id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,801.06869 | Counter-propagating waves in a system of transport-reaction equations | Hyperbolic transport-reaction equations are abundant in the description of
movement of motile organisms. Here, we focus on system of four coupled
transport-reaction equations that arises from an age-structuring of a species
of turning individuals. The highlight consists of the explicit construction and
characterizati... | math.AP | hyperbolic transportreaction equations are abundant in the description of movement of motile organisms here we focus on system of four coupled transportreaction equations that arises from an agestructuring of a species of turning individuals the highlight consists of the explicit construction and characterization of co... | [['hyperbolic', 'transportreaction', 'equations', 'are', 'abundant', 'in', 'the', 'description', 'of', 'movement', 'of', 'motile', 'organisms', 'here', 'we', 'focus', 'on', 'system', 'of', 'four', 'coupled', 'transportreaction', 'equations', 'that', 'arises', 'from', 'an', 'agestructuring', 'of', 'a', 'species', 'of', ... | [-0.18584847304913582, 0.1595468857331346, -0.05766547732337406, 0.010073422045080048, -0.035009098376824775, -0.10034603073092346, -0.02774794086475264, 0.30764578061291215, -0.221321091204035, -0.27467677794806095, 0.08200408227981604, -0.2944339241507943, -0.21038807416334748, 0.18228202001332786, -0.010372740216553... |
1,801.0687 | Raman Detection Threshold Measurements for Acetic Acid in Martian
Regolith Simulant JSC-1 in the Presence of Hydrated Metallic Sulfates | Several measurements, including the data from the laser spectrometer in the
Sample Analysis at Mars instrument suite on the Curiosity Rover in Gale crater,
have measured seasonal variations in atmospheric methane at the 0.7 ppbv (parts
per billion volume) level. As a result, models have been proposed to understand
th... | astro-ph.EP | several measurements including the data from the laser spectrometer in the sample analysis at mars instrument suite on the curiosity rover in gale crater have measured seasonal variations in atmospheric methane at the 07 ppbv parts per billion volume level as a result models have been proposed to understand the methane... | [['several', 'measurements', 'including', 'the', 'data', 'from', 'the', 'laser', 'spectrometer', 'in', 'the', 'sample', 'analysis', 'at', 'mars', 'instrument', 'suite', 'on', 'the', 'curiosity', 'rover', 'in', 'gale', 'crater', 'have', 'measured', 'seasonal', 'variations', 'in', 'atmospheric', 'methane', 'at', 'the', '... | [-0.015572706570471578, 0.20208852984922848, -0.08087046823036004, 0.03094271769332562, -0.0017129387117073506, -0.09921655052376888, 0.06221318564413092, 0.4012928725876511, -0.23287966509422342, -0.34830873001382573, 0.08428210719171243, -0.30737290671353135, -0.10098553059489038, 0.20008454719393315, -0.044655767613... |
1,801.06871 | On large $q$ expansion in the Sachdev-Ye-Kitaev model | We consider the Sachdev-Ye-Kitaev (SYK) model where interaction involves $q$
fermions at a time. We find the next order correction to the thermal two-point
function in the large $q$ expansion. Using this result we find the next order
correction to the SYK free energy.
| hep-th cond-mat.str-el | we consider the sachdevyekitaev syk model where interaction involves q fermions at a time we find the next order correction to the thermal twopoint function in the large q expansion using this result we find the next order correction to the syk free energy | [['we', 'consider', 'the', 'sachdevyekitaev', 'syk', 'model', 'where', 'interaction', 'involves', 'q', 'fermions', 'at', 'a', 'time', 'we', 'find', 'the', 'next', 'order', 'correction', 'to', 'the', 'thermal', 'twopoint', 'function', 'in', 'the', 'large', 'q', 'expansion', 'using', 'this', 'result', 'we', 'find', 'the'... | [-0.1369568885367533, 0.16950034507846629, -0.038187328482639386, 0.10306055342979645, -0.013669525304893878, -0.11341278643389656, 0.019557068568908355, 0.2969774419272488, -0.24674715211784298, -0.2722381115467711, 0.019566895120078698, -0.31904690873555164, -0.14879787191536956, 0.06720288867787035, 0.05427573415958... |
1,801.06872 | Existence of ground state solution and concentration of maxima for a
class of indefinite variational problems | In this paper we study the existence of ground state solution and
concentration of maxima for a class of strongly indefinite problem like $$
\left\{\begin{array}{l} -\Delta u+V(x)u=A(\epsilon x)f(u) \quad \mbox{in} \quad
\R^{N}, \\ u\in H^{1}(\R^{N}), \end{array}\right. \eqno{(P)_{\epsilon}} $$
where $N \geq 1$, $\ep... | math.AP | in this paper we study the existence of ground state solution and concentration of maxima for a class of strongly indefinite problem like leftbeginarrayl delta uvxuaepsilon xfu quad mboxin quad rn uin h1rn endarrayright eqnop_epsilon where n geq 1 epsilon is a positive parameter f mathbbr to mathbbr is a continuous fun... | [['in', 'this', 'paper', 'we', 'study', 'the', 'existence', 'of', 'ground', 'state', 'solution', 'and', 'concentration', 'of', 'maxima', 'for', 'a', 'class', 'of', 'strongly', 'indefinite', 'problem', 'like', 'leftbeginarrayl', 'delta', 'uvxuaepsilon', 'xfu', 'quad', 'mboxin', 'quad', 'rn', 'uin', 'h1rn', 'endarrayrigh... | [-0.23105529223435692, 0.09237994841532782, 0.0529946997163019, -0.0420651820770997, -0.06539169396550971, -0.21097551818959237, -0.03482198781040054, 0.3516934483167937, -0.3192534812814778, -0.1282176991392459, 0.1258462597657594, -0.40667076037442756, -0.1125661700415159, 0.12309654690103516, -0.038718923998420085, ... |
1,801.06873 | Partially Coherent Sources with Inhomogeneous Azimuth | A new model of physically realizable electromagnetic source is proposed. The
source is partially coherent and non-uniformly totally polarized. The coherence
and polarization characteristics of this new source are analyzed. The spatial
coherence area of the source can be easily modified at will. The state of
polarizat... | physics.optics | a new model of physically realizable electromagnetic source is proposed the source is partially coherent and nonuniformly totally polarized the coherence and polarization characteristics of this new source are analyzed the spatial coherence area of the source can be easily modified at will the state of polarization is ... | [['a', 'new', 'model', 'of', 'physically', 'realizable', 'electromagnetic', 'source', 'is', 'proposed', 'the', 'source', 'is', 'partially', 'coherent', 'and', 'nonuniformly', 'totally', 'polarized', 'the', 'coherence', 'and', 'polarization', 'characteristics', 'of', 'this', 'new', 'source', 'are', 'analyzed', 'the', 's... | [-0.1430677730176184, 0.16379018419549404, -0.0953490604462539, 0.02806725786757414, -0.07250569903372246, -0.10360978993322746, 0.00280196863560029, 0.4129339823798265, -0.33256888625292497, -0.2691517914587885, 0.07304480492947968, -0.2667412265767286, -0.03447240050652145, 0.25940710553083063, -0.01748338350336309, ... |
1,801.06874 | Optimal Co-Optimizing of Distributed Generation and ESS Facilities
Considering Voltage Stability | The paper deals with the optimal sizing and allocation of dispersed
generation, and distributed storage systems. The optimization aims at
minimizing the sum of the costs sustained by the distributor for the power
losses, for network upgrading, for carrying out the reactive power service and
the costs of storage and c... | math.OC | the paper deals with the optimal sizing and allocation of dispersed generation and distributed storage systems the optimization aims at minimizing the sum of the costs sustained by the distributor for the power losses for network upgrading for carrying out the reactive power service and the costs of storage and capacit... | [['the', 'paper', 'deals', 'with', 'the', 'optimal', 'sizing', 'and', 'allocation', 'of', 'dispersed', 'generation', 'and', 'distributed', 'storage', 'systems', 'the', 'optimization', 'aims', 'at', 'minimizing', 'the', 'sum', 'of', 'the', 'costs', 'sustained', 'by', 'the', 'distributor', 'for', 'the', 'power', 'losses'... | [-0.19657048176070957, 0.030437488883564418, -0.05767425068964561, -0.013856999282584046, -0.0063886511591122, -0.12810454030210774, 0.0973002978247788, 0.36505993832692957, -0.2903311917614756, -0.32186335570771585, 0.16405680703958778, -0.2556344852415901, -0.06419206254438244, 0.20751389270422585, -0.073715675828244... |
1,801.06875 | The jet-ISM interactions in IC 5063 | The interstellar medium of the radio galaxy IC 5063 is highly perturbed by an
AGN jet expanding in the gaseous disc of the galaxy. We model this interaction
with relativistic hydrodynamic simulations and multiphase initial conditions
for the interstellar medium and compare the results with recent observations.
As the... | astro-ph.HE astro-ph.GA | the interstellar medium of the radio galaxy ic 5063 is highly perturbed by an agn jet expanding in the gaseous disc of the galaxy we model this interaction with relativistic hydrodynamic simulations and multiphase initial conditions for the interstellar medium and compare the results with recent observations as the jet... | [['the', 'interstellar', 'medium', 'of', 'the', 'radio', 'galaxy', 'ic', '5063', 'is', 'highly', 'perturbed', 'by', 'an', 'agn', 'jet', 'expanding', 'in', 'the', 'gaseous', 'disc', 'of', 'the', 'galaxy', 'we', 'model', 'this', 'interaction', 'with', 'relativistic', 'hydrodynamic', 'simulations', 'and', 'multiphase', 'i... | [-0.08402436825106978, 0.11803514594534677, -0.049992946228264154, 0.057794843539218044, -0.0275860912342732, -0.021301038895507118, -0.0429582667942914, 0.43776483278016787, -0.19073037868617354, -0.2873689049603166, 0.03234725219096888, -0.2709965306006976, 0.004415431539402217, 0.1805858488521866, 0.0398334433022584... |
1,801.06876 | Static and Dynamic Verification of Relational Properties on
Self-Composed C Code | Function contracts are a well-established way of formally specifying the
intended behavior of a function. However, they usually only describe what
should happen during a single call. Relational properties, on the other hand,
link several function calls. They include such properties as non-interference,
continuity and... | cs.SE | function contracts are a wellestablished way of formally specifying the intended behavior of a function however they usually only describe what should happen during a single call relational properties on the other hand link several function calls they include such properties as noninterference continuity and monotonici... | [['function', 'contracts', 'are', 'a', 'wellestablished', 'way', 'of', 'formally', 'specifying', 'the', 'intended', 'behavior', 'of', 'a', 'function', 'however', 'they', 'usually', 'only', 'describe', 'what', 'should', 'happen', 'during', 'a', 'single', 'call', 'relational', 'properties', 'on', 'the', 'other', 'hand', ... | [-0.09295621276707262, -0.0005459127688899988, -0.14480053864771852, 0.10538129491127424, -0.14066075472085662, -0.17931049100651936, 0.06224508366887332, 0.3741643262573996, -0.3085751521677987, -0.2924912067583284, 0.1325643103796284, -0.23310496668406838, -0.14959512501074052, 0.23252284063523435, -0.083585274838716... |
1,801.06877 | Limiting Distributions of Spectral Radii for Product of Matrices from
the Spherical Ensemble | Consider the product of $m$ independent $n\times n$ random matrices from the
spherical ensemble for $m\ge 1$. The spectral radius is defined as the maximum
absolute value of the $n$ eigenvalues of the product matrix. When $m=1$, the
limiting distribution for the spectral radii has been obtained by Jiang and Qi
(2017)... | math.ST stat.TH | consider the product of m independent ntimes n random matrices from the spherical ensemble for mge 1 the spectral radius is defined as the maximum absolute value of the n eigenvalues of the product matrix when m1 the limiting distribution for the spectral radii has been obtained by jiang and qi 2017 in this paper we in... | [['consider', 'the', 'product', 'of', 'm', 'independent', 'ntimes', 'n', 'random', 'matrices', 'from', 'the', 'spherical', 'ensemble', 'for', 'mge', '1', 'the', 'spectral', 'radius', 'is', 'defined', 'as', 'the', 'maximum', 'absolute', 'value', 'of', 'the', 'n', 'eigenvalues', 'of', 'the', 'product', 'matrix', 'when', ... | [-0.09281213975257495, 0.15169363715685905, -0.07642357373948802, 0.0317856930587864, 0.024738638304089282, -0.11477686032991517, 0.011713984500966034, 0.35409376919269564, -0.21662671456790783, -0.26700217715803193, 0.09877589967059479, -0.3040396899323572, -0.09325634197924625, 0.11162798104553738, -0.055016782575562... |
1,801.06878 | Density profiles of a self-gravitating lattice gas in one, two, and
three dimensions | We consider a lattice gas in spaces of dimensionality $\mathcal{D}=1,2,3$.
