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1,803.02067 | On cycles of pairing-friendly elliptic curves | A cycle of elliptic curves is a list of elliptic curves over finite fields
such that the number of points on one curve is equal to the size of the field
of definition of the next, in a cyclic way. We study cycles of elliptic curves
in which every curve is pairing-friendly. These have recently found notable
applicatio... | math.NT math.AG | a cycle of elliptic curves is a list of elliptic curves over finite fields such that the number of points on one curve is equal to the size of the field of definition of the next in a cyclic way we study cycles of elliptic curves in which every curve is pairingfriendly these have recently found notable applications in ... | [['a', 'cycle', 'of', 'elliptic', 'curves', 'is', 'a', 'list', 'of', 'elliptic', 'curves', 'over', 'finite', 'fields', 'such', 'that', 'the', 'number', 'of', 'points', 'on', 'one', 'curve', 'is', 'equal', 'to', 'the', 'size', 'of', 'the', 'field', 'of', 'definition', 'of', 'the', 'next', 'in', 'a', 'cyclic', 'way', 'we... | [-0.23653443430568538, 0.11355904746776471, -0.10313597738488832, 0.0310713122167939, -0.0211303167788965, -0.1266685987145386, 0.040963397214685074, 0.3634057166780551, -0.2737015265814186, -0.27918083636791674, 0.11045280118267257, -0.2705042368153907, -0.15115363040316077, 0.31242425890046766, -0.12344707227795833, ... |
1,803.02068 | Infinite energy solutions to the Navier-Stokes equations in the
half-space and applications | This short note serves as an introduction to the papers arXiv:1711.01651 and
arXiv:1711.04486 by Maekawa, Miura and Prange. These two works deal with the
existence of mild solutions on the one hand and local energy weak solutions on
the other hand to the Navier-Stokes equations in the half-space $\R^3_+$. We
emphasiz... | math.AP | this short note serves as an introduction to the papers arxiv171101651 and arxiv171104486 by maekawa miura and prange these two works deal with the existence of mild solutions on the one hand and local energy weak solutions on the other hand to the navierstokes equations in the halfspace r3_ we emphasize a concentratio... | [['this', 'short', 'note', 'serves', 'as', 'an', 'introduction', 'to', 'the', 'papers', 'arxiv171101651', 'and', 'arxiv171104486', 'by', 'maekawa', 'miura', 'and', 'prange', 'these', 'two', 'works', 'deal', 'with', 'the', 'existence', 'of', 'mild', 'solutions', 'on', 'the', 'one', 'hand', 'and', 'local', 'energy', 'wea... | [-0.11279801368348401, 0.05411817715837576, -0.09076718249628823, 0.05954981506393115, -0.07327549525763134, -0.11625413834494916, -0.010473626499013925, 0.27830877545214183, -0.2384422545044406, -0.27940775748543645, 0.1794646458505225, -0.32946558601248105, -0.12700898277673972, 0.1787185864774762, -0.103912501948306... |
1,803.02069 | Sequences of consecutive squares on quartic elliptic curves | Let $C: y^2=ax^4+bx^2+c$, be an elliptic curve defined over $\mathbb Q$. A
set of rational points $(x_i,y_i) \in C(\mathbb Q)$, $i=1,2,\cdots,$ is said to
be a sequence of consecutive squares if $x_i= (u + i)^2$, $i=1,2,\cdots$, for
some $u\in \mathbb Q$. Using ideas of Mestre, we construct infinitely many
elliptic c... | math.NT | let c y2ax4bx2c be an elliptic curve defined over mathbb q a set of rational points x_iy_i in cmathbb q i12cdots is said to be a sequence of consecutive squares if x_i u i2 i12cdots for some uin mathbb q using ideas of mestre we construct infinitely many elliptic curves c with sequences of consecutive squares of length... | [['let', 'c', 'y2ax4bx2c', 'be', 'an', 'elliptic', 'curve', 'defined', 'over', 'mathbb', 'q', 'a', 'set', 'of', 'rational', 'points', 'x_iy_i', 'in', 'cmathbb', 'q', 'i12cdots', 'is', 'said', 'to', 'be', 'a', 'sequence', 'of', 'consecutive', 'squares', 'if', 'x_i', 'u', 'i2', 'i12cdots', 'for', 'some', 'uin', 'mathbb',... | [-0.23587487776389468, 0.1063484816441245, -0.08550299514763962, -0.013510073979045743, 0.002928617303738388, -0.21828648352246977, 0.01102153837972399, 0.3644072014281404, -0.34945467218895937, -0.18754161061353494, 0.09235984729559413, -0.3618639962591022, -0.10101050675071985, 0.20821847333181126, -0.105544224982019... |
1,803.0207 | SOS-Convex Lyapunov Functions and Stability of Difference Inclusions | We introduce the concept of sos-convex Lyapunov functions for stability
analysis of both linear and nonlinear difference inclusions (also known as
discrete-time switched systems). These are polynomial Lyapunov functions that
have an algebraic certificate of convexity and that can be efficiently found
via semidefinite... | math.OC cs.SY math.DS | we introduce the concept of sosconvex lyapunov functions for stability analysis of both linear and nonlinear difference inclusions also known as discretetime switched systems these are polynomial lyapunov functions that have an algebraic certificate of convexity and that can be efficiently found via semidefinite progra... | [['we', 'introduce', 'the', 'concept', 'of', 'sosconvex', 'lyapunov', 'functions', 'for', 'stability', 'analysis', 'of', 'both', 'linear', 'and', 'nonlinear', 'difference', 'inclusions', 'also', 'known', 'as', 'discretetime', 'switched', 'systems', 'these', 'are', 'polynomial', 'lyapunov', 'functions', 'that', 'have', ... | [-0.20023618112926753, 0.03366815807996979, -0.14871992326913064, 0.10836180996439411, -0.07139035300166473, -0.19542561038344336, 0.030561419160221703, 0.3230810706882039, -0.3580826092088087, -0.17793920724811454, 0.18550124436825915, -0.20675576911889948, -0.24120113949968733, 0.22293968006984374, -0.036116414421485... |
1,803.02071 | Coupled charge and spin dynamics in a photo-excited Mott insulator | Using a nonequilibrium implementation of the extended dynamical mean field
theory (EDMFT) we simulate the relaxation after photo excitation in a strongly
correlated electron system with antiferromagnetic spin interactions. We
consider the $t$-$J$ model and focus on the interplay between the charge- and
spin-dynamics ... | cond-mat.str-el | using a nonequilibrium implementation of the extended dynamical mean field theory edmft we simulate the relaxation after photo excitation in a strongly correlated electron system with antiferromagnetic spin interactions we consider the tj model and focus on the interplay between the charge and spindynamics in different... | [['using', 'a', 'nonequilibrium', 'implementation', 'of', 'the', 'extended', 'dynamical', 'mean', 'field', 'theory', 'edmft', 'we', 'simulate', 'the', 'relaxation', 'after', 'photo', 'excitation', 'in', 'a', 'strongly', 'correlated', 'electron', 'system', 'with', 'antiferromagnetic', 'spin', 'interactions', 'we', 'cons... | [-0.18222970510760206, 0.21390021312618046, -0.07501587519917408, 0.10018276074697496, 0.02474393376178341, -0.13623632132748753, 0.05026962418560288, 0.3550975838006707, -0.2658934896244318, -0.2743118444486754, 0.008502619634782604, -0.317200161756773, -0.10960983026416216, 0.15445808307958941, 0.1037652599879948, -0... |
1,803.02072 | Nearly isentropic flow at sizeable $\eta/s$ | Non-linearities in the harmonic spectra of hadron-nucleus and nucleus-nucleus
collisions provide evidence for the dynamical response to azimuthal spatial
eccentricities. Here, we demonstrate within the framework of transport theory
that even the mildest interaction correction to a picture of free-streaming
particle d... | hep-ph hep-ex nucl-ex nucl-th | nonlinearities in the harmonic spectra of hadronnucleus and nucleusnucleus collisions provide evidence for the dynamical response to azimuthal spatial eccentricities here we demonstrate within the framework of transport theory that even the mildest interaction correction to a picture of freestreaming particle distribut... | [['nonlinearities', 'in', 'the', 'harmonic', 'spectra', 'of', 'hadronnucleus', 'and', 'nucleusnucleus', 'collisions', 'provide', 'evidence', 'for', 'the', 'dynamical', 'response', 'to', 'azimuthal', 'spatial', 'eccentricities', 'here', 'we', 'demonstrate', 'within', 'the', 'framework', 'of', 'transport', 'theory', 'tha... | [-0.1429042632687924, 0.1962386877670724, -0.13584266789548566, 0.08826102205566713, 0.00048248994571622463, -0.07033903111951076, -0.09827041027674568, 0.3067928828080767, -0.2722441728314152, -0.2910060465859715, -0.034924855638382726, -0.3151139022840653, -0.04567734797747107, 0.13810261759367676, 0.0529052734586002... |
1,803.02073 | Formal Intercept of Sturmian words | We give a combinatorial definition of the second parameter describing
Sturmian words, that we call formal intercept, as an infinite Ostrowski
expansion. We recall the well-known properties of Sturmian words, study factors
graphs and repetition function, and end with the definition of formal
intercepts.
| math.CO | we give a combinatorial definition of the second parameter describing sturmian words that we call formal intercept as an infinite ostrowski expansion we recall the wellknown properties of sturmian words study factors graphs and repetition function and end with the definition of formal intercepts | [['we', 'give', 'a', 'combinatorial', 'definition', 'of', 'the', 'second', 'parameter', 'describing', 'sturmian', 'words', 'that', 'we', 'call', 'formal', 'intercept', 'as', 'an', 'infinite', 'ostrowski', 'expansion', 'we', 'recall', 'the', 'wellknown', 'properties', 'of', 'sturmian', 'words', 'study', 'factors', 'grap... | [-0.17354264063760638, 0.10361401877790657, -0.1385680129751563, 0.11542306626638905, -0.17777534338264642, -0.14092036204370248, 0.12187270081432705, 0.3263946663461287, -0.3251902773468332, -0.22261775422587313, 0.035129976755177435, -0.30917658961632033, -0.17788393664258448, 0.1473692528167951, -0.135563879633661, ... |
1,803.02074 | "Massless" spin-2 field in de Sitter space | In this paper, admitting a de Sitter (dS)-invariant vacuum in an indefinite
inner product space, we present a Gupta-Bleuler type setting for causal and
full dS-covariant quantization of free "massless" spin-2 field in dS spacetime.
The term "massless" stands for the fact that the field displays gauge and
conformal in... | gr-qc | in this paper admitting a de sitter dsinvariant vacuum in an indefinite inner product space we present a guptableuler type setting for causal and full dscovariant quantization of free massless spin2 field in ds spacetime the term massless stands for the fact that the field displays gauge and conformal invariance proper... | [['in', 'this', 'paper', 'admitting', 'a', 'de', 'sitter', 'dsinvariant', 'vacuum', 'in', 'an', 'indefinite', 'inner', 'product', 'space', 'we', 'present', 'a', 'guptableuler', 'type', 'setting', 'for', 'causal', 'and', 'full', 'dscovariant', 'quantization', 'of', 'free', 'massless', 'spin2', 'field', 'in', 'ds', 'spac... | [-0.160988901498226, 0.16910090388286894, -0.11097294511008, 0.0787456058162766, -0.08902261474241431, -0.08403292704516878, -0.03799844104348897, 0.31873718708610305, -0.22581776834021394, -0.20342735204344187, 0.07155055089835793, -0.26831274072353084, -0.14790400139351662, 0.09732931185191354, -0.09633444968897563, ... |
1,803.02075 | Development of a New Spectral Collocation Method Using Laplacian
Eigenbasis for Elliptic Partial Differential Equations in an Extended Domain | The recent development of spectral method has been praised for its high-order
convergence in simulating complex physical problems. The combination of
embedded boundary method and spectral method becomes a mainstream way to tackle
geometrically complicated problems. However, the convergence is deteriorated
when embedd... | math.NA | the recent development of spectral method has been praised for its highorder convergence in simulating complex physical problems the combination of embedded boundary method and spectral method becomes a mainstream way to tackle geometrically complicated problems however the convergence is deteriorated when embedded bou... | [['the', 'recent', 'development', 'of', 'spectral', 'method', 'has', 'been', 'praised', 'for', 'its', 'highorder', 'convergence', 'in', 'simulating', 'complex', 'physical', 'problems', 'the', 'combination', 'of', 'embedded', 'boundary', 'method', 'and', 'spectral', 'method', 'becomes', 'a', 'mainstream', 'way', 'to', '... | [-0.07213189718345853, 0.008958705049735727, -0.11299293259184601, 0.07393546234428262, -0.1004820305116785, -0.115778730240547, -0.0034530149889178572, 0.3628499823363705, -0.3065663824026059, -0.26404239341726576, 0.13884737699538366, -0.21804988858186536, -0.16104254639810986, 0.217111251094482, -0.09819394113082025... |
1,803.02076 | Invariant Smoothing on Lie Groups | In this paper we propose a (non-linear) smoothing algorithm for group-affine
observation systems, a recently introduced class of estimation problems on Lie
groups that bear a particular structure. As most non-linear smoothing methods,
the proposed algorithm is based on a maximum a posteriori estimator, determined
by ... | cs.RO | in this paper we propose a nonlinear smoothing algorithm for groupaffine observation systems a recently introduced class of estimation problems on lie groups that bear a particular structure as most nonlinear smoothing methods the proposed algorithm is based on a maximum a posteriori estimator determined by optimizatio... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'nonlinear', 'smoothing', 'algorithm', 'for', 'groupaffine', 'observation', 'systems', 'a', 'recently', 'introduced', 'class', 'of', 'estimation', 'problems', 'on', 'lie', 'groups', 'that', 'bear', 'a', 'particular', 'structure', 'as', 'most', 'nonlinear', 'smoothing', 'me... | [-0.08838619369769342, -0.001995536435431647, -0.09688259730538244, 0.05377712192068112, -0.1121631145423043, -0.1476938991843569, 0.02032356386387142, 0.3934451698244197, -0.2567200436611723, -0.3160625918959358, 0.17241933019786568, -0.22914004011206257, -0.206209111861541, 0.24055523461282471, -0.10003314743234405, ... |
1,803.02077 | The Contextual Loss for Image Transformation with Non-Aligned Data | Feed-forward CNNs trained for image transformation problems rely on loss
functions that measure the similarity between the generated image and a target
image. Most of the common loss functions assume that these images are spatially
aligned and compare pixels at corresponding locations. However, for many tasks,
aligne... | cs.CV cs.LG | feedforward cnns trained for image transformation problems rely on loss functions that measure the similarity between the generated image and a target image most of the common loss functions assume that these images are spatially aligned and compare pixels at corresponding locations however for many tasks aligned train... | [['feedforward', 'cnns', 'trained', 'for', 'image', 'transformation', 'problems', 'rely', 'on', 'loss', 'functions', 'that', 'measure', 'the', 'similarity', 'between', 'the', 'generated', 'image', 'and', 'a', 'target', 'image', 'most', 'of', 'the', 'common', 'loss', 'functions', 'assume', 'that', 'these', 'images', 'ar... | [-0.028253979619592428, 0.01072695462894626, -0.06240170784853399, 0.10454466267023235, -0.10023642277345061, -0.14820395212620496, -0.011427939568180591, 0.48215259730815885, -0.28143965317774566, -0.31952156499028206, 0.09681539266556502, -0.2726891626678407, -0.141199267975986, 0.22333337433636188, -0.11251641501486... |
1,803.02078 | Finite sample improvement of Akaike's Information Criterion | We emphasize that it is possible to improve the principle of unbiased risk
estimation for model selection by addressing excess risk deviations in the
design of penalization procedures. Indeed, we propose a modification of
Akaike's Information Criterion that avoids overfitting, even when the sample
size is small. We c... | math.ST cs.IT math.IT stat.TH | we emphasize that it is possible to improve the principle of unbiased risk estimation for model selection by addressing excess risk deviations in the design of penalization procedures indeed we propose a modification of akaikes information criterion that avoids overfitting even when the sample size is small we call thi... | [['we', 'emphasize', 'that', 'it', 'is', 'possible', 'to', 'improve', 'the', 'principle', 'of', 'unbiased', 'risk', 'estimation', 'for', 'model', 'selection', 'by', 'addressing', 'excess', 'risk', 'deviations', 'in', 'the', 'design', 'of', 'penalization', 'procedures', 'indeed', 'we', 'propose', 'a', 'modification', 'o... | [-0.04213900923280528, -0.00025984039681066793, -0.12040095921191904, 0.1275080496057247, -0.0768155003397691, -0.15770747116594402, 0.10211226365494508, 0.3958343795604176, -0.24153047807652642, -0.2971136636618111, 0.12107911037488116, -0.24822585818668205, -0.1608866426679823, 0.20595828729974866, -0.188453405205574... |
1,803.02079 | $\boldsymbol{\mathcal{\alpha}}$ decay properties of
$\boldsymbol{^{296}}$Og within the two-potential approach | The present work is a continuations of our previous paper [J.-G. Deng, et
al., Chin. Phys. C, {\bf41}: 124109 (2017)]. In present work, the
$\mathcal{\alpha}$ decay half-life of unknown nucleus $^{296}$Og is predicted
within the two-potential approach and the hindrance factors of all 20 even-even
nuclei in the same r... | nucl-th nucl-ex | the present work is a continuations of our previous paper jg deng et al chin phys c bf41 124109 2017 in present work the mathcalalpha decay halflife of unknown nucleus 296og is predicted within the twopotential approach and the hindrance factors of all 20 eveneven nuclei in the same region with 296og ie proton number 8... | [['the', 'present', 'work', 'is', 'a', 'continuations', 'of', 'our', 'previous', 'paper', 'jg', 'deng', 'et', 'al', 'chin', 'phys', 'c', 'bf41', '124109', '2017', 'in', 'present', 'work', 'the', 'mathcalalpha', 'decay', 'halflife', 'of', 'unknown', 'nucleus', '296og', 'is', 'predicted', 'within', 'the', 'twopotential',... | [-0.04558185945139625, 0.1381790537808019, -0.020340275823120743, 0.029701557173841417, 0.010462610489832094, -0.04003146136920595, 0.1126964768392589, 0.3060825249233928, -0.15937723115516397, -0.35379161548693305, -0.020987180119846016, -0.3047884375644991, -0.05244050325395969, 0.1702930349543189, -0.009605232569111... |
1,803.0208 | Constructive approach to limiting periodic orbits with exponential and
power law dynamics | In dynamical systems limit cycles arise as a result of a Hopf bifurcation,
after a control parameter has crossed its critical value. In this study we
present a constructive method to produce dissipative dynamics which lead to
stable periodic orbits as time grows, with predesigned transient dynamics.
