id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,802.0546 | Shape invariance and equivalence relations for pseudowronskians of
Laguerre and Jacobi polynomials | In a previous paper we derived equivalence relations for pseudo-Wronskian
determinants of Hermite polynomials. In this paper we obtain the analogous
result for Laguerre and Jacobi polynomials. The equivalence formulas are richer
in this case since rational Darboux transformations can be defined for four
families of s... | math.CA math-ph math.MP nlin.SI | in a previous paper we derived equivalence relations for pseudowronskian determinants of hermite polynomials in this paper we obtain the analogous result for laguerre and jacobi polynomials the equivalence formulas are richer in this case since rational darboux transformations can be defined for four families of seed f... | [['in', 'a', 'previous', 'paper', 'we', 'derived', 'equivalence', 'relations', 'for', 'pseudowronskian', 'determinants', 'of', 'hermite', 'polynomials', 'in', 'this', 'paper', 'we', 'obtain', 'the', 'analogous', 'result', 'for', 'laguerre', 'and', 'jacobi', 'polynomials', 'the', 'equivalence', 'formulas', 'are', 'riche... | [-0.13137471205222287, 0.11563412731214028, -0.05203613955278082, 0.11983862274168391, -0.08939706720411777, -0.12644888752713865, 0.006548231502945002, 0.35821359982115347, -0.27542917255777866, -0.23045628170283244, 0.09163298417947122, -0.250968669932003, -0.20611510178397502, 0.23024564593755972, -0.071859986508180... |
1,802.05461 | Supermixed labyrinth fractals | Labyrinth fractals are dendrites in the unit square. They were introduced and
studied in the last decade first in the self-similar case [Cristea & Steinsky
(2009,2011)], then in the mixed case [Cristea & Steinsky (2017), Cristea &
Leobacher (2017)]. Supermixed fractals constitute a significant generalisation
of mixed... | math.GT math.DS | labyrinth fractals are dendrites in the unit square they were introduced and studied in the last decade first in the selfsimilar case cristea steinsky 20092011 then in the mixed case cristea steinsky 2017 cristea leobacher 2017 supermixed fractals constitute a significant generalisation of mixed labyrinth fractals each... | [['labyrinth', 'fractals', 'are', 'dendrites', 'in', 'the', 'unit', 'square', 'they', 'were', 'introduced', 'and', 'studied', 'in', 'the', 'last', 'decade', 'first', 'in', 'the', 'selfsimilar', 'case', 'cristea', 'steinsky', '20092011', 'then', 'in', 'the', 'mixed', 'case', 'cristea', 'steinsky', '2017', 'cristea', 'le... | [-0.08600298540356259, 0.12992065541590903, -0.08636797317931204, 0.11800709551989583, -0.055092714459417345, -0.10906151875008083, -0.0005056073728962042, 0.3426505043996987, -0.25412374782765695, -0.23166955118100588, 0.13373374128185794, -0.2667064391710657, -0.21467266157467632, 0.18149038593463124, -0.084020445625... |
1,802.05462 | Geometric Properties of Bessel function derivatives | In this paper our aim is to find the radii of starlikeness and convexity of
Bessel function derivatives for three different kind of normalization. The key
tools in the proof of our main results are the Mittag-Leffler expansion for nth
derivative of Bessel function and properties of real zeros of it. In addition,
by u... | math.CV | in this paper our aim is to find the radii of starlikeness and convexity of bessel function derivatives for three different kind of normalization the key tools in the proof of our main results are the mittagleffler expansion for nth derivative of bessel function and properties of real zeros of it in addition by using t... | [['in', 'this', 'paper', 'our', 'aim', 'is', 'to', 'find', 'the', 'radii', 'of', 'starlikeness', 'and', 'convexity', 'of', 'bessel', 'function', 'derivatives', 'for', 'three', 'different', 'kind', 'of', 'normalization', 'the', 'key', 'tools', 'in', 'the', 'proof', 'of', 'our', 'main', 'results', 'are', 'the', 'mittagle... | [-0.10406681763096934, 0.03331975449497501, -0.08737131034556245, 0.11527157132292078, -0.072152210585773, -0.01564751517559801, -0.006942904543220287, 0.3101390349013465, -0.2553647702648526, -0.25211846611152094, 0.12044644166183259, -0.28546150277058285, -0.19057908675500324, 0.24995411312030186, -0.0478578281921467... |
1,802.05463 | Spontaneous symmetry breaking of domain walls in phase-competing regions | We study the nature of domain walls in an ordered phase in the
phase-competing region of two Ising-type order parameters. Considering a
two-component $\phi^4$ theory, we show that the domain wall of the ground-state
(primary) order parameter shows a second-order phase transition associated with
the secondary order pa... | cond-mat.stat-mech cond-mat.str-el | we study the nature of domain walls in an ordered phase in the phasecompeting region of two isingtype order parameters considering a twocomponent phi4 theory we show that the domain wall of the groundstate primary order parameter shows a secondorder phase transition associated with the secondary order parameter of the ... | [['we', 'study', 'the', 'nature', 'of', 'domain', 'walls', 'in', 'an', 'ordered', 'phase', 'in', 'the', 'phasecompeting', 'region', 'of', 'two', 'isingtype', 'order', 'parameters', 'considering', 'a', 'twocomponent', 'phi4', 'theory', 'we', 'show', 'that', 'the', 'domain', 'wall', 'of', 'the', 'groundstate', 'primary',... | [-0.19018398689764454, 0.23799931890632783, -0.06770211311282012, 0.005780540204984297, -0.04949082801287095, -0.05497417816539006, 0.07645027367659074, 0.3493206290335491, -0.25673979950731557, -0.2633347931992391, 0.08406283919787805, -0.28319650898077364, -0.16087733870693322, 0.04187482566540611, 0.0629601178925127... |
1,802.05464 | Estimates for a general fractional relaxation equation and application
to an inverse source problem | A general fractional relaxation equation is considered with a convolutional
derivative in time introduced by A. Kochubei (Integr. Equ. Oper. Theory 71
(2011), 583-600). This equation generalizes the single-term, multi-term and
distributed-order fractional relaxation equations. The fundamental and the
impulse-response... | math.AP | a general fractional relaxation equation is considered with a convolutional derivative in time introduced by a kochubei integr equ oper theory 71 2011 583600 this equation generalizes the singleterm multiterm and distributedorder fractional relaxation equations the fundamental and the impulseresponse solutions are stud... | [['a', 'general', 'fractional', 'relaxation', 'equation', 'is', 'considered', 'with', 'a', 'convolutional', 'derivative', 'in', 'time', 'introduced', 'by', 'a', 'kochubei', 'integr', 'equ', 'oper', 'theory', '71', '2011', '583600', 'this', 'equation', 'generalizes', 'the', 'singleterm', 'multiterm', 'and', 'distributed... | [-0.0981790533660034, 0.05060151394485446, -0.07530789490386808, 0.1177213069625669, -0.096336396625808, -0.0971940701818365, -0.018331483156800055, 0.2779686015361504, -0.2973990907250605, -0.261282826312682, 0.16900157668623278, -0.2639709620655162, -0.15579891901065424, 0.22309923945763374, -0.059604294647833386, 0.... |
1,802.05465 | Massivizing Computer Systems: a Vision to Understand, Design, and
Engineer Computer Ecosystems through and beyond Modern Distributed Systems | Our society is digital: industry, science, governance, and individuals
depend, often transparently, on the inter-operation of large numbers of
distributed computer systems. Although the society takes them almost for
granted, these computer ecosystems are not available for all, may not be
affordable for long, and rais... | cs.DC cs.SE | our society is digital industry science governance and individuals depend often transparently on the interoperation of large numbers of distributed computer systems although the society takes them almost for granted these computer ecosystems are not available for all may not be affordable for long and raise numerous ot... | [['our', 'society', 'is', 'digital', 'industry', 'science', 'governance', 'and', 'individuals', 'depend', 'often', 'transparently', 'on', 'the', 'interoperation', 'of', 'large', 'numbers', 'of', 'distributed', 'computer', 'systems', 'although', 'the', 'society', 'takes', 'them', 'almost', 'for', 'granted', 'these', 'co... | [-0.11291065151844897, 0.07711742292227808, -0.05745299572451735, 0.049409196163013355, -0.14590119314727498, -0.1376667985442414, 0.03405742866418032, 0.37700902047343793, -0.2909010646920373, -0.37786193754968805, 0.17282744387856253, -0.25364251244020886, -0.20697582151858943, 0.2661212150271593, -0.1121550133875779... |
1,802.05466 | 2D materials coupled to hybrid metal-dielectric waveguides for THz
technology | In this letter, we propose hybrid metal-dielectric waveguides coupled to 2D
materials that provide strong light-matter interaction at THz frequencies. We
investigate the properties of the fundamental propagating modes and show that
the strength of in-plane electric field components is maximized at the top of
the diel... | physics.optics | in this letter we propose hybrid metaldielectric waveguides coupled to 2d materials that provide strong lightmatter interaction at thz frequencies we investigate the properties of the fundamental propagating modes and show that the strength of inplane electric field components is maximized at the top of the dielectric ... | [['in', 'this', 'letter', 'we', 'propose', 'hybrid', 'metaldielectric', 'waveguides', 'coupled', 'to', '2d', 'materials', 'that', 'provide', 'strong', 'lightmatter', 'interaction', 'at', 'thz', 'frequencies', 'we', 'investigate', 'the', 'properties', 'of', 'the', 'fundamental', 'propagating', 'modes', 'and', 'show', 't... | [-0.18546659397927798, 0.1909692062609741, 0.004606528247197, -0.0917739957065282, -0.027045047262086057, -0.16671285977727682, 0.03643199548186769, 0.5092082403354207, -0.24987169269929235, -0.2737065300450854, -0.03075742031082968, -0.28563783410936594, -0.14978406654521473, 0.2548610303212695, 0.05585429393949936, 0... |
1,802.05467 | Nonlinear characterisation of a silicon integrated Bragg waveguide
filter | Bragg waveguides are promising optical filters for pump suppression in
spontaneous Four-Wave Mixing (FWM) photon sources. In this work, we investigate
the generation of unwanted photon pairs in the filter itself. We do this by
taking advantage of the relation between spontaneous and classical FWM, which
allows for th... | quant-ph physics.optics | bragg waveguides are promising optical filters for pump suppression in spontaneous fourwave mixing fwm photon sources in this work we investigate the generation of unwanted photon pairs in the filter itself we do this by taking advantage of the relation between spontaneous and classical fwm which allows for the precise... | [['bragg', 'waveguides', 'are', 'promising', 'optical', 'filters', 'for', 'pump', 'suppression', 'in', 'spontaneous', 'fourwave', 'mixing', 'fwm', 'photon', 'sources', 'in', 'this', 'work', 'we', 'investigate', 'the', 'generation', 'of', 'unwanted', 'photon', 'pairs', 'in', 'the', 'filter', 'itself', 'we', 'do', 'this'... | [-0.09901913010358714, 0.11945412131437855, -0.07477467823452477, 0.03525699058844676, -0.03440529867717675, -0.1032382583695239, 0.05642476466660998, 0.4306157465446098, -0.2690227524216833, -0.27795870891162033, 0.03884427006163731, -0.2850625080700787, -0.12593731295702787, 0.24568279806187313, -0.006644795301916271... |
1,802.05468 | Digital Cultural Heritage imaging via osmosis filtering | In Cultural Heritage (CH) imaging, data acquired within different spectral
regions are often used to inspect surface and sub-surface features. Due to the
experimental setup, these images may suffer from intensity inhomogeneities,
which may prevent conservators from distinguishing the physical properties of
the object... | math.NA | in cultural heritage ch imaging data acquired within different spectral regions are often used to inspect surface and subsurface features due to the experimental setup these images may suffer from intensity inhomogeneities which may prevent conservators from distinguishing the physical properties of the object under re... | [['in', 'cultural', 'heritage', 'ch', 'imaging', 'data', 'acquired', 'within', 'different', 'spectral', 'regions', 'are', 'often', 'used', 'to', 'inspect', 'surface', 'and', 'subsurface', 'features', 'due', 'to', 'the', 'experimental', 'setup', 'these', 'images', 'may', 'suffer', 'from', 'intensity', 'inhomogeneities',... | [0.012436570400333875, 0.026486746142562544, -0.10822692917251628, 0.06561502124173312, -0.10059788315046629, -0.09964064543760598, -0.004133543537846728, 0.4093272181192719, -0.2834426757882745, -0.3540776779505182, 0.12156907466721836, -0.29427750278519443, -0.146039832769319, 0.21866146677766915, -0.1475706067482848... |
1,802.05469 | Second order optimality on orthogonal Stiefel manifolds | The main tool to study a second order optimality problem is the Hessian
operator associated to the cost function that defines the optimization problem.
