed three methods with Pr = 30dBm make +a better rate performance improvement than that of AF re- +lay+passive IRS, AF relay+passive IRS with random phase +and only AF relay with PR = Pi + Pr. For example, when +Pi equals 40dBm, the proposed worst method, WF-GPI-GRR +method, can harvest up to 49.8% rate gain over AF re- +lay+passive IRS. The best method HP-SDR-FP approximately +has a 53.3% rate gain over AF relay+passive IRS. This shows +that as Pi increases, significant rate gains are achieved for +the proposed hybrid IRS-aided AF relay wireless network. +Moreover, the rate performance of LC-SCA-FP is getting +closer to that of HP-SDR-FP, and the gap between LC-SCA- +FP and WF-GPI-GRR becomes smaller. +10 +15 +20 +25 +30 +35 +40 + Pi (dBm) +3 +4 +5 +6 +7 +8 +9 +Achivable Rate (bits/s/Hz) +Proposed HP-SDR-FP +Proposed LC-SCA-FP +Proposed WF-GPI-GRR +AF relay+passive IRS +AF relay+passive IRS with random phase +Only AF relay +Fig. 6. Achievable rate versus P i with (M, N, K, Ps) = (2, 32, 4, 30dBm). +0 +1 +2 +3 +4 +5 +log2K +4 +5 +6 +7 +8 +9 +10 +Achivable Rate(bits/s/Hz) +Proposed HP-SDR-FP +Proposed LC-SCA-FP +Proposed WF-GPI-GRR +AF relay+passive IRS +AF relay+passive IRS with random phase +Only AF relay +Fig. 7. Achievable rate versus K with (M, N, Ps) = (2, 32, 30dBm). +Fig. 7 presents the achievable rate versus the number of +active IRS elements K with (M, N, Ps) = (2, 32, 30dBm) +for the proposed three methods with (Pi, Pr) = (30dBm, +30dBm) and the three benchmark schemes with PR = 33dBm. +From Fig. 7, it can be observed that as the number of active +IRS elements K increases, the rate gains of the proposed +three methods over AF relay+passive IRS, AF relay+passive +IRS with random phase and only AF relay increase gradually +and become more significant. Meanwhile, the proposed three +methods have the following increasing order on rate: HP- +SDR-FP, LC-SCA-FP and WF-GPI-GRR. Compared with the +benchmark scheme of AF relay+passive IRS, our proposed +three methods perform much better, which shows that the +optimization of beamforming is important and efficient. +VII. CONCLUSIONS +In this paper, we have made an investigation of beamform- +ing methods of optimizing the beamforming matrix at AF +relay and reflecting coefficient matrices at IRS in a hybrid +IRS-aided AF relay network, where the hybrid IRS includes +few active elements amplifying and reflecting the incident +signal. By using the criterion of Max SNR, three schemes, +namely HP-SDR-FP, LC-SCA-FP and WF-GPI-GRR, have + +14 +been proposed to improve the rate performance. Simulation +results show that the proposed three methods can make a +dramatic rate enhancement compared to AF relay+passive +IRS, AF relay+passive IRS with random phase and only +AF relay, which verifies the active IRS elements can break +the “double fading” effect caused by conventional passive +IRS. For instance, an approximate 50.0% rate gain over the +three benchmark schemes can be achieved in the high power +budget region of hybrid IRS. Therefore, a hybrid IRS-aided +AF relay network can provide an enhancement in accordance +with rate performance and extended coverage for the mobile +communications. +REFERENCES +[1] D. C. Nguyen, M. Ding, P. N. Pathirana, A. Seneviratne, J. Li, D. Niyato, +O. Dobre, and H. V. Poor, “6G internet of things: A comprehensive +survey,” IEEE Internet Things J., vol. 9, no. 1, pp. 359–383, Jan. 2022. +[2] L. Chettri and R. Bera, “A comprehensive survey on internet of things +(IoT) toward 5G wireless systems,” IEEE Internet Things J., vol. 7, +no. 1, pp. 16–32, Jan. 2020. +[3] B. M. Lee, “Adaptive switching scheme for rs overhead reduction in +massive MIMO with industrial internet of things,” IEEE Internet Things +J., vol. 8, no. 4, pp. 2585–2602, Feb. 2021. +[4] G. Yu, X. Chen, C. Zhong, D. W. Kwan Ng, and Z. 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Areas Commun., vol. 37, no. 2, pp. 253–268, Feb. 2019. + diff --git a/8dE1T4oBgHgl3EQfCAI3/content/tmp_files/load_file.txt b/8dE1T4oBgHgl3EQfCAI3/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..5d4957813753a08531e1bc759e7257b8c7bbf867 --- /dev/null +++ b/8dE1T4oBgHgl3EQfCAI3/content/tmp_files/load_file.txt @@ -0,0 +1,1085 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf,len=1084 +page_content='arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='02858v1 [eess.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='SP] 7 Jan 2023 1 Three Efficient Beamforming Methods for Hybrid IRS-aided AF Relay Wireless Networks Xuehui Wang, Feng Shu, Mengxing Huang, Fuhui Zhou, Riqing Chen, Cunhua Pan, Yongpeng Wu, and Jiangzhou Wang, Fellow, IEEE Abstract—Due to the “double fading” effect caused by con- ventional passive intelligent reflecting surface (IRS), the signal via the reflection link is weak.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To enhance the received signal, active elements with the ability to amplify the reflected signal are introduced to the passive IRS forming hybrid IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In this paper, a hybrid IRS-aided amplify-and-forward (AF) relay wireless network is considered, where an optimization problem is formulated to maximize signal-to-noise ratio (SNR) by jointly optimizing the beamforming matrix at AF relay and the reflecting coefficient matrices at IRS subject to the constraints of transmit power budgets at the source/AF relay/hybrid IRS and that of unit-modulus for passive IRS phase shifts.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To achieve high rate performance and extend the coverage range, a high-performance method based on semidefinite relaxation and fractional program- ming (HP-SDR-FP) algorithm is presented.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Due to its extremely high complexity, a low-complexity method based on successive convex approximation and FP (LC-SCA-FP) algorithm is put forward.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To further reduce the complexity, a lower-complexity method based on whitening filter, general power iterative and generalized Rayleigh-Ritz (WF-GPI-GRR) is proposed, where different from the above two methods, it is assumed that the amplifying coefficient of each active IRS element is equal, and the corresponding analytical solution of the amplifying coefficient can be obtained according to the transmit powers at AF relay and hybrid IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Simulation results show that the proposed three methods can greatly improve the rate performance compared to the existing networks, such as the passive IRS-aided AF relay and only AF relay network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In particular, a 50.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='0% rate gain over the existing networks is approximately achieved in the high power budget region of hybrid IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, it is verified that the proposed three efficient beamforming methods have an increasing This work was supported in part by the National Natural Science Foundation of China (Nos.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='U22A2002, 62071234 and 61972093), the Major Science and Technology plan of Hainan Province under Grant ZDKJ2021022, and the Scientific Research Fund Project of Hainan University under Grant KYQD(ZR)-21008.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (Corresponding authors: Feng Shu).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Xuehui Wang and Mengxing Huang are with the School of Information and Communication Engineering, Hainan University, Haikou, 570228, China.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Feng Shu is with the School of Information and Communication Engi- neering, Hainan University, Haikou 570228, China, and also with the School of Electronic and Optical Engineering, Nanjing University of Science and Technology, Nanjing 210094, China (e-mail: shufeng0101@163.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='com).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fuhui Zhou is with the College of Electronic and Information Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing 210000, China, also with the Key Laboratory of Dynamic Cognitive System of Electromag- netic Spectrum Space, Nanjing University of Aeronautics and Astronautics, Nanjing 210000, China, and also with the Ministry of Industry and Informa- tion Technology, Nanjing 211106, China (e-mail: zhoufuhui@ieee.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='org).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Riqing Chen is with the Digital Fujian Institute of Big Data for Agriculture, Fujian Agriculture and Forestry University, Fuzhou 350002, China (e-mail: riqing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='chen@fafu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='edu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='cn).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Cunhua Pan is with National Mobile Communications Research Laboratory, Southeast University, Nanjing 211111, China (e-mail: cpan@seu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='edu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='cn).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Yongpeng Wu is with the Shanghai Key Laboratory of Navigation and Location Based Services, Shanghai Jiao Tong University, Minhang 200240, China.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (e-mail: yongpeng.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='wu2016@gmail.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='com).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Jiangzhou Wang is with the School of Engineering, University of Kent, Canterbury CT2 7NT, U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Email: (e-mail: j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='wang@kent.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='ac.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='uk).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' order in rate performance: WF-GPI-GRR, LC-SCA-FP and HP- SDR-FP.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Index Terms—Double fading, intelligent reflecting surface, active elements, hybrid IRS, AF relay.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' INTRODUCTION With the rapid expansion of Internet-of-Things (IoT), the smart devices and data traffic explosively grows [1]–[3].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' There are more stringent requirements for IoT in terms of massive connectivity, extended coverage, low-latency, low-power, and low-cost [4]–[6].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Because of high hardware cost and energy consumption, some existing technologies [7], such as mil- limeter wave (mmWave), massive multiple-input multiple-out (MIMO), coordinated multi-point, wireless network coding, are far away from meeting the demands, e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', autonomous, ultra-large-scale, highly dynamic and fully intelligent services [8].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the existing wireless networks, adding relay nodes can not only save the number of base stations, but also realize the cooperation of multiple communication nodes, so as to improve the throughput and reliability [9], [10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' However, the relay is an active device, which needs much energy to process signals.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, it is imperative to develop a future wireless network, which is innovative, efficient and resource saving.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Owing to the advantages of low circuit cost, low energy con- sumption, programmability and easy deployment, intelligent reflecting surface (IRS) is attractive, which has gained much research attention from both academia and industry [11]–[13].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' IRS is composed of a large number of passive electromagnetic units, which are dynamically controlled to reflect incident signal forming an intelligent wireless propagation environment in a software-defined manner [14]–[17].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' From the perspective of electromagnetic theory, radiation pattern and physics nature of IRS unit, the free-space path loss models for IRS-assisted wireless communications were well introduced in [18].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A IRS-aided dual-hop visible light communication (VLC)/radio frequency (RF) system was proposed in [19] , where the performance analysis related to the outage probability and bit error rate (BER) were presented.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Because of reconfigurability, IRS has been viewed as an enabling and potential technology to achieve performance enhancement, spectral and energy efficiency improvement.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' With more and more research on IRS, IRS has been widely applied to the following scenarios, physi- cal layer security [20]–[22], simultaneous wireless information and power transfer (SWIPT) [23], [24], multicell MIMO communications [25], [26], covert communications [27], [28], and wireless powered communication network (WPCN) [29]– [31].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To maximize secrecy rate for IRS-assisted multi-antenna 2 systems in [22], where an efficient alternating algorithm was developed to jointly optimize the transmit covariance of the source and the phase shift matrix of the IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For multicell communication systems [25], IRS was deployed at the cell boundary.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' While a method of jointly optimizing the active precoding matrices at the base stations (BSs) and the phase shifts at the IRS was proposed to maximize the weighted sum rate of all users.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A IRS-aided secure MIMO WPCN is consid- ered in [31], by jointly optimizing the downlink (DL)/uplink (UL) time allocation, the energy transmit covariance matrix of hybrid access point (AP), the transmit beamforming matrix of users and the phase shifts of IRS, the maximum secrecy throughput of all users was achieved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Combining the advantages of IRS and relay is interesting, which can strike a good balance among cost, energy and per- formance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Recently, there were some related research works on the combination of IRS and relay appeared, which proved the combination could well serve for the wireless communication network in terms of coverage extension [32], [33], energy efficiency [34], spectral efficiency [35] and rate performance [36], [37].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The authors proposed an IRS-assisted dual-hop free space optical and radio frequency (FSO-RF) communication system with a decode-and-forward (DF) relaying protocol, and derived the exact closed-form expressions for the outage probability and bit error rate (BER) [32].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The simulation results verified that the combination can improve the coverage.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' An IRS-aided multi-antenna DF relay network was proposed in [36], where three methods, an alternately iterative structure, null-space projection plus maximum ratio combining (MRC) and IRS element selection plus MRC, were put forward to improve the rate performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Obviously, the rate performance was improved by optimizing beamforming at relay and phase shifts at IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, compared with only IRS network, the hybrid network consisting of an IRS and a single-antenna DF relay can achieve the same rate performance with less IRS elements [37].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' However, the above existing research work focused on conventional passive IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Since the received signal via the reflecting channel link experiences large-scale fading twice (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', “double fading” effect), the received signal is weak in fact.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Aiming at eliminating the “double fading” effect, the active IRS with extra power supply emerges, which can reflect and amplify the incident signals for obvious performance ad- vancement.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In [38], the authors proposed the concept of active IRS and came up with a joint transmit and reflect precoding al- gorithm to solve the problem of capacity maximization, which existed in a signal model for active IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It was verified that the proposed active IRS could achieve a noticeable capacity gain compared to the existing passive IRS, which showed that the “double fading” effect could be broken by active IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' With the same overall power budget, a fair performance comparison between active IRS and passive IRS was made theoretically in [39], where it proved that the active IRS surpassed passive IRS in the case of a small or medium number of IRS elements or sufficient power budget.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Accordingly, a novel active IRS- assisted secure wireless transmission was proposed in [40], where the non-convex secrecy rate optimization problem was solved by jointly optimizing the beamformer at transmitter and reflecting coefficient matrix at IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It was demonstrated that with the aid of active IRS, a significantly higher secrecy performance gain could be obtained compared with existing solutions with passive IRS and without IRS design.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Considering that active IRS has the ability to amplify signal, and in order to achieve higher rate performance or save more passive IRS elements of the combination network of IRS and relay, we propose that adding active IRS elements to passive IRS, thereby a combination network of hybrid IRS and relay is generated, which makes full use of the advantages of passive IRS, active IRS and relay to strike a good balance among circuit cost, energy efficiency and rate performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To our best knowledge, it is lack of little research work on the hybrid IRS-aided amplify-and-forward (AF) relay network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In this case, using the criterion of Max SNR, three efficient beamforming methods are proposed to improve the rate perfor- mance of the proposed hybrid IRS-aided AF relay network or dramatically extend its coverage range.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The main contributions of the paper are summarized as follows: 1) To achieve a high rate, a high-performance method based on semidefinite relaxation and fractional programming (HP-SDR-FP) algorithm is presented to jointly optimize the beamforming matrix at AF relay and the reflecting coefficient matrices at IRS by optimizing one and fixing the other two.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' However, it is difficult to directly solve the non-convex optimization problem with fractional and non-concave objective function and non-convex con- straints.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To address this issue, some operations such as vectorization, Kronecker product and Hadamard product are applied to simplify the non-convex optimization problem, then SDR algorithm, Charnes-Cooper trans- formation of FP algorithm and Gaussian randomization method are adopted to obtain the optimization variable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The proposed HP-SDR-FP method can harvest up to 80% rate gain over the passive IRS-aided AF relay network as the number of active IRS elements tends to large.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Additionally, its convergence rate is fast, and its highest order of computational complexity is M 13 and N 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='5 FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2) To reduce the extremely high computational complexity of the proposed HP-SDR-FP method, a low-complexity method based on successive convex approximation and FP (LC-SCA-FP) algorithm is presented.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For the non- convex optimization problem, Dinkelbach’s transforma- tion of FP algorithm is firstly performed to simplify the objective function.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Then by utilizing the first-order Tay- lor approximation of the simplified objective function and relaxing the unit-modulus constraint for passive IRS phase shifts, the non-convex optimization problem is transformed to convex, and can be solved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The proposed LC-SCA-FP method performs much better than passive IRS-aided AF relay network, passive IRS-aided AF relay network with random phase and only AF relay network in terms of rate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Its rate is 60% higher than that of passive IRS-aided AF relay system.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Furthermore, it is convergent, and its highest order of computational complexity is M 6 and N 3 FLOPs, which is much lower than that of HP-SDR-FP method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3 3) To further reduce the computational complexity of the above two methods, a lower-complexity method based on whitening filter, general power iterative algorithm and generalized Rayleigh-Ritz theorem (WF-GPI-GRR) is put forward, where it is assumed that the amplifying coefficient of each active IRS element is equal in the first time slot or the second time slot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To exploit the colored property of noise, whitening filter operation is performed to the received signal.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In line with the transmit power at AF relay and hybrid IRS, the analytical solution of the amplifying coefficient can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, the closed-form expression of beamforming matrix at AF relay is derived by utilizing maximum-ratio combining and maximum-ratio transmission (MRC-MRT) scheme, GPI and GRR are respectively applied to obtain the phase shift matrices at IRS for the first time slot and the second time slot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Compared with passive IRS-aided AF relay network, its rate can be improved by 49%.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Its highest order of computational complexity is M 3 and N 3 FLOPs, which is lower than the above two methods.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The remainder of this paper is organized as follows.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In Section II, a hybrid IRS-aided AF relay network is described.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In Section III, we propose a high-performance method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Section IV describes a a low-complexity method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A lower-complexity method is presented in Section V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' We present our simulation results in Section VI, and draw conclusions in Section VII.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Notation: Scalars, vectors and matrices are respectively represented by letters of lower case, bold lower case, and bold upper case.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (·)∗, (·)T , (·)H, and (·)−1 stand for matrix conju- gate, transpose, conjugate transpose, and inverse, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' E{·}, | · |, ∥ · ∥, tr(·), and arg(·) denote expectation operation, the modulus of a scalar, 2-norm, the trace of a matrix, and the phase of a complex number, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' ⊗ and ⊙ respectively denote Kronecker product and Hadamard product.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The sign IN is the N × N identity matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' II.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' SYSTEM MODEL A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Signal Model Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' System model for a hybrid IRS-aided AF relay wireless network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1 sketches a hybrid IRS-aided AF relay network operated in a time division half-duplex scenario, where source (S) and destination (D) are respectively equipped with a single antenna, a AF relay is with M antennas, and an IRS includes N elements consisting of K active elements and L passive elements, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', N = K + L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The active elements reflect the incident signal by adjusting the amplitude and phase, while the passive elements reflect the incident signal only by shifting the phase.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Let us define EN , EK and EL as the sets of N elements, K active elements and L passive elements, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fur- thermore, EN = EK ∪ EL and EK ∩ EL = ∅.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The reflecting coefficient matrices of EN , EK and EL are respectively denoted by Θ, Φ and Ψ, where Θ = diag(α1, · · · , αN), and the reflecting coefficients of ith element in Θ is expressed by αi = � |βi|ejθi i ∈ EK, (1a) ejθi i ∈ EL, (1b) where |βi| and θi ∈ (0, 2π] are amplifying coefficient and phase shift of the ith element.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For convenience of derivation below, we have the following definitions Θ = Φ + Ψ, Φ = EKΘ, Ψ = EKΘ, (2) where EK + EK = IN and EKEK = 0N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Φ, Ψ, EK and EK are sparse diagonal matrices.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' EK ∈ RN×N and EK ∈ RN×N are respectively depended on the location distribution of K active and L passive elements in the IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In other words, the kth non-zero value of the diagonal corresponding to the kth active element is 1, thus there are K values being 1 and the rest L values being 0 on the diagonal of EK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Additionally, EK is similar to EK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is assumed that the direct channel between S and D is blocked, and the power of signals reflected by the IRS twice or more are such weak that they can be ignored.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the first time slot, the received signal at IRS can be denoted as yr 1i = � Pshsix + n1i, (3) where x and Ps are the transmit signal and power from S, E{xHx} = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' We assume all channels follow Rayleigh fading, hsi ∈ CN×1 is the channel from S to IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' n1i represents the additive white Gaussian noise (AWGN) at IRS with distribution n1i ∼ CN(0, σ2 1iEKIN), which is caused by K active elements.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The received signal at AF relay is given by yr = � Ps(hsr + HirΘ1hsi)x + HirEKΘ1n1i + nr, (4) where hsr ∈ CM×1 and Hir ∈ CM×N are the channels from S to AF relay and IRS to AF relay.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Θ1 = diag(α11, · · · , α1N) and Φ1 = diag(φ11, · · · , φ1N) are the reflecting coeffi- cient matrices of EN and EK in the first time slot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' nr ∼ CN(0, σ2 rIM) is the AWGN at AF relay.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' After performing receive and transmit beamforming, the transmit signal at AF relay can be expressed as yt = Ayr, (5) where A ∈ CM×M is the beamforming matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the second time slot, the received signal at IRS is written by yr 2i = HH iryt + n2i, (6) Hybrid IRS First time slot Active element > Second time slot Passive element H nid H :Hir Hir Destination (S) (D) H nrd AF relay4 SNR = γs|(hH rd + hH idΘ2HH ir)A(hsr + HirΘ1hsi)|2 ∥(hH rd + hH idΘ2HH ir)AHirEKΘ1∥2 + ∥(hH rd + hH idΘ2HH ir)A∥2 + ∥hH idEKΘ2∥2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (10) where HH ir ∈ CN×M is the channel from AF relay to IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' n2i ∼ CN(0, σ2 2iEKIN) is the noise.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The received signal at D is as follows yd = (hH rd + hH idΘ2HH ir)yt + hH idEKΘ2n2i + nd, (7) where hH rd ∈ C1×M and hH id ∈ C1×N are the channels from AF relay to D and IRS to D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Θ2 = diag(α21, · · · , α2N) and Φ2 = diag(φ21, · · · , φ2N) are the reflecting coefficient matri- ces of EN and EK in the second time slot.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' nd ∼ CN(0, σ2 d) is the AWGN at D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Substituting (4) and (5) into (7) yields yd = � Ps(hH rd + hH idΘ2HH ir)A(hsr + HirΘ1hsi)x + (hH rd + hH idΘ2HH ir)A(HirEKΘ1n1i + nr) + hH idEKΘ2n2i + nd.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (8) It is assumed that σ2 1i = σ2 2i = σ2 r = σ2 d = σ2 and γs = Ps σ2 , the achievable system rate can be defined as R = 1 2 log2(1 + SNR), (9) where SNR can be formulated as (10), as shown at the top of next page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Problem Formulation To enhance the system rate performance, it is necessary to maximize system rate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Maximizing rate is equivalent to maximize SNR due to the fact that the log function is a monotone increasing function of SNR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The optimization problem is casted as max Θ1,Θ2,A SNR (11a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' |Θ1(i, i)| = 1, |Θ2(i, i)| = 1, for i ∈ EL, (11b) γs∥EKΘ1hsi∥2 + ∥EKΘ1∥2 F ≤ γi, (11c) γs∥A(hsr + HirΘ1hsi)∥2 + ∥AHirEKΘ1∥2 F + ∥A∥2 F ≤ γr, (11d) γs∥EKΘ2HH irA(hsr + HirΘ1hsi)∥2 + ∥EKΘ2HH irAHirEKΘ1∥2 F + ∥EKΘ2HH irA∥2 F + ∥EKΘ2∥2 F ≤ γi, (11e) where γi = Pi σ2 and γr = Pr σ2 , Pi and Pr respectively denote the transmit power budgets at IRS and AF relay.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Since the IRS is hybrid consisting of active and passive elements, it is difficult to solve the optimization problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To enhance the rate performance, three efficient beamforming methods: 1) HP- SDR-FP;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2) LC-SCA-FP;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' and 3) WF-GPI-GRR, are proposed to optimize AF relay beamforming matrix A, IRS reflecting coefficient matrices Θ1 and Θ2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' III.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' PROPOSED A HIGH-PERFORMANCE SDR-FP-BASED MAX-SNR METHOD In this section, a HP-SDR-FP method is proposed to solve problem (11).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To facilitate processing, problem (11) is de- coupled into three subproblems by optimizing one and fixing the other two.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For each subproblem, we relax it as an SDR problem, and combine Charnes-Cooper transformation of FP algorithm to transform the SDR problem into an semidefinite programming (SDP) problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Furthermore, Gaussian random- ization method is applied to recover the rank-1 solution.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimization of A Given Θ1 and Θ2 Given Θ1 and Θ2, the optimization problem is reduced to max A SNR s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (11d), (11e).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (12) Let us define a = vec(A) ∈ CM2×1, SNR can be translated to SNR = γsaHB1a aH(B2 + B3)a + ∥hH idEKΘ2∥2 + 1, (13) where B1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] ⊗ [(hH rd + hH idΘ2HH ir)H(hH rd + hH idΘ2HH ir)], (14a) B2 = [(HirEKΘ1)∗(HirEKΘ1)T ] ⊗ [(hH rd + hH idΘ2HH ir)H(hH rd + hH idΘ2HH ir)], (14b) B3 = IM ⊗ [(hH rd + hH idΘ2HH ir)H(hH rd + hH idΘ2HH ir)].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (14c) In the same manner, the constraints (11d) and (11e) can be respectively converted to aH(γsC1 + C2 + IM2)a ≤ γr, (15a) aH(γsD1 + D2 + D3)a + ∥EKΘ2∥2 F ≤ γi, (15b) where C1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] ⊗ IM, (16a) C2 = [(HirEKΘ1)∗(HirEKΘ1)T ] ⊗ IM, (16b) D1 = [(hsr + HirΘ1hsi)∗(hsr + HirΘ1hsi)T ] ⊗ [(EKΘ2HH ir)H(EKΘ2HH ir)], (16c) D2 = [(HirEKΘ1)∗(HirEKΘ1)T ] ⊗ [(EKΘ2HH ir)H(EKΘ2HH ir)], (16d) D3 = IM ⊗ [(EKΘ2HH ir)H(EKΘ2HH ir)].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (16e) Let us define �A = aaH ∈ CM2×M2, in accordance with the rank inequality: rank P ≤ min{m, n}, where P ∈ Cm×n, we 5 can get rank(�A) ≤ rank(a) = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The optimization problem can be recast as max �A γstr(B1�A) tr{(B2 + B3)�A} + ∥hH idEKΘ2∥2 + 1 (17a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' tr{(γsC1 + C2 + IM2)�A} ≤ γr, (17b) tr{(γsD1 + D2 + D3)�A} + ∥EKΘ2∥2 F ≤ γi, (17c) �A ⪰ 0, rank(�A) = 1, (17d) which is a non-convex problem because of rank-one constraint.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' After removing rank(�A) = 1 constraint, we have the SDR problem of (17) as follows max �A γstr(B1�A) tr{(B2 + B3)�A} + ∥hH idEKΘ2∥2 + 1 (18a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (17b), (17c), �A ⪰ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (18b) The objective function (18a) is a linear fractional function with respect to �A, which is a quasi-convex function with the denom- inator > 0, so problem (18) is a quasi-convex problem with convex constraints.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is necessary to apply Charnes-Cooper transformation, which helps convert the optimization problem from quasi-convex to convex.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Introducing a slack variable m and defining m = (tr{(B2 + B3)�A} + ∥hH idEKΘ2∥2 + 1)−1, the above problem (18) is further rewritten as follows max �A,m γstr{B1�A} (19a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' tr{(γsC1 + C2 + IM2)�A} ≤ mγr, (19b) tr{(γsD1 + D2 + D3)�A} + m∥EKΘ2∥2 F ≤ mγi, (19c) tr{(B2 + B3)�A} + m∥hH idEKΘ2∥2 + m = 1, (19d) �A ⪰ 0, m > 0, (19e) where �A = m�A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Clearly, the above optimization problem has become a SDP problem, which is directly solved by CVX.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The solution to problem (18) is �A = �A/m.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' However, the rank-one constraint rank(�A) = 1 is not considered in the SDR problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Since the obtained solution �A is not generally rank- one matrix, the Gaussian randomization method is applied to achieve a rank-one solution �A, thereby, AF relay beamforming matrix A is achieved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimization of Θ1 Given A and Θ2 Given that A and Θ2 are fixed, the optimization problem can be represented by as follows max Θ1 γs|hH rid(hsr + HirΘ1hsi)|2 ∥hH ridHirEKΘ1∥2 + ∥hH rid∥2 + ∥hH idEKΘ2∥2 + 1 (20a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' |Θ1(i, i)| = 1, for i ∈ EL, (20b) (11c), (11d), (11e), (20c) where hrid = [(hH rd + hH idΘ2HH ir)A]H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In order to further simplify the objective function and constraints of the optimization problem, let us define u1 = [α11, · · · , α1N]T , we have hsr + HirΘ1hsi = Hsirv1 and hH ridHirEKΘ1 = uT 1 diag{hH ridHirEK}, where v1 = [u1;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1] and Hsir = [Hirdiag{hsi}, hsr].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Substituting these for- mulas into (20a), and due to ∥uT 1 diag{hH ridHirEK}∥2 = ∥diag{hH ridHirEK}u1∥2, the object function can be further rewritten as vH 1 F1v1 vH 1 F2v1 , (21) where F1 = γsHH sirhridhH ridHsir and F2 is written as (22) at the top of next page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The constraint (20b) for passive elements EL can be rewritten as |v1(i)|2 = 1, for i ∈ EL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (23) Obviously, ∥EKΘ1∥2 F = ∥EKu1∥2, and the constraint (11c) can be translated to vH 1 G1v1 ≤ γi, (24) where G1 = � γsdiag{hH si}EKdiag{hsi} + EK 0N×1 01×N 0 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (25) Then for constraint (11d),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' according to the property of Hadamard product: tr(X(Y ⊙ Z)) = tr((X ⊙ YT )Z),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' where X ∈ Cm×n,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Y ∈ Cn×m and Z ∈ Cn×m,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' we have ∥AHirEKΘ1∥2 F = ∥AHirEKdiag{u1}∥2 F = tr{EKHH irAHAHirEKdiag{u1}diag{uH 1 }} = tr{EKHH irAHAHir[EK ⊙ (u1uH 1 )]} = uH 1 [(EKHH irAHAHir) ⊙ EK]u1 = uH 1 [(HH irAHAHir) ⊙ EK]u1 (26) Inserting hsr + HirΘ1hsi = Hsirv1 and (26) back into the constraint (11d),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' which can be rewritten as vH 1 G2v1 ≤ γr,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (27) where G2 =γsHH sirAHAHsir + � (HH irAHAHir) ⊙ EK 0N×1 01×N ∥A∥2 F � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (28) Similarly, (11e) can be written in the following form vH 1 G3v1 ≤ γi, (29) where G3 is written as (30), as shown at the top of the page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Substituting the simplified objective function and constraints into (20), the optimization problem can be equivalently trans- formed into max v1 (21) (31a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (23), (24), (27), (29), v1(N + 1) = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (31b) Aiming at further transforming the optimization problem, and defining V1 = v1vH 1 , problem (31) can be equivalently given by max V1 tr(F1V1) tr(F2V1) (32a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' V1(i, i) = 1, for i ∈ EL, (32b) V1(N + 1, N + 1) = 1, (32c) tr(G1V1) ≤ γi, tr(G2V1) ≤ γr, (32d) tr(G3V1) ≤ γi, rank(V1) = 1, V1 ⪰ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (32e) 6 F2 = � diag{EKHH irhrid}diag{hH ridHirEK} 0N×1 01×N ∥hH rid∥2 + ∥hH idEKΘ2∥2 + 1 � , (22) G3 =γsHH sirAHHirΘH 2 EKΘ2HH irAHsir + � (HH irAHHirΘH 2 EKΘ2HH irAHir) ⊙ EK 0N×1 01×N ∥EKΘ2HH irA∥2 F + ∥EKΘ2∥2 F � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (30) Due to the fact that the object function is quasi-convex and constraint rank(V1) = 1 is non-convex, (32) is still a non-convex problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Relaxing the rank-1 constraint, the problem is transformed into a SDR problem, which can also be solved by applying Charnes-Cooper transformation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, introducing a slack variable τ, then defining τ = tr(F2V1)−1 and �V1 = τV1, the SDR problem of (32) can be translated to a SDP problem, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', max �V1,τ tr(F1�V1) (33a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' �V1(i, i) = τ, for i ∈ EL, (33b) �V1(N + 1, N + 1) = τ, τ > 0, (33c) tr(G1�V1) ≤ τγi, tr(G2�V1) ≤ τγr, (33d) tr(G3�V1) ≤ τγi, tr(F2�V1) = 1, �V1 ⪰ 0, (33e) which can be directly solved by CVX, thereby the solution V1 of SDR problem of (32) is achieved, and Gaussian randomiza- tion method is used to recover a rank-one solution V1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Then the solution v1 is extracted from the eigenvalue decomposition of V1, subsequently, IRS reflecting coefficient matrix Θ1 can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimization of Θ2 Given A and Θ1 In the subsection, defining u2 = [α21, · · · , α2N]H, we have hH rd +hH idΘ2HH ir = vH 2 Hrid and Θ2HH irA(hsr +HirΘ1hsi) = diag{HH irA(hsr + HirΘ1hsi)}u∗ 2, where v2 = [u2;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1] and Hrid = [diag{hH id}HH ir;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' hH rd].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Similarly, when A and Θ1 are fixed, the SDP problem to optimize �V2 can be expressed as max �V2,ρ tr(H1�V2) (34a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' �V2(i, i) = ρ, for i ∈ EL, (34b) �V2(N + 1, N + 1) = ρ, ρ > 0, (34c) tr(J�V2) ≤ ργi, tr(H2�V2) = 1, �V2 ⪰ 0, (34d) where ρ = tr(H2v2vH 2 )−1 is a slack variable, �V2 = ρv2vH 2 , H1 = γsHridA(hsr + HirΘ1hsi)[HridA(hsr + HirΘ1hsi)]H, H2 =HridA(HirEKΘ1ΘH 1 EKHH ir + IM)AHHH rid + � diag{hH idEK}diag{EKhid} 0N×1 01×N 1 � , (35) and J is written as (36) at the top of next page, where H3 = EKdiag{HT irA∗(hsr + HirΘ1hsi)∗} and H4 = HH irAHirEKΘ1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is observed that (34) is similar to (33), thus (34) can be solved in the same way as (33).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Finally the solutions v2 and Θ2 are obtained, and the details are omitted here for brevity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Overall Algorithm and Complexity Analysis Since the objective function of problem (11) is non- decreasing and the transmit powers of S, AF relay and IRS active elements are limited, the objective function has an upper bound.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, the convergence of the proposed HP- SDR-FP algorithm can be guaranteed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Our idea is alternative iteration, that is, the alternative iteration process are performed among A, Θ1 and Θ2 until the convergence criterion is satisfied, while the system rate is maximum.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The proposed HP-SDR-FP method is summarized in Algorithm 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Algorithm 1 Proposed HP-SDR-FP Method 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Initialize A0, Θ0 1 and Θ0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' According to (9), R0 can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' set the convergence error δ and the iteration number t = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given Θt 1 and Θt 2, solve problem (19) for �A t+1, recover rank-1 solution �A t+1 via Gaussian randomization, obtain At+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given At+1 and Θt 2, solve problem (33) for �V t+1 1 , recover rank-1 solution Vt+1 1 via Gaussian randomization, obtain Θt+1 1 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given At+1 and Θt+1 1 , solve problem (34) for �V t+1 2 , recover rank-1 solution Vt+1 2 via Gaussian randomization, obtain Θt+1 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Calculate Rt+1 by using At+1, Θt+1 1 and Θt+1 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update t = t + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until ��Rt+1 − Rt�� ≤ δ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' After that, the complexity of Algorithm 1 is calculated and analyzed according to problems (19), (33) and (34).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Problem (19) has 4 linear constraints with dimension 1, one linear matrix inequality (LMI) constraint of size M 2 and M 4+1 decision variables.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Hence, the computational complex- ity of problem (19) is denoted as O{nA √ M 2 + 4(M 6 + 4 + nA(M 4 + 4) + n2 A)ln(1/ε)} float-point operations (FLOPs), where nA = M 4 + 1 and ε represents the computation accuracy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For problem (33), there exit L + 6 linear constraints with dimension 1, one LMI constraint of size N + 1 and (N +1)2+1 decision variables, so the computational complex- ity of problem (33) is written as O{nV1 √ N + L + 7((N + 7 J = � γsHH 3 H3 + (H4HH 4 + HH irAAHHir + IN) ⊙ EK 0N×1 01×N 0 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (36) 1)3 + L + 6 + nV1((N + 1)2 + L + 6) + n2 V1)ln(1/ε)} FLOPs, where nV1 = (N + 1)2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For problem (34), there are L + 4 linear constraints with dimension 1, one LMI constraint of size N + 1 and (N + 1)2 + 1 decision variables.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Thus, the computational complexity of problem (34) is expressed as O{nV2 √ N + L + 5((N + 1)3 + L + 4 + nV2((N + 1)2 + L + 4) + n2 V2)ln(1/ε)} FLOPs, where nV2 = (N + 1)2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, the total computational complexity of Algorithm 1 is written by O{D1[nA � M 2 + 4(M 6 + 4 + nA(M 4 + 4) + n2 A) + nV1 √ N + L + 7((N + 1)3 + L + 6 + nV1((N + 1)2 + L + 6) + n2 V1) + nV2 √ N + L + 5((N + 1)3 + L + 4 + nV2((N + 1)2 + L + 4) + n2 V2)]ln(1/ε)} (37) FLOPs, where D1 is the maximum number of alternating iterations needed for convergence in Algorithm 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is obvious that the highest order of computational complexity is M 13 and N 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='5 FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' IV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' PROPOSED A LOW-COMPLEXITY SCA-FP-BASED MAX-SNR METHOD In the previous section, HP-SDR-FP method is proposed to obtain AF relay beamforming matrix A, IRS reflecting coefficient matrices Θ1 and Θ2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' However, its computational complexity is very high because of SDR algorithm with lots of FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' To reduce the high computational complexity of HP- SDR-FP method, a low-complexity SCA-FP-based Max-SNR method is proposed in this section.