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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1,801.03469 | The photon and a preferred frame scenario | Structure of the space of photonic states is discussed in the context of a
working hypothesis of existence of a preferred frame for photons. Two
polarisation experiments are proposed to test the preferred frame scenario.
| quant-ph gr-qc hep-th | structure of the space of photonic states is discussed in the context of a working hypothesis of existence of a preferred frame for photons two polarisation experiments are proposed to test the preferred frame scenario | [['structure', 'of', 'the', 'space', 'of', 'photonic', 'states', 'is', 'discussed', 'in', 'the', 'context', 'of', 'a', 'working', 'hypothesis', 'of', 'existence', 'of', 'a', 'preferred', 'frame', 'for', 'photons', 'two', 'polarisation', 'experiments', 'are', 'proposed', 'to', 'test', 'the', 'preferred', 'frame', 'scena... | [-0.19755572285503148, 0.13012803765013814, -0.07119255359617195, 0.05694770601777626, -0.0426305463803666, -0.10925088383789573, 0.0327649049593934, 0.40688685758837634, -0.19957337964858327, -0.2749897477882249, 0.07018986769752311, -0.19884972380075072, -0.03696008271404675, 0.19034601439322743, 0.015942776894995143... |
1,801.0347 | Poisson-Fermi Modeling of Ion Activities in Aqueous Single and Mixed
Electrolyte Solutions at Variable Temperature | The combinatorial explosion of empirical parameters in tens of thousands
presents a tremendous challenge for extended Debye-H\"uckel models to calculate
activity coefficients of aqueous mixtures of most important salts in chemistry.
The explosion of parameters originates from the phenomenological extension of
the Deb... | cond-mat.soft physics.chem-ph physics.comp-ph | the combinatorial explosion of empirical parameters in tens of thousands presents a tremendous challenge for extended debyehuckel models to calculate activity coefficients of aqueous mixtures of most important salts in chemistry the explosion of parameters originates from the phenomenological extension of the debyehuck... | [['the', 'combinatorial', 'explosion', 'of', 'empirical', 'parameters', 'in', 'tens', 'of', 'thousands', 'presents', 'a', 'tremendous', 'challenge', 'for', 'extended', 'debyehuckel', 'models', 'to', 'calculate', 'activity', 'coefficients', 'of', 'aqueous', 'mixtures', 'of', 'most', 'important', 'salts', 'in', 'chemistr... | [-0.06673539100214838, 0.11394387917335344, -0.023533027898520232, 0.04224162936343678, 0.012172226969684874, -0.1448111955076456, 0.017321341407618353, 0.3583999295106956, -0.22281626357164766, -0.3289663970789739, 0.02986278010864875, -0.3093182474042156, -0.09340353756876929, 0.14147950369997747, -0.0022031134087592... |
1,801.03471 | Rapid calculation of maximum particle lifetime for diffusion in complex
geometries | Diffusion of molecules within biological cells and tissues is strongly
influenced by crowding. A key quantity to characterize diffusion is the
particle lifetime, which is the time taken for a diffusing particle to exit by
hitting an absorbing boundary. Calculating the particle lifetime provides
valuable information, ... | physics.bio-ph physics.comp-ph | diffusion of molecules within biological cells and tissues is strongly influenced by crowding a key quantity to characterize diffusion is the particle lifetime which is the time taken for a diffusing particle to exit by hitting an absorbing boundary calculating the particle lifetime provides valuable information for ex... | [['diffusion', 'of', 'molecules', 'within', 'biological', 'cells', 'and', 'tissues', 'is', 'strongly', 'influenced', 'by', 'crowding', 'a', 'key', 'quantity', 'to', 'characterize', 'diffusion', 'is', 'the', 'particle', 'lifetime', 'which', 'is', 'the', 'time', 'taken', 'for', 'a', 'diffusing', 'particle', 'to', 'exit',... | [-0.03853279826315967, 0.19839332694854503, -0.08300997493100691, 0.06680947785322187, -0.017005155664501767, -0.11697498984267991, 0.05679441524359087, 0.35928443814204497, -0.2591132897601435, -0.3255324748147166, 0.07451296360514155, -0.25234841948346887, -0.06727431149532398, 0.18430219871542333, -0.038976763765976... |
1,801.03472 | Orbifolds from a metric viewpoint | We characterize Riemannian orbifolds and their coverings in terms of metric
geometry. In particular, we show that the metric double of a Riemannian
orbifold along the closure of its codimension one stratum is a Riemannian
orbifold and that the natural projection is an orbifold covering.