By regarding an orthogonal Stiefel manifold as a constraint manifold embedded
in an Euclidean space we obtain a concise matrix formula for the Hessian of a
cost funct... | math.NA cs.NA | the main tool to study a second order optimality problem is the hessian operator associated to the cost function that defines the optimization problem by regarding an orthogonal stiefel manifold as a constraint manifold embedded in an euclidean space we obtain a concise matrix formula for the hessian of a cost function... | [['the', 'main', 'tool', 'to', 'study', 'a', 'second', 'order', 'optimality', 'problem', 'is', 'the', 'hessian', 'operator', 'associated', 'to', 'the', 'cost', 'function', 'that', 'defines', 'the', 'optimization', 'problem', 'by', 'regarding', 'an', 'orthogonal', 'stiefel', 'manifold', 'as', 'a', 'constraint', 'manifol... | [-0.14203158276021674, -0.04389919933368029, -0.08759002834238916, 0.10241831139679633, -0.10164576011338557, -0.09257775588947184, 0.010865422101916588, 0.37612881936784226, -0.29031786577337804, -0.25765727756216245, 0.16395988383595192, -0.21281902246432854, -0.220467297037686, 0.17251492704088295, -0.11136353495256... |
1,802.0547 | Chromatic symmetric functions via the group algebra of $S_n$ | We prove some Schur positivity results for the chromatic symmetric function
$X_G$ of a (hyper)graph $G$, using connections to the group algebra of the
symmetric group. The first such connection works for (hyper)forests $F$: we
describe the Schur coefficients of $X_F$ in terms of eigenvalues of a product
of Hermitian ... | math.CO math.RT | we prove some schur positivity results for the chromatic symmetric function x_g of a hypergraph g using connections to the group algebra of the symmetric group the first such connection works for hyperforests f we describe the schur coefficients of x_f in terms of eigenvalues of a product of hermitian idempotents in th... | [['we', 'prove', 'some', 'schur', 'positivity', 'results', 'for', 'the', 'chromatic', 'symmetric', 'function', 'x_g', 'of', 'a', 'hypergraph', 'g', 'using', 'connections', 'to', 'the', 'group', 'algebra', 'of', 'the', 'symmetric', 'group', 'the', 'first', 'such', 'connection', 'works', 'for', 'hyperforests', 'f', 'we',... | [-0.17898447620019392, 0.06781052487257819, -0.11071411427110434, 0.05254732799293806, -0.13295534355195843, -0.11485680120238503, 0.0014513775533595622, 0.3420899299695002, -0.3128047859086501, -0.19081991485363206, 0.07406898905964111, -0.21555653683045595, -0.1970530395204855, 0.14979984967457438, -0.092165221162572... |
1,802.05471 | Smooth heaps and a dual view of self-adjusting data structures | We present a new connection between self-adjusting binary search trees (BSTs)
and heaps, two fundamental, extensively studied, and practically relevant
families of data structures. Roughly speaking, we map an arbitrary heap
algorithm within a natural model, to a corresponding BST algorithm with the
same cost on a dua... | cs.DS math.CO | we present a new connection between selfadjusting binary search trees bsts and heaps two fundamental extensively studied and practically relevant families of data structures roughly speaking we map an arbitrary heap algorithm within a natural model to a corresponding bst algorithm with the same cost on a dual sequence ... | [['we', 'present', 'a', 'new', 'connection', 'between', 'selfadjusting', 'binary', 'search', 'trees', 'bsts', 'and', 'heaps', 'two', 'fundamental', 'extensively', 'studied', 'and', 'practically', 'relevant', 'families', 'of', 'data', 'structures', 'roughly', 'speaking', 'we', 'map', 'an', 'arbitrary', 'heap', 'algorith... | [-0.10373582441997886, 0.0706291904583513, -0.12970024414395018, 0.10963038949476969, -0.114037476476989, -0.1721181272028911, 0.1252025069306708, 0.3818663754569436, -0.31610016437178406, -0.33780931650350493, 0.11135458479197782, -0.20798825814595653, -0.17624668537777055, 0.19857544998155424, -0.07368813674051866, 0... |
1,802.05472 | Admissible Time Series Motif Discovery with Missing Data | The discovery of time series motifs has emerged as one of the most useful
primitives in time series data mining. Researchers have shown its utility for
exploratory data mining, summarization, visualization, segmentation,
classification, clustering, and rule discovery. Although there has been more
than a decade of ext... | cs.LG cs.AI stat.ML | the discovery of time series motifs has emerged as one of the most useful primitives in time series data mining researchers have shown its utility for exploratory data mining summarization visualization segmentation classification clustering and rule discovery although there has been more than a decade of extensive res... | [['the', 'discovery', 'of', 'time', 'series', 'motifs', 'has', 'emerged', 'as', 'one', 'of', 'the', 'most', 'useful', 'primitives', 'in', 'time', 'series', 'data', 'mining', 'researchers', 'have', 'shown', 'its', 'utility', 'for', 'exploratory', 'data', 'mining', 'summarization', 'visualization', 'segmentation', 'class... | [-0.11987014067805528, 0.011468833351197341, -0.09155168401775882, 0.05712494506426285, -0.13179822650757464, -0.11534510275103255, 0.08330402107741167, 0.40494706072948045, -0.24375705223145713, -0.36944116972800756, 0.11660610090135985, -0.291662967725036, -0.1779308741065001, 0.2261437375111402, -0.06993086089561176... |
1,802.05473 | Beta - and gamma-decay transition rates in the two-group shell model | In the framework of the two-group configuration model we obtain formulas for
the reduced transition rates for beta- and gamma-transitions in even-even,
odd-odd, even-odd, and odd-even nuclei. We explored dependencies of the
transition rates on the occupancies of the involved subshells, as well as on
the spin values o... | nucl-th | in the framework of the twogroup configuration model we obtain formulas for the reduced transition rates for beta and gammatransitions in eveneven oddodd evenodd and oddeven nuclei we explored dependencies of the transition rates on the occupancies of the involved subshells as well as on the spin values of the initial ... | [['in', 'the', 'framework', 'of', 'the', 'twogroup', 'configuration', 'model', 'we', 'obtain', 'formulas', 'for', 'the', 'reduced', 'transition', 'rates', 'for', 'beta', 'and', 'gammatransitions', 'in', 'eveneven', 'oddodd', 'evenodd', 'and', 'oddeven', 'nuclei', 'we', 'explored', 'dependencies', 'of', 'the', 'transiti... | [-0.06398126155254431, 0.14955735087860375, -0.023366824723780155, 0.15099024552619084, 0.09624874696601182, -0.07546791250351817, 0.10864899880834855, 0.3525922612287104, -0.16924097043520306, -0.30298182719852773, 0.026099246939702427, -0.2945766066084616, -0.04451332243042998, 0.20171689281414729, 0.0664715746297588... |
1,802.05474 | Gauge invariant determination of charged hadron masses | In this paper we show, for the first time, that charged-hadron masses can be
calculated on the lattice without relying on gauge fixing at any stage of the
calculations. In our simulations we follow a recent proposal and formulate full
QCD+QED on a finite volume, without spoiling locality, by imposing C-periodic
bound... | hep-lat | in this paper we show for the first time that chargedhadron masses can be calculated on the lattice without relying on gauge fixing at any stage of the calculations in our simulations we follow a recent proposal and formulate full qcdqed on a finite volume without spoiling locality by imposing cperiodic boundary condit... | [['in', 'this', 'paper', 'we', 'show', 'for', 'the', 'first', 'time', 'that', 'chargedhadron', 'masses', 'can', 'be', 'calculated', 'on', 'the', 'lattice', 'without', 'relying', 'on', 'gauge', 'fixing', 'at', 'any', 'stage', 'of', 'the', 'calculations', 'in', 'our', 'simulations', 'we', 'follow', 'a', 'recent', 'propos... | [-0.09823533623719848, 0.1900800921374451, -0.10171929293231952, 0.06382836305477736, -0.021240920240108836, -0.09054180727778188, 0.031044284268035648, 0.39602380475362403, -0.18180194693819515, -0.3109822618768902, 0.059685379784825625, -0.22796887966699356, -0.0855117661952479, 0.14936407586861872, -0.02105122776270... |
1,802.05475 | Robust and sparse Gaussian graphical modeling under cell-wise
contamination | Graphical modeling explores dependences among a collection of variables by
inferring a graph that encodes pairwise conditional independences. For jointly
Gaussian variables, this translates into detecting the support of the precision
matrix. Many modern applications feature high-dimensional and contaminated data
that... | stat.ME | graphical modeling explores dependences among a collection of variables by inferring a graph that encodes pairwise conditional independences for jointly gaussian variables this translates into detecting the support of the precision matrix many modern applications feature highdimensional and contaminated data that compl... | [['graphical', 'modeling', 'explores', 'dependences', 'among', 'a', 'collection', 'of', 'variables', 'by', 'inferring', 'a', 'graph', 'that', 'encodes', 'pairwise', 'conditional', 'independences', 'for', 'jointly', 'gaussian', 'variables', 'this', 'translates', 'into', 'detecting', 'the', 'support', 'of', 'the', 'preci... | [-0.06185463805181476, 0.01908244100027682, -0.07168701709955573, 0.09285992787156899, -0.11111557969259313, -0.17014193924002868, 0.05427336243715567, 0.4064263310820724, -0.2826548610598995, -0.2935188717584914, 0.12979126032307528, -0.2680586491120406, -0.1923637922781591, 0.21849973973943493, -0.15033033565403178, ... |
1,802.05476 | Quantum Walks of kicked Bose-Einstein condensates | We analytically investigate the recently proposed and implemented
discrete-time quantum walk based on kicked ultra-cold atoms. We show how the
internal level structure of the kicked atoms leads to the emergence of a
relative light-shift phase immediately relevant for the experimental
realization. Analytical solutions... | quant-ph cond-mat.quant-gas | we analytically investigate the recently proposed and implemented discretetime quantum walk based on kicked ultracold atoms we show how the internal level structure of the kicked atoms leads to the emergence of a relative lightshift phase immediately relevant for the experimental realization analytical solutions are pr... | [['we', 'analytically', 'investigate', 'the', 'recently', 'proposed', 'and', 'implemented', 'discretetime', 'quantum', 'walk', 'based', 'on', 'kicked', 'ultracold', 'atoms', 'we', 'show', 'how', 'the', 'internal', 'level', 'structure', 'of', 'the', 'kicked', 'atoms', 'leads', 'to', 'the', 'emergence', 'of', 'a', 'relat... | [-0.13971687544167774, 0.19164444570292216, -0.057901144313977145, 0.04981273718097879, 0.002755908352765636, -0.1536831887454161, 0.07166081154146461, 0.375500353022677, -0.22437379191644857, -0.2167476767246596, 0.038759210818737254, -0.23836428587149341, -0.15250345276760274, 0.21870918933790726, 0.03666660050693594... |
1,802.05477 | Approximate quantum Markov chains | This book is an introduction to quantum Markov chains and explains how this
concept is connected to the question of how well a lost quantum mechanical
system can be recovered from a correlated subsystem. To achieve this goal, we
strengthen the data-processing inequality such that it reveals a statement
about the reco... | quant-ph cs.IT math-ph math.IT math.MP | this book is an introduction to quantum markov chains and explains how this concept is connected to the question of how well a lost quantum mechanical system can be recovered from a correlated subsystem to achieve this goal we strengthen the dataprocessing inequality such that it reveals a statement about the reconstru... | [['this', 'book', 'is', 'an', 'introduction', 'to', 'quantum', 'markov', 'chains', 'and', 'explains', 'how', 'this', 'concept', 'is', 'connected', 'to', 'the', 'question', 'of', 'how', 'well', 'a', 'lost', 'quantum', 'mechanical', 'system', 'can', 'be', 'recovered', 'from', 'a', 'correlated', 'subsystem', 'to', 'achiev... | [-0.08296347421256939, 0.12602089366366512, -0.09876491178537189, 0.12940367126839947, -0.07896823949021035, -0.18471432314640251, 0.03765422546559461, 0.34033223796759354, -0.33105566227057365, -0.2810120159188975, 0.12941969122843128, -0.2788383261485859, -0.1945661200282488, 0.1898913068075546, -0.11695770318947928,... |
1,802.05478 | Enhanced non-Markovian behavior in quantum walks with Markovian disorder | Non-Markovian quantum effects are typically observed in systems interacting
with structured reservoirs. Discrete-time quantum walks are prime example of
such systems in which, quantum memory arises due to the controlled interaction
between the coin and position degrees of freedom. Here we show that the
information ba... | quant-ph | nonmarkovian quantum effects are typically observed in systems interacting with structured reservoirs discretetime quantum walks are prime example of such systems in which quantum memory arises due to the controlled interaction between the coin and position degrees of freedom here we show that the information backflow ... | [['nonmarkovian', 'quantum', 'effects', 'are', 'typically', 'observed', 'in', 'systems', 'interacting', 'with', 'structured', 'reservoirs', 'discretetime', 'quantum', 'walks', 'are', 'prime', 'example', 'of', 'such', 'systems', 'in', 'which', 'quantum', 'memory', 'arises', 'due', 'to', 'the', 'controlled', 'interaction... | [-0.1769147699659054, 0.22119507553222462, -0.07220404751114244, 0.06263719094990884, -0.010951628115376442, -0.20253310459703813, 0.017244366163244033, 0.3747259059360599, -0.3119536869651903, -0.27207691034650416, 0.06520017619032746, -0.28748233442959503, -0.19177208927732597, 0.16030502931510165, -0.069542018496014... |
1,802.05479 | Voros symbols as cluster coordinates | We show that the Borel sums of the Voros symbols considered in the theory of
exact WKB analysis arise naturally as Fock-Goncharov coordinates of framed
$PGL_2(\mathbb{C})$-local systems on a marked bordered surface. Using this
result, we show that these Borel sums can be meromorphically continued to any
point of $\ma... | math.CA hep-th math.GT | we show that the borel sums of the voros symbols considered in the theory of exact wkb analysis arise naturally as fockgoncharov coordinates of framed pgl_2mathbbclocal systems on a marked bordered surface using this result we show that these borel sums can be meromorphically continued to any point of mathbbc and we pr... | [['we', 'show', 'that', 'the', 'borel', 'sums', 'of', 'the', 'voros', 'symbols', 'considered', 'in', 'the', 'theory', 'of', 'exact', 'wkb', 'analysis', 'arise', 'naturally', 'as', 'fockgoncharov', 'coordinates', 'of', 'framed', 'pgl_2mathbbclocal', 'systems', 'on', 'a', 'marked', 'bordered', 'surface', 'using', 'this',... | [-0.21178901326627686, 0.054452038708796655, -0.16288163719268944, 0.08144789001940247, -0.05323346283000249, -0.06380889205835187, 0.05625489642306303, 0.3255933488969906, -0.3360684633255005, -0.19099240876161136, 0.07592983030570814, -0.2311340688683021, -0.24627189209254888, 0.18952844025423893, -0.1654560782158604... |
1,802.0548 | Evolution of Images with Diversity and Constraints Using a Generator
Network | Evolutionary search has been extensively used to generate artistic images.
Raw images have high dimensionality which makes a direct search for an image
challenging. In previous work this problem has been addressed by using compact
symbolic encodings or by constraining images with priors. Recent developments
in deep l... | cs.NE | evolutionary search has been extensively used to generate artistic images raw images have high dimensionality which makes a direct search for an image challenging in previous work this problem has been addressed by using compact symbolic encodings or by constraining images with priors recent developments in deep learni... | [['evolutionary', 'search', 'has', 'been', 'extensively', 'used', 'to', 'generate', 'artistic', 'images', 'raw', 'images', 'have', 'high', 'dimensionality', 'which', 'makes', 'a', 'direct', 'search', 'for', 'an', 'image', 'challenging', 'in', 'previous', 'work', 'this', 'problem', 'has', 'been', 'addressed', 'by', 'usi... | [-0.010266394398238418, 0.03705760421036285, -0.10269334448435355, 0.08383693845071657, -0.14097143918201097, -0.1562647166184759, -0.010176570171254607, 0.48193175101905694, -0.22947211824371883, -0.36713525424079024, 0.08704047961545718, -0.2884176391475822, -0.18119718890815376, 0.17743472672171062, -0.1256026464433... |
1,802.05481 | Chaos in Kuramoto oscillator networks | Kuramoto oscillators are widely used to explain collective phenomena in
networks of coupled oscillatory units. We show that simple networks of two
populations with a generic coupling scheme, where both coupling strengths and
phase lags between and within populations are distinct, can exhibit chaotic
dynamics as conje... | nlin.CD math.DS nlin.AO | kuramoto oscillators are widely used to explain collective phenomena in networks of coupled oscillatory units we show that simple networks of two populations with a generic coupling scheme where both coupling strengths and phase lags between and within populations are distinct can exhibit chaotic dynamics as conjecture... | [['kuramoto', 'oscillators', 'are', 'widely', 'used', 'to', 'explain', 'collective', 'phenomena', 'in', 'networks', 'of', 'coupled', 'oscillatory', 'units', 'we', 'show', 'that', 'simple', 'networks', 'of', 'two', 'populations', 'with', 'a', 'generic', 'coupling', 'scheme', 'where', 'both', 'coupling', 'strengths', 'an... | [-0.17907272800221108, 0.20206608624236347, -0.03665969017310999, 0.09146449493709952, 0.02504429307979687, -0.21747463908104692, 0.01687874007135785, 0.36187310062814504, -0.2560847804464477, -0.3070036464099151, 0.03906667749834014, -0.2539075568590003, -0.2534134133214441, 0.19886061081585163, -0.019190335444970213,... |
1,802.05482 | DMRG simulations of SU(N) Heisenberg chains using standard Young
tableaux: fundamental representation and comparison with finite-size Bethe
ansatz | We develop an efficient method to perform density matrix renormalization
group simulations of the SU(N) Heisenberg chain with open boundary conditions
taking full advantage of the SU(N) symmetry of the problem. This method is an
extension of the method previously developed for exact diagonalizations and
