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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1,712.10101 | A variant of the plane wave least squares method for the time-harmonic
Maxwell's equations | In this paper we are concerned with the plane wave method for the
discretization of time-harmonic Maxwell's equations in three dimensions. As
pointed out in [6], it is difficult to derive a satisfactory L2 error estimate
of the standard plane wave approximation of the time-harmonic Maxwell's
equations. We propose a v... | math.NA | in this paper we are concerned with the plane wave method for the discretization of timeharmonic maxwells equations in three dimensions as pointed out in 6 it is difficult to derive a satisfactory l2 error estimate of the standard plane wave approximation of the timeharmonic maxwells equations we propose a variant of t... | [['in', 'this', 'paper', 'we', 'are', 'concerned', 'with', 'the', 'plane', 'wave', 'method', 'for', 'the', 'discretization', 'of', 'timeharmonic', 'maxwells', 'equations', 'in', 'three', 'dimensions', 'as', 'pointed', 'out', 'in', '6', 'it', 'is', 'difficult', 'to', 'derive', 'a', 'satisfactory', 'l2', 'error', 'estima... | [-0.14860804319021487, 0.033641828781977856, -0.05377358956842349, 0.11036076295664007, -0.10256773074385973, -0.08128769533216672, 0.0009150217574985944, 0.35420047787000547, -0.23239542130284221, -0.2536568629801414, 0.12637847475268227, -0.29142139201878375, -0.1885185862665135, 0.23920562310047658, -0.0054961884974... |
1,712.10102 | Lagrangian description and Hamiltonian density for the electrodynamics
of dispersive metamaterials | The Lagrangians and dissipation functions are proposed for use in the
electrodynamics of the double-negative and chiral metamaterials with finite
loss. The double-negative metamaterial considered here is the wires and split
rings periodic structure, while the chiral metamaterial is the single-resonance
helical resona... | physics.class-ph physics.app-ph | the lagrangians and dissipation functions are proposed for use in the electrodynamics of the doublenegative and chiral metamaterials with finite loss the doublenegative metamaterial considered here is the wires and split rings periodic structure while the chiral metamaterial is the singleresonance helical resonators ar... | [['the', 'lagrangians', 'and', 'dissipation', 'functions', 'are', 'proposed', 'for', 'use', 'in', 'the', 'electrodynamics', 'of', 'the', 'doublenegative', 'and', 'chiral', 'metamaterials', 'with', 'finite', 'loss', 'the', 'doublenegative', 'metamaterial', 'considered', 'here', 'is', 'the', 'wires', 'and', 'split', 'rin... | [-0.18922343518998888, 0.15503976783818668, -0.07847219020870522, 0.028146333107923787, -0.09251406078792027, -0.1076729609631002, -0.0012793254324147461, 0.37119757960367405, -0.22392724889020124, -0.28957967119466543, 0.016497199758927092, -0.2684244459383508, -0.16013333636274338, 0.16478454753653043, 0.010366316240... |
1,712.10103 | A Discontinuous Galerkin Method by Patch Reconstruction for Biharmonic
Problem | We propose a new discontinuous Galerkin method based on the least-squares
patch reconstruction for the biharmonic problem. We prove the optimal error
estimate of the proposed method. The two-dimensional and three-dimensional
numerical examples are presented to confirm the accuracy and efficiency of the
method with se... | math.NA | we propose a new discontinuous galerkin method based on the leastsquares patch reconstruction for the biharmonic problem we prove the optimal error estimate of the proposed method the twodimensional and threedimensional numerical examples are presented to confirm the accuracy and efficiency of the method with several b... | [['we', 'propose', 'a', 'new', 'discontinuous', 'galerkin', 'method', 'based', 'on', 'the', 'leastsquares', 'patch', 'reconstruction', 'for', 'the', 'biharmonic', 'problem', 'we', 'prove', 'the', 'optimal', 'error', 'estimate', 'of', 'the', 'proposed', 'method', 'the', 'twodimensional', 'and', 'threedimensional', 'nume... | [-0.0725857068604806, -0.08736425883283741, -0.07471101897719659, 0.02299122623445695, -0.0612462671073317, -0.122317250025573, 0.017932364300481583, 0.4220356780447458, -0.2720142546551008, -0.2923195936570042, 0.16695980647611514, -0.23016720056010967, -0.18311712725533238, 0.23104132483141465, -0.13115465386133446, ... |
1,712.10104 | Prospects for $\gamma\gamma\to$ Higgs observation in ultraperipheral ion
collisions at the Future Circular Collider | We study the two-photon production of the Higgs boson, $\rm \gamma\gamma\to
H$, at the Future Circular Collider (FCC) in ultraperipheral PbPb and pPb
collisions at $\sqrt{s_{NN}} = 39$ and 63 TeV. Signal and background events are
generated with MADGRAPH 5, including $\gamma$ fluxes from the proton and lead
ions in th... | hep-ph hep-ex nucl-ex nucl-th | we study the twophoton production of the higgs boson rm gammagammato h at the future circular collider fcc in ultraperipheral pbpb and ppb collisions at sqrts_nn 39 and 63 tev signal and background events are generated with madgraph 5 including gamma fluxes from the proton and lead ions in the equivalent photon approxi... | [['we', 'study', 'the', 'twophoton', 'production', 'of', 'the', 'higgs', 'boson', 'rm', 'gammagammato', 'h', 'at', 'the', 'future', 'circular', 'collider', 'fcc', 'in', 'ultraperipheral', 'pbpb', 'and', 'ppb', 'collisions', 'at', 'sqrts_nn', '39', 'and', '63', 'tev', 'signal', 'and', 'background', 'events', 'are', 'gen... | [-0.01156727248858029, 0.23108616480367036, -0.035469911092797575, 0.1750117099964281, 0.05352261874398564, -0.13701242246907758, -0.056706727036448606, 0.383752118783778, -0.14950315914337792, -0.3146609636339343, -0.04829511570278555, -0.4139635889175332, 0.1749587877677217, 0.1433843312137839, 0.12228093521622152, 0... |
1,712.10105 | Variance swaps under L\'{e}vy process with stochastic volatility and
stochastic interest rate in incomplete markets | This paper focuses on the pricing of the variance swap in an incomplete
market where the stochastic interest rate and the price of the stock are
respectively driven by Cox-Ingersoll-Ross model and Heston model with
simultaneous L\'{e}vy jumps. By using the equilibrium framework, we obtain the
pricing kernel and the e... | q-fin.PR | this paper focuses on the pricing of the variance swap in an incomplete market where the stochastic interest rate and the price of the stock are respectively driven by coxingersollross model and heston model with simultaneous levy jumps by using the equilibrium framework we obtain the pricing kernel and the equivalent ... | [['this', 'paper', 'focuses', 'on', 'the', 'pricing', 'of', 'the', 'variance', 'swap', 'in', 'an', 'incomplete', 'market', 'where', 'the', 'stochastic', 'interest', 'rate', 'and', 'the', 'price', 'of', 'the', 'stock', 'are', 'respectively', 'driven', 'by', 'coxingersollross', 'model', 'and', 'heston', 'model', 'with', ... | [-0.05816992364449763, 0.04640121053874237, -0.061348163064752444, 0.12151522762962755, -0.05176591211700904, -0.12170609452792244, 0.12267081089342609, 0.4117487853118142, -0.30286976847736563, -0.2184106459665555, 0.1742738723644193, -0.27026865172551057, -0.131280951339324, 0.19444251057050635, -0.12848703516074686,... |
1,712.10106 | An Optimal EDG Method for Distributed Control of Convection Diffusion
PDEs | We propose an embedded discontinuous Galerkin (EDG) method to approximate the
solution of a distributed control problem governed by convection diffusion
PDEs, and obtain optimal a priori error estimates for the state, dual state,
their fluxes, and the control. Moreover, we prove the optimize-then-discretize
(OD) and ... | math.NA | we propose an embedded discontinuous galerkin edg method to approximate the solution of a distributed control problem governed by convection diffusion pdes and obtain optimal a priori error estimates for the state dual state their fluxes and the control moreover we prove the optimizethendiscretize od and discrtizetheno... | [['we', 'propose', 'an', 'embedded', 'discontinuous', 'galerkin', 'edg', 'method', 'to', 'approximate', 'the', 'solution', 'of', 'a', 'distributed', 'control', 'problem', 'governed', 'by', 'convection', 'diffusion', 'pdes', 'and', 'obtain', 'optimal', 'a', 'priori', 'error', 'estimates', 'for', 'the', 'state', 'dual', ... | [-0.10724162424660542, 0.0036065121205121446, -0.0790576486763629, 0.043857036289674314, -0.07170030264691873, -0.14275046730922028, 0.09369392113929445, 0.38101166744123804, -0.29804229997098447, -0.2590346330946142, 0.160698579471897, -0.2529837612232024, -0.12925178911536933, 0.17808543532790447, -0.1223327195779843... |
1,712.10107 | Objective evaluation metrics for automatic classification of EEG events | The evaluation of machine learning algorithms in biomedical fields for
applications involving sequential data lacks standardization. Common
quantitative scalar evaluation metrics such as sensitivity and specificity can
often be misleading depending on the requirements of the application.
Evaluation metrics must ultim... | cs.LG eess.SP stat.ML | the evaluation of machine learning algorithms in biomedical fields for applications involving sequential data lacks standardization common quantitative scalar evaluation metrics such as sensitivity and specificity can often be misleading depending on the requirements of the application evaluation metrics must ultimatel... | [['the', 'evaluation', 'of', 'machine', 'learning', 'algorithms', 'in', 'biomedical', 'fields', 'for', 'applications', 'involving', 'sequential', 'data', 'lacks', 'standardization', 'common', 'quantitative', 'scalar', 'evaluation', 'metrics', 'such', 'as', 'sensitivity', 'and', 'specificity', 'can', 'often', 'be', 'mis... | [-0.0979214881389991, 0.005662843819745645, -0.07116962475131969, 0.09137109070042224, -0.1219936712179333, -0.1622698050178825, 0.08394758435184782, 0.41518995831435435, -0.17495885201651432, -0.3382089044138485, 0.12296661657556815, -0.266132259171228, -0.16831074841415547, 0.26311633015165525, -0.13228073368034307, ... |
1,712.10108 | Probing the Light Sterile Neutrino Through the Heavy Charged Higgs Decay
on the LHC | We show the 13 TeV proton-proton collider simulation in a
$\nu$-two-Higgs-doublet-model ($\nu$-THDM). The heavy charged Higgs bosons are
produced in pairs through the electroweak processes and decay to the light
sterile neutrinos. The light sterile neutrino further decays into a jet-like
object with a muon in it. Thi... | hep-ph | we show the 13 tev protonproton collider simulation in a nutwohiggsdoubletmodel nuthdm the heavy charged higgs bosons are produced in pairs through the electroweak processes and decay to the light sterile neutrinos the light sterile neutrino further decays into a jetlike object with a muon in it this helps us discrimin... | [['we', 'show', 'the', '13', 'tev', 'protonproton', 'collider', 'simulation', 'in', 'a', 'nutwohiggsdoubletmodel', 'nuthdm', 'the', 'heavy', 'charged', 'higgs', 'bosons', 'are', 'produced', 'in', 'pairs', 'through', 'the', 'electroweak', 'processes', 'and', 'decay', 'to', 'the', 'light', 'sterile', 'neutrinos', 'the', ... | [-0.013392763177398593, 0.3336000127252191, -0.08321392176828037, 0.2477698547998443, -0.046255265129730105, -0.1781474813974152, -0.006415160238975659, 0.3191960151617726, -0.22783653477672489, -0.2915464309975505, -0.05533052832082224, -0.382407419445614, 0.07391960962365071, 0.14335462325640644, 0.10680327985125283,... |
1,712.10109 | Abrupt transitions between Markovian and non-Markovian dynamics in open
quantum systems | A rapid restoration of the bath state is usually required to induce Markovian
dynamics for an open quantum system, which typically can be realized only in
limits such as weak system-bath coupling and infinitely large bath. In this
work, we investigate the Markovianity of a qubit system coupled to a
single-qubit bath ... | quant-ph | a rapid restoration of the bath state is usually required to induce markovian dynamics for an open quantum system which typically can be realized only in limits such as weak systembath coupling and infinitely large bath in this work we investigate the markovianity of a qubit system coupled to a singlequbit bath with th... | [['a', 'rapid', 'restoration', 'of', 'the', 'bath', 'state', 'is', 'usually', 'required', 'to', 'induce', 'markovian', 'dynamics', 'for', 'an', 'open', 'quantum', 'system', 'which', 'typically', 'can', 'be', 'realized', 'only', 'in', 'limits', 'such', 'as', 'weak', 'systembath', 'coupling', 'and', 'infinitely', 'large'... | [-0.160024540247519, 0.22166451010934002, -0.09887958474346245, 0.05440821800772594, 0.012946117940722712, -0.18242701293209826, 0.061284627935028826, 0.34376365053066554, -0.2888945641153375, -0.23104478871536177, 0.07173078273891761, -0.2633787645612973, -0.08475297350214411, 0.18489952030782866, 0.002040349317110137... |
1,712.1011 | Beyond Keywords and Relevance: A Personalized Ad Retrieval Framework in
E-Commerce Sponsored Search | On most sponsored search platforms, advertisers bid on some keywords for
their advertisements (ads). Given a search request, ad retrieval module
rewrites the query into bidding keywords, and uses these keywords as keys to
select Top N ads through inverted indexes. In this way, an ad will not be
retrieved even if quer... | cs.IR stat.ML | on most sponsored search platforms advertisers bid on some keywords for their advertisements ads given a search request ad retrieval module rewrites the query into bidding keywords and uses these keywords as keys to select top n ads through inverted indexes in this way an ad will not be retrieved even if queries are re... | [['on', 'most', 'sponsored', 'search', 'platforms', 'advertisers', 'bid', 'on', 'some', 'keywords', 'for', 'their', 'advertisements', 'ads', 'given', 'a', 'search', 'request', 'ad', 'retrieval', 'module', 'rewrites', 'the', 'query', 'into', 'bidding', 'keywords', 'and', 'uses', 'these', 'keywords', 'as', 'keys', 'to', ... | [-0.048420283190078205, 0.015367481553370857, -0.036737891054815716, 0.11699810471799639, -0.20121007770248173, -0.22728150202582278, 0.14489076093667083, 0.45831569003562134, -0.2417714931950387, -0.335477264109585, 0.12085846556350589, -0.359676311744584, -0.18600606847244006, 0.17508283690497692, -0.0990729523750229... |
1,712.10111 | On the synchronization theory of Kuramoto oscillators under the effect
of inertia | We investigate the synchronized collective behavior of the Kuramoto
oscillators with inertia effect. Both the frequency synchronization for
nonidentical case and the phase synchronization for identical case are in view.