The particles are subject to a hardcore exclusion interaction and an attractive
pair interaction that satisfies Gauss' law as do Newtonian gravity in
$\mathcal{D}=3$, a logarithmic potential in $\mathcal{D}=2$, and a
distance-independent force... | cond-mat.stat-mech | we consider a lattice gas in spaces of dimensionality mathcald123 the particles are subject to a hardcore exclusion interaction and an attractive pair interaction that satisfies gauss law as do newtonian gravity in mathcald3 a logarithmic potential in mathcald2 and a distanceindependent force in mathcald1 under mild ad... | [['we', 'consider', 'a', 'lattice', 'gas', 'in', 'spaces', 'of', 'dimensionality', 'mathcald123', 'the', 'particles', 'are', 'subject', 'to', 'a', 'hardcore', 'exclusion', 'interaction', 'and', 'an', 'attractive', 'pair', 'interaction', 'that', 'satisfies', 'gauss', 'law', 'as', 'do', 'newtonian', 'gravity', 'in', 'mat... | [-0.1432089308426118, 0.17115279762564825, -0.1310764249410495, 0.07490736694238427, -0.008074667959648419, -0.13813368676682986, 0.046935277061181634, 0.3535932694720401, -0.23135241396183454, -0.25232257153764664, 0.05050825520207089, -0.28544947123563147, -0.04342547194676036, 0.14983387821329855, 0.0274179331639195... |
1,801.06879 | Bayesian Deep Convolutional Encoder-Decoder Networks for Surrogate
Modeling and Uncertainty Quantification | We are interested in the development of surrogate models for uncertainty
quantification and propagation in problems governed by stochastic PDEs using a
deep convolutional encoder-decoder network in a similar fashion to approaches
considered in deep learning for image-to-image regression tasks. Since normal
neural net... | physics.comp-ph cs.CV cs.LG stat.ML | we are interested in the development of surrogate models for uncertainty quantification and propagation in problems governed by stochastic pdes using a deep convolutional encoderdecoder network in a similar fashion to approaches considered in deep learning for imagetoimage regression tasks since normal neural networks ... | [['we', 'are', 'interested', 'in', 'the', 'development', 'of', 'surrogate', 'models', 'for', 'uncertainty', 'quantification', 'and', 'propagation', 'in', 'problems', 'governed', 'by', 'stochastic', 'pdes', 'using', 'a', 'deep', 'convolutional', 'encoderdecoder', 'network', 'in', 'a', 'similar', 'fashion', 'to', 'approa... | [-0.019860299327314146, -0.008087043922345726, -0.04416885495637988, 0.11079516826164658, -0.08906015678003616, -0.17486854758175452, 0.004009068685610821, 0.46668370190188596, -0.29355824592134905, -0.33420903600087676, 0.09298941019589914, -0.24781889214926242, -0.17866996206880326, 0.2223439542335145, -0.13479878124... |
1,801.0688 | A multiwavelength survey of HI-excess galaxies with surprisingly
inefficient star formation | We present the results of a multiwavelength survey of HI-excess galaxies, an
intriguing population with large HI reservoirs associated with little current
star formation. These galaxies have stellar masses $M_{\star} >10^{10}$
M$_{\odot}$, and were identified as outliers in the gas fraction vs. NUV$-r$
color and stel... | astro-ph.GA | we present the results of a multiwavelength survey of hiexcess galaxies an intriguing population with large hi reservoirs associated with little current star formation these galaxies have stellar masses m_star 1010 m_odot and were identified as outliers in the gas fraction vs nuvr color and stellar mass surface density... | [['we', 'present', 'the', 'results', 'of', 'a', 'multiwavelength', 'survey', 'of', 'hiexcess', 'galaxies', 'an', 'intriguing', 'population', 'with', 'large', 'hi', 'reservoirs', 'associated', 'with', 'little', 'current', 'star', 'formation', 'these', 'galaxies', 'have', 'stellar', 'masses', 'm_star', '1010', 'm_odot', ... | [-0.08150192712102426, 0.06813745347779143, -0.06167847231826242, 0.11659935478311242, -0.10411674876250829, -0.06259684916804305, 0.008543156833986931, 0.46120892412645714, -0.11376368156030332, -0.3480511101975517, 0.06194954560282574, -0.3071808332463665, -0.03853273381011237, 0.19633896236675202, -0.009798573522430... |
1,801.06881 | The symplectic area of a geodesic triangle in a Hermitian symmetric
space of compact type | Let $M$ be an irreducible Hermitian symmetric space of compact type, and let
$\omega$ be its K\"ahler form. For a triplet $(p_1,p_2,p_3)$ of points in $M$
we study conditions under which a geodesic triangle $\mathcal T(p_1,p_2,p_3)$
with vertices $p_1,p_2,p_3$ can be unambiguously defined. We consider the
integral $A... | math.DG | let m be an irreducible hermitian symmetric space of compact type and let omega be its kahler form for a triplet p_1p_2p_3 of points in m we study conditions under which a geodesic triangle mathcal tp_1p_2p_3 with vertices p_1p_2p_3 can be unambiguously defined we consider the integral ap_1p_2p_3int_sigma omega where s... | [['let', 'm', 'be', 'an', 'irreducible', 'hermitian', 'symmetric', 'space', 'of', 'compact', 'type', 'and', 'let', 'omega', 'be', 'its', 'kahler', 'form', 'for', 'a', 'triplet', 'p_1p_2p_3', 'of', 'points', 'in', 'm', 'we', 'study', 'conditions', 'under', 'which', 'a', 'geodesic', 'triangle', 'mathcal', 'tp_1p_2p_3', '... | [-0.21644424714301666, 0.10686635631454638, -0.09005081189853936, 0.058755697842120896, -0.10096287117675715, -0.1582650207079102, 0.013464071970317782, 0.34215474685596436, -0.24468274399177314, -0.18310928857434042, 0.10627632362758453, -0.26661011311177585, -0.13557160435935733, 0.1797022705960097, -0.10831931266050... |
1,801.06882 | Generalized Laminar Matroids | Nested matroids were introduced by Crapo in 1965 and have appeared frequently
in the literature since then. A flat of a matroid $M$ is Hamiltonian if it has
a spanning circuit. A matroid $M$ is nested if and only if its Hamiltonian
flats form a chain under inclusion; $M$ is laminar if and only if, for every
$1$-eleme... | math.CO | nested matroids were introduced by crapo in 1965 and have appeared frequently in the literature since then a flat of a matroid m is hamiltonian if it has a spanning circuit a matroid m is nested if and only if its hamiltonian flats form a chain under inclusion m is laminar if and only if for every 1element independent ... | [['nested', 'matroids', 'were', 'introduced', 'by', 'crapo', 'in', '1965', 'and', 'have', 'appeared', 'frequently', 'in', 'the', 'literature', 'since', 'then', 'a', 'flat', 'of', 'a', 'matroid', 'm', 'is', 'hamiltonian', 'if', 'it', 'has', 'a', 'spanning', 'circuit', 'a', 'matroid', 'm', 'is', 'nested', 'if', 'and', 'o... | [-0.15606131130456924, 0.14862956449016929, -0.02422305995412171, 0.012984791409224272, -0.0842278207782656, -0.1335234980247915, 0.01819647474726662, 0.38238429983658717, -0.2998841824345291, -0.2543557699425146, 0.11883968704054132, -0.2649900366514921, -0.1522673508375883, 0.17267092016339303, -0.09702105015516281, ... |
1,801.06883 | Dialectica Categories for the Lambek Calculus | We revisit the old work of de Paiva on the models of the Lambek Calculus in
dialectica models making sure that the syntactic details that were sketchy on
the first version got completed and verified. We extend the Lambek Calculus
with a \kappa modality, inspired by Yetter's work, which makes the calculus
commutative.... | cs.LO | we revisit the old work of de paiva on the models of the lambek calculus in dialectica models making sure that the syntactic details that were sketchy on the first version got completed and verified we extend the lambek calculus with a kappa modality inspired by yetters work which makes the calculus commutative then we... | [['we', 'revisit', 'the', 'old', 'work', 'of', 'de', 'paiva', 'on', 'the', 'models', 'of', 'the', 'lambek', 'calculus', 'in', 'dialectica', 'models', 'making', 'sure', 'that', 'the', 'syntactic', 'details', 'that', 'were', 'sketchy', 'on', 'the', 'first', 'version', 'got', 'completed', 'and', 'verified', 'we', 'extend'... | [-0.024869024060948305, 0.013441430782398381, -0.1267332504757782, 0.12237061690852172, -0.16570018070256887, -0.14519027502133175, 0.06664048279870395, 0.34195333626903907, -0.29752520786034836, -0.24702396894953832, 0.10691003334276113, -0.24000116893980053, -0.13957303885307884, 0.16913282170797847, -0.1772894943029... |
1,801.06884 | On the Existence of Normal Square and Nth Roots of Operators | The primary purpose of this paper is to show the existence of normal square
and nth roots of some classes of bounded operators on Hilbert spaces. Two
interesting simple results hold. Namely, under simple conditions we show that
if any operator $T$ is such that $T^2=0$, then this implies that $T$ is normal
and so $T=0... | math.FA math.OA | the primary purpose of this paper is to show the existence of normal square and nth roots of some classes of bounded operators on hilbert spaces two interesting simple results hold namely under simple conditions we show that if any operator t is such that t20 then this implies that t is normal and so t0 also we will se... | [['the', 'primary', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'show', 'the', 'existence', 'of', 'normal', 'square', 'and', 'nth', 'roots', 'of', 'some', 'classes', 'of', 'bounded', 'operators', 'on', 'hilbert', 'spaces', 'two', 'interesting', 'simple', 'results', 'hold', 'namely', 'under', 'simple', 'conditions', '... | [-0.13944631448986244, 0.18650008425379702, -0.069376872275287, 0.05696869100129206, -0.08791606313168583, -0.1282677016102932, -0.03464686295876778, 0.3636045160270493, -0.3055376861454316, -0.1425015458863386, 0.13881039620757524, -0.26929564059147953, -0.20940244079134623, 0.20084140479276089, -0.09258065663251869, ... |
1,801.06885 | Floquet Engineering in Quantum Chains | We consider a one-dimensional interacting spinless fermion model, which
displays the well-known Luttinger liquid (LL) to charge density wave (CDW)
transition as a function of the ratio between the strength of the interaction,
$U$, and the hopping, $J$. We subject this system to a spatially uniform drive
which is ramp... | cond-mat.str-el cond-mat.quant-gas cond-mat.stat-mech | we consider a onedimensional interacting spinless fermion model which displays the wellknown luttinger liquid ll to charge density wave cdw transition as a function of the ratio between the strength of the interaction u and the hopping j we subject this system to a spatially uniform drive which is ramped up over a fini... | [['we', 'consider', 'a', 'onedimensional', 'interacting', 'spinless', 'fermion', 'model', 'which', 'displays', 'the', 'wellknown', 'luttinger', 'liquid', 'll', 'to', 'charge', 'density', 'wave', 'cdw', 'transition', 'as', 'a', 'function', 'of', 'the', 'ratio', 'between', 'the', 'strength', 'of', 'the', 'interaction', '... | [-0.19797867773545544, 0.24630356208771403, -0.08036763232145737, 0.03135908954656354, 0.01296535247834909, -0.1607112903286939, 0.07010266781247114, 0.33829623012252114, -0.27123294373167983, -0.23490943988687846, 0.06935324702314588, -0.28455597493306395, -0.08739696091865722, 0.17176277939287687, 0.05123650993623618... |
1,801.06886 | An Intuitionistic Linear Logical Semantics of SAND Attack Trees | In this paper we introduce a new logical foundation of SAND attack trees in
intuitionistic linear logic. This new foundation is based on a new logic called
the Attack Tree Linear Logic (ATLL). Before introducing ATLL we given several
new logical models of attack trees, the first, is a very basic model based in
truth ... | cs.LO | in this paper we introduce a new logical foundation of sand attack trees in intuitionistic linear logic this new foundation is based on a new logic called the attack tree linear logic atll before introducing atll we given several new logical models of attack trees the first is a very basic model based in truth tables t... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'new', 'logical', 'foundation', 'of', 'sand', 'attack', 'trees', 'in', 'intuitionistic', 'linear', 'logic', 'this', 'new', 'foundation', 'is', 'based', 'on', 'a', 'new', 'logic', 'called', 'the', 'attack', 'tree', 'linear', 'logic', 'atll', 'before', 'introducing', 'atll... | [-0.1022538382501242, 0.06984908077232901, -0.13309753303714458, 0.10085454095806022, -0.1812310139219123, -0.19708361552160197, 0.12365119437827249, 0.3202330788724052, -0.2996989005579821, -0.22884713029217663, 0.10634243059326957, -0.17647620417105342, -0.17220355531435858, 0.16720769222536422, -0.15696649124068254,... |
1,801.06887 | The extremal functions for triangle-free graphs with excluded minors | We prove two results:
1. A graph $G$ on at least seven vertices with a vertex $v$ such that $G-v$
is planar and $t$ triangles satisfies $|E(G)| \leq 3|V(G)|- 9 + t/3$.
2. For $p=2,3,\ldots,9$, a triangle-free graph $G$ on at least $2p-5$
vertices with no $K_p$-minor satisfies $|E(G)|\leq (p-2)|V(G)| - (p-2)^2$.
| math.CO | we prove two results 1 a graph g on at least seven vertices with a vertex v such that gv is planar and t triangles satisfies eg leq 3vg 9 t3 2 for p23ldots9 a trianglefree graph g on at least 2p5 vertices with no k_pminor satisfies egleq p2vg p22 | [['we', 'prove', 'two', 'results', '1', 'a', 'graph', 'g', 'on', 'at', 'least', 'seven', 'vertices', 'with', 'a', 'vertex', 'v', 'such', 'that', 'gv', 'is', 'planar', 'and', 't', 'triangles', 'satisfies', 'eg', 'leq', '3vg', '9', 't3', '2', 'for', 'p23ldots9', 'a', 'trianglefree', 'graph', 'g', 'on', 'at', 'least', '2p... | [-0.20785651274997255, 0.1478214657197342, 0.005386904185718816, -0.01745178759776299, -0.08462359484932992, -0.2591202509002355, 0.026964968274747345, 0.41873540772813495, -0.19383899201436536, -0.3262086228427032, 0.05948857889186753, -0.47938668501117954, -0.07080812703656114, 0.08234136808744591, -0.029506334174505... |
1,801.06888 | On Lagrangians with Reduced-Order Euler-Lagrange Equations | If a Lagrangian defining a variational problem has order $k$ then its
Euler-Lagrange equations generically have order $2k$. This paper considers the
case where the Euler-Lagrange equations have order strictly less than $2k$, and
shows that in such a case the Lagrangian must be a polynomial in the
highest-order deriva... | math.DG | if a lagrangian defining a variational problem has order k then its eulerlagrange equations generically have order 2k this paper considers the case where the eulerlagrange equations have order strictly less than 2k and shows that in such a case the lagrangian must be a polynomial in the highestorder derivative variable... | [['if', 'a', 'lagrangian', 'defining', 'a', 'variational', 'problem', 'has', 'order', 'k', 'then', 'its', 'eulerlagrange', 'equations', 'generically', 'have', 'order', '2k', 'this', 'paper', 'considers', 'the', 'case', 'where', 'the', 'eulerlagrange', 'equations', 'have', 'order', 'strictly', 'less', 'than', '2k', 'and... | [-0.1755624912243257, 0.08543649074721195, -0.09216415993943612, 0.022943683267085555, -0.11715829920301095, -0.10380223623298585, -0.03244488158986527, 0.27041723334448453, -0.27266141790104037, -0.30517463974575415, 0.09029678840987741, -0.2791661237752897, -0.21869661641168467, 0.1485016494394934, -0.039267548305438... |
1,801.06889 | Visual Analytics in Deep Learning: An Interrogative Survey for the Next
Frontiers | Deep learning has recently seen rapid development and received significant
attention due to its state-of-the-art performance on previously-thought hard
problems. However, because of the internal complexity and nonlinear structure
of deep neural networks, the underlying decision making processes for why these
models a... | cs.HC cs.AI cs.LG stat.ML | deep learning has recently seen rapid development and received significant attention due to its stateoftheart performance on previouslythought hard problems however because of the internal complexity and nonlinear structure of deep neural networks the underlying decision making processes for why these models are achiev... | [['deep', 'learning', 'has', 'recently', 'seen', 'rapid', 'development', 'and', 'received', 'significant', 'attention', 'due', 'to', 'its', 'stateoftheart', 'performance', 'on', 'previouslythought', 'hard', 'problems', 'however', 'because', 'of', 'the', 'internal', 'complexity', 'and', 'nonlinear', 'structure', 'of', '... | [-0.011833047168781457, 0.017975692474509326, -0.08469923063931824, 0.08501760864311612, -0.17730637191053372, -0.1685912876195801, 0.036715204716723376, 0.4515080841548359, -0.2688479691572053, -0.3398825339972973, 0.10531008402360333, -0.2593004729992086, -0.24090154720831988, 0.22592987445662321, -0.1262757593643788... |
1,801.0689 | Isomorph theory of physical aging | This paper derives and discusses the configuration-space Langevin equation
describing a physically aging R-simple system and the corresponding
Smoluchowski equation. Externally controlled thermodynamic variables like
temperature, density, pressure enter the description via the single parameter
${T}_{\rm s}/T$ in whic... | cond-mat.soft cond-mat.stat-mech | this paper derives and discusses the configurationspace langevin equation describing a physically aging rsimple system and the corresponding smoluchowski equation externally controlled thermodynamic variables like temperature density pressure enter the description via the single parameter t_rm st in which t is the bath... | [['this', 'paper', 'derives', 'and', 'discusses', 'the', 'configurationspace', 'langevin', 'equation', 'describing', 'a', 'physically', 'aging', 'rsimple', 'system', 'and', 'the', 'corresponding', 'smoluchowski', 'equation', 'externally', 'controlled', 'thermodynamic', 'variables', 'like', 'temperature', 'density', 'pr... | [-0.12766752916630048, 0.21305672755956623, -0.13427421376520757, 0.005048425764601822, 0.007673773533813861, -0.16384586193007084, 0.0700390517868575, 0.3187858189831781, -0.26305832658786305, -0.2715753416186044, 0.07492621968055237, -0.2948284172530168, -0.08315836431108703, 0.13675819314470855, -0.00289307831843172... |
1,801.06891 | Law of the first passage triple of a spectrally positive strictly stable
process | For a spectrally positive and strictly stable process with index in (1,2), a
series representation is obtained for the joint distribution of the "first
passage triple" that consists of the time of first passage and the undershoot
and the overshoot at first passage. The result leads to several corollaries,
including 1... | math.PR | for a spectrally positive and strictly stable process with index in 12 a series representation is obtained for the joint distribution of the first passage triple that consists of the time of first passage and the undershoot and the overshoot at first passage the result leads to several corollaries including 1 the joint... | [['for', 'a', 'spectrally', 'positive', 'and', 'strictly', 'stable', 'process', 'with', 'index', 'in', '12', 'a', 'series', 'representation', 'is', 'obtained', 'for', 'the', 'joint', 'distribution', 'of', 'the', 'first', 'passage', 'triple', 'that', 'consists', 'of', 'the', 'time', 'of', 'first', 'passage', 'and', 'the... | [-0.11697927688326791, 0.10282687646136662, -0.12669486269598532, -0.0030840722228676217, -0.00225076561784981, -0.0743271218978356, 0.07535726229429558, 0.3429697967856844, -0.30992443470510644, -0.27436881348769243, 0.14663362249222836, -0.25180809325378095, -0.09333124833407803, 0.16619033401039926, 0.01015253248406... |
1,801.06892 | Two-photon processes based on quantum commutators | We developed a new method to calculate two-photon processes in quantum
mechanics that replaces the infinite summation over the intermediate states by
a perturbation expansion. This latter consists of a series of commutators that
involve position, momentum and hamiltonian quantum operators. We analyzed
several single-... | quant-ph physics.atm-clus physics.atom-ph | we developed a new method to calculate twophoton processes in quantum mechanics that replaces the infinite summation over the intermediate states by a perturbation expansion this latter consists of a series of commutators that involve position momentum and hamiltonian quantum operators we analyzed several single and ma... | [['we', 'developed', 'a', 'new', 'method', 'to', 'calculate', 'twophoton', 'processes', 'in', 'quantum', 'mechanics', 'that', 'replaces', 'the', 'infinite', 'summation', 'over', 'the', 'intermediate', 'states', 'by', 'a', 'perturbation', 'expansion', 'this', 'latter', 'consists', 'of', 'a', 'series', 'of', 'commutators... | [-0.11051277828495949, 0.13240616324916482, -0.1171796707753092, 0.10938057519495487, -0.036691828483715654, -0.13410856087878348, 0.04664360174536705, 0.3235369657278061, -0.2605610076186713, -0.22956134021282196, 0.05930526456236839, -0.2892313259318471, -0.1764410149566829, 0.22916223406232894, 0.009043818624690175,... |
