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 |
|---|---|---|---|---|---|---|
1,801.04169 | Hopf-link multi-Weyl-loop topological semimetals | We construct a generic two-band model which can describe topological Weyl
semimetals with multiple closed Weyl loops. All the existing multi-Weyl-loop
semimetals including the nodal-net, or nodal-chain and Hopf-link states can be
examined within one same framework. Based on a two-loop model, the
corresponding drum-he... | cond-mat.mes-hall cond-mat.mtrl-sci | we construct a generic twoband model which can describe topological weyl semimetals with multiple closed weyl loops all the existing multiweylloop semimetals including the nodalnet or nodalchain and hopflink states can be examined within one same framework based on a twoloop model the corresponding drumhead surface sta... | [['we', 'construct', 'a', 'generic', 'twoband', 'model', 'which', 'can', 'describe', 'topological', 'weyl', 'semimetals', 'with', 'multiple', 'closed', 'weyl', 'loops', 'all', 'the', 'existing', 'multiweylloop', 'semimetals', 'including', 'the', 'nodalnet', 'or', 'nodalchain', 'and', 'hopflink', 'states', 'can', 'be', ... | [-0.20174766796032997, 0.21223902363572578, -0.03567751687912902, 0.07804810442222852, -0.061059385155181375, -0.233119469986505, 0.04606946187347851, 0.3480824192924317, -0.24473800166117504, -0.27380647715796863, 0.028742349414108706, -0.2846392049754331, -0.18155204989631807, 0.16657681162430604, 0.02913870296464109... |
1,801.0417 | Multilayered Model of Speech | Human speech is the most important part of General Artificial Intelligence
and subject of much research. The hypothesis proposed in this article provides
explanation of difficulties that modern science tackles in the field of human
brain simulation. The hypothesis is based on the author's conviction that the
brain of... | cs.AI | human speech is the most important part of general artificial intelligence and subject of much research the hypothesis proposed in this article provides explanation of difficulties that modern science tackles in the field of human brain simulation the hypothesis is based on the authors conviction that the brain of any ... | [['human', 'speech', 'is', 'the', 'most', 'important', 'part', 'of', 'general', 'artificial', 'intelligence', 'and', 'subject', 'of', 'much', 'research', 'the', 'hypothesis', 'proposed', 'in', 'this', 'article', 'provides', 'explanation', 'of', 'difficulties', 'that', 'modern', 'science', 'tackles', 'in', 'the', 'field... | [-0.05587137750590524, 0.05973672999167129, -0.11479430074350123, 0.06570237237086698, -0.160974805929551, -0.1435365692075146, -0.03375805092754921, 0.34906771886897714, -0.22059903241920678, -0.3439451570501612, 0.0780092528194042, -0.24487193891974657, -0.2643610665446, 0.21306079716764784, -0.15477544652592196, 0.0... |
1,801.04171 | Properties and rotation of molecular clouds in M 33 | The sample of 566 molecular clouds identified in the CO(2--1) IRAM survey
covering the disk of M~33 is explored in detail.The clouds were found using
CPROPS and were subsequently catalogued in terms of their star-forming
properties as non-star-forming (A), with embedded star formation (B), or with
exposed star format... | astro-ph.GA | the sample of 566 molecular clouds identified in the co21 iram survey covering the disk of m33 is explored in detailthe clouds were found using cprops and were subsequently catalogued in terms of their starforming properties as nonstarforming a with embedded star formation b or with exposed star formation cwe find that... | [['the', 'sample', 'of', '566', 'molecular', 'clouds', 'identified', 'in', 'the', 'co21', 'iram', 'survey', 'covering', 'the', 'disk', 'of', 'm33', 'is', 'explored', 'in', 'detailthe', 'clouds', 'were', 'found', 'using', 'cprops', 'and', 'were', 'subsequently', 'catalogued', 'in', 'terms', 'of', 'their', 'starforming',... | [-0.1201159570493299, 0.13164412806401668, -0.05444525947237586, 0.10351164128873634, -0.05751833305487966, -0.04786513753318463, 0.02271356300890748, 0.42255706458294084, -0.1838915540331569, -0.3625890179245124, 0.037498369797500625, -0.27974852206706535, 0.003891140886675223, 0.19122062258704178, -0.0122039726101088... |
1,801.04172 | Fast iterative solvers for an optimal transport problem | Optimal transport problems pose many challenges when considering their
numerical treatment. We investigate the solution of a PDE-constrained
optimisation problem subject to a particular transport equation arising from
the modelling of image metamorphosis. We present the nonlinear optimisation
problem, and discuss the... | math.NA | optimal transport problems pose many challenges when considering their numerical treatment we investigate the solution of a pdeconstrained optimisation problem subject to a particular transport equation arising from the modelling of image metamorphosis we present the nonlinear optimisation problem and discuss the discr... | [['optimal', 'transport', 'problems', 'pose', 'many', 'challenges', 'when', 'considering', 'their', 'numerical', 'treatment', 'we', 'investigate', 'the', 'solution', 'of', 'a', 'pdeconstrained', 'optimisation', 'problem', 'subject', 'to', 'a', 'particular', 'transport', 'equation', 'arising', 'from', 'the', 'modelling'... | [-0.0775601660113847, -0.031512681525527386, -0.11233965832364272, 0.03196209827295031, -0.07446626956133466, -0.13979378106530038, 0.028984740239633412, 0.36951783214483347, -0.3571769548049033, -0.2740869749819435, 0.1579542071956798, -0.22416577471028032, -0.18878672374902586, 0.19686932011768876, -0.086821376313373... |
1,801.04173 | Magnetic Induction Dependence of Hall Resistance in Fractional Quantum
Hall Effect | We constructed a Hall resistance formula for the fractional quantum Hall
effect by analyzing the experimental data reported in [J. P. Eisenstein and H.
L. Stormer, {Science} {\bf 248}, 1510 (1990)]. The formula is given as a
function of magnetic induction, chemical potential and temperature. The Hall
resistance funct... | cond-mat.mes-hall | we constructed a hall resistance formula for the fractional quantum hall effect by analyzing the experimental data reported in j p eisenstein and h l stormer science bf 248 1510 1990 the formula is given as a function of magnetic induction chemical potential and temperature the hall resistance function contains a singl... | [['we', 'constructed', 'a', 'hall', 'resistance', 'formula', 'for', 'the', 'fractional', 'quantum', 'hall', 'effect', 'by', 'analyzing', 'the', 'experimental', 'data', 'reported', 'in', 'j', 'p', 'eisenstein', 'and', 'h', 'l', 'stormer', 'science', 'bf', '248', '1510', '1990', 'the', 'formula', 'is', 'given', 'as', 'a'... | [-0.20089698814694862, 0.16370092603252628, -0.08523008107095138, 0.03464499813540337, -0.07106826388901406, -0.14622852858155966, 0.03704464912752283, 0.28477749169118455, -0.23769497688204705, -0.35227658409256857, 0.026503071396171557, -0.26307737717793866, -0.12457453530373891, 0.24079072362600037, -0.0184607848136... |
1,801.04174 | Chemical and Physical Picture of IRAS 16293-2422 Source B at a
Sub-arcsecond Scale Studied with ALMA | We have analyzed the OCS, H$_2$CS, CH$_3$OH, and HCOOCH$_3$ data observed
toward the low-mass protostar IRAS 16293--2422 Source B at a sub-arcsecond
resolution with ALMA. A clear chemical differentiation is seen in their
distributions; OCS and H$_2$CS are extended with a slight rotation signature,
while CH$_3$OH and ... | astro-ph.SR astro-ph.GA | we have analyzed the ocs h_2cs ch_3oh and hcooch_3 data observed toward the lowmass protostar iras 162932422 source b at a subarcsecond resolution with alma a clear chemical differentiation is seen in their distributions ocs and h_2cs are extended with a slight rotation signature while ch_3oh and hcooch_3 are concentra... | [['we', 'have', 'analyzed', 'the', 'ocs', 'h_2cs', 'ch_3oh', 'and', 'hcooch_3', 'data', 'observed', 'toward', 'the', 'lowmass', 'protostar', 'iras', '162932422', 'source', 'b', 'at', 'a', 'subarcsecond', 'resolution', 'with', 'alma', 'a', 'clear', 'chemical', 'differentiation', 'is', 'seen', 'in', 'their', 'distributio... | [-0.100143964355123, 0.07547940345681635, -0.046551498389171976, 0.03430025405513363, -0.060858497996964765, -0.08561357956940449, 0.0035074351014949944, 0.46221084127663287, -0.22021798507882512, -0.2728775636423179, 0.07655020680351143, -0.2415967418521803, 0.0076924196634722015, 0.10134102675127446, -0.0109203392063... |
1,801.04175 | A fast spectral divide-and-conquer method for banded matrices | Based on the spectral divide-and-conquer algorithm by Nakatsukasa and Higham
[SIAM J. Sci. Comput., 35(3): A1325-A1349, 2013], we propose a new algorithm
for computing all the eigenvalues and eigenvectors of a symmetric banded
matrix. For this purpose, we combine our previous work on the fast computation
of spectral ... | math.NA cs.NA | based on the spectral divideandconquer algorithm by nakatsukasa and higham siam j sci comput 353 a1325a1349 2013 we propose a new algorithm for computing all the eigenvalues and eigenvectors of a symmetric banded matrix for this purpose we combine our previous work on the fast computation of spectral projectors in the ... | [['based', 'on', 'the', 'spectral', 'divideandconquer', 'algorithm', 'by', 'nakatsukasa', 'and', 'higham', 'siam', 'j', 'sci', 'comput', '353', 'a1325a1349', '2013', 'we', 'propose', 'a', 'new', 'algorithm', 'for', 'computing', 'all', 'the', 'eigenvalues', 'and', 'eigenvectors', 'of', 'a', 'symmetric', 'banded', 'matri... | [-0.055396049061197446, 0.013052948284894228, -0.07393089967478193, -0.021231664637029593, -0.06204816948262636, -0.10374040221689608, 0.03527815226698294, 0.36611289281228726, -0.24318571664414115, -0.32396240234480833, 0.11747658617704557, -0.21995801955348393, -0.2129383017229636, 0.20541931898862292, -0.04789581540... |
1,801.04176 | Non-meagre subgroups of reals disjoint with meagre sets | Let $(X, +)$ denote $(\mathbb{R}, +)$ or $(2^{\omega}, +_2)$. We prove that
for any meagre set $F \subseteq X$ there exists a subgroup $G \le X$ without
the Baire property, disjoint with some translation of F. We point out several
consequences of this fact and indicate why analogous result for the measure
cannot be e... | math.GN | let x denote mathbbr or 2omega _2 we prove that for any meagre set f subseteq x there exists a subgroup g le x without the baire property disjoint with some translation of f we point out several consequences of this fact and indicate why analogous result for the measure cannot be established in zfc we extend proof tech... | [['let', 'x', 'denote', 'mathbbr', 'or', '2omega', '_2', 'we', 'prove', 'that', 'for', 'any', 'meagre', 'set', 'f', 'subseteq', 'x', 'there', 'exists', 'a', 'subgroup', 'g', 'le', 'x', 'without', 'the', 'baire', 'property', 'disjoint', 'with', 'some', 'translation', 'of', 'f', 'we', 'point', 'out', 'several', 'conseque... | [-0.167975297293571, 0.10709915284122176, -0.0960307807476698, 0.035608494919656286, -0.08045676324571319, -0.16785352736684112, 0.10246429117122556, 0.3734178240137065, -0.3305489154299721, -0.162367552107967, 0.04353510505376, -0.3153913378414205, -0.08049393641447429, 0.21184918370358097, -0.13812935475588722, -0.03... |
1,801.04177 | Acoustic boundary layers as boundary conditions | The linearized, compressible Navier-Stokes equations can be used to model
acoustic wave propagation in the presence of viscous and thermal boundary
layers. However, acoustic boundary layers are notorious for invoking
prohibitively high resolution requirements on numerical solutions of the
equations. We derive and pre... | physics.comp-ph | the linearized compressible navierstokes equations can be used to model acoustic wave propagation in the presence of viscous and thermal boundary layers however acoustic boundary layers are notorious for invoking prohibitively high resolution requirements on numerical solutions of the equations we derive and present a ... | [['the', 'linearized', 'compressible', 'navierstokes', 'equations', 'can', 'be', 'used', 'to', 'model', 'acoustic', 'wave', 'propagation', 'in', 'the', 'presence', 'of', 'viscous', 'and', 'thermal', 'boundary', 'layers', 'however', 'acoustic', 'boundary', 'layers', 'are', 'notorious', 'for', 'invoking', 'prohibitively'... | [-0.14200725331288344, 0.10021415861433704, -0.04734151621668152, 0.022936073475261585, -0.09491863477183139, -0.1397596809767392, -0.02145670142527083, 0.3119088060380231, -0.2881379401316778, -0.2761838685842158, 0.1373083171990194, -0.27150407328552706, -0.08674484383091184, 0.19595617781609562, -0.02081470395893034... |
1,801.04178 | The affine VW supercategory | We define the affine VW supercategory
$\mathit{s}\hspace{-0.7mm}\bigvee\mkern-15mu\bigvee$, which arises from
studying the action of the periplectic Lie superalgebra $\mathfrak{p}(n)$ on
the tensor product $M\otimes V^{\otimes a}$ of an arbitrary representation $M$
with several copies of the vector representation $V$... | math.RT | we define the affine vw supercategory mathitshspace07mmbigveemkern15mubigvee which arises from studying the action of the periplectic lie superalgebra mathfrakpn on the tensor product motimes votimes a of an arbitrary representation m with several copies of the vector representation v of mathfrakpn it plays a role anal... | [['we', 'define', 'the', 'affine', 'vw', 'supercategory', 'mathitshspace07mmbigveemkern15mubigvee', 'which', 'arises', 'from', 'studying', 'the', 'action', 'of', 'the', 'periplectic', 'lie', 'superalgebra', 'mathfrakpn', 'on', 'the', 'tensor', 'product', 'motimes', 'votimes', 'a', 'of', 'an', 'arbitrary', 'representati... | [-0.1501527503861406, 0.07382016005515213, -0.09591200532467693, 0.015784564074825775, -0.09892931598916549, -0.08303441290053076, -0.04265264102153252, 0.31826086420578514, -0.35468671486085773, -0.20485862688522558, 0.10025972761308813, -0.2243521681251828, -0.20626583840178492, 0.17741406075086216, -0.11182911580643... |
1,801.04179 | Arhuaco: Deep Learning and Isolation Based Security for Distributed
High-Throughput Computing | Grid computing systems require innovative methods and tools to identify
cybersecurity incidents and perform autonomous actions i.e. without
administrator intervention. They also require methods to isolate and trace job
payload activity in order to protect users and find evidence of malicious
behavior. We introduce an... | cs.DC cs.CR cs.LG | grid computing systems require innovative methods and tools to identify cybersecurity incidents and perform autonomous actions ie without administrator intervention they also require methods to isolate and trace job payload activity in order to protect users and find evidence of malicious behavior we introduce an integ... | [['grid', 'computing', 'systems', 'require', 'innovative', 'methods', 'and', 'tools', 'to', 'identify', 'cybersecurity', 'incidents', 'and', 'perform', 'autonomous', 'actions', 'ie', 'without', 'administrator', 'intervention', 'they', 'also', 'require', 'methods', 'to', 'isolate', 'and', 'trace', 'job', 'payload', 'act... | [-0.12964711365632, -0.04521405757525979, -0.0705570146869521, 0.03384162624864058, -0.05884150600766543, -0.18227287111312196, 0.07705731055791842, 0.4091348926368985, -0.2090022237045887, -0.375130908505887, 0.13074017230852258, -0.3043945612941192, -0.14012478104350012, 0.21720393895105058, -0.11885369227120295, 0.1... |
1,801.0418 | Boosted Top Tagging Method Overview | We briefly review common tools and methods to identify boosted, hadronically
decaying top quarks at the LHC experiments. This includes generic jet
substructure variables, specific top identification algorithms, and recent
developments in deep learning techniques.
| hep-ph | we briefly review common tools and methods to identify boosted hadronically decaying top quarks at the lhc experiments this includes generic jet substructure variables specific top identification algorithms and recent developments in deep learning techniques | [['we', 'briefly', 'review', 'common', 'tools', 'and', 'methods', 'to', 'identify', 'boosted', 'hadronically', 'decaying', 'top', 'quarks', 'at', 'the', 'lhc', 'experiments', 'this', 'includes', 'generic', 'jet', 'substructure', 'variables', 'specific', 'top', 'identification', 'algorithms', 'and', 'recent', 'developme... | [0.018012442626059055, 0.15383461471647025, -0.1028550895330097, 0.18047076100150922, -0.16242307158453123, -0.24841079855603831, 0.01681219493704183, 0.40511459968984126, -0.25095279083720273, -0.24543363797877515, 0.029793157744487483, -0.31805845153118883, -0.04997887861515794, 0.17866154600467002, 0.015041919638003... |
1,801.04181 | Moving magnets in a micromagnetic finite difference framework | We present a method and an implementation for smooth linear motion in a
finite difference-based micromagnetic simulation code, to be used in simulating
magnetic friction and other phenomena involving moving microscale magnets. Our
aim is to accurately simulate the magnetization dynamics and relative motion of
magnets... | physics.comp-ph | we present a method and an implementation for smooth linear motion in a finite differencebased micromagnetic simulation code to be used in simulating magnetic friction and other phenomena involving moving microscale magnets our aim is to accurately simulate the magnetization dynamics and relative motion of magnets whil... | [['we', 'present', 'a', 'method', 'and', 'an', 'implementation', 'for', 'smooth', 'linear', 'motion', 'in', 'a', 'finite', 'differencebased', 'micromagnetic', 'simulation', 'code', 'to', 'be', 'used', 'in', 'simulating', 'magnetic', 'friction', 'and', 'other', 'phenomena', 'involving', 'moving', 'microscale', 'magnets'... | [-0.15785036778428638, 0.09680853927897796, -0.05129610450907809, -0.0002880860387240766, -0.09489065715585088, -0.13572418989735793, 0.006601120710523692, 0.41075583663387377, -0.27894549545847247, -0.318154314899298, 0.08862546987385016, -0.22245367775197888, -0.10735336201051708, 0.27572327062151714, -0.003011215905... |
1,801.04182 | n-Torsion Clean Rings | Let n be an arbitrary natural number. The class of (strongly) n-torsion clean
rings is introduced and investigated. Abelian n-torsion clean rings are
somewhat characterized and a complete characterization of strongly n-torsion
clean rings is given in the case when n is odd. Some open questions are posed
at the end.