relies on a s... | cond-mat.str-el | we develop an efficient method to perform density matrix renormalization group simulations of the sun heisenberg chain with open boundary conditions taking full advantage of the sun symmetry of the problem this method is an extension of the method previously developed for exact diagonalizations and relies on a systemat... | [['we', 'develop', 'an', 'efficient', 'method', 'to', 'perform', 'density', 'matrix', 'renormalization', 'group', 'simulations', 'of', 'the', 'sun', 'heisenberg', 'chain', 'with', 'open', 'boundary', 'conditions', 'taking', 'full', 'advantage', 'of', 'the', 'sun', 'symmetry', 'of', 'the', 'problem', 'this', 'method', '... | [-0.0775048855541493, 0.11160619465021335, -0.05417348418114296, 0.06194020579432082, -0.013422258788555422, -0.14371067874736207, 0.06822272131411249, 0.3600430892780423, -0.19642155774156836, -0.3282766779336859, 0.10508935556212878, -0.3125292610486641, -0.05183153697974322, 0.17872556962059152, 0.038415202029350705... |
1,802.05483 | Extensive study of electron acceleration by relativistic surface
plasmons | The excitation of surface plasmons with ultra-intense ($I\sim 5\times
10^{19}$ W/cm$^2$), high contrast ($\sim 10^{12}$) laser pulses on
periodically-modulated solid targets has been recently demonstrated to produce
collimated bunches of energetic electrons along the target surface [Fedeli et
al., Phys. Rev. Lett. 11... | physics.plasm-ph | the excitation of surface plasmons with ultraintense isim 5times 1019 wcm2 high contrast sim 1012 laser pulses on periodicallymodulated solid targets has been recently demonstrated to produce collimated bunches of energetic electrons along the target surface fedeli et al phys rev lett 116 5001 2016 here we report an ex... | [['the', 'excitation', 'of', 'surface', 'plasmons', 'with', 'ultraintense', 'isim', '5times', '1019', 'wcm2', 'high', 'contrast', 'sim', '1012', 'laser', 'pulses', 'on', 'periodicallymodulated', 'solid', 'targets', 'has', 'been', 'recently', 'demonstrated', 'to', 'produce', 'collimated', 'bunches', 'of', 'energetic', '... | [-0.07776651006119634, 0.1810000811918815, -0.011520030266306932, -0.01954338693984522, -0.028047276763934915, -0.10701782188550071, 0.03631823813515598, 0.4682017733598381, -0.12982217923204586, -0.40842623153285496, -0.047515649556462626, -0.3165181658990247, -0.018642518750744536, 0.2737968259353136, -0.041366443526... |
1,802.05484 | On the P vs NP question: a proof of inequality | The analysis discussed in this paper is based on a well-known NP-complete
problem which is called satisfiability problem or SAT. From SAT a new
NP-complete problem is derived, which is described by a Boolean function called
core function. In this paper it is proved that the cost of the minimal
implementation of core ... | cs.CC | the analysis discussed in this paper is based on a wellknown npcomplete problem which is called satisfiability problem or sat from sat a new npcomplete problem is derived which is described by a boolean function called core function in this paper it is proved that the cost of the minimal implementation of core function... | [['the', 'analysis', 'discussed', 'in', 'this', 'paper', 'is', 'based', 'on', 'a', 'wellknown', 'npcomplete', 'problem', 'which', 'is', 'called', 'satisfiability', 'problem', 'or', 'sat', 'from', 'sat', 'a', 'new', 'npcomplete', 'problem', 'is', 'derived', 'which', 'is', 'described', 'by', 'a', 'boolean', 'function', '... | [-0.09289337687746242, 0.06466328458056389, -0.0553589594538933, 0.09629957475067105, -0.11054517236756689, -0.16742101096099726, 0.04846693850467326, 0.3325057645374334, -0.33701027603245076, -0.29875028301835244, 0.12845024837031502, -0.22564834092433253, -0.19766765949028878, 0.17089191678031865, -0.1033552204040281... |
1,802.05485 | Electron drag in ferromagnetic structures separated by an insulating
interface | We consider electron drag in a system of two ferromagnetic layers separated
by an insulating interface. The source of it is expected to be magnon-electron
interactions. Namely, we assume that the external voltage is applied to the
"active" layer stimulating electric current through this layer. In its turn,
the scatte... | cond-mat.mes-hall cond-mat.supr-con | we consider electron drag in a system of two ferromagnetic layers separated by an insulating interface the source of it is expected to be magnonelectron interactions namely we assume that the external voltage is applied to the active layer stimulating electric current through this layer in its turn the scattering of th... | [['we', 'consider', 'electron', 'drag', 'in', 'a', 'system', 'of', 'two', 'ferromagnetic', 'layers', 'separated', 'by', 'an', 'insulating', 'interface', 'the', 'source', 'of', 'it', 'is', 'expected', 'to', 'be', 'magnonelectron', 'interactions', 'namely', 'we', 'assume', 'that', 'the', 'external', 'voltage', 'is', 'app... | [-0.16610194550378732, 0.20469632767762286, -0.03525476028853855, 0.0010439154726487618, -0.03595870762580523, -0.12303182626298319, 0.07116329307879184, 0.3511763088819053, -0.3298465683883815, -0.2835648380806325, -0.006161362522376563, -0.32748862984805815, -0.08278559299058677, 0.17649403048886192, 0.04184636157609... |
1,802.05486 | An autonomous single-piston engine with a quantum rotor | Pistons are elementary components of a wide variety of thermal engines,
allowing to convert input fuel into rotational motion. Here, we propose a
single-piston engine where the rotational degree of freedom is effectively
realized by the flux of a Josephson loop -- a quantum rotor -- while the
working volume correspon... | quant-ph | pistons are elementary components of a wide variety of thermal engines allowing to convert input fuel into rotational motion here we propose a singlepiston engine where the rotational degree of freedom is effectively realized by the flux of a josephson loop a quantum rotor while the working volume corresponds to the ef... | [['pistons', 'are', 'elementary', 'components', 'of', 'a', 'wide', 'variety', 'of', 'thermal', 'engines', 'allowing', 'to', 'convert', 'input', 'fuel', 'into', 'rotational', 'motion', 'here', 'we', 'propose', 'a', 'singlepiston', 'engine', 'where', 'the', 'rotational', 'degree', 'of', 'freedom', 'is', 'effectively', 'r... | [-0.1516845349429382, 0.16789408263233513, -0.06683488604526415, -0.019024374056176317, -0.11647241254319886, -0.19256260762146363, 0.07229300593651176, 0.37383298898391704, -0.24621376767323386, -0.3184143867240184, 0.0663705398587303, -0.22333312726415763, -0.08305914277971843, 0.26231201506581986, -0.057638441066956... |
1,802.05487 | Shannon entropy and particle decays | We deploy Shannon's information entropy to the distribution of branching
fractions in a particle decay. This serves to quantify how important a given
new reported decay channel is, from the point of view of the information that
it adds to the already known ones. Because the entropy is additive, one can
subdivide the ... | hep-ph hep-ex nucl-th | we deploy shannons information entropy to the distribution of branching fractions in a particle decay this serves to quantify how important a given new reported decay channel is from the point of view of the information that it adds to the already known ones because the entropy is additive one can subdivide the set of ... | [['we', 'deploy', 'shannons', 'information', 'entropy', 'to', 'the', 'distribution', 'of', 'branching', 'fractions', 'in', 'a', 'particle', 'decay', 'this', 'serves', 'to', 'quantify', 'how', 'important', 'a', 'given', 'new', 'reported', 'decay', 'channel', 'is', 'from', 'the', 'point', 'of', 'view', 'of', 'the', 'info... | [-0.0678696979292033, 0.183693698977303, -0.12353444889744866, 0.12541586847945385, -0.07934020926618826, -0.14310519768482197, 0.10979603334312614, 0.2886241383014995, -0.31159485328211406, -0.30065018152731043, 0.10506779031292753, -0.3080123663819003, -0.08791507637807142, 0.16137545124984512, -0.040829733780054285,... |
1,802.05488 | Phase and micromotion of Bose-Einstein condensates in a time-averaged
ring trap | Rapidly scanning magnetic and optical dipole traps have been widely utilised
to form time-averaged potentials for ultracold quantum gas experiments. Here we
theoretically and experimentally characterise the dynamic properties of
Bose-Einstein condensates in ring-shaped potentials that are formed by scanning
an optica... | cond-mat.quant-gas physics.atom-ph quant-ph | rapidly scanning magnetic and optical dipole traps have been widely utilised to form timeaveraged potentials for ultracold quantum gas experiments here we theoretically and experimentally characterise the dynamic properties of boseeinstein condensates in ringshaped potentials that are formed by scanning an optical dipo... | [['rapidly', 'scanning', 'magnetic', 'and', 'optical', 'dipole', 'traps', 'have', 'been', 'widely', 'utilised', 'to', 'form', 'timeaveraged', 'potentials', 'for', 'ultracold', 'quantum', 'gas', 'experiments', 'here', 'we', 'theoretically', 'and', 'experimentally', 'characterise', 'the', 'dynamic', 'properties', 'of', '... | [-0.15303036373341455, 0.2024086171164111, -0.11726103551419718, 0.018992331574138786, 0.009714432403977428, -0.1307771823794714, 0.03066363346297294, 0.46054855878864015, -0.24068031151496272, -0.26405635091343094, 0.03911674740591219, -0.26872183105974856, -0.10887303888265576, 0.21920827875445997, 0.0568073435766356... |
1,802.05489 | Optimal control of the customer dynamics based on marketing policy | We consider an optimal control problem for a non-autonomous model of ODEs
that describes the evolution of the number of customers in some firm. Namely we
study the best marketing strategy. Considering a $L^2$ cost functional, we
establish the existence and uniqueness of optimal solutions, using an inductive
argument ... | math.OC | we consider an optimal control problem for a nonautonomous model of odes that describes the evolution of the number of customers in some firm namely we study the best marketing strategy considering a l2 cost functional we establish the existence and uniqueness of optimal solutions using an inductive argument to obtain ... | [['we', 'consider', 'an', 'optimal', 'control', 'problem', 'for', 'a', 'nonautonomous', 'model', 'of', 'odes', 'that', 'describes', 'the', 'evolution', 'of', 'the', 'number', 'of', 'customers', 'in', 'some', 'firm', 'namely', 'we', 'study', 'the', 'best', 'marketing', 'strategy', 'considering', 'a', 'l2', 'cost', 'func... | [-0.11303391965636372, -0.013323336544495083, -0.07266089818644317, 0.08574556075308444, -0.08228331623449378, -0.13265029418819252, 0.10697684565560729, 0.36365442808690296, -0.282265320474649, -0.2734623460411808, 0.16420471058380076, -0.2666098509106214, -0.14894769298606111, 0.22389034840217145, -0.0905931034383710... |
1,802.0549 | Grammar-based Compression of Unranked Trees | We introduce forest straight-line programs (FSLPs) as a compressed
representation of unranked ordered node-labelled trees. FSLPs are based on the
operations of forest algebra and generalize tree straight-line programs. We
compare the succinctness of FSLPs with two other compression schemes for
unranked trees: top dag... | cs.DS cs.FL | we introduce forest straightline programs fslps as a compressed representation of unranked ordered nodelabelled trees fslps are based on the operations of forest algebra and generalize tree straightline programs we compare the succinctness of fslps with two other compression schemes for unranked trees top dags and tree... | [['we', 'introduce', 'forest', 'straightline', 'programs', 'fslps', 'as', 'a', 'compressed', 'representation', 'of', 'unranked', 'ordered', 'nodelabelled', 'trees', 'fslps', 'are', 'based', 'on', 'the', 'operations', 'of', 'forest', 'algebra', 'and', 'generalize', 'tree', 'straightline', 'programs', 'we', 'compare', 't... | [-0.14050691856169387, 0.15356994174714936, -0.0394435025163387, 0.12380723931066888, -0.15376654686406255, -0.15326660203894502, 0.07784095855527802, 0.4380379472123949, -0.36874351012765577, -0.27124167872396737, 0.11043763235456457, -0.28344187176737345, -0.10340381566386082, 0.1702031528356632, -0.09535287226746349... |
1,802.05491 | Biorthogonal systems on unit interval and zeta dilation operators | An elementary 'quantum-mechanical' derivation of the conditions for a system
of functions to form a Reisz basis of a Hilbert space on a finite interval is
presented.
| math-ph math.MP | an elementary quantummechanical derivation of the conditions for a system of functions to form a reisz basis of a hilbert space on a finite interval is presented | [['an', 'elementary', 'quantummechanical', 'derivation', 'of', 'the', 'conditions', 'for', 'a', 'system', 'of', 'functions', 'to', 'form', 'a', 'reisz', 'basis', 'of', 'a', 'hilbert', 'space', 'on', 'a', 'finite', 'interval', 'is', 'presented']] | [-0.17968120384547445, 0.10044932643574646, -0.16815986456694426, 0.07040165194430975, -0.06276605801691336, -0.03949597222661531, 0.046688373179036985, 0.31907460155586403, -0.22176969316960485, -0.13089379757918693, 0.10113384412532603, -0.2210466737203576, -0.08916438509132368, 0.2467007200682053, -0.020439517787761... |
1,802.05492 | Measurement of the Branching Fraction For the Semi-Leptonic Decays
$D^{0(+)}\to \pi^{-(0)}\mu^+\nu_\mu$ and Test of Lepton Flavor Universality | Using a data sample corresponding to an integrated luminosity of $2.93\,\rm
fb^{-1}$ taken at a center-of-mass energy of 3.773\,GeV with the BESIII
detector operated at the BEPCII collider, we perform an analysis of the
semi-leptonic decays $D^{0(+)}\to \pi^{-(0)}\mu^+\nu_\mu$. The branching
fractions of $D^0\to \pi^... | hep-ex | using a data sample corresponding to an integrated luminosity of 293rm fb1 taken at a centerofmass energy of 3773gev with the besiii detector operated at the bepcii collider we perform an analysis of the semileptonic decays d0to pi0munu_mu the branching fractions of d0to pimunu_mu and dto pi0munu_mu are measured to be ... | [['using', 'a', 'data', 'sample', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', '293rm', 'fb1', 'taken', 'at', 'a', 'centerofmass', 'energy', 'of', '3773gev', 'with', 'the', 'besiii', 'detector', 'operated', 'at', 'the', 'bepcii', 'collider', 'we', 'perform', 'an', 'analysis', 'of', 'the', 'semileptoni... | [-0.07319649816054152, 0.16076564795041218, -0.040272519452724066, 0.050063811826188805, 0.01631367555015267, -0.10804913573481731, 0.056023036838221164, 0.30978004721385477, -0.16929757461873937, -0.292829955143756, 0.005899297077312919, -0.4191525086368385, 0.1018854814909374, 0.17849940785182347, -0.0136139556768619... |
1,802.05493 | A (2+1)-dimensional Anisotropic KPZ growth model with a smooth phase | Stochastic growth processes in dimension $(2+1)$ were conjectured by D. Wolf,
on the basis of renormalization-group arguments, to fall into two distinct
universality classes, according to whether the Hessian $H_\rho$ of the speed of
growth $v(\rho)$ as a function of the average slope $\rho$ satisfies $\det
H_\rho>0$ ... | math.PR math-ph math.MP | stochastic growth processes in dimension 21 were conjectured by d wolf on the basis of renormalizationgroup arguments to fall into two distinct universality classes according to whether the hessian h_rho of the speed of growth vrho as a function of the average slope rho satisfies det h_rho0 isotropic kpz class or det h... | [['stochastic', 'growth', 'processes', 'in', 'dimension', '21', 'were', 'conjectured', 'by', 'd', 'wolf', 'on', 'the', 'basis', 'of', 'renormalizationgroup', 'arguments', 'to', 'fall', 'into', 'two', 'distinct', 'universality', 'classes', 'according', 'to', 'whether', 'the', 'hessian', 'h_rho', 'of', 'the', 'speed', 'o... | [-0.11251421808451414, 0.19019987236947053, -0.08301759804273025, 0.09031141781461338, -0.05051643894473091, -0.20010826161131262, -0.013740774356178008, 0.3343246129978215, -0.29536874609300867, -0.20563100207224488, 0.0964588388390839, -0.31955941114993763, -0.13014046695642173, 0.15428429223690182, -0.04995294504752... |
1,802.05494 | Non-idempotent types for classical calculi in natural deduction style | In the first part of this paper, we define two resource aware typing systems
for the {\lambda}{\mu}-calculus based on non-idempotent intersection and union
types. The non-idempotent approach provides very simple combinatorial
arguments-based on decreasing measures of type derivations-to characterize head
and strongly... | cs.LO | in the first part of this paper we define two resource aware typing systems for the lambdamucalculus based on nonidempotent intersection and union types the nonidempotent approach provides very simple combinatorial argumentsbased on decreasing measures of type derivationsto characterize head and strongly normalizing te... | [['in', 'the', 'first', 'part', 'of', 'this', 'paper', 'we', 'define', 'two', 'resource', 'aware', 'typing', 'systems', 'for', 'the', 'lambdamucalculus', 'based', 'on', 'nonidempotent', 'intersection', 'and', 'union', 'types', 'the', 'nonidempotent', 'approach', 'provides', 'very', 'simple', 'combinatorial', 'arguments... | [-0.13661882475749076, 0.033123533202149155, -0.0955435972455449, 0.06374289234733488, -0.12015357373766308, -0.15231602859324006, 0.10123080521359981, 0.29960664219450295, -0.3122566673504995, -0.2545981521124211, 0.10094127819165734, -0.22666000670159425, -0.13349274370734998, 0.18874496308808017, -0.1592433194393350... |
1,802.05495 | How Much Data Do You Need? An Operational, Pre-Asymptotic Metric for
Fat-tailedness | This note presents an operational measure of fat-tailedness for univariate
probability distributions, in $[0,1]$ where 0 is maximally thin-tailed
(Gaussian) and 1 is maximally fat-tailed. Among others,1) it helps assess the
sample size needed to establish a comparative $n$ needed for statistical
significance, 2) allo... | stat.ME q-fin.ST | this note presents an operational measure of fattailedness for univariate probability distributions in 01 where 0 is maximally thintailed gaussian and 1 is maximally fattailed among others1 it helps assess the sample size needed to establish a comparative n needed for statistical significance 2 allows practical compari... | [['this', 'note', 'presents', 'an', 'operational', 'measure', 'of', 'fattailedness', 'for', 'univariate', 'probability', 'distributions', 'in', '01', 'where', '0', 'is', 'maximally', 'thintailed', 'gaussian', 'and', '1', 'is', 'maximally', 'fattailed', 'among', 'others1', 'it', 'helps', 'assess', 'the', 'sample', 'size... | [-0.07544778370708631, 0.13437819384664232, -0.11817825553999266, 0.09766385732542232, -0.06372691186679534, -0.1566323441989545, 0.07533116215656743, 0.35668742885335686, -0.2448973371395135, -0.3261297820959684, 0.06415521728491834, -0.2961553722521352, -0.06251179583459783, 0.17323766935604965, -0.07594472905015741,... |