As an application of our general theory, we show the unconditional frequency
synchronization for t... | math.DS | we investigate the synchronized collective behavior of the kuramoto oscillators with inertia effect both the frequency synchronization for nonidentical case and the phase synchronization for identical case are in view as an application of our general theory we show the unconditional frequency synchronization for the th... | [['we', 'investigate', 'the', 'synchronized', 'collective', 'behavior', 'of', 'the', 'kuramoto', 'oscillators', 'with', 'inertia', 'effect', 'both', 'the', 'frequency', 'synchronization', 'for', 'nonidentical', 'case', 'and', 'the', 'phase', 'synchronization', 'for', 'identical', 'case', 'are', 'in', 'view', 'as', 'an'... | [-0.2654923298092478, 0.1773998412514313, -0.017134400226337755, 0.010603781020187813, -0.0001366351447675539, -0.12578412321517649, 0.04565059922827894, 0.3492510311467492, -0.21667426579591373, -0.21484335382347522, 0.08070378773592655, -0.22806580994359177, -0.2459925988122173, 0.20717100685705309, -0.05232082588760... |
1,712.10112 | Toward precise neutrino measurements: An efficient energy response model
for liquid scintillator detectors | Liquid scintillator detectors are playing an increasingly important role in
low-energy neutrino experiments. In this article, we describe a generic energy
response model of liquid scintillator detectors that provides energy
estimations of sub-percent accuracy. This model fits a minimal set of
physically-motivated par... | physics.ins-det hep-ex | liquid scintillator detectors are playing an increasingly important role in lowenergy neutrino experiments in this article we describe a generic energy response model of liquid scintillator detectors that provides energy estimations of subpercent accuracy this model fits a minimal set of physicallymotivated parameters ... | [['liquid', 'scintillator', 'detectors', 'are', 'playing', 'an', 'increasingly', 'important', 'role', 'in', 'lowenergy', 'neutrino', 'experiments', 'in', 'this', 'article', 'we', 'describe', 'a', 'generic', 'energy', 'response', 'model', 'of', 'liquid', 'scintillator', 'detectors', 'that', 'provides', 'energy', 'estima... | [-0.06541404785882486, 0.134192673302421, -0.08926366359534624, 0.10881425895801697, -0.029576636776695715, -0.13040930535154124, 0.045874806385683385, 0.38097007442020664, -0.21562710020593123, -0.38045323779316326, 0.04641958505135814, -0.3365332403465321, -0.08765884926787725, 0.19049631095442332, -0.059122831344996... |
1,712.10113 | Directed flow in Au+Au collisions from the RHIC Beam Energy Scan at the
STAR experiment | We report results of $v_1(y)$ and $dv_1/dy$ near mid-rapidity for
$\pi^{\pm}$, $K^{\pm}$, $K_s^0$, $p$, $\overline{p}$, $\Lambda$,
$\overline{\Lambda}$ and $\phi$ from Beam Energy Scan Au+Au collisions at
$\sqrt{s_{NN}} = $ 7.7 - 200 GeV using the STAR detector at RHIC. The
$dv_{1}/dy$ of $\pi^{\pm}$, $K^{\pm}$ and $... | nucl-ex hep-ex nucl-th | we report results of v_1y and dv_1dy near midrapidity for pipm kpm k_s0 p overlinep lambda overlinelambda and phi from beam energy scan auau collisions at sqrts_nn 77 200 gev using the star detector at rhic the dv_1dy of pipm kpm and k_s0 mesons remains negative over all beam energies the dv_1dy of p and lambda baryons... | [['we', 'report', 'results', 'of', 'v_1y', 'and', 'dv_1dy', 'near', 'midrapidity', 'for', 'pipm', 'kpm', 'k_s0', 'p', 'overlinep', 'lambda', 'overlinelambda', 'and', 'phi', 'from', 'beam', 'energy', 'scan', 'auau', 'collisions', 'at', 'sqrts_nn', '77', '200', 'gev', 'using', 'the', 'star', 'detector', 'at', 'rhic', 'th... | [-0.07764138336703702, 0.2675800337325912, -0.17903384113345633, 0.10297179263021475, 0.023121158543557344, -0.1390442438977217, -0.00018154127340946164, 0.3204063468098224, -0.21157804925085885, -0.3094083020216101, -0.12594346500203743, -0.413168430562828, 0.15218933940037982, 0.15393214232053842, 0.12848460069903128... |
1,712.10114 | An Efficient and Fair Multi-Resource Allocation Mechanism for
Heterogeneous Servers | Efficient and fair allocation of multiple types of resources is a crucial
objective in a cloud/distributed computing cluster. Users may have diverse
resource needs. Furthermore, diversity in server properties/ capabilities may
mean that only a subset of servers may be usable by a given user. In platforms
with such he... | cs.DC | efficient and fair allocation of multiple types of resources is a crucial objective in a clouddistributed computing cluster users may have diverse resource needs furthermore diversity in server properties capabilities may mean that only a subset of servers may be usable by a given user in platforms with such heterogene... | [['efficient', 'and', 'fair', 'allocation', 'of', 'multiple', 'types', 'of', 'resources', 'is', 'a', 'crucial', 'objective', 'in', 'a', 'clouddistributed', 'computing', 'cluster', 'users', 'may', 'have', 'diverse', 'resource', 'needs', 'furthermore', 'diversity', 'in', 'server', 'properties', 'capabilities', 'may', 'me... | [-0.17483656329451475, -0.010559935948092505, -0.10728237679200106, 0.07789448693502302, -0.14342432155451695, -0.21057979964262727, 0.14197216680242408, 0.44569469668233214, -0.3187656251587273, -0.3108252865079809, 0.061106673793413266, -0.21538278072646552, -0.16095027845614968, 0.15334103315724668, -0.1470406550022... |
1,712.10115 | Critical role of quantum dynamical effects in the Raman spectroscopy of
liquid water | Understanding the Raman spectroscopy at the atomistic level is important for
the elucidation of dynamical processes in liquid water. Because the
polarizability (or its time derivative) is often a highly nonlinear function of
coordinates or/and momenta, we employ the linearized semiclassical initial
value representati... | physics.chem-ph cond-mat.mes-hall physics.comp-ph | understanding the raman spectroscopy at the atomistic level is important for the elucidation of dynamical processes in liquid water because the polarizability or its time derivative is often a highly nonlinear function of coordinates orand momenta we employ the linearized semiclassical initial value representation for ... | [['understanding', 'the', 'raman', 'spectroscopy', 'at', 'the', 'atomistic', 'level', 'is', 'important', 'for', 'the', 'elucidation', 'of', 'dynamical', 'processes', 'in', 'liquid', 'water', 'because', 'the', 'polarizability', 'or', 'its', 'time', 'derivative', 'is', 'often', 'a', 'highly', 'nonlinear', 'function', 'of... | [-0.1397669457988481, 0.18729783794422436, -0.10325067988489944, 0.03346391052437699, -0.02338802372461793, -0.10115979663904148, 0.02831796266266848, 0.4008474973771645, -0.29916525615987427, -0.23733335077211412, 0.03534769243738918, -0.27351662997341697, -0.15220492450539402, 0.15185124523894938, 0.05523100887423462... |
1,712.10116 | A momentum conserving $N$-body scheme with individual timesteps | $N$-body simulations study the dynamics of $N$ particles under the influence
of mutual long-distant forces such as gravity. In practice, $N$-body codes will
violate Newton's third law if they use either an approximate Poisson solver or
individual timesteps. In this study, we construct a novel $N$-body scheme by
combi... | astro-ph.IM astro-ph.CO astro-ph.GA | nbody simulations study the dynamics of n particles under the influence of mutual longdistant forces such as gravity in practice nbody codes will violate newtons third law if they use either an approximate poisson solver or individual timesteps in this study we construct a novel nbody scheme by combining a fast multipo... | [['nbody', 'simulations', 'study', 'the', 'dynamics', 'of', 'n', 'particles', 'under', 'the', 'influence', 'of', 'mutual', 'longdistant', 'forces', 'such', 'as', 'gravity', 'in', 'practice', 'nbody', 'codes', 'will', 'violate', 'newtons', 'third', 'law', 'if', 'they', 'use', 'either', 'an', 'approximate', 'poisson', 's... | [-0.15052328118757838, 0.08751754258445295, -0.13045927242577599, 0.06759583674575896, -0.07753530525525285, -0.12575311533632913, -0.015349804222061756, 0.35229914675757384, -0.29506765858264294, -0.34144464563459725, 0.04891711396126634, -0.21251412829574032, -0.11120805283563484, 0.19211969894629896, 0.0120108844475... |
1,712.10117 | Negative flare in the He I 10830 \AA\ line in facula | A small-scale flare SOL2012-09-21T02:19 (B2) occurred in a spotless active
region that we observed at a ground-based telescope equipped with a
spectrograph. During the flare, we registered an increase in absorption in the
He I 10830 \AA\ line by 25%, while other chromospheric and coronal spectral
lines demonstrated i... | astro-ph.SR | a smallscale flare sol20120921t0219 b2 occurred in a spotless active region that we observed at a groundbased telescope equipped with a spectrograph during the flare we registered an increase in absorption in the he i 10830 aa line by 25 while other chromospheric and coronal spectral lines demonstrated increase in brig... | [['a', 'smallscale', 'flare', 'sol20120921t0219', 'b2', 'occurred', 'in', 'a', 'spotless', 'active', 'region', 'that', 'we', 'observed', 'at', 'a', 'groundbased', 'telescope', 'equipped', 'with', 'a', 'spectrograph', 'during', 'the', 'flare', 'we', 'registered', 'an', 'increase', 'in', 'absorption', 'in', 'the', 'he', ... | [-0.05097358879734715, 0.18163254986484745, 0.02901651772799773, 0.09575566740149315, -0.018206761863647964, -0.11738143275321573, 0.034994687794903404, 0.531919901433187, -0.18007331397402523, -0.3473498529794441, 0.05623045763868752, -0.29917755544345087, -0.06903714291839262, 0.13046018279371385, -0.0185490399438268... |
1,712.10118 | Ward Identity and Basis Tensor Gauge Theory at One Loop | Basis tensor gauge theory (BTGT) is a reformulation of ordinary gauge theory
that is an analog of the vierbein formulation of gravity and is related to the
Wilson line formulation. To match ordinary gauge theories coupled to matter,
the BTGT formalism requires a continuous symmetry that we call the BTGT
symmetry in a... | hep-th | basis tensor gauge theory btgt is a reformulation of ordinary gauge theory that is an analog of the vierbein formulation of gravity and is related to the wilson line formulation to match ordinary gauge theories coupled to matter the btgt formalism requires a continuous symmetry that we call the btgt symmetry in additio... | [['basis', 'tensor', 'gauge', 'theory', 'btgt', 'is', 'a', 'reformulation', 'of', 'ordinary', 'gauge', 'theory', 'that', 'is', 'an', 'analog', 'of', 'the', 'vierbein', 'formulation', 'of', 'gravity', 'and', 'is', 'related', 'to', 'the', 'wilson', 'line', 'formulation', 'to', 'match', 'ordinary', 'gauge', 'theories', 'c... | [-0.13797684496079207, 0.15225776552996634, -0.13951499977196424, 0.09961066898491265, -0.1290318053215742, -0.150125876755722, -0.03265782596022522, 0.3036655996811687, -0.21168899064157473, -0.28106522973887305, 0.06011281128463698, -0.25603920704353667, -0.20652995036837993, 0.048798255989391165, -0.0175847490712747... |
1,712.10119 | Remarks on $p$-monotone operators | In this paper, we deal with three aspects of $p$-monotone operators. First we
study $p$-monotone operators with a unique maximal extension (called
pre-maximal), and with convex graph. We then deal with linear operators, and
provide characterizations of $p$-monotonicity and maximal $p$-monotonicity.
Finally we show th... | math.OC math.FA | in this paper we deal with three aspects of pmonotone operators first we study pmonotone operators with a unique maximal extension called premaximal and with convex graph we then deal with linear operators and provide characterizations of pmonotonicity and maximal pmonotonicity finally we show that the brezisbrowder th... | [['in', 'this', 'paper', 'we', 'deal', 'with', 'three', 'aspects', 'of', 'pmonotone', 'operators', 'first', 'we', 'study', 'pmonotone', 'operators', 'with', 'a', 'unique', 'maximal', 'extension', 'called', 'premaximal', 'and', 'with', 'convex', 'graph', 'we', 'then', 'deal', 'with', 'linear', 'operators', 'and', 'provi... | [-0.08686161879450083, 0.0734060724795449, -0.05444354593169456, 0.07020595601038533, -0.09894554552110825, -0.11430074697287351, -0.004562173949499779, 0.39803583759303185, -0.30293306942079584, -0.14488874067205423, 0.15413651158279904, -0.3324640976885955, -0.2133496020208387, 0.16077127510353045, -0.184218417049623... |
1,712.1012 | Decomposing the Quantile Ratio Index with applications to Australian
income and wealth data | The quantile ratio index introduced by Prendergast and Staudte 2017 is a
simple and effective measure of relative inequality for income data that is
resistant to outliers. It measures the average relative distance of a randomly
chosen income from its symmetric quantile. Another useful property of this
index is invest... | stat.ME | the quantile ratio index introduced by prendergast and staudte 2017 is a simple and effective measure of relative inequality for income data that is resistant to outliers it measures the average relative distance of a randomly chosen income from its symmetric quantile another useful property of this index is investigat... | [['the', 'quantile', 'ratio', 'index', 'introduced', 'by', 'prendergast', 'and', 'staudte', '2017', 'is', 'a', 'simple', 'and', 'effective', 'measure', 'of', 'relative', 'inequality', 'for', 'income', 'data', 'that', 'is', 'resistant', 'to', 'outliers', 'it', 'measures', 'the', 'average', 'relative', 'distance', 'of', ... | [-0.007686853361147361, 0.0891836878429277, -0.12415195785748853, 0.14243480833943964, -0.038104651129151894, -0.14322944264125637, 0.10332069372552938, 0.3634817166708586, -0.2789103169082187, -0.31427797202504876, 0.11694918161049103, -0.30066591844431995, -0.07278975344439015, 0.20638881801759576, -0.127285021060241... |
1,712.10121 | Reexamination of microscopic optical potentials based on multiple
scattering theory | Microscopic optical potentials have been successful in describing
nucleon-nucleus and nucleus-nucleus scattering. Some essential ingredients of
the framework, however, have not been examined in detail. Applicability of the
microscopic folding model is systematically investigated. Effect of an
antisymmetrization facto... | nucl-th | microscopic optical potentials have been successful in describing nucleonnucleus and nucleusnucleus scattering some essential ingredients of the framework however have not been examined in detail applicability of the microscopic folding model is systematically investigated effect of an antisymmetrization factor asf app... | [['microscopic', 'optical', 'potentials', 'have', 'been', 'successful', 'in', 'describing', 'nucleonnucleus', 'and', 'nucleusnucleus', 'scattering', 'some', 'essential', 'ingredients', 'of', 'the', 'framework', 'however', 'have', 'not', 'been', 'examined', 'in', 'detail', 'applicability', 'of', 'the', 'microscopic', 'f... | [-0.04032233499972626, 0.15866978211102778, -0.06866458417625426, 0.16408959438558668, 0.013253383352456237, -0.11042422562714183, 0.0306839293444046, 0.3724372251995636, -0.20928420570917092, -0.30327892273356366, -0.052823333953738325, -0.3538469476100141, -0.024669064087198024, 0.19029177703257455, 0.095540539473575... |
1,712.10122 | The number of inversions of permutations with fixed shape | The Robinson-Schensted correspondence can be viewed as a map from
permutations to partitions. In this work, we study the number of inversions of
permutations corresponding to a fixed partition $\lambda$ under this map.
Hohlweg characterized permutations having shape $\lambda$ with the minimum
number of inversions. He... | math.CO math.PR | the robinsonschensted correspondence can be viewed as a map from permutations to partitions in this work we study the number of inversions of permutations corresponding to a fixed partition lambda under this map hohlweg characterized permutations having shape lambda with the minimum number of inversions here we give th... | [['the', 'robinsonschensted', 'correspondence', 'can', 'be', 'viewed', 'as', 'a', 'map', 'from', 'permutations', 'to', 'partitions', 'in', 'this', 'work', 'we', 'study', 'the', 'number', 'of', 'inversions', 'of', 'permutations', 'corresponding', 'to', 'a', 'fixed', 'partition', 'lambda', 'under', 'this', 'map', 'hohlwe... | [-0.18028766510657745, 0.16372064215310914, -0.04011690716655685, 0.043699125793882375, -0.0682136713282786, -0.08564072749623568, 0.050864331763108624, 0.33913922133523566, -0.2979526368135789, -0.3238028200841186, 0.08063112074592252, -0.2525971546759921, -0.1208170109824969, 0.1342618304609072, -0.07493500580716103,... |
1,712.10123 | Rowmotion in slow motion | Rowmotion is a simple cyclic action on the distributive lattice of order
ideals of a poset: it sends the order ideal x to the order ideal generated by
the minimal elements not in x. It can also be computed in "slow motion" as a
sequence of local moves. We use the setting of trim lattices to generalize both
definition... | math.CO | rowmotion is a simple cyclic action on the distributive lattice of order ideals of a poset it sends the order ideal x to the order ideal generated by the minimal elements not in x it can also be computed in slow motion as a sequence of local moves we use the setting of trim lattices to generalize both definitions of ro... | [['rowmotion', 'is', 'a', 'simple', 'cyclic', 'action', 'on', 'the', 'distributive', 'lattice', 'of', 'order', 'ideals', 'of', 'a', 'poset', 'it', 'sends', 'the', 'order', 'ideal', 'x', 'to', 'the', 'order', 'ideal', 'generated', 'by', 'the', 'minimal', 'elements', 'not', 'in', 'x', 'it', 'can', 'also', 'be', 'computed... | [-0.16046806416453274, 0.13320390126646908, -0.08981770448582738, 0.03398890702467048, -0.10977970793339095, -0.10482210517839942, 0.052238689715399834, 0.3872930038006122, -0.35802755168380035, -0.19155913356103396, 0.11206547229172648, -0.26064799067781386, -0.1610275985659065, 0.1524361838495597, -0.1068891994445059... |
1,712.10124 | The height distribution in root systems | We prove several formulas for the distribution of positive roots.
| math.CO | we prove several formulas for the distribution of positive roots | [['we', 'prove', 'several', 'formulas', 'for', 'the', 'distribution', 'of', 'positive', 'roots']] | [-0.1981498397886753, 0.022738849837332965, -0.11468633906915784, 0.153906343691051, -0.05513004623353481, -0.08262606300413608, 0.004536564648151398, 0.3156529158353806, -0.26923652589321134, -0.18655170034617186, 0.0979181460570544, -0.33916105479002, -0.1602511666715145, 0.2641961752902716, 0.020273661853570955, 0.1... |
1,712.10125 | Log Picard algebroids and meromorphic line bundles | We introduce logarithmic Picard algebroids, a natural class of Lie algebroids
adapted to a simple normal crossings divisor on a smooth projective variety. We
show that such algebroids are classified by a subspace of the de Rham
cohomology of the divisor complement determined by its mixed Hodge structure.
We then solv... | math.AG math.DG | we introduce logarithmic picard algebroids a natural class of lie algebroids adapted to a simple normal crossings divisor on a smooth projective variety we show that such algebroids are classified by a subspace of the de rham cohomology of the divisor complement determined by its mixed hodge structure we then solve the... | [['we', 'introduce', 'logarithmic', 'picard', 'algebroids', 'a', 'natural', 'class', 'of', 'lie', 'algebroids', 'adapted', 'to', 'a', 'simple', 'normal', 'crossings', 'divisor', 'on', 'a', 'smooth', 'projective', 'variety', 'we', 'show', 'that', 'such', 'algebroids', 'are', 'classified', 'by', 'a', 'subspace', 'of', 't... | [-0.23587739915237763, -0.04921295744279632, -0.0998040818492882, 0.11558453693432966, -0.20827523092739283, -0.18020687455427833, 0.015205074096775207, 0.3863284790888429, -0.3377382244041655, -0.1895535322080832, 0.09386213134275749, -0.18539851723471656, -0.20243988857837394, 0.19365443321003112, -0.1724934895857586... |
1,712.10126 | Traps in hadron spectroscopy: Thresholds, triangle singularities, etc | The knowledge of hadron spectrum is based on experimental observations of
hadronic resonances. The resonances are normally observed as peaks in certain
invariant mass distributions. However, neither is a peak necessarily due to the
presence of a resonance, nor does a resonance necessarily lead to a peak.