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize A With Fixed Θ1 and Θ2 For given Θ1 and Θ2, the optimization problem based on (13) is given by max a γsaHB1a aH(B2 + B3)a + ∥hH idEKΘ2∥2 + 1 (38a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (15a), (15b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (38b) Observing the above objective function, it is seen that (38) is also a fractional optimization problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the subsection, Dinkelbachs transformation is introduced to solve problem (38).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Here, introducing a slack variables µ, the problem (38) is reformulated as max a,µ γsaHB1a − µ[aH(B2 + B3)a + ∥hH idEKΘ2∥2 + 1] (39a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (15a), (15b), (39b) where µ is iteratively updated by µ(t + 1) = γsaH(t)B1a(t) aH(t)(B2 + B3)a(t) + ∥hH idEKΘ2∥2 + 1, (40) where t is the iteration number.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' µ is nondecreasing after each iteration, which guarantees the convergence of the objective function (39a).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Note that the above problem is still non- convex due to the first term of the objective function is non- concave, which can be solved by using SCA method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' We approximate the first term by using a linear function, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', its first-order Taylor expansion at feasible vector �a, which is γsaHB1a ≥ 2γsℜ{aHB1�a} − γs�aHB1�a, where �a is the solution of previous iteration.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Inserting the low bound of γsaHB1a back into problem (39) yields max a 2γsℜ{aHB1�a} − γs�aHB1�a − µ[aH(B2 + B3)a + ∥hH idEKΘ2∥2 + 1] (41a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (15a), (15b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (41b) It is known that the above optimization problem consists of a concave objective function and several convex constraints.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, problem (41) is a convex optimization problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' When �a and µ are fixed, a can be directly achieved by CVX.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Correspondingly, A can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize Θ1 With Fixed A and Θ2 It is assumed that AF relay beamforming matrix A and Θ2 are given.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The constraint (11b) can be re-expressed as |u1(i)|2 = 1, for i ∈ EL, (42) which can be relaxed as uH 1 (i)u1(i) ≤ 1, for i ∈ EL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (43) Problem (11) with respect to u1 can be rearranged as max u1 γs|hH 1 u1 + a|2 ∥diag{hH ridHirEK}u1∥2 + b (44a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' uH 1 (i)u1(i) ≤ 1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' for i ∈ EL,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (44b) γs∥EKdiag{hsi}u1∥2 + ∥EKu1∥2 ≤ γi,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (44c) γs∥Ahsr + P1u1∥2 + ∥AHirEKdiag{u1}∥2 F + ∥A∥2 F ≤ γr,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (44d) γs∥h2 + P2u1∥2 + ∥P3EKdiag{u1}∥2 F ≤ �γi,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (44e) where h1 = [(hH rd + hH idΘ2HH ir)AHirdiag{hsi}]H,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45a) h2 = EKΘ2HH irAhsr,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' P1 = AHirdiag{hsi},' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45b) P2 = EKΘ2HH irAHirdiag{hsi},' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45c) P3 = EKΘ2HH irAHir,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' a = (hH rd + hH idΘ2HH ir)Ahsr,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45d) b = ∥(hH rd + hH idΘ2HH ir)A∥2 + ∥hH idEKΘ2∥2 + 1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45e) �γi = γi − ∥EKΘ2HH irA∥2 F − ∥EKΘ2∥2 F .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (45f) 8 Problem (44) can be further converted to max u1 γs|hH 1 u1 + a|2 ∥diag{hH ridHirEK}u1∥2 + b (46a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' uH 1 (i)u1(i) ≤ 1, for i ∈ EL, (46b) uH 1 (γsdiag{hH si}EKdiag{hsi} + EK)u1 ≤ γi, (46c) uH 1 [γsPH 1 P1 + (HH irAHAHir) ⊙ EK]u1 + ∥A∥2 F + 2γsℜ{uH 1 PH 1 Ahsr} + γshH srAHAhsr ≤ γr, (46d) uH 1 [γsPH 2 P2 + (PH 3 P3) ⊙ EK]u1 + 2γsℜ{uH 1 PH 2 h2} + γshH 2 h2 ≤ �γi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (46e) In the same manner, Dinkelbach’s transformation is also introduced to problem (46).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Problem (46) can be rewritten as max u1 γs|hH 1 u1 + a|2 − ωb − ωuH 1 diag{EKHH irhrid}diag{hH ridHirEK}u1 (47a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (46b), (46c), (46d), (46e), (47b) where ω is a variable scalar, which is defined as ω(t + 1) = γs|hH 1 u1(t) + a|2 ∥diag{hH ridHirEK}u1(t)∥2 + b.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (48) Similarly, aiming at converting the objective function (47a) to convex, the first-order Taylor expansion at the point �u1 is employed to γs|hH 1 u1 + a|2 and transform it into the linear function, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', |hH 1 u1 + a|2 ≥ 2ℜ{uH 1 h1(hH 1 �u1 + a)} + a∗a − �uH 1 h1hH 1 �u1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Inserting the low bound of ��hH 1 u1 + a ��2 back into problem (47) yields the following optimization problem max u1 2γsℜ{uH 1 h1(hH 1 �u1 + a)} + γsa∗a − γs�uH 1 h1hH 1 �u1− ω(b + uH 1 diag{EKHH irhrid}diag{hH ridHirEK}u1) (49a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (46b), (46c), (46d), (46e), (49b) where the object function is concave and the constraints are convex, thus problem (49) is convex.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For a given feasible vector �u1 and ω, problem (49) can be solved by CVX directly, thereby u1 is achieved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize Θ2 With Fixed A and Θ1 Similarly, given AF relay beamforming matrix A and Θ1, the optimization problem with respect to u2 is modeled as max u2 2γsℜ{uH 2 h3(hH 3 �u2 + c∗)} + γscc∗ − γs�uH 2 h3hH 3 �u2 − λ(uH 2 Q1QH 1 u2 + 2ℜ{uH 2 Q1h4} + hH 4 h4) − λ(uH 2 Q2QH 2 u2 + 2ℜ{uH 2 Q2AHhrd}) − λhH rdAAHhrd − λuH 2 Q3QH 3 u2 − λ (50a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' uH 2 (i)u2(i) ≤ 1, for i ∈ EL, (50b) uH 2 [γsHH 3 H3 + (H4HH 4 + HH irAAHHir + IN) ⊙ EK]u2 ≤ γi, (50c) where λ is a variable, �u2 is a feasible vector, and h3 = diag{hH id}HH irA(hsr + HirΘ1hsi), (51a) h4 = (hH rdAHirEKΘ1)H, (51b) Q1 = diag{hH id}HH irAHirEKΘ1, (51c) Q2 = diag{hH id}HH irA, Q3 = diag{hH idEK}, (51d) c = hH rdA(hsr + HirΘ1hsi), (51e) λ(t + 1) = γs|uH 2 (t)h3 + c|2 ∥uH 2 (t)Q1 + hH 4 ∥2 + ∥uH 2 (t)Q2 + hH rdA∥2 + ∥uH 2 (t)Q3∥2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (51f) It is clear that problem (50) is a convex optimization problem with concave objective function and convex constraints.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given �u2 and λ, u2 can be effectively obtained by CVX.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Overall Algorithm and Complexity Analysis In the same manner, the proposed LC-SCA-FP method is convergent with an upper bound.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The alternate iteration idea is roughly as follows: for given Θ1 and Θ2, first- order Taylor expansion is applied in problem (39), AF relay beamforming vector a can be calculated by solving problem (41) iteratively;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' similarly, for given A and Θ2, reflecting coefficient vector u1 can be obtained by solving problem (49) iteratively;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' for given A and Θ1, reflecting coefficient vector u2 can be achieved by solving problem (50) iteratively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Then the alternative iteration process are operated among A, Θ1 and Θ2 until the convergence criterion is satisfied, while the system rate is maximum.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The proposed LC-SCA-FP method is summarized in Algorithm 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Furthermore, we calculate and analyze the complexity of Algorithm 2 in accordance with problems (41), (49) and (50).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is observed that problem (41) consists of one SOC constraint of dimension M 2 and one SOC constraint of dimension M 2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The number of decision variables na = M 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The computational complexity corresponding to problem (41) is represented as O{2na(M 4+(M 2+1)2+n2 a)ln(1/ε)} FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Problem (49) includes L SOC constraints of dimension 1, one SOC constraint of dimension N, one SOC constraint of dimension N +1 and one SOC constraint of dimension N +2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The number of decision variables nu1 = N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The computa- tional complexity corresponding to problem (49) is written as O{nu1 √ 2L + 6(L+N 2+(N +1)2+(N +2)2+n2 u1)ln(1/ε)} FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Problem (50) is composed of L SOC constraints of dimension 1 and one SOC constraint of dimension N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The number of decision variables nu2 = N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The computational complexity corresponding to problem (50) is expressed as O{nu2 √2L + 2(L+N 2+n2 u2)ln(1/ε)} FLOPs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Consequently, the total computational complexity of Algorithm 2 is denoted as O{D2[2na(M 4 + (M 2 + 1)2 + n2 a) + nu1 √ 2L + 6 (L + N 2 + (N + 1)2 + (N + 2)2 + n2 u1) + nu2 √ 2L + 2(L + N 2 + n2 u2)]ln(1/ε)} (52) FLOPs, where D2 is the maximum number of alternating iterations to obtain a, u1 and u2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For Algorithm 2, its highest 9 Algorithm 2 Proposed LC-SCA-FP Method 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Initialize A0, Θ0 1 and Θ0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' According to (9), R0 can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' set the convergence error δ and the iteration number t = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix Θt 1 and Θt 2, initialize �a0, set δ and t1 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update solution at1+1 with (�at1, µt1) by solving problem (41), t1 = t1 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Set �at1+1 = at1+1 and update µt1+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until (41a) converges, update at+1 = at1+1 and obtain At+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix At+1 and Θt 2, initialize �u0 1, set δ and t2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update solution ut2+1 1 with (�ut2 1 , wt2) by solving problem (49), t2 = t2 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Set �ut2+1 1 = ut2+1 1 and update wt2+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 13.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until (49a) converges, update ut+1 1 = ut2+1 1 and obtain Θt+1 1 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 14.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix At+1 and Θt+1 1 , initialize �u0 2, set δ and t3 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 15.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 16.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update solution ut3+1 2 with (�ut3 2 , λt3) by solving problem (50), t3 = t3 + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 17.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Set �ut3+1 2 = ut3+1 2 and update λt3+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 18.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until (50a) converges, update ut+1 2 = ut3+1 2 and obtain Θt+1 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 19.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Calculate R by using At+1, Θt+1 1 and Θt+1 2 , t = t+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 20.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until ��Rt+1 − Rt�� ≤ δ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' order of computational complexity is M 6 and N 3 FLOPS, which is greatly reduced compared to the complexity of HP- SDR-FP method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' PROPOSED A LOWER-COMPLEXITY WF-GPI-GRR-BASED MAX-SNR METHOD In what follows, to further reduce the computational com- plexity, a lower-complexity WF-GPI-GRR-based Max-SNR method is put forward.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For gaining rate enhancement, we ap- ply WF operation to exploit the colored property of noise and present the related system model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Here, active IRS reflecting coefficient matrix is split into amplifying coefficient and IRS phase-shift matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The details of derivation on the amplifying coefficients, AF relay beamforming matrix and IRS phase-shift matrices are described as below.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' System Model For brevity, it is assumed that the amplifying coefficients of each IRS active element in the first time slot and the second time slot are |β1| and |β2|, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Let us define Ψ1 = EK �Θ1, Φ1 = |β1|EK �Θ1, (53a) Ψ2 = EK �Θ2, Φ2 = |β2|EK �Θ2, (53b) where the phase-shift matrix �Θ1 = diag(ejθ1i, · · · , ejθ1N ), �Θ2 = diag(ejθ2i, · · · , ejθ2N), | �Θ1(i, i)| = 1 and | �Θ2(i, i)| = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Thus we have Θ1 = (EK + |β1|EK) �Θ1, Θ2 = (EK + |β2|EK) �Θ2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (54) In the first time slot, the received signal at AF relay can be redescribed as yr = � Ps[hsr + Hir(EK + |β1|EK) �Θ1hsi]x + (|β1|HirEK �Θ1n1i + nr) � �� � n1r .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (55) As matter of fact, n1r is color, not white.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is necessary for us to whiten the color noise n1r by using covariance matrix Cn.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The covariance W1r of n1r is given by W1r = β2 1∥HirEK �Θ1∥2 F σ2 + σ2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (56) While n1i and nr are the independent and identically dis- tributed random vectors, n1r has a mean vector of all-zeros and covariance matrix C1r = β2 1σ2HirEK �Θ1 �ΘH 1 EKHH ir + σ2IM, (57) where obviously C1r is a positive definite matrix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Defining the WF matrix W1r with W1rWH 1r = C−1 1r , which yields W1r = C − 1 2 1r = (Q1rΛ1rQH 1r)− 1 2 = Q1rΛ − 1 2 1r QH 1r, (58) where Q1r is an unitary matrix, and Λ1r is a diagonal matrix consisting of eigenvalues.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Performing the WF operation to (55) yields yr = � PsW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]x + W1r(|β1|HirEK �Θ1n1i + nr) � �� � n1r , (59) where n1r is the standard white noise with covariance matrix IM.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The transmit signal at AF relay is yt = Ayr.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the second time slot, the received signal at D is denoted as yd = � Ps[hH rd + hH id(EK + |β2|EK) �Θ2HH ir]AW1r [hsr + Hir(EK + |β1|EK) �Θ1hsi]x + [hH rd + hH id(EK + |β2|EK) �Θ2HH ir]An1r + |β2|hH idEK �Θ2n2i + nd.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (60) The corresponding SNR can be represented as (61), as shown at the top of next page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is assumed that the power budgets Ps, Pr and Pi are respectively fully used to transmit signals at S, AF relay and IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, the optimization problem can be converted to max |β1|,|β2|, � Θ1, � Θ2,A (61) (62a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' | �Θ1(i, i)| = 1, | �Θ2(i, i)| = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (62b) It is necessary to solve the above problem for optimal |β1|, |β2|, �Θ1, �Θ2 and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 10 SNR = γs|[hH rd + hH id(EK + |β2|EK) �Θ2HH ir]AW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]|2 β2 1∥[hH rd + hH id(EK + |β2|EK) �Θ2HH ir]AW1rHirEK �Θ1∥2 + ∥[hH rd + hH id(EK + |β2|EK) �Θ2HH ir]AW1r∥2 + β2 2∥hH idEK �Θ2∥2 + 1 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (61) B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Solve |β1| and |β2| In the first time slot, the reflected signal at IRS is written by yt 1i = � PsΘ1hsix + Φ1n1i, = � PsEK �Θ1hsix � �� � ypt 1i + � Ps|β1|EK �Θ1hsix + |β1|EK �Θ1n1i � �� � yat 1i , (63) where ypt 1i and yat 1i are respectively the signals reflected by passive elements EL and active elements EK.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Additionally, the power consumed by the active elements is Pi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' We have Pi = Psβ2 1∥EK �Θ1hsi∥2 + β2 1∥EK �Θ1∥2 F σ2 1i = β2 1Ps K � k=1 |ejθ1khk si|2 + β2 1 K � k=1 |ejθ1k|2σ2 1i = β2 1Ps K � k=1 |hk si|2 + Kβ2 1σ2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (64) where θ1k is the phase shift of the kth IRS active element in the first time slot,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' hk si is the channel between S and the kth IRS active element and follows Rayleigh distribution with the expression hk si = � PLk sigk sie−jϕsk,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' where PLk si,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' gk si and ϕsk denote the path loss,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' the channel gain and the channel phase from S to the kth IRS active element,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' |gk si|2 follows Exponential distribution [41], and the corresponding probability density function is given by f|gk si|2(x) = \uf8f1 \uf8f2 \uf8f3 1 λsi e− x λsi x ∈ [0, +∞), (65a) 0 otherwise, (65b) where λsi is the Exponential distribution parameter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Let us define PLk si is equal to the path loss from S to IRS (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', PLsi).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Using the weak law of large numbers, (64) can be further written as Pi = β2 1Ps K � k=1 | � PLsigk sie−jϕsk|2 + Kβ2 1σ2 = β2 1PsPLsi K � k=1 |gk si|2 + Kβ2 1σ2 ≈ Kβ2 1PsPLsi · E(|gk si|2) + Kβ2 1σ2 = Kβ2 1PsPLsiλsi + Kβ2 1σ2, (66) β1 can be achieved as |β1| = � Pi KPsPLsiλsi + Kσ2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (67) Similarly, the received signal of the kth active IRS element in the second time slot is yrk 2i = hH rkAyr + n2i,k = hH rkyt + n2i,k, (68) where hH rk ∈ C1×M represents the channel between AF relay and the kth active IRS element, hH rk = [ � PL1k ri g1k ri e−jϕ1k, · · · , � PLMk ri gMk ri e−jϕMk], (69) where PLmk ri , gmk ri and ϕmk are the path loss, the channel gain and the channel phase between the mth antenna at AF relay and the kth active IRS element.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Defining PLmk ri = PLri, PLri is the path loss from AF relay to IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The reflected signal of the kth active IRS element is ytk 2i = |β2|ejθ2khH rkyt + |β2|ejθ2kn2i,k = |β2||hH rk||yt|ej(θ2k+ϕrkt) + |β2|ejθ2kn2i,k, (70) where θ2k is the phase shift of the kth IRS active element in the second time slot, ϕrkt is the phase of hH rkyt.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is assumed that the transmit power of AF relay is Pr, the corresponding power of the reflected signal of the kth active IRS element is P tk 2i = β2 2|hH rk|2|yt|2 + β2 2σ2 2i,k = β2 2PrPLri M � m=1 |gmk ri |2 + β2 2σ2 K = Mβ2 2PrPLriλri + β2 2σ2 K , (71) where σ2 2i,k = σ2 2i/K = σ2/K, λri is the Exponential distribution parameter of channel from AF relay to IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Thus the power of the reflected signal of K active IRS elements is Pi = K � k=1 P tk 2i = KMβ2 2PrPLriλri + β2 2σ2, (72) which yields |β2| = � Pi KMPrPLriλri + σ2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (73) C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize A Given �Θ1 and �Θ2 Aiming at maximizing the received signal power, MRC- MRT method are applied to solve A as follows A = A [hrd + Hir �ΘH 2 (EK + |β2|EK)hid] ∥hH rd + hH id(EK + |β2|EK) �Θ2HH ir∥ [hsr + Hir(EK + |β1|EK) �Θ1hsi]HWH 1r ∥W1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]∥ = AΥ, (74) where A is the amplify factor of AF relay.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Since the transmit power of AF relay is Pr, we have A as shown in (75) at the top of next page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Inserting A back into (74), A can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 11 A = � γr γs∥ΥW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]∥2 + β2 1∥ΥW1rHirEK �Θ1∥2 F + ∥ΥW1r∥2 F , (75) �F2 = � β2 1diag{EKHH ir�hrid}diag{�h H ridHirEK} 0N×1 01×N ∥�h H rid∥2 + β2 2∥hH idEK �Θ2∥2 + 1 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (77) D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize �Θ1 Given A and �Θ2 By defining �u1 = [ejθ1i, · · · , ejθ1N ]T , �v1 = [�u1;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1] and �Hsir = [Hir(EK + |β1|EK)diag{hsi}, hsr].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given A and �Θ2, the optimization problem is equivalent to max �v1 �vH 1 �F1�v1 �vH 1 �F2�v1 (76a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' |�v1(i)| = 1, ∀i = 1, 2, · · · , N, (76b) �v1(N + 1) = 1, (76c) where �F1 and �F2 are Hermitian matrices, and �F2 is positive semi-definite.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' �F1 = γs �H H sir�hrid�h H rid �Hsir, �hrid = [(hH rd + hH id(EK +|β2|EK) �Θ2HH ir)AW1r]H, and �F2 is denoted as (77) at the top of next page.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The above problem can be relaxed to max �v1 �vH 1 �F1�v1 �vH 1 �F2�v1 s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' ∥�v1∥2 = N + 1, (78) which can be constructed as max �v1 �vH 1 �F1�v1 �vH 1 �F2�v1 �vH 1 IN+1�v1 �vH 1 IN+1�v1 s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' ∥�v1∥2 = N + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (79) �v1 can be solved by using GPI algorithm, the details of GPI procedure is presented in Algorithm 3, where we define Ω(�vt 1) = (�vH 1 �F1�v1)IN+1 + (�vH 1 IN+1�v1)�F1 and Ξ1(�vt 1) = (�vH 1 �F2�v1)IN+1 + (�vH 1 IN+1�v1)�F2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Algorithm 3 GPI Algorithm to Compute Phase-Shift Vector �v1 with Given A and �Θ2 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Given A and �Θ2, and initialize �v0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Set the tolerance factor ξ and the iteration number t = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Compute the function matrix Ω(�vt 1) and Ξ1(�vt 1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Calculate yt = Ξ1(�vt 1)†Ω(�vt 1)�vt 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update �vt+1 1 = yt ∥yt∥.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update t = t + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until ∥�vt+1 1 − �vt 1∥ ≤ ξ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Optimize �Θ2 Given A and �Θ1 If A and �Θ1 are fixed, let us define �u2 = [ejθ2i, · · · , ejθ2N ]H, �v2 = [�u2;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1], �Hrid = [diag{hH id(EK + |β2|EK)}HH ir;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' hH rd].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Accordingly, the optimization problem is reduced to max �v2 �vH 2 �H1�v2 �vH 2 �H2�v2 (80a) s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' |�v2(i)| = 1, ∀i = 1, 2, · · · , N, (80b) �v2(N + 1) = 1, (80c) where �H1 and �H2 are Hermitian matrices, and �H2 is positive definite.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' �H1 = γs �HridAW1r[hsr +Hir(EK +|β1|EK) �Θ1hsi]· {�HridAW1r[hsr + Hir(EK + |β1|EK) �Θ1hsi]}H, and �H2 = �HridAW1r(β2 1HirEK �Θ1 �ΘH 1 EKHH ir + IM)WH 1rAH· �H H rid + � β2 2diag{hH idEK}diag{EKhid} 0N×1 01×N 1 � .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' (81) We have the following relaxed transformation max �v2 �vH 2 �H1�v2 �vH 2 �H2�v2 s.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='t.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' �vH 2 �v2 = 1 (82) where �v2 = �v2 √N+1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, in line with the GRR theorem, the optimal �v2 is obtained as the eigenvector corresponding to the largest eigenvalue of �H −1 2 �H1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Thereby �v2 and �Θ2 is achieved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Overall Algorithm and Complexity Analysis The proposed lower-complexity WF-GPI-GRR method is summarized in Algorithm 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The main idea consists of two parts: the amplifying coefficient of active element and the iterative idea.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The analytic solutions of amplifying coefficients of IRS active elements in the first time slot and the second time slot, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', β1 and β2, are determined by the transmit power of S, AF relay, IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Furthermore, β1 and β2 are denoted as (67) and (73).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The iterative idea can be described as follows: for given �Θ1 and �Θ2, the closed-form expression of A are represented as (74) by utilizing MRC-MRT;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' for given A and �Θ2, GPI is applied to achieve �Θ1;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' for given A and �Θ1, �Θ2 is obtained in a closed-form expression by using GRR theorem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The alternative iteration process are performed among A, �Θ1 and �Θ2 until the stop criterion is satisfied, while the system rate is maximum.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In the following, the total computational complexity of Algorithm 4 is calculated as O{D3(N 3 + 4M 3 + 4M 2N + 2MN 2 + 2M 2K+ 8M 2 + 6N 2 + 9MN + 5MK + 5M + 11N+ 3 + D4(7N 3 + 27N 2 + 43N + 18))} (83) 12 Algorithm 4 Proposed WF-GPI-GRR Method 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Calculate β1 and β2 through (67) and (73).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Initialize A0, �Θ0 1 and �Θ0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' According to (9) and (61), R0 can be obtained.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' set the convergence error δ and the iteration number t = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' repeat 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix �Θt 1 and �Θt 2, compute At+1 through (74).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix At+1 and �Θt 2, solve problem (79) to achieve �vt+1 1 based on GPI presented in Algorithm 3, �Θt+1 1 = diag{�vt+1 1 (1 : N)}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fix At+1 and �Θt+1 1 , solve problem (82) to achieve �vt+1 2 based on GRR theorem, �Θt+1 2 = diag{�vt+1 2 (1 : N)}.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update Rt+1 by using β1, β2, At+1, �Θt+1 1 and �Θt+1 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Update t = t + 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' until ��Rt+1 − Rt�� ≤ δ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' FLOPs, where D3 is the maximum number of alternating iterations for Algorithm 4 and D4 is the number of iteration in GPI algorithm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Its highest order of computational complexity is M 3 and N 3 FLOPs, which is lower than the complexity of Algorithm 1 and Algorithm 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' VI.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' SIMULATION AND NUMERICAL RESULTS In this section, in order to evaluate the rate performance among the proposed three methods, numerical simulations are performed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, it is assumed that S, D, hybrid IRS and AF relay are located in three-dimensional (3D) space, the related coordinate simulation setup is shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2, where S, D, hybrid IRS and AF relay are located at (0, 0, 0), (0, 100, 0), (−10, 50, 20) and (10, 50, 10) in meter (m), respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The path loss is modeled as PL(d) = PL0 − 10αlog10( d d0 ), where PL0 = −30dB is the path loss at the reference distance d0 = 1m, d is the distance between transmitter and receiver, and α is the path loss exponent, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Here, the path loss exponents of each channel link associated with IRS, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=', S-IRS, IRS-AF relay and IRS-D, are set as 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='0, and those of S-AF relay and AF relay-D links are considered as 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The remaining system parameters are set as follow: σ2 = −80dBm and EK is randomly generated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Simulation setup.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Additionally, to demonstrate the proposed three methods, the following three benchmark schemes are taken into account.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 1) AF relay+passive IRS: A passive IRS-aided AF relay network is considered, where IRS only reflects the signal without amplifying the reflected signal, and the reflecting coefficient of each IRS element is set as 1;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2) AF relay+passive IRS with random phase: With ran- dom phase of each reflection element uniformly and indepen- dently generated from the interval (0, 2π], the beamforming matrix A at AF relay is optimized.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3) Only AF relay: A AF relay network without IRS is considered, while the AF relay beamforming matrix A can be achieved by MRC-MRT, which is given by A = � Pr Ps∥Γhsr∥2+σ2∥Γ∥2 F Γ, where Γ = hrdhH sr ∥hH rd∥∥hsr∥.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Towards a fair comparison between a hybrid IRS-aided AF relay wireless network and the above three benchmark schemes, let us define that the total transmit power budgets of S and AF relay in the three benchmark schemes are the same as that of S, AF relay and IRS in the hybrid IRS-aided AF relay network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For instance, the AF relay transmit power budget PR in the three benchmark schemes is equal to Pi+Pr.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 4 5 6 7 8 9 10 11 12 log2N 105 1010 1015 1020 1025 1030 Computational Complexity (FLOPs) Proposed HP-SDR-FP Proposed LC-SCA-FP Proposed WF-GPI-GRR Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Computational complexity versus N with (M, K, D1, D2, D3, D4) = (2, 4, 6, 10, 5, 2).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 3 plots the computational complexity of the proposed three methods.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' By suppressing ln(1/ε) [42], the computational complexities of the proposed three methods, 1) HP-SDR- FP;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 2) LC-SCA-FP;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' and 3) WF-GPI-GRR, increase as N increases.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is clear that the first method has the highest computational complexity, which is much higher than those of the other two methods.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' In addition, the third method has the lowest computational complexity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 4 demonstrates the proposed three methods are con- vergent under different Ps, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Obviously, for Ps = 10dBm, the proposed HP-SDR-FP, LC-SCA-FP and WF-GPI- GRR methods require about only four iterations to achieve the rate ceil.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' While for Ps = 30dBm, it takes ten iterations for the proposed three methods to converge to the rate ceil.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' From the above two cases, we conclude that the proposed three methods are feasible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 5 shows the achievable rate versus Ps with (M, N, K) = (2, 32, 4).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It can be seen that the proposed HP-SDR- FP, LC-SCA-FP and WF-GPI-GRR methods with (Pi, Pr) = (30dBm, 30dBm) perform better than AF relay+passive IRS, Hybrid IRS (-10, 50, 20) y AF relay (10, 50, 10) S (0, 0, 0) (0, 100, 0) X13 0 3 6 9 12 15 18 Number of iterations 4 5 6 7 8 9 10 Achivable Rate(bits/s/Hz) Proposed HP-SDR-FP Proposed LC-SCA-FP Proposed WF-GPI-GRR 30dBm 10dBm Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Convergence of proposed methods with (M, N, K, Pi, Pr) = (2, 32, 4, 30dBm, 30dBm).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 0 5 10 15 20 25 30 Ps (dBm) 0 1 2 3 4 5 6 7 8 9 Achivable Rate (bits/s/Hz) Proposed HP-SDR-FP Proposed LC-SCA-FP Proposed WF-GPI-GRR AF relay+passive IRS AF relay+passive IRS with random phase Only AF relay Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Achievable rate versus Ps with (M, N, K) = (2, 32, 4).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' AF relay+passive IRS with random phase and only AF relay with PR = 33dBm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Furthermore, the rate performance of LC- SCA-FP method is the most closest to that of HP-SDR-FP method in the low and medium power Ps region.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For instance, when power Ps is equal to 15dBm, the rate performance gaps between the method LC-SCA-FP, the worst method WF-GPI- GRR and the best method HP-SDR-FP method are respectively 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='037bits/s/Hz and 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='245bits/s/Hz.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 6 illustrates the achievable rate versus Pi with (M, N, K, Ps) = (2, 32, 4, 30dBm).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' It is particularly noted that the proposed three methods with Pr = 30dBm make a better rate performance improvement than that of AF re- lay+passive IRS, AF relay+passive IRS with random phase and only AF relay with PR = Pi + Pr.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For example, when Pi equals 40dBm, the proposed worst method, WF-GPI-GRR method, can harvest up to 49.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='8% rate gain over AF re- lay+passive IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' The best method HP-SDR-FP approximately has a 53.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='3% rate gain over AF relay+passive IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' This shows that as Pi increases, significant rate gains are achieved for the proposed hybrid IRS-aided AF relay wireless network.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Moreover, the rate performance of LC-SCA-FP is getting closer to that of HP-SDR-FP, and the gap between LC-SCA- FP and WF-GPI-GRR becomes smaller.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 10 15 20 25 30 35 40 Pi (dBm) 3 4 5 6 7 8 9 Achivable Rate (bits/s/Hz) Proposed HP-SDR-FP Proposed LC-SCA-FP Proposed WF-GPI-GRR AF relay+passive IRS AF relay+passive IRS with random phase Only AF relay Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Achievable rate versus P i with (M, N, K, Ps) = (2, 32, 4, 30dBm).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 0 1 2 3 4 5 log2K 4 5 6 7 8 9 10 Achivable Rate(bits/s/Hz) Proposed HP-SDR-FP Proposed LC-SCA-FP Proposed WF-GPI-GRR AF relay+passive IRS AF relay+passive IRS with random phase Only AF relay Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Achievable rate versus K with (M, N, Ps) = (2, 32, 30dBm).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7 presents the achievable rate versus the number of active IRS elements K with (M, N, Ps) = (2, 32, 30dBm) for the proposed three methods with (Pi, Pr) = (30dBm, 30dBm) and the three benchmark schemes with PR = 33dBm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' From Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' 7, it can be observed that as the number of active IRS elements K increases, the rate gains of the proposed three methods over AF relay+passive IRS, AF relay+passive IRS with random phase and only AF relay increase gradually and become more significant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Meanwhile, the proposed three methods have the following increasing order on rate: HP- SDR-FP, LC-SCA-FP and WF-GPI-GRR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Compared with the benchmark scheme of AF relay+passive IRS, our proposed three methods perform much better, which shows that the optimization of beamforming is important and efficient.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' VII.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' CONCLUSIONS In this paper, we have made an investigation of beamform- ing methods of optimizing the beamforming matrix at AF relay and reflecting coefficient matrices at IRS in a hybrid IRS-aided AF relay network, where the hybrid IRS includes few active elements amplifying and reflecting the incident signal.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' By using the criterion of Max SNR, three schemes, namely HP-SDR-FP, LC-SCA-FP and WF-GPI-GRR, have 14 been proposed to improve the rate performance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Simulation results show that the proposed three methods can make a dramatic rate enhancement compared to AF relay+passive IRS, AF relay+passive IRS with random phase and only AF relay, which verifies the active IRS elements can break the “double fading” effect caused by conventional passive IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' For instance, an approximate 50.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content='0% rate gain over the three benchmark schemes can be achieved in the high power budget region of hybrid IRS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' Therefore, a hybrid IRS-aided AF relay network can provide an enhancement in accordance with rate performance and extended coverage for the mobile communications.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' REFERENCES [1] D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/8dE1T4oBgHgl3EQfCAI3/content/2301.02858v1.pdf'} +page_content=' C.' metadata={'source': 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The Science Education +of Preservice Elementary Teachers +CATHERINE RIEGLE-CRUMB,1 KARISMA MORTON,1 CHELSEA MOORE,2 +ANTONIA CHIMONIDOU,3 CYNTHIA LABRAKE,4 SACHA KOPP5 +1Department of Curriculum and Instruction, STEM Education, University of Texas at +Austin; 2Department of Psychology, University of Massachusetts, Amherst; 3UTeach +Primary, College of Natural Sciences, University of Texas at Austin; 4Department of +Chemistry, University of Texas at Austin; and 5College of Arts and Sciences, SUNY +Stonybrook +Received 26 June 2014; revised 27 February 2015; accepted 30 March 2015 +DOI 10.1002/sce.21177 +Published online 14 July 2015 in Wiley Online Library (wileyonlinelibrary.com). +ABSTRACT: Owing to their potential impact on students’ cognitive and noncognitive +outcomes, the negative attitudes toward science held by many elementary teachers are a +critical issue that needs to be addressed. This study focuses on the science education of +preservice elementary teachers with the goal of improving their attitudes before they begin +their professional lives as classroom teachers. Specifically, this study builds on a small +body of research to examine whether exposure to inquiry-based science content courses +that actively involve students in the collaborative process of learning and discovery can +promote a positive change in attitudes toward science across several different dimensions. +To examine this issue, surveys and administrative data were collected from over 200 students +enrolled in the Hands on Science (HoS) program for preservice teachers at the University +of Texas at Austin, as well as more than 200 students in a comparison group enrolled +in traditional lecture-style classes. Quantitative analyses reveal that after participating in +HoS courses, preservice teachers significantly increased their scores on scales measuring +confidence, enjoyment, anxiety, and perceptions of relevance, while those in the comparison +group experienced a decline in favorable attitudes to science. These patterns offer empirical +support for the attitudinal benefits of inquiry-based instruction and have implications for +the future learning opportunities available to students at all education levels. +C⃝ 2015 +Wiley Periodicals, Inc. Sci Ed 99:819–836, 2015 +Correspondence to: Dr. Catherine Riegle-Crumb; e-mail: riegle@austin.utexas.edu +C⃝ 2015 Wiley Periodicals, Inc. + +820 +RIEGLE-CRUMB ET AL. +INTRODUCTION +While the metaphor of science, technology, engineering, and mathematics (STEM) as a +pipeline has been rightly criticized as too simplistic, it is nevertheless clear that students’ +early experiences in science classrooms shape their future achievement and interests (Xie & +Shauman, 2003). With the goal of better understanding and ultimately improving elemen- +tary science education in the United States, researchers and policymakers have increased +their attention toward teachers. A growing body of research now focuses on the science +content knowledge of elementary science teachers, as the subject matter expertise that +they possess has clear implications for what students learn (Diamond, Maerten-Rivera, +Rohrer, & Lee, 2014; Heller, Daehler, Wong, Shinohara, & Miratrix, 2012; Kanter & Kon- +stantopoulus, 2010; Sadler, Sonnert, Coyle, Cook-Smith, & Miller, 2013). Compared to +secondary teachers, elementary teachers are much more likely to be trained as generalists +and consequently less likely to have extensive content knowledge, and this pattern appears +particularly pronounced for science (Haefner & Zembal-Saul, 2004). Clearly there are con- +tinued concerns about the need for teacher training programs and professional development +to focus on increasing subject matter expertise. +Yet content knowledge is a necessary but insufficient characteristic of a successful teacher. +Teachers’ attitudes about the content they teach is another critical factor that has implications +for classroom learning, and importantly, negative attitudes can exist independent of content- +area expertise (Beilock, Gunderson, Ramirez, & Levine, 2010; Tosun, 2000). While there +is comparatively less research on elementary teachers’ attitudes toward science than math +(Bursal & Paznokas, 2006), there is nevertheless evidence that many elementary teachers +are not favorably inclined toward science. Such negative attitudes on the part of teachers can +impact their students’ attitudes toward science and can inhibit students’ learning (Beilock +et al., 2010; Jarrett, 1999; Ramey-Gassert, Shroyer, & Staver, 1996), creating a vicious +cycle that must be interrupted. However, effectively changing how teachers view science is +a challenging task (Mulholland & Wallace, 1996; Palmer, 2002). +The goal of this study is to examine whether inquiry-based science content classes might +function to help break this cycle by improving preservice teachers’ attitudes at a critical +juncture before they begin their professional lives as classroom teachers. While there is +much research on the positive impact of inquiry on outcomes for K–12 students (Borman, +Gamoran, & Bowdon, 2008; Diamond et al., 2014; National Research Council, 2012b), we +build on a smaller body of qualitative research regarding the benefits of inquiry instruction +in college for preservice elementary teachers (Mulholland & Wallace, 1996; Palmer, 2002). +Specifically, we suggest that students can become empowered and enthusiastic about the +domain of science through active involvement in the process of inquiry, defined as engaging +in the pursuit of scientific questions via data collection, experimentation, exploration, and +discussion (National Research Council, 2000). +To examine this issue, we collected data from the hands-on science (HoS) undergraduate +program at the University of Texas at Austin (Ludwig et al., 2013) to determine whether +exposure to these inquiry-based science content courses promoted a change in the science +attitudes of a sample of over 200 preservice elementary teachers. In exploring preservice +teachers’ attitudes, we go beyond the typical singular focus of much research on self- +efficacy to instead consider personal attitudes toward science across several dimensions +(van Aalderen-Smeets, Walma van der Molen, & Asma, 2012). Additionally, to ensure +the robustness of our results, our design utilizes a comparison group of noneducation and +nonscience majors enrolled in more traditional lecture-based science courses; our analyses +also account for students’ social and academic background. Our study offers promising +evidence that science content classes in college can be a positive vehicle for changing the +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +821 +attitudes of future elementary teachers, and subsequently has potential implications for +the opportunities to learn both cognitive and noncognitive skills that are offered to future +generations of elementary science students. +LITERATURE REVIEW +Framework: Considering Attitudes Across Multiple Dimensions +When exploring attitudes toward science, it is critical to recognize multiple relevant +dimensions. Based on a comprehensive review of prior research on teacher attitudes, and +motivated by the lack of substantive