id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,712.09801 | Topological magnon bands in the zigzag and stripy phases of
antiferromagnetic honeycomb lattice | We investigated the topological property of magnon bands in the collinear
magnetic orders of zigzag and stripy phases for the antiferromagnetic honeycomb
lattice and identified Berry curvature and symmetry constraints on the magnon
band structure. Different symmetries of both zigzag and stripy phases lead to
differen... | cond-mat.mes-hall | we investigated the topological property of magnon bands in the collinear magnetic orders of zigzag and stripy phases for the antiferromagnetic honeycomb lattice and identified berry curvature and symmetry constraints on the magnon band structure different symmetries of both zigzag and stripy phases lead to different t... | [['we', 'investigated', 'the', 'topological', 'property', 'of', 'magnon', 'bands', 'in', 'the', 'collinear', 'magnetic', 'orders', 'of', 'zigzag', 'and', 'stripy', 'phases', 'for', 'the', 'antiferromagnetic', 'honeycomb', 'lattice', 'and', 'identified', 'berry', 'curvature', 'and', 'symmetry', 'constraints', 'on', 'the... | [-0.2993761468051861, 0.2510070232293891, -0.021068195212417498, 0.04347742697707592, -0.09951482126108693, -0.10347451267387861, 0.045540564601721525, 0.38844521273858845, -0.2841057101300416, -0.22972492415171403, 0.0028579541932021338, -0.32362588013235766, -0.1213057993266445, 0.09027934481855482, 0.125419128247393... |
1,712.09802 | Search for $tZ$ Flavour Changing Neutral Currents in top-quark decays
with the ATLAS detector | A search for flavour-changing neutral current (FCNC) processes in top-quark
decays is presented. Data collected from proton-proton collisions at the LHC at
a centre-of-mass energy of $\sqrt{s}=13$ TeV corresponding to an integrated
luminosity of 36 fb$^{-1}$, are analysed. A search is performed for top-quark
pair-pro... | hep-ex | a search for flavourchanging neutral current fcnc processes in topquark decays is presented data collected from protonproton collisions at the lhc at a centreofmass energy of sqrts13 tev corresponding to an integrated luminosity of 36 fb1 are analysed a search is performed for topquark pairproduction events with one to... | [['a', 'search', 'for', 'flavourchanging', 'neutral', 'current', 'fcnc', 'processes', 'in', 'topquark', 'decays', 'is', 'presented', 'data', 'collected', 'from', 'protonproton', 'collisions', 'at', 'the', 'lhc', 'at', 'a', 'centreofmass', 'energy', 'of', 'sqrts13', 'tev', 'corresponding', 'to', 'an', 'integrated', 'lum... | [-0.06653251337710946, 0.20727570794588246, -0.00911612662842826, 0.17750358919746598, -0.05147880200050114, -0.19694400465745918, 0.07902340407342896, 0.31978337221559794, -0.19196020683739334, -0.2765243087128243, 0.040710927828673873, -0.397955264971482, 0.13578429166569977, 0.1742388212313766, 0.1561321681296891, 0... |
1,712.09803 | An Innovative Approach to Achieve Compositionality Efficiently using
Multi-Version Object Based Transactional Systems | In the modern era of multicore processors, utilizing cores is a tedious job.
Synchronization and communication among processors involve high cost. Software
transaction memory systems (STMs) addresses this issues and provide better
concurrency in which programmer need not have to worry about consistency
issues. Anothe... | cs.DC | in the modern era of multicore processors utilizing cores is a tedious job synchronization and communication among processors involve high cost software transaction memory systems stms addresses this issues and provide better concurrency in which programmer need not have to worry about consistency issues another advant... | [['in', 'the', 'modern', 'era', 'of', 'multicore', 'processors', 'utilizing', 'cores', 'is', 'a', 'tedious', 'job', 'synchronization', 'and', 'communication', 'among', 'processors', 'involve', 'high', 'cost', 'software', 'transaction', 'memory', 'systems', 'stms', 'addresses', 'this', 'issues', 'and', 'provide', 'bette... | [-0.14469636874295808, 0.01930867275894763, -0.05606198048917577, 0.028332006282513388, -0.10815318059892609, -0.20435883433271487, 0.10756915494342907, 0.38793883429249176, -0.25477281022243775, -0.3899544794542285, 0.09959067729203246, -0.27000857427393876, -0.09559615469322755, 0.21760665953624994, -0.12736240826690... |
1,712.09804 | A Global ILC Approach in Pixel Space over Large Angular Scales of the
Sky using CMB Covariance Matrix | We propose a new internal linear combination (ILC) method in the pixel space,
applicable on large angular scales of the sky, to estimate a foreground
minimized Cosmic Microwave Background (CMB) temperature anisotropy map by
incorporating prior knowledge about the theoretical CMB covariance matrix.
Usual ILC method in... | astro-ph.CO | we propose a new internal linear combination ilc method in the pixel space applicable on large angular scales of the sky to estimate a foreground minimized cosmic microwave background cmb temperature anisotropy map by incorporating prior knowledge about the theoretical cmb covariance matrix usual ilc method in pixel sp... | [['we', 'propose', 'a', 'new', 'internal', 'linear', 'combination', 'ilc', 'method', 'in', 'the', 'pixel', 'space', 'applicable', 'on', 'large', 'angular', 'scales', 'of', 'the', 'sky', 'to', 'estimate', 'a', 'foreground', 'minimized', 'cosmic', 'microwave', 'background', 'cmb', 'temperature', 'anisotropy', 'map', 'by'... | [-0.012921728066447272, 0.044210932715094256, -0.07254940445522128, 0.10143792921449717, -0.12748623204090076, -0.09051136453168203, -0.0020482530222023457, 0.39280147446940344, -0.2621190103970162, -0.3184179158660171, 0.0933826760480342, -0.3304135049544445, -0.06995470743104348, 0.21978112740960976, -0.0155740009598... |
1,712.09805 | Reggeon cuts in QCD amplitudes with negative signature | Reggeon cuts in QCD amplitudes with negative signature are discussed. These
cuts appear in the next-to-next-to-leading logarithmic approximation (NNLLA)
and greatly complicate the derivation of the BFKL equation. Feynman diagrams
responsible for appearance of these cuts are indicated and the cut
contributions are cal... | hep-ph | reggeon cuts in qcd amplitudes with negative signature are discussed these cuts appear in the nexttonexttoleading logarithmic approximation nnlla and greatly complicate the derivation of the bfkl equation feynman diagrams responsible for appearance of these cuts are indicated and the cut contributions are calculated in... | [['reggeon', 'cuts', 'in', 'qcd', 'amplitudes', 'with', 'negative', 'signature', 'are', 'discussed', 'these', 'cuts', 'appear', 'in', 'the', 'nexttonexttoleading', 'logarithmic', 'approximation', 'nnlla', 'and', 'greatly', 'complicate', 'the', 'derivation', 'of', 'the', 'bfkl', 'equation', 'feynman', 'diagrams', 'respo... | [-0.13100069069303572, 0.1494722974859178, -0.14079068549625845, 0.2019194570183754, -0.07651427734643221, -0.046533267046324905, 0.03835857556259725, 0.3595901005808264, -0.17182060122489928, -0.2928145915269852, 0.0012558789947070181, -0.33383345684036614, -0.12325202845036984, 0.12262611968792043, 0.0681902374327182... |
1,712.09806 | VO$_2$ as a natural optical metamaterial | VO$_2$ is a unique phase change material with strongly anisotropic electronic
properties. Recently, samples have been prepared that present a co-existence of
phases and thus form metal-insulator junctions of the same chemical compound.
Using first principles calculations, the optical properties of metallic and
semico... | cond-mat.mtrl-sci | vo_2 is a unique phase change material with strongly anisotropic electronic properties recently samples have been prepared that present a coexistence of phases and thus form metalinsulator junctions of the same chemical compound using first principles calculations the optical properties of metallic and semiconducting v... | [['vo_2', 'is', 'a', 'unique', 'phase', 'change', 'material', 'with', 'strongly', 'anisotropic', 'electronic', 'properties', 'recently', 'samples', 'have', 'been', 'prepared', 'that', 'present', 'a', 'coexistence', 'of', 'phases', 'and', 'thus', 'form', 'metalinsulator', 'junctions', 'of', 'the', 'same', 'chemical', 'c... | [-0.1464416194380126, 0.20641628461214537, -0.03665684633497291, -0.05034846477103882, -0.07871822225470237, -0.13331345600993125, 0.09148061344798171, 0.4765468634743215, -0.24205928473939536, -0.28265853862470114, 0.02851306859320314, -0.31484737728530443, -0.18442213237072333, 0.18232901620266262, 0.0349848058007174... |
1,712.09807 | Control theory for the Burgers equation: Agrachev-Sarychev approach | This paper is devoted to a description of a general approach introduced by
Agrachev and Sarychev in 2005 for studying some control problems for
Navier-Stokes equations. The example of a 1D Burgers equation is used to
illustrate the main ideas. We begin with a short discussion of the Cauchy
problem and establish a con... | math.AP math.OC | this paper is devoted to a description of a general approach introduced by agrachev and sarychev in 2005 for studying some control problems for navierstokes equations the example of a 1d burgers equation is used to illustrate the main ideas we begin with a short discussion of the cauchy problem and establish a continui... | [['this', 'paper', 'is', 'devoted', 'to', 'a', 'description', 'of', 'a', 'general', 'approach', 'introduced', 'by', 'agrachev', 'and', 'sarychev', 'in', '2005', 'for', 'studying', 'some', 'control', 'problems', 'for', 'navierstokes', 'equations', 'the', 'example', 'of', 'a', '1d', 'burgers', 'equation', 'is', 'used', '... | [-0.13858948962762951, 0.03671892370097339, -0.08787577349692582, 0.0943964866094757, -0.0741790210083127, -0.13878616314847023, 0.0017619247559923679, 0.3153208699449897, -0.31797706461045894, -0.24198850182816387, 0.13392245328403077, -0.2320411538821645, -0.1726340668834746, 0.19153485415503382, -0.0664441453688778,... |
1,712.09808 | Kato square root problem with unbounded leading coefficients | We prove the Kato conjecture for elliptic operators,
$L=-\nabla\cdot\left((\mathbf A+\mathbf D)\nabla\ \right)$, with $\mathbf A$ a
complex measurable bounded coercive matrix and $\mathbf D$ a measurable
real-valued skew-symmetric matrix in $\mathbb{R}^n$ with entries in
$BMO(\mathbb{R}^n)$;\, i.e., the domain of $\s... | math.AP | we prove the kato conjecture for elliptic operators lnablacdotleftmathbf amathbf dnabla right with mathbf a a complex measurable bounded coercive matrix and mathbf d a measurable realvalued skewsymmetric matrix in mathbbrn with entries in bmomathbbrn ie the domain of sqrtl is the sobolev space dot h1mathbbrn in any dim... | [['we', 'prove', 'the', 'kato', 'conjecture', 'for', 'elliptic', 'operators', 'lnablacdotleftmathbf', 'amathbf', 'dnabla', 'right', 'with', 'mathbf', 'a', 'a', 'complex', 'measurable', 'bounded', 'coercive', 'matrix', 'and', 'mathbf', 'd', 'a', 'measurable', 'realvalued', 'skewsymmetric', 'matrix', 'in', 'mathbbrn', 'w... | [-0.19894407010050835, 0.11075507661465693, 0.061294298679395405, -0.01460345398798516, -0.10259617285164832, -0.18240236719483854, -0.08990242385684892, 0.34357337053451276, -0.35547604429087154, -0.05759128069298135, 0.11875888252742933, -0.3278439313095684, -0.09927597463710872, 0.13640323811624613, -0.1132120875171... |
1,712.09809 | A Multi-Scale and Multi-Depth Convolutional Neural Network for Remote
Sensing Imagery Pan-Sharpening | Pan-sharpening is a fundamental and significant task in the field of remote
sensing imagery processing, in which high-resolution spatial details from
panchromatic images are employed to enhance the spatial resolution of
multi-spectral (MS) images. As the transformation from low spatial resolution
MS image to high-res... | cs.CV | pansharpening is a fundamental and significant task in the field of remote sensing imagery processing in which highresolution spatial details from panchromatic images are employed to enhance the spatial resolution of multispectral ms images as the transformation from low spatial resolution ms image to highresolution ms... | [['pansharpening', 'is', 'a', 'fundamental', 'and', 'significant', 'task', 'in', 'the', 'field', 'of', 'remote', 'sensing', 'imagery', 'processing', 'in', 'which', 'highresolution', 'spatial', 'details', 'from', 'panchromatic', 'images', 'are', 'employed', 'to', 'enhance', 'the', 'spatial', 'resolution', 'of', 'multisp... | [-0.0040678891264611765, -0.039605807058424466, -0.07755067996451602, 0.04354819523665818, -0.07396630140849286, -0.1592750491381305, -0.058336267410407934, 0.4869004413189869, -0.2885874895127638, -0.3369724326235767, 0.09309410412670187, -0.23793316533463815, -0.22274501575157046, 0.17029425370994777, -0.156765240739... |
1,712.0981 | Observational Properties of SNe Ia Progenitors Close to the Explosion | We determine the expected signal in various observational bands of Supernovae
Ia progenitors just before the explosion by assuming the rotating Double
Degenerate scenario. Our results are valid also for all the evolutionary
scenarios invoking rotation as the driving mechanism of the accretion process
as well as the e... | astro-ph.SR astro-ph.HE | we determine the expected signal in various observational bands of supernovae ia progenitors just before the explosion by assuming the rotating double degenerate scenario our results are valid also for all the evolutionary scenarios invoking rotation as the driving mechanism of the accretion process as well as the evol... | [['we', 'determine', 'the', 'expected', 'signal', 'in', 'various', 'observational', 'bands', 'of', 'supernovae', 'ia', 'progenitors', 'just', 'before', 'the', 'explosion', 'by', 'assuming', 'the', 'rotating', 'double', 'degenerate', 'scenario', 'our', 'results', 'are', 'valid', 'also', 'for', 'all', 'the', 'evolutionar... | [-0.0743670757577495, 0.1623823381278122, -0.03266462051790574, 0.10820314094173197, -0.07606886837585661, -0.07332431518884956, 0.08083129685265242, 0.3788109311345415, -0.2472611279837543, -0.3673627012577213, 0.12536587058108484, -0.26851344151330775, -0.021155116699834463, 0.1982491095178211, -0.02603191355356997, ... |
1,712.09811 | Lie point symmetries and ODEs passing the Painlev\'e test | The Lie point symmetries of ordinary differential equations (ODEs) that are
candidates for having the Painlev\'e property are explored for ODEs of order $n
=2, \dots ,5$. Among the 6 ODEs identifying the Painlev\'e transcendents only
$P_{III}$, $P_V$ and $P_{VI}$ have nontrivial symmetry algebras and that only
for ve... | nlin.SI | the lie point symmetries of ordinary differential equations odes that are candidates for having the painleve property are explored for odes of order n 2 dots 5 among the 6 odes identifying the painleve transcendents only p_iii p_v and p_vi have nontrivial symmetry algebras and that only for very special values of the p... | [['the', 'lie', 'point', 'symmetries', 'of', 'ordinary', 'differential', 'equations', 'odes', 'that', 'are', 'candidates', 'for', 'having', 'the', 'painleve', 'property', 'are', 'explored', 'for', 'odes', 'of', 'order', 'n', '2', 'dots', '5', 'among', 'the', '6', 'odes', 'identifying', 'the', 'painleve', 'transcendents... | [-0.15993814020028968, 0.040916041757977445, -0.035534808848522545, 0.10304073522996715, -0.12008043826653028, -0.21209171516307462, -0.04961605092847911, 0.29925548239779753, -0.25330636637490683, -0.2998585561070386, 0.12666094214673793, -0.3415830588265227, -0.14917871282907114, 0.17716464620655564, -0.0324644694447... |
1,712.09812 | Kappa-deformed Dirac oscillator in an external magnetic field | We study the solutions of the (2+1)-dimensional kappa-deformed Dirac
oscillator in the presence of a constant transverse magnetic field. We
demonstrate how the deformation parameter affects the energy eigenvalues of the
system and the corresponding eigenfunctions. Our findings suggest that this
system could be used t... | hep-th | we study the solutions of the 21dimensional kappadeformed dirac oscillator in the presence of a constant transverse magnetic field we demonstrate how the deformation parameter affects the energy eigenvalues of the system and the corresponding eigenfunctions our findings suggest that this system could be used to detect ... | [['we', 'study', 'the', 'solutions', 'of', 'the', '21dimensional', 'kappadeformed', 'dirac', 'oscillator', 'in', 'the', 'presence', 'of', 'a', 'constant', 'transverse', 'magnetic', 'field', 'we', 'demonstrate', 'how', 'the', 'deformation', 'parameter', 'affects', 'the', 'energy', 'eigenvalues', 'of', 'the', 'system', '... | [-0.16883064366156758, 0.1320140426090802, -0.0942749377747532, 0.06134181312954752, -0.06728018279536627, -0.07121842663618735, 0.011036231578327716, 0.31076195132918655, -0.2770720065105706, -0.28644239432178437, 0.06836358230648329, -0.24683089330792427, -0.20234284124162513, 0.14573376801563426, -0.0233185136923566... |
1,712.09813 | Accurate Bayesian Data Classification without Hyperparameter
Cross-validation | We extend the standard Bayesian multivariate Gaussian generative data
classifier by considering a generalization of the conjugate, normal-Wishart
prior distribution and by deriving the hyperparameters analytically via
evidence maximization. The behaviour of the optimal hyperparameters is explored
in the high-dimensio... | stat.ME cs.LG math.ST stat.TH | we extend the standard bayesian multivariate gaussian generative data classifier by considering a generalization of the conjugate normalwishart prior distribution and by deriving the hyperparameters analytically via evidence maximization the behaviour of the optimal hyperparameters is explored in the highdimensional da... | [['we', 'extend', 'the', 'standard', 'bayesian', 'multivariate', 'gaussian', 'generative', 'data', 'classifier', 'by', 'considering', 'a', 'generalization', 'of', 'the', 'conjugate', 'normalwishart', 'prior', 'distribution', 'and', 'by', 'deriving', 'the', 'hyperparameters', 'analytically', 'via', 'evidence', 'maximiza... | [-0.009030643485681111, -0.053606036021860676, -0.09345697922937905, 0.12330241158340516, -0.12915551202343917, -0.17412190316522966, 0.11649778304593776, 0.36233188323120574, -0.27553817265277813, -0.31991214774298804, 0.09454650107819809, -0.2302207025723643, -0.14419567818517115, 0.15880576910954072, -0.097396847993... |