Depending on the ... | nlin.CD | in dynamical systems limit cycles arise as a result of a hopf bifurcation after a control parameter has crossed its critical value in this study we present a constructive method to produce dissipative dynamics which lead to stable periodic orbits as time grows with predesigned transient dynamics depending on the constr... | [['in', 'dynamical', 'systems', 'limit', 'cycles', 'arise', 'as', 'a', 'result', 'of', 'a', 'hopf', 'bifurcation', 'after', 'a', 'control', 'parameter', 'has', 'crossed', 'its', 'critical', 'value', 'in', 'this', 'study', 'we', 'present', 'a', 'constructive', 'method', 'to', 'produce', 'dissipative', 'dynamics', 'which... | [-0.19578862785196038, 0.10654689265272911, -0.17194639983622786, 0.02535976510709868, -0.08015619245214531, -0.16759524624033545, 0.06627408506868121, 0.32780392127684677, -0.3083943123391901, -0.2542604334459891, 0.13273307197512343, -0.20044071136656455, -0.17651221341265438, 0.2479044902608551, -0.0763343418814027,... |
1,803.02081 | Statistical-mechanical analysis of compressed sensing for Hamiltonian
estimation of Ising spin glass | Several powerful machines, such as the D-Wave 2000Q, dedicated to solving
combinatorial optimization problems through the Ising-model formulation have
been developed. To input problems into the machines, the unknown parameters on
the Ising model must be determined, and this is necessarily a nontrivial task.
It could ... | cond-mat.stat-mech | several powerful machines such as the dwave 2000q dedicated to solving combinatorial optimization problems through the isingmodel formulation have been developed to input problems into the machines the unknown parameters on the ising model must be determined and this is necessarily a nontrivial task it could be benefic... | [['several', 'powerful', 'machines', 'such', 'as', 'the', 'dwave', '2000q', 'dedicated', 'to', 'solving', 'combinatorial', 'optimization', 'problems', 'through', 'the', 'isingmodel', 'formulation', 'have', 'been', 'developed', 'to', 'input', 'problems', 'into', 'the', 'machines', 'the', 'unknown', 'parameters', 'on', '... | [-0.07690875820385722, 0.05489375517846873, -0.11012572159525007, 0.04116069579210419, -0.08986632319597097, -0.13652495057322084, 0.04314065212115215, 0.387382055604114, -0.2896677559778954, -0.321955437399447, 0.1313156633091589, -0.21755199265451386, -0.17171863147568028, 0.23828102659004238, -0.01274448256724729, 0... |
1,803.02082 | Partitioning signed networks | Signed networks appear naturally in contexts where conflict or animosity is
apparent. In this book chapter we review some of the literature on signed
networks, especially in the context of partitioning. Most of the work is
founded in what is known as structural balance theory. We cover the basic
mathematical principl... | physics.soc-ph cs.SI | signed networks appear naturally in contexts where conflict or animosity is apparent in this book chapter we review some of the literature on signed networks especially in the context of partitioning most of the work is founded in what is known as structural balance theory we cover the basic mathematical principles of ... | [['signed', 'networks', 'appear', 'naturally', 'in', 'contexts', 'where', 'conflict', 'or', 'animosity', 'is', 'apparent', 'in', 'this', 'book', 'chapter', 'we', 'review', 'some', 'of', 'the', 'literature', 'on', 'signed', 'networks', 'especially', 'in', 'the', 'context', 'of', 'partitioning', 'most', 'of', 'the', 'wor... | [-0.10541582842900728, 0.05226282877886964, -0.09423789452193887, 0.10974149538499962, -0.10586683731283604, -0.0803888769733021, 0.06268317996970534, 0.3434535683700233, -0.2836210978239251, -0.32576862845841487, 0.10767627272677298, -0.2693053315015277, -0.26290013172789867, 0.13189082000705335, -0.1214196950677433, ... |
1,803.02083 | Detection of topological phase transitions through entropy measurements:
the case of germanene | We propose a characterization tool for studies of the band structure of new
materials promising for the observation of topological phase transitions. We
show that a specific resonant feature in the entropy per electron dependence on
the chemical potential may be considered as a fingerprint of the transition
between t... | cond-mat.mes-hall | we propose a characterization tool for studies of the band structure of new materials promising for the observation of topological phase transitions we show that a specific resonant feature in the entropy per electron dependence on the chemical potential may be considered as a fingerprint of the transition between topo... | [['we', 'propose', 'a', 'characterization', 'tool', 'for', 'studies', 'of', 'the', 'band', 'structure', 'of', 'new', 'materials', 'promising', 'for', 'the', 'observation', 'of', 'topological', 'phase', 'transitions', 'we', 'show', 'that', 'a', 'specific', 'resonant', 'feature', 'in', 'the', 'entropy', 'per', 'electron'... | [-0.1538047802643804, 0.1708281515814846, -0.06659836763752375, 0.039953331138408134, 0.006561803318726927, -0.11669526980559698, 0.11558152712066079, 0.3297933383024673, -0.24354060175156786, -0.3121432273634779, 0.013943217652479177, -0.3349207517996764, -0.1347619647540115, 0.15921119579915605, 0.03702223787908975, ... |
1,803.02084 | Long-range Low-power Wireless Networks and Sampling Strategies in
Electricity Metering | This paper studies a specific low-power wireless technology capable of
reaching a long range, namely LoRa. Such a technology can be used by different
applications in cities involving many transmitting devices while requiring
loose communication constrains. We focus on electricity grids, where LoRa
end-devices are sma... | eess.SP cs.SY | this paper studies a specific lowpower wireless technology capable of reaching a long range namely lora such a technology can be used by different applications in cities involving many transmitting devices while requiring loose communication constrains we focus on electricity grids where lora enddevices are smartmeters... | [['this', 'paper', 'studies', 'a', 'specific', 'lowpower', 'wireless', 'technology', 'capable', 'of', 'reaching', 'a', 'long', 'range', 'namely', 'lora', 'such', 'a', 'technology', 'can', 'be', 'used', 'by', 'different', 'applications', 'in', 'cities', 'involving', 'many', 'transmitting', 'devices', 'while', 'requiring... | [-0.1613106860146338, 0.06754695566628997, -0.05165341532710703, 0.055993997598663796, -0.07190943500850329, -0.2020529009342626, 0.11618884098047175, 0.39873842246706975, -0.25438408148655084, -0.33417329241557675, 0.1311512997789432, -0.2892958199520446, -0.14343391154900462, 0.2216720310006373, -0.1616643148973502, ... |
1,803.02085 | Semileptonic $\Lambda_{b}\rightarrow \Lambda_{c}{\ell}\bar\nu_{\ell}$
Transition in Full QCD | The tree-level $b\rightarrow c{\ell}\bar\nu_{\ell}$ based hadronic
transitions have been on the focus of much attention since recording
significant deviations of the experimental data, on the ratios of the branching
fractions in $ \tau $ and $ e-\mu $ channels of the semileptonic $ B
\rightarrow D $ transition, from ... | hep-ph hep-ex hep-lat | the treelevel brightarrow cellbarnu_ell based hadronic transitions have been on the focus of much attention since recording significant deviations of the experimental data on the ratios of the branching fractions in tau and emu channels of the semileptonic b rightarrow d transition from the sm predictions by babar coll... | [['the', 'treelevel', 'brightarrow', 'cellbarnu_ell', 'based', 'hadronic', 'transitions', 'have', 'been', 'on', 'the', 'focus', 'of', 'much', 'attention', 'since', 'recording', 'significant', 'deviations', 'of', 'the', 'experimental', 'data', 'on', 'the', 'ratios', 'of', 'the', 'branching', 'fractions', 'in', 'tau', 'a... | [-0.0493991047886918, 0.16842993141736265, -0.060540059403439234, 0.08867780791942599, -0.03836968318399066, -0.09357100027571817, 0.108180837641221, 0.30367523530249, -0.19871649957576376, -0.2501155190958766, 0.05447446116228487, -0.32268907096990307, -0.053486294138681285, 0.1518642205587784, 0.04969245030776046, 0.... |
1,803.02086 | Classes of Exactly Solvable Generalized Semi-Classical Rabi Systems | The exact quantum dynamics of a single spin-1/2 in a generic time-dependent
classical magnetic field is investigated and compared with the quantum motion
of a spin-1/2 studied by Rabi and Schwinger. The possibility of regarding the
scenario studied in this paper as a generalization of that considered by Rabi
and Schw... | quant-ph | the exact quantum dynamics of a single spin12 in a generic timedependent classical magnetic field is investigated and compared with the quantum motion of a spin12 studied by rabi and schwinger the possibility of regarding the scenario studied in this paper as a generalization of that considered by rabi and schwinger is... | [['the', 'exact', 'quantum', 'dynamics', 'of', 'a', 'single', 'spin12', 'in', 'a', 'generic', 'timedependent', 'classical', 'magnetic', 'field', 'is', 'investigated', 'and', 'compared', 'with', 'the', 'quantum', 'motion', 'of', 'a', 'spin12', 'studied', 'by', 'rabi', 'and', 'schwinger', 'the', 'possibility', 'of', 'reg... | [-0.16054421720748885, 0.19174313052567316, -0.06218090623944126, 0.08610382099992576, -0.03031292919718482, -0.14006876171952945, 0.03620711928964196, 0.3442495665735902, -0.22118806599718618, -0.2630606075167344, 0.0429337765263552, -0.23794758226227095, -0.1472217949624966, 0.21846802965514955, -0.017263297602147894... |
1,803.02087 | Two limit theorems for the high-dimensional two-stage contact process | In this paper we are concerned with the two-stage contact process introduced
in \cite{Krone1999} on a high-dimensional lattice. By comparing this process
with an auxiliary model which is a linear system, we obtain two limit theorems
for this process as the dimension of the lattice grows to infinity. The first
theorem... | math.PR | in this paper we are concerned with the twostage contact process introduced in citekrone1999 on a highdimensional lattice by comparing this process with an auxiliary model which is a linear system we obtain two limit theorems for this process as the dimension of the lattice grows to infinity the first theorem is about ... | [['in', 'this', 'paper', 'we', 'are', 'concerned', 'with', 'the', 'twostage', 'contact', 'process', 'introduced', 'in', 'citekrone1999', 'on', 'a', 'highdimensional', 'lattice', 'by', 'comparing', 'this', 'process', 'with', 'an', 'auxiliary', 'model', 'which', 'is', 'a', 'linear', 'system', 'we', 'obtain', 'two', 'limi... | [-0.11159918864217142, 0.10482165340537271, -0.1014139809716574, 0.06865513766722317, -0.02424611221573761, -0.10703369816157805, 0.06792339876815474, 0.3258707295981762, -0.2846527123094901, -0.2471751737985355, 0.17250342553344797, -0.2733278361392086, -0.14817124157739076, 0.1967222275409807, -0.06631755148080866, 0... |
1,803.02088 | Explain Yourself: A Natural Language Interface for Scrutable Autonomous
Robots | Autonomous systems in remote locations have a high degree of autonomy and
there is a need to explain what they are doing and why in order to increase
transparency and maintain trust. Here, we describe a natural language chat
interface that enables vehicle behaviour to be queried by the user. We obtain
an interpretabl... | cs.CL cs.AI cs.HC | autonomous systems in remote locations have a high degree of autonomy and there is a need to explain what they are doing and why in order to increase transparency and maintain trust here we describe a natural language chat interface that enables vehicle behaviour to be queried by the user we obtain an interpretable mod... | [['autonomous', 'systems', 'in', 'remote', 'locations', 'have', 'a', 'high', 'degree', 'of', 'autonomy', 'and', 'there', 'is', 'a', 'need', 'to', 'explain', 'what', 'they', 'are', 'doing', 'and', 'why', 'in', 'order', 'to', 'increase', 'transparency', 'and', 'maintain', 'trust', 'here', 'we', 'describe', 'a', 'natural'... | [-0.07100990021394359, 0.09994375065246087, -0.07399015485619505, 0.08480496002744918, -0.1627931813558529, -0.18898050113650108, 0.06327230420343026, 0.4494146750981195, -0.2468814300718131, -0.36463662616356657, 0.07945537769140813, -0.2975665670302179, -0.17946547410381888, 0.13263198643862442, -0.15180454646771843,... |
1,803.02089 | Optimal Independence-Checking Coding For Secure Uplink Training in
Large-Scale MISO-OFDM Systems | Due to the publicly-known deterministic character- istic of pilot tones,
pilot-aware attack, by jamming, nulling and spoofing pilot tones, can
significantly paralyze the uplink channel training in large-scale MISO-OFDM
systems. To solve this, we in this paper develop an independence-checking
coding based (ICCB) uplin... | eess.SP | due to the publiclyknown deterministic character istic of pilot tones pilotaware attack by jamming nulling and spoofing pilot tones can significantly paralyze the uplink channel training in largescale misoofdm systems to solve this we in this paper develop an independencechecking coding based iccb uplink training archi... | [['due', 'to', 'the', 'publiclyknown', 'deterministic', 'character', 'istic', 'of', 'pilot', 'tones', 'pilotaware', 'attack', 'by', 'jamming', 'nulling', 'and', 'spoofing', 'pilot', 'tones', 'can', 'significantly', 'paralyze', 'the', 'uplink', 'channel', 'training', 'in', 'largescale', 'misoofdm', 'systems', 'to', 'sol... | [-0.19304135243821366, 0.04034812089039447, -0.0315270236444689, 0.04768657741510754, -0.0654454776928739, -0.24180058158546416, 0.11618061061781026, 0.3976306402760798, -0.27226097713228803, -0.2768744673733747, 0.10697564391321313, -0.20044154334234968, -0.19168341102771783, 0.13123738122745776, -0.14664924683995392,... |
1,803.0209 | Spectroscopy of $\Omega_{ccb}$ baryon in Hypercentral Quark Model | We extract the mass spectra of triply heavy baryon $\Omega_{ccb}$ using
Hypercentral constituent quark model. The first order correction is also added
to the potential term of Hamiltonian. The radial and orbital excited state
masses are also determined. Moreover, the Regge trajectories and magnetic
moments are also g... | hep-ph | we extract the mass spectra of triply heavy baryon omega_ccb using hypercentral constituent quark model the first order correction is also added to the potential term of hamiltonian the radial and orbital excited state masses are also determined moreover the regge trajectories and magnetic moments are also given for th... | [['we', 'extract', 'the', 'mass', 'spectra', 'of', 'triply', 'heavy', 'baryon', 'omega_ccb', 'using', 'hypercentral', 'constituent', 'quark', 'model', 'the', 'first', 'order', 'correction', 'is', 'also', 'added', 'to', 'the', 'potential', 'term', 'of', 'hamiltonian', 'the', 'radial', 'and', 'orbital', 'excited', 'state... | [-0.10039181978094812, 0.25779387910905127, -0.07648669583175112, 0.1366395138788457, -0.06769867420342623, -0.07961506268703471, 0.055044793350366404, 0.3093001681434758, -0.2231236832289427, -0.29419880937419685, -0.03212239855316048, -0.3485199824779057, -0.0037179941987144013, 0.08119538897082355, 0.068524037798245... |
1,803.02091 | On-off intermittency and chaotic walks | We consider a class of skew product maps of interval diffeomorphisms over the
doubling map. The interval maps fix the end points of the interval. It is
assumed that the system has zero fiber Lyapunov exponent at one endpoint and
zero or positive fiber Lyapunov exponent at the other endpoint. We prove the
appearance o... | math.DS | we consider a class of skew product maps of interval diffeomorphisms over the doubling map the interval maps fix the end points of the interval it is assumed that the system has zero fiber lyapunov exponent at one endpoint and zero or positive fiber lyapunov exponent at the other endpoint we prove the appearance of ono... | [['we', 'consider', 'a', 'class', 'of', 'skew', 'product', 'maps', 'of', 'interval', 'diffeomorphisms', 'over', 'the', 'doubling', 'map', 'the', 'interval', 'maps', 'fix', 'the', 'end', 'points', 'of', 'the', 'interval', 'it', 'is', 'assumed', 'that', 'the', 'system', 'has', 'zero', 'fiber', 'lyapunov', 'exponent', 'at... | [-0.20275905031528438, 0.17428710920371346, -0.09675444220286962, 0.06740656448648186, -0.013979656589409509, -0.18773745295601255, 0.09781146569888002, 0.36819499673456263, -0.30088185964958725, -0.13118971262568818, 0.17683731016616538, -0.28163672795461625, -0.14859742767503964, 0.2093864623241165, -0.04912412048499... |