clarity and empirical transparency of most prior +research, van Aalderen-Smeets et al. (2012) recently advanced a new theoretical framework +to provide a cohesive model that captures primary teachers’ attitudes toward science. +Specifically, they developed a tripartite model of primary teachers’ attitudes toward science +that distinguishes between three overarching dimensions, each of which is composed of +different elements: (1) perceived control (which includes elements such as self-efficacy), (2) +affective states (which includes enjoyment and anxiety), and (3) cognitive beliefs (such as +perceived relevance). This framework is informed by earlier theoretical models of attitudes +(Eagly & Chaiken, 1993), but departs from prior models by considering perceived control +(e.g., self-efficacy) as a core dimension, and furthermore defining behavioral intentions +as a consequence rather than a component of science attitudes. Their model also calls for +researchers to make a clear distinction regarding whether the focus is on teachers’ personal +attitudes toward science or their professional attitudes toward teaching science, as studies +that combine teachers’ views of science as a domain with their views on science instruction +in their own classroom into one empirical scale blur the object of teachers’ attitudes, making +substantive interpretation difficult. +The three dimensions of attitudes (whether personal or professional) advanced by van +Aalderen-Smeets et al. (2012) are logically related to one another. For example, Bursal and +Paznokas(2006) found that teachers with higher levels of self-efficacy had lower anxiety, +a finding supported by several other studies (Bleicher, 2007; Palmer, 2002). Yet while +related, they nevertheless capture somewhat distinct thoughts and beliefs. For instance, an +individual might expect to master an activity or believe that it is useful, but nevertheless +find it is unappealing (e.g., flossing their teeth) or even anxietyproducing (e.g., running 10 +miles). Therefore, considering elements of all three dimensions is critical to developing a +comprehensive picture of teachers’ attitudes toward science. +Yet most of the literature about the attitudes of elementary science teachers (either +preservice or in-service) focuses on their perceived control in the form of self-efficacy, +as there is relatively scant research on either the cognitive beliefs or affective attitudes +of teachers (van Aalderen-Smeets et al., 2012). Thus, a key contribution of our study is +our consideration of elements of all three dimensions of attitude to more fully capture the +complexity of preservice teachers’ attitudes toward science.1 Below we discuss the prior +literature on the science attitudes of preservice elementary teachers in more detail, including +how such attitudes may influence the outcomes of future students. Because our research +questions and subsequent empirical analyses focus on preservice teachers well before they +1In this paper, we address all three dimensions of van Aalderen-Smeets et al.’s (2012) theoretical model, +but do not discuss (or model) every element within each dimension. For example, while the authors include +context dependency as an element that falls under the dimension of perceived control, we do not address this +here as it refers to the support that practicing teachers receive from their administrators and therefore is not +particularly relevant for a study concerning the personal (rather than professional) attitudes of preservice +teachers. +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +822 +RIEGLE-CRUMB ET AL. +actually enter the elementary classroom, we concentrate on literature on personal attitudes +toward science. We then turn to a discussion of why inquiry-based science content classes +for preservice teachers have the potential to increase individuals’ attitudes across all three +dimensions. +Perceived Control: Considering Self-Efficacy. +A key element of the attitudinal dimen- +sion of perceived control is self-efficacy, which according to Bandura’s (1977, 1982) +foundational work is defined as an individual’s belief that she can successfully master a +situation or deal with an obstacle that arises. An individual’s self-efficacy has logical im- +plications for her subsequent behaviors and choices, as she is likely to attempt to avoid +those situations or activities where she does not feel she can be efficacious, and persist +where she feels confident that she can be successful. While research has demonstrated +that in-service elementary teachers exhibit low levels of efficacy in their science teaching +(see, for example,Atwater, Gardner, & Kight, 1991; Harlen, 1997; Ramey-Gassert et al., +1996), not surprisingly this pattern is also evident among preservice teachers, who feel less +efficacious about their own ability to learn science. For example, Skamp (1991) determined +that less than half of the preservice elementary teachers in his study reported having even +a fair amount of confidence in their science ability. Similarly, Bleicher’s (2007) study of +preservice elementary teachers found that participants in a science methods class exhibited +low scores on science self-efficacy scales. Low efficacy is often attributed to prior negative +educational experiences in science. For example, in a study of five preservice teachers, +Mulholland and Wallace (1996) found that their respondents reported very little confidence +in their own science abilities and attributed this to negative experiences in their own science +schooling as children. +Affective States: Considering Enjoyment and Anxiety. +Individuals’ affect toward a +domain represents another attitudinal dimension. As articulated by van Aalderen-Smeets +et al. (2012), the dimension of affect can be further categorized into the positive element +of enjoyment and the negative element of anxiety. Beginning with the former, Liang and +Gabel (2005) found that most preservice elementary teachers in their study reported that +science had never been enjoyable for them. These teachers also indicated that they took +science courses only because it was required for their degree program. Smith (2000) and +Howes (2002) found similar results. Additionally, the preservice participants in all of these +studies attributed their low levels of enjoyment to negative experiences in either (or both) +their high school and college science courses, a point to which we will return to later. +Anxiety captures the negative aspect of the affective dimension. Early research by Mallow +(1981; also Mallow & Greenburg, 1983) as well as Westerback (1984) define science anxiety +as the fear, worry, or apprehension that some individuals experience when presented with +the task of learning science. While research on the math anxiety of preservice teachers is +extensive (Udo, Ramsey, & Mallow, 2004), and research considering both math anxiety and +science anxiety find a strong association between the two (Cady & Rearden, 2007), there is +comparatively little research focusing specifically on science anxiety (Bursal & Paznokas, +2006). Yet several studies do provide evidence that preservice elementary teachers report +relatively high levels of science anxiety about teaching science, as well as more generalized +anxiety about learning science themselves (Cady & Rearden, 2007; Udo et al., 2004; +Westerback & Long, 1990). +Cognitive Beliefs: Considering the Relevance of Science. +Finally, we discuss research +on preservice elementary teachers’ beliefs in the relevance of science, a critical element +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +823 +of the attitudinal dimension of cognitive beliefs. The limited extant research on this topic +focuses on perceptions of science as useful or relevant for society and for them personally, +and finds that preservice elementary teachers report generally favorable views. Specifically, +in a study of 200 preservice teachers, Coulson (1992) used a survey instrument that in- +cluded a personal usefulness science scale and found that on average, respondents indicated +moderate levels of agreement. Cobern and Loving’s (2002) study at a large Midwestern +university also found that on Likert scales measuring the perceived importance of science +to all citizens, preservice elementary teachers on average agreed with this sentiment. These +findings echo the sentiments of the general population, which generally regard science and +technology as useful for making their lives better (Evans & Durant, 1995; Kohut, Keeter, +Doherty, & Dimock, 2009). Therefore among the three attitudinal dimensions discussed, +promoting preservice teachers’ views of the relevance of science is perhaps somewhat less +of a pressing problem than promoting both their perceived control in the form of science +efficacy and their affective attitudes of enjoyment and anxiety. +Examining the Impact of Teacher Attitudes +There is a logical connection between teachers’ attitudes toward a subject and student +outcomes, both in terms of impacting students’ opportunities to learn science and their own +developing attitudes. First, research indicates that the negative attitudes toward science held +by many elementary teachers are likely to result in less coverage of science content and +less engaging and effective instruction. Teachers who are not confident in their own science +knowledge are likely to worry that they cannot effectively answer students’ questions nor +keep them engaged with interesting activities (Jarrett, 1999). Consequently, elementary +teachers who feel less efficacious and more anxious are likely to try to avoid teaching +science and spend less time teaching when they cannot avoid it altogether (Brownlow, +Jacobi, & Rogers, 2000; Pine et al., 2006; Ramey-Gassert et al., 1996). Appleton and Kindt +(1999) also found evidence that avoidance occurred when teachers did not find science to +be as relevant as other subjects such as English or math. One such teacher reported that “If +you’re running out of time in the week, you think ‘Oh I just won’t worry about that science +activity’” (p. 162). +When teachers do teach science, their negative attitudes can impact their pedagogical +practices and subsequently their capacity to reach and engage students. Appleton and +Kindt’s (1999) study of in-service elementary teachers found that those exhibiting low +confidence were less likely to engage their students in hands-on learning. Ramey-Gassert +et al. (1996) found that elementary teachers with low science self-efficacy had a minimal +desire to engage in professional development activities that could improve their teaching of +science. Lack of belief in the usefulness or relevance of science could also logically result +in a reduced effort to provide engaging instruction to students. +Additionally, the negative attitudes toward science held by many elementary teachers can +result in the socialization of students toward a negative stance toward science. As students +look to their teachers as role models and authorities, they begin to mimic and potentially +internalize such attitudes as their own (Jussim & Eccles, 1992; McKown & Weinstein, +2002). This can lead to a vicious cycle where negative attitudes such as anxiety and low +efficacy are passed from teachers to their students, and therefore from one generation +to the next. For example, Beilock et al. (2010) found that elementary teachers’ math +anxiety influenced students’ own attitudes toward math, with girls in particular more likely +to evidence declining math attitudes and increasingly gender-stereotyped views of math +over the course of the year. This particular study highlights additional concerns regarding +gender rolemodeling; as most elementary teachers are female, and a substantial number +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +824 +RIEGLE-CRUMB ET AL. +of them exhibit negative attitudes toward science (as well as math), this could be a strong +conduit through which young girls begin to believe that these subjects are less interesting, +less important, and overall less-suited for them. Furthermore, as students’ own attitudes +decline, so does their engagement and motivation to learn, which further impacts their +achievement (Eccles, 1994). +In sum, the research literature provides compelling evidence that teachers’ negative +attitudes can impact students’ learning and attitudinal outcomes, and as such are a critical +issue that needs to be addressed. To effectively break this cycle, necessitates intervening +to change teachers’ attitudes before they enter the classroom. In short, the education of +preservice teachers is an ideal place to focus. +Educating Preservice Teachers: Inquiry as a Tool for Improving +Attitudes +As mentioned earlier, the negative attitudes of preservice elementary teachers can at +least in part be traced back to their own negative experiences with science classes in high +school and in college. For example, Liang and Gabel (2005) found that preservice teachers +attributed their lack of enjoyment of science to their prior experiences in classes dominated +by lectures that necessitated copious amounts of note-taking and memorization. Similarly, +Smith (2000) reports that preservice elementary teachers in his study often complained +about the boredom of their procedure-based high school and college science courses. +Simply put, many preservice teachers have had little exposure to inquiry-based science +instruction in their lives as students. We posit that exposure while in college to pedagogy +that actively involves them in the process of scientific discovery can ultimately help them to +see that science is meaningful, interesting, and accessible, thereby changing their attitudes +toward science. +Several studies support the supposition that inquiry classes can promote such changes, +in spite of the possibility of some initial student frustration with an approach that deviates +from teachers’ didactic presentations of the “right” answer (Volkmann, Abell, & Zgagacz, +2005). For example, in a qualitative study of preservice teachers at a large university in +the southwest, Kelly (2000) found that after completing an active, inquiry-based science +methods course, most participants reported that their interest in science had increased. +Kelly (2000) attributes this shift to the use of hands-on explorations and discussions where +students came to embody the process of scientific inquiry by formulating and exploring +ideas. Similarly, in a study of preservice elementary teachers, Palmer (2002) interviewed +four participants who reported that their attitudes toward science had changed from negative +to positive due to the excitement of inquiry-based lessons. A study of five teachers by +Mulholland and Wallace (1996) reported similar results. Finally, in a quantitative study +of 112 preservice elementary teachers, Jarrett (1999) found that an inquiry-based science +methods class increased the participants’ personal interest in science. The author attributed +this change to preservice teachers becoming active agents in the classroom and learning to +view science as a process of discovery. Thus, a small body of research finds that inquiry- +based pedagogy in science educational methods courses can have a positive impact on +preservice elementary teachers’ attitudes. +CURRENT STUDY +Building on the insights of this prior research, we posit that required science content +courses could also represent a powerful venue for change for college students at the +beginning stages of preparing for their careers as future teachers. Specifically, the purpose +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +825 +of this study is to examine whether inquiry-based science content courses promote a change +in attitudes toward science among preservice elementary teachers. The courses are part of +the HoS undergraduate program, developed at The University of Texas at Austin in the +College of Natural Sciences, with cooperation from the College of Education. HoS is +required of all students in the elementary education program and covers four semesters of +science courses with a curriculum that is composed heavily of the topics that preservice +teachers will be expected to teach their students once they become teachers (Ludwig et al., +2013). The design of the HoS program is based on the Physics and Everyday Thinking +(Goldberg, 2008) framework that centers around the development of students’ physical +science understandings through experimentation and follows the example of work from +Western Washington University extending this framework to other disciplines (Nelson, +2008). The curriculum is based upon big ideas in science, with specific emphasis on the +themes of Matter and Energy, which are integrated across different science disciplines. The +course sequence focuses on physics in Semester 1, chemistry and geology in Semester 2, +biological systems in Semester 3, and astronomy and earth science in Semester 4. +HoS classes were designed to utilize the essential elements of inquiry-based learning +as defined by the influential National Research Council report on inquiry (Forbes, 2011; +National Research Council, 2000); specifically, students engage in scientifically oriented +questions by collecting, organizing, and analyzing data. From that data they formulate +explanations, connect them to scientific knowledge, and subsequently evaluate their expla- +nations in contrast to alternative explanations. Additionally, students share and justify those +explanations with others. +The HoS program is best categorized as teacher-directed or guided inquiry (Cuevas, Lee, +Hart, & Deaktor, 2005; National Research Council, 2000; Volkmann et al., 2005). Initial +questions are posed by the instructor and all activities are carefully designed to present +opportunities for students to confront misconceptions, with both topics and skills developed +in a structured progression. The instructor does not lecture but probes student knowledge and +offers helpful nudges in the right direction, working with students both in small groups and +via whole class discussions to construct knowledge and develop explanations (Volkmann +et al., 2005). Finally, consistent with inquiry approaches to learning, the course emphasizes +big ideas in science while engaging students in hands-on learning and constant exploration +and discussion while in groups with their peers (National Research Council, 2000, 2012b). +An example of a typical 2-hour class session is a lesson on sound that begins with the +following teacher-generated questions: How does sound travel through a room? How does +sound travel from your classmate to you? Students then work in groups of three or four to +answer these questions and discuss their initial ideas or preconceptions; they subsequently +share their ideas with the entire class, so that there is a collective knowledge of alternative +ways of thinking about how sound travels. Working in their small groups, students then +engage in a series of experiments, using an “airzooka” and candles, a string telephone, and +a loudspeaker, that require that they gather data and then generate models based on these +data. They are regularly prompted by the instructor to make predictions and connect trends +to other previously seen concepts. Finally, students reflect and summarize key ideas and +connect them to other contexts by using evidence-based reasoning from the data collected +in their experiments. These questions are the basis for whole-class discussions, where +students present and justify their ideas to their peers. Students typically end lessons by +writing a scientific narrative summarizing how their thinking was revised from their initial +ideas, drawing on evidence gained through the experiments and whole class sharing and +discussion. For example, a student might share how her initial idea that “sound travels as a +wave” has become more sophisticated, discussing the role of vibrations and the transfer of +mechanical energy from the source to the receiver. +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +826 +RIEGLE-CRUMB ET AL. +Our examination of whether the inquiry-based science content courses of the HoS pro- +gram promote a change in attitudes toward science among preservice elementary teachers is +described in detail below. Here, we briefly note that our study contributes to the literature a +rigorous quantitative examination of change in attitudes across multiple dimensions among +preservice elementary teachers, utilizing a comparison group of students in more traditional +science content courses, as well as accounting for differences among students in academic +and social background characteristics that may have implications for their attitudes. +Data and Method +Analytic Sample. +Our analytic sample includes 238 preservice elementary teachers who +enrolled in the HoS program between Fall 2010 and Spring 2012. Students completed +presurveys prior to the start of the first course and postsurveys at the end of the second +course in the sequence.2 Surveys were done online, and were administered during class +by members of the research team. Additionally, our sample includes a comparison group +composed of 263 nonscience and noneducation majors enrolled in traditional lecture-style +undergraduate science courses in Spring 2012. While our design falls shorts of a pure +treatment versus control comparison, we chose courses that represent what our sample of +preservice elementary teachers would have been required to take in the absence of the +HoS program. Therefore, our comparison group includes students who were enrolled in +either an introductory-level chemistry or biology class. These students were surveyed at +the beginning and end of the semester. As the time period between pre- and postsurveys +is longer for HoS students than for non-HoS students, we discuss the implications and +limitations of this comparison later. +Administrative records were linked to student surveys, allowing us to examine the demo- +graphic and academic background information of students in our sample and to consider +how HoS students differed from those in the comparison group. Not surprisingly given the +gender composition of the elementary teacher population nationwide, HoS students were +overwhelmingly female (95%), compared to 65% of our comparison sample of nonedu- +cation and nonscience majors. There were no statistically significant differences between +the two groups of students by mother’s education; for race/ethnicity, there were signifi- +cantly fewer students who identified as American Indian among HoS students compared +to non-HoS students. Regarding academic background prior to college entry, HoS students +had lower SAT math scores than their fellow students taking typical science classes by +more than one-third of a standard deviation (see Table 1). To ensure that any differences +observed between the two groups in their changes in attitudes over time are not confounded +by differences in their background characteristics, our subsequent multivariate models will +control for all of these factors.3 +Student Attitude Surveys. +The pre- and postsurveys administered to both groups con- +sisted of 21 items geared toward assessing student attitudes toward science. To examine +multiple dimensions of attitudes, we selected items from preexisting surveys to measure +2At the time of this study, students were only required to take the first two semesters of the total four +semester sequence. +3Mother’s education level is an ordinal variable with the following categories: (1) did not attend high +school, (2) attended high school but did not graduate, (3) high school diploma or GED, (4) some college, (5) +earned associate’s degree, (6) bachelor’s degree, (7) graduate or professional degree. Math SAT score and +mother’s education level were imputed for those students who had missing values. We utilized information +on gender, race, high school rank, family income, and father’s education to conduct single imputation using +Stata. Analyses using list-wise deletion produced similar results. +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +827 +TABLE 1 +Descriptive Statistics +Hands-on Science +(HoS) Students +Non-HoS Students +N = 238 +N = 263 +Gender +Female*** +94.5% +65.4% +Race/ethnicity +White (non-Hispanic) +63.4% +60.1% +Black +2.9% +3.4% +Hispanic +21% +19% +Asian +11.3% +14.4% +American Indian** +0.4% +2.7% +Native Hawaiian/Pacific Islander +0.8% +0.4% +Other background characteristics +Mean +SD +Mean +SD +SAT math score*** +574.87 +75.60 +607.62 +73.39 +Mother’s educational level +5.10 +1.60 +5.07 +1.69 +***p < .001, **p < .01, *p < .05, p < .10. +confidence (an element of perceived control)4, enjoyment and anxiety (positive and neg- +ative elements of affective states), and relevance (a key element of cognitive beliefs). To +measure anxiety, we used the Math Anxiety Rating Scale (Hopko, 2003) and substituted +the word science for all references to math. To measure all other attitudes, we selected +items developed by the National Center for Education Statistics (www.nces.ed.gov), and +used in national surveys, including the Educational Longitudinal Study, the High School +Longitudinal Study, and the U.S. component of the Trends in International Mathematics +and Science Study. Principal component analyses with promax rotation using the complete +set of 21 survey items revealed four factors with Eigenvalues greater than one. We sub- +sequently created separate scales (described below) composed of the individual items that +loaded onto each of the four factors. The scales clearly corresponded to the elements of +confidence, enjoyment, anxiety, and relevance; using the full sample, the Cronbach’s alpha +for each scale was .8 or higher.5 +The confidence scale is composed of four items that gauge students’ level of confidence +when engaging in scientific activities. The items were as follows: “I have always done well +in science,” “Science is not one of my strengths” (reverse coded), “I am confident that I can +understand the most difficult material presented in my science textbooks,” and “Science +4Because the questions ask students to reflect more on their assessment of their current success in science, +we refer to this scale as measuring confidence rather than self-efficacy for future success. However, prior +research has consistently noted a very strong correspondence between indicators of self-confidence and +self-efficacy (Wigfield & Eccles, 2000). +5To further test the reliability of the four scales, we calculated Cronbach’s alphas separately for (a) +treatment and reference groups; (b) first year cohort and second year cohorts (for treatment group), and +(c) survey responses at time 1 and time 2 (for different cohorts and for different treatment groups). In all, +we calculated alpha reliabilities for each of our four scales for 15 different subsamples with remarkably +consistent results ranging from a low of .77 to a high of .88. (exploratory factor analyses using each of +these groups also yielded the same four factor model). +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +828 +RIEGLE-CRUMB ET AL. +has always been one of my best subjects.” The five items in the enjoyment scale capture +students’ level of positive affect for science and included “I enjoy learning science,” “I look +forward to going to science courses,” “Science is fun,” “I like science,” and “Science is +boring” (reversecoded for inclusion in the scale). Categories of response were the same as +those for the confidence scale. +For each of the eight items in the anxiety scale, students were asked to indicate how +much the situation made them feel anxious or worried. Similar to the other measures, the +responses ranged from (1) not at all anxious to (5) very much anxious or worried. The items +included “Looking through the pages in a science text,” “Thinking about an upcoming +science test one day before the test,” “Reading and interpreting a scientific graph, chart, or +illustration,” “Taking an exam in a science course,” “Watching and listening to a teacher +explaining a scientific concept or phenomena,” “Waiting to get a science test returned in +which you expected to do well,” “Walking on campus and thinking about a science course,” +and “Being given a ‘pop’ quiz in science class.” +Finally, the four items making up the relevance scale include questions that focused +on students’ perception of the meaning or usefulness of science in their daily lives. The +items are as follows: “The subject of science is not very relevant to most people,” “It is not +important for most people to understand science,” “I think learning science will help me in +my daily life,” and “Science is important to me personally.” Students indicated the extent to +which they agreed or disagreed with the statements with possible responses ranging from +strongly agree (1) to strongly disagree (5). +ANALYSES AND RESULTS +To examine whether inquiry-based science content courses promote a positive change +in attitudes toward science for preservice elementary teachers, we begin by comparing the +means on the pre- and postmeasures of our four attitudinal scales for HoS students. Results +of paired t-tests indicate a statistically significant improvement over time for each scale. +Specifically, for confidence, the mean increased from 2.61 to 2.98 (p < .001), reflecting +a 0.37 point increase or almost half of a standard deviation change from pre to post. HoS +students’ science enjoyment increased by about a fourth of point (and about a third of a +standard deviation), from the presurvey mean of 3.24 to a postsurvey mean of 3.51 (p < +.001). The largest change was observed for the anxiety scale, where the average decreased +(meaning that students became less anxious over time) from a presurvey mean of 3.11 to a +postsurvey mean of 2.63 (p < .001), a difference of almost half of a point and approximately +two-thirds of a standard deviation. Finally, as discussed earlier, students view science as a +relevant domain, as evidenced by a relatively high presurvey mean of 3.66 on the utility +scale. Nevertheless, they slightly increased their views of the relevance of science after +taking HoS courses (p < .05) to a postsurvey mean of 3.74, a change of about a tenth of a +standard deviation. +Subsequently, we turn to an examination of how the changes we observe for HoS students +compare to changes in attitudes toward science among students taking more traditional +lecture-based science content courses. Here, we utilize multilevel mixed-effects models, +an extension of regression analysis that is similar to a mixed-design analysis of variance +and appropriate when data are nested. For this study, repeated measures of attitudes are +nested within individuals with time treated as a random effect (Rabe-Hesketh & Skrondal, +2008).The goal of this analysis was to determine whether the change in different dimensions +of science attitudes observed for HoS students was similar or different than that observed +for non-HoS students while controlling for students’ background characteristics (which +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +829 +TABLE 2 +Regression Analyses Predicting Attitudes to Sciencea +Model 1 +Model 2 +Model 3 +Model 4 +Confidence +Enjoyment +Anxiety +Relevance +Hands-on science (HoS) students +(ref = non-HoS students) +–0.391*** +–0.163* +0.106 +–0.051 +(0.071) +(0.072) +(0.066) +(0.059) +Time (change from pre- to postsurvey) +–0.127** +–0.131*** +0.074� +–0.116** +(0.039) +(0.039) +(0.041) +(0.036) +Time ×HoS +0.500*** +0.391*** +–0.553*** +0.200*** +(0.056) +(0.056) +(0.060) +(0.052) +Female +–0.402*** +–0.395*** +0.311*** +0.046 +(0.085) +(0.084) +(0.076) +(0.069) +Race/ethnicity (ref = white) +Black +0.078 +–0.069 +0.018 +–0.159 +(0.188) +(0.185) +(0.168) +(0.149) +Hispanic +–0.136 +0.054 +0.055 +–0.023 +(0.093) +(0.091) +(0.083) +(0.073) +Asian +–0.314** +–0.110 +0.232** +–0.002 +(0.098) +(0.097) +(0.088) +(0.078) +American Indian/Alaska native +–0.591* +–0.181 +0.287 +0.112 +(0.251) +(0.249) +(0.224) +(0.204) +Native Hawaiian/other Pacific +Islander +0.635 +0.380 +–0.524 +0.537� +(0.418) +(0.407) +(0.374) +(0.322) +SAT math score +0.002*** +–0.000 +–0.002*** +0.000 +(0.000) +(0.000) +(0.000) +(0.000) +Mother’s education level +–0.038� +–0.013 +0.029 +–0.003 +(0.022) +(0.022) +(0.020) +(0.017) +Constant +2.680*** +4.179*** +3.748*** +3.762*** +(0.320) +(0.315) +(0.288) +(0.255) +aCoefficients calculated from a multilevel regression model in Stata where observations of +attitudes are nested within individuals. +***p < .001, **p < .01, *p < .05, �p < .1; standard errors in parentheses; n = 501. +is particularly important as our two groups of students differed by gender and math SAT +scores, both factors which likely predict attitudes). +Table 2 displays the results of separate analyses for each dependent variable. The first +row displays the coefficient comparing HoS and non-HoS students on the presurvey (or +time 1) for each attitudinal dimension. The second row displays the average change over +time between the pre- and postsurvey, while the third row displays the interaction between +student group (HoS or non-HoS) and time. The change in attitudes from pre- to postsurvey +for HoS students is calculated as the sum of the main effect of time and the interaction term, +while change for non-HoS students is captured by the main effect of time only. To simplify +the presentation of results, we include figures for each attitudinal outcome (Figures 1–4) +that display the changes over time for each group, adjusted for the social and academic +characteristics discussed above.6 +6Figures 1–4 display the adjusted pre and post means for each group. These are calculated using a +postestimation command in Stata where all other variables in the model(other than student group, time, and +the interaction) are set to the mean (or alternatively to the mode for categorical variables). +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +830 +RIEGLE-CRUMB ET AL. +Figure 1. Confidence. +Figure 2. Enjoyment. +Figure 3. Anxiety. +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +3.8 +3.6 +3.4 +score +3.2 +Adjusted +HoSstudents +3 +...Non-Hosstudents +2.8 +2.6 +2.4 +Pre +Post3.8 +3.6 +3.4 +score +3.2 +Adjusted : +HoSstudents +3 +...Non-Hos students +2.8 +2.6 +2.4 +Pre +Post3.8 +3.6 +3.4 +Adjusted score +3.2 +HoSstudents +3 +.Non-HoSstudents +2.8 +2.6 +2.4 +Pre +PostDO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +831 +Figure 4. Relevance. +Beginning with the first column predicting confidence, the results reveal that compared to +their peers in traditional science classes, HoS students reported significantly lower science +confidence on the presurvey (–.391***). The coefficient for time is negative and significant, +yet the interaction between time and student group is positive and significant, indicating +that HoS students increased their confidence over time relative to non-HoS students. To help +clarify the patterns for the two groups, Figure 1 displays the trends for each group. Here, we +see clearly that changes in attitudes occurred for both groups in opposite directions. While +HoS students initially had lower confidence than their non-HoS peers, they significantly +increased their confidence over time. In contrast, non-HoS students significantly decreased +their science confidence (–.127***), such that their confidence was slightly lower than +non-HoS students on the postsurvey. +Returning to Table 2, we see a similar pattern when predicting change in science en- +joyment. HoS students initially reported significantly lower levels of enjoyment than their +peers in more traditional classes (–.163**). However, once again we see a negative main +effect of time but a positive and significant interaction between student group and time, in- +dicating opposite directions of change for each group. As displayed graphically in Figure 2, +HoS students significantly increase their enjoyment over time, while on average non-HoS +students report a decrease in their affect toward science (–.131***), and end their course +reporting lower enjoyment than HoS students. +Regarding changes in anxiety, we note that HoS and non-HoS students do not differ +significantly on the presurvey. The main effect of time is positive and borderline significant, +yet the interaction term reveals a statistically significant difference between the two groups’ +average change in anxiety. Figure 3 clearly shows the marked decrease in anxiety from the +pre- to the postsurvey for HoS students. For their non-HoS peers, however, the figure shows +a slight increase in anxiety (�.074). +Finally, Table 2 displays the results for models predicting changes in attitudes toward +the relevance of science. HoS and non-HoS students do not differ significantly on the +presurvey. But once again the interaction term reveals a statistically significant difference +between groups in change over time, and the sign of the coefficient is positive in contrast +to negative main effect of time. Figure 4 displays the disordinal patterns for the groups. +HoS students’ views of relevance increase a small amount from the pre- to the postsurvey, +whereas their peers’ perceptions of the relevance of science decreases (–.116**). +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +3.8 +3.6 +3.4 +score +3.2 +Adjusted +HoSstudents +3 +... Non-HoS students +2.8 +2.6 +2.4 +Pre +Post832 +RIEGLE-CRUMB ET AL. +Finally, while the main focus of our analyses was to assess differences between HoS and +non-HoS students regarding changes in their science attitudes, our multivariate analyses +revealed patterns consistent with prior research, namely that females are significantly less +confident in their science ability and report significantly less enjoyment and more science +anxiety than their male peers (Correll, 2001; Eccles, 1994). Our models also indicate some +evidence of racial/ethnic differences in attitudes (see the models predicting confidence and +anxiety), as well as differences by prior math achievement, as those with higher scores on +the math portion of the SAT report significantly higher levels of confidence in their science +ability and less anxiety. Given the differential distribution of HoS and non-HoS students on +several of these covariates (see Table 1), including them in our models generally decreased +the size of the difference between groups on the presurvey (e.g., the more male composition +of the non-HoS group helped to account for their initially stronger math confidence), and +also revealed larger differences between the groups on the postsurvey than could be detected +in simpler models that did not account for these factors. +DISCUSSION AND CONCLUSION +The goal of this study was to focus on future elementary teachers’ views toward science +at a point when they are still explicitly occupying the role of a learner, before they are tasked +with assuming the role of a science teacher. Specifically, we investigated whether enrollment +in HoS, a program of inquiry-based science content courses, promoted a favorable change +in the science attitudes of a sample of over 200 preservice elementary teachers. Building +on the theoretical framework advanced by van Aalderen-Smeets and colleagues (2012), our +study examined changes in attitudes on multiple dimensions, and also utilized a comparison +group of noneducation/nonscience majors to help contextualize the changes observed for +our focal sample of elementary preservice teachers. +Data analyses reveal a remarkably consistent and positive story for HoS students; students +significantly changed their views toward science from the pre- to the postsurvey, such that +after participating in inquiry-based content courses they reported more confidence in their +skills as science learners, more enjoyment and less anxiety toward science, and perceived it +as more relevant. Conversely, patterns for those in the comparison group revealed a decline +in favorable attitudes toward science after enrolling in a traditional, lecture-based content +course. Importantly, these results are independent of differences between HoS and non-HoS +students (e.g., gender and SAT math score) that are associated with attitudes; therefore, +our analyses indicates that it was differences in the courses that the two groups of students +enrolled in, rather than characteristics of the individual students themselves, that led to +changes in attitudes. +Our study has several likely implications for the future classrooms of preservice teach- +ers, as prior research suggests that teachers with negative views toward science may both +socialize their young students to develop similar views, as well as offer less science instruc- +tion in class due to a desire to avoid the subject (Bursal & Paznokas, 2006; Jarrett, 1999). +Thus, to the extent that HoS students have more positive attitudes toward science as a result +of inquiry-based instruction, we have positively intervened to disrupt the vicious cycle of +elementary school teachers passing their negative views of science onto the next generation. +Instead, future elementary students could ultimately be the beneficiaries, having teachers +who are favorably inclined and excited about teaching science and therefore spend more +time and focus on it. +Additionally, we suggest that our results have potential implications for gender equity in +the classroom, particularly because, while all observed changes for HoS students were in +a favorable direction, the largest changes were for decreasing anxiety. Recent research by +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +DO INQUIRING MINDS HAVE POSITIVE ATTITUDES? +833 +Beilock et al. (2010) offered evidence that the math anxiety of female elementary teachers +had a negative impact on their female students in particular. The authors argue that due +to the inclination for children to more strongly connect to adults of the same gender as +role models, young girls in the classroom were more susceptible to teachers’ math anxiety, +and consequently exhibited more negative attitudes of their own as well as lower math +achievement. Their study provides powerful evidence that teacher role-modeling can be a +key factor that leads to the development of the gender gap in math as early as elementary +school (Beilock et al., 2010). Such a pattern can be logically extended to science anxiety; +thus by intervening to decrease the anxiety of (predominantly female) preservice elementary +teachers, more young girls could have the opportunity to interact with a positive female role +model, thereby thwarting emerging gender disparities in children’s views and performance +(Eccles, 1994). +Our study also has potential ramifications for the type of instruction and classrooms +experienced by future elementary students. As research suggests that preservice teachers +tend to teach their students in ways similar to how they were taught (Gess-Newsome & +Lederman, 1999), programs such as HoS can serve as a powerful model for implement- +ing inquiry in their own classrooms, and thus ultimately contribute to greater uptake of +recommended science reform. The Next Generation Science Standards call for elementary +teachers to engage their students in inquiry-based practices, as well as emphasize disci- +plinary core ideas in the classroom (National Research Council, 2012b). The HoS classes +offer preservice teachers the critical opportunity to develop an understanding of and real +experience with inquiry-based teaching and learning that is consistent with these standards. +We concur with Volkmann et al. (2005), who argue that “if learning through inquiry is to +become a reality in today’s schools, then university science courses must model inquiry so +that pre-service teachers may experience it” (p. 867). Programs such as HoS have the power +to do exactly this, and thereby help break the cycle of teacher-centered didactic instruction. +While the primary focus of this study is the educational experiences of preservice teachers +during college and the subsequent implications for future elementary classrooms, our study +also speaks to the need to improve undergraduate science education more broadly. A recent +meta-analysis of student academic performance in STEM undergraduate courses provides +evidence that traditional lecture formats lead to higher failure rates and lower achievement +when compared to classes that are more constructivist based (Freeman et al., 2014 ). Our +study focuses on attitudinal rather than performance outcomes, and in doing so heeds recent +calls by the National Research Council to examine a more comprehensive range of student +outcomes at the postsecondary level (National Research Council, 2012). Specifically, we +find that, even after adjusting for differences in social and academic background between +our two groups (preservice education students and noneducation/nonscience students), +enrollment in traditional lecture classes has the opposite effect of enrolling in inquiry- +based content classes. We suggest that the decline in confidence, affect, and utility, as well +as a slight increase in anxiety that we observed for students in traditional lecture-based +science content classes, are important consequences of their relatively low engagement in +the classroom, and perhaps linked to patterns of lower performance documented elsewhere +(Freeman et al., 2014; Seymour & Hewitt, 1997). +As with any study, ours has limitations. First, we note a lack of parallel time frames for +our focal HoS students (two semesters between pre- and postsurveys) and our comparison +group (one semester between pre- and postsurveys). Therefore, it is possible that part of the +positive change in attitudes observed for HoS students is due to the longer exposure period; +while we cannot dismiss this possibility entirely we are nevertheless skeptical that a shorter +survey window for HoS students would have substantively changed our findings regarding +opposite directions of change for the two groups. Indeed, we did collect postsurveys for a +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + +834 +RIEGLE-CRUMB ET AL. +small subsample of HoS students at the end of the first semester, and the results, although +slightly weaker in magnitude, were statistically significant and in the same positive direction +as the full sample of HoS students included here. +Additionally, we did not collect data to assess what features of these inquiry-based +classes students found most favorable; for instance, it could be that the significant amount +of time spent on group work was a particularly influential factor leading to their change +in attitudes (Park Rogers & Abell, 2008). We think this is an important area for future +research to address, to better ascertain which aspects of inquiry-based classrooms are most +effective at promoting favorable shifts on different dimensions of science attitudes. More +long-term studies are also needed to assess whether and how the potential implications we +discuss above come to fruition and make a difference for elementary students in the science +classroom. +Finally, it is important to point out that designing and implementing inquiry-based science +content courses that depart from the typical lecture-based format of most postsecondary +instruction is certainly not without its challenges and difficulties (Allen & Tanner, 2005; +Armbruster, Johnson, & Weiss, 2009). One such obstacle is convincing science instructors +and university administrators of the benefits of inquiry-based instruction for their students. +Our study contributes to the small number of studies that offer robust empirical evidence +on this topic (Seymour, 2002), and in doing so offers additional support to the call to +implement inquiry-based science instruction at all levels and for all students. +This research was supported by a grant from the National Science Foundation (NSF DUE 0942943, +PI: Sacha Kopp), and a grant from the Eunice Kennedy Shriver National Institute of Health and Child +Development (5 R24 HD042849) awarded to the Population Research Center at The University of +Texas at Austin. Opinions reflect those of the authors and do not necessarily reflect those of the +granting agencies. +REFERENCES +Allen, D., & Tanner, K. (2005). Infusing active learning into the large-enrollment biology class: Seven strategies, +from the simple to complex. 