| math.RA | let n be an arbitrary natural number the class of strongly ntorsion clean rings is introduced and investigated abelian ntorsion clean rings are somewhat characterized and a complete characterization of strongly ntorsion clean rings is given in the case when n is odd some open questions are posed at the end | [['let', 'n', 'be', 'an', 'arbitrary', 'natural', 'number', 'the', 'class', 'of', 'strongly', 'ntorsion', 'clean', 'rings', 'is', 'introduced', 'and', 'investigated', 'abelian', 'ntorsion', 'clean', 'rings', 'are', 'somewhat', 'characterized', 'and', 'a', 'complete', 'characterization', 'of', 'strongly', 'ntorsion', 'c... | [-0.23709733873678773, 0.17498839452352566, -0.010491170893039773, 0.07132613805679641, -0.05684338579429131, -0.24187058874168524, -0.07581520616989948, 0.3345634473451212, -0.3092340064764607, -0.25541834259296164, 0.10118396122090738, -0.2920332762102286, -0.05928236062127147, 0.22963008536573717, -0.117979334685586... |
1,801.04183 | Tensor network formulation for two-dimensional lattice $\mathcal{N}=1$
Wess-Zumino model | Supersymmetric models with spontaneous supersymmetry breaking suffer from the
notorious sign problem in stochastic approaches. By contrast, the tensor
network approaches do not have such a problem since they are based on
deterministic procedures. In this work, we present a tensor network formulation
of the two-dimens... | hep-lat | supersymmetric models with spontaneous supersymmetry breaking suffer from the notorious sign problem in stochastic approaches by contrast the tensor network approaches do not have such a problem since they are based on deterministic procedures in this work we present a tensor network formulation of the twodimensional l... | [['supersymmetric', 'models', 'with', 'spontaneous', 'supersymmetry', 'breaking', 'suffer', 'from', 'the', 'notorious', 'sign', 'problem', 'in', 'stochastic', 'approaches', 'by', 'contrast', 'the', 'tensor', 'network', 'approaches', 'do', 'not', 'have', 'such', 'a', 'problem', 'since', 'they', 'are', 'based', 'on', 'de... | [-0.06155602199214627, 0.07428818332118681, -0.017860811327409465, 0.05745766441941669, -0.07942619171808474, -0.1857818955759285, -0.012292749819607707, 0.39029557193862274, -0.21330211166787194, -0.2798713809224864, 0.14803953392402036, -0.2744519636762561, -0.24473263605614193, 0.12169516326503071, -0.06920845587592... |
1,801.04184 | How pairwise coevolutionary models capture the collective residue
variability in proteins | Global coevolutionary models of homologous protein families, as constructed
by direct coupling analysis (DCA), have recently gained popularity in
particular due to their capacity to accurately predict residue-residue contacts
from sequence information alone, and thereby to facilitate tertiary and
quaternary protein s... | q-bio.QM cond-mat.stat-mech q-bio.BM | global coevolutionary models of homologous protein families as constructed by direct coupling analysis dca have recently gained popularity in particular due to their capacity to accurately predict residueresidue contacts from sequence information alone and thereby to facilitate tertiary and quaternary protein structure... | [['global', 'coevolutionary', 'models', 'of', 'homologous', 'protein', 'families', 'as', 'constructed', 'by', 'direct', 'coupling', 'analysis', 'dca', 'have', 'recently', 'gained', 'popularity', 'in', 'particular', 'due', 'to', 'their', 'capacity', 'to', 'accurately', 'predict', 'residueresidue', 'contacts', 'from', 's... | [-0.09857908871066191, 0.12268542150899367, -0.07253233092281071, 0.15001797011975093, -0.06880502568810273, -0.15087288475343, 0.05756490131585519, 0.4284994700949674, -0.29441865137343026, -0.33112484111426677, 0.010397180355650104, -0.25561108164796353, -0.2170759342626068, 0.1425608973155912, -0.00953495625850405, ... |
1,801.04185 | A reference model for interaction semantics | In this article, we introduce a reference model for interaction semantics
among communicating discrete systems to guide the discourse on
interoperability.
The necessary set of unifying concepts is small and comprises essentially the
notion of discrete systems interacting by exchanging information. It is based
on a ... | cs.SE cs.LO | in this article we introduce a reference model for interaction semantics among communicating discrete systems to guide the discourse on interoperability the necessary set of unifying concepts is small and comprises essentially the notion of discrete systems interacting by exchanging information it is based on a simple ... | [['in', 'this', 'article', 'we', 'introduce', 'a', 'reference', 'model', 'for', 'interaction', 'semantics', 'among', 'communicating', 'discrete', 'systems', 'to', 'guide', 'the', 'discourse', 'on', 'interoperability', 'the', 'necessary', 'set', 'of', 'unifying', 'concepts', 'is', 'small', 'and', 'comprises', 'essential... | [-0.16624854143252984, 0.11114326869428623, -0.07603079832939935, 0.08158551124943188, -0.10756794320380626, -0.2015979243791662, 0.04321262500161538, 0.41934599516292415, -0.31095570060812555, -0.32993507928501153, 0.06421915491179485, -0.2836829163231111, -0.14587892617855686, 0.1529868598867324, -0.06912866234391307... |
1,801.04186 | Anomalous Nernst effect on the nanometer scale: Exploring
three-dimensional temperature gradients in magnetic tunnel junctions | Localized laser heating creates temperature gradients in all directions and
thus leads to three-dimensional electron flux in metallic materials.
Temperature gradients in combination with material magnetization generate
thermomagnetic voltages. The interplay between these direction-dependent
temperature gradients and ... | cond-mat.mes-hall | localized laser heating creates temperature gradients in all directions and thus leads to threedimensional electron flux in metallic materials temperature gradients in combination with material magnetization generate thermomagnetic voltages the interplay between these directiondependent temperature gradients and the ma... | [['localized', 'laser', 'heating', 'creates', 'temperature', 'gradients', 'in', 'all', 'directions', 'and', 'thus', 'leads', 'to', 'threedimensional', 'electron', 'flux', 'in', 'metallic', 'materials', 'temperature', 'gradients', 'in', 'combination', 'with', 'material', 'magnetization', 'generate', 'thermomagnetic', 'v... | [-0.16839650624724042, 0.19226398452761395, -0.003465009064107906, -0.007156591960637766, -0.07619648710966735, -0.14131910439655326, 0.06340351035365904, 0.437291570157097, -0.3019360591504609, -0.3345017943083387, 0.009680017266859735, -0.27513431434841507, -0.06959654111248523, 0.2657336836222218, -0.023102720631535... |
1,801.04187 | MSDNN: Multi-Scale Deep Neural Network for Salient Object Detection | Salient object detection is a fundamental problem and has been received a
great deal of attentions in computer vision. Recently deep learning model
became a powerful tool for image feature extraction. In this paper, we propose
a multi-scale deep neural network (MSDNN) for salient object detection. The
proposed model ... | cs.CV | salient object detection is a fundamental problem and has been received a great deal of attentions in computer vision recently deep learning model became a powerful tool for image feature extraction in this paper we propose a multiscale deep neural network msdnn for salient object detection the proposed model first ext... | [['salient', 'object', 'detection', 'is', 'a', 'fundamental', 'problem', 'and', 'has', 'been', 'received', 'a', 'great', 'deal', 'of', 'attentions', 'in', 'computer', 'vision', 'recently', 'deep', 'learning', 'model', 'became', 'a', 'powerful', 'tool', 'for', 'image', 'feature', 'extraction', 'in', 'this', 'paper', 'we... | [-0.0056774665990815265, -0.09923696962141548, -0.08233747087433585, 0.053588191978633404, -0.10180047503308742, -0.21557931230563554, -0.06723412236806325, 0.47919102970627137, -0.2933352664367703, -0.2929105656949105, 0.05628190693187207, -0.2826589426585997, -0.25576662724779453, 0.15933456584025407, -0.122740781755... |
1,801.04188 | Racetrack Fixed Field Accelerator with pulsed quadrupoles for variable
energy extraction | In this paper, a novel concept combining a fixed field alternating gradient
accelerator with time-varying quadrupoles is presented which solves some of the
major problems of conventional fixed field accelerators. This concept combines
a stable racetrack fixed field configuration with dispersion free straight
sections... | physics.acc-ph | in this paper a novel concept combining a fixed field alternating gradient accelerator with timevarying quadrupoles is presented which solves some of the major problems of conventional fixed field accelerators this concept combines a stable racetrack fixed field configuration with dispersion free straight sections to e... | [['in', 'this', 'paper', 'a', 'novel', 'concept', 'combining', 'a', 'fixed', 'field', 'alternating', 'gradient', 'accelerator', 'with', 'timevarying', 'quadrupoles', 'is', 'presented', 'which', 'solves', 'some', 'of', 'the', 'major', 'problems', 'of', 'conventional', 'fixed', 'field', 'accelerators', 'this', 'concept',... | [-0.12831576645655174, 0.1578275155515589, -0.05543901269058032, 0.058359000485368254, -0.13906712024213952, -0.19006281854244805, -0.007721748747234602, 0.413466753829169, -0.30349303472654093, -0.2835774211506803, 0.058321969865429556, -0.2268372230889601, -0.07159522421924132, 0.2119364370665853, -0.0510517288893756... |
1,801.04189 | Divisibility of L-Polynomials for a Family of Curves | We consider the question of when the L-polynomial of one curve divides the
L-polynomial of another curve. A theorem of Tate gives an answer in terms of
jacobians. We consider the question in terms of the curves. The last author
gave an invited talk at the 12th International Conference on Finite Fields and
Their Appli... | math.AG | we consider the question of when the lpolynomial of one curve divides the lpolynomial of another curve a theorem of tate gives an answer in terms of jacobians we consider the question in terms of the curves the last author gave an invited talk at the 12th international conference on finite fields and their applications... | [['we', 'consider', 'the', 'question', 'of', 'when', 'the', 'lpolynomial', 'of', 'one', 'curve', 'divides', 'the', 'lpolynomial', 'of', 'another', 'curve', 'a', 'theorem', 'of', 'tate', 'gives', 'an', 'answer', 'in', 'terms', 'of', 'jacobians', 'we', 'consider', 'the', 'question', 'in', 'terms', 'of', 'the', 'curves', ... | [-0.19194431637059634, 0.03840803977103681, -0.12424585010371053, 0.059411365627376755, -0.06428463106424036, -0.10960248118581277, 0.01713922123988749, 0.25957546091940203, -0.25935234827264936, -0.29099037133577005, 0.10591141073669398, -0.29039049620779467, -0.1444679024288247, 0.23020444523123368, -0.19043939824307... |
1,801.0419 | Youla Coding and Computation of Gaussian Feedback Capacity | In this paper, we propose an approach to numerically compute the feedback
capacity of stationary finite dimensional Gaussian channels and construct
(arbitrarily close to) capacity-achieving feedback codes. In particular, we
first extend the interpretation of feedback communication over stationary
finite dimensional G... | cs.IT math.IT | in this paper we propose an approach to numerically compute the feedback capacity of stationary finite dimensional gaussian channels and construct arbitrarily close to capacityachieving feedback codes in particular we first extend the interpretation of feedback communication over stationary finite dimensional gaussian ... | [['in', 'this', 'paper', 'we', 'propose', 'an', 'approach', 'to', 'numerically', 'compute', 'the', 'feedback', 'capacity', 'of', 'stationary', 'finite', 'dimensional', 'gaussian', 'channels', 'and', 'construct', 'arbitrarily', 'close', 'to', 'capacityachieving', 'feedback', 'codes', 'in', 'particular', 'we', 'first', '... | [-0.15597192709961163, 0.06032288542152017, -0.07585677120445017, 0.07275711758339205, -0.05269919134359929, -0.24606654924809251, 0.12209346121271426, 0.38092554623589797, -0.28461712855675253, -0.2504686315671778, 0.12391558885833041, -0.18578897796425164, -0.15244189371945324, 0.22432835372103974, -0.119033785229107... |
1,801.04191 | Computing permanents of complex diagonally dominant matrices and tensors | We prove that for any $\lambda > 1$, fixed in advance, the permanent of an $n
\times n$ complex matrix, where the absolute value of each diagonal entry is at
least $\lambda$ times bigger than the sum of the absolute values of all other
entries in the same row, can be approximated within any relative error $0 <
\epsil... | math.CO cs.DM cs.DS | we prove that for any lambda 1 fixed in advance the permanent of an n times n complex matrix where the absolute value of each diagonal entry is at least lambda times bigger than the sum of the absolute values of all other entries in the same row can be approximated within any relative error 0 epsilon 1 in quasipolynomi... | [['we', 'prove', 'that', 'for', 'any', 'lambda', '1', 'fixed', 'in', 'advance', 'the', 'permanent', 'of', 'an', 'n', 'times', 'n', 'complex', 'matrix', 'where', 'the', 'absolute', 'value', 'of', 'each', 'diagonal', 'entry', 'is', 'at', 'least', 'lambda', 'times', 'bigger', 'than', 'the', 'sum', 'of', 'the', 'absolute',... | [-0.15457178741628522, 0.13396518351662454, 0.01951983228304185, 0.008449518619928249, 0.011479486795250586, -0.15017296687894782, 0.03390796378601429, 0.3467211667448282, -0.2867603974720073, -0.27081608819926895, 0.10504353992900876, -0.29687364407013667, -0.07101245732371543, 0.10148773837271471, -0.0531527037261227... |
1,801.04192 | On the edge energy of graphene | Surface/edge energy is typically modeled as a continuous function of
orientation, $\gamma({\bf n})$. We put forward a simple geometric argument that
suggests this picture is inadequate for crystals with a non-Bravais lattice
structure. In the case of the idealized graphene/hexagonal lattice, our
arguments indicate th... | cond-mat.mtrl-sci | surfaceedge energy is typically modeled as a continuous function of orientation gammabf n we put forward a simple geometric argument that suggests this picture is inadequate for crystals with a nonbravais lattice structure in the case of the idealized graphenehexagonal lattice our arguments indicate that the edge energ... | [['surfaceedge', 'energy', 'is', 'typically', 'modeled', 'as', 'a', 'continuous', 'function', 'of', 'orientation', 'gammabf', 'n', 'we', 'put', 'forward', 'a', 'simple', 'geometric', 'argument', 'that', 'suggests', 'this', 'picture', 'is', 'inadequate', 'for', 'crystals', 'with', 'a', 'nonbravais', 'lattice', 'structur... | [-0.15365830391837174, 0.14041214958449608, -0.11575848709874074, 0.0451156801684513, -0.08797915238777504, -0.1287045150598073, 0.06892943639746484, 0.43273904667619395, -0.2652329377391759, -0.24695014378384633, 0.08486931265489307, -0.2314211347633425, -0.1488640201586189, 0.15920763742863475, 0.0021106962162508246,... |
1,801.04193 | Thermo - mechanical instabilities in friction contact | The phenomenon of corrugated surfaces is a known technical problem of
tribological systems; considerable work has been published in the past on the
aspect of rail corrugation of railway systems. Less known is a similar
phenomenon observed within the cylinder-piston system of advanced automotive
engines using aluminiu... | cond-mat.mtrl-sci cond-mat.soft | the phenomenon of corrugated surfaces is a known technical problem of tribological systems considerable work has been published in the past on the aspect of rail corrugation of railway systems less known is a similar phenomenon observed within the cylinderpiston system of advanced automotive engines using aluminium cyl... | [['the', 'phenomenon', 'of', 'corrugated', 'surfaces', 'is', 'a', 'known', 'technical', 'problem', 'of', 'tribological', 'systems', 'considerable', 'work', 'has', 'been', 'published', 'in', 'the', 'past', 'on', 'the', 'aspect', 'of', 'rail', 'corrugation', 'of', 'railway', 'systems', 'less', 'known', 'is', 'a', 'simila... | [-0.20050598196287797, 0.10046768651866331, -0.07494749854947251, 0.028549401487064797, -0.042551781179580264, -0.12703840473924227, 0.009213489628911806, 0.3417497423545616, -0.2401888593274161, -0.2980501866725281, 0.10579779267129374, -0.2726213810586832, -0.21216583591166552, 0.2592166178193458, -0.0813099521314498... |
1,801.04194 | Electronic properties of curved few-layers graphene: a geometrical
approach | We show the presence of non-relativistic L\'evy-Leblond fermions in flat
three- and four-layers graphene with AB stacking, extending the results
obtained in [Curvatronics2017] for bilayer graphene. When the layer is curved
we obtain a set of equations for Galilean fermions that are a variation of