1,803.02092 | Resonant excitation of infra-red emission in GaN:(Mn,Mg) | By combining experimental photoluminescence excitation spectroscopy and
calculations based on density functional theory and many-body Green's
functions, the most efficient excitation channels of infra-red (IR) emission
from Mn-Mg$_{k}$ paramagnetic complexes stabilized in GaN:(Mn,Mg) are here
identified. Moreover, a ... | cond-mat.mtrl-sci | by combining experimental photoluminescence excitation spectroscopy and calculations based on density functional theory and manybody greens functions the most efficient excitation channels of infrared ir emission from mnmg_k paramagnetic complexes stabilized in ganmnmg are here identified moreover a tanabesugano energy... | [['by', 'combining', 'experimental', 'photoluminescence', 'excitation', 'spectroscopy', 'and', 'calculations', 'based', 'on', 'density', 'functional', 'theory', 'and', 'manybody', 'greens', 'functions', 'the', 'most', 'efficient', 'excitation', 'channels', 'of', 'infrared', 'ir', 'emission', 'from', 'mnmg_k', 'paramagn... | [-0.08185165194473007, 0.13638477592862078, -0.07063644407926836, 0.10095280295354314, 0.009443954198754259, -0.11969917142275899, 0.07849536842661023, 0.46361474887955756, -0.21630669762851626, -0.29255070777920383, 0.034513827971836906, -0.31030070001465254, -0.08480782970409131, 0.1565859451227533, 0.109419873089618... |
1,803.02093 | Twist-induced crossover from 2D to 3D turbulence in active nematics | While studies of active nematics in two dimensions have shed light on various
aspects of the flow regimes and topology of active matter, three-dimensional
properties of topological defects and chaotic flows remain unexplored. By
confining a film of active nematics between two parallel plates, we use
continuum simulat... | cond-mat.soft physics.flu-dyn | while studies of active nematics in two dimensions have shed light on various aspects of the flow regimes and topology of active matter threedimensional properties of topological defects and chaotic flows remain unexplored by confining a film of active nematics between two parallel plates we use continuum simulations a... | [['while', 'studies', 'of', 'active', 'nematics', 'in', 'two', 'dimensions', 'have', 'shed', 'light', 'on', 'various', 'aspects', 'of', 'the', 'flow', 'regimes', 'and', 'topology', 'of', 'active', 'matter', 'threedimensional', 'properties', 'of', 'topological', 'defects', 'and', 'chaotic', 'flows', 'remain', 'unexplore... | [-0.19229524072543686, 0.2407155359784762, -0.05768501893980495, 0.03153263993234314, -0.02197034148406898, -0.15769721618820484, 0.02588997909416121, 0.3802025201895558, -0.25977351776066615, -0.2843040902669548, 0.0663493775864997, -0.2794843210462243, -0.18550968382190516, 0.15437492026438845, -0.008226998029289114,... |
1,803.02094 | Developments of Multi-wavelength Spectro-Polarimeter on the Domeless
Solar Telescope at Hida Observatory | To obtain full Stokes spectra in multi-wavelength windows simultaneously, we
developed a new spectro-polarimeter on the Domeless Solar Telescope at Hida
Observatory. The new polarimeter consists of a 60 cm aperture vacuum telescope
on an altazimuth mount, an image rotator, a high dispersion spectrograph,
polarization... | astro-ph.IM astro-ph.SR | to obtain full stokes spectra in multiwavelength windows simultaneously we developed a new spectropolarimeter on the domeless solar telescope at hida observatory the new polarimeter consists of a 60 cm aperture vacuum telescope on an altazimuth mount an image rotator a high dispersion spectrograph polarization modulato... | [['to', 'obtain', 'full', 'stokes', 'spectra', 'in', 'multiwavelength', 'windows', 'simultaneously', 'we', 'developed', 'a', 'new', 'spectropolarimeter', 'on', 'the', 'domeless', 'solar', 'telescope', 'at', 'hida', 'observatory', 'the', 'new', 'polarimeter', 'consists', 'of', 'a', '60', 'cm', 'aperture', 'vacuum', 'tel... | [-0.11087838672591667, 0.15803356395849014, -0.06197768634140773, 0.015105225276324507, -0.07842564294421064, -0.1656949179516615, -0.00021398041127739767, 0.42536499007654033, -0.2080285908654332, -0.3864411989815141, 0.08909119865734522, -0.2730206401467991, -0.03341679340105896, 0.27566196222814093, -0.0485289876986... |
1,803.02095 | Local negative circuits and cyclic attractors in Boolean networks with
at most five components | We consider the following question on the relationship between the asymptotic
behaviours of asynchronous dynamics of Boolean networks and their regulatory
structures: does the presence of a cyclic attractor imply the existence of a
local negative circuit in the regulatory graph? When the number of model
components $n... | cs.DM | we consider the following question on the relationship between the asymptotic behaviours of asynchronous dynamics of boolean networks and their regulatory structures does the presence of a cyclic attractor imply the existence of a local negative circuit in the regulatory graph when the number of model components n veri... | [['we', 'consider', 'the', 'following', 'question', 'on', 'the', 'relationship', 'between', 'the', 'asymptotic', 'behaviours', 'of', 'asynchronous', 'dynamics', 'of', 'boolean', 'networks', 'and', 'their', 'regulatory', 'structures', 'does', 'the', 'presence', 'of', 'a', 'cyclic', 'attractor', 'imply', 'the', 'existenc... | [-0.2198746842223891, 0.1122305466136498, -0.00474244971261468, 0.07440434728546949, -0.03698306208721889, -0.1701719962717431, 0.07092697775828861, 0.3025668828437726, -0.27044918990239153, -0.30690638027550987, 0.0770482843896995, -0.25393427420378656, -0.17319294049354025, 0.15823361436997058, -0.033994313805948854,... |
1,803.02096 | Cooperative Tracking of Cyclists Based on Smart Devices and
Infrastructure | In future traffic scenarios, vehicles and other traffic participants will be
interconnected and equipped with various types of sensors, allowing for
cooperation based on data or information exchange. This article presents an
approach to cooperative tracking of cyclists using smart devices and
infrastructure-based sen... | cs.CY cs.AI | in future traffic scenarios vehicles and other traffic participants will be interconnected and equipped with various types of sensors allowing for cooperation based on data or information exchange this article presents an approach to cooperative tracking of cyclists using smart devices and infrastructurebased sensors a... | [['in', 'future', 'traffic', 'scenarios', 'vehicles', 'and', 'other', 'traffic', 'participants', 'will', 'be', 'interconnected', 'and', 'equipped', 'with', 'various', 'types', 'of', 'sensors', 'allowing', 'for', 'cooperation', 'based', 'on', 'data', 'or', 'information', 'exchange', 'this', 'article', 'presents', 'an', ... | [-0.16632681011400197, 0.04506323625177624, -0.05163947238686254, -0.02513409887631476, -0.09702451127120869, -0.19769270245372997, 0.053405813096494024, 0.4034611873611222, -0.22038873891461264, -0.35143810703701683, 0.11582334995010785, -0.3429202090744766, -0.1327105636650885, 0.21895461998555515, -0.188207987606985... |
1,803.02097 | Where is my Device? - Detecting the Smart Device's Wearing Location in
the Context of Active Safety for Vulnerable Road Users | This article describes an approach to detect the wearing location of smart
devices worn by pedestrians and cyclists. The detection, which is based solely
on the sensors of the smart devices, is important context-information which can
be used to parametrize subsequent algorithms, e.g. for dead reckoning or
intention d... | cs.HC cs.AI cs.CV | this article describes an approach to detect the wearing location of smart devices worn by pedestrians and cyclists the detection which is based solely on the sensors of the smart devices is important contextinformation which can be used to parametrize subsequent algorithms eg for dead reckoning or intention detection ... | [['this', 'article', 'describes', 'an', 'approach', 'to', 'detect', 'the', 'wearing', 'location', 'of', 'smart', 'devices', 'worn', 'by', 'pedestrians', 'and', 'cyclists', 'the', 'detection', 'which', 'is', 'based', 'solely', 'on', 'the', 'sensors', 'of', 'the', 'smart', 'devices', 'is', 'important', 'contextinformatio... | [-0.10719536165567733, 0.0625509573034664, -0.06950728580627623, -0.0147193352813621, -0.11004876463459723, -0.2029539478769674, 0.05022557162699306, 0.3805692410838287, -0.215076064633255, -0.3484794567874839, 0.1480663083895497, -0.30070463813989695, -0.160754946365425, 0.1967058398171567, -0.20477557137956034, 0.024... |
1,803.02098 | Orbit equivalence and classification of weak solenoids | In this work, we study minimal equicontinuous actions which are locally
quasi-analytic. The first main result shows that for minimal equicontinuous
actions which are locally quasi-analytic, continuous orbit equivalence of the
actions implies return equivalence. This generalizes results of Cortez and
Medynets, and of ... | math.DS | in this work we study minimal equicontinuous actions which are locally quasianalytic the first main result shows that for minimal equicontinuous actions which are locally quasianalytic continuous orbit equivalence of the actions implies return equivalence this generalizes results of cortez and medynets and of li the se... | [['in', 'this', 'work', 'we', 'study', 'minimal', 'equicontinuous', 'actions', 'which', 'are', 'locally', 'quasianalytic', 'the', 'first', 'main', 'result', 'shows', 'that', 'for', 'minimal', 'equicontinuous', 'actions', 'which', 'are', 'locally', 'quasianalytic', 'continuous', 'orbit', 'equivalence', 'of', 'the', 'act... | [-0.1938311615553887, 0.14853806909235098, -0.0716721075561667, 0.05021298698240729, -0.10460344707066922, -0.10954281105153749, 0.01780009799150993, 0.39163468420282815, -0.3028663197916973, -0.15784680607485707, 0.12672035613112434, -0.23285128127621568, -0.19667976965074954, 0.21257997062259718, -0.18984845173848874... |
1,803.02099 | A Hybrid Method for Traffic Flow Forecasting Using Multimodal Deep
Learning | Traffic flow forecasting has been regarded as a key problem of intelligent
transport systems. In this work, we propose a hybrid multimodal deep learning
method for short-term traffic flow forecasting, which can jointly and
adaptively learn the spatial-temporal correlation features and long temporal
interdependence of... | cs.LG cs.SY | traffic flow forecasting has been regarded as a key problem of intelligent transport systems in this work we propose a hybrid multimodal deep learning method for shortterm traffic flow forecasting which can jointly and adaptively learn the spatialtemporal correlation features and long temporal interdependence of multim... | [['traffic', 'flow', 'forecasting', 'has', 'been', 'regarded', 'as', 'a', 'key', 'problem', 'of', 'intelligent', 'transport', 'systems', 'in', 'this', 'work', 'we', 'propose', 'a', 'hybrid', 'multimodal', 'deep', 'learning', 'method', 'for', 'shortterm', 'traffic', 'flow', 'forecasting', 'which', 'can', 'jointly', 'and... | [-0.07009687540744236, 0.015005509251269667, -0.08569942680513783, 0.07807039424137859, -0.11583669346039462, -0.21902018763231718, -0.0298948422012032, 0.46670632313486116, -0.3314887550066279, -0.2803445650786636, 0.03752633179078223, -0.26767108788725674, -0.23818822984530288, 0.16621943811031806, -0.143365977634527... |
1,803.021 | The ORCA Hub: Explainable Offshore Robotics through Intelligent
Interfaces | We present the UK Robotics and Artificial Intelligence Hub for Offshore
Robotics for Certification of Assets (ORCA Hub), a 3.5 year EPSRC funded,
multi-site project. The ORCA Hub vision is to use teams of robots and
autonomous intelligent systems (AIS) to work on offshore energy platforms to
enable cheaper, safer and... | cs.AI cs.HC cs.RO | we present the uk robotics and artificial intelligence hub for offshore robotics for certification of assets orca hub a 35 year epsrc funded multisite project the orca hub vision is to use teams of robots and autonomous intelligent systems ais to work on offshore energy platforms to enable cheaper safer and more effici... | [['we', 'present', 'the', 'uk', 'robotics', 'and', 'artificial', 'intelligence', 'hub', 'for', 'offshore', 'robotics', 'for', 'certification', 'of', 'assets', 'orca', 'hub', 'a', '35', 'year', 'epsrc', 'funded', 'multisite', 'project', 'the', 'orca', 'hub', 'vision', 'is', 'to', 'use', 'teams', 'of', 'robots', 'and', '... | [-0.14604422363513353, 0.1244559963016846, -0.022995321282550045, 0.05775923611124781, -0.1310488958510437, -0.16754899142448854, 0.0659911758092851, 0.394735839839747, -0.202171452543033, -0.34772556119234016, 0.1558917932933983, -0.2972572995537765, -0.17356326812133482, 0.22223676359194175, -0.15904031971307553, 0.0... |
1,803.02101 | VIPE: A new interactive classification framework for large sets of short
texts - application to opinion mining | This paper presents a new interactive opinion mining tool that helps users to
classify large sets of short texts originated from Web opinion polls, technical
forums or Twitter. From a manual multi-label pre-classification of a very
limited text subset, a learning algorithm predicts the labels of the remaining
texts o... | cs.IR | this paper presents a new interactive opinion mining tool that helps users to classify large sets of short texts originated from web opinion polls technical forums or twitter from a manual multilabel preclassification of a very limited text subset a learning algorithm predicts the labels of the remaining texts of the c... | [['this', 'paper', 'presents', 'a', 'new', 'interactive', 'opinion', 'mining', 'tool', 'that', 'helps', 'users', 'to', 'classify', 'large', 'sets', 'of', 'short', 'texts', 'originated', 'from', 'web', 'opinion', 'polls', 'technical', 'forums', 'or', 'twitter', 'from', 'a', 'manual', 'multilabel', 'preclassification', '... | [-0.06826775193523213, 0.021577199285660507, -0.05458921333034997, 0.10513018891392907, -0.17838454614709115, -0.13287101429492487, 0.12572014768375084, 0.4001394797242799, -0.25054382635931627, -0.3168345090057069, 0.07189442960533582, -0.3525775443107458, -0.1345186048459609, 0.20527522422381186, -0.13236033390433985... |
1,803.02102 | On a degenerate singular elliptic problem | In this article we provide existence, uniqueness and regularity results of a
degenerate singular elliptic boundary value problem whose prototype is given by
\begin{gather*}
\begin{cases}
-\operatorname{div}(w(x)|\nabla u|^{p-2}\nabla
u)=\frac{f(x)}{u^\delta}\,\,\text{ in }\,\,\Omega,
u>0\text{ in }\Omega,\\ u =... | math.AP | in this article we provide existence uniqueness and regularity results of a degenerate singular elliptic boundary value problem whose prototype is given by begingather begincases operatornamedivwxnabla up2nabla ufracfxudeltatext in omega u0text in omega u 0 text on partialomega endcases endgather where omega is a bound... | [['in', 'this', 'article', 'we', 'provide', 'existence', 'uniqueness', 'and', 'regularity', 'results', 'of', 'a', 'degenerate', 'singular', 'elliptic', 'boundary', 'value', 'problem', 'whose', 'prototype', 'is', 'given', 'by', 'begingather', 'begincases', 'operatornamedivwxnabla', 'up2nabla', 'ufracfxudeltatext', 'in',... | [-0.21502491565317744, 0.062143062868421514, 0.02431869670140764, -0.0007148731286482265, -0.15271805026956523, -0.23649598565599364, -0.05388367975926182, 0.3480538295633677, -0.3404767815954983, -0.08817554679181841, 0.15469632204298656, -0.38409145559287733, -0.027818038254433002, 0.1425902692798344, -0.140102431889... |
