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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1,801.03269 | Topological phase, supercritical point and emergent phenomena in
extended $\mathbb{Z}_3$ parafermion chain | Topological orders and associated topological protected excitations
satisfying non-Abelian statistics have been widely explored in various
platforms. The $\mathbb{Z}_3$ parafermions are regarded as the most natural
generation of the Majorana fermions to realize these topological orders. Here
we investigate the topolo... | cond-mat.str-el | topological orders and associated topological protected excitations satisfying nonabelian statistics have been widely explored in various platforms the mathbbz_3 parafermions are regarded as the most natural generation of the majorana fermions to realize these topological orders here we investigate the topological phas... | [['topological', 'orders', 'and', 'associated', 'topological', 'protected', 'excitations', 'satisfying', 'nonabelian', 'statistics', 'have', 'been', 'widely', 'explored', 'in', 'various', 'platforms', 'the', 'mathbbz_3', 'parafermions', 'are', 'regarded', 'as', 'the', 'most', 'natural', 'generation', 'of', 'the', 'majo... | [-0.18725095427286653, 0.2796237747391494, -0.06921619813066798, 0.08498890308645106, -0.05795751011313556, -0.19256985362304688, 0.03819995509557329, 0.351593241228589, -0.2448304119926587, -0.26964987117748757, 0.06929134704208896, -0.2552493985427858, -0.18973673779484151, 0.13340404573616318, 0.020273181869854013, ... |
1,801.0327 | Functional metasurfaces: Do we need normal polarizations? | We consider reciprocal metasurfaces with engineered reflection and
transmission coefficients and study the role of normal (with respect to the
metasurface plane) electric and magnetic polarizations on the possibilities to
shape the reflection and transmission responses. We demonstrate in general and
on a representati... | physics.app-ph cond-mat.mtrl-sci | we consider reciprocal metasurfaces with engineered reflection and transmission coefficients and study the role of normal with respect to the metasurface plane electric and magnetic polarizations on the possibilities to shape the reflection and transmission responses we demonstrate in general and on a representative ex... | [['we', 'consider', 'reciprocal', 'metasurfaces', 'with', 'engineered', 'reflection', 'and', 'transmission', 'coefficients', 'and', 'study', 'the', 'role', 'of', 'normal', 'with', 'respect', 'to', 'the', 'metasurface', 'plane', 'electric', 'and', 'magnetic', 'polarizations', 'on', 'the', 'possibilities', 'to', 'shape',... | [-0.17025854699518328, 0.10359979867116435, -0.014590561175002502, -0.05625089717092463, -0.12308134860103274, -0.1262157449996416, 0.027412426634947515, 0.46833293270933757, -0.26313084044626783, -0.2630706415083106, 0.05350917789849688, -0.28010448702907825, -0.2076520940114918, 0.17408044286236002, -0.04654701816552... |
1,801.03271 | Existence and non-existence of maximizers for the Moser-Trudinger type
inequalities under inhomogeneous constraints | In this paper, we study the existence and non-existence of maximizers for the
Moser-Trudinger type inequalities in $\Bbb R^N$ of the form \[
D_{N,\alpha}(a,b):= \sup_{u\in W^{1,N}(\Bbb R^N),\,\|\nabla u\|_{L^N(\Bbb
R^N)}^a+\|u\|_{L^N(\Bbb R^N)}^b=1} \int_{\Bbb
R^N}\Phi_N\left(\alpha|u|^{N'}\right)dx. \] Here $N\geq 2... | math.AP | in this paper we study the existence and nonexistence of maximizers for the mosertrudinger type inequalities in bbb rn of the form d_nalphaab sup_uin w1nbbb rnnabla u_lnbbb rnau_lnbbb rnb1 int_bbb rnphi_nleftalphaunrightdx here ngeq 2 nfracnn1 ab0 alpha in 0alpha_n and phi_ntetsum_j0n2fractjj where alpha_n n omega_n11n... | [['in', 'this', 'paper', 'we', 'study', 'the', 'existence', 'and', 'nonexistence', 'of', 'maximizers', 'for', 'the', 'mosertrudinger', 'type', 'inequalities', 'in', 'bbb', 'rn', 'of', 'the', 'form', 'd_nalphaab', 'sup_uin', 'w1nbbb', 'rnnabla', 'u_lnbbb', 'rnau_lnbbb', 'rnb1', 'int_bbb', 'rnphi_nleftalphaunrightdx', 'h... | [-0.17701022734801317, 0.08480771119310253, 0.00732945854743493, 0.016546241035845517, 0.051191125940210344, -0.14030929779013, 0.017929711070008063, 0.31974819002822896, -0.2490125255466535, -0.17661960379504224, 0.1127802973837945, -0.3292871328263447, -0.14965159272582368, 0.18698508023744684, -0.08398637479577942, ... |
1,801.03272 | Quintessential inflation: A unified scenario of inflation and dark
energy | Quintessential inflation unifies inflation and late time acceleration by a
single scalar field. Such a scenario, with canonical and non-canonical scalar
fields, has been discussed . The scalar field behaves as an inflaton field
during inflation and as a quintessence field during late time. Also the
predictions of the... | gr-qc astro-ph.CO | quintessential inflation unifies inflation and late time acceleration by a single scalar field such a scenario with canonical and noncanonical scalar fields has been discussed the scalar field behaves as an inflaton field during inflation and as a quintessence field during late time also the predictions of the models h... | [['quintessential', 'inflation', 'unifies', 'inflation', 'and', 'late', 'time', 'acceleration', 'by', 'a', 'single', 'scalar', 'field', 'such', 'a', 'scenario', 'with', 'canonical', 'and', 'noncanonical', 'scalar', 'fields', 'has', 'been', 'discussed', 'the', 'scalar', 'field', 'behaves', 'as', 'an', 'inflaton', 'field... | [-0.14911614626384617, 0.2306874345667893, -0.14455191295986114, 0.09816245747762814, -0.10302620977490094, -0.19733722165651751, -0.1619038187098085, 0.3092416890063568, -0.1706477510824538, -0.33275727891739, 0.07769301193847991, -0.18968975535806334, -0.10851186218981941, 0.1687652278985632, -0.010402565895530739, 0... |
1,801.03273 | Prediction of a magnetic Weyl semimetal without spin-orbit coupling and
strong anomalous Hall effect in the Heusler compensated ferrimagnet Ti2MnAl | We predict a magnetic Weyl semimetal in the inverse Heusler Ti2MnAl, a
compensated ferrimagnet with a vanishing net magnetic moment and a Curie
temperature of over 650 K. Despite the vanishing net magnetic moment, we
calculate a large intrinsic anomalous Hall effect (AHE) of about 300 S/cm. It
derives from the Berry ... | cond-mat.mtrl-sci | we predict a magnetic weyl semimetal in the inverse heusler ti2mnal a compensated ferrimagnet with a vanishing net magnetic moment and a curie temperature of over 650 k despite the vanishing net magnetic moment we calculate a large intrinsic anomalous hall effect ahe of about 300 scm it derives from the berry curvature... | [['we', 'predict', 'a', 'magnetic', 'weyl', 'semimetal', 'in', 'the', 'inverse', 'heusler', 'ti2mnal', 'a', 'compensated', 'ferrimagnet', 'with', 'a', 'vanishing', 'net', 'magnetic', 'moment', 'and', 'a', 'curie', 'temperature', 'of', 'over', '650', 'k', 'despite', 'the', 'vanishing', 'net', 'magnetic', 'moment', 'we',... | [-0.22551879171720324, 0.20678079681293188, -0.0055501095543638995, 0.02406689414838642, -0.1243189797789776, -0.14410643971807854, 0.10066132675249818, 0.3407575390365233, -0.2970617687859878, -0.29531122027004153, -0.007478772907150017, -0.3503957254178196, -0.1276488501731181, 0.14099298603490323, 0.0219589961959761... |
1,801.03274 | Accurate effective temperatures of the metal-poor benchmark stars HD
140283, HD 122563 and HD 103095 from CHARA interferometry | Large stellar surveys of the Milky Way require validation with reference to a
set of "benchmark" stars whose fundamental properties are well-determined. For
metal-poor benchmark stars, disagreement between spectroscopic and
interferometric effective temperatures has called the reliability of the
temperature scale int... | astro-ph.SR | large stellar surveys of the milky way require validation with reference to a set of benchmark stars whose fundamental properties are welldetermined for metalpoor benchmark stars disagreement between spectroscopic and interferometric effective temperatures has called the reliability of the temperature scale into questi... | [['large', 'stellar', 'surveys', 'of', 'the', 'milky', 'way', 'require', 'validation', 'with', 'reference', 'to', 'a', 'set', 'of', 'benchmark', 'stars', 'whose', 'fundamental', 'properties', 'are', 'welldetermined', 'for', 'metalpoor', 'benchmark', 'stars', 'disagreement', 'between', 'spectroscopic', 'and', 'interfero... | [-0.08483640936404542, 0.11595794208460118, -0.053940553780897856, -0.02861090530945578, -0.11211360294381204, -0.14480101423520575, 0.08281895954187622, 0.4282335257298084, -0.09460776191129906, -0.39979272755096906, 0.04545485190157989, -0.3297068091511876, 0.0412536417063906, 0.23737344961267096, -0.0635735261576933... |
1,801.03275 | Skyrmion states in thin confined polygonal nanostructures | Recent studies have demonstrated that skyrmionic states can be the ground
state in thin-film FeGe disk nanostructures in the absence of a stabilising
applied magnetic field. In this work, we advance this understanding by
investigating to what extent this stabilisation of skyrmionic structures
through confinement exis... | cond-mat.mes-hall | recent studies have demonstrated that skyrmionic states can be the ground state in thinfilm fege disk nanostructures in the absence of a stabilising applied magnetic field in this work we advance this understanding by investigating to what extent this stabilisation of skyrmionic structures through confinement exists in... | [['recent', 'studies', 'have', 'demonstrated', 'that', 'skyrmionic', 'states', 'can', 'be', 'the', 'ground', 'state', 'in', 'thinfilm', 'fege', 'disk', 'nanostructures', 'in', 'the', 'absence', 'of', 'a', 'stabilising', 'applied', 'magnetic', 'field', 'in', 'this', 'work', 'we', 'advance', 'this', 'understanding', 'by'... | [-0.14899372826330365, 0.13699283563396117, -0.06856006267325332, 0.01427542966712887, -0.0400956779702877, -0.06600737009818355, 0.01916125120439877, 0.4078963467975458, -0.24712213969479005, -0.3063649273927634, 0.09875755618093535, -0.21063241871694724, -0.11532128541109463, 0.1765038384939544, -0.007858698284253477... |
1,801.03276 | Anti-triplet charmed baryon decays with SU(3) Flavor Symmetry | We study the decays of the anti-triplet charmed baryon state
$(\Xi_c^0,\Xi_c^+,\Lambda_c^+)$ based on the $SU(3)$ flavor symmetry. In
particular, after predicting ${\cal B}(\Xi_c^0\to \Xi^-\pi^+)=(15.7 \pm
0.7)\times 10^{-3}$ and ${\cal B}(\Xi_c^+\to\Xi^-\pi^+\pi^+)=(14.7\pm
8.4)\times 10^{-3}$, we extract that ${\ca... | hep-ph hep-ex | we study the decays of the antitriplet charmed baryon state xi_c0xi_clambda_c based on the su3 flavor symmetry in particular after predicting cal bxi_c0to xipi157 pm 07times 103 and cal bxi_ctoxipipi147pm 84times 103 we extract that cal bxi_c0tolambda kpilambda kkxi enu_e168pm 23045pm 011487pm 174times 103 and cal bxi_... | [['we', 'study', 'the', 'decays', 'of', 'the', 'antitriplet', 'charmed', 'baryon', 'state', 'xi_c0xi_clambda_c', 'based', 'on', 'the', 'su3', 'flavor', 'symmetry', 'in', 'particular', 'after', 'predicting', 'cal', 'bxi_c0to', 'xipi157', 'pm', '07times', '103', 'and', 'cal', 'bxi_ctoxipipi147pm', '84times', '103', 'we',... | [-0.10238021154325888, 0.28466122197057825, 0.08019234053790569, 0.045948352694694855, 0.048308685069243455, -0.1229506324732093, 0.10240792504140185, 0.27421843774165167, -0.02460595860964421, -0.3362705343299442, 0.03661710722724709, -0.4083077959114253, 0.05986505625016912, 0.06860098402683783, 0.049529216781427916,... |
1,801.03277 | Hyperbolic Metamaterial Resonator-Antenna Scheme for Large, Broadband
Emission Enhancement and Single Photon Collection | We model the broadband enhancement of single-photon emission from color
centres in silicon carbide nanocrystals coupled to a planar hyperbolic
metamaterial, HMM resonator. The design is based on positioning the single
photon emitters within the HMM resonator, made of a dielectric index-matched
with silicon-carbide ma... | quant-ph physics.optics | we model the broadband enhancement of singlephoton emission from color centres in silicon carbide nanocrystals coupled to a planar hyperbolic metamaterial hmm resonator the design is based on positioning the single photon emitters within the hmm resonator made of a dielectric indexmatched with siliconcarbide material t... | [['we', 'model', 'the', 'broadband', 'enhancement', 'of', 'singlephoton', 'emission', 'from', 'color', 'centres', 'in', 'silicon', 'carbide', 'nanocrystals', 'coupled', 'to', 'a', 'planar', 'hyperbolic', 'metamaterial', 'hmm', 'resonator', 'the', 'design', 'is', 'based', 'on', 'positioning', 'the', 'single', 'photon', ... | [-0.08879460355778955, 0.12165138049144902, 0.019049807655266225, -0.046955864450408474, -0.03985281699554777, -0.15473014665656679, 0.059898079123985, 0.49670132308859716, -0.18463828849459563, -0.36183988540614775, -0.0005424617587092828, -0.34306321789820987, -0.023282509631763548, 0.19481183828290116, 0.00106758995... |
1,801.03278 | How bright was the Big Bang? | It is generally believed that in the epoch prior to the formation of the
first stars, the Universe was completely dark (the period is therefore known as
the Dark Ages). Usually, the start of this epoch is placed at the photon
decoupling. In this work, we investigate the question, whether there was enough
light during... | physics.pop-ph | it is generally believed that in the epoch prior to the formation of the first stars the universe was completely dark the period is therefore known as the dark ages usually the start of this epoch is placed at the photon decoupling in this work we investigate the question whether there was enough light during the dark ... | [['it', 'is', 'generally', 'believed', 'that', 'in', 'the', 'epoch', 'prior', 'to', 'the', 'formation', 'of', 'the', 'first', 'stars', 'the', 'universe', 'was', 'completely', 'dark', 'the', 'period', 'is', 'therefore', 'known', 'as', 'the', 'dark', 'ages', 'usually', 'the', 'start', 'of', 'this', 'epoch', 'is', 'placed... | [-0.058580067126751116, 0.15976617633100224, -0.1257741172208425, 0.12762080201849238, -0.06993419286547177, -0.07026934253325293, 0.01626047198105296, 0.38989899445906145, -0.18841178494360333, -0.3819337205260719, 0.0855978983518488, -0.2631654762449341, -0.0486833237692577, 0.17058013381282672, -0.06954914199854803,... |
1,801.03279 | Study of Active Brownian Particle Diffusion in Polymer Solutions | The diffusion behavior of an active Brownian particle (ABP) in polymer
solutions is studied using Langevin dynamics simulations. We find that the long
time diffusion coefficient $D$ can show a non-monotonic dependence on the
particle size $R$ if the active force $F_{a}$ is large enough, wherein a bigger
particle woul... | cond-mat.soft | the diffusion behavior of an active brownian particle abp in polymer solutions is studied using langevin dynamics simulations we find that the long time diffusion coefficient d can show a nonmonotonic dependence on the particle size r if the active force f_a is large enough wherein a bigger particle would diffuse faste... | [['the', 'diffusion', 'behavior', 'of', 'an', 'active', 'brownian', 'particle', 'abp', 'in', 'polymer', 'solutions', 'is', 'studied', 'using', 'langevin', 'dynamics', 'simulations', 'we', 'find', 'that', 'the', 'long', 'time', 'diffusion', 'coefficient', 'd', 'can', 'show', 'a', 'nonmonotonic', 'dependence', 'on', 'the... | [-0.13234203285796362, 0.2002250413251103, -0.11421516136421511, 0.03718925387365744, -0.0497690117407021, -0.15315833347332147, -0.024702300789714273, 0.34041957561340597, -0.2722702162650724, -0.3004731968252195, 0.05648593263273748, -0.28397606995163693, -0.16366875406561626, 0.19076793018935456, 0.00999995390625877... |
1,801.0328 | Algebraic separatrices for non-dicritical foliations on projective
spaces of dimension at least four | Non-dicritical codimension one foliations on projective spaces of dimension
four or higher always have an invariant algebraic hypersurface. The proof
relies on a strengthening of a result by Rossi on the
algebraization/continuation of analytic subvarieties of projective spaces.