Kinematic si... | hep-ph hep-ex nucl-th | the knowledge of hadron spectrum is based on experimental observations of hadronic resonances the resonances are normally observed as peaks in certain invariant mass distributions however neither is a peak necessarily due to the presence of a resonance nor does a resonance necessarily lead to a peak kinematic singulari... | [['the', 'knowledge', 'of', 'hadron', 'spectrum', 'is', 'based', 'on', 'experimental', 'observations', 'of', 'hadronic', 'resonances', 'the', 'resonances', 'are', 'normally', 'observed', 'as', 'peaks', 'in', 'certain', 'invariant', 'mass', 'distributions', 'however', 'neither', 'is', 'a', 'peak', 'necessarily', 'due', ... | [-0.11162772727424675, 0.1578106569870601, -0.15669834328758897, 0.12402692077695533, -0.13228535175210598, -0.11708003271258238, 0.011783459781189307, 0.37288580719155795, -0.1718946738225041, -0.3044176534326239, 0.06053085986941093, -0.3014039099075352, -0.10442194236075562, 0.15250481416781744, -0.03115398805080489... |
1,712.10127 | Nanoscopy of pairs of atoms by fluorescence in a magnetic field | Spontaneous emission spectra of two initially excited closely spaced
identical atoms are very sensitive to the strength and the direction of the
applied magnetic field. The relevant schemes are considered that ensure the
determination of the mutual spatial orientation of the atoms and the distance
between them by ent... | physics.atom-ph physics.optics quant-ph | spontaneous emission spectra of two initially excited closely spaced identical atoms are very sensitive to the strength and the direction of the applied magnetic field the relevant schemes are considered that ensure the determination of the mutual spatial orientation of the atoms and the distance between them by entire... | [['spontaneous', 'emission', 'spectra', 'of', 'two', 'initially', 'excited', 'closely', 'spaced', 'identical', 'atoms', 'are', 'very', 'sensitive', 'to', 'the', 'strength', 'and', 'the', 'direction', 'of', 'the', 'applied', 'magnetic', 'field', 'the', 'relevant', 'schemes', 'are', 'considered', 'that', 'ensure', 'the',... | [-0.17631476460221826, 0.21515142241233579, 0.007682488097667705, 0.04858522841690997, 0.02271133849122138, -0.12757487694563513, -0.008250107888174667, 0.41151113249361515, -0.24848018085520546, -0.328801015751775, -0.01113773832251106, -0.2571854074273936, -0.046082312960854986, 0.17953142370838163, 0.088056173344904... |
1,712.10128 | Structured decentralized control of positive systems with applications
to combination drug therapy and leader selection in directed networks | We study a class of structured optimal control problems in which the main
diagonal of the dynamic matrix is a linear function of the design variable.
While such problems are in general challenging and nonconvex, for positive
systems we prove convexity of the $H_2$ and $H_\infty$ optimal control
formulations which all... | math.OC cs.DC cs.SY | we study a class of structured optimal control problems in which the main diagonal of the dynamic matrix is a linear function of the design variable while such problems are in general challenging and nonconvex for positive systems we prove convexity of the h_2 and h_infty optimal control formulations which allow for ar... | [['we', 'study', 'a', 'class', 'of', 'structured', 'optimal', 'control', 'problems', 'in', 'which', 'the', 'main', 'diagonal', 'of', 'the', 'dynamic', 'matrix', 'is', 'a', 'linear', 'function', 'of', 'the', 'design', 'variable', 'while', 'such', 'problems', 'are', 'in', 'general', 'challenging', 'and', 'nonconvex', 'fo... | [-0.09900192124842772, 0.02693532491869093, -0.026480838434094316, 0.07896721703914006, -0.10683971255593284, -0.18655214176728402, 0.06857925741948022, 0.3966571650279191, -0.28607314250938876, -0.267244991693127, 0.17063502872457045, -0.20972855094690585, -0.19376993906548648, 0.18497836976194212, -0.1210875344327120... |
1,712.10129 | Role of Non-Equilibrium Conformations on Driven Polymer Translocation | One of the major theoretical methods in understanding polymer translocation
through a nanopore is the Fokker-Planck formalism based on the assumption of
quasi-equilibrium of polymer conformations. The criterion for applicability of
the quasi-equilibrium approximation for polymer translocation is that the
average tran... | cond-mat.soft | one of the major theoretical methods in understanding polymer translocation through a nanopore is the fokkerplanck formalism based on the assumption of quasiequilibrium of polymer conformations the criterion for applicability of the quasiequilibrium approximation for polymer translocation is that the average translocat... | [['one', 'of', 'the', 'major', 'theoretical', 'methods', 'in', 'understanding', 'polymer', 'translocation', 'through', 'a', 'nanopore', 'is', 'the', 'fokkerplanck', 'formalism', 'based', 'on', 'the', 'assumption', 'of', 'quasiequilibrium', 'of', 'polymer', 'conformations', 'the', 'criterion', 'for', 'applicability', 'o... | [-0.1506230387712267, 0.18734850242146223, -0.11706593641935874, 0.029902321835112596, 0.04451766656617434, -0.14113908024271007, -0.019120425489252274, 0.41894904233756575, -0.27393737224567877, -0.24403093407978774, 0.04112699284144726, -0.235382369391409, -0.058461244532891254, 0.18320144965645183, 0.052666577248741... |
1,712.1013 | Recovery from Maunder-like Grand Minima in a Babcock--Leighton Solar
Dynamo Model | The Sun occasionally goes through Maunder-like extended grand minima when its
magnetic activity drops considerably from the normal activity level for several
decades. Many possible theories have been proposed to explain the origin of
these minima. However, how the Sun managed to recover from such inactive phases
ever... | astro-ph.SR astro-ph.EP | the sun occasionally goes through maunderlike extended grand minima when its magnetic activity drops considerably from the normal activity level for several decades many possible theories have been proposed to explain the origin of these minima however how the sun managed to recover from such inactive phases every time... | [['the', 'sun', 'occasionally', 'goes', 'through', 'maunderlike', 'extended', 'grand', 'minima', 'when', 'its', 'magnetic', 'activity', 'drops', 'considerably', 'from', 'the', 'normal', 'activity', 'level', 'for', 'several', 'decades', 'many', 'possible', 'theories', 'have', 'been', 'proposed', 'to', 'explain', 'the', ... | [-0.1148002282065602, 0.21007580334471407, -0.038135513992165214, 0.1515878324119769, -0.018764435079617378, -0.0760000075906133, 0.05157268481711164, 0.3380506530905572, -0.2703613122447561, -0.37817687360713115, 0.10804814770758056, -0.19534153511079075, -0.19356081698042077, 0.18146265899069988, -0.0744391202675895,... |
1,712.10131 | Sparse Polynomial Chaos Expansions via Compressed Sensing and D-optimal
Design | In the field of uncertainty quantification, sparse polynomial chaos (PC)
expansions are commonly used by researchers for a variety of purposes, such as
surrogate modeling. Ideas from compressed sensing may be employed to exploit
this sparsity in order to reduce computational costs. A class of greedy
compressed sensin... | stat.ME math.PR stat.CO | in the field of uncertainty quantification sparse polynomial chaos pc expansions are commonly used by researchers for a variety of purposes such as surrogate modeling ideas from compressed sensing may be employed to exploit this sparsity in order to reduce computational costs a class of greedy compressed sensing algori... | [['in', 'the', 'field', 'of', 'uncertainty', 'quantification', 'sparse', 'polynomial', 'chaos', 'pc', 'expansions', 'are', 'commonly', 'used', 'by', 'researchers', 'for', 'a', 'variety', 'of', 'purposes', 'such', 'as', 'surrogate', 'modeling', 'ideas', 'from', 'compressed', 'sensing', 'may', 'be', 'employed', 'to', 'ex... | [-0.055568564180040574, 0.0006386850128749957, -0.09727767024412472, 0.02898382682249487, -0.1001335151305192, -0.13602227777633327, 0.07714857582799908, 0.41047865260838906, -0.29351502221316617, -0.3069053811146721, 0.11824242765439695, -0.23334475778294414, -0.17574577179954523, 0.2129923955546971, -0.07453650957991... |
1,712.10132 | The Multilinear Structure of ReLU Networks | We study the loss surface of neural networks equipped with a hinge loss
criterion and ReLU or leaky ReLU nonlinearities. Any such network defines a
piecewise multilinear form in parameter space. By appealing to harmonic
analysis we show that all local minima of such network are non-differentiable,
except for those mi... | cs.LG | we study the loss surface of neural networks equipped with a hinge loss criterion and relu or leaky relu nonlinearities any such network defines a piecewise multilinear form in parameter space by appealing to harmonic analysis we show that all local minima of such network are nondifferentiable except for those minima t... | [['we', 'study', 'the', 'loss', 'surface', 'of', 'neural', 'networks', 'equipped', 'with', 'a', 'hinge', 'loss', 'criterion', 'and', 'relu', 'or', 'leaky', 'relu', 'nonlinearities', 'any', 'such', 'network', 'defines', 'a', 'piecewise', 'multilinear', 'form', 'in', 'parameter', 'space', 'by', 'appealing', 'to', 'harmon... | [-0.11270324267710732, 0.028400130022241964, -0.05131025337078403, 0.14350145957762359, -0.07197398647039602, -0.20001471037687982, 0.01872691144523895, 0.45756472640596657, -0.3058546961993968, -0.23472836417397402, 0.12331779057518538, -0.2688302011105471, -0.31363541809677153, 0.19986527664916573, -0.125715427547003... |
1,712.10133 | Stationary C*-dynamical systems | We introduce the notion of stationary actions in the context of C*-algebras.
We develop the basics of the theory, and provide applications to several
ergodic theoretical and operator algebraic rigidity problems.
| math.OA math.GR | we introduce the notion of stationary actions in the context of calgebras we develop the basics of the theory and provide applications to several ergodic theoretical and operator algebraic rigidity problems | [['we', 'introduce', 'the', 'notion', 'of', 'stationary', 'actions', 'in', 'the', 'context', 'of', 'calgebras', 'we', 'develop', 'the', 'basics', 'of', 'the', 'theory', 'and', 'provide', 'applications', 'to', 'several', 'ergodic', 'theoretical', 'and', 'operator', 'algebraic', 'rigidity', 'problems']] | [-0.11261785761903852, 0.09509272963529633, -0.11879636386349317, 0.11036688449882692, -0.08910880418073747, -0.09340197839323551, 0.030396781722834755, 0.3448176999846774, -0.33172895350763876, -0.19363279868998834, 0.1485065389837649, -0.2590096309300392, -0.22149909561079356, 0.1572641527220126, -0.18577010803405317... |
1,712.10134 | Coupled Self-Organized Hydrodynamics and Navier-Stokes models: local
well-posedness and the limit from the Self-Organized Kinetic-fluid models | A coupled system of self-organized hydrodynamics and Navier-Stokes equations
(SOH-NS), which models self-propelled particles in a viscous fluid, was
recently derived by Degond et al. \cite{DMVY-2017-arXiv}, starting from a
micro-macro particle system of Vicsek-Navier-Stokes model, through an
intermediate step of a se... | math.AP | a coupled system of selforganized hydrodynamics and navierstokes equations sohns which models selfpropelled particles in a viscous fluid was recently derived by degond et al citedmvy2017arxiv starting from a micromacro particle system of vicseknavierstokes model through an intermediate step of a selforganized kineticki... | [['a', 'coupled', 'system', 'of', 'selforganized', 'hydrodynamics', 'and', 'navierstokes', 'equations', 'sohns', 'which', 'models', 'selfpropelled', 'particles', 'in', 'a', 'viscous', 'fluid', 'was', 'recently', 'derived', 'by', 'degond', 'et', 'al', 'citedmvy2017arxiv', 'starting', 'from', 'a', 'micromacro', 'particle... | [-0.09315525989281014, 0.08482462366708204, -0.18118808231782169, 0.020995971149532125, 0.004133207341656089, -0.12637768873479216, 0.008617516169324517, 0.23870994137600066, -0.285034807624761, -0.28500529373064637, 0.04522456859936938, -0.23742209866060876, -0.17878501288359985, 0.13923531250446103, -0.00026899954536... |
1,712.10135 | Higher order nonclassicalities of finite dimensional coherent states: A
comparative study | Conventional coherent states (CSs) are defined in various ways. For example,
CS is defined as an infinite Poissonian expansion in Fock states, as displaced
vacuum state, or as an eigenket of annihilation operator. In the infinite
dimensional Hilbert space, these definitions are equivalent. However, these
definitions ... | quant-ph | conventional coherent states css are defined in various ways for example cs is defined as an infinite poissonian expansion in fock states as displaced vacuum state or as an eigenket of annihilation operator in the infinite dimensional hilbert space these definitions are equivalent however these definitions are not equi... | [['conventional', 'coherent', 'states', 'css', 'are', 'defined', 'in', 'various', 'ways', 'for', 'example', 'cs', 'is', 'defined', 'as', 'an', 'infinite', 'poissonian', 'expansion', 'in', 'fock', 'states', 'as', 'displaced', 'vacuum', 'state', 'or', 'as', 'an', 'eigenket', 'of', 'annihilation', 'operator', 'in', 'the',... | [-0.09622761673243665, 0.19075842519256136, -0.08472169671346107, 0.09515785726347334, 0.012582758056452951, -0.1306509043014533, 0.0015865868901380816, 0.3424565665121819, -0.2327343450003379, -0.23196833082348914, 0.07737255602559025, -0.26682443391733074, -0.07987577623587001, 0.18087587963059745, -0.029435847772637... |
1,712.10136 | Learning Deep and Compact Models for Gesture Recognition | We look at the problem of developing a compact and accurate model for gesture
recognition from videos in a deep-learning framework. Towards this we propose a
joint 3DCNN-LSTM model that is end-to-end trainable and is shown to be better
suited to capture the dynamic information in actions. The solution achieves
close ... | cs.CV | we look at the problem of developing a compact and accurate model for gesture recognition from videos in a deeplearning framework towards this we propose a joint 3dcnnlstm model that is endtoend trainable and is shown to be better suited to capture the dynamic information in actions the solution achieves close to state... | [['we', 'look', 'at', 'the', 'problem', 'of', 'developing', 'a', 'compact', 'and', 'accurate', 'model', 'for', 'gesture', 'recognition', 'from', 'videos', 'in', 'a', 'deeplearning', 'framework', 'towards', 'this', 'we', 'propose', 'a', 'joint', '3dcnnlstm', 'model', 'that', 'is', 'endtoend', 'trainable', 'and', 'is', '... | [-0.04599763662163012, 0.01658604820767621, -0.08654388237916746, 0.05815982787689867, -0.07620372855644517, -0.1905327593093785, 0.030397096160650568, 0.4182116774325611, -0.19576395006592096, -0.34625077615844224, 0.0870498497882357, -0.27913620290072527, -0.1385497532827983, 0.2223951571010554, -0.12765922049836545,... |
1,712.10137 | Symmetry Preservation and Critical Fluctuations in a Pseudospin
Crossover Perovskite LaCoO$_3$ | Spin-state crossover beyond a conventional ligand-field theory has been a
fundamental issue in condensed matter physics. Here, we report microscopic
observations of spin states and low-energy dynamics through orbital-resolved
NMR spectroscopy in the prototype compound LaCoO$_3$. The $^{59}$Co NMR
spectrum shows the p... | cond-mat.str-el | spinstate crossover beyond a conventional ligandfield theory has been a fundamental issue in condensed matter physics here we report microscopic observations of spin states and lowenergy dynamics through orbitalresolved nmr spectroscopy in the prototype compound lacoo_3 the 59co nmr spectrum shows the preserved crystal... | [['spinstate', 'crossover', 'beyond', 'a', 'conventional', 'ligandfield', 'theory', 'has', 'been', 'a', 'fundamental', 'issue', 'in', 'condensed', 'matter', 'physics', 'here', 'we', 'report', 'microscopic', 'observations', 'of', 'spin', 'states', 'and', 'lowenergy', 'dynamics', 'through', 'orbitalresolved', 'nmr', 'spe... | [-0.15321566851252294, 0.2771137950284907, -0.08137354902248448, 0.04956686295803607, -0.01791746895320303, -0.14515187580314443, 0.0742036359669736, 0.3340131358690853, -0.28120215573003443, -0.26683501887509203, -0.01249946795007962, -0.30643145899163693, -0.08553356545661965, 0.09963149509180015, 0.10631477043369976... |
1,712.10138 | On the Diophantine equation F_{n}-F_{m}=2^{a} | In this paper, we solve Diophantine equation in the tittle in nonnegative
integers m,n, and a. In order to prove our result, we use lower bounds for
linear forms in logarithms and and a version of the Baker-Davenport reduction
method in diophantine approximation.