| math.DG math.MG | we characterize riemannian orbifolds and their coverings in terms of metric geometry in particular we show that the metric double of a riemannian orbifold along the closure of its codimension one stratum is a riemannian orbifold and that the natural projection is an orbifold covering | [['we', 'characterize', 'riemannian', 'orbifolds', 'and', 'their', 'coverings', 'in', 'terms', 'of', 'metric', 'geometry', 'in', 'particular', 'we', 'show', 'that', 'the', 'metric', 'double', 'of', 'a', 'riemannian', 'orbifold', 'along', 'the', 'closure', 'of', 'its', 'codimension', 'one', 'stratum', 'is', 'a', 'rieman... | [-0.19488225246055257, 0.03383427599942984, -0.10684150432546934, 0.12265622043050825, -0.09412482034208046, -0.11751159764826298, -0.06469301953911781, 0.37682583100265926, -0.28525447762674755, -0.16771734485195744, 0.12849865791180895, -0.29530835242735015, -0.16884859837591648, 0.16758531542080973, -0.2359488891644... |
1,801.03473 | Strong existence and uniqueness for stable stochastic differential
equations with distributional drift | We consider the stochastic differential equation $$ dX_t = b(X_t) dt +
dL_t,$$ where the drift $b$ is a generalized function and $L$ is a symmetric
one dimensional $\alpha$-stable L\'evy processes, $\alpha \in (1, 2)$. We
define the notion of solution to this equation and establish strong existence
and uniqueness whe... | math.PR | we consider the stochastic differential equation dx_t bx_t dt dl_t where the drift b is a generalized function and l is a symmetric one dimensional alphastable levy processes alpha in 1 2 we define the notion of solution to this equation and establish strong existence and uniqueness whenever b belongs to the besovholde... | [['we', 'consider', 'the', 'stochastic', 'differential', 'equation', 'dx_t', 'bx_t', 'dt', 'dl_t', 'where', 'the', 'drift', 'b', 'is', 'a', 'generalized', 'function', 'and', 'l', 'is', 'a', 'symmetric', 'one', 'dimensional', 'alphastable', 'levy', 'processes', 'alpha', 'in', '1', '2', 'we', 'define', 'the', 'notion', '... | [-0.12034343163083706, 0.12022925403601091, -0.03586730754302282, 0.07359694589935575, -0.08444549601491806, -0.20525630438766843, -0.009211329227712537, 0.28849747574089896, -0.3476085154605763, -0.13822652639022895, 0.09800335012135163, -0.29534266579763163, -0.13552307157910295, 0.09131378575693816, -0.0445452232712... |
1,801.03474 | Tunable $\Gamma - K$ Valley Populations in Hole-Doped Trilayer WSe$_2$ | We present a combined experimental and theoretical study of valley
populations in the valence bands of trilayer WSe$_2$. Shubnikov$-$de Haas
oscillations show that trilayer holes populate two distinct subbands associated
with the $K$ and $\Gamma$ valleys, with effective masses 0.5$m_e$ and $1.2m_e$,
respectively; $m_... | cond-mat.mes-hall cond-mat.str-el | we present a combined experimental and theoretical study of valley populations in the valence bands of trilayer wse_2 shubnikovde haas oscillations show that trilayer holes populate two distinct subbands associated with the k and gamma valleys with effective masses 05m_e and 12m_e respectively m_e is the bare electron ... | [['we', 'present', 'a', 'combined', 'experimental', 'and', 'theoretical', 'study', 'of', 'valley', 'populations', 'in', 'the', 'valence', 'bands', 'of', 'trilayer', 'wse_2', 'shubnikovde', 'haas', 'oscillations', 'show', 'that', 'trilayer', 'holes', 'populate', 'two', 'distinct', 'subbands', 'associated', 'with', 'the'... | [-0.19870854146930195, 0.2393384528764981, -0.013700422076887429, 0.07444353106020149, 0.009462220212552956, -0.1183088663423997, 0.11260307223676856, 0.3859254891529333, -0.1980377843516857, -0.34288823931629575, -0.11921901237165425, -0.36241138956054697, -0.06960314953548097, 0.14551484454856362, 0.03433924104996719... |
1,801.03475 | Supercritical degenerate parabolic-parabolic Keller-Segel system --
existence criterion given by the best constant in Sobolev's inequality | This article presents a relationship between the sharp constant of the
Sobolev inequality and the initial criterion to the global existence of
degenerate parabolic-parabolic Keller-Segel system with the diffusion exponent
$\frac{2n}{2+n}<m<2-\frac{2}{n}$. The global weak solution obtained in this