those of L\'evy-Lebl... | cond-mat.mes-hall cond-mat.mtrl-sci gr-qc hep-th | we show the presence of nonrelativistic levyleblond fermions in flat three and fourlayers graphene with ab stacking extending the results obtained in curvatronics2017 for bilayer graphene when the layer is curved we obtain a set of equations for galilean fermions that are a variation of those of levyleblond with a well... | [['we', 'show', 'the', 'presence', 'of', 'nonrelativistic', 'levyleblond', 'fermions', 'in', 'flat', 'three', 'and', 'fourlayers', 'graphene', 'with', 'ab', 'stacking', 'extending', 'the', 'results', 'obtained', 'in', 'curvatronics2017', 'for', 'bilayer', 'graphene', 'when', 'the', 'layer', 'is', 'curved', 'we', 'obtai... | [-0.17813650057851818, 0.18066043167180335, -0.016542830303760952, 0.03862151237333129, -0.03947258601928579, -0.1321564338459023, 0.0051091476953749, 0.37017002262431997, -0.2217621449381113, -0.2978544168712186, -0.008848246789119881, -0.3061054795530849, -0.1441921767770666, 0.1175913565888487, -0.016715107909564313... |
1,801.04195 | Periodic points of a Landen transformation | We prove the existence of 3-periodic orbits in a dynamical system associated
to a Landen transformation previously studied by Boros, Chamberland and Moll,
disproving a conjecture on the dynamics of this planar map introduced by the
latter author. To this end we present a systematic methodology to determine and
locate... | math.DS | we prove the existence of 3periodic orbits in a dynamical system associated to a landen transformation previously studied by boros chamberland and moll disproving a conjecture on the dynamics of this planar map introduced by the latter author to this end we present a systematic methodology to determine and locate analy... | [['we', 'prove', 'the', 'existence', 'of', '3periodic', 'orbits', 'in', 'a', 'dynamical', 'system', 'associated', 'to', 'a', 'landen', 'transformation', 'previously', 'studied', 'by', 'boros', 'chamberland', 'and', 'moll', 'disproving', 'a', 'conjecture', 'on', 'the', 'dynamics', 'of', 'this', 'planar', 'map', 'introdu... | [-0.1643855575814672, 0.04637289304157783, -0.13328852365462474, 0.060504234595299196, -0.05481743598463892, -0.12209595424315796, 0.052747063242412844, 0.3225448141195651, -0.2955838788043836, -0.2646786868679284, 0.12243254156381791, -0.2408931472876655, -0.22037463584491962, 0.19702852103088436, -0.0785453221921263,... |
1,801.04196 | Detection of collective optic excitations in molten NaI | High-resolution inelastic x-ray scattering measurements were carried out on
molten NaI near the melting point at 680$^\circ$C at SPring-8. Small and damped
indications of longitudinal optic excitation modes were observed on the tails
of the longitudinal acoustic modes at small momentum transfers, $Q\sim5$
nm$^{-1}$. ... | cond-mat.mtrl-sci cond-mat.dis-nn | highresolution inelastic xray scattering measurements were carried out on molten nai near the melting point at 680circc at spring8 small and damped indications of longitudinal optic excitation modes were observed on the tails of the longitudinal acoustic modes at small momentum transfers qsim5 nm1 the measured spectra ... | [['highresolution', 'inelastic', 'xray', 'scattering', 'measurements', 'were', 'carried', 'out', 'on', 'molten', 'nai', 'near', 'the', 'melting', 'point', 'at', '680circc', 'at', 'spring8', 'small', 'and', 'damped', 'indications', 'of', 'longitudinal', 'optic', 'excitation', 'modes', 'were', 'observed', 'on', 'the', 't... | [-0.12893082054962188, 0.18056663183137925, -0.08034020399844105, 0.018695362232098677, 0.0036009680291618964, -0.12461607669470738, 0.022751432674174957, 0.4411275787937521, -0.23646773428231657, -0.2832003633087181, 0.01659008514752254, -0.36816969949921424, -0.0577844013695163, 0.20897351647962373, 0.096185952349744... |
1,801.04197 | Ab-initio study of the Coulomb interaction in NbxCo clusters: Strong
on-site versus weak non-local screening | By means of ab-initio calculations in conjunction with the random-phase
approximation (RPA) within the full-potential linearized augmented plane wave
method we study the screening of the Coulomb interaction in NbxCo (1<=x<=9)
clusters. In addition, these results are compared with pure bcc Nb bulk. We
find that for al... | cond-mat.mtrl-sci | by means of abinitio calculations in conjunction with the randomphase approximation rpa within the fullpotential linearized augmented plane wave method we study the screening of the coulomb interaction in nbxco 1x9 clusters in addition these results are compared with pure bcc nb bulk we find that for all clusters the o... | [['by', 'means', 'of', 'abinitio', 'calculations', 'in', 'conjunction', 'with', 'the', 'randomphase', 'approximation', 'rpa', 'within', 'the', 'fullpotential', 'linearized', 'augmented', 'plane', 'wave', 'method', 'we', 'study', 'the', 'screening', 'of', 'the', 'coulomb', 'interaction', 'in', 'nbxco', '1x9', 'clusters'... | [-0.10058957010219076, 0.1578569295613662, -0.005244242889309151, 0.10654045332379361, 0.01766646135690975, -0.13120158863548906, 0.058317596590296825, 0.4079697139977668, -0.22959505749854797, -0.2833220049860361, -0.06895067861089657, -0.37128493423943887, -0.11876488191087192, 0.07219327658686718, 0.1199840071440460... |
1,801.04198 | Non-integrability of the minimum-time Kepler problem | We prove that the minimum-time controlled Kepler problem is not Liouville
integrable in the class of meromorphic functions, via the Moral\`es-Ramis
theory.
| math.DS math-ph math.MP math.OC | we prove that the minimumtime controlled kepler problem is not liouville integrable in the class of meromorphic functions via the moralesramis theory | [['we', 'prove', 'that', 'the', 'minimumtime', 'controlled', 'kepler', 'problem', 'is', 'not', 'liouville', 'integrable', 'in', 'the', 'class', 'of', 'meromorphic', 'functions', 'via', 'the', 'moralesramis', 'theory']] | [-0.1673528170001439, 0.08869770359755917, -0.08631677959452976, 0.140933695953043, -0.13186678772961552, -0.13538709265941923, -0.028910008581905542, 0.28427377631041134, -0.3591460499235175, -0.1562641616064039, 0.07897855555744503, -0.2360846445980397, -0.2699210192076862, 0.2619786409830505, -0.12146974465047772, 0... |
1,801.04199 | SwarmRob: A Toolkit for Reproducibility and Sharing of Experimental
Artifacts in Robotics Research | Due to the complexity of robotics, the reproducibility of results and
experiments is one of the fundamental problems in robotics research. While the
problem has been identified by the community, the approaches that address the
problem appropriately are limited. The toolkit proposed in this paper tries to
deal with th... | cs.RO | due to the complexity of robotics the reproducibility of results and experiments is one of the fundamental problems in robotics research while the problem has been identified by the community the approaches that address the problem appropriately are limited the toolkit proposed in this paper tries to deal with the prob... | [['due', 'to', 'the', 'complexity', 'of', 'robotics', 'the', 'reproducibility', 'of', 'results', 'and', 'experiments', 'is', 'one', 'of', 'the', 'fundamental', 'problems', 'in', 'robotics', 'research', 'while', 'the', 'problem', 'has', 'been', 'identified', 'by', 'the', 'community', 'the', 'approaches', 'that', 'addres... | [-0.08485209066499055, 0.03438545817603698, -0.07870274922270484, -0.010261360272186017, -0.12056532610959116, -0.12047716739250958, 0.022517294390127063, 0.40482629309682283, -0.2504186355861045, -0.3552133500059487, 0.09456885277250578, -0.26979630974223134, -0.17443917687011867, 0.22168237903006688, -0.1660148377663... |
1,801.042 | Wake fields effects in dielectric capillary | Plasma wake-field acceleration experiments are performed at the SPARC LAB
test facility by using a gas-filled capillary plasma source composed of a
dielectric capillary. The electron can reach GeV energy in a few centimeters,
with an accelerating gradient orders of magnitude larger than provided by
conventional techn... | physics.acc-ph | plasma wakefield acceleration experiments are performed at the sparc lab test facility by using a gasfilled capillary plasma source composed of a dielectric capillary the electron can reach gev energy in a few centimeters with an accelerating gradient orders of magnitude larger than provided by conventional techniques ... | [['plasma', 'wakefield', 'acceleration', 'experiments', 'are', 'performed', 'at', 'the', 'sparc', 'lab', 'test', 'facility', 'by', 'using', 'a', 'gasfilled', 'capillary', 'plasma', 'source', 'composed', 'of', 'a', 'dielectric', 'capillary', 'the', 'electron', 'can', 'reach', 'gev', 'energy', 'in', 'a', 'few', 'centimet... | [-0.12624140674990877, 0.21877221570124478, -0.055571994819753875, 0.038381296746445366, -0.03092659286040863, -0.11072288796217558, -0.04892422631697578, 0.41272749933036595, -0.2142840463170983, -0.2948369880496348, -0.004230830183636548, -0.21062301249696394, -0.01617496826912503, 0.25473832722629003, 0.033900117788... |
1,801.04201 | A Probabilistic Approach to the Drag-Based Model | The forecast of the time of arrival of a coronal mass ejection (CME) to Earth
is of critical importance for our high-technology society and for any future
manned exploration of the Solar System. As critical as the forecast accuracy is
the knowledge of its precision, i.e. the error associated to the estimate. We
propo... | physics.space-ph astro-ph.EP astro-ph.SR physics.geo-ph | the forecast of the time of arrival of a coronal mass ejection cme to earth is of critical importance for our hightechnology society and for any future manned exploration of the solar system as critical as the forecast accuracy is the knowledge of its precision ie the error associated to the estimate we propose a stati... | [['the', 'forecast', 'of', 'the', 'time', 'of', 'arrival', 'of', 'a', 'coronal', 'mass', 'ejection', 'cme', 'to', 'earth', 'is', 'of', 'critical', 'importance', 'for', 'our', 'hightechnology', 'society', 'and', 'for', 'any', 'future', 'manned', 'exploration', 'of', 'the', 'solar', 'system', 'as', 'critical', 'as', 'the... | [-0.07983550225416648, 0.08827401390941493, -0.07694912784138759, 0.08749631611428266, -0.043717948414770696, -0.07433859756933632, 0.09592390621961469, 0.3735910298880832, -0.19461649988949214, -0.38964024855990775, 0.14416453701807935, -0.24808547477607198, -0.11476240571669902, 0.2431825206517349, -0.048846371501822... |
1,801.04202 | A Simple and Efficient Estimation Method for Models with Nonignorable
Missing Data | This paper proposes a simple and efficient estimation procedure for the model
with non-ignorable missing data studied by Morikawa and Kim (2016). Their
semiparametrically efficient estimator requires explicit nonparametric
estimation and so suffers from the curse of dimensionality and requires a
bandwidth selection. ... | stat.ME | this paper proposes a simple and efficient estimation procedure for the model with nonignorable missing data studied by morikawa and kim 2016 their semiparametrically efficient estimator requires explicit nonparametric estimation and so suffers from the curse of dimensionality and requires a bandwidth selection we prop... | [['this', 'paper', 'proposes', 'a', 'simple', 'and', 'efficient', 'estimation', 'procedure', 'for', 'the', 'model', 'with', 'nonignorable', 'missing', 'data', 'studied', 'by', 'morikawa', 'and', 'kim', '2016', 'their', 'semiparametrically', 'efficient', 'estimator', 'requires', 'explicit', 'nonparametric', 'estimation'... | [-0.04849079116534646, 0.019248614321428523, -0.08256517610933682, 0.08081481798730586, -0.08866613626333388, -0.16025079072497733, 0.05729208629951519, 0.3916900609811283, -0.2064492607043501, -0.3434119393653555, 0.11459700898299223, -0.21482095659123607, -0.15046699405392658, 0.17502700583211925, -0.1260170814715172... |
1,801.04203 | Vector boson scattering: Recent experimental and theory developments | This document summarises the talks and discussions happened during the VBSCan
Split17 workshop, the first general meeting of the VBSCan COST Action network.
This collaboration is aiming at a consistent and coordinated study of
vector-boson scattering from the phenomenological and experimental point of
view, for the b... | hep-ph hep-ex | this document summarises the talks and discussions happened during the vbscan split17 workshop the first general meeting of the vbscan cost action network this collaboration is aiming at a consistent and coordinated study of vectorboson scattering from the phenomenological and experimental point of view for the best ex... | [['this', 'document', 'summarises', 'the', 'talks', 'and', 'discussions', 'happened', 'during', 'the', 'vbscan', 'split17', 'workshop', 'the', 'first', 'general', 'meeting', 'of', 'the', 'vbscan', 'cost', 'action', 'network', 'this', 'collaboration', 'is', 'aiming', 'at', 'a', 'consistent', 'and', 'coordinated', 'study... | [-0.09159733914641728, 0.1068136419073261, -0.09210212401050175, 0.027509722302683854, -0.11027665631363875, -0.09756995743172693, 0.06761247186182902, 0.314040811341015, -0.21106317634533706, -0.32302453906018413, 0.120501558778101, -0.33930934599504387, -0.11040586085412009, 0.16082361319849012, -0.032949399315463056... |
1,801.04204 | Influence of misalignments on performance of externally occulted solar
coronagraphs. Application to PROBA-3/ASPIICS | ASPIICS is a novel externally occulted coronagraph that will be launched
onboard the PROBA-3 mission of ESA. The external occulter (EO) will be placed
on one satellite ~150 m ahead of the second satellite with an optical
instrument. During part of each orbit, the satellites will fly in a precise
formation, constituti... | astro-ph.IM astro-ph.SR | aspiics is a novel externally occulted coronagraph that will be launched onboard the proba3 mission of esa the external occulter eo will be placed on one satellite 150 m ahead of the second satellite with an optical instrument during part of each orbit the satellites will fly in a precise formation constituting a giant... | [['aspiics', 'is', 'a', 'novel', 'externally', 'occulted', 'coronagraph', 'that', 'will', 'be', 'launched', 'onboard', 'the', 'proba3', 'mission', 'of', 'esa', 'the', 'external', 'occulter', 'eo', 'will', 'be', 'placed', 'on', 'one', 'satellite', '150', 'm', 'ahead', 'of', 'the', 'second', 'satellite', 'with', 'an', 'o... | [-0.1528221190643702, 0.14162371011530872, -0.08791322494902602, 0.013182674699065674, -0.09609641030534997, -0.0699117294108899, 0.03536716817554177, 0.4226283088987498, -0.23561038739427312, -0.355210696610824, 0.09981435838308499, -0.26410719729181287, -0.11956432797959061, 0.22771978993241518, -0.11014842396232437,... |
1,801.04205 | Determining Projection Constants of Univariate Polynomial Spaces | The long-standing problem of minimal projections is addressed from a
computational point of view. Techniques to determine bounds on the projection
constants of univariate polynomial spaces are presented. The upper bound,
produced by a linear program, and the lower bound, produced by a semidefinite
program exploiting ... | math.NA math.FA math.OC | the longstanding problem of minimal projections is addressed from a computational point of view techniques to determine bounds on the projection constants of univariate polynomial spaces are presented the upper bound produced by a linear program and the lower bound produced by a semidefinite program exploiting the meth... | [['the', 'longstanding', 'problem', 'of', 'minimal', 'projections', 'is', 'addressed', 'from', 'a', 'computational', 'point', 'of', 'view', 'techniques', 'to', 'determine', 'bounds', 'on', 'the', 'projection', 'constants', 'of', 'univariate', 'polynomial', 'spaces', 'are', 'presented', 'the', 'upper', 'bound', 'produce... | [-0.10799433465179956, 0.045161703464992604, -0.047644200465834605, 0.08144692705787622, -0.0751223511881484, -0.11712446616529006, 0.06297866893322046, 0.32745825397332423, -0.3086083931527261, -0.337456189758337, 0.16149799964101663, -0.27185716056104364, -0.0953630620999069, 0.22776151744745157, -0.04015589289463543... |
1,801.04206 | Spiked Monopoles | We introduce the spiked monopole, which is a 't Hooft-Polyakov monopole with
two charged scalar Higgs fields, of which one enjoys a quartic
self-interaction. The free Higgs field behaves as in a BPS monopole, reducing
the inter-monopole repulsion. The other Higgs has a spiked profile similar to a
non-BPS monopole. Us... | hep-th hep-ph | we introduce the spiked monopole which is a t hooftpolyakov monopole with two charged scalar higgs fields of which one enjoys a quartic selfinteraction the free higgs field behaves as in a bps monopole reducing the intermonopole repulsion the other higgs has a spiked profile similar to a nonbps monopole using the metho... | [['we', 'introduce', 'the', 'spiked', 'monopole', 'which', 'is', 'a', 't', 'hooftpolyakov', 'monopole', 'with', 'two', 'charged', 'scalar', 'higgs', 'fields', 'of', 'which', 'one', 'enjoys', 'a', 'quartic', 'selfinteraction', 'the', 'free', 'higgs', 'field', 'behaves', 'as', 'in', 'a', 'bps', 'monopole', 'reducing', 't... | [-0.14432128208697026, 0.216760945613267, -0.05530805342504373, 0.19071695701119903, -0.08956763538394551, -0.1764571520606758, -0.03378277877059414, 0.32292876315119934, -0.14554889266547122, -0.29499121617953306, 0.03506863858936293, -0.3115508395598316, -0.1327315526842674, 0.10778809517057093, 0.01062288496750178, ... |