1,803.02103 | Event-based Electricity Metering: An Autonomous Method to Determine
Transmission Thresholds | This paper provides an in-depth analysis of the event-based metering strategy
proposed by Simonov et al. This strategy is an alternative to the traditional
periodic (time-based) metering where the power demand is averaged in fixed time
periods (e.g. every 15 minutes). The event-based approach considers two
thresholds... | cs.SY | this paper provides an indepth analysis of the eventbased metering strategy proposed by simonov et al this strategy is an alternative to the traditional periodic timebased metering where the power demand is averaged in fixed time periods eg every 15 minutes the eventbased approach considers two thresholds that trigger ... | [['this', 'paper', 'provides', 'an', 'indepth', 'analysis', 'of', 'the', 'eventbased', 'metering', 'strategy', 'proposed', 'by', 'simonov', 'et', 'al', 'this', 'strategy', 'is', 'an', 'alternative', 'to', 'the', 'traditional', 'periodic', 'timebased', 'metering', 'where', 'the', 'power', 'demand', 'is', 'averaged', 'in... | [-0.11750323428008666, 0.041666867571389654, -0.08167069758466214, 0.03726284008343957, -0.059143407960729186, -0.14166175898142977, 0.09376281585525506, 0.36463730987645904, -0.2649923503867248, -0.35057729054134706, 0.08451367010809266, -0.2761529472724177, -0.11389160762417179, 0.22747475829384575, -0.12736773827904... |
1,803.02104 | Effect of fluid inertia on swimming of a sphere in a viscous
incompressible fluid | Swimming of a sphere in a viscous incompressible fluid is studied on the
basis of the Navier-Stokes equations for wave-type distortions of the spherical
shape. At sizable values of the dimensionless scale number the mean swimming
velocity is the result of a delicate balance between the net time-averaged flow
generate... | physics.flu-dyn | swimming of a sphere in a viscous incompressible fluid is studied on the basis of the navierstokes equations for wavetype distortions of the spherical shape at sizable values of the dimensionless scale number the mean swimming velocity is the result of a delicate balance between the net timeaveraged flow generated dire... | [['swimming', 'of', 'a', 'sphere', 'in', 'a', 'viscous', 'incompressible', 'fluid', 'is', 'studied', 'on', 'the', 'basis', 'of', 'the', 'navierstokes', 'equations', 'for', 'wavetype', 'distortions', 'of', 'the', 'spherical', 'shape', 'at', 'sizable', 'values', 'of', 'the', 'dimensionless', 'scale', 'number', 'the', 'me... | [-0.1692418235963067, 0.18193928989916083, -0.10663681961775112, 0.0008355670695145351, -0.0430354765591731, -0.045843883184716105, -0.02673413253386314, 0.252193922857539, -0.3004399840421497, -0.3329555613394731, 0.045929104182272196, -0.23350714784091672, -0.0749230423467592, 0.20793269499121472, -0.0361212201969465... |
1,803.02105 | Nonlinear Photoelasticity to Explicate Acoustic Dephasing Dynamics | Detection and controlling of acoustic (AC) phonon phase have been strenuous
tasks although such capability is crucial for further manipulating thermal
properties. Here, we present a versatile formalism for tracing AC nanowaves
with arbitrary strain compositions by incorporating the nonlinear
photoelasticity (PE) into... | physics.app-ph cond-mat.mes-hall | detection and controlling of acoustic ac phonon phase have been strenuous tasks although such capability is crucial for further manipulating thermal properties here we present a versatile formalism for tracing ac nanowaves with arbitrary strain compositions by incorporating the nonlinear photoelasticity pe into ultrafa... | [['detection', 'and', 'controlling', 'of', 'acoustic', 'ac', 'phonon', 'phase', 'have', 'been', 'strenuous', 'tasks', 'although', 'such', 'capability', 'is', 'crucial', 'for', 'further', 'manipulating', 'thermal', 'properties', 'here', 'we', 'present', 'a', 'versatile', 'formalism', 'for', 'tracing', 'ac', 'nanowaves',... | [-0.1325370625182808, 0.21978308302328062, -0.04021244756119887, -0.010642597656786157, -0.0746226725213087, -0.153362573309396, 0.08080125684765252, 0.41552175695196897, -0.3013862459630701, -0.26775515745043016, 0.05666362462703441, -0.28331588753209447, -0.12178620670668104, 0.261342157019329, 0.030698328884986883, ... |
1,803.02106 | The PoGO+ Balloon-Borne Hard X-ray Polarimetry Mission | The PoGO mission, including the PoGOLite Pathfinder and PoGO+, aims to
provide polarimetric measurements of the Crab system and Cygnus X-1 in the hard
X-ray band. Measurements are conducted from a stabilized balloon-borne
platform, launched on a 1 million cubic meter balloon from the Esrange Space
Center in Sweden to... | astro-ph.IM | the pogo mission including the pogolite pathfinder and pogo aims to provide polarimetric measurements of the crab system and cygnus x1 in the hard xray band measurements are conducted from a stabilized balloonborne platform launched on a 1 million cubic meter balloon from the esrange space center in sweden to an altitu... | [['the', 'pogo', 'mission', 'including', 'the', 'pogolite', 'pathfinder', 'and', 'pogo', 'aims', 'to', 'provide', 'polarimetric', 'measurements', 'of', 'the', 'crab', 'system', 'and', 'cygnus', 'x1', 'in', 'the', 'hard', 'xray', 'band', 'measurements', 'are', 'conducted', 'from', 'a', 'stabilized', 'balloonborne', 'pla... | [-0.11237037955741573, 0.11534366934279634, -0.07661633939429555, -0.010863781400367548, -0.07251453902220951, -0.0863929989951979, 0.029807880898621283, 0.4013568840191682, -0.1782432260993376, -0.37630514795276915, 0.1909690141987565, -0.3638361032331749, -0.05150474640013615, 0.31124867871403694, -0.0156234275496933... |
1,803.02107 | Optimal Grassmann Manifold Eavesdropping: A Huge Security Disaster for
M-1-2 Wiretap Channels | We in this paper introduce an advanced eavesdropper that aims to paralyze the
artificial-noise-aided secure communications. We consider the M-1-2 Gaussian
MISO wiretap channel, which consists of a M-antenna transmitter, a
single-antenna receiver, and a two-antenna eavesdropper. This type of
eavesdropper, by adopting ... | cs.CR cs.IT math.IT | we in this paper introduce an advanced eavesdropper that aims to paralyze the artificialnoiseaided secure communications we consider the m12 gaussian miso wiretap channel which consists of a mantenna transmitter a singleantenna receiver and a twoantenna eavesdropper this type of eavesdropper by adopting an optimal gras... | [['we', 'in', 'this', 'paper', 'introduce', 'an', 'advanced', 'eavesdropper', 'that', 'aims', 'to', 'paralyze', 'the', 'artificialnoiseaided', 'secure', 'communications', 'we', 'consider', 'the', 'm12', 'gaussian', 'miso', 'wiretap', 'channel', 'which', 'consists', 'of', 'a', 'mantenna', 'transmitter', 'a', 'singleante... | [-0.22281726676797897, 0.015420354931173035, -0.03629012063827327, 0.03556035549808229, -0.08413598979126449, -0.26905369219495, 0.09960222440308497, 0.3605068032677794, -0.28068951333959385, -0.23379223926152468, 0.126396890420025, -0.2572408749106263, -0.18828299726580375, 0.12140972327114534, -0.14658778861837735, 0... |
1,803.02108 | HexaConv | The effectiveness of Convolutional Neural Networks stems in large part from
their ability to exploit the translation invariance that is inherent in many
learning problems. Recently, it was shown that CNNs can exploit other
invariances, such as rotation invariance, by using group convolutions instead
of planar convolu... | cs.LG stat.ML | the effectiveness of convolutional neural networks stems in large part from their ability to exploit the translation invariance that is inherent in many learning problems recently it was shown that cnns can exploit other invariances such as rotation invariance by using group convolutions instead of planar convolutions ... | [['the', 'effectiveness', 'of', 'convolutional', 'neural', 'networks', 'stems', 'in', 'large', 'part', 'from', 'their', 'ability', 'to', 'exploit', 'the', 'translation', 'invariance', 'that', 'is', 'inherent', 'in', 'many', 'learning', 'problems', 'recently', 'it', 'was', 'shown', 'that', 'cnns', 'can', 'exploit', 'oth... | [-0.09532200248213485, 0.07246430476090678, -0.03588673868216574, 0.019444446902028022, -0.12384653058153454, -0.13926640011255964, 0.01855030504246418, 0.47664437952609556, -0.2985836268130268, -0.3154502813528591, 0.1076433232525267, -0.24995284285044894, -0.1951797153506393, 0.18073360096248095, -0.11834071088968864... |
1,803.02109 | A global stochastic maximum principle for fully coupled forward-backward
stochastic systems | We study a stochastic optimal control problem for fully coupled
forward-backward stochastic control systems with a nonempty control domain. For
our problem, the first-order and second-order variational equations are fully
coupled linear FBSDEs. Inspired by Hu (Hu, Probability, Uncertainty and
Quantitative Risk, 2(1) ... | math.OC | we study a stochastic optimal control problem for fully coupled forwardbackward stochastic control systems with a nonempty control domain for our problem the firstorder and secondorder variational equations are fully coupled linear fbsdes inspired by hu hu probability uncertainty and quantitative risk 21 2017pp 120 we ... | [['we', 'study', 'a', 'stochastic', 'optimal', 'control', 'problem', 'for', 'fully', 'coupled', 'forwardbackward', 'stochastic', 'control', 'systems', 'with', 'a', 'nonempty', 'control', 'domain', 'for', 'our', 'problem', 'the', 'firstorder', 'and', 'secondorder', 'variational', 'equations', 'are', 'fully', 'coupled', ... | [-0.1396426044171676, 0.04692087224349962, -0.050105870524421336, 0.08097432111972011, -0.13050115526653827, -0.15765251045115292, 0.05138524886686355, 0.2643534201011062, -0.38059679137775676, -0.27032944324426356, 0.13495787736494094, -0.25730533625930546, -0.16710999336850363, 0.17517155225854367, -0.082909071706235... |
1,803.0211 | Localization control of few-photon states in parity-symmetric photonic
molecules under balanced pumping | We theoretically investigate the problem of localization control of
few-photon states in driven-dissipative parity-symmetric photonic molecules. We
show that a quantum feedback loop can utilize the information of the
spontaneously-emitted photons from each cavity to induce asymmetric photon
population in the system, ... | quant-ph | we theoretically investigate the problem of localization control of fewphoton states in drivendissipative paritysymmetric photonic molecules we show that a quantum feedback loop can utilize the information of the spontaneouslyemitted photons from each cavity to induce asymmetric photon population in the system while ma... | [['we', 'theoretically', 'investigate', 'the', 'problem', 'of', 'localization', 'control', 'of', 'fewphoton', 'states', 'in', 'drivendissipative', 'paritysymmetric', 'photonic', 'molecules', 'we', 'show', 'that', 'a', 'quantum', 'feedback', 'loop', 'can', 'utilize', 'the', 'information', 'of', 'the', 'spontaneouslyemit... | [-0.16308528434258895, 0.14609301914939674, -0.07353533906470462, 0.07502954293077237, -0.024200600032285552, -0.1686131664786801, 0.05955193224732947, 0.4275327851282102, -0.266124560523813, -0.2914022481260456, 0.0347511577539616, -0.2857962220637389, -0.1500197983233728, 0.18981073822643363, -0.03320488047342156, 0.... |
1,803.02111 | Algorithmic bias amplifies opinion polarization: A bounded confidence
model | The flow of information reaching us via the online media platforms is
optimized not by the information content or relevance but by popularity and
proximity to the target. This is typically performed in order to maximise
platform usage. As a side effect, this introduces an algorithmic bias that is
believed to enhance ... | physics.soc-ph cs.MA cs.SI | the flow of information reaching us via the online media platforms is optimized not by the information content or relevance but by popularity and proximity to the target this is typically performed in order to maximise platform usage as a side effect this introduces an algorithmic bias that is believed to enhance polar... | [['the', 'flow', 'of', 'information', 'reaching', 'us', 'via', 'the', 'online', 'media', 'platforms', 'is', 'optimized', 'not', 'by', 'the', 'information', 'content', 'or', 'relevance', 'but', 'by', 'popularity', 'and', 'proximity', 'to', 'the', 'target', 'this', 'is', 'typically', 'performed', 'in', 'order', 'to', 'ma... | [-0.10062090588526103, 0.10916832622582859, -0.09968654995660575, 0.08007627531115884, -0.09868121848737388, -0.14298095890228146, 0.09910355012155452, 0.38047704263038545, -0.2879154860644526, -0.30113350720612675, 0.10422127325776347, -0.2923792809053761, -0.11428435701740049, 0.12151421638320407, -0.0546267799019303... |
1,803.02112 | Nonlocality-Reinforced Convolutional Neural Networks for Image Denoising | We introduce a paradigm for nonlocal sparsity reinforced deep convolutional
neural network denoising. It is a combination of a local multiscale denoising
by a convolutional neural network (CNN) based denoiser and a nonlocal denoising
based on a nonlocal filter (NLF) exploiting the mutual similarities between
groups o... | eess.IV cs.CV | we introduce a paradigm for nonlocal sparsity reinforced deep convolutional neural network denoising it is a combination of a local multiscale denoising by a convolutional neural network cnn based denoiser and a nonlocal denoising based on a nonlocal filter nlf exploiting the mutual similarities between groups of patch... | [['we', 'introduce', 'a', 'paradigm', 'for', 'nonlocal', 'sparsity', 'reinforced', 'deep', 'convolutional', 'neural', 'network', 'denoising', 'it', 'is', 'a', 'combination', 'of', 'a', 'local', 'multiscale', 'denoising', 'by', 'a', 'convolutional', 'neural', 'network', 'cnn', 'based', 'denoiser', 'and', 'a', 'nonlocal'... | [-0.030200178733538474, -0.05093265901690224, -0.09410918883721882, 0.055726999761461, -0.0818673310824102, -0.23289637560236867, -0.03591550815456766, 0.4717360901669031, -0.3076262747096579, -0.272495296011429, 0.027194410846455068, -0.25254337498312435, -0.2820489860965106, 0.11779926026739725, -0.1280955818436313, ... |
1,803.02113 | Propagators for the time-dependent Kohn-Sham equations: multistep,
Runge-Kutta, exponential Runge-Kutta, and commutator free Magnus methods | We examine various integration schemes for the time-dependent Kohn-Sham
equations. Contrary to the time-dependent Schr\"odinger's equation, this set of
equations is non-linear, due to the dependence of the Hamiltonian on the
electronic density. We discuss some of their exact properties, and in
particular their symple... | physics.comp-ph physics.chem-ph | we examine various integration schemes for the timedependent kohnsham equations contrary to the timedependent schrodingers equation this set of equations is nonlinear due to the dependence of the hamiltonian on the electronic density we discuss some of their exact properties and in particular their symplectic structure... | [['we', 'examine', 'various', 'integration', 'schemes', 'for', 'the', 'timedependent', 'kohnsham', 'equations', 'contrary', 'to', 'the', 'timedependent', 'schrodingers', 'equation', 'this', 'set', 'of', 'equations', 'is', 'nonlinear', 'due', 'to', 'the', 'dependence', 'of', 'the', 'hamiltonian', 'on', 'the', 'electroni... | [-0.13591935803983793, 0.025936549794751892, -0.10840984009379565, 0.10974957989239993, -0.080834783772512, -0.10400683089166649, -0.019023711760636677, 0.40695169854948887, -0.2614288433658432, -0.272011570401432, 0.10061164059073398, -0.23787488734580634, -0.1474533243097596, 0.1958878665834001, -0.046797543182940216... |
1,803.02114 | A continuous-time persistent random walk model for flocking | Random walkers characterized by random positions and random velocities lead
to normal diffusion. A random walk was originally proposed by Einstein to model
Brownian motion and to demonstrate the existence of atoms and molecules. Such a
walker represents an inanimate particle driven by environmental fluctuations.