article does not nee... | math.AP | this article presents a relationship between the sharp constant of the sobolev inequality and the initial criterion to the global existence of degenerate parabolicparabolic kellersegel system with the diffusion exponent frac2n2nm2frac2n the global weak solution obtained in this article does not need any smallness assum... | [['this', 'article', 'presents', 'a', 'relationship', 'between', 'the', 'sharp', 'constant', 'of', 'the', 'sobolev', 'inequality', 'and', 'the', 'initial', 'criterion', 'to', 'the', 'global', 'existence', 'of', 'degenerate', 'parabolicparabolic', 'kellersegel', 'system', 'with', 'the', 'diffusion', 'exponent', 'frac2n2... | [-0.14141551487597773, 0.026783185029988377, -0.08934155603075462, 0.06473603961264386, -0.06749079787509851, -0.1354999661215403, 0.06422143443121334, 0.2833865318196208, -0.32179094447095075, -0.2612161027565808, 0.15880615334811338, -0.23622754184801256, -0.07733322683789799, 0.12997353501785336, -0.0539172289034958... |
1,801.03476 | Schlieren Imaging for the Determination of the Radius of an Excited
Rubidium Column | AWAKE develops a new plasma wakefield accelerator using the CERN SPS proton
bunch as a driver. The proton bunch propagates through a 10 m long rubidium
plasma, induced by an ionizing laser pulse. The co-propagation of the laser
pulse with the proton bunch seeds the self modulation instability of the proton
bunch that... | physics.atom-ph | awake develops a new plasma wakefield accelerator using the cern sps proton bunch as a driver the proton bunch propagates through a 10 m long rubidium plasma induced by an ionizing laser pulse the copropagation of the laser pulse with the proton bunch seeds the self modulation instability of the proton bunch that trans... | [['awake', 'develops', 'a', 'new', 'plasma', 'wakefield', 'accelerator', 'using', 'the', 'cern', 'sps', 'proton', 'bunch', 'as', 'a', 'driver', 'the', 'proton', 'bunch', 'propagates', 'through', 'a', '10', 'm', 'long', 'rubidium', 'plasma', 'induced', 'by', 'an', 'ionizing', 'laser', 'pulse', 'the', 'copropagation', 'o... | [-0.06852475330684214, 0.25718057780817305, -0.05419706323895083, 0.009022177611377531, 0.019725223056851857, -0.13352469696822294, 0.019868620099269495, 0.4615059238407881, -0.21210432929232195, -0.26958833861174764, 0.026672267557186907, -0.2555321531134948, 0.07475765171005161, 0.20674056749946126, 0.024586248697252... |
1,801.03477 | Small System Collectivity in Relativistic Hadron and Nuclear Collisions | The bulk motion of nuclear matter at the ultra-high temperatures created in
heavy-ion collisions at the Relativistic Heavy Ion Collider and the Large
Hadron Collider is well described in terms of nearly inviscid hydrodynamics,
thereby establishing this system of quarks and gluons as the most perfect fluid
in nature. ... | nucl-ex hep-ph nucl-th | the bulk motion of nuclear matter at the ultrahigh temperatures created in heavyion collisions at the relativistic heavy ion collider and the large hadron collider is well described in terms of nearly inviscid hydrodynamics thereby establishing this system of quarks and gluons as the most perfect fluid in nature a revo... | [['the', 'bulk', 'motion', 'of', 'nuclear', 'matter', 'at', 'the', 'ultrahigh', 'temperatures', 'created', 'in', 'heavyion', 'collisions', 'at', 'the', 'relativistic', 'heavy', 'ion', 'collider', 'and', 'the', 'large', 'hadron', 'collider', 'is', 'well', 'described', 'in', 'terms', 'of', 'nearly', 'inviscid', 'hydrodyn... | [-0.10184896750485196, 0.27327403976198505, -0.13471941943554316, 0.09313810448682702, 0.004336545408210333, -0.09283213186461259, -0.09633913070839994, 0.2708110648673028, -0.2207412293249303, -0.30670128740808544, 0.0012543137828983804, -0.3235502488034613, 0.03538134811062585, 0.1545140397241887, 0.04825170643846778... |
1,801.03478 | Empirical Temperature Measurement in Protoplanetary Disks | Accurate measurement of temperature in protoplanetary disks is critical to
understanding many key features of disk evolution and planet formation, from
disk chemistry and dynamics, to planetesimal formation. This paper explores the
techniques available to determine temperatures from observations of single,