| math.AG math.CA math.CV | nondicritical codimension one foliations on projective spaces of dimension four or higher always have an invariant algebraic hypersurface the proof relies on a strengthening of a result by rossi on the algebraizationcontinuation of analytic subvarieties of projective spaces | [['nondicritical', 'codimension', 'one', 'foliations', 'on', 'projective', 'spaces', 'of', 'dimension', 'four', 'or', 'higher', 'always', 'have', 'an', 'invariant', 'algebraic', 'hypersurface', 'the', 'proof', 'relies', 'on', 'a', 'strengthening', 'of', 'a', 'result', 'by', 'rossi', 'on', 'the', 'algebraizationcontinua... | [-0.24288066275216438, 0.017766402974941867, -0.1169643418586536, 0.08275057808370204, -0.092457446584327, -0.13693565862706383, -0.05445107706897968, 0.2555672040058149, -0.1780777919433407, -0.13819656636867975, 0.1612391700414387, -0.26714069864435774, -0.09093875632419982, 0.30612830374062666, -0.21075313946081176,... |
1,801.03281 | Large thermoelectric efficiency of doped polythiophene junction: a
density functional study | The thermoelectric properties of polythiophene (PT) coupled to the Au (111)
electrodes are studied based on density functional theory combined with
nonequilibrium Green function formalism. Specially, the effect of Li and Cl
adsorbents on the thermoelectric efficiency of the PT junction is investigated
in different co... | cond-mat.mes-hall | the thermoelectric properties of polythiophene pt coupled to the au 111 electrodes are studied based on density functional theory combined with nonequilibrium green function formalism specially the effect of li and cl adsorbents on the thermoelectric efficiency of the pt junction is investigated in different concentrat... | [['the', 'thermoelectric', 'properties', 'of', 'polythiophene', 'pt', 'coupled', 'to', 'the', 'au', '111', 'electrodes', 'are', 'studied', 'based', 'on', 'density', 'functional', 'theory', 'combined', 'with', 'nonequilibrium', 'green', 'function', 'formalism', 'specially', 'the', 'effect', 'of', 'li', 'and', 'cl', 'ads... | [-0.15643262247763703, 0.09744555697824549, -0.035972185400796344, -0.009269684567196488, 0.04046542653693529, -0.14282486065499614, 0.06817687408705563, 0.37837556310415527, -0.24350579911521797, -0.3255191313359758, -0.04592532668953184, -0.32594983871014593, -0.13544777398206423, 0.17482967478833322, 0.0004849072128... |
1,801.03282 | The effect of long-range interactions on the dynamics and statistics of
1D Hamiltonian lattices with on-site potential | We examine the role of long--range interactions on the dynamical and
statistical properties of two 1D lattices with on--site potentials that are
known to support discrete breathers: the Klein--Gordon (KG) lattice which
includes linear dispersion and the Gorbach--Flach (GF) lattice, which shares
the same on--site pote... | nlin.CD | we examine the role of longrange interactions on the dynamical and statistical properties of two 1d lattices with onsite potentials that are known to support discrete breathers the kleingordon kg lattice which includes linear dispersion and the gorbachflach gf lattice which shares the same onsite potential but its disp... | [['we', 'examine', 'the', 'role', 'of', 'longrange', 'interactions', 'on', 'the', 'dynamical', 'and', 'statistical', 'properties', 'of', 'two', '1d', 'lattices', 'with', 'onsite', 'potentials', 'that', 'are', 'known', 'to', 'support', 'discrete', 'breathers', 'the', 'kleingordon', 'kg', 'lattice', 'which', 'includes', ... | [-0.1519887743470354, 0.19133391870754912, -0.06609835584779009, 0.06781198010392331, -0.02990630769322788, -0.15924796842465255, -0.007297439674963941, 0.3391150087006613, -0.25987332908737804, -0.249057456468996, 0.04925477380507408, -0.3206475839077378, -0.13764022481571994, 0.1784747349806576, 0.055474567756892516,... |
1,801.03283 | Generation of long-living entanglement between two distant three-level
atoms in non-Markovian environments | In this paper, a scheme for the generation of long-living entanglement
between two distant {\Lambda}-type three-level atoms separately trapped in two
dissipative cavities is proposed. In this scheme, two dissipative cavities are
coupled to their own non-Markovian environments and two three-level atoms are
driven by t... | quant-ph | in this paper a scheme for the generation of longliving entanglement between two distant lambdatype threelevel atoms separately trapped in two dissipative cavities is proposed in this scheme two dissipative cavities are coupled to their own nonmarkovian environments and two threelevel atoms are driven by the classical ... | [['in', 'this', 'paper', 'a', 'scheme', 'for', 'the', 'generation', 'of', 'longliving', 'entanglement', 'between', 'two', 'distant', 'lambdatype', 'threelevel', 'atoms', 'separately', 'trapped', 'in', 'two', 'dissipative', 'cavities', 'is', 'proposed', 'in', 'this', 'scheme', 'two', 'dissipative', 'cavities', 'are', 'c... | [-0.17344765743525983, 0.267502579280083, -0.020968278576326264, 0.014649191050085466, 0.051825025186009774, -0.20981965750992834, -0.0003662114482591147, 0.3971235099760396, -0.2443776274503598, -0.26290167898342415, -0.008514882856140937, -0.29027458221592883, -0.04153181520617894, 0.2226420144827382, 0.0611214562065... |
1,801.03284 | Markovian tricks for non-Markovian trees: contour process, extinction
and scaling limits | In this work, we study a family of non-Markovian trees modeling populations
where individuals live and reproduce independently with possibly time-dependent
birth-rate and lifetime distribution. To this end, we use the coding process
introduced by Lambert. We show that, in our situation, this process is no
longer a L{... | math.PR | in this work we study a family of nonmarkovian trees modeling populations where individuals live and reproduce independently with possibly timedependent birthrate and lifetime distribution to this end we use the coding process introduced by lambert we show that in our situation this process is no longer a levy process ... | [['in', 'this', 'work', 'we', 'study', 'a', 'family', 'of', 'nonmarkovian', 'trees', 'modeling', 'populations', 'where', 'individuals', 'live', 'and', 'reproduce', 'independently', 'with', 'possibly', 'timedependent', 'birthrate', 'and', 'lifetime', 'distribution', 'to', 'this', 'end', 'we', 'use', 'the', 'coding', 'pr... | [-0.05991921593304605, 0.1170892554400548, -0.13059460291057634, 0.12327394634137667, -0.09119401894254717, -0.14076143288006115, 0.12531262671776638, 0.40623328131979486, -0.283071754402392, -0.24290233024745989, 0.14417460436078536, -0.23433662335863664, -0.15746119703822598, 0.1900654425384821, -0.08619806444966442,... |
1,801.03285 | A Composition Theorem via Conflict Complexity | Let $\R(\cdot)$ stand for the bounded-error randomized query complexity. We
show that for any relation $f \subseteq \{0,1\}^n \times \mathcal{S}$ and
partial Boolean function $g \subseteq \{0,1\}^n \times \{0,1\}$, $\R_{1/3}(f
\circ g^n) = \Omega(\R_{4/9}(f) \cdot \sqrt{\R_{1/3}(g)})$. Independently of
us, Gavinsky, ... | cs.CC | let rcdot stand for the boundederror randomized query complexity we show that for any relation f subseteq 01n times mathcals and partial boolean function g subseteq 01n times 01 r_13f circ gn omegar_49f cdot sqrtr_13g independently of us gavinsky lee and santha citenewcomp proved this result by an example demonstrated ... | [['let', 'rcdot', 'stand', 'for', 'the', 'boundederror', 'randomized', 'query', 'complexity', 'we', 'show', 'that', 'for', 'any', 'relation', 'f', 'subseteq', '01n', 'times', 'mathcals', 'and', 'partial', 'boolean', 'function', 'g', 'subseteq', '01n', 'times', '01', 'r_13f', 'circ', 'gn', 'omegar_49f', 'cdot', 'sqrtr_1... | [-0.18747838610602963, 0.11551872333051681, -0.0022963337720401824, 0.007321314409285063, -0.059482878659881895, -0.17025692683834864, 0.10698540429634754, 0.33389293718882784, -0.3205465779299297, -0.27046911037897553, -0.010233396990975786, -0.2723915486406254, -0.16738470111002204, 0.18924801375076014, -0.1564142877... |
1,801.03286 | Long-lived non-classical correlations for scalable quantum repeaters at
room temperature | Heralded single-photon sources with on-demand readout are promising
candidates for quantum repeaters enabling long-distance quantum communication.
The need for scalability of such systems requires simple experimental
solutions, thus favouring room-temperature systems. For quantum repeater
applications, long delays be... | quant-ph | heralded singlephoton sources with ondemand readout are promising candidates for quantum repeaters enabling longdistance quantum communication the need for scalability of such systems requires simple experimental solutions thus favouring roomtemperature systems for quantum repeater applications long delays between hera... | [['heralded', 'singlephoton', 'sources', 'with', 'ondemand', 'readout', 'are', 'promising', 'candidates', 'for', 'quantum', 'repeaters', 'enabling', 'longdistance', 'quantum', 'communication', 'the', 'need', 'for', 'scalability', 'of', 'such', 'systems', 'requires', 'simple', 'experimental', 'solutions', 'thus', 'favou... | [-0.15936127728591226, 0.2187983578657859, -0.013083897859547031, -0.0037721218856223795, 0.017325861066937037, -0.2125647059858662, 0.12407789889831504, 0.4409185192254308, -0.21976880006147675, -0.3223509419046036, 0.028545570723259542, -0.2753706419687361, -0.024355329815553477, 0.2614205776241748, -0.02578728700579... |
1,801.03287 | Convergence of Pascal-Like Triangles in Parry-Bertrand Numeration
Systems | We pursue the investigation of generalizations of the Pascal triangle based
on binomial coefficients of finite words. These coefficients count the number
of times a finite word appears as a subsequence of another finite word. The
finite words occurring in this paper belong to the language of a Parry
numeration system... | math.CO | we pursue the investigation of generalizations of the pascal triangle based on binomial coefficients of finite words these coefficients count the number of times a finite word appears as a subsequence of another finite word the finite words occurring in this paper belong to the language of a parry numeration system sat... | [['we', 'pursue', 'the', 'investigation', 'of', 'generalizations', 'of', 'the', 'pascal', 'triangle', 'based', 'on', 'binomial', 'coefficients', 'of', 'finite', 'words', 'these', 'coefficients', 'count', 'the', 'number', 'of', 'times', 'a', 'finite', 'word', 'appears', 'as', 'a', 'subsequence', 'of', 'another', 'finite... | [-0.14481747452373384, 0.09789477255981183, -0.09020251287438441, 0.07351341447520099, -0.08973067178885685, -0.11918640916337608, 0.06806333945746701, 0.30108974111499265, -0.3129727618143079, -0.2187377921291045, 0.07123181910992571, -0.35250868402363267, -0.11822230411598866, 0.17782836882452102, -0.1137359310769170... |
1,801.03288 | Heat capacity evidence for conventional superconductivity in the Type-II
Dirac semi-metal PdTe$_2$ | We use electrical transport, magnetoresistance, and heat capacity
measurements on high quality single crystals of the recently discovered
superconducting Type-II Dirac semi-metal PdTe$_2$, to probe the nature of it's
superconducting phase. The magnitude of the electronic heat capacity anomaly at
$T_c$, the low temper... | cond-mat.supr-con cond-mat.str-el | we use electrical transport magnetoresistance and heat capacity measurements on high quality single crystals of the recently discovered superconducting typeii dirac semimetal pdte_2 to probe the nature of its superconducting phase the magnitude of the electronic heat capacity anomaly at t_c the low temperature exponent... | [['we', 'use', 'electrical', 'transport', 'magnetoresistance', 'and', 'heat', 'capacity', 'measurements', 'on', 'high', 'quality', 'single', 'crystals', 'of', 'the', 'recently', 'discovered', 'superconducting', 'typeii', 'dirac', 'semimetal', 'pdte_2', 'to', 'probe', 'the', 'nature', 'of', 'its', 'superconducting', 'ph... | [-0.24227836360001848, 0.199893823447859, -0.01645995830005545, -0.017103803514536203, -0.12515979865843074, -0.17956214141477608, 0.23127902002583833, 0.31861695638369947, -0.2709067723314677, -0.2946325868722938, -0.00021813343378848264, -0.3758119928783604, -0.10627733314842251, 0.18370793053569892, 0.02959232932577... |
1,801.03289 | Simple waves in a two-component Bose-Einstein condensate | We consider dynamics of simple waves in a two-component Bose-Einstein
condensates. The evolution of the condensate is described by the
Gross-Pitaevskii equations which can be reduced for simple wave solutions to a
system of ordinary differential equations which coincide with those derived by
Ovsyannikov for the two-l... | cond-mat.quant-gas | we consider dynamics of simple waves in a twocomponent boseeinstein condensates the evolution of the condensate is described by the grosspitaevskii equations which can be reduced for simple wave solutions to a system of ordinary differential equations which coincide with those derived by ovsyannikov for the twolayer fu... | [['we', 'consider', 'dynamics', 'of', 'simple', 'waves', 'in', 'a', 'twocomponent', 'boseeinstein', 'condensates', 'the', 'evolution', 'of', 'the', 'condensate', 'is', 'described', 'by', 'the', 'grosspitaevskii', 'equations', 'which', 'can', 'be', 'reduced', 'for', 'simple', 'wave', 'solutions', 'to', 'a', 'system', 'o... | [-0.19278892518904728, 0.13627063368972486, -0.05413973247871185, 0.09015558404364409, -0.031775844689363085, -0.14672532411387715, -0.04567144795631369, 0.2928869357475868, -0.2572588479289642, -0.2596035796480301, 0.06508765141748321, -0.2746173669225894, -0.15873580967458203, 0.2039665263444663, 0.0660343244433021, ... |
1,801.0329 | Efficient Machine-type Communication using Multi-metric
Context-awareness for Cars used as Mobile Sensors in Upcoming 5G Networks | Upcoming 5G-based communication networks will be confronted with huge
increases in the amount of transmitted sensor data related to massive
deployments of static and mobile Internet of Things (IoT) systems. Cars acting
as mobile sensors will become important data sources for cloud-based
applications like predictive m... | cs.NI | upcoming 5gbased communication networks will be confronted with huge increases in the amount of transmitted sensor data related to massive deployments of static and mobile internet of things iot systems cars acting as mobile sensors will become important data sources for cloudbased applications like predictive maintena... | [['upcoming', '5gbased', 'communication', 'networks', 'will', 'be', 'confronted', 'with', 'huge', 'increases', 'in', 'the', 'amount', 'of', 'transmitted', 'sensor', 'data', 'related', 'to', 'massive', 'deployments', 'of', 'static', 'and', 'mobile', 'internet', 'of', 'things', 'iot', 'systems', 'cars', 'acting', 'as', '... | [-0.22693521397415423, 0.06392181291604883, 0.00875191686480689, 0.030424343174226307, -0.09820365894191607, -0.22767479376913122, 0.0688867060520452, 0.4074266926368321, -0.25260862720661736, -0.3237498706760902, 0.14307021043926516, -0.29480438565469685, -0.16486098927280013, 0.23854973106045116, -0.16224951122778875... |
1,801.03291 | A Radio-fingerprinting-based Vehicle Classification System for
Intelligent Traffic Control in Smart Cities | The measurement and provision of precise and upto-date traffic-related key
performance indicators is a key element and crucial factor for intelligent
traffic controls systems in upcoming smart cities. The street network is
considered as a highly-dynamic Cyber Physical System (CPS) where measured
information forms the... | cs.NI | the measurement and provision of precise and uptodate trafficrelated key performance indicators is a key element and crucial factor for intelligent traffic controls systems in upcoming smart cities the street network is considered as a highlydynamic cyber physical system cps where measured information forms the foundat... | [['the', 'measurement', 'and', 'provision', 'of', 'precise', 'and', 'uptodate', 'trafficrelated', 'key', 'performance', 'indicators', 'is', 'a', 'key', 'element', 'and', 'crucial', 'factor', 'for', 'intelligent', 'traffic', 'controls', 'systems', 'in', 'upcoming', 'smart', 'cities', 'the', 'street', 'network', 'is', 'c... | [-0.11952635722065513, 0.008452084184755957, -0.03621738169323465, 0.052485929366972564, -0.06686743013701882, -0.1737341235575238, 0.08056983786530444, 0.35644266784727346, -0.22918371054034614, -0.37760073039445535, 0.15750704304817265, -0.2672640728115132, -0.11462279131302064, 0.2393069990788295, -0.147972179254554... |
1,801.03292 | Can ultraprecision polishing techniques improve the coherence times of
nitrogen-vacancy centers in diamond? | We investigate the correlation between surface roughness and corresponding
$T_2$ times of nearsurface nitrogen-vacancy centers (~7 nm/ 5 keV implantation
energy) in diamond. For this purpose we compare five different polishing
techniques, including both purely mechanical as well as chemical mechanical
approaches, two... | cond-mat.mes-hall | we investigate the correlation between surface roughness and corresponding t_2 times of nearsurface nitrogenvacancy centers 7 nm 5 kev implantation energy in diamond for this purpose we compare five different polishing techniques including both purely mechanical as well as chemical mechanical approaches two different s... | [['we', 'investigate', 'the', 'correlation', 'between', 'surface', 'roughness', 'and', 'corresponding', 't_2', 'times', 'of', 'nearsurface', 'nitrogenvacancy', 'centers', '7', 'nm', '5', 'kev', 'implantation', 'energy', 'in', 'diamond', 'for', 'this', 'purpose', 'we', 'compare', 'five', 'different', 'polishing', 'techn... | [-0.01657657538069993, 0.2019093897275349, -0.0014693450122590988, 0.019590921596103216, 0.13890454269224597, -0.15686686461170515, 0.02048926233684504, 0.5388238077522606, -0.21080700598496904, -0.35332390716079104, 0.07499729581327448, -0.34653298703012286, -0.02473281165184353, 0.1977040452822562, -0.017410168894917... |
1,801.03293 | Unconventional superconducting gap structure protected by space group
symmetry | Recent superconducting gap classifications based on space group symmetry have
revealed nontrivial gap structures that were not shown by point group symmetry.