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Women in science: Career processes and outcomes (Vol. 26, No. 73.4). +Cambridge, MA: Harvard University Press. +Science Education, Vol. 99, No. 5, pp. 819–836 (2015) + diff --git a/C9E2T4oBgHgl3EQfoAjs/content/tmp_files/load_file.txt b/C9E2T4oBgHgl3EQfoAjs/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..fe50bfc885ce054a5b944c3be2f0d10f4ddf1994 --- /dev/null +++ b/C9E2T4oBgHgl3EQfoAjs/content/tmp_files/load_file.txt @@ -0,0 +1,1009 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf,len=1008 +page_content='Science Education Do Inquiring Minds Have Positive Attitudes?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The Science Education of Preservice Elementary Teachers CATHERINE RIEGLE-CRUMB,1 KARISMA MORTON,1 CHELSEA MOORE,2 ANTONIA CHIMONIDOU,3 CYNTHIA LABRAKE,4 SACHA KOPP5 1Department of Curriculum and Instruction, STEM Education, University of Texas at Austin;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 2Department of Psychology, University of Massachusetts, Amherst;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 3UTeach Primary, College of Natural Sciences, University of Texas at Austin;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 4Department of Chemistry, University of Texas at Austin;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' and 5College of Arts and Sciences, SUNY Stonybrook Received 26 June 2014;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' revised 27 February 2015;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' accepted 30 March 2015 DOI 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='1002/sce.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='21177 Published online 14 July 2015 in Wiley Online Library (wileyonlinelibrary.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='com).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' ABSTRACT: Owing to their potential impact on students’ cognitive and noncognitive outcomes, the negative attitudes toward science held by many elementary teachers are a critical issue that needs to be addressed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' This study focuses on the science education of preservice elementary teachers with the goal of improving their attitudes before they begin their professional lives as classroom teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, this study builds on a small body of research to examine whether exposure to inquiry-based science content courses that actively involve students in the collaborative process of learning and discovery can promote a positive change in attitudes toward science across several different dimensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To examine this issue, surveys and administrative data were collected from over 200 students enrolled in the Hands on Science (HoS) program for preservice teachers at the University of Texas at Austin, as well as more than 200 students in a comparison group enrolled in traditional lecture-style classes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Quantitative analyses reveal that after participating in HoS courses, preservice teachers significantly increased their scores on scales measuring confidence, enjoyment, anxiety, and perceptions of relevance, while those in the comparison group experienced a decline in favorable attitudes to science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These patterns offer empirical support for the attitudinal benefits of inquiry-based instruction and have implications for the future learning opportunities available to students at all education levels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' C⃝ 2015 Wiley Periodicals, Inc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Sci Ed 99:819–836, 2015 Correspondence to: Dr.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Catherine Riegle-Crumb;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' e-mail: riegle@austin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='utexas.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='edu C⃝ 2015 Wiley Periodicals, Inc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 820 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' INTRODUCTION While the metaphor of science, technology, engineering, and mathematics (STEM) as a pipeline has been rightly criticized as too simplistic, it is nevertheless clear that students’ early experiences in science classrooms shape their future achievement and interests (Xie & Shauman, 2003).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' With the goal of better understanding and ultimately improving elemen- tary science education in the United States, researchers and policymakers have increased their attention toward teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' A growing body of research now focuses on the science content knowledge of elementary science teachers, as the subject matter expertise that they possess has clear implications for what students learn (Diamond, Maerten-Rivera, Rohrer, & Lee, 2014;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Heller, Daehler, Wong, Shinohara, & Miratrix, 2012;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Kanter & Kon- stantopoulus, 2010;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Sadler, Sonnert, Coyle, Cook-Smith, & Miller, 2013).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Compared to secondary teachers, elementary teachers are much more likely to be trained as generalists and consequently less likely to have extensive content knowledge, and this pattern appears particularly pronounced for science (Haefner & Zembal-Saul, 2004).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Clearly there are con- tinued concerns about the need for teacher training programs and professional development to focus on increasing subject matter expertise.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Yet content knowledge is a necessary but insufficient characteristic of a successful teacher.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Teachers’ attitudes about the content they teach is another critical factor that has implications for classroom learning, and importantly, negative attitudes can exist independent of content- area expertise (Beilock, Gunderson, Ramirez, & Levine, 2010;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Tosun, 2000).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While there is comparatively less research on elementary teachers’ attitudes toward science than math (Bursal & Paznokas, 2006), there is nevertheless evidence that many elementary teachers are not favorably inclined toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Such negative attitudes on the part of teachers can impact their students’ attitudes toward science and can inhibit students’ learning (Beilock et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2010;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Jarrett, 1999;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Ramey-Gassert, Shroyer, & Staver, 1996), creating a vicious cycle that must be interrupted.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' However, effectively changing how teachers view science is a challenging task (Mulholland & Wallace, 1996;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Palmer, 2002).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The goal of this study is to examine whether inquiry-based science content classes might function to help break this cycle by improving preservice teachers’ attitudes at a critical juncture before they begin their professional lives as classroom teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While there is much research on the positive impact of inquiry on outcomes for K–12 students (Borman, Gamoran, & Bowdon, 2008;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Diamond et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2014;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' National Research Council, 2012b), we build on a smaller body of qualitative research regarding the benefits of inquiry instruction in college for preservice elementary teachers (Mulholland & Wallace, 1996;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Palmer, 2002).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, we suggest that students can become empowered and enthusiastic about the domain of science through active involvement in the process of inquiry, defined as engaging in the pursuit of scientific questions via data collection, experimentation, exploration, and discussion (National Research Council, 2000).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To examine this issue, we collected data from the hands-on science (HoS) undergraduate program at the University of Texas at Austin (Ludwig et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2013) to determine whether exposure to these inquiry-based science content courses promoted a change in the science attitudes of a sample of over 200 preservice elementary teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' In exploring preservice teachers’ attitudes, we go beyond the typical singular focus of much research on self- efficacy to instead consider personal attitudes toward science across several dimensions (van Aalderen-Smeets, Walma van der Molen, & Asma, 2012).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, to ensure the robustness of our results, our design utilizes a comparison group of noneducation and nonscience majors enrolled in more traditional lecture-based science courses;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' our analyses also account for students’ social and academic background.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our study offers promising evidence that science content classes in college can be a positive vehicle for changing the Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 821 attitudes of future elementary teachers, and subsequently has potential implications for the opportunities to learn both cognitive and noncognitive skills that are offered to future generations of elementary science students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' LITERATURE REVIEW Framework: Considering Attitudes Across Multiple Dimensions When exploring attitudes toward science, it is critical to recognize multiple relevant dimensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Based on a comprehensive review of prior research on teacher attitudes, and motivated by the lack of substantive clarity and empirical transparency of most prior research, van Aalderen-Smeets et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2012) recently advanced a new theoretical framework to provide a cohesive model that captures primary teachers’ attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, they developed a tripartite model of primary teachers’ attitudes toward science that distinguishes between three overarching dimensions, each of which is composed of different elements: (1) perceived control (which includes elements such as self-efficacy), (2) affective states (which includes enjoyment and anxiety), and (3) cognitive beliefs (such as perceived relevance).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' This framework is informed by earlier theoretical models of attitudes (Eagly & Chaiken, 1993), but departs from prior models by considering perceived control (e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', self-efficacy) as a core dimension, and furthermore defining behavioral intentions as a consequence rather than a component of science attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Their model also calls for researchers to make a clear distinction regarding whether the focus is on teachers’ personal attitudes toward science or their professional attitudes toward teaching science, as studies that combine teachers’ views of science as a domain with their views on science instruction in their own classroom into one empirical scale blur the object of teachers’ attitudes, making substantive interpretation difficult.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The three dimensions of attitudes (whether personal or professional) advanced by van Aalderen-Smeets et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2012) are logically related to one another.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, Bursal and Paznokas(2006) found that teachers with higher levels of self-efficacy had lower anxiety, a finding supported by several other studies (Bleicher, 2007;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Palmer, 2002).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Yet while related, they nevertheless capture somewhat distinct thoughts and beliefs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For instance, an individual might expect to master an activity or believe that it is useful, but nevertheless find it is unappealing (e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', flossing their teeth) or even anxietyproducing (e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', running 10 miles).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Therefore, considering elements of all three dimensions is critical to developing a comprehensive picture of teachers’ attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Yet most of the literature about the attitudes of elementary science teachers (either preservice or in-service) focuses on their perceived control in the form of self-efficacy, as there is relatively scant research on either the cognitive beliefs or affective attitudes of teachers (van Aalderen-Smeets et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2012).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Thus, a key contribution of our study is our consideration of elements of all three dimensions of attitude to more fully capture the complexity of preservice teachers’ attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='1 Below we discuss the prior literature on the science attitudes of preservice elementary teachers in more detail, including how such attitudes may influence the outcomes of future students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Because our research questions and subsequent empirical analyses focus on preservice teachers well before they 1In this paper, we address all three dimensions of van Aalderen-Smeets et al.’s (2012) theoretical model, but do not discuss (or model) every element within each dimension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, while the authors include context dependency as an element that falls under the dimension of perceived control, we do not address this here as it refers to the support that practicing teachers receive from their administrators and therefore is not particularly relevant for a study concerning the personal (rather than professional) attitudes of preservice teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 822 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' actually enter the elementary classroom, we concentrate on literature on personal attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We then turn to a discussion of why inquiry-based science content classes for preservice teachers have the potential to increase individuals’ attitudes across all three dimensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Perceived Control: Considering Self-Efficacy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' A key element of the attitudinal dimen- sion of perceived control is self-efficacy, which according to Bandura’s (1977, 1982) foundational work is defined as an individual’s belief that she can successfully master a situation or deal with an obstacle that arises.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' An individual’s self-efficacy has logical im- plications for her subsequent behaviors and choices, as she is likely to attempt to avoid those situations or activities where she does not feel she can be efficacious, and persist where she feels confident that she can be successful.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While research has demonstrated that in-service elementary teachers exhibit low levels of efficacy in their science teaching (see, for example,Atwater, Gardner, & Kight, 1991;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Harlen, 1997;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Ramey-Gassert et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 1996), not surprisingly this pattern is also evident among preservice teachers, who feel less efficacious about their own ability to learn science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, Skamp (1991) determined that less than half of the preservice elementary teachers in his study reported having even a fair amount of confidence in their science ability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Similarly, Bleicher’s (2007) study of preservice elementary teachers found that participants in a science methods class exhibited low scores on science self-efficacy scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Low efficacy is often attributed to prior negative educational experiences in science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, in a study of five preservice teachers, Mulholland and Wallace (1996) found that their respondents reported very little confidence in their own science abilities and attributed this to negative experiences in their own science schooling as children.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Affective States: Considering Enjoyment and Anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Individuals’ affect toward a domain represents another attitudinal dimension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As articulated by van Aalderen-Smeets et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2012), the dimension of affect can be further categorized into the positive element of enjoyment and the negative element of anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Beginning with the former, Liang and Gabel (2005) found that most preservice elementary teachers in their study reported that science had never been enjoyable for them.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These teachers also indicated that they took science courses only because it was required for their degree program.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Smith (2000) and Howes (2002) found similar results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, the preservice participants in all of these studies attributed their low levels of enjoyment to negative experiences in either (or both) their high school and college science courses, a point to which we will return to later.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Anxiety captures the negative aspect of the affective dimension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Early research by Mallow (1981;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' also Mallow & Greenburg, 1983) as well as Westerback (1984) define science anxiety as the fear, worry, or apprehension that some individuals experience when presented with the task of learning science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While research on the math anxiety of preservice teachers is extensive (Udo, Ramsey, & Mallow, 2004), and research considering both math anxiety and science anxiety find a strong association between the two (Cady & Rearden, 2007), there is comparatively little research focusing specifically on science anxiety (Bursal & Paznokas, 2006).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Yet several studies do provide evidence that preservice elementary teachers report relatively high levels of science anxiety about teaching science, as well as more generalized anxiety about learning science themselves (Cady & Rearden, 2007;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Udo et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2004;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Westerback & Long, 1990).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Cognitive Beliefs: Considering the Relevance of Science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, we discuss research on preservice elementary teachers’ beliefs in the relevance of science, a critical element Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 823 of the attitudinal dimension of cognitive beliefs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The limited extant research on this topic focuses on perceptions of science as useful or relevant for society and for them personally, and finds that preservice elementary teachers report generally favorable views.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, in a study of 200 preservice teachers, Coulson (1992) used a survey instrument that in- cluded a personal usefulness science scale and found that on average, respondents indicated moderate levels of agreement.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Cobern and Loving’s (2002) study at a large Midwestern university also found that on Likert scales measuring the perceived importance of science to all citizens, preservice elementary teachers on average agreed with this sentiment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These findings echo the sentiments of the general population, which generally regard science and technology as useful for making their lives better (Evans & Durant, 1995;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Kohut, Keeter, Doherty, & Dimock, 2009).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Therefore among the three attitudinal dimensions discussed, promoting preservice teachers’ views of the relevance of science is perhaps somewhat less of a pressing problem than promoting both their perceived control in the form of science efficacy and their affective attitudes of enjoyment and anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Examining the Impact of Teacher Attitudes There is a logical connection between teachers’ attitudes toward a subject and student outcomes, both in terms of impacting students’ opportunities to learn science and their own developing attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' First, research indicates that the negative attitudes toward science held by many elementary teachers are likely to result in less coverage of science content and less engaging and effective instruction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Teachers who are not confident in their own science knowledge are likely to worry that they cannot effectively answer students’ questions nor keep them engaged with interesting activities (Jarrett, 1999).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Consequently, elementary teachers who feel less efficacious and more anxious are likely to try to avoid teaching science and spend less time teaching when they cannot avoid it altogether (Brownlow, Jacobi, & Rogers, 2000;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Pine et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2006;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Ramey-Gassert et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 1996).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Appleton and Kindt (1999) also found evidence that avoidance occurred when teachers did not find science to be as relevant as other subjects such as English or math.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' One such teacher reported that “If you’re running out of time in the week, you think ‘Oh I just won’t worry about that science activity’” (p.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 162).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' When teachers do teach science, their negative attitudes can impact their pedagogical practices and subsequently their capacity to reach and engage students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Appleton and Kindt’s (1999) study of in-service elementary teachers found that those exhibiting low confidence were less likely to engage their students in hands-on learning.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Ramey-Gassert et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (1996) found that elementary teachers with low science self-efficacy had a minimal desire to engage in professional development activities that could improve their teaching of science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Lack of belief in the usefulness or relevance of science could also logically result in a reduced effort to provide engaging instruction to students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, the negative attitudes toward science held by many elementary teachers can result in the socialization of students toward a negative stance toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As students look to their teachers as role models and authorities, they begin to mimic and potentially internalize such attitudes as their own (Jussim & Eccles, 1992;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' McKown & Weinstein, 2002).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' This can lead to a vicious cycle where negative attitudes such as anxiety and low efficacy are passed from teachers to their students, and therefore from one generation to the next.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, Beilock et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2010) found that elementary teachers’ math anxiety influenced students’ own attitudes toward math, with girls in particular more likely to evidence declining math attitudes and increasingly gender-stereotyped views of math over the course of the year.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' This particular study highlights additional concerns regarding gender rolemodeling;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' as most elementary teachers are female, and a substantial number Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 824 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' of them exhibit negative attitudes toward science (as well as math), this could be a strong conduit through which young girls begin to believe that these subjects are less interesting, less important, and overall less-suited for them.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Furthermore, as students’ own attitudes decline, so does their engagement and motivation to learn, which further impacts their achievement (Eccles, 1994).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' In sum, the research literature provides compelling evidence that teachers’ negative attitudes can impact students’ learning and attitudinal outcomes, and as such are a critical issue that needs to be addressed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To effectively break this cycle, necessitates intervening to change teachers’ attitudes before they enter the classroom.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' In short, the education of preservice teachers is an ideal place to focus.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Educating Preservice Teachers: Inquiry as a Tool for Improving Attitudes As mentioned earlier, the negative attitudes of preservice elementary teachers can at least in part be traced back to their own negative experiences with science classes in high school and in college.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, Liang and Gabel (2005) found that preservice teachers attributed their lack of enjoyment of science to their prior experiences in classes dominated by lectures that necessitated copious amounts of note-taking and memorization.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Similarly, Smith (2000) reports that preservice elementary teachers in his study often complained about the boredom of their procedure-based high school and college science courses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Simply put, many preservice teachers have had little exposure to inquiry-based science instruction in their lives as students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We posit that exposure while in college to pedagogy that actively involves them in the process of scientific discovery can ultimately help them to see that science is meaningful, interesting, and accessible, thereby changing their attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Several studies support the supposition that inquiry classes can promote such changes, in spite of the possibility of some initial student frustration with an approach that deviates from teachers’ didactic presentations of the “right” answer (Volkmann, Abell, & Zgagacz, 2005).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, in a qualitative study of preservice teachers at a large university in the southwest, Kelly (2000) found that after completing an active, inquiry-based science methods course, most participants reported that their interest in science had increased.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Kelly (2000) attributes this shift to the use of hands-on explorations and discussions where students came to embody the process of scientific inquiry by formulating and exploring ideas.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Similarly, in a study of preservice elementary teachers, Palmer (2002) interviewed four participants who reported that their attitudes toward science had changed from negative to positive due to the excitement of inquiry-based lessons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' A study of five teachers by Mulholland and Wallace (1996) reported similar results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, in a quantitative study of 112 preservice elementary teachers, Jarrett (1999) found that an inquiry-based science methods class increased the participants’ personal interest in science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The author attributed this change to preservice teachers becoming active agents in the classroom and learning to view science as a process of discovery.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Thus, a small body of research finds that inquiry- based pedagogy in science educational methods courses can have a positive impact on preservice elementary teachers’ attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' CURRENT STUDY Building on the insights of this prior research, we posit that required science content courses could also represent a powerful venue for change for college students at the beginning stages of preparing for their careers as future teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, the purpose Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 825 of this study is to examine whether inquiry-based science content courses promote a change in attitudes toward science among preservice elementary teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The courses are part of the HoS undergraduate program, developed at The University of Texas at Austin in the College of Natural Sciences, with cooperation from the College of Education.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS is required of all students in the elementary education program and covers four semesters of science courses with a curriculum that is composed heavily of the topics that preservice teachers will be expected to teach their students once they become teachers (Ludwig et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2013).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The design of the HoS program is based on the Physics and Everyday Thinking (Goldberg, 2008) framework that centers around the development of students’ physical science understandings through experimentation and follows the example of work from Western Washington University extending this framework to other disciplines (Nelson, 2008).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The curriculum is based upon big ideas in science, with specific emphasis on the themes of Matter and Energy, which are integrated across different science disciplines.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The course sequence focuses on physics in Semester 1, chemistry and geology in Semester 2, biological systems in Semester 3, and astronomy and earth science in Semester 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS classes were designed to utilize the essential elements of inquiry-based learning as defined by the influential National Research Council report on inquiry (Forbes, 2011;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' National Research Council, 2000);' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' specifically, students engage in scientifically oriented questions by collecting, organizing, and analyzing data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' From that data they formulate explanations, connect them to scientific knowledge, and subsequently evaluate their expla- nations in contrast to alternative explanations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, students share and justify those explanations with others.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The HoS program is best categorized as teacher-directed or guided inquiry (Cuevas, Lee, Hart, & Deaktor, 2005;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' National Research Council, 2000;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Volkmann et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2005).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Initial questions are posed by the instructor and all activities are carefully designed to present opportunities for students to confront misconceptions, with both topics and skills developed in a structured progression.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The instructor does not lecture but probes student knowledge and offers helpful nudges in the right direction, working with students both in small groups and via whole class discussions to construct knowledge and develop explanations (Volkmann et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2005).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, consistent with inquiry approaches to learning, the course emphasizes big ideas in science while engaging students in hands-on learning and constant exploration and discussion while in groups with their peers (National Research Council, 2000, 2012b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' An example of a typical 2-hour class session is a lesson on sound that begins with the following teacher-generated questions: How does sound travel through a room?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' How does sound travel from your classmate to you?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Students then work in groups of three or four to answer these questions and discuss their initial ideas or preconceptions;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' they subsequently share their ideas with the entire class, so that there is a collective knowledge of alternative ways of thinking about how sound travels.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Working in their small groups, students then engage in a series of experiments, using an “airzooka” and candles, a string telephone, and a loudspeaker, that require that they gather data and then generate models based on these data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' They are regularly prompted by the instructor to make predictions and connect trends to other previously seen concepts.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, students reflect and summarize key ideas and connect them to other contexts by using evidence-based reasoning from the data collected in their experiments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These questions are the basis for whole-class discussions, where students present and justify their ideas to their peers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Students typically end lessons by writing a scientific narrative summarizing how their thinking was revised from their initial ideas, drawing on evidence gained through the experiments and whole class sharing and discussion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For example, a student might share how her initial idea that “sound travels as a wave” has become more sophisticated, discussing the role of vibrations and the transfer of mechanical energy from the source to the receiver.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 826 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our examination of whether the inquiry-based science content courses of the HoS pro- gram promote a change in attitudes toward science among preservice elementary teachers is described in detail below.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Here, we briefly note that our study contributes to the literature a rigorous quantitative examination of change in attitudes across multiple dimensions among preservice elementary teachers, utilizing a comparison group of students in more traditional science content courses, as well as accounting for differences among students in academic and social background characteristics that may have implications for their attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Data and Method Analytic Sample.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our analytic sample includes 238 preservice elementary teachers who enrolled in the HoS program between Fall 2010 and Spring 2012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Students completed presurveys prior to the start of the first course and postsurveys at the end of the second course in the sequence.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='2 Surveys were done online, and were administered during class by members of the research team.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, our sample includes a comparison group composed of 263 nonscience and noneducation majors enrolled in traditional lecture-style undergraduate science courses in Spring 2012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While our design falls shorts of a pure treatment versus control comparison, we chose courses that represent what our sample of preservice elementary teachers would have been required to take in the absence of the HoS program.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Therefore, our comparison group includes students who were enrolled in either an introductory-level chemistry or biology class.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These students were surveyed at the beginning and end of the semester.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As the time period between pre- and postsurveys is longer for HoS students than for non-HoS students, we discuss the implications and limitations of this comparison later.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Administrative records were linked to student surveys, allowing us to examine the demo- graphic and academic background information of students in our sample and to consider how HoS students differed from those in the comparison group.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Not surprisingly given the gender composition of the elementary teacher population nationwide, HoS students were overwhelmingly female (95%), compared to 65% of our comparison sample of nonedu- cation and nonscience majors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' There were no statistically significant differences between the two groups of students by mother’s education;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' for race/ethnicity, there were signifi- cantly fewer students who identified as American Indian among HoS students compared to non-HoS students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Regarding academic background prior to college entry, HoS students had lower SAT math scores than their fellow students taking typical science classes by more than one-third of a standard deviation (see Table 1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To ensure that any differences observed between the two groups in their changes in attitudes over time are not confounded by differences in their background characteristics, our subsequent multivariate models will control for all of these factors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='3 Student Attitude Surveys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The pre- and postsurveys administered to both groups con- sisted of 21 items geared toward assessing student attitudes toward science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To examine multiple dimensions of attitudes, we selected items from preexisting surveys to measure 2At the time of this study, students were only required to take the first two semesters of the total four semester sequence.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 3Mother’s education level is an ordinal variable with the following categories: (1) did not attend high school, (2) attended high school but did not graduate, (3) high school diploma or GED, (4) some college, (5) earned associate’s degree, (6) bachelor’s degree, (7) graduate or professional degree.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Math SAT score and mother’s education level were imputed for those students who had missing values.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We utilized information on gender, race, high school rank, family income, and father’s education to conduct single imputation using Stata.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Analyses using list-wise deletion produced similar results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 827 TABLE 1 Descriptive Statistics Hands-on Science (HoS) Students Non-HoS Students N = 238 N = 263 Gender Female*** 94.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='5% 65.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% Race/ethnicity White (non-Hispanic) 63.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% 60.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='1% Black 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='9% 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% Hispanic 21% 19% Asian 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='3% 14.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% American Indian** 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='7% Native Hawaiian/Pacific Islander 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8% 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4% Other background characteristics Mean SD Mean SD SAT math score*** 574.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='87 75.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='60 607.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='62 73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='39 Mother’s educational level 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='10 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='60 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='07 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='69 ***p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='001, **p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='01, *p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='05, p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' confidence (an element of perceived control)4, enjoyment and anxiety (positive and neg- ative elements of affective states), and relevance (a key element of cognitive beliefs).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To measure anxiety, we used the Math Anxiety Rating Scale (Hopko, 2003) and substituted the word science for all references to math.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To measure all other attitudes, we selected items developed by the National Center for Education Statistics (www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='nces.