| math.NT | in this paper we solve diophantine equation in the tittle in nonnegative integers mn and a in order to prove our result we use lower bounds for linear forms in logarithms and and a version of the bakerdavenport reduction method in diophantine approximation | [['in', 'this', 'paper', 'we', 'solve', 'diophantine', 'equation', 'in', 'the', 'tittle', 'in', 'nonnegative', 'integers', 'mn', 'and', 'a', 'in', 'order', 'to', 'prove', 'our', 'result', 'we', 'use', 'lower', 'bounds', 'for', 'linear', 'forms', 'in', 'logarithms', 'and', 'and', 'a', 'version', 'of', 'the', 'bakerdaven... | [-0.15004262079795203, -0.02350940089672804, -0.0926007063881982, 0.076172424909947, -0.048054893634149005, -0.07688400257999699, 0.061815999118456, 0.2680195534069623, -0.29102436098314466, -0.2654539677979691, 0.0798011492727147, -0.2861106236953111, -0.19179603191358702, 0.19188150169239157, -0.0908323544121924, 0.0... |
1,712.10139 | Enumeration of Unsensed Orientable Maps on Surfaces of a Given Genus | In this work for the first time we enumerate unlabelled maps on orientable
genus $g$ surfaces with respect to all homeomorphisms, including both
orientation-preserving and orientation-reversing. We show that in the latter
case as an intermediate step one has to enumerate rooted maps of a special kind
(quotient maps) ... | math.CO | in this work for the first time we enumerate unlabelled maps on orientable genus g surfaces with respect to all homeomorphisms including both orientationpreserving and orientationreversing we show that in the latter case as an intermediate step one has to enumerate rooted maps of a special kind quotient maps on orienta... | [['in', 'this', 'work', 'for', 'the', 'first', 'time', 'we', 'enumerate', 'unlabelled', 'maps', 'on', 'orientable', 'genus', 'g', 'surfaces', 'with', 'respect', 'to', 'all', 'homeomorphisms', 'including', 'both', 'orientationpreserving', 'and', 'orientationreversing', 'we', 'show', 'that', 'in', 'the', 'latter', 'case'... | [-0.17878254390527287, 0.08989472088102378, -0.03819025357483656, 0.05340496426472416, -0.08623093990125245, -0.13231541429247176, 0.05178609185598113, 0.38970839962750287, -0.2660780823509838, -0.2865872630318808, 0.10599150000194499, -0.30189250311028065, -0.17930383514310536, 0.22055634205507768, -0.1560794691700343... |
1,712.1014 | Weyl Solutions and J-selfadjointness for Dirac operators | We consider a non-selfadjoint Dirac-type differential expression
\begin{equation} D(Q)y:= J_n \frac{dy}{dx} + Q(x)y, \quad\quad\quad (1)
\end{equation} with a non-selfadjoint potential matrix $Q \in
L^1_{loc}({\mathcal I},\mathbb{C}^{n\times n})$ and a signature matrix $J_n
=-J_n^{-1} = -J_n^*\in \mathbb{C}^{n\ti... | math.SP | we consider a nonselfadjoint diractype differential expression beginequation dqy j_n fracdydx qxy quadquadquad 1 endequation with a nonselfadjoint potential matrix q in l1_locmathcal imathbbcntimes n and a signature matrix j_n j_n1 j_nin mathbbcntimes n here mathcal i denotes either the line mathbbr or the halfline mat... | [['we', 'consider', 'a', 'nonselfadjoint', 'diractype', 'differential', 'expression', 'beginequation', 'dqy', 'j_n', 'fracdydx', 'qxy', 'quadquadquad', '1', 'endequation', 'with', 'a', 'nonselfadjoint', 'potential', 'matrix', 'q', 'in', 'l1_locmathcal', 'imathbbcntimes', 'n', 'and', 'a', 'signature', 'matrix', 'j_n', '... | [-0.16571318559046533, 0.08144316831422731, -0.027379267864130637, 0.038506441322356665, -0.04963035068499881, -0.18511046682157226, -0.03849231874117175, 0.3195554247654572, -0.2673889347024866, -0.16442178650538916, 0.08816297266827393, -0.3665332144176638, -0.17773214262356427, 0.1305705861352082, -0.054703763099638... |
1,712.10141 | Scattering amplitude from Bethe-Salpeter wave function inside the
interaction range | We propose a method to calculate scattering amplitudes using the
Bethe-Salpeter wave function inside the interaction range on the lattice. For
an exploratory study of this method, we evaluate a scattering length of $I=2$
S-wave two pions by the use of the on-shell scattering amplitude. Our result is
confirmed to be c... | hep-lat | we propose a method to calculate scattering amplitudes using the bethesalpeter wave function inside the interaction range on the lattice for an exploratory study of this method we evaluate a scattering length of i2 swave two pions by the use of the onshell scattering amplitude our result is confirmed to be consistent w... | [['we', 'propose', 'a', 'method', 'to', 'calculate', 'scattering', 'amplitudes', 'using', 'the', 'bethesalpeter', 'wave', 'function', 'inside', 'the', 'interaction', 'range', 'on', 'the', 'lattice', 'for', 'an', 'exploratory', 'study', 'of', 'this', 'method', 'we', 'evaluate', 'a', 'scattering', 'length', 'of', 'i2', '... | [-0.11815134724737078, 0.15875602602149677, -0.1261768106209195, 0.08166042081775494, -0.03129566339370997, -0.03975317177727171, 0.04963753601887088, 0.37400181699490204, -0.22882962311901475, -0.21144416113046632, 0.023126870424122266, -0.30041655416235974, -0.13874903109356546, 0.18051233934913424, 0.094242987938333... |
1,712.10142 | Existence of supersingular representations of p-adic reductive groups | Let G be a connected simple adjoint p-adic group not isomorphic to a
projective linear group PGL(m,D) of a division algebra D, or an adjoint
ramified unitary group of a split hermitian form in 3 variables. We prove that
G admits an irreducible admissible supercuspidal (i.e. supersingular)
representation over any fiel... | math.NT | let g be a connected simple adjoint padic group not isomorphic to a projective linear group pglmd of a division algebra d or an adjoint ramified unitary group of a split hermitian form in 3 variables we prove that g admits an irreducible admissible supercuspidal ie supersingular representation over any field of charact... | [['let', 'g', 'be', 'a', 'connected', 'simple', 'adjoint', 'padic', 'group', 'not', 'isomorphic', 'to', 'a', 'projective', 'linear', 'group', 'pglmd', 'of', 'a', 'division', 'algebra', 'd', 'or', 'an', 'adjoint', 'ramified', 'unitary', 'group', 'of', 'a', 'split', 'hermitian', 'form', 'in', '3', 'variables', 'we', 'pro... | [-0.3020618245497627, 0.10886837170022223, -0.2203255978254777, -0.039117328509609306, -0.2128006973356571, -0.21468041443599845, -0.04096424515482108, 0.3414067983065011, -0.38325524910019254, -0.10514788888394833, 0.02432163790492165, -0.16548258658357948, -0.12008855325380727, 0.15259123210057193, -0.150589690365793... |
1,712.10143 | A new compact young moving group around V1062 Sco | Aims. We are searching for new open clusters or moving groups in the Solar
neighbourhood. Methods. We used the Gaia-TGAS catalogue, cut it into narrow
proper motion and parallax slices and searched for significant spatial
over-densities of stars in each slice. We then examined stars forming
over-densities in optical ... | astro-ph.SR astro-ph.GA | aims we are searching for new open clusters or moving groups in the solar neighbourhood methods we used the gaiatgas catalogue cut it into narrow proper motion and parallax slices and searched for significant spatial overdensities of stars in each slice we then examined stars forming overdensities in optical and nearin... | [['aims', 'we', 'are', 'searching', 'for', 'new', 'open', 'clusters', 'or', 'moving', 'groups', 'in', 'the', 'solar', 'neighbourhood', 'methods', 'we', 'used', 'the', 'gaiatgas', 'catalogue', 'cut', 'it', 'into', 'narrow', 'proper', 'motion', 'and', 'parallax', 'slices', 'and', 'searched', 'for', 'significant', 'spatia... | [-0.051591236268265034, 0.11947055050081366, -0.09653728699757064, 0.06630434925965448, -0.12758052319447785, -0.050286866802640294, 0.13498435724816066, 0.46808237473359676, -0.15213776467566345, -0.3957375794222268, 0.03843037328948008, -0.3293084154655743, 0.03430313047094926, 0.22372780179581173, -0.059820952286288... |
1,712.10144 | About multiplicities and applications to Bezout numbers | Let $(A,\mathfrak{m},\Bbbk)$ denote a local Noetherian ring and
$\mathfrak{q}$ an ideal such that $\ell_A(M/\mathfrak{q}M) < \infty$ for a
finitely generated $A$-module $M$. Let $\au = a_1,\ldots,a_d$ denote a system
of parameters of $M$ such that $a_i \in \mathfrak{q}^{c_i} \setminus
\mathfrak{q}^{c_i+1}$ for $i=1,\... | math.AC | let amathfrakmbbbk denote a local noetherian ring and mathfrakq an ideal such that ell_ammathfrakqm infty for a finitely generated amodule m let au a_1ldotsa_d denote a system of parameters of m such that a_i in mathfrakqc_i setminus mathfrakqc_i1 for i1ldotsd it follows that chi e_0aum c cdot e_0mathfrakqm geq 0 where... | [['let', 'amathfrakmbbbk', 'denote', 'a', 'local', 'noetherian', 'ring', 'and', 'mathfrakq', 'an', 'ideal', 'such', 'that', 'ell_ammathfrakqm', 'infty', 'for', 'a', 'finitely', 'generated', 'amodule', 'm', 'let', 'au', 'a_1ldotsa_d', 'denote', 'a', 'system', 'of', 'parameters', 'of', 'm', 'such', 'that', 'a_i', 'in', '... | [-0.2327449237262564, 0.12171422681993656, -0.006075665986697588, -0.07248619628981465, -0.03420480345154092, -0.21085072062643512, -0.054480051943322734, 0.2869386660334255, -0.34867193144635256, -0.1964956226299927, 0.060902722587343305, -0.33728880242311526, -0.06293683175352358, 0.22442603128729388, -0.073347635256... |
1,712.10145 | Secure Transmission and Self-Energy Recycling for Wireless-Powered Relay
Systems with Partial Eavesdropper Channel State Information | This paper focuses on the secure transmission of wireless-powered relay
systems with imperfect eavesdropper channel state information (ECSI). For
efficient energy transfer and information relaying, a novel two-phase protocol
is proposed, in which the relay operates in full-duplex (FD) mode to achieve
simultaneous wir... | cs.IT math.IT | this paper focuses on the secure transmission of wirelesspowered relay systems with imperfect eavesdropper channel state information ecsi for efficient energy transfer and information relaying a novel twophase protocol is proposed in which the relay operates in fullduplex fd mode to achieve simultaneous wireless power ... | [['this', 'paper', 'focuses', 'on', 'the', 'secure', 'transmission', 'of', 'wirelesspowered', 'relay', 'systems', 'with', 'imperfect', 'eavesdropper', 'channel', 'state', 'information', 'ecsi', 'for', 'efficient', 'energy', 'transfer', 'and', 'information', 'relaying', 'a', 'novel', 'twophase', 'protocol', 'is', 'propo... | [-0.23802670210403246, -0.036622327666027486, -0.04087404600823246, -0.014896546472865806, -0.09132006576013904, -0.3254156954942709, 0.1065496742967479, 0.4000020566808275, -0.29482832382177093, -0.26857458182658805, 0.08125136079836222, -0.25358511127004646, -0.15340687569919084, 0.14627267221782905, -0.1116241450083... |
1,712.10146 | About a variation of local cohomology | Let $\mathfrak{q}$ denote an ideal of a local ring $(A,\mathfrak{m})$. For a
system of elements $\underline{a} = a_1,\ldots,a_t$ such that $a_i \in
\mathfrak{q}^{c_i}, i = 1, \ldots,t,$ and $n \in \mathbb{Z}$ we investigate a
subcomplex resp. a factor complex of the \v{C}ech complex
$\check{C}_{\underline{a}} \otimes... | math.AC | let mathfrakq denote an ideal of a local ring amathfrakm for a system of elements underlinea a_1ldotsa_t such that a_i in mathfrakqc_i i 1 ldotst and n in mathbbz we investigate a subcomplex resp a factor complex of the vcech complex checkc_underlinea otimes_a m for a finitely generated amodule m we start with the insp... | [['let', 'mathfrakq', 'denote', 'an', 'ideal', 'of', 'a', 'local', 'ring', 'amathfrakm', 'for', 'a', 'system', 'of', 'elements', 'underlinea', 'a_1ldotsa_t', 'such', 'that', 'a_i', 'in', 'mathfrakqc_i', 'i', '1', 'ldotst', 'and', 'n', 'in', 'mathbbz', 'we', 'investigate', 'a', 'subcomplex', 'resp', 'a', 'factor', 'comp... | [-0.26257742198303025, 0.06559700661795857, -0.039174371209500874, -0.007155381232262292, 0.0004996581230946678, -0.1536090304639111, -0.04753891047724384, 0.33344193849157777, -0.39856172317361577, -0.15402861751933047, 0.0865086003025855, -0.25216274343906564, -0.134300953552543, 0.1571216095868062, -0.11796505108693... |
1,712.10147 | Controlling cargo trafficking in multicomponent membranes | Biological membranes typically contain a large number of different components
dispersed in small concentrations in the main membrane phase, including
proteins, sugars, and lipids of varying geometrical properties. Most of these
components do not bind the cargo. Here, we show that such `inert' components
can be crucia... | cond-mat.soft | biological membranes typically contain a large number of different components dispersed in small concentrations in the main membrane phase including proteins sugars and lipids of varying geometrical properties most of these components do not bind the cargo here we show that such inert components can be crucial for prec... | [['biological', 'membranes', 'typically', 'contain', 'a', 'large', 'number', 'of', 'different', 'components', 'dispersed', 'in', 'small', 'concentrations', 'in', 'the', 'main', 'membrane', 'phase', 'including', 'proteins', 'sugars', 'and', 'lipids', 'of', 'varying', 'geometrical', 'properties', 'most', 'of', 'these', '... | [-0.09417661367961676, 0.24610086708412607, -0.0009986707447373335, 0.002747025533860531, -0.030187147540399934, -0.1854208363404516, 0.009101736438109097, 0.3957579472554055, -0.2783276055078483, -0.29474625000637944, 0.0358582047369829, -0.23220137113389458, -0.21065038832660654, 0.13638789812045282, -0.1016584472891... |
1,712.10148 | Magnetic field buoyancy in accretion disks of young stars | Buoyancy of the fossil magnetic field in the accretion disks of young stars
is investigated. It is assumed that the Parker instability leads to the
formation of slender flux tubes of toroidal magnetic field in the regions of
effective magnetic field generation. Stationary solution of the induction
equation is written... | astro-ph.SR | buoyancy of the fossil magnetic field in the accretion disks of young stars is investigated it is assumed that the parker instability leads to the formation of slender flux tubes of toroidal magnetic field in the regions of effective magnetic field generation stationary solution of the induction equation is written in ... | [['buoyancy', 'of', 'the', 'fossil', 'magnetic', 'field', 'in', 'the', 'accretion', 'disks', 'of', 'young', 'stars', 'is', 'investigated', 'it', 'is', 'assumed', 'that', 'the', 'parker', 'instability', 'leads', 'to', 'the', 'formation', 'of', 'slender', 'flux', 'tubes', 'of', 'toroidal', 'magnetic', 'field', 'in', 'the... | [-0.16994170853797033, 0.23821605323238, 0.018755082815942417, 0.10221566942179192, -0.07629432961813935, -0.00901863750831032, -0.04139923493338763, 0.3569262682616654, -0.2275941532908562, -0.33245989617728094, 0.04085886746357046, -0.18936950160289995, -0.009449972968392131, 0.20455990241527672, 0.008964025778056101... |
1,712.10149 | Cutoff on Hyperbolic Surfaces | In this paper we study the common distance between points and the behavior of
a constant length step discrete random walk on finite area hyperbolic surfaces.