1,802.05496 | Extremals For Fractional Order Hardy-Sobolev-Maz'ya Inequality | In this article, we derive the existence of positive solutions of a
semi-linear, non-local elliptic PDE, involving a singular perturbation of the
fractional laplacian, coming from the fractional Hardy-Sobolev-Maz'ya
inequality, derived in this paper. We also derive symmetry properties and a
precise asymptotic behavio... | math.AP math.FA | in this article we derive the existence of positive solutions of a semilinear nonlocal elliptic pde involving a singular perturbation of the fractional laplacian coming from the fractional hardysobolevmazya inequality derived in this paper we also derive symmetry properties and a precise asymptotic behaviour of solutio... | [['in', 'this', 'article', 'we', 'derive', 'the', 'existence', 'of', 'positive', 'solutions', 'of', 'a', 'semilinear', 'nonlocal', 'elliptic', 'pde', 'involving', 'a', 'singular', 'perturbation', 'of', 'the', 'fractional', 'laplacian', 'coming', 'from', 'the', 'fractional', 'hardysobolevmazya', 'inequality', 'derived',... | [-0.18517496716231108, -0.0052902479453579235, -0.12663851871215942, 0.06837763507222838, -0.13349878585532957, -0.11231796462696207, -0.005022422063832536, 0.18230355449992677, -0.3001670180010083, -0.23302698443117348, 0.17763371206313858, -0.33170736641825543, -0.1867262210858905, 0.14600046672453376, -0.07495641410... |
1,802.05497 | Nano-Opto-Electro-Mechanical Systems | A new class of hybrid systems that couple optical, electrical and mechanical
degrees of freedom in nanoscale devices is under development in laboratories
worldwide. These nano-opto-electro-mechanical systems (NOEMS) offer
unprecedented opportunities to dynamically control the flow of light in
nanophotonic structures,... | physics.optics quant-ph | a new class of hybrid systems that couple optical electrical and mechanical degrees of freedom in nanoscale devices is under development in laboratories worldwide these nanooptoelectromechanical systems noems offer unprecedented opportunities to dynamically control the flow of light in nanophotonic structures at high s... | [['a', 'new', 'class', 'of', 'hybrid', 'systems', 'that', 'couple', 'optical', 'electrical', 'and', 'mechanical', 'degrees', 'of', 'freedom', 'in', 'nanoscale', 'devices', 'is', 'under', 'development', 'in', 'laboratories', 'worldwide', 'these', 'nanooptoelectromechanical', 'systems', 'noems', 'offer', 'unprecedented',... | [-0.16675137137108056, 0.15241700868592462, -0.045244558440810705, -0.06685520319954166, -0.08975152609173606, -0.1381322705566666, 0.06022974714134974, 0.4100896665482845, -0.2773821611517986, -0.31632097741787873, 0.094333827550957, -0.26619839811589097, -0.1812380604678765, 0.3212727392092347, -0.07490487887695865, ... |
1,802.05498 | Dynamics of high-order solitons in the nonlocal nonlinear
Schr\"{o}dinger equations | A study of high-order solitons in three nonlocal nonlinear Schr\"{o}dinger
equations is presented, which includes the \PT-symmetric, reverse-time, and
reverse-space-time nonlocal nonlinear Schr\"{o}dinger equations. General
high-order solitons in three different equations are derived from the same
Riemann-Hilbert sol... | nlin.PS | a study of highorder solitons in three nonlocal nonlinear schrodinger equations is presented which includes the ptsymmetric reversetime and reversespacetime nonlocal nonlinear schrodinger equations general highorder solitons in three different equations are derived from the same riemannhilbert solutions of the akns hie... | [['a', 'study', 'of', 'highorder', 'solitons', 'in', 'three', 'nonlocal', 'nonlinear', 'schrodinger', 'equations', 'is', 'presented', 'which', 'includes', 'the', 'ptsymmetric', 'reversetime', 'and', 'reversespacetime', 'nonlocal', 'nonlinear', 'schrodinger', 'equations', 'general', 'highorder', 'solitons', 'in', 'three... | [-0.14897686957310607, 0.1192497099748232, -0.10237284169181601, 0.10090655161600028, -0.07868891479538197, -0.15752378161149946, -0.12141849457338458, 0.36397168637773436, -0.26495548245775236, -0.23379870059041233, 0.1059818733483553, -0.27975954191589897, -0.1766936238174774, 0.2098578939277848, 0.008916004784647134... |
1,802.05499 | On the $L^p$ norm of the torsion unction | Bounds are obtained for the $L^p$ norm of the torsion function $v_{\Omega}$,
i.e. the solution of $-\Delta v=1,\, v\in H_0^1(\Omega),$ in terms of the
Lebesgue measure of $\Omega$ and the principal eigenvalue $\lambda_1(\Omega)$
of the Dirichlet Laplacian acting in $L^2(\Omega)$. We show that these bounds
are sharp f... | math.AP | bounds are obtained for the lp norm of the torsion function v_omega ie the solution of delta v1 vin h_01omega in terms of the lebesgue measure of omega and the principal eigenvalue lambda_1omega of the dirichlet laplacian acting in l2omega we show that these bounds are sharp for 1le ple 2 | [['bounds', 'are', 'obtained', 'for', 'the', 'lp', 'norm', 'of', 'the', 'torsion', 'function', 'v_omega', 'ie', 'the', 'solution', 'of', 'delta', 'v1', 'vin', 'h_01omega', 'in', 'terms', 'of', 'the', 'lebesgue', 'measure', 'of', 'omega', 'and', 'the', 'principal', 'eigenvalue', 'lambda_1omega', 'of', 'the', 'dirichlet'... | [-0.1680353890748366, 0.07294967611703802, -0.022673309210564613, 0.05157706265648206, -0.04375673268063396, -0.13971566147737058, -0.07411443453062982, 0.3563987349762636, -0.3174344789163739, -0.16512077929926852, 0.13834312029055082, -0.37660737138460665, -0.10453952151788946, 0.16949002093900287, -0.063004925936077... |
1,802.055 | 2PI effective action for the SYK model and tensor field theories | We discuss the two-particle irreducible (2PI) effective action for the SYK
model and for tensor field theories. For the SYK model the 2PI effective action
reproduces the bilocal reformulation of the model without using replicas. In
general tensor field theories the 2PI formalism is the only way to obtain a
bilocal re... | hep-th gr-qc | we discuss the twoparticle irreducible 2pi effective action for the syk model and for tensor field theories for the syk model the 2pi effective action reproduces the bilocal reformulation of the model without using replicas in general tensor field theories the 2pi formalism is the only way to obtain a bilocal reformula... | [['we', 'discuss', 'the', 'twoparticle', 'irreducible', '2pi', 'effective', 'action', 'for', 'the', 'syk', 'model', 'and', 'for', 'tensor', 'field', 'theories', 'for', 'the', 'syk', 'model', 'the', '2pi', 'effective', 'action', 'reproduces', 'the', 'bilocal', 'reformulation', 'of', 'the', 'model', 'without', 'using', '... | [-0.13766487166708843, 0.13874302345277761, -0.10102843762036752, 0.08663482685700398, -0.0698083452203057, -0.12200676802630452, -0.010147094638721849, 0.30034321565181016, -0.20298718782988462, -0.2753942933441563, 0.03944738144478337, -0.2849613901227713, -0.20336413509635762, 0.1261913935145871, 0.00101824802007864... |
1,802.05501 | Finding small-width connected path decompositions in polynomial time | A connected path decomposition of a simple graph $G$ is a path decomposition
$(X_1,\ldots,X_l)$ such that the subgraph of $G$ induced by $X_1\cup\cdots\cup
X_i$ is connected for each $i\in\{1,\ldots,l\}$. The connected pathwidth of $G$
is then the minimum width over all connected path decompositions of $G$. We
prove ... | cs.DS cs.CC cs.DM | a connected path decomposition of a simple graph g is a path decomposition x_1ldotsx_l such that the subgraph of g induced by x_1cupcdotscup x_i is connected for each iin1ldotsl the connected pathwidth of g is then the minimum width over all connected path decompositions of g we prove that for each fixed k the connecte... | [['a', 'connected', 'path', 'decomposition', 'of', 'a', 'simple', 'graph', 'g', 'is', 'a', 'path', 'decomposition', 'x_1ldotsx_l', 'such', 'that', 'the', 'subgraph', 'of', 'g', 'induced', 'by', 'x_1cupcdotscup', 'x_i', 'is', 'connected', 'for', 'each', 'iin1ldotsl', 'the', 'connected', 'pathwidth', 'of', 'g', 'is', 'th... | [-0.20956373238522147, 0.13965495019365334, -0.038144713567776815, -0.028380908601037744, -0.16900133040681894, -0.19148391113202606, 0.07546530808839533, 0.42004396291190965, -0.35721520497981046, -0.28757210050502585, 0.0796574427629821, -0.26680308253400853, -0.14964796538050804, 0.11807917128058357, -0.131357879786... |
1,802.05502 | Sharp Lower Bounds for the First Eigenvalues of the Bi-Laplace Operator | We obtain sharp lower bounds for the first eigenvalue of four types of
eigenvalue problem defined by the bi-Laplace operator on compact manifolds with
boundary and determine all the eigenvalues and the corresponding eigenfunctions
of a Wentzell-type bi-Laplace problem on Euclidean balls.
| math.AP | we obtain sharp lower bounds for the first eigenvalue of four types of eigenvalue problem defined by the bilaplace operator on compact manifolds with boundary and determine all the eigenvalues and the corresponding eigenfunctions of a wentzelltype bilaplace problem on euclidean balls | [['we', 'obtain', 'sharp', 'lower', 'bounds', 'for', 'the', 'first', 'eigenvalue', 'of', 'four', 'types', 'of', 'eigenvalue', 'problem', 'defined', 'by', 'the', 'bilaplace', 'operator', 'on', 'compact', 'manifolds', 'with', 'boundary', 'and', 'determine', 'all', 'the', 'eigenvalues', 'and', 'the', 'corresponding', 'eig... | [-0.12511859318086258, 0.04991964879168552, -0.030272489003393622, 0.09576221491165814, -0.06486972942504854, -0.10299677323062151, 0.0048996613671382265, 0.2848629044989745, -0.2058864470039095, -0.2628001691773534, 0.19694194351766436, -0.32932520205421106, -0.11952078609084267, 0.19691068889750613, -0.06977291496115... |
1,802.05503 | Energy cascade rate in isothermal compressible magnetohydrodynamic
turbulence | Three-dimensional direct numerical simulations are used to study the energy
cascade rate in isothermal compressible magnetohydrodynamic turbulence. Our
analysis is guided by a two-point exact law derived recently for this problem
in which flux, source, hybrid, and mixed terms are present. The relative
importance of e... | physics.plasm-ph astro-ph.EP physics.space-ph | threedimensional direct numerical simulations are used to study the energy cascade rate in isothermal compressible magnetohydrodynamic turbulence our analysis is guided by a twopoint exact law derived recently for this problem in which flux source hybrid and mixed terms are present the relative importance of each term ... | [['threedimensional', 'direct', 'numerical', 'simulations', 'are', 'used', 'to', 'study', 'the', 'energy', 'cascade', 'rate', 'in', 'isothermal', 'compressible', 'magnetohydrodynamic', 'turbulence', 'our', 'analysis', 'is', 'guided', 'by', 'a', 'twopoint', 'exact', 'law', 'derived', 'recently', 'for', 'this', 'problem'... | [-0.1487738492009078, 0.15396171409536138, -0.015560444796194686, 0.030669074232560968, -0.0746732026581531, -0.06532811138616956, -0.033102918639601936, 0.3330973053639552, -0.2514069816806232, -0.32734868748356466, 0.0874960918135121, -0.21956414694938323, -0.07293753595719032, 0.23517664283028114, 0.0152601419300164... |
1,802.05504 | The spectral dimension controls the decay of the quantum first detection
probability | We consider a quantum system that is initially localized at $x_{in}$ and that
is repeatedly projectively probed with a fixed period $\tau$ at position $x_d$.
We ask for the probability that the system is detected in $x_d$ for the very
first time, $F_n$, where $n$ is the number of detection attempts. We relate the
asy... | cond-mat.stat-mech quant-ph | we consider a quantum system that is initially localized at x_in and that is repeatedly projectively probed with a fixed period tau at position x_d we ask for the probability that the system is detected in x_d for the very first time f_n where n is the number of detection attempts we relate the asymptotic decay and osc... | [['we', 'consider', 'a', 'quantum', 'system', 'that', 'is', 'initially', 'localized', 'at', 'x_in', 'and', 'that', 'is', 'repeatedly', 'projectively', 'probed', 'with', 'a', 'fixed', 'period', 'tau', 'at', 'position', 'x_d', 'we', 'ask', 'for', 'the', 'probability', 'that', 'the', 'system', 'is', 'detected', 'in', 'x_d... | [-0.14156702169845492, 0.18482586193435777, -0.10721694650673683, 0.047341620122171836, 0.0030973483158485988, -0.13246990562646255, 0.03188293686013809, 0.3280537474760148, -0.2549402917167555, -0.25361151926614955, 0.07265793029155122, -0.31333910089437866, -0.13107360875607174, 0.1877651561787376, -0.024041712847027... |
1,802.05505 | Quantum state engineering with a trapped atom and a set of static
impurities | Hybrid systems of ultracold atoms and trapped ions or Rydberg atoms can be
useful for quantum simulation purposes. By tuning the geometric arrangement of
the impurities it is possible to mimic solid state and molecular systems. Here
we study a single trapped atom interacting with a set of arbitrarily arranged
static ... | quant-ph cond-mat.quant-gas physics.atom-ph | hybrid systems of ultracold atoms and trapped ions or rydberg atoms can be useful for quantum simulation purposes by tuning the geometric arrangement of the impurities it is possible to mimic solid state and molecular systems here we study a single trapped atom interacting with a set of arbitrarily arranged static impu... | [['hybrid', 'systems', 'of', 'ultracold', 'atoms', 'and', 'trapped', 'ions', 'or', 'rydberg', 'atoms', 'can', 'be', 'useful', 'for', 'quantum', 'simulation', 'purposes', 'by', 'tuning', 'the', 'geometric', 'arrangement', 'of', 'the', 'impurities', 'it', 'is', 'possible', 'to', 'mimic', 'solid', 'state', 'and', 'molecul... | [-0.14610697565235428, 0.1815737263437843, -0.022611293298451556, 0.03749477200854579, 0.04519975527439305, -0.2028841960397501, 0.0463452704740477, 0.37548972101709277, -0.2347357933668746, -0.2768813881869476, 0.03742667078160556, -0.29624982573783276, -0.12058921251205977, 0.19942188925186613, 0.028283376858171227, ... |
1,802.05506 | Universal Super Vector Bundles | A new generalization of Grassmannians, called {\nu}-grassmannians, and a
canonical super vector bundle over this new space, say {\Gamma}, are
introduced. Then, constructing a Gauss supermap of a super vector bundle, the
universal property of {\Gamma} is discussed. Finally, we generalize one of the
main theorems of ho... | math.DG | a new generalization of grassmannians called nugrassmannians and a canonical super vector bundle over this new space say gamma are introduced then constructing a gauss supermap of a super vector bundle the universal property of gamma is discussed finally we generalize one of the main theorems of homotopy classification... | [['a', 'new', 'generalization', 'of', 'grassmannians', 'called', 'nugrassmannians', 'and', 'a', 'canonical', 'super', 'vector', 'bundle', 'over', 'this', 'new', 'space', 'say', 'gamma', 'are', 'introduced', 'then', 'constructing', 'a', 'gauss', 'supermap', 'of', 'a', 'super', 'vector', 'bundle', 'the', 'universal', 'pr... | [-0.16121493548787427, 0.12552617166415383, -0.06815643366074788, 0.10026331184396767, -0.1533191795197298, -0.1509860515383617, 0.008087509294163506, 0.33087056411324806, -0.3197488198583981, -0.11225861079171563, 0.07376349211081792, -0.1864426296274617, -0.2147573774926505, 0.20274054076311723, -0.15983786777030887,... |
1,802.05507 | Surfaces in Laguerre Geometry | This exposition gives an introduction to the theory of surfaces in Laguerre
geometry and surveys some results, mostly obtained by the authors, about three
important classes of surfaces in Laguerre geometry, namely L-isothermic,
L-minimal, and generalized L-minimal surfaces. The quadric model of Lie sphere
geometry is... | math.DG | this exposition gives an introduction to the theory of surfaces in laguerre geometry and surveys some results mostly obtained by the authors about three important classes of surfaces in laguerre geometry namely lisothermic lminimal and generalized lminimal surfaces the quadric model of lie sphere geometry is adopted fo... | [['this', 'exposition', 'gives', 'an', 'introduction', 'to', 'the', 'theory', 'of', 'surfaces', 'in', 'laguerre', 'geometry', 'and', 'surveys', 'some', 'results', 'mostly', 'obtained', 'by', 'the', 'authors', 'about', 'three', 'important', 'classes', 'of', 'surfaces', 'in', 'laguerre', 'geometry', 'namely', 'lisothermi... | [-0.11380621973241604, 0.021045651428217075, -0.0943905905392157, 0.048654117541605216, -0.060195072302526804, -0.11728875030743054, -0.040718122069548855, 0.3068325203999768, -0.23042796397527313, -0.302009625550713, 0.12132342962758874, -0.28259264460907585, -0.18893904962583724, 0.23190757948191443, -0.1689011455058... |
1,802.05508 | NNLO classical solution for Lipatov's effective action for reggeized
gluons | We consider the formalism of small-x effective action for reggeized gluons,
Gribov (Sov Phys JETP 26:414, 1968), Lipatov (Nucl Phys B 452:369, 1995; Phys
Rep 286:131, 1997; Subnucl Ser 49:131, 2013, Int J Mod Phys Conf Ser
39:1560082, 2015; Int J Mod Phys A 31(28/29):1645011, 2016; EPJ Web Conf
125:01010, 2016) and L... | hep-ph | we consider the formalism of smallx effective action for reggeized gluons gribov sov phys jetp 26414 1968 lipatov nucl phys b 452369 1995 phys rep 286131 1997 subnucl ser 49131 2013 int j mod phys conf ser 391560082 2015 int j mod phys a 3128291645011 2016 epj web conf 12501010 2016 and lipatov et al sov j nucl phys 23... | [['we', 'consider', 'the', 'formalism', 'of', 'smallx', 'effective', 'action', 'for', 'reggeized', 'gluons', 'gribov', 'sov', 'phys', 'jetp', '26414', '1968', 'lipatov', 'nucl', 'phys', 'b', '452369', '1995', 'phys', 'rep', '286131', '1997', 'subnucl', 'ser', '49131', '2013', 'int', 'j', 'mod', 'phys', 'conf', 'ser', '... | [-0.06133215511905267, 0.04835830797322545, -0.0601854324965869, -0.13785890860001762, -0.09111726741562753, -0.08170582017792552, 0.09115707513019942, 0.22460499587125027, -0.05085707809026009, -0.37480244808361535, -0.09697568717165757, -0.2505948471653333, -0.15356846271245272, 0.12494830884064403, -0.21013254514151... |
1,802.05509 | On the thin film Muskat and the thin film Stokes equations | The present paper is concerned with the analysis of two strongly coupled