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='ed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='gov), and used in national surveys, including the Educational Longitudinal Study, the High School Longitudinal Study, and the U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' component of the Trends in International Mathematics and Science Study.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Principal component analyses with promax rotation using the complete set of 21 survey items revealed four factors with Eigenvalues greater than one.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We sub- sequently created separate scales (described below) composed of the individual items that loaded onto each of the four factors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The scales clearly corresponded to the elements of confidence, enjoyment, anxiety, and relevance;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' using the full sample, the Cronbach’s alpha for each scale was .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 or higher.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='5 The confidence scale is composed of four items that gauge students’ level of confidence when engaging in scientific activities.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The items were as follows: “I have always done well in science,” “Science is not one of my strengths” (reverse coded), “I am confident that I can understand the most difficult material presented in my science textbooks,” and “Science 4Because the questions ask students to reflect more on their assessment of their current success in science, we refer to this scale as measuring confidence rather than self-efficacy for future success.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' However, prior research has consistently noted a very strong correspondence between indicators of self-confidence and self-efficacy (Wigfield & Eccles, 2000).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5To further test the reliability of the four scales, we calculated Cronbach’s alphas separately for (a) treatment and reference groups;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (b) first year cohort and second year cohorts (for treatment group), and (c) survey responses at time 1 and time 2 (for different cohorts and for different treatment groups).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' In all, we calculated alpha reliabilities for each of our four scales for 15 different subsamples with remarkably consistent results ranging from a low of .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='77 to a high of .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='88.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (exploratory factor analyses using each of these groups also yielded the same four factor model).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 828 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' has always been one of my best subjects.” The five items in the enjoyment scale capture students’ level of positive affect for science and included “I enjoy learning science,” “I look forward to going to science courses,” “Science is fun,” “I like science,” and “Science is boring” (reversecoded for inclusion in the scale).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Categories of response were the same as those for the confidence scale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For each of the eight items in the anxiety scale, students were asked to indicate how much the situation made them feel anxious or worried.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Similar to the other measures, the responses ranged from (1) not at all anxious to (5) very much anxious or worried.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The items included “Looking through the pages in a science text,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Thinking about an upcoming science test one day before the test,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Reading and interpreting a scientific graph,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' chart,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' or illustration,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Taking an exam in a science course,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Watching and listening to a teacher explaining a scientific concept or phenomena,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Waiting to get a science test returned in which you expected to do well,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' “Walking on campus and thinking about a science course,”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' and “Being given a ‘pop’ quiz in science class.”' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' the four items making up the relevance scale include questions that focused on students’ perception of the meaning or usefulness of science in their daily lives.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The items are as follows: “The subject of science is not very relevant to most people,” “It is not important for most people to understand science,” “I think learning science will help me in my daily life,” and “Science is important to me personally.” Students indicated the extent to which they agreed or disagreed with the statements with possible responses ranging from strongly agree (1) to strongly disagree (5).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' ANALYSES AND RESULTS To examine whether inquiry-based science content courses promote a positive change in attitudes toward science for preservice elementary teachers, we begin by comparing the means on the pre- and postmeasures of our four attitudinal scales for HoS students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Results of paired t-tests indicate a statistically significant improvement over time for each scale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, for confidence, the mean increased from 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='61 to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='98 (p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='001), reflecting a 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='37 point increase or almost half of a standard deviation change from pre to post.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS students’ science enjoyment increased by about a fourth of point (and about a third of a standard deviation), from the presurvey mean of 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='24 to a postsurvey mean of 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='51 (p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='001).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The largest change was observed for the anxiety scale, where the average decreased (meaning that students became less anxious over time) from a presurvey mean of 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='11 to a postsurvey mean of 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='63 (p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='001), a difference of almost half of a point and approximately two-thirds of a standard deviation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, as discussed earlier, students view science as a relevant domain, as evidenced by a relatively high presurvey mean of 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='66 on the utility scale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Nevertheless, they slightly increased their views of the relevance of science after taking HoS courses (p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='05) to a postsurvey mean of 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='74, a change of about a tenth of a standard deviation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Subsequently, we turn to an examination of how the changes we observe for HoS students compare to changes in attitudes toward science among students taking more traditional lecture-based science content courses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Here, we utilize multilevel mixed-effects models, an extension of regression analysis that is similar to a mixed-design analysis of variance and appropriate when data are nested.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For this study, repeated measures of attitudes are nested within individuals with time treated as a random effect (Rabe-Hesketh & Skrondal, 2008).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='The goal of this analysis was to determine whether the change in different dimensions of science attitudes observed for HoS students was similar or different than that observed for non-HoS students while controlling for students’ background characteristics (which Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 829 TABLE 2 Regression Analyses Predicting Attitudes to Sciencea Model 1 Model 2 Model 3 Model 4 Confidence Enjoyment Anxiety Relevance Hands-on science (HoS) students (ref = non-HoS 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+page_content='038� –0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='013 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='029 –0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='003 (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='022) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='022) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='020) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='017) Constant 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='680*** 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='179*** 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='748*** 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='762*** (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='320) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='315) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='288) (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='255) aCoefficients calculated from a multilevel regression model in Stata where observations of attitudes are nested within individuals.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' ***p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='001, **p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='01, *p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='05, �p < .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='1;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' standard errors in parentheses;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' n = 501.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' is particularly important as our two groups of students differed by gender and math SAT scores, both factors which likely predict attitudes).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Table 2 displays the results of separate analyses for each dependent variable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The first row displays the coefficient comparing HoS and non-HoS students on the presurvey (or time 1) for each attitudinal dimension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The second row displays the average change over time between the pre- and postsurvey, while the third row displays the interaction between student group (HoS or non-HoS) and time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The change in attitudes from pre- to postsurvey for HoS students is calculated as the sum of the main effect of time and the interaction term, while change for non-HoS students is captured by the main effect of time only.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To simplify the presentation of results, we include figures for each attitudinal outcome (Figures 1–4) that display the changes over time for each group, adjusted for the social and academic characteristics discussed above.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 6Figures 1–4 display the adjusted pre and post means for each group.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' These are calculated using a postestimation command in Stata where all other variables in the model(other than student group, time, and the interaction) are set to the mean (or alternatively to the mode for categorical variables).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 830 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Figure 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Confidence.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Figure 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Enjoyment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Figure 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 score 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='2 Adjusted HoSstudents 3 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='Non-Hosstudents 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 Pre Post3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 score 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='2 Adjusted : HoSstudents 3 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='Non-Hos students 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 Pre Post3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 Adjusted score 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='2 HoSstudents 3 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='Non-HoSstudents 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 Pre PostDO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 831 Figure 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Relevance.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Beginning with the first column predicting confidence, the results reveal that compared to their peers in traditional science classes, HoS students reported significantly lower science confidence on the presurvey (–.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='391***).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The coefficient for time is negative and significant, yet the interaction between time and student group is positive and significant, indicating that HoS students increased their confidence over time relative to non-HoS students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' To help clarify the patterns for the two groups, Figure 1 displays the trends for each group.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Here, we see clearly that changes in attitudes occurred for both groups in opposite directions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While HoS students initially had lower confidence than their non-HoS peers, they significantly increased their confidence over time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' In contrast, non-HoS students significantly decreased their science confidence (–.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='127***), such that their confidence was slightly lower than non-HoS students on the postsurvey.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Returning to Table 2, we see a similar pattern when predicting change in science en- joyment.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS students initially reported significantly lower levels of enjoyment than their peers in more traditional classes (–.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='163**).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' However, once again we see a negative main effect of time but a positive and significant interaction between student group and time, in- dicating opposite directions of change for each group.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As displayed graphically in Figure 2, HoS students significantly increase their enjoyment over time, while on average non-HoS students report a decrease in their affect toward science (–.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='131***), and end their course reporting lower enjoyment than HoS students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Regarding changes in anxiety, we note that HoS and non-HoS students do not differ significantly on the presurvey.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The main effect of time is positive and borderline significant, yet the interaction term reveals a statistically significant difference between the two groups’ average change in anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Figure 3 clearly shows the marked decrease in anxiety from the pre- to the postsurvey for HoS students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' For their non-HoS peers, however, the figure shows a slight increase in anxiety (�.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='074).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, Table 2 displays the results for models predicting changes in attitudes toward the relevance of science.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS and non-HoS students do not differ significantly on the presurvey.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' But once again the interaction term reveals a statistically significant difference between groups in change over time, and the sign of the coefficient is positive in contrast to negative main effect of time.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Figure 4 displays the disordinal patterns for the groups.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' HoS students’ views of relevance increase a small amount from the pre- to the postsurvey, whereas their peers’ perceptions of the relevance of science decreases (–.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='116**).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 score 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='2 Adjusted HoSstudents 3 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='..' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Non-HoS students 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='4 Pre Post832 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, while the main focus of our analyses was to assess differences between HoS and non-HoS students regarding changes in their science attitudes, our multivariate analyses revealed patterns consistent with prior research, namely that females are significantly less confident in their science ability and report significantly less enjoyment and more science anxiety than their male peers (Correll, 2001;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Eccles, 1994).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our models also indicate some evidence of racial/ethnic differences in attitudes (see the models predicting confidence and anxiety), as well as differences by prior math achievement, as those with higher scores on the math portion of the SAT report significantly higher levels of confidence in their science ability and less anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Given the differential distribution of HoS and non-HoS students on several of these covariates (see Table 1), including them in our models generally decreased the size of the difference between groups on the presurvey (e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', the more male composition of the non-HoS group helped to account for their initially stronger math confidence), and also revealed larger differences between the groups on the postsurvey than could be detected in simpler models that did not account for these factors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' DISCUSSION AND CONCLUSION The goal of this study was to focus on future elementary teachers’ views toward science at a point when they are still explicitly occupying the role of a learner, before they are tasked with assuming the role of a science teacher.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, we investigated whether enrollment in HoS, a program of inquiry-based science content courses, promoted a favorable change in the science attitudes of a sample of over 200 preservice elementary teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Building on the theoretical framework advanced by van Aalderen-Smeets and colleagues (2012), our study examined changes in attitudes on multiple dimensions, and also utilized a comparison group of noneducation/nonscience majors to help contextualize the changes observed for our focal sample of elementary preservice teachers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Data analyses reveal a remarkably consistent and positive story for HoS students;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' students significantly changed their views toward science from the pre- to the postsurvey, such that after participating in inquiry-based content courses they reported more confidence in their skills as science learners, more enjoyment and less anxiety toward science, and perceived it as more relevant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Conversely, patterns for those in the comparison group revealed a decline in favorable attitudes toward science after enrolling in a traditional, lecture-based content course.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Importantly, these results are independent of differences between HoS and non-HoS students (e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', gender and SAT math score) that are associated with attitudes;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' therefore, our analyses indicates that it was differences in the courses that the two groups of students enrolled in, rather than characteristics of the individual students themselves, that led to changes in attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our study has several likely implications for the future classrooms of preservice teach- ers, as prior research suggests that teachers with negative views toward science may both socialize their young students to develop similar views, as well as offer less science instruc- tion in class due to a desire to avoid the subject (Bursal & Paznokas, 2006;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Jarrett, 1999).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Thus, to the extent that HoS students have more positive attitudes toward science as a result of inquiry-based instruction, we have positively intervened to disrupt the vicious cycle of elementary school teachers passing their negative views of science onto the next generation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Instead, future elementary students could ultimately be the beneficiaries, having teachers who are favorably inclined and excited about teaching science and therefore spend more time and focus on it.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, we suggest that our results have potential implications for gender equity in the classroom, particularly because, while all observed changes for HoS students were in a favorable direction, the largest changes were for decreasing anxiety.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Recent research by Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) DO INQUIRING MINDS HAVE POSITIVE ATTITUDES?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 833 Beilock et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2010) offered evidence that the math anxiety of female elementary teachers had a negative impact on their female students in particular.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The authors argue that due to the inclination for children to more strongly connect to adults of the same gender as role models, young girls in the classroom were more susceptible to teachers’ math anxiety, and consequently exhibited more negative attitudes of their own as well as lower math achievement.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Their study provides powerful evidence that teacher role-modeling can be a key factor that leads to the development of the gender gap in math as early as elementary school (Beilock et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2010).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Such a pattern can be logically extended to science anxiety;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' thus by intervening to decrease the anxiety of (predominantly female) preservice elementary teachers, more young girls could have the opportunity to interact with a positive female role model, thereby thwarting emerging gender disparities in children’s views and performance (Eccles, 1994).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our study also has potential ramifications for the type of instruction and classrooms experienced by future elementary students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As research suggests that preservice teachers tend to teach their students in ways similar to how they were taught (Gess-Newsome & Lederman, 1999), programs such as HoS can serve as a powerful model for implement- ing inquiry in their own classrooms, and thus ultimately contribute to greater uptake of recommended science reform.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The Next Generation Science Standards call for elementary teachers to engage their students in inquiry-based practices, as well as emphasize disci- plinary core ideas in the classroom (National Research Council, 2012b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' The HoS classes offer preservice teachers the critical opportunity to develop an understanding of and real experience with inquiry-based teaching and learning that is consistent with these standards.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We concur with Volkmann et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' (2005), who argue that “if learning through inquiry is to become a reality in today’s schools, then university science courses must model inquiry so that pre-service teachers may experience it” (p.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 867).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Programs such as HoS have the power to do exactly this, and thereby help break the cycle of teacher-centered didactic instruction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' While the primary focus of this study is the educational experiences of preservice teachers during college and the subsequent implications for future elementary classrooms, our study also speaks to the need to improve undergraduate science education more broadly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' A recent meta-analysis of student academic performance in STEM undergraduate courses provides evidence that traditional lecture formats lead to higher failure rates and lower achievement when compared to classes that are more constructivist based (Freeman et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2014 ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our study focuses on attitudinal rather than performance outcomes, and in doing so heeds recent calls by the National Research Council to examine a more comprehensive range of student outcomes at the postsecondary level (National Research Council, 2012).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Specifically, we find that, even after adjusting for differences in social and academic background between our two groups (preservice education students and noneducation/nonscience students), enrollment in traditional lecture classes has the opposite effect of enrolling in inquiry- based content classes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We suggest that the decline in confidence, affect, and utility, as well as a slight increase in anxiety that we observed for students in traditional lecture-based science content classes, are important consequences of their relatively low engagement in the classroom, and perhaps linked to patterns of lower performance documented elsewhere (Freeman et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=', 2014;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Seymour & Hewitt, 1997).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' As with any study, ours has limitations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' First, we note a lack of parallel time frames for our focal HoS students (two semesters between pre- and postsurveys) and our comparison group (one semester between pre- and postsurveys).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Therefore, it is possible that part of the positive change in attitudes observed for HoS students is due to the longer exposure period;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' while we cannot dismiss this possibility entirely we are nevertheless skeptical that a shorter survey window for HoS students would have substantively changed our findings regarding opposite directions of change for the two groups.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Indeed, we did collect postsurveys for a Science Education, Vol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 99, No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 5, pp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' 819–836 (2015) 834 RIEGLE-CRUMB ET AL.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' small subsample of HoS students at the end of the first semester, and the results, although slightly weaker in magnitude, were statistically significant and in the same positive direction as the full sample of HoS students included here.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Additionally, we did not collect data to assess what features of these inquiry-based classes students found most favorable;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' for instance, it could be that the significant amount of time spent on group work was a particularly influential factor leading to their change in attitudes (Park Rogers & Abell, 2008).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' We think this is an important area for future research to address, to better ascertain which aspects of inquiry-based classrooms are most effective at promoting favorable shifts on different dimensions of science attitudes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' More long-term studies are also needed to assess whether and how the potential implications we discuss above come to fruition and make a difference for elementary students in the science classroom.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Finally, it is important to point out that designing and implementing inquiry-based science content courses that depart from the typical lecture-based format of most postsecondary instruction is certainly not without its challenges and difficulties (Allen & Tanner, 2005;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Armbruster, Johnson, & Weiss, 2009).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' One such obstacle is convincing science instructors and university administrators of the benefits of inquiry-based instruction for their students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' Our study contributes to the small number of studies that offer robust empirical evidence on this topic (Seymour, 2002), and in doing so offers additional support to the call to implement inquiry-based science instruction at all levels and for all students.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/C9E2T4oBgHgl3EQfoAjs/content/2301.04015v1.pdf'} +page_content=' This research was supported by a grant from the National Science Foundation (NSF DUE 0942943, PI: Sacha Kopp), and a grant from the Eunice Kennedy Shriver 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Bouchè,1, a Salvatore Capozziello,1, 2, 3, b and V. Salzano4, c +1Dipartimento di Fisica “E. Pancini”, Università di Napoli “Federico II", Via Cinthia 21, I-80126, Napoli, Italy +2DipaScuola Superiore Meridionale, Largo S. Marcellino 10, I-80138, Napoli, Italy +3Istituto Nazionale di Fisica Nucleare, Sez. di Napoli, Via Cinthia 21, I-80126, Napoli, Italy +4Institute of Physics, University of Szczecin, Wielkopolska 15, 70-451 Szczecin, Poland +(Dated: January 5, 2023) +Alternative cosmological models have been under deep scrutiny in recent years, aiming to address +the main shortcomings of the ΛCDM model. Moreover, as the accuracy of cosmological surveys +improved, new tensions have risen between the model-dependent analysis of the Cosmic Microwave +Background and lower redshift probes. Within this framework, we review two quantum-inspired +non-locally extended theories of gravity, whose main cosmological feature is a geometrically driven +accelerated expansion. The models are especially investigated in light of the Hubble and growth +tension, and promising features emerge for the Deser–Woodard one. On the one hand, the cosmolog- +ical analysis of the phenomenological formulation of the model shows a lowered growth of structures +but an equivalent background with respect to ΛCDM. On the other hand, the study of the lensing +features at the galaxy cluster scale of a new formulation of non-local cosmology, based on Noether +symmetries, makes room for the possibility of alleviating both the H0 and σ8 tension. However, the +urgent need for a screening mechanism arises for this non-local theory of gravity. +I. +INTRODUCTION +Recent astrophysical and cosmological surveys, both from ground-based and space experiments, have provided +extremely high-quality data. The observations point towards a Universe in which the cosmological principle holds +on large scales, namely the Universe appears homogeneous and isotropic if averaged over scales of ∼100 h−1Mpc or +more [1, 2]. Moreover, the Universe is undergoing an accelerated expansion phase [3, 4], subsequent to a decelerated +era in which the structure formation occurred. All these features, together with the nuclei abundances produced in +the Big Bang Nucleosynthesis (BBN), the Baryon Acoustic Oscillations (BAO) and many others, are well predicted +by the Lambda Cold Dark Matter (ΛCDM) model, which has been adopted as the standard cosmological model +accordingly. Such a model provides an effective description of the Universe, which relies on the assumption that +General Relativity (GR) is the final theory of gravitation that governs the cosmic dynamics. As a consequence, two +more fluids other than baryonic matter and radiation must be inserted in the matter–energy content of the Universe +in order to adjust GR predictions to data: the Dark Energy (DE), responsible for the late time cosmic acceleration, +and the Dark Matter (DM), which accounts for the structure formation. Together, they should represent ∼95% of +the matter–energy budget of the Universe [5–7], thus dominating the cosmic dynamics at all scales. +Building on its capability to fit the whole cosmological and astrophysical dataset with a relatively small number of +parameters, the ΛCDM model stands as the pillar of our comprehension of the Universe. However, several shortcomings +[8] and recently risen tensions [9–11] affect its reliability. On the one hand, we have a huge assortment of candidates +but no final solution for DM [12, 13] and DE [14–16]. On the other hand, the presence of singularities, as well as the +inconsistency at quantum level, undermine the credibility of GR as the final theory of gravity. Even more puzzling +are the cosmological tensions, which have emerged in recent years as the result of the growing availability of a wide +range of extremely precise data. A multitude of independent observations appears indeed to be in a ≳2σ tension +with the reference ΛCDM estimates by the Planck collaboration [5]. Even though systematic experimental errors may +account for part of these tensions, their statistical significance and their persistence after several check analyses have +thrown up some serious red flags. Since the Planck constraints for the cosmological parameters relies on a strongly +ΛCDM-model-dependent analysis of the Cosmic Microwave Background (CMB), such tensions may be the signature +of the brakedown of the concordance model, hence of new physics. In this paper, we pay particular attention to the +two most well-known tensions: the H0 tension [10], which emerges from the comparison between early-time [5] and +late-time measurements [17] of the Hubble constant, and the growth tension [11] between the CMB value [5] of the +aElectronic address: filippo.bouche-ssm@unina.it +bElectronic address: capozziello@na.infn.it +cElectronic address: vincenzo.salzano@usz.edu.pl +arXiv:2301.01503v1 [astro-ph.CO] 4 Jan 2023 + +2 +cosmological parameters ΩM and σ8 and those from lower redshift probes, such as Weak Lensing (WL) [18], Cluster +Counts (CC) [19] and Redshift Space Distortion (RSD) [20]. +In order to meet the challenges posed by ΛCDM theoretical shortcomings, as well as by its observational tensions, a +zoo of alternative cosmological models has been formulated in recent years. The common feature of any proposed model +is the introduction of additional degrees of freedom, whether in the gravitational or the matter–energy Lagrangian. +Several approaches have been adopted: from the simple generalization of the Hilbert–Einstein action to functions +of the curvature scalar, namely f(R) theories [21–27], to the addition of further geometric invariants such as the +torsion scalar T [27–32] or the Gauss–Bonnet scalar G [33–36]. The introduction of scalar/vector fields minimally or +non-minimally coupled to gravity [37–41], as well as the emergence of non-trivial dynamics in the dark sector [42–46], +also represent intriguing possibilities in the extremely wide framework of the alternatives to GR/ΛCDM (see [47, 48] +for the state of the art). In this paper, we want to inquire into a specific class of alternative cosmological models +ruled by non-local gravitational interactions [49]. Among others, we investigate the cosmological implications of two +non-locally extended theories of gravity: the Deser–Woodard (DW) model [50] and the Ricci-Transverse (RT) model +[51]. These theories have drawn increasing attention in recent years due to their capability to account for late-time +cosmic acceleration, thus avoiding the introduction of any form of unknown dark energy. Moreover, the non-local +corrections may provide a viable mechanism to alleviate some of the main cosmological tensions. +The paper is organized as follow: in Section II, we outline the main motives for formulating non-local theories +of gravity, and we present the two ways in which dynamical non-locality can be implemented. Then, we introduce +the two chosen models and their theoretical features. In Section III, we investigate the mechanisms through which +the DW and the RT model account for the accelerated expansion of the Universe. In Section IV, we present the +non-locally driven evolution of cosmological perturbations for the two models and the resulting impact on the σ8 +tension. Moreover, in Section V, we assess the H0 tension in light of the non-local theories. Finally, in Section VI, +we present the main astrophysical tests of the non-local gravity models. The conclusions are drawn in Section VII. +II. +NON-LOCAL GRAVITY +Non-locality naturally emerges in Quantum Physics, both as a kinematical and a dynamical feature. On the other +hand, locality is a key property of classical field theories, and thus represents one of the main obstacles to overcome +in order to merge gravitational interaction formalism with that of Quantum Field Theory (QFT). As a consequence, +the introduction of non-locality in our theory of gravitation seems to be an unavoidable step towards the unification +of the fundamental interactions. +There exist at least two ways to achieve non-locality: at fundamental level, in +which kinematical non-locality can be implemented by discretizing spacetime and introducing a minimal length scale +(usually the Planck length); as an effective approach, in which non-local geometrical operators can be added to the +gravitational Lagrangian to obtain a non-local dynamics in a continuum background spacetime [52]. Here, we want +to focus on the latter scenario, which is of great interest for cosmological applications. +Two main classes of non-locally extended theories of gravity have been developed in recent years [49]: Infinite +Derivative theories of Gravity (IDGs), involving entire analytic transcendental functions of a differential operator, +and Integral Kernel theories of Gravity (IKGs) based on integral kernels of differential operators, such as +□−1R(x) = +� +d4x′G(x, x′)R(x′) , +(2.1) +where G(x′x′) is the Green function associated to the inverse d’Alembertian. IDGs usually address the ultraviolet (UV) +problems of the ΛCDM model by ensuring classical asymptotic freedom. The gravitational interaction is weakened +on small scales and the singularities disappear accordingly. Non-singular black holes [53], as well as inflationary [54] +and bouncing cosmologies [55], are indeed forecast in the IDG framework. On the other hand, IKGs are introduced +to account for the infrared (IR) shortcomings of the concordance model of cosmology. The phenomenology of both +dark fluids can be actually reproduced by non-local corrections that switch on at large scales [50, 56, 57]. +In this paper, we focus on two specific curvature-based IKGs [50, 51] and their cosmological features. IKGs indeed +have special relevance due to the fact that they combine suitable cosmological behavior with well-justified Lagrangians +at the fundamental level. GR is actually plagued by quantum IR divergences that already appear for pure gravity in +flat space [58]. This pathological behavior implies that the long-range dynamics of the gravitational interaction may +be non-trivial, and non-perturbative techniques are thus required. Applying such non-perturbative methods to the +renormalization of the quantum effective action of the gravity theory, non-local terms emerge both associated [59, 60] +or not associated [61, 62] to a dynamical mass scale. Analogous results can be recovered through the trace anomaly +[63]. + +3 +A. +The Deser–Woodard Model +The first model that we want to highlight is an IKG initially proposed in [50]. The non-locally extended gravitational +action of the Deser–Woodard model reads +S = +1 +16πG +� +d4x√−g +� +R +� +1 + f(□−1R) +�� +, +(2.2) +where the non-local correction is given by the so-called distortion function, namely a general function of the inverse +box of the Ricci scalar, as in Equation (2.1).It is worth noticing that the non-local theory reduces to GR as soon as +f(□−1R) vanishes. The modified field equations descending from Equation (2.2) are +Gµν + ∆Gµν = κT (m) +µν +, +(2.3) +where the non-local correction reads +∆Gµν = +� +Gµν + gµν□ − ∇µ∇ν +�� +f +� +□−1R +� ++ □−1� +Rf ′� +□−1R +��� ++ +� +1 +2 +� +δα +µδβ +ν + δβ +µδα +ν +� +− 1 +2gµνgαβ +� +∂α +� +□−1R +� +∂β +� +□−1� +Rf ′� +□−1R +��� +. +(2.4) +Furthermore, the non-local gravitational action in Equation (2.2) can be easily rewritten under the standard of +local scalar–tensor theories by introducing an auxiliary scalar field +R(x) = □η(x) , +(2.5) +which does not carry any independent degree of freedom. +The local canonical form of the scalar–tensor action, +equivalent to the non-local theory, thus reads [64] +S = 1 +2κ +� +d4x√−g +� +R +� +1 + f +� +η +�� +− ∂µξ∂µη − ξR +� +, +(2.6) +where ξ(x) is a Lagrangian multiplier which has been promoted to a position- and time-dependent scalar field. In this +formulation, the gravitational field equation is +Gµν = +1 +1 + f(η) − ξ +� +κT (m) +µν +− 1 +2gµν∂αξ∂αη + 1 +2 +� +∂µξ∂νη + ∂µη∂νξ +� +− +� +gµν□ − ∇µ∇ν +�� +f(η) − ξ +� +� +, +(2.7) +while the Klein–Gordon equations for the two auxiliary scalar fields are +□η = R , +(2.8) +□ξ = −R∂f(η) +∂η +. +(2.9) +B. +The Ricci-Transverse Model +The second non-local model that we investigate through this paper is a metric IKG proposed in [51]. This is a +quantum-inspired model, whose quantum effective action is +Γ = +1 +64πG +� +d4x +� +hµνEµν,αβhαβ − 2 +3m2� +P µνhµν +�2 +� +, +(2.10) + +4 +where gµν = ηµν+κhµν is the linearized metric tensor, Eµν,αβ is the Lichnerowicz operator1, P µν = ηµν−(∂µ∂ν/□) is a +projector operator and m is the mass of the conformal mode of the gravitational field. Performing the covariantization +of Equation (2.10), the modified gravitational field equation reads +Gµν − 1 +3m2(gµν□−1R)T = κTµν , +(2.11) +where we take the transverse part of the symmetric non-local tensor Sµν = gµν□−1R +Sµν = ST +µν + 1 +2(∇µSν + ∇νSµ) , +(2.12) +and Sµ is an associated four-vector. The Bianchi identities are guaranteed accordingly, i.e., ∇µST +µν = 0. +In the same way as the DW model, the Ricci-Transverse model can be localized through a scalar–tensor–vector +formulation [51, 65]. Here, we introduce two auxiliary objects, namely +U(x) = −□−1R(x) , +Sµν(x) = −U(x)gµν(x) = gµν(x)□−1R(x) . +(2.13) +An auxiliary four-vector field Sµ(x) therefore enters the localized equations because of Equation (2.12). +The +gravitational field equation, Equation (2.11), turns into +Gµν + m2 +6 +� +2Ugµν + ∇µSν + ∇νSµ +� += κTµν +(2.14) +plus the two equations of motions of the two auxiliary fields +□U = −R , +(2.15) +� +δµ +ν □ + ∇µ∇ν +� +Sµ = −2∂νU . +(2.16) +III. +THE LATE-TIME COSMIC ACCELERATION +The Universe is currently undergoing an accelerated expansion. The first evidence of this peculiar behavior dates +back to the end of the twentieth century, when the observation of several Type Ia Supernovae (SNIa) [3, 4] pointed out +the unavoidable necessity of a cosmological constant to fit the cosmic expansion history. On the one hand, these results +have been corroborated by the observations of all the recent surveys [5, 66–68]. On the other hand, the theoretical +explanation of this issue has two main drawbacks: the fine tuning problem [69] and the coincidence problem [70]. The +former is related to the huge discrepancy (∼120 orders of magnitude) between the observed value of the cosmological +constant and the vacuum energy density calculated via QFT. The latter is linked with the similar current values of +ΩΛ and ΩM, despite their radically different evolution laws. +The next generation of cosmological surveys should boost the investigation of the nature of the so-called cosmological +constant, providing powerful data to discriminate between DE solutions and extended theories of gravity. Within this +framework, non-local gravity provides viable mechanisms that could account for the observed accelerated