On t... | cond-mat.stat-mech | random walkers characterized by random positions and random velocities lead to normal diffusion a random walk was originally proposed by einstein to model brownian motion and to demonstrate the existence of atoms and molecules such a walker represents an inanimate particle driven by environmental fluctuations on the ot... | [['random', 'walkers', 'characterized', 'by', 'random', 'positions', 'and', 'random', 'velocities', 'lead', 'to', 'normal', 'diffusion', 'a', 'random', 'walk', 'was', 'originally', 'proposed', 'by', 'einstein', 'to', 'model', 'brownian', 'motion', 'and', 'to', 'demonstrate', 'the', 'existence', 'of', 'atoms', 'and', 'm... | [-0.10676190666157015, 0.2600907791020818, -0.03635339251216636, 0.026015105712956385, -0.03323693520160041, -0.1657389694676343, 0.03234097115686478, 0.3913271295262168, -0.24601551491299256, -0.3106725586101341, 0.04316593864415255, -0.3042494172234862, -0.18694373646949008, 0.1447823163518988, -0.03329734585657356, ... |
1,803.02115 | Subradiant states of quantum bits coupled to a one-dimensional waveguide | The properties of coupled emitters can differ dramatically from those of
their individual constituents. Canonical examples include sub- and
super-radiance, wherein the decay rate of a collective excitation is reduced or
enhanced due to correlated interactions with the environment. Here, we
systematically study the pr... | quant-ph | the properties of coupled emitters can differ dramatically from those of their individual constituents canonical examples include sub and superradiance wherein the decay rate of a collective excitation is reduced or enhanced due to correlated interactions with the environment here we systematically study the properties... | [['the', 'properties', 'of', 'coupled', 'emitters', 'can', 'differ', 'dramatically', 'from', 'those', 'of', 'their', 'individual', 'constituents', 'canonical', 'examples', 'include', 'sub', 'and', 'superradiance', 'wherein', 'the', 'decay', 'rate', 'of', 'a', 'collective', 'excitation', 'is', 'reduced', 'or', 'enhanced... | [-0.15229334930578867, 0.2707534293793807, -0.07081287720280843, 0.05866963919609026, -0.013558010876988106, -0.20754511868913791, 0.03156907483796766, 0.39836945964045645, -0.2605185918267428, -0.2628848842855188, -0.004591389591777919, -0.33327025059718707, -0.07765622413734534, 0.18391774113600454, 0.088076340397709... |
1,803.02116 | Quasi-invariance of completely random measure | Let $X$ be a locally compact Polish space. Let $\mathbb K(X)$ denote the
space of discrete Radon measures on $X$. Let $\mu$ be a completely random
discrete measure on $X$, i.e., $\mu$ is (the distribution of) a completely
random measure on $X$ that is concentrated on $\mathbb K(X)$. We consider the
multiplicative (cu... | math.PR | let x be a locally compact polish space let mathbb kx denote the space of discrete radon measures on x let mu be a completely random discrete measure on x ie mu is the distribution of a completely random measure on x that is concentrated on mathbb kx we consider the multiplicative current group c_0xtomathbb r_ consisti... | [['let', 'x', 'be', 'a', 'locally', 'compact', 'polish', 'space', 'let', 'mathbb', 'kx', 'denote', 'the', 'space', 'of', 'discrete', 'radon', 'measures', 'on', 'x', 'let', 'mu', 'be', 'a', 'completely', 'random', 'discrete', 'measure', 'on', 'x', 'ie', 'mu', 'is', 'the', 'distribution', 'of', 'a', 'completely', 'random... | [-0.17092616610771574, 0.1173175062488662, -0.06398955836823773, -0.007045762710606492, -0.03316172418492171, -0.11935000784840401, 0.020986503674734144, 0.37448893699350705, -0.3223696474173884, -0.06530667402260347, 0.10862005092449264, -0.32759052310288467, -0.06408478435846644, 0.17458360763950223, -0.1494932330043... |
1,803.02117 | Equality case in van der Corput's inequality and collisions in multiple
lattice tilings | Van der Corput's provides the sharp bound vol(C) \le m 2^d on the volume of a
d-dimensional origin-symmetric convex body C that has 2m-1 points of the
integer lattice in its interior. For m=1, a characterization of the equality
case vol(C)= m 2^d is equivalent to the well-known problem of characterizing
tilings by tr... | math.CO math.MG | van der corputs provides the sharp bound volc le m 2d on the volume of a ddimensional originsymmetric convex body c that has 2m1 points of the integer lattice in its interior for m1 a characterization of the equality case volc m 2d is equivalent to the wellknown problem of characterizing tilings by translations of a co... | [['van', 'der', 'corputs', 'provides', 'the', 'sharp', 'bound', 'volc', 'le', 'm', '2d', 'on', 'the', 'volume', 'of', 'a', 'ddimensional', 'originsymmetric', 'convex', 'body', 'c', 'that', 'has', '2m1', 'points', 'of', 'the', 'integer', 'lattice', 'in', 'its', 'interior', 'for', 'm1', 'a', 'characterization', 'of', 'th... | [-0.15276057579190613, 0.07904326786300656, -0.038468759554490764, 0.04972812126006957, -0.05092941050607921, -0.15263605363417784, 0.03414780940224325, 0.3102249335136894, -0.20484910979473464, -0.28536448391928326, 0.11283297183625006, -0.30917674211562207, -0.15262962678696593, 0.21835834825326178, -0.07107034275098... |
1,803.02118 | Neural Network Operations and Susuki-Trotter evolution of Neural Network
States | It was recently proposed to leverage the representational power of artificial
neural networks, in particular Restricted Boltzmann Machines, in order to model
complex quantum states of many-body systems [Science, 355(6325), 2017]. States
represented in this way, called Neural Network States (NNSs), were shown to
displ... | quant-ph | it was recently proposed to leverage the representational power of artificial neural networks in particular restricted boltzmann machines in order to model complex quantum states of manybody systems science 3556325 2017 states represented in this way called neural network states nnss were shown to display interesting p... | [['it', 'was', 'recently', 'proposed', 'to', 'leverage', 'the', 'representational', 'power', 'of', 'artificial', 'neural', 'networks', 'in', 'particular', 'restricted', 'boltzmann', 'machines', 'in', 'order', 'to', 'model', 'complex', 'quantum', 'states', 'of', 'manybody', 'systems', 'science', '3556325', '2017', 'stat... | [-0.08804357355413629, 0.13538965727261212, -0.09797828192674544, 0.07867909583152854, -0.07762258828757186, -0.1833266765603223, 0.0578711742474352, 0.3891029821596908, -0.32058406354676006, -0.3036247282157333, 0.05465940802601617, -0.23350959911517957, -0.20034971685426856, 0.18135816588452375, -0.06643653326046073,... |
1,803.02119 | Chaotic motion of neutral and charged particles in the magnetized
Ernst-Schwarzschild spacetime | Neutral test particles around a Schwarzschild black hole immersed in an
external uniform magnetic field have no interactions of electromagnetic forces,
but their motions can be chaotic. This chaotic behavior is induced owing to the
gravitational effect of the magnetic field leading to the nonintegrability of
the magn... | gr-qc | neutral test particles around a schwarzschild black hole immersed in an external uniform magnetic field have no interactions of electromagnetic forces but their motions can be chaotic this chaotic behavior is induced owing to the gravitational effect of the magnetic field leading to the nonintegrability of the magnetiz... | [['neutral', 'test', 'particles', 'around', 'a', 'schwarzschild', 'black', 'hole', 'immersed', 'in', 'an', 'external', 'uniform', 'magnetic', 'field', 'have', 'no', 'interactions', 'of', 'electromagnetic', 'forces', 'but', 'their', 'motions', 'can', 'be', 'chaotic', 'this', 'chaotic', 'behavior', 'is', 'induced', 'owin... | [-0.22091857331831288, 0.22867246330559216, -0.08318348362314831, 0.08757813173491191, -0.07689607287054213, -0.05138693626021158, -0.04013165981368214, 0.32448034802065145, -0.23344844297664064, -0.32860338589712484, 0.03931937675334443, -0.2476483901439867, -0.10365722806386228, 0.1835880580156128, -0.009392587801898... |
1,803.0212 | Magnon-assisted tunnelling in van der Waals heterostructures based on
CrBr3 | The growing family of two-dimensional (2D) materials that are now available
can be used to assemble van der Waals heterostructures with a wide range of
properties. Of particular interest are tunnelling heterostructures, which have
been used to study the electronic states both in the tunnelling barrier and in
the emit... | cond-mat.mes-hall | the growing family of twodimensional 2d materials that are now available can be used to assemble van der waals heterostructures with a wide range of properties of particular interest are tunnelling heterostructures which have been used to study the electronic states both in the tunnelling barrier and in the emitter and... | [['the', 'growing', 'family', 'of', 'twodimensional', '2d', 'materials', 'that', 'are', 'now', 'available', 'can', 'be', 'used', 'to', 'assemble', 'van', 'der', 'waals', 'heterostructures', 'with', 'a', 'wide', 'range', 'of', 'properties', 'of', 'particular', 'interest', 'are', 'tunnelling', 'heterostructures', 'which'... | [-0.13293679306682732, 0.21025307340148305, -0.01466106075427628, 0.04514317416719028, -0.01993852233281359, -0.19138900611017431, 0.05763326225403164, 0.41669314948189173, -0.2571796635697995, -0.31532087132467757, -0.04066817089499507, -0.3530278648316328, -0.07512836671500867, 0.21987378190471127, 0.0738347623164632... |
1,803.02121 | Super-intense Single Attosecond Pulse Generation by Plasma Gating | A robust plasma gating to generate a single ultra-intense attosecond pulse is
developed. It is a manifestation of the hole-boring effect that limits the
strongest attosecond pulse emission within one laser cycle. The generated pulse
is characterized by a stabilized harmonic phase $\psi \approx \pm\pi/2$ and a
slowly ... | physics.plasm-ph | a robust plasma gating to generate a single ultraintense attosecond pulse is developed it is a manifestation of the holeboring effect that limits the strongest attosecond pulse emission within one laser cycle the generated pulse is characterized by a stabilized harmonic phase psi approx pmpi2 and a slowly decaying expo... | [['a', 'robust', 'plasma', 'gating', 'to', 'generate', 'a', 'single', 'ultraintense', 'attosecond', 'pulse', 'is', 'developed', 'it', 'is', 'a', 'manifestation', 'of', 'the', 'holeboring', 'effect', 'that', 'limits', 'the', 'strongest', 'attosecond', 'pulse', 'emission', 'within', 'one', 'laser', 'cycle', 'the', 'gener... | [-0.14293507994840515, 0.29955132689792663, -0.08528802911413633, 0.08118751049121121, -0.004183544724417681, -0.13521058079045775, 0.021710839447967537, 0.41892914699432865, -0.2696941142732447, -0.2405085744420913, 0.05797491535486188, -0.2557365000221497, -0.0983600490144454, 0.24820843523114242, 0.00536760063054812... |
1,803.02122 | Smartphone-based Home Robotics | Humanoid robotics is a promising field because the strong human preference to
interact with anthropomorphic interfaces. Despite this, humanoid robots are far
from reaching main stream adoption and the features available in such robots
seem to lag that of the latest smartphones. A fragmented robot ecosystem and
low in... | cs.RO cs.CY cs.HC | humanoid robotics is a promising field because the strong human preference to interact with anthropomorphic interfaces despite this humanoid robots are far from reaching main stream adoption and the features available in such robots seem to lag that of the latest smartphones a fragmented robot ecosystem and low incenti... | [['humanoid', 'robotics', 'is', 'a', 'promising', 'field', 'because', 'the', 'strong', 'human', 'preference', 'to', 'interact', 'with', 'anthropomorphic', 'interfaces', 'despite', 'this', 'humanoid', 'robots', 'are', 'far', 'from', 'reaching', 'main', 'stream', 'adoption', 'and', 'the', 'features', 'available', 'in', '... | [-0.1310416632395263, 0.04873897536296626, -0.08912376664677116, 0.019280215458616575, -0.20342068971122051, -0.2267459499377276, 0.03269250308429556, 0.46656876726418123, -0.20366687497257122, -0.3527000799274617, 0.09508325846954471, -0.2904476363458956, -0.1778760875233126, 0.1950974462096117, -0.18613258604836164, ... |
1,803.02123 | Towards Mission-Critical Control at the Edge and Over 5G | With the emergence of industrial IoT and cloud computing, and the advent of
5G and edge clouds, there are ambitious expectations on elasticity, economies
of scale, and fast time to market for demanding use cases in the next
generation of ICT networks. Responsiveness and reliability of wireless
communication links and... | cs.SY cs.DC | with the emergence of industrial iot and cloud computing and the advent of 5g and edge clouds there are ambitious expectations on elasticity economies of scale and fast time to market for demanding use cases in the next generation of ict networks responsiveness and reliability of wireless communication links and servic... | [['with', 'the', 'emergence', 'of', 'industrial', 'iot', 'and', 'cloud', 'computing', 'and', 'the', 'advent', 'of', '5g', 'and', 'edge', 'clouds', 'there', 'are', 'ambitious', 'expectations', 'on', 'elasticity', 'economies', 'of', 'scale', 'and', 'fast', 'time', 'to', 'market', 'for', 'demanding', 'use', 'cases', 'in',... | [-0.19244426970073147, 0.02637802838917533, -0.023042724626268156, -0.009277447751999178, -0.06500689223240544, -0.13288834224631837, 0.08528638458853864, 0.39709644907809516, -0.2513728532282618, -0.3159013642806612, 0.13475856143708775, -0.2494817678730383, -0.16163180789724854, 0.22160554975939536, -0.08284836773182... |
1,803.02124 | MIRIAM: A Multimodal Chat-Based Interface for Autonomous Systems | We present MIRIAM (Multimodal Intelligent inteRactIon for Autonomous
systeMs), a multimodal interface to support situation awareness of autonomous
vehicles through chat-based interaction. The user is able to chat about the
vehicle's plan, objectives, previous activities and mission progress. The
system is mixed initi... | cs.AI cs.HC | we present miriam multimodal intelligent interaction for autonomous systems a multimodal interface to support situation awareness of autonomous vehicles through chatbased interaction the user is able to chat about the vehicles plan objectives previous activities and mission progress the system is mixed initiative in th... | [['we', 'present', 'miriam', 'multimodal', 'intelligent', 'interaction', 'for', 'autonomous', 'systems', 'a', 'multimodal', 'interface', 'to', 'support', 'situation', 'awareness', 'of', 'autonomous', 'vehicles', 'through', 'chatbased', 'interaction', 'the', 'user', 'is', 'able', 'to', 'chat', 'about', 'the', 'vehicles'... | [-0.20716888120100982, 0.059526343168555824, -0.0657955586127397, 0.052177176814175386, -0.15813798874454654, -0.20812323213676395, 0.06334710699182165, 0.42016989089872525, -0.2198914526489334, -0.33814147336111555, 0.09379142736577416, -0.32238661822444503, -0.19763752446928318, 0.17132790706565845, -0.18077238360959... |
1,803.02125 | Statistical properties for flows with unbounded roof function, including
the Lorenz attractor | For geometric Lorenz attractors (including the classical Lorenz attractor) we
obtain a greatly simplified proof of the central limit theorem which applies
also to the more general class of codimension two singular hyperbolic
attractors. We also obtain the functional central limit theorem and moment
estimates, as well... | math.DS | for geometric lorenz attractors including the classical lorenz attractor we obtain a greatly simplified proof of the central limit theorem which applies also to the more general class of codimension two singular hyperbolic attractors we also obtain the functional central limit theorem and moment estimates as well as it... | [['for', 'geometric', 'lorenz', 'attractors', 'including', 'the', 'classical', 'lorenz', 'attractor', 'we', 'obtain', 'a', 'greatly', 'simplified', 'proof', 'of', 'the', 'central', 'limit', 'theorem', 'which', 'applies', 'also', 'to', 'the', 'more', 'general', 'class', 'of', 'codimension', 'two', 'singular', 'hyperboli... | [-0.14432255603008878, 0.06605829796694124, -0.11927474402368833, 0.148249151940362, -0.04794552244054966, -0.15533383576145682, 0.006661789758184638, 0.18315896924991065, -0.28806658504674065, -0.19972564537937826, 0.15900077022916564, -0.24703367709970245, -0.2026841115588561, 0.26515367448043364, -0.1291438741430353... |
1,803.02126 | Frozen Superparaelectric State of Local Polar Regions in GdMn2O5 and
Gd0.8Ce0.2Mn2O5 | A comparative study of the dielectric properties and electric polarization of
multiferroics GdMn2O5 and Gd0.8Ce0.2Mn2O5 has been carried out in the
temperature range from 5 up to 300 K. The polarization properties in the
ferroelectric state that forms due to a charge ordering and exchange striction
have been studied ... | cond-mat.mtrl-sci | a comparative study of the dielectric properties and electric polarization of multiferroics gdmn2o5 and gd08ce02mn2o5 has been carried out in the temperature range from 5 up to 300 k the polarization properties in the ferroelectric state that forms due to a charge ordering and exchange striction have been studied at t ... | [['a', 'comparative', 'study', 'of', 'the', 'dielectric', 'properties', 'and', 'electric', 'polarization', 'of', 'multiferroics', 'gdmn2o5', 'and', 'gd08ce02mn2o5', 'has', 'been', 'carried', 'out', 'in', 'the', 'temperature', 'range', 'from', '5', 'up', 'to', '300', 'k', 'the', 'polarization', 'properties', 'in', 'the'... | [-0.15986093404018772, 0.2058215576545459, -0.01666663107833108, -0.010702868976601424, -0.025861290658502716, -0.09266661578558583, 0.07901822330545535, 0.4221806280908331, -0.25976949496672747, -0.2895805870669078, 0.05606987698630026, -0.31955308181983705, -0.015144168597077373, 0.16130114549490732, 0.09364062588274... |
1,803.02127 | Robust Continuous System Integration for Critical Deep-Sea Robot
Operations Using Knowledge-Enabled Simulation in the Loop | Deep-sea robot operations demand a high level of safety, efficiency and
reliability. As a consequence, measures within the development stage have to be
implemented to extensively evaluate and benchmark system components ranging
from data acquisition, perception and localization to control. We present an
approach base... | cs.RO | deepsea robot operations demand a high level of safety efficiency and reliability as a consequence measures within the development stage have to be implemented to extensively evaluate and benchmark system components ranging from data acquisition perception and localization to control we present an approach based on hig... | [['deepsea', 'robot', 'operations', 'demand', 'a', 'high', 'level', 'of', 'safety', 'efficiency', 'and', 'reliability', 'as', 'a', 'consequence', 'measures', 'within', 'the', 'development', 'stage', 'have', 'to', 'be', 'implemented', 'to', 'extensively', 'evaluate', 'and', 'benchmark', 'system', 'components', 'ranging'... | [-0.09592428544606083, 0.0176096494916128, -0.09044435334578156, 0.00644297026284039, -0.019465570382773877, -0.12815012031048537, 0.04573083384893835, 0.404249712664634, -0.22090122950077057, -0.38939634566009046, 0.14047233147360386, -0.22475447585631628, -0.1810910347700119, 0.2576138608157635, -0.1172966991160065, ... |
1,803.02128 | Impact of beads and drops on a repellent solid surface: a unified
description | We investigate freely expanding sheets formed by ultrasoft gel beads, and
liquid and viscoelastic drops, produced by the impact of the bead or drop on a
silicon wafer covered with a thin layer of liquid nitrogen that suppresses
viscous dissipation thanks to an inverse Leidenfrost effect. Our experiments
show a unifie... | cond-mat.soft physics.flu-dyn | we investigate freely expanding sheets formed by ultrasoft gel beads and liquid and viscoelastic drops produced by the impact of the bead or drop on a silicon wafer covered with a thin layer of liquid nitrogen that suppresses viscous dissipation thanks to an inverse leidenfrost effect our experiments show a unified beh... | [['we', 'investigate', 'freely', 'expanding', 'sheets', 'formed', 'by', 'ultrasoft', 'gel', 'beads', 'and', 'liquid', 'and', 'viscoelastic', 'drops', 'produced', 'by', 'the', 'impact', 'of', 'the', 'bead', 'or', 'drop', 'on', 'a', 'silicon', 'wafer', 'covered', 'with', 'a', 'thin', 'layer', 'of', 'liquid', 'nitrogen', ... | [-0.10266863746941089, 0.22511613589257468, -0.12915690387412906, 0.003515372141264379, -0.03057304844260216, -0.11822819928079843, 0.01927219983190298, 0.3096076876819134, -0.2759522446766496, -0.2558539432734251, 0.036861919078975916, -0.2734028659462929, -0.1600791699849069, 0.16889720358327032, -0.00382017689943313... |
1,803.02129 | A Non-Technical Survey on Deep Convolutional Neural Network
Architectures | Artificial neural networks have recently shown great results in many
disciplines and a variety of applications, including natural language
understanding, speech processing, games and image data generation. One
particular application in which the strong performance of artificial neural
networks was demonstrated is the... | cs.CV | artificial neural networks have recently shown great results in many disciplines and a variety of applications including natural language understanding speech processing games and image data generation one particular application in which the strong performance of artificial neural networks was demonstrated is the recog... | [['artificial', 'neural', 'networks', 'have', 'recently', 'shown', 'great', 'results', 'in', 'many', 'disciplines', 'and', 'a', 'variety', 'of', 'applications', 'including', 'natural', 'language', 'understanding', 'speech', 'processing', 'games', 'and', 'image', 'data', 'generation', 'one', 'particular', 'application',... | [-0.08033128697360452, -0.026478287649337694, -0.04955674473506709, 0.07887403017246268, -0.10856577513687726, -0.16742805189763507, -0.05372966298730009, 0.4826850945957833, -0.2543179276981391, -0.32205271867472524, 0.08753052570391447, -0.22905437658126984, -0.2894631768809631, 0.19904158932363822, -0.15276809775580... |
1,803.0213 | STADS: Software Testing as Species Discovery | A fundamental challenge of software testing is the statistically
well-grounded extrapolation from program behaviors observed during testing. For
instance, a security researcher who has run the fuzzer for a week has currently
no means (i) to estimate the total number of feasible program branches, given
that only a fra... | cs.SE | a fundamental challenge of software testing is the statistically wellgrounded extrapolation from program behaviors observed during testing for instance a security researcher who has run the fuzzer for a week has currently no means i to estimate the total number of feasible program branches given that only a fraction ha... | [['a', 'fundamental', 'challenge', 'of', 'software', 'testing', 'is', 'the', 'statistically', 'wellgrounded', 'extrapolation', 'from', 'program', 'behaviors', 'observed', 'during', 'testing', 'for', 'instance', 'a', 'security', 'researcher', 'who', 'has', 'run', 'the', 'fuzzer', 'for', 'a', 'week', 'has', 'currently', ... | [-0.0607332416404728, 0.0408902954044489, -0.09172525205298938, 0.09548255883108851, -0.08311725854473088, -0.15291198963920274, 0.1121393586122965, 0.3464395080068846, -0.220945620717394, -0.36490076903494134, 0.1147347805762036, -0.2701188098776111, -0.116455735710089, 0.18035716694399154, -0.08887453365563598, 0.052... |
1,803.02131 | Electron spin inversion in gated silicene nanoribbons | We study locally gated silicene nanoribbons as spin active devices. We find
that the gated segments of nanoribbons with zigzag edge can be used to perform
a spin inversion for the electron spins injected with an in-plane orientation.