1,801.06893 | Schubert Decomposition for Milnor Fibers of the Varieties of Singular
Matrices | We consider the varieties of singular $m \times m$ complex matrices which may
be either general, symmetric or skew-symmetric (with $m$ even). For these
varieties we have shown in another paper that they had compact "model
submanifolds", for the homotopy types of the Milnor fibers which are classical
symmetric spaces ... | math.AG | we consider the varieties of singular m times m complex matrices which may be either general symmetric or skewsymmetric with m even for these varieties we have shown in another paper that they had compact model submanifolds for the homotopy types of the milnor fibers which are classical symmetric spaces in the sense of... | [['we', 'consider', 'the', 'varieties', 'of', 'singular', 'm', 'times', 'm', 'complex', 'matrices', 'which', 'may', 'be', 'either', 'general', 'symmetric', 'or', 'skewsymmetric', 'with', 'm', 'even', 'for', 'these', 'varieties', 'we', 'have', 'shown', 'in', 'another', 'paper', 'that', 'they', 'had', 'compact', 'model',... | [-0.20937438625233798, 0.05676854758486584, -0.04384159067800889, 0.04002660531400717, -0.07133392461533235, -0.12829187512309573, -0.03567413914380736, 0.33190964544932783, -0.31391583317467436, -0.18445585919085494, 0.14533519129084502, -0.20606087428821024, -0.1910125221669053, 0.15831539166692615, -0.17036980044124... |
1,801.06894 | Transport of secondary electrons through coatings of ion-irradiated
metallic nanoparticles | The transport of low-energy electrons through the coating of a
radiosensitizing metallic nanoparticle under fast ion irradiation is analyzed
theoretically and numerically. As a case study, we consider a poly(ethylene
glycol)-coated gold nanoparticle of diameter 1.6~nm excited by a carbon ion in
the Bragg peak region ... | physics.atm-clus physics.atom-ph physics.bio-ph physics.chem-ph | the transport of lowenergy electrons through the coating of a radiosensitizing metallic nanoparticle under fast ion irradiation is analyzed theoretically and numerically as a case study we consider a polyethylene glycolcoated gold nanoparticle of diameter 16nm excited by a carbon ion in the bragg peak region in water a... | [['the', 'transport', 'of', 'lowenergy', 'electrons', 'through', 'the', 'coating', 'of', 'a', 'radiosensitizing', 'metallic', 'nanoparticle', 'under', 'fast', 'ion', 'irradiation', 'is', 'analyzed', 'theoretically', 'and', 'numerically', 'as', 'a', 'case', 'study', 'we', 'consider', 'a', 'polyethylene', 'glycolcoated',... | [-0.06695472392427276, 0.21007178694436868, -0.023952609865874466, 0.017818556683085348, 0.04102279839479172, -0.11265059251020411, 0.032173159424149035, 0.40231644319340826, -0.2456781214310063, -0.3027055038948588, 0.00821245190574758, -0.3465337747992534, -0.045329410253861356, 0.17475083592303453, 0.075643035137401... |
1,801.06895 | The $T\overline T$ deformation of quantum field theory as random
geometry | We revisit the results of Zamolodchikov and others on the deformation of
two-dimensional quantum field theory by the determinant $\det T$ of the stress
tensor, commonly referred to as $T\overline T$. Infinitesimally this is
equivalent to a random coordinate transformation, with a local action which is,
however, a tot... | hep-th | we revisit the results of zamolodchikov and others on the deformation of twodimensional quantum field theory by the determinant det t of the stress tensor commonly referred to as toverline t infinitesimally this is equivalent to a random coordinate transformation with a local action which is however a total derivative ... | [['we', 'revisit', 'the', 'results', 'of', 'zamolodchikov', 'and', 'others', 'on', 'the', 'deformation', 'of', 'twodimensional', 'quantum', 'field', 'theory', 'by', 'the', 'determinant', 'det', 't', 'of', 'the', 'stress', 'tensor', 'commonly', 'referred', 'to', 'as', 'toverline', 't', 'infinitesimally', 'this', 'is', '... | [-0.13760980425509983, 0.13097704662821996, -0.08280815513163774, 0.06716411353514777, -0.10346663564555028, -0.11792822874700412, 0.02464626462927136, 0.3385622673628167, -0.2833185587675335, -0.2088218921214406, 0.12268387139118157, -0.24092995912298307, -0.20897119829200336, 0.14666087498975933, -0.08716776926452532... |
1,801.06896 | Ranking Causal Influence of Financial Markets via Directed Information
Graphs | A non-parametric method for ranking stock indices according to their mutual
causal influences is presented. Under the assumption that indices reflect the
underlying economy of a country, such a ranking indicates which countries exert
the most economic influence in an examined subset of the global economy. The
propose... | q-fin.ST eess.SP | a nonparametric method for ranking stock indices according to their mutual causal influences is presented under the assumption that indices reflect the underlying economy of a country such a ranking indicates which countries exert the most economic influence in an examined subset of the global economy the proposed meth... | [['a', 'nonparametric', 'method', 'for', 'ranking', 'stock', 'indices', 'according', 'to', 'their', 'mutual', 'causal', 'influences', 'is', 'presented', 'under', 'the', 'assumption', 'that', 'indices', 'reflect', 'the', 'underlying', 'economy', 'of', 'a', 'country', 'such', 'a', 'ranking', 'indicates', 'which', 'countr... | [-0.07404767750749286, 0.1265725548071825, -0.1080439563500673, 0.09839315313688467, -0.09099216583215505, -0.1006373179302564, 0.07566637187696634, 0.37754239166426545, -0.24843375104645643, -0.32172376568376704, 0.09179674026921408, -0.33940303795249527, -0.16620804464768077, 0.18431224184960102, -0.0609191230010731,... |
1,801.06897 | The Optimal Majority Threshold as a Function of the Variation
Coefficient of the Environment | Within the model of social dynamics determined by collective decisions in a
stochastic environment (ViSE model), we consider the case of a homogeneous
society consisting of classically rational economic agents (or homines
economici, or egoists). We present expressions for the optimal majority
threshold and the maximu... | math.OC cs.MA cs.SY math.PR physics.soc-ph | within the model of social dynamics determined by collective decisions in a stochastic environment vise model we consider the case of a homogeneous society consisting of classically rational economic agents or homines economici or egoists we present expressions for the optimal majority threshold and the maximum expecte... | [['within', 'the', 'model', 'of', 'social', 'dynamics', 'determined', 'by', 'collective', 'decisions', 'in', 'a', 'stochastic', 'environment', 'vise', 'model', 'we', 'consider', 'the', 'case', 'of', 'a', 'homogeneous', 'society', 'consisting', 'of', 'classically', 'rational', 'economic', 'agents', 'or', 'homines', 'eco... | [-0.14364631712436676, 0.1149479189394818, -0.03810746718818943, 0.0445349776558578, -0.02180078996345401, -0.10281508017331362, 0.1195840720180422, 0.32678813601533574, -0.26849056002994376, -0.2801094114780426, 0.09966711326657483, -0.2578687847902377, -0.15609272879005098, 0.1434652757893006, -0.05564538556151092, 0... |
1,801.06898 | The early evolution of viscous and self-gravitating circumstellar disks
with a dust component | The long-term evolution of a circumstellar disk starting from its formation
and ending in the T Tauri phase was simulated numerically with the purpose of
studying the evolution of dust in the disk with distinct values of viscous
\alpha-parameter and dust fragmentation velocity v_frag. We solved numerical
hydrodynamic... | astro-ph.EP astro-ph.GA astro-ph.SR | the longterm evolution of a circumstellar disk starting from its formation and ending in the t tauri phase was simulated numerically with the purpose of studying the evolution of dust in the disk with distinct values of viscous alphaparameter and dust fragmentation velocity v_frag we solved numerical hydrodynamics equa... | [['the', 'longterm', 'evolution', 'of', 'a', 'circumstellar', 'disk', 'starting', 'from', 'its', 'formation', 'and', 'ending', 'in', 'the', 't', 'tauri', 'phase', 'was', 'simulated', 'numerically', 'with', 'the', 'purpose', 'of', 'studying', 'the', 'evolution', 'of', 'dust', 'in', 'the', 'disk', 'with', 'distinct', 'va... | [-0.08835842276655384, 0.17312250810209662, -0.04249002545509698, 0.02619772602783367, -0.021759396930333966, -0.05340930988350239, -0.02974667609669268, 0.3691271972950876, -0.24602340362012773, -0.3144607966086306, 0.09769118480375563, -0.2697098490155343, 0.0007865040910096382, 0.1636583639034978, -0.022833802656116... |
1,801.06899 | Enhanced thermoelectric performance in Ca substituted Sr3SnO | We report 45% enhancement in the thermoelectric figure of merit, ZT of Sr3SnO
via Ca substitution. First-principles calculations have been performed to study
the electronic and thermoelectric transport properties of Ca substituted Sr3SnO
(Sr3-xCaxSnO). The effects of Ca subtitution on bandgap are studied and
detailed... | cond-mat.mtrl-sci | we report 45 enhancement in the thermoelectric figure of merit zt of sr3sno via ca substitution firstprinciples calculations have been performed to study the electronic and thermoelectric transport properties of ca substituted sr3sno sr3xcaxsno the effects of ca subtitution on bandgap are studied and detailed mechanism... | [['we', 'report', '45', 'enhancement', 'in', 'the', 'thermoelectric', 'figure', 'of', 'merit', 'zt', 'of', 'sr3sno', 'via', 'ca', 'substitution', 'firstprinciples', 'calculations', 'have', 'been', 'performed', 'to', 'study', 'the', 'electronic', 'and', 'thermoelectric', 'transport', 'properties', 'of', 'ca', 'substitut... | [-0.07823250207981867, 0.08253942067882546, -0.040014908092505325, -0.06197087249360842, -0.006952367615091001, -0.12554184236086724, 0.09922001470709446, 0.4056895364802785, -0.2211912185862297, -0.32632906827621344, 0.02213339989255296, -0.39636438374475735, -0.1023640859417799, 0.26098824911580487, 0.023475500143973... |
1,801.069 | Efficient Learning of Optimal Markov Network Topology with k-Tree
Modeling | The seminal work of Chow and Liu (1968) shows that approximation of a finite
probabilistic system by Markov trees can achieve the minimum information loss
with the topology of a maximum spanning tree. Our current paper generalizes the
result to Markov networks of tree width $\leq k$, for every fixed $k\geq 2$. In
par... | cs.DS cs.AI | the seminal work of chow and liu 1968 shows that approximation of a finite probabilistic system by markov trees can achieve the minimum information loss with the topology of a maximum spanning tree our current paper generalizes the result to markov networks of tree width leq k for every fixed kgeq 2 in particular we pr... | [['the', 'seminal', 'work', 'of', 'chow', 'and', 'liu', '1968', 'shows', 'that', 'approximation', 'of', 'a', 'finite', 'probabilistic', 'system', 'by', 'markov', 'trees', 'can', 'achieve', 'the', 'minimum', 'information', 'loss', 'with', 'the', 'topology', 'of', 'a', 'maximum', 'spanning', 'tree', 'our', 'current', 'pa... | [-0.15240767300400856, 0.11446858168410538, -0.0584070755603866, 0.0722894965361695, -0.08894734121485184, -0.15155903746910993, 0.08134125823403171, 0.3872568129126771, -0.31450671328054947, -0.3109184843420058, 0.10198570130032616, -0.22946258940237718, -0.1805358070771407, 0.15979122434382456, -0.08731629034286759, ... |
1,801.06901 | Investigation of the energy shielding of kidney stones by cavitation
bubble clouds during burst wave lithotripsy | We conduct experiments and numerical simulations of the dynamics of bubble
clouds nucleated on the surface of an epoxy cylindrical stone model during
burst wave lithotripsy (BWL). In the experiment, the bubble clouds are
visualized and bubble-scattered acoustics are measured. In the numerical
simulation, we combine m... | physics.med-ph | we conduct experiments and numerical simulations of the dynamics of bubble clouds nucleated on the surface of an epoxy cylindrical stone model during burst wave lithotripsy bwl in the experiment the bubble clouds are visualized and bubblescattered acoustics are measured in the numerical simulation we combine methods fo... | [['we', 'conduct', 'experiments', 'and', 'numerical', 'simulations', 'of', 'the', 'dynamics', 'of', 'bubble', 'clouds', 'nucleated', 'on', 'the', 'surface', 'of', 'an', 'epoxy', 'cylindrical', 'stone', 'model', 'during', 'burst', 'wave', 'lithotripsy', 'bwl', 'in', 'the', 'experiment', 'the', 'bubble', 'clouds', 'are',... | [-0.13458244889865026, 0.11541633547963369, -0.07294696495929898, 0.05927233944975716, -0.01622394311844426, -0.006655171502600698, 0.04891161700738046, 0.36778827068560266, -0.22809767927152708, -0.3291837250923409, 0.06658971383482876, -0.3012108903871301, -0.09761268612243892, 0.21450279421474347, 0.0490175026667523... |
1,801.06902 | Ex Vivo Mouse Brain Microscopy at 15T with Loop-Gap RF Coil | The design of a loop-gap-resonator RF coil optimized for ex vivo mouse brain
microscopy at ultra high fields is described and its properties characterized
using simulations, phantoms and experimental scans of mouse brains fixed in 10%
formalin containing 4 mM Magnevist. The RF (B1) and magnetic field (B0)
homogeneiti... | physics.med-ph | the design of a loopgapresonator rf coil optimized for ex vivo mouse brain microscopy at ultra high fields is described and its properties characterized using simulations phantoms and experimental scans of mouse brains fixed in 10 formalin containing 4 mm magnevist the rf b1 and magnetic field b0 homogeneities are expe... | [['the', 'design', 'of', 'a', 'loopgapresonator', 'rf', 'coil', 'optimized', 'for', 'ex', 'vivo', 'mouse', 'brain', 'microscopy', 'at', 'ultra', 'high', 'fields', 'is', 'described', 'and', 'its', 'properties', 'characterized', 'using', 'simulations', 'phantoms', 'and', 'experimental', 'scans', 'of', 'mouse', 'brains', ... | [-0.05801250581902002, 0.10350081420402188, -0.00818275765287785, 0.024889092746691235, -0.048024423581985186, -0.1486099282609058, 0.015317611718236715, 0.44762884293283733, -0.1908222524507437, -0.3690788573553773, 0.07342443157456258, -0.2531128843397308, -0.1179987943294097, 0.23201788223323216, -0.0525642161092841... |
1,801.06903 | Unveiling the phase diagram of a striped cuprate at high magnetic
fields: Hidden order of Cooper pairs | The interplay of charge orders with superconductivity in underdoped cuprates
at high magnetic fields ($H$) is an open question, and even the value of the
upper critical field ($H_{c2}$), a measure of the strength of
superconductivity, has been the subject of a long-term debate. We combined
three complementary transpo... | cond-mat.supr-con cond-mat.dis-nn cond-mat.str-el | the interplay of charge orders with superconductivity in underdoped cuprates at high magnetic fields h is an open question and even the value of the upper critical field h_c2 a measure of the strength of superconductivity has been the subject of a longterm debate we combined three complementary transport techniques on ... | [['the', 'interplay', 'of', 'charge', 'orders', 'with', 'superconductivity', 'in', 'underdoped', 'cuprates', 'at', 'high', 'magnetic', 'fields', 'h', 'is', 'an', 'open', 'question', 'and', 'even', 'the', 'value', 'of', 'the', 'upper', 'critical', 'field', 'h_c2', 'a', 'measure', 'of', 'the', 'strength', 'of', 'supercon... | [-0.22180797864380658, 0.2538868344088874, -0.05431817486925332, 0.04988459026238622, -0.037866815389499694, -0.1298177163262915, 0.14770986638592645, 0.3065365109719453, -0.23204479459185562, -0.27410420042301736, 0.020294157407217274, -0.330586717069071, -0.05261685909869159, 0.1829380877730461, 0.04702442403470108, ... |
1,801.06904 | The exact Power Law for Buffon's needle landing near some Random Cantor
Sets | In this paper, we study the Favard length of some random Cantor sets of
Hausdorff dimension 1. We start with a unit disk in the plane and replace the
unit disk by $4$ disjoint subdisks (with equal distance to each other) of
radius $1/4$ inside and tangent to the unit disk. By repeating this operation
in a self-simila... | math.AP math.CA math.PR | in this paper we study the favard length of some random cantor sets of hausdorff dimension 1 we start with a unit disk in the plane and replace the unit disk by 4 disjoint subdisks with equal distance to each other of radius 14 inside and tangent to the unit disk by repeating this operation in a selfsimilar manner and ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'favard', 'length', 'of', 'some', 'random', 'cantor', 'sets', 'of', 'hausdorff', 'dimension', '1', 'we', 'start', 'with', 'a', 'unit', 'disk', 'in', 'the', 'plane', 'and', 'replace', 'the', 'unit', 'disk', 'by', '4', 'disjoint', 'subdisks', 'with', 'equal', 'distance', 'to... | [-0.15074548249630385, 0.1801382585589486, -0.012584938194572806, 0.037096671904549454, -0.012034382050236067, -0.1306238222725121, 0.04534736923157166, 0.31607255097791875, -0.25176803553738747, -0.2240881542095458, 0.09379212999806168, -0.3207581969254826, -0.0942529679601451, 0.16043092092278463, -0.0722094357507415... |
1,801.06905 | Holographic superconductor with nonlinear arcsin-electrodynamics | We investigate holographic s-wave superconductors with nonlinear
arcsin-electrodynamics in the background of Schwarzschild anti-de Sitter black
holes. The analytical Sturm-Liouville eigenvalue problem is explored and we
assume that the scalar and electromagnetic fields do not influence on the
background metric (the p... | hep-th | we investigate holographic swave superconductors with nonlinear arcsinelectrodynamics in the background of schwarzschild antide sitter black holes the analytical sturmliouville eigenvalue problem is explored and we assume that the scalar and electromagnetic fields do not influence on the background metric the probe lim... | [['we', 'investigate', 'holographic', 'swave', 'superconductors', 'with', 'nonlinear', 'arcsinelectrodynamics', 'in', 'the', 'background', 'of', 'schwarzschild', 'antide', 'sitter', 'black', 'holes', 'the', 'analytical', 'sturmliouville', 'eigenvalue', 'problem', 'is', 'explored', 'and', 'we', 'assume', 'that', 'the', ... | [-0.13473951908933923, 0.11498713989591139, -0.07650287686354988, 0.08358492727232415, -0.07402012608727683, -0.12138386362050546, 0.02069481385008591, 0.3343556871471124, -0.15576770616036545, -0.26056897134436824, 0.08169109251717394, -0.3210882406257759, -0.15079529084855828, 0.1848128528317164, 0.036060650359718054... |
1,801.06906 | Summatory function of the number of prime factors | We consider the summatory function of the number of prime factors for
integers $\leq x$ over arithmetic progressions. Numerical experiments suggest
that some arithmetic progressions consist more number of prime factors than
others. Greg Martin conjectured that the difference of the summatory functions
should attain a... | math.NT | we consider the summatory function of the number of prime factors for integers leq x over arithmetic progressions numerical experiments suggest that some arithmetic progressions consist more number of prime factors than others greg martin conjectured that the difference of the summatory functions should attain a consta... | [['we', 'consider', 'the', 'summatory', 'function', 'of', 'the', 'number', 'of', 'prime', 'factors', 'for', 'integers', 'leq', 'x', 'over', 'arithmetic', 'progressions', 'numerical', 'experiments', 'suggest', 'that', 'some', 'arithmetic', 'progressions', 'consist', 'more', 'number', 'of', 'prime', 'factors', 'than', 'o... | [-0.22022509194348105, 0.08917156622636241, -0.10224245418492076, 0.14612874103704007, -0.039199334768844504, -0.13633669548752633, 0.06942815116497797, 0.30749126325373527, -0.23751521950841628, -0.26325697339647874, 0.03263161667205345, -0.27467122468069294, -0.1583248431032354, 0.2702948244246231, -0.102805638927724... |