systems of degenerate parabolic partial differential equations arising in
multiphase thin film flows. In particular, we consider the two-phase thin film
Muskat problem and the two-phase thin film approximation of the Stokes flow
under the influe... | math.AP | the present paper is concerned with the analysis of two strongly coupled systems of degenerate parabolic partial differential equations arising in multiphase thin film flows in particular we consider the twophase thin film muskat problem and the twophase thin film approximation of the stokes flow under the influence of... | [['the', 'present', 'paper', 'is', 'concerned', 'with', 'the', 'analysis', 'of', 'two', 'strongly', 'coupled', 'systems', 'of', 'degenerate', 'parabolic', 'partial', 'differential', 'equations', 'arising', 'in', 'multiphase', 'thin', 'film', 'flows', 'in', 'particular', 'we', 'consider', 'the', 'twophase', 'thin', 'fil... | [-0.15348662483296868, 0.10862899255806267, -0.06682513042074377, 0.06083849751489087, -0.06963946969574657, -0.11316553420679522, -0.026873815023802546, 0.3269817158154953, -0.32520380277648897, -0.23210414004236812, 0.16473858023103136, -0.26582798505555433, -0.0654946749887164, 0.18770649047554844, -0.03532652642504... |
1,802.0551 | Neutron star equation of state from the quark level in the light of
GW170817 | Matter state inside neutron stars is an exciting problem in astrophysics,
nuclear physics and particle physics. The equation of state (EOS) of neutron
stars plays a crucial role in the present multimessenger astronomy, especially
after the event of GW170817. We propose a new neutron star EOS "QMF18" from the
quark le... | nucl-th astro-ph.HE astro-ph.SR | matter state inside neutron stars is an exciting problem in astrophysics nuclear physics and particle physics the equation of state eos of neutron stars plays a crucial role in the present multimessenger astronomy especially after the event of gw170817 we propose a new neutron star eos qmf18 from the quark level which ... | [['matter', 'state', 'inside', 'neutron', 'stars', 'is', 'an', 'exciting', 'problem', 'in', 'astrophysics', 'nuclear', 'physics', 'and', 'particle', 'physics', 'the', 'equation', 'of', 'state', 'eos', 'of', 'neutron', 'stars', 'plays', 'a', 'crucial', 'role', 'in', 'the', 'present', 'multimessenger', 'astronomy', 'espe... | [-0.07066712746514923, 0.19232190797017196, -0.1482088187827714, 0.12059634454577925, -0.17432438451538068, -0.05526897150077044, 0.03528863830041022, 0.2876829533645558, -0.2071605764536394, -0.365792006860295, 0.016920264701299842, -0.2905833263671772, -0.035960460377354474, 0.19443122501806578, 0.0466163676668195, 0... |
1,802.05511 | Charge Symmetry Breaking Effects in Pion and Kaon Structure | Charge symmetry breaking (CSB) effects associated with the $u$ and $d$ quark
mass difference are investigated in the quark distribution functions and
spacelike electromagnetic form factors of the pion and kaon. We use a confining
version of the Nambu--Jona-Lasinio model, where CSB effects at the infrared
scale associ... | nucl-th hep-ph | charge symmetry breaking csb effects associated with the u and d quark mass difference are investigated in the quark distribution functions and spacelike electromagnetic form factors of the pion and kaon we use a confining version of the nambujonalasinio model where csb effects at the infrared scale associated with the... | [['charge', 'symmetry', 'breaking', 'csb', 'effects', 'associated', 'with', 'the', 'u', 'and', 'd', 'quark', 'mass', 'difference', 'are', 'investigated', 'in', 'the', 'quark', 'distribution', 'functions', 'and', 'spacelike', 'electromagnetic', 'form', 'factors', 'of', 'the', 'pion', 'and', 'kaon', 'we', 'use', 'a', 'co... | [-0.10853357113852066, 0.2999128119720678, -0.054632868813184486, 0.13944401928737143, -0.04554252326904264, -0.08833527604916266, 0.07365703912884262, 0.3162683666263807, -0.1585980762735874, -0.2716590270408363, -0.029863735473814552, -0.3264454357267823, -0.019684157354017122, 0.08080193560142236, 0.1071703767156577... |
1,802.05512 | Intriguing X-ray and optical variations of the gamma Cas analog HD45314 | A growing number of Be and Oe stars, named the gamma Cas stars, are known for
their unusually hard and intense X-ray emission. This emission could either
trace accretion by a compact companion or magnetic interaction between the star
and its decretion disk. To test these scenarios, we carried out a detailed
optical m... | astro-ph.SR astro-ph.HE | a growing number of be and oe stars named the gamma cas stars are known for their unusually hard and intense xray emission this emission could either trace accretion by a compact companion or magnetic interaction between the star and its decretion disk to test these scenarios we carried out a detailed optical monitorin... | [['a', 'growing', 'number', 'of', 'be', 'and', 'oe', 'stars', 'named', 'the', 'gamma', 'cas', 'stars', 'are', 'known', 'for', 'their', 'unusually', 'hard', 'and', 'intense', 'xray', 'emission', 'this', 'emission', 'could', 'either', 'trace', 'accretion', 'by', 'a', 'compact', 'companion', 'or', 'magnetic', 'interaction... | [-0.08970580335191794, 0.12828587111097908, -0.050495300946446754, 0.07401858088958665, -0.10144460520486494, -0.09308712857187186, 0.0539168608349364, 0.472924055070938, -0.22124627815240897, -0.3475471272954325, 0.09028974521176056, -0.29921912782613125, -0.013905290674557093, 0.1987996678074348, 0.00782724909623268,... |
1,802.05513 | Extreme points of Gram spectrahedra of binary forms | The Gram spectrahedron $\text{Gram}(f)$ of a form $f$ with real coefficients
parametrizes the sum of squares decompositions of $f$, modulo orthogonal
equivalence. For $f$ a sufficiently general positive binary form of arbitrary
degree, we show that $\text{Gram}(f)$ has extreme points of all ranks in the
Pataki range.... | math.OC math.CO | the gram spectrahedron textgramf of a form f with real coefficients parametrizes the sum of squares decompositions of f modulo orthogonal equivalence for f a sufficiently general positive binary form of arbitrary degree we show that textgramf has extreme points of all ranks in the pataki range this is the first example... | [['the', 'gram', 'spectrahedron', 'textgramf', 'of', 'a', 'form', 'f', 'with', 'real', 'coefficients', 'parametrizes', 'the', 'sum', 'of', 'squares', 'decompositions', 'of', 'f', 'modulo', 'orthogonal', 'equivalence', 'for', 'f', 'a', 'sufficiently', 'general', 'positive', 'binary', 'form', 'of', 'arbitrary', 'degree',... | [-0.2010724377440344, 0.0909655127585877, -0.025031980908577247, 0.008268925172304459, -0.01912736738709235, -0.12458279445343236, 0.022156603394611046, 0.31671312325956796, -0.26391921537273594, -0.21707891169382204, 0.09899443899175281, -0.27849998032803286, -0.15316155544795687, 0.15898486730264555, -0.0297773663158... |
1,802.05514 | Experimental and theoretical study of the B(2)$^2 \Sigma^+ \rightarrow$
X(1)$^2 \Sigma^+$ system in the KSr molecule | Spectral bands for the B(2)$^{2}\Sigma^{+}\rightarrow$ X(1)$^{2}\Sigma^{+}$
electronic transition in the doubly-polar open-shell KSr molecule are recorded
at moderate resolution using the thermoluminescence technique. The spectra are
simulated using three kinds of advanced electronic structure calculations,
allowing ... | physics.atom-ph physics.chem-ph | spectral bands for the b22sigmarightarrow x12sigma electronic transition in the doublypolar openshell ksr molecule are recorded at moderate resolution using the thermoluminescence technique the spectra are simulated using three kinds of advanced electronic structure calculations allowing for an assessment of their accu... | [['spectral', 'bands', 'for', 'the', 'b22sigmarightarrow', 'x12sigma', 'electronic', 'transition', 'in', 'the', 'doublypolar', 'openshell', 'ksr', 'molecule', 'are', 'recorded', 'at', 'moderate', 'resolution', 'using', 'the', 'thermoluminescence', 'technique', 'the', 'spectra', 'are', 'simulated', 'using', 'three', 'ki... | [-0.08635734098895294, 0.1363018338382883, -0.040488037530605384, 0.03434520347963837, 0.005826735392031147, -0.13977875863769795, 0.07112674347391897, 0.3981390555684523, -0.16394011117517948, -0.3167856881258691, 0.06992061865351322, -0.3400300599680078, -0.032601431980388375, 0.209238770559839, 0.10594843968567325, ... |
1,802.05515 | Equation for the Nakanishi weight function using the inverse Stieltjes
transform | The bound state Bethe-Salpeter amplitude was expressed by Nakanishi in terms
of a smooth weight function g. By using the generalized Stieltjes transform, we
derive an integral equation for the Nakanishi function g for a bound state
case. It has the standard form g= Vg, where V is a two-dimensional integral
operator. ... | hep-ph nucl-th | the bound state bethesalpeter amplitude was expressed by nakanishi in terms of a smooth weight function g by using the generalized stieltjes transform we derive an integral equation for the nakanishi function g for a bound state case it has the standard form g vg where v is a twodimensional integral operator the prescr... | [['the', 'bound', 'state', 'bethesalpeter', 'amplitude', 'was', 'expressed', 'by', 'nakanishi', 'in', 'terms', 'of', 'a', 'smooth', 'weight', 'function', 'g', 'by', 'using', 'the', 'generalized', 'stieltjes', 'transform', 'we', 'derive', 'an', 'integral', 'equation', 'for', 'the', 'nakanishi', 'function', 'g', 'for', '... | [-0.14935259018093347, 0.05924433335923303, -0.1347888340874176, 0.03775435355159321, -0.11105114207603037, -0.10520040780705, 0.038177777953179816, 0.3154538848038231, -0.2588511394303558, -0.24392419976315327, 0.030435856563105646, -0.2855307453578072, -0.1452552082283156, 0.15799204499926417, 0.02235653635912708, 0.... |
1,802.05516 | A characterization of BMO in terms of endpoint bounds for commutators of
singular integrals | We provide a characterization of $\mathrm{BMO}$ in terms of endpoint
boundedness of commutators of singular integrals. In particular, in one
dimension, we show that $\|b\|_{\mathrm{BMO}}\eqsim B$, where $B$ is the best
constant in the endpoint $L\log L$ modular estimate for the commutator $[H,b]$.
We provide a simila... | math.CA | we provide a characterization of mathrmbmo in terms of endpoint boundedness of commutators of singular integrals in particular in one dimension we show that b_mathrmbmoeqsim b where b is the best constant in the endpoint llog l modular estimate for the commutator hb we provide a similar characterization of the space ma... | [['we', 'provide', 'a', 'characterization', 'of', 'mathrmbmo', 'in', 'terms', 'of', 'endpoint', 'boundedness', 'of', 'commutators', 'of', 'singular', 'integrals', 'in', 'particular', 'in', 'one', 'dimension', 'we', 'show', 'that', 'b_mathrmbmoeqsim', 'b', 'where', 'b', 'is', 'the', 'best', 'constant', 'in', 'the', 'end... | [-0.1412522274256623, 0.08828482972610324, -0.05545831062595978, 0.10006756830425219, -0.08604981821839845, -0.0246956965616234, 0.006560393356692011, 0.3114344795521732, -0.2683377606080514, -0.16652709884551642, 0.13725747701181013, -0.2789416654366199, -0.13687134158817146, 0.20970144020132372, -0.10875217839379177,... |
1,802.05517 | Quantum cryptography: key distribution and beyond | Uniquely among the sciences, quantum cryptography has driven both
foundational research as well as practical real-life applications. We review
the progress of quantum cryptography in the last decade, covering quantum key
distribution and other applications.
| quant-ph physics.app-ph | uniquely among the sciences quantum cryptography has driven both foundational research as well as practical reallife applications we review the progress of quantum cryptography in the last decade covering quantum key distribution and other applications | [['uniquely', 'among', 'the', 'sciences', 'quantum', 'cryptography', 'has', 'driven', 'both', 'foundational', 'research', 'as', 'well', 'as', 'practical', 'reallife', 'applications', 'we', 'review', 'the', 'progress', 'of', 'quantum', 'cryptography', 'in', 'the', 'last', 'decade', 'covering', 'quantum', 'key', 'distrib... | [-0.078199003636837, 0.08069185332528182, -0.04535220664526735, 0.009882909006306104, -0.06928239043003746, -0.1921091935464314, -0.04913168385890978, 0.3584721299154418, -0.3334557448114668, -0.3209525371236461, 0.15356155372823455, -0.2560100667710815, -0.2469966639897653, 0.35663225996707165, -0.1430872157216072, 0.... |
1,802.05518 | Learning from a Handful Volumes: MRI Resolution Enhancement with
Volumetric Super-Resolution Forests | Magnetic resonance imaging (MRI) enables 3-D imaging of anatomical
structures. However, the acquisition of MR volumes with high spatial resolution
leads to long scan times. To this end, we propose volumetric super-resolution
forests (VSRF) to enhance MRI resolution retrospectively. Our method learns a
locally linear ... | cs.CV | magnetic resonance imaging mri enables 3d imaging of anatomical structures however the acquisition of mr volumes with high spatial resolution leads to long scan times to this end we propose volumetric superresolution forests vsrf to enhance mri resolution retrospectively our method learns a locally linear mapping betwe... | [['magnetic', 'resonance', 'imaging', 'mri', 'enables', '3d', 'imaging', 'of', 'anatomical', 'structures', 'however', 'the', 'acquisition', 'of', 'mr', 'volumes', 'with', 'high', 'spatial', 'resolution', 'leads', 'to', 'long', 'scan', 'times', 'to', 'this', 'end', 'we', 'propose', 'volumetric', 'superresolution', 'fore... | [0.021590459089473647, -0.0015077371529098283, -0.030626106099620208, 0.05916803928439395, -0.12164189757274116, -0.17607093967449994, -0.005044083259960289, 0.4977132395478123, -0.28908258415285054, -0.3290635671893774, 0.09592600976081439, -0.25399858038083223, -0.14006011389487943, 0.17264646509172932, -0.1465511445... |
1,802.05519 | Thin film flow dynamics on fiber nets | We analyze existence and qualitative behavior of non-negative weak solutions
for fourth order degenerate parabolic equations on graph domains with
Kirchhoff's boundary conditions at the inner nodes and Neumann boundary
conditions at the boundary nodes. The problem is originated from industrial
constructions of spray ... | math.AP | we analyze existence and qualitative behavior of nonnegative weak solutions for fourth order degenerate parabolic equations on graph domains with kirchhoffs boundary conditions at the inner nodes and neumann boundary conditions at the boundary nodes the problem is originated from industrial constructions of spray coate... | [['we', 'analyze', 'existence', 'and', 'qualitative', 'behavior', 'of', 'nonnegative', 'weak', 'solutions', 'for', 'fourth', 'order', 'degenerate', 'parabolic', 'equations', 'on', 'graph', 'domains', 'with', 'kirchhoffs', 'boundary', 'conditions', 'at', 'the', 'inner', 'nodes', 'and', 'neumann', 'boundary', 'conditions... | [-0.1665364055883228, 0.0958857103140049, -0.06611027027524653, -0.016022388605744623, -0.0675721087082777, -0.1421234707869146, 0.017177053541499412, 0.3554497210369889, -0.2824824878591157, -0.24605384379503362, 0.15475476382111775, -0.29717434879525434, -0.05939921406319454, 0.16525569114656674, -0.07447965286805161... |
1,802.0552 | Cumulative displacement induced by a magnetosonic soliton bouncing in a
bounded plasma slab | The passage of a magnetosonic (MS) soliton in a cold plasma leads to the
displacement of charged particles in the direction of a compressive pulse and
in the opposite direction of a rarefaction pulse. In the overdense plasma
limit, the displacement induced by a weakly nonlinear MS soliton is derived
analytically. Thi... | physics.plasm-ph | the passage of a magnetosonic ms soliton in a cold plasma leads to the displacement of charged particles in the direction of a compressive pulse and in the opposite direction of a rarefaction pulse in the overdense plasma limit the displacement induced by a weakly nonlinear ms soliton is derived analytically this resul... | [['the', 'passage', 'of', 'a', 'magnetosonic', 'ms', 'soliton', 'in', 'a', 'cold', 'plasma', 'leads', 'to', 'the', 'displacement', 'of', 'charged', 'particles', 'in', 'the', 'direction', 'of', 'a', 'compressive', 'pulse', 'and', 'in', 'the', 'opposite', 'direction', 'of', 'a', 'rarefaction', 'pulse', 'in', 'the', 'over... | [-0.1342842687229906, 0.22670889368038946, -0.11353499031572686, 0.023437072068634556, -0.027886085000222292, -0.058474768901516386, -0.013056763109932767, 0.4072670821645638, -0.27361131207903894, -0.2365920401019294, 0.05499521735203793, -0.23356699340170387, -0.02610109948999877, 0.20344595939140556, -0.004768364220... |
1,802.05521 | Deep Learning for Lip Reading using Audio-Visual Information for Urdu
Language | Human lip-reading is a challenging task. It requires not only knowledge of
underlying language but also visual clues to predict spoken words. Experts need
certain level of experience and understanding of visual expressions learning to
decode spoken words. Now-a-days, with the help of deep learning it is possible
to t... | cs.CV cs.SD eess.AS | human lipreading is a challenging task it requires not only knowledge of underlying language but also visual clues to predict spoken words experts need certain level of experience and understanding of visual expressions learning to decode spoken words nowadays with the help of deep learning it is possible to translate ... | [['human', 'lipreading', 'is', 'a', 'challenging', 'task', 'it', 'requires', 'not', 'only', 'knowledge', 'of', 'underlying', 'language', 'but', 'also', 'visual', 'clues', 'to', 'predict', 'spoken', 'words', 'experts', 'need', 'certain', 'level', 'of', 'experience', 'and', 'understanding', 'of', 'visual', 'expressions',... | [-0.008916652813974408, 0.01038510093405362, -0.05823986398717088, 0.10867077483224773, -0.17101121238402783, -0.20630491655620356, 0.013023109192163833, 0.4794840996724463, -0.3068403293108267, -0.3198212149169957, 0.04607572202916227, -0.28984204677023717, -0.2241418017438733, 0.17755003716578827, -0.1849546302109956... |
1,802.05522 | Unsupervised Learning of Depth and Ego-Motion from Monocular Video Using
3D Geometric Constraints | We present a novel approach for unsupervised learning of depth and ego-motion
from monocular video. Unsupervised learning removes the need for separate
supervisory signals (depth or ego-motion ground truth, or multi-view video).