1,801.04207 | NA62 sensitivity to heavy neutral leptons in the low scale seesaw model | The sensitivity of beam dump experiments to heavy neutral leptons depends on
the relative strength of their couplings to individual lepton flavours in the
Standard Model. We study the impact of present neutrino oscillation data on
these couplings in the minimal type I seesaw model and find that it
significantly const... | hep-ph hep-ex | the sensitivity of beam dump experiments to heavy neutral leptons depends on the relative strength of their couplings to individual lepton flavours in the standard model we study the impact of present neutrino oscillation data on these couplings in the minimal type i seesaw model and find that it significantly constrai... | [['the', 'sensitivity', 'of', 'beam', 'dump', 'experiments', 'to', 'heavy', 'neutral', 'leptons', 'depends', 'on', 'the', 'relative', 'strength', 'of', 'their', 'couplings', 'to', 'individual', 'lepton', 'flavours', 'in', 'the', 'standard', 'model', 'we', 'study', 'the', 'impact', 'of', 'present', 'neutrino', 'oscillat... | [-0.07428982499487964, 0.25034449957976385, -0.015734113774461937, 0.11718719117343426, -0.05656940319708415, -0.14216705200794552, 0.07911323847615027, 0.341089046497031, -0.21807657492214017, -0.3273423218500933, 0.06797564374033495, -0.28548874813131986, -0.0378400321006276, 0.1974759081328687, 0.0462935730798303, 0... |
1,801.04208 | Minkowski Conformal Blocks and the Regge Limit for SYK-like Models | We discuss scattering in a CFT via the conformal partial-wave analysis and
the Regge limit. The focus of this paper is on understanding an OPE with
Minkowski conformal blocks. Starting with a t-channel OPE, it leads to an
expansion for an s-channel scattering amplitude in terms of t-channel
exchanges. By contrasting ... | hep-th | we discuss scattering in a cft via the conformal partialwave analysis and the regge limit the focus of this paper is on understanding an ope with minkowski conformal blocks starting with a tchannel ope it leads to an expansion for an schannel scattering amplitude in terms of tchannel exchanges by contrasting with eucli... | [['we', 'discuss', 'scattering', 'in', 'a', 'cft', 'via', 'the', 'conformal', 'partialwave', 'analysis', 'and', 'the', 'regge', 'limit', 'the', 'focus', 'of', 'this', 'paper', 'is', 'on', 'understanding', 'an', 'ope', 'with', 'minkowski', 'conformal', 'blocks', 'starting', 'with', 'a', 'tchannel', 'ope', 'it', 'leads',... | [-0.11073992039456747, 0.14035073696296307, -0.09082913562854372, 0.06976061904389248, -0.06727511701015845, -0.13958168875491608, -0.004193720879096502, 0.3370943357309019, -0.21033957557418176, -0.20237094699179084, 0.08923510418248644, -0.33064090052294065, -0.15417106840217, 0.14920922289139057, 0.01383642597775002... |
1,801.04209 | Slant H-Toeplitz Operators on the Hardy space | The notion of slant H-Toeplitz operator $V_\phi$ on the Hardy space $H^2$ is
introduced and its characterizations are obtained. We have shown that an
operator on the space $H^2$ is slant H-Toeplitz if and only if its matrix is a
slant H-Toeplitz matrix. In addition the conditions under which slant Toeplitz
and slant ... | math.FA | the notion of slant htoeplitz operator v_phi on the hardy space h2 is introduced and its characterizations are obtained we have shown that an operator on the space h2 is slant htoeplitz if and only if its matrix is a slant htoeplitz matrix in addition the conditions under which slant toeplitz and slant hankel operators... | [['the', 'notion', 'of', 'slant', 'htoeplitz', 'operator', 'v_phi', 'on', 'the', 'hardy', 'space', 'h2', 'is', 'introduced', 'and', 'its', 'characterizations', 'are', 'obtained', 'we', 'have', 'shown', 'that', 'an', 'operator', 'on', 'the', 'space', 'h2', 'is', 'slant', 'htoeplitz', 'if', 'and', 'only', 'if', 'its', 'm... | [-0.13648149160660744, 0.1554454161371048, -0.0073522402934970395, 0.1429074238366147, -0.10184450246649043, -0.09525402242528094, -0.10002106758615663, 0.4833228321926248, -0.29294228758062085, -0.08304723496398618, 0.17981885286280885, -0.34732684532120345, -0.270262828622494, 0.16789857734505448, -0.1331435841838679... |
1,801.0421 | Asymptotic Dirichlet problems in warped products | We study the asymptotic Dirichlet problem for Killing graphs with prescribed
mean curvature $H$ in warped product manifolds $M\times_\varrho \mathbb{R}$. In
the first part of the paper, we prove the existence of Killing graphs with
prescribed boundary on geodesic balls under suitable assumptions on $H$ and the
mean c... | math.DG | we study the asymptotic dirichlet problem for killing graphs with prescribed mean curvature h in warped product manifolds mtimes_varrho mathbbr in the first part of the paper we prove the existence of killing graphs with prescribed boundary on geodesic balls under suitable assumptions on h and the mean curvature of the... | [['we', 'study', 'the', 'asymptotic', 'dirichlet', 'problem', 'for', 'killing', 'graphs', 'with', 'prescribed', 'mean', 'curvature', 'h', 'in', 'warped', 'product', 'manifolds', 'mtimes_varrho', 'mathbbr', 'in', 'the', 'first', 'part', 'of', 'the', 'paper', 'we', 'prove', 'the', 'existence', 'of', 'killing', 'graphs', ... | [-0.17479539588641593, 0.08682167144862059, -0.047121136081413544, 0.04296774937827596, -0.12687127846156193, -0.10573287299313747, -0.028961636843365234, 0.3689113625201999, -0.2515826664791401, -0.2310044265301686, 0.1453252178445623, -0.29375374350039396, -0.10737479295323069, 0.11504412950221997, -0.111689591819680... |
1,801.04211 | Towards Arbitrary Noise Augmentation - Deep Learning for Sampling from
Arbitrary Probability Distributions | Accurate noise modelling is important for training of deep learning
reconstruction algorithms. While noise models are well known for traditional
imaging techniques, the noise distribution of a novel sensor may be difficult
to determine a priori. Therefore, we propose learning arbitrary noise
distributions. To do so, ... | cs.LG stat.ML | accurate noise modelling is important for training of deep learning reconstruction algorithms while noise models are well known for traditional imaging techniques the noise distribution of a novel sensor may be difficult to determine a priori therefore we propose learning arbitrary noise distributions to do so this pap... | [['accurate', 'noise', 'modelling', 'is', 'important', 'for', 'training', 'of', 'deep', 'learning', 'reconstruction', 'algorithms', 'while', 'noise', 'models', 'are', 'well', 'known', 'for', 'traditional', 'imaging', 'techniques', 'the', 'noise', 'distribution', 'of', 'a', 'novel', 'sensor', 'may', 'be', 'difficult', '... | [-0.024500231020855946, 0.05966584070944276, -0.1332676452291491, 0.1102745452182615, -0.0699009540901109, -0.17269392215184398, 0.07069035994712837, 0.45513320469356083, -0.28992397738685766, -0.34520901343785226, 0.07043661384263655, -0.23924355371041106, -0.15750192812240155, 0.1395995359586135, -0.12437748749064165... |
1,801.04212 | Multinomial logistic model for coinfection diagnosis between arbovirus
and malaria in Kedougou | In tropical regions, populations continue to suffer morbidity and mortality
from malaria and arboviral diseases. In Kedougou (Senegal), these illnesses are
all endemic due to the climate and its geographical position. The
co-circulation of malaria parasites and arboviruses can explain the observation
of coinfected ca... | stat.AP math.ST stat.ML stat.TH | in tropical regions populations continue to suffer morbidity and mortality from malaria and arboviral diseases in kedougou senegal these illnesses are all endemic due to the climate and its geographical position the cocirculation of malaria parasites and arboviruses can explain the observation of coinfected cases indee... | [['in', 'tropical', 'regions', 'populations', 'continue', 'to', 'suffer', 'morbidity', 'and', 'mortality', 'from', 'malaria', 'and', 'arboviral', 'diseases', 'in', 'kedougou', 'senegal', 'these', 'illnesses', 'are', 'all', 'endemic', 'due', 'to', 'the', 'climate', 'and', 'its', 'geographical', 'position', 'the', 'cocir... | [-0.054179003777508644, 0.11348333040611493, -0.021644351181194118, 0.13918797455147544, -0.06326716382582692, -0.18557972531565237, 0.11724719286696868, 0.349947330095041, -0.19009719416707954, -0.2766344902615142, 0.16749302869622967, -0.3402787652999505, -0.18884926681268976, 0.1765911192048525, -0.17931854110245066... |
1,801.04213 | Gauss-Bonnet dark energy on Ho\v{r}ava-Lifshitz cosmology | We investigate the Gauss-Bonnet dark energy model and its deformed version on
Ho\v{r}ava-Lifshitz cosmology, which belongs to the class of cosmologies
obtained from the so-called projectable version of Ho\v{r}ava-Lifshitz gravity.
In particular, we investigate the bulk/boundary interaction in this scenario
through th... | gr-qc hep-th | we investigate the gaussbonnet dark energy model and its deformed version on hovravalifshitz cosmology which belongs to the class of cosmologies obtained from the socalled projectable version of hovravalifshitz gravity in particular we investigate the bulkboundary interaction in this scenario through the q function whi... | [['we', 'investigate', 'the', 'gaussbonnet', 'dark', 'energy', 'model', 'and', 'its', 'deformed', 'version', 'on', 'hovravalifshitz', 'cosmology', 'which', 'belongs', 'to', 'the', 'class', 'of', 'cosmologies', 'obtained', 'from', 'the', 'socalled', 'projectable', 'version', 'of', 'hovravalifshitz', 'gravity', 'in', 'pa... | [-0.1276022277148017, 0.11349304519085722, -0.1526507101318037, 0.12505161437967963, -0.061919898268851366, -0.1169867387761108, 0.015697486776943236, 0.3052014905112711, -0.28796952082352206, -0.28572617333213035, 0.08588960994966328, -0.24576370902359485, -0.11510995543900539, 0.12849244761111384, -0.0342241834341125... |
1,801.04214 | Heuristics in direction of a p-adic Brauer--Siegel theorem | Let p be a fixed prime number. Let K be a totally real number field of
discriminant D\_K and let T\_K be the torsion group of the Galois group of the
maximal abelian p-ramified pro-p-extension of K (under Leopoldt's conjecture).
We conjecture the existence of a constant C\_p>0 such that log(\#T\_K) $\le$
C\_p log(\sq... | math.NT | let p be a fixed prime number let k be a totally real number field of discriminant d_k and let t_k be the torsion group of the galois group of the maximal abelian pramified propextension of k under leopoldts conjecture we conjecture the existence of a constant c_p0 such that logt_k le c_p logsqrtd_k when k varies in so... | [['let', 'p', 'be', 'a', 'fixed', 'prime', 'number', 'let', 'k', 'be', 'a', 'totally', 'real', 'number', 'field', 'of', 'discriminant', 'd_k', 'and', 'let', 't_k', 'be', 'the', 'torsion', 'group', 'of', 'the', 'galois', 'group', 'of', 'the', 'maximal', 'abelian', 'pramified', 'propextension', 'of', 'k', 'under', 'leopo... | [-0.2189600383973725, 0.11291009931278134, -0.1333364540792351, 0.0398825365512893, -0.11389453027757111, -0.15678720207264027, 0.050090124835531234, 0.2630058366105591, -0.2801212579499753, -0.2629172055632191, 0.0607057036456243, -0.25443056626393207, -0.11543237523141282, 0.2228501006756372, -0.07608431314485316, -0... |
1,801.04215 | A unifying Perron-Frobenius theorem for nonnegative tensors via
multi-homogeneous maps | We introduce the concept of shape partition of a tensor and formulate a
general tensor eigenvalue problem that includes all previously studied
eigenvalue problems as special cases. We formulate irreducibility and symmetry
properties of a nonnegative tensor $T$ in terms of the associated shape
partition. We recast the... | math.SP cs.DM cs.NA math.FA math.NA math.OC | we introduce the concept of shape partition of a tensor and formulate a general tensor eigenvalue problem that includes all previously studied eigenvalue problems as special cases we formulate irreducibility and symmetry properties of a nonnegative tensor t in terms of the associated shape partition we recast the eigen... | [['we', 'introduce', 'the', 'concept', 'of', 'shape', 'partition', 'of', 'a', 'tensor', 'and', 'formulate', 'a', 'general', 'tensor', 'eigenvalue', 'problem', 'that', 'includes', 'all', 'previously', 'studied', 'eigenvalue', 'problems', 'as', 'special', 'cases', 'we', 'formulate', 'irreducibility', 'and', 'symmetry', '... | [-0.12318031327249329, 0.02220101169783805, -0.08131384903748261, 0.08548334779668233, -0.11756351205222614, -0.1319821042115571, 0.0018782622407984416, 0.3115557088806737, -0.2904204045914755, -0.2317833990377725, 0.12731342377774724, -0.21531044108209632, -0.18544940491107706, 0.13197045082314185, -0.0436858670577525... |
1,801.04216 | Poincar\'e inequality on complete Riemannian manifolds with Ricci
curvature bounded below | We prove that complete Riemannian manifolds with polynomial growth and Ricci
curvature bounded from below, admit uniform Poincar\'e inequalities. A global,
uniform Poincar\'e inequality for horospheres in the universal cover of a
closed, $n$-dimensional Riemannian manifold with pinched negative sectional
curvature fo... | math.DG | we prove that complete riemannian manifolds with polynomial growth and ricci curvature bounded from below admit uniform poincare inequalities a global uniform poincare inequality for horospheres in the universal cover of a closed ndimensional riemannian manifold with pinched negative sectional curvature follows as a co... | [['we', 'prove', 'that', 'complete', 'riemannian', 'manifolds', 'with', 'polynomial', 'growth', 'and', 'ricci', 'curvature', 'bounded', 'from', 'below', 'admit', 'uniform', 'poincare', 'inequalities', 'a', 'global', 'uniform', 'poincare', 'inequality', 'for', 'horospheres', 'in', 'the', 'universal', 'cover', 'of', 'a',... | [-0.1779692639907201, 0.10640390339410967, -0.08950690821641022, 0.11077953005830447, -0.1723451583749718, -0.24311987050912445, -0.1000441684284144, 0.3151540610421863, -0.28859345249754065, -0.1723013492508067, 0.13623132125940174, -0.27481427523824903, -0.1395978910745018, 0.19621116363753874, -0.17650066529297168, ... |
1,801.04217 | Early gray dust formation in the type IIn SN 2005ip | The physical characteristics of dust formed in supernovae is poorly known. In
this paper, we investigate the extinction properties of dust formed in the type
IIn SN 2005ip. The observed light curves of SN 2005ip all exhibit a sudden drop
around 50 days after discovery. This has been attributed to dust formation in
th... | astro-ph.SR astro-ph.HE | the physical characteristics of dust formed in supernovae is poorly known in this paper we investigate the extinction properties of dust formed in the type iin sn 2005ip the observed light curves of sn 2005ip all exhibit a sudden drop around 50 days after discovery this has been attributed to dust formation in the dens... | [['the', 'physical', 'characteristics', 'of', 'dust', 'formed', 'in', 'supernovae', 'is', 'poorly', 'known', 'in', 'this', 'paper', 'we', 'investigate', 'the', 'extinction', 'properties', 'of', 'dust', 'formed', 'in', 'the', 'type', 'iin', 'sn', '2005ip', 'the', 'observed', 'light', 'curves', 'of', 'sn', '2005ip', 'all... | [-0.05365443985471204, 0.11361342794623346, -0.09393783913474513, 0.06327457134728852, -0.046161749861607135, -0.09951812753317767, 0.08967246799293871, 0.45231998636978404, -0.24505029670621978, -0.32110729488676, 0.05214390828440042, -0.31240336290352283, -0.06818918067298524, 0.16827665097356592, -0.0728260158459771... |
1,801.04218 | Coexistence of several currencies in presence of increasing returns to
adoption | We present a simplistic model of the competition between different
currencies. Each individual is free to choose the currency that minimizes his
transaction costs, which arise whenever his exchanging relations have chosen a
different currency. We show that competition between currencies does not
necessarily converge ... | q-fin.GN physics.soc-ph | we present a simplistic model of the competition between different currencies each individual is free to choose the currency that minimizes his transaction costs which arise whenever his exchanging relations have chosen a different currency we show that competition between currencies does not necessarily converge to th... | [['we', 'present', 'a', 'simplistic', 'model', 'of', 'the', 'competition', 'between', 'different', 'currencies', 'each', 'individual', 'is', 'free', 'to', 'choose', 'the', 'currency', 'that', 'minimizes', 'his', 'transaction', 'costs', 'which', 'arise', 'whenever', 'his', 'exchanging', 'relations', 'have', 'chosen', 'a... | [-0.17877845940490564, 0.16418774300565322, -0.10378947360130648, 0.10176409016363323, -0.06362177129834891, -0.19206231418589595, 0.1149116029497236, 0.3763578110933304, -0.3060361174121499, -0.24413822896778584, 0.03520970865152776, -0.35309866244594257, -0.12014960193696121, 0.10279654727006952, -0.11739333886653185... |
1,801.04219 | Abbott-Deser energy in connection with Thirring's superpotentials | We linearize vacuum Einstein field equations with a cosmological constant
around a curved background to elaborate on the reconstruction of the
Abbott-Deser charges and incorporate a spin connection into the definition
using the algebra of differential forms on a given curved background spacetime.