optically ... | astro-ph.EP | accurate measurement of temperature in protoplanetary disks is critical to understanding many key features of disk evolution and planet formation from disk chemistry and dynamics to planetesimal formation this paper explores the techniques available to determine temperatures from observations of single optically thick ... | [['accurate', 'measurement', 'of', 'temperature', 'in', 'protoplanetary', 'disks', 'is', 'critical', 'to', 'understanding', 'many', 'key', 'features', 'of', 'disk', 'evolution', 'and', 'planet', 'formation', 'from', 'disk', 'chemistry', 'and', 'dynamics', 'to', 'planetesimal', 'formation', 'this', 'paper', 'explores', ... | [-0.022673166373278944, 0.0605906796506606, -0.047633359760046005, 0.07480777463549748, -0.07881257104128599, -0.0916053311675787, 0.03797560978296678, 0.438578280556947, -0.23246434278786182, -0.33794519924558697, 0.09385158200934529, -0.2538804240208119, -0.048594590045744554, 0.18211382571049034, -0.0513940740043763... |
1,801.03479 | The hidden magnetization in ferromagnetic material: Miamagnetism | This paper presents the hidden magnetization features of ferromagnetic
materials: called miamagnetism. As we know, we have several forms of
magnetization: the diamagnetism, the paramagnetism, the ferromagnetism etc. The
main character of the diamagnetism is that its magnetic susceptibility is
negative (from -1e-9 for... | cond-mat.mtrl-sci | this paper presents the hidden magnetization features of ferromagnetic materials called miamagnetism as we know we have several forms of magnetization the diamagnetism the paramagnetism the ferromagnetism etc the main character of the diamagnetism is that its magnetic susceptibility is negative from 1e9 for gas and 1e6... | [['this', 'paper', 'presents', 'the', 'hidden', 'magnetization', 'features', 'of', 'ferromagnetic', 'materials', 'called', 'miamagnetism', 'as', 'we', 'know', 'we', 'have', 'several', 'forms', 'of', 'magnetization', 'the', 'diamagnetism', 'the', 'paramagnetism', 'the', 'ferromagnetism', 'etc', 'the', 'main', 'character... | [-0.12449012971070085, 0.2062824280271607, -0.05665886029000244, 0.03307678364592815, -0.1114877326819565, -0.11622994424054219, 0.04446337392568708, 0.36255824309923956, -0.268898046905956, -0.28922162627981557, 0.0879760354126413, -0.3215978169288006, -0.12565537704335106, 0.20609132266423155, 0.0027793209188647808, ... |
1,801.0348 | Smooth Version of Johnson's Problem Concerning Derivations of Group
Algebras | A description of the algebra of outer derivations of a group algebra of a
finitely presented discrete group is given in terms of the Cayley complex of
the groupoid of the adjoint action of the group. This task is a smooth version
of Johnson's problem concerning the derivations of a group algebra. It is shown
that the... | math.AT math.CT math.FA math.GR | a description of the algebra of outer derivations of a group algebra of a finitely presented discrete group is given in terms of the cayley complex of the groupoid of the adjoint action of the group this task is a smooth version of johnsons problem concerning the derivations of a group algebra it is shown that the alge... | [['a', 'description', 'of', 'the', 'algebra', 'of', 'outer', 'derivations', 'of', 'a', 'group', 'algebra', 'of', 'a', 'finitely', 'presented', 'discrete', 'group', 'is', 'given', 'in', 'terms', 'of', 'the', 'cayley', 'complex', 'of', 'the', 'groupoid', 'of', 'the', 'adjoint', 'action', 'of', 'the', 'group', 'this', 'ta... | [-0.2186167604634987, 0.05122926175953394, -0.12222511370677545, -0.013029964408607233, -0.15569058540894323, -0.03726962259802294, -0.0334994885060622, 0.3336684106882796, -0.3396225865223411, -0.2107805979763528, 0.13972620465596353, -0.21219888351947427, -0.15013617012335592, 0.20937831396887818, -0.1314237967963857... |
1,801.03481 | Latent Factor Analysis of Gaussian Distributions under Graphical
Constraints | In this paper, we explore the algebraic structures of solution spaces for
Gaussian latent factor analysis when the population covariance matrix
$\Sigma_x$ has an additional latent graphical constraint, namely, a latent star
topology. In particular, we give sufficient and necessary conditions under