expansion +of the Universe. +1 Eµν,αβ = 1 +2 (ηµρηνσ + ηµσηνρ − 2ηµνηρσ)□ + (ηρσ∂µ∂ν + ηµν∂ρ∂σ) − 1 +2 (ηµρ∂σ∂ν + ηνρ∂σ∂µ + ηµσ∂ρ∂ν + ηµσ∂ρ∂µ) + +5 +A. +The DW Case: Delayed Response to Cosmic Events +The main reason why the DW model has been in the spotlight since its formulation is its effective way to explain +late-time cosmic acceleration without the introduction of any form of dark energy. Computing the non-local correction +of Equation (2.2) in the Friedmann–Lemaitre–Robertson–Walker (FLRW) metric, +ds2 = −dt2 + a2(t)d⃗x · d⃗x , +(3.1) +one obtains a non-negligible geometrical contribution, +� +□−1R +� +(t) = +� t +0 +dt′ +1 +a3(t′) +� t′ +0 +dt′′a3(t′′)R(t′′) = −6s(2s − 1) +3s − 1 +� +�ln +� +t +teq +� +− +1 +3s − 1 + +1 +3s − 1 +� +teq +t +�3s−1� +� , +(3.2) +where a(t) ∼ t s, and the integration constant is set to make the non-local correction vanish before the radiation– +matter equivalence time, teq. Then, for t > teq the non-local correction starts to grow, becoming non-negligible at +late time and driving the accelerated cosmic expansion. Non-locality thus emerges in the cosmological framework as +a delayed response to the radiation-to-matter dominance transition, i.e., as a time-like non-local effect. +The introduction of non-locality may therefore have beneficial effects on cosmological scales, both at background +level and perturbations level. Two different approaches can be adopted for the DW model: on the one hand, one can +exploit the freedom guaranteed by the undetermined form of the distortion function to fit the observed expansion +history of the universe. In such a scenario, the DW cosmology is made equivalent to ΛCDM at the background +level. However, different features emerge when perturbations are taken into account, and the physics of structure +formation is affected accordingly. On the other hand, one can select the form of the distortion function building on +some fundamental principles, such as the Noether symmetries of the system. In this case, the non-local cosmology is +also modified at background level and stronger deviations from the concordance model should rise. +In [71], the first method has been applied, and the ΛCDM expansion history of the Universe has been accurately +reproduced by matching the data through a non-trivial form of the distortion function +f(□−1R) = 0.245 +� +tanh +� +0.350X + 0.032X2 + 0.003X3� +− 1 +� +, +(3.3) +where X = □−1R + 16.5. +B. +The RT Case: Dynamical Dark Energy +Considering a spatially flat FLRW metric, Equation (3.1), the equations of motion of the RT model, Equa- +tions (2.14)–(2.16), become [72] +H2 − m2 +9 (U − ˙S0) = 8πG +3 +ρ , +(3.4) +¨U + 3H ˙U = 6 ˙H + 12H2 , +(3.5) +¨S0 + 3H ˙S0 − 3H2S0 = ˙U , +(3.6) +where the spatial components of the vector field Sµ vanish to preserve the rotational invariance of the FLRW metric, +and the stress–energy tensor is taken to be T µ +ν +=diag(−ρ, p, p, p). +Defining Y = U − ˙S0, ˜h = H/H0 and the +dimensionless variable x ≡ ln a(t), then the modified Friedmann equation, Equation (3.4), reads +˜h2(x) = ΩMe−3x + γY (x) , +(3.7) + +6 +with γ ≡ m2/(9H2 +0). An effective dark energy thus appears +ρDE(t) = ρ0γY (t) , +(3.8) +where ρ0 = 3H2 +0/(8πG). Once the initial conditions for the auxiliary fields are set (see [56] for details), the evolution +of ρDE(t)/ρT OT (t) can be studied: the non-local effective dark energy is actually negligible until recent time and then +starts to dominate the cosmic expansion. Moreover, it is possible to study the DE equation of state +˙ρDE + 3H(1 + ωDE)ρDE = 0 , +(3.9) +and different evolutions for ρDE(z) follow from different choices for the initial conditions of the auxiliary fields. For +small values of the initial conditions, one obtains a fully phantom DE, namely ωDE(z) is always less than −1. For +large values of the initial conditions, ρDE(z) has a "phantom crossing" behavior, i.e., there is a transition from the +phantom regime to −1 < ωDE < 0 of about z ≃ 0.3. Regardless of the initial conditions, therefore, the non-local +model provides a dynamical DE density which drives the accelerated expansion of the Universe. +IV. +THE GROWTH OF PERTURBATIONS AND THE σ8 TENSION +Building on the primordial density fluctuations emerged from the inflation, cosmic structures have formed due +to gravitational instability. Studying the large-scale structure of the Universe and its evolution through the cosmic +epochs, it is possible to trace the growth of the so-called cosmological perturbations. +Associated to this observable, one of the main cosmological tensions has risen: the growth tension. It has come +about as the result of the discrepancy between the Planck value of the cosmological parameters ΩM and σ8 and those +from WL measurements, CC and RSD data. The former dynamical probes point towards lower values of the amplitude +(σ8) or the rate (fσ8 = [ΩM(z = 0)]0.55σ8) of growth of structures with respect to the CMB experiments, giving rise to +a 2−3σ tension [9, 11]. Moreover, the Planck 2018 value of the joint parameter S8 = σ8 +� +ΩM/0.3 (S8 = 0.834±0.016 +[5]) is confirmed by another recent CMB analysis by the ACT + WMAP collaboration (S8 = 0.840 ± 0.030 [66]), +thus erasing the possibility of a systematic error related to the excess of lensing amplitude measured by Planck [73]. +A 2.3σ tension emerges accordingly with both the original WL analysis of KiDS-450 [74] and KiDS-450 + VIKING +data [75], while updated constraints from the same datasets [76, 77] show greater discrepancies. +The same 2.3σ +tension also occurs with the data from DES’s first year release (DESY1) [78], while the combination of KiDS-450 + +VIKING + DESY1 weak lensing datasets results in a 2.5σ [79] or 3.2σ [80] tension depending on the analysis. The +most recent cosmic shear data release from both KiDS-1000 and DESY3 confirms the previous estimates [18, 81–84] +(S8 = 0.759+0.024 +−0.021 from KiDS-1000 [18]). Analogous results have been obtained with the 3 × 2 pt correlation function +analysis (cosmic shear correlation function, galaxy clustering angular auto-correlation function and galaxy–galaxy +lensing cross-correlation function) of KiDS-1000 + BOSS + 2dFLenS datset [85]. Additional results, in agreement +with those from WL surveys, have been achieved by number counting of galaxy clusters, using multiwavelength +datasets [19, 86–91]. Supplementary observational evidence for the weaker growth of structures is also given by the +exploitation of RSD data [20, 92–95]. +A. +The Deser–Woodard Evolution of Scalar Perturbations +To investigate the growth of structures in the non-local DW model, we select the phenomenological form of the +distortion function given by Equation (3.3). As a consequence, the non-local background evolution is made equivalent +to that of ΛCDM, and any deviation is enclosed in the cosmological perturbations. +Consider the field equations of the scalar–tensor equivalent of the DW model, Equations (2.7)–(2.9). Specializing +to the cosmological case by assuming the FLRW metric, Equation (3.1), the field equations now read +H2� +1 + f − ξ +� ++ H +� +f ′ ˙η − ˙ξ +� +− 1 +6 ˙η ˙ξ = 8πG +3 +ρ , +(4.1) +˙H +� +1 + f − ξ +� +− H +2 +� +f ′ ˙η − ˙ξ +� ++ 1 +2 ˙η ˙ξ + 1 +2 +� +f ′′ ˙η2 + f ′¨η − ¨ξ +� += −4πG(p + ρ) , +(4.2) + +7 +¨η + 3H ˙η = −6 +� ˙H + 2H2� +, +(4.3) +¨ξ + 3H ˙ξ = 6f ′� ˙H + 2H2� +, +(4.4) +where the former two are the (0,0) and the (1,1) component of Equation (2.7), while the latter two are the cosmological +formulation of Equations (2.8) and (2.9). +The linear perturbation equations have been derived in [96] for the scalar–tensor equivalent of the non-local theory, +and then analogous results have been found in [97] for the original formulation. Using the perturbed FLRW metric +in the Newtonian gauge, +ds2 = −(1 + 2Ψ)dt2 + a2(t)(1 + 2Φ)δijdxidxj , +(4.5) +the growth equation reads +¨δM + (2 − ξ) ˙δM = +3H2 +0 +� +1 − ξ − 8f ′(η) + f(η) +� +Ω0 +M +2a3H2� +1 − ξ − 6f ′(η) + f(η) +�� +1 + f(η) − ξ +� δM , +(4.6) +where δM = δρM/ρM is the matter density perturbation in the sub-horizon limit. +Numerical results for the growth rate fσ8 ≡ σ8δ′ +M/δM have been obtained in [96] and [97] for both the formulations +of the Deser–Woodard model, and good agreement with the Redshift Space Distortion (RSD) data has emerged +(σNL +8 += 0.78). Moreover, when the DW cosmological parameters are inferred by matching the CMB data [98], a lower +growth amplitude with respect to that of ΛCDM turns out. The non-local model thus alleviates the growth tension, +predicting compatible values of σ8 both from Planck–CMB and the other dynamical probes, as shown in Figure 1. +However, even though the non-local clustering of linear structures is weakened with respect to ΛCDM, and the DW +prediction for the matter power spectrum is about 10% lower [98], the non-local lensing response is counterintuitively +enhanced due to a severe increase in the lensing potential. This peculiar behavior results in a slight tension between +CMB and RSD [98]: performing the joint fit, the RSD dataset tends to push the DW predictions for the CMB lensing +potential Cφφ +ℓ +out of the 1σ error bars at low-ℓ. Applying the Bayesian tools for the model selection, a “weak evidence” +[103] for the ΛCDM model consequently emerges. +B. +The Ricci-Transverse Evolution of Scalar Perturbations +The scalar perturbations of the RT model have been investigated in [56, 104], using the FLRW metric in the +Newtonian gauge, Equation (4.5), and perturbing the auxiliary fields as +U(t, x) = ¯U(t) + δU(t, x) , +(4.7) +Sµ(t, x) = ¯S0(t) + δSµ(t, x) = ¯S0(t) + δS0(t, x) + ∂i +� +δS(t, x) +� +, +(4.8) +where the spatial part of the vector perturbation does not vanish and, for scalar perturbations, only depends on +δS. Building on the RT cosmological equations Equations (3.4)–(3.6), the growth equation for the matter density +perturbation in the sub-horizon limit reads [104] +¨δM + 2H ˙δM = 3 +2 +Geff +G +H2 +0ΩMδM , +(4.9) +where in Geff +� +Ψ, Φ, δU, δS0, S +� +is encoded the deviation of the non-local theory from GR. In the sub-horizon modes, +namely ˆk ≫ 1, such deviation is + +8 +0.70 +0.75 +0.80 +0.85 +S8 +CMB Planck (DW non-local) +CMB Planck + RSD + JLA (DW non-local) +CMB Planck + BAO + Pantheon (RT-minimal non-local) +CMB Planck + BAO + Pantheon (RT non-local, ΔN=64) +CMB Planck TT,TE,EE + lowE +CMB ACT + WMAP +WL KiDS-1000 +WL DES-Y3 +WL CFHTLenS +WL KiDS + VIKING + DES-Y1 +WL + CMB lensing DES-Y3 + SPT + Planck +WL + GC KiDS-1000 3×2pt +WL + GC DES-Y3 3×2pt +WL + GC KiDS + VIKING-450 + BOSS +GC BOSS + eBOSS +GC BOSS power spectra +GC + CMB lensing DESI + Plank +CC AMICO KiDS-DR3 +CC SDSS-DR8 +CC Planck tSZ +RSD + BAO + Pantheon +RSD +RSD +0.70 +0.75 +0.80 +0.85 +S8 +FIG. 1: Estimates of S8 provided by the two non-local cosmological analyses [56, 98], and the ΛCDM fit of the CMB [5, 66], +the WL data [18, 20, 80, 83, 84, 99], the combination of WL and galaxy clustering observations [100–102], cluster counting +[19, 87, 88] and RSD surveys [92, 94]. The colored band corresponds to the S8 value derived by the analysis of the Planck–CMB +data in the ΛCDM framework [5]. +1 − Geff +G += O +� 1 +ˆk2 +� +, +(4.10) +and the RT model is thus safe regarding the time variation of the effective Newton’s constant. Geff indeed reduces +to G at the Solar System scale, while a deviation of ∼1% rises at cosmological scales. +In [56], the growth rate f(z, k) ≡ d ln δM/d ln a is also derived. The results do not differ from those of ΛCDM +cosmology: f(z, k) can be fitted with a k-independent function f(z) = [ΩM(z)]γ, where γ ≃ 0.55 is roughly constant. +Accordingly, any possible deviation in the growth of perturbations should be due to the amplitude σ8. In order to find +any signature of the non-local model at perturbation level, which could account for the growth tension, the theory was +compared with cosmological observations: Planck–CMB, Pantheon SNIa and SDSS-BAO. The Bayesian parameter +estimation shows a full equivalence between the RT non-local cosmology and the ΛCDM one. No statistically signifi- +cant deviation in the σ8 parameter emerges for any of the tested versions of the Ricci-Transverse model. Eventually, +this theory cannot alleviate the growth tension, as shown in Figure 1. +V. +HUBBLE TENSION IN LIGHT OF THE NON-LOCAL MODELS +Hubble tension is certainly the most renowned and significant tension of the ΛCDM model. It emerges from the +comparison between early-time and late-time measurements of the Hubble constant. From one side, CMB analysis +[5, 66, 105–108], BAO surveys [6, 101, 109, 110] with standard BBN constraints [111] and combinations of CMB, +BAO, SNIa [112], RSD and cosmic shear data [78, 113, 114] point towards lower values of H0 (H0 = 67.4 ± 0.5 km +s−1Mpc−1 from Planck 2018 [5]). On the other side, the local measurements based on standard candles prefer higher +values for the Hubble constant [115] (H0 = 73.04 ± 1.04 km s−1Mpc−1 from SH0ES 2022 [17]). The main results are +achieved by the SH0ES collaboration using Hubble Space Telescope observations: on the one hand, they analyzed + +9 +65 +70 +75 +80 +H0 ( km s-1 Mpc-1 ) +CMB Planck (DW non-local) +CMB Planck + RSD + JLA (DW non-local) +CMB Planck + BAO + Pantheon (RT-minimal non-local) +CMB Planck + BAO + Pantheon (RT non-local, ΔN=64) +CMB Planck +CMB Planck + lensing +SPT-3G CMB +ACT + WMAP CMB +Planck + SPT + ACT CMB +BOSS correlation function + BAO + BBN +BOSS power spectrum + BAO + BBN +BOSS DR12 + BBN +BAO + RSD +LSS equivalence-time ruler +LSS equivalence-time ruler + lensing +SNIa-Cepheid +SNIa-TRGB +SNIa-Miras +SneII +SnIa-Cepheid + TD lensing +Time-delay lensing +Time-delay lensing +Time-delay lensing + SLACS +GW Standard Sirens +GW Standard Sirens +GW Standard Sirens +Masers +Masers +Tully Fisher +Surface Brightness Fluctuations +0.70 +0.72 +0.74 +0.76 +0.78 +0.80 +S8 +FIG. 2: Estimates of H0 provided by the two non-local cosmological analyses [56, 98], and the ΛCDM fit of the CMB [5, 66, +105, 107], the matter power spectrum combined with BAO [20, 110, 126] and RSD [127], the Large Scale Structure teq standard +ruler [128, 129], the supernovae [17, 121, 124, 130, 131], the time-delay lensing [121, 132, 133], the gravitational waves [134–136], +the water megamasers [125, 137], the Tully–Fisher relation [138] and the SBF [139]. The colored bands correspond to the H0 +estimates derived by the Planck–CMB analysis in the ΛCDM framework (purple) [5] and the SNIa–Cepheids analysis by SH0ES +(orange) [17]. +SNIa data with distance calibration by Cepheid variables in the host galaxies [116, 117]; on the other hand, they +targeted long-period pulsating Cepheid variables [17, 118], calibrating the geometric distance to the Large Magellanic +Cloud, both from eclipsing binaries and parallaxes from the Gaia satellite [119, 120]. Moreover, other independent +local measurement of H0 have been performed by using time delays between multiple images of strong lensed quasars +[121, 122], the tip of the Red Giant Branch [123] and Miras (variable red giant stars) [124] with water megamaser as +distance indicator [125]. All these measurements agree on higher values of the Hubble constant, thus generating a +4 − 5σ tension with early-time model-dependent estimates. +A. +The Deser–Woodard Expansion History +The stat-of-the-art investigation of the DW non-local model does not allow any attempt to address H0 tension. To +make the model predictive, the form of the distortion function needs to be specified, and most of the analyses have +been focused on the phenomenological ΛCDM form of Equation (3.3), until now (see [98] for the latest results). This +choice implies that the DW cosmology is made equivalent to that of the concordance model at background level, and +the same expansion history, as well as the same H0, are thus predicted (see Figure 2). +However, another option is also available for the selection of the distortion function. In [57, 140, 141], a specific +form of f(η) has been derived by exploiting the Noether symmetries [142] of a spherically symmetric background +spacetime +f(η) = 1 + e η . +(5.1) +The accurate cosmological analysis of this form of the DW model has yet to be carried out, but some results have +already been achieved, such as exact solutions [49] and a phase-space view of solutions [143]. Furthermore, several + +10 +astrophysical tests have been performed on very different scales, and viable results turned out. In [141], the lensing +properties of the galaxy clusters have been investigated in light of the exponential DW model, and a fully non-local +regime with enhanced lensing strength has been highlighted. This feature clearly resembles the improved lensing +response of the phenomenological form of the DW model, which is co-responsible for the lowered estimate of the σ8 +parameter. A promising insight upon the cosmological behavior of the non-local theory based on Equation (5.1) thus +emerges. Therefore, this model may alleviate not only the growth tension but also the Hubble tension, since it also +deviates from GR at the background level [144]. Further analysis of the exponential DW model should be carried out +accordingly. +B. +The Ricci-Transverse Expansion History +For what concerns the RT model, the most updated cosmological analysis is due to Belgacem et al. [56]. As we +saw in Section IV, different versions of the non-local model, relying on different choices for initial conditions of the +auxiliary fields, have been compared against Planck–CMB, Pantheon SNIa and SDSS-BAO data. Since the RT model +has no freedom with regard to the functional form of the action, the theory cannot be adjusted to data, and no +background equivalence to the ΛCDM cosmology can be established a priori. In such a scenario, the solution to the +Hubble tension may thus be possible. However, the estimator tool defined in Equation (4.10), which accounts for +the deviation from GR of the non-local theory, only shows little discrepancies. This manifests in the values of the +cosmological parameters inferred via Markov Chain Monte Carlo (MCMC), which are almost equivalent to those of +the concordance model. The only model that exhibits some slight discrepancies is the so-called "RT-minimal", which +relies on the assumption that the auxiliary scalar field U(x) starts its evolution during the radiation dominance era. +On the one hand, this model predict a non-vanishing value for the sum of neutrino masses, while the ΛCDM model +and the other versions of the RT model show a marginalized posterior which is peaked in zero. On the other hand, +the RT-minimal model provides a barely higher estimate of the Hubble constant, i.e., H0 = 68.74+0.59 +−0.51 km s−1Mpc−1. +Accordingly, the Hubble tension is just reduced to ∼4σ, as shown in Figure 2. +The RT model in its minimal setup thus provides a viable mechanism to account for the late-time cosmic acceleration, +as well as for the inclusion of non-zero neutrino masses. However, the predictions for both the background evolution +and the linear perturbations are too similar to that of the ΛCDM model, hence the cosmological tensions cannot be +alleviated. +VI. +ASTROPHYSICAL TESTS OF NON-LOCAL GRAVITY +As we saw, good cosmological behavior emerges for both of the non-local models, thus enabling the possibility to +avoid the introduction of any form of unknown dark energy. In order to further investigate the viability of such models +as alternatives to GR, it is then necessary to test the non-local predictions down to astrophysical scales. Moreover, +an accurate investigation of the possible screening mechanisms should be performed, if necessary. +A. +Testing the Deser–Woodard Model by Galaxy Clusters, Elliptical Galaxies and the S2 Star +The DW model has been tested on a wide range of astrophysical scales, from the galaxy clusters [141] to the stellar +orbits around Sagittarius A* [140]. Most of the tests have been carried out for the exponential form of the non-local +model, namely +S = 1 +2κ +� +d4x√−g +� +R +� +2 + e η� +− ∂µξ∂µη − ξR +� +, +(6.1) +where the distortion function has been picked out by exploiting the Noether Symmetry Approach [145]. The analyses +presented are all performed in the post-Newtonian limit, hence the non-local gravitational and metric potential are +φ(r) = − GMηc +r ++ G2M 2 +2c2r2 +� +14 +9 η2 +c + 18rξ − 11rη +6rηrξ +r +� +− G3M 3 +2c4r3 +� +50rξ − 7rη +12rηrξ +ηcr + 16 +27η3 +c − +2r2 +ξ − r2 +η +r2ηr2 +ξ +r2 +� +, +(6.2) +ψ(r) = −GMηc +3r +− G2M 2 +2c2r2 +� +2 +9η2 +c + 3rη − 2rξ +2rηrξ +r +� +, +(6.3) + +11 +where ηc is set to 1 so as to recover GR in the limit of φ(r). The two length scales rη and rξ are the characteristic +non-local parameters that define the scale at which the non-local gravity corrections become effective. +The first test of this form of the DW model has been carried out in [140], where the weak field non-local predictions +have been compared against the NTT/VLT observations of S2 star orbit [146]. Exploiting a modified Marquardt– +Levenberg algorithm, the fit between the simulated orbit and the observed one has shown a slightly better agreement +for the non-local model with respect to the Keplerian orbit. Moreover, some constraints have been set on the non-local +length scales. +A further test has been subsequently performed in [141], exploiting the CLASH lensing data from 19 massive clusters +[147, 148]. The point-mass potentials of Equations (6.2) and (6.3) were extended to a spherically symmetric mass +distribution, i.e., the Navarro–Frenk–White density profile, and the non-local predictions for the lensing convergence +were achieved. Therefore, the MCMC analysis has highlighted two effective regimes in which the non-local model +is able to match the observations at the same level of statistical significance as GR. In the high-value limit of the +non-local parameters, the non-local model reduces to a GR-like theory, whose lensing strength is 2/3 of the standard +one. In this scenario, the DW theory is thus able to fit the data at the cost of increased cluster mass estimates. +On the other hand, approaching the low-value limit of the non-local length scales, the non-local corrections to the +lensing potential become larger and comparable to the zeroth-order terms. In this regime, the non-local model is +able to reproduce GR phenomenology, neither affecting the mass estimates nor the statistical viability of the model. +Furthermore, when the non-local contributions becomes completely dominant, the non-local theory seems to be able +to fit the lensing observations with extremely low cluster masses. Accordingly, an intriguing possibility to fit data +with no dark matter emerges. Additional constraints on the non-local parameters were also derived. +The most recent astrophysical test of the exponential-DW model was carried out in [57], using the velocity distri- +bution of elliptical galaxies [149]. Computing the non-local velocity dispersion as a function of the galaxy effective +radius, the empirical relation of the so-called Fundamental Plane has been recovered so as to constrain the non-local +gravity parameters. The results of the fit highlight the possibility to recover the fundamental plane without the dark +matter hypothesis, setting new constraints for rη and rξ. +It is worth noticing, however, that the non-local Deser–Woodard model exhibits worrisome features at the scale of +the Solar System. Indeed, in [150], it was demonstrated that the screening mechanism proposed by the same authors +of the non-local model does not work. As a consequence, the DW model would show a time dependence of the effective +Newton constant in the small-scale limit, and it would be ruled out by Lunar Laser Ranging (LLR) observations. This +conclusion, however, seems to be too strong, since it is still not clear how an FLRW background quantity behaves +when evaluated from cosmological scales down to Solar System ones, where the system decouples from the Hubble +flow. In fact, a full non-linear time- and scale-dependent solution around a non-linear structure would be necessary. +A number of proposals go in this direction, and the so-called Vainshtein mechanism [151] can be regarded as the +paradigm to realize the screening. Basically, any screening mechanism requires a scalar field coupled to matter and +mediating a fifth force which might span from Solar System up to cosmological scales. Since non-local terms can be +“localized”, thus resulting in effective scalar fields depending on the scale, some screening mechanism could naturally +emerge so as to solve the above reported problems. +B. +Testing the Ricci-Transverse Model by Solar System Observations and Gravitational Waves Detection +The main astrophysical tests of the RT model are related to Solar System observations. As we saw in the previous +sub-section, any theory that extends GR has to reduce to Einstein’s theory at small scales. However, this is highly +non-trivial when additional degrees of freedom are included, and screening mechanisms involving non-linear features +are required. The RT model, instead, smoothly reduces to GR already at linear level, and no vDVZ discontinuity +arises when m → 0 [56]. Note that such results are valid both in the flat and the Schwarzschild spacetime. Moreover, +the non-local model passes the LLR test about the time variation of the effective Newton constant [150]. As stated +in Equation (4.10), indeed, the deviation parameter Geff reduces to GN as soon as the system’s characteristic scale +decreases. +Another non-local feature of the RT model that has been investigated is the deviation from GR of the predicted +gravitational radiation [152, 153]. The RT model, similarly to some other extended theories of gravity such as f(R) +gravity and DHOST theories, has survived the GW170817 event, which set a stringent constraint on the Gravitational +Waves (GW) speed [154]. Indeed, this non-local model only modifies the friction term in the GW propagation equation, +thus predicting a massless graviton. Moreover, neither the coupling with matter nor the gravitational interaction +between the coalescing binaries are affected (the RT model reduces to GR at short distances), and the only difference +will therefore be due to the free propagation of the GW from the source to the observer. The GW amplitude indeed +undergoes a modified dampening in the non-local model + +12 +˜hA(η, k) ∼ +1 +dgw +L (z) = +� +dem +L (z) exp +� +− +� z +0 +dz′ +1 + z′ δ(z′) +��−1 +, +(6.4) +where +δ(η) = m2 ¯S0(η) +6H(η) , +(6.5) +and ˜hA(η, k) are the Fourier modes of the GW amplitude, with A = ×, + labeling the polarization. Computing +the ratio between the non-local behavior given by Equation (6.4) and the GR behavior, ˜hA(η, k) ∼ 1/dem +L (z), little +deviation emerges for the RT-minimal model, while a 20−80% deviation manifests at large z for the RT formulations +in which the auxiliary fields start their evolution during the de Sitter inflation. The more e-folds we consider between +the onset of the auxiliary fields and the end of the inflation, the greater the deviation from GR. We can use a simple +parametrization for the considered ratio +dgw +L (z) +dem +L (z) = Ξ0 + 1 − Ξ0 +(1 + z)n , +(6.6) +where Ξ0 is the asymptotic value reached by the ratio and n is the rate at which Ξ0 is approached. Then, +δ(z) = +δ(0) +1 − Ξ0 + Ξ0(1 + z)n , +(6.7) +with δ(0) = n(1 − Ξ0), and the event GW170817 provided the following constraint for such a parameter [153]: +δ(0) = −7.8+9.7 +−18.4. +More stringent constraints will certainly be set with the next generation of GW detectors by +exploiting the observations of GW events with electromagnetic counterparts. +VII. +CONCLUSIONS AND PERSPECTIVES +In this paper, we reviewed the cosmological properties of two of the main proposals in the framework of the non- +locally extended theories of gravity. In particular, we considered two metric IKGs that are inspired by quantum +corrections and manifest a suitable cosmological behavior as well. Both the DW and RT models are able to reproduce +the expansion history of the Universe, exhibiting a late-time accelerated expansion driven by the onset of the non-local +corrections. The non-local extensions of the Hilbert–Einstein Lagrangian thus provide a viable mechanism to avoid +the introduction of any form of unknown dark energy. Building on these appealing properties, we inquired into the +chance of addressing the two main cosmological tensions, namely the σ8 and H0 tensions. +On the one hand, the non-local DW model has shown suitable features towards this aim. The phenomenological +formulation of the model indeed predicts a lowered amplitude of growth of perturbations, therefore solving the σ8 +tension. However, this model is made equivalent to the ΛCDM cosmology at the background level, hence no chance +to account for the Hubble tension arises. Another formulation of the DW theory, based on the Noether symmetries +of the system, may address both the tensions. This model lacks a proper cosmological analysis, but the investigation +of its lensing properties at the galaxy clusters scale has shown the same features that, in the phenomenological DW +model, allow the weakening of the growth of structures. Moreover, this formulation of the non-local theory deviates +from GR also at background level, thus enabling the possibility to alleviate the Hubble tension as well. The model has +been also tested on astrophysical scales, and substantial statistical equivalence to GR has emerged in very different +systems, such as the S2 star, the elliptical galaxies and the galaxy clusters. The main drawback of the DW model, +however, is the absence of an effective screening mechanism on small scales, which has to be further investigated. +On the other hand, the non-local RT model perfectly reduces to GR at the Solar System scale, thus avoiding the +necessity of non-trivial screening mechanisms. Accordingly, the model is not ruled out by the LLR test. Moreover, the +non-minimal formulations of the RT model show a strong deviation from GR for what concerns the GW propagation +at large redshift. A powerful tool to test the model with the next generation of GW detectors thus emerges. However, +this non-local model is not able to address any of the cosmological tensions, as it mimics the ΛCDM evolution both +at the background and linear perturbations level. + +13 +In view of the fact that the next generation of cosmological surveys are expected to provide sufficiently accurate +data to reach a turning point in our comprehension of the Universe, it is of great interest to further investigate the +main alternatives to GR. A complete cosmological analysis should especially be carried out for the non-local DW +model in its formulation based on the Noether Symmetry Approach. This model indeed provides one of the most +promising windows towards the solution of both the cosmological tensions and the dark energy problem. The large- +scale structure especially appears as a privileged environment for testing the non-local models, since one of their main +features is the emergence of characteristic length scales. However, it must be stressed that as long as no screening +mechanism will be found for the DW model, its reliability will be compromised. +Acknowledgments +This article is based upon work from COST Action CA21136 Addressing observational tensions in cosmology +with systematic and fundamental physics (CosmoVerse) supported by COST (European Cooperation in Science and +Technology). FB and SC acknowledge the support of Istituto Nazionale di Fisica Nucleare (INFN), iniziative specifiche +QGSKY and MOONLIGHT2. +Appendix A: Abbreviations +The following abbreviations are used in this manuscript: +BBN +Big Bang Nucleosynthesis +BAO +Baryon Acoustic Oscillations +ΛCDM Lambda Cold Dark Matter +GR +General Relativity +DE +Dark Energy +DM +Dark Matter +CMB +Cosmic Microwave Background +WL +Weak Lensing +CC +Cluster Counts +RSD +Redshift Space Distortion +DW +Deser–Woodard +RT +Ricci-Transverse +QFT +Quantum Field Theory +IDG +Infinite Derivative Theory of Gravity +IKG +Integral Kernel Theory of Gravity +UV +UltraViolet +IR +InfraRed +SNIa +Type Ia Supernovae +FLRW Friedmann–Lemaitre–Robertson–Walker +MCMC Markov Chain Monte Carlo +LLR +Lunar Laser Ranging +GW +Gravitational Waves +[1] Hogg, D.W.; Eisenstein, D.J.; Blanton, M.R.; Bahcall, N.A.; Brinkmann, J.; Gunn, J.E.; Schneider, D.P. +Cosmic +homogeneity demonstrated with luminous red galaxies. Astrophys. 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J. 2017, 848, L13. https://doi.org/10.3847/2041-8213/aa920c. + diff --git a/EdAzT4oBgHgl3EQfiv0h/content/tmp_files/load_file.txt b/EdAzT4oBgHgl3EQfiv0h/content/tmp_files/load_file.txt new file mode 100644 index 0000000000000000000000000000000000000000..2ad3c7b821f3d6e58c704d807e3193967efc6068 --- /dev/null +++ b/EdAzT4oBgHgl3EQfiv0h/content/tmp_files/load_file.txt @@ -0,0 +1,3644 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf,len=3643 +page_content='Addressing Cosmological Tensions by Non-Local Gravity Filippo Bouchè,1, a Salvatore Capozziello,1, 2, 3, b and V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Salzano4, c 1Dipartimento di Fisica “E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Pancini”, Università di Napoli “Federico II", Via Cinthia 21, I-80126, Napoli, Italy 2DipaScuola Superiore Meridionale, Largo S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Marcellino 10, I-80138, Napoli, Italy 3Istituto Nazionale di Fisica Nucleare, Sez.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' di Napoli, Via Cinthia 21, I-80126, Napoli, Italy 4Institute of Physics, University of Szczecin, Wielkopolska 15, 70-451 Szczecin, Poland (Dated: January 5, 2023) Alternative cosmological models have been under deep scrutiny in recent years, aiming to address the main shortcomings of the ΛCDM model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, as the accuracy of cosmological surveys improved, new tensions have risen between the model-dependent analysis of the Cosmic Microwave Background and lower redshift probes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Within this framework, we review two quantum-inspired non-locally extended theories of gravity, whose main cosmological feature is a geometrically driven accelerated expansion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The models are especially investigated in light of the Hubble and growth tension, and promising features emerge for the Deser–Woodard one.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the one hand, the cosmolog- ical analysis of the phenomenological formulation of the model shows a lowered growth of structures but an equivalent background with respect to ΛCDM.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, the study of the lensing features at the galaxy cluster scale of a new formulation of non-local cosmology, based on Noether symmetries, makes room for the possibility of alleviating both the H0 and σ8 tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, the urgent need for a screening mechanism arises for this non-local theory of gravity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' INTRODUCTION Recent astrophysical and cosmological surveys, both from ground-based and space experiments, have provided extremely high-quality data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The observations point towards a Universe in which the cosmological principle holds on large scales, namely the Universe appears homogeneous and isotropic if averaged over scales of ∼100 h−1Mpc or more [1, 2].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, the Universe is undergoing an accelerated expansion phase [3, 4], subsequent to a decelerated era in which the structure formation occurred.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' All these features, together with the nuclei abundances produced in the Big Bang Nucleosynthesis (BBN), the Baryon Acoustic Oscillations (BAO) and many others, are well predicted by the Lambda Cold Dark Matter (ΛCDM) model, which has been adopted as the standard cosmological model accordingly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Such a model provides an effective description of the Universe, which relies on the assumption that General Relativity (GR) is the final theory of gravitation that governs the cosmic dynamics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As a consequence, two more fluids other than baryonic matter and radiation must be inserted in the matter–energy content of the Universe in order to adjust GR predictions to data: the Dark Energy (DE), responsible for the late time cosmic acceleration, and the Dark Matter (DM), which accounts for the structure formation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Together, they should represent ∼95% of the matter–energy budget of the Universe [5–7], thus dominating the cosmic dynamics at all scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Building on its capability to fit the whole cosmological and astrophysical dataset with a relatively small number of parameters, the ΛCDM model stands as the pillar of our comprehension of the Universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, several shortcomings [8] and recently risen tensions [9–11] affect its reliability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the one hand, we have a huge assortment of candidates but no final solution for DM [12, 13] and DE [14–16].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, the presence of singularities, as well as the inconsistency at quantum level, undermine the credibility of GR as the final theory of gravity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Even more puzzling are the cosmological tensions, which have emerged in recent years as the result of the growing availability of a wide range of extremely precise data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A multitude of independent observations appears indeed to be in a ≳2σ tension with the reference ΛCDM estimates by the Planck collaboration [5].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Even though systematic experimental errors may account for part of these tensions, their statistical significance and their persistence after several check analyses have thrown up some serious red flags.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Since the Planck constraints for the cosmological parameters relies on a strongly ΛCDM-model-dependent analysis of the Cosmic Microwave Background (CMB), such tensions may be the signature of the brakedown of the concordance model, hence of new physics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this paper, we pay particular attention to the two most well-known tensions: the H0 tension [10], which emerges from the comparison between early-time [5] and late-time measurements [17] of the Hubble constant, and the growth tension [11] between the CMB value [5] of the aElectronic address: filippo.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='bouche-ssm@unina.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='it bElectronic address: capozziello@na.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='infn.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='it cElectronic address: vincenzo.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='salzano@usz.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='edu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='pl arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='01503v1 [astro-ph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='CO] 4 Jan 2023 2 cosmological parameters ΩM and σ8 and those from lower redshift probes, such as Weak Lensing (WL) [18], Cluster Counts (CC) [19] and Redshift Space Distortion (RSD) [20].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In order to meet the challenges posed by ΛCDM theoretical shortcomings, as well as by its observational tensions, a zoo of alternative cosmological models has been formulated in recent years.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The common feature of any proposed model is the introduction of additional degrees of freedom, whether in the gravitational or the matter–energy Lagrangian.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Several approaches have been adopted: from the simple generalization of the Hilbert–Einstein action to functions of the curvature scalar, namely f(R) theories [21–27], to the addition of further geometric invariants such as the torsion scalar T [27–32] or the Gauss–Bonnet scalar G [33–36].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The introduction of scalar/vector fields minimally or non-minimally coupled to gravity [37–41], as well as the emergence of non-trivial dynamics in the dark sector [42–46], also represent intriguing possibilities in the extremely wide framework of the alternatives to GR/ΛCDM (see [47, 48] for the state of the art).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this paper, we want to inquire into a specific class of alternative cosmological models ruled by non-local gravitational interactions [49].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Among others, we investigate the cosmological implications of two non-locally extended theories of gravity: the Deser–Woodard (DW) model [50] and the Ricci-Transverse (RT) model [51].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' These theories have drawn increasing attention in recent years due to their capability to account for late-time cosmic acceleration, thus avoiding the introduction of any form of unknown dark energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, the non-local corrections may provide a viable mechanism to alleviate some of the main cosmological tensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The paper is organized as follow: in Section II, we outline the main motives for formulating non-local theories of gravity, and we present the two ways in which dynamical non-locality can be implemented.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Then, we introduce the two chosen models and their theoretical features.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In Section III, we investigate the mechanisms through which the DW and the RT model account for the accelerated expansion of the Universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In Section IV, we present the non-locally driven evolution of cosmological perturbations for the two models and the resulting impact on the σ8 tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, in Section V, we assess the H0 tension in light of the non-local theories.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Finally, in Section VI, we present the main astrophysical tests of the non-local gravity models.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The conclusions are drawn in Section VII.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' II.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' NON-LOCAL GRAVITY Non-locality naturally emerges in Quantum Physics, both as a kinematical and a dynamical feature.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, locality is a key property of classical field theories, and thus represents one of the main obstacles to overcome in order to merge gravitational interaction formalism with that of Quantum Field Theory (QFT).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As a consequence, the introduction of non-locality in our theory of gravitation seems to be an unavoidable step towards the unification of the fundamental interactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' There exist at least two ways to achieve non-locality: at fundamental level, in which kinematical non-locality can be implemented by discretizing spacetime and introducing a minimal length scale (usually the Planck length);' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' as an effective approach, in which non-local geometrical operators can be added to the gravitational Lagrangian to obtain a non-local dynamics in a continuum background spacetime [52].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Here, we want to focus on the latter scenario, which is of great interest for cosmological applications.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Two main classes of non-locally extended theories of gravity have been developed in recent years [49]: Infinite Derivative theories of Gravity (IDGs), involving entire analytic transcendental functions of a differential operator, and Integral Kernel theories of Gravity (IKGs) based on integral kernels of differential operators, such as □−1R(x) = � d4x′G(x, x′)R(x′) , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) where G(x′x′) is the Green function associated to the inverse d’Alembertian.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' IDGs usually address the ultraviolet (UV) problems of the ΛCDM model by ensuring classical asymptotic freedom.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The gravitational interaction is weakened on small scales and the singularities disappear accordingly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Non-singular black holes [53], as well as inflationary [54] and bouncing cosmologies [55], are indeed forecast in the IDG framework.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, IKGs are introduced to account for the infrared (IR) shortcomings of the concordance model of cosmology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The phenomenology of both dark fluids can be actually reproduced by non-local corrections that switch on at large scales [50, 56, 57].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this paper, we focus on two specific curvature-based IKGs [50, 51] and their cosmological features.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' IKGs indeed have special relevance due to the fact that they combine suitable cosmological behavior with well-justified Lagrangians at the fundamental level.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' GR is actually plagued by quantum IR divergences that already appear for pure gravity in flat space [58].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This pathological behavior implies that the long-range dynamics of the gravitational interaction may be non-trivial, and non-perturbative techniques are thus required.