| gr-qc | we linearize vacuum einstein field equations with a cosmological constant around a curved background to elaborate on the reconstruction of the abbottdeser charges and incorporate a spin connection into the definition using the algebra of differential forms on a given curved background spacetime | [['we', 'linearize', 'vacuum', 'einstein', 'field', 'equations', 'with', 'a', 'cosmological', 'constant', 'around', 'a', 'curved', 'background', 'to', 'elaborate', 'on', 'the', 'reconstruction', 'of', 'the', 'abbottdeser', 'charges', 'and', 'incorporate', 'a', 'spin', 'connection', 'into', 'the', 'definition', 'using',... | [-0.1559009480095187, 0.07904075170585582, -0.10438070688829866, 0.06331961931184281, -0.15760878651121327, -0.1085902986138366, -0.08128159679472446, 0.2998033377320267, -0.19080309735795178, -0.2879847333181736, 0.07264746316210476, -0.2564025973511297, -0.09318633975331174, 0.1340899954571627, -0.05423823813366335, ... |
1,801.0422 | Nonlinearity-induced localization in a periodically-driven semi-discrete
system | We demonstrate that nonlinearity plays a constructive role in supporting the
robustness of dynamical localization in a model which is discrete, in one
dimension and continuous in the orthogonal one. In the linear regime,
time-periodic modulation of the gradient strength along the discrete axis leads
to the usual rapi... | nlin.PS physics.atom-ph | we demonstrate that nonlinearity plays a constructive role in supporting the robustness of dynamical localization in a model which is discrete in one dimension and continuous in the orthogonal one in the linear regime timeperiodic modulation of the gradient strength along the discrete axis leads to the usual rapid spre... | [['we', 'demonstrate', 'that', 'nonlinearity', 'plays', 'a', 'constructive', 'role', 'in', 'supporting', 'the', 'robustness', 'of', 'dynamical', 'localization', 'in', 'a', 'model', 'which', 'is', 'discrete', 'in', 'one', 'dimension', 'and', 'continuous', 'in', 'the', 'orthogonal', 'one', 'in', 'the', 'linear', 'regime'... | [-0.21616558732446467, 0.19883240578309425, -0.06163768758674586, 0.0346459608518122, -0.032580477061063644, -0.15621107747999602, -0.013840710467919431, 0.37504570973612883, -0.28636424278490025, -0.19627307287168386, 0.05959050809632581, -0.23232488210617316, -0.18856415675842378, 0.17719114246307918, 0.0022561976981... |
1,801.04221 | Radiation- and pair-loaded shocks | We consider the structure of mildly relativistic shocks in dense media,
taking into account the radiation and pair loading, and diffusive radiation
energy transfer within the flow. For increasing shock velocity (increasing
post-shock temperature), the first important effect is the efficient energy
redistribution by r... | astro-ph.HE | we consider the structure of mildly relativistic shocks in dense media taking into account the radiation and pair loading and diffusive radiation energy transfer within the flow for increasing shock velocity increasing postshock temperature the first important effect is the efficient energy redistribution by radiation ... | [['we', 'consider', 'the', 'structure', 'of', 'mildly', 'relativistic', 'shocks', 'in', 'dense', 'media', 'taking', 'into', 'account', 'the', 'radiation', 'and', 'pair', 'loading', 'and', 'diffusive', 'radiation', 'energy', 'transfer', 'within', 'the', 'flow', 'for', 'increasing', 'shock', 'velocity', 'increasing', 'po... | [-0.1287110548629056, 0.21463539795536596, -0.05926868049241709, 0.07511006618964501, -0.06679942503401506, -0.09412828053066892, -0.008157873768285508, 0.35588269869959543, -0.28382770502052845, -0.2825854516455105, 0.05436881224621117, -0.2672076043007629, 0.030513600015731914, 0.17503902564723312, 0.0977098455482591... |
1,801.04222 | Crater mound formation by wind erosion on Mars | Most of Mars' ancient sedimentary rocks by volume are in wind-eroded
sedimentary mounds, but the connections between mound form and wind erosion are
unclear. We perform mesoscale simulations of different crater and mound
morphologies to understand the formation of sedimentary mounds. As crater depth
increases, slope ... | astro-ph.EP | most of mars ancient sedimentary rocks by volume are in winderoded sedimentary mounds but the connections between mound form and wind erosion are unclear we perform mesoscale simulations of different crater and mound morphologies to understand the formation of sedimentary mounds as crater depth increases slope winds pr... | [['most', 'of', 'mars', 'ancient', 'sedimentary', 'rocks', 'by', 'volume', 'are', 'in', 'winderoded', 'sedimentary', 'mounds', 'but', 'the', 'connections', 'between', 'mound', 'form', 'and', 'wind', 'erosion', 'are', 'unclear', 'we', 'perform', 'mesoscale', 'simulations', 'of', 'different', 'crater', 'and', 'mound', 'm... | [-0.06465459761228137, 0.22572183567231172, -0.10812673979528303, 0.0798094774552809, -0.0617527291522788, -0.038182494042468776, -0.017612216237180046, 0.34366250711635415, -0.21723765363570377, -0.3112719711455347, 0.11623302185930899, -0.2895395530446827, -0.12020420981341688, 0.22745119349508008, -0.138060059544908... |
1,801.04223 | Machine Intelligence Techniques for Next-Generation Context-Aware
Wireless Networks | The next generation wireless networks (i.e. 5G and beyond), which would be
extremely dynamic and complex due to the ultra-dense deployment of
heterogeneous networks (HetNets), poses many critical challenges for network
planning, operation, management and troubleshooting. At the same time,
generation and consumption o... | cs.IT math.IT | the next generation wireless networks ie 5g and beyond which would be extremely dynamic and complex due to the ultradense deployment of heterogeneous networks hetnets poses many critical challenges for network planning operation management and troubleshooting at the same time generation and consumption of wireless data... | [['the', 'next', 'generation', 'wireless', 'networks', 'ie', '5g', 'and', 'beyond', 'which', 'would', 'be', 'extremely', 'dynamic', 'and', 'complex', 'due', 'to', 'the', 'ultradense', 'deployment', 'of', 'heterogeneous', 'networks', 'hetnets', 'poses', 'many', 'critical', 'challenges', 'for', 'network', 'planning', 'op... | [-0.1928251620356763, 0.014411947444972137, -0.0057081393978517985, 0.021360783254899814, -0.12397711721208432, -0.20453727459939924, 0.06664036028188369, 0.4086656511153864, -0.2882144132952975, -0.3176786988305495, 0.12590714541122155, -0.23182664803107794, -0.20807314888452705, 0.22081864643032137, -0.11148272897342... |
1,801.04224 | Reducibility of first order linear operators on tori via Moser's theorem | In this paper we prove reducibility of classes of linear first order
operators on tori by applying a generalization of Moser's theorem on
straightening of vector fields on a torus. We consider vector fields which are
a $C^\infty$ perturbations of a constant vector field, and prove that they are
conjugated --by a $C^\... | math.AP | in this paper we prove reducibility of classes of linear first order operators on tori by applying a generalization of mosers theorem on straightening of vector fields on a torus we consider vector fields which are a cinfty perturbations of a constant vector field and prove that they are conjugated by a cinfty torus di... | [['in', 'this', 'paper', 'we', 'prove', 'reducibility', 'of', 'classes', 'of', 'linear', 'first', 'order', 'operators', 'on', 'tori', 'by', 'applying', 'a', 'generalization', 'of', 'mosers', 'theorem', 'on', 'straightening', 'of', 'vector', 'fields', 'on', 'a', 'torus', 'we', 'consider', 'vector', 'fields', 'which', 'a... | [-0.1823188642871687, 0.10303039922386066, -0.07859615801912662, 0.048847552940768424, -0.0851578772555013, -0.08514905629238782, 0.007856814021898703, 0.3129572379082896, -0.3123031400485348, -0.21007049052428653, 0.15100079223972154, -0.23348460573958987, -0.15203339354086665, 0.20250903413353757, -0.1176188716821315... |
1,801.04225 | Biexciton fine structure in monolayer transition metal dichalcogenides | The optical properties of atomically thin transition metal dichalcogenide
(TMDC) semiconductors are shaped by the emergence of correlated many-body
complexes due to strong Coulomb interaction. Exceptional electron-hole exchange
predestines TMDCs to study fundamental and applied properties of Coulomb
complexes such as... | cond-mat.mtrl-sci | the optical properties of atomically thin transition metal dichalcogenide tmdc semiconductors are shaped by the emergence of correlated manybody complexes due to strong coulomb interaction exceptional electronhole exchange predestines tmdcs to study fundamental and applied properties of coulomb complexes such as valley... | [['the', 'optical', 'properties', 'of', 'atomically', 'thin', 'transition', 'metal', 'dichalcogenide', 'tmdc', 'semiconductors', 'are', 'shaped', 'by', 'the', 'emergence', 'of', 'correlated', 'manybody', 'complexes', 'due', 'to', 'strong', 'coulomb', 'interaction', 'exceptional', 'electronhole', 'exchange', 'predestine... | [-0.12406789702458346, 0.1598557625694492, -0.01543475080362274, 0.11585670391962465, 0.004270039591265107, -0.1959637770251859, 0.0804494754640943, 0.5268620132614358, -0.2313208123352252, -0.2739718988867236, -0.0849957463472486, -0.29902083169491517, -0.1648342816577274, 0.19898445778138316, 0.08000647620342317, -0.... |
1,801.04226 | "Divide and Conquer" Semiclassical Molecular Dynamics: A practical
method for Spectroscopic calculations of High Dimensional Molecular Systems | We extensively describe our recently established "divide-and-conquer"
semiclassical method [M. Ceotto, G. Di Liberto and R. Conte, Phys. Rev. Lett.
119, 010401 (2017)] and propose a new implementation of it to increase the
accuracy of results. The technique permits to perform spectroscopic
calculations of high dimens... | physics.chem-ph quant-ph | we extensively describe our recently established divideandconquer semiclassical method m ceotto g di liberto and r conte phys rev lett 119 010401 2017 and propose a new implementation of it to increase the accuracy of results the technique permits to perform spectroscopic calculations of high dimensional systems by div... | [['we', 'extensively', 'describe', 'our', 'recently', 'established', 'divideandconquer', 'semiclassical', 'method', 'm', 'ceotto', 'g', 'di', 'liberto', 'and', 'r', 'conte', 'phys', 'rev', 'lett', '119', '010401', '2017', 'and', 'propose', 'a', 'new', 'implementation', 'of', 'it', 'to', 'increase', 'the', 'accuracy', '... | [-0.07381152403245048, 0.02927051293174865, -0.08840367405865733, 0.02035602839221118, -0.060755742770408724, -0.14147823560244574, 0.08983576883792167, 0.3639007074840737, -0.1828345352891853, -0.3163834056081842, 0.02079466604228898, -0.24730533723809783, -0.16215664897119184, 0.2142798644915038, -0.03954193156305186... |
1,801.04227 | Observation of the Unconventional Photon Blockade in the Microwave
Domain | We have observed the unconventional photon blockade effect for microwave
photons using two coupled superconducting resonators. As opposed to the
conventional blockade, only weakly nonlinear resonators are required. The
blockade is revealed through measurements of the second order correlation
function $g^{(2)}(t)$ of ... | quant-ph | we have observed the unconventional photon blockade effect for microwave photons using two coupled superconducting resonators as opposed to the conventional blockade only weakly nonlinear resonators are required the blockade is revealed through measurements of the second order correlation function g2t of the microwave ... | [['we', 'have', 'observed', 'the', 'unconventional', 'photon', 'blockade', 'effect', 'for', 'microwave', 'photons', 'using', 'two', 'coupled', 'superconducting', 'resonators', 'as', 'opposed', 'to', 'the', 'conventional', 'blockade', 'only', 'weakly', 'nonlinear', 'resonators', 'are', 'required', 'the', 'blockade', 'is... | [-0.20739537572635094, 0.23014765149249192, -0.041467879277964435, 0.03421674009240676, -0.02717403944448701, -0.17503192544072158, 0.012291759441030167, 0.3587947168077032, -0.18549986132642343, -0.31643482412965523, -0.04428513741835819, -0.3644200965229954, -0.055437625031031314, 0.24459772650152445, 0.0651962051509... |
1,801.04228 | Detection of the Aromatic Molecule Benzonitrile ($c$-C$_6$H$_5$CN) in
the Interstellar Medium | Polycyclic aromatic hydrocarbons and polycyclic aromatic nitrogen
heterocycles are thought to be widespread throughout the Universe, because
these classes of molecules are probably responsible for the unidentified
infrared bands, a set of emission features seen in numerous Galactic and
extragalactic sources. Despite ... | astro-ph.GA | polycyclic aromatic hydrocarbons and polycyclic aromatic nitrogen heterocycles are thought to be widespread throughout the universe because these classes of molecules are probably responsible for the unidentified infrared bands a set of emission features seen in numerous galactic and extragalactic sources despite their... | [['polycyclic', 'aromatic', 'hydrocarbons', 'and', 'polycyclic', 'aromatic', 'nitrogen', 'heterocycles', 'are', 'thought', 'to', 'be', 'widespread', 'throughout', 'the', 'universe', 'because', 'these', 'classes', 'of', 'molecules', 'are', 'probably', 'responsible', 'for', 'the', 'unidentified', 'infrared', 'bands', 'a'... | [-0.09385087942196564, 0.08653617374471981, 0.014978669456798922, 0.06753395552831618, -0.026031385429351676, -0.07365181941369718, 0.0518038529119539, 0.4937424355779182, -0.25279508162797854, -0.270077235234732, -0.020556483763820407, -0.292828559469093, -0.04908020538701253, 0.09603690433908593, 0.016436274777251212... |
1,801.04229 | List Decoding of Locally Repairable Codes | We show that locally repairable codes (LRCs) can be list decoded efficiently
beyond the Johnson radius for a large range of parameters by utilizing the
local error correction capabilities. The new decoding radius is derived and the
asymptotic behavior is analyzed. We give a general list decoding algorithm for
LRCs th... | cs.IT math.IT | we show that locally repairable codes lrcs can be list decoded efficiently beyond the johnson radius for a large range of parameters by utilizing the local error correction capabilities the new decoding radius is derived and the asymptotic behavior is analyzed we give a general list decoding algorithm for lrcs that ach... | [['we', 'show', 'that', 'locally', 'repairable', 'codes', 'lrcs', 'can', 'be', 'list', 'decoded', 'efficiently', 'beyond', 'the', 'johnson', 'radius', 'for', 'a', 'large', 'range', 'of', 'parameters', 'by', 'utilizing', 'the', 'local', 'error', 'correction', 'capabilities', 'the', 'new', 'decoding', 'radius', 'is', 'de... | [-0.19588682552178702, 0.006689667098402131, -0.06259083344290654, 0.1006282708131248, -0.033921282548435974, -0.265734429337384, 0.0873398176908236, 0.39119902176075966, -0.2846727005109705, -0.2827462503343992, 0.12472804617230385, -0.2070580585859716, -0.1571972841950904, 0.23032829713547368, -0.18605563182640691, 0... |
1,801.0423 | Asymptotics for the resolvent equation associated to the game-theoretic
$p$-laplacian | We consider the (viscosity) solution $u^\varepsilon$ of the elliptic equation
$\varepsilon^2\Delta_p^G u= u$ in a domain (not necessarily bounded),
satisfying $u=1$ on its boundary. Here, $\Delta_p^G$ is the {\it game-theoretic
or normalized $p$-laplacian}. We derive asymptotic formulas for $\varepsilon\to
0^+$ invol... | math.AP | we consider the viscosity solution uvarepsilon of the elliptic equation varepsilon2delta_pg u u in a domain not necessarily bounded satisfying u1 on its boundary here delta_pg is the it gametheoretic or normalized plaplacian we derive asymptotic formulas for varepsilonto 0 involving the values of uvarepsilon in the spi... | [['we', 'consider', 'the', 'viscosity', 'solution', 'uvarepsilon', 'of', 'the', 'elliptic', 'equation', 'varepsilon2delta_pg', 'u', 'u', 'in', 'a', 'domain', 'not', 'necessarily', 'bounded', 'satisfying', 'u1', 'on', 'its', 'boundary', 'here', 'delta_pg', 'is', 'the', 'it', 'gametheoretic', 'or', 'normalized', 'plaplac... | [-0.1684591574273233, 0.03636747036643069, -0.07418014921633334, 0.042545125799671075, -0.09012625704455221, -0.14363157539360824, 0.04825655646600771, 0.2832401227848283, -0.28059537600907875, -0.1803416010292097, 0.14264162714812562, -0.3146661828518256, -0.11059058750123214, 0.15341110647945055, -0.10222988291800787... |
1,801.04231 | Measurements of differential $t\bar{t}$ production cross sections at CMS | An overview of recent measurements of differential top quark pair production
cross sections performed by the CMS experiment at the LHC is presented.
Measurements at different proton-proton center-of-mass energies are available
using the dilepton, lepton+jets, and all-jets decay channels of the top quark.