We show that if the second smallest eigenvalue of the Laplacian is at least
1/4, then the distances on the surface are highly concentrated around the
minimal po... | math.GT | in this paper we study the common distance between points and the behavior of a constant length step discrete random walk on finite area hyperbolic surfaces we show that if the second smallest eigenvalue of the laplacian is at least 14 then the distances on the surface are highly concentrated around the minimal possibl... | [['in', 'this', 'paper', 'we', 'study', 'the', 'common', 'distance', 'between', 'points', 'and', 'the', 'behavior', 'of', 'a', 'constant', 'length', 'step', 'discrete', 'random', 'walk', 'on', 'finite', 'area', 'hyperbolic', 'surfaces', 'we', 'show', 'that', 'if', 'the', 'second', 'smallest', 'eigenvalue', 'of', 'the',... | [-0.12423567404489844, 0.13027296082507217, -0.10797449450098699, 0.08432588302905882, -0.08072099812448986, -0.12374464059548994, 0.08514143830961397, 0.35669384620062283, -0.2661014286801219, -0.29590677926917713, 0.10182131785644039, -0.30409355859212095, -0.17159341749615006, 0.2076055313190145, -0.1037927038426841... |
1,712.1015 | Higher Arithmetic Intersection Theory | We give a new definition of higher arithmetic Chow groups for smooth
projective varieties defined over a number field, which is similar to Gillet
and Soul\'e's definition of arithmetic Chow groups. We also give a compact
description of the intersection theory of such groups. A consequence of this
theory is the defini... | math.AG math.KT math.NT | we give a new definition of higher arithmetic chow groups for smooth projective varieties defined over a number field which is similar to gillet and soules definition of arithmetic chow groups we also give a compact description of the intersection theory of such groups a consequence of this theory is the definition of ... | [['we', 'give', 'a', 'new', 'definition', 'of', 'higher', 'arithmetic', 'chow', 'groups', 'for', 'smooth', 'projective', 'varieties', 'defined', 'over', 'a', 'number', 'field', 'which', 'is', 'similar', 'to', 'gillet', 'and', 'soules', 'definition', 'of', 'arithmetic', 'chow', 'groups', 'we', 'also', 'give', 'a', 'comp... | [-0.24943413254559824, 0.09058545180800649, -0.16946499964647127, 0.12045584784579676, -0.06811556518649715, -0.1299028104056784, 0.025797391034103112, 0.25815244679126825, -0.2729636325598939, -0.23651111233783395, 0.0457945888874268, -0.20133273493653783, -0.16617447459710794, 0.23670832978626877, -0.1684357148570645... |
1,712.10151 | Significance of Softmax-based Features in Comparison to Distance Metric
Learning-based Features | The extraction of useful deep features is important for many computer vision
tasks. Deep features extracted from classification networks have proved to
perform well in those tasks. To obtain features of greater usefulness,
end-to-end distance metric learning (DML) has been applied to train the feature
extractor direc... | cs.CV | the extraction of useful deep features is important for many computer vision tasks deep features extracted from classification networks have proved to perform well in those tasks to obtain features of greater usefulness endtoend distance metric learning dml has been applied to train the feature extractor directly howev... | [['the', 'extraction', 'of', 'useful', 'deep', 'features', 'is', 'important', 'for', 'many', 'computer', 'vision', 'tasks', 'deep', 'features', 'extracted', 'from', 'classification', 'networks', 'have', 'proved', 'to', 'perform', 'well', 'in', 'those', 'tasks', 'to', 'obtain', 'features', 'of', 'greater', 'usefulness',... | [-0.030929185915738344, -0.030783715785351874, -0.10530090494842752, 0.09899842352470396, -0.08369291361326175, -0.17852458860861123, -0.011659083964411903, 0.46270300189617775, -0.2662173067525464, -0.3524711865143184, 0.06627780767276638, -0.309097014748267, -0.1783116937149316, 0.21657199655102063, -0.08557797042503... |
1,712.10152 | Exploring the significance of using perceptually relevant image
decolorization method for scene classification | A color image contains luminance and chrominance components representing the
intensity and color information respectively. The objective of the work
presented in this paper is to show the significance of incorporating the
chrominance information for the task of scene classification. An improved
color-to-grayscale ima... | cs.CV | a color image contains luminance and chrominance components representing the intensity and color information respectively the objective of the work presented in this paper is to show the significance of incorporating the chrominance information for the task of scene classification an improved colortograyscale image con... | [['a', 'color', 'image', 'contains', 'luminance', 'and', 'chrominance', 'components', 'representing', 'the', 'intensity', 'and', 'color', 'information', 'respectively', 'the', 'objective', 'of', 'the', 'work', 'presented', 'in', 'this', 'paper', 'is', 'to', 'show', 'the', 'significance', 'of', 'incorporating', 'the', '... | [-0.005880678540947389, -0.08289521336855567, -0.11294165217387611, 0.044460350623441176, -0.05548994695536136, -0.10021216716072064, 0.002827778218526374, 0.4386463121998418, -0.23553142294895696, -0.35674262807313645, 0.10463306588999001, -0.26275279864166995, -0.18054257586617697, 0.17695308949586022, -0.15592986857... |
1,712.10153 | Nonsymmorphic symmetry protected node-line semimetal in the trigonal YH3 | Using ab initio calculations based on density-functional theory and effective
model analysis, we propose that the trigonal YH3(Space Group: P-3c1) at ambient
pressure is a node-line semimetal when spin-orbit coupling (SOC) is ignored.
This trigonal YH3 has very clean electronic structure near Fermi level and its
noda... | cond-mat.mtrl-sci | using ab initio calculations based on densityfunctional theory and effective model analysis we propose that the trigonal yh3space group p3c1 at ambient pressure is a nodeline semimetal when spinorbit coupling soc is ignored this trigonal yh3 has very clean electronic structure near fermi level and its nodal lines locat... | [['using', 'ab', 'initio', 'calculations', 'based', 'on', 'densityfunctional', 'theory', 'and', 'effective', 'model', 'analysis', 'we', 'propose', 'that', 'the', 'trigonal', 'yh3space', 'group', 'p3c1', 'at', 'ambient', 'pressure', 'is', 'a', 'nodeline', 'semimetal', 'when', 'spinorbit', 'coupling', 'soc', 'is', 'ignor... | [-0.20237363571123707, 0.14545103734687603, -0.06417054301176298, 0.05937692567683934, -0.0642400510072808, -0.17330622437764845, 0.09586933678725645, 0.3670757942744309, -0.23828836528673059, -0.29280810549056957, 0.04006082791023627, -0.289975833580164, -0.138499530124855, 0.14648739190694565, 0.021583947837020136, -... |
1,712.10154 | Superhard and Superconducting B6C | Crystal structure searching and ab initio calculations have been used here to
explore low-energy structures of boron carbides under high pressure. Under
pressures of 85-110 GPa, a metastable B6C with R-3m symmetry is found to be
energetically more stable than the mixture of previous B4C and elemental boron.
This B6C ... | cond-mat.mtrl-sci cond-mat.supr-con | crystal structure searching and ab initio calculations have been used here to explore lowenergy structures of boron carbides under high pressure under pressures of 85110 gpa a metastable b6c with r3m symmetry is found to be energetically more stable than the mixture of previous b4c and elemental boron this b6c is a rho... | [['crystal', 'structure', 'searching', 'and', 'ab', 'initio', 'calculations', 'have', 'been', 'used', 'here', 'to', 'explore', 'lowenergy', 'structures', 'of', 'boron', 'carbides', 'under', 'high', 'pressure', 'under', 'pressures', 'of', '85110', 'gpa', 'a', 'metastable', 'b6c', 'with', 'r3m', 'symmetry', 'is', 'found'... | [-0.12191857868329473, 0.2332905892625318, -0.09452438066314374, -0.05151898777245411, -0.014772966726283941, -0.13204242998268456, 0.13992635659341301, 0.45062596023082735, -0.27355608422841343, -0.3056307925177472, 0.03525899909569749, -0.3021254114593778, -0.0566255834259625, 0.12053498249634036, 0.07593765682008649... |
1,712.10155 | Secret Sharing for Cloud Data Security | Cloud computing helps reduce costs, increase business agility and deploy
solutions with a high return on investment for many types of applications.
However, data security is of premium importance to many users and often
restrains their adoption of cloud technologies. Various approaches, i.e., data
encryption, anonymi... | cs.DB cs.CR | cloud computing helps reduce costs increase business agility and deploy solutions with a high return on investment for many types of applications however data security is of premium importance to many users and often restrains their adoption of cloud technologies various approaches ie data encryption anonymization repl... | [['cloud', 'computing', 'helps', 'reduce', 'costs', 'increase', 'business', 'agility', 'and', 'deploy', 'solutions', 'with', 'a', 'high', 'return', 'on', 'investment', 'for', 'many', 'types', 'of', 'applications', 'however', 'data', 'security', 'is', 'of', 'premium', 'importance', 'to', 'many', 'users', 'and', 'often',... | [-0.18288926569813932, -0.06597078507938595, -0.05245251694901122, 0.0811465332883893, -0.13752070719729764, -0.26293901233778644, 0.14848429053543238, 0.36009493680601873, -0.30655636643253575, -0.3417810722781319, 0.1941120118987143, -0.31105143159921106, -0.050642409879300326, 0.1868766503736239, -0.2004932037980998... |
1,712.10156 | Doppler-free spectroscopy of metastable Sr atoms using a hollow cathode
lamp | We report on the demonstration of Doppler-free spectroscopy of metastable Sr
atoms using a hollow cathode lamp (HCL). We employed a custom Sr HCL which is
filled with a mixture of 0.5-Torr Ne and 0.5-Torr Xe as a buffer gas to
suppress velocity changing collisions and increase the populations in all the
$(5s5p){}^3P_... | physics.atom-ph | we report on the demonstration of dopplerfree spectroscopy of metastable sr atoms using a hollow cathode lamp hcl we employed a custom sr hcl which is filled with a mixture of 05torr ne and 05torr xe as a buffer gas to suppress velocity changing collisions and increase the populations in all the 5s5p3p_jj0 1 2 metastab... | [['we', 'report', 'on', 'the', 'demonstration', 'of', 'dopplerfree', 'spectroscopy', 'of', 'metastable', 'sr', 'atoms', 'using', 'a', 'hollow', 'cathode', 'lamp', 'hcl', 'we', 'employed', 'a', 'custom', 'sr', 'hcl', 'which', 'is', 'filled', 'with', 'a', 'mixture', 'of', '05torr', 'ne', 'and', '05torr', 'xe', 'as', 'a',... | [-0.042813593171814227, 0.18292344090518323, -0.006448753437111049, -0.04017911031005088, 0.06920101573910523, -0.18269911365520752, 0.13012560272296325, 0.44938262062816975, -0.21247519978604626, -0.28333099992171434, 0.013145321256774112, -0.27685657495193267, -0.01619885131465585, 0.11426995270833205, -0.00098714445... |
1,712.10157 | Signed Graph Analysis for the Interpretation of Voting Behavior | In a signed graph, each link is labeled with either a positive or a negative
sign. This is particularly appropriate to model polarized systems. Such a graph
can be characterized through the notion of structural balance, which relies on
the partitioning of the graph into internally solidary but mutually hostile
subgro... | cs.SI cs.CY physics.soc-ph | in a signed graph each link is labeled with either a positive or a negative sign this is particularly appropriate to model polarized systems such a graph can be characterized through the notion of structural balance which relies on the partitioning of the graph into internally solidary but mutually hostile subgroups in... | [['in', 'a', 'signed', 'graph', 'each', 'link', 'is', 'labeled', 'with', 'either', 'a', 'positive', 'or', 'a', 'negative', 'sign', 'this', 'is', 'particularly', 'appropriate', 'to', 'model', 'polarized', 'systems', 'such', 'a', 'graph', 'can', 'be', 'characterized', 'through', 'the', 'notion', 'of', 'structural', 'bala... | [-0.12378140557120787, 0.09349511557957157, -0.12344730979627154, 0.08965157750450696, -0.1431035142741166, -0.14183860743651167, 0.077162667272205, 0.4041424874449149, -0.30689977803558577, -0.32097167989316705, 0.10730841191495226, -0.28118393029581057, -0.17666764653646774, 0.13483074092800962, -0.09866262079352357,... |
1,712.10158 | Non-linear motor control by local learning in spiking neural networks | Learning weights in a spiking neural network with hidden neurons, using
local, stable and online rules, to control non-linear body dynamics is an open
problem. Here, we employ a supervised scheme, Feedback-based Online Local
Learning Of Weights (FOLLOW), to train a network of heterogeneous spiking
neurons with hidden... | q-bio.NC cs.LG cs.NE cs.SY stat.ML | learning weights in a spiking neural network with hidden neurons using local stable and online rules to control nonlinear body dynamics is an open problem here we employ a supervised scheme feedbackbased online local learning of weights follow to train a network of heterogeneous spiking neurons with hidden layers to co... | [['learning', 'weights', 'in', 'a', 'spiking', 'neural', 'network', 'with', 'hidden', 'neurons', 'using', 'local', 'stable', 'and', 'online', 'rules', 'to', 'control', 'nonlinear', 'body', 'dynamics', 'is', 'an', 'open', 'problem', 'here', 'we', 'employ', 'a', 'supervised', 'scheme', 'feedbackbased', 'online', 'local',... | [-0.08065403209536508, 0.04307962669475615, -0.06484702199839862, 0.052727572659955944, -0.1411177746975308, -0.259875488817502, 0.08755866458764075, 0.46368762500773947, -0.3690365183517147, -0.2582154735910949, 0.03300043117628688, -0.21410582935627384, -0.2625407407942742, 0.14030926137759236, -0.10974836599446572, ... |
1,712.10159 | About reaction-diffusion systems involving the Holling-type II and the
Beddington-DeAngelis functional responses for predator-prey models | We consider in this paper a microscopic model (that is, a system of three
reaction-diffusion equations) incorporating the dynamics of handling and
searching predators, and show that its solutions converge when a small
parameter tends to $0$ towards the solutions of a reaction-cross diffusion
system of predator-prey t... | math.AP | we consider in this paper a microscopic model that is a system of three reactiondiffusion equations incorporating the dynamics of handling and searching predators and show that its solutions converge when a small parameter tends to 0 towards the solutions of a reactioncross diffusion system of predatorprey type involvi... | [['we', 'consider', 'in', 'this', 'paper', 'a', 'microscopic', 'model', 'that', 'is', 'a', 'system', 'of', 'three', 'reactiondiffusion', 'equations', 'incorporating', 'the', 'dynamics', 'of', 'handling', 'and', 'searching', 'predators', 'and', 'show', 'that', 'its', 'solutions', 'converge', 'when', 'a', 'small', 'param... | [-0.13576013733108994, 0.07402523855368297, -0.06227509559054548, 0.052350069404686415, -0.045212864701170474, -0.152917017810978, 0.017672025170516765, 0.2541947610346445, -0.2994029721788441, -0.21590160308793807, 0.12552159759995143, -0.29957916812660795, -0.190714795118159, 0.13673123561511602, -0.00640162053296459... |
1,712.1016 | Characterizing Moonshine Functions by Vertex-Operator-Algebraic
Conditions | Given a holomorphic $C_2$-cofinite vertex operator algebra $V$ with graded
dimension $j-744$, Borcherds's proof of the monstrous moonshine conjecture
implies any finite order automorphism of $V$ has graded trace given by a
"completely replicable function", and by work of Cummins and Gannon, these
functions are princi... | math.RT math.NT math.QA | given a holomorphic c_2cofinite vertex operator algebra v with graded dimension j744 borcherdss proof of the monstrous moonshine conjecture implies any finite order automorphism of v has graded trace given by a completely replicable function and by work of cummins and gannon these functions are principal moduli of genu... | [['given', 'a', 'holomorphic', 'c_2cofinite', 'vertex', 'operator', 'algebra', 'v', 'with', 'graded', 'dimension', 'j744', 'borcherdss', 'proof', 'of', 'the', 'monstrous', 'moonshine', 'conjecture', 'implies', 'any', 'finite', 'order', 'automorphism', 'of', 'v', 'has', 'graded', 'trace', 'given', 'by', 'a', 'completely... | [-0.16663567961326667, 0.10165818864070289, -0.09096034511841916, 0.058077859661572584, -0.1698412905999838, -0.16087679230034924, -0.029762256296945143, 0.3467824430829221, -0.3387560722581878, -0.19759652741089628, 0.0971881064770559, -0.28026934269723575, -0.2100101197343115, 0.18345507168835337, -0.1104908875947060... |
1,712.10161 | On the anomalously large extension of the Pulsar Wind Nebula HESS
J1825-137 | The very high energy (VHE) gamma-ray emission reported from a number of
pulsar wind nebulae (PWNe) is naturally explained by the inverse Compton
scattering of multi-TeV electrons. However, the physical dimensions of some
gamma-ray-emitting PWNe significantly exceed the scales anticipated by the
standard hydrodynamica... | astro-ph.HE | the very high energy vhe gammaray emission reported from a number of pulsar wind nebulae pwne is naturally explained by the inverse compton scattering of multitev electrons however the physical dimensions of some gammarayemitting pwne significantly exceed the scales anticipated by the standard hydrodynamical paradigm o... | [['the', 'very', 'high', 'energy', 'vhe', 'gammaray', 'emission', 'reported', 'from', 'a', 'number', 'of', 'pulsar', 'wind', 'nebulae', 'pwne', 'is', 'naturally', 'explained', 'by', 'the', 'inverse', 'compton', 'scattering', 'of', 'multitev', 'electrons', 'however', 'the', 'physical', 'dimensions', 'of', 'some', 'gamma... | [-0.11204290353369745, 0.16439709740868574, -0.04326256804794133, 0.11457090144024913, -0.10185552649162258, -0.06020953694381091, 0.010770388983985643, 0.3919083754228511, -0.2319503317776547, -0.3239135568328051, 0.05181494053605914, -0.23397044344477144, -0.01650666652101437, 0.20932368557100836, -0.0249918364473856... |
1,712.10162 | Resonant pinning spectroscopy with spin-vortex pairs | Vortex pairs in magnetic nanopillars with strongly coupled cores and pinning
of one of the cores by a morphological defect, are used to perform resonant
pinning spectroscopy, in which a microwave excitation applied to the nanopillar
produces pinning or depinning of the cores only when the excitation is in
resonance w... | cond-mat.mes-hall | vortex pairs in magnetic nanopillars with strongly coupled cores and pinning of one of the cores by a morphological defect are used to perform resonant pinning spectroscopy in which a microwave excitation applied to the nanopillar produces pinning or depinning of the cores only when the excitation is in resonance with ... | [['vortex', 'pairs', 'in', 'magnetic', 'nanopillars', 'with', 'strongly', 'coupled', 'cores', 'and', 'pinning', 'of', 'one', 'of', 'the', 'cores', 'by', 'a', 'morphological', 'defect', 'are', 'used', 'to', 'perform', 'resonant', 'pinning', 'spectroscopy', 'in', 'which', 'a', 'microwave', 'excitation', 'applied', 'to', ... | [-0.15327161209416204, 0.2024962642699256, -0.04962693297836397, 0.03391174475060202, -0.050586889644986706, -0.14169523587688468, 0.04708390451680617, 0.4175694231434088, -0.2581042243006702, -0.2867021136602065, 0.02184376322149642, -0.250248425199013, -0.07316057018837646, 0.1956714667358849, 0.07160918062720868, 0.... |
1,712.10163 | Estimation under group actions: recovering orbits from invariants | We study a class of orbit recovery problems in which we observe independent
copies of an unknown element of $\mathbb{R}^p$, each linearly acted upon by a
random element of some group (such as $\mathbb{Z}/p$ or $\mathrm{SO}(3)$) and