1,712.09814 | Electroweak production of two jets in association with a Z boson in
proton-proton collisions at $\sqrt{s}= $ 13 TeV | A measurement of the electroweak (EW) production of two jets in association
with a Z boson in proton-proton collisions at $\sqrt{s} = $ 13 TeV is
presented, based on data recorded in 2016 by the CMS experiment at the LHC
corresponding to an integrated luminosity of 35.9 fb$^{-1}$. The measurement is
performed in the ... | hep-ex | a measurement of the electroweak ew production of two jets in association with a z boson in protonproton collisions at sqrts 13 tev is presented based on data recorded in 2016 by the cms experiment at the lhc corresponding to an integrated luminosity of 359 fb1 the measurement is performed in the ellellmathrmjj final s... | [['a', 'measurement', 'of', 'the', 'electroweak', 'ew', 'production', 'of', 'two', 'jets', 'in', 'association', 'with', 'a', 'z', 'boson', 'in', 'protonproton', 'collisions', 'at', 'sqrts', '13', 'tev', 'is', 'presented', 'based', 'on', 'data', 'recorded', 'in', '2016', 'by', 'the', 'cms', 'experiment', 'at', 'the', 'l... | [-0.08661831117777981, 0.22527439132495286, -0.03183256558834869, 0.144959012443638, 0.0036361087972726575, -0.1088649612866382, 0.02027406988672932, 0.3622330794021248, -0.1293369135545457, -0.3993758736526902, 0.005781823795358526, -0.3784051079024127, 0.1084590278974271, 0.15593373052586607, 0.06646779544849477, 0.0... |
1,712.09815 | On log motives | We define the categories of log motives and log mixed motives. The latter
gives a new formulation for the category of mixed motives. We prove that the
former is a semisimple abelian category if and only if the numerical
equivalence and homological equivalence coincide, and that it is also
equivalent to that the latte... | math.AG | we define the categories of log motives and log mixed motives the latter gives a new formulation for the category of mixed motives we prove that the former is a semisimple abelian category if and only if the numerical equivalence and homological equivalence coincide and that it is also equivalent to that the latter is ... | [['we', 'define', 'the', 'categories', 'of', 'log', 'motives', 'and', 'log', 'mixed', 'motives', 'the', 'latter', 'gives', 'a', 'new', 'formulation', 'for', 'the', 'category', 'of', 'mixed', 'motives', 'we', 'prove', 'that', 'the', 'former', 'is', 'a', 'semisimple', 'abelian', 'category', 'if', 'and', 'only', 'if', 'th... | [-0.1527187907685564, 0.024073035162809776, -0.16350709851065728, 0.1592331604939592, -0.11310814703776412, -0.20386264323295183, -0.011251412510667762, 0.3530446699986311, -0.37707223975393056, -0.2119656659547903, 0.1119592283032707, -0.17309430255618405, -0.1570597218017872, 0.16478855040383666, -0.24811090240637734... |
1,712.09816 | Extremal Behavior of Aggregated Data with an Application to Downscaling | The distribution of spatially aggregated data from a stochastic process $X$
may exhibit a different tail behavior than its marginal distributions. For a
large class of aggregating functionals $\ell$ we introduce the $\ell$-extremal
coefficient that quantifies this difference as a function of the extremal
spatial depe... | stat.ME stat.AP | the distribution of spatially aggregated data from a stochastic process x may exhibit a different tail behavior than its marginal distributions for a large class of aggregating functionals ell we introduce the ellextremal coefficient that quantifies this difference as a function of the extremal spatial dependence in x ... | [['the', 'distribution', 'of', 'spatially', 'aggregated', 'data', 'from', 'a', 'stochastic', 'process', 'x', 'may', 'exhibit', 'a', 'different', 'tail', 'behavior', 'than', 'its', 'marginal', 'distributions', 'for', 'a', 'large', 'class', 'of', 'aggregating', 'functionals', 'ell', 'we', 'introduce', 'the', 'ellextremal... | [-0.05689185397892163, 0.05301820691915807, -0.1406990632406789, 0.12223612089571895, -0.04953831828777389, -0.08347853773819475, 0.06553245730344848, 0.36866255382011676, -0.288127825219698, -0.2902444396649712, 0.09370505334568563, -0.295470537834576, -0.12520663926120976, 0.17751065295045104, -0.04351637223685273, 0... |
1,712.09817 | Quantum-to-Quantum Bernoulli Factory | Given a coin with unknown bias $p\in [0,1]$, can we exactly simulate another
coin with bias $f(p)$? The exact set of simulable functions has been well
characterized 20 years ago. In this paper, we ask the quantum counterpart of
this question: Given the quantum coin
$|p\rangle=\sqrt{p}|0\rangle+\sqrt{1-p}|1\rangle$, c... | quant-ph | given a coin with unknown bias pin 01 can we exactly simulate another coin with bias fp the exact set of simulable functions has been well characterized 20 years ago in this paper we ask the quantum counterpart of this question given the quantum coin pranglesqrtp0ranglesqrt1p1rangle can we exactly simulate another quan... | [['given', 'a', 'coin', 'with', 'unknown', 'bias', 'pin', '01', 'can', 'we', 'exactly', 'simulate', 'another', 'coin', 'with', 'bias', 'fp', 'the', 'exact', 'set', 'of', 'simulable', 'functions', 'has', 'been', 'well', 'characterized', '20', 'years', 'ago', 'in', 'this', 'paper', 'we', 'ask', 'the', 'quantum', 'counter... | [-0.09433943454929616, 0.14181848392927146, -0.08462232688253515, 0.07152906969304751, -0.045894062293044637, -0.22977040581970234, 0.06384993512366553, 0.4116895929648635, -0.2965547785455926, -0.2912174592558504, 0.08028203047147502, -0.27413447942124325, -0.16789145137214762, 0.2010972092576911, -0.10850411076935824... |
1,712.09818 | Automated Formal Equivalence Verification of Pipelined Nested Loops in
Datapath Designs | In this paper, we present an efficient formal approach to check the
equivalence of synthesized RTL against the high-level specification in the
presence of pipelining transformations. To increase the scalability of our
proposed method, we dynamically divide the designs into several smaller parts
called segments by int... | cs.AR | in this paper we present an efficient formal approach to check the equivalence of synthesized rtl against the highlevel specification in the presence of pipelining transformations to increase the scalability of our proposed method we dynamically divide the designs into several smaller parts called segments by introduci... | [['in', 'this', 'paper', 'we', 'present', 'an', 'efficient', 'formal', 'approach', 'to', 'check', 'the', 'equivalence', 'of', 'synthesized', 'rtl', 'against', 'the', 'highlevel', 'specification', 'in', 'the', 'presence', 'of', 'pipelining', 'transformations', 'to', 'increase', 'the', 'scalability', 'of', 'our', 'propos... | [-0.09918020749531668, 0.009000477194900524, -0.04771308923856973, 0.03363355112084177, -0.07272962886013426, -0.14481785913060807, 0.07339043439080771, 0.4204370735443375, -0.2576293262046124, -0.3495499552070592, 0.12176611153683572, -0.22993597643334795, -0.10211289661748105, 0.19635208874412424, -0.0775140708134499... |
1,712.09819 | Geometrical Proof of Generalized Mirror Transformation of Projective
Hypersurfaces | In this paper, we propose a geometrical proof of the generalized mirror
transformation of genus 0 Gromov-Witten invariants of degree k hypersurface in
CP^{N-1}.
| math.AG hep-th | in this paper we propose a geometrical proof of the generalized mirror transformation of genus 0 gromovwitten invariants of degree k hypersurface in cpn1 | [['in', 'this', 'paper', 'we', 'propose', 'a', 'geometrical', 'proof', 'of', 'the', 'generalized', 'mirror', 'transformation', 'of', 'genus', '0', 'gromovwitten', 'invariants', 'of', 'degree', 'k', 'hypersurface', 'in', 'cpn1']] | [-0.2657184750617792, 0.06621184723917395, -0.14504112396389246, 0.010217051152721979, -0.06566144394067426, -0.19125096156494692, -0.027656972442249145, 0.24375648136871556, -0.30293029143164557, -0.2538928353848557, -0.024507881520548835, -0.2024301908677444, -0.265793114900589, 0.06065101735293865, -0.21418228303082... |
1,712.0982 | Some new results on functions in $C(X)$ having their support on ideals
of closed sets | For any ideal $\mathcal{P}$ of closed sets in $X$, let $C_\mathcal{P}(X)$ be
the family of those functions in $C(X)$ whose support lie on $\mathcal{P}$.
Further let $C^\mathcal{P}_\infty(X)$ contain precisely those functions $f$ in
$C(X)$ for which for each $\epsilon >0, \{x\in X: \lvert f(x)\rvert\geq
\epsilon\}$ is... | math.GN | for any ideal mathcalp of closed sets in x let c_mathcalpx be the family of those functions in cx whose support lie on mathcalp further let cmathcalp_inftyx contain precisely those functions f in cx for which for each epsilon 0 xin x lvert fxrvertgeq epsilon is a member of mathcalp let upsilon_c_mathcalpx stand for the... | [['for', 'any', 'ideal', 'mathcalp', 'of', 'closed', 'sets', 'in', 'x', 'let', 'c_mathcalpx', 'be', 'the', 'family', 'of', 'those', 'functions', 'in', 'cx', 'whose', 'support', 'lie', 'on', 'mathcalp', 'further', 'let', 'cmathcalp_inftyx', 'contain', 'precisely', 'those', 'functions', 'f', 'in', 'cx', 'for', 'which', '... | [-0.17401624641038085, 0.11699100456906691, -0.05076055200035243, 0.012631449610068414, -0.018498200277405744, -0.16122299856261202, 0.008258435408903383, 0.3801784796542243, -0.3336392543768804, -0.14232502563268337, 0.08424590021604672, -0.2976031684365712, -0.079698225277427, 0.20232498564659374, -0.0427218435356687... |
1,712.09821 | An adaptive $hp$-refinement strategy with computable guaranteed bound on
the error reduction factor | We propose a new practical adaptive refinement strategy for $hp$-finite
element approximations of elliptic problems. Following recent theoretical
developments in polynomial-degree-robust a posteriori error analysis, we solve
two types of discrete local problems on vertex-based patches. The first type
involves the sol... | math.NA | we propose a new practical adaptive refinement strategy for hpfinite element approximations of elliptic problems following recent theoretical developments in polynomialdegreerobust a posteriori error analysis we solve two types of discrete local problems on vertexbased patches the first type involves the solution on ea... | [['we', 'propose', 'a', 'new', 'practical', 'adaptive', 'refinement', 'strategy', 'for', 'hpfinite', 'element', 'approximations', 'of', 'elliptic', 'problems', 'following', 'recent', 'theoretical', 'developments', 'in', 'polynomialdegreerobust', 'a', 'posteriori', 'error', 'analysis', 'we', 'solve', 'two', 'types', 'of... | [-0.11565693869133056, 0.013591675440403152, -0.08399734951057275, 0.04574595241066278, -0.049620365820160495, -0.1451389677276039, 0.09662290199543896, 0.3355036805079979, -0.28301902809683144, -0.28553904441705613, 0.12090994387935025, -0.2305243890896492, -0.11536780700520416, 0.18265819719346554, -0.100771041190609... |
1,712.09822 | On intrinsic quadrics | An intrinsic quadric is a normal projective variety with a Cox ring defined by a single quadratic relation. We provide explicit descriptions of these varieties in the smooth case for small Picard numbers. As applications, we figure out in this setting the Fano examples and (affirmatively) test Fujita's base point free ... | math.AG | an intrinsic quadric is a normal projective variety with a cox ring defined by a single quadratic relation we provide explicit descriptions of these varieties in the smooth case for small picard numbers as applications we figure out in this setting the fano examples and affirmatively test fujitas base point free conjec... | [['an', 'intrinsic', 'quadric', 'is', 'a', 'normal', 'projective', 'variety', 'with', 'a', 'cox', 'ring', 'defined', 'by', 'a', 'single', 'quadratic', 'relation', 'we', 'provide', 'explicit', 'descriptions', 'of', 'these', 'varieties', 'in', 'the', 'smooth', 'case', 'for', 'small', 'picard', 'numbers', 'as', 'applicati... | [-0.20242347072165173, -0.035017312797348356, -0.05165582908711468, 0.10781063271972996, -0.08033867595860592, -0.2082758876047312, 0.012399404220139751, 0.3298542912547978, -0.2991002437013846, -0.22497127101255152, 0.044797393515741885, -0.21749810579394063, -0.19461352101419693, 0.2833588891304456, -0.18041027170749... |
1,712.09823 | Conformal Quantum Mechanics and Sine-Square Deformation | We revisit conformal quantum mechanics (CQM) from the perspective of
sine-square deformation (SSD) and the entanglement Hamiltonian. The operators
that correspond to SSD and the entanglement Hamiltonian are identified. Thus,
the nature of SSD and entanglement can be discussed in a much simpler CQM
setting than higher... | hep-th cond-mat.stat-mech | we revisit conformal quantum mechanics cqm from the perspective of sinesquare deformation ssd and the entanglement hamiltonian the operators that correspond to ssd and the entanglement hamiltonian are identified thus the nature of ssd and entanglement can be discussed in a much simpler cqm setting than higherdimensiona... | [['we', 'revisit', 'conformal', 'quantum', 'mechanics', 'cqm', 'from', 'the', 'perspective', 'of', 'sinesquare', 'deformation', 'ssd', 'and', 'the', 'entanglement', 'hamiltonian', 'the', 'operators', 'that', 'correspond', 'to', 'ssd', 'and', 'the', 'entanglement', 'hamiltonian', 'are', 'identified', 'thus', 'the', 'nat... | [-0.08974890383815735, 0.19852605407430354, -0.10813823585607568, 0.13193397266714244, -0.018601057599583755, -0.21858712636428523, -0.053851175088701506, 0.2670421202534011, -0.21160164177037624, -0.23798444103069452, 0.0665128786444702, -0.26498225568888745, -0.169990498263731, 0.1703527888891344, -0.1030422148237727... |
1,712.09824 | $K \to \pi$ matrix elements of the chromomagnetic operator on the
lattice | We present the results of the first lattice QCD calculation of the $K \to
\pi$ matrix elements of the chromomagnetic operator $O_{CM} = g\, \bar s\,
\sigma_{\mu\nu} G_{\mu\nu} d$, which appears in the effective Hamiltonian
describing $\Delta S = 1$ transitions in and beyond the Standard Model. Having
dimension 5, the... | hep-lat hep-ph | we present the results of the first lattice qcd calculation of the k to pi matrix elements of the chromomagnetic operator o_cm g bar s sigma_munu g_munu d which appears in the effective hamiltonian describing delta s 1 transitions in and beyond the standard model having dimension 5 the chromomagnetic operator is charac... | [['we', 'present', 'the', 'results', 'of', 'the', 'first', 'lattice', 'qcd', 'calculation', 'of', 'the', 'k', 'to', 'pi', 'matrix', 'elements', 'of', 'the', 'chromomagnetic', 'operator', 'o_cm', 'g', 'bar', 's', 'sigma_munu', 'g_munu', 'd', 'which', 'appears', 'in', 'the', 'effective', 'hamiltonian', 'describing', 'del... | [-0.1106245767376903, 0.2444799808818245, -0.055214661527472085, 0.05522302857593097, -0.0017209207507395984, -0.1125104208106429, 0.049117796889134695, 0.3114512725592111, -0.17861456929640185, -0.27959437012869975, 0.0779094836066684, -0.30632030609242544, -0.07057380690997833, 0.11764137687707188, 0.0496833401525186... |
1,712.09825 | On the statistical properties of turbulent energy transfer rate in the
inner Heliosphere | The transfer of energy from large to small scales in solar wind turbulence is
an important ingredient of the longstanding question about the mechanism of the
interplanetary plasma heating. Previous studies have shown that
magnetohydrodynamic (MHD) turbulence is statistically compatible with the
observed solar wind he... | physics.space-ph astro-ph.SR physics.flu-dyn physics.plasm-ph | the transfer of energy from large to small scales in solar wind turbulence is an important ingredient of the longstanding question about the mechanism of the interplanetary plasma heating previous studies have shown that magnetohydrodynamic mhd turbulence is statistically compatible with the observed solar wind heating... | [['the', 'transfer', 'of', 'energy', 'from', 'large', 'to', 'small', 'scales', 'in', 'solar', 'wind', 'turbulence', 'is', 'an', 'important', 'ingredient', 'of', 'the', 'longstanding', 'question', 'about', 'the', 'mechanism', 'of', 'the', 'interplanetary', 'plasma', 'heating', 'previous', 'studies', 'have', 'shown', 'th... | [-0.11348509824305189, 0.1843201311132825, -0.04376250338904998, 0.1352758465690867, -0.04186819287144816, -0.0692068680399554, -0.0314629868688701, 0.35015491207732874, -0.26709950402853827, -0.35981230817589105, 0.06420931865680306, -0.24170282402021043, -0.08311264953375155, 0.2288665372805268, -0.011990765714104854... |
1,712.09826 | Holographic Complexity of Einstein-Maxwell-Dilaton Gravity | We study the holographic complexity of Einstein-Maxwell-Dilaton gravity using
the recently proposed "complexity = volume" and "complexity = action"
dualities. The model we consider has a ground state that is represented in the
bulk via a so-called hyperscaling violating geometry. We calculate the action
growth of the... | hep-th cond-mat.stat-mech quant-ph | we study the holographic complexity of einsteinmaxwelldilaton gravity using the recently proposed complexity volume and complexity action dualities the model we consider has a ground state that is represented in the bulk via a socalled hyperscaling violating geometry we calculate the action growth of the wheelerdewitt ... | [['we', 'study', 'the', 'holographic', 'complexity', 'of', 'einsteinmaxwelldilaton', 'gravity', 'using', 'the', 'recently', 'proposed', 'complexity', 'volume', 'and', 'complexity', 'action', 'dualities', 'the', 'model', 'we', 'consider', 'has', 'a', 'ground', 'state', 'that', 'is', 'represented', 'in', 'the', 'bulk', '... | [-0.1429241878714988, 0.10220200568532223, -0.09059693956202487, 0.07043270519328856, -0.07531378490517174, -0.12607426419324144, 0.04020287809000025, 0.28947081823068543, -0.19645356371756492, -0.25567469573239, 0.08294997402614482, -0.304296953194752, -0.1919958377578788, 0.1285384371081685, -0.05705030635377862, 0.0... |
1,712.09827 | A Syntactic Approach to Domain-Specific Automatic Question Generation | Factoid questions are questions that require short fact-based answers.