First, we review a comprehensive classification of symmetry-protected line
nodes within the range of centrosymmetric space groups. Next, we show an
additional c... | cond-mat.supr-con cond-mat.str-el | recent superconducting gap classifications based on space group symmetry have revealed nontrivial gap structures that were not shown by point group symmetry first we review a comprehensive classification of symmetryprotected line nodes within the range of centrosymmetric space groups next we show an additional constrai... | [['recent', 'superconducting', 'gap', 'classifications', 'based', 'on', 'space', 'group', 'symmetry', 'have', 'revealed', 'nontrivial', 'gap', 'structures', 'that', 'were', 'not', 'shown', 'by', 'point', 'group', 'symmetry', 'first', 'we', 'review', 'a', 'comprehensive', 'classification', 'of', 'symmetryprotected', 'li... | [-0.2623372784542082, 0.13186314486532555, -0.04241366838900054, 0.028160970068888784, -0.13171508543693075, -0.13129989797868424, 0.16927152036592683, 0.4412084352792945, -0.25795437774916247, -0.2919240467557002, 0.03338596326861212, -0.29092820646900047, -0.15719783486565575, 0.1351611241669871, 0.023812955675544444... |
1,801.03294 | A First Look at Identity Management Schemes on the Blockchain | The emergence of distributed ledger technology (DLT) based upon a blockchain
data structure, has given rise to new approaches to identity management that
aim to upend dominant approaches to providing and consuming digital identities.
These new approaches to identity management (IdM) propose to enhance
decentralisatio... | cs.CR | the emergence of distributed ledger technology dlt based upon a blockchain data structure has given rise to new approaches to identity management that aim to upend dominant approaches to providing and consuming digital identities these new approaches to identity management idm propose to enhance decentralisation transp... | [['the', 'emergence', 'of', 'distributed', 'ledger', 'technology', 'dlt', 'based', 'upon', 'a', 'blockchain', 'data', 'structure', 'has', 'given', 'rise', 'to', 'new', 'approaches', 'to', 'identity', 'management', 'that', 'aim', 'to', 'upend', 'dominant', 'approaches', 'to', 'providing', 'and', 'consuming', 'digital', ... | [-0.13444384555147942, -0.004485628833892838, -0.10276716965133104, 0.06673214595654223, -0.1815550086355888, -0.22046072573613118, 0.08514931952894324, 0.34806231238722507, -0.2725409244343934, -0.31621493384389593, 0.08378146916033129, -0.2434935522044428, -0.16268141541888217, 0.1892311581650214, -0.1451595891820322... |
1,801.03295 | On the origin of the quasi-particle peak in Cr(001) surfaces | In the spectral density of Cr(001) surfaces a sharp resonance close to the
Fermi level is observed in both experiment and theory. For the physical origin
of this peak two mechanisms were proposed. A single particle dz2 surface state
renormalised by electron-phonon coupling and an orbital Kondo effect due to the
degen... | cond-mat.str-el | in the spectral density of cr001 surfaces a sharp resonance close to the fermi level is observed in both experiment and theory for the physical origin of this peak two mechanisms were proposed a single particle dz2 surface state renormalised by electronphonon coupling and an orbital kondo effect due to the degenerate d... | [['in', 'the', 'spectral', 'density', 'of', 'cr001', 'surfaces', 'a', 'sharp', 'resonance', 'close', 'to', 'the', 'fermi', 'level', 'is', 'observed', 'in', 'both', 'experiment', 'and', 'theory', 'for', 'the', 'physical', 'origin', 'of', 'this', 'peak', 'two', 'mechanisms', 'were', 'proposed', 'a', 'single', 'particle',... | [-0.15105966332781498, 0.15265269580089602, -0.09876223858709465, 0.13694991422158156, -0.018678349087823114, -0.12945618684675966, 0.08590268551916727, 0.332960583605663, -0.2739992167958814, -0.2849532302100001, -7.143029372014526e-05, -0.3097273360674252, -0.13142851849771894, 0.16449562891008648, 0.0361989126553899... |
1,801.03296 | A derivation of Weyl-Lanczos equations | The Lanczos potential for the Weyl tensor is derived from a quadratic
curvature Lagrangian by making use of the exterior algebra of forms and the
variational principles with constraints.
| gr-qc | the lanczos potential for the weyl tensor is derived from a quadratic curvature lagrangian by making use of the exterior algebra of forms and the variational principles with constraints | [['the', 'lanczos', 'potential', 'for', 'the', 'weyl', 'tensor', 'is', 'derived', 'from', 'a', 'quadratic', 'curvature', 'lagrangian', 'by', 'making', 'use', 'of', 'the', 'exterior', 'algebra', 'of', 'forms', 'and', 'the', 'variational', 'principles', 'with', 'constraints']] | [-0.1572762686630775, 0.05149690941746893, -0.09850209822942471, 0.0009582771895581793, -0.19650960508091697, -0.10764277943185177, -0.0170127528494802, 0.25656634864622146, -0.36532783842292327, -0.26443765941878844, 0.13024174926224455, -0.25639896364561443, -0.21066443159662443, 0.13468884378029355, 0.03931687666295... |
1,801.03297 | Design of Graded Photonic Crystals Antennas via Inverse Scattering based
techniques | A new approach to the design of graded Photonic Crystals (GPCs) devices is
proposed by exploiting the inverse scattering framework as a synthesis tool.
The introduced general methodology can be applied to arbitrary far-field
specifications, thus allowing to design non-canonical devices. In particular,
two different s... | physics.app-ph physics.optics | a new approach to the design of graded photonic crystals gpcs devices is proposed by exploiting the inverse scattering framework as a synthesis tool the introduced general methodology can be applied to arbitrary farfield specifications thus allowing to design noncanonical devices in particular two different strategies ... | [['a', 'new', 'approach', 'to', 'the', 'design', 'of', 'graded', 'photonic', 'crystals', 'gpcs', 'devices', 'is', 'proposed', 'by', 'exploiting', 'the', 'inverse', 'scattering', 'framework', 'as', 'a', 'synthesis', 'tool', 'the', 'introduced', 'general', 'methodology', 'can', 'be', 'applied', 'to', 'arbitrary', 'farfie... | [-0.09788635703643747, 0.0818923178131371, -0.0853633563965559, 0.02509613614301106, -0.11427577881422503, -0.169376360164237, 0.002287060755846742, 0.40162630790077586, -0.29560957491105677, -0.29806190568442437, 0.1045202737410851, -0.19157050560027652, -0.18002345925197005, 0.21286894834533432, -0.05789050721254099,... |
1,801.03298 | Imaging black holes: past, present and future | This paper briefly reviews past, current, and future efforts to image black
holes in the radio regime. Black holes seem like mystical objects, but they are
an integral part of current astrophysics and are at the center of attempts to
unify quantum physics and general relativity. Yet, nobody has ever seen a black
hole... | astro-ph.HE astro-ph.IM | this paper briefly reviews past current and future efforts to image black holes in the radio regime black holes seem like mystical objects but they are an integral part of current astrophysics and are at the center of attempts to unify quantum physics and general relativity yet nobody has ever seen a black hole what do... | [['this', 'paper', 'briefly', 'reviews', 'past', 'current', 'and', 'future', 'efforts', 'to', 'image', 'black', 'holes', 'in', 'the', 'radio', 'regime', 'black', 'holes', 'seem', 'like', 'mystical', 'objects', 'but', 'they', 'are', 'an', 'integral', 'part', 'of', 'current', 'astrophysics', 'and', 'are', 'at', 'the', 'c... | [-0.09661300115753857, 0.09778923818178545, -0.08923370986320507, 0.11717784700030283, -0.14311279442118502, -0.1125453609320419, 0.012245913392550158, 0.4082996528720576, -0.17555757290309018, -0.35276369179395595, 0.15637132512955032, -0.32836480170017346, -0.06392965945629296, 0.2348522335381008, -0.0799065241592372... |
1,801.03299 | Simultaneous Tensor Completion and Denoising by Noise Inequality
Constrained Convex Optimization | Tensor completion is a technique of filling missing elements of the
incomplete data tensors. It being actively studied based on the convex
optimization scheme such as nuclear-norm minimization. When given data tensors
include some noises, the nuclear-norm minimization problem is usually converted
to the nuclear-norm ... | cs.CV | tensor completion is a technique of filling missing elements of the incomplete data tensors it being actively studied based on the convex optimization scheme such as nuclearnorm minimization when given data tensors include some noises the nuclearnorm minimization problem is usually converted to the nuclearnorm regulari... | [['tensor', 'completion', 'is', 'a', 'technique', 'of', 'filling', 'missing', 'elements', 'of', 'the', 'incomplete', 'data', 'tensors', 'it', 'being', 'actively', 'studied', 'based', 'on', 'the', 'convex', 'optimization', 'scheme', 'such', 'as', 'nuclearnorm', 'minimization', 'when', 'given', 'data', 'tensors', 'includ... | [-0.05481588874911714, 0.029336498843299016, -0.06317775099713387, 0.09352864767026761, -0.09883610618103725, -0.1864558915890212, -0.0048269820528932745, 0.39745490382720006, -0.34861636334934676, -0.3433422587939307, 0.1754742397331736, -0.27082666096578023, -0.183438482027676, 0.15911007060920104, -0.122296649385562... |
1,801.033 | Shapley effects for sensitivity analysis with dependent inputs:
bootstrap and kriging-based algorithms | In global sensitivity analysis, the well known Sobol' sensitivity indices aim
to quantify how the variance in the output of a mathematical model can be
apportioned to the different variances of its input random variables. These
indices are based on the functional variance decomposition and their
interpretation become... | math.ST stat.TH | in global sensitivity analysis the well known sobol sensitivity indices aim to quantify how the variance in the output of a mathematical model can be apportioned to the different variances of its input random variables these indices are based on the functional variance decomposition and their interpretation become diff... | [['in', 'global', 'sensitivity', 'analysis', 'the', 'well', 'known', 'sobol', 'sensitivity', 'indices', 'aim', 'to', 'quantify', 'how', 'the', 'variance', 'in', 'the', 'output', 'of', 'a', 'mathematical', 'model', 'can', 'be', 'apportioned', 'to', 'the', 'different', 'variances', 'of', 'its', 'input', 'random', 'variab... | [-0.06774387308929246, 0.0485108427457808, -0.10693232171858351, 0.13053868315472217, -0.05102361025333877, -0.09672538319426538, 0.0838978704336141, 0.38758030537034, -0.21805258920481105, -0.3452085655701546, 0.1337338967135278, -0.2682612070243861, -0.14576821706509124, 0.17295227612401196, -0.09576505482363612, 0.0... |
1,801.03301 | An ab-initio study of the electron-phonon coupling within a
Cr(001)-surface | It is experimentally well established that the Cr(001)-surface exhibits a
sharp resonance around the Fermi level. However, there is no consensus about
its physical origin. It is proposed to be either due to a single particle dz2
surface state renormalised by electron-phonon coupling or the orbital Kondo
effect involv... | cond-mat.mtrl-sci cond-mat.mes-hall | it is experimentally well established that the cr001surface exhibits a sharp resonance around the fermi level however there is no consensus about its physical origin it is proposed to be either due to a single particle dz2 surface state renormalised by electronphonon coupling or the orbital kondo effect involving the d... | [['it', 'is', 'experimentally', 'well', 'established', 'that', 'the', 'cr001surface', 'exhibits', 'a', 'sharp', 'resonance', 'around', 'the', 'fermi', 'level', 'however', 'there', 'is', 'no', 'consensus', 'about', 'its', 'physical', 'origin', 'it', 'is', 'proposed', 'to', 'be', 'either', 'due', 'to', 'a', 'single', 'pa... | [-0.12069327490469996, 0.16631187845349923, -0.05446364615628872, 0.08249417075120068, -0.022349129638446426, -0.12626207246652615, 0.08373496435290695, 0.3738156398770356, -0.24096187216910134, -0.2927148452516008, 0.00946737853617171, -0.31713979520926666, -0.12239637181833579, 0.19148744060356324, 0.0381386820757713... |
1,801.03302 | An improvement in the linear stable ranges for ordered configuration
spaces | Recently, Church-Miller-Nagpal-Reinhold [arXiv:1706.03845] obtained linear
stable ranges for the integral cohomology of ordered configuration spaces, in
the sense of representation stability. We note that the constants in these
linear stable ranges can be further improved for an orientable manifold of
dimension at le... | math.RT math.AT | recently churchmillernagpalreinhold arxiv170603845 obtained linear stable ranges for the integral cohomology of ordered configuration spaces in the sense of representation stability we note that the constants in these linear stable ranges can be further improved for an orientable manifold of dimension at least 3 the id... | [['recently', 'churchmillernagpalreinhold', 'arxiv170603845', 'obtained', 'linear', 'stable', 'ranges', 'for', 'the', 'integral', 'cohomology', 'of', 'ordered', 'configuration', 'spaces', 'in', 'the', 'sense', 'of', 'representation', 'stability', 'we', 'note', 'that', 'the', 'constants', 'in', 'these', 'linear', 'stabl... | [-0.1401343324083697, 0.12885464645336875, -0.09640763959571443, 0.07114730531530869, -0.07593741492989163, -0.0861874256214058, -0.0028240702878166405, 0.39756194329648104, -0.35116408955892203, -0.2589163616368616, 0.13313954937944394, -0.19529807912530722, -0.13491528367416727, 0.16854814027815504, -0.11374192457232... |
1,801.03303 | Recent IR-Improved results for LHC/FCC physics | We present recent developments in the theory and application of IR-improved
QED$\otimes$QCD resummation methods, realized by MC event generator methods,
for LHC and FCC physics scenarios.