In addition ... | hep-ex | an overview of recent measurements of differential top quark pair production cross sections performed by the cms experiment at the lhc is presented measurements at different protonproton centerofmass energies are available using the dilepton leptonjets and alljets decay channels of the top quark in addition to the meas... | [['an', 'overview', 'of', 'recent', 'measurements', 'of', 'differential', 'top', 'quark', 'pair', 'production', 'cross', 'sections', 'performed', 'by', 'the', 'cms', 'experiment', 'at', 'the', 'lhc', 'is', 'presented', 'measurements', 'at', 'different', 'protonproton', 'centerofmass', 'energies', 'are', 'available', 'u... | [-0.04271615549274113, 0.2436439836067502, -0.09732830992940328, 0.09261645839002955, -0.028066965660242284, -0.10520330205883668, 0.01908838756220496, 0.3508847574500934, -0.15619775482412915, -0.29979232109111287, 0.0018825184553861618, -0.3925016901496312, 0.10116614498926893, 0.192677808053913, 0.10737244551596434,... |
1,801.04232 | Physical Principles of Retroviral Integration in the Human Genome | Certain retroviruses, including HIV, insert their DNA in a non-random
fraction of the host genome via poorly understood selection mechanisms. Here,
we develop a biophysical model for retroviral integrations as stochastic and
quasi-equilibrium topological reconnections between polymers. We discover that
physical effec... | q-bio.SC cond-mat.soft physics.bio-ph | certain retroviruses including hiv insert their dna in a nonrandom fraction of the host genome via poorly understood selection mechanisms here we develop a biophysical model for retroviral integrations as stochastic and quasiequilibrium topological reconnections between polymers we discover that physical effects such a... | [['certain', 'retroviruses', 'including', 'hiv', 'insert', 'their', 'dna', 'in', 'a', 'nonrandom', 'fraction', 'of', 'the', 'host', 'genome', 'via', 'poorly', 'understood', 'selection', 'mechanisms', 'here', 'we', 'develop', 'a', 'biophysical', 'model', 'for', 'retroviral', 'integrations', 'as', 'stochastic', 'and', 'q... | [-0.10753567011406025, 0.15898813396692277, -0.0024692872042457264, 0.1125172079188269, -0.043821917672175914, -0.1554220334223161, 0.08739532325494413, 0.4067655054293573, -0.27446009249581643, -0.2800152405599753, 0.06275144916338225, -0.2389258512109518, -0.23819744752099117, 0.14773655560139257, -0.0347858428367180... |
1,801.04233 | Artin group injection in the Hecke algebra for right-angled groups | We prove some injectivity results: that a Coxeter monoid $\mathbb{Z}$-algebra
(or $0$-Hecke algebra) injects in the incidence $\mathbb{Z}$-algebra of the
corresponding Bruhat poset, for any Coxeter group; that the Hecke algebra of a
right-angled Coxeter group injects in the Coxeter monoid
$\mathbb{Z}[q,q^{-1}]$-algeb... | math.RT | we prove some injectivity results that a coxeter monoid mathbbzalgebra or 0hecke algebra injects in the incidence mathbbzalgebra of the corresponding bruhat poset for any coxeter group that the hecke algebra of a rightangled coxeter group injects in the coxeter monoid mathbbzqq1algebra and then in the incidence mathbbz... | [['we', 'prove', 'some', 'injectivity', 'results', 'that', 'a', 'coxeter', 'monoid', 'mathbbzalgebra', 'or', '0hecke', 'algebra', 'injects', 'in', 'the', 'incidence', 'mathbbzalgebra', 'of', 'the', 'corresponding', 'bruhat', 'poset', 'for', 'any', 'coxeter', 'group', 'that', 'the', 'hecke', 'algebra', 'of', 'a', 'right... | [-0.18078237207185838, 0.12736973341980634, -0.0919405947369273, 0.003935430459277604, -0.1778099093115538, -0.1288913310735777, -0.0011655460262010174, 0.32755409928178914, -0.49888426584181605, -0.12085269282381701, 0.11201436144440004, -0.2834837221570553, -0.11450707282800908, 0.1710532755035186, -0.236877534238080... |
1,801.04234 | Gas cell density characterization for laser wakefield acceleration | In the design of laser plasma electron injectors for multi-stage laser driven
wakefield accelerators, the control of plasma density is a key element to
stabilize the acceleration process. A cell with variable parameters is used to
confine the gas and tailor the density profile. The gas filling process was
characteriz... | physics.acc-ph physics.plasm-ph | in the design of laser plasma electron injectors for multistage laser driven wakefield accelerators the control of plasma density is a key element to stabilize the acceleration process a cell with variable parameters is used to confine the gas and tailor the density profile the gas filling process was characterized bot... | [['in', 'the', 'design', 'of', 'laser', 'plasma', 'electron', 'injectors', 'for', 'multistage', 'laser', 'driven', 'wakefield', 'accelerators', 'the', 'control', 'of', 'plasma', 'density', 'is', 'a', 'key', 'element', 'to', 'stabilize', 'the', 'acceleration', 'process', 'a', 'cell', 'with', 'variable', 'parameters', 'i... | [-0.07433235658359952, 0.17026450540969504, -0.07778635524966299, 0.02465335394527814, 0.016215296454747466, -0.11825483109544407, 0.022277808386555062, 0.4142859260294032, -0.24778913339956643, -0.3177428221171524, 0.05816682917437457, -0.22727936051756223, -0.05921056151310814, 0.21195897507540723, 0.0201956384636937... |
1,801.04235 | The characteristic functions of quantum heat with baths at different
temperatures | This paper is about quantum heat defined as the change in energy of a bath
during a process. The presentation takes into account recent developments in
classical strong-coupling thermodynamics, and addresses a version of quantum
heat which satisfies quantum-classical correspondence. The characteristic
function and th... | cond-mat.stat-mech quant-ph | this paper is about quantum heat defined as the change in energy of a bath during a process the presentation takes into account recent developments in classical strongcoupling thermodynamics and addresses a version of quantum heat which satisfies quantumclassical correspondence the characteristic function and the full ... | [['this', 'paper', 'is', 'about', 'quantum', 'heat', 'defined', 'as', 'the', 'change', 'in', 'energy', 'of', 'a', 'bath', 'during', 'a', 'process', 'the', 'presentation', 'takes', 'into', 'account', 'recent', 'developments', 'in', 'classical', 'strongcoupling', 'thermodynamics', 'and', 'addresses', 'a', 'version', 'of'... | [-0.09166251589671116, 0.1550263956316154, -0.12231331247497688, 0.045458923587764065, -0.04552757323465564, -0.14222938444211403, 0.04446853928119791, 0.292621800665405, -0.2617259114642035, -0.28406141904098064, 0.050811295954256576, -0.31082938162779267, -0.09757325518558818, 0.2561842694412917, -0.05498285346918485... |
1,801.04236 | A Manin-Mumford theorem for the maximal compact subgroup of a universal
vectorial extension of a product of elliptic curves | We study the intersection of an algebraic variety with the maximal compact
subgroup of a universal vectorial extension of a product of elliptic curves.
For this intersection we show a Manin-Mumford type statement. This answers some
questions posed by Corvaja-Masser-Zannier which arose in connection with their
investi... | math.NT | we study the intersection of an algebraic variety with the maximal compact subgroup of a universal vectorial extension of a product of elliptic curves for this intersection we show a maninmumford type statement this answers some questions posed by corvajamasserzannier which arose in connection with their investigation ... | [['we', 'study', 'the', 'intersection', 'of', 'an', 'algebraic', 'variety', 'with', 'the', 'maximal', 'compact', 'subgroup', 'of', 'a', 'universal', 'vectorial', 'extension', 'of', 'a', 'product', 'of', 'elliptic', 'curves', 'for', 'this', 'intersection', 'we', 'show', 'a', 'maninmumford', 'type', 'statement', 'this', ... | [-0.1871521644199551, 0.04094317266276063, -0.1453820289649322, 0.06829323872166165, -0.10672011855058372, -0.11362659153765288, 0.06187902499874264, 0.27825266239627944, -0.30155513681455565, -0.2589414133611372, 0.14069282178573658, -0.23141905539116617, -0.14133713289826982, 0.24937203471248937, -0.1547791556735381,... |
1,801.04237 | Inverse problem of potential theory | P. Novikov in 1938 has proved that if $u_1(x)=u_2(x)$ for $|x|>R$, where
$R>0$ is a large number, $$u_j(x):=\int_{D_j}g_0(x,y)dy, \quad g_0(x,y):=\frac
1 {4\pi |x-y|},$$ and $D_j\subset \mathbb{R}^3$, $j=1,2,$ $D_j\subset B_R$, are
bounded, connected, smooth domains, star-shaped with respect to a common point,
then $... | math.AP | p novikov in 1938 has proved that if u_1xu_2x for xr where r0 is a large number u_jxint_d_jg_0xydy quad g_0xyfrac 1 4pi xy and d_jsubset mathbbr3 j12 d_jsubset b_r are bounded connected smooth domains starshaped with respect to a common point then d_1d_2 here b_r x xle r our basic results are a the removal of the assum... | [['p', 'novikov', 'in', '1938', 'has', 'proved', 'that', 'if', 'u_1xu_2x', 'for', 'xr', 'where', 'r0', 'is', 'a', 'large', 'number', 'u_jxint_d_jg_0xydy', 'quad', 'g_0xyfrac', '1', '4pi', 'xy', 'and', 'd_jsubset', 'mathbbr3', 'j12', 'd_jsubset', 'b_r', 'are', 'bounded', 'connected', 'smooth', 'domains', 'starshaped', '... | [-0.19700159730346894, 0.11263317679558163, -0.006878178502465117, 0.0011321553550981756, -0.07293267559056738, -0.22743531174144183, -0.014686789446585309, 0.31712236038633973, -0.30424287358577223, -0.165127034553985, 0.09832140651595747, -0.34423572833425015, -0.0848814129358393, 0.16390922134635091, -0.090508239680... |
1,801.04238 | Hadronic light-by-light scattering contribution to the muon g-2 on the
lattice | We briefly review several activities at Mainz related to hadronic
light-by-light scattering (HLbL) using lattice QCD. First we present a
position-space approach to the HLbL contribution in the muon g-2, where we
focus on exploratory studies of the pion-pole contribution in a simple model
and the lepton loop in QED in... | hep-lat hep-ph | we briefly review several activities at mainz related to hadronic lightbylight scattering hlbl using lattice qcd first we present a positionspace approach to the hlbl contribution in the muon g2 where we focus on exploratory studies of the pionpole contribution in a simple model and the lepton loop in qed in the contin... | [['we', 'briefly', 'review', 'several', 'activities', 'at', 'mainz', 'related', 'to', 'hadronic', 'lightbylight', 'scattering', 'hlbl', 'using', 'lattice', 'qcd', 'first', 'we', 'present', 'a', 'positionspace', 'approach', 'to', 'the', 'hlbl', 'contribution', 'in', 'the', 'muon', 'g2', 'where', 'we', 'focus', 'on', 'ex... | [-0.0717641690004341, 0.2285737056216156, -0.0832552021127884, 0.09787376747915039, -0.0723465973407858, -0.04779573822118066, 0.0875923366855002, 0.3567216576180524, -0.17461314511105971, -0.18320246107220925, -0.04095010495899866, -0.34372086108972627, -0.05348029543680173, 0.14008811002562718, 0.09715585725325919, 0... |
1,801.04239 | Commutative modified Rota-Baxter algebras, shuffle products and Hopf
algebras | In this paper, we begin a systematic study of modified Rota-Baxter algebras,
as an associative analogue of the modified classical Yang-Baxter equation. We
construct free commutative modified Rota-Baxter algebras by a variation of the
shuffle product and describe the structure both recursively and explicitly. We
then ... | math.RA math.AC | in this paper we begin a systematic study of modified rotabaxter algebras as an associative analogue of the modified classical yangbaxter equation we construct free commutative modified rotabaxter algebras by a variation of the shuffle product and describe the structure both recursively and explicitly we then provide t... | [['in', 'this', 'paper', 'we', 'begin', 'a', 'systematic', 'study', 'of', 'modified', 'rotabaxter', 'algebras', 'as', 'an', 'associative', 'analogue', 'of', 'the', 'modified', 'classical', 'yangbaxter', 'equation', 'we', 'construct', 'free', 'commutative', 'modified', 'rotabaxter', 'algebras', 'by', 'a', 'variation', '... | [-0.13301215475519834, 0.061183458804083844, -0.09920772719907306, 0.11208842891086904, -0.18186712615444497, -0.14661983282194804, -0.05520001547687324, 0.3303051932509673, -0.49732034123044905, -0.18542141917208999, 0.10839058607974547, -0.18704804011731077, -0.23238731390338832, 0.14325168319993606, -0.1471380948452... |
1,801.0424 | Weak mixing below the weak scale in dark-matter direct detection | If dark matter couples predominantly to the axial-vector currents with heavy
quarks, the leading contribution to dark-matter scattering on nuclei is either
due to one-loop weak corrections or due to the heavy-quark axial charges of the
nucleons. We calculate the effects of Higgs and weak gauge-boson exchanges for
dar... | hep-ph | if dark matter couples predominantly to the axialvector currents with heavy quarks the leading contribution to darkmatter scattering on nuclei is either due to oneloop weak corrections or due to the heavyquark axial charges of the nucleons we calculate the effects of higgs and weak gaugeboson exchanges for dark matter ... | [['if', 'dark', 'matter', 'couples', 'predominantly', 'to', 'the', 'axialvector', 'currents', 'with', 'heavy', 'quarks', 'the', 'leading', 'contribution', 'to', 'darkmatter', 'scattering', 'on', 'nuclei', 'is', 'either', 'due', 'to', 'oneloop', 'weak', 'corrections', 'or', 'due', 'to', 'the', 'heavyquark', 'axial', 'ch... | [-0.11817081562286719, 0.28535278366359496, -0.08176844894106305, 0.20809866394982998, -0.0906134832780375, -0.07989119880475364, 0.0174635557639196, 0.31501802186979805, -0.2076023637674489, -0.24922494803620285, -0.03921069833585386, -0.34513997051020173, 0.006680160238364235, 0.06727815420247701, 0.11173970873371514... |
1,801.04241 | Optimal Streaming Codes for Channels with Burst and Arbitrary Erasures | This paper considers transmitting a sequence of messages (a streaming source)
over a packet erasure channel. In each time slot, the source constructs a
packet based on the current and the previous messages and transmits the packet,
which may be erased when the packet travels from the source to the destination.