1,801.06907 | Ab initio Simulations of Superionic H2O, H2O2, and H9O4 Compounds | Using density functional molecular dynamics simulations, we study the
behavior of different hydrogen-oxygen compounds at megabar pressures and
several thousands of degrees Kelvin where water has been predicted to occur in
superionic form. When we study the close packed hcp and dhcp structures of
superionic water, we ... | cond-mat.mtrl-sci astro-ph.EP | using density functional molecular dynamics simulations we study the behavior of different hydrogenoxygen compounds at megabar pressures and several thousands of degrees kelvin where water has been predicted to occur in superionic form when we study the close packed hcp and dhcp structures of superionic water we find t... | [['using', 'density', 'functional', 'molecular', 'dynamics', 'simulations', 'we', 'study', 'the', 'behavior', 'of', 'different', 'hydrogenoxygen', 'compounds', 'at', 'megabar', 'pressures', 'and', 'several', 'thousands', 'of', 'degrees', 'kelvin', 'where', 'water', 'has', 'been', 'predicted', 'to', 'occur', 'in', 'supe... | [-0.07063834463338275, 0.21211730176071217, -0.06561088909850465, 0.009889268661096979, -0.01560542799256087, -0.08596965121770543, 0.09174500579132115, 0.44885938800359654, -0.19796480804779004, -0.30199403461237734, 0.02528080965486959, -0.3154724156688694, -0.11992863452082479, 0.11869863257359631, 0.068384396619736... |
1,801.06908 | Spectral analysis of the spin-boson Hamiltonian with two photons for
arbitrary coupling | We study the spectrum of the spin-boson model with two photons in
$\mathbb{R}^d$ for arbitrary coupling $\alpha>0$. It is shown that the discrete
spectrum is finite and the essential spectrum consists of a half-line the
bottom of which is a unique zero of a simple Nevanlinna function. Besides the
simplicity and more ... | math.SP math-ph math.MP | we study the spectrum of the spinboson model with two photons in mathbbrd for arbitrary coupling alpha0 it is shown that the discrete spectrum is finite and the essential spectrum consists of a halfline the bottom of which is a unique zero of a simple nevanlinna function besides the simplicity and more abstract nature ... | [['we', 'study', 'the', 'spectrum', 'of', 'the', 'spinboson', 'model', 'with', 'two', 'photons', 'in', 'mathbbrd', 'for', 'arbitrary', 'coupling', 'alpha0', 'it', 'is', 'shown', 'that', 'the', 'discrete', 'spectrum', 'is', 'finite', 'and', 'the', 'essential', 'spectrum', 'consists', 'of', 'a', 'halfline', 'the', 'botto... | [-0.11738688512167965, 0.10757095554473405, -0.1072036623954773, 0.05615041648539213, -0.06107066276495178, -0.11959240334227872, 0.008635527024475427, 0.33270419501842785, -0.23654016907302997, -0.233986636910301, 0.07080441962655944, -0.2800317227553863, -0.1337183257445502, 0.18617567282396918, -0.028072674102030504... |
1,801.06909 | Admissible modules and normality of classical nilpotent orbits I | In the case of complex symplectic and orthogonal groups, we find
$(\mathfrak{g}, K)-$modules with the property that their $K-$structure matches
the structure of regular functions on the closures of nilpotent orbits. This
establishes a version of the Orbit Method of Kirrilov-Kostant-Souriau as
proposed by Vogan. In th... | math.RT math.AG | in the case of complex symplectic and orthogonal groups we find mathfrakg kmodules with the property that their kstructure matches the structure of regular functions on the closures of nilpotent orbits this establishes a version of the orbit method of kirrilovkostantsouriau as proposed by vogan in the process we give a... | [['in', 'the', 'case', 'of', 'complex', 'symplectic', 'and', 'orthogonal', 'groups', 'we', 'find', 'mathfrakg', 'kmodules', 'with', 'the', 'property', 'that', 'their', 'kstructure', 'matches', 'the', 'structure', 'of', 'regular', 'functions', 'on', 'the', 'closures', 'of', 'nilpotent', 'orbits', 'this', 'establishes', ... | [-0.1979894607146788, 0.03161012647776968, -0.11503129373563246, 0.019552863496579045, -0.0867444412692243, -0.07044516377694283, 0.033035485125664205, 0.33713107435808826, -0.2893615420907736, -0.20579342973522013, 0.09266073117356023, -0.1808582456142176, -0.16868876442054492, 0.21456843520152485, -0.1305366518338107... |
1,801.0691 | Variable coefficient Wolff-type inequalities and sharp local smoothing
estimates for wave equations on manifolds | The sharp Wolff-type decoupling estimates of Bourgain--Demeter are extended
to the variable coefficient setting. These results are applied to obtain new
sharp local smoothing estimates for wave equations on compact Riemannian
manifolds, away from the endpoint regularity exponent. More generally, local
smoothing estim... | math.AP math.CA | the sharp wolfftype decoupling estimates of bourgaindemeter are extended to the variable coefficient setting these results are applied to obtain new sharp local smoothing estimates for wave equations on compact riemannian manifolds away from the endpoint regularity exponent more generally local smoothing estimates are ... | [['the', 'sharp', 'wolfftype', 'decoupling', 'estimates', 'of', 'bourgaindemeter', 'are', 'extended', 'to', 'the', 'variable', 'coefficient', 'setting', 'these', 'results', 'are', 'applied', 'to', 'obtain', 'new', 'sharp', 'local', 'smoothing', 'estimates', 'for', 'wave', 'equations', 'on', 'compact', 'riemannian', 'ma... | [-0.1023899933664749, 0.07687200711419186, -0.0896332202355067, 0.16380063549149781, -0.08786369540030137, -0.14081903748835126, -0.005214681476354599, 0.3346472087005774, -0.2666129535684983, -0.20853117940326532, 0.16391189989323418, -0.2898483311136564, -0.1102905763934056, 0.26917768048122526, -0.09336492773145437,... |
1,801.06911 | Braces of order $p^2q$ | In this article we classify the left braces of order $p^2q$ where $p,q$ are
primes fulfilling $q > p+1$. This classification includes a proof of three
conjectures of Guarnieri and Vendramin (\cite[Conjectures
6.2-6.4]{Vendramin_skew}) concerning the number of isomorphism classes of left
braces of order $p^2q$ for cer... | math.QA | in this article we classify the left braces of order p2q where pq are primes fulfilling q p1 this classification includes a proof of three conjectures of guarnieri and vendramin citeconjectures 6264vendramin_skew concerning the number of isomorphism classes of left braces of order p2q for certain values of pq | [['in', 'this', 'article', 'we', 'classify', 'the', 'left', 'braces', 'of', 'order', 'p2q', 'where', 'pq', 'are', 'primes', 'fulfilling', 'q', 'p1', 'this', 'classification', 'includes', 'a', 'proof', 'of', 'three', 'conjectures', 'of', 'guarnieri', 'and', 'vendramin', 'citeconjectures', '6264vendramin_skew', 'concerni... | [-0.24113178930859616, 0.0759038420077017, -0.00021194181642792326, 0.06335281570283498, -0.04315774569763465, -0.1640582616401321, -0.015073208639304093, 0.26184836465944633, -0.3144234045547374, -0.2758935471957034, 0.13082136891217547, -0.2861319059862735, -0.07324630088430453, 0.15509913861751556, -0.10517785317720... |
1,801.06912 | Magnus-Zassenhaus methods for the semiclassical Schr\"odinger equation
with oscillatory time-dependent potentials | Schr\"odinger equations with time-dependent potentials are of central
importance in quantum physics and theoretical chemistry, where they aid in the
simulation and design of systems and processes at atomic scales. Numerical
approximation of these equations is particularly difficult in the semiclassical
regime because... | math.NA physics.chem-ph | schrodinger equations with timedependent potentials are of central importance in quantum physics and theoretical chemistry where they aid in the simulation and design of systems and processes at atomic scales numerical approximation of these equations is particularly difficult in the semiclassical regime because of the... | [['schrodinger', 'equations', 'with', 'timedependent', 'potentials', 'are', 'of', 'central', 'importance', 'in', 'quantum', 'physics', 'and', 'theoretical', 'chemistry', 'where', 'they', 'aid', 'in', 'the', 'simulation', 'and', 'design', 'of', 'systems', 'and', 'processes', 'at', 'atomic', 'scales', 'numerical', 'appro... | [-0.12267250074286952, 0.11645835961165432, -0.08520318313594197, 0.06599978681916784, -0.0568524094277154, -0.13121390382169199, 0.019063359618769916, 0.3572185155828945, -0.27645147603204234, -0.279604640810658, 0.0970395689302316, -0.24230619411009546, -0.18553072885869654, 0.22883609282777054, -0.04281606452667531,... |
1,801.06913 | Magnus-Lanczos methods with simplified commutators for the Schr\"odinger
equation with a time-dependent potential | The computation of the Schr\"odinger equation featuring time-dependent
potentials is of great importance in quantum control of atomic and molecular
processes. These applications often involve highly oscillatory potentials and
require inexpensive but accurate solutions over large spatio-temporal windows.
In this work ... | math.NA physics.chem-ph | the computation of the schrodinger equation featuring timedependent potentials is of great importance in quantum control of atomic and molecular processes these applications often involve highly oscillatory potentials and require inexpensive but accurate solutions over large spatiotemporal windows in this work we devel... | [['the', 'computation', 'of', 'the', 'schrodinger', 'equation', 'featuring', 'timedependent', 'potentials', 'is', 'of', 'great', 'importance', 'in', 'quantum', 'control', 'of', 'atomic', 'and', 'molecular', 'processes', 'these', 'applications', 'often', 'involve', 'highly', 'oscillatory', 'potentials', 'and', 'require'... | [-0.10587956428672875, 0.10889430898890572, -0.10759313835105935, 0.05129115489124488, -0.1073420772321339, -0.14081487911142654, 0.03009383774889236, 0.372532482350581, -0.2573215015868076, -0.250716333185918, 0.08934582891248044, -0.23054050093673678, -0.16204218344942314, 0.24177018326104116, -0.03264944220212723, 0... |
1,801.06914 | Maximal metrics for the first Steklov eigenvalue on surfaces | In recent years, eigenvalue optimization problems have received a lot of
attention, in particular, due to their connection with the theory of minimal
surfaces. In the present paper we prove that on any orientable surface there
exists a smooth metric maximizing the first normalized Steklov eigenvalue. For
surfaces of ... | math.DG math.SP | in recent years eigenvalue optimization problems have received a lot of attention in particular due to their connection with the theory of minimal surfaces in the present paper we prove that on any orientable surface there exists a smooth metric maximizing the first normalized steklov eigenvalue for surfaces of genus z... | [['in', 'recent', 'years', 'eigenvalue', 'optimization', 'problems', 'have', 'received', 'a', 'lot', 'of', 'attention', 'in', 'particular', 'due', 'to', 'their', 'connection', 'with', 'the', 'theory', 'of', 'minimal', 'surfaces', 'in', 'the', 'present', 'paper', 'we', 'prove', 'that', 'on', 'any', 'orientable', 'surfac... | [-0.15679164668906806, 0.07392136880450371, -0.10740017714159726, 0.02353844756274077, -0.09163917976802269, -0.15901551711671416, 0.003720756253969033, 0.35688561399114654, -0.21781905809218444, -0.264604475855538, 0.12517652050840658, -0.2903361029705955, -0.2079624602507836, 0.1821168703705217, -0.18283805065761202,... |
1,801.06915 | Generically free representations III: extremely bad characteristic | In parts I and II, we determined which faithful irreducible representations
$V$ of a simple linear algebraic group $G$ are generically free for Lie($G$),
i.e., which $V$ have an open subset consisting of vectors whose stabilizer in
Lie($G$) is zero, with some assumptions on the characteristic of the field.
This paper... | math.RT math.GR | in parts i and ii we determined which faithful irreducible representations v of a simple linear algebraic group g are generically free for lieg ie which v have an open subset consisting of vectors whose stabilizer in lieg is zero with some assumptions on the characteristic of the field this paper settles the remaining ... | [['in', 'parts', 'i', 'and', 'ii', 'we', 'determined', 'which', 'faithful', 'irreducible', 'representations', 'v', 'of', 'a', 'simple', 'linear', 'algebraic', 'group', 'g', 'are', 'generically', 'free', 'for', 'lieg', 'ie', 'which', 'v', 'have', 'an', 'open', 'subset', 'consisting', 'of', 'vectors', 'whose', 'stabilize... | [-0.16398845693246195, 0.13136677647586717, -0.0761806158670446, -0.0008286788776916053, -0.10510283995175823, -0.19132438783292724, -0.005723422274015667, 0.36135161929719506, -0.2882908910479663, -0.22520884523345602, 0.10496743008566443, -0.22348464018709602, -0.13857699808708968, 0.20133629820442625, -0.07843659041... |
1,801.06916 | On multi-poly-Bernoulli-Carlitz numbers | We introduce multi-poly-Bernoulli-Carlitz numbers, function field analogues
of multi-poly-Bernoulli numbers of Imatomi-Kaneko-Takeda. We explicitly
describe multi-poly-Bernoulli Carlitz numbers in terms of the Carlitz factorial
and the Stirling-Carlitz numbers of the second kind and also show their
relationships with... | math.NT | we introduce multipolybernoullicarlitz numbers function field analogues of multipolybernoulli numbers of imatomikanekotakeda we explicitly describe multipolybernoulli carlitz numbers in terms of the carlitz factorial and the stirlingcarlitz numbers of the second kind and also show their relationships with function fiel... | [['we', 'introduce', 'multipolybernoullicarlitz', 'numbers', 'function', 'field', 'analogues', 'of', 'multipolybernoulli', 'numbers', 'of', 'imatomikanekotakeda', 'we', 'explicitly', 'describe', 'multipolybernoulli', 'carlitz', 'numbers', 'in', 'terms', 'of', 'the', 'carlitz', 'factorial', 'and', 'the', 'stirlingcarlit... | [-0.2456166140724566, 0.14941465173085983, -0.08110459610311822, 0.15090717032382434, -0.07230714518068866, -0.018488528376275844, 0.030499576696787368, 0.2538593556858938, -0.30959137207405135, -0.31667218935167923, 0.007761518203716894, -0.21090588820251552, -0.2136810682290657, 0.2249018476048315, -0.065652127039026... |
1,801.06917 | Magnified Image Spatial Spectrum (MISS) microscopy for nanometer and
millisecond scale label-free imaging | Label-free imaging of rapidly moving, sub-diffraction sized structures has
important applications in both biology and material science, as it removes the
limitations associated with fluorescence tagging. However, unlabeled nanoscale
particles in suspension are difficult to image due to their transparency and
fast Bro... | physics.optics physics.bio-ph | labelfree imaging of rapidly moving subdiffraction sized structures has important applications in both biology and material science as it removes the limitations associated with fluorescence tagging however unlabeled nanoscale particles in suspension are difficult to image due to their transparency and fast brownian mo... | [['labelfree', 'imaging', 'of', 'rapidly', 'moving', 'subdiffraction', 'sized', 'structures', 'has', 'important', 'applications', 'in', 'both', 'biology', 'and', 'material', 'science', 'as', 'it', 'removes', 'the', 'limitations', 'associated', 'with', 'fluorescence', 'tagging', 'however', 'unlabeled', 'nanoscale', 'par... | [-0.03962215268640013, 0.1346544395472142, -0.08076209851303662, 0.021947417703743737, -0.08826776076460907, -0.17953147864817867, 0.010218764588990409, 0.46492829927127566, -0.3065001573303395, -0.34813012182712555, 0.08482810642471063, -0.2918872179287161, -0.14447966072268884, 0.2327808992895532, -0.1045593635052354... |
1,801.06918 | Rational extensions of the representation ring global functor and a
splitting of global equivariant $K$-theory | We identify the group of homomorphisms
$\operatorname{Hom}_{\mathcal{GF}}(F,\mathbf{RU}_{\mathbb Q})$ in the category
of ($\operatorname{fin}$)-global functors to the rationalization of the unitary
representation ring functor and deduce that the higher
$\operatorname{Ext}$-groups
$\operatorname{Ext}^n_{\mathcal{GF}}(... | math.AT math.RT | we identify the group of homomorphisms operatornamehom_mathcalgffmathbfru_mathbb q in the category of operatornamefinglobal functors to the rationalization of the unitary representation ring functor and deduce that the higher operatornameextgroups operatornameextn_mathcalgffmathbfru_mathbb q ngeq 2 have to vanish this ... | [['we', 'identify', 'the', 'group', 'of', 'homomorphisms', 'operatornamehom_mathcalgffmathbfru_mathbb', 'q', 'in', 'the', 'category', 'of', 'operatornamefinglobal', 'functors', 'to', 'the', 'rationalization', 'of', 'the', 'unitary', 'representation', 'ring', 'functor', 'and', 'deduce', 'that', 'the', 'higher', 'operato... | [-0.22663930783455727, 0.06257912905753724, -0.12894431141072085, 0.05635913487390748, -0.08185767706350557, -0.12595862615853548, -0.014008585574837135, 0.340039886906743, -0.3931294286623597, -0.21280126398695368, 0.0381091464344146, -0.21682936711004003, -0.11658554023264774, 0.14145012775968227, -0.1516779288117374... |
1,801.06919 | Looking for the phase transition - recent NA61/SHINE results | The fixed-target NA61/SHINE experiment (SPS CERN) looks for the critical
point of strongly interacting matter and the properties of the onset of
deconfinement. It is a two dimensional scan of measurements of particle spectra
and fluctuations in proton-proton, proton-nucleus and nucleus-nucleus
interactions as a funct... | hep-ex hep-ph | the fixedtarget na61shine experiment sps cern looks for the critical point of strongly interacting matter and the properties of the onset of deconfinement it is a two dimensional scan of measurements of particle spectra and fluctuations in protonproton protonnucleus and nucleusnucleus interactions as a function of coll... | [['the', 'fixedtarget', 'na61shine', 'experiment', 'sps', 'cern', 'looks', 'for', 'the', 'critical', 'point', 'of', 'strongly', 'interacting', 'matter', 'and', 'the', 'properties', 'of', 'the', 'onset', 'of', 'deconfinement', 'it', 'is', 'a', 'two', 'dimensional', 'scan', 'of', 'measurements', 'of', 'particle', 'spectr... | [-0.06974702024076512, 0.26931259602871793, -0.16246255439909874, 0.11260950509323805, -0.023423441297685105, -0.09782393637072781, -0.021063130542946357, 0.32154212151552836, -0.20185399157049108, -0.31567035892478906, -0.004482025928471399, -0.37419359013438225, 0.0042999042822318015, 0.14017864902068497, 0.064239060... |
1,801.0692 | Cross-Domain Transfer in Reinforcement Learning using Target Apprentice | In this paper, we present a new approach to Transfer Learning (TL) in
Reinforcement Learning (RL) for cross-domain tasks. Many of the available
techniques approach the transfer architecture as a method of speeding up the
target task learning. We propose to adapt and reuse the mapped source task
optimal-policy directl... | cs.AI cs.LG stat.ML | in this paper we present a new approach to transfer learning tl in reinforcement learning rl for crossdomain tasks many of the available techniques approach the transfer architecture as a method of speeding up the target task learning we propose to adapt and reuse the mapped source task optimalpolicy directly in relate... | [['in', 'this', 'paper', 'we', 'present', 'a', 'new', 'approach', 'to', 'transfer', 'learning', 'tl', 'in', 'reinforcement', 'learning', 'rl', 'for', 'crossdomain', 'tasks', 'many', 'of', 'the', 'available', 'techniques', 'approach', 'the', 'transfer', 'architecture', 'as', 'a', 'method', 'of', 'speeding', 'up', 'the',... | [-0.01474386227891955, -0.027643819731451913, -0.06874636871361872, 0.05212796758678451, -0.1256297614236246, -0.17000855441801832, 0.10584367834962904, 0.48043456056620926, -0.3226561558112735, -0.3582323785230983, 0.044678540590211924, -0.20957096093479777, -0.15386900122393854, 0.22997749883325014, -0.17167212880303... |
1,801.06921 | String topology with gravitational descendants, and periods of
Landau-Ginzburg potentials | This paper introduces new operations on the string topology of a smooth
manifold: gravitational descendants of its cotangent bundle, which are
augmentations of the Chas-Sullivan $L_\infty$ algebra structure of the loop
space. The definition extends to Liouville domains. Descendants of the
$n$-torus are computed.