The strong intrinsic spin-orbit coupling for low Fermi energy in presence of an
exte... | cond-mat.mes-hall | we study locally gated silicene nanoribbons as spin active devices we find that the gated segments of nanoribbons with zigzag edge can be used to perform a spin inversion for the electron spins injected with an inplane orientation the strong intrinsic spinorbit coupling for low fermi energy in presence of an external v... | [['we', 'study', 'locally', 'gated', 'silicene', 'nanoribbons', 'as', 'spin', 'active', 'devices', 'we', 'find', 'that', 'the', 'gated', 'segments', 'of', 'nanoribbons', 'with', 'zigzag', 'edge', 'can', 'be', 'used', 'to', 'perform', 'a', 'spin', 'inversion', 'for', 'the', 'electron', 'spins', 'injected', 'with', 'an',... | [-0.23984108343634994, 0.20096761363888493, 0.03414024347268523, 0.015068127578252568, -0.05856100297607738, -0.1727475536658232, 0.005027265249486637, 0.4991512494418052, -0.3016574367658671, -0.2864550889273166, 0.02062892627372586, -0.2629637052945861, -0.07431517006966089, 0.18538724300408854, 0.07279154532076364, ... |
1,803.02132 | A complete FFT-based decomposition formalism for the redshift-space
bispectrum | To fully extract cosmological information from nonlinear galaxy distribution
in redshift space, it is essential to include higher-order statistics beyond
the two-point correlation function. In this paper, we propose a new
decomposition formalism for computing the anisotropic bispectrum in redshift
space and for measu... | astro-ph.CO astro-ph.GA | to fully extract cosmological information from nonlinear galaxy distribution in redshift space it is essential to include higherorder statistics beyond the twopoint correlation function in this paper we propose a new decomposition formalism for computing the anisotropic bispectrum in redshift space and for measuring it... | [['to', 'fully', 'extract', 'cosmological', 'information', 'from', 'nonlinear', 'galaxy', 'distribution', 'in', 'redshift', 'space', 'it', 'is', 'essential', 'to', 'include', 'higherorder', 'statistics', 'beyond', 'the', 'twopoint', 'correlation', 'function', 'in', 'this', 'paper', 'we', 'propose', 'a', 'new', 'decompo... | [-0.08584147667995869, 0.07959278574876058, -0.13443227436689015, 0.10329122987828808, -0.14546172312111594, -0.04695889991349899, -0.035869746955331024, 0.3414994139994423, -0.26917042324203067, -0.28577986461683536, 0.03476900707307952, -0.29920941257688144, -0.09729493424730698, 0.1798533016509072, 0.043761518674448... |
1,803.02133 | Trees within trees: Simple nested coalescents | We consider the compact space of pairs of nested partitions of $\mathbb N$,
where by analogy with models used in molecular evolution, we call "gene
partition" the finer partition and "species partition" the coarser one. We
introduce the class of nondecreasing processes valued in nested partitions,
assumed Markovian a... | math.PR | we consider the compact space of pairs of nested partitions of mathbb n where by analogy with models used in molecular evolution we call gene partition the finer partition and species partition the coarser one we introduce the class of nondecreasing processes valued in nested partitions assumed markovian and with excha... | [['we', 'consider', 'the', 'compact', 'space', 'of', 'pairs', 'of', 'nested', 'partitions', 'of', 'mathbb', 'n', 'where', 'by', 'analogy', 'with', 'models', 'used', 'in', 'molecular', 'evolution', 'we', 'call', 'gene', 'partition', 'the', 'finer', 'partition', 'and', 'species', 'partition', 'the', 'coarser', 'one', 'we... | [-0.11270732919710051, 0.20235569456141858, -0.021929525547219733, 0.09519814268696791, -0.02270313699999334, -0.10131168918390022, 0.07795605738402198, 0.35435452820046953, -0.27692852006293833, -0.20628363382267326, 0.06091469472310947, -0.27762664824626165, -0.09359532433843828, 0.12159430140041207, -0.0139046368078... |
1,803.02134 | Relative-locality phenomenology on Snyder spacetime | We study the effects of relative locality dynamics in the case of the Snyder
model. Several properties of this model differ from those of the widely studied
$\kappa$-Poincar\'e models: for example, in the Snyder case the action of the
Lorentz group is preserved, and the composition law of momenta is deformed by
terms... | gr-qc hep-th | we study the effects of relative locality dynamics in the case of the snyder model several properties of this model differ from those of the widely studied kappapoincare models for example in the snyder case the action of the lorentz group is preserved and the composition law of momenta is deformed by terms quadratic i... | [['we', 'study', 'the', 'effects', 'of', 'relative', 'locality', 'dynamics', 'in', 'the', 'case', 'of', 'the', 'snyder', 'model', 'several', 'properties', 'of', 'this', 'model', 'differ', 'from', 'those', 'of', 'the', 'widely', 'studied', 'kappapoincare', 'models', 'for', 'example', 'in', 'the', 'snyder', 'case', 'the'... | [-0.10236049584674244, 0.1540461765596261, -0.08287763436181614, 0.11354825062563834, -0.06262185607248774, -0.07538361947398442, -0.0340773226493277, 0.33967852179044616, -0.2530623742271788, -0.2968797205607049, 0.09109598597831045, -0.2680507990462968, -0.14983252653081974, 0.20650988387299152, -0.055873345058315836... |
1,803.02135 | Hidden Conformal Symmetry for Vector Field on Various Black Hole
Backgrounds | Hidden conformal symmetries of scalar field on various black hole backgrounds
have been investigated for years, but whether those features holds for other
fields are still open questions. Recently, with proper assumptions, Lunin
achieves to the separation of variables for Maxwell equations on Kerr
background. In this... | gr-qc hep-th | hidden conformal symmetries of scalar field on various black hole backgrounds have been investigated for years but whether those features holds for other fields are still open questions recently with proper assumptions lunin achieves to the separation of variables for maxwell equations on kerr background in this paper ... | [['hidden', 'conformal', 'symmetries', 'of', 'scalar', 'field', 'on', 'various', 'black', 'hole', 'backgrounds', 'have', 'been', 'investigated', 'for', 'years', 'but', 'whether', 'those', 'features', 'holds', 'for', 'other', 'fields', 'are', 'still', 'open', 'questions', 'recently', 'with', 'proper', 'assumptions', 'lu... | [-0.13190697175450622, 0.13697482625414667, -0.04804797004908323, 0.08779096598859484, -0.13696425754674954, -0.1618718775871553, -0.007304703281261027, 0.38007436873097167, -0.1670309550668064, -0.2755082906959088, 0.14023937730878394, -0.2913257411436031, -0.11977209664489094, 0.18420344962689436, -0.0470630228476549... |
1,803.02136 | Limit distribution of the quartet balance index for Aldous's b>=0-model | This paper builds up on T. Martinez-Coronado, A. Mir, F. Rossello and G.
Valiente's work "A balance index for phylogenetic trees based on quartets",
introducing a new balance index for trees. We show here that this balance
index, in the case of Aldous's b>=0-model, convergences weakly to a
distribution that can be ch... | q-bio.PE math.PR | this paper builds up on t martinezcoronado a mir f rossello and g valientes work a balance index for phylogenetic trees based on quartets introducing a new balance index for trees we show here that this balance index in the case of aldouss b0model convergences weakly to a distribution that can be characterized as the f... | [['this', 'paper', 'builds', 'up', 'on', 't', 'martinezcoronado', 'a', 'mir', 'f', 'rossello', 'and', 'g', 'valientes', 'work', 'a', 'balance', 'index', 'for', 'phylogenetic', 'trees', 'based', 'on', 'quartets', 'introducing', 'a', 'new', 'balance', 'index', 'for', 'trees', 'we', 'show', 'here', 'that', 'this', 'balanc... | [-0.115733977677601, 0.17046457742746438, -0.1411597022726651, 0.050769903347827494, -0.06777832520780183, -0.09733443843921827, 0.14296190075918042, 0.3770306812178704, -0.27317318537332597, -0.28228556563056284, 0.0664797455106201, -0.2551350109279156, -0.16190716969750582, 0.15833566325806803, -0.08428550360634202, ... |
1,803.02137 | 9C spectral-index distributions and source-count estimates from 15 to 93
GHz - a re-assessment | In an earlier paper (2007), we used follow-up observations of a sample of
sources from the 9C survey at 15.2 GHz to derive a set of spectral-index
distributions up to a frequency of 90 GHz. These were based on simultaneous
measurements made at 15.2 GHz with the Ryle telescope and at 22 and 43 GHz with
the Karl G. Jan... | astro-ph.GA | in an earlier paper 2007 we used followup observations of a sample of sources from the 9c survey at 152 ghz to derive a set of spectralindex distributions up to a frequency of 90 ghz these were based on simultaneous measurements made at 152 ghz with the ryle telescope and at 22 and 43 ghz with the karl g jansky very la... | [['in', 'an', 'earlier', 'paper', '2007', 'we', 'used', 'followup', 'observations', 'of', 'a', 'sample', 'of', 'sources', 'from', 'the', '9c', 'survey', 'at', '152', 'ghz', 'to', 'derive', 'a', 'set', 'of', 'spectralindex', 'distributions', 'up', 'to', 'a', 'frequency', 'of', '90', 'ghz', 'these', 'were', 'based', 'on'... | [-0.06005727267779548, 0.07604963601130521, -0.019339711671818804, 0.037305861564163934, -0.06519438289615209, -0.08016218233387917, 0.1226965473265409, 0.4214611434508697, -0.12744515181748284, -0.42349487430328736, 0.15957570555428902, -0.30696529323540744, -0.03896357184930821, 0.21132685513407523, -0.02132363792043... |
1,803.02138 | Transition from homogeneous to inhomogeneous limit cycles: Effect of
local filtering in coupled oscillators | We report an interesting symmetry-breaking transition in coupled identical
oscillators, namely the continuous transition from homogeneous to inhomogeneous
limit cycle oscillations. The observed transition is the oscillatory analog of
the Turing-type symmetry-breaking transition from amplitude death (i.e., stable
homo... | nlin.CD nlin.AO physics.app-ph | we report an interesting symmetrybreaking transition in coupled identical oscillators namely the continuous transition from homogeneous to inhomogeneous limit cycle oscillations the observed transition is the oscillatory analog of the turingtype symmetrybreaking transition from amplitude death ie stable homogeneous ste... | [['we', 'report', 'an', 'interesting', 'symmetrybreaking', 'transition', 'in', 'coupled', 'identical', 'oscillators', 'namely', 'the', 'continuous', 'transition', 'from', 'homogeneous', 'to', 'inhomogeneous', 'limit', 'cycle', 'oscillations', 'the', 'observed', 'transition', 'is', 'the', 'oscillatory', 'analog', 'of', ... | [-0.21592517778850517, 0.21337593365203178, -0.02280952879227698, 0.020116640264705683, -0.014585645468189166, -0.1594682157648584, 0.09431915401409452, 0.3053168948077095, -0.2643981787197005, -0.21311876031641777, 0.08912238483138096, -0.24963116425161178, -0.23849893750515408, 0.12398309008254169, 0.0099702735807603... |
1,803.02139 | Connecting Randomized Response, Post-Randomization, Differential Privacy
and t-Closeness via Deniability and Permutation | We explore some novel connections between the main privacy models in use and
we recall a few known ones. We show these models to be more related than
commonly understood, around two main principles: deniability and permutation.