Automatic generation (AQG) of factoid questions from a given text can
contribute to educational activities, interactive question answering systems,
search engines, and other applications. The goal of our research is to generate
factoid source-ques... | cs.CL | factoid questions are questions that require short factbased answers automatic generation aqg of factoid questions from a given text can contribute to educational activities interactive question answering systems search engines and other applications the goal of our research is to generate factoid sourcequestionanswer ... | [['factoid', 'questions', 'are', 'questions', 'that', 'require', 'short', 'factbased', 'answers', 'automatic', 'generation', 'aqg', 'of', 'factoid', 'questions', 'from', 'a', 'given', 'text', 'can', 'contribute', 'to', 'educational', 'activities', 'interactive', 'question', 'answering', 'systems', 'search', 'engines', ... | [-0.062161691533164025, 0.009774313100414085, -0.06579988689770047, 0.07952008964743332, -0.17012586188027445, -0.1564553825265481, 0.09312685199787368, 0.3914875730739108, -0.2553040942614328, -0.35499858468466877, 0.07413563316471741, -0.2997917222424543, -0.11745308127316019, 0.25520999658358645, -0.1039655742898336... |
1,712.09828 | Extension Theorems for differential forms on low-dimensional good
quotients | In this paper we will show that the pull-back of any regular differential
form defined on the smooth locus of a good quotient of dimension three and four
to any resolution yields a regular differential form.
| math.AG | in this paper we will show that the pullback of any regular differential form defined on the smooth locus of a good quotient of dimension three and four to any resolution yields a regular differential form | [['in', 'this', 'paper', 'we', 'will', 'show', 'that', 'the', 'pullback', 'of', 'any', 'regular', 'differential', 'form', 'defined', 'on', 'the', 'smooth', 'locus', 'of', 'a', 'good', 'quotient', 'of', 'dimension', 'three', 'and', 'four', 'to', 'any', 'resolution', 'yields', 'a', 'regular', 'differential', 'form']] | [-0.20627753470196492, -0.027539361087191436, -0.10998801054019067, 0.04832111703581177, -0.08875704922765079, -0.08362213633437124, -0.03882350273003491, 0.3061729656118486, -0.282265215801696, -0.19126136518186992, 0.08814248602720909, -0.25350645029296476, -0.18550900287098354, 0.2244947607525521, -0.145280794757935... |
1,712.09829 | A Probabilistic Analysis on a Lattice Attack against DSA | Analyzing the security of cryptosystems under attacks based on the malicious
modification of memory registers is a research topic of high importance. This
type of attacks may affect the randomness of the secret parameters by forcing a
limited number of bits to a certain value which can be unknown to the attacker.
In ... | cs.CR math.NT | analyzing the security of cryptosystems under attacks based on the malicious modification of memory registers is a research topic of high importance this type of attacks may affect the randomness of the secret parameters by forcing a limited number of bits to a certain value which can be unknown to the attacker in this... | [['analyzing', 'the', 'security', 'of', 'cryptosystems', 'under', 'attacks', 'based', 'on', 'the', 'malicious', 'modification', 'of', 'memory', 'registers', 'is', 'a', 'research', 'topic', 'of', 'high', 'importance', 'this', 'type', 'of', 'attacks', 'may', 'affect', 'the', 'randomness', 'of', 'the', 'secret', 'paramete... | [-0.1327610606350936, 0.04712716488943746, -0.09744337451139776, 0.06591307753891064, -0.07854459368934234, -0.13297561069368385, 0.11634187151057025, 0.31898225830247007, -0.2719996135123074, -0.3018725276148568, 0.13014998022156457, -0.24065969919785857, -0.17027307920934012, 0.19260253718898943, -0.14044943403452634... |
1,712.0983 | Rigorous results in space-periodic two-dimensional turbulence | We survey the recent advance in the rigorous qualitative theory of the 2d
stochastic Navier-Stokes system that are relevant to the description of
turbulence in two-dimensional fluids. After discussing briefly the
initial-boundary value problem and the associated Markov process, we formulate
results on the existence, ... | math-ph math.AP math.MP math.PR physics.flu-dyn | we survey the recent advance in the rigorous qualitative theory of the 2d stochastic navierstokes system that are relevant to the description of turbulence in twodimensional fluids after discussing briefly the initialboundary value problem and the associated markov process we formulate results on the existence uniquene... | [['we', 'survey', 'the', 'recent', 'advance', 'in', 'the', 'rigorous', 'qualitative', 'theory', 'of', 'the', '2d', 'stochastic', 'navierstokes', 'system', 'that', 'are', 'relevant', 'to', 'the', 'description', 'of', 'turbulence', 'in', 'twodimensional', 'fluids', 'after', 'discussing', 'briefly', 'the', 'initialboundar... | [-0.12144385418793727, 0.07693220718946552, -0.06573786671821759, 0.11260699239082726, -0.04180793126035377, -0.08680442026946868, 0.04690484669838518, 0.29570464755051606, -0.31090232068846857, -0.24740137854399524, 0.17303303365049466, -0.27565386567795735, -0.1523053355549819, 0.19956467948227286, -0.071804557770281... |
1,712.09831 | Quantum-secured data transmission in urban fibre-optic communication
lines | Quantum key distribution (QKD) provides theoretic information security in
communications based on the laws of quantum physics. In this work, we report an
implementation of quantum-secured data transmission in the infrastructure of
Sberbank of Russia in standard communication lines in Moscow. The experiment is
realize... | quant-ph cs.CR | quantum key distribution qkd provides theoretic information security in communications based on the laws of quantum physics in this work we report an implementation of quantumsecured data transmission in the infrastructure of sberbank of russia in standard communication lines in moscow the experiment is realized on the... | [['quantum', 'key', 'distribution', 'qkd', 'provides', 'theoretic', 'information', 'security', 'in', 'communications', 'based', 'on', 'the', 'laws', 'of', 'quantum', 'physics', 'in', 'this', 'work', 'we', 'report', 'an', 'implementation', 'of', 'quantumsecured', 'data', 'transmission', 'in', 'the', 'infrastructure', 'o... | [-0.21708848776023199, 0.04965952709347968, -0.10238904863542961, 0.02418123729450333, 0.010393325565004252, -0.2582804232086169, 0.09622111668757247, 0.35169704756661646, -0.2318520867265761, -0.2769532653510692, 0.08519464634109015, -0.24097590202965388, -0.09501001431144834, 0.29691628231931994, -0.1305520688145747,... |
1,712.09832 | An Adiabatic Decomposition of the Hodge Cohomology of Manifolds Fibred
over Graphs | In this article we use the combinatorial and geometric structure of manifolds
with embedded cylinders in order to develop an adiabatic decomposition of the
Hodge cohomology of these manifolds. We will on the one hand describe the
adiabatic behaviour of spaces of harmonic forms by means of a certain
\v{C}ech-de Rham c... | math.DG math.AT | in this article we use the combinatorial and geometric structure of manifolds with embedded cylinders in order to develop an adiabatic decomposition of the hodge cohomology of these manifolds we will on the one hand describe the adiabatic behaviour of spaces of harmonic forms by means of a certain vcechde rham complex ... | [['in', 'this', 'article', 'we', 'use', 'the', 'combinatorial', 'and', 'geometric', 'structure', 'of', 'manifolds', 'with', 'embedded', 'cylinders', 'in', 'order', 'to', 'develop', 'an', 'adiabatic', 'decomposition', 'of', 'the', 'hodge', 'cohomology', 'of', 'these', 'manifolds', 'we', 'will', 'on', 'the', 'one', 'hand... | [-0.15697815019494474, 0.07253378228064818, -0.11617396752646363, 0.061015075544657356, -0.1232952299781821, -0.09296962651847439, -0.008553784018890424, 0.3175291062078693, -0.2703484731938013, -0.25159576538611544, 0.12338795782998205, -0.23453708001497117, -0.19670567368580535, 0.19272142432799394, -0.14611313071271... |
1,712.09833 | Full Asymptotics and Laurent Series of Layer Potentials for Laplace's
Equation on the Half-Space | We probe the application of the calculus of conormal distributions, in
particular the Pull-Back and Push-Forward Theorems, to the method of layer
potentials to solve the Dirichlet and Neumann problems on half-spaces. We
obtain full asymptotic expansions for the solutions (provided these exist for
the boundary data) a... | math.AP | we probe the application of the calculus of conormal distributions in particular the pullback and pushforward theorems to the method of layer potentials to solve the dirichlet and neumann problems on halfspaces we obtain full asymptotic expansions for the solutions provided these exist for the boundary data and a new p... | [['we', 'probe', 'the', 'application', 'of', 'the', 'calculus', 'of', 'conormal', 'distributions', 'in', 'particular', 'the', 'pullback', 'and', 'pushforward', 'theorems', 'to', 'the', 'method', 'of', 'layer', 'potentials', 'to', 'solve', 'the', 'dirichlet', 'and', 'neumann', 'problems', 'on', 'halfspaces', 'we', 'obta... | [-0.09137754067415457, 0.001446572431457152, -0.13472805122648357, 0.09545550965319533, -0.11999057076973926, -0.12542265541039818, 0.030255689999139912, 0.30607920918622217, -0.3232019189574303, -0.24483037500753316, 0.1645287413250467, -0.2560785791768325, -0.1451984956121465, 0.22307717553211734, -0.0938643952062644... |
1,712.09834 | Formation of adsorbate structures induced by external electric field in
plasma-condensate systems | We present a new model of plasma-condensate system, by taking into account an
anisotropy of transference reactions of adatoms between neighbor layers of
multi-layer system, caused by the strength of the electric field near
substrate. We discuss an influence of the strength of the electric field onto
first-order phase... | cond-mat.mes-hall | we present a new model of plasmacondensate system by taking into account an anisotropy of transference reactions of adatoms between neighbor layers of multilayer system caused by the strength of the electric field near substrate we discuss an influence of the strength of the electric field onto firstorder phase transit... | [['we', 'present', 'a', 'new', 'model', 'of', 'plasmacondensate', 'system', 'by', 'taking', 'into', 'account', 'an', 'anisotropy', 'of', 'transference', 'reactions', 'of', 'adatoms', 'between', 'neighbor', 'layers', 'of', 'multilayer', 'system', 'caused', 'by', 'the', 'strength', 'of', 'the', 'electric', 'field', 'near... | [-0.1885251641694475, 0.18622544168223007, -0.015990800629934354, -0.016895547437462768, 0.022739525152972402, -0.1316139023878019, 0.06735380833752153, 0.36244534366209097, -0.28969613957510454, -0.3030158725915232, -0.02295053379864178, -0.2556605122212057, -0.14848057137369508, 0.1606975710466316, 0.0652795826541165... |
1,712.09835 | Connecting Software Metrics across Versions to Predict Defects | Accurate software defect prediction could help software practitioners
allocate test resources to defect-prone modules effectively and efficiently. In
the last decades, much effort has been devoted to build accurate defect
prediction models, including developing quality defect predictors and modeling
techniques. Howev... | cs.SE cs.LG | accurate software defect prediction could help software practitioners allocate test resources to defectprone modules effectively and efficiently in the last decades much effort has been devoted to build accurate defect prediction models including developing quality defect predictors and modeling techniques however curr... | [['accurate', 'software', 'defect', 'prediction', 'could', 'help', 'software', 'practitioners', 'allocate', 'test', 'resources', 'to', 'defectprone', 'modules', 'effectively', 'and', 'efficiently', 'in', 'the', 'last', 'decades', 'much', 'effort', 'has', 'been', 'devoted', 'to', 'build', 'accurate', 'defect', 'predicti... | [0.006616825853436164, -0.03724284398956352, -0.058838389086902254, 0.13993450083053674, -0.10079514487225512, -0.2008430757814993, -0.0016820101874357421, 0.47639955572579823, -0.24224585299268492, -0.3277691279614523, 0.11600345229229264, -0.2456196702726517, -0.19416192121531062, 0.19746064270482946, -0.124829781723... |
1,712.09836 | Development of high vorticity structures and geometrical properties of
the vortex line representation | The incompressible three-dimensional Euler equations develop very thin
pancake-like regions of increasing vorticity. These regions evolve with the
scaling $\omega_{max}\sim\ell^{-2/3}$ between the vorticity maximum and the
pancake thickness, as was observed in the recent numerical experiments [D.S.