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Applying such non-perturbative methods to the renormalization of the quantum effective action of the gravity theory, non-local terms emerge both associated [59, 60] or not associated [61, 62] to a dynamical mass scale.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Analogous results can be recovered through the trace anomaly [63].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 3 A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Deser–Woodard Model The first model that we want to highlight is an IKG initially proposed in [50].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The non-locally extended gravitational action of the Deser–Woodard model reads S = 1 16πG � d4x√−g � R � 1 + f(□−1R) �� , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) where the non-local correction is given by the so-called distortion function, namely a general function of the inverse box of the Ricci scalar, as in Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='It is worth noticing that the non-local theory reduces to GR as soon as f(□−1R) vanishes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The modified field equations descending from Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) are Gµν + ∆Gµν = κT (m) µν , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3) where the non-local correction reads ∆Gµν = � Gµν + gµν□ − ∇µ∇ν �� f � □−1R � + □−1� Rf ′� □−1R ��� + � 1 2 � δα µδβ ν + δβ µδα ν � − 1 2gµνgαβ � ∂α � □−1R � ∂β � □−1� Rf ′� □−1R ��� .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4) Furthermore, the non-local gravitational action in Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) can be easily rewritten under the standard of local scalar–tensor theories by introducing an auxiliary scalar field R(x) = □η(x) , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5) which does not carry any independent degree of freedom.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The local canonical form of the scalar–tensor action, equivalent to the non-local theory, thus reads [64] S = 1 2κ � d4x√−g � R � 1 + f � η �� − ∂µξ∂µη − ξR � , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='6) where ξ(x) is a Lagrangian multiplier which has been promoted to a position- and time-dependent scalar field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this formulation, the gravitational field equation is Gµν = 1 1 + f(η) − ξ � κT (m) µν − 1 2gµν∂αξ∂αη + 1 2 � ∂µξ∂νη + ∂µη∂νξ � − � gµν□ − ∇µ∇ν �� f(η) − ξ � � , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7) while the Klein–Gordon equations for the two auxiliary scalar fields are □η = R , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='8) □ξ = −R∂f(η) ∂η .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='9) B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Ricci-Transverse Model The second non-local model that we investigate through this paper is a metric IKG proposed in [51].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This is a quantum-inspired model, whose quantum effective action is Γ = 1 64πG � d4x � hµνEµν,αβhαβ − 2 3m2� P µνhµν �2 � , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='10) 4 where gµν = ηµν+κhµν is the linearized metric tensor, Eµν,αβ is the Lichnerowicz operator1, P µν = ηµν−(∂µ∂ν/□) is a projector operator and m is the mass of the conformal mode of the gravitational field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Performing the covariantization of Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='10), the modified gravitational field equation reads Gµν − 1 3m2(gµν□−1R)T = κTµν , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='11) where we take the transverse part of the symmetric non-local tensor Sµν = gµν□−1R Sµν = ST µν + 1 2(∇µSν + ∇νSµ) , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='12) and Sµ is an associated four-vector.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Bianchi identities are guaranteed accordingly, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=', ∇µST µν = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In the same way as the DW model, the Ricci-Transverse model can be localized through a scalar–tensor–vector formulation [51, 65].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Here, we introduce two auxiliary objects, namely U(x) = −□−1R(x) , Sµν(x) = −U(x)gµν(x) = gµν(x)□−1R(x) .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='13) An auxiliary four-vector field Sµ(x) therefore enters the localized equations because of Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='12).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The gravitational field equation, Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='11), turns into Gµν + m2 6 � 2Ugµν + ∇µSν + ∇νSµ � = κTµν (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='14) plus the two equations of motions of the two auxiliary fields □U = −R , (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='15) � δµ ν □ + ∇µ∇ν � Sµ = −2∂νU .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='16) III.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' THE LATE-TIME COSMIC ACCELERATION The Universe is currently undergoing an accelerated expansion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The first evidence of this peculiar behavior dates back to the end of the twentieth century, when the observation of several Type Ia Supernovae (SNIa) [3, 4] pointed out the unavoidable necessity of a cosmological constant to fit the cosmic expansion history.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the one hand, these results have been corroborated by the observations of all the recent surveys [5, 66–68].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, the theoretical explanation of this issue has two main drawbacks: the fine tuning problem [69] and the coincidence problem [70].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The former is related to the huge discrepancy (∼120 orders of magnitude) between the observed value of the cosmological constant and the vacuum energy density calculated via QFT.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The latter is linked with the similar current values of ΩΛ and ΩM, despite their radically different evolution laws.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The next generation of cosmological surveys should boost the investigation of the nature of the so-called cosmological constant, providing powerful data to discriminate between DE solutions and extended theories of gravity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Within this framework, non-local gravity provides viable mechanisms that could account for the observed accelerated expansion of the Universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 1 Eµν,αβ = 1 2 (ηµρηνσ + ηµσηνρ − 2ηµνηρσ)□ + (ηρσ∂µ∂ν + ηµν∂ρ∂σ) − 1 2 (ηµρ∂σ∂ν + ηνρ∂σ∂µ + ηµσ∂ρ∂ν + ηµσ∂ρ∂µ) 5 A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The DW Case: Delayed Response to Cosmic Events The main reason why the DW model has been in the spotlight since its formulation is its effective way to explain late-time cosmic acceleration without the introduction of any form of dark energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Computing the non-local correction of Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) in the Friedmann–Lemaitre–Robertson–Walker (FLRW) metric, ds2 = −dt2 + a2(t)d⃗x · d⃗x , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) one obtains a non-negligible geometrical contribution, � □−1R � (t) = � t 0 dt′ 1 a3(t′) � t′ 0 dt′′a3(t′′)R(t′′) = −6s(2s − 1) 3s − 1 � �ln � t teq � − 1 3s − 1 + 1 3s − 1 � teq t �3s−1� � , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) where a(t) ∼ t s, and the integration constant is set to make the non-local correction vanish before the radiation– matter equivalence time, teq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Then, for t > teq the non-local correction starts to grow, becoming non-negligible at late time and driving the accelerated cosmic expansion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Non-locality thus emerges in the cosmological framework as a delayed response to the radiation-to-matter dominance transition, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=', as a time-like non-local effect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The introduction of non-locality may therefore have beneficial effects on cosmological scales, both at background level and perturbations level.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Two different approaches can be adopted for the DW model: on the one hand, one can exploit the freedom guaranteed by the undetermined form of the distortion function to fit the observed expansion history of the universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In such a scenario, the DW cosmology is made equivalent to ΛCDM at the background level.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, different features emerge when perturbations are taken into account, and the physics of structure formation is affected accordingly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, one can select the form of the distortion function building on some fundamental principles, such as the Noether symmetries of the system.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this case, the non-local cosmology is also modified at background level and stronger deviations from the concordance model should rise.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In [71], the first method has been applied, and the ΛCDM expansion history of the Universe has been accurately reproduced by matching the data through a non-trivial form of the distortion function f(□−1R) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='245 � tanh � 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='350X + 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='032X2 + 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='003X3� − 1 � , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3) where X = □−1R + 16.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The RT Case: Dynamical Dark Energy Considering a spatially flat FLRW metric, Equation (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1), the equations of motion of the RT model, Equa- tions (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='14)–(2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='16), become [72] H2 − m2 9 (U − ˙S0) = 8πG 3 ρ , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4) ¨U + 3H ˙U = 6 ˙H + 12H2 , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5) ¨S0 + 3H ˙S0 − 3H2S0 = ˙U , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='6) where the spatial components of the vector field Sµ vanish to preserve the rotational invariance of the FLRW metric, and the stress–energy tensor is taken to be T µ ν =diag(−ρ, p, p, p).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Defining Y = U − ˙S0, ˜h = H/H0 and the dimensionless variable x ≡ ln a(t), then the modified Friedmann equation, Equation (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4), reads ˜h2(x) = ΩMe−3x + γY (x) , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7) 6 with γ ≡ m2/(9H2 0).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' An effective dark energy thus appears ρDE(t) = ρ0γY (t) , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='8) where ρ0 = 3H2 0/(8πG).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Once the initial conditions for the auxiliary fields are set (see [56] for details), the evolution of ρDE(t)/ρT OT (t) can be studied: the non-local effective dark energy is actually negligible until recent time and then starts to dominate the cosmic expansion.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, it is possible to study the DE equation of state ˙ρDE + 3H(1 + ωDE)ρDE = 0 , (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='9) and different evolutions for ρDE(z) follow from different choices for the initial conditions of the auxiliary fields.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' For small values of the initial conditions, one obtains a fully phantom DE, namely ωDE(z) is always less than −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' For large values of the initial conditions, ρDE(z) has a "phantom crossing" behavior, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=', there is a transition from the phantom regime to −1 < ωDE < 0 of about z ≃ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Regardless of the initial conditions, therefore, the non-local model provides a dynamical DE density which drives the accelerated expansion of the Universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' IV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' THE GROWTH OF PERTURBATIONS AND THE σ8 TENSION Building on the primordial density fluctuations emerged from the inflation, cosmic structures have formed due to gravitational instability.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Studying the large-scale structure of the Universe and its evolution through the cosmic epochs, it is possible to trace the growth of the so-called cosmological perturbations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Associated to this observable, one of the main cosmological tensions has risen: the growth tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' It has come about as the result of the discrepancy between the Planck value of the cosmological parameters ΩM and σ8 and those from WL measurements, CC and RSD data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The former dynamical probes point towards lower values of the amplitude (σ8) or the rate (fσ8 = [ΩM(z = 0)]0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='55σ8) of growth of structures with respect to the CMB experiments, giving rise to a 2−3σ tension [9, 11].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, the Planck 2018 value of the joint parameter S8 = σ8 � ΩM/0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3 (S8 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='834±0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='016 [5]) is confirmed by another recent CMB analysis by the ACT + WMAP collaboration (S8 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='840 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='030 [66]), thus erasing the possibility of a systematic error related to the excess of lensing amplitude measured by Planck [73].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3σ tension emerges accordingly with both the original WL analysis of KiDS-450 [74] and KiDS-450 + VIKING data [75], while updated constraints from the same datasets [76, 77] show greater discrepancies.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The same 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3σ tension also occurs with the data from DES’s first year release (DESY1) [78], while the combination of KiDS-450 + VIKING + DESY1 weak lensing datasets results in a 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5σ [79] or 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2σ [80] tension depending on the analysis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The most recent cosmic shear data release from both KiDS-1000 and DESY3 confirms the previous estimates [18, 81–84] (S8 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='759+0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='024 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='021 from KiDS-1000 [18]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Analogous results have been obtained with the 3 × 2 pt correlation function analysis (cosmic shear correlation function, galaxy clustering angular auto-correlation function and galaxy–galaxy lensing cross-correlation function) of KiDS-1000 + BOSS + 2dFLenS datset [85].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Additional results, in agreement with those from WL surveys, have been achieved by number counting of galaxy clusters, using multiwavelength datasets [19, 86–91].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Supplementary observational evidence for the weaker growth of structures is also given by the exploitation of RSD data [20, 92–95].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Deser–Woodard Evolution of Scalar Perturbations To investigate the growth of structures in the non-local DW model, we select the phenomenological form of the distortion function given by Equation (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As a consequence, the non-local background evolution is made equivalent to that of ΛCDM, and any deviation is enclosed in the cosmological perturbations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Consider the field equations of the scalar–tensor equivalent of the DW model, Equations (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7)–(2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='9).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Specializing to the cosmological case by assuming the FLRW metric, Equation (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1), the field equations now read H2� 1 + f − ξ � + H � f ′ ˙η − ˙ξ � − 1 6 ˙η ˙ξ = 8πG 3 ρ , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) ˙H � 1 + f − ξ � − H 2 � f ′ ˙η − ˙ξ � + 1 2 ˙η ˙ξ + 1 2 � f ′′ ˙η2 + f ′¨η − ¨ξ � = −4πG(p + ρ) , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) 7 ¨η + 3H ˙η = −6 � ˙H + 2H2� , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3) ¨ξ + 3H ˙ξ = 6f ′� ˙H + 2H2� , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4) where the former two are the (0,0) and the (1,1) component of Equation (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7), while the latter two are the cosmological formulation of Equations (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='8) and (2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='9).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The linear perturbation equations have been derived in [96] for the scalar–tensor equivalent of the non-local theory, and then analogous results have been found in [97] for the original formulation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Using the perturbed FLRW metric in the Newtonian gauge, ds2 = −(1 + 2Ψ)dt2 + a2(t)(1 + 2Φ)δijdxidxj , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5) the growth equation reads ¨δM + (2 − ξ) ˙δM = 3H2 0 � 1 − ξ − 8f ′(η) + f(η) � Ω0 M 2a3H2� 1 − ξ − 6f ′(η) + f(η) �� 1 + f(η) − ξ � δM , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='6) where δM = δρM/ρM is the matter density perturbation in the sub-horizon limit.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Numerical results for the growth rate fσ8 ≡ σ8δ′ M/δM have been obtained in [96] and [97] for both the formulations of the Deser–Woodard model, and good agreement with the Redshift Space Distortion (RSD) data has emerged (σNL 8 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='78).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, when the DW cosmological parameters are inferred by matching the CMB data [98], a lower growth amplitude with respect to that of ΛCDM turns out.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The non-local model thus alleviates the growth tension, predicting compatible values of σ8 both from Planck–CMB and the other dynamical probes, as shown in Figure 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, even though the non-local clustering of linear structures is weakened with respect to ΛCDM, and the DW prediction for the matter power spectrum is about 10% lower [98], the non-local lensing response is counterintuitively enhanced due to a severe increase in the lensing potential.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This peculiar behavior results in a slight tension between CMB and RSD [98]: performing the joint fit, the RSD dataset tends to push the DW predictions for the CMB lensing potential Cφφ ℓ out of the 1σ error bars at low-ℓ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Applying the Bayesian tools for the model selection, a “weak evidence” [103] for the ΛCDM model consequently emerges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Ricci-Transverse Evolution of Scalar Perturbations The scalar perturbations of the RT model have been investigated in [56, 104], using the FLRW metric in the Newtonian gauge, Equation (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5), and perturbing the auxiliary fields as U(t, x) = ¯U(t) + δU(t, x) , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7) Sµ(t, x) = ¯S0(t) + δSµ(t, x) = ¯S0(t) + δS0(t, x) + ∂i � δS(t, x) � , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='8) where the spatial part of the vector perturbation does not vanish and, for scalar perturbations, only depends on δS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Building on the RT cosmological equations Equations (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4)–(3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='6), the growth equation for the matter density perturbation in the sub-horizon limit reads [104] ¨δM + 2H ˙δM = 3 2 Geff G H2 0ΩMδM , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='9) where in Geff � Ψ, Φ, δU, δS0, S � is encoded the deviation of the non-local theory from GR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In the sub-horizon modes, namely ˆk ≫ 1, such deviation is 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='70 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='75 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='80 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='85 S8 CMB Planck (DW non-local) CMB Planck + RSD + JLA (DW non-local) CMB Planck + BAO + Pantheon (RT-minimal non-local) CMB Planck + BAO + Pantheon (RT non-local,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ΔN=64) CMB Planck TT,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='TE,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='EE + lowE CMB ACT + WMAP WL KiDS-1000 WL DES-Y3 WL CFHTLenS WL KiDS + VIKING + DES-Y1 WL + CMB lensing DES-Y3 + SPT + Planck WL + GC KiDS-1000 3×2pt WL + GC DES-Y3 3×2pt WL + GC KiDS + VIKING-450 + BOSS GC BOSS + eBOSS GC BOSS power spectra GC + CMB lensing DESI + Plank CC AMICO KiDS-DR3 CC SDSS-DR8 CC Planck tSZ RSD + BAO + Pantheon RSD RSD 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='70 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='75 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='80 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='85 S8 FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 1: Estimates of S8 provided by the two non-local cosmological analyses [56, 98], and the ΛCDM fit of the CMB [5, 66], the WL data [18, 20, 80, 83, 84, 99], the combination of WL and galaxy clustering observations [100–102], cluster counting [19, 87, 88] and RSD surveys [92, 94].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The colored band corresponds to the S8 value derived by the analysis of the Planck–CMB data in the ΛCDM framework [5].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 1 − Geff G = O � 1 ˆk2 � , (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='10) and the RT model is thus safe regarding the time variation of the effective Newton’s constant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Geff indeed reduces to G at the Solar System scale, while a deviation of ∼1% rises at cosmological scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In [56], the growth rate f(z, k) ≡ d ln δM/d ln a is also derived.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The results do not differ from those of ΛCDM cosmology: f(z, k) can be fitted with a k-independent function f(z) = [ΩM(z)]γ, where γ ≃ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='55 is roughly constant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Accordingly, any possible deviation in the growth of perturbations should be due to the amplitude σ8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In order to find any signature of the non-local model at perturbation level, which could account for the growth tension, the theory was compared with cosmological observations: Planck–CMB, Pantheon SNIa and SDSS-BAO.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Bayesian parameter estimation shows a full equivalence between the RT non-local cosmology and the ΛCDM one.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' No statistically signifi- cant deviation in the σ8 parameter emerges for any of the tested versions of the Ricci-Transverse model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Eventually, this theory cannot alleviate the growth tension, as shown in Figure 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' HUBBLE TENSION IN LIGHT OF THE NON-LOCAL MODELS Hubble tension is certainly the most renowned and significant tension of the ΛCDM model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' It emerges from the comparison between early-time and late-time measurements of the Hubble constant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' From one side, CMB analysis [5, 66, 105–108], BAO surveys [6, 101, 109, 110] with standard BBN constraints [111] and combinations of CMB, BAO, SNIa [112], RSD and cosmic shear data [78, 113, 114] point towards lower values of H0 (H0 = 67.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5 km s−1Mpc−1 from Planck 2018 [5]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other side, the local measurements based on standard candles prefer higher values for the Hubble constant [115] (H0 = 73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='04 ± 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='04 km s−1Mpc−1 from SH0ES 2022 [17]).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The main results are achieved by the SH0ES collaboration using Hubble Space Telescope observations: on the one hand,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' they analyzed 9 65 70 75 80 H0 ( km s-1 Mpc-1 ) CMB Planck (DW non-local) CMB Planck + RSD + JLA (DW non-local) CMB Planck + BAO + Pantheon (RT-minimal non-local) CMB Planck + BAO + Pantheon (RT non-local,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ΔN=64) ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='CMB Planck ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='CMB Planck + lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SPT-3G CMB ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='ACT + WMAP CMB ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Planck + SPT + ACT CMB ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BOSS correlation function + BAO + BBN ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BOSS power spectrum + BAO + BBN ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BOSS DR12 + BBN ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BAO + RSD ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='LSS equivalence-time ruler ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='LSS equivalence-time ruler + lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SNIa-Cepheid ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SNIa-TRGB ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SNIa-Miras ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SneII ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SnIa-Cepheid + TD lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Time-delay lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Time-delay lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Time-delay lensing + SLACS ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='GW Standard Sirens ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='GW Standard Sirens ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='GW Standard Sirens ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Masers ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Masers ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Tully Fisher ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Surface Brightness Fluctuations ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='70 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='72 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='74 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='76 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='78 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='80 S8 FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2: Estimates of H0 provided by the two non-local cosmological analyses [56, 98], and the ΛCDM fit of the CMB [5, 66, 105, 107], the matter power spectrum combined with BAO [20, 110, 126] and RSD [127], the Large Scale Structure teq standard ruler [128, 129], the supernovae [17, 121, 124, 130, 131], the time-delay lensing [121, 132, 133], the gravitational waves [134–136], the water megamasers [125, 137], the Tully–Fisher relation [138] and the SBF [139].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The colored bands correspond to the H0 estimates derived by the Planck–CMB analysis in the ΛCDM framework (purple) [5] and the SNIa–Cepheids analysis by SH0ES (orange) [17].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' SNIa data with distance calibration by Cepheid variables in the host galaxies [116, 117];' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' on the other hand, they targeted long-period pulsating Cepheid variables [17, 118], calibrating the geometric distance to the Large Magellanic Cloud, both from eclipsing binaries and parallaxes from the Gaia satellite [119, 120].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, other independent local measurement of H0 have been performed by using time delays between multiple images of strong lensed quasars [121, 122], the tip of the Red Giant Branch [123] and Miras (variable red giant stars) [124] with water megamaser as distance indicator [125].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' All these measurements agree on higher values of the Hubble constant, thus generating a 4 − 5σ tension with early-time model-dependent estimates.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Deser–Woodard Expansion History The stat-of-the-art investigation of the DW non-local model does not allow any attempt to address H0 tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' To make the model predictive, the form of the distortion function needs to be specified, and most of the analyses have been focused on the phenomenological ΛCDM form of Equation (3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3), until now (see [98] for the latest results).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This choice implies that the DW cosmology is made equivalent to that of the concordance model at background level, and the same expansion history, as well as the same H0, are thus predicted (see Figure 2).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, another option is also available for the selection of the distortion function.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In [57, 140, 141], a specific form of f(η) has been derived by exploiting the Noether symmetries [142] of a spherically symmetric background spacetime f(η) = 1 + e η .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' (5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) The accurate cosmological analysis of this form of the DW model has yet to be carried out, but some results have already been achieved, such as exact solutions [49] and a phase-space view of solutions [143].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Furthermore, several 10 astrophysical tests have been performed on very different scales, and viable results turned out.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In [141], the lensing properties of the galaxy clusters have been investigated in light of the exponential DW model, and a fully non-local regime with enhanced lensing strength has been highlighted.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This feature clearly resembles the improved lensing response of the phenomenological form of the DW model, which is co-responsible for the lowered estimate of the σ8 parameter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A promising insight upon the cosmological behavior of the non-local theory based on Equation (5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) thus emerges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Therefore, this model may alleviate not only the growth tension but also the Hubble tension, since it also deviates from GR at the background level [144].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Further analysis of the exponential DW model should be carried out accordingly.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Ricci-Transverse Expansion History For what concerns the RT model, the most updated cosmological analysis is due to Belgacem et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [56].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As we saw in Section IV, different versions of the non-local model, relying on different choices for initial conditions of the auxiliary fields, have been compared against Planck–CMB, Pantheon SNIa and SDSS-BAO data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Since the RT model has no freedom with regard to the functional form of the action, the theory cannot be adjusted to data, and no background equivalence to the ΛCDM cosmology can be established a priori.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In such a scenario, the solution to the Hubble tension may thus be possible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, the estimator tool defined in Equation (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='10), which accounts for the deviation from GR of the non-local theory, only shows little discrepancies.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This manifests in the values of the cosmological parameters inferred via Markov Chain Monte Carlo (MCMC), which are almost equivalent to those of the concordance model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The only model that exhibits some slight discrepancies is the so-called "RT-minimal", which relies on the assumption that the auxiliary scalar field U(x) starts its evolution during the radiation dominance era.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the one hand, this model predict a non-vanishing value for the sum of neutrino masses, while the ΛCDM model and the other versions of the RT model show a marginalized posterior which is peaked in zero.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, the RT-minimal model provides a barely higher estimate of the Hubble constant, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=', H0 = 68.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='74+0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='59 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='51 km s−1Mpc−1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Accordingly, the Hubble tension is just reduced to ∼4σ, as shown in Figure 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The RT model in its minimal setup thus provides a viable mechanism to account for the late-time cosmic acceleration, as well as for the inclusion of non-zero neutrino masses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, the predictions for both the background evolution and the linear perturbations are too similar to that of the ΛCDM model, hence the cosmological tensions cannot be alleviated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' VI.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ASTROPHYSICAL TESTS OF NON-LOCAL GRAVITY As we saw, good cosmological behavior emerges for both of the non-local models, thus enabling the possibility to avoid the introduction of any form of unknown dark energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In order to further investigate the viability of such models as alternatives to GR, it is then necessary to test the non-local predictions down to astrophysical scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, an accurate investigation of the possible screening mechanisms should be performed, if necessary.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Testing the Deser–Woodard Model by Galaxy Clusters, Elliptical Galaxies and the S2 Star The DW model has been tested on a wide range of astrophysical scales, from the galaxy clusters [141] to the stellar orbits around Sagittarius A* [140].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Most of the tests have been carried out for the exponential form of the non-local model, namely S = 1 2κ � d4x√−g � R � 2 + e η� − ∂µξ∂µη − ξR � , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1) where the distortion function has been picked out by exploiting the Noether Symmetry Approach [145].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The analyses presented are all performed in the post-Newtonian limit, hence the non-local gravitational and metric potential are φ(r) = − GMηc r + G2M 2 2c2r2 � 14 9 η2 c + 18rξ − 11rη 6rηrξ r � − G3M 3 2c4r3 � 50rξ − 7rη 12rηrξ ηcr + 16 27η3 c − 2r2 ξ − r2 η r2ηr2 ξ r2 � , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) ψ(r) = −GMηc 3r − G2M 2 2c2r2 � 2 9η2 c + 3rη − 2rξ 2rηrξ r � , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3) 11 where ηc is set to 1 so as to recover GR in the limit of φ(r).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The two length scales rη and rξ are the characteristic non-local parameters that define the scale at which the non-local gravity corrections become effective.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The first test of this form of the DW model has been carried out in [140], where the weak field non-local predictions have been compared against the NTT/VLT observations of S2 star orbit [146].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Exploiting a modified Marquardt– Levenberg algorithm, the fit between the simulated orbit and the observed one has shown a slightly better agreement for the non-local model with respect to the Keplerian orbit.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, some constraints have been set on the non-local length scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A further test has been subsequently performed in [141], exploiting the CLASH lensing data from 19 massive clusters [147, 148].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The point-mass potentials of Equations (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2) and (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3) were extended to a spherically symmetric mass distribution, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=', the Navarro–Frenk–White density profile, and the non-local predictions for the lensing convergence were achieved.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Therefore, the MCMC analysis has highlighted two effective regimes in which the non-local model is able to match the observations at the same level of statistical significance as GR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In the high-value limit of the non-local parameters, the non-local model reduces to a GR-like theory, whose lensing strength is 2/3 of the standard one.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this scenario, the DW theory is thus able to fit the data at the cost of increased cluster mass estimates.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, approaching the low-value limit of the non-local length scales, the non-local corrections to the lensing potential become larger and comparable to the zeroth-order terms.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In this regime, the non-local model is able to reproduce GR phenomenology, neither affecting the mass estimates nor the statistical viability of the model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Furthermore, when the non-local contributions becomes completely dominant, the non-local theory seems to be able to fit the lensing observations with extremely low cluster masses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Accordingly, an intriguing possibility to fit data with no dark matter emerges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Additional constraints on the non-local parameters were also derived.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The most recent astrophysical test of the exponential-DW model was carried out in [57], using the velocity distri- bution of elliptical galaxies [149].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Computing the non-local velocity dispersion as a function of the galaxy effective radius, the empirical relation of the so-called Fundamental Plane has been recovered so as to constrain the non-local gravity parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The results of the fit highlight the possibility to recover the fundamental plane without the dark matter hypothesis, setting new constraints for rη and rξ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' It is worth noticing, however, that the non-local Deser–Woodard model exhibits worrisome features at the scale of the Solar System.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Indeed, in [150], it was demonstrated that the screening mechanism proposed by the same authors of the non-local model does not work.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As a consequence, the DW model would show a time dependence of the effective Newton constant in the small-scale limit, and it would be ruled out by Lunar Laser Ranging (LLR) observations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This conclusion, however, seems to be too strong, since it is still not clear how an FLRW background quantity behaves when evaluated from cosmological scales down to Solar System ones, where the system decouples from the Hubble flow.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In fact, a full non-linear time- and scale-dependent solution around a non-linear structure would be necessary.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A number of proposals go in this direction, and the so-called Vainshtein mechanism [151] can be regarded as the paradigm to realize the screening.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Basically, any screening mechanism requires a scalar field coupled to matter and mediating a fifth force which might span from Solar System up to cosmological scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Since non-local terms can be “localized”, thus resulting in effective scalar fields depending on the scale, some screening mechanism could naturally emerge so as to solve the above reported problems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Testing the Ricci-Transverse Model by Solar System Observations and Gravitational Waves Detection The main astrophysical tests of the RT model are related to Solar System observations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As we saw in the previous sub-section, any theory that extends GR has to reduce to Einstein’s theory at small scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, this is highly non-trivial when additional degrees of freedom are included, and screening mechanisms involving non-linear features are required.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The RT model, instead, smoothly reduces to GR already at linear level, and no vDVZ discontinuity arises when m → 0 [56].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Note that such results are valid both in the flat and the Schwarzschild spacetime.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, the non-local model passes the LLR test about the time variation of the effective Newton constant [150].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' As stated in Equation (4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='10), indeed, the deviation parameter Geff reduces to GN as soon as the system’s characteristic scale decreases.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Another non-local feature of the RT model that has been investigated is the deviation from GR of the predicted gravitational radiation [152, 153].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The RT model, similarly to some other extended theories of gravity such as f(R) gravity and DHOST theories, has survived the GW170817 event, which set a stringent constraint on the Gravitational Waves (GW) speed [154].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Indeed, this non-local model only modifies the friction term in the GW propagation equation, thus predicting a massless graviton.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, neither the coupling with matter nor the gravitational interaction between the coalescing binaries are affected (the RT model reduces to GR at short distances), and the only difference will therefore be due to the free propagation of the GW from the source to the observer.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The GW amplitude indeed undergoes a modified dampening in the non-local model 12 ˜hA(η, k) ∼ 1 dgw L (z) = � dem L (z) exp � − � z 0 dz′ 1 + z′ δ(z′) ��−1 , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4) where δ(η) = m2 ¯S0(η) 6H(η) , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='5) and ˜hA(η, k) are the Fourier modes of the GW amplitude, with A = ×, + labeling the polarization.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Computing the ratio between the non-local behavior given by Equation (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4) and the GR behavior, ˜hA(η, k) ∼ 1/dem L (z), little deviation emerges for the RT-minimal model, while a 20−80% deviation manifests at large z for the RT formulations in which the auxiliary fields start their evolution during the de Sitter inflation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The more e-folds we consider between the onset of the auxiliary fields and the end of the inflation, the greater the deviation from GR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' We can use a simple parametrization for the considered ratio dgw L (z) dem L (z) = Ξ0 + 1 − Ξ0 (1 + z)n , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='6) where Ξ0 is the asymptotic value reached by the ratio and n is the rate at which Ξ0 is approached.