Every ... | cs.IT math.IT | this paper considers transmitting a sequence of messages a streaming source over a packet erasure channel in each time slot the source constructs a packet based on the current and the previous messages and transmits the packet which may be erased when the packet travels from the source to the destination every source m... | [['this', 'paper', 'considers', 'transmitting', 'a', 'sequence', 'of', 'messages', 'a', 'streaming', 'source', 'over', 'a', 'packet', 'erasure', 'channel', 'in', 'each', 'time', 'slot', 'the', 'source', 'constructs', 'a', 'packet', 'based', 'on', 'the', 'current', 'and', 'the', 'previous', 'messages', 'and', 'transmits... | [-0.2501121835162242, 0.07277237963721608, -0.040545864248027405, 0.015768944563575187, -0.04170263740234077, -0.2678511481478133, 0.14496635302308608, 0.4097291708444104, -0.3558777035185785, -0.21442753839673417, 0.12508034255764813, -0.253830084421806, -0.08882045724824297, 0.15546368254969517, -0.11556129228097922,... |
1,801.04242 | Development of Energy Models for Design Space Exploration of Embedded
Many-Core Systems | This paper introduces a methodology to develop energy models for the design
space exploration of embedded many-core systems. The design process of such
systems can benefit from sophisticated models. Software and hardware can be
specifically optimized based on comprehensive knowledge about application
scenario and har... | cs.DC | this paper introduces a methodology to develop energy models for the design space exploration of embedded manycore systems the design process of such systems can benefit from sophisticated models software and hardware can be specifically optimized based on comprehensive knowledge about application scenario and hardware... | [['this', 'paper', 'introduces', 'a', 'methodology', 'to', 'develop', 'energy', 'models', 'for', 'the', 'design', 'space', 'exploration', 'of', 'embedded', 'manycore', 'systems', 'the', 'design', 'process', 'of', 'such', 'systems', 'can', 'benefit', 'from', 'sophisticated', 'models', 'software', 'and', 'hardware', 'can... | [-0.11148564159362154, -0.014286989120327317, -0.07895040310316041, 0.013520048276752112, -0.05380093027752909, -0.14229198528707704, 0.07205571276664903, 0.3878804798830639, -0.23865489395896228, -0.39459298678081145, 0.11118678691775792, -0.21624790736558763, -0.15835580850623293, 0.24675615720916538, -0.090083831544... |
1,801.04243 | Inexact cuts in Deterministic and Stochastic Dual Dynamic Programming
applied to linear optimization problems | We introduce an extension of Dual Dynamic Programming (DDP) to solve linear
dynamic programming equations. We call this extension IDDP-LP which applies to
situations where some or all primal and dual subproblems to be solved along the
iterations of the method are solved with a bounded error (inexactly). We
provide co... | math.OC | we introduce an extension of dual dynamic programming ddp to solve linear dynamic programming equations we call this extension iddplp which applies to situations where some or all primal and dual subproblems to be solved along the iterations of the method are solved with a bounded error inexactly we provide convergence... | [['we', 'introduce', 'an', 'extension', 'of', 'dual', 'dynamic', 'programming', 'ddp', 'to', 'solve', 'linear', 'dynamic', 'programming', 'equations', 'we', 'call', 'this', 'extension', 'iddplp', 'which', 'applies', 'to', 'situations', 'where', 'some', 'or', 'all', 'primal', 'and', 'dual', 'subproblems', 'to', 'be', 's... | [-0.09305600801203125, -0.009260149798514432, -0.06991444514050374, 0.10909255970332815, -0.1405869536845774, -0.2012679717068136, 0.0526938701748363, 0.3602555144423916, -0.364269150994145, -0.25638283108024906, 0.1932581779064842, -0.2405898863431266, -0.12484111273578594, 0.2243844894664748, -0.0984265617544063, 0.1... |
1,801.04244 | Porous medium equation with nonlocal pressure | We provide a rather complete description of the results obtained so far on
the nonlinear diffusion equation $u_t=\nabla\cdot (u^{m-1}\nabla
(-\Delta)^{-s}u)$, which describes a flow through a porous medium driven by a
nonlocal pressure. We consider constant parameters $m>1$ and $0<s<1$, we assume
that the solutions a... | math.AP | we provide a rather complete description of the results obtained so far on the nonlinear diffusion equation u_tnablacdot um1nabla deltasu which describes a flow through a porous medium driven by a nonlocal pressure we consider constant parameters m1 and 0s1 we assume that the solutions are nonnegative and the problem i... | [['we', 'provide', 'a', 'rather', 'complete', 'description', 'of', 'the', 'results', 'obtained', 'so', 'far', 'on', 'the', 'nonlinear', 'diffusion', 'equation', 'u_tnablacdot', 'um1nabla', 'deltasu', 'which', 'describes', 'a', 'flow', 'through', 'a', 'porous', 'medium', 'driven', 'by', 'a', 'nonlocal', 'pressure', 'we'... | [-0.13942640862922678, 0.08757598254292666, -0.04214684143117084, 0.03797141066123102, -0.058404478588485506, -0.117116550994651, 0.008472346887411969, 0.31076794575799155, -0.2462087995750276, -0.26228327875503815, 0.15745978960389825, -0.3105308066986434, -0.16841024700300516, 0.1711363990304505, -0.02360854114967960... |
1,801.04245 | Experimental Determination of Power Losses and Heat Generation in Solar
Cells for Photovoltaic-Thermal Applications | Solar cell thermal recovery is recently attracting more and more attention in
the research community as a viable solution to increase photovoltaic
efficiency. However the convenience of the implementation of such strategy is
bound to the precise evaluation of the recoverable thermal power, and to a
proper definition ... | physics.app-ph | solar cell thermal recovery is recently attracting more and more attention in the research community as a viable solution to increase photovoltaic efficiency however the convenience of the implementation of such strategy is bound to the precise evaluation of the recoverable thermal power and to a proper definition of t... | [['solar', 'cell', 'thermal', 'recovery', 'is', 'recently', 'attracting', 'more', 'and', 'more', 'attention', 'in', 'the', 'research', 'community', 'as', 'a', 'viable', 'solution', 'to', 'increase', 'photovoltaic', 'efficiency', 'however', 'the', 'convenience', 'of', 'the', 'implementation', 'of', 'such', 'strategy', '... | [-0.10632355490831064, 0.12216310938937572, -0.02122538598956472, 0.017490296822689787, -0.04946740699629665, -0.08968651189385908, 0.07452077331894238, 0.3898789784359058, -0.2675059628746038, -0.3228315157932839, 0.0751098866406243, -0.2586711858501609, -0.15229541296992666, 0.25367164044855506, -0.10904279539464602,... |
1,801.04246 | Characterization of sub-monolayer coatings as novel calibration samples
for X-ray spectroscopy | With the advent of both modern X-ray fluorescence (XRF) methods and improved
analytical reliability requirements the demand for suitable reference samples
has increased. Especially in nanotechnology with the very low areal mass
depositions, quantification becomes considerably more difficult. However, the
availability... | physics.app-ph physics.ins-det | with the advent of both modern xray fluorescence xrf methods and improved analytical reliability requirements the demand for suitable reference samples has increased especially in nanotechnology with the very low areal mass depositions quantification becomes considerably more difficult however the availability of suite... | [['with', 'the', 'advent', 'of', 'both', 'modern', 'xray', 'fluorescence', 'xrf', 'methods', 'and', 'improved', 'analytical', 'reliability', 'requirements', 'the', 'demand', 'for', 'suitable', 'reference', 'samples', 'has', 'increased', 'especially', 'in', 'nanotechnology', 'with', 'the', 'very', 'low', 'areal', 'mass'... | [-0.014971906368690913, 0.12567856021363427, -0.03164458832279755, 0.05859906382330149, 0.008266522352603417, -0.15458880301882763, 0.03643456878258832, 0.4393648175749356, -0.19690508531436088, -0.38045780087954234, 0.1315222972364623, -0.3047195016036904, -0.010061925506248834, 0.27470570085718043, -0.045983740733443... |
1,801.04247 | Pseudogap in electron-doped cuprates: Strong correlation leading to band
splitting | The pseudogap phenomena have been a long-standing mystery of the cuprate
high-temperature superconductors. The pseudogap in the electron-doped cuprates
has been attributed to band folding due to antiferromagnetic (AFM) long-range
order or short-range correlation. We performed an angle-resolved photoemission
spectrosc... | cond-mat.supr-con cond-mat.str-el | the pseudogap phenomena have been a longstanding mystery of the cuprate hightemperature superconductors the pseudogap in the electrondoped cuprates has been attributed to band folding due to antiferromagnetic afm longrange order or shortrange correlation we performed an angleresolved photoemission spectroscopy arpes st... | [['the', 'pseudogap', 'phenomena', 'have', 'been', 'a', 'longstanding', 'mystery', 'of', 'the', 'cuprate', 'hightemperature', 'superconductors', 'the', 'pseudogap', 'in', 'the', 'electrondoped', 'cuprates', 'has', 'been', 'attributed', 'to', 'band', 'folding', 'due', 'to', 'antiferromagnetic', 'afm', 'longrange', 'orde... | [-0.1487194193879876, 0.2123389494691792, -0.0789879998488521, 0.09558038291323817, -0.07200993992190695, -0.16010509115559132, 0.15066894963807004, 0.40520148836640696, -0.23803563744224834, -0.2707302693503373, -0.04677302904610494, -0.4009254805066369, -0.07459764890584418, 0.1480230323645766, 0.06050682150702359, 0... |
1,801.04248 | Spinning pulsating strings in $(AdS_5 \times S^5)_{\varkappa}$ | We study a general class of spinning pulsating strings in $(AdS_5 \times
S^5)_{\varkappa}$ background. For these family of solitons, we examine the
scaling relation between the energy, spin or angular momentum. We verify that
in $\varkappa \rightarrow 0 $ limit these relations reduce to the undeformed
$AdS_5 \times S... | hep-th | we study a general class of spinning pulsating strings in ads_5 times s5_varkappa background for these family of solitons we examine the scaling relation between the energy spin or angular momentum we verify that in varkappa rightarrow 0 limit these relations reduce to the undeformed ads_5 times s5 case we further stud... | [['we', 'study', 'a', 'general', 'class', 'of', 'spinning', 'pulsating', 'strings', 'in', 'ads_5', 'times', 's5_varkappa', 'background', 'for', 'these', 'family', 'of', 'solitons', 'we', 'examine', 'the', 'scaling', 'relation', 'between', 'the', 'energy', 'spin', 'or', 'angular', 'momentum', 'we', 'verify', 'that', 'in... | [-0.1649878485446894, 0.16000155322303486, -0.030400514106364233, 0.12678719137482786, -0.05003390889798634, -0.0943761604323395, 0.013722052528081756, 0.3573747120405498, -0.1827424398476356, -0.23482590075582266, 0.06316732584443678, -0.31496246811002493, -0.0840028312676096, 0.16831150840918876, -0.03713693649287483... |
1,801.04249 | Safe Privatization in Transactional Memory | Transactional memory (TM) facilitates the development of concurrent
applications by letting the programmer designate certain code blocks as atomic.
Programmers using a TM often would like to access the same data both inside and
outside transactions, e.g., to improve performance or to support legacy code.
In this case... | cs.DC | transactional memory tm facilitates the development of concurrent applications by letting the programmer designate certain code blocks as atomic programmers using a tm often would like to access the same data both inside and outside transactions eg to improve performance or to support legacy code in this case programme... | [['transactional', 'memory', 'tm', 'facilitates', 'the', 'development', 'of', 'concurrent', 'applications', 'by', 'letting', 'the', 'programmer', 'designate', 'certain', 'code', 'blocks', 'as', 'atomic', 'programmers', 'using', 'a', 'tm', 'often', 'would', 'like', 'to', 'access', 'the', 'same', 'data', 'both', 'inside'... | [-0.1522875433518744, 0.056546838288717295, -0.07582526255182215, 0.0922644272404482, -0.16427657326306055, -0.19716866049265233, 0.11885271387240962, 0.37227731420766913, -0.29085459169562394, -0.30142122945183253, 0.11186629079747945, -0.22543267501777306, -0.111256241924852, 0.17573242178808995, -0.11653173087538092... |
1,801.0425 | Graph cover-saturation | Graph $G$ is $F$-saturated if $G$ contains no copy of graph $F$ but any edge
added to $G$ produces at least one copy of $F$. One common variant of
saturation is to remove the former restriction: $G$ is $F$-semi-saturated if
any edge added to $G$ produces at least one new copy of $F$. In this paper we
take this idea o... | math.CO | graph g is fsaturated if g contains no copy of graph f but any edge added to g produces at least one copy of f one common variant of saturation is to remove the former restriction g is fsemisaturated if any edge added to g produces at least one new copy of f in this paper we take this idea one step further rather than ... | [['graph', 'g', 'is', 'fsaturated', 'if', 'g', 'contains', 'no', 'copy', 'of', 'graph', 'f', 'but', 'any', 'edge', 'added', 'to', 'g', 'produces', 'at', 'least', 'one', 'copy', 'of', 'f', 'one', 'common', 'variant', 'of', 'saturation', 'is', 'to', 'remove', 'the', 'former', 'restriction', 'g', 'is', 'fsemisaturated', '... | [-0.17847020651058604, 0.14066658698759663, -0.10849934861063958, 0.019087938657030463, -0.12473371783581873, -0.15240702286052207, 0.10184686238411814, 0.3695725336112082, -0.23376532869723937, -0.3265920972079039, 0.06587828832445666, -0.3069906017975882, -0.1202670822191673, 0.13630292809257905, -0.1050111313148712,... |
1,801.04251 | Testing (modified) gravity with 3D and tomographic cosmic shear | Cosmic shear is one of the primary probes to test gravity with current and
future surveys. There are two main techniques to analyse a cosmic shear survey;
a tomographic method, where correlations between the lensing signal in
different redshift bins are used to recover redshift information, and a 3D
approach, where t... | astro-ph.CO | cosmic shear is one of the primary probes to test gravity with current and future surveys there are two main techniques to analyse a cosmic shear survey a tomographic method where correlations between the lensing signal in different redshift bins are used to recover redshift information and a 3d approach where the full... | [['cosmic', 'shear', 'is', 'one', 'of', 'the', 'primary', 'probes', 'to', 'test', 'gravity', 'with', 'current', 'and', 'future', 'surveys', 'there', 'are', 'two', 'main', 'techniques', 'to', 'analyse', 'a', 'cosmic', 'shear', 'survey', 'a', 'tomographic', 'method', 'where', 'correlations', 'between', 'the', 'lensing', ... | [-0.09112082957570632, 0.06518925471474692, -0.08004536749944689, 0.09453856926757363, -0.07706648612069528, -0.09136534925834482, 0.003318863430426991, 0.32945379203215364, -0.23085128036271557, -0.31830639824510576, 0.085404926740815, -0.31083848775480405, -0.08970976738730468, 0.18531031635062523, 0.0081385892711160... |
1,801.04252 | Waveguide quantum electrodynamics in squeezed vacuum | We study the dynamics of a general multi-emitter system coupled to the
squeezed vacuum reservoir and derive a master equation for this system based on
the Weisskopf-Wigner approximation. In this theory, we include the effect of
positions of the squeezing sources which is usually neglected in the previous
studies. We ... | quant-ph | we study the dynamics of a general multiemitter system coupled to the squeezed vacuum reservoir and derive a master equation for this system based on the weisskopfwigner approximation in this theory we include the effect of positions of the squeezing sources which is usually neglected in the previous studies we apply t... | [['we', 'study', 'the', 'dynamics', 'of', 'a', 'general', 'multiemitter', 'system', 'coupled', 'to', 'the', 'squeezed', 'vacuum', 'reservoir', 'and', 'derive', 'a', 'master', 'equation', 'for', 'this', 'system', 'based', 'on', 'the', 'weisskopfwigner', 'approximation', 'in', 'this', 'theory', 'we', 'include', 'the', 'e... | [-0.14603953974641812, 0.19608627525484487, -0.06511406707176998, 0.03145261090603121, 0.01740460149101486, -0.145725945209503, 0.03764527801062414, 0.3819438151905467, -0.2190073414610782, -0.25360676851664865, 0.035009483799373936, -0.2762985561742999, -0.0647150323619461, 0.195949951306899, 0.004153921138376567, 0.0... |
1,801.04253 | Revisiting scalar leptoquark at the LHC | We investigate the Standard Model (SM) extended with a colored charged
scalar, leptoquark, having fractional electromagnetic charge $-1/3$. We mostly
focus on the decays of the leptoquark into second and third generations via
$c\,\mu, t\, \tau$ decay modes. We perform a PYTHIA-based simulation
considering all the dom... | hep-ph | we investigate the standard model sm extended with a colored charged scalar leptoquark having fractional electromagnetic charge 13 we mostly focus on the decays of the leptoquark into second and third generations via cmu t tau decay modes we perform a pythiabased simulation considering all the dominant sm backgrounds a... | [['we', 'investigate', 'the', 'standard', 'model', 'sm', 'extended', 'with', 'a', 'colored', 'charged', 'scalar', 'leptoquark', 'having', 'fractional', 'electromagnetic', 'charge', '13', 'we', 'mostly', 'focus', 'on', 'the', 'decays', 'of', 'the', 'leptoquark', 'into', 'second', 'and', 'third', 'generations', 'via', 'c... | [-0.0646225907463197, 0.24295673098276893, -0.032113588914987355, 0.13439566367100375, -0.05528421036947025, -0.17083305775475524, 0.021985950344755752, 0.3255664636723368, -0.2039181085454081, -0.2994545816156246, 0.03407050570796641, -0.3309649417094667, 0.06483354934778832, 0.14972290838726193, 0.10832867740228881, ... |
1,801.04254 | Optimal data-driven estimation of generalized Markov state models for
non-equilibrium dynamics | There are multiple ways in which a stochastic system can be out of
statistical equilibrium. It might be subject to time-varying forcing; or be in
a transient phase on its way towards equilibrium; it might even be in
equilibrium without us noticing it, due to insufficient observations; and it
even might be a system fa... | math.DS | there are multiple ways in which a stochastic system can be out of statistical equilibrium it might be subject to timevarying forcing or be in a transient phase on its way towards equilibrium it might even be in equilibrium without us noticing it due to insufficient observations and it even might be a system failing to... | [['there', 'are', 'multiple', 'ways', 'in', 'which', 'a', 'stochastic', 'system', 'can', 'be', 'out', 'of', 'statistical', 'equilibrium', 'it', 'might', 'be', 'subject', 'to', 'timevarying', 'forcing', 'or', 'be', 'in', 'a', 'transient', 'phase', 'on', 'its', 'way', 'towards', 'equilibrium', 'it', 'might', 'even', 'be'... | [-0.08916675357613713, 0.09806959828173327, -0.14784575237190703, 0.08958541727422373, -0.0425797501238117, -0.15028163530624242, 0.0715587895323077, 0.3757508408980093, -0.31219353459680965, -0.30024375353663135, 0.15451957684675016, -0.2567212784163438, -0.1693630384709821, 0.17460638845838822, -0.055416219418515066,... |
1,801.04255 | Three-dimensional surface codes: Transversal gates and fault-tolerant
architectures | One of the leading quantum computing architectures is based on the