then corrupted by additive Gaussian noise. We prove matching upper and lower
bounds on... | math.ST cs.DS cs.IT math.AC math.IT stat.TH | we study a class of orbit recovery problems in which we observe independent copies of an unknown element of mathbbrp each linearly acted upon by a random element of some group such as mathbbzp or mathrmso3 and then corrupted by additive gaussian noise we prove matching upper and lower bounds on the number of samples re... | [['we', 'study', 'a', 'class', 'of', 'orbit', 'recovery', 'problems', 'in', 'which', 'we', 'observe', 'independent', 'copies', 'of', 'an', 'unknown', 'element', 'of', 'mathbbrp', 'each', 'linearly', 'acted', 'upon', 'by', 'a', 'random', 'element', 'of', 'some', 'group', 'such', 'as', 'mathbbzp', 'or', 'mathrmso3', 'and... | [-0.08194321309394367, 0.059239066209671995, -0.08053189145224127, 0.05060169059779006, -0.056741192888434794, -0.14089234488198693, 0.054863655578073246, 0.3845104841279431, -0.3072144576736591, -0.3382822117237248, 0.12219618945761807, -0.2497548872765103, -0.178607636352588, 0.21638841160080013, -0.1201993703644099,... |
1,712.10164 | Polyp detection inside the capsule endoscopy: an approach for power
consumption reduction | Capsule endoscopy is a novel and non-invasive method for diagnosis, which
assists gastroenterologists to monitor the digestive track. Although this new
technology has many advantages over the conventional endoscopy, there are
weaknesses that limits the usage of this technology. Some weaknesses are due to
using small-... | eess.IV cs.CV | capsule endoscopy is a novel and noninvasive method for diagnosis which assists gastroenterologists to monitor the digestive track although this new technology has many advantages over the conventional endoscopy there are weaknesses that limits the usage of this technology some weaknesses are due to using smallsize bat... | [['capsule', 'endoscopy', 'is', 'a', 'novel', 'and', 'noninvasive', 'method', 'for', 'diagnosis', 'which', 'assists', 'gastroenterologists', 'to', 'monitor', 'the', 'digestive', 'track', 'although', 'this', 'new', 'technology', 'has', 'many', 'advantages', 'over', 'the', 'conventional', 'endoscopy', 'there', 'are', 'we... | [-0.10100739677387112, 0.020509627989513127, -0.0473356371766521, -0.007427967217889555, -0.10749382934869921, -0.16942216907479266, 0.04167699901773495, 0.41004897354844405, -0.24587536340163269, -0.3267241281635584, 0.10518164400685023, -0.2567450061782283, -0.14973893740209454, 0.23317006822710143, -0.15754613601305... |
1,712.10165 | SUSY (ATLAS) | During the LHC Run-II data-taking period, several searches for supersymmetric
particles were performed by the ATLAS collaboration. The results from these
searches are concisely reviewed. Model-independent and model-dependent limits
on new particle production are set, and interpretations in supersymmetric
models are g... | hep-ph | during the lhc runii datataking period several searches for supersymmetric particles were performed by the atlas collaboration the results from these searches are concisely reviewed modelindependent and modeldependent limits on new particle production are set and interpretations in supersymmetric models are given | [['during', 'the', 'lhc', 'runii', 'datataking', 'period', 'several', 'searches', 'for', 'supersymmetric', 'particles', 'were', 'performed', 'by', 'the', 'atlas', 'collaboration', 'the', 'results', 'from', 'these', 'searches', 'are', 'concisely', 'reviewed', 'modelindependent', 'and', 'modeldependent', 'limits', 'on', ... | [-0.007271303479293627, 0.2822419980740441, -0.06630773234757639, 0.14243271428027324, -0.07914343434164212, -0.15650991946347945, -0.017677814034479006, 0.33156004964950536, -0.13869728442902365, -0.3731601041342531, 0.13972916505909302, -0.3687987955719499, 0.008077088832145645, 0.2569458344202888, 0.0383532859739803... |
1,712.10166 | On interstellar light polarization by diamagnetic silicate and carbon
dust in the infrared | The motion of diamagnetic dust particles in interstellar magnetic fields is
studied numerically with several different sets of parameters. Two types of
behavior are observed, depending on the value of the critical number $R$, which
is a function of the grain inertia, the magnetic susceptibility of the material
and of... | astro-ph.GA | the motion of diamagnetic dust particles in interstellar magnetic fields is studied numerically with several different sets of parameters two types of behavior are observed depending on the value of the critical number r which is a function of the grain inertia the magnetic susceptibility of the material and of the str... | [['the', 'motion', 'of', 'diamagnetic', 'dust', 'particles', 'in', 'interstellar', 'magnetic', 'fields', 'is', 'studied', 'numerically', 'with', 'several', 'different', 'sets', 'of', 'parameters', 'two', 'types', 'of', 'behavior', 'are', 'observed', 'depending', 'on', 'the', 'value', 'of', 'the', 'critical', 'number', ... | [-0.12358468221598436, 0.18554335250118018, -0.05580171438752212, 0.03428427573014921, -0.05308988363107788, -0.085796701731367, 0.002838592309391596, 0.40283168258284713, -0.2594201942322619, -0.32092042105646684, 0.07289135919570505, -0.2705274378297694, -0.0766721547126474, 0.18349424438337822, -0.03169900243071178,... |
1,712.10167 | Simple cubic graphs with no short traveling salesman tour | Let $tsp(G)$ denote the length of a shortest travelling salesman tour in a
graph $G$. We prove that for any $\varepsilon>0$, there exists a simple
$2$-connected planar cubic graph $G_1$ such that $tsp(G_1)\ge
(1.25-\varepsilon)\cdot|V(G_1)|$, a simple $2$-connected bipartite cubic graph
$G_2$ such that $tsp(G_2)\ge (... | cs.DM | let tspg denote the length of a shortest travelling salesman tour in a graph g we prove that for any varepsilon0 there exists a simple 2connected planar cubic graph g_1 such that tspg_1ge 125varepsiloncdotvg_1 a simple 2connected bipartite cubic graph g_2 such that tspg_2ge 12varepsiloncdotvg_2 and a simple 3connected ... | [['let', 'tspg', 'denote', 'the', 'length', 'of', 'a', 'shortest', 'travelling', 'salesman', 'tour', 'in', 'a', 'graph', 'g', 'we', 'prove', 'that', 'for', 'any', 'varepsilon0', 'there', 'exists', 'a', 'simple', '2connected', 'planar', 'cubic', 'graph', 'g_1', 'such', 'that', 'tspg_1ge', '125varepsiloncdotvg_1', 'a', '... | [-0.31282184596116447, 0.1333434299508832, -0.03663069665508003, 0.022088010472302536, -0.23060772780861175, -0.22978641848288933, -0.0002588081477704097, 0.46800136718214774, -0.284305766186848, -0.2460238565975914, 0.01901405265469256, -0.34046294585782655, -0.25183982301351365, 0.12188357437903784, -0.05434630051901... |
1,712.10168 | Can winds driven by active galactic nuclei account for the extragalactic
gamma-ray and neutrino backgrounds? | Various observations are revealing the widespread occurrence of fast and
powerful winds in active galactic nuclei (AGNs) that are distinct from
relativistic jets, likely launched from accretion disks and interacting
strongly with the gas of their host galaxies. During the interaction, strong
shocks are expected to fo... | astro-ph.HE | various observations are revealing the widespread occurrence of fast and powerful winds in active galactic nuclei agns that are distinct from relativistic jets likely launched from accretion disks and interacting strongly with the gas of their host galaxies during the interaction strong shocks are expected to form that... | [['various', 'observations', 'are', 'revealing', 'the', 'widespread', 'occurrence', 'of', 'fast', 'and', 'powerful', 'winds', 'in', 'active', 'galactic', 'nuclei', 'agns', 'that', 'are', 'distinct', 'from', 'relativistic', 'jets', 'likely', 'launched', 'from', 'accretion', 'disks', 'and', 'interacting', 'strongly', 'wi... | [-0.04948135088094022, 0.2411428983842601, -0.023636862178606614, 0.20954904156619317, -0.07564953915328203, -0.0713159084185044, 0.010401394072795446, 0.4097194682424161, -0.1984849834864869, -0.3551660541472714, 0.025236489882235688, -0.3131071188518272, 0.0015037498544195327, 0.22811194716045655, 0.04336229649105812... |
1,712.10169 | Boundary-induced inhomogeneity of particle layers in the solidification
of suspensions | When a suspension freezes, a compacted particle layer builds up at the
solidification front with noticeable implications on the freezing process. In a
directional solidification experiment of monodispersed suspensions in thin
samples, we evidence a link between the thickness of this layer and the sample
depth. We att... | cond-mat.soft cond-mat.mtrl-sci | when a suspension freezes a compacted particle layer builds up at the solidification front with noticeable implications on the freezing process in a directional solidification experiment of monodispersed suspensions in thin samples we evidence a link between the thickness of this layer and the sample depth we attribute... | [['when', 'a', 'suspension', 'freezes', 'a', 'compacted', 'particle', 'layer', 'builds', 'up', 'at', 'the', 'solidification', 'front', 'with', 'noticeable', 'implications', 'on', 'the', 'freezing', 'process', 'in', 'a', 'directional', 'solidification', 'experiment', 'of', 'monodispersed', 'suspensions', 'in', 'thin', '... | [-0.0637965881246024, 0.17051610433759698, -0.1253645624080017, -0.01426671879502285, -0.056489791091479044, -0.07206375145314026, 0.06585465674124606, 0.3900642732000897, -0.2645750891640258, -0.34239215868021833, 0.05745585117830147, -0.2937008078196939, -0.08749329478076773, 0.15998719651317617, -0.03833150125148011... |
1,712.1017 | Revisiting an approximation in the Wilson G-matrix formalism and its
impact on molecular quantum dynamics | Quantum dynamics simulations of reactive molecular processes are commonly
performed in a low-dimensional space spanned by highly optimized reactive
coordinates. Usually, these sets of reactive coordinates consist of non-linear
coordinates. The Wilson G-matrix formalism allows to formulate the Hamiltonian
in arbitrary... | physics.chem-ph | quantum dynamics simulations of reactive molecular processes are commonly performed in a lowdimensional space spanned by highly optimized reactive coordinates usually these sets of reactive coordinates consist of nonlinear coordinates the wilson gmatrix formalism allows to formulate the hamiltonian in arbitrary coordin... | [['quantum', 'dynamics', 'simulations', 'of', 'reactive', 'molecular', 'processes', 'are', 'commonly', 'performed', 'in', 'a', 'lowdimensional', 'space', 'spanned', 'by', 'highly', 'optimized', 'reactive', 'coordinates', 'usually', 'these', 'sets', 'of', 'reactive', 'coordinates', 'consist', 'of', 'nonlinear', 'coordin... | [-0.14831982876291905, 0.07683122220707404, -0.08526483569936506, 0.05155750379721024, -0.010914892664757269, -0.1074319432339706, 0.02766084542829843, 0.39143672422773534, -0.26976682569553284, -0.24439946590954886, 0.02604560271419328, -0.21170870158784547, -0.2136975637016197, 0.16593627747276735, -0.035789038581859... |
1,712.10171 | Characterization of individual layers in a bilayer electron system
produced in a wide quantum well | Here we report on a transparent method to characterize individual layers in a
double-layer electron system which forms in a wide quantum well and to
determine their electron densities. The technique relies on the simultaneous
measurement of the capacitances between the electron system and gates located
on either side... | cond-mat.mes-hall | here we report on a transparent method to characterize individual layers in a doublelayer electron system which forms in a wide quantum well and to determine their electron densities the technique relies on the simultaneous measurement of the capacitances between the electron system and gates located on either side of ... | [['here', 'we', 'report', 'on', 'a', 'transparent', 'method', 'to', 'characterize', 'individual', 'layers', 'in', 'a', 'doublelayer', 'electron', 'system', 'which', 'forms', 'in', 'a', 'wide', 'quantum', 'well', 'and', 'to', 'determine', 'their', 'electron', 'densities', 'the', 'technique', 'relies', 'on', 'the', 'simu... | [-0.12280141976054595, 0.1400202657188461, -0.03536395888409654, 0.05166852620491029, 0.0008155182044467201, -0.14887636997939452, 0.09068266851827503, 0.35735031901656283, -0.27899877936376827, -0.3518527951091528, 0.03727997304648971, -0.2830775894548582, -0.09813849182860197, 0.2161894913762808, 0.001321339526254198... |
1,712.10172 | Primal dual mixed finite element methods for the elliptic Cauchy problem | We consider primal-dual mixed finite element methods for the solution of the
elliptic Cauchy problem, or other related data assimilation problems. The
method has a local conservation property. We derive a priori error estimates
using known conditional stability estimates and determine the minimal amount of
weakly con... | math.NA | we consider primaldual mixed finite element methods for the solution of the elliptic cauchy problem or other related data assimilation problems the method has a local conservation property we derive a priori error estimates using known conditional stability estimates and determine the minimal amount of weakly consisten... | [['we', 'consider', 'primaldual', 'mixed', 'finite', 'element', 'methods', 'for', 'the', 'solution', 'of', 'the', 'elliptic', 'cauchy', 'problem', 'or', 'other', 'related', 'data', 'assimilation', 'problems', 'the', 'method', 'has', 'a', 'local', 'conservation', 'property', 'we', 'derive', 'a', 'priori', 'error', 'esti... | [-0.07133002047221242, 0.02346212056270519, -0.10496042310097796, 0.07996049108522468, -0.08336159508935241, -0.15172532446368403, 0.0172349309303722, 0.3198684352791197, -0.29894396644166865, -0.29268248380313433, 0.18966013798084067, -0.2500198331951207, -0.12057954687652243, 0.20197061588310875, -0.12283596838689084... |
1,712.10173 | Diffusion-approximation for a kinetic equation with perturbed velocity
redistribution process | We derive the hydrodynamic limit of a kinetic equation with a stochastic,
short range perturbation of the velocity operator. Under some mixing hypotheses
on the stochastic perturbation, we establish a diffusion-approximation result:
the limit we obtain is a parabolic stochastic partial differential equation on
the ma... | math.AP math.PR | we derive the hydrodynamic limit of a kinetic equation with a stochastic short range perturbation of the velocity operator under some mixing hypotheses on the stochastic perturbation we establish a diffusionapproximation result the limit we obtain is a parabolic stochastic partial differential equation on the macroscop... | [['we', 'derive', 'the', 'hydrodynamic', 'limit', 'of', 'a', 'kinetic', 'equation', 'with', 'a', 'stochastic', 'short', 'range', 'perturbation', 'of', 'the', 'velocity', 'operator', 'under', 'some', 'mixing', 'hypotheses', 'on', 'the', 'stochastic', 'perturbation', 'we', 'establish', 'a', 'diffusionapproximation', 'res... | [-0.1795556224046313, 0.09173131215253047, -0.12560215915496253, 0.08583566351860229, -0.08538119952973662, -0.04764760357840937, 0.03047186531582657, 0.24135007479285098, -0.31703679496897574, -0.23025589413484748, 0.11428863164607664, -0.2566435526942416, -0.11749020880278276, 0.1587129167271588, -0.01329047017141568... |
1,712.10174 | From colossal to zero: Controlling the Anomalous Hall Effect in Magnetic
Heusler Compounds via Berry Curvature Design | Since the discovery of the anomalous Hall effect (AHE), the anomalous Hall
conductivity (AHC) has been thought to be zero when there is no net
magnetization. However, the recently found relation between the intrinsic AHE
and the Berry curvature predicts other possibilities, such as a large AHC in
non-colinear antifer... | cond-mat.mtrl-sci | since the discovery of the anomalous hall effect ahe the anomalous hall conductivity ahc has been thought to be zero when there is no net magnetization however the recently found relation between the intrinsic ahe and the berry curvature predicts other possibilities such as a large ahc in noncolinear antiferromagnets w... | [['since', 'the', 'discovery', 'of', 'the', 'anomalous', 'hall', 'effect', 'ahe', 'the', 'anomalous', 'hall', 'conductivity', 'ahc', 'has', 'been', 'thought', 'to', 'be', 'zero', 'when', 'there', 'is', 'no', 'net', 'magnetization', 'however', 'the', 'recently', 'found', 'relation', 'between', 'the', 'intrinsic', 'ahe',... | [-0.16600843496426138, 0.24198747573420773, -0.06758599109723692, 0.017780736409263285, -0.12428367082759019, -0.15127652701980707, 0.048360021479864006, 0.37618629894914885, -0.32321463909023734, -0.3123385540940622, 0.04264945418520866, -0.30658475212941444, -0.1548760524550099, 0.19742844013285032, -0.01451506099923... |
1,712.10175 | Deflection of light by black holes and massless wormholes in massive
gravity | Weak gravitational lensing by black holes and wormholes in the context of
massive gravity (Bebronne and Tinyakov 2009) theory is studied. The particular
solution examined is characterized by two integration constants, the mass $M$
and an extra parameter $S$ namely `scalar charge'. These black hole reduce to
the stand... | gr-qc | weak gravitational lensing by black holes and wormholes in the context of massive gravity bebronne and tinyakov 2009 theory is studied the particular solution examined is characterized by two integration constants the mass m and an extra parameter s namely scalar charge these black hole reduce to the standard schwarzsc... | [['weak', 'gravitational', 'lensing', 'by', 'black', 'holes', 'and', 'wormholes', 'in', 'the', 'context', 'of', 'massive', 'gravity', 'bebronne', 'and', 'tinyakov', '2009', 'theory', 'is', 'studied', 'the', 'particular', 'solution', 'examined', 'is', 'characterized', 'by', 'two', 'integration', 'constants', 'the', 'mas... | [-0.1738839883591264, 0.09847405660225668, -0.03851641666630439, 0.10392444829796005, -0.07479230602836154, -0.15342173887774568, 0.0004034911040354318, 0.30045928194972094, -0.19366973962891718, -0.3033318803255708, 0.07460713020601571, -0.2914653244288409, -0.11772208951019081, 0.17882550055083127, -0.046535577770698... |
1,712.10176 | Study of the ${X^\pm(5568)}$ state with semileptonic decays of the
${B_s^0}$ meson | We present a study of the $X^\pm(5568)$ using semileptonic decays of the
$B_s^0$ meson using the full Run II integrated luminosity of 10.4 fb$^{-1}$ in
proton-antiproton collisions at a center of mass energy of 1.96\,TeV collected
with the D0 detector at the Fermilab Tevatron Collider. We report evidence for
a narrow... | hep-ex | we present a study of the xpm5568 using semileptonic decays of the b_s0 meson using the full run ii integrated luminosity of 104 fb1 in protonantiproton collisions at a center of mass energy of 196tev collected with the d0 detector at the fermilab tevatron collider we report evidence for a narrow structure xpm5568 in t... | [['we', 'present', 'a', 'study', 'of', 'the', 'xpm5568', 'using', 'semileptonic', 'decays', 'of', 'the', 'b_s0', 'meson', 'using', 'the', 'full', 'run', 'ii', 'integrated', 'luminosity', 'of', '104', 'fb1', 'in', 'protonantiproton', 'collisions', 'at', 'a', 'center', 'of', 'mass', 'energy', 'of', '196tev', 'collected',... | [-0.05518537403002162, 0.2214062529759865, -0.08145751383306239, 0.07189093097386991, -0.009543990141109508, -0.10420482745051712, 0.037174459962818006, 0.25612567778786316, -0.16450199717505978, -0.24759806023554548, -0.04934357558223008, -0.4232726203387274, 0.1771027882282129, 0.1342114172944361, 0.11141885187124204... |
1,712.10177 | Cosmological production of black holes: a way to constrain alternative
theories of gravity | Primordial black holes are considered to be pair created quantum-mechanically
during inflation. In the context of General Relativity (GR), it has been shown
that the pair creation rate is exponentially decreasing during inflation.