Agafontsev et al, ... | physics.flu-dyn | the incompressible threedimensional euler equations develop very thin pancakelike regions of increasing vorticity these regions evolve with the scaling omega_maxsimell23 between the vorticity maximum and the pancake thickness as was observed in the recent numerical experiments ds agafontsev et al phys fluids 27 085102 ... | [['the', 'incompressible', 'threedimensional', 'euler', 'equations', 'develop', 'very', 'thin', 'pancakelike', 'regions', 'of', 'increasing', 'vorticity', 'these', 'regions', 'evolve', 'with', 'the', 'scaling', 'omega_maxsimell23', 'between', 'the', 'vorticity', 'maximum', 'and', 'the', 'pancake', 'thickness', 'as', 'w... | [-0.17036094963081555, 0.10420554569460076, -0.05642453177409957, -0.03510466865600719, -0.04301461056812847, -0.06928863848405455, -0.030499199450538635, 0.3105133575749108, -0.24699321384508188, -0.31367659509699564, 0.06712193738940514, -0.25928475022007774, -0.11900094899235011, 0.1637327731385988, -0.0020665384212... |
1,712.09837 | Revisiting Hyperbolicity of Relativistic Fluids | Motivated by the desire for highly accurate numerical computations of compact
binary spacetimes in the era of gravitational wave astronomy, we reexamine
hyperbolicity and well-posedness of the initial value problem for popular
models of general relativistic fluids. Our analysis relies heavily on the
dual-frame formal... | gr-qc | motivated by the desire for highly accurate numerical computations of compact binary spacetimes in the era of gravitational wave astronomy we reexamine hyperbolicity and wellposedness of the initial value problem for popular models of general relativistic fluids our analysis relies heavily on the dualframe formalism wh... | [['motivated', 'by', 'the', 'desire', 'for', 'highly', 'accurate', 'numerical', 'computations', 'of', 'compact', 'binary', 'spacetimes', 'in', 'the', 'era', 'of', 'gravitational', 'wave', 'astronomy', 'we', 'reexamine', 'hyperbolicity', 'and', 'wellposedness', 'of', 'the', 'initial', 'value', 'problem', 'for', 'popular... | [-0.10236420481027488, 0.09490905806071846, -0.09740764736215009, 0.08025841470990402, -0.1280319512182591, -0.1433530868067607, -0.023067498403400475, 0.3260732864011444, -0.24212430717775088, -0.27390843767526685, 0.09144721958448417, -0.21308876406321503, -0.13977209626167428, 0.22945339214148036, -0.060607049276244... |
1,712.09838 | Cosmic evolution of AGN with moderate-to-high radiative luminosity in
the COSMOS field | We study the moderate-to-high radiative luminosity active galactic nuclei
(HLAGN) within the VLA-COSMOS 3 GHz Large Project. The survey covers 2.6 square
degrees centered on the COSMOS field with a 1$\sigma$ sensitivity of 2.3
$\mathrm{\mu Jy}$/beam across the field. This provides the simultaneously
largest and deepe... | astro-ph.GA | we study the moderatetohigh radiative luminosity active galactic nuclei hlagn within the vlacosmos 3 ghz large project the survey covers 26 square degrees centered on the cosmos field with a 1sigma sensitivity of 23 mathrmmu jybeam across the field this provides the simultaneously largest and deepest radio continuum su... | [['we', 'study', 'the', 'moderatetohigh', 'radiative', 'luminosity', 'active', 'galactic', 'nuclei', 'hlagn', 'within', 'the', 'vlacosmos', '3', 'ghz', 'large', 'project', 'the', 'survey', 'covers', '26', 'square', 'degrees', 'centered', 'on', 'the', 'cosmos', 'field', 'with', 'a', '1sigma', 'sensitivity', 'of', '23', ... | [-0.040723484180959536, 0.06725537426235965, -0.023148479184047097, 0.09761677441649697, -0.09359168310152353, -0.018308420025673854, 0.09474036954089898, 0.4762306399643421, -0.09869683386922694, -0.3751875299985717, 0.08046817400280487, -0.31697746321913745, 0.043405617927407, 0.1484640173290913, 0.05318445905878329,... |
1,712.09839 | Maximally Supersymmetric AdS Solutions in Gauged Supergravity | In this thesis we study maximally supersymmetric solutions of gauged
supergravity theories, with special focus on anti-de Sitter solutions. The
latter are relevant in the context of the AdS/CFT correspondence. In the first
part we classify all maximally supersymmetric solutions of all gauged or
deformed supergravity ... | hep-th | in this thesis we study maximally supersymmetric solutions of gauged supergravity theories with special focus on antide sitter solutions the latter are relevant in the context of the adscft correspondence in the first part we classify all maximally supersymmetric solutions of all gauged or deformed supergravity theorie... | [['in', 'this', 'thesis', 'we', 'study', 'maximally', 'supersymmetric', 'solutions', 'of', 'gauged', 'supergravity', 'theories', 'with', 'special', 'focus', 'on', 'antide', 'sitter', 'solutions', 'the', 'latter', 'are', 'relevant', 'in', 'the', 'context', 'of', 'the', 'adscft', 'correspondence', 'in', 'the', 'first', '... | [-0.131868685947313, 0.14744592452307745, 0.04689214703607924, 0.10748928849352524, -0.055311546461390595, -0.18852567309703755, -0.08611286356474976, 0.28132781312249755, -0.10702877568689231, -0.22697389959025063, 0.14420544637880306, -0.31074215846411807, -0.19632712223481538, 0.020618033785449, -0.09051934616849283... |
1,712.0984 | Theoretical calculation of transport properties of oxide material using
narrow band model | We report about the results of theoretical calculations of temperature
dependence of resistivity ($\rho$) and Seebeck coefficient ($S$) for
thermoelectric (TE) and superconductivity (SC) phases by arithmetic equations
based on narrow band model with oxygen deficient structure, as the functions of
band-filling degree ... | cond-mat.mtrl-sci | we report about the results of theoretical calculations of temperature dependence of resistivity rho and seebeck coefficient s for thermoelectric te and superconductivity sc phases by arithmetic equations based on narrow band model with oxygen deficient structure as the functions of bandfilling degree f and band width ... | [['we', 'report', 'about', 'the', 'results', 'of', 'theoretical', 'calculations', 'of', 'temperature', 'dependence', 'of', 'resistivity', 'rho', 'and', 'seebeck', 'coefficient', 's', 'for', 'thermoelectric', 'te', 'and', 'superconductivity', 'sc', 'phases', 'by', 'arithmetic', 'equations', 'based', 'on', 'narrow', 'ban... | [-0.16562878414510918, 0.15231534498982513, -0.030338966156332157, -0.019990588481633518, -0.0008496366656170442, -0.14872339555922037, 0.150985584474909, 0.38271386405596364, -0.25187586864026695, -0.30991603937955237, 0.00715216867124232, -0.34980197866948753, -0.10218549989020595, 0.1579054180944625, 0.0895824374583... |
1,712.09841 | Resurrecting Quartic and Quadratic inflaton potentials in two-field
inflationary model | After the release of the PLANCK data, it is evident that inflationary
paradigm has stood the test of time. Even though, it is difficult to realise
inflationary paradigm in a particle physics model as the present observations
have ruled out the simplest quartic and quadratic inflationary potentials,
which generically ... | astro-ph.CO hep-ph | after the release of the planck data it is evident that inflationary paradigm has stood the test of time even though it is difficult to realise inflationary paradigm in a particle physics model as the present observations have ruled out the simplest quartic and quadratic inflationary potentials which generically arise ... | [['after', 'the', 'release', 'of', 'the', 'planck', 'data', 'it', 'is', 'evident', 'that', 'inflationary', 'paradigm', 'has', 'stood', 'the', 'test', 'of', 'time', 'even', 'though', 'it', 'is', 'difficult', 'to', 'realise', 'inflationary', 'paradigm', 'in', 'a', 'particle', 'physics', 'model', 'as', 'the', 'present', '... | [-0.11253850750238469, 0.17852395164248133, -0.1195824213625331, 0.14336298598105454, -0.10666252417026303, -0.24506244136136957, -0.05640844112661268, 0.31384544322333696, -0.22177050705067813, -0.31195158967083053, 0.08402395587784538, -0.24239137721347756, -0.16719041684908525, 0.2224512940696773, -0.020044567275493... |
1,712.09842 | Impact parameter smearing effects on isospin sensitive observables in
heavy ion collisions | The validity of impact parameter estimation from the multiplicity of charged
particles at low-intermediate energies is checked within the framework of ImQMD
model. The simulations show that the multiplicity of charged particles cannot
estimate the impact parameter of heavy ion collisions very well, especially for
cen... | nucl-th nucl-ex | the validity of impact parameter estimation from the multiplicity of charged particles at lowintermediate energies is checked within the framework of imqmd model the simulations show that the multiplicity of charged particles cannot estimate the impact parameter of heavy ion collisions very well especially for central ... | [['the', 'validity', 'of', 'impact', 'parameter', 'estimation', 'from', 'the', 'multiplicity', 'of', 'charged', 'particles', 'at', 'lowintermediate', 'energies', 'is', 'checked', 'within', 'the', 'framework', 'of', 'imqmd', 'model', 'the', 'simulations', 'show', 'that', 'the', 'multiplicity', 'of', 'charged', 'particle... | [-0.058255263218597975, 0.23699141859273928, -0.0843683816169337, 0.13304895647161175, 0.06018049352188917, -0.11964859407509301, -0.017914636868786495, 0.31823214805738714, -0.17304640954870804, -0.34617324280015266, -0.022194459271514252, -0.3206482616414388, 0.08634109479065116, 0.17048430386561308, 0.05074124891521... |
1,712.09843 | Localization of $U(1)$ gauge vector field on flat branes with
five-dimension (asymptotic) AdS$_{5}$ spacetime | In order to localize $U(1)$ gauge vector field on Randall-Sundrum-like
braneworld model with infinite extra dimension, we propose a new kind of
non-minimal coupling between the $U(1)$ gauge field and the gravity. We propose
three kinds of coupling methods and they all support the localization of zero
mode. In additio... | hep-th gr-qc hep-ph | in order to localize u1 gauge vector field on randallsundrumlike braneworld model with infinite extra dimension we propose a new kind of nonminimal coupling between the u1 gauge field and the gravity we propose three kinds of coupling methods and they all support the localization of zero mode in addition one of them ca... | [['in', 'order', 'to', 'localize', 'u1', 'gauge', 'vector', 'field', 'on', 'randallsundrumlike', 'braneworld', 'model', 'with', 'infinite', 'extra', 'dimension', 'we', 'propose', 'a', 'new', 'kind', 'of', 'nonminimal', 'coupling', 'between', 'the', 'u1', 'gauge', 'field', 'and', 'the', 'gravity', 'we', 'propose', 'thre... | [-0.16785789131143586, 0.20461238799400108, -0.04691646243770455, 0.08139093864579187, -0.1107356377747343, -0.18708874596564404, -0.006223719502084477, 0.3683211839822836, -0.19419763917319996, -0.28448601179691246, 0.08729909883465531, -0.23194194491952658, -0.1422927775528542, 0.11672130690855083, -0.018633059550856... |
1,712.09844 | Wheeler-DeWitt Quantization of Gravity Models of Unified Dark Energy and
Dark Matter | First, we describe the construction of a new type of gravity-matter models
based on the formalism of non-Riemannian space-time volume forms - alternative
generally covariant integration measure densities (volume elements) defined in
terms of auxiliary antisymmetric tensor gauge fields. Here gravity couples in a
non-c... | gr-qc hep-th | first we describe the construction of a new type of gravitymatter models based on the formalism of nonriemannian spacetime volume forms alternative generally covariant integration measure densities volume elements defined in terms of auxiliary antisymmetric tensor gauge fields here gravity couples in a nonconventional ... | [['first', 'we', 'describe', 'the', 'construction', 'of', 'a', 'new', 'type', 'of', 'gravitymatter', 'models', 'based', 'on', 'the', 'formalism', 'of', 'nonriemannian', 'spacetime', 'volume', 'forms', 'alternative', 'generally', 'covariant', 'integration', 'measure', 'densities', 'volume', 'elements', 'defined', 'in', ... | [-0.19002266093380302, 0.20374576480847276, -0.11319594834213184, 0.12869321395403255, -0.12699526466528918, -0.13331238407922927, -0.057150237354265894, 0.27972915508745316, -0.18641241159412764, -0.29185459219633103, 0.01670222751891051, -0.1842807052499464, -0.1375199345464701, 0.07916069711268528, 0.020778087960433... |
1,712.09845 | Century of $\Lambda$ | The cosmological constant was proposed 100 years ago in order to make the
model of static Universe, imagined then by most scientists, possible. Today it
is the main candidate for the physical essence causing the observed accelerated
expansion of our Universe. But, as well as a hundred years ago, its nature is
unknown... | physics.hist-ph astro-ph.CO | the cosmological constant was proposed 100 years ago in order to make the model of static universe imagined then by most scientists possible today it is the main candidate for the physical essence causing the observed accelerated expansion of our universe but as well as a hundred years ago its nature is unknown this pa... | [['the', 'cosmological', 'constant', 'was', 'proposed', '100', 'years', 'ago', 'in', 'order', 'to', 'make', 'the', 'model', 'of', 'static', 'universe', 'imagined', 'then', 'by', 'most', 'scientists', 'possible', 'today', 'it', 'is', 'the', 'main', 'candidate', 'for', 'the', 'physical', 'essence', 'causing', 'the', 'obs... | [-0.0258781591906432, 0.11104076891467812, -0.08894355936771196, 0.05849277163761553, -0.13218111107439806, -0.1016020609296105, 0.0076367475335705984, 0.32231636027271826, -0.2455085337834349, -0.3908819448140063, 0.10835005213333859, -0.27041879377924327, -0.11531803448778692, 0.1901512962603795, -0.05582697285611308... |
1,712.09846 | Rating Protocol Design for Extortion and Cooperation in the
Crowdsourcing Contest Dilemma | Crowdsourcing has emerged as a paradigm for leveraging human intelligence and
activity to solve a wide range of tasks. However, strategic workers will find
enticement in their self-interest to free-ride and attack in a crowdsourcing
contest dilemma game. Hence, incentive mechanisms are of great importance to
overcome... | cs.GT | crowdsourcing has emerged as a paradigm for leveraging human intelligence and activity to solve a wide range of tasks however strategic workers will find enticement in their selfinterest to freeride and attack in a crowdsourcing contest dilemma game hence incentive mechanisms are of great importance to overcome the ine... | [['crowdsourcing', 'has', 'emerged', 'as', 'a', 'paradigm', 'for', 'leveraging', 'human', 'intelligence', 'and', 'activity', 'to', 'solve', 'a', 'wide', 'range', 'of', 'tasks', 'however', 'strategic', 'workers', 'will', 'find', 'enticement', 'in', 'their', 'selfinterest', 'to', 'freeride', 'and', 'attack', 'in', 'a', '... | [-0.12348771138123185, -0.009246164242586478, -0.054658193715214215, 0.07579020959868406, -0.15969904374467642, -0.24263087182183457, 0.13590151442019646, 0.43971855969478685, -0.2754695474527626, -0.35074236144245874, 0.07224417213559847, -0.25723652593598045, -0.18213580996844672, 0.12075137765842932, -0.180534727250... |
1,712.09847 | Multi-particle instability in a spin-imbalanced Fermi gas | Weak attractive interactions in a spin-imbalanced Fermi gas induce a
multi-particle instability, binding multiple fermions together. The maximum
binding energy per particle is achieved when the ratio of the number of up- and
down-spin particles in the instability is equal to the ratio of the up- and
down-spin densiti... | cond-mat.str-el cond-mat.quant-gas cond-mat.supr-con | weak attractive interactions in a spinimbalanced fermi gas induce a multiparticle instability binding multiple fermions together the maximum binding energy per particle is achieved when the ratio of the number of up and downspin particles in the instability is equal to the ratio of the up and downspin densities of stat... | [['weak', 'attractive', 'interactions', 'in', 'a', 'spinimbalanced', 'fermi', 'gas', 'induce', 'a', 'multiparticle', 'instability', 'binding', 'multiple', 'fermions', 'together', 'the', 'maximum', 'binding', 'energy', 'per', 'particle', 'is', 'achieved', 'when', 'the', 'ratio', 'of', 'the', 'number', 'of', 'up', 'and',... | [-0.19732433515649367, 0.2137985515535547, -0.07984738194936654, 0.11656446964188945, 0.006131164539450159, -0.12695093791699036, 0.0901130571544248, 0.2648217048030347, -0.21871962768297332, -0.28283390591386703, -0.06749366204506563, -0.3211441210471094, -0.04635593334484535, 0.1386244462870915, 0.06328005914886793, ... |
1,712.09848 | Game-Theoretic Design of Optimal Two-Sided Rating Protocols for Service
Exchange Dilemma in Crowdsourcing | Despite the increasing popularity and successful examples of crowdsourcing,
it is stripped of aureole when collective efforts are derailed or severely
hindered by elaborate sabotage. A service exchange dilemma arises when
non-cooperation among self-interested users, and zero social welfare is
obtained at myopic equil... | cs.GT | despite the increasing popularity and successful examples of crowdsourcing it is stripped of aureole when collective efforts are derailed or severely hindered by elaborate sabotage a service exchange dilemma arises when noncooperation among selfinterested users and zero social welfare is obtained at myopic equilibrium ... | [['despite', 'the', 'increasing', 'popularity', 'and', 'successful', 'examples', 'of', 'crowdsourcing', 'it', 'is', 'stripped', 'of', 'aureole', 'when', 'collective', 'efforts', 'are', 'derailed', 'or', 'severely', 'hindered', 'by', 'elaborate', 'sabotage', 'a', 'service', 'exchange', 'dilemma', 'arises', 'when', 'nonc... | [-0.13956595163787736, 0.032546705648378235, -0.042328123262989646, 0.07959423153877539, -0.15837664547504082, -0.26335574839824594, 0.18129124792562634, 0.44506591427824005, -0.2523557979086068, -0.32138761564439156, 0.05813766938718695, -0.27376770429968406, -0.16162053073202137, 0.1035620062519277, -0.14984080026161... |
1,712.09849 | Search for magnetic monopoles with the MoEDAL forward trapping detector
in 2.11 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC | We update our previous search for trapped magnetic monopoles in LHC Run 2
using nearly six times more integrated luminosity and including additional