| hep-ph | we present recent developments in the theory and application of irimproved qedotimesqcd resummation methods realized by mc event generator methods for lhc and fcc physics scenarios | [['we', 'present', 'recent', 'developments', 'in', 'the', 'theory', 'and', 'application', 'of', 'irimproved', 'qedotimesqcd', 'resummation', 'methods', 'realized', 'by', 'mc', 'event', 'generator', 'methods', 'for', 'lhc', 'and', 'fcc', 'physics', 'scenarios']] | [-0.011248002778022336, 0.08704016903916803, -0.1065372044686228, 0.14196968608750746, -0.018112077521016963, -0.1117463677835006, -0.046012495416037455, 0.4030423970319904, -0.16960434701580268, -0.2901797090442135, 0.12752180696518806, -0.2871335473520538, -0.13149464116073573, 0.2290858530367796, 0.01308996051263350... |
1,801.03304 | Quantum frequency conversion to telecom of single photons from a
nitrogen-vacancy center in diamond | We report on the conversion to telecom wavelength of single photons emitted
by a nitrogen-vacancy (NV) defect in diamond. By means of difference frequency
generation, we convert spin-selective photons at 637 nm, associated with the
coherent NV zero-phonon-line, to the target wavelength of 1588 nm in the
L-telecom ban... | quant-ph | we report on the conversion to telecom wavelength of single photons emitted by a nitrogenvacancy nv defect in diamond by means of difference frequency generation we convert spinselective photons at 637 nm associated with the coherent nv zerophononline to the target wavelength of 1588 nm in the ltelecom band the success... | [['we', 'report', 'on', 'the', 'conversion', 'to', 'telecom', 'wavelength', 'of', 'single', 'photons', 'emitted', 'by', 'a', 'nitrogenvacancy', 'nv', 'defect', 'in', 'diamond', 'by', 'means', 'of', 'difference', 'frequency', 'generation', 'we', 'convert', 'spinselective', 'photons', 'at', '637', 'nm', 'associated', 'wi... | [-0.10259979708314819, 0.17376470150205947, -0.0035286238315059754, -0.025556100282799383, 0.07024667401675706, -0.16035856737884402, 0.1049752012897881, 0.5089438008348437, -0.2006870823692238, -0.3237814098820906, -0.0050594980180956916, -0.32862747151975646, 0.017759987100428584, 0.2120584771801874, -0.0071314341336... |
1,801.03305 | Probabilistic performance estimators for computational chemistry
methods: the empirical cumulative distribution function of absolute errors | Benchmarking studies in computational chemistry use reference datasets to
assess the accuracy of a method through error statistics. The commonly used
error statistics, such as the mean signed and mean unsigned errors, do not
inform end-users on the expected amplitude of prediction errors attached to
these methods. We... | physics.chem-ph physics.data-an | benchmarking studies in computational chemistry use reference datasets to assess the accuracy of a method through error statistics the commonly used error statistics such as the mean signed and mean unsigned errors do not inform endusers on the expected amplitude of prediction errors attached to these methods we show t... | [['benchmarking', 'studies', 'in', 'computational', 'chemistry', 'use', 'reference', 'datasets', 'to', 'assess', 'the', 'accuracy', 'of', 'a', 'method', 'through', 'error', 'statistics', 'the', 'commonly', 'used', 'error', 'statistics', 'such', 'as', 'the', 'mean', 'signed', 'and', 'mean', 'unsigned', 'errors', 'do', '... | [-0.043622187546464956, 0.042187288240215406, -0.07940959300718863, 0.17896815235872054, -0.035859871430809355, -0.10714471437015825, 0.11813656411620534, 0.39159496153958817, -0.22242146294394677, -0.36989056860329583, 0.10782641898086612, -0.2593676032900641, -0.08996254311535846, 0.23841405300547855, -0.144126935404... |
1,801.03306 | Secure Quantum Network Code without Classical Communication | We consider the secure quantum communication over a network with the presence
of a malicious adversary who can eavesdrop and contaminate the states. The
network consists of noiseless quantum channels with the unit capacity and the
nodes which applies noiseless quantum operations. As the main result, when the
maximum ... | quant-ph | we consider the secure quantum communication over a network with the presence of a malicious adversary who can eavesdrop and contaminate the states the network consists of noiseless quantum channels with the unit capacity and the nodes which applies noiseless quantum operations as the main result when the maximum numbe... | [['we', 'consider', 'the', 'secure', 'quantum', 'communication', 'over', 'a', 'network', 'with', 'the', 'presence', 'of', 'a', 'malicious', 'adversary', 'who', 'can', 'eavesdrop', 'and', 'contaminate', 'the', 'states', 'the', 'network', 'consists', 'of', 'noiseless', 'quantum', 'channels', 'with', 'the', 'unit', 'capac... | [-0.21720275454920185, 0.07429075700096543, -0.01035311870107064, 0.022901108172325324, -0.001709536039753694, -0.24086450566918408, 0.116487266611507, 0.3003805146769345, -0.2798412887104231, -0.27829881270164214, 0.11769219895871649, -0.2561065109282638, -0.14163007716203121, 0.19209666936160447, -0.09610735074655041... |
1,801.03307 | Piezoelectric field, exciton lifetime, and cathodoluminescence intensity
at threading dislocations in GaN{0001} | The strain field of a dislocation emerging at a free surface is partially
relaxed to ensure stress free boundary conditions. We show that this relaxation
strain at the outcrop of edge threading dislocations in GaN{0001} gives rise to
a piezoelectric volume charge. The electric field produced by this charge
distributi... | cond-mat.mtrl-sci | the strain field of a dislocation emerging at a free surface is partially relaxed to ensure stress free boundary conditions we show that this relaxation strain at the outcrop of edge threading dislocations in gan0001 gives rise to a piezoelectric volume charge the electric field produced by this charge distribution is ... | [['the', 'strain', 'field', 'of', 'a', 'dislocation', 'emerging', 'at', 'a', 'free', 'surface', 'is', 'partially', 'relaxed', 'to', 'ensure', 'stress', 'free', 'boundary', 'conditions', 'we', 'show', 'that', 'this', 'relaxation', 'strain', 'at', 'the', 'outcrop', 'of', 'edge', 'threading', 'dislocations', 'in', 'gan000... | [-0.15270981991377014, 0.21007784270944121, -0.057802445717896216, -0.005917993262231063, -0.019727899451166965, -0.05884877188752095, 0.03003389173402236, 0.4356467740562482, -0.2812054853599805, -0.2783200196348704, 0.009214554416338125, -0.24439552474098328, -0.06603536773950626, 0.11173407649860168, -0.018834081911... |
1,801.03308 | On minimal actions of countable groups | Our purpose here is to review some recent developments in the theory of
dynamical systems whose common theme is a link between minimal dynamical
systems, certain Ramsey type combinatorial properties, and the Lovasz local
lemma (LLL). For a general countable group G the two classes of minimal systems
we will deal with... | math.DS math.PR | our purpose here is to review some recent developments in the theory of dynamical systems whose common theme is a link between minimal dynamical systems certain ramsey type combinatorial properties and the lovasz local lemma lll for a general countable group g the two classes of minimal systems we will deal with are i ... | [['our', 'purpose', 'here', 'is', 'to', 'review', 'some', 'recent', 'developments', 'in', 'the', 'theory', 'of', 'dynamical', 'systems', 'whose', 'common', 'theme', 'is', 'a', 'link', 'between', 'minimal', 'dynamical', 'systems', 'certain', 'ramsey', 'type', 'combinatorial', 'properties', 'and', 'the', 'lovasz', 'local... | [-0.23204123336712226, 0.15463381610153354, -0.054952332180212525, 0.08565253945451011, -0.08561895581729272, -0.1731073561206679, 0.05480773294454112, 0.313149395672714, -0.3349899666274295, -0.22922706252352595, 0.10886186530868358, -0.28991214307298996, -0.1528462739661336, 0.15560106192783946, -0.15376970954650246,... |
1,801.03309 | Bounds on graviton mass using weak lensing and SZ effect in galaxy
clusters | In General Relativity (GR), the graviton is massless. However, a common
feature in several theoretical alternatives of GR is a non-zero mass for the
graviton. These theories can be described as massive gravity theories. Despite
many theoretical complexities in these theories, on phenomenological grounds,
the implicat... | astro-ph.CO astro-ph.GA astro-ph.HE gr-qc | in general relativity gr the graviton is massless however a common feature in several theoretical alternatives of gr is a nonzero mass for the graviton these theories can be described as massive gravity theories despite many theoretical complexities in these theories on phenomenological grounds the implications of mass... | [['in', 'general', 'relativity', 'gr', 'the', 'graviton', 'is', 'massless', 'however', 'a', 'common', 'feature', 'in', 'several', 'theoretical', 'alternatives', 'of', 'gr', 'is', 'a', 'nonzero', 'mass', 'for', 'the', 'graviton', 'these', 'theories', 'can', 'be', 'described', 'as', 'massive', 'gravity', 'theories', 'des... | [-0.1028407406834204, 0.1387654727001152, -0.10584760668301364, 0.15558951996504108, -0.11046241706169051, -0.09221698548531206, 0.021730929758490586, 0.3075530401885328, -0.14353891069342087, -0.3340903177630247, 0.036409580906307915, -0.25859698022874755, -0.04906813599759849, 0.2323578139028807, 0.010787506097013403... |
1,801.0331 | Length-scale dependent average structures, piezoelectricity enhancement
and depolarization mechanisms in a non-MPB high-performance piezoelectric
alloy system PbTiO3-Bi(Zr1/2Ni1/2)O3 | There is a general perception that large piezoelectric response in
ferroelectric alloys requires tuning the system towards a morphotropic phase
boundary (MPB), i.e., a composition driven inter-ferroelectric instability.
Here we show that high piezoelectric response can be realized even in non-MPB
alloy systems. This ... | cond-mat.mtrl-sci | there is a general perception that large piezoelectric response in ferroelectric alloys requires tuning the system towards a morphotropic phase boundary mpb ie a composition driven interferroelectric instability here we show that high piezoelectric response can be realized even in nonmpb alloy systems this is demonstra... | [['there', 'is', 'a', 'general', 'perception', 'that', 'large', 'piezoelectric', 'response', 'in', 'ferroelectric', 'alloys', 'requires', 'tuning', 'the', 'system', 'towards', 'a', 'morphotropic', 'phase', 'boundary', 'mpb', 'ie', 'a', 'composition', 'driven', 'interferroelectric', 'instability', 'here', 'we', 'show', ... | [-0.1740801235055099, 0.20065732288753016, -0.0645011006843172, -0.03500963721675256, -0.09211496997950147, -0.12595279667259746, 0.06182682533489622, 0.405534090727423, -0.26396780460168723, -0.24470839733755198, 0.09663880135789424, -0.24754374148776231, -0.19323087030641953, 0.17332240959032646, -0.02995939840909238... |
1,801.03311 | The effect of microwaves on superconductors for kinetic inductance
detection and parametric amplification | We address, using concepts of the microscopic theory of superconductivity,
parametric amplifiers and kinetic inductance detectors focusing on the
interaction of microwave radiation with the superconducting condensate. This
interaction was identified recently as the source of the apparent dissipation
in microwave supe... | cond-mat.supr-con | we address using concepts of the microscopic theory of superconductivity parametric amplifiers and kinetic inductance detectors focusing on the interaction of microwave radiation with the superconducting condensate this interaction was identified recently as the source of the apparent dissipation in microwave supercond... | [['we', 'address', 'using', 'concepts', 'of', 'the', 'microscopic', 'theory', 'of', 'superconductivity', 'parametric', 'amplifiers', 'and', 'kinetic', 'inductance', 'detectors', 'focusing', 'on', 'the', 'interaction', 'of', 'microwave', 'radiation', 'with', 'the', 'superconducting', 'condensate', 'this', 'interaction',... | [-0.13167826239285724, 0.12541224551504065, -0.05784271892376377, 0.05155104214125978, -0.05279384433067337, -0.11772482824328888, 0.04655529048406087, 0.3548615006231038, -0.1940763526945375, -0.31003785389475524, 0.05235474664680494, -0.2809773961780593, -0.09806525214142832, 0.24288479668653704, 0.007389266218524426... |
1,801.03312 | Continuum spectral energy distribution of GRB, SLSN, SB and AGN host
galaxies at intermediate redshifts | Continuum SED models of gamma-ray burst (GRB) and obscured GRB host galaxies
at moderately high redshifts are presented and compared with those of
superluminous supernovae (SLSN), starburst (SB) and active galactic nuclei
(AGN). We consider that continuum radiation (bremsstrahlung) is emitted from
the same clouds whi... | astro-ph.GA | continuum sed models of gammaray burst grb and obscured grb host galaxies at moderately high redshifts are presented and compared with those of superluminous supernovae slsn starburst sb and active galactic nuclei agn we consider that continuum radiation bremsstrahlung is emitted from the same clouds which emit the lin... | [['continuum', 'sed', 'models', 'of', 'gammaray', 'burst', 'grb', 'and', 'obscured', 'grb', 'host', 'galaxies', 'at', 'moderately', 'high', 'redshifts', 'are', 'presented', 'and', 'compared', 'with', 'those', 'of', 'superluminous', 'supernovae', 'slsn', 'starburst', 'sb', 'and', 'active', 'galactic', 'nuclei', 'agn', '... | [0.015947549471862076, 0.09318842863150663, -0.039828859382433836, 0.16266432362917652, -0.0841073507356659, -0.10143573942459813, 0.05282396872614309, 0.4917009358111884, -0.1251356573853421, -0.32272201398694794, 0.0004857986794602241, -0.34242618948607656, 0.058387606216409454, 0.19446174371579528, -0.01715977732743... |
1,801.03313 | The Reidemeister graph is a complete knot invariant | We describe two locally finite graphs naturally associated to each knot type
K, called Reidemeister graphs. We determine several local and global properties
of these graphs and prove that in one case the graph-isomorphism type is a
complete knot invariant up to mirroring. Lastly, we introduce another object,
relating... | math.GT | we describe two locally finite graphs naturally associated to each knot type k called reidemeister graphs we determine several local and global properties of these graphs and prove that in one case the graphisomorphism type is a complete knot invariant up to mirroring lastly we introduce another object relating the rei... | [['we', 'describe', 'two', 'locally', 'finite', 'graphs', 'naturally', 'associated', 'to', 'each', 'knot', 'type', 'k', 'called', 'reidemeister', 'graphs', 'we', 'determine', 'several', 'local', 'and', 'global', 'properties', 'of', 'these', 'graphs', 'and', 'prove', 'that', 'in', 'one', 'case', 'the', 'graphisomorphism... | [-0.19353767684660853, 0.09526637364178896, -0.08489798197212318, 0.1311623903728711, -0.1531418931360046, -0.1581384902819991, 0.023441994274617173, 0.3854833382375849, -0.3388813861956199, -0.28205157813305654, 0.11084458033825892, -0.24843885727847617, -0.16589643792249262, 0.14761447737303873, -0.12998599554412066,... |
1,801.03314 | BigRoots: An Effective Approach for Root-cause Analysis of Stragglers in
Big Data System | Stragglers are commonly believed to have a great impact on the performance of
big data system. However, the reason to cause straggler is complicated.
Previous works mostly focus on straggler detection, schedule level optimization
and coarse-grained cause analysis. These methods cannot provide valuable
insights to hel... | cs.DC | stragglers are commonly believed to have a great impact on the performance of big data system however the reason to cause straggler is complicated previous works mostly focus on straggler detection schedule level optimization and coarsegrained cause analysis these methods cannot provide valuable insights to help users ... | [['stragglers', 'are', 'commonly', 'believed', 'to', 'have', 'a', 'great', 'impact', 'on', 'the', 'performance', 'of', 'big', 'data', 'system', 'however', 'the', 'reason', 'to', 'cause', 'straggler', 'is', 'complicated', 'previous', 'works', 'mostly', 'focus', 'on', 'straggler', 'detection', 'schedule', 'level', 'optim... | [-0.12823631103538838, -0.00016414039762493987, -0.06889918448276217, 0.08965273166468703, -0.10575825988491476, -0.18147420484040463, 0.09888712466645246, 0.3984748417025675, -0.25135776094849344, -0.40428090575064374, 0.1124450409964236, -0.2547785234203713, -0.1532934015755605, 0.20796083247069247, -0.15122304152789... |
1,801.03315 | Chemical and valence reconstruction at the surface of SmB6 revealed with
resonant soft x-ray reflectometry | Samarium hexaboride (SmB$_6$), a Kondo insulator with mixed valence, has
recently attracted much attention as a possible host for correlated topological
surface states. Here, we use a combination of x-ray absorption and
reflectometry techniques, backed up with a theoretical model for the resonant
$M_{4,5}$ absorption... | cond-mat.str-el | samarium hexaboride smb_6 a kondo insulator with mixed valence has recently attracted much attention as a possible host for correlated topological surface states here we use a combination of xray absorption and reflectometry techniques backed up with a theoretical model for the resonant m_45 absorption edge of sm and p... | [['samarium', 'hexaboride', 'smb_6', 'a', 'kondo', 'insulator', 'with', 'mixed', 'valence', 'has', 'recently', 'attracted', 'much', 'attention', 'as', 'a', 'possible', 'host', 'for', 'correlated', 'topological', 'surface', 'states', 'here', 'we', 'use', 'a', 'combination', 'of', 'xray', 'absorption', 'and', 'reflectome... | [-0.08404711811255189, 0.19389846660804166, -0.06720002199326475, 0.042029265363509795, -0.007360687647130548, -0.1848985232884261, 0.15467149929016227, 0.42670779564903805, -0.2695682014176703, -0.3502804805699632, 0.031656553880571855, -0.35268260883051694, -0.07323184905151449, 0.19056169321704136, 0.023821187039485... |
1,801.03316 | Modeling of gap gene regulatory networks in Drosophila with the account
of the gene modular structure (in Russian) | Genes are frequently regulated in complex manners, necessitating modelling
approaches which go beyond simple (linear) gene-to-gene interactions and
address the modularity of cis-regulatory regions and alternate transcription
initiation sites. In particular, sharp expression patterns (peaks or stripes)
indicate that g... | q-bio.MN | genes are frequently regulated in complex manners necessitating modelling approaches which go beyond simple linear genetogene interactions and address the modularity of cisregulatory regions and alternate transcription initiation sites in particular sharp expression patterns peaks or stripes indicate that gene regulati... | [['genes', 'are', 'frequently', 'regulated', 'in', 'complex', 'manners', 'necessitating', 'modelling', 'approaches', 'which', 'go', 'beyond', 'simple', 'linear', 'genetogene', 'interactions', 'and', 'address', 'the', 'modularity', 'of', 'cisregulatory', 'regions', 'and', 'alternate', 'transcription', 'initiation', 'sit... | [-0.14395069169973873, 0.09051328189266117, 0.018520946968245605, 0.12459692689893848, -0.02332252188909637, -0.1419229006819913, 0.07371821667057583, 0.38569339076462, -0.26440346637821716, -0.24191786299419143, 0.01271831035796229, -0.22390759420054762, -0.23939842552796978, 0.1649552379876537, -0.038694623169367726,... |
1,801.03317 | Radio-based Traffic Flow Detection and Vehicle Classification for Future
Smart Cities | Intelligent Transportation Systems (ITSs) providing vehicle-related
statistical data are one of the key components for future smart cities. In this
context, knowledge about the current traffic flow is used for travel time
reduction and proactive jam avoidance by intelligent traffic control
mechanisms. In addition, th... | cs.NI | intelligent transportation systems itss providing vehiclerelated statistical data are one of the key components for future smart cities in this context knowledge about the current traffic flow is used for travel time reduction and proactive jam avoidance by intelligent traffic control mechanisms in addition the monitor... | [['intelligent', 'transportation', 'systems', 'itss', 'providing', 'vehiclerelated', 'statistical', 'data', 'are', 'one', 'of', 'the', 'key', 'components', 'for', 'future', 'smart', 'cities', 'in', 'this', 'context', 'knowledge', 'about', 'the', 'current', 'traffic', 'flow', 'is', 'used', 'for', 'travel', 'time', 'redu... | [-0.1694445866190933, 0.027835239887558268, -0.03662213305665168, 0.02220618287301838, -0.06085355463900313, -0.16038295484166468, 0.08407331480789584, 0.3721117087892744, -0.2307384077703198, -0.36743137354203903, 0.163830405286982, -0.282126820653936, -0.11099663263939272, 0.23293119259887923, -0.19145059636146422, 0... |
1,801.03318 | Unsupervised Despeckling | Contrast and quality of ultrasound images are adversely affected by the
excessive presence of speckle. However, being an inherent imaging property,
speckle helps in tissue characterization and tracking. Thus, despeckling of the
ultrasound images requires the reduction of speckle extent without any
oversmoothing. In t... | cs.CV | contrast and quality of ultrasound images are adversely affected by the excessive presence of speckle however being an inherent imaging property speckle helps in tissue characterization and tracking thus despeckling of the ultrasound images requires the reduction of speckle extent without any oversmoothing in this lett... | [['contrast', 'and', 'quality', 'of', 'ultrasound', 'images', 'are', 'adversely', 'affected', 'by', 'the', 'excessive', 'presence', 'of', 'speckle', 'however', 'being', 'an', 'inherent', 'imaging', 'property', 'speckle', 'helps', 'in', 'tissue', 'characterization', 'and', 'tracking', 'thus', 'despeckling', 'of', 'the',... | [-0.02521869819975109, -0.006245889916158376, -0.05565914978797082, 0.05702281716548896, -0.09532827252405696, -0.15190161397549673, -0.0016098971755127423, 0.45392426746548153, -0.2946083505448769, -0.33321405413153116, 0.04636174511506397, -0.29286962240439607, -0.23735739184121485, 0.15856514283223078, -0.2198285245... |
1,801.03319 | No eigenvalues outside the limiting support of the spectral distribution
of general sample covariance matrices | This paper is to investigate the spectral properties of sample covariance
matrices under a more general population. We consider a class of matrices of
the form $\mathbf S_n=\frac1n\mathbf B_n\mathbf X_n\mathbf X_n^*\mathbf B_n^*$,
where $\mathbf B_n$ is a $p\times m$ non-random matrix and $\mathbf X_n$ is an
$m\times... | math.PR | this paper is to investigate the spectral properties of sample covariance matrices under a more general population we consider a class of matrices of the form mathbf s_nfrac1nmathbf b_nmathbf x_nmathbf x_nmathbf b_n where mathbf b_n is a ptimes m nonrandom matrix and mathbf x_n is an mtimes n matrix consisting of iid s... | [['this', 'paper', 'is', 'to', 'investigate', 'the', 'spectral', 'properties', 'of', 'sample', 'covariance', 'matrices', 'under', 'a', 'more', 'general', 'population', 'we', 'consider', 'a', 'class', 'of', 'matrices', 'of', 'the', 'form', 'mathbf', 's_nfrac1nmathbf', 'b_nmathbf', 'x_nmathbf', 'x_nmathbf', 'b_n', 'where... | [-0.17750518766782938, 0.1436596853553623, -0.007254198022665234, 0.016078024042061094, -0.009623259493927344, -0.15911546208118216, -0.00856613944425598, 0.36916954470200275, -0.2570296172736161, -0.13573162715642825, 0.1102083416211359, -0.3089425282706635, -0.12350625916567862, 0.11995006480399485, -0.10863920025006... |
1,801.0332 | A Canonical Form for a Symplectic Involution | We present a canonical form for a symplectic involution $S\in
Sp(2g,\mathbb{Z})$, $S^2=1$; the construction is algorithmic. Application is
made in the Riemann surface setting.