Prior work in unsupervised depth learning uses pixel-wise or gradient-based
losses, which... | cs.CV | we present a novel approach for unsupervised learning of depth and egomotion from monocular video unsupervised learning removes the need for separate supervisory signals depth or egomotion ground truth or multiview video prior work in unsupervised depth learning uses pixelwise or gradientbased losses which only conside... | [['we', 'present', 'a', 'novel', 'approach', 'for', 'unsupervised', 'learning', 'of', 'depth', 'and', 'egomotion', 'from', 'monocular', 'video', 'unsupervised', 'learning', 'removes', 'the', 'need', 'for', 'separate', 'supervisory', 'signals', 'depth', 'or', 'egomotion', 'ground', 'truth', 'or', 'multiview', 'video', '... | [-0.024308707707413387, -0.02129478878599581, -0.040741016093207606, 0.04346731169233945, -0.10729529842501506, -0.1674677159446715, 0.03825398995011876, 0.5052916173696179, -0.24016317874404855, -0.36561793868683956, 0.06346498023432849, -0.28424911405044523, -0.1554494036911902, 0.20122287055921995, -0.21443743133832... |
1,802.05523 | Scalar Casimir densities and forces for parallel plates in cosmic string
spacetime | We analyze the Casimir densities and forces associated with a massive scalar
quantum field confined between two parallel plates in a D-dimensional cosmic
string spacetime. The plates are placed orthogonal to the string and the field
obeys the Robin boundary conditions on them. The boundary-induced contributions
are e... | hep-th gr-qc | we analyze the casimir densities and forces associated with a massive scalar quantum field confined between two parallel plates in a ddimensional cosmic string spacetime the plates are placed orthogonal to the string and the field obeys the robin boundary conditions on them the boundaryinduced contributions are explici... | [['we', 'analyze', 'the', 'casimir', 'densities', 'and', 'forces', 'associated', 'with', 'a', 'massive', 'scalar', 'quantum', 'field', 'confined', 'between', 'two', 'parallel', 'plates', 'in', 'a', 'ddimensional', 'cosmic', 'string', 'spacetime', 'the', 'plates', 'are', 'placed', 'orthogonal', 'to', 'the', 'string', 'a... | [-0.19872581111970553, 0.20431468520135038, -0.06336898876130369, 0.030670828140298707, -0.10691271363369499, -0.0975134672981868, -0.06611219639065287, 0.3230041732693078, -0.24311345688288888, -0.20145991018054904, 0.08410016318602073, -0.2963780846855823, -0.05904617820892276, 0.14386996487600198, -0.009675896095965... |
1,802.05524 | Metallicity Distribution of Disk Stars and the Formation History of the
Milky Way | We investigate the formation history of the stellar disk component in the
Milky Way (MW) based on our new chemical evolution model. Our model considers
several fundamental baryonic processes, including gas infall, re-accretion of
outflowing gas, and radial migration of disk stars. Each of these baryonic
processes in ... | astro-ph.GA | we investigate the formation history of the stellar disk component in the milky way mw based on our new chemical evolution model our model considers several fundamental baryonic processes including gas infall reaccretion of outflowing gas and radial migration of disk stars each of these baryonic processes in the disk e... | [['we', 'investigate', 'the', 'formation', 'history', 'of', 'the', 'stellar', 'disk', 'component', 'in', 'the', 'milky', 'way', 'mw', 'based', 'on', 'our', 'new', 'chemical', 'evolution', 'model', 'our', 'model', 'considers', 'several', 'fundamental', 'baryonic', 'processes', 'including', 'gas', 'infall', 'reaccretion'... | [-0.03276073740440139, 0.07952802434285805, -0.09614269772129712, 0.09455270788459086, -0.08987032346713099, -0.009487140681125036, 0.015243021868161481, 0.36689698610830457, -0.22156590786410355, -0.32324054397783486, 0.017241618202748794, -0.23731595943407977, -0.03923265903713324, 0.2208895531400819, 0.0057031324779... |
1,802.05525 | A misaligned magneto-optical trap to enable miniaturized atom chip
systems | We describe the application of displaced, or misaligned, beams in a
mirror-based magneto-optical trap (MOT) to enable portable and miniaturized
atom chip experiments, where optical access is limited to a single window. Two
different geometries of beam displacement are investigated: a variation on the
well-known 'vort... | physics.atom-ph | we describe the application of displaced or misaligned beams in a mirrorbased magnetooptical trap mot to enable portable and miniaturized atom chip experiments where optical access is limited to a single window two different geometries of beam displacement are investigated a variation on the wellknown vortexmot and the... | [['we', 'describe', 'the', 'application', 'of', 'displaced', 'or', 'misaligned', 'beams', 'in', 'a', 'mirrorbased', 'magnetooptical', 'trap', 'mot', 'to', 'enable', 'portable', 'and', 'miniaturized', 'atom', 'chip', 'experiments', 'where', 'optical', 'access', 'is', 'limited', 'to', 'a', 'single', 'window', 'two', 'dif... | [-0.10066641449272383, 0.20117949154909429, -0.026081945424865385, -0.00924995145334567, -0.015657541804901528, -0.19195719107860562, 0.0424670157599172, 0.4108548143469706, -0.2133795708877875, -0.30449144462714106, 0.07396096898890214, -0.2757265581295076, -0.023649355761491034, 0.26172709615372985, -0.02259584039126... |
1,802.05526 | The Next Generation Virgo Cluster Survey (NGVS). XVIII. Measurement and
Calibration of Surface Brightness Fluctuation Distances for Bright Galaxies
in Virgo (and Beyond) | We describe a program to measure surface brightness fluctuation (SBF)
distances to galaxies observed in the Next Generation Virgo Cluster Survey
(NGVS), a photometric imaging survey covering $104~deg^2$ of the Virgo cluster
in the ${u}^*,g,i,z$ bandpasses with the Canada-France Hawaii Telescope. We
describe the selec... | astro-ph.GA | we describe a program to measure surface brightness fluctuation sbf distances to galaxies observed in the next generation virgo cluster survey ngvs a photometric imaging survey covering 104deg2 of the virgo cluster in the ugiz bandpasses with the canadafrance hawaii telescope we describe the selection of the sample gal... | [['we', 'describe', 'a', 'program', 'to', 'measure', 'surface', 'brightness', 'fluctuation', 'sbf', 'distances', 'to', 'galaxies', 'observed', 'in', 'the', 'next', 'generation', 'virgo', 'cluster', 'survey', 'ngvs', 'a', 'photometric', 'imaging', 'survey', 'covering', '104deg2', 'of', 'the', 'virgo', 'cluster', 'in', '... | [-0.04214716765866615, 0.049434746078331954, -0.09709435703232884, 0.08912122391769663, -0.0850118015180342, -0.025932894913479686, 0.07208839641138912, 0.44860647010803223, -0.14715917795524, -0.37777102254633793, 0.05711895579751581, -0.32443882101774213, -0.03193100140430033, 0.2198201055203099, -0.07735524521116167... |
1,802.05527 | Singular control and optimal stopping of memory mean-field processes | The purpose of this paper is to study the following topics and the relation
between them: (i) Optimal singular control of mean-field stochastic
differential equations with memory, (ii) reflected advanced mean-field backward
stochastic differential equations, and (iii) optimal stopping of mean-field
stochastic differe... | math.OC | the purpose of this paper is to study the following topics and the relation between them i optimal singular control of meanfield stochastic differential equations with memory ii reflected advanced meanfield backward stochastic differential equations and iii optimal stopping of meanfield stochastic differential equation... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'study', 'the', 'following', 'topics', 'and', 'the', 'relation', 'between', 'them', 'i', 'optimal', 'singular', 'control', 'of', 'meanfield', 'stochastic', 'differential', 'equations', 'with', 'memory', 'ii', 'reflected', 'advanced', 'meanfield', 'backward', 'stoch... | [-0.16284427129021087, 0.034960395907816105, -0.09941998118948606, 0.14025052830025, -0.13284424354141164, -0.16682906425126862, 0.04548049208824523, 0.2801162418219502, -0.368133630776019, -0.24838300294208307, 0.13742733366476992, -0.284240084316547, -0.1771112424450823, 0.1384645557921397, -0.08105946037728616, 0.13... |
1,802.05528 | Spherical CR uniformization of Dehn surgeries of the Whitehead link
complement | We apply a spherical CR Dehn surgery theorem in order to obtain infinitely
many Dehn surgeries of the Whitehead link complement that carry spherical CR
structures. We consider as starting point the spherical CR uniformization of
the Whitehead link complement constructed by Parker and Will, using a Ford
domain in the ... | math.GT | we apply a spherical cr dehn surgery theorem in order to obtain infinitely many dehn surgeries of the whitehead link complement that carry spherical cr structures we consider as starting point the spherical cr uniformization of the whitehead link complement constructed by parker and will using a ford domain in the comp... | [['we', 'apply', 'a', 'spherical', 'cr', 'dehn', 'surgery', 'theorem', 'in', 'order', 'to', 'obtain', 'infinitely', 'many', 'dehn', 'surgeries', 'of', 'the', 'whitehead', 'link', 'complement', 'that', 'carry', 'spherical', 'cr', 'structures', 'we', 'consider', 'as', 'starting', 'point', 'the', 'spherical', 'cr', 'unifo... | [-0.24129799742729882, 0.05830769878869162, -0.08848715910839068, 0.1025165521918884, -0.11106289762097436, -0.13758342302202978, -0.01999501258487234, 0.33020665327942855, -0.2634501305371019, -0.26698923438497996, 0.11516167000061958, -0.29262113828539243, -0.1552770813908176, 0.2651281389690986, -0.07026733407661054... |
1,802.05529 | Observation of broadband entanglement in microwave radiation from a
single time-varying boundary condition | Entangled pairs of microwave photons are commonly produced in the narrow
frequency band of a resonator, which represents a modified vacuum density of
states. We use a broadband, semi-infinite transmission line terminated by a
superconducting quantum interference device (SQUID). A weak pump signal
modulates the SQUID ... | quant-ph | entangled pairs of microwave photons are commonly produced in the narrow frequency band of a resonator which represents a modified vacuum density of states we use a broadband semiinfinite transmission line terminated by a superconducting quantum interference device squid a weak pump signal modulates the squid inductanc... | [['entangled', 'pairs', 'of', 'microwave', 'photons', 'are', 'commonly', 'produced', 'in', 'the', 'narrow', 'frequency', 'band', 'of', 'a', 'resonator', 'which', 'represents', 'a', 'modified', 'vacuum', 'density', 'of', 'states', 'we', 'use', 'a', 'broadband', 'semiinfinite', 'transmission', 'line', 'terminated', 'by',... | [-0.22845992972758145, 0.19911159369290876, -0.018758840578481217, -0.005072388498030539, -0.016323544772934507, -0.20563208901810207, 0.051793137350945144, 0.40489986943165684, -0.23768903745803982, -0.2817908670774407, -0.007362154320369221, -0.3023938404142179, -0.04025775922293013, 0.22687947359571065, 0.0044362926... |
1,802.0553 | Gaussian process modeling of heterogeneity and discontinuities using
Voronoi tessellations | Many methods for modelling spatial processes assume global smoothness
properties; such assumptions are often violated in practice. We introduce a
method for modelling spatial processes that display heterogeneity or contain
discontinuities. The problem of non-stationarity is dealt with by using a
combination of Vorono... | stat.ME | many methods for modelling spatial processes assume global smoothness properties such assumptions are often violated in practice we introduce a method for modelling spatial processes that display heterogeneity or contain discontinuities the problem of nonstationarity is dealt with by using a combination of voronoi tess... | [['many', 'methods', 'for', 'modelling', 'spatial', 'processes', 'assume', 'global', 'smoothness', 'properties', 'such', 'assumptions', 'are', 'often', 'violated', 'in', 'practice', 'we', 'introduce', 'a', 'method', 'for', 'modelling', 'spatial', 'processes', 'that', 'display', 'heterogeneity', 'or', 'contain', 'discon... | [-0.058284325663187316, 0.04762658318004193, -0.08195961891694671, 0.08050579679863376, -0.09709576918094447, -0.12173961327679342, 0.034083202318993935, 0.4334237537431446, -0.30385002635011915, -0.29496191994456405, 0.11925234276339214, -0.2591097700677699, -0.17617378556910393, 0.171901271361011, -0.0952757871739529... |
1,802.05531 | Linear maps on $M_n(\mathbb{R})$ preserving Schur stable matrices | An $n \times n$ matrix $A$ with real entries is said to be Schur stable if
all the eigenvalues of $A$ are inside the open unit disc. We investigate the
structure of linear maps on $M_n(\mathbb{R})$ that preserve the collection
$\mathcal{S}$ of Schur stable matrices. We prove that if $L$ is a linear map
such that $L(\... | math.FA | an n times n matrix a with real entries is said to be schur stable if all the eigenvalues of a are inside the open unit disc we investigate the structure of linear maps on m_nmathbbr that preserve the collection mathcals of schur stable matrices we prove that if l is a linear map such that lmathcals subseteq mathcals t... | [['an', 'n', 'times', 'n', 'matrix', 'a', 'with', 'real', 'entries', 'is', 'said', 'to', 'be', 'schur', 'stable', 'if', 'all', 'the', 'eigenvalues', 'of', 'a', 'are', 'inside', 'the', 'open', 'unit', 'disc', 'we', 'investigate', 'the', 'structure', 'of', 'linear', 'maps', 'on', 'm_nmathbbr', 'that', 'preserve', 'the', ... | [-0.12414240822630021, 0.08884474656499981, -0.022434382080055267, 0.02852135731440797, -0.0055176837650100586, -0.11671243175339785, -0.02597542065512208, 0.3749727886712667, -0.32234060074975807, -0.17712275493546453, 0.13867650297583414, -0.3149484301944381, -0.1435774478844358, 0.15711137683139842, -0.0537071923354... |
1,802.05532 | Strongly gravitational lensed SNe Ia as multi-messengers: Direct test of
the Friedmann-Lema\^{\i}tre-Robertson-Walker metric | We present a new idea of testing the validity of the
Friedman-Lema\^{\i}tre-Robertson-Walker metric, through the multiple
measurements of galactic-scale strong gravitational lensing systems with type
Ia supernovae in the role of sources. Each individual lensing system will
provide a model-independent measurement of t... | astro-ph.CO astro-ph.GA gr-qc | we present a new idea of testing the validity of the friedmanlemaitrerobertsonwalker metric through the multiple measurements of galacticscale strong gravitational lensing systems with type ia supernovae in the role of sources each individual lensing system will provide a modelindependent measurement of the spatial cur... | [['we', 'present', 'a', 'new', 'idea', 'of', 'testing', 'the', 'validity', 'of', 'the', 'friedmanlemaitrerobertsonwalker', 'metric', 'through', 'the', 'multiple', 'measurements', 'of', 'galacticscale', 'strong', 'gravitational', 'lensing', 'systems', 'with', 'type', 'ia', 'supernovae', 'in', 'the', 'role', 'of', 'sourc... | [-0.10645449738067946, 0.06117675395103768, -0.1027898500375088, 0.08997741059820592, -0.16523737052582133, -0.1235692724286018, 3.1759395056123874e-05, 0.32340323934964477, -0.21816755860175902, -0.32318480714287573, 0.03548390747305657, -0.2962051278649314, -0.0755700682949962, 0.22142307963493524, -0.019984589982961... |
1,802.05533 | The role of noise modeling in the estimation of resting-state brain
effective connectivity | Causal relations among neuronal populations of the brain are studied through
the so-called effective connectivity (EC) network. The latter is estimated from
EEG or fMRI measurements, by inverting a generative model of the corresponding
data. It is clear that the goodness of the estimated network heavily depends on
th... | cs.SY q-bio.NC | causal relations among neuronal populations of the brain are studied through the socalled effective connectivity ec network the latter is estimated from eeg or fmri measurements by inverting a generative model of the corresponding data it is clear that the goodness of the estimated network heavily depends on the underl... | [['causal', 'relations', 'among', 'neuronal', 'populations', 'of', 'the', 'brain', 'are', 'studied', 'through', 'the', 'socalled', 'effective', 'connectivity', 'ec', 'network', 'the', 'latter', 'is', 'estimated', 'from', 'eeg', 'or', 'fmri', 'measurements', 'by', 'inverting', 'a', 'generative', 'model', 'of', 'the', 'c... | [-0.08591428401313699, 0.08075048005708528, -0.05513608942015304, 0.1443164790003204, -0.06768556261711099, -0.12317156487569948, 0.04225763829028303, 0.3843085005603455, -0.25953228046426285, -0.30208439149399413, 0.09769807417049176, -0.25876536096135777, -0.2725417181579281, 0.1553729228577634, -0.06874485912928242,... |
1,802.05534 | Opportunity in Conflict: Understanding Tension Among Key Groups on the
Trail | This paper examines the question of who technology users on the trail are,
what their technological uses and needs are, and what conflicts exist between
different trail users regarding technology use and experience, toward
understanding how experiences of trail users contribute to designers. We argue
that exploring t... | cs.HC | this paper examines the question of who technology users on the trail are what their technological uses and needs are and what conflicts exist between different trail users regarding technology use and experience toward understanding how experiences of trail users contribute to designers we argue that exploring these t... | [['this', 'paper', 'examines', 'the', 'question', 'of', 'who', 'technology', 'users', 'on', 'the', 'trail', 'are', 'what', 'their', 'technological', 'uses', 'and', 'needs', 'are', 'and', 'what', 'conflicts', 'exist', 'between', 'different', 'trail', 'users', 'regarding', 'technology', 'use', 'and', 'experience', 'towar... | [-0.08787419889539258, 0.09277712878312415, -0.08671945359543967, 0.08563162302146596, -0.1784381263180455, -0.18802632604127945, 0.11729790991929763, 0.4448947626263348, -0.24470953960249672, -0.3844488931458388, 0.08775392830816668, -0.30763779579898093, -0.20622710552789383, 0.16125635922288717, -0.14906921824301356... |
1,802.05535 | Point island dynamics under fixed rate deposition | In this paper we consider the dynamics of point islands during submonolayer
deposition, in which the fragmentation of subcritical size islands is allowed.