To... | math.SG math.AG math.AT | this paper introduces new operations on the string topology of a smooth manifold gravitational descendants of its cotangent bundle which are augmentations of the chassullivan l_infty algebra structure of the loop space the definition extends to liouville domains descendants of the ntorus are computed to a monotone lagr... | [['this', 'paper', 'introduces', 'new', 'operations', 'on', 'the', 'string', 'topology', 'of', 'a', 'smooth', 'manifold', 'gravitational', 'descendants', 'of', 'its', 'cotangent', 'bundle', 'which', 'are', 'augmentations', 'of', 'the', 'chassullivan', 'l_infty', 'algebra', 'structure', 'of', 'the', 'loop', 'space', 'th... | [-0.24944869807346703, 0.056486900684211964, -0.07614833710249513, 0.08294437825432087, -0.14759802826719873, -0.11110818362794816, -0.039015174860709365, 0.27961093579676555, -0.30243061657281634, -0.21771108298661543, 0.07278166871215712, -0.21391923051386913, -0.19455128177465436, 0.12330229843451464, -0.18597150127... |
1,801.06922 | Chiral symmetry breaking and monopoles in gauge theories | QCD monopoles are magnetically charged quasiparticles whose Bose-Einstein
condensation (BEC) at $T<T_c$ creates electric confinement and flux tubes. The
"magnetic scenario" of QCD proposes that scattering on the non-condensed
component of the monopole ensemble at $T>T_c$ plays an important role in
explaining the prop... | hep-ph nucl-th | qcd monopoles are magnetically charged quasiparticles whose boseeinstein condensation bec at tt_c creates electric confinement and flux tubes the magnetic scenario of qcd proposes that scattering on the noncondensed component of the monopole ensemble at tt_c plays an important role in explaining the properties of stron... | [['qcd', 'monopoles', 'are', 'magnetically', 'charged', 'quasiparticles', 'whose', 'boseeinstein', 'condensation', 'bec', 'at', 'tt_c', 'creates', 'electric', 'confinement', 'and', 'flux', 'tubes', 'the', 'magnetic', 'scenario', 'of', 'qcd', 'proposes', 'that', 'scattering', 'on', 'the', 'noncondensed', 'component', 'o... | [-0.1768251093472265, 0.28712314567295094, -0.08484958528665601, 0.05130610018775793, -0.0074880228164327, -0.08231192871714664, 0.019915680808851578, 0.3603372609741084, -0.17348087606892273, -0.23577016306103796, 0.0042738191691482335, -0.3394773883662026, -0.08560346693369993, 0.05981443852414585, 0.0864363619108583... |
1,801.06923 | Anomalous energy shift of laterally confined two-dimensional excitons | We theoretically investigate the energy of the ground state exciton confined
to two-dimensional (2D) monolayers with circular shape. Within an effective
mass approach employing a nonlocal screening effect on the Coulomb potential
energy, we demonstrate how the exciton energy is correlated with the radius of
the circl... | cond-mat.mes-hall cond-mat.mtrl-sci | we theoretically investigate the energy of the ground state exciton confined to twodimensional 2d monolayers with circular shape within an effective mass approach employing a nonlocal screening effect on the coulomb potential energy we demonstrate how the exciton energy is correlated with the radius of the circle elect... | [['we', 'theoretically', 'investigate', 'the', 'energy', 'of', 'the', 'ground', 'state', 'exciton', 'confined', 'to', 'twodimensional', '2d', 'monolayers', 'with', 'circular', 'shape', 'within', 'an', 'effective', 'mass', 'approach', 'employing', 'a', 'nonlocal', 'screening', 'effect', 'on', 'the', 'coulomb', 'potentia... | [-0.10926509288878276, 0.17030444534795877, -0.02075131747994743, 0.049292214184025324, 0.01799039010375995, -0.11857119585847718, 0.04673870121150267, 0.42438050522201365, -0.24432809002183634, -0.295103593611683, -0.045265760029205813, -0.2992150177269232, -0.13200315164573406, 0.13696609908747004, 0.0315181444848662... |
1,801.06924 | Hyperuniform States of Matter | Hyperuniform states of matter are correlated systems that are characterized
by an anomalous suppression of long-wavelength (i.e., large-length-scale)
density fluctuations compared to those found in garden-variety disordered
systems, such as ordinary fluids and amorphous solids. All perfect crystals,
perfect quasicrys... | cond-mat.stat-mech | hyperuniform states of matter are correlated systems that are characterized by an anomalous suppression of longwavelength ie largelengthscale density fluctuations compared to those found in gardenvariety disordered systems such as ordinary fluids and amorphous solids all perfect crystals perfect quasicrystals and speci... | [['hyperuniform', 'states', 'of', 'matter', 'are', 'correlated', 'systems', 'that', 'are', 'characterized', 'by', 'an', 'anomalous', 'suppression', 'of', 'longwavelength', 'ie', 'largelengthscale', 'density', 'fluctuations', 'compared', 'to', 'those', 'found', 'in', 'gardenvariety', 'disordered', 'systems', 'such', 'as... | [-0.1496656759083271, 0.20491885891236597, -0.07258344310987741, 0.05691948136175051, -0.044271193681284786, -0.15544191314466296, 0.014477952857036144, 0.35554482059925796, -0.2865476275607943, -0.2747633228190243, 0.07378870201064273, -0.2960719116907567, -0.2284206713018939, 0.14966955126915127, -0.02420036752102896... |
1,801.06925 | Quantum fluctuation theorem to benchmark quantum annealers | Near term quantum hardware promises unprecedented computational advantage.
Crucial in its development is the characterization and minimization of
computational errors. We propose the use of the quantum fluctuation theorem to
benchmark the performance of quantum annealers. This versatile tool provides
simple means to ... | quant-ph cond-mat.stat-mech | near term quantum hardware promises unprecedented computational advantage crucial in its development is the characterization and minimization of computational errors we propose the use of the quantum fluctuation theorem to benchmark the performance of quantum annealers this versatile tool provides simple means to deter... | [['near', 'term', 'quantum', 'hardware', 'promises', 'unprecedented', 'computational', 'advantage', 'crucial', 'in', 'its', 'development', 'is', 'the', 'characterization', 'and', 'minimization', 'of', 'computational', 'errors', 'we', 'propose', 'the', 'use', 'of', 'the', 'quantum', 'fluctuation', 'theorem', 'to', 'benc... | [-0.12100034146837817, 0.10828910193542081, -0.13085988788666686, 0.07032161305679448, -0.04880105570387723, -0.171367010698141, 0.051018275576905255, 0.3322285478516074, -0.29886442394613216, -0.3028637042708611, 0.08239935786499945, -0.23836031979410333, -0.14335707413147758, 0.25624421009469484, -0.0976721438045582,... |
1,801.06926 | Multiplexed Quantum Random Number Generation | Fast secure random number generation is essential for high-speed encrypted
communication, and is the backbone of information security. Generation of truly
random numbers depends on the intrinsic randomness of the process used and is
usually limited by electronic bandwidth and signal processing data rates. Here
we use... | quant-ph | fast secure random number generation is essential for highspeed encrypted communication and is the backbone of information security generation of truly random numbers depends on the intrinsic randomness of the process used and is usually limited by electronic bandwidth and signal processing data rates here we use a mul... | [['fast', 'secure', 'random', 'number', 'generation', 'is', 'essential', 'for', 'highspeed', 'encrypted', 'communication', 'and', 'is', 'the', 'backbone', 'of', 'information', 'security', 'generation', 'of', 'truly', 'random', 'numbers', 'depends', 'on', 'the', 'intrinsic', 'randomness', 'of', 'the', 'process', 'used',... | [-0.20761020211538186, 0.12105971915551697, -0.02343355468077458, 0.013717178563624519, -0.04158821296490108, -0.19622403031539623, 0.11646085813867324, 0.41056079942394386, -0.2878795832564885, -0.3155445579552289, 0.11299987325698814, -0.2657139901138814, -0.07566158022646877, 0.2626560474763568, -0.06806080470524842... |
1,801.06927 | Implications of new physics in the decays $B_c \to
(J/\psi,\eta_c)\tau\nu$ | We study the semileptonic decays of the $B_c$ meson into final charmonium
states within the standard model and beyond. The relevant hadronic transition
form factors are calculated in the framework of the covariant confined quark
model developed by us. We focus on the tau mode of these decays, which may
provide some h... | hep-ph | we study the semileptonic decays of the b_c meson into final charmonium states within the standard model and beyond the relevant hadronic transition form factors are calculated in the framework of the covariant confined quark model developed by us we focus on the tau mode of these decays which may provide some hints of... | [['we', 'study', 'the', 'semileptonic', 'decays', 'of', 'the', 'b_c', 'meson', 'into', 'final', 'charmonium', 'states', 'within', 'the', 'standard', 'model', 'and', 'beyond', 'the', 'relevant', 'hadronic', 'transition', 'form', 'factors', 'are', 'calculated', 'in', 'the', 'framework', 'of', 'the', 'covariant', 'confine... | [-0.0471960107456003, 0.21167826422502653, -0.06498877749046576, 0.1077825523264307, -0.05885432851209771, -0.1377483580352938, 0.08044161850661372, 0.258152967002908, -0.21067022300537377, -0.21494245826865413, -0.0061045461812422475, -0.29482266707678456, -0.06251937809117537, 0.1349302349366813, 0.08782919759271733,... |
1,801.06928 | Edge-Preserving Piecewise Linear Image Smoothing Using Piecewise
Constant Filters | Most image smoothing filters in the literature assume a piecewise constant
model of smoothed output images. However, the piecewise constant model
assumption can cause artifacts such as gradient reversals in applications such
as image detail enhancement, HDR tone mapping, etc. In these applications, a
piecewise linear... | cs.GR | most image smoothing filters in the literature assume a piecewise constant model of smoothed output images however the piecewise constant model assumption can cause artifacts such as gradient reversals in applications such as image detail enhancement hdr tone mapping etc in these applications a piecewise linear model a... | [['most', 'image', 'smoothing', 'filters', 'in', 'the', 'literature', 'assume', 'a', 'piecewise', 'constant', 'model', 'of', 'smoothed', 'output', 'images', 'however', 'the', 'piecewise', 'constant', 'model', 'assumption', 'can', 'cause', 'artifacts', 'such', 'as', 'gradient', 'reversals', 'in', 'applications', 'such',... | [-0.03556330728902852, 0.03784542754348592, -0.07058271191837491, 0.04141152866117387, -0.08204834866730204, -0.16348367326623614, 0.007850458633003151, 0.45621323782153966, -0.3215350980136869, -0.33443080854226265, 0.08947207887323169, -0.20289886740025087, -0.19871352730649916, 0.21071937029300458, -0.10860524985221... |
1,801.06929 | Introduction to teleparallel gravities | We give a pedagogical introduction into the field of (modified) teleparallel
theories of gravity. Our presentation is fairly self-contained. In particular,
we carefully explain the basic principles of metric-affine approaches to
gravity.