Specifically, tiny black holes are favored in the early universe, but they can
grow wit... | gr-qc | primordial black holes are considered to be pair created quantummechanically during inflation in the context of general relativity gr it has been shown that the pair creation rate is exponentially decreasing during inflation specifically tiny black holes are favored in the early universe but they can grow with the hori... | [['primordial', 'black', 'holes', 'are', 'considered', 'to', 'be', 'pair', 'created', 'quantummechanically', 'during', 'inflation', 'in', 'the', 'context', 'of', 'general', 'relativity', 'gr', 'it', 'has', 'been', 'shown', 'that', 'the', 'pair', 'creation', 'rate', 'is', 'exponentially', 'decreasing', 'during', 'inflat... | [-0.1315303006205509, 0.16225371739293745, -0.11596918269845374, 0.14911682383952599, -0.07453564074403199, -0.15708664843545744, -0.011209177203853143, 0.32305565171644846, -0.17748924648111916, -0.29514117953053604, 0.10864168574727465, -0.24829950186246064, -0.11571991437355454, 0.17974801419506875, -0.0722124698359... |
1,712.10178 | Common Slots of Bilinear and Quadratic Pfister Forms | We show that over any field $F$ of $\operatorname{char}(F)=2$ and 2-rank $n$,
there exist $2^n$ bilinear $n$-fold Pfister forms that have no slot in common.
This answers a question of Becher's in the negative. We provide an analogous
result also for quadratic Pfister forms.
| math.AC | we show that over any field f of operatornamecharf2 and 2rank n there exist 2n bilinear nfold pfister forms that have no slot in common this answers a question of bechers in the negative we provide an analogous result also for quadratic pfister forms | [['we', 'show', 'that', 'over', 'any', 'field', 'f', 'of', 'operatornamecharf2', 'and', '2rank', 'n', 'there', 'exist', '2n', 'bilinear', 'nfold', 'pfister', 'forms', 'that', 'have', 'no', 'slot', 'in', 'common', 'this', 'answers', 'a', 'question', 'of', 'bechers', 'in', 'the', 'negative', 'we', 'provide', 'an', 'analo... | [-0.2360274788901903, 0.08991698878796955, -0.048469860626514566, 0.05607394597677211, -0.06298894682076088, -0.17356969791919338, 0.02091862794098466, 0.36789168010270873, -0.24971739211401275, -0.22430297318672718, 0.02910036584470681, -0.2542557774198263, -0.24792147753218752, 0.21850528511040043, -0.047188896317641... |
1,712.10179 | RedDwarfData: a simplified dataset of StarCraft matches | The game Starcraft is one of the most interesting arenas to test new machine
learning and computational intelligence techniques; however, StarCraft matches
take a long time and creating a good dataset for training can be hard. Besides,
analyzing match logs to extract the main characteristics can also be done in
many ... | cs.AI | the game starcraft is one of the most interesting arenas to test new machine learning and computational intelligence techniques however starcraft matches take a long time and creating a good dataset for training can be hard besides analyzing match logs to extract the main characteristics can also be done in many differ... | [['the', 'game', 'starcraft', 'is', 'one', 'of', 'the', 'most', 'interesting', 'arenas', 'to', 'test', 'new', 'machine', 'learning', 'and', 'computational', 'intelligence', 'techniques', 'however', 'starcraft', 'matches', 'take', 'a', 'long', 'time', 'and', 'creating', 'a', 'good', 'dataset', 'for', 'training', 'can', ... | [-0.05696165463221925, 0.04553552027812527, -0.13991117315433388, 0.08548441746554869, -0.14045495909272826, -0.17000495168779578, 0.04782106354084265, 0.4050456197932363, -0.261720891886424, -0.3655429967279945, 0.11930570373744039, -0.2929823905595445, -0.10896212784906051, 0.24217421754729002, -0.12279330921758498, ... |
1,712.1018 | Strong decays of the higher isovector scalar mesons | Under the assignment of $a_0(1450)$ as the ground isovector scalar meson, the
strong decays of $a_0(1950)$ and $a_0(2020)$ are evaluated in the $^3P_0$
model. Our calculations suggest that $a_0(1950)$ and $a_0(2020)$ can be
regarded as the same resonance referring to $a_0(3^3P_0)$. The masses and
strong decays of $a_... | hep-ph hep-ex | under the assignment of a_01450 as the ground isovector scalar meson the strong decays of a_01950 and a_02020 are evaluated in the 3p_0 model our calculations suggest that a_01950 and a_02020 can be regarded as the same resonance referring to a_033p_0 the masses and strong decays of a_023p_0 and a_043p_0 are also predi... | [['under', 'the', 'assignment', 'of', 'a_01450', 'as', 'the', 'ground', 'isovector', 'scalar', 'meson', 'the', 'strong', 'decays', 'of', 'a_01950', 'and', 'a_02020', 'are', 'evaluated', 'in', 'the', '3p_0', 'model', 'our', 'calculations', 'suggest', 'that', 'a_01950', 'and', 'a_02020', 'can', 'be', 'regarded', 'as', 't... | [-0.05505039573218378, 0.23308235962712576, -0.0721959617166292, 0.1556948417805076, -0.04357899398735118, -0.1448678687392246, 0.021923978107109193, 0.34209839609407244, -0.1836988055516803, -0.24336108539460433, 0.017786361729829676, -0.27871263133628027, -0.048431092784518286, 0.13587281739501844, 0.1108215033032354... |
1,712.10181 | Symplectic slice for subgroup actions | Given a symplectic manifold $(M,\omega)$ endowed with a proper Hamiltonian
action of a Lie group $G$, we consider the action induced by a Lie subgroup $H$
of $G$. We propose a construction for two compatible Witt-Artin decompositions
of the tangent space of $M$, one relative to the $G$-action and one relative to
the ... | math.SG | given a symplectic manifold momega endowed with a proper hamiltonian action of a lie group g we consider the action induced by a lie subgroup h of g we propose a construction for two compatible wittartin decompositions of the tangent space of m one relative to the gaction and one relative to the haction in particular w... | [['given', 'a', 'symplectic', 'manifold', 'momega', 'endowed', 'with', 'a', 'proper', 'hamiltonian', 'action', 'of', 'a', 'lie', 'group', 'g', 'we', 'consider', 'the', 'action', 'induced', 'by', 'a', 'lie', 'subgroup', 'h', 'of', 'g', 'we', 'propose', 'a', 'construction', 'for', 'two', 'compatible', 'wittartin', 'decom... | [-0.2509993904771713, 0.07951425065559586, -0.08528545365597193, 0.026802789154820716, -0.15277072335951603, -0.10327455619923197, 0.0233717540708872, 0.4245338151088128, -0.29704481604007577, -0.2529640282719181, 0.053814936355830956, -0.2038799217902124, -0.12220600104102722, 0.1548690222741033, -0.14284840588672804,... |
1,712.10182 | Critical Emission from a High-Spin Black Hole | We consider a rapidly spinning black hole surrounded by an equatorial,
geometrically thin, slowly accreting disk that is stationary and axisymmetric.
We analytically compute the broadening of electromagnetic line emissions from
the innermost part of the disk, which resides in the near-horizon region. The
result is in... | gr-qc astro-ph.HE hep-th | we consider a rapidly spinning black hole surrounded by an equatorial geometrically thin slowly accreting disk that is stationary and axisymmetric we analytically compute the broadening of electromagnetic line emissions from the innermost part of the disk which resides in the nearhorizon region the result is independen... | [['we', 'consider', 'a', 'rapidly', 'spinning', 'black', 'hole', 'surrounded', 'by', 'an', 'equatorial', 'geometrically', 'thin', 'slowly', 'accreting', 'disk', 'that', 'is', 'stationary', 'and', 'axisymmetric', 'we', 'analytically', 'compute', 'the', 'broadening', 'of', 'electromagnetic', 'line', 'emissions', 'from', ... | [-0.14229868878036328, 0.15036079199858687, -0.0383773925777984, 0.05051911275113027, -0.08810949496516626, -0.06651806613838632, -0.0223318129803424, 0.3593954792603442, -0.20650673290229823, -0.2624679966829717, 0.1367051031485149, -0.2922773498783449, -0.07053451887204325, 0.2228259376205555, -0.038823565510053774, ... |
1,712.10183 | Nonlinear Opinion Dynamics in Systems with Leadership Effect | Opinion dynamics of a group of individuals is the change in the members'
opinions through mutual interaction with each other. The related literature
contains works in which the dynamics is modeled as a continuous system, of
which behavioral patterns are analyzed in regard to the parameters contained in
the system. Th... | math.DS nlin.AO | opinion dynamics of a group of individuals is the change in the members opinions through mutual interaction with each other the related literature contains works in which the dynamics is modeled as a continuous system of which behavioral patterns are analyzed in regard to the parameters contained in the system these mo... | [['opinion', 'dynamics', 'of', 'a', 'group', 'of', 'individuals', 'is', 'the', 'change', 'in', 'the', 'members', 'opinions', 'through', 'mutual', 'interaction', 'with', 'each', 'other', 'the', 'related', 'literature', 'contains', 'works', 'in', 'which', 'the', 'dynamics', 'is', 'modeled', 'as', 'a', 'continuous', 'syst... | [-0.1905567802199233, 0.1047721271546941, -0.1182878759783544, 0.029067581750358604, -0.04235708362915937, -0.11030478570551588, 0.06057071423611971, 0.3538838039707987, -0.2643135420845023, -0.2751462451737969, 0.12021659074660328, -0.287324798661245, -0.17687352025145744, 0.15356663456030129, -0.04504349678285232, 0.... |
1,712.10184 | Meeting yield and conservation objectives by balancing harvesting of
juveniles and adults | Sustainable yields that are at least 80% of the maximum sustainable yield are
sometimes referred to as pretty good yield (PGY). The range of PGY harvesting
strategies is generally broad and thus leaves room to account for additional
objectives besides high yield. Here, we analyze stage-dependent harvesting
strategies... | q-bio.PE math.DS | sustainable yields that are at least 80 of the maximum sustainable yield are sometimes referred to as pretty good yield pgy the range of pgy harvesting strategies is generally broad and thus leaves room to account for additional objectives besides high yield here we analyze stagedependent harvesting strategies that rea... | [['sustainable', 'yields', 'that', 'are', 'at', 'least', '80', 'of', 'the', 'maximum', 'sustainable', 'yield', 'are', 'sometimes', 'referred', 'to', 'as', 'pretty', 'good', 'yield', 'pgy', 'the', 'range', 'of', 'pgy', 'harvesting', 'strategies', 'is', 'generally', 'broad', 'and', 'thus', 'leaves', 'room', 'to', 'accoun... | [-0.09145815581538116, 0.13162764153151096, -0.07728053197520328, 0.10633474941406508, -0.032559250170985855, -0.21065271556989162, 0.05886671354985047, 0.4058467273499963, -0.2070613513728056, -0.3583402992294663, 0.1083006956300689, -0.28082833556440095, -0.14725674421859758, 0.2158498917637831, -0.09674135306005494,... |
1,712.10185 | Controlled trapping of single particle states on a periodic substrate by
deterministic stubbing | A periodic array of atomic sites, described within a tight binding formalism
is shown to be capable of trapping electronic states as it grows in size and
gets stubbed by an atom or an atomic clusters from a side in a deterministic
way. We prescribe a method based on a real space renormalization group method,
that unr... | cond-mat.dis-nn cond-mat.mes-hall | a periodic array of atomic sites described within a tight binding formalism is shown to be capable of trapping electronic states as it grows in size and gets stubbed by an atom or an atomic clusters from a side in a deterministic way we prescribe a method based on a real space renormalization group method that unravels... | [['a', 'periodic', 'array', 'of', 'atomic', 'sites', 'described', 'within', 'a', 'tight', 'binding', 'formalism', 'is', 'shown', 'to', 'be', 'capable', 'of', 'trapping', 'electronic', 'states', 'as', 'it', 'grows', 'in', 'size', 'and', 'gets', 'stubbed', 'by', 'an', 'atom', 'or', 'an', 'atomic', 'clusters', 'from', 'a'... | [-0.1302059724271643, 0.18729447202337812, -0.08513430663339433, 0.06137382613603897, 0.017963428914006197, -0.13079674412391237, 0.08124123633869233, 0.3726040356296806, -0.2551226119600957, -0.25127822129927097, 0.05374923556002848, -0.30082940161528604, -0.12815595760982815, 0.16249653450194596, 0.03629890296349091,... |
1,712.10186 | Nonequilibrium Steady State of a Weakly-Driven Kardar-Parisi-Zhang
Equation | We consider an infinite interface in $d>2$ dimensions, governed by the
Kardar-Parisi-Zhang (KPZ) equation with a weak Gaussian noise which is
delta-correlated in time and has short-range spatial correlations. We study the
probability distribution of the interface height $H$ at a point of the
substrate, when the inter... | cond-mat.stat-mech | we consider an infinite interface in d2 dimensions governed by the kardarparisizhang kpz equation with a weak gaussian noise which is deltacorrelated in time and has shortrange spatial correlations we study the probability distribution of the interface height h at a point of the substrate when the interface is initiall... | [['we', 'consider', 'an', 'infinite', 'interface', 'in', 'd2', 'dimensions', 'governed', 'by', 'the', 'kardarparisizhang', 'kpz', 'equation', 'with', 'a', 'weak', 'gaussian', 'noise', 'which', 'is', 'deltacorrelated', 'in', 'time', 'and', 'has', 'shortrange', 'spatial', 'correlations', 'we', 'study', 'the', 'probabilit... | [-0.12616040754666621, 0.1832989945742156, -0.12256113461141165, 0.07396803363614406, 0.03869418824238151, -0.13951012102404126, -0.021766857660690288, 0.3658717537505759, -0.29893198054870246, -0.22396143766161036, 0.044264197617950335, -0.2984023634791676, -0.10566717359944489, 0.1355099141030762, 0.02417798391629562... |
1,712.10187 | Extended periodic links and HOMFLYPT polynomial | Extended strongly periodic links have been introduced by Przytycki and
Sokolov as a symmetric surgery presentation of three-manifolds on which the
finite cyclic group acts without fixed points. The purpose of this paper is to
prove that the symmetry of these links is reflected by the first coefficients
of the HOMFLYP... | math.GT | extended strongly periodic links have been introduced by przytycki and sokolov as a symmetric surgery presentation of threemanifolds on which the finite cyclic group acts without fixed points the purpose of this paper is to prove that the symmetry of these links is reflected by the first coefficients of the homflypt po... | [['extended', 'strongly', 'periodic', 'links', 'have', 'been', 'introduced', 'by', 'przytycki', 'and', 'sokolov', 'as', 'a', 'symmetric', 'surgery', 'presentation', 'of', 'threemanifolds', 'on', 'which', 'the', 'finite', 'cyclic', 'group', 'acts', 'without', 'fixed', 'points', 'the', 'purpose', 'of', 'this', 'paper', '... | [-0.22761239349627152, 0.14609301351727202, -0.10815094576145594, 0.005396659318089055, -0.1256624198420188, -0.1533150453424941, -0.007964465402227897, 0.3207439838263851, -0.288442612804759, -0.22510361996515152, 0.13959058384912518, -0.21427832581461048, -0.22033585890984306, 0.17080472329129967, -0.1195923314752200... |
1,712.10188 | Relay entanglement and clusters of correlated spins | Considering a spin-1/2 chain, we {suppose} that the entanglement passes from
a given pair of particles to another one, thus establishing the relay transfer
of entanglement along the chain. Therefore, we introduce the relay entanglement
as a sum of all pairwise entanglements in a spin chain. For more detailed
studying... | quant-ph | considering a spin12 chain we suppose that the entanglement passes from a given pair of particles to another one thus establishing the relay transfer of entanglement along the chain therefore we introduce the relay entanglement as a sum of all pairwise entanglements in a spin chain for more detailed studying the effect... | [['considering', 'a', 'spin12', 'chain', 'we', 'suppose', 'that', 'the', 'entanglement', 'passes', 'from', 'a', 'given', 'pair', 'of', 'particles', 'to', 'another', 'one', 'thus', 'establishing', 'the', 'relay', 'transfer', 'of', 'entanglement', 'along', 'the', 'chain', 'therefore', 'we', 'introduce', 'the', 'relay', '... | [-0.20312401152062062, 0.1965759295657595, -0.053136104850896766, 0.03712780216821037, 0.009982959311206028, -0.17024977839069574, 0.06961706753645558, 0.345744786218607, -0.30543346466064186, -0.25449681147957953, 0.03763609184222462, -0.32361225745574174, -0.052291494503151625, 0.13807525195547246, 0.0235206833209044... |
1,712.10189 | Ordered carbon nanotubes and globular opals as a model of multiscaling
photonic crystals | Experimental data on carbon nanotube carpet and synthetic opals have been
compared by visible, infrared spectroscopy, and electron microscopy. Spectral
features of the objects under study in infrared region are registered. Three