To understand asymptotics of solutions, we use methods of centre manifold
theory, and for globalisation, we employ results from the theories of
compartmental syste... | math.CA | in this paper we consider the dynamics of point islands during submonolayer deposition in which the fragmentation of subcritical size islands is allowed to understand asymptotics of solutions we use methods of centre manifold theory and for globalisation we employ results from the theories of compartmental systems and ... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'dynamics', 'of', 'point', 'islands', 'during', 'submonolayer', 'deposition', 'in', 'which', 'the', 'fragmentation', 'of', 'subcritical', 'size', 'islands', 'is', 'allowed', 'to', 'understand', 'asymptotics', 'of', 'solutions', 'we', 'use', 'methods', 'of', 'centre', 'm... | [-0.10201788573428544, 0.0978131887238862, -0.118655466405091, 0.06265123839031404, 0.021591613708592174, -0.08166073321246667, 0.056309604767098356, 0.3335517113333318, -0.20377253255904165, -0.27067179791629314, 0.11856029152786776, -0.2689849247794543, -0.19024534100916848, 0.17827443746544086, -0.0475894362012397, ... |
1,802.05536 | Graph Operator Modeling over Large Graph Datasets | As graph representations of data emerge in multiple domains, data analysts
need to be able to intelligently select among a magnitude of different data
graphs based on the effects different graph operators have on them. Exhaustive
execution of an operator over the bulk of available data sources is impractical
due to t... | cs.SI physics.soc-ph | as graph representations of data emerge in multiple domains data analysts need to be able to intelligently select among a magnitude of different data graphs based on the effects different graph operators have on them exhaustive execution of an operator over the bulk of available data sources is impractical due to the m... | [['as', 'graph', 'representations', 'of', 'data', 'emerge', 'in', 'multiple', 'domains', 'data', 'analysts', 'need', 'to', 'be', 'able', 'to', 'intelligently', 'select', 'among', 'a', 'magnitude', 'of', 'different', 'data', 'graphs', 'based', 'on', 'the', 'effects', 'different', 'graph', 'operators', 'have', 'on', 'the... | [-0.10085831929927294, 0.030654169010022176, -0.08433053032630711, 0.10049191259108695, -0.14100702528845185, -0.1364471945590656, 0.049346214708492375, 0.4248446479475903, -0.26300466907644665, -0.35750868904756977, 0.10665597354041557, -0.29541489895369893, -0.1259621793203038, 0.22853818366380896, -0.091907054891140... |
1,802.05537 | The Effect of $\alpha$-Vacua on the Scalar and Tensor Spectral Indices:
Slow-Roll Approximation | Since the duration of inflation is finite, imposing the initial condition in
infinite past, i.e. the Bunch-Davies vacuum, is inherently ambiguous. In this
paper, we resort to the mixed states as initial condition which are called the
$\alpha$-vacua and then introduce a physical momentum cutoff $\Lambda$
[Danielsson:2... | gr-qc | since the duration of inflation is finite imposing the initial condition in infinite past ie the bunchdavies vacuum is inherently ambiguous in this paper we resort to the mixed states as initial condition which are called the alphavacua and then introduce a physical momentum cutoff lambda danielsson2002kx in which the ... | [['since', 'the', 'duration', 'of', 'inflation', 'is', 'finite', 'imposing', 'the', 'initial', 'condition', 'in', 'infinite', 'past', 'ie', 'the', 'bunchdavies', 'vacuum', 'is', 'inherently', 'ambiguous', 'in', 'this', 'paper', 'we', 'resort', 'to', 'the', 'mixed', 'states', 'as', 'initial', 'condition', 'which', 'are'... | [-0.16746149433242996, 0.20339491353737876, -0.12562005044293334, 0.07068774595036993, -0.048708761609241105, -0.09650733450847018, -0.005326244097110429, 0.333285489270725, -0.24856493553713138, -0.2738261337539083, 0.12194280935674688, -0.2388481934669248, -0.08500932189036836, 0.1293163302876001, -0.0055325346881774... |
1,802.05538 | Singlet and triplet trions in WS$_2$ monolayer encapsulated in hexagonal
boron nitride | Embedding a WS$_2$ monolayer in flakes of hexagonal boron nitride allowed us
to resolve and study the photoluminescence response due to both singlet and
triplet states of negatively charged excitons (trions) in this atomically thin
semiconductor. The energy separation between the singlet and triplet states has
been f... | cond-mat.mes-hall | embedding a ws_2 monolayer in flakes of hexagonal boron nitride allowed us to resolve and study the photoluminescence response due to both singlet and triplet states of negatively charged excitons trions in this atomically thin semiconductor the energy separation between the singlet and triplet states has been found to... | [['embedding', 'a', 'ws_2', 'monolayer', 'in', 'flakes', 'of', 'hexagonal', 'boron', 'nitride', 'allowed', 'us', 'to', 'resolve', 'and', 'study', 'the', 'photoluminescence', 'response', 'due', 'to', 'both', 'singlet', 'and', 'triplet', 'states', 'of', 'negatively', 'charged', 'excitons', 'trions', 'in', 'this', 'atomic... | [-0.10118068310607603, 0.24707765266488213, -0.014794539695646128, 0.11010416607672781, 0.023867533758174683, -0.21327940221416994, 0.049848079586914486, 0.47622750602338626, -0.23798188625200503, -0.2800857138927972, -0.07410711238069621, -0.321413340397935, -0.04472313050950027, 0.11083680514475681, 0.095461353158537... |
1,802.05539 | Using mathematical modeling to ask meaningful biological questions
through combination of bifurcation analysis and population heterogeneity | Classical approaches to analyzing dynamical systems, including bifurcation
analysis, can provide invaluable insights into underlying structure of a
mathematical model, and the spectrum of all possible dynamical behaviors.
However, these models frequently fail to take into account population
heterogeneity, which, whil... | q-bio.PE | classical approaches to analyzing dynamical systems including bifurcation analysis can provide invaluable insights into underlying structure of a mathematical model and the spectrum of all possible dynamical behaviors however these models frequently fail to take into account population heterogeneity which while critica... | [['classical', 'approaches', 'to', 'analyzing', 'dynamical', 'systems', 'including', 'bifurcation', 'analysis', 'can', 'provide', 'invaluable', 'insights', 'into', 'underlying', 'structure', 'of', 'a', 'mathematical', 'model', 'and', 'the', 'spectrum', 'of', 'all', 'possible', 'dynamical', 'behaviors', 'however', 'thes... | [-0.07479240822227752, 0.05466129927944782, -0.13705730724138437, 0.11954940244197465, -0.10669149987409593, -0.15849745423490463, 0.061381365793916114, 0.34086580859917787, -0.2837640053883035, -0.35307078708403855, 0.11672103087986088, -0.2388998257130527, -0.21024488044216708, 0.20121862028815574, -0.047223290756484... |
1,802.0554 | No correction for the light propagation within the cube: comment on
"Relativistic theory of the falling retroreflector gravimeter" | Although the equation of motion developed in the paper (Ashby 2018 Metrologia
55 1) depends on the parameters of the falling cube, such as depth and
refraction index, the parameters are only associated with powers of time no
greater than one, and so do not affect the acceleration. The paper's correction
due to the li... | physics.ins-det | although the equation of motion developed in the paper ashby 2018 metrologia 55 1 depends on the parameters of the falling cube such as depth and refraction index the parameters are only associated with powers of time no greater than one and so do not affect the acceleration the papers correction due to the light propa... | [['although', 'the', 'equation', 'of', 'motion', 'developed', 'in', 'the', 'paper', 'ashby', '2018', 'metrologia', '55', '1', 'depends', 'on', 'the', 'parameters', 'of', 'the', 'falling', 'cube', 'such', 'as', 'depth', 'and', 'refraction', 'index', 'the', 'parameters', 'are', 'only', 'associated', 'with', 'powers', 'of... | [-0.0801310058318309, 0.12607227540670982, -0.06667305687538434, -0.0004703696449911318, -0.07948260136985595, -0.08473910411493372, 0.014082670068973195, 0.33014786592924716, -0.25138372038827117, -0.34330225298085165, 0.12250359671084766, -0.3053149720557879, -0.10035478342900571, 0.24572491629130794, -0.073476680753... |
1,802.05541 | Novel weak form quadrature elements for non-classical higher order beam
and plate theories | Based on Lagrange and Hermite interpolation two novel versions of weak form
quadrature element are proposed for a non-classical Euler-Bernoulli beam
theory. By extending these concept two new plate elements are formulated using
Lagrange-Lagrange and mixed Lagrange-Hermite interpolations for a non-classical
Kirchhoff ... | cs.CE | based on lagrange and hermite interpolation two novel versions of weak form quadrature element are proposed for a nonclassical eulerbernoulli beam theory by extending these concept two new plate elements are formulated using lagrangelagrange and mixed lagrangehermite interpolations for a nonclassical kirchhoff plate th... | [['based', 'on', 'lagrange', 'and', 'hermite', 'interpolation', 'two', 'novel', 'versions', 'of', 'weak', 'form', 'quadrature', 'element', 'are', 'proposed', 'for', 'a', 'nonclassical', 'eulerbernoulli', 'beam', 'theory', 'by', 'extending', 'these', 'concept', 'two', 'new', 'plate', 'elements', 'are', 'formulated', 'us... | [-0.11250936894855917, 0.09372815093956888, -0.08454948599187737, 0.01107220592886269, -0.0750902683394862, -0.1400016659073175, -0.0035907970023083876, 0.36876794310445166, -0.271484601616047, -0.2659841633718857, 0.09716022675584486, -0.2737211284544715, -0.1385902008438047, 0.19308299578273014, -0.0701336918170861, ... |
1,802.05542 | Repdigits in Euler functions of Pell and associated pell numbers | A natural number $n$ is called a repdigit if all its digits are same. In this
paper, we prove that Euler totient function of no Pell number is a repdigit
with at least two digits. This study is also extended to certain subclass of
associated Pell numbers.
| math.NT | a natural number n is called a repdigit if all its digits are same in this paper we prove that euler totient function of no pell number is a repdigit with at least two digits this study is also extended to certain subclass of associated pell numbers | [['a', 'natural', 'number', 'n', 'is', 'called', 'a', 'repdigit', 'if', 'all', 'its', 'digits', 'are', 'same', 'in', 'this', 'paper', 'we', 'prove', 'that', 'euler', 'totient', 'function', 'of', 'no', 'pell', 'number', 'is', 'a', 'repdigit', 'with', 'at', 'least', 'two', 'digits', 'this', 'study', 'is', 'also', 'extend... | [-0.25769089774952997, 0.1502209186553955, -0.06362852045438355, 0.1054100585816842, -0.10523956915777591, -0.111771661001775, -0.03021586547450473, 0.30061776174439325, -0.30280181558595765, -0.2643106698989868, 0.06640668560802522, -0.32342411688942874, -0.20361611371756427, 0.20558899227115843, -0.09106062153975168,... |
1,802.05543 | On the Radar detection of high-energy neutrino-induced cascades in ice;
From Radar scattering cross-section to sensitivity | In recent works we discussed the feasibility of the radar detection technique
as a new method to probe high-energy cosmic-neutrino induced plasmas in ice.
Using the different properties of the induced ionization plasma, an energy
threshold of several PeV was derived for the over-dense scattering of a radio
wave off t... | astro-ph.HE | in recent works we discussed the feasibility of the radar detection technique as a new method to probe highenergy cosmicneutrino induced plasmas in ice using the different properties of the induced ionization plasma an energy threshold of several pev was derived for the overdense scattering of a radio wave off the plas... | [['in', 'recent', 'works', 'we', 'discussed', 'the', 'feasibility', 'of', 'the', 'radar', 'detection', 'technique', 'as', 'a', 'new', 'method', 'to', 'probe', 'highenergy', 'cosmicneutrino', 'induced', 'plasmas', 'in', 'ice', 'using', 'the', 'different', 'properties', 'of', 'the', 'induced', 'ionization', 'plasma', 'an... | [-0.07382908921116157, 0.13892417736641216, -0.07427557466157318, 0.09832385939031926, -0.038584968848111995, -0.05640580369839193, 0.020221757299795345, 0.3733872473155996, -0.23885800231348825, -0.3404266424812712, 0.08341067996524223, -0.2634463483585162, -0.07768070220166969, 0.24510762138084533, 0.0257352719822560... |
1,802.05544 | Integration in terms of exponential integrals and incomplete gamma
functions I | This paper provides a Liouville principle for integration in terms of
exponential integrals and incomplete gamma functions.
| math.NT cs.SC | this paper provides a liouville principle for integration in terms of exponential integrals and incomplete gamma functions | [['this', 'paper', 'provides', 'a', 'liouville', 'principle', 'for', 'integration', 'in', 'terms', 'of', 'exponential', 'integrals', 'and', 'incomplete', 'gamma', 'functions']] | [-0.1537104942561949, 0.055458631695193404, -0.1444182749837637, 0.1442647568319979, -0.08850715824348085, -0.034092612948049515, 0.08591995035599478, 0.2781461459748885, -0.2647342098986401, -0.20045261830091476, 0.07871225105790312, -0.2113326895324623, -0.19642373985227415, 0.2352122848524767, -0.07624067524995874, ... |
1,802.05545 | Constraining screened fifth forces with the electron magnetic moment | Chameleon and symmetron theories serve as archetypal models for how light
scalar fields can couple to matter with gravitational strength or greater, yet
evade the stringent constraints from classical tests of gravity on Earth and in
the Solar System. In this work, we investigate how a precision measurement of
the ele... | hep-ph astro-ph.CO physics.atom-ph | chameleon and symmetron theories serve as archetypal models for how light scalar fields can couple to matter with gravitational strength or greater yet evade the stringent constraints from classical tests of gravity on earth and in the solar system in this work we investigate how a precision measurement of the electron... | [['chameleon', 'and', 'symmetron', 'theories', 'serve', 'as', 'archetypal', 'models', 'for', 'how', 'light', 'scalar', 'fields', 'can', 'couple', 'to', 'matter', 'with', 'gravitational', 'strength', 'or', 'greater', 'yet', 'evade', 'the', 'stringent', 'constraints', 'from', 'classical', 'tests', 'of', 'gravity', 'on', ... | [-0.10595576146422413, 0.13713802830903327, -0.06984103668577851, 0.10165910507841648, -0.11235489721186984, -0.13832444634491867, 0.026344630739759838, 0.3178871542405547, -0.213789827641244, -0.36803042799444263, 0.07455329663504709, -0.24684293553705366, -0.08452391008187321, 0.2250201229397929, 0.002352619396820238... |
1,802.05546 | A viable laser driver for a user plasma accelerator | The construction of a novel user facility employing laser-driven plasma
acceleration with superior beam quality will require an industrial grade, high
repetition rate petawatt laser driver which is beyond existing technology.