This contribution is based on our talk "Teleparallel gravity, its
modification... | gr-qc hep-th | we give a pedagogical introduction into the field of modified teleparallel theories of gravity our presentation is fairly selfcontained in particular we carefully explain the basic principles of metricaffine approaches to gravity this contribution is based on our talk teleparallel gravity its modifications and the loca... | [['we', 'give', 'a', 'pedagogical', 'introduction', 'into', 'the', 'field', 'of', 'modified', 'teleparallel', 'theories', 'of', 'gravity', 'our', 'presentation', 'is', 'fairly', 'selfcontained', 'in', 'particular', 'we', 'carefully', 'explain', 'the', 'basic', 'principles', 'of', 'metricaffine', 'approaches', 'to', 'gr... | [-0.10187312113837554, 0.08183263280930428, -0.20073981838873944, 0.1169400258652436, -0.21736470320476936, -0.1548075570939825, -0.06031179973998895, 0.2342210822380506, -0.1828427373073422, -0.35457554379334816, 0.04732952785248367, -0.23868051374760957, -0.17417210221577148, 0.12159036552676787, -0.16864212655390684... |
1,801.0693 | Alternance Theorems and Chebyshev Splines Approximation | One of the purposes in this paper is to provide a better understanding of the
alternance property which occurs in Chebyshev polynomial approximation and
piecewise polynomial approximation problems. In the first part of this paper,
we propose an original approach to obtain new proofs of the well known
necessary and su... | math.NA | one of the purposes in this paper is to provide a better understanding of the alternance property which occurs in chebyshev polynomial approximation and piecewise polynomial approximation problems in the first part of this paper we propose an original approach to obtain new proofs of the well known necessary and suffic... | [['one', 'of', 'the', 'purposes', 'in', 'this', 'paper', 'is', 'to', 'provide', 'a', 'better', 'understanding', 'of', 'the', 'alternance', 'property', 'which', 'occurs', 'in', 'chebyshev', 'polynomial', 'approximation', 'and', 'piecewise', 'polynomial', 'approximation', 'problems', 'in', 'the', 'first', 'part', 'of', '... | [-0.08575062435980428, 0.0026486745051415845, -0.1250489086760625, 0.1113339376448195, -0.10527214977487143, -0.1350525657806212, 0.016932629502322803, 0.35295729896526284, -0.279991527852505, -0.2862834222136941, 0.13827867667562566, -0.1686528359379953, -0.19684139759898353, 0.20399978660992277, -0.10449756138415923,... |
1,801.06931 | Multipole analysis in the radiation field for linearized $f(R)$ gravity
with irreducible Cartesian tensors | The $1/r$-expansion in the distance to the source is applied to the
linearized $f(R)$ gravity, and its multipole expansion in the radiation field
with irreducible Cartesian tensors is presented. Then, the energy, momentum,
and angular momentum in the gravitational waves are provided for linearized
$f(R)$ gravity. All... | gr-qc | the 1rexpansion in the distance to the source is applied to the linearized fr gravity and its multipole expansion in the radiation field with irreducible cartesian tensors is presented then the energy momentum and angular momentum in the gravitational waves are provided for linearized fr gravity all of these results ha... | [['the', '1rexpansion', 'in', 'the', 'distance', 'to', 'the', 'source', 'is', 'applied', 'to', 'the', 'linearized', 'fr', 'gravity', 'and', 'its', 'multipole', 'expansion', 'in', 'the', 'radiation', 'field', 'with', 'irreducible', 'cartesian', 'tensors', 'is', 'presented', 'then', 'the', 'energy', 'momentum', 'and', 'a... | [-0.16763362200244478, 0.09738895669694389, -0.07364016447396002, 0.07839181857886152, -0.09833501624515313, -0.08021110914271783, -0.14265833120474494, 0.26929466275236846, -0.22448963211163095, -0.28492857833605323, 0.0548581109441441, -0.2527398315274663, -0.10583186033998795, 0.1384468073058024, 0.00239616212549439... |
1,801.06932 | Soft X-ray Imager aboard Hitomi (ASTRO-H) | The Soft X-ray Imager (SXI) is an imaging spectrometer using charge-coupled
devices (CCDs) aboard the Hitomi X-ray observatory. The SXI sensor has four
CCDs with an imaging area size of $31~{\rm mm} \times 31~{\rm mm}$ arranged in
a $2 \times 2$ array. Combined with the X-ray mirror, the Soft X-ray Telescope,
the SXI... | astro-ph.IM | the soft xray imager sxi is an imaging spectrometer using chargecoupled devices ccds aboard the hitomi xray observatory the sxi sensor has four ccds with an imaging area size of 31rm mm times 31rm mm arranged in a 2 times 2 array combined with the xray mirror the soft xray telescope the sxi detects xrays between 04rm k... | [['the', 'soft', 'xray', 'imager', 'sxi', 'is', 'an', 'imaging', 'spectrometer', 'using', 'chargecoupled', 'devices', 'ccds', 'aboard', 'the', 'hitomi', 'xray', 'observatory', 'the', 'sxi', 'sensor', 'has', 'four', 'ccds', 'with', 'an', 'imaging', 'area', 'size', 'of', '31rm', 'mm', 'times', '31rm', 'mm', 'arranged', '... | [-0.0714068273967617, 0.16360705582716642, -0.010969666869641514, 0.03526538871543986, -0.011363702607923187, -0.12732644389810352, 0.019392392054442098, 0.47361825685948133, -0.19408437562378822, -0.40479863435029984, 0.1074060212437568, -0.3701173370354809, -0.023967730904890534, 0.2156010253832695, -0.08521500847321... |
1,801.06933 | Heirarchical and synergistic self-assembly in composites of model
Wormlike micellar-polymers and nanoparticles results in nanostructures with
diverse morphologies | Using Monte Carlo simulations, we investigate the self-assembly of model
nanoparticles inside a matrix of model equilibrium polymers (or matrix of
Wormlike micelles) as a function of the polymeric matrix density and the
excluded volume parameter between polymers and nanoparticles. In this paper, we
show morphological... | cond-mat.soft | using monte carlo simulations we investigate the selfassembly of model nanoparticles inside a matrix of model equilibrium polymers or matrix of wormlike micelles as a function of the polymeric matrix density and the excluded volume parameter between polymers and nanoparticles in this paper we show morphological transit... | [['using', 'monte', 'carlo', 'simulations', 'we', 'investigate', 'the', 'selfassembly', 'of', 'model', 'nanoparticles', 'inside', 'a', 'matrix', 'of', 'model', 'equilibrium', 'polymers', 'or', 'matrix', 'of', 'wormlike', 'micelles', 'as', 'a', 'function', 'of', 'the', 'polymeric', 'matrix', 'density', 'and', 'the', 'ex... | [-0.10490327120603372, 0.2003665381959743, -0.08345616453223759, -0.028582276837486358, 0.017010256450416313, -0.10234471620991827, 0.02974787266769757, 0.4369103492165191, -0.27215603369805547, -0.293486037419902, 0.025171990105364885, -0.26865531090853945, -0.18465966394792, 0.09256082247942686, 0.05062861415454083, ... |
1,801.06934 | On the Iteration Complexity Analysis of Stochastic Primal-Dual Hybrid
Gradient Approach with High Probability | In this paper, we propose a stochastic Primal-Dual Hybrid Gradient (PDHG)
approach for solving a wide spectrum of regularized stochastic minimization
problems, where the regularization term is composite with a linear function. It
has been recognized that solving this kind of problem is challenging since the
closed-fo... | cs.LG stat.ML | in this paper we propose a stochastic primaldual hybrid gradient pdhg approach for solving a wide spectrum of regularized stochastic minimization problems where the regularization term is composite with a linear function it has been recognized that solving this kind of problem is challenging since the closedform soluti... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'stochastic', 'primaldual', 'hybrid', 'gradient', 'pdhg', 'approach', 'for', 'solving', 'a', 'wide', 'spectrum', 'of', 'regularized', 'stochastic', 'minimization', 'problems', 'where', 'the', 'regularization', 'term', 'is', 'composite', 'with', 'a', 'linear', 'function', '... | [-0.10458103944917886, 0.003096286974720318, -0.0740814591249959, 0.07067364857572432, -0.07879224669093012, -0.14482813930160113, 0.05098470736001301, 0.3536018487806855, -0.3197823331078821, -0.31252742902142927, 0.13640351132727863, -0.26536803573121276, -0.16199947000925682, 0.2025116171544968, -0.0786114803565645,... |
1,801.06935 | A procedure for observing rocky exoplanets to maximize the likelihood
that atmospheric oxygen will be a biosignature | Here we advocate an observational strategy to help prioritize exoplanet
observations. It starts with more easily obtained observational data, and ranks
exoplanets for more difficult follow-up observations based on the likelihood of
avoiding planets for which oxygen is a false positives or even an inconclusive
signatu... | astro-ph.EP | here we advocate an observational strategy to help prioritize exoplanet observations it starts with more easily obtained observational data and ranks exoplanets for more difficult followup observations based on the likelihood of avoiding planets for which oxygen is a false positives or even an inconclusive signature of... | [['here', 'we', 'advocate', 'an', 'observational', 'strategy', 'to', 'help', 'prioritize', 'exoplanet', 'observations', 'it', 'starts', 'with', 'more', 'easily', 'obtained', 'observational', 'data', 'and', 'ranks', 'exoplanets', 'for', 'more', 'difficult', 'followup', 'observations', 'based', 'on', 'the', 'likelihood',... | [-0.06913636914773465, 0.1883490167116785, -0.07157621151526217, 0.12593626700820298, -0.15078500540780457, -0.1461907837031133, 0.14234089144587483, 0.40419068965302024, -0.1775775068025622, -0.3322815362846962, 0.18169476997206435, -0.2605348887801584, -0.13454399686479182, 0.2424901997028091, -0.13438313283215933, 0... |
1,801.06936 | Evolution of Regional Innovation with Spatial Knowledge Spillovers:
Convergence or Divergence? | This paper extends endogenous economic growth models to incorporate knowledge
externality. We explores whether spatial knowledge spillovers among regions
exist, whether spatial knowledge spillovers promote regional innovative
activities, and whether external knowledge spillovers affect the evolution of
regional innov... | econ.EM stat.AP | this paper extends endogenous economic growth models to incorporate knowledge externality we explores whether spatial knowledge spillovers among regions exist whether spatial knowledge spillovers promote regional innovative activities and whether external knowledge spillovers affect the evolution of regional innovation... | [['this', 'paper', 'extends', 'endogenous', 'economic', 'growth', 'models', 'to', 'incorporate', 'knowledge', 'externality', 'we', 'explores', 'whether', 'spatial', 'knowledge', 'spillovers', 'among', 'regions', 'exist', 'whether', 'spatial', 'knowledge', 'spillovers', 'promote', 'regional', 'innovative', 'activities',... | [-0.039204368741337425, 0.046982797772710624, -0.06815718499563851, 0.11769367132937192, -0.12895604499697105, -0.059237019708199265, 0.06230016409089445, 0.41131784679205385, -0.24800977490823128, -0.3488244448191694, 0.10319220323626459, -0.2761493885021621, -0.166259386511723, 0.1322814007131473, -0.0678660158538124... |
1,801.06937 | The $^{87}$Rubidium Atomic Clock Maser in Giant Stars | We conducted a Green Bank Telescope search for the ground state 6.8 GHz
hyperfine transition of rubidium ($^{87}$Rb) toward giant stars detected in Rb
I optical resonance lines. The spin-flip transition of $^{87}$Rb is one of the
principal transitions used in atomic clocks, in addition to the hydrogen 21 cm
maser and... | astro-ph.SR | we conducted a green bank telescope search for the ground state 68 ghz hyperfine transition of rubidium 87rb toward giant stars detected in rb i optical resonance lines the spinflip transition of 87rb is one of the principal transitions used in atomic clocks in addition to the hydrogen 21 cm maser and the 133cs hyperfi... | [['we', 'conducted', 'a', 'green', 'bank', 'telescope', 'search', 'for', 'the', 'ground', 'state', '68', 'ghz', 'hyperfine', 'transition', 'of', 'rubidium', '87rb', 'toward', 'giant', 'stars', 'detected', 'in', 'rb', 'i', 'optical', 'resonance', 'lines', 'the', 'spinflip', 'transition', 'of', '87rb', 'is', 'one', 'of',... | [-0.12414121384678695, 0.2103571672207461, 0.09925200390772751, -0.030744729432626627, 0.037040378381229505, -0.15299127894776085, 0.16461521742614701, 0.45598557501552234, -0.08383444368910904, -0.24087360909638497, 0.005348429120763635, -0.26654196299540883, 0.03455387188408237, 0.1197750291612465, 0.0988429543884614... |
1,801.06938 | Randomized sampling for basis functions construction in generalized
finite element methods | In the framework of generalized finite element methods for elliptic equations
with rough coefficients, efficiency and accuracy of the numerical method depend
critically on the use of appropriate basis functions. This work explores
several random sampling strategies that construct approximations to the optimal
set of ... | math.OC math.NA | in the framework of generalized finite element methods for elliptic equations with rough coefficients efficiency and accuracy of the numerical method depend critically on the use of appropriate basis functions this work explores several random sampling strategies that construct approximations to the optimal set of basi... | [['in', 'the', 'framework', 'of', 'generalized', 'finite', 'element', 'methods', 'for', 'elliptic', 'equations', 'with', 'rough', 'coefficients', 'efficiency', 'and', 'accuracy', 'of', 'the', 'numerical', 'method', 'depend', 'critically', 'on', 'the', 'use', 'of', 'appropriate', 'basis', 'functions', 'this', 'work', 'e... | [-0.07855233028071162, 0.04480685889835895, -0.12455168394026933, 0.06384785807214355, -0.05085699483867229, -0.12760342698958185, 0.09566485267822389, 0.4155157505086175, -0.24577329097959547, -0.2542750377575924, 0.1074706686899227, -0.21571758248049905, -0.17479733488074056, 0.23455223396282504, -0.07999204801694479... |
1,801.06939 | Binary energy source of the HH 250 outflow and its circumstellar
environment | Herbig-Haro flows are signposts of recent major accretion and outflow
episodes. We aim to determine the nature and properties of the little-known
outflow source HH 250-IRS, which is embedded in the Aquila clouds. We have
obtained adaptive optics-assisted L-band images with the NACO instrument on the
Very Large Telesc... | astro-ph.SR astro-ph.GA | herbigharo flows are signposts of recent major accretion and outflow episodes we aim to determine the nature and properties of the littleknown outflow source hh 250irs which is embedded in the aquila clouds we have obtained adaptive opticsassisted lband images with the naco instrument on the very large telescope vlt to... | [['herbigharo', 'flows', 'are', 'signposts', 'of', 'recent', 'major', 'accretion', 'and', 'outflow', 'episodes', 'we', 'aim', 'to', 'determine', 'the', 'nature', 'and', 'properties', 'of', 'the', 'littleknown', 'outflow', 'source', 'hh', '250irs', 'which', 'is', 'embedded', 'in', 'the', 'aquila', 'clouds', 'we', 'have'... | [-0.0730080349720508, 0.0637833454686958, -0.041221120214619995, 0.007989459473938837, -0.08194064171848832, -0.11116933194668896, 0.0007910948857685456, 0.46684569101372775, -0.18134399348815536, -0.3274104166639982, 0.12290681494602995, -0.2973045838825119, -0.02389073933399942, 0.16798477250480187, 0.008309589071585... |
1,801.0694 | MRI Cross-Modality NeuroImage-to-NeuroImage Translation | We present a cross-modality generation framework that learns to generate
translated modalities from given modalities in MR images without real
acquisition. Our proposed method performs NeuroImage-to-NeuroImage translation
(abbreviated as N2N) by means of a deep learning model that leverages
conditional generative adv... | cs.CV | we present a crossmodality generation framework that learns to generate translated modalities from given modalities in mr images without real acquisition our proposed method performs neuroimagetoneuroimage translation abbreviated as n2n by means of a deep learning model that leverages conditional generative adversarial... | [['we', 'present', 'a', 'crossmodality', 'generation', 'framework', 'that', 'learns', 'to', 'generate', 'translated', 'modalities', 'from', 'given', 'modalities', 'in', 'mr', 'images', 'without', 'real', 'acquisition', 'our', 'proposed', 'method', 'performs', 'neuroimagetoneuroimage', 'translation', 'abbreviated', 'as'... | [0.027033347116823262, -0.029484398382326634, -0.06446585552725892, 0.07917146814478324, -0.09317319448175737, -0.1661728971723943, -0.05203468949915554, 0.47798357825594984, -0.27441842374617503, -0.33433351343259676, 0.041377502058669594, -0.24431558280756557, -0.25529920476558515, 0.20380103477945608, -0.16695247610... |
1,801.06941 | Finite-temperature behavior of a classical spin-orbit-coupled model for
$\textrm{YbMgGaO}_4$ with and without bond disorder | We present the results of finite-temperature classical Monte Carlo
simulations of a strongly spin-orbit-coupled nearest-neighbor
triangular-lattice model for the candidate $\mathrm{U}(1)$ quantum spin liquid
$\mathrm{YbMgGaO}_4$ at large system sizes. We find a single continuous
finite-temperature stripe-ordering tra... | cond-mat.str-el | we present the results of finitetemperature classical monte carlo simulations of a strongly spinorbitcoupled nearestneighbor triangularlattice model for the candidate mathrmu1 quantum spin liquid mathrmybmggao_4 at large system sizes we find a single continuous finitetemperature stripeordering transition with slowly di... | [['we', 'present', 'the', 'results', 'of', 'finitetemperature', 'classical', 'monte', 'carlo', 'simulations', 'of', 'a', 'strongly', 'spinorbitcoupled', 'nearestneighbor', 'triangularlattice', 'model', 'for', 'the', 'candidate', 'mathrmu1', 'quantum', 'spin', 'liquid', 'mathrmybmggao_4', 'at', 'large', 'system', 'sizes... | [-0.1823828473999879, 0.21129156171554958, -0.052011143555524796, 0.08771485602398178, -0.019353402744516406, -0.16733882742777575, 0.07962120436454859, 0.35019721016015887, -0.24985809454245725, -0.25469799972662743, 0.05306369380899671, -0.28771598083748867, -0.1524088817587408, 0.08845904766731508, 0.050439324727907... |
1,801.06942 | Evaluation of the Interplanetary Magnetic Field Strength Using the
Cosmic-Ray Shadow of the Sun | We analyze the Sun's shadow observed with the Tibet-III air shower array and
find that the shadow's center deviates northward (southward) from the optical
solar disc center in the "Away" ("Toward") IMF sector. By comparing with
numerical simulations based on the solar magnetic field model, we find that the
average IM... | astro-ph.SR astro-ph.EP physics.space-ph | we analyze the suns shadow observed with the tibetiii air shower array and find that the shadows center deviates northward southward from the optical solar disc center in the away toward imf sector by comparing with numerical simulations based on the solar magnetic field model we find that the average imf strength in t... | [['we', 'analyze', 'the', 'suns', 'shadow', 'observed', 'with', 'the', 'tibetiii', 'air', 'shower', 'array', 'and', 'find', 'that', 'the', 'shadows', 'center', 'deviates', 'northward', 'southward', 'from', 'the', 'optical', 'solar', 'disc', 'center', 'in', 'the', 'away', 'toward', 'imf', 'sector', 'by', 'comparing', 'w... | [-0.09910994178958629, 0.14591831969783495, -0.037788509197631166, 0.057996523941523936, 0.007261858409956882, -0.03714503796379033, 0.008552005497346584, 0.38027018026301734, -0.15867091283986443, -0.4343943761367547, 0.043759008700420196, -0.31224430888204985, -0.052894833056550274, 0.22591041294661793, -0.0532522318... |
1,801.06943 | Strictly unital A-infinity algebras | Given a graded module over a commutative ring, we define a dg-Lie algebra
whose Maurer-Cartan elements are the strictly unital A-infinity algebra
structures on that module. We use this to generalize Positselski's result that
a curvature term on the bar construction compensates for a lack of
augmentation, from a field... | math.KT | given a graded module over a commutative ring we define a dglie algebra whose maurercartan elements are the strictly unital ainfinity algebra structures on that module we use this to generalize positselskis result that a curvature term on the bar construction compensates for a lack of augmentation from a field to arbit... | [['given', 'a', 'graded', 'module', 'over', 'a', 'commutative', 'ring', 'we', 'define', 'a', 'dglie', 'algebra', 'whose', 'maurercartan', 'elements', 'are', 'the', 'strictly', 'unital', 'ainfinity', 'algebra', 'structures', 'on', 'that', 'module', 'we', 'use', 'this', 'to', 'generalize', 'positselskis', 'result', 'that... | [-0.1863905610464346, 0.034990706329307196, -0.08020179626647006, 0.026451077341007885, -0.15656258153279176, -0.1450822786061784, -0.061274046481199815, 0.36391368091859844, -0.4461897603979104, -0.1378190452860815, 0.0863260869564635, -0.15932237619620465, -0.199360557873681, 0.16345168521439427, -0.19920548003459915... |
1,801.06944 | Fine-Tuning, Complexity, and Life in the Multiverse | The physical processes that determine the properties of our everyday world,
and of the wider cosmos, are determined by some key numbers: the 'constants' of
micro-physics and the parameters that describe the expanding universe in which
we have emerged. We identify various steps in the emergence of stars, planets
and l... | physics.hist-ph astro-ph.CO astro-ph.GA physics.pop-ph | the physical processes that determine the properties of our everyday world and of the wider cosmos are determined by some key numbers the constants of microphysics and the parameters that describe the expanding universe in which we have emerged we identify various steps in the emergence of stars planets and life that a... | [['the', 'physical', 'processes', 'that', 'determine', 'the', 'properties', 'of', 'our', 'everyday', 'world', 'and', 'of', 'the', 'wider', 'cosmos', 'are', 'determined', 'by', 'some', 'key', 'numbers', 'the', 'constants', 'of', 'microphysics', 'and', 'the', 'parameters', 'that', 'describe', 'the', 'expanding', 'univers... | [-0.09671000780687088, 0.18742119950248198, -0.12293888635950971, 0.1379716898733457, -0.13270993526650113, -0.13212757133849481, 0.018920396977402974, 0.37509921192537127, -0.23228078074284694, -0.32325810163557156, 0.11596533150189563, -0.22756976499837242, -0.15903385023955466, 0.2198265731179466, -0.054519593838672... |
1,801.06945 | Localization of magnon modes in a curved magnetic nanowire | Spin waves in magnetic nanowires can be bound by a local bending of the wire.