models for the interpretation of the data. The MoEDAL forward trapping
detector, comprising 222~kg of aluminium samples, was exposed to 2.11~fb$^{-1}$
of 13 TeV proton-p... | hep-ex hep-ph | we update our previous search for trapped magnetic monopoles in lhc run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data the moedal forward trapping detector comprising 222kg of aluminium samples was exposed to 211fb1 of 13 tev protonproton collision... | [['we', 'update', 'our', 'previous', 'search', 'for', 'trapped', 'magnetic', 'monopoles', 'in', 'lhc', 'run', '2', 'using', 'nearly', 'six', 'times', 'more', 'integrated', 'luminosity', 'and', 'including', 'additional', 'models', 'for', 'the', 'interpretation', 'of', 'the', 'data', 'the', 'moedal', 'forward', 'trapping... | [-0.10359610294813826, 0.23029820647824442, 0.00771488734718525, 0.09280696834409327, -0.00753902885921751, -0.13604018443870838, 0.03632346479483231, 0.38080675008523307, -0.1643338211543971, -0.3742199955564557, 0.035006205745351814, -0.3762622470544143, 0.033966408398665604, 0.1709528714277302, 0.09061594447032831, ... |
1,712.0985 | On Pareto Joint Inversion of guided waves | We use the Pareto Joint Inversion, together with the Particle Swarm
Optimization, to invert the Love and quasi-Rayleigh surface-wave speeds,
obtained from dispersion curves, in order to infer the elasticity parameters,
mass densities and layer thickness of the model for which these curves are
generated. For both wave... | physics.geo-ph | we use the pareto joint inversion together with the particle swarm optimization to invert the love and quasirayleigh surfacewave speeds obtained from dispersion curves in order to infer the elasticity parameters mass densities and layer thickness of the model for which these curves are generated for both waves we use t... | [['we', 'use', 'the', 'pareto', 'joint', 'inversion', 'together', 'with', 'the', 'particle', 'swarm', 'optimization', 'to', 'invert', 'the', 'love', 'and', 'quasirayleigh', 'surfacewave', 'speeds', 'obtained', 'from', 'dispersion', 'curves', 'in', 'order', 'to', 'infer', 'the', 'elasticity', 'parameters', 'mass', 'dens... | [-0.07848237319052578, 0.14067669184998308, -0.012067104674835894, 0.05271507706778147, -0.09113152322289658, -0.12177616351826943, 0.050317732606053274, 0.37919898352580755, -0.24133606702288524, -0.3653985171872664, 0.11743027406724738, -0.29029492353572245, -0.11610125890001655, 0.2476427694415315, -0.02032512767031... |
1,712.09851 | Lp-estimates for the square root of elliptic systems with mixed boundary
conditions | This article focuses on Lp-estimates for the square root of elliptic systems
of second order in divergence form on a bounded domain. We treat complex
bounded measurable coefficients and allow for mixed Dirichlet/Neumann boundary
conditions on domains beyond the Lipschitz class. If there is an associated
bounded semig... | math.CA math.AP | this article focuses on lpestimates for the square root of elliptic systems of second order in divergence form on a bounded domain we treat complex bounded measurable coefficients and allow for mixed dirichletneumann boundary conditions on domains beyond the lipschitz class if there is an associated bounded semigroup o... | [['this', 'article', 'focuses', 'on', 'lpestimates', 'for', 'the', 'square', 'root', 'of', 'elliptic', 'systems', 'of', 'second', 'order', 'in', 'divergence', 'form', 'on', 'a', 'bounded', 'domain', 'we', 'treat', 'complex', 'bounded', 'measurable', 'coefficients', 'and', 'allow', 'for', 'mixed', 'dirichletneumann', 'b... | [-0.1326719767676958, 0.06981636151355822, -0.0258841444177911, 0.07766635796422658, -0.11178715228654292, -0.12900954123814495, 0.01704045338239394, 0.3280591125430565, -0.32932628954754395, -0.18455832947020223, 0.18458886419701687, -0.2775529914117437, -0.10983841673496375, 0.25663158881674414, -0.12111199514775657,... |
1,712.09852 | Exact Solutions to Non-Linear Symmetron Theory: One and Two Mirror
Systems | We derive the exact analytical solutions to the symmetron field theory
equations in the presence of a one or two mirror system. The one dimensional
equations of motion are integrated exactly for both systems and their solutions
can be expressed in terms of Jacobi elliptic functions. Surprisingly, in the
case of two p... | gr-qc astro-ph.CO hep-ph | we derive the exact analytical solutions to the symmetron field theory equations in the presence of a one or two mirror system the one dimensional equations of motion are integrated exactly for both systems and their solutions can be expressed in terms of jacobi elliptic functions surprisingly in the case of two parall... | [['we', 'derive', 'the', 'exact', 'analytical', 'solutions', 'to', 'the', 'symmetron', 'field', 'theory', 'equations', 'in', 'the', 'presence', 'of', 'a', 'one', 'or', 'two', 'mirror', 'system', 'the', 'one', 'dimensional', 'equations', 'of', 'motion', 'are', 'integrated', 'exactly', 'for', 'both', 'systems', 'and', 't... | [-0.17859898875870456, 0.0903504319005431, -0.09157417500570703, 0.05732952461739142, -0.05771228607940989, -0.13805615345392233, -0.03665491415281744, 0.3037027146559782, -0.2542297068665413, -0.30584470324146634, 0.10372555224939088, -0.2913193340019251, -0.1285308403390585, 0.21755564100861263, 0.010585852647916628,... |
1,712.09853 | A Partially Supervised Bayesian Image Classification Model with
Applications in Diagnosis of Sentinel Lymph Node Metastases in Breast Cancer | A method has been developed for the analysis of images of sentinel lymph
nodes generated by a spectral scanning device. The aim is to classify the
nodes, excised during surgery for breast cancer, as normal or metastatic. The
data from one node constitute spectra at 86 wavelengths for each pixel of a
20*20 grid. For t... | stat.AP | a method has been developed for the analysis of images of sentinel lymph nodes generated by a spectral scanning device the aim is to classify the nodes excised during surgery for breast cancer as normal or metastatic the data from one node constitute spectra at 86 wavelengths for each pixel of a 2020 grid for the analy... | [['a', 'method', 'has', 'been', 'developed', 'for', 'the', 'analysis', 'of', 'images', 'of', 'sentinel', 'lymph', 'nodes', 'generated', 'by', 'a', 'spectral', 'scanning', 'device', 'the', 'aim', 'is', 'to', 'classify', 'the', 'nodes', 'excised', 'during', 'surgery', 'for', 'breast', 'cancer', 'as', 'normal', 'or', 'met... | [-0.03386416746147535, 0.03893748948418244, -0.06989691942922016, 0.05682461578522025, -0.0602738530229416, -0.17698044517171868, 0.06769703542567494, 0.3949728766763952, -0.23791996793529646, -0.3246476111835123, 0.09539402631216062, -0.2897610893095577, -0.08758481800974663, 0.16755989161735432, -0.07160330724508587,... |
1,712.09854 | No arbitrage and lead-lag relationships | The existence of time-lagged cross-correlations between the returns of a pair
of assets, which is known as the lead-lag relationship, is a well-known
stylized fact in financial econometrics. Recently some continuous-time models
have been proposed to take account of the lead-lag relationship. Such a model
does not fol... | q-fin.MF math.PR | the existence of timelagged crosscorrelations between the returns of a pair of assets which is known as the leadlag relationship is a wellknown stylized fact in financial econometrics recently some continuoustime models have been proposed to take account of the leadlag relationship such a model does not follow a semima... | [['the', 'existence', 'of', 'timelagged', 'crosscorrelations', 'between', 'the', 'returns', 'of', 'a', 'pair', 'of', 'assets', 'which', 'is', 'known', 'as', 'the', 'leadlag', 'relationship', 'is', 'a', 'wellknown', 'stylized', 'fact', 'in', 'financial', 'econometrics', 'recently', 'some', 'continuoustime', 'models', 'h... | [-0.1316938910025115, 0.07062565867343029, -0.13650585869232154, 0.1742633001389438, -0.10718997998391183, -0.12761373622152877, 0.06528211356383007, 0.4272099902178636, -0.30827097539618914, -0.26344101464112135, 0.14882287947337466, -0.2921004054963361, -0.18208602592301537, 0.1310636083885305, -0.14401417152423943, ... |
1,712.09855 | Beyond-Planarity: Density Results for Bipartite Graphs | Beyond-planarity focuses on the study of geometric and topological graphs
that are in some sense nearly-planar. Here, planarity is relaxed by allowing
edge crossings, but only with respect to some local forbidden crossing
configurations. Early research dates back to the 1960s (e.g., Avital and Hanani
1966) for extrem... | cs.DM cs.CG | beyondplanarity focuses on the study of geometric and topological graphs that are in some sense nearlyplanar here planarity is relaxed by allowing edge crossings but only with respect to some local forbidden crossing configurations early research dates back to the 1960s eg avital and hanani 1966 for extremal problems o... | [['beyondplanarity', 'focuses', 'on', 'the', 'study', 'of', 'geometric', 'and', 'topological', 'graphs', 'that', 'are', 'in', 'some', 'sense', 'nearlyplanar', 'here', 'planarity', 'is', 'relaxed', 'by', 'allowing', 'edge', 'crossings', 'but', 'only', 'with', 'respect', 'to', 'some', 'local', 'forbidden', 'crossing', 'c... | [-0.13791368555710973, 0.11983853332892275, -0.017882607275583218, 0.059771449345459075, -0.14432402659843832, -0.15010099561128876, 0.06477317197990631, 0.3895090699477103, -0.2566141519300169, -0.38070240402784394, 0.11295828263512767, -0.2964748470423891, -0.16615381980739016, 0.18563293774455492, -0.154206935414873... |
1,712.09856 | Tight Bounds for Maximal Identifiability of Failure Nodes in Boolean
Network Tomography | We study maximal identifiability, a measure recently introduced in Boolean
Network Tomography to characterize networks' capability to localize failure
nodes in end-to-end path measurements. We prove tight upper and lower bounds on
the maximal identifiability of failure nodes for specific classes of network
topologies... | cs.DS cs.NI | we study maximal identifiability a measure recently introduced in boolean network tomography to characterize networks capability to localize failure nodes in endtoend path measurements we prove tight upper and lower bounds on the maximal identifiability of failure nodes for specific classes of network topologies such a... | [['we', 'study', 'maximal', 'identifiability', 'a', 'measure', 'recently', 'introduced', 'in', 'boolean', 'network', 'tomography', 'to', 'characterize', 'networks', 'capability', 'to', 'localize', 'failure', 'nodes', 'in', 'endtoend', 'path', 'measurements', 'we', 'prove', 'tight', 'upper', 'and', 'lower', 'bounds', 'o... | [-0.16307146289997387, 0.06873224724746163, 0.022600863848431373, 0.06550389636204162, -0.05477106142284192, -0.20205094427408943, 0.10062862568358184, 0.4049603941665222, -0.238439434121015, -0.30499289597171436, 0.11537044004997216, -0.26606743053970744, -0.19397127419339874, 0.1439814532767555, -0.08562840236871957,... |
1,712.09857 | Galaxy Evolution in the Cluster Abell 85: New Insights from the Dwarf
Population | We present the first results of a new spectroscopic survey of the cluster
Abell 85 targeting 1466 candidate cluster members within the central $\sim$1
deg$^2$ of the cluster and having magnitudes $m_r < 20.5$ using VIMOS/VLT and
HYDRA/WIYN. A total of 520 galaxies are confirmed as either relaxed cluster
members or pa... | astro-ph.GA | we present the first results of a new spectroscopic survey of the cluster abell 85 targeting 1466 candidate cluster members within the central sim1 deg2 of the cluster and having magnitudes m_r 205 using vimosvlt and hydrawiyn a total of 520 galaxies are confirmed as either relaxed cluster members or part of an infalli... | [['we', 'present', 'the', 'first', 'results', 'of', 'a', 'new', 'spectroscopic', 'survey', 'of', 'the', 'cluster', 'abell', '85', 'targeting', '1466', 'candidate', 'cluster', 'members', 'within', 'the', 'central', 'sim1', 'deg2', 'of', 'the', 'cluster', 'and', 'having', 'magnitudes', 'm_r', '205', 'using', 'vimosvlt', ... | [-0.07416634030935178, 0.1291880710156467, -0.05350619204922435, 0.13097043536592914, -0.0842760851835543, -0.011612316880551777, 0.06918122512810253, 0.45730402934011716, -0.06128801548440042, -0.3933454387548283, 0.03946264196139086, -0.27228274332873265, -0.018774429594110378, 0.164506850855983, 0.005403393932220783... |
1,712.09858 | Prolongations vs. Tulczyjew triples in Geometric Mechanics | In the scientific literature there are basically two schools of formulating
Lagrangian (or Hamiltonian) mechanics in the (Lie) algebroid setting: in terms
of prolongations and in terms of Tulczyjew triples. Despite the fact that in
both approaches we describe the same phenomena, so far no comparison between
prolongat... | math-ph math.DG math.MP | in the scientific literature there are basically two schools of formulating lagrangian or hamiltonian mechanics in the lie algebroid setting in terms of prolongations and in terms of tulczyjew triples despite the fact that in both approaches we describe the same phenomena so far no comparison between prolongations and ... | [['in', 'the', 'scientific', 'literature', 'there', 'are', 'basically', 'two', 'schools', 'of', 'formulating', 'lagrangian', 'or', 'hamiltonian', 'mechanics', 'in', 'the', 'lie', 'algebroid', 'setting', 'in', 'terms', 'of', 'prolongations', 'and', 'in', 'terms', 'of', 'tulczyjew', 'triples', 'despite', 'the', 'fact', '... | [-0.1384788275973641, 0.059225819828354995, -0.08091326284462984, 0.12573433372720533, -0.12692302067795497, -0.09769003038305078, 0.0212268146864149, 0.3934741810047894, -0.26299601646789006, -0.31071104896202517, 0.03487476230117628, -0.25643293090750663, -0.2071056180525528, 0.14716371894667574, -0.14636294814768466... |
1,712.09859 | A Secure and Authenticated Key Management Protocol (SA-KMP) for
Vehicular Networks | Public key infrastructure (PKI) is the most widely used security mechanism
for securing communications over the network. However, there are known
performance issues, making it unsuitable for use in vehicular networks. In this
paper, we propose a secure and authenticated key management protocol (SA-KMP)
to overcome th... | cs.CR | public key infrastructure pki is the most widely used security mechanism for securing communications over the network however there are known performance issues making it unsuitable for use in vehicular networks in this paper we propose a secure and authenticated key management protocol sakmp to overcome the shortcomin... | [['public', 'key', 'infrastructure', 'pki', 'is', 'the', 'most', 'widely', 'used', 'security', 'mechanism', 'for', 'securing', 'communications', 'over', 'the', 'network', 'however', 'there', 'are', 'known', 'performance', 'issues', 'making', 'it', 'unsuitable', 'for', 'use', 'in', 'vehicular', 'networks', 'in', 'this',... | [-0.22088797284245337, -0.04912162172695389, -0.05054138297078396, 0.04362618461264075, -0.03826300279822611, -0.2591664017639507, 0.11835083749557529, 0.37867693700015953, -0.2612002409183967, -0.2827438833277433, 0.13146166432512188, -0.260775674420725, -0.14194245541381753, 0.24776719486631385, -0.16335651938965834,... |
1,712.0986 | The cyclic-homology Chern-Weil homomorphism for principal coactions | We view the space of cotraces in the structural coalgebra of a principal
coaction as a noncommutative counterpart of the classical Cartan model. Then we
define the cyclic-homology Chern-Weil homomorphism by extending the
Chern-Galois character from the characters of finite-dimensional comodules to
arbitrary cotraces.... | math.KT math.QA | we view the space of cotraces in the structural coalgebra of a principal coaction as a noncommutative counterpart of the classical cartan model then we define the cyclichomology chernweil homomorphism by extending the cherngalois character from the characters of finitedimensional comodules to arbitrary cotraces to redu... | [['we', 'view', 'the', 'space', 'of', 'cotraces', 'in', 'the', 'structural', 'coalgebra', 'of', 'a', 'principal', 'coaction', 'as', 'a', 'noncommutative', 'counterpart', 'of', 'the', 'classical', 'cartan', 'model', 'then', 'we', 'define', 'the', 'cyclichomology', 'chernweil', 'homomorphism', 'by', 'extending', 'the', '... | [-0.1507563056158168, 0.05000409766669217, -0.07865889270265564, 0.08957326146059849, -0.15082026366927043, -0.14569896588321118, -0.004937289763993325, 0.3352737760625216, -0.4625280580225111, -0.1615053913282121, 0.1107349858106654, -0.20029705996659855, -0.1684677331168361, 0.1206928145809553, -0.18441044948721194, ... |
1,712.09861 | Variations of the Primitive Normal Basis Theorem | The celebrated Primitive Normal Basis Theorem states that for any $n\ge 2$
and any finite field $\mathbb F_q$, there exists an element $\alpha\in \mathbb
F_{q^n}$ that is simultaneously primitive and normal over $\mathbb F_q$. In
this paper, we prove some variations of this result, completing the proof of a
conjectur... | math.NT | the celebrated primitive normal basis theorem states that for any nge 2 and any finite field mathbb f_q there exists an element alphain mathbb f_qn that is simultaneously primitive and normal over mathbb f_q in this paper we prove some variations of this result completing the proof of a conjecture proposed by anderson ... | [['the', 'celebrated', 'primitive', 'normal', 'basis', 'theorem', 'states', 'that', 'for', 'any', 'nge', '2', 'and', 'any', 'finite', 'field', 'mathbb', 'f_q', 'there', 'exists', 'an', 'element', 'alphain', 'mathbb', 'f_qn', 'that', 'is', 'simultaneously', 'primitive', 'and', 'normal', 'over', 'mathbb', 'f_q', 'in', 't... | [-0.21124717414185598, 0.09769834739676912, -0.05007665667247463, -0.07131289631013407, 0.009094399315389719, -0.13602992124226573, -0.01812172481372904, 0.29334179401494465, -0.29753041291585214, -0.1400375540501305, 0.0669556289363967, -0.26338912260887976, -0.1455265712234881, 0.206998799721916, -0.15392856626444823... |
1,712.09862 | A non-biased trust model for wireless mesh networks | Trust models that rely on recommendation trusts are vulnerable to badmouthing
and ballot-stuffing attacks. To cope with these attacks, existing trust models
use different trust aggregation techniques to process the recommendation trusts
and combine them with the direct trust values to form a combined trust value.