| math.RT math-ph math.MP math.SG | we present a canonical form for a symplectic involution sin sp2gmathbbz s21 the construction is algorithmic application is made in the riemann surface setting | [['we', 'present', 'a', 'canonical', 'form', 'for', 'a', 'symplectic', 'involution', 'sin', 'sp2gmathbbz', 's21', 'the', 'construction', 'is', 'algorithmic', 'application', 'is', 'made', 'in', 'the', 'riemann', 'surface', 'setting']] | [-0.2325743647137036, 0.04879283924431851, -0.1190047535346821, 0.038546412921277806, -0.1450497619031618, -0.1270240058268731, 0.0009775027380480121, 0.3657708168029785, -0.25384009070694447, -0.18967268522828817, 0.09604508111078758, -0.2198511912332227, -0.23258984927088022, 0.21190062685248753, -0.16447241709101945... |
1,801.03321 | Primordial Black Holes from Inflaton Fragmentation into Oscillons | We show that fragmentation of the inflaton into long-lived spatially
localized oscillon configurations can lead to copious production of black
holes. In a single-field inflation model primordial black holes of sublunar
mass can form, and they can account for all of the dark matter. We also explore
the possibility tha... | astro-ph.CO gr-qc hep-ph hep-th | we show that fragmentation of the inflaton into longlived spatially localized oscillon configurations can lead to copious production of black holes in a singlefield inflation model primordial black holes of sublunar mass can form and they can account for all of the dark matter we also explore the possibility that solar... | [['we', 'show', 'that', 'fragmentation', 'of', 'the', 'inflaton', 'into', 'longlived', 'spatially', 'localized', 'oscillon', 'configurations', 'can', 'lead', 'to', 'copious', 'production', 'of', 'black', 'holes', 'in', 'a', 'singlefield', 'inflation', 'model', 'primordial', 'black', 'holes', 'of', 'sublunar', 'mass', '... | [-0.16338882758634898, 0.25559753323481843, -0.09266750548020795, 0.2370085547621729, -0.07653087543351858, -0.1002501851709729, -0.05841229018529482, 0.2920502975413745, -0.17220132905199673, -0.3184349823912436, 0.010346195976263985, -0.2675691873018602, -0.07393591923579207, 0.20598631820316907, 0.02945280982407205,... |
1,801.03322 | Ballistic electron channels including weakly protected topological
states in delaminated bilayer graphene | We show that delaminations in bilayer graphene (BLG) with electrostatically
induced interlayer asymmetry can provide one with ballistic channels for
electrons with energies inside the electrostatically induced BLG gap. These
channels are formed by a combination of valley-polarised evanescent states
propagating along ... | cond-mat.mes-hall | we show that delaminations in bilayer graphene blg with electrostatically induced interlayer asymmetry can provide one with ballistic channels for electrons with energies inside the electrostatically induced blg gap these channels are formed by a combination of valleypolarised evanescent states propagating along the de... | [['we', 'show', 'that', 'delaminations', 'in', 'bilayer', 'graphene', 'blg', 'with', 'electrostatically', 'induced', 'interlayer', 'asymmetry', 'can', 'provide', 'one', 'with', 'ballistic', 'channels', 'for', 'electrons', 'with', 'energies', 'inside', 'the', 'electrostatically', 'induced', 'blg', 'gap', 'these', 'chann... | [-0.18327059099415327, 0.2041361058586963, -0.023274992350671514, 0.0273714995744419, -0.019895459227400887, -0.13617391881359486, 0.03402004754924051, 0.42915545837661506, -0.2733079916911711, -0.29445747007597606, 0.013546518402804127, -0.2878284036254912, -0.11980183885887027, 0.14594856429589437, 0.0508044973817852... |
1,801.03323 | Noncommutative quantum Hall effect in graphene | We discuss the quantum Hall effect on a single-layer graphene in the
framework of noncommutative (NC) phase space. We find it induces a shift in the
Hall resistivity. Furthermore, comparison with experimental data reveals an
upper bound on the magnitude of the momentum NC parameter $\eta$ in about
$\sqrt{\eta}\leq 2.... | hep-th cond-mat.mes-hall quant-ph | we discuss the quantum hall effect on a singlelayer graphene in the framework of noncommutative nc phase space we find it induces a shift in the hall resistivity furthermore comparison with experimental data reveals an upper bound on the magnitude of the momentum nc parameter eta in about sqrtetaleq 25 mathrmevc | [['we', 'discuss', 'the', 'quantum', 'hall', 'effect', 'on', 'a', 'singlelayer', 'graphene', 'in', 'the', 'framework', 'of', 'noncommutative', 'nc', 'phase', 'space', 'we', 'find', 'it', 'induces', 'a', 'shift', 'in', 'the', 'hall', 'resistivity', 'furthermore', 'comparison', 'with', 'experimental', 'data', 'reveals', ... | [-0.18730435246240576, 0.17804637725485195, -0.09441619489950184, 0.016026797426427354, -0.016109687143138478, -0.08182056535187425, 0.11568764659424065, 0.3455658228307658, -0.2377229355731789, -0.3170664926838814, -0.019872525191333677, -0.28584454166797957, -0.17469553425147824, 0.2448002299179836, -0.03591286554476... |
1,801.03324 | Homology groups of cubical sets | The paper is devoted to homology groups of cubical sets with coefficients in
contravariant systems of Abelian groups. The study is based on the proof of the
assertion that the homology groups of the category of cubes with coefficients
in the diagram of Abelian groups are isomorphic to the homology groups of
normalize... | math.AT math.CT | the paper is devoted to homology groups of cubical sets with coefficients in contravariant systems of abelian groups the study is based on the proof of the assertion that the homology groups of the category of cubes with coefficients in the diagram of abelian groups are isomorphic to the homology groups of normalized c... | [['the', 'paper', 'is', 'devoted', 'to', 'homology', 'groups', 'of', 'cubical', 'sets', 'with', 'coefficients', 'in', 'contravariant', 'systems', 'of', 'abelian', 'groups', 'the', 'study', 'is', 'based', 'on', 'the', 'proof', 'of', 'the', 'assertion', 'that', 'the', 'homology', 'groups', 'of', 'the', 'category', 'of', ... | [-0.16964057692990306, 0.012879025937397912, -0.11771766806085562, 0.0559073439585152, -0.06873349603747242, -0.07127050651858251, 0.02982514787427867, 0.3234609127173136, -0.3393881122405031, -0.2420167621765714, 0.10729652042594343, -0.23697036245721392, -0.11897609516678528, 0.18384993261652302, -0.1963200822804423,... |
1,801.03325 | Gravitational corrections to light propagation in a perturbed
FLRW-universe and corresponding weak lensing spectra | When the gravitational lensing of the large-scale structure is calculated
from a cosmological model a few assumptions enter: $(i)$ one assumes that the
photons follow unperturbed background geodesics, which is usually referred to
as the Born-approximation, $(ii)$ the lenses move slowly, $(iii)$ the
source-redshift di... | astro-ph.CO | when the gravitational lensing of the largescale structure is calculated from a cosmological model a few assumptions enter i one assumes that the photons follow unperturbed background geodesics which is usually referred to as the bornapproximation ii the lenses move slowly iii the sourceredshift distribution is evaluat... | [['when', 'the', 'gravitational', 'lensing', 'of', 'the', 'largescale', 'structure', 'is', 'calculated', 'from', 'a', 'cosmological', 'model', 'a', 'few', 'assumptions', 'enter', 'i', 'one', 'assumes', 'that', 'the', 'photons', 'follow', 'unperturbed', 'background', 'geodesics', 'which', 'is', 'usually', 'referred', 't... | [-0.09863866672644185, 0.10586362048569653, -0.06758468510583043, 0.12563093111125959, -0.09472407169122662, -0.09773287761956453, -0.021506084714265954, 0.3532237123532428, -0.26823329312519895, -0.3272678606708844, 0.09745343944057822, -0.32366770166981346, -0.09392367000200061, 0.19293987680226565, 0.017804780918070... |
1,801.03326 | Expected Policy Gradients for Reinforcement Learning | We propose expected policy gradients (EPG), which unify stochastic policy
gradients (SPG) and deterministic policy gradients (DPG) for reinforcement
learning. Inspired by expected sarsa, EPG integrates (or sums) across actions
when estimating the gradient, instead of relying only on the action in the
sampled trajecto... | stat.ML cs.AI | we propose expected policy gradients epg which unify stochastic policy gradients spg and deterministic policy gradients dpg for reinforcement learning inspired by expected sarsa epg integrates or sums across actions when estimating the gradient instead of relying only on the action in the sampled trajectory for continu... | [['we', 'propose', 'expected', 'policy', 'gradients', 'epg', 'which', 'unify', 'stochastic', 'policy', 'gradients', 'spg', 'and', 'deterministic', 'policy', 'gradients', 'dpg', 'for', 'reinforcement', 'learning', 'inspired', 'by', 'expected', 'sarsa', 'epg', 'integrates', 'or', 'sums', 'across', 'actions', 'when', 'est... | [-0.04663364418350587, 0.03813407781020336, -0.09923483296491516, 0.08679424270424836, -0.12046148610776679, -0.1609835386358706, 0.11607647734187292, 0.44846660104425, -0.28497098630759865, -0.2501755585972205, 0.11092920785510312, -0.21615695106326407, -0.1953305062840324, 0.21400723822807777, -0.15074745847596205, 0... |
1,801.03327 | Priority Attachment: a Comprehensive Mechanism for Generating Networks | We claim that networks are created according to the priority attachment
mechanism and we show a simple model which uses the priority attachment to
generate both synthetic and close to empirical networks. Priority attachment is
a mechanism which generalizes previously proposed mechanisms, such as small
world creation ... | cs.SI physics.soc-ph | we claim that networks are created according to the priority attachment mechanism and we show a simple model which uses the priority attachment to generate both synthetic and close to empirical networks priority attachment is a mechanism which generalizes previously proposed mechanisms such as small world creation or p... | [['we', 'claim', 'that', 'networks', 'are', 'created', 'according', 'to', 'the', 'priority', 'attachment', 'mechanism', 'and', 'we', 'show', 'a', 'simple', 'model', 'which', 'uses', 'the', 'priority', 'attachment', 'to', 'generate', 'both', 'synthetic', 'and', 'close', 'to', 'empirical', 'networks', 'priority', 'attach... | [-0.10688198296297712, 0.06023117115691039, -0.0599173234948358, 0.08700240628920274, -0.10449519285327749, -0.1388892050977451, 0.11596498050609765, 0.4487373221492925, -0.2572502461940494, -0.33828211595483176, 0.018722340913292095, -0.230781084019074, -0.23697270464232278, 0.13364385768604645, -0.06412867007357691, ... |
1,801.03328 | Near-horizon symmetries of the Schwarzschild black hole with
supertranslation field | Using the exact solution to Einstein equations of Compere and Long for the
Schwarzschild metric containing supertranslation field, we study the
near-horizon symmetries of the metric. We consider class of metrics with
supertranslation field depending only on a spherical angle $\theta $. After
reviewing the action of s... | hep-th gr-qc | using the exact solution to einstein equations of compere and long for the schwarzschild metric containing supertranslation field we study the nearhorizon symmetries of the metric we consider class of metrics with supertranslation field depending only on a spherical angle theta after reviewing the action of supertransl... | [['using', 'the', 'exact', 'solution', 'to', 'einstein', 'equations', 'of', 'compere', 'and', 'long', 'for', 'the', 'schwarzschild', 'metric', 'containing', 'supertranslation', 'field', 'we', 'study', 'the', 'nearhorizon', 'symmetries', 'of', 'the', 'metric', 'we', 'consider', 'class', 'of', 'metrics', 'with', 'supertr... | [-0.2082824500465996, 0.06843214978207572, -0.06060305399443494, 0.06405121036491283, -0.10259609761271166, -0.08362195626217767, -0.015583847811592094, 0.3185120305946369, -0.2013008366914445, -0.23270509396208805, 0.11180336774409268, -0.3093887706067455, -0.13299418314035688, 0.07883352033919498, -0.0594362704916543... |
1,801.03329 | Weakly Supervised One-Shot Detection with Attention Similarity Networks | Neural network models that are not conditioned on class identities were shown
to facilitate knowledge transfer between classes and to be well-suited for
one-shot learning tasks. Following this motivation, we further explore and
establish such models and present a novel neural network architecture for the
task of weak... | stat.ML cs.LG | neural network models that are not conditioned on class identities were shown to facilitate knowledge transfer between classes and to be wellsuited for oneshot learning tasks following this motivation we further explore and establish such models and present a novel neural network architecture for the task of weakly sup... | [['neural', 'network', 'models', 'that', 'are', 'not', 'conditioned', 'on', 'class', 'identities', 'were', 'shown', 'to', 'facilitate', 'knowledge', 'transfer', 'between', 'classes', 'and', 'to', 'be', 'wellsuited', 'for', 'oneshot', 'learning', 'tasks', 'following', 'this', 'motivation', 'we', 'further', 'explore', 'a... | [-0.027480023200252512, 0.018327509254985656, -0.03479540041830067, 0.06699307223080077, -0.12773326737468765, -0.22307221886054004, 0.028127414840813457, 0.448675076349004, -0.2769311543189637, -0.3557363593734909, 0.04449286273144105, -0.23768433453380197, -0.20878962938424092, 0.22894034497068683, -0.116092891751221... |
1,801.0333 | Quantum state transfer in spin chains via shortcuts to adiabaticity | Based on shortcuts to adiabaticity and quantum Zeno dynamics, we present a
protocol to implement quantum state transfer (QST) in a quantum spin-1/2 chain.