The eigenfrequency of a truly local magnon mode is determined by the curvature:
a general analytical expression is established for any infinitesimally weak
localized curvature of the wire. The interaction of the local mode with spin
waves, ... | cond-mat.mes-hall cond-mat.str-el | spin waves in magnetic nanowires can be bound by a local bending of the wire the eigenfrequency of a truly local magnon mode is determined by the curvature a general analytical expression is established for any infinitesimally weak localized curvature of the wire the interaction of the local mode with spin waves propag... | [['spin', 'waves', 'in', 'magnetic', 'nanowires', 'can', 'be', 'bound', 'by', 'a', 'local', 'bending', 'of', 'the', 'wire', 'the', 'eigenfrequency', 'of', 'a', 'truly', 'local', 'magnon', 'mode', 'is', 'determined', 'by', 'the', 'curvature', 'a', 'general', 'analytical', 'expression', 'is', 'established', 'for', 'any',... | [-0.24086497229204248, 0.22075976507126618, -0.07140451497328815, 0.029007722552407033, -0.07477885579217726, -0.1415926304840441, -0.003952540234843297, 0.3426383664247705, -0.25772543348816795, -0.24546395946961286, 0.049359880193178336, -0.263119492624233, -0.12591247092376448, 0.19989010082808004, 0.099829942530104... |
1,801.06946 | Yet Another Convex Sets Subtraction with Application in
Nondifferentiable Optimization | This paper introduces a new subtraction operation for convex sets, which
defines their difference as a collection of inclusion-minimal convex sets with
appropriate definitions of linear operations on them. With these operations the
set of collections becomes a linear vector space with common zero and
possibility to i... | math.OC | this paper introduces a new subtraction operation for convex sets which defines their difference as a collection of inclusionminimal convex sets with appropriate definitions of linear operations on them with these operations the set of collections becomes a linear vector space with common zero and possibility to invert... | [['this', 'paper', 'introduces', 'a', 'new', 'subtraction', 'operation', 'for', 'convex', 'sets', 'which', 'defines', 'their', 'difference', 'as', 'a', 'collection', 'of', 'inclusionminimal', 'convex', 'sets', 'with', 'appropriate', 'definitions', 'of', 'linear', 'operations', 'on', 'them', 'with', 'these', 'operations... | [-0.14092527172114286, 0.06517288893357748, -0.08809478397274183, 0.02903597911063116, -0.10364150416312946, -0.09079054239878638, 0.08202440362947527, 0.33984438945642775, -0.3363365064530323, -0.23990608062336427, 0.10930406317574023, -0.25052673417505705, -0.14062120110934806, 0.19562919937177664, -0.125746359531250... |
1,801.06947 | Generalized coinvariant algebras for $G(r,1,n)$ in the Stanley-Reisner
setting | Let $r$ and $n$ be positive integers, let $G_n$ be the complex reflection
group of $n \times n$ monomial matrices whose entries are $r^{\textrm{th}}$
roots of unity and let $0 \leq k \leq n$ be an integer. Recently, Haglund,
Rhoades and Shimozono ($r=1$) and Chan and Rhoades ($r>1$) introduced quotients
$R_{n,k}$ (fo... | math.CO | let r and n be positive integers let g_n be the complex reflection group of n times n monomial matrices whose entries are rtextrmth roots of unity and let 0 leq k leq n be an integer recently haglund rhoades and shimozono r1 and chan and rhoades r1 introduced quotients r_nk for r1 and s_nk for r geq 1 of the polynomial... | [['let', 'r', 'and', 'n', 'be', 'positive', 'integers', 'let', 'g_n', 'be', 'the', 'complex', 'reflection', 'group', 'of', 'n', 'times', 'n', 'monomial', 'matrices', 'whose', 'entries', 'are', 'rtextrmth', 'roots', 'of', 'unity', 'and', 'let', '0', 'leq', 'k', 'leq', 'n', 'be', 'an', 'integer', 'recently', 'haglund', '... | [-0.24950470383770354, 0.15125768209771367, -0.027451650870186608, -0.04830832114556848, -0.06562507716850854, -0.25527164038256045, -0.04774566749055818, 0.28387420457296486, -0.36356154304203087, -0.2040699995892841, 0.08708724162841994, -0.3336697709783325, -0.11427563560785593, 0.12423217683429207, -0.1219692596667... |
1,801.06948 | Measurement of low-energy background events due to $^{222}$Rn
contamination on the surface of a NaI(Tl) crystal | It has been known that decays of daughter elements of $^{222}$Rn on the
surface of a detector cause significant background at energies below 10 keV. In
particular $^{210}$Pb and $^{210}$Po decays on the crystal surface result in
significant background for dark matter search experiments with NaI(Tl)
crystals. In this ... | astro-ph.IM hep-ex nucl-ex | it has been known that decays of daughter elements of 222rn on the surface of a detector cause significant background at energies below 10 kev in particular 210pb and 210po decays on the crystal surface result in significant background for dark matter search experiments with naitl crystals in this report measurement of... | [['it', 'has', 'been', 'known', 'that', 'decays', 'of', 'daughter', 'elements', 'of', '222rn', 'on', 'the', 'surface', 'of', 'a', 'detector', 'cause', 'significant', 'background', 'at', 'energies', 'below', '10', 'kev', 'in', 'particular', '210pb', 'and', '210po', 'decays', 'on', 'the', 'crystal', 'surface', 'result', ... | [-0.010200816134113024, 0.28143165862859515, -0.06244654444687557, 0.08899688152271919, 0.042891037429026405, -0.10312956760133632, 0.038493910994281476, 0.36626415180622557, -0.16274739448057457, -0.3490005716696748, 0.005270491761621088, -0.43111159408190214, 0.03484643581819522, 0.22914045521432197, 0.01615689227693... |
1,801.06949 | Simple equivariant C*-algebras whose full and reduced crossed products
coincide | For any second countable locally compact group G, we construct a simple
G-C*-algebra whose full and reduced crossed product norms coincide. We then
construct its G-equivariant representation on another simple G-C*-algebra
without the coincidence condition. This settles two problems posed by
Anantharaman-Delaroche in ... | math.OA math.DS | for any second countable locally compact group g we construct a simple gcalgebra whose full and reduced crossed product norms coincide we then construct its gequivariant representation on another simple gcalgebra without the coincidence condition this settles two problems posed by anantharamandelaroche in 2002 some con... | [['for', 'any', 'second', 'countable', 'locally', 'compact', 'group', 'g', 'we', 'construct', 'a', 'simple', 'gcalgebra', 'whose', 'full', 'and', 'reduced', 'crossed', 'product', 'norms', 'coincide', 'we', 'then', 'construct', 'its', 'gequivariant', 'representation', 'on', 'another', 'simple', 'gcalgebra', 'without', '... | [-0.13798810726068184, 0.09889660561092052, -0.06400295436455339, 0.09782794904758167, -0.15411453197399774, -0.16796462641408047, 0.030244534960765318, 0.38608376628847096, -0.33764064600965116, -0.17291630607317476, 0.14070898943407206, -0.18764161795158596, -0.09595210297836684, 0.1838812141635857, -0.19877572837924... |
1,801.0695 | A unified framework for asymptotic analysis and computation of finite
Hankel transform | In this paper we present a unified framework for asymptotic analysis and
computation of the finite Hankel transform. This framework enables us to derive
asymptotic expansions of the transform, including the cases where the
oscillator has zeros and stationary points. As a consequence, two efficient and
affordable meth... | math.NA | in this paper we present a unified framework for asymptotic analysis and computation of the finite hankel transform this framework enables us to derive asymptotic expansions of the transform including the cases where the oscillator has zeros and stationary points as a consequence two efficient and affordable methods fo... | [['in', 'this', 'paper', 'we', 'present', 'a', 'unified', 'framework', 'for', 'asymptotic', 'analysis', 'and', 'computation', 'of', 'the', 'finite', 'hankel', 'transform', 'this', 'framework', 'enables', 'us', 'to', 'derive', 'asymptotic', 'expansions', 'of', 'the', 'transform', 'including', 'the', 'cases', 'where', 't... | [-0.08857386296615005, -0.04022580325603485, -0.16831686505426963, 0.09427465286571532, -0.06407375615711014, -0.09573691841835777, 0.09294419611959408, 0.34841210885594287, -0.18877690395029884, -0.2642720635732015, 0.18627216634495805, -0.258134004175663, -0.21248293850338087, 0.23599398386043807, -0.0151038821969026... |
1,801.06951 | Giant Vortex Clusters in a Two-Dimensional Quantum Fluid | Adding energy to a system through transient stirring usually leads to more
disorder. In contrast, point-like vortices in a bounded two-dimensional fluid
are predicted to reorder above a certain energy, forming persistent vortex
clusters. Here we realize experimentally these vortex clusters in a planar
superfluid: a $... | cond-mat.quant-gas physics.flu-dyn | adding energy to a system through transient stirring usually leads to more disorder in contrast pointlike vortices in a bounded twodimensional fluid are predicted to reorder above a certain energy forming persistent vortex clusters here we realize experimentally these vortex clusters in a planar superfluid a 87rb bosee... | [['adding', 'energy', 'to', 'a', 'system', 'through', 'transient', 'stirring', 'usually', 'leads', 'to', 'more', 'disorder', 'in', 'contrast', 'pointlike', 'vortices', 'in', 'a', 'bounded', 'twodimensional', 'fluid', 'are', 'predicted', 'to', 'reorder', 'above', 'a', 'certain', 'energy', 'forming', 'persistent', 'vorte... | [-0.1611787166839993, 0.2602223604063728, -0.0699375443473722, 0.06840131495897947, 0.009096290386669271, -0.12427663023014908, 0.04534456585183641, 0.37797024166953247, -0.23611894587005397, -0.25994092353982273, 0.021999950207506135, -0.2852618264578349, -0.058670314292596504, 0.157060083162567, 0.029615648577105157,... |
1,801.06952 | Order from chaos: Observation of large-scale flow from turbulence in a
two-dimensional superfluid | Interacting systems driven far from equilibrium tend to evolve to steady
states exhibiting large-scale structure and order. In two-dimensional turbulent
flow the seemingly random swirling motion of a fluid can evolve towards
persistent large-scale vortices. Lars Onsager proposed a model based on
statistical mechanics... | cond-mat.quant-gas physics.flu-dyn | interacting systems driven far from equilibrium tend to evolve to steady states exhibiting largescale structure and order in twodimensional turbulent flow the seemingly random swirling motion of a fluid can evolve towards persistent largescale vortices lars onsager proposed a model based on statistical mechanics of qua... | [['interacting', 'systems', 'driven', 'far', 'from', 'equilibrium', 'tend', 'to', 'evolve', 'to', 'steady', 'states', 'exhibiting', 'largescale', 'structure', 'and', 'order', 'in', 'twodimensional', 'turbulent', 'flow', 'the', 'seemingly', 'random', 'swirling', 'motion', 'of', 'a', 'fluid', 'can', 'evolve', 'towards', ... | [-0.16963854326168076, 0.22532448989635062, -0.118251348141348, 0.042103986046276985, -0.02400478282943368, -0.12539521295111627, 0.023988871057129775, 0.3376396001937489, -0.28974727736009903, -0.27842200874971845, 0.014834051146560038, -0.26405558232509063, -0.11880915123814097, 0.16821525213551164, 0.028562821743298... |
1,801.06953 | On The Effect of Vibration on Shape Sensing of Continuum Manipulators
Using Fiber Bragg Gratings | Fiber Bragg Grating (FBG) has shown great potential in shape and force
sensing of continuum manipulators (CM) and biopsy needles. In the recent years,
many researchers have studied different manufacturing and modeling techniques
of FBG-based force and shape sensors for medical applications. These studies
mainly focus... | cs.RO | fiber bragg grating fbg has shown great potential in shape and force sensing of continuum manipulators cm and biopsy needles in the recent years many researchers have studied different manufacturing and modeling techniques of fbgbased force and shape sensors for medical applications these studies mainly focus on obtain... | [['fiber', 'bragg', 'grating', 'fbg', 'has', 'shown', 'great', 'potential', 'in', 'shape', 'and', 'force', 'sensing', 'of', 'continuum', 'manipulators', 'cm', 'and', 'biopsy', 'needles', 'in', 'the', 'recent', 'years', 'many', 'researchers', 'have', 'studied', 'different', 'manufacturing', 'and', 'modeling', 'technique... | [-0.10860098856607113, 0.08720804003527306, -0.07874117687937211, -0.022973126030297247, -0.05143680004402995, -0.1489181589311013, -0.005585812392807868, 0.4331562543989389, -0.23500118077586726, -0.31543248783276934, 0.12373544227833823, -0.24409808688373727, -0.16913249474714281, 0.21747748691485833, -0.102391759408... |
1,801.06954 | A port-Hamiltonian approach to the control of nonholonomic systems | In this paper a method of controlling nonholonomic systems within the
port-Hamiltonian (pH) framework is presented. It is well known that
nonholonomic systems can be represented as pH systems without Lagrange
multipliers by considering a reduced momentum space. Here, we revisit the
modelling of these systems for the ... | cs.SY | in this paper a method of controlling nonholonomic systems within the porthamiltonian ph framework is presented it is well known that nonholonomic systems can be represented as ph systems without lagrange multipliers by considering a reduced momentum space here we revisit the modelling of these systems for the purpose ... | [['in', 'this', 'paper', 'a', 'method', 'of', 'controlling', 'nonholonomic', 'systems', 'within', 'the', 'porthamiltonian', 'ph', 'framework', 'is', 'presented', 'it', 'is', 'well', 'known', 'that', 'nonholonomic', 'systems', 'can', 'be', 'represented', 'as', 'ph', 'systems', 'without', 'lagrange', 'multipliers', 'by',... | [-0.1740060538190921, 0.06761868636039864, -0.07396888895128227, 0.03911377509319239, -0.03127929711805993, -0.1430810963597576, -0.00912615335947208, 0.3311759758984945, -0.27878362043821786, -0.2909763619822801, 0.12853552339995494, -0.1936432029822933, -0.2189972382611366, 0.23211452108426173, -0.08342406204634453, ... |
1,801.06955 | Transport evidence of asymmetric spin-orbit coupling in few$-$layer
superconducting 1Td$-$MoTe$_2$ | Two-dimensional (2D) transition metal dichalcogenides (TMDCs) MX2 (M=W, Mo,
Nb, and X=Te, Se, S) with strong spin-orbit coupling (SOC) possess plenty of
novel physics including superconductivity. Due to the Ising SOC, monolayer
NbSe$_2$ and gated MoS$_2$ of 2H structure can realize the Ising
superconductivity phase, ... | cond-mat.supr-con | twodimensional 2d transition metal dichalcogenides tmdcs mx2 mw mo nb and xte se s with strong spinorbit coupling soc possess plenty of novel physics including superconductivity due to the ising soc monolayer nbse_2 and gated mos_2 of 2h structure can realize the ising superconductivity phase which manifests itself wit... | [['twodimensional', '2d', 'transition', 'metal', 'dichalcogenides', 'tmdcs', 'mx2', 'mw', 'mo', 'nb', 'and', 'xte', 'se', 's', 'with', 'strong', 'spinorbit', 'coupling', 'soc', 'possess', 'plenty', 'of', 'novel', 'physics', 'including', 'superconductivity', 'due', 'to', 'the', 'ising', 'soc', 'monolayer', 'nbse_2', 'an... | [-0.17403739566365495, 0.16902654447722643, -0.00690683456352697, 0.0029882500867526502, -0.07809402163406141, -0.1829054671817292, 0.12079334517176717, 0.39853358073398854, -0.23657954095934447, -0.262659245040805, -0.027113715922818162, -0.29381483558756416, -0.176968439680357, 0.20349496354301197, 0.0554443997133953... |
1,801.06956 | The Capacity of Degraded Cognitive Interference Channel with
Unidirectional Destination Cooperation | Previous works established the capacity region for some special cases of
discrete memoryless degraded cognitive interference channel (CIC) with
unidirectional destination cooperation (UDC). In this letter, we characterize
the capacity region of the general discrete memoryless degraded CIC-UDC. The
obtained results im... | cs.IT math.IT | previous works established the capacity region for some special cases of discrete memoryless degraded cognitive interference channel cic with unidirectional destination cooperation udc in this letter we characterize the capacity region of the general discrete memoryless degraded cicudc the obtained results imply that t... | [['previous', 'works', 'established', 'the', 'capacity', 'region', 'for', 'some', 'special', 'cases', 'of', 'discrete', 'memoryless', 'degraded', 'cognitive', 'interference', 'channel', 'cic', 'with', 'unidirectional', 'destination', 'cooperation', 'udc', 'in', 'this', 'letter', 'we', 'characterize', 'the', 'capacity',... | [-0.20984654581931594, 0.026021033054688475, -0.02971063658165244, 0.031235193646932533, -0.06298816314089921, -0.3194820197902947, 0.18605757636724266, 0.37518541572185665, -0.3004113512502594, -0.1870344956251946, 0.09404778319083482, -0.19219101041524703, -0.15364825880605276, 0.10494339132456335, -0.158670939738890... |
1,801.06957 | K2-155: A Bright Metal-Poor M Dwarf with Three Transiting Super-Earths | We report on the discovery of three transiting super-Earths around K2-155
(EPIC 210897587), a relatively bright early M dwarf ($V=12.81$ mag) observed
during Campaign 13 of the NASA K2 mission. To characterize the system and
validate the planet candidates, we conducted speckle imaging and
high-dispersion optical spec... | astro-ph.EP astro-ph.SR | we report on the discovery of three transiting superearths around k2155 epic 210897587 a relatively bright early m dwarf v1281 mag observed during campaign 13 of the nasa k2 mission to characterize the system and validate the planet candidates we conducted speckle imaging and highdispersion optical spectroscopy includi... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'three', 'transiting', 'superearths', 'around', 'k2155', 'epic', '210897587', 'a', 'relatively', 'bright', 'early', 'm', 'dwarf', 'v1281', 'mag', 'observed', 'during', 'campaign', '13', 'of', 'the', 'nasa', 'k2', 'mission', 'to', 'characterize', 'the', 'system', 'and', ... | [-0.1154183040592162, 0.18311148174646352, -0.07175304108600625, 0.021453615198112733, -0.12998657082504245, -0.060187566114644354, 0.09958447706537531, 0.34599970571477623, -0.1347810625938662, -0.3736333535988724, 0.13512780158963128, -0.32091155843241437, -0.09002966456133507, 0.23166499645951405, -0.094686271779138... |
1,801.06958 | Relativistic anisotropic stars with the polytropic equation of state in
general relativity | Spherically symmetric relativistic stars with the polytropic equation of
state, which possess the local pressure anisotropy, are considered in the
context of general relativity. The modified Lane-Emden equations are derived
for the special ansatz for the anisotropy parameter $\Delta$ in the form of the
differential r... | gr-qc astro-ph.HE | spherically symmetric relativistic stars with the polytropic equation of state which possess the local pressure anisotropy are considered in the context of general relativity the modified laneemden equations are derived for the special ansatz for the anisotropy parameter delta in the form of the differential relation b... | [['spherically', 'symmetric', 'relativistic', 'stars', 'with', 'the', 'polytropic', 'equation', 'of', 'state', 'which', 'possess', 'the', 'local', 'pressure', 'anisotropy', 'are', 'considered', 'in', 'the', 'context', 'of', 'general', 'relativity', 'the', 'modified', 'laneemden', 'equations', 'are', 'derived', 'for', '... | [-0.18108705769564154, 0.12714137479698262, -0.09126325145576007, 0.0835316003715808, -0.08994225915992939, -0.1265295769244173, -0.08030014377841845, 0.23847596330238105, -0.22752388156478917, -0.3012248846831955, 0.017356466357537275, -0.2774168331960004, -0.04593375667080849, 0.16823980386687232, 0.04559523327264322... |
1,801.06959 | Asymptotic behaviour of instantons on Cylinder Manifolds | IIn this article, we study the instanton equation on the cylinder over a
closed manifold $X$ which admits non-zero smooth $3$-form $P$ and $4$-form $Q$.