How... | cs.CR | trust models that rely on recommendation trusts are vulnerable to badmouthing and ballotstuffing attacks to cope with these attacks existing trust models use different trust aggregation techniques to process the recommendation trusts and combine them with the direct trust values to form a combined trust value however t... | [['trust', 'models', 'that', 'rely', 'on', 'recommendation', 'trusts', 'are', 'vulnerable', 'to', 'badmouthing', 'and', 'ballotstuffing', 'attacks', 'to', 'cope', 'with', 'these', 'attacks', 'existing', 'trust', 'models', 'use', 'different', 'trust', 'aggregation', 'techniques', 'to', 'process', 'the', 'recommendation'... | [-0.08364369543776728, -0.03698895243765153, -0.06116893737314221, 0.1092864654072167, -0.11800837589380068, -0.25994890589171493, 0.09996283314823627, 0.42906030914149224, -0.22180970774915737, -0.27878061472318877, 0.0841722876054402, -0.3295588416548876, -0.1966648077365393, 0.11601749891594339, -0.13929503565558637... |
1,712.09863 | Functional Renormalization Analytically Continued | We discuss a method to analytically continue functional renormalization group
equations from imaginary Matsubara frequencies to the real frequency axis. In
this formalism, we investigate the analytic structure of the flowing action and
the propagator for a theory of scalar fields with $O(N)$ symmetry. We go on to
sho... | hep-th | we discuss a method to analytically continue functional renormalization group equations from imaginary matsubara frequencies to the real frequency axis in this formalism we investigate the analytic structure of the flowing action and the propagator for a theory of scalar fields with on symmetry we go on to show how it ... | [['we', 'discuss', 'a', 'method', 'to', 'analytically', 'continue', 'functional', 'renormalization', 'group', 'equations', 'from', 'imaginary', 'matsubara', 'frequencies', 'to', 'the', 'real', 'frequency', 'axis', 'in', 'this', 'formalism', 'we', 'investigate', 'the', 'analytic', 'structure', 'of', 'the', 'flowing', 'a... | [-0.12817706660049535, 0.10600160355498679, -0.14761543180083675, 0.06632042856938092, -0.13490084177110254, -0.052166347394742796, 0.02784012685524209, 0.39869005051327916, -0.24550873246441438, -0.2313744069485948, 0.05835425961058496, -0.2589738493736992, -0.1690595411559249, 0.16126074365811513, 0.02162618299650891... |
1,712.09864 | TEDS: A Trusted Entropy and Dempster Shafer Mechanism for Routing in
Wireless Mesh Networks | Wireless Mesh Networks (WMNs) have emerged as a key technology for the next
generation of wireless networking due to its self-forming, self-organizing and
self-healing properties. However, due to the multi-hop nature of communications
in WMN, we cannot assume that all nodes in the network are cooperative. Nodes
may d... | cs.CR | wireless mesh networks wmns have emerged as a key technology for the next generation of wireless networking due to its selfforming selforganizing and selfhealing properties however due to the multihop nature of communications in wmn we cannot assume that all nodes in the network are cooperative nodes may drop all of th... | [['wireless', 'mesh', 'networks', 'wmns', 'have', 'emerged', 'as', 'a', 'key', 'technology', 'for', 'the', 'next', 'generation', 'of', 'wireless', 'networking', 'due', 'to', 'its', 'selfforming', 'selforganizing', 'and', 'selfhealing', 'properties', 'however', 'due', 'to', 'the', 'multihop', 'nature', 'of', 'communicat... | [-0.2101011346597728, 0.007131325985883941, -0.06420422078840234, 0.03808933043399373, -0.09228369312209858, -0.22143252018486728, 0.1250429401438482, 0.39309032559143126, -0.25053511353184443, -0.28633580723827756, 0.07142981093729267, -0.2924672049822638, -0.21212165705054192, 0.11110597483914446, -0.1619110188799331... |
1,712.09865 | The physicist's guide to one of biotechnology's hottest new topics:
CRISPR-Cas | Clustered regularly interspaced short palindromic repeats (CRISPR) and
CRISPR-associated proteins (Cas) constitute a multi-functional, constantly
evolving immune system in bacteria and archaea cells. A heritable, molecular
memory is generated of phage, plasmids, or other mobile genetic elements that
attempt to attack... | q-bio.PE | clustered regularly interspaced short palindromic repeats crispr and crisprassociated proteins cas constitute a multifunctional constantly evolving immune system in bacteria and archaea cells a heritable molecular memory is generated of phage plasmids or other mobile genetic elements that attempt to attack the cell thi... | [['clustered', 'regularly', 'interspaced', 'short', 'palindromic', 'repeats', 'crispr', 'and', 'crisprassociated', 'proteins', 'cas', 'constitute', 'a', 'multifunctional', 'constantly', 'evolving', 'immune', 'system', 'in', 'bacteria', 'and', 'archaea', 'cells', 'a', 'heritable', 'molecular', 'memory', 'is', 'generated... | [-0.09325884203281021, 0.15171618952590507, -0.008219466726950486, 0.06433120601686823, -0.09440495373492012, -0.21047734229650814, 0.07719540846464952, 0.4032708097714931, -0.28997300217743033, -0.26114481437543874, 0.07416523148494888, -0.25129061422485394, -0.26134598676435417, 0.17234391670062904, -0.13662072668666... |
1,712.09866 | Magnetospheric Multiscale Dayside Reconnection Electron Diffusion Region
Events | We have used the high-resolution data of the Magnetospheric Multiscale (MMS)
mission dayside phase to identify twenty-one previously unreported encounters
with the electron diffusion region (EDR), as evidenced by electron agyrotropy,
ion jet reversals, and j dot E greater than 0. Three of the new EDR encounters,
whic... | physics.space-ph | we have used the highresolution data of the magnetospheric multiscale mms mission dayside phase to identify twentyone previously unreported encounters with the electron diffusion region edr as evidenced by electron agyrotropy ion jet reversals and j dot e greater than 0 three of the new edr encounters which occurred wi... | [['we', 'have', 'used', 'the', 'highresolution', 'data', 'of', 'the', 'magnetospheric', 'multiscale', 'mms', 'mission', 'dayside', 'phase', 'to', 'identify', 'twentyone', 'previously', 'unreported', 'encounters', 'with', 'the', 'electron', 'diffusion', 'region', 'edr', 'as', 'evidenced', 'by', 'electron', 'agyrotropy',... | [-0.14623083170214346, 0.2125230457456602, 0.036196170166006375, 0.07019719818069053, -0.03158294055851754, -0.10559540137316732, 0.01756519029765315, 0.3573888199746437, -0.20983864845515326, -0.39466057102806096, 0.07473494179597681, -0.2905968344748962, -0.028726639640892202, 0.23129404283225022, -0.0001749409251945... |
1,712.09867 | Future Frame Prediction for Anomaly Detection -- A New Baseline | Anomaly detection in videos refers to the identification of events that do
not conform to expected behavior. However, almost all existing methods tackle
the problem by minimizing the reconstruction errors of training data, which
cannot guarantee a larger reconstruction error for an abnormal event. In this
paper, we p... | cs.CV | anomaly detection in videos refers to the identification of events that do not conform to expected behavior however almost all existing methods tackle the problem by minimizing the reconstruction errors of training data which cannot guarantee a larger reconstruction error for an abnormal event in this paper we propose ... | [['anomaly', 'detection', 'in', 'videos', 'refers', 'to', 'the', 'identification', 'of', 'events', 'that', 'do', 'not', 'conform', 'to', 'expected', 'behavior', 'however', 'almost', 'all', 'existing', 'methods', 'tackle', 'the', 'problem', 'by', 'minimizing', 'the', 'reconstruction', 'errors', 'of', 'training', 'data',... | [-0.07437376216565648, 0.022014704239581778, -0.06282296422559527, 0.10888548626531955, -0.11219572750201752, -0.08683842587782893, 0.05191505320835858, 0.4077946936495082, -0.23888493830955393, -0.36497781695798037, 0.1113332616203183, -0.2972071462787341, -0.1352879059392699, 0.16085977257272704, -0.13877637322537253... |
1,712.09868 | Aspects of electron scattering, the elastic, and the inelastic | A electron of mass $m$, when electrically scatters of nucleus, of mass $M$,
transfers momentum $q$ to the nucleus. The energy lost by electron is more than
the energy gained by the nucleus. The resulting energy goes in exciting the
atom to a higher energy state as in Frank Hertz experiment and sodium, neon,
mercury v... | quant-ph cond-mat.mes-hall | a electron of mass m when electrically scatters of nucleus of mass m transfers momentum q to the nucleus the energy lost by electron is more than the energy gained by the nucleus the resulting energy goes in exciting the atom to a higher energy state as in frank hertz experiment and sodium neon mercury vapor lamps or i... | [['a', 'electron', 'of', 'mass', 'm', 'when', 'electrically', 'scatters', 'of', 'nucleus', 'of', 'mass', 'm', 'transfers', 'momentum', 'q', 'to', 'the', 'nucleus', 'the', 'energy', 'lost', 'by', 'electron', 'is', 'more', 'than', 'the', 'energy', 'gained', 'by', 'the', 'nucleus', 'the', 'resulting', 'energy', 'goes', 'i... | [-0.06847246044417532, 0.25419739841874756, -0.07326193363578873, 0.11233222794019683, -0.013806152988405254, -0.11167753766075324, 0.067982580921514, 0.38655784168041774, -0.2572827933366552, -0.3087564351632854, -0.03749122446771628, -0.39181605830778227, -0.04418051464926299, 0.17257418575026717, 0.03285838138886821... |
1,712.09869 | Tensor network states in time-bin quantum optics | The current shift in the quantum optics community towards large-size
experiments -- with many modes and photons -- necessitates new classical
simulation techniques that go beyond the usual phase space formulation of
quantum mechanics. To address this pressing demand we formulate linear quantum
optics in the language ... | quant-ph | the current shift in the quantum optics community towards largesize experiments with many modes and photons necessitates new classical simulation techniques that go beyond the usual phase space formulation of quantum mechanics to address this pressing demand we formulate linear quantum optics in the language of tensor ... | [['the', 'current', 'shift', 'in', 'the', 'quantum', 'optics', 'community', 'towards', 'largesize', 'experiments', 'with', 'many', 'modes', 'and', 'photons', 'necessitates', 'new', 'classical', 'simulation', 'techniques', 'that', 'go', 'beyond', 'the', 'usual', 'phase', 'space', 'formulation', 'of', 'quantum', 'mechani... | [-0.10010539194924496, 0.15721978527063163, -0.07827220824096472, 0.07374120188466403, -0.05806230504306093, -0.23012430408108298, 0.04056012612186693, 0.3763449925288398, -0.2915223342396559, -0.26486795456699463, 0.03409817781654857, -0.25527884309450466, -0.18107386491191324, 0.22254309694843508, -0.0608745374439588... |
1,712.0987 | Indirect Inference for L\'evy-driven continuous-time GARCH models | We advocate the use of an Indirect Inference method to estimate the parameter
of a COGARCH(1,1) process for equally spaced observations. This requires that
the true model can be simulated and a reasonable estimation method for an
approximate auxiliary model. We follow previous approaches and use linear
projections le... | stat.ME | we advocate the use of an indirect inference method to estimate the parameter of a cogarch11 process for equally spaced observations this requires that the true model can be simulated and a reasonable estimation method for an approximate auxiliary model we follow previous approaches and use linear projections leading t... | [['we', 'advocate', 'the', 'use', 'of', 'an', 'indirect', 'inference', 'method', 'to', 'estimate', 'the', 'parameter', 'of', 'a', 'cogarch11', 'process', 'for', 'equally', 'spaced', 'observations', 'this', 'requires', 'that', 'the', 'true', 'model', 'can', 'be', 'simulated', 'and', 'a', 'reasonable', 'estimation', 'met... | [-0.043372351199831044, 0.03633841678963773, -0.14984050350171244, 0.10797113778315191, -0.08858206389135027, -0.12595554662485284, 0.08867363393156466, 0.3767493094271379, -0.25486475789377877, -0.29574050914565536, 0.11724312828378157, -0.2365972906060464, -0.10865021569791401, 0.20064092176497406, -0.086768501808087... |
1,712.09871 | Coherence orders, decoherence and quantum metrology | Since the dawn of quantum theory, coherence was attributed as a key to
understand the weirdness of fundamental concepts like the wave-particle duality
and the Stern-Gerlach experiment. Recently, based on a resource theory
approach, the notion of quantum coherence was revisited and a plethora of
coherence quantifiers ... | quant-ph | since the dawn of quantum theory coherence was attributed as a key to understand the weirdness of fundamental concepts like the waveparticle duality and the sterngerlach experiment recently based on a resource theory approach the notion of quantum coherence was revisited and a plethora of coherence quantifiers were pro... | [['since', 'the', 'dawn', 'of', 'quantum', 'theory', 'coherence', 'was', 'attributed', 'as', 'a', 'key', 'to', 'understand', 'the', 'weirdness', 'of', 'fundamental', 'concepts', 'like', 'the', 'waveparticle', 'duality', 'and', 'the', 'sterngerlach', 'experiment', 'recently', 'based', 'on', 'a', 'resource', 'theory', 'a... | [-0.10381753178924777, 0.1406939589482455, -0.11185317001668096, 0.09359039514830322, -0.04119855517393533, -0.1283254235812271, 0.07156820523549041, 0.3184109391068741, -0.2622300562349269, -0.2906383863323233, 0.06723113530155499, -0.22014243396724226, -0.17508594839627506, 0.1654310801940906, -0.07416769758378731, 0... |
1,712.09872 | Handwritten Bangla Character Recognition Using The State-of-Art Deep
Convolutional Neural Networks | In spite of advances in object recognition technology, Handwritten Bangla
Character Recognition (HBCR) remains largely unsolved due to the presence of
many ambiguous handwritten characters and excessively cursive Bangla
handwritings. Even the best existing recognizers do not lead to satisfactory
performance for pract... | cs.CV | in spite of advances in object recognition technology handwritten bangla character recognition hbcr remains largely unsolved due to the presence of many ambiguous handwritten characters and excessively cursive bangla handwritings even the best existing recognizers do not lead to satisfactory performance for practical a... | [['in', 'spite', 'of', 'advances', 'in', 'object', 'recognition', 'technology', 'handwritten', 'bangla', 'character', 'recognition', 'hbcr', 'remains', 'largely', 'unsolved', 'due', 'to', 'the', 'presence', 'of', 'many', 'ambiguous', 'handwritten', 'characters', 'and', 'excessively', 'cursive', 'bangla', 'handwritings'... | [-0.04409260150546638, -0.07695197711360142, -0.01627531550416844, 0.04665959326649559, -0.10865474347653385, -0.20438828186776775, -0.0104520516346082, 0.46166734510933505, -0.24594895280456755, -0.31694438041652107, 0.07961066103314418, -0.29282897543272324, -0.19456893208811402, 0.25432878302977857, -0.1808140942848... |
1,712.09873 | Higgs Portals for Thermal Dark Matter - EFT Perspectives and the NMSSM - | We analyze a low energy effective model of Dark Matter in which the thermal
relic density is provided by a singlet Majorana fermion which interacts with
the Higgs fields via higher dimensional operators. Direct detection signatures
may be reduced if blind spot solutions exist, which naturally appear in models
with ex... | hep-ph astro-ph.CO | we analyze a low energy effective model of dark matter in which the thermal relic density is provided by a singlet majorana fermion which interacts with the higgs fields via higher dimensional operators direct detection signatures may be reduced if blind spot solutions exist which naturally appear in models with extend... | [['we', 'analyze', 'a', 'low', 'energy', 'effective', 'model', 'of', 'dark', 'matter', 'in', 'which', 'the', 'thermal', 'relic', 'density', 'is', 'provided', 'by', 'a', 'singlet', 'majorana', 'fermion', 'which', 'interacts', 'with', 'the', 'higgs', 'fields', 'via', 'higher', 'dimensional', 'operators', 'direct', 'detec... | [-0.11556063457640077, 0.2676223623264512, -0.061009698240638954, 0.1554846571954453, -0.09386165503464225, -0.16505268830870692, 0.01865692982553608, 0.29649860259895733, -0.19202373678099657, -0.31360354299087906, 0.036652765913728486, -0.23720999784914223, -0.035637267013684054, 0.10242870803900857, 0.03419788230705... |
1,712.09874 | Two-dimensional simulation of quantum reflection | A propagation method for the scattering of a quantum wave packet from a
potential surface is presented. It is used to model the quantum reflection of
single atoms from a corrugated (metallic) surface. Our numerical procedure
works well in two spatial dimensions requiring only reasonable amounts of
memory and computin... | quant-ph | a propagation method for the scattering of a quantum wave packet from a potential surface is presented it is used to model the quantum reflection of single atoms from a corrugated metallic surface our numerical procedure works well in two spatial dimensions requiring only reasonable amounts of memory and computing time... | [['a', 'propagation', 'method', 'for', 'the', 'scattering', 'of', 'a', 'quantum', 'wave', 'packet', 'from', 'a', 'potential', 'surface', 'is', 'presented', 'it', 'is', 'used', 'to', 'model', 'the', 'quantum', 'reflection', 'of', 'single', 'atoms', 'from', 'a', 'corrugated', 'metallic', 'surface', 'our', 'numerical', 'p... | [-0.09970739682245514, 0.08808262318210758, -0.116904522226516, 0.04227967232050698, -0.027247344596696126, -0.14505442551782596, 0.07264015937866845, 0.40449537743773795, -0.23449750025959118, -0.30279775098998746, 0.05646735619318307, -0.28075035450899083, -0.16886841737078098, 0.2674889490792892, 0.01542329418715899... |
1,712.09875 | Ergodicity of the zigzag process | The zigzag process is a Piecewise Deterministic Markov Process which can be