In the protocol, the complex Hamiltonian of an $N$-site system is simplified,
and a simple effective Hamiltonian is present. It is shown that only the
control of t... | quant-ph | based on shortcuts to adiabaticity and quantum zeno dynamics we present a protocol to implement quantum state transfer qst in a quantum spin12 chain in the protocol the complex hamiltonian of an nsite system is simplified and a simple effective hamiltonian is present it is shown that only the control of the coupling st... | [['based', 'on', 'shortcuts', 'to', 'adiabaticity', 'and', 'quantum', 'zeno', 'dynamics', 'we', 'present', 'a', 'protocol', 'to', 'implement', 'quantum', 'state', 'transfer', 'qst', 'in', 'a', 'quantum', 'spin12', 'chain', 'in', 'the', 'protocol', 'the', 'complex', 'hamiltonian', 'of', 'an', 'nsite', 'system', 'is', 's... | [-0.21021764021642614, 0.18387646078006636, -0.0774471414393013, 0.044630774301341145, 0.01107299552091117, -0.230516274473223, 0.03494536376205608, 0.38461413619660056, -0.25567338204246415, -0.2618861614061899, 0.059029986018324, -0.23865479647715404, -0.10758286370280949, 0.22074983344024535, 0.005558400315422456, 0... |
1,801.03331 | Reasoning about Unforeseen Possibilities During Policy Learning | Methods for learning optimal policies in autonomous agents often assume that
the way the domain is conceptualised---its possible states and actions and
their causal structure---is known in advance and does not change during
learning. This is an unrealistic assumption in many scenarios, because new
evidence can reveal... | cs.AI | methods for learning optimal policies in autonomous agents often assume that the way the domain is conceptualisedits possible states and actions and their causal structureis known in advance and does not change during learning this is an unrealistic assumption in many scenarios because new evidence can reveal important... | [['methods', 'for', 'learning', 'optimal', 'policies', 'in', 'autonomous', 'agents', 'often', 'assume', 'that', 'the', 'way', 'the', 'domain', 'is', 'conceptualisedits', 'possible', 'states', 'and', 'actions', 'and', 'their', 'causal', 'structureis', 'known', 'in', 'advance', 'and', 'does', 'not', 'change', 'during', '... | [-0.09117544769381719, 0.0746690069246989, -0.09354401601414228, 0.07294007945195612, -0.16801969856826654, -0.16831726165937966, 0.1071816457563947, 0.44280846532562684, -0.2862630551424006, -0.31564575892969454, 0.10817743901661116, -0.2677652462803084, -0.1965171679553319, 0.14936482538790283, -0.10784545898565959, ... |
1,801.03332 | Gaussian fluctuations for linear spectral statistics of Wigner beta
ensembles | As an important topic in Mathematical Physics and statistics, random matrices
theory has found uses in many aspects of modern physics and multivariate
analysis. This paper is to investigate the Gaussian fluctuations for linear
spectral statistics (LSS) of Wigner beta ensembles. We first establish a
central limit theo... | math.PR | as an important topic in mathematical physics and statistics random matrices theory has found uses in many aspects of modern physics and multivariate analysis this paper is to investigate the gaussian fluctuations for linear spectral statistics lss of wigner beta ensembles we first establish a central limit theorem clt... | [['as', 'an', 'important', 'topic', 'in', 'mathematical', 'physics', 'and', 'statistics', 'random', 'matrices', 'theory', 'has', 'found', 'uses', 'in', 'many', 'aspects', 'of', 'modern', 'physics', 'and', 'multivariate', 'analysis', 'this', 'paper', 'is', 'to', 'investigate', 'the', 'gaussian', 'fluctuations', 'for', '... | [-0.027864735799084883, 0.13570462796838, -0.1648687604465522, 0.17090257116069552, 0.008695357724718633, -0.12567080854205415, -0.019016626560187433, 0.30097022173868027, -0.26117108648759313, -0.19223846375825815, 0.07767199301815708, -0.23399829916161252, -0.18283958651591092, 0.16849562057177536, -0.045792217199050... |
1,801.03333 | Semi-classical Computation of Low-energy Collisions Cross Section in
Mutual Neutralization of Helium and Hydrogen Ions | A Semi-classical model is employed to theoretically study mutual
neutralization in the collisions of $\mathrm{^4He^+}$ and $\mathrm{H^-}$. The
model includes nine covalent states of $\mathrm{^2\Sigma^+}$ symmetry. Here the
assumption is that only two states are interacting at a given internuclear
position. The reacti... | physics.atm-clus physics.atom-ph physics.chem-ph | a semiclassical model is employed to theoretically study mutual neutralization in the collisions of mathrm4he and mathrmh the model includes nine covalent states of mathrm2sigma symmetry here the assumption is that only two states are interacting at a given internuclear position the reaction is studied for collisions e... | [['a', 'semiclassical', 'model', 'is', 'employed', 'to', 'theoretically', 'study', 'mutual', 'neutralization', 'in', 'the', 'collisions', 'of', 'mathrm4he', 'and', 'mathrmh', 'the', 'model', 'includes', 'nine', 'covalent', 'states', 'of', 'mathrm2sigma', 'symmetry', 'here', 'the', 'assumption', 'is', 'that', 'only', 't... | [-0.13448496296581242, 0.17446496375956602, -0.0559058846993139, 0.08837220827568203, 0.06937277903254595, -0.13308484457252967, 0.003725052837492718, 0.3772061473179248, -0.20162040144655732, -0.2986476579793699, -0.05049712901311596, -0.3812128177153007, -0.019525139765333262, 0.12884236367479449, 0.05044500664840715... |
1,801.03334 | Applications of deep learning to relativistic hydrodynamics | Relativistic hydrodynamics is a powerful tool to simulate the evolution of
the quark gluon plasma (QGP) in relativistic heavy ion collisions. Using 10000
initial and final profiles generated from 2+1-d relativistic hydrodynamics
VISH2+1 with MC-Glauber initial conditions, we train a deep neural network
based on stack... | nucl-th astro-ph.HE cond-mat.dis-nn hep-ph | relativistic hydrodynamics is a powerful tool to simulate the evolution of the quark gluon plasma qgp in relativistic heavy ion collisions using 10000 initial and final profiles generated from 21d relativistic hydrodynamics vish21 with mcglauber initial conditions we train a deep neural network based on stacked unet an... | [['relativistic', 'hydrodynamics', 'is', 'a', 'powerful', 'tool', 'to', 'simulate', 'the', 'evolution', 'of', 'the', 'quark', 'gluon', 'plasma', 'qgp', 'in', 'relativistic', 'heavy', 'ion', 'collisions', 'using', '10000', 'initial', 'and', 'final', 'profiles', 'generated', 'from', '21d', 'relativistic', 'hydrodynamics'... | [-0.006872923408921521, 0.1388534743195543, -0.18522528992750897, 0.1301115947086006, -0.0051611608001761716, -0.1252845612497857, -0.13269826328525178, 0.37217653900958025, -0.22724579488858582, -0.32389007586126145, 0.006532156846235291, -0.2726523307259553, -0.04501221121754497, 0.15784855567527792, 0.03370856083213... |
1,801.03335 | The Blazar PG 1553+113 as a Binary System of Supermassive Black Holes | The BL Lac PG 1553+113 has been continuously monitored in gamma rays with
Fermi-LAT for over 9 years. Its updated light curve now includes 5 iterations
of a main pattern comprising a high peak and a longer trough, with a period P
\sim 2.2 yr. Our analysis of 2015-2017 data confirms the occurrence in January
2017 of a... | astro-ph.HE | the bl lac pg 1553113 has been continuously monitored in gamma rays with fermilat for over 9 years its updated light curve now includes 5 iterations of a main pattern comprising a high peak and a longer trough with a period p sim 22 yr our analysis of 20152017 data confirms the occurrence in january 2017 of a new peak ... | [['the', 'bl', 'lac', 'pg', '1553113', 'has', 'been', 'continuously', 'monitored', 'in', 'gamma', 'rays', 'with', 'fermilat', 'for', 'over', '9', 'years', 'its', 'updated', 'light', 'curve', 'now', 'includes', '5', 'iterations', 'of', 'a', 'main', 'pattern', 'comprising', 'a', 'high', 'peak', 'and', 'a', 'longer', 'tro... | [-0.1386372431611923, 0.18255522015268014, -0.05625798579508444, 0.10943314749867626, -0.07810543649016864, -0.11145012591048957, 0.05159827958633532, 0.394735649228096, -0.20293990136650836, -0.3092380520325923, 0.0786310154963137, -0.3249728987584748, -0.03130080548137249, 0.23306218261686376, 0.0011558626493853, -0.... |
1,801.03336 | BSDE formulation of combined regular and singular stochastic control
problems | In this paper we study a class of combined regular and singular stochastic
control problems that can be expressed as constrained BSDEs. In the Markovian
case, this reduces to a characterization through a PDE with gradient
constraint. But the BSDE formulation makes it possible to move beyond Markovian
models and consi... | math.OC | in this paper we study a class of combined regular and singular stochastic control problems that can be expressed as constrained bsdes in the markovian case this reduces to a characterization through a pde with gradient constraint but the bsde formulation makes it possible to move beyond markovian models and consider p... | [['in', 'this', 'paper', 'we', 'study', 'a', 'class', 'of', 'combined', 'regular', 'and', 'singular', 'stochastic', 'control', 'problems', 'that', 'can', 'be', 'expressed', 'as', 'constrained', 'bsdes', 'in', 'the', 'markovian', 'case', 'this', 'reduces', 'to', 'a', 'characterization', 'through', 'a', 'pde', 'with', 'g... | [-0.10383393786507536, 0.02362423213248564, -0.0614072204518475, 0.08519092645483876, -0.1281212940812111, -0.1784324586195381, 0.07615896875780125, 0.33829253225734357, -0.37077079777066646, -0.26512377157709316, 0.1586781184152259, -0.23468646290712059, -0.16401777507149076, 0.2191636069726787, -0.1509196301922202, 0... |
1,801.03337 | Distribution of the absolute indicator of random Boolean functions | The absolute indicator is one of the measures used to determine the
resistance offered by a Boolean function when used in the design of a symmetric
cryptosystem. It was proposed along with the sum of square indicator to
evaluate the quality of the diffusion property of block ciphers and hash
functions. While the beha... | cs.IT math.IT | the absolute indicator is one of the measures used to determine the resistance offered by a boolean function when used in the design of a symmetric cryptosystem it was proposed along with the sum of square indicator to evaluate the quality of the diffusion property of block ciphers and hash functions while the behaviou... | [['the', 'absolute', 'indicator', 'is', 'one', 'of', 'the', 'measures', 'used', 'to', 'determine', 'the', 'resistance', 'offered', 'by', 'a', 'boolean', 'function', 'when', 'used', 'in', 'the', 'design', 'of', 'a', 'symmetric', 'cryptosystem', 'it', 'was', 'proposed', 'along', 'with', 'the', 'sum', 'of', 'square', 'ind... | [-0.10721168542133257, 0.06238912847852634, -0.0958869095227801, 0.0861537312837502, -0.0058780613903989, -0.11269961953126263, 0.05767868603187807, 0.3694120982643401, -0.30731067201583695, -0.24951100295944378, 0.1345791715821989, -0.25572753332481524, -0.19464237065663062, 0.1852732826125725, -0.056610890350645725, ... |
1,801.03338 | Accelerating population transfer in a transmon qutrit via Shortcuts to
adiabaticity | In this paper, a method to accelerate population transfer by designing
nonadiabatic evolution paths is proposed. We apply the method to realize robust
and accelerated population transfer with a transmon qutrit. By numerical
simulation, we show that this method allows a robust population transfer
between the ground st... | quant-ph | in this paper a method to accelerate population transfer by designing nonadiabatic evolution paths is proposed we apply the method to realize robust and accelerated population transfer with a transmon qutrit by numerical simulation we show that this method allows a robust population transfer between the ground states i... | [['in', 'this', 'paper', 'a', 'method', 'to', 'accelerate', 'population', 'transfer', 'by', 'designing', 'nonadiabatic', 'evolution', 'paths', 'is', 'proposed', 'we', 'apply', 'the', 'method', 'to', 'realize', 'robust', 'and', 'accelerated', 'population', 'transfer', 'with', 'a', 'transmon', 'qutrit', 'by', 'numerical'... | [-0.09369644063524901, 0.103964128063526, -0.10599438586737961, 0.0596425856766291, -0.03427349324570969, -0.1784891130961478, 0.046012582181720066, 0.4556312610208988, -0.26150505477562547, -0.32701905344147236, 0.06411275118240155, -0.2132629220468516, -0.13358059339225292, 0.28122916028834877, -0.0628662856388837, 0... |
1,801.03339 | Fooling End-to-end Speaker Verification by Adversarial Examples | Automatic speaker verification systems are increasingly used as the primary
means to authenticate costumers. Recently, it has been proposed to train
speaker verification systems using end-to-end deep neural models. In this
paper, we show that such systems are vulnerable to adversarial example attack.
Adversarial exam... | cs.LG cs.CL | automatic speaker verification systems are increasingly used as the primary means to authenticate costumers recently it has been proposed to train speaker verification systems using endtoend deep neural models in this paper we show that such systems are vulnerable to adversarial example attack adversarial examples are ... | [['automatic', 'speaker', 'verification', 'systems', 'are', 'increasingly', 'used', 'as', 'the', 'primary', 'means', 'to', 'authenticate', 'costumers', 'recently', 'it', 'has', 'been', 'proposed', 'to', 'train', 'speaker', 'verification', 'systems', 'using', 'endtoend', 'deep', 'neural', 'models', 'in', 'this', 'paper'... | [-0.0790276467812442, 0.025020383961559346, -0.053317130168842285, 0.05963066846105875, -0.07459048097041081, -0.23628543855708822, 0.010773163196419548, 0.4379198031221545, -0.20842935300441748, -0.31045401856764077, 0.12608522583236054, -0.32860688579487185, -0.24325589529963537, 0.2574173518223688, -0.16249358492480... |
1,801.0334 | The critical 1-arm exponent for the ferromagnetic Ising model on the
Bethe lattice | We consider the ferromagnetic nearest-neighbor Ising model on regular trees
(Bethe lattice), which is well-known to undergo a phase transition in the
absence of an external magnetic field. The behavior of the model at critical
temperature can be described in terms of various critical exponents; one of
them is the cri... | math.PR | we consider the ferromagnetic nearestneighbor ising model on regular trees bethe lattice which is wellknown to undergo a phase transition in the absence of an external magnetic field the behavior of the model at critical temperature can be described in terms of various critical exponents one of them is the critical 1ar... | [['we', 'consider', 'the', 'ferromagnetic', 'nearestneighbor', 'ising', 'model', 'on', 'regular', 'trees', 'bethe', 'lattice', 'which', 'is', 'wellknown', 'to', 'undergo', 'a', 'phase', 'transition', 'in', 'the', 'absence', 'of', 'an', 'external', 'magnetic', 'field', 'the', 'behavior', 'of', 'the', 'model', 'at', 'cri... | [-0.17542572298703749, 0.1878795280613472, -0.05963631011373191, 0.05127980752311285, -0.0113298313277752, -0.11455090465972682, 0.07131937703525182, 0.2889449780497536, -0.2771179664969505, -0.23004149272525898, 0.09664358343784611, -0.2993273055159349, -0.10845676016308264, 0.15276652588875517, -0.0034599518850747563... |
1,801.03341 | Harder-Narasimhan filtrations for Breuil-Kisin-Fargues modules | We define and study Harder-Narasimhan filtrations on Breuil-Kisin-Fargues
modules and related objects relevant to p-adic Hodge theory.
| math.AG math.NT | we define and study hardernarasimhan filtrations on breuilkisinfargues modules and related objects relevant to padic hodge theory | [['we', 'define', 'and', 'study', 'hardernarasimhan', 'filtrations', 'on', 'breuilkisinfargues', 'modules', 'and', 'related', 'objects', 'relevant', 'to', 'padic', 'hodge', 'theory']] | [-0.15872766688356504, 0.02097542436026475, -0.1912671296912081, 0.2150983411599608, -0.1555560816298513, -0.1535873509505216, -0.025207089130109286, 0.3336809843997745, -0.4340195953845978, -0.1743835184504004, 0.07481520603794385, -0.1361179625725045, -0.23744044343338294, 0.19892240951166434, -0.36026791307856054, -... |
1,801.03342 | Quantum Pyragas control: Selective-control of individual photon
probabilities | Pyragas control allows to stabilize unstable states in applied nonlinear
science. We propose to apply a quantum version of the Pyragas protocol to
control individual photon-probabilities in an otherwise only globally
accessible photon-probability distribution of a quantum light emitter. The
versatility of quantum Pyr... | quant-ph | pyragas control allows to stabilize unstable states in applied nonlinear science we propose to apply a quantum version of the pyragas protocol to control individual photonprobabilities in an otherwise only globally accessible photonprobability distribution of a quantum light emitter the versatility of quantum pyragas c... | [['pyragas', 'control', 'allows', 'to', 'stabilize', 'unstable', 'states', 'in', 'applied', 'nonlinear', 'science', 'we', 'propose', 'to', 'apply', 'a', 'quantum', 'version', 'of', 'the', 'pyragas', 'protocol', 'to', 'control', 'individual', 'photonprobabilities', 'in', 'an', 'otherwise', 'only', 'globally', 'accessibl... | [-0.14575550662896905, 0.17223318457775652, -0.056364455927784246, 0.02839026451013827, -0.044398605908888084, -0.21679348839291682, 0.08126582466162896, 0.413602026583006, -0.2666674922569655, -0.2827570688018265, 0.02783468613536873, -0.24592913793567278, -0.12061522581110087, 0.2431684197062471, -0.06526123232906685... |
1,801.03343 | Some remarks on the optimality of the Bruno-R{\"u}ssmann condition | We prove that the Bruno-R{\"u}ssmann condition is optimal for the analytic
preservation of a quasi-periodic invariant curve for an analytic twist map. The
proof is based on Yoccoz's corresponding result for analytic circle
diffeomorphisms and the uniqueness of invariant curves with a given irrational
rotation number.... | math.DS | we prove that the brunorussmann condition is optimal for the analytic preservation of a quasiperiodic invariant curve for an analytic twist map the proof is based on yoccozs corresponding result for analytic circle diffeomorphisms and the uniqueness of invariant curves with a given irrational rotation number we also pr... | [['we', 'prove', 'that', 'the', 'brunorussmann', 'condition', 'is', 'optimal', 'for', 'the', 'analytic', 'preservation', 'of', 'a', 'quasiperiodic', 'invariant', 'curve', 'for', 'an', 'analytic', 'twist', 'map', 'the', 'proof', 'is', 'based', 'on', 'yoccozs', 'corresponding', 'result', 'for', 'analytic', 'circle', 'dif... | [-0.21562736111170636, 0.07959219116008437, -0.11641279380859398, 0.08898177966986578, -0.06004282081976715, -0.15851292839251097, 0.03233397438860976, 0.3001440145620486, -0.20736133716091876, -0.2541573021146355, 0.10756718415607948, -0.2356100111927201, -0.147344809082314, 0.2500839439084435, -0.10125607663461024, 0... |
1,801.03344 | BV functions in Hilbert spaces | We study $BV$ functions in a Hilbert space $X$ endowed with a probability
measure $\nu$, assuming that $\nu$ is Fomin differentiable along suitable
directions. We establish basic characterizations, and we apply the general
theory to relevant examples, including invariant measures of some stochastic
PDEs.