In particular, randomized response turns out to be very modern in spite of it
having been ... | cs.CR | we explore some novel connections between the main privacy models in use and we recall a few known ones we show these models to be more related than commonly understood around two main principles deniability and permutation in particular randomized response turns out to be very modern in spite of it having been introdu... | [['we', 'explore', 'some', 'novel', 'connections', 'between', 'the', 'main', 'privacy', 'models', 'in', 'use', 'and', 'we', 'recall', 'a', 'few', 'known', 'ones', 'we', 'show', 'these', 'models', 'to', 'be', 'more', 'related', 'than', 'commonly', 'understood', 'around', 'two', 'main', 'principles', 'deniability', 'and'... | [-0.09002301782442111, 0.04344720362468126, -0.07329277286562555, 0.11351295961150733, -0.08970899419011381, -0.19358440807289973, 0.06667069736087394, 0.390158566618394, -0.2966197216046784, -0.3481459619120477, 0.10999067335858004, -0.27086103054658933, -0.19479346344272555, 0.21473306241482887, -0.14573023324514445,... |
1,803.0214 | Conceptualization of Object Compositions Using Persistent Homology | A topological shape analysis is proposed and utilized to learn concepts that
reflect shape commonalities. Our approach is two-fold: i) a spatial topology
analysis of point cloud segment constellations within objects. Therein
constellations are decomposed and described in an hierarchical manner - from
single segments ... | cs.CV cs.RO | a topological shape analysis is proposed and utilized to learn concepts that reflect shape commonalities our approach is twofold i a spatial topology analysis of point cloud segment constellations within objects therein constellations are decomposed and described in an hierarchical manner from single segments to segmen... | [['a', 'topological', 'shape', 'analysis', 'is', 'proposed', 'and', 'utilized', 'to', 'learn', 'concepts', 'that', 'reflect', 'shape', 'commonalities', 'our', 'approach', 'is', 'twofold', 'i', 'a', 'spatial', 'topology', 'analysis', 'of', 'point', 'cloud', 'segment', 'constellations', 'within', 'objects', 'therein', 'c... | [-0.1223094844741322, 0.039388392539541725, -0.13224856381247377, 0.08572920841540684, -0.08200456806164431, -0.11643445601262022, 0.03598245681394218, 0.45510821988838807, -0.3199115231379932, -0.3336358822130582, 0.03642402207499305, -0.26904210512804094, -0.20011957209933093, 0.15275283531988398, -0.1334092975042662... |
1,803.02141 | A note on joint functional convergence of partial sum and maxima for
linear processes | Recently, for the joint partial sum and partial maxima processes constructed
from linear processes with independent identically distributed innovations that
are regularly varying with tail index $\alpha \in (0, 2)$, a functional limit
theorem with the Skorohod weak $M_{2}$ topology has been obtained. In this
paper we... | math.PR | recently for the joint partial sum and partial maxima processes constructed from linear processes with independent identically distributed innovations that are regularly varying with tail index alpha in 0 2 a functional limit theorem with the skorohod weak m_2 topology has been obtained in this paper we show that if al... | [['recently', 'for', 'the', 'joint', 'partial', 'sum', 'and', 'partial', 'maxima', 'processes', 'constructed', 'from', 'linear', 'processes', 'with', 'independent', 'identically', 'distributed', 'innovations', 'that', 'are', 'regularly', 'varying', 'with', 'tail', 'index', 'alpha', 'in', '0', '2', 'a', 'functional', 'l... | [-0.17038645516096176, 0.14607557432790255, -0.0447335459891407, 0.05814590585958641, -0.021824718891889198, -0.09901760492859216, 0.029765346688325464, 0.38378023458965893, -0.32434034171974524, -0.18705293103709988, 0.10424583427736471, -0.2783663600908014, -0.13989117092067568, 0.1467576715345869, -0.043697213383402... |
1,803.02142 | Nuclear quantum shape-phase transitions in odd-mass systems | Microscopic signatures of nuclear ground-state shape phase transitions in
odd-mass Eu isotopes are explored starting from excitation spectra and
collective wave functions obtained by diagonalization of a core-quasiparticle
coupling Hamiltonian based on energy density functionals. As functions of the
physical control ... | nucl-th nucl-ex | microscopic signatures of nuclear groundstate shape phase transitions in oddmass eu isotopes are explored starting from excitation spectra and collective wave functions obtained by diagonalization of a corequasiparticle coupling hamiltonian based on energy density functionals as functions of the physical control parame... | [['microscopic', 'signatures', 'of', 'nuclear', 'groundstate', 'shape', 'phase', 'transitions', 'in', 'oddmass', 'eu', 'isotopes', 'are', 'explored', 'starting', 'from', 'excitation', 'spectra', 'and', 'collective', 'wave', 'functions', 'obtained', 'by', 'diagonalization', 'of', 'a', 'corequasiparticle', 'coupling', 'h... | [-0.06870507969430534, 0.2598725541925272, -0.01954688256097247, 0.14040419819811695, 0.014837609456597472, -0.12139428418595344, 0.05560045210282794, 0.3431445490166867, -0.20916111211513552, -0.30127554892716435, -0.10093823464406426, -0.37296830349863114, -0.018895730788146544, 0.10163406932579098, 0.109704429464642... |
1,803.02143 | A comparison of semi-Lagrangian discontinuous Galerkin and spline based
Vlasov solvers in four dimensions | The purpose of the present paper is to compare two semi-Lagrangian methods in
the context of the four-dimensional Vlasov--Poisson equation. More
specifically, our goal is to compare the performance of the more recently
developed semi-Lagrangian discontinuous Galerkin scheme with the de facto
standard in Eulerian Vlas... | math.NA cs.NA physics.comp-ph | the purpose of the present paper is to compare two semilagrangian methods in the context of the fourdimensional vlasovpoisson equation more specifically our goal is to compare the performance of the more recently developed semilagrangian discontinuous galerkin scheme with the de facto standard in eulerian vlasov simula... | [['the', 'purpose', 'of', 'the', 'present', 'paper', 'is', 'to', 'compare', 'two', 'semilagrangian', 'methods', 'in', 'the', 'context', 'of', 'the', 'fourdimensional', 'vlasovpoisson', 'equation', 'more', 'specifically', 'our', 'goal', 'is', 'to', 'compare', 'the', 'performance', 'of', 'the', 'more', 'recently', 'devel... | [-0.1052413823338363, 0.022268767706753515, -0.13429265335964208, 0.08124377426826289, -0.061239479609701615, -0.15161978381961075, 0.008390320548972919, 0.3635417374104939, -0.2155190744617192, -0.2600326740331101, 0.0911947857100379, -0.20769976214929062, -0.13525259775236587, 0.239171159226151, -0.039106212026540146... |
1,803.02144 | Dark Matter Direct Detection from new interactions in models with
spin-two mediators | We consider models where a massive spin-two resonance acts as the mediator
between Dark Matter (DM) and the SM particles through the energy-momentum
tensor. We examine the effective theory for fermion, vector and scalar DM
generated in these models and find novel types of DM-SM interaction never
considered before. We... | hep-ph | we consider models where a massive spintwo resonance acts as the mediator between dark matter dm and the sm particles through the energymomentum tensor we examine the effective theory for fermion vector and scalar dm generated in these models and find novel types of dmsm interaction never considered before we identify ... | [['we', 'consider', 'models', 'where', 'a', 'massive', 'spintwo', 'resonance', 'acts', 'as', 'the', 'mediator', 'between', 'dark', 'matter', 'dm', 'and', 'the', 'sm', 'particles', 'through', 'the', 'energymomentum', 'tensor', 'we', 'examine', 'the', 'effective', 'theory', 'for', 'fermion', 'vector', 'and', 'scalar', 'd... | [-0.12980111658742483, 0.23791536835558486, -0.05646120998926103, 0.20325649248770053, -0.11582753577533018, -0.1631683550746829, 0.016316993635928617, 0.3252612664693534, -0.21321441007853306, -0.33707214874977415, -0.045598571505068304, -0.2914257114941273, -0.09852245686143035, 0.10432097265929585, 0.158557209680139... |
1,803.02145 | Genarris: Random Generation of Molecular Crystal Structures and Fast
Screening with a Harris Approximation | We present Genarris, a Python package that performs configuration space
screening for molecular crystals of rigid molecules by random sampling with
physical constraints. For fast energy evaluations Genarris employs a Harris
approximation, whereby the total density of a molecular crystal is constructed
via superpositi... | physics.comp-ph cond-mat.mtrl-sci | we present genarris a python package that performs configuration space screening for molecular crystals of rigid molecules by random sampling with physical constraints for fast energy evaluations genarris employs a harris approximation whereby the total density of a molecular crystal is constructed via superposition of... | [['we', 'present', 'genarris', 'a', 'python', 'package', 'that', 'performs', 'configuration', 'space', 'screening', 'for', 'molecular', 'crystals', 'of', 'rigid', 'molecules', 'by', 'random', 'sampling', 'with', 'physical', 'constraints', 'for', 'fast', 'energy', 'evaluations', 'genarris', 'employs', 'a', 'harris', 'ap... | [-0.11376451132966248, 0.07159911685206073, -0.10154305576164832, 0.06095068395102996, -0.05241875593074137, -0.12313489085759154, 0.06935688944589667, 0.40446540372895784, -0.2325230859455535, -0.3080647867547626, 0.03600718354908, -0.20531798077040705, -0.1368941191561124, 0.18735873188834165, -0.0008106178941269373,... |
1,803.02146 | Regularity and Green's relations for the semigroup of partial
contractions of a finite chain | Let $[n]=\{1,2,\ldots,n\}$ be a finite chain and let $\mathcal{P}_{n}$ be the
semigroup of partial transformations on $[n]$. Let
$\mathcal{CP}_{n}=\{\alpha\in \mathcal{P}_{n}: (for~all ~x,y\in
Dom~\alpha)~|x\alpha-y\alpha|\leq|x-y|\}$, then $\mathcal{CP}_{n}$ is a
subsemigroup of $\mathcal{P}_{n}$. In this paper, we ... | math.GR | let n12ldotsn be a finite chain and let mathcalp_n be the semigroup of partial transformations on n let mathcalcp_nalphain mathcalp_n forall xyin domalphaxalphayalphaleqxy then mathcalcp_n is a subsemigroup of mathcalp_n in this paper we give a necessary and sufficient condition for an element in mathcalp_n to be regul... | [['let', 'n12ldotsn', 'be', 'a', 'finite', 'chain', 'and', 'let', 'mathcalp_n', 'be', 'the', 'semigroup', 'of', 'partial', 'transformations', 'on', 'n', 'let', 'mathcalcp_nalphain', 'mathcalp_n', 'forall', 'xyin', 'domalphaxalphayalphaleqxy', 'then', 'mathcalcp_n', 'is', 'a', 'subsemigroup', 'of', 'mathcalp_n', 'in', '... | [-0.16409470195815498, 0.14249695492643305, -0.0565870096740712, 0.0188163273103003, -0.0792096395660857, -0.14410500289107273, -0.0031445013197039123, 0.3385165434862886, -0.3735541551639991, -0.07346231452122863, 0.12940520530849295, -0.3554639080539346, -0.046392197450456606, 0.15154839416832797, -0.0977786495766070... |
1,803.02147 | Amplitude death criteria for coupled complex Ginzburg-Landau systems | Amplitude death, which occurs in a system when one or more macroscopic
wavefunctions collapse to zero, has been observed in mutually coupled
solid-state lasers, analog circuits, and thermoacoustic oscillators, to name a
few applications. While studies have considered amplitude death on oscillator
systems and in exter... | nlin.PS | amplitude death which occurs in a system when one or more macroscopic wavefunctions collapse to zero has been observed in mutually coupled solidstate lasers analog circuits and thermoacoustic oscillators to name a few applications while studies have considered amplitude death on oscillator systems and in externally for... | [['amplitude', 'death', 'which', 'occurs', 'in', 'a', 'system', 'when', 'one', 'or', 'more', 'macroscopic', 'wavefunctions', 'collapse', 'to', 'zero', 'has', 'been', 'observed', 'in', 'mutually', 'coupled', 'solidstate', 'lasers', 'analog', 'circuits', 'and', 'thermoacoustic', 'oscillators', 'to', 'name', 'a', 'few', '... | [-0.1699683957194793, 0.1227783257790179, -0.038969644397730006, 0.0499767675610201, -0.07703052943543298, -0.19387964014022147, 0.02046239005649113, 0.3413822167480248, -0.17984751793555914, -0.23312241845414974, 0.11102185099225607, -0.25250195203116166, -0.21283757427008823, 0.28380190594907617, -0.01822061023194692... |
1,803.02148 | Noise-induced distributed entanglement in atom-cavity-fiber system | The distributed quantum computation plays an important role in large-scale
quantum information processing. In the atom-cavity-fiber system, we put forward
two efficient proposals to prepare the steady entanglement of two distant atoms
with dissipation. The atomic spontaneous emission and the loss of fiber are
exploit... | quant-ph | the distributed quantum computation plays an important role in largescale quantum information processing in the atomcavityfiber system we put forward two efficient proposals to prepare the steady entanglement of two distant atoms with dissipation the atomic spontaneous emission and the loss of fiber are exploited activ... | [['the', 'distributed', 'quantum', 'computation', 'plays', 'an', 'important', 'role', 'in', 'largescale', 'quantum', 'information', 'processing', 'in', 'the', 'atomcavityfiber', 'system', 'we', 'put', 'forward', 'two', 'efficient', 'proposals', 'to', 'prepare', 'the', 'steady', 'entanglement', 'of', 'two', 'distant', '... | [-0.18878107062354685, 0.18468154662370215, -0.015612809292972088, 0.013295289372093975, -0.008747037630528212, -0.21068398497998714, 0.047778226360678674, 0.4185360150039196, -0.24530548035353422, -0.269456913843751, 0.06554003553278744, -0.24261580127989874, -0.0873518289513886, 0.23247951715346427, 0.002124641631031... |
1,803.02149 | Signatures of Anderson localization and delocalized random quantum
states | We consider the notion of equilibration for an isolated quantum system
exhibiting Anderson localization. The system is assumed to be in a pure state,
i.e., described by a wave-function undergoing unitary dynamics. We focus on the
simplest model of a 1D disordered chain and we analyse both the dynamics of an
initially... | quant-ph cond-mat.stat-mech | we consider the notion of equilibration for an isolated quantum system exhibiting anderson localization the system is assumed to be in a pure state ie described by a wavefunction undergoing unitary dynamics we focus on the simplest model of a 1d disordered chain and we analyse both the dynamics of an initially localize... | [['we', 'consider', 'the', 'notion', 'of', 'equilibration', 'for', 'an', 'isolated', 'quantum', 'system', 'exhibiting', 'anderson', 'localization', 'the', 'system', 'is', 'assumed', 'to', 'be', 'in', 'a', 'pure', 'state', 'ie', 'described', 'by', 'a', 'wavefunction', 'undergoing', 'unitary', 'dynamics', 'we', 'focus', ... | [-0.1600156278270756, 0.2161001539808611, -0.08674461901692909, 0.0469985552899487, 0.07595180595805212, -0.12804048154978606, 0.051138203059860936, 0.3407225341021254, -0.2715123246412013, -0.2277991880111816, 0.09073886670939572, -0.28977051964947875, -0.07261624789967293, 0.1062387951213578, 0.024690811296852803, 0.... |
1,803.0215 | Effect of short-range correlations on spectral properties of doped Mott
insulators | In the framework of cluster perturbation theory for the 2D Hubbard and
Hubbard-Holstein models at low hole doping we have studied the effect of local
and short-range correlations in strongly correlated systems on the anomalous
features in the electronic spectrum by investigating the fine structure of
quasiparticle ba... | cond-mat.str-el | in the framework of cluster perturbation theory for the 2d hubbard and hubbardholstein models at low hole doping we have studied the effect of local and shortrange correlations in strongly correlated systems on the anomalous features in the electronic spectrum by investigating the fine structure of quasiparticle bands ... | [['in', 'the', 'framework', 'of', 'cluster', 'perturbation', 'theory', 'for', 'the', '2d', 'hubbard', 'and', 'hubbardholstein', 'models', 'at', 'low', 'hole', 'doping', 'we', 'have', 'studied', 'the', 'effect', 'of', 'local', 'and', 'shortrange', 'correlations', 'in', 'strongly', 'correlated', 'systems', 'on', 'the', '... | [-0.16681582813433718, 0.2020359629623885, -0.04238480486739636, 0.10627623069625913, -0.0043487266148178935, -0.16795243616372849, 0.07558811970481523, 0.3624722666494297, -0.2481362276155962, -0.29630951976843095, -0.053400534912132855, -0.3502744231242268, -0.1285240600863995, 0.11735159815079794, 0.0644147381071378... |
1,803.02151 | A functional CLT for partial traces of random matrices | In this paper we show a functional central limit theorem for the sum of the
first $\lfloor t n \rfloor$ diagonal elements of $f(Z)$ as a function in $t$,
for $Z$ a random real symmetric or complex Hermitian $n\times n$ matrix. The
result holds for orthogonal or unitarily invariant distributions of $Z$, in the
cases w... | math.PR | in this paper we show a functional central limit theorem for the sum of the first lfloor t n rfloor diagonal elements of fz as a function in t for z a random real symmetric or complex hermitian ntimes n matrix the result holds for orthogonal or unitarily invariant distributions of z in the cases when the linear eigenva... | [['in', 'this', 'paper', 'we', 'show', 'a', 'functional', 'central', 'limit', 'theorem', 'for', 'the', 'sum', 'of', 'the', 'first', 'lfloor', 't', 'n', 'rfloor', 'diagonal', 'elements', 'of', 'fz', 'as', 'a', 'function', 'in', 't', 'for', 'z', 'a', 'random', 'real', 'symmetric', 'or', 'complex', 'hermitian', 'ntimes', ... | [-0.1365575250428246, 0.12632451982864615, -0.07281197981946931, 0.07384932285115109, 0.03897273943436389, -0.15710792021008627, 0.05410750668462632, 0.3175828034433593, -0.28362802945894705, -0.18879054941008894, 0.0737579991596713, -0.321664298865564, -0.16366350144261912, 0.12984776892936883, -0.006365032980636675, ... |
1,803.02152 | Induced and Weak Induced Arboricities | We define the induced arboricity of a graph $G$, denoted by ${\rm ia}(G)$, as
the smallest $k$ such that the edges of $G$ can be covered with $k$ induced
forests in $G$. This notion generalizes the classical notions of the arboricity
and strong chromatic index.
For a class $\mathcal{F}$ of graphs and a graph parame... | math.CO cs.DM | we define the induced arboricity of a graph g denoted by rm iag as the smallest k such that the edges of g can be covered with k induced forests in g this notion generalizes the classical notions of the arboricity and strong chromatic index for a class mathcalf of graphs and a graph parameter p let pmathcalf suppg mid ... | [['we', 'define', 'the', 'induced', 'arboricity', 'of', 'a', 'graph', 'g', 'denoted', 'by', 'rm', 'iag', 'as', 'the', 'smallest', 'k', 'such', 'that', 'the', 'edges', 'of', 'g', 'can', 'be', 'covered', 'with', 'k', 'induced', 'forests', 'in', 'g', 'this', 'notion', 'generalizes', 'the', 'classical', 'notions', 'of', 't... | [-0.18863426376275763, 0.18089261154410338, 0.03660356784675118, -0.006135310298948391, -0.10664430638361308, -0.1242209690056567, 0.0001736597249240816, 0.3719405207172995, -0.29541940317824156, -0.31806271901484906, 0.061513838872220915, -0.31404927011296063, -0.1074489655711127, 0.17090712303203143, -0.0981167714732... |
1,803.02153 | Ladder Limit for Correlators of Wilson Loops | We study the correlator of concentric circular Wilson loops for arbitrary
radii, spatial and internal space separations. For real values of the
parameters specifying the dual string configuration, a typical Gross-Ooguri
phase transition is observed. In addition, we explore some analytic
continuation of a parameter $\... | hep-th | we study the correlator of concentric circular wilson loops for arbitrary radii spatial and internal space separations for real values of the parameters specifying the dual string configuration a typical grossooguri phase transition is observed in addition we explore some analytic continuation of a parameter gamma that... | [['we', 'study', 'the', 'correlator', 'of', 'concentric', 'circular', 'wilson', 'loops', 'for', 'arbitrary', 'radii', 'spatial', 'and', 'internal', 'space', 'separations', 'for', 'real', 'values', 'of', 'the', 'parameters', 'specifying', 'the', 'dual', 'string', 'configuration', 'a', 'typical', 'grossooguri', 'phase', ... | [-0.19801119461655617, 0.17893319453578443, -0.07685346627607942, 0.1037840990780387, -0.062064202167093754, -0.10296844420372508, 0.05388325363979675, 0.3624537358246744, -0.1916502957465127, -0.24771843006834388, 0.07059235817636363, -0.2520667834766209, -0.10575868630316108, 0.14962175937835126, 0.051156354274135084... |
1,803.02154 | The homotopy type of spaces of real resultants with bounded multiplicity | For positive integers $d,m,n\geq 1$ with $(m,n)\not= (1,1)$ and $\Bbb K=\Bbb
R$ or $\Bbb C$, let $Q^{d,m}_{n}(\Bbb K)$ denote the space of $m$-tuples
$(f_1(z),\cdots ,f_m(z))\in \Bbb K [z]^m$ of $\Bbb K$-coefficients monic
polynomials of the same degree $d$ such that polynomials $\{f_k(z)\}_{k=1}^m$
have no common {\... | math.AT | for positive integers dmngeq 1 with mnnot 11 and bbb kbbb r or bbb c let qdm_nbbb k denote the space of mtuples f_1zcdots f_mzin bbb k zm of bbb kcoefficients monic polynomials of the same degree d such that polynomials f_kz_k1m have no common it real root of multiplicity geq n but may have complex common root of any m... | [['for', 'positive', 'integers', 'dmngeq', '1', 'with', 'mnnot', '11', 'and', 'bbb', 'kbbb', 'r', 'or', 'bbb', 'c', 'let', 'qdm_nbbb', 'k', 'denote', 'the', 'space', 'of', 'mtuples', 'f_1zcdots', 'f_mzin', 'bbb', 'k', 'zm', 'of', 'bbb', 'kcoefficients', 'monic', 'polynomials', 'of', 'the', 'same', 'degree', 'd', 'such'... | [-0.1894451230607071, 0.12731759568575668, -0.01522106204081226, 0.039287967098717416, -0.029456682134050508, -0.16894653994120187, -0.06455178052786872, 0.302221905037358, -0.29528937809303535, -0.22600432521387512, 0.09540009933947544, -0.2644220176698254, -0.13481663494278584, 0.17773257636230205, -0.086614422252619... |
1,803.02155 | Self-Attention with Relative Position Representations | Relying entirely on an attention mechanism, the Transformer introduced by
Vaswani et al. (2017) achieves state-of-the-art results for machine
translation. In contrast to recurrent and convolutional neural networks, it
does not explicitly model relative or absolute position information in its
structure. Instead, it re... | cs.CL | relying entirely on an attention mechanism the transformer introduced by vaswani et al 2017 achieves stateoftheart results for machine translation in contrast to recurrent and convolutional neural networks it does not explicitly model relative or absolute position information in its structure instead it requires adding... | [['relying', 'entirely', 'on', 'an', 'attention', 'mechanism', 'the', 'transformer', 'introduced', 'by', 'vaswani', 'et', 'al', '2017', 'achieves', 'stateoftheart', 'results', 'for', 'machine', 'translation', 'in', 'contrast', 'to', 'recurrent', 'and', 'convolutional', 'neural', 'networks', 'it', 'does', 'not', 'explic... | [-0.05904298762382992, 0.01590855178094621, -0.07715165928494952, 0.025278049605363544, -0.08805509117029026, -0.11758729068443496, 0.08766790532345177, 0.4815697263635642, -0.27796333755782626, -0.37405160912940055, 0.021906925259646794, -0.2546991789548374, -0.158527515521884, 0.20740528507257236, -0.1671572056077156... |
1,803.02156 | Chebyshev Filter Diagonalization on Modern Manycore Processors and
GPGPUs | Chebyshev filter diagonalization is well established in quantum chemistry and
quantum physics to compute bulks of eigenvalues of large sparse matrices.