However, with the ongoing fast development of chirped pulse amplification and
high average p... | physics.acc-ph physics.ins-det | the construction of a novel user facility employing laserdriven plasma acceleration with superior beam quality will require an industrial grade high repetition rate petawatt laser driver which is beyond existing technology however with the ongoing fast development of chirped pulse amplification and high average power l... | [['the', 'construction', 'of', 'a', 'novel', 'user', 'facility', 'employing', 'laserdriven', 'plasma', 'acceleration', 'with', 'superior', 'beam', 'quality', 'will', 'require', 'an', 'industrial', 'grade', 'high', 'repetition', 'rate', 'petawatt', 'laser', 'driver', 'which', 'is', 'beyond', 'existing', 'technology', 'h... | [-0.1137167783576603, 0.16162058680799274, -0.03541329900096906, 0.0035130932118351524, -0.08220262495114615, -0.21108952143817747, -0.002589364893930523, 0.460854743303437, -0.22411825844135724, -0.32767462261621594, 0.11085699343392136, -0.18013369742241736, -0.029144584137554233, 0.32504185951854053, -0.082188000495... |
1,802.05547 | Dynamics of small solutions in KdV type equations: decay inside the
linearly dominated region | In this paper we prove that all small, uniformly in time $L^1\cap H^1$
bounded solutions to KdV and related perturbations must converge to zero, as
time goes to infinity, locally in an increasing-in-time region of space of
order $t^{1/2}$ around any compact set in space. This set is included in the
linearly dominated... | math.AP math-ph math.MP nlin.SI | in this paper we prove that all small uniformly in time l1cap h1 bounded solutions to kdv and related perturbations must converge to zero as time goes to infinity locally in an increasingintime region of space of order t12 around any compact set in space this set is included in the linearly dominated dispersive region ... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'all', 'small', 'uniformly', 'in', 'time', 'l1cap', 'h1', 'bounded', 'solutions', 'to', 'kdv', 'and', 'related', 'perturbations', 'must', 'converge', 'to', 'zero', 'as', 'time', 'goes', 'to', 'infinity', 'locally', 'in', 'an', 'increasingintime', 'region', 'of', 'space', ... | [-0.1511123329477985, 0.14141398211202705, -0.06851524759030109, 0.05974192859908981, -0.08786374420381712, -0.08894423039799387, 0.0003033275610174645, 0.3334475977746539, -0.30486161494242753, -0.182353637282244, 0.1188819383642413, -0.2867747205040179, -0.12540041048210576, 0.17273641341512114, -0.06015534956856777,... |
1,802.05548 | Damping's effect on the magnetodynamics of spin Hall nano-oscillators | We study the impact of spin wave damping ($\alpha$) on the auto-oscillation
properties of nano-constriction based spin Hall nano-oscillators (SHNOs). The
SHNOs are based on a 5 nm Pt layer interfaced to a 5 nm
Py$_{100-x-y}$Pt$_{x}$Ag$_{y}$ magnetic layer, where the Pt and Ag contents are
co-varied to keep the satura... | cond-mat.mes-hall | we study the impact of spin wave damping alpha on the autooscillation properties of nanoconstriction based spin hall nanooscillators shnos the shnos are based on a 5 nm pt layer interfaced to a 5 nm py_100xypt_xag_y magnetic layer where the pt and ag contents are covaried to keep the saturation magnetization constant w... | [['we', 'study', 'the', 'impact', 'of', 'spin', 'wave', 'damping', 'alpha', 'on', 'the', 'autooscillation', 'properties', 'of', 'nanoconstriction', 'based', 'spin', 'hall', 'nanooscillators', 'shnos', 'the', 'shnos', 'are', 'based', 'on', 'a', '5', 'nm', 'pt', 'layer', 'interfaced', 'to', 'a', '5', 'nm', 'py_100xypt_xa... | [-0.17483514420765509, 0.1862262073401852, -0.011954791157653457, -0.01837752382868386, -0.04098655724757057, -0.09174626770943992, 0.028522196204377043, 0.36824231044585376, -0.2550032600166129, -0.32178465011039453, 0.06068382926260758, -0.2722544616676475, -0.07973468456858475, 0.19791197672633357, 0.065495672575994... |
1,802.05549 | Stochastic homogenization of a scalar viscoelastic model exhibiting
stress-strain hysteresis | Motivated by rate-independent stress-strain hysteresis observed in filled
rubber, this article considers a scalar viscoelastic model in which the
constitutive law is random and varies on a lengthscale which is small relative
to the overall size of the solid. Using stochastic two-scale convergence as
introduced by Bou... | math.AP | motivated by rateindependent stressstrain hysteresis observed in filled rubber this article considers a scalar viscoelastic model in which the constitutive law is random and varies on a lengthscale which is small relative to the overall size of the solid using stochastic twoscale convergence as introduced by bourgeat m... | [['motivated', 'by', 'rateindependent', 'stressstrain', 'hysteresis', 'observed', 'in', 'filled', 'rubber', 'this', 'article', 'considers', 'a', 'scalar', 'viscoelastic', 'model', 'in', 'which', 'the', 'constitutive', 'law', 'is', 'random', 'and', 'varies', 'on', 'a', 'lengthscale', 'which', 'is', 'small', 'relative', ... | [-0.11240119541869954, 0.15367084516354068, -0.06981920147739837, 0.0021293405658545216, -0.030131006390666185, -0.13395531649154652, 0.010915942647008469, 0.32409942569211125, -0.2773629531831197, -0.26259286869722215, 0.1031908028032732, -0.22478084768796258, -0.21294299982812093, 0.18335021009071448, -0.085736698579... |
1,802.0555 | ICA based on Split Generalized Gaussian | Independent Component Analysis (ICA) - one of the basic tools in data
analysis - aims to find a coordinate system in which the components of the data
are independent. Most popular ICA methods use kurtosis as a metric of
non-Gaussianity to maximize, such as FastICA and JADE. However, their
assumption of fourth-order m... | stat.ML | independent component analysis ica one of the basic tools in data analysis aims to find a coordinate system in which the components of the data are independent most popular ica methods use kurtosis as a metric of nongaussianity to maximize such as fastica and jade however their assumption of fourthorder moment kurtosis... | [['independent', 'component', 'analysis', 'ica', 'one', 'of', 'the', 'basic', 'tools', 'in', 'data', 'analysis', 'aims', 'to', 'find', 'a', 'coordinate', 'system', 'in', 'which', 'the', 'components', 'of', 'the', 'data', 'are', 'independent', 'most', 'popular', 'ica', 'methods', 'use', 'kurtosis', 'as', 'a', 'metric', ... | [-0.03846687790534393, 0.00712547186894093, -0.1496829506537811, 0.10928674860707095, -0.10352938576036785, -0.15927473247403234, -0.021489323443168496, 0.35278305211416117, -0.24837779362344983, -0.2609683102158111, 0.1548865765734671, -0.2941604479744033, -0.12419391427130445, 0.1845004191974134, -0.05859831363896795... |
1,802.05551 | Measurement of Radio-Frequency Radiation Pressure | We perform measurements of the radiation pressure of a radio-frequency (RF)
electromagnetic field which may lead to a new SI-traceable power calibration.
There are several groups around the world investigating methods to perform more
direct SI traceable measurement of RF power (where RF is defined to range from
100s ... | physics.app-ph physics.ins-det | we perform measurements of the radiation pressure of a radiofrequency rf electromagnetic field which may lead to a new sitraceable power calibration there are several groups around the world investigating methods to perform more direct si traceable measurement of rf power where rf is defined to range from 100s of mhz t... | [['we', 'perform', 'measurements', 'of', 'the', 'radiation', 'pressure', 'of', 'a', 'radiofrequency', 'rf', 'electromagnetic', 'field', 'which', 'may', 'lead', 'to', 'a', 'new', 'sitraceable', 'power', 'calibration', 'there', 'are', 'several', 'groups', 'around', 'the', 'world', 'investigating', 'methods', 'to', 'perfo... | [-0.1324855184807491, 0.1295493715491734, -0.04670746068127061, -0.04367115328970708, -0.09371702119610027, -0.11841656263231447, 0.09214023047273881, 0.40262693941201033, -0.2394987860106324, -0.34040185569932585, 0.05082530448286745, -0.25420599905283825, -0.012276805211838923, 0.26847537228543505, -0.022454684148607... |
1,802.05552 | Searching for galactic axions through magnetized media: QUAX status
report | The current status of the QUAX R\&D program is presented. QUAX is a
feasibility study for a detection of axion as dark matter based on the coupling
to the electrons. The relevant signal is a magnetization change of a magnetic
material placed inside a resonant microwave cavity and polarized with a static
magnetic fiel... | physics.ins-det hep-ph | the current status of the quax rd program is presented quax is a feasibility study for a detection of axion as dark matter based on the coupling to the electrons the relevant signal is a magnetization change of a magnetic material placed inside a resonant microwave cavity and polarized with a static magnetic field | [['the', 'current', 'status', 'of', 'the', 'quax', 'rd', 'program', 'is', 'presented', 'quax', 'is', 'a', 'feasibility', 'study', 'for', 'a', 'detection', 'of', 'axion', 'as', 'dark', 'matter', 'based', 'on', 'the', 'coupling', 'to', 'the', 'electrons', 'the', 'relevant', 'signal', 'is', 'a', 'magnetization', 'change',... | [-0.21413532782483985, 0.16644043489186852, -0.042604141127042194, 0.01378990452590019, -0.10881379381236103, -0.09142375527881086, 0.03503885037584782, 0.3352553168380702, -0.20089710427068727, -0.307657314395463, 0.09172822059028679, -0.25828129874059447, -0.030407241536994225, 0.22116775555467164, 0.0701596391370037... |
1,802.05553 | Turbulence Excitation in Counter-Streaming Paraxial Superfluids of Light | Turbulence in the quantum (superfluid) regime, similarly to its classical
counterpart, continues to attract a great deal of scientific inquiry, due to
the yet high number of unresolved problems. While turbulent states can be
routinely created in degenerate atomic gases, there is no generic scheme to
produce turbulenc... | quant-ph cond-mat.quant-gas physics.optics physics.plasm-ph | turbulence in the quantum superfluid regime similarly to its classical counterpart continues to attract a great deal of scientific inquiry due to the yet high number of unresolved problems while turbulent states can be routinely created in degenerate atomic gases there is no generic scheme to produce turbulence in flui... | [['turbulence', 'in', 'the', 'quantum', 'superfluid', 'regime', 'similarly', 'to', 'its', 'classical', 'counterpart', 'continues', 'to', 'attract', 'a', 'great', 'deal', 'of', 'scientific', 'inquiry', 'due', 'to', 'the', 'yet', 'high', 'number', 'of', 'unresolved', 'problems', 'while', 'turbulent', 'states', 'can', 'be... | [-0.14981206170294523, 0.22218788739153614, -0.08430510918235516, 0.06467237628455605, -0.06745531854359933, -0.14324236382049338, -0.018645262581631742, 0.3105474448542521, -0.2867815936064368, -0.2393812507576239, 0.026994109909821262, -0.2798671418530566, -0.13186040996719073, 0.18891839660398702, 0.0428752584407594... |
1,802.05554 | New way of second quantized theory of fermions with either Clifford or
Grassmann coordinates and spin-charge-family theory | Fermions with the internal degrees of freedom described in Clifford space
carry in any dimension a half integer spin. There are two kinds of spins in
Clifford space. The spin-charge-family theory,assuming even d=13+1, uses one
kind of spins to describe in d=3+1 spins and charges of quarks and leptons and
antiquarks a... | physics.gen-ph | fermions with the internal degrees of freedom described in clifford space carry in any dimension a half integer spin there are two kinds of spins in clifford space the spinchargefamily theoryassuming even d131 uses one kind of spins to describe in d31 spins and charges of quarks and leptons and antiquarks and antilepto... | [['fermions', 'with', 'the', 'internal', 'degrees', 'of', 'freedom', 'described', 'in', 'clifford', 'space', 'carry', 'in', 'any', 'dimension', 'a', 'half', 'integer', 'spin', 'there', 'are', 'two', 'kinds', 'of', 'spins', 'in', 'clifford', 'space', 'the', 'spinchargefamily', 'theoryassuming', 'even', 'd131', 'uses', '... | [-0.15239828999494304, 0.23330355136876796, -0.03441230309189117, 0.11519324050742208, -0.07086237661771663, -0.13761414722610674, 0.0012671134251223462, 0.31868081782415186, -0.22765605465388394, -0.26583402669191253, 0.05456663376907986, -0.2827306110813892, -0.11003455334940168, 0.16658444108990886, -0.0316060665063... |
1,802.05555 | Adaptive Boundaries in Multiscale Simulations | Combined-resolution simulations are an effective way to study molecular
properties across a range of length- and time-scales. These simulations can
benefit from adaptive boundaries that allow the high-resolution region to adapt
(change size and/or shape) as the simulation progresses. The number of degrees
of freedom ... | physics.comp-ph cond-mat.stat-mech | combinedresolution simulations are an effective way to study molecular properties across a range of length and timescales these simulations can benefit from adaptive boundaries that allow the highresolution region to adapt change size andor shape as the simulation progresses the number of degrees of freedom required to... | [['combinedresolution', 'simulations', 'are', 'an', 'effective', 'way', 'to', 'study', 'molecular', 'properties', 'across', 'a', 'range', 'of', 'length', 'and', 'timescales', 'these', 'simulations', 'can', 'benefit', 'from', 'adaptive', 'boundaries', 'that', 'allow', 'the', 'highresolution', 'region', 'to', 'adapt', 'c... | [-0.0989035332097605, 0.10421404803163764, -0.1070314372518386, 0.05189158459271472, -0.07184364969136035, -0.06263173695385846, 0.049504108886764035, 0.43046053598811423, -0.28702452642313553, -0.339090436118734, 0.11271259755130517, -0.18496509411926168, -0.17051774544604853, 0.18610226276050645, -0.04821426499185298... |
1,802.05556 | Hopf Real Hypersurfaces in the Indefinite Complex Projective Space | We wish to attack the problems that H.~Anciaux and K.~Panagiotidou posed in
[1], for non-degenerate real hypersurfaces in indefinite complex projective
space. We will slightly change these authors' point of view, obtaining cleaner
equations for the almost contact metric structure. To make the theory
meaningful, we co... | math.DG | we wish to attack the problems that hanciaux and kpanagiotidou posed in 1 for nondegenerate real hypersurfaces in indefinite complex projective space we will slightly change these authors point of view obtaining cleaner equations for the almost contact metric structure to make the theory meaningful we construct new fam... | [['we', 'wish', 'to', 'attack', 'the', 'problems', 'that', 'hanciaux', 'and', 'kpanagiotidou', 'posed', 'in', '1', 'for', 'nondegenerate', 'real', 'hypersurfaces', 'in', 'indefinite', 'complex', 'projective', 'space', 'we', 'will', 'slightly', 'change', 'these', 'authors', 'point', 'of', 'view', 'obtaining', 'cleaner',... | [-0.18597914153244346, 0.06708239966537803, -0.05709621535614133, 0.09165284106275066, -0.14802178841084243, -0.17978976882994174, -0.034309314725687726, 0.3698681364953518, -0.2945487107289955, -0.23040511276572942, 0.11347667948313755, -0.287022725250572, -0.23271659806370734, 0.20216020832769574, -0.1212667241040617... |
1,802.05557 | The Gauss-Bonnet Theorem for coherent tangent bundles over surfaces with
boundary and its applications | In [31,32,33] the Gauss-Bonnet formulas for coherent tangent bundles over
compact oriented surfaces (without boundary) were proved. We establish the
Gauss-Bonnet theorem for coherent tangent bundles over compact oriented
surfaces with boundary. We apply this theorem to investigate global properties
of maps between su... | math.DG | in 313233 the gaussbonnet formulas for coherent tangent bundles over compact oriented surfaces without boundary were proved we establish the gaussbonnet theorem for coherent tangent bundles over compact oriented surfaces with boundary we apply this theorem to investigate global properties of maps between surfaces with ... | [['in', '313233', 'the', 'gaussbonnet', 'formulas', 'for', 'coherent', 'tangent', 'bundles', 'over', 'compact', 'oriented', 'surfaces', 'without', 'boundary', 'were', 'proved', 'we', 'establish', 'the', 'gaussbonnet', 'theorem', 'for', 'coherent', 'tangent', 'bundles', 'over', 'compact', 'oriented', 'surfaces', 'with',... | [-0.2138847653838721, 0.0654126719116572, -0.10729401677169582, 0.07975704693129625, -0.10040548115291378, -0.09701049318537117, 0.016082100313029844, 0.3702741802754727, -0.2582978759807619, -0.186566813853146, 0.09359582958700643, -0.23077223338186742, -0.17208049477247353, 0.2307127388067205, -0.09563821322557156, 0... |
1,802.05558 | Generalizing Choi-like maps | A problem of further generalization of generalized Choi maps $\Phi_{[a,b,c]}$
acting on $\mathbb{M}_3$ introduced by Cho, Kye and Lee is discussed. Some
necessary conditions for positivity of the generalized maps are provided as
well as some sufficient conditions. Also some sufficient condition for
decomposability of... | math.OA | a problem of further generalization of generalized choi maps phi_abc acting on mathbbm_3 introduced by cho kye and lee is discussed some necessary conditions for positivity of the generalized maps are provided as well as some sufficient conditions also some sufficient condition for decomposability of these maps is show... | [['a', 'problem', 'of', 'further', 'generalization', 'of', 'generalized', 'choi', 'maps', 'phi_abc', 'acting', 'on', 'mathbbm_3', 'introduced', 'by', 'cho', 'kye', 'and', 'lee', 'is', 'discussed', 'some', 'necessary', 'conditions', 'for', 'positivity', 'of', 'the', 'generalized', 'maps', 'are', 'provided', 'as', 'well'... | [-0.09717082144801524, 0.09127058162096333, -0.03781187491729222, 0.1252097297866056, -0.049205364074875066, -0.16053520417475003, -0.02303224453762015, 0.331498577953019, -0.2552172176024698, -0.2433715783693689, 0.20743758802084214, -0.15246589895971913, -0.25823460400421566, 0.2346185212756725, -0.14819546271749634,... |
1,802.05559 | Fine-Grained Complexity of Safety Verification | We study the fine-grained complexity of Leader Contributor Reachability (LCR)
and Bounded-Stage Reachability (BSR), two variants of the safety verification
problem for shared memory concurrent programs. For both problems, the memory is
a single variable over a finite data domain. Our contributions are new
verificatio... | cs.LO cs.DC cs.DS | we study the finegrained complexity of leader contributor reachability lcr and boundedstage reachability bsr two variants of the safety verification problem for shared memory concurrent programs for both problems the memory is a single variable over a finite data domain our contributions are new verification algorithms... | [['we', 'study', 'the', 'finegrained', 'complexity', 'of', 'leader', 'contributor', 'reachability', 'lcr', 'and', 'boundedstage', 'reachability', 'bsr', 'two', 'variants', 'of', 'the', 'safety', 'verification', 'problem', 'for', 'shared', 'memory', 'concurrent', 'programs', 'for', 'both', 'problems', 'the', 'memory', '... | [-0.16259867009274395, 0.0851950908962213, -0.05362104858670916, 0.07667508419461748, -0.07553767927124032, -0.1625186591982908, 0.10440472474313407, 0.3437232741799172, -0.29279291453172585, -0.33499398619834597, 0.12854939493907816, -0.24910477266779968, -0.080256178367251, 0.20299100439795958, -0.037811498337188304,... |
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