| math.FA | we study bv functions in a hilbert space x endowed with a probability measure nu assuming that nu is fomin differentiable along suitable directions we establish basic characterizations and we apply the general theory to relevant examples including invariant measures of some stochastic pdes | [['we', 'study', 'bv', 'functions', 'in', 'a', 'hilbert', 'space', 'x', 'endowed', 'with', 'a', 'probability', 'measure', 'nu', 'assuming', 'that', 'nu', 'is', 'fomin', 'differentiable', 'along', 'suitable', 'directions', 'we', 'establish', 'basic', 'characterizations', 'and', 'we', 'apply', 'the', 'general', 'theory',... | [-0.14649603205775333, 0.10186181160282683, -0.06843009917065501, 0.15672310019726865, -0.0886071330275048, -0.1575834090525115, 0.03586058762845245, 0.4001380606893111, -0.32111944021149114, -0.13561998289713467, 0.07290417232963425, -0.2611515842912592, -0.18984670412134041, 0.19995143643411045, -0.14710120069371027,... |
1,801.03345 | Optimal functional supervised classification with separation condition | We consider the binary supervised classification problem with the Gaussian
functional model introduced in [7]. Taking advantage of the Gaussian structure,
we design a natural plug-in classifier and derive a family of upper bounds on
its worst-case excess risk over Sobolev spaces. These bounds are parametrized
by a se... | math.ST stat.TH | we consider the binary supervised classification problem with the gaussian functional model introduced in 7 taking advantage of the gaussian structure we design a natural plugin classifier and derive a family of upper bounds on its worstcase excess risk over sobolev spaces these bounds are parametrized by a separation ... | [['we', 'consider', 'the', 'binary', 'supervised', 'classification', 'problem', 'with', 'the', 'gaussian', 'functional', 'model', 'introduced', 'in', '7', 'taking', 'advantage', 'of', 'the', 'gaussian', 'structure', 'we', 'design', 'a', 'natural', 'plugin', 'classifier', 'and', 'derive', 'a', 'family', 'of', 'upper', '... | [-0.06799118955820507, 0.026007012108012158, -0.07582582823256505, 0.12857327955391476, -0.08493883117540356, -0.15660609155391142, 0.13156224151116833, 0.35418527128686217, -0.2788747706788355, -0.3430526041900556, 0.11863308651692361, -0.28053825193395215, -0.16054297469592854, 0.20144322717775745, -0.103801452536501... |
1,801.03346 | Statistical Blockage Modeling and Robustness of Beamforming in
Millimeter Wave Systems | There has been a growing interest in the commercialization of millimeter wave
(mmW) technology as a part of the Fifth-Generation New Radio (5G-NR) wireless
standardization efforts. In this direction, many sets of independent
measurement campaigns show that wireless propagation at mmW carrier frequencies
is only margi... | cs.IT math.IT | there has been a growing interest in the commercialization of millimeter wave mmw technology as a part of the fifthgeneration new radio 5gnr wireless standardization efforts in this direction many sets of independent measurement campaigns show that wireless propagation at mmw carrier frequencies is only marginally wors... | [['there', 'has', 'been', 'a', 'growing', 'interest', 'in', 'the', 'commercialization', 'of', 'millimeter', 'wave', 'mmw', 'technology', 'as', 'a', 'part', 'of', 'the', 'fifthgeneration', 'new', 'radio', '5gnr', 'wireless', 'standardization', 'efforts', 'in', 'this', 'direction', 'many', 'sets', 'of', 'independent', 'm... | [-0.2140215981720929, 0.09094970172517142, 0.027512727598747556, 0.013031274957564782, -0.09766578960214864, -0.14840882194913782, 0.08362967018301616, 0.39997858399039854, -0.22032368812789122, -0.27788901097615654, 0.12154371058129056, -0.2723923482387415, -0.19281192514430381, 0.2074809093142526, -0.0948226943339730... |
1,801.03347 | A Polynomial Algorithm for Balanced Clustering via Graph Partitioning | The objective of clustering is to discover natural groups in datasets and to
identify geometrical structures which might reside there, without assuming any
prior knowledge on the characteristics of the data. The problem can be seen as
detecting the inherent separations between groups of a given point set in a
metric ... | cs.CG cs.DS | the objective of clustering is to discover natural groups in datasets and to identify geometrical structures which might reside there without assuming any prior knowledge on the characteristics of the data the problem can be seen as detecting the inherent separations between groups of a given point set in a metric spac... | [['the', 'objective', 'of', 'clustering', 'is', 'to', 'discover', 'natural', 'groups', 'in', 'datasets', 'and', 'to', 'identify', 'geometrical', 'structures', 'which', 'might', 'reside', 'there', 'without', 'assuming', 'any', 'prior', 'knowledge', 'on', 'the', 'characteristics', 'of', 'the', 'data', 'the', 'problem', '... | [-0.11126337155258952, 0.04076658069815501, -0.12928528971401335, 0.10459937692319324, -0.12371167443507841, -0.09695693280704262, 0.06929147299485751, 0.38251176789289215, -0.33096090658702926, -0.36677664637437646, 0.08378689801444847, -0.24242349977630373, -0.16355465998062652, 0.14188341898061618, -0.07448928377356... |
1,801.03348 | Side Disks of a Spherical Great Polygon | Take a circle and mark $n\in\mathbb{N}$ points on it designated as vertices.
For any arc segment between two consecutive vertices which does not pass
through any other vertex, there is a disk centered at its midpoint and has its
end points on the boundary. We analyze intersection behaviour of these disks
and show tha... | math.CO math.MG | take a circle and mark ninmathbbn points on it designated as vertices for any arc segment between two consecutive vertices which does not pass through any other vertex there is a disk centered at its midpoint and has its end points on the boundary we analyze intersection behaviour of these disks and show that the numbe... | [['take', 'a', 'circle', 'and', 'mark', 'ninmathbbn', 'points', 'on', 'it', 'designated', 'as', 'vertices', 'for', 'any', 'arc', 'segment', 'between', 'two', 'consecutive', 'vertices', 'which', 'does', 'not', 'pass', 'through', 'any', 'other', 'vertex', 'there', 'is', 'a', 'disk', 'centered', 'at', 'its', 'midpoint', '... | [-0.18220494964565986, 0.051501184582519226, -0.09168162544628079, 0.009395138593390584, -0.0920654211479884, -0.1602820619307936, 0.12697263764074215, 0.4272844476195482, -0.27169272747750467, -0.24109194867121866, 0.11825161624866991, -0.37573207810652465, -0.11497745936951385, 0.1086931937875656, -0.0811529925301259... |
1,801.03349 | Mean-field backward stochastic differential equations and applications | In this paper we study the mean-field backward stochastic differential
equations (mean-field bsde) of the form dY(t) =-f(t,Y(t),Z(t),K(t, .
),E[\varphi(Y(t),Z(t),K(t,.))])dt+Z(t)dB(t)
+\int_{R_{0}}K(t,\zeta)\tilde{N}(dt,d\zeta), where B is a Brownian motion,
\tilde{N} is the compensated Poisson random measure.
Unde... | math.OC | in this paper we study the meanfield backward stochastic differential equations meanfield bsde of the form dyt ftytztkt evarphiytztktdtztdbt int_r_0ktzetatildendtdzeta where b is a brownian motion tilden is the compensated poisson random measure under some mild conditions we prove the existence and uniqueness of the so... | [['in', 'this', 'paper', 'we', 'study', 'the', 'meanfield', 'backward', 'stochastic', 'differential', 'equations', 'meanfield', 'bsde', 'of', 'the', 'form', 'dyt', 'ftytztkt', 'evarphiytztktdtztdbt', 'int_r_0ktzetatildendtdzeta', 'where', 'b', 'is', 'a', 'brownian', 'motion', 'tilden', 'is', 'the', 'compensated', 'pois... | [-0.14262995278196675, 0.02209496210187873, -0.10957656394069394, 0.14760757101522315, -0.10437678970795657, -0.1505154903002438, 0.01057396080189695, 0.3300382455190023, -0.325433463709695, -0.19201466112974144, 0.10431956261219014, -0.2841135122103705, -0.1658239884922902, 0.1566933057581385, -0.08849710570204826, 0.... |
1,801.0335 | New results on the multiplicity and centre-of-mass energy dependence of
identified particle production in pp collisions with ALICE | The study of identified particle production in proton-proton (pp) collisions
as a function of center-of-mass energy ($\sqrt{s}$) and event charged-particle
multiplicity is a key tool for understanding similarities and differences
between small and large collision systems. We report on new measurements of the
producti... | hep-ex nucl-ex | the study of identified particle production in protonproton pp collisions as a function of centerofmass energy sqrts and event chargedparticle multiplicity is a key tool for understanding similarities and differences between small and large collision systems we report on new measurements of the production of identified... | [['the', 'study', 'of', 'identified', 'particle', 'production', 'in', 'protonproton', 'pp', 'collisions', 'as', 'a', 'function', 'of', 'centerofmass', 'energy', 'sqrts', 'and', 'event', 'chargedparticle', 'multiplicity', 'is', 'a', 'key', 'tool', 'for', 'understanding', 'similarities', 'and', 'differences', 'between', ... | [-0.06568134415584956, 0.2241915519516472, -0.13661247628612375, 0.15594986282292925, 0.03463825578197338, -0.12734647469485966, -0.11263602834231917, 0.3621064623852872, -0.17489669579529363, -0.37537083569836166, -0.04587174602004867, -0.41378151731678603, 0.10625606092281452, 0.2009562248306614, 0.07924528210350823,... |
1,801.03351 | A triple comparison between anticipating stochastic integrals in
financial modeling | We consider a simplified version of the problem of insider trading in a
financial market. We approach it by means of anticipating stochastic calculus
and compare the use of the Hitsuda-Skorokhod, the Ayed-Kuo, and the
Russo-Vallois forward integrals within this context. Our results give some
indication that, while th... | math.PR | we consider a simplified version of the problem of insider trading in a financial market we approach it by means of anticipating stochastic calculus and compare the use of the hitsudaskorokhod the ayedkuo and the russovallois forward integrals within this context our results give some indication that while the forward ... | [['we', 'consider', 'a', 'simplified', 'version', 'of', 'the', 'problem', 'of', 'insider', 'trading', 'in', 'a', 'financial', 'market', 'we', 'approach', 'it', 'by', 'means', 'of', 'anticipating', 'stochastic', 'calculus', 'and', 'compare', 'the', 'use', 'of', 'the', 'hitsudaskorokhod', 'the', 'ayedkuo', 'and', 'the', ... | [-0.10337354570130208, 0.007492400649733519, -0.1347611412155227, 0.09032502240465524, -0.09770488054849781, -0.0786320600228814, 0.05940022227855829, 0.3343910140630144, -0.2584536133199715, -0.24172840362701278, 0.13765133605159532, -0.27598733959468796, -0.1816478631960658, 0.20505332466161166, -0.09312116496193294,... |
1,801.03352 | Revisiting the Stellar Velocity Ellipsoid - Hubble type relation:
observations versus simulations | The stellar velocity ellipsoid (SVE) in galaxies can provide important
information on the processes that participate in the dynamical heating of their
disc components (e.g. giant molecular clouds, mergers, spiral density waves,
bars). Earlier findings suggested a strong relation between the shape of the
disc SVE and ... | astro-ph.GA | the stellar velocity ellipsoid sve in galaxies can provide important information on the processes that participate in the dynamical heating of their disc components eg giant molecular clouds mergers spiral density waves bars earlier findings suggested a strong relation between the shape of the disc sve and hubble type ... | [['the', 'stellar', 'velocity', 'ellipsoid', 'sve', 'in', 'galaxies', 'can', 'provide', 'important', 'information', 'on', 'the', 'processes', 'that', 'participate', 'in', 'the', 'dynamical', 'heating', 'of', 'their', 'disc', 'components', 'eg', 'giant', 'molecular', 'clouds', 'mergers', 'spiral', 'density', 'waves', 'b... | [-0.11633179611348847, 0.08170916315053947, -0.10826684719630343, 0.0795252989665734, -0.07823182486187098, -0.03412337505832804, 0.011905217014935847, 0.4077294336758175, -0.2024442032049854, -0.3192341098703949, 0.05864323237644493, -0.2490482748351928, -0.1168945383229214, 0.2192765133025251, -0.01676490294636805, -... |
1,801.03353 | Bohmian quantum gravity and cosmology | Quantum gravity aims to describe gravity in quantum mechanical terms. How
exactly this needs to be done remains an open question. Various proposals have
been put on the table, such as canonical quantum gravity, loop quantum gravity,
string theory, etc. These proposals often encounter technical and conceptual
problems... | gr-qc quant-ph | quantum gravity aims to describe gravity in quantum mechanical terms how exactly this needs to be done remains an open question various proposals have been put on the table such as canonical quantum gravity loop quantum gravity string theory etc these proposals often encounter technical and conceptual problems in this ... | [['quantum', 'gravity', 'aims', 'to', 'describe', 'gravity', 'in', 'quantum', 'mechanical', 'terms', 'how', 'exactly', 'this', 'needs', 'to', 'be', 'done', 'remains', 'an', 'open', 'question', 'various', 'proposals', 'have', 'been', 'put', 'on', 'the', 'table', 'such', 'as', 'canonical', 'quantum', 'gravity', 'loop', '... | [-0.11073398032274685, 0.16733021046912702, -0.1517902972421756, 0.13137889997482202, -0.08510544781426066, -0.18062633266182324, -0.020221618963803752, 0.28155376528340736, -0.26457866184217366, -0.3017922639405649, 0.06247688172458622, -0.2525422743031461, -0.18050946846457297, 0.18318981404514298, -0.130159910841795... |
1,801.03354 | Planning with Pixels in (Almost) Real Time | Recently, width-based planning methods have been shown to yield
state-of-the-art results in the Atari 2600 video games. For this, the states
were associated with the (RAM) memory states of the simulator. In this work, we
consider the same planning problem but using the screen instead. By using the
same visual inputs,... | cs.AI | recently widthbased planning methods have been shown to yield stateoftheart results in the atari 2600 video games for this the states were associated with the ram memory states of the simulator in this work we consider the same planning problem but using the screen instead by using the same visual inputs the planning r... | [['recently', 'widthbased', 'planning', 'methods', 'have', 'been', 'shown', 'to', 'yield', 'stateoftheart', 'results', 'in', 'the', 'atari', '2600', 'video', 'games', 'for', 'this', 'the', 'states', 'were', 'associated', 'with', 'the', 'ram', 'memory', 'states', 'of', 'the', 'simulator', 'in', 'this', 'work', 'we', 'co... | [-0.008373127658973988, 0.05708455450522913, -0.10073015132200039, 0.05685224119582001, -0.036881011698329656, -0.11748893774653736, 0.0071815455070974536, 0.47951900279312804, -0.23136469743443294, -0.3543028956802006, 0.11058099442079924, -0.2682096307623413, -0.17761241087052776, 0.24406644301652386, -0.135590527300... |
1,801.03355 | Axiomatizations of inconsistency indices for triads | Pairwise comparison matrices often exhibit inconsistency, therefore many
indices have been suggested to measure their deviation from a consistent
matrix. A set of axioms has been proposed recently that is required to be
satisfied by any reasonable inconsistency index. This set seems to be not
exhaustive as illustrate... | cs.AI | pairwise comparison matrices often exhibit inconsistency therefore many indices have been suggested to measure their deviation from a consistent matrix a set of axioms has been proposed recently that is required to be satisfied by any reasonable inconsistency index this set seems to be not exhaustive as illustrated by ... | [['pairwise', 'comparison', 'matrices', 'often', 'exhibit', 'inconsistency', 'therefore', 'many', 'indices', 'have', 'been', 'suggested', 'to', 'measure', 'their', 'deviation', 'from', 'a', 'consistent', 'matrix', 'a', 'set', 'of', 'axioms', 'has', 'been', 'proposed', 'recently', 'that', 'is', 'required', 'to', 'be', '... | [-0.07943130317914733, 0.08618165459576092, -0.07618133576495022, 0.11287237583285749, -0.08918162282149662, -0.1321579084861171, 0.029749957765911668, 0.3875292112106379, -0.22184601284212654, -0.33045211288435256, 0.10185128700768602, -0.3105359179374408, -0.14892231681200505, 0.1741549302090097, -0.0781119156327151,... |
1,801.03356 | Two-field cosmological models and the uniformization theorem | We propose a class of two-field cosmological models derived from gravity
coupled to non-linear sigma models whose target space is a non-compact and
geometrically-finite hyperbolic surface, which provide a wide generalization of
so-called $\alpha$-attractor models and can be studied using uniformization