used in a MCMC framework to sample from a given target distribution. We prove
the convergence of this process to its target under very weak assumptions, and
establish a central limit theorem for empirical averages under stronger
assumptions o... | math.PR | the zigzag process is a piecewise deterministic markov process which can be used in a mcmc framework to sample from a given target distribution we prove the convergence of this process to its target under very weak assumptions and establish a central limit theorem for empirical averages under stronger assumptions on th... | [['the', 'zigzag', 'process', 'is', 'a', 'piecewise', 'deterministic', 'markov', 'process', 'which', 'can', 'be', 'used', 'in', 'a', 'mcmc', 'framework', 'to', 'sample', 'from', 'a', 'given', 'target', 'distribution', 'we', 'prove', 'the', 'convergence', 'of', 'this', 'process', 'to', 'its', 'target', 'under', 'very', ... | [-0.06212383979460695, 0.06905042397492862, -0.14412375621415757, 0.12418567114754306, -0.03133504268403708, -0.11245862946712545, 0.1298094046312374, 0.39424614762314236, -0.32657271437346935, -0.2310321097170095, 0.12743795806526687, -0.20131673966278577, -0.0832454179423851, 0.20130927955915967, -0.07420488060605558... |
1,712.09876 | Reliable Messaging to Millions of Users with MigratoryData | Web-based notification services are used by a large range of businesses to
selectively distribute live updates to customers, following the
publish/subscribe (pub/sub) model. Typical deployments can involve millions of
subscribers expecting ordering and delivery guarantees together with low
latencies. Notification ser... | cs.DC cs.SE | webbased notification services are used by a large range of businesses to selectively distribute live updates to customers following the publishsubscribe pubsub model typical deployments can involve millions of subscribers expecting ordering and delivery guarantees together with low latencies notification services must... | [['webbased', 'notification', 'services', 'are', 'used', 'by', 'a', 'large', 'range', 'of', 'businesses', 'to', 'selectively', 'distribute', 'live', 'updates', 'to', 'customers', 'following', 'the', 'publishsubscribe', 'pubsub', 'model', 'typical', 'deployments', 'can', 'involve', 'millions', 'of', 'subscribers', 'expe... | [-0.23789449458860834, 0.03878543975398592, -0.0008591175646237705, 0.020391766945629015, -0.12413934887913258, -0.2308570421908213, 0.17709522779383088, 0.4239812282116517, -0.22599024370960566, -0.3527403827594674, 0.12610500149995738, -0.28989446257119594, -0.0919771022168393, 0.15510145072906237, -0.162513670552036... |
1,712.09877 | Liouville type results for a nonlocal obstacle problem | This paper is concerned with qualitative properties of solutions to nonlocal
reaction-diffusion equations of the form$$ \int\_{\mathbb{R}^N\setminus K}
J(x-y)\,\big( u(y)-u(x) \big)\,\D y+f(u(x))=0, \quad x\in\R^N\setminus K,$$set
in a perforated open set $\mathbb{R}^N\setminus K$, where
$K\subset\mathbb{R}^N$ is a b... | math.AP | this paper is concerned with qualitative properties of solutions to nonlocal reactiondiffusion equations of the form int_mathbbrnsetminus k jxybig uyux bigd yfux0 quad xinrnsetminus kset in a perforated open set mathbbrnsetminus k where ksubsetmathbbrn is a bounded compact obstacle and f is a bistable nonlinearity when... | [['this', 'paper', 'is', 'concerned', 'with', 'qualitative', 'properties', 'of', 'solutions', 'to', 'nonlocal', 'reactiondiffusion', 'equations', 'of', 'the', 'form', 'int_mathbbrnsetminus', 'k', 'jxybig', 'uyux', 'bigd', 'yfux0', 'quad', 'xinrnsetminus', 'kset', 'in', 'a', 'perforated', 'open', 'set', 'mathbbrnsetminu... | [-0.2284425739198923, 0.045964555741686904, -0.04263163967989385, -0.0011539568692179663, -0.1021996951662004, -0.20842435914756996, 0.014715305597720933, 0.32063280671302763, -0.2808761346553053, -0.1690187561458775, 0.12523496688310323, -0.3389724664390087, -0.12636425734630652, 0.16811967164810215, -0.09547761757192... |
1,712.09878 | Gauge invariant canonical cosmological perturbation theory with
geometrical clocks in extended phase space - a review and applications | The theory of cosmological perturbations is a well elaborated field. To deal
with the diffeomorphism invariance of general relativity one generally
introduces combinations of the metric and matter perturbations which are gauge
invariant up to the considered order in the perturbations. For linear
cosmological perturba... | gr-qc | the theory of cosmological perturbations is a well elaborated field to deal with the diffeomorphism invariance of general relativity one generally introduces combinations of the metric and matter perturbations which are gauge invariant up to the considered order in the perturbations for linear cosmological perturbation... | [['the', 'theory', 'of', 'cosmological', 'perturbations', 'is', 'a', 'well', 'elaborated', 'field', 'to', 'deal', 'with', 'the', 'diffeomorphism', 'invariance', 'of', 'general', 'relativity', 'one', 'generally', 'introduces', 'combinations', 'of', 'the', 'metric', 'and', 'matter', 'perturbations', 'which', 'are', 'gaug... | [-0.11212495589333267, 0.12205426109936672, -0.1153210077299032, 0.0954921981173729, -0.08749375390180995, -0.11753080880511689, -0.026941098236286414, 0.3027422584943831, -0.23294982993872182, -0.2877842763892454, 0.08690424357339864, -0.2341383402493552, -0.1679314032009703, 0.13775990858100134, -0.06807036640988559,... |
1,712.09879 | Emergence of Spatial Order in Highly Interacting Rydberg Gases | We describe the emergence of strong spatial correlations, akin to liquid-like
behavior and crystallization effects, in low (one and two) dimensional gases of
cold Rydberg atoms. The presence of an external electric field permanently
polarizes the atoms, which became highly correlated due to the long-range
dipole-dipo... | physics.atom-ph cond-mat.stat-mech physics.plasm-ph | we describe the emergence of strong spatial correlations akin to liquidlike behavior and crystallization effects in low one and two dimensional gases of cold rydberg atoms the presence of an external electric field permanently polarizes the atoms which became highly correlated due to the longrange dipoledipole interact... | [['we', 'describe', 'the', 'emergence', 'of', 'strong', 'spatial', 'correlations', 'akin', 'to', 'liquidlike', 'behavior', 'and', 'crystallization', 'effects', 'in', 'low', 'one', 'and', 'two', 'dimensional', 'gases', 'of', 'cold', 'rydberg', 'atoms', 'the', 'presence', 'of', 'an', 'external', 'electric', 'field', 'per... | [-0.15726582791818225, 0.24998240088752938, -0.03846978463192025, 0.06483632638827776, 0.009317502984777093, -0.17653459239265193, -0.0019346966064008682, 0.35986724781763296, -0.2527473199464705, -0.2774562986972539, -0.026654439821393917, -0.3013188737201626, -0.1331582694152451, 0.14869653825324192, 0.10118743627858... |
1,712.0988 | The Fourier transform on 2-step Lie groups | In this paper, we investigate the behavior of the Fourier transform on finite
dimensional 2-step Lie groups and develop a general theory akin to that of the
whole space or the torus. We provide a familiar framework in which computations
are made sensibly easier than with the usual representation-theoretic Fourier
tra... | math.CA | in this paper we investigate the behavior of the fourier transform on finite dimensional 2step lie groups and develop a general theory akin to that of the whole space or the torus we provide a familiar framework in which computations are made sensibly easier than with the usual representationtheoretic fourier transform... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'behavior', 'of', 'the', 'fourier', 'transform', 'on', 'finite', 'dimensional', '2step', 'lie', 'groups', 'and', 'develop', 'a', 'general', 'theory', 'akin', 'to', 'that', 'of', 'the', 'whole', 'space', 'or', 'the', 'torus', 'we', 'provide', 'a', 'familiar', 'framewo... | [-0.0954134328244254, 0.08449112821836025, -0.11263584589818493, 0.0931754015374463, -0.12373171672224999, -0.08314496410544962, 0.03329767229501158, 0.32853676479309796, -0.2826278092805296, -0.2259259600006044, 0.1214055710437242, -0.2308158226357773, -0.1907055762433447, 0.17938831630395724, -0.03445264001376927, -0... |
1,712.09881 | On the rate of convergence for the length of the longest common
subsequences in hidden Markov models | Let $(X, Y) = (X_n, Y_n)_{n \geq 1}$ be the output process generated by a
hidden chain $Z = (Z_n)_{n \geq 1}$, where $Z$ is a finite state, aperiodic,
time homogeneous, and irreducible Markov chain. Let $LC_n$ be the length of the
longest common subsequences of $X_1, \ldots, X_n$ and $Y_1, \ldots, Y_n$. Under
a mixin... | math.PR | let x y x_n y_n_n geq 1 be the output process generated by a hidden chain z z_n_n geq 1 where z is a finite state aperiodic time homogeneous and irreducible markov chain let lc_n be the length of the longest common subsequences of x_1 ldots x_n and y_1 ldots y_n under a mixing hypothesis a rate of convergence result is... | [['let', 'x', 'y', 'x_n', 'y_n_n', 'geq', '1', 'be', 'the', 'output', 'process', 'generated', 'by', 'a', 'hidden', 'chain', 'z', 'z_n_n', 'geq', '1', 'where', 'z', 'is', 'a', 'finite', 'state', 'aperiodic', 'time', 'homogeneous', 'and', 'irreducible', 'markov', 'chain', 'let', 'lc_n', 'be', 'the', 'length', 'of', 'the'... | [-0.24158960950398256, 0.29744273524672266, -0.05395146015854109, -0.02863676806745865, 0.034959493714961265, -0.21601139065173883, 0.0004807900459993453, 0.40306058070725864, -0.40631855196423, -0.0820680885087876, 0.09533038781955838, -0.30713718860513634, 0.02503694503730725, 0.13248317187563294, -0.0134431745945697... |
1,712.09882 | A survey of TiO{\lambda}567 nm absorption in solar-type stars | Molecular absorption bands are estimators of stellar activity and spot cycles
on magnetically active stars. We have previously introduced a new color index
that compare absorption strength of the titanium oxide (TiO) at 567 nm with
nearby continuum. In this paper we implement this index to measure long-term
activity ... | astro-ph.SR | molecular absorption bands are estimators of stellar activity and spot cycles on magnetically active stars we have previously introduced a new color index that compare absorption strength of the titanium oxide tio at 567 nm with nearby continuum in this paper we implement this index to measure longterm activity variati... | [['molecular', 'absorption', 'bands', 'are', 'estimators', 'of', 'stellar', 'activity', 'and', 'spot', 'cycles', 'on', 'magnetically', 'active', 'stars', 'we', 'have', 'previously', 'introduced', 'a', 'new', 'color', 'index', 'that', 'compare', 'absorption', 'strength', 'of', 'the', 'titanium', 'oxide', 'tio', 'at', '5... | [-0.05123759091467313, 0.13509556012476145, -0.06812478669250951, 0.0352801844330869, -0.04333480340226189, -0.05592800372118211, 0.1315582077659201, 0.45103488903006783, -0.17844612621094869, -0.409391056260337, 0.06742072030623525, -0.31121472128744126, -0.08134621593331837, 0.18766118786753277, -0.10212155101496888,... |
1,712.09883 | Thermal expansion of boron subnitrides | The lattice parameters of two boron subnitrides, B13N2 and B50N2, have been
measured as a function of temperature between 298 and 1273 K, and the
corresponding thermal expansion coefficients have been determined. Thermal
expansion of both boron subnitrides was found to be quasi-linear, and the
volume thermal expansio... | cond-mat.mtrl-sci | the lattice parameters of two boron subnitrides b13n2 and b50n2 have been measured as a function of temperature between 298 and 1273 k and the corresponding thermal expansion coefficients have been determined thermal expansion of both boron subnitrides was found to be quasilinear and the volume thermal expansion coeffi... | [['the', 'lattice', 'parameters', 'of', 'two', 'boron', 'subnitrides', 'b13n2', 'and', 'b50n2', 'have', 'been', 'measured', 'as', 'a', 'function', 'of', 'temperature', 'between', '298', 'and', '1273', 'k', 'and', 'the', 'corresponding', 'thermal', 'expansion', 'coefficients', 'have', 'been', 'determined', 'thermal', 'e... | [-0.10855922967656165, 0.17789709308029464, -0.0476381253771564, -0.07203266557346108, 0.006358136182590839, -0.08654925675301622, 0.05755583023632406, 0.40281381986794934, -0.20614213380281643, -0.33089562351264623, 0.0811028265762293, -0.374244566716414, -0.05825864840098607, 0.16402018248474085, 0.08893463902816337,... |
1,712.09884 | Regularity of push-forward of Monge-Amp{\`e}re measures | We prove that the image under any dominant meromorphic map of the
Monge-Amp{\`e}re measure of a H{\"o}lder continuous quasi-psh function still
possesses a H{\"o}lder potential. We also discuss the case of lower regularity.
| math.CV | we prove that the image under any dominant meromorphic map of the mongeampere measure of a holder continuous quasipsh function still possesses a holder potential we also discuss the case of lower regularity | [['we', 'prove', 'that', 'the', 'image', 'under', 'any', 'dominant', 'meromorphic', 'map', 'of', 'the', 'mongeampere', 'measure', 'of', 'a', 'holder', 'continuous', 'quasipsh', 'function', 'still', 'possesses', 'a', 'holder', 'potential', 'we', 'also', 'discuss', 'the', 'case', 'of', 'lower', 'regularity']] | [-0.17128554979960123, -0.031162533288200695, -0.13022340138471036, 0.13808423658889352, -0.0872648178289334, -0.14656590961032745, 0.02806636422985431, 0.3697057115760716, -0.3297086814418435, -0.08729016261570381, 0.14356062569740144, -0.24471461533032585, -0.16197281263091348, 0.2245560624552044, -0.1188458072755372... |
1,712.09885 | Models for a multimode bosonic tunneling junction | We discuss the relaxation dynamics for a bosonic tunneling junction with two
modes in the central potential well. We use a master equation description for
ultracold bosons tunneling in the presence of noise and incoherent coupling
processes into the two central modes. Whilst we cannot quantitatively reproduce
the exp... | cond-mat.quant-gas quant-ph | we discuss the relaxation dynamics for a bosonic tunneling junction with two modes in the central potential well we use a master equation description for ultracold bosons tunneling in the presence of noise and incoherent coupling processes into the two central modes whilst we cannot quantitatively reproduce the experim... | [['we', 'discuss', 'the', 'relaxation', 'dynamics', 'for', 'a', 'bosonic', 'tunneling', 'junction', 'with', 'two', 'modes', 'in', 'the', 'central', 'potential', 'well', 'we', 'use', 'a', 'master', 'equation', 'description', 'for', 'ultracold', 'bosons', 'tunneling', 'in', 'the', 'presence', 'of', 'noise', 'and', 'incoh... | [-0.1683718605861798, 0.14969245555774108, -0.052867011924949935, 0.017194681566448423, 0.024223312388594244, -0.13912491884319952, 0.08168820740527236, 0.33990255413650006, -0.17479685454528926, -0.28355507775410715, -0.04871083568557914, -0.30208637864401966, -0.11340585082072328, 0.19207408798255904, -0.021127521836... |
1,712.09886 | Quasar -- CIV forest cross-correlation with SDSS DR12 | We present a new determination of the large-scale clustering of the CIV
forest (i.e., the absorption due to all CIV absorbers) using its
cross-correlation with quasars in the Sloan Digital Sky Survey (SDSS) Data
Release 12 (DR12). We fit a linear bias model to the measured
cross-correlation. We find that the transmis... | astro-ph.CO | we present a new determination of the largescale clustering of the civ forest ie the absorption due to all civ absorbers using its crosscorrelation with quasars in the sloan digital sky survey sdss data release 12 dr12 we fit a linear bias model to the measured crosscorrelation we find that the transmission bias of the... | [['we', 'present', 'a', 'new', 'determination', 'of', 'the', 'largescale', 'clustering', 'of', 'the', 'civ', 'forest', 'ie', 'the', 'absorption', 'due', 'to', 'all', 'civ', 'absorbers', 'using', 'its', 'crosscorrelation', 'with', 'quasars', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'data', 'release', '1... | [-0.05652411602069299, 0.06158320351915304, 0.023858793240127175, 0.06739234599815465, -0.0921823579969621, -0.12133434753605099, 0.07305192875264342, 0.4292691296616266, -0.18688156881564577, -0.31880388592781367, 0.04124933405519398, -0.3753672959291116, -0.0038448120705610097, 0.1788756835198593, 0.00476973645529861... |
1,712.09887 | On the positivity of the logarithmic cotangent bundle | The aim of this work is to construct examples of pairs whose logarithmic
cotangent bundles have strong positivity properties. These examples are
constructed from any smooth n-dimensional complex projective varieties by
considering the sum of at least n general sufficiently ample hypersurfaces.
| math.AG math.CV | the aim of this work is to construct examples of pairs whose logarithmic cotangent bundles have strong positivity properties these examples are constructed from any smooth ndimensional complex projective varieties by considering the sum of at least n general sufficiently ample hypersurfaces | [['the', 'aim', 'of', 'this', 'work', 'is', 'to', 'construct', 'examples', 'of', 'pairs', 'whose', 'logarithmic', 'cotangent', 'bundles', 'have', 'strong', 'positivity', 'properties', 'these', 'examples', 'are', 'constructed', 'from', 'any', 'smooth', 'ndimensional', 'complex', 'projective', 'varieties', 'by', 'conside... | [-0.19988776166878996, 0.04591459749194439, -0.013799472456975352, 0.053615356352002846, -0.08309817578022678, -0.18044965962568918, -0.06973928621612556, 0.3436664302079451, -0.26188518447313636, -0.21255007945001125, 0.10036599275744743, -0.28590491478375735, -0.1713279511036706, 0.1786958517595416, -0.10713876606453... |
1,712.09888 | Improved Inception-Residual Convolutional Neural Network for Object
Recognition | Machine learning and computer vision have driven many of the greatest
advances in the modeling of Deep Convolutional Neural Networks (DCNNs).