Our results are (1) if $X$ is a \textbf{good} manifold, i.e., $P,Q$ satisfying
$d\ast_{X}P=d\ast_{X}Q=0$, then the instanton with integrable curvature decays
exponen... | math.DG | iin this article we study the instanton equation on the cylinder over a closed manifold x which admits nonzero smooth 3form p and 4form q our results are 1 if x is a textbfgood manifold ie pq satisfying dast_xpdast_xq0 then the instanton with integrable curvature decays exponentially at the ends and 2 if x is a real ki... | [['iin', 'this', 'article', 'we', 'study', 'the', 'instanton', 'equation', 'on', 'the', 'cylinder', 'over', 'a', 'closed', 'manifold', 'x', 'which', 'admits', 'nonzero', 'smooth', '3form', 'p', 'and', '4form', 'q', 'our', 'results', 'are', '1', 'if', 'x', 'is', 'a', 'textbfgood', 'manifold', 'ie', 'pq', 'satisfying', '... | [-0.23900196233176088, 0.14522803385472416, -0.07781705522211269, 0.058509895090920555, -0.10466482845367864, -0.23439499800166996, -0.03867460557682391, 0.3443712806329131, -0.22807265562618054, -0.12251335177815666, 0.08552836424841141, -0.3096279257565345, -0.15770771385072485, 0.1099936296599672, -0.061300135275814... |
1,801.0696 | Majorana neutrino and the vacuum of Bogoliubov quasiparticle | The Lagrangian of the seesaw mechanism is C violating but the same Lagrangian
when re-written in terms of Majorana neutrinos is manifestly C invariant. To
resolve this puzzling feature, a relativistic analogue of Bogoliubov
transformation, which preserves CP but explicitly breaks C and P separately,
was introduced to... | hep-th hep-ph | the lagrangian of the seesaw mechanism is c violating but the same lagrangian when rewritten in terms of majorana neutrinos is manifestly c invariant to resolve this puzzling feature a relativistic analogue of bogoliubov transformation which preserves cp but explicitly breaks c and p separately was introduced together ... | [['the', 'lagrangian', 'of', 'the', 'seesaw', 'mechanism', 'is', 'c', 'violating', 'but', 'the', 'same', 'lagrangian', 'when', 'rewritten', 'in', 'terms', 'of', 'majorana', 'neutrinos', 'is', 'manifestly', 'c', 'invariant', 'to', 'resolve', 'this', 'puzzling', 'feature', 'a', 'relativistic', 'analogue', 'of', 'bogoliub... | [-0.15159646644502695, 0.26648452874186285, -0.11255524640308659, 0.15122527618566814, -0.06938912796050858, -0.1494251503751962, 0.05464531064741999, 0.25136457444197197, -0.23129261054235734, -0.24290218264253044, -0.06582291401848425, -0.2488388872185459, -0.09584445353208876, 0.038874789155402614, 0.000518415970270... |
1,801.06961 | Stable lattices in modular Galois representations and Hida deformation | In this paper, we discuss the variation of the numbers of the isomorphic
classes of stable lattices when the weight and the level varies in a Hida
deformation by using the Kubota-Leopoldt $p$-adic $L$-function. As a corollary,
we give a sufficient condition for the numbers of the isomorphic classes of
stable lattices... | math.NT | in this paper we discuss the variation of the numbers of the isomorphic classes of stable lattices when the weight and the level varies in a hida deformation by using the kubotaleopoldt padic lfunction as a corollary we give a sufficient condition for the numbers of the isomorphic classes of stable lattices in hida def... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'variation', 'of', 'the', 'numbers', 'of', 'the', 'isomorphic', 'classes', 'of', 'stable', 'lattices', 'when', 'the', 'weight', 'and', 'the', 'level', 'varies', 'in', 'a', 'hida', 'deformation', 'by', 'using', 'the', 'kubotaleopoldt', 'padic', 'lfunction', 'as', 'a', 'co... | [-0.19289651946646386, 0.14519853433915253, -0.12888090424881926, 0.08361809589932191, -0.04182247534908097, -0.06233461128130298, 0.020421286846173864, 0.30469169278211633, -0.3255865094091358, -0.2305604118797607, 0.11024661677094691, -0.18424426582802472, -0.1667394235665942, 0.20732223709788303, -0.1251997437552902... |
1,801.06962 | Symmetry Breaking in Haloscope Microwave Cavities | Axion haloscope detectors use microwave cavities permeated by a magnetic
field to resonate photons that are converted from axions due to the inverse
Primakoff effect. The sensitivity of a detector is proportional to the form
factor of the cavity's search mode. Transverse symmetry breaking is used to
tune the search m... | physics.ins-det | axion haloscope detectors use microwave cavities permeated by a magnetic field to resonate photons that are converted from axions due to the inverse primakoff effect the sensitivity of a detector is proportional to the form factor of the cavitys search mode transverse symmetry breaking is used to tune the search modes ... | [['axion', 'haloscope', 'detectors', 'use', 'microwave', 'cavities', 'permeated', 'by', 'a', 'magnetic', 'field', 'to', 'resonate', 'photons', 'that', 'are', 'converted', 'from', 'axions', 'due', 'to', 'the', 'inverse', 'primakoff', 'effect', 'the', 'sensitivity', 'of', 'a', 'detector', 'is', 'proportional', 'to', 'the... | [-0.16586385621521316, 0.24615373099451793, -0.05281485130124893, 0.06836368946060843, -0.1534651664894868, -0.10389451440576403, 0.03320178000702996, 0.3502069105562128, -0.2249941953198343, -0.36965475193240116, 0.07382701721603478, -0.2876591336088957, -0.05986918705958323, 0.1966286154910464, 0.08641448796375609, 0... |
1,801.06963 | Local density of states in two-dimensional topological superconductors
under a magnetic field: signature of an exterior Majorana bound state | We study quasiparticle states on a surface of a topological insulator (TI)
with proximity-induced superconductivity under an external magnetic field. An
applied magnetic field creates two Majorana bound states: a vortex Majorana
state localized inside a vortex core and an exterior Majorana state localized
along a cir... | cond-mat.supr-con cond-mat.mes-hall | we study quasiparticle states on a surface of a topological insulator ti with proximityinduced superconductivity under an external magnetic field an applied magnetic field creates two majorana bound states a vortex majorana state localized inside a vortex core and an exterior majorana state localized along a circle cen... | [['we', 'study', 'quasiparticle', 'states', 'on', 'a', 'surface', 'of', 'a', 'topological', 'insulator', 'ti', 'with', 'proximityinduced', 'superconductivity', 'under', 'an', 'external', 'magnetic', 'field', 'an', 'applied', 'magnetic', 'field', 'creates', 'two', 'majorana', 'bound', 'states', 'a', 'vortex', 'majorana'... | [-0.226896340501879, 0.2313380667010096, -0.06238278580350749, 0.04741097524590102, -0.04444588251209941, -0.14219749652702046, 0.0647994063319601, 0.3398881948265026, -0.22558960891945892, -0.27033954008246763, -0.05058487637452856, -0.29778889460062763, -0.08067201783910513, 0.14292520203302245, 0.029109124857259083,... |
1,801.06964 | Opportunism in Dynamic Spectrum Access for 5G: A Concept and Its
Application to Duplexing | With the envisioned massive Internet-of-Things (IoT) era, one of the
challenges for 5G wireless systems will be handling the unprecedented spectrum
crunch. A potential solution has emerged in the form of spectrum sharing, which
deviates from a monopolistic spectrum usage system. This article investigates
the medium a... | cs.IT cs.NI math.IT | with the envisioned massive internetofthings iot era one of the challenges for 5g wireless systems will be handling the unprecedented spectrum crunch a potential solution has emerged in the form of spectrum sharing which deviates from a monopolistic spectrum usage system this article investigates the medium access cont... | [['with', 'the', 'envisioned', 'massive', 'internetofthings', 'iot', 'era', 'one', 'of', 'the', 'challenges', 'for', '5g', 'wireless', 'systems', 'will', 'be', 'handling', 'the', 'unprecedented', 'spectrum', 'crunch', 'a', 'potential', 'solution', 'has', 'emerged', 'in', 'the', 'form', 'of', 'spectrum', 'sharing', 'whi... | [-0.21256957961345763, 0.0046513316772448755, -0.06023653777742337, -0.019758168747291662, -0.06330080096662608, -0.19804864098704508, 0.10875170308446407, 0.3644415306285428, -0.2506886290513717, -0.2873616105775823, 0.09723968250415604, -0.2499201601192153, -0.1624741439953587, 0.17591825999508454, -0.043654491129893... |
1,801.06965 | An Efficient Density-based Clustering Algorithm for Higher-Dimensional
Data | DBSCAN is a typically used clustering algorithm due to its clustering ability
for arbitrarily-shaped clusters and its robustness to outliers. Generally, the
complexity of DBSCAN is O(n^2) in the worst case, and it practically becomes
more severe in higher dimension. Grid-based DBSCAN is one of the recent
improved alg... | cs.DB cs.IR | dbscan is a typically used clustering algorithm due to its clustering ability for arbitrarilyshaped clusters and its robustness to outliers generally the complexity of dbscan is on2 in the worst case and it practically becomes more severe in higher dimension gridbased dbscan is one of the recent improved algorithms aim... | [['dbscan', 'is', 'a', 'typically', 'used', 'clustering', 'algorithm', 'due', 'to', 'its', 'clustering', 'ability', 'for', 'arbitrarilyshaped', 'clusters', 'and', 'its', 'robustness', 'to', 'outliers', 'generally', 'the', 'complexity', 'of', 'dbscan', 'is', 'on2', 'in', 'the', 'worst', 'case', 'and', 'it', 'practically... | [-0.07540171527580242, -0.028834818298400934, -0.08002264383831062, 0.11773125795807574, -0.10884181191358948, -0.1378787959984038, 0.06138541894106311, 0.42643239099998026, -0.2604570372350281, -0.363595135443029, 0.10231854602752719, -0.2621980339376023, -0.15920189037569799, 0.1760182951726165, -0.1221222144755302, ... |
1,801.06966 | Accurate Evaluation of Asset Pricing Under Uncertainty and Ambiguity of
Information | Since exchange economy considerably varies in the market assets, asset prices
have become an attractive research area for investigating and modeling
ambiguous and uncertain information in today markets. This paper proposes a new
generative uncertainty mechanism based on the Bayesian Inference and
Correntropy (BIC) te... | q-fin.GN econ.EM | since exchange economy considerably varies in the market assets asset prices have become an attractive research area for investigating and modeling ambiguous and uncertain information in today markets this paper proposes a new generative uncertainty mechanism based on the bayesian inference and correntropy bic techniqu... | [['since', 'exchange', 'economy', 'considerably', 'varies', 'in', 'the', 'market', 'assets', 'asset', 'prices', 'have', 'become', 'an', 'attractive', 'research', 'area', 'for', 'investigating', 'and', 'modeling', 'ambiguous', 'and', 'uncertain', 'information', 'in', 'today', 'markets', 'this', 'paper', 'proposes', 'a',... | [-0.06933764771868785, 0.006169788042025175, -0.14447131731236976, 0.20285490322081992, -0.10504395672120154, -0.1557560588962709, 0.13550425314887737, 0.4157668479159474, -0.3156682428562393, -0.2933353720360901, 0.15718606216289724, -0.2963538125964503, -0.15928698306165945, 0.16307227839509628, -0.16577199050070096,... |
1,801.06967 | Lower bounds of Lipschitz constants on foliations | In this paper we consider Llarull's theorem in the foliation case and get a
lower bound of the Lipschitz constant of the map $M\to S^n$ in the foliation
case under the spin condition.
| math.DG | in this paper we consider llarulls theorem in the foliation case and get a lower bound of the lipschitz constant of the map mto sn in the foliation case under the spin condition | [['in', 'this', 'paper', 'we', 'consider', 'llarulls', 'theorem', 'in', 'the', 'foliation', 'case', 'and', 'get', 'a', 'lower', 'bound', 'of', 'the', 'lipschitz', 'constant', 'of', 'the', 'map', 'mto', 'sn', 'in', 'the', 'foliation', 'case', 'under', 'the', 'spin', 'condition']] | [-0.19271504582138732, 0.0749959131644573, -0.06745270610554144, 0.04300165718814242, -0.019243562303017825, -0.1389429042901611, 0.04772151244469569, 0.31731966440565884, -0.263701502000913, -0.19276502402499318, 0.10361202068270359, -0.2392844376154244, -0.11904789111576974, 0.1814666735881474, -0.11991655416204594, ... |
1,801.06968 | Convexity of mutual information along the heat flow | We study the convexity of mutual information along the evolution of the heat
equation. We prove that if the initial distribution is log-concave, then mutual
information is always a convex function of time. We also prove that if the
initial distribution is either bounded, or has finite fourth moment and Fisher
informa... | cs.IT math.IT | we study the convexity of mutual information along the evolution of the heat equation we prove that if the initial distribution is logconcave then mutual information is always a convex function of time we also prove that if the initial distribution is either bounded or has finite fourth moment and fisher information th... | [['we', 'study', 'the', 'convexity', 'of', 'mutual', 'information', 'along', 'the', 'evolution', 'of', 'the', 'heat', 'equation', 'we', 'prove', 'that', 'if', 'the', 'initial', 'distribution', 'is', 'logconcave', 'then', 'mutual', 'information', 'is', 'always', 'a', 'convex', 'function', 'of', 'time', 'we', 'also', 'pr... | [-0.12516437131392805, 0.11862394639255502, -0.15137654495325317, 0.10904908365911886, -0.09868397490015324, -0.1377465625623642, -0.0038503519623375297, 0.3762131267362805, -0.3752956373404853, -0.204522688467869, 0.1708842637606814, -0.33504252692189396, -0.13181203925876017, 0.1292307357380426, -0.09108521256601744,... |
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