theory. We ill... | hep-th | we propose a class of twofield cosmological models derived from gravity coupled to nonlinear sigma models whose target space is a noncompact and geometricallyfinite hyperbolic surface which provide a wide generalization of socalled alphaattractor models and can be studied using uniformization theory we illustrate cosmo... | [['we', 'propose', 'a', 'class', 'of', 'twofield', 'cosmological', 'models', 'derived', 'from', 'gravity', 'coupled', 'to', 'nonlinear', 'sigma', 'models', 'whose', 'target', 'space', 'is', 'a', 'noncompact', 'and', 'geometricallyfinite', 'hyperbolic', 'surface', 'which', 'provide', 'a', 'wide', 'generalization', 'of',... | [-0.08700571595857452, 0.08021258865483105, -0.09977212977329535, 0.10982244386728521, -0.10925927392340132, -0.18794805048465996, -0.07170982813529138, 0.30753299279604107, -0.25335716602525543, -0.26000795198238585, 0.10192380832449999, -0.2243135488824919, -0.2077935059205629, 0.22000170096621982, -0.075540773179714... |
1,801.03357 | Singular equivalences of functor categories via Auslander-Buchweitz approximations | The aim of this paper is to construct singular equivalences between functor categories. As a special case, we show that there exists a singular equivalence arising from a cotilting module $T$, namely, the singularity category of $(^\perp T)/[T]$ and that of $(\mod A)/[T]$ are triangle equivalent. In particular, the can... | math.CT math.RT | the aim of this paper is to construct singular equivalences between functor categories as a special case we show that there exists a singular equivalence arising from a cotilting module t namely the singularity category of perp tt and that of mod at are triangle equivalent in particular the canonical module omega over ... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'construct', 'singular', 'equivalences', 'between', 'functor', 'categories', 'as', 'a', 'special', 'case', 'we', 'show', 'that', 'there', 'exists', 'a', 'singular', 'equivalence', 'arising', 'from', 'a', 'cotilting', 'module', 't', 'namely', 'the', 'singularity', 'cate... | [-0.20094066499777644, 0.002190922148603702, -0.1107423707833785, 0.06838713638095674, -0.08790164911956752, -0.1998693877333793, -0.03812418535726995, 0.3300601834322787, -0.4138698318692883, -0.11811247057037301, 0.05305689063208015, -0.22420580067911447, -0.14510332354461974, 0.16422381349590617, -0.1895505338409933... |
1,801.03358 | Improved linear direct solution for asynchronous radio network
localization (RNL) | In the field of localization the linear least square solution is frequently
used. This solution is compared to nonlinear solvers more effected by noise,
but able to provide a position estimation without the knowledge of any starting
condition. The linear least square solution is able to minimize Gaussian noise
by sol... | eess.SP | in the field of localization the linear least square solution is frequently used this solution is compared to nonlinear solvers more effected by noise but able to provide a position estimation without the knowledge of any starting condition the linear least square solution is able to minimize gaussian noise by solving ... | [['in', 'the', 'field', 'of', 'localization', 'the', 'linear', 'least', 'square', 'solution', 'is', 'frequently', 'used', 'this', 'solution', 'is', 'compared', 'to', 'nonlinear', 'solvers', 'more', 'effected', 'by', 'noise', 'but', 'able', 'to', 'provide', 'a', 'position', 'estimation', 'without', 'the', 'knowledge', '... | [-0.08329177117330902, -0.0011376683532944298, -0.09813536889851093, 0.06965422097386585, -0.14271008815234787, -0.18401909991452056, -0.01760018294185607, 0.3511024706984042, -0.32542443382165703, -0.24392915458762823, 0.19355606977397757, -0.2826810796525226, -0.14602581006733495, 0.18196516893739398, -0.079505455350... |
1,801.03359 | Symbolic dynamics for one dimensional maps with nonuniform expansion | Given a piecewise $C^{1+\beta}$ map of the interval, possibly with critical
points and discontinuities, we construct a symbolic model for invariant
probability measures with nonuniform expansion that do not approach the
critical points and discontinuities exponentially fast almost surely. More
specifically, we code t... | math.DS | given a piecewise c1beta map of the interval possibly with critical points and discontinuities we construct a symbolic model for invariant probability measures with nonuniform expansion that do not approach the critical points and discontinuities exponentially fast almost surely more specifically we code the lift of th... | [['given', 'a', 'piecewise', 'c1beta', 'map', 'of', 'the', 'interval', 'possibly', 'with', 'critical', 'points', 'and', 'discontinuities', 'we', 'construct', 'a', 'symbolic', 'model', 'for', 'invariant', 'probability', 'measures', 'with', 'nonuniform', 'expansion', 'that', 'do', 'not', 'approach', 'the', 'critical', 'p... | [-0.15012832790909506, 0.09876093236221509, -0.09842207361520691, 0.08869377482174472, -0.003097779642451893, -0.1511624495752833, 0.09407303670251911, 0.3717684162611311, -0.3053291380405426, -0.1971416594121944, 0.1243722056356174, -0.29086713773960415, -0.1903317099098455, 0.18818595444741235, -0.07590016465718773, ... |
1,801.0336 | On an Electro-Magneto-Elasto-Dynamic Transmission Problem | We consider a coupled system describing the interaction between acoustic and
elastic regions, where the coupling occurs not via material properties but
through an interaction on an interface separating the two regimes. Evolutionary
well-posedness in the sense of Hadamard well-posedness supplemented by causal
dependen... | math-ph math.MP | we consider a coupled system describing the interaction between acoustic and elastic regions where the coupling occurs not via material properties but through an interaction on an interface separating the two regimes evolutionary wellposedness in the sense of hadamard wellposedness supplemented by causal dependence is ... | [['we', 'consider', 'a', 'coupled', 'system', 'describing', 'the', 'interaction', 'between', 'acoustic', 'and', 'elastic', 'regions', 'where', 'the', 'coupling', 'occurs', 'not', 'via', 'material', 'properties', 'but', 'through', 'an', 'interaction', 'on', 'an', 'interface', 'separating', 'the', 'two', 'regimes', 'evol... | [-0.18986425027509946, 0.1022624070788475, -0.06613913344012366, 0.06209349006351175, -0.0694637191798078, -0.11009504582250008, 0.005860501141459854, 0.3450204919402798, -0.28815142359630563, -0.25245766890706656, 0.12258544501871514, -0.26125508261683544, -0.15340641635343616, 0.19634814953638446, 0.00208372987783801... |
1,801.03361 | Regularity for evolution equations with non-autonomous perturbations in
Banach spaces | We provide regularity of solutions to a large class of evolution equations on
Banach spaces where the generator is composed of a static principal part plus a
non-autonomous perturbation. Regularity is examined with respect to the graph
norm of the iterations of the principal part. The results are applied to the
Schr\... | math-ph math.AP math.MP | we provide regularity of solutions to a large class of evolution equations on banach spaces where the generator is composed of a static principal part plus a nonautonomous perturbation regularity is examined with respect to the graph norm of the iterations of the principal part the results are applied to the schrodinge... | [['we', 'provide', 'regularity', 'of', 'solutions', 'to', 'a', 'large', 'class', 'of', 'evolution', 'equations', 'on', 'banach', 'spaces', 'where', 'the', 'generator', 'is', 'composed', 'of', 'a', 'static', 'principal', 'part', 'plus', 'a', 'nonautonomous', 'perturbation', 'regularity', 'is', 'examined', 'with', 'respe... | [-0.15002619580064022, 0.015464555977148488, -0.06573746626594917, 0.08192364722293552, -0.07494309923978863, -0.07578213318762644, -0.08226787056249212, 0.30882216470552165, -0.2818658244599339, -0.19917832154692086, 0.1799805607649983, -0.31101711062898096, -0.10052141507195544, 0.16930247330710188, -0.06914817166685... |
1,801.03362 | On an Elasto-Acoustic Transmission Problem in Anisotropic, Inhomogeneous
Media | We consider a coupled system describing the interaction between acoustic and
elastic regions, where the coupling occurs not via material properties but
through an interaction on an interface separating the two regimes. Evolutionary
well-posedness in the sense of Hadamard well-posedness supplemented by causal
dependen... | math-ph math.MP | we consider a coupled system describing the interaction between acoustic and elastic regions where the coupling occurs not via material properties but through an interaction on an interface separating the two regimes evolutionary wellposedness in the sense of hadamard wellposedness supplemented by causal dependence is ... | [['we', 'consider', 'a', 'coupled', 'system', 'describing', 'the', 'interaction', 'between', 'acoustic', 'and', 'elastic', 'regions', 'where', 'the', 'coupling', 'occurs', 'not', 'via', 'material', 'properties', 'but', 'through', 'an', 'interaction', 'on', 'an', 'interface', 'separating', 'the', 'two', 'regimes', 'evol... | [-0.18986425027509946, 0.1022624070788475, -0.06613913344012366, 0.06209349006351175, -0.0694637191798078, -0.11009504582250008, 0.005860501141459854, 0.3450204919402798, -0.28815142359630563, -0.25245766890706656, 0.12258544501871514, -0.26125508261683544, -0.15340641635343616, 0.19634814953638446, 0.00208372987783801... |
1,801.03363 | Multicanonical Sampling of the Space of States of H(2,n)-Vector Models | Problems of temperature behavior of specific heat are solved by the entropy
simulation method for Ising models on a simple square lattice and a square spin
ice (SSI) lattice with nearest neighbor interaction, models of hexagonal
lattices with short-range (SR) dipole interaction, as well as with long-range
(LR) dipole... | cond-mat.dis-nn | problems of temperature behavior of specific heat are solved by the entropy simulation method for ising models on a simple square lattice and a square spin ice ssi lattice with nearest neighbor interaction models of hexagonal lattices with shortrange sr dipole interaction as well as with longrange lr dipole interaction... | [['problems', 'of', 'temperature', 'behavior', 'of', 'specific', 'heat', 'are', 'solved', 'by', 'the', 'entropy', 'simulation', 'method', 'for', 'ising', 'models', 'on', 'a', 'simple', 'square', 'lattice', 'and', 'a', 'square', 'spin', 'ice', 'ssi', 'lattice', 'with', 'nearest', 'neighbor', 'interaction', 'models', 'of... | [-0.15479796892032027, 0.17106380004467944, -0.03851452816865946, 0.06560639090082412, -0.020091305034676273, -0.19505503925274273, 0.025261877167136654, 0.4345411803965506, -0.24873479093964163, -0.2621408906324129, 0.07226265137770066, -0.30878292623123055, -0.11709254003178916, 0.1441809294537004, 0.0689231630978419... |
1,801.03364 | Mean-Field Delayed BSDEs with Jumps | We establish sufficient conditions for the existence and uniqueness of
mean-field backward stochastic differential equations with time delayed
generator in the sense that at t, the generator may depend on previous values
up to a delay constant {\delta} not on the hole past as in Delong and Imkeller
[10], [13]. For su... | math.OC | we establish sufficient conditions for the existence and uniqueness of meanfield backward stochastic differential equations with time delayed generator in the sense that at t the generator may depend on previous values up to a delay constant delta not on the hole past as in delong and imkeller 10 13 for sufficiently sm... | [['we', 'establish', 'sufficient', 'conditions', 'for', 'the', 'existence', 'and', 'uniqueness', 'of', 'meanfield', 'backward', 'stochastic', 'differential', 'equations', 'with', 'time', 'delayed', 'generator', 'in', 'the', 'sense', 'that', 'at', 't', 'the', 'generator', 'may', 'depend', 'on', 'previous', 'values', 'up... | [-0.15215506379791438, 0.0985388973964128, -0.045175010790186584, 0.05835357504382507, -0.07807340430888111, -0.17075638327080367, 0.0729797089389011, 0.3365991414149306, -0.27129755967032554, -0.29124110481187476, 0.14500571083565897, -0.2656217017836535, -0.04239276665221177, 0.19948700280276252, -0.05118447230823005... |
1,801.03365 | Five Proofs of Chernoff's Bound with Applications | We discuss five ways of proving Chernoff's bound and show how they lead to
different extensions of the basic bound.
| cs.DM | we discuss five ways of proving chernoffs bound and show how they lead to different extensions of the basic bound | [['we', 'discuss', 'five', 'ways', 'of', 'proving', 'chernoffs', 'bound', 'and', 'show', 'how', 'they', 'lead', 'to', 'different', 'extensions', 'of', 'the', 'basic', 'bound']] | [-0.09906960967928172, 0.13900630539283157, -0.14242450194433331, 0.1600457102060318, -0.03026984427124262, -0.16929856464266776, 0.07892793321516364, 0.2951530609279871, -0.2754373935982585, -0.3765854925804888, 0.10566030729096383, -0.2228903144132346, -0.22029997780919075, 0.23282888457179068, -0.09042392875999213, ... |
1,801.03366 | On the Availability of ESO Data Papers on arXiv/astro-ph | Using the ESO Telescope Bibliography database telbib, we have investigated
the percentage of ESO data papers that were submitted to the arXiv/astro-ph
e-print server and that are therefore free to read. Our study revealed an
availability of up to 96% of telbib papers on arXiv over the years 2010 to
2017. We also comp... | astro-ph.IM cs.DL | using the eso telescope bibliography database telbib we have investigated the percentage of eso data papers that were submitted to the arxivastroph eprint server and that are therefore free to read our study revealed an availability of up to 96 of telbib papers on arxiv over the years 2010 to 2017 we also compared the ... | [['using', 'the', 'eso', 'telescope', 'bibliography', 'database', 'telbib', 'we', 'have', 'investigated', 'the', 'percentage', 'of', 'eso', 'data', 'papers', 'that', 'were', 'submitted', 'to', 'the', 'arxivastroph', 'eprint', 'server', 'and', 'that', 'are', 'therefore', 'free', 'to', 'read', 'our', 'study', 'revealed',... | [-0.053959517237464234, 0.03582412287096737, -0.07738759346705462, 0.022164632087307318, -0.10435731524512881, -0.09016997505955043, 0.10211471285050114, 0.3991348139409508, -0.12490577672031664, -0.4232621464523531, 0.11038923603704288, -0.3786867605078788, -0.07069905245942729, 0.24059166346366206, -0.131621816847473... |
1,801.03367 | Quantitative Analysis of Smart Contracts | Smart contracts are computer programs that are executed by a network of
mutually distrusting agents, without the need of an external trusted authority.
Smart contracts handle and transfer assets of considerable value (in the form
of crypto-currency like Bitcoin). Hence, it is crucial that their
implementation is bug-... | cs.PL | smart contracts are computer programs that are executed by a network of mutually distrusting agents without the need of an external trusted authority smart contracts handle and transfer assets of considerable value in the form of cryptocurrency like bitcoin hence it is crucial that their implementation is bugfree we id... | [['smart', 'contracts', 'are', 'computer', 'programs', 'that', 'are', 'executed', 'by', 'a', 'network', 'of', 'mutually', 'distrusting', 'agents', 'without', 'the', 'need', 'of', 'an', 'external', 'trusted', 'authority', 'smart', 'contracts', 'handle', 'and', 'transfer', 'assets', 'of', 'considerable', 'value', 'in', '... | [-0.11648269765671271, -0.009654383853717042, -0.08357764939094885, 0.10338251838783814, -0.12900541952892558, -0.2130408406877004, 0.07100981316931582, 0.39731903645454103, -0.28640091762814707, -0.32500027150969085, 0.1363942651891882, -0.2805116900697224, -0.1194327768883261, 0.1806269121340485, -0.14336987520631367... |
1,801.03368 | Spherical Indicatrices of a Bertrand Curve in Three Lie Groups | In this paper, new representations of a Bertrand curve pair in three
dimensional Lie groups with bi-invariant metric are given. Besides, the
spherical indicatrices of a Bertrand curve pair are obtain and the relations
between the spherical indicatrices and new representations of Bertrand curve
pair are shown.
| math.DG | in this paper new representations of a bertrand curve pair in three dimensional lie groups with biinvariant metric are given besides the spherical indicatrices of a bertrand curve pair are obtain and the relations between the spherical indicatrices and new representations of bertrand curve pair are shown | [['in', 'this', 'paper', 'new', 'representations', 'of', 'a', 'bertrand', 'curve', 'pair', 'in', 'three', 'dimensional', 'lie', 'groups', 'with', 'biinvariant', 'metric', 'are', 'given', 'besides', 'the', 'spherical', 'indicatrices', 'of', 'a', 'bertrand', 'curve', 'pair', 'are', 'obtain', 'and', 'the', 'relations', 'b... | [-0.19582406647176423, 0.07137399802400553, -0.16318920785759358, 0.09753651079533503, -0.13310909371803256, -0.1823446571311735, -0.04195036154309724, 0.44458337461060665, -0.2535965882756926, -0.23474013551752618, -0.021292970282956958, -0.3110384464343178, -0.23913379732836434, 0.22955684657109546, -0.13240609982080... |
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