Nowadays, most of the research has been focused on improving recognition
accuracy with better DCNN models and learning approaches. The recurrent
convolutional approach is not a... | cs.CV | machine learning and computer vision have driven many of the greatest advances in the modeling of deep convolutional neural networks dcnns nowadays most of the research has been focused on improving recognition accuracy with better dcnn models and learning approaches the recurrent convolutional approach is not applied ... | [['machine', 'learning', 'and', 'computer', 'vision', 'have', 'driven', 'many', 'of', 'the', 'greatest', 'advances', 'in', 'the', 'modeling', 'of', 'deep', 'convolutional', 'neural', 'networks', 'dcnns', 'nowadays', 'most', 'of', 'the', 'research', 'has', 'been', 'focused', 'on', 'improving', 'recognition', 'accuracy',... | [-0.026394164281390232, -0.0713081096539914, -0.03220668166150378, 0.022556085895538387, -0.03896902514707916, -0.20851128715972334, -0.04148138503761581, 0.4619851793489746, -0.21546344010565704, -0.31297814823205233, 0.0695461335094847, -0.29496501969590666, -0.2377328927220568, 0.21589240782020405, -0.13658367755056... |
1,712.09889 | The Heavy Quark Form Factors at Two Loops | We compute the two-loop QCD corrections to the heavy quark form factors in
case of the vector, axial-vector, scalar and pseudo-scalar currents up to
second order in the dimensional parameter $\epsilon = (4-D)/2$. These terms are
required in the renormalization of the higher order corrections to these form
factors.
| hep-ph | we compute the twoloop qcd corrections to the heavy quark form factors in case of the vector axialvector scalar and pseudoscalar currents up to second order in the dimensional parameter epsilon 4d2 these terms are required in the renormalization of the higher order corrections to these form factors | [['we', 'compute', 'the', 'twoloop', 'qcd', 'corrections', 'to', 'the', 'heavy', 'quark', 'form', 'factors', 'in', 'case', 'of', 'the', 'vector', 'axialvector', 'scalar', 'and', 'pseudoscalar', 'currents', 'up', 'to', 'second', 'order', 'in', 'the', 'dimensional', 'parameter', 'epsilon', '4d2', 'these', 'terms', 'are',... | [-0.1289880359157299, 0.24154093331405116, 0.011870193139960369, 0.09985595988109708, -0.06019296797846133, -0.03227020241320133, 0.05265556284090659, 0.29968604470680776, -0.18180232491188994, -0.23621231189463288, -0.0024950855295173824, -0.3271398760455971, -0.07155247502184163, 0.06852966589697947, 0.09385984534552... |
1,712.0989 | Hamiltonian ratchets with ultra-cold atoms | Quantum-resonance ratchets have been realized over the last ten years for the
production of directed currents of atoms. These non-dissipative systems are
based on the interaction of a Bose-Einstein condensate with an optical standing
wave potential to produce a current of atoms in momentum space. In this paper
we pro... | quant-ph cond-mat.quant-gas | quantumresonance ratchets have been realized over the last ten years for the production of directed currents of atoms these nondissipative systems are based on the interaction of a boseeinstein condensate with an optical standing wave potential to produce a current of atoms in momentum space in this paper we provide a ... | [['quantumresonance', 'ratchets', 'have', 'been', 'realized', 'over', 'the', 'last', 'ten', 'years', 'for', 'the', 'production', 'of', 'directed', 'currents', 'of', 'atoms', 'these', 'nondissipative', 'systems', 'are', 'based', 'on', 'the', 'interaction', 'of', 'a', 'boseeinstein', 'condensate', 'with', 'an', 'optical'... | [-0.15576459812554752, 0.17538297922874335, -0.0887301631005747, 0.026172883093490133, -0.02338018796761476, -0.11834136377133074, 0.024871704420296563, 0.42841848904887836, -0.23386266935794126, -0.24204699782033762, 0.08407113030552864, -0.24794598211135183, -0.14418863192466752, 0.23348721572242323, -0.0135168462925... |
1,712.09891 | Fractional Sturm-Liouville eigenvalue problems, I | We introduce and present the general solution of three two-term fractional
differential equations of mixed Caputo/Riemann Liouville type. We then solve a
Dirichlet type Sturm-Liouville eigenvalue problem for a fractional differential
equation derived from a special composition of a Caputo and a Riemann-Liouville
oper... | math.CA | we introduce and present the general solution of three twoterm fractional differential equations of mixed caputoriemann liouville type we then solve a dirichlet type sturmliouville eigenvalue problem for a fractional differential equation derived from a special composition of a caputo and a riemannliouville operator on... | [['we', 'introduce', 'and', 'present', 'the', 'general', 'solution', 'of', 'three', 'twoterm', 'fractional', 'differential', 'equations', 'of', 'mixed', 'caputoriemann', 'liouville', 'type', 'we', 'then', 'solve', 'a', 'dirichlet', 'type', 'sturmliouville', 'eigenvalue', 'problem', 'for', 'a', 'fractional', 'differenti... | [-0.14269985262287296, 0.09182715800405411, -0.055901316805156295, 0.08213543175736925, -0.13854409215143984, -0.1546770606569394, -0.015859007523222654, 0.3110819095538722, -0.3007148440237398, -0.24309527594596148, 0.17062102844248767, -0.3369476377360385, -0.14706596098840236, 0.1833011617815053, -0.0577797143047468... |
1,712.09892 | A Specification Format and a Verification Method of Fault-Tolerant
Quantum Circuits | Quantum computations are expressed in general as quantum circuits, which are
specified by ordered lists of quantum gates. The resulting specifications are
used during the optimisation and execution of the expressed computations.
However, the specification format makes it difficult to verify that optimised
or executed... | quant-ph | quantum computations are expressed in general as quantum circuits which are specified by ordered lists of quantum gates the resulting specifications are used during the optimisation and execution of the expressed computations however the specification format makes it difficult to verify that optimised or executed compu... | [['quantum', 'computations', 'are', 'expressed', 'in', 'general', 'as', 'quantum', 'circuits', 'which', 'are', 'specified', 'by', 'ordered', 'lists', 'of', 'quantum', 'gates', 'the', 'resulting', 'specifications', 'are', 'used', 'during', 'the', 'optimisation', 'and', 'execution', 'of', 'the', 'expressed', 'computation... | [-0.17823000348021165, 0.09323900041285182, -0.0045502713570992155, 0.06608883432667464, -0.036403076337643815, -0.24398119423987594, 0.05342856483989732, 0.40183990369451805, -0.2447757060732032, -0.35390970406802835, 0.10463006950416173, -0.18305497341601473, -0.10653642507217137, 0.2483423450426694, -0.0699860243298... |
1,712.09893 | On the possibility of superluminal energy propagation in a hyperbolic
metamaterial of metal-dielectric layers | The energy propagation of electromagnetic fields in the effective medium of a
one-dimensional photonic crystal consisting of dielectric and metallic layers
is investigated. We show that the medium behaves like Drude and Lorentz medium,
respectively, when the electric field is parallel and perpendicular to the
layers.... | physics.optics physics.class-ph | the energy propagation of electromagnetic fields in the effective medium of a onedimensional photonic crystal consisting of dielectric and metallic layers is investigated we show that the medium behaves like drude and lorentz medium respectively when the electric field is parallel and perpendicular to the layers for ar... | [['the', 'energy', 'propagation', 'of', 'electromagnetic', 'fields', 'in', 'the', 'effective', 'medium', 'of', 'a', 'onedimensional', 'photonic', 'crystal', 'consisting', 'of', 'dielectric', 'and', 'metallic', 'layers', 'is', 'investigated', 'we', 'show', 'that', 'the', 'medium', 'behaves', 'like', 'drude', 'and', 'lor... | [-0.2326843713804749, 0.22469406462563524, -0.06358284490375683, 0.0038935876258745276, -0.11745961789234445, -0.10396402017924512, -0.0006968891078215138, 0.43333285534983784, -0.2540495635487433, -0.2297595380507226, 0.02055737545904176, -0.25834334435014816, -0.12690965864311884, 0.17276166918632468, 0.0525644311837... |
1,712.09894 | Fractional Sturm-Liouville eigenvalue problems, II | We continue the study of a non self-adjoint fractional three-term
Sturm-Liouville boundary value problem (with a potential term) formed by the
composition of a left Caputo and left-Riemann-Liouville fractional integral
under {\it Dirichlet type} boundary conditions. We study the existence and
asymptotic behavior of t... | math.CA | we continue the study of a non selfadjoint fractional threeterm sturmliouville boundary value problem with a potential term formed by the composition of a left caputo and leftriemannliouville fractional integral under it dirichlet type boundary conditions we study the existence and asymptotic behavior of the real eigen... | [['we', 'continue', 'the', 'study', 'of', 'a', 'non', 'selfadjoint', 'fractional', 'threeterm', 'sturmliouville', 'boundary', 'value', 'problem', 'with', 'a', 'potential', 'term', 'formed', 'by', 'the', 'composition', 'of', 'a', 'left', 'caputo', 'and', 'leftriemannliouville', 'fractional', 'integral', 'under', 'it', '... | [-0.1487850264172282, 0.11110764844220523, -0.0500272923075643, 0.051832043031728905, -0.09107373076033566, -0.10896061750929475, 0.020249587271297186, 0.3276990870128206, -0.3004413943067847, -0.22214681448480278, 0.17935127487994337, -0.321243687875961, -0.15194645229923098, 0.1681115584317268, -0.025751189724950677,... |
1,712.09895 | Asymmetric many-body loss in a bosonic double well | A Bose gas in a double well is investigated in the presence of
single-particle, two-body and three-body asymmetric loss. The loss induces an
interesting decay behavior of the total population as well as a possibility to
control the dynamics of the system. In the noninteracting limit with asymmetric
single-body dissip... | cond-mat.quant-gas | a bose gas in a double well is investigated in the presence of singleparticle twobody and threebody asymmetric loss the loss induces an interesting decay behavior of the total population as well as a possibility to control the dynamics of the system in the noninteracting limit with asymmetric singlebody dissipation the... | [['a', 'bose', 'gas', 'in', 'a', 'double', 'well', 'is', 'investigated', 'in', 'the', 'presence', 'of', 'singleparticle', 'twobody', 'and', 'threebody', 'asymmetric', 'loss', 'the', 'loss', 'induces', 'an', 'interesting', 'decay', 'behavior', 'of', 'the', 'total', 'population', 'as', 'well', 'as', 'a', 'possibility', '... | [-0.11429909787026797, 0.11762273155697282, -0.1123148215895829, 0.14373317103430358, 0.012137269630329683, -0.1116845056336994, 0.052388949974556454, 0.3221669335228701, -0.26150478133543703, -0.2810585622695119, 0.019827494949519558, -0.287759652777216, -0.13337486104380028, 0.1389597765325258, 0.03208911258358663, 0... |
1,712.09896 | Scalaron from $R^2$-gravity as a Heavy Field | We study a model of inflation in which a scalar field $\chi$ is non-minimally
coupled to Starobinsky's $R^2$ gravity. After transforming it to the Einstein
frame, a new scalar field, the scalaron $\phi$, will appear and couple to
$\chi$ with a nontrivial field metric, while $\chi$ acquires a positive mass
via the non... | astro-ph.CO gr-qc hep-th | we study a model of inflation in which a scalar field chi is nonminimally coupled to starobinskys r2 gravity after transforming it to the einstein frame a new scalar field the scalaron phi will appear and couple to chi with a nontrivial field metric while chi acquires a positive mass via the nonminimal coupling initial... | [['we', 'study', 'a', 'model', 'of', 'inflation', 'in', 'which', 'a', 'scalar', 'field', 'chi', 'is', 'nonminimally', 'coupled', 'to', 'starobinskys', 'r2', 'gravity', 'after', 'transforming', 'it', 'to', 'the', 'einstein', 'frame', 'a', 'new', 'scalar', 'field', 'the', 'scalaron', 'phi', 'will', 'appear', 'and', 'coup... | [-0.19930670077248694, 0.2341480846090293, -0.07373508220344059, 0.05560996523188883, -0.08745567734164998, -0.15690527616336228, 0.0003911303665905081, 0.25399805627084593, -0.26562053322831686, -0.30475343615212974, 0.07309500674068174, -0.2797459522708062, -0.10843772800797795, 0.1344169265407316, 0.0335276291471598... |
1,712.09897 | Phi-entropies for Fokker-Planck and kinetic Fokker-Planck equations | This paper is devoted to $\phi$-entropies applied to Fokker-Planck and
kinetic Fokker-Planck equations in the whole space, with confinement. The
so-called $\phi$-entropies are Lyapunov functionals which typically interpolate
between Gibbs entropies and L2 estimates. We review some of their properties in
the case of d... | math.AP | this paper is devoted to phientropies applied to fokkerplanck and kinetic fokkerplanck equations in the whole space with confinement the socalled phientropies are lyapunov functionals which typically interpolate between gibbs entropies and l2 estimates we review some of their properties in the case of diffusion equatio... | [['this', 'paper', 'is', 'devoted', 'to', 'phientropies', 'applied', 'to', 'fokkerplanck', 'and', 'kinetic', 'fokkerplanck', 'equations', 'in', 'the', 'whole', 'space', 'with', 'confinement', 'the', 'socalled', 'phientropies', 'are', 'lyapunov', 'functionals', 'which', 'typically', 'interpolate', 'between', 'gibbs', 'e... | [-0.06699109288318524, 0.1018919705824565, -0.10966388226094606, 0.11810414904249276, -0.06539829118471396, -0.14428813017316555, 0.034494957921560855, 0.32545210688718057, -0.2794312705163305, -0.23755936562818916, 0.09731998349245834, -0.273846312955414, -0.08983472060461185, 0.2306637294884575, -0.05332401933050469,... |
1,712.09898 | SU(2$|$1) supersymmetric mechanics on curved spaces | We present SU$(2|1)$ supersymmetric mechanics on $n$-dimensional Riemannian
manifolds within the Hamiltonian approach. The structure functions including
prepotentials entering the supercharges and the Hamiltonian obey extended
curved WDVV equations specified by the manifold's metric and curvature tensor.
We consider ... | hep-th math-ph math.MP | we present su21 supersymmetric mechanics on ndimensional riemannian manifolds within the hamiltonian approach the structure functions including prepotentials entering the supercharges and the hamiltonian obey extended curved wdvv equations specified by the manifolds metric and curvature tensor we consider the most gene... | [['we', 'present', 'su21', 'supersymmetric', 'mechanics', 'on', 'ndimensional', 'riemannian', 'manifolds', 'within', 'the', 'hamiltonian', 'approach', 'the', 'structure', 'functions', 'including', 'prepotentials', 'entering', 'the', 'supercharges', 'and', 'the', 'hamiltonian', 'obey', 'extended', 'curved', 'wdvv', 'equ... | [-0.152334879891461, 0.10600801895349793, -0.0014723865144491276, 0.13066547192410444, -0.1442832558962476, -0.2176729212919979, -0.12795019337310173, 0.35229013315604435, -0.1794153682890085, -0.25126555187465704, 0.06926195581099423, -0.28808990739407425, -0.19182060899860834, 0.12040800455977897, -0.0595078358411505... |
1,712.09899 | Entanglement Spreading and Oscillation | We study dynamics of quantum entanglement in smooth global quenches with a
finite rate, by computing the time evolution of entanglement entropy in 1 + 1
dimensional free scalar theory with time-dependent masses which start from a
nonzero value at early time and either crosses or approaches zero. The
time-dependence i... | hep-th cond-mat.stat-mech quant-ph | we study dynamics of quantum entanglement in smooth global quenches with a finite rate by computing the time evolution of entanglement entropy in 1 1 dimensional free scalar theory with timedependent masses which start from a nonzero value at early time and either crosses or approaches zero the timedependence is chosen... | [['we', 'study', 'dynamics', 'of', 'quantum', 'entanglement', 'in', 'smooth', 'global', 'quenches', 'with', 'a', 'finite', 'rate', 'by', 'computing', 'the', 'time', 'evolution', 'of', 'entanglement', 'entropy', 'in', '1', '1', 'dimensional', 'free', 'scalar', 'theory', 'with', 'timedependent', 'masses', 'which', 'start... | [-0.17940767285260326, 0.2548015797455644, -0.1183653253343101, 0.08368494191423999, 0.041217245577463826, -0.15781042533497172, 0.029165984103704794, 0.30698837536992957, -0.29447970354875314, -0.2257676672131655, 0.10901588431753906, -0.2886089518557764, -0.057530290380491, 0.1616437850843265, 0.03234715071208413, 0.... |
1,712.099 | Measure contraction properties for two-step analytic sub-Riemannian
structures and Lipschitz Carnot groups | We prove that two-step analytic sub-Riemannian structures on a compact
analytic manifold equipped with a smooth measure and Lipschitz Carnot groups
satisfy measure contraction properties.
| math.DG | we prove that twostep analytic subriemannian structures on a compact analytic manifold equipped with a smooth measure and lipschitz carnot groups satisfy measure contraction properties | [['we', 'prove', 'that', 'twostep', 'analytic', 'subriemannian', 'structures', 'on', 'a', 'compact', 'analytic', 'manifold', 'equipped', 'with', 'a', 'smooth', 'measure', 'and', 'lipschitz', 'carnot', 'groups', 'satisfy', 'measure', 'contraction', 'properties']] | [-0.15213921681046486, 0.009347417913377285, -0.15289813913404943, 0.137497265227139, -0.21542791798710823, -0.1429984387382865, 0.012119141593575477, 0.5121090996265412, -0.280084669739008, -0.08374131405726075, 0.10319958148524165, -0.23217956811189652, -0.14262406732887029, 0.2773634622246027, -0.1562512688525021, 0... |
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