regions of abnormal behavior of reflectance and absorbance for carbon nanotube
carpet and... | physics.optics | experimental data on carbon nanotube carpet and synthetic opals have been compared by visible infrared spectroscopy and electron microscopy spectral features of the objects under study in infrared region are registered three regions of abnormal behavior of reflectance and absorbance for carbon nanotube carpet and two r... | [['experimental', 'data', 'on', 'carbon', 'nanotube', 'carpet', 'and', 'synthetic', 'opals', 'have', 'been', 'compared', 'by', 'visible', 'infrared', 'spectroscopy', 'and', 'electron', 'microscopy', 'spectral', 'features', 'of', 'the', 'objects', 'under', 'study', 'in', 'infrared', 'region', 'are', 'registered', 'three... | [-0.07158392815229793, 0.18603524945986769, -0.052379925234601145, -0.01955814584572282, 0.0350553788141244, -0.13143878088643154, 0.026367982745459477, 0.534676358655647, -0.20556560602832447, -0.2914373216184753, 0.07460171424167196, -0.36075130430981517, -0.0973945810153425, 0.22456454601638984, 0.018869184431322437... |
1,712.1019 | Detecting Cross-Lingual Plagiarism Using Simulated Word Embeddings | Cross-lingual plagiarism (CLP) occurs when texts written in one language are
translated into a different language and used without acknowledging the
original sources. One of the most common methods for detecting CLP requires
online machine translators (such as Google or Microsoft translate) which are
not always avail... | cs.CL cs.IR | crosslingual plagiarism clp occurs when texts written in one language are translated into a different language and used without acknowledging the original sources one of the most common methods for detecting clp requires online machine translators such as google or microsoft translate which are not always available and... | [['crosslingual', 'plagiarism', 'clp', 'occurs', 'when', 'texts', 'written', 'in', 'one', 'language', 'are', 'translated', 'into', 'a', 'different', 'language', 'and', 'used', 'without', 'acknowledging', 'the', 'original', 'sources', 'one', 'of', 'the', 'most', 'common', 'methods', 'for', 'detecting', 'clp', 'requires'... | [-0.05145658340177566, 0.0029885377287789147, -0.01791274552153537, 0.11110604717573933, -0.14251008459174905, -0.19916107960557208, 0.04793792753569241, 0.4049882611743253, -0.2720599027771773, -0.34376778902365107, 0.07584793349809746, -0.32340964669617644, -0.0948748233067887, 0.25692039518017246, -0.117435415265619... |
1,712.10191 | Coupling of Magneto-Thermal and Mechanical Superconducting Magnet Models
by Means of Mesh-Based Interpolation | In this paper we present an algorithm for the coupling of magneto-thermal and
mechanical finite element models representing superconducting accelerator
magnets. The mechanical models are used during the design of the mechanical
structure as well as the optimization of the magnetic field quality under
nominal conditio... | physics.acc-ph cs.CE math.NA physics.comp-ph | in this paper we present an algorithm for the coupling of magnetothermal and mechanical finite element models representing superconducting accelerator magnets the mechanical models are used during the design of the mechanical structure as well as the optimization of the magnetic field quality under nominal conditions t... | [['in', 'this', 'paper', 'we', 'present', 'an', 'algorithm', 'for', 'the', 'coupling', 'of', 'magnetothermal', 'and', 'mechanical', 'finite', 'element', 'models', 'representing', 'superconducting', 'accelerator', 'magnets', 'the', 'mechanical', 'models', 'are', 'used', 'during', 'the', 'design', 'of', 'the', 'mechanica... | [-0.17032144029999707, 0.14666744739101828, -0.061682870508740086, 0.009891520809932526, -0.049519648423188595, -0.15920586955685218, 0.005458942661742233, 0.3712109147038843, -0.26636787750093, -0.31986627489624714, 0.10335223406913098, -0.2472615744434781, -0.12466808515238006, 0.23249331655512964, 0.0070722993197185... |
1,712.10192 | Ratchet Effect in the Quantum Kicked Rotor and its Destruction by
Dynamical Localization | We study experimentally a quantum kicked rotor with broken parity symmetry,
supporting a ratchet effect due to the presence of a classical accelerator
mode. We show that the short-time dynamics is very well described by the
classical dynamics, characterized by a strongly asymmetric momentum
distribution with directed... | quant-ph cond-mat.dis-nn cond-mat.quant-gas | we study experimentally a quantum kicked rotor with broken parity symmetry supporting a ratchet effect due to the presence of a classical accelerator mode we show that the shorttime dynamics is very well described by the classical dynamics characterized by a strongly asymmetric momentum distribution with directed motio... | [['we', 'study', 'experimentally', 'a', 'quantum', 'kicked', 'rotor', 'with', 'broken', 'parity', 'symmetry', 'supporting', 'a', 'ratchet', 'effect', 'due', 'to', 'the', 'presence', 'of', 'a', 'classical', 'accelerator', 'mode', 'we', 'show', 'that', 'the', 'shorttime', 'dynamics', 'is', 'very', 'well', 'described', 'b... | [-0.18061881627266604, 0.2242921245257215, -0.11861559035566946, 0.057410434753013155, -0.032362939516703285, -0.17106839317362754, -0.0007255345986535152, 0.3384530059993267, -0.2847789766887824, -0.2547248927752177, 0.07047339259025952, -0.2458225419620673, -0.16630870724717775, 0.19061312259485325, 0.004600658553342... |
1,712.10193 | A multi-candidate electronic voting scheme with unlimited participants | In this paper a new multi-candidate electronic voting scheme is constructed
with unlimited participants. The main idea is to express a ballot to allow
voting for up to k out of the m candidates and unlimited participants. The
purpose of vote is to select more than one winner among $m$ candidates. Our
result is comple... | cs.CR | in this paper a new multicandidate electronic voting scheme is constructed with unlimited participants the main idea is to express a ballot to allow voting for up to k out of the m candidates and unlimited participants the purpose of vote is to select more than one winner among m candidates our result is complementary ... | [['in', 'this', 'paper', 'a', 'new', 'multicandidate', 'electronic', 'voting', 'scheme', 'is', 'constructed', 'with', 'unlimited', 'participants', 'the', 'main', 'idea', 'is', 'to', 'express', 'a', 'ballot', 'to', 'allow', 'voting', 'for', 'up', 'to', 'k', 'out', 'of', 'the', 'm', 'candidates', 'and', 'unlimited', 'par... | [-0.15077023400433018, 0.004903156554709512, -0.09792061275540412, 0.03689590573528821, -0.14840429489573476, -0.23556601728398538, 0.1865259746150675, 0.36113248622797905, -0.2557048749390012, -0.3341902454667692, 0.06732295350838743, -0.25744792257711385, -0.11035770417607212, 0.16929010271279682, -0.1530952149843599... |
1,712.10194 | Quantum Lower Bounds for Tripartite Versions of the Hidden Shift and the
Set Equality Problems | In this paper, we study quantum query complexity of the following rather
natural tripartite generalisations (in the spirit of the 3-sum problem) of the
hidden shift and the set equality problems, which we call the 3-shift-sum and
the 3-matching-sum problems.
The 3-shift-sum problem is as follows: given a table of $... | quant-ph cs.CC | in this paper we study quantum query complexity of the following rather natural tripartite generalisations in the spirit of the 3sum problem of the hidden shift and the set equality problems which we call the 3shiftsum and the 3matchingsum problems the 3shiftsum problem is as follows given a table of 3times n elements ... | [['in', 'this', 'paper', 'we', 'study', 'quantum', 'query', 'complexity', 'of', 'the', 'following', 'rather', 'natural', 'tripartite', 'generalisations', 'in', 'the', 'spirit', 'of', 'the', '3sum', 'problem', 'of', 'the', 'hidden', 'shift', 'and', 'the', 'set', 'equality', 'problems', 'which', 'we', 'call', 'the', '3sh... | [-0.10886996717045518, 0.15046718143156335, -0.03081726360657852, 0.05902314879405249, -0.0687703336780406, -0.13949743423240948, 0.09391027193258146, 0.3323760182048156, -0.31947600884898886, -0.2871046767774204, 0.12141340668313205, -0.28766331493803493, -0.15413461658786282, 0.17160463018649041, -0.08537390300476197... |
1,712.10195 | Growing Attributed Networks through Local Processes | This paper proposes an attributed network growth model. Despite the knowledge
that individuals use limited resources to form connections to similar others,
we lack an understanding of how local and resource-constrained mechanisms
explain the emergence of rich structural properties found in real-world
networks. We mak... | cs.SI | this paper proposes an attributed network growth model despite the knowledge that individuals use limited resources to form connections to similar others we lack an understanding of how local and resourceconstrained mechanisms explain the emergence of rich structural properties found in realworld networks we make three... | [['this', 'paper', 'proposes', 'an', 'attributed', 'network', 'growth', 'model', 'despite', 'the', 'knowledge', 'that', 'individuals', 'use', 'limited', 'resources', 'to', 'form', 'connections', 'to', 'similar', 'others', 'we', 'lack', 'an', 'understanding', 'of', 'how', 'local', 'and', 'resourceconstrained', 'mechanis... | [-0.11962487033318753, 0.04564962742315282, -0.07423083029468269, 0.10694594923224227, -0.12643001988846686, -0.13497161139350602, 0.09286475720666228, 0.40261201755283704, -0.2906209263414924, -0.31698697924711344, -0.0037436606529856623, -0.2584077249816771, -0.26975875034368313, 0.09795866909077744, -0.0800890596431... |
1,712.10196 | Chaotic Dynamics and Optical Power Saturation in Parity-Time (PT)
Symmetric Double Ring Resonator | We report emergence of saturation and chaotic spiking of optical power in a
double ring resonator with balanced loss and gain, obeying the so-called
parity-time symmetry. We have modeled the system using a discrete-time
iterative equation known as the Ikeda Map. In the linear regime, evolution of
optical power in the... | physics.optics nlin.CD | we report emergence of saturation and chaotic spiking of optical power in a double ring resonator with balanced loss and gain obeying the socalled paritytime symmetry we have modeled the system using a discretetime iterative equation known as the ikeda map in the linear regime evolution of optical power in the system s... | [['we', 'report', 'emergence', 'of', 'saturation', 'and', 'chaotic', 'spiking', 'of', 'optical', 'power', 'in', 'a', 'double', 'ring', 'resonator', 'with', 'balanced', 'loss', 'and', 'gain', 'obeying', 'the', 'socalled', 'paritytime', 'symmetry', 'we', 'have', 'modeled', 'the', 'system', 'using', 'a', 'discretetime', '... | [-0.20208053606329485, 0.11945570054231211, -0.09143283018202056, 0.020205655707991356, -0.014749591668805805, -0.16637087655253707, 0.05240353982444503, 0.31093512997031214, -0.2640518009895459, -0.20696023204363884, 0.08782473667015438, -0.29925520045217124, -0.17697112691821532, 0.19387920580920764, -0.0275740803754... |
1,712.10197 | Interesting Paths in the Mapper | The Mapper produces a compact summary of high dimensional data as a
simplicial complex. We study the problem of quantifying the interestingness of
subpopulations in a Mapper, which appear as long paths, flares, or loops.
First, we create a weighted directed graph G using the 1-skeleton of the
Mapper. We use the avera... | cs.CG cs.DS math.AT | the mapper produces a compact summary of high dimensional data as a simplicial complex we study the problem of quantifying the interestingness of subpopulations in a mapper which appear as long paths flares or loops first we create a weighted directed graph g using the 1skeleton of the mapper we use the average values ... | [['the', 'mapper', 'produces', 'a', 'compact', 'summary', 'of', 'high', 'dimensional', 'data', 'as', 'a', 'simplicial', 'complex', 'we', 'study', 'the', 'problem', 'of', 'quantifying', 'the', 'interestingness', 'of', 'subpopulations', 'in', 'a', 'mapper', 'which', 'appear', 'as', 'long', 'paths', 'flares', 'or', 'loops... | [-0.16425836622011938, 0.10941764990826901, -0.05875603985376169, 0.05133988385404889, -0.12072194312801668, -0.11856982979795658, 0.08277121494604835, 0.4348345952248505, -0.3092068284689114, -0.3127666564210884, 0.059555872628812255, -0.30052010597907663, -0.15296815902761676, 0.10722955260227976, -0.0851490988192191... |
1,712.10198 | The graphs of projective codes | Consider the Grassmann graph formed by $k$-dimensional subspaces of an
$n$-dimensional vector space over the field of $q$ elements ($1<k<n-1$) and
denote by $\Pi(n,k)_q$ the restriction of this graph to the set of projective
$[n,k]_q$ codes. In the case when $q\ge \binom{n}{2}$, we show that the graph
$\Pi(n,k)_q$ is... | math.CO math.AG | consider the grassmann graph formed by kdimensional subspaces of an ndimensional vector space over the field of q elements 1kn1 and denote by pink_q the restriction of this graph to the set of projective nk_q codes in the case when qge binomn2 we show that the graph pink_q is connected its diameter is equal to the diam... | [['consider', 'the', 'grassmann', 'graph', 'formed', 'by', 'kdimensional', 'subspaces', 'of', 'an', 'ndimensional', 'vector', 'space', 'over', 'the', 'field', 'of', 'q', 'elements', '1kn1', 'and', 'denote', 'by', 'pink_q', 'the', 'restriction', 'of', 'this', 'graph', 'to', 'the', 'set', 'of', 'projective', 'nk_q', 'cod... | [-0.19819691048864768, 0.12203952114502482, 0.0009717278287939305, 0.010594159747992273, -0.061984658245665, -0.13589044886131613, 0.001062150526229503, 0.36364448341136835, -0.3167403984533728, -0.22177194904992883, 0.09115674619712287, -0.3177091390737947, -0.15174505191872706, 0.14137651139589133, -0.109561194147352... |
1,712.10199 | Asymptotic period of an aperiodic Markov chain | We introduce the concept of asymptotic period for an irreducible and
aperiodic, discrete-time Markov chain X on a countable state space, and develop
the theory leading to its formal definition. The asymptotic period of X equals
one - its period - if X is recurrent, but may be larger than one if X is
transient; X is a... | math.PR | we introduce the concept of asymptotic period for an irreducible and aperiodic discretetime markov chain x on a countable state space and develop the theory leading to its formal definition the asymptotic period of x equals one its period if x is recurrent but may be larger than one if x is transient x is asymptoticall... | [['we', 'introduce', 'the', 'concept', 'of', 'asymptotic', 'period', 'for', 'an', 'irreducible', 'and', 'aperiodic', 'discretetime', 'markov', 'chain', 'x', 'on', 'a', 'countable', 'state', 'space', 'and', 'develop', 'the', 'theory', 'leading', 'to', 'its', 'formal', 'definition', 'the', 'asymptotic', 'period', 'of', '... | [-0.17759854847203574, 0.1691389386595412, -0.1024170845739718, 0.07847922215379251, -0.055519722493564974, -0.17096141312088417, 0.0670139814932814, 0.37799914069806356, -0.26190711380747544, -0.1595220202933498, 0.18827285152968085, -0.2535803314614376, -0.11656348609540146, 0.16842338123751688, -0.08755702682537958,... |
1,712.102 | Non-stoichiometry effects on the extreme magnetoresistance in Weyl
semimetal WTe2 | Non-stoichiometry effect on the extreme magnetoresistance is systematically
investigated for the Weyl semimetal WTe2. Magnetoresistance and Hall
resistivity are measured for the as-grown samples with a slight difference in
Te vacancies and the annealed samples with increased Te vacancies. The fittings
to a two-carrie... | cond-mat.mtrl-sci | nonstoichiometry effect on the extreme magnetoresistance is systematically investigated for the weyl semimetal wte2 magnetoresistance and hall resistivity are measured for the asgrown samples with a slight difference in te vacancies and the annealed samples with increased te vacancies the fittings to a twocarrier model... | [['nonstoichiometry', 'effect', 'on', 'the', 'extreme', 'magnetoresistance', 'is', 'systematically', 'investigated', 'for', 'the', 'weyl', 'semimetal', 'wte2', 'magnetoresistance', 'and', 'hall', 'resistivity', 'are', 'measured', 'for', 'the', 'asgrown', 'samples', 'with', 'a', 'slight', 'difference', 'in', 'te', 'vaca... | [-0.1639489324189964, 0.21320622914936393, -0.018129939075421403, 0.010539068179679345, -0.016054207407351997, -0.17622616636152896, 0.12663374078046116, 0.3887466635313575, -0.262294242710427, -0.31869911155081354, -0.029515808546286146, -0.3696294916724717, -0.13253680012551033, 0.16404198055938146, -0.01536109784717... |
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