Choosing a block vector implementation, we investigate optimization
opportunities on the new class of high-performance compute devices featuring
both high-bandwidth a... | cs.MS cs.PF physics.comp-ph | chebyshev filter diagonalization is well established in quantum chemistry and quantum physics to compute bulks of eigenvalues of large sparse matrices choosing a block vector implementation we investigate optimization opportunities on the new class of highperformance compute devices featuring both highbandwidth and low... | [['chebyshev', 'filter', 'diagonalization', 'is', 'well', 'established', 'in', 'quantum', 'chemistry', 'and', 'quantum', 'physics', 'to', 'compute', 'bulks', 'of', 'eigenvalues', 'of', 'large', 'sparse', 'matrices', 'choosing', 'a', 'block', 'vector', 'implementation', 'we', 'investigate', 'optimization', 'opportunitie... | [-0.19663629449970094, 0.06034682103725131, 0.0014833600078461438, 0.029232347076868958, -0.08212775534663636, -0.22066989578802645, 0.0804314321050277, 0.41763935482801773, -0.24432507757450173, -0.34348255605299094, 0.12447914277057345, -0.261319020928277, -0.12061648823723153, 0.22677299925181243, -0.058927066154542... |
1,803.02157 | Kak's three-stage protocol of secure quantum communication revisited:
Hitherto unknown strengths and weaknesses of the protocol | Kak's three-stage protocol for quantum key distribution is revisited with
special focus on its hitherto unknown strengths and weaknesses. It is shown
that this protocol can be used for secure direct quantum communication.
Further, the implementability of this protocol in the realistic situation is
analyzed by conside... | quant-ph | kaks threestage protocol for quantum key distribution is revisited with special focus on its hitherto unknown strengths and weaknesses it is shown that this protocol can be used for secure direct quantum communication further the implementability of this protocol in the realistic situation is analyzed by considering va... | [['kaks', 'threestage', 'protocol', 'for', 'quantum', 'key', 'distribution', 'is', 'revisited', 'with', 'special', 'focus', 'on', 'its', 'hitherto', 'unknown', 'strengths', 'and', 'weaknesses', 'it', 'is', 'shown', 'that', 'this', 'protocol', 'can', 'be', 'used', 'for', 'secure', 'direct', 'quantum', 'communication', '... | [-0.1653438030572169, 0.11830139069900923, -0.07618175524864988, 0.05916641465382886, 0.006632643634046631, -0.23918557919872305, 0.05595982702242896, 0.4033070203858888, -0.28231840631014654, -0.2771099971596623, 0.10361633430122687, -0.17462726175148124, -0.15533725223129338, 0.23041544008957243, -0.10782303550045123... |
1,803.02158 | Engineering steady Knill-Laflamme-Milburn state of Rydberg atoms by
dissipation | The Knill-Laflamme-Milburn (KLM) states have been proved to be a useful
resource for quantum information processing [Nature 409, 46 (2001)]. For atomic
KLM states, several schemes have been put forward based on the time-dependent
unitary dynamics, but the dissipative generation of these states has not been
reported. ... | quant-ph | the knilllaflammemilburn klm states have been proved to be a useful resource for quantum information processing nature 409 46 2001 for atomic klm states several schemes have been put forward based on the timedependent unitary dynamics but the dissipative generation of these states has not been reported this work discus... | [['the', 'knilllaflammemilburn', 'klm', 'states', 'have', 'been', 'proved', 'to', 'be', 'a', 'useful', 'resource', 'for', 'quantum', 'information', 'processing', 'nature', '409', '46', '2001', 'for', 'atomic', 'klm', 'states', 'several', 'schemes', 'have', 'been', 'put', 'forward', 'based', 'on', 'the', 'timedependent'... | [-0.1260584653667008, 0.17897798512331065, -0.07995693272927643, 0.030937004353160904, 0.014256322186806105, -0.19914921585586853, 0.07713948913026668, 0.354202338594145, -0.2228165353590157, -0.28458211072055356, 0.0511948831065508, -0.2539873619347678, -0.03749501150533823, 0.18856214924848505, 0.020615990822469548, ... |
1,803.02159 | Exogenous Approach to Grid Cost Allocation in Peer-to-Peer Electricity
Markets | The deployment of distributed energy resources, combined with a more
proactive demand side, is inducing a new paradigm in power system operation and
electricity markets. Within a consumer-centric market framework, peer-to-peer
approaches have gained substantial interest. Peer-to-peer markets rely on
multi-bilateral d... | cs.SY math.OC | the deployment of distributed energy resources combined with a more proactive demand side is inducing a new paradigm in power system operation and electricity markets within a consumercentric market framework peertopeer approaches have gained substantial interest peertopeer markets rely on multibilateral direct negotia... | [['the', 'deployment', 'of', 'distributed', 'energy', 'resources', 'combined', 'with', 'a', 'more', 'proactive', 'demand', 'side', 'is', 'inducing', 'a', 'new', 'paradigm', 'in', 'power', 'system', 'operation', 'and', 'electricity', 'markets', 'within', 'a', 'consumercentric', 'market', 'framework', 'peertopeer', 'appr... | [-0.14892851093973986, 0.025443605252427195, -0.06703041099552494, 0.025910521683486544, -0.09920804764829233, -0.15362428989389848, 0.15761249460515447, 0.4151812873525818, -0.2665137258176317, -0.31765544529664386, 0.11371417510411541, -0.29251847832581435, -0.11860784992639875, 0.20684100416135684, -0.15096263403418... |
1,803.0216 | A PTAS for vertex guarding weakly-visible polygons - An extended
abstract | In this extended abstract, we present a PTAS for guarding the vertices of a
weakly-visible polygon $P$ from a subset of its vertices, or in other words, a
PTAS for computing a minimum dominating set of the visibility graph of the
vertices of $P$. We then show how to obtain a PTAS for vertex guarding $P$'s
boundary.
| cs.CG | in this extended abstract we present a ptas for guarding the vertices of a weaklyvisible polygon p from a subset of its vertices or in other words a ptas for computing a minimum dominating set of the visibility graph of the vertices of p we then show how to obtain a ptas for vertex guarding ps boundary | [['in', 'this', 'extended', 'abstract', 'we', 'present', 'a', 'ptas', 'for', 'guarding', 'the', 'vertices', 'of', 'a', 'weaklyvisible', 'polygon', 'p', 'from', 'a', 'subset', 'of', 'its', 'vertices', 'or', 'in', 'other', 'words', 'a', 'ptas', 'for', 'computing', 'a', 'minimum', 'dominating', 'set', 'of', 'the', 'visibi... | [-0.20768393256834575, 0.05181109476169305, -0.07666377264208027, 0.05890002245307967, -0.1264107677021197, -0.15116794641029888, 0.16858212104749068, 0.3525906341674272, -0.3012967320558216, -0.2835362582284558, 0.08656533922684113, -0.3032238247854236, -0.1238138787988906, 0.08998442130749547, -0.07913024623745255, 0... |
1,803.02161 | The December 2015 re-brightening of V404 Cyg: Variable absorption from
the accretion disc outflow | In December 2015 the black hole binary V404 Cyg underwent a secondary
outburst after the main June 2015 event. We monitored this re-brightening with
the INTEGRAL and Swift satellites, and in this paper we report the results of
the time-resolved spectral analysis of these data. The December outburst shared
similar cha... | astro-ph.HE | in december 2015 the black hole binary v404 cyg underwent a secondary outburst after the main june 2015 event we monitored this rebrightening with the integral and swift satellites and in this paper we report the results of the timeresolved spectral analysis of these data the december outburst shared similar characteri... | [['in', 'december', '2015', 'the', 'black', 'hole', 'binary', 'v404', 'cyg', 'underwent', 'a', 'secondary', 'outburst', 'after', 'the', 'main', 'june', '2015', 'event', 'we', 'monitored', 'this', 'rebrightening', 'with', 'the', 'integral', 'and', 'swift', 'satellites', 'and', 'in', 'this', 'paper', 'we', 'report', 'the... | [-0.038693136743814596, 0.1570811117199724, -0.09462003266298265, 0.10577691828058856, -0.08895426088030327, -0.13397563230158444, 0.04522297226358205, 0.4646086819083342, -0.16339124822187379, -0.41467669454034206, 0.11684347493266511, -0.3587254917705959, -0.04114035296095711, 0.21042717952118695, -0.0971091868355870... |
1,803.02162 | Contrarian compulsions produce time dependent flocking of active
particles | Animals having a trend to align their velocities to an average of their
neighbors' may flock as illustrated by the Vicsek model and its variants. If,
in addition, they feel a systematic contrarian trend, the result may be a time
periodic adjustment of the flock or period doubling in time. This is
demonstrated by anal... | cond-mat.stat-mech cond-mat.soft | animals having a trend to align their velocities to an average of their neighbors may flock as illustrated by the vicsek model and its variants if in addition they feel a systematic contrarian trend the result may be a time periodic adjustment of the flock or period doubling in time this is demonstrated by analyzing a ... | [['animals', 'having', 'a', 'trend', 'to', 'align', 'their', 'velocities', 'to', 'an', 'average', 'of', 'their', 'neighbors', 'may', 'flock', 'as', 'illustrated', 'by', 'the', 'vicsek', 'model', 'and', 'its', 'variants', 'if', 'in', 'addition', 'they', 'feel', 'a', 'systematic', 'contrarian', 'trend', 'the', 'result', ... | [-0.16211329615447106, 0.15866898839540358, -0.10255335027472579, 0.06794018258479685, -0.07467298651542917, -0.13456855186348338, 0.06912776553608048, 0.39183415897297774, -0.24881905317976535, -0.3081592852065487, 0.08038515097582244, -0.25966858910396695, -0.15835800555219753, 0.1306731478987838, -0.0185872828185879... |
1,803.02163 | Revisit of cosmic ray antiprotons from dark matter annihilation with
updated constraints on the background model from AMS-02 and collider data | We study the cosmic ray antiprotons with updated constraints on the
propagation, proton injection, and solar modulation parameters based on the
newest AMS-02 data near the Earth and Voyager data in the local interstellar
space, and on the cross section of antiproton production due to proton-proton
collisions based on... | astro-ph.HE hep-ph | we study the cosmic ray antiprotons with updated constraints on the propagation proton injection and solar modulation parameters based on the newest ams02 data near the earth and voyager data in the local interstellar space and on the cross section of antiproton production due to protonproton collisions based on new co... | [['we', 'study', 'the', 'cosmic', 'ray', 'antiprotons', 'with', 'updated', 'constraints', 'on', 'the', 'propagation', 'proton', 'injection', 'and', 'solar', 'modulation', 'parameters', 'based', 'on', 'the', 'newest', 'ams02', 'data', 'near', 'the', 'earth', 'and', 'voyager', 'data', 'in', 'the', 'local', 'interstellar'... | [-0.05870859927779211, 0.2134219804376057, -0.0977721403138511, 0.15236076958336794, -0.06827966308911337, -0.038746426372349985, 0.006606662954143483, 0.3108942641762735, -0.22007030564889635, -0.35607539716330794, -0.05377011618948803, -0.3646801763663082, 0.11564663365791492, 0.20027825504159488, 0.07093274570740224... |
1,803.02164 | An Enriques Classification Theorem for Surfaces in Positive
Characteristic | We prove that a smooth projective surface $S$ over an algebraically closed
field of characteristic $p>3$ is birational to an abelian surface if
$P_1(S)=P_4(S)=1$ and $h^1(S,\mathcal{O}_S)=2$.
| math.AG | we prove that a smooth projective surface s over an algebraically closed field of characteristic p3 is birational to an abelian surface if p_1sp_4s1 and h1smathcalo_s2 | [['we', 'prove', 'that', 'a', 'smooth', 'projective', 'surface', 's', 'over', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'p3', 'is', 'birational', 'to', 'an', 'abelian', 'surface', 'if', 'p_1sp_4s1', 'and', 'h1smathcalo_s2']] | [-0.2650615447588886, 0.11372456297128035, -0.1403991582337767, 0.04451312026261197, -0.08954557085720201, -0.2047961264809904, -0.09574446400317053, 0.3799733333289623, -0.3791263233870268, -0.11140388793622454, 0.007338342470272134, -0.17027180422640717, -0.12286152517966305, 0.3190974114889589, -0.17679059819784015,... |
1,803.02165 | Sparsity of curves and additive and multiplicative expansion of rational
maps over finite fields | For a prime $p$ and a polynomial $F(X,Y)$ over a finite field $\mathbb{F}_p$
of $p$ elements, we give upper bounds on the number of solutions $$ F(x,y)=0,
\quad x\in\mathcal{A}, \ y\in \mathcal{B}, $$ where $\mathcal{A}$ and
$\mathcal{B}$ are very small intervals or subgroups. These bounds can be
considered as positi... | math.NT | for a prime p and a polynomial fxy over a finite field mathbbf_p of p elements we give upper bounds on the number of solutions fxy0 quad xinmathcala yin mathcalb where mathcala and mathcalb are very small intervals or subgroups these bounds can be considered as positive characteristic analogues of the result of bombier... | [['for', 'a', 'prime', 'p', 'and', 'a', 'polynomial', 'fxy', 'over', 'a', 'finite', 'field', 'mathbbf_p', 'of', 'p', 'elements', 'we', 'give', 'upper', 'bounds', 'on', 'the', 'number', 'of', 'solutions', 'fxy0', 'quad', 'xinmathcala', 'yin', 'mathcalb', 'where', 'mathcala', 'and', 'mathcalb', 'are', 'very', 'small', 'i... | [-0.24136317288891102, 0.11472497297234238, -0.0717407022551116, 0.06404310408462253, -0.036692129315472104, -0.12320806847678291, 0.03436521117885907, 0.34212702706249226, -0.3171126284326116, -0.22512846020464267, 0.10717224033497688, -0.29525700905877683, -0.08148370459158387, 0.2719913790416386, -0.1201252851428257... |
1,803.02166 | Observation of the Semileptonic Decay $D^0 \to a_0(980)^- e^+ \nu_e$ and
Evidence for $D^+ \to a_0(980)^0 e^+ \nu_e$ | Using an $e^+e^-$ collision data sample of 2.93 fb$^{-1}$ collected at a
center-of-mass energy of 3.773 GeV by the BESIII detector at BEPCII, we report
the observation of $D^0 \to a_0(980)^- e^+ \nu_e$ and evidence for $D^+ \to
a_0(980)^0 e^+ \nu_e~$ with significances of $6.4\sigma$ and $2.9\sigma$,
respectively. Th... | hep-ex | using an ee collision data sample of 293 fb1 collected at a centerofmass energy of 3773 gev by the besiii detector at bepcii we report the observation of d0 to a_0980 e nu_e and evidence for d to a_09800 e nu_e with significances of 64sigma and 29sigma respectively the absolute branching fractions are determined to be ... | [['using', 'an', 'ee', 'collision', 'data', 'sample', 'of', '293', 'fb1', 'collected', 'at', 'a', 'centerofmass', 'energy', 'of', '3773', 'gev', 'by', 'the', 'besiii', 'detector', 'at', 'bepcii', 'we', 'report', 'the', 'observation', 'of', 'd0', 'to', 'a_0980', 'e', 'nu_e', 'and', 'evidence', 'for', 'd', 'to', 'a_09800... | [-0.1027109943909806, 0.19168888260949413, -0.08408545459119174, 0.06777848688512017, -0.024232822900208142, -0.1092825157741842, 0.138812283862505, 0.30065412529754443, -0.15877232755851614, -0.2982327365776995, -0.07995115143789368, -0.4289751502756889, 0.12374819788549628, 0.17794045283213503, 0.06358847170965848, 0... |
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