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Then, δ(z) = δ(0) 1 − Ξ0 + Ξ0(1 + z)n , (6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7) with δ(0) = n(1 − Ξ0), and the event GW170817 provided the following constraint for such a parameter [153]: δ(0) = −7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='8+9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='7 −18.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' More stringent constraints will certainly be set with the next generation of GW detectors by exploiting the observations of GW events with electromagnetic counterparts.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' VII.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' CONCLUSIONS AND PERSPECTIVES In this paper, we reviewed the cosmological properties of two of the main proposals in the framework of the non- locally extended theories of gravity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' In particular, we considered two metric IKGs that are inspired by quantum corrections and manifest a suitable cosmological behavior as well.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Both the DW and RT models are able to reproduce the expansion history of the Universe, exhibiting a late-time accelerated expansion driven by the onset of the non-local corrections.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The non-local extensions of the Hilbert–Einstein Lagrangian thus provide a viable mechanism to avoid the introduction of any form of unknown dark energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Building on these appealing properties, we inquired into the chance of addressing the two main cosmological tensions, namely the σ8 and H0 tensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the one hand, the non-local DW model has shown suitable features towards this aim.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The phenomenological formulation of the model indeed predicts a lowered amplitude of growth of perturbations, therefore solving the σ8 tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, this model is made equivalent to the ΛCDM cosmology at the background level, hence no chance to account for the Hubble tension arises.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Another formulation of the DW theory, based on the Noether symmetries of the system, may address both the tensions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This model lacks a proper cosmological analysis, but the investigation of its lensing properties at the galaxy clusters scale has shown the same features that, in the phenomenological DW model, allow the weakening of the growth of structures.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, this formulation of the non-local theory deviates from GR also at background level, thus enabling the possibility to alleviate the Hubble tension as well.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The model has been also tested on astrophysical scales, and substantial statistical equivalence to GR has emerged in very different systems, such as the S2 star, the elliptical galaxies and the galaxy clusters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The main drawback of the DW model, however, is the absence of an effective screening mechanism on small scales, which has to be further investigated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' On the other hand, the non-local RT model perfectly reduces to GR at the Solar System scale, thus avoiding the necessity of non-trivial screening mechanisms.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Accordingly, the model is not ruled out by the LLR test.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Moreover, the non-minimal formulations of the RT model show a strong deviation from GR for what concerns the GW propagation at large redshift.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A powerful tool to test the model with the next generation of GW detectors thus emerges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, this non-local model is not able to address any of the cosmological tensions, as it mimics the ΛCDM evolution both at the background and linear perturbations level.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 13 In view of the fact that the next generation of cosmological surveys are expected to provide sufficiently accurate data to reach a turning point in our comprehension of the Universe, it is of great interest to further investigate the main alternatives to GR.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A complete cosmological analysis should especially be carried out for the non-local DW model in its formulation based on the Noether Symmetry Approach.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' This model indeed provides one of the most promising windows towards the solution of both the cosmological tensions and the dark energy problem.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The large- scale structure especially appears as a privileged environment for testing the non-local models, since one of their main features is the emergence of characteristic length scales.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' However, it must be stressed that as long as no screening mechanism will be found for the DW model, its reliability will be compromised.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Acknowledgments This article is based upon work from COST Action CA21136 Addressing observational tensions in cosmology with systematic and fundamental physics (CosmoVerse) supported by COST (European Cooperation in Science and Technology).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' FB and SC acknowledge the support of Istituto Nazionale di Fisica Nucleare (INFN), iniziative specifiche QGSKY and MOONLIGHT2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Appendix A: Abbreviations ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='The following abbreviations are used in this manuscript: ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BBN ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Big Bang Nucleosynthesis ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='BAO ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Baryon Acoustic Oscillations ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='ΛCDM Lambda Cold Dark Matter ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='GR ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='General Relativity ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='DE ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Dark Energy ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='DM ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Dark Matter ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='CMB ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Cosmic Microwave Background ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='WL ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Weak Lensing ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='CC ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Cluster Counts ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='RSD ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Redshift Space Distortion ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='DW ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Deser–Woodard ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='RT ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Ricci-Transverse ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='QFT ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Quantum Field Theory ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='IDG ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Infinite Derivative Theory of Gravity ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='IKG ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Integral Kernel Theory of Gravity ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='UV ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='UltraViolet ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='IR ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='InfraRed ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='SNIa ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Type Ia Supernovae ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='FLRW Friedmann–Lemaitre–Robertson–Walker ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='MCMC Markov Chain Monte Carlo ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='LLR ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Lunar Laser Ranging ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='GW ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='Gravitational Waves ' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='[1] Hogg,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Eisenstein, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Planck 2018 results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' VI.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Cosmological parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astron.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astrophys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Dark Universe 2016, 12, 56–99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='dark.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2016.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} 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'/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2022, 95, 101659.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='newar.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2022.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='101659.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [10] Di Valentino, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Anchordoqui, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Özgür Akarsu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Ali-Haimoud, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Amendola, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Arendse, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Ballardini, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Basilakos, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Battistelli, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Snowmass2021—Letter of interest cosmology intertwined II: The hubble constant tension.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astropart.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2021, 131, 102605.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='astropartphys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='2021.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='102605.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [11] Di Valentino, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Anchordoqui, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Özgür Akarsu.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Ali-Haimoud, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Amendola, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Arendse, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Ballardini, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Basilakos, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Battistelli, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Roncarelli, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' AMICO galaxy clusters in KiDS-DR3: Cosmological constraints from counts and stacked weak lensing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astron.' metadata={'source': 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+page_content=' Nunes, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Measurements of H0 in modified gravity theories: The role of lensed quasars in the late-time Universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' D 2020, 101, 103505.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1103/physrevd.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='101.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='103505.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [28] Nesseris, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Basilakos, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Saridakis, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Perivolaropoulos, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Viable f(T) models are practically indistinguishable from ΛCDM.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='103010.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [29] Cai, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Capozziello, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' De Laurentis, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Saridakis, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' f(T) teleparallel gravity and cosmology.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rep.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Prog.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} 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'/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Koivisto, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Cosmological perturbations in modified teleparallel gravity models.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Cosmol.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astropart.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': 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D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Can f(T) gravity resolve the H0 tension?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' D 2020, 102, 063530.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Zahn, O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Cosmic microwave weak lensing data as a test for the dark universe.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' D 2008, 77, 123531.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Viola, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Heymans, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Joudaki, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Kuijken, K.' 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Wright, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Blake, C.' metadata={'source': 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'/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astrophys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2020, 633, A69.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1051/0004-6361/201834878.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [76] Köhlinger, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Viola, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Joachimi, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hoekstra, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' van Uitert, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hildebrandt, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Choi, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Erben, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Heymans, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Joudaki, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' KiDS-450: The tomographic weak lensing power spectrum and constraints on cosmological parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Mon.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Not.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astron.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Soc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2017, 471, 4412–4435.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1093/mnras/stx1820.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [77] Wright, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hildebrandt, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': 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MacCrann, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Zuntz, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Eifler, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Krause, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Dodelson, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Gruen, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Blazek, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Friedrich, O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Samuroff, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Dark Energy Survey Year 1 results: Cosmological constraints from cosmic shear.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' D 2018, 98, 043528.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='1103/physrevd.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='98.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='043528.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' [79] Joudaki, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hildebrandt, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Traykova, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Chisari, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Heymans, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Kannawadi, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Kuijken, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Wright, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Erben, T.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Heymans, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hildebrandt, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' van den Busch, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Wright, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Choi, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Erben, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Cuceu, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Stölzner, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Tröster, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Wright, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Bilicki, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Tröster, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Asgari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Blake, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hildebrandt, H.' 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constant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astrophys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' 2016, 826, 56.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='3847/0004-637x/826/1/56.' metadata={'source': 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Biermann, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Creevey, O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Evans, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Eyer, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Gaia Early Data Release 3—Summary of the contents and survey properties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astron.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astrophys.' metadata={'source': 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Bastian, U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Biermann, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Bombrun, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' de Torres, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Gerlach, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Geyer, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hernández, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hilger, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Hobbs, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='.;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Gaia Early Data Release 3 - Parallax bias versus magnitude, colour, and position.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Astronomy & Astrophysics 2021, 649, A1.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Chen, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Rusu, C.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Treu, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Agnello, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=';' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Buckley-Geer, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='J.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' ;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Zheng, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' A 5% measurement of the Hubble constant from Type II supernovae.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Mon.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Not.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' R.' metadata={'source': 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metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content='R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' The Hubble constant from eight time-delay galaxy lenses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Mon.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' Not.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/EdAzT4oBgHgl3EQfiv0h/content/2301.01503v1.pdf'} 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ryan.toth}@quantropi.com +ABSTRACT +This paper proposes a new homomorphic functional encryption using modular multiplications over +a hidden ring. Unlike traditional homomorphic encryption where users can only passively perform +ciphertext addition or multiplication, the homomorphic functional encryption retains homomorphic +addition and scalar multiplication properties, but also allows for the user’s inputs through polynomial +variables. The homomorphic encryption key consists of a pair of values, one used to create the hidden +ring and the other taken from this ring to form an encryption operator for modular multiplication en- +cryption. The proposed homomorphic encryption can be applied to any polynomials over a finite field, +with their coefficients considered as their privacy. We denote the polynomials before homomorphic +encryption as plain polynomials and after homomorphic encryption as cipher polynomials. A cipher +polynomial can be evaluated with variables from the finite field, GF(p), by calculating the monomials +of variables modulo a prime p. These properties allow functional homomorphic encryption to be +used for public key encryption of certain asymmetric cryptosystems, such as Multivariate Public Key +Cryptography schemes or MPKC to hide the structure of its central map construction. We propose +a new variant of MPKC with homomorphic encryption of its public key. This variant simplifies +MPKC central map to two multivariate polynomials constructed from polynomial multiplications, +applying homomorphic encryption to the map, and changing its decryption from employing inverse +maps to a polynomial division. We propose to use a single plaintext vector and a noise vector of +multiple variables to be associated with the central map, in place of the secret plaintext vector to be +encrypted in MPKC. We call this variant of encrypted MPKC, a Homomorphic Polynomial Public +Key algorithm or HPPK algorithm. The HPPK algorithm holds the property of indistinguishability +under the chosen-plaintext attacks or IND-CPA. The overall classical complexity to crack the HPPK +algorithm is exponential in the size of the prime field GF(p). We briefly report on benchmarking +performance results using the SUPERCOP toolkit. Benchmarking results demonstrate that HPPK +offers rather fast performance, which is comparable and in some cases outperforms the NIST PQC +finalists for key generation, encryption, and decryption. +Keywords Homomorphic Functional Encryption · Post-Quantum Cryptography · Public-Key Cryptography · PQC · +Key Encapsulation Mechanism · KEM · Multivariate Public Key Cryptosystem · MPKC · PQC Performance. +1 +Introduction +Homomorphic encryption was first proposed by Rivest et al. in 1978 [1], one year after filing the patent for the +RSA public key cryptography [2]. Homomorphic encryption commonly refers to privacy encryption for computation +in an encrypted mode, without knowing the homomorphic key and the decryption procedure. This is noticeably +different from the cryptographic algorithms used to encrypt data for secure communications or storage with public key +mechanisms such as RSA [2] and Diffie-Hellman [3], and Elliptic Curve Cryptography [4, 5] to establish the shared key +for symmetric encryption using algorithms as Advanced Encryption Standard or AES. +arXiv:2301.11995v1 [cs.CR] 27 Jan 2023 + +Novel Homomorphic Functional Encryption over a Hidden Ring +Homomorphic encryption can be classified into partially homomorphic and fully homomorphic. The partially homomor- +phic encryption supports either multiplicative or additive homomorphic operations, RSA [6] and ElGamal cryptosystems +[7] are multiplicatively homomorphic; Goldwasser–Micali [8], Benaloh [9], and Paillier [10] are additively homo- +morphic. The first milestone for fully homomorphic encryption was achieved by Gentry in 2009 using lattice-based +cryptography [11] to support both addition and multiplication operators in the encrypted mode. Meanwhile, Chan in +2009 proposed a symmetric homomorphic scheme based on improved Hill Cipher [12]. Kipnis and Hibshoosh proposed +their symmetric homomorphic scheme in 2012 [13] with a randomization function for non-deterministic encryption. +Gupta and Sharma proposed their symmetric homomorphic scheme based on linear algebraic computation in 2013 [14]. +Very recently, Li et al. in 2016 proposed a new symmetric homomorphic scheme, called Li-Scheme for outsourcing +databases [15]. Their scheme, at large, is associated with two finite fields: a secret small field Fq and a big public field +Fp, with modular exponentiation with its secret base s followed by modular multiplication with plaintext message m. +Li-Scheme supports both additive and multiplicative operations so it is a full homomorphic encryption. Wang et al. +performed a cryptoanalysis of the Li-Scheme in 2018 [16] and broke the scheme with certain known plaintext-ciphertext +pairs. Wang et al. further improved their cryptoanalysis in 2019 and successfully recovered the secret key with the +ciphertext-only attack using lattice reduction algorithm [17]. +Homomorphic encryption solely focuses on addition and multiplication operations on the encrypted data for plain data +privacy. However, it would be very interesting to see an extension of homomorphic encryption from data privacy to +functional privacy with variables to take the user’s inputs in a framework of a public key scheme. It is rarely seen +that a public key cryptosystem, more precisely quantum-safe public key cryptosystem, is purposely designed with +careful considerations not only to leverage homomorphic properties of ciphertext addition and scalar multiplication +but also to take user’s secrets into ciphertext computation. This served as a motivation for our paper. We introduce a +new Homomorphic Polynomial Public Key encapsulation or HPPK, which is an asymmetric key encapsulation scheme, +with public keys encrypted using functional homomorphic encryption. HPPK uses multivariate polynomials to not +only leverage homomorphic properties of addition and scalar multiplication but also allows for encrypting party’s +input during the ciphertext creation. That is, the public key polynomial coefficients are encrypted using homomorphic +function to ensure they are never truly public and hide the structure of the public key, at the same time, treating variables +of the said public key polynomials as user input allows for freedom during the encryption process. +HPPK cryptosystem has two distinct features, namely, the homomorphic encryption of the public key that allows +for the user’s input during ciphertext creation, and the use of a hidden ring. HPPK is not the first cryptosystem to +use hidden structure. For instance, the work of Li et al. describes a cryptosystem with a hidden prime ring [15]. +Another important example is Hidden Field Equations (HFE) cryptosystems. The examples of asymmetric multivariate +encryption schemes that are based on HFE include [18, 19, 20, 21]. Various signature schemes based on HFE were +also proposed [22, 23, 24, 25, 26]. In the framework of HFE, the private polynomials as well as the structure they are +defined over, a field extension, are both hidden using affine transformations. +The algorithms based on HFE, mentioned above fall in the category of quantum-safe algorithms. More precisely, +multivariate quantum-safe algorithms. Quantum computing developments have been receiving a lot of focus from the +academic community as well as industry leaders since Google announced its first quantum advantage in 2019 [27]. +But it was the National Institution of Standards and Technology (NIST) that opened the arena for quantum-resistant +cryptography, when they started the post-quantum cryptography (PQC) standardization process in November 2017. +Recently, they have announced third-round finalists which include four key exchange mechanism schemes (KEM) and +three finalists for digital signatures [28]. Four KEM finalists include code-based Classic McEliece [29], lattice-based +CRYSTALS-KYBER [30], NTRU [31, 32], and Saber [33] algorithms. At the latest announcement, NIST selected +CRYSTALS-KYBER to be standardized algorithm for KEM. In addition to the aforementioned finalists for KEM, the +Multivariate Public Key Cryptosystems or MPKC is worth a special discussion. Algorithms based on multivariate +polynomial problems are considered to be quantum-safe, but they also make an excellent candidate for homomorphic +encryption due to the use of multivariate polynomials. +The framework of MPKC is built on a system of quadratic polynomials. The public key is represented by a central map +P : Fm +p → Fℓ +p with m variables and ℓ polynomials [34]. Many variants of MPKC central map constructions have been +proposed since Matsumoto and Imai first introduced this cryptosystem in 1988 [35], including single field systems and +mixed field systems [36]. Single field MPKC includes several Triangular systems and the Oil and Vinegar system since +Patarin and Goubin in 1997 [37] and unbalanced Oil and Vinegar scheme by Kipnis et. al. in 1999 [18]. The mixed +field MPKC refers to Matsumoto-Imai system [35] and Hidden Field Equation [38]. In addition, Wang et al. in 2006 +proposed a Medium-Field MPKC scheme [39] and an improved scheme in 2008 [40]. Ding and Schmidt proposed +Rainbow as a MPKC digital signature scheme in 2005 [25]. +Attacks on MPKC cryptosystems are mainly classified into two categories: algebraic solving attacks and linear algebra +attacks. Algebra solving attacks attempt to solve the MPKC multivariate equation system from the public key with +2 + +Novel Homomorphic Functional Encryption over a Hidden Ring +ciphertext (z1, z2, . . . , zℓ) to recover the pre-image (x1, x2, . . . , xm). Faugére reported his first attack on MPKC in +1999[41] and in 2002[42] using Gröber bases (F4), later in 2003 Faugére and Antoine reported their attack on HFE +Gröber bases (F5). Ding et. al. proposed their new Zhuang-Zi algorithm to solve the multivariate system in 2006 [43]. +In linear algebra attacks, Courtois et al. reported their attack on MPKC using the relinearization technique, aclled XL +in 2000 [44]. The Minrank attack has been successfully applied by Goubin and Courtois on the single field system in +2000 [45] and by Kipnis and Patarin on the mixed field system in 1999 [46]. +A new type of polynomial public key has been recently proposed by Kuang in 2021 [47], based on univariate polynomial +multiplications, by Kuang and Barbeau in 2021 [48, 49, 50], based on multivariate polynomial multiplications with two +noise functions to increase the public key security against possible public key attacks. The digital signature scheme of +the multivariate polynomial public key or MPPK has been prosoed by Kuang, Perepechaenko and Barbeau in 2022 [51]. +This paper explores the possibility to combine a new homomorphic encryption to key construction to further enhance +the security of the MPPK cryptography for key encapsulation mechanism or KEM. +The proposed HPPK scheme can be also considered as a new variant of MPKC scheme with public keys being +encrypted using homomorphic functional encryption. We begin by introducing the proposed symmetric homomorphic +encryption scheme in A New Symmetric Homomorphic Functional Encryption over a Hidden Ring. The proposed +HPPK algorithm is then discussed in Homomorphic Polynomial Public Key Cryptosystem. We present the reader with +thorough security analysis of HPPK in HPPK Security Analysis, and report on benchmarking the performance of HPPK +in Brief Benchmarking Performance. We conclude with Conclusion. +2 +A New Symmetric Homomorphic Functional Encryption over a Hidden Ring +In contrast to conventional homomorphic cryptography used for data privacy, in this paper we propose homomorphic +functional encryption to be applied to the public key in the framework of multivariate asymmetric cryptography. This +will allow for an asymmetric scheme with encrypted public keys. Moreover, by construction, functional homomorphic +encryption allows for user’s input during the ciphertext generation procedure. That is, the ciphertext can be created +with the input of the encrypting party, however, the public key used for encryption is itself encrypted using functional +homomorphic operator. The decrypting party is the only party that has knowledge of the private key associated +with the functional homomorphic encryption operator as well as the asymmetric scheme private key. Essentially, the +homomorphic functional encryption defined in this paper provides a round-trip envelope for a public key encryption. +In a way, such approach combines three main areas of cryptography, namely, asymmetric cryptography, homomorphic +encryption, and symmetric cryptography with self-shared key. This phenomenon is illustrated in Fig. 1. In the figure, the +traditional public key derived from a given assymetric algorithm is called plain public key or PPK, the homomorphically +encrypted PPK is called cipher public key or CPK. The cipher is produced by evaluating the public key polynomial +values using a user-selected secret. The decryption would perform in two stages: homomorphic decryption and then +secret extraction. +Figure 1: Illustration of a cryptosystem combining asymmetric cryptography, symmetric cryptography with a single +self-shared key, and homomorphic encryption. +We begin by introducing the Homomorphic Functional Encryption Operator. In order to allow for the user’s input during +ciphertext creation, and leverage additive and scalar multiplicative homomorphic features, the functional homomorphic +3 + +Symmetric +Encrypt +0 +Enc +Crypto +PPK +Dec +Dec +HPPK +997 +CPK +Cipher +Homomorphic CryptoNovel Homomorphic Functional Encryption over a Hidden Ring +encryption is applied to polynomials. We discuss the reason for this further. Hence, when introducing the said operator +we assume that it will be applied to polynomials. +2.1 +Homomorphic Encryption Operator +Let S be a positive integer, and R be a randomly chosen value such that R ∈ ZS and gcd(R, S) = 1. We propose a +Homomorphic Functional Encryption Operator ˆE(R,S), with a secret homomorphic key being a tuple (R, S). The values +S and R are never shared. +In its general form, the encryption operator is defined as a multiplicative operation modulo a hidden value S as +ˆE(R,S)(f) = (R ◦ f) mod S, +(1) +where f denotes any univariate or multivariate polynomial f = �k +i=0 fiXi, over Fp with Xi being its monomials. The +encryption operator acts on the coefficients of f, which we refer to as plain coefficients. This produces what we call +cipher coefficients, denoted hi, as +ˆE(R,S)fi = Rfi mod S = hi +for every i. Similarly, we can define a Homomorphic Functional Decryption Operator as +ˆE(R−1,S)h = (R−1 ◦ h) mod S. +(2) +Such operator decrypts the coefficients of the polynomial h. That is, it successfully decrypts the cipher coefficients +back to the plain coefficients. More precisely, +ˆE(R−1,S)hi = R−1(Rfi) mod S = (R−1R)fi mod S = fi +for any i. +The above defined homomorphic operator ˆE(R,S) holds following homomorphic properties: +• ˆE(R,S) is additively homomorphic: if a and b are two plain constants, then ˆE(R,S)(a+b) = R(a+b) mod S = +Ra + Rb mod S = ˆE(R,S)a + ˆE(R,S)b; +• ˆE(R,S) is scalar multiplicatively homomorphic: if a is a plain constant and x is a variable, then ˆE(R,S)(ax) = +R(ax) = (Ra)x = [ ˆE(R,S)a]x. +Thus, the operator ˆE(R,S) offers partially homomorphic encryption. We leave it to the reader to verify that the +same properties hold true for the proposed homomorphic functional decryption operator ˆE(R−1,S). Note that these +homomorphic properties come from linearity, and thus are natural to polynomials. Indeed, polynomials hold additive +and scalar multiplicative properties through their coefficients. Moreover, polynomials can be defined and evaluated with +coefficients in a field or a ring, different from a field or a ring for variables. We leverage this property, and thus, apply +the functional homomorphic encryption to public key cryptosystems with polynomial public keys. +2.2 +Homomorphically Encrypted Polynomials +As we have previously stated, the proposed homomorphic encryption is applicable to all polynomials over a ring Zp +or finite field Fp characterized by a prime p. In this work, when we refer to polynomials, we imply that the plain +polynomials, to be encrypted, are considered modulo p, unless stated otherwise. A generic multivariate polynomial has +the following form +p(x1, . . . , xm) = +ℓ1 +� +j1=1 +· · · +ℓm +� +jm=1 +pij1...jmxj1 +1 · · · xjm +m . +Alternatively, let Xj = xj1 +1 · · · xjm +m denote the monomials of such polynomial, then +p(x1, . . . , xm) = +L +� +j=1 +pjXj, +(3) +where L denotes the total number of terms. +To successfully encrypt and decrypt any polynomial p(x1, . . . , xm) using the functional homomorphic encryption and +decryption operators defined in Eq. (1) and (2) respectively, the following conditions must be met: +4 + +Novel Homomorphic Functional Encryption over a Hidden Ring +• The monomials Xj are to be computed as Xj = (Xj mod p). The values of monomials reduced modulo p are +used to compute the value of the polynomial p(x1, . . . , xm). +• The homomorphic secret key value S should satisfy the bit length condition: |S|2 > 2|p|2 + |L|2. +The first condition ensures that polynomial p(x1, . . . , xm) is evaluated as if the mononials Xj are new variables over +Fp, Indeed, the operator ˆE(R,S) is applied to the polynomial p(x1, . . . , xm) in the following way +ˆE(R,S)p(x1, . . . , xm) = +L +� +j=1 +[Rpj mod S]Xj. +(4) +Such encrypted polynomial can be computed as +L +� +j=1 +[Rpj mod S](Xj mod p) = ¯p. +Note that the computed value was not reduced modulo any integer, nor is the arithmetic performed modulo any integer. +Thus, the user’s input through monomials Xj remains intact and can be decrypted correctly. Let the plain value of the +polynomial with user’s input, that is, if the polynomial was not encrypted with ˆE(R,S), be +ˆp = +L +� +j=1 +pjXj mod p. +To ensure successful decryption, the second condition must be met. If the size of S is sufficiently large, the values of +coefficients and variables remains the same after decryption, and it is possible to recover ˆp. Indeed, +ˆE(R−1,S)¯p = +L +� +j=1 +[R−1Rpj mod S](Xj mod p) = +L +� +j=1 +pj(Xj mod p), +(5) +and then the value �L +j=1 pj(Xj mod p) can be reduced modulo p to yield �L +j=1 pjXj mod p = ˆp. +To elaborate more on this, we present the reader with two examples of functional homomorphic encryption of linear +and quadratic polynomials. +2.2.1 +Linear Polynomials +Recall, that we encrypt the coefficients of the polynomials defined over Fp, which successfully maps polynomials from +Fp[x1, . . . , xm] to ZS[x1, . . . , xm], leaving x1, . . . , xm ∈ Fp. A generic linear multivariate polynomial over a finite +field Fp has form +p(x1, x2, . . . , xm) = +m +� +j=1 +pjxj mod p. +(6) +Conventionally, in the asymmetric encryption schemes, the public key inherits mathematical logic from the private +key, making it vulnerable. Hence, if public key consists of polynomials, we wish to encrypt the coefficients of the said +polynomials using functional homomorphic operator, to hide the mathematical logic. In this case we share the cipher +public key, encrypted using functional homomorphic operator. To ensure that the ciphertext can be still created in the +framework of asymmetric public key scheme, the variables in the public key polynomials are used for user’s input. +They are not encrypted using homomorphic encryption, but only using the encryption procedure from the asymmetric +scheme. Such variable values can consist of the plaintext only, or plaintext and noise used for obscurity. +Applying homomorphic encryption operator to the above linear polynomial, defined in Eq.(6), produces a cipher linear +polynomial with coefficients in a hidden ring ZS, and variables in Fp : +P(x1, x2, . . . , xm) = ˆE(R,S)p(x1, x2, . . . , xm) += +m +� +j=1 +(Rpj mod S)xj = +m +� +j=1 +Pjxj. +(7) +5 + +Novel Homomorphic Functional Encryption over a Hidden Ring +While the plain coefficients, pj, are encrypted into cipher coefficients, Pj, the cipher polynomial P(x1, x2, . . . , xm) +can still be evaluated with a set of chosen values r1, . . . , rm ∈ Fp to produce value ¯P +¯P = P(r1, r2, . . . , rm) = +m +� +j=1 +Pj(rj mod p). +(8) +Let the value ¯p = �m +i=1 pjrj mod p, be the original ciphertext of the asymmetric scheme. However, it is encrypted +into the value ¯P using homomorphic encryption. To recover the plain polynomial value, that is, decrypt the cipher +coefficients, into the plain coefficients and evaluate polynomial modulo p, we first apply the functional homomorphic +decryption operator ˆE(R−1,S) to get ˆE(R−1,S) ¯P, and then reduce this value modulo p. More precisely, +ˆE(R−1,S) ¯P = +m +� +j=1 +[R−1Pj mod S](rj mod p) = +m +� +i=1 +pj(rj mod p), +which reduced modulo p is +m +� +i=1 +pjrj mod p = ¯p. +In a framework of asymmetric scheme with functional homomorphic encryption element, polynomials such as in Eq. (6) +are associated with plain coefficients, that is, the original public keys. The cipher polynomials have form as in Eq. (7), +with coefficients being encrypted from the plain public keys, using homomorphic encryption. Such cipher public keys +are shared, and the plain public keys are stored securely and never shared. The ciphertext in this combined algorithm +is of the form as in Eq. (8). The decrypting party first needs to decrypt the ciphertext to nullify the homomorphic +encryption of the public key, as shown in Eq. (8). Afterwards, the decryption party can perform decryption procedure +that corresponds to the given asymmetric scheme. +2.2.2 +Quadratic Polynomials +Multivariate quadratic polynomials serve as the foundation of Multivariate Public Key Cryptosystem or MPKC[34, +52, 53]. Thus, we want to pay special attention on applications of functional homomorphic encryption on multivariate +quadratic polynomials. A general quadratic multivariate polynomial p(x1, x2, . . . , xn) over a finite field Fp has the +following form +p(x1, x2, . . . , xm) = +m +� +1≤i≤j +pijxixj mod p, +(9) +where the coefficients pij are considered as the privacy constants for this polynomial function so they must be hidden +from public. This is done by applying the functional homomorphic encryption operator to this polynomial as follows +P(x1, x2, . . . , xm) = ˆE(R,S)p(x1, x2, . . . , xm) +(10) += +m +� +1≤i≤j +(Rpij mod S)xixj = +m +� +1≤i≤j +Pijxixj. +(11) +(12) +Here, the encrypted coefficients are defined over the hidden ring ZS, however, all the variables x1, . . . , xm are still +elements of the field Fp. As we have previously mentioned, we refer to the coefficients pij as plain coefficients, and Pij +are referred to as cipher coefficients. Similarly, P(x1, x2, . . . , xm) and p(x1, x2, . . . , xm) are referred to as cipher and +plain polynomials respectively. +While coefficients are encrypted with homomorphic encryption operator, the polynomial P(x1, x2, . . . , xm) still accepts +user’s input. That is, the cipher polynomial value ¯P can be still calculated with a chosen set of r1, . . . , rm from the +field Fp as follows +¯P = P(r1, r2, . . . , rm) = +m +� +1≤i≤j +Pij(xixj mod p). +(13) +Note that the computed value ¯P is an integer. The arithmetic to compute such value was not performned modulo any +integer. The plain polynomial values are securely hidden through the hidden ring ZS. To recover the plain polynomial +6 + +Novel Homomorphic Functional Encryption over a Hidden Ring +equation, decryption opertor ˆE(R−1,S) can be applied to the cipher polynomial value ¯P, followed by reduction mod p: +ˆE(R−1,S) ¯P = R−1 ¯P mod S, then +(14) +(R−1 ¯P mod S) mod p = p(r1, r2, . . . , rm) = ¯p. +(15) +The value ¯p is the plain polynomial value for the chosen values of variables x1, . . . , xm by the encrypting party. +Similar to the linear case, the public key of the asymmetric scheme consist of quadratic polynomials of the form (9), to +be encrypted using homomorphic functional encryption operators. The cipher public keys are of the form (10). Such +cipher public keys are the ones shared, while the plain public keys are not. The ciphertext in the combined scheme is of +the form (13), which needs to be decrypted back to the plain value. For that a homomorphic decryption operator is +applied, as in Eq (14), and the plain ciphertext value is recovered. +3 +Homomorphic Polynomial Public Key Cryptosystem +3.1 +Brief Summary of MPKC +An interested reader can find the detail description of MPKC schemes by Ding and Yang [34]. In this section, we +briefly outline the basic mechanism of MPKC algorithms. The framework mainly consists of ℓ quadratic multivariate +polynomials +p1(x1, . . . , xm), p2(x1, . . . , xm), . . . , pℓ(x1, . . . , xm) +in m variables over finite field Fp. Each polynomial pk(x1, . . . , xm) can be written in its expanded form as +pk(x1, . . . , xm) = +m +� +i