two-dimensional (2D) surface code. This code has many advantageous properties
such as a high error threshold and a planar layout of physical qubits where
each physical qubit need only interact with its nearest neighbours. However,
the transversal logi... | quant-ph | one of the leading quantum computing architectures is based on the twodimensional 2d surface code this code has many advantageous properties such as a high error threshold and a planar layout of physical qubits where each physical qubit need only interact with its nearest neighbours however the transversal logical gate... | [['one', 'of', 'the', 'leading', 'quantum', 'computing', 'architectures', 'is', 'based', 'on', 'the', 'twodimensional', '2d', 'surface', 'code', 'this', 'code', 'has', 'many', 'advantageous', 'properties', 'such', 'as', 'a', 'high', 'error', 'threshold', 'and', 'a', 'planar', 'layout', 'of', 'physical', 'qubits', 'wher... | [-0.13236783640784797, 0.10004839425196808, -0.04044558352901425, 0.06838732163737629, -0.0058551054000670075, -0.26538067595055786, 0.021570676952683467, 0.42650156384241755, -0.2753596146139178, -0.30011898949557897, 0.09705742550806354, -0.219409216831595, -0.1714419891082654, 0.24451489619839253, -0.091658218674872... |
1,801.04256 | Higgs Inflation at the LC | Most cosmological models of inflation are far away from providing a smoking
gun at low energies. A model of Higgs inflation in the Next-to-Minimal
Supersymmetric Standard Model, however, changes the NMSSM phenomenology
drastically and may be well distinguished from the pure NMSSM or MSSM at a
future Linear Collider. ... | hep-ph | most cosmological models of inflation are far away from providing a smoking gun at low energies a model of higgs inflation in the nexttominimal supersymmetric standard model however changes the nmssm phenomenology drastically and may be well distinguished from the pure nmssm or mssm at a future linear collider we point... | [['most', 'cosmological', 'models', 'of', 'inflation', 'are', 'far', 'away', 'from', 'providing', 'a', 'smoking', 'gun', 'at', 'low', 'energies', 'a', 'model', 'of', 'higgs', 'inflation', 'in', 'the', 'nexttominimal', 'supersymmetric', 'standard', 'model', 'however', 'changes', 'the', 'nmssm', 'phenomenology', 'drastic... | [-0.06485962346886043, 0.22291534507854116, -0.07880105960102361, 0.22856846276992632, -0.09695524177628995, -0.26691164787467797, -0.005377867175726059, 0.2734728827382679, -0.24420375626011073, -0.28851786624341286, 0.06658026841641576, -0.25576524411753554, -0.03472882564708499, 0.14920600357373465, 0.02557617560442... |
1,801.04257 | On projective and affine equivalence of sub-Riemannian metrics | Consider a smooth manifold $M$ equipped with a bracket generating
distribution $D$. Two sub-Riemannian metrics on $(M,D)$ are said to be
projectively (resp. affinely) equivalent if they have the same geodesics up to
reparameterization (resp. up to affine reparameterization). A sub-Riemannian
metric $g$ is called rigi... | math.DG math.OC | consider a smooth manifold m equipped with a bracket generating distribution d two subriemannian metrics on md are said to be projectively resp affinely equivalent if they have the same geodesics up to reparameterization resp up to affine reparameterization a subriemannian metric g is called rigid resp conformally rigi... | [['consider', 'a', 'smooth', 'manifold', 'm', 'equipped', 'with', 'a', 'bracket', 'generating', 'distribution', 'd', 'two', 'subriemannian', 'metrics', 'on', 'md', 'are', 'said', 'to', 'be', 'projectively', 'resp', 'affinely', 'equivalent', 'if', 'they', 'have', 'the', 'same', 'geodesics', 'up', 'to', 'reparameterizati... | [-0.18445066543171343, 0.07481750103236708, -0.07663206417515153, 0.05813401524102156, -0.14349336156683895, -0.20651987026407484, -0.0868082236157571, 0.42797486579173755, -0.3031352857113937, -0.1887079817426848, 0.0736356935793617, -0.2936761117398351, -0.16851932835180078, 0.15042085565633545, -0.16001382144687343,... |
1,801.04258 | Analysis of axisymmetric boundary layers | Axisymmetric boundary layers are studied using integral analysis of the
governing equations for axial flow over a circular cylinder. The analysis
includes the effect of pressure gradient and focuses on the effect of
transverse curvature on boundary layer parameters such as shape factor ($H$)
and skin-friction coeffic... | physics.flu-dyn | axisymmetric boundary layers are studied using integral analysis of the governing equations for axial flow over a circular cylinder the analysis includes the effect of pressure gradient and focuses on the effect of transverse curvature on boundary layer parameters such as shape factor h and skinfriction coefficient c_f... | [['axisymmetric', 'boundary', 'layers', 'are', 'studied', 'using', 'integral', 'analysis', 'of', 'the', 'governing', 'equations', 'for', 'axial', 'flow', 'over', 'a', 'circular', 'cylinder', 'the', 'analysis', 'includes', 'the', 'effect', 'of', 'pressure', 'gradient', 'and', 'focuses', 'on', 'the', 'effect', 'of', 'tra... | [-0.18047568604502587, 0.14142855651110237, -0.059739025677309224, -0.02101466579196637, -0.05921820238265291, -0.08737358969924917, -0.027790290965597902, 0.36211439736231027, -0.29105767473164534, -0.27974271652021865, 0.08986664383484279, -0.2765285347680948, -0.07104131974938886, 0.1785926356399704, -0.016712770952... |
1,801.04259 | The smallest Laplace eigenvalue of homogeneous 3-spheres | We establish an explicit expression for the smallest non-zero eigenvalue of
the Laplace--Beltrami operator on every homogeneous metric on the 3-sphere, or
equivalently, on SU(2) endowed with left-invariant metric. For the subfamily of
3-dimensional Berger spheres, we obtain a full description of their spectra. We
als... | math.DG math.SP | we establish an explicit expression for the smallest nonzero eigenvalue of the laplacebeltrami operator on every homogeneous metric on the 3sphere or equivalently on su2 endowed with leftinvariant metric for the subfamily of 3dimensional berger spheres we obtain a full description of their spectra we also give several ... | [['we', 'establish', 'an', 'explicit', 'expression', 'for', 'the', 'smallest', 'nonzero', 'eigenvalue', 'of', 'the', 'laplacebeltrami', 'operator', 'on', 'every', 'homogeneous', 'metric', 'on', 'the', '3sphere', 'or', 'equivalently', 'on', 'su2', 'endowed', 'with', 'leftinvariant', 'metric', 'for', 'the', 'subfamily', ... | [-0.19376489329699645, 0.06622612702085462, -0.025111038141938692, 0.0785951265014078, -0.14118096286855528, -0.12746763341334266, -0.06550757797873195, 0.3704067864147125, -0.19891666091964855, -0.22475409774137112, 0.11536471939368365, -0.3269285748829134, -0.17130968925159643, 0.21206314631511786, -0.071390047666414... |
1,801.0426 | Conditional Probability Models for Deep Image Compression | Deep Neural Networks trained as image auto-encoders have recently emerged as
a promising direction for advancing the state-of-the-art in image compression.
The key challenge in learning such networks is twofold: To deal with
quantization, and to control the trade-off between reconstruction error
(distortion) and entr... | cs.CV cs.LG | deep neural networks trained as image autoencoders have recently emerged as a promising direction for advancing the stateoftheart in image compression the key challenge in learning such networks is twofold to deal with quantization and to control the tradeoff between reconstruction error distortion and entropy rate of ... | [['deep', 'neural', 'networks', 'trained', 'as', 'image', 'autoencoders', 'have', 'recently', 'emerged', 'as', 'a', 'promising', 'direction', 'for', 'advancing', 'the', 'stateoftheart', 'in', 'image', 'compression', 'the', 'key', 'challenge', 'in', 'learning', 'such', 'networks', 'is', 'twofold', 'to', 'deal', 'with', ... | [-0.0289658353381762, -0.007674411358929126, -0.1055680846738996, 0.07884533705761318, -0.08752473128790206, -0.1550381698730317, 0.035765198544091124, 0.4295031110219883, -0.3409395506549062, -0.31346261366411593, 0.04055949702619039, -0.25718983737187406, -0.22630094234923354, 0.15184556221250783, -0.1453203524716875... |
1,801.04261 | Deep saliency: What is learnt by a deep network about saliency? | Deep convolutional neural networks have achieved impressive performance on a
broad range of problems, beating prior art on established benchmarks, but it
often remains unclear what are the representations learnt by those systems and
how they achieve such performance. This article examines the specific problem
of sali... | cs.CV | deep convolutional neural networks have achieved impressive performance on a broad range of problems beating prior art on established benchmarks but it often remains unclear what are the representations learnt by those systems and how they achieve such performance this article examines the specific problem of saliency ... | [['deep', 'convolutional', 'neural', 'networks', 'have', 'achieved', 'impressive', 'performance', 'on', 'a', 'broad', 'range', 'of', 'problems', 'beating', 'prior', 'art', 'on', 'established', 'benchmarks', 'but', 'it', 'often', 'remains', 'unclear', 'what', 'are', 'the', 'representations', 'learnt', 'by', 'those', 'sy... | [-0.050301416581108545, 0.03730689468017469, -0.04677799126754204, 0.06950816788982289, -0.1009104282866853, -0.15988341195043176, -0.0024834507135286306, 0.4830120808444917, -0.2795154520388072, -0.33577967722861407, 0.05263087051571347, -0.21873020706698298, -0.2772037370596081, 0.19012782589610044, -0.13901477108011... |
1,801.04262 | A note on Herglotz's theorem for time series on function spaces | In this article, we prove Herglotz's theorem for Hilbert-valued time series.
This requires the notion of an operator-valued measure, which we shall make
precise for our setting. Herglotz's theorem for functional time series allows
to generalize existing results that are central to frequency domain analysis on
the fun... | math.ST stat.TH | in this article we prove herglotzs theorem for hilbertvalued time series this requires the notion of an operatorvalued measure which we shall make precise for our setting herglotzs theorem for functional time series allows to generalize existing results that are central to frequency domain analysis on the function spac... | [['in', 'this', 'article', 'we', 'prove', 'herglotzs', 'theorem', 'for', 'hilbertvalued', 'time', 'series', 'this', 'requires', 'the', 'notion', 'of', 'an', 'operatorvalued', 'measure', 'which', 'we', 'shall', 'make', 'precise', 'for', 'our', 'setting', 'herglotzs', 'theorem', 'for', 'functional', 'time', 'series', 'al... | [-0.09604767783254874, 0.048242972036069795, -0.14227134442972172, 0.0762705356531517, -0.079178782607444, -0.06251064365821295, 0.05431638431418535, 0.36205257550187286, -0.2647495019577871, -0.23507201070057565, 0.12507593489946706, -0.216041726588971, -0.13808286127435868, 0.21751220898366855, -0.1097377432724003, 0... |
1,801.04263 | Efficient Probabilistic Model Checking of Smart Building Maintenance
using Fault Maintenance Trees | Cyber-physical systems, like Smart Buildings and power plants, have to meet
high standards, both in terms of reliability and availability. Such metrics are
typically evaluated using Fault trees (FTs) and do not consider maintenance
strategies which can significantly improve lifespan and reliability. Fault
Maintenance... | cs.LO cs.SY | cyberphysical systems like smart buildings and power plants have to meet high standards both in terms of reliability and availability such metrics are typically evaluated using fault trees fts and do not consider maintenance strategies which can significantly improve lifespan and reliability fault maintenance trees fmt... | [['cyberphysical', 'systems', 'like', 'smart', 'buildings', 'and', 'power', 'plants', 'have', 'to', 'meet', 'high', 'standards', 'both', 'in', 'terms', 'of', 'reliability', 'and', 'availability', 'such', 'metrics', 'are', 'typically', 'evaluated', 'using', 'fault', 'trees', 'fts', 'and', 'do', 'not', 'consider', 'maint... | [-0.09370638638860751, 0.02610759965584133, -0.05456750375165973, 0.07262966939857311, -0.05810864802168788, -0.1457411170550534, 0.09108937494661776, 0.3876053813153749, -0.22832746045523375, -0.33076597594087886, 0.15449445951018342, -0.20103332709161192, -0.15120691825993032, 0.2269247469203781, -0.14184450452675773... |
1,801.04264 | Real-world Anomaly Detection in Surveillance Videos | Surveillance videos are able to capture a variety of realistic anomalies. In
this paper, we propose to learn anomalies by exploiting both normal and
anomalous videos. To avoid annotating the anomalous segments or clips in
training videos, which is very time consuming, we propose to learn anomaly
through the deep mult... | cs.CV | surveillance videos are able to capture a variety of realistic anomalies in this paper we propose to learn anomalies by exploiting both normal and anomalous videos to avoid annotating the anomalous segments or clips in training videos which is very time consuming we propose to learn anomaly through the deep multiple in... | [['surveillance', 'videos', 'are', 'able', 'to', 'capture', 'a', 'variety', 'of', 'realistic', 'anomalies', 'in', 'this', 'paper', 'we', 'propose', 'to', 'learn', 'anomalies', 'by', 'exploiting', 'both', 'normal', 'and', 'anomalous', 'videos', 'to', 'avoid', 'annotating', 'the', 'anomalous', 'segments', 'or', 'clips', ... | [-0.08449113753180157, 0.04162121123496305, -0.02991757993952854, 0.08650831778369913, -0.1489476390502036, -0.1712712096153862, 0.03578523772087431, 0.4387618054566836, -0.2353661470046198, -0.3938049280205397, 0.08921810502867662, -0.3256855731836468, -0.19408670761406904, 0.18110781698573933, -0.14394689297812335, 0... |
1,801.04265 | Polar Field Correction for HMI Line-of-Sight Synoptic Data | This document provides some technical notes on the polar field correction
scheme for the HMI synoptic maps and daily updated synchronic frames. It is
intended as a reference for the new data products and for some minor updates on
our previous scheme for MDI (Sun et al. 2011).
| astro-ph.SR | this document provides some technical notes on the polar field correction scheme for the hmi synoptic maps and daily updated synchronic frames it is intended as a reference for the new data products and for some minor updates on our previous scheme for mdi sun et al 2011 | [['this', 'document', 'provides', 'some', 'technical', 'notes', 'on', 'the', 'polar', 'field', 'correction', 'scheme', 'for', 'the', 'hmi', 'synoptic', 'maps', 'and', 'daily', 'updated', 'synchronic', 'frames', 'it', 'is', 'intended', 'as', 'a', 'reference', 'for', 'the', 'new', 'data', 'products', 'and', 'for', 'some'... | [-0.09332742081217778, 0.061901816094177775, -0.05513701853336291, 0.09384384341926004, -0.11078843466627102, -0.07871491204908428, 0.059355823478351034, 0.42502467419641715, -0.202989205912066, -0.3490465774666518, 0.13236451075954392, -0.2510928114255269, -0.13816845185162188, 0.2901200367001972, -0.1812073628922614,... |
1,801.04266 | Understanding the Impact of Pythia Hadronization in Top Quark Mass
Determinations at the LHC | Most of the methods to measure the top quark mass suffer from the jet energy
scaling in achieving better precision. As a way to circumvent this issue, the
study of $B$-hadron observables is motivated. While they do not involve such an
issue, understanding underlying hadronization models is a key to achieve $\sim
0.5\... | hep-ph | most of the methods to measure the top quark mass suffer from the jet energy scaling in achieving better precision as a way to circumvent this issue the study of bhadron observables is motivated while they do not involve such an issue understanding underlying hadronization models is a key to achieve sim 05 precision or... | [['most', 'of', 'the', 'methods', 'to', 'measure', 'the', 'top', 'quark', 'mass', 'suffer', 'from', 'the', 'jet', 'energy', 'scaling', 'in', 'achieving', 'better', 'precision', 'as', 'a', 'way', 'to', 'circumvent', 'this', 'issue', 'the', 'study', 'of', 'bhadron', 'observables', 'is', 'motivated', 'while', 'they', 'do'... | [-0.010056010716402069, 0.17640667419656328, -0.10420539989216446, 0.13752611279327037, -0.06717956511721272, -0.09395436148143149, 0.0587600062135607, 0.3531118257549302, -0.21248417509547113, -0.345960195995225, 0.047249901735681464, -0.27721503955424476, 0.03872035601746355, 0.18437851585823128, -0.01564445713904268... |
1,801.04267 | Management's Perspective on Critical Success Factors Affecting Mobile
Learning in Higher Education Institutions - An Empirical Study | Mobile learning (m-Learning) is considered to be one of the fastest growing
learning platforms. The immense interest in m-Learning is attributed to the
incredible rate of growth of mobile technology and its proliferation into every
aspect of modern life. Despite this, m-Learning has not experienced a similar
adoption... | cs.CY | mobile learning mlearning is considered to be one of the fastest growing learning platforms the immense interest in mlearning is attributed to the incredible rate of growth of mobile technology and its proliferation into every aspect of modern life despite this mlearning has not experienced a similar adoption rate in t... | [['mobile', 'learning', 'mlearning', 'is', 'considered', 'to', 'be', 'one', 'of', 'the', 'fastest', 'growing', 'learning', 'platforms', 'the', 'immense', 'interest', 'in', 'mlearning', 'is', 'attributed', 'to', 'the', 'incredible', 'rate', 'of', 'growth', 'of', 'mobile', 'technology', 'and', 'its', 'proliferation', 'in... | [-0.08733414991265051, 0.0872572443282501, -0.06125445034549886, 0.04627293155806319, -0.12647919659502804, -0.15420547780350793, 0.077118748923096, 0.3611665270422762, -0.21256372881267804, -0.34162364859717437, 0.13811643679306496, -0.2813181150704622, -0.16579696066405467, 0.201941546911082, -0.15754815152038382, 0.... |
1,801.04268 | Cosmological Backgrounds of Gravitational Waves | Gravitational waves (GWs) have a great potential to probe cosmology. We
review early universe sources that can lead to cosmological backgrounds of GWs.
We begin by presenting definitions of GWs in flat space-time and in a
cosmological setting, and discussing the reasons why GW backgrounds from the
early universe are ... | astro-ph.CO gr-qc hep-ph | gravitational waves gws have a great potential to probe cosmology we review early universe sources that can lead to cosmological backgrounds of gws we begin by presenting definitions of gws in flat spacetime and in a cosmological setting and discussing the reasons why gw backgrounds from the early universe are of a sto... | [['gravitational', 'waves', 'gws', 'have', 'a', 'great', 'potential', 'to', 'probe', 'cosmology', 'we', 'review', 'early', 'universe', 'sources', 'that', 'can', 'lead', 'to', 'cosmological', 'backgrounds', 'of', 'gws', 'we', 'begin', 'by', 'presenting', 'definitions', 'of', 'gws', 'in', 'flat', 'spacetime', 'and', 'in'... | [-0.12477074029907842, 0.17641080758691607, -0.0865552762958717, 0.18537730023968416, -0.12138205998903745, -0.06515649418003637, -0.030515125955180848, 0.31085734835370277, -0.19330233074845626, -0.2890578093288418, 0.1198076305883731, -0.2924583689105552, -0.13887701888197784, 0.21565335839296373, 0.01156888482285849... |
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