which the solutions... | cs.IT math.IT | in this paper we explore the algebraic structures of solution spaces for gaussian latent factor analysis when the population covariance matrix sigma_x has an additional latent graphical constraint namely a latent star topology in particular we give sufficient and necessary conditions under which the solutions to constr... | [['in', 'this', 'paper', 'we', 'explore', 'the', 'algebraic', 'structures', 'of', 'solution', 'spaces', 'for', 'gaussian', 'latent', 'factor', 'analysis', 'when', 'the', 'population', 'covariance', 'matrix', 'sigma_x', 'has', 'an', 'additional', 'latent', 'graphical', 'constraint', 'namely', 'a', 'latent', 'star', 'top... | [-0.11471988678909838, 0.09567088409923599, -0.0596736576128751, 0.07969065370620228, -0.12041948879836127, -0.1428032478131354, 0.04539980306639336, 0.3790121079306118, -0.287919162819162, -0.2892330969683826, 0.1713655204628594, -0.23156828060746193, -0.14501062865834682, 0.12283007738878951, -0.055454660047544166, 0... |
1,801.03482 | Cohomological Hall algebra of Higgs sheaves on a curve | We define the cohomological Hall algebra ${AHA}_{Higgs(X)}$ of the
($2$-dimensional) Calabi-Yau category of Higgs sheaves on a smooth projective
curve $X$, as well as its nilpotent and semistable variants, in the context of
an arbitrary oriented Borel-Moore homology theory. In the case of usual
Borel-Moore homology, ... | math.AG math.RT | we define the cohomological hall algebra aha_higgsx of the 2dimensional calabiyau category of higgs sheaves on a smooth projective curve x as well as its nilpotent and semistable variants in the context of an arbitrary oriented borelmoore homology theory in the case of usual borelmoore homology aha_higgsx is a module o... | [['we', 'define', 'the', 'cohomological', 'hall', 'algebra', 'aha_higgsx', 'of', 'the', '2dimensional', 'calabiyau', 'category', 'of', 'higgs', 'sheaves', 'on', 'a', 'smooth', 'projective', 'curve', 'x', 'as', 'well', 'as', 'its', 'nilpotent', 'and', 'semistable', 'variants', 'in', 'the', 'context', 'of', 'an', 'arbitr... | [-0.2368075921004148, 0.035652734959608336, -0.09872814383553831, 0.05327971572987735, -0.06305583977189504, -0.13847473185313375, -0.041671823932005, 0.3587108645784228, -0.3911535743574955, -0.15929183610469888, 0.0825382578198945, -0.20324068484631808, -0.11888117473572493, 0.21965284450469832, -0.18917240288206622,... |
1,801.03483 | On Rational Choice and the Representation of Decision Problems | In economic theory, an agent chooses from available alternatives -- modeled
as a set. In decisions in the field or in the lab, however, agents do not have
access to the set of alternatives at once. Instead, alternatives are
represented by the outside world in a structured way. Online search results are
lists of items... | cs.GT | in economic theory an agent chooses from available alternatives modeled as a set in decisions in the field or in the lab however agents do not have access to the set of alternatives at once instead alternatives are represented by the outside world in a structured way online search results are lists of items wine menus ... | [['in', 'economic', 'theory', 'an', 'agent', 'chooses', 'from', 'available', 'alternatives', 'modeled', 'as', 'a', 'set', 'in', 'decisions', 'in', 'the', 'field', 'or', 'in', 'the', 'lab', 'however', 'agents', 'do', 'not', 'have', 'access', 'to', 'the', 'set', 'of', 'alternatives', 'at', 'once', 'instead', 'alternative... | [-0.054498300927728685, 0.06742049079624408, -0.08350636714288194, 0.08457558163177172, -0.15530009391366234, -0.17617215530864977, 0.12028394734287369, 0.4528921034729497, -0.2901893294119573, -0.33560139858146837, 0.10783146321816173, -0.26881759006004685, -0.12381994986101548, 0.17688683938318625, -0.098518013971219... |
1,801.03484 | ONETS: Online Network Slice Broker From Theory to Practice | Network slicing allows mobile network operators to open their physical
network infrastructure platform to the concurrent deployment of multiple
logical self-contained networks, i.e., network slices. In this paper we propose
and analyze ONETS: an Online NETwork Slicing solution that (i) builds on the
budgeted lock-up ... | cs.NI | network slicing allows mobile network operators to open their physical network infrastructure platform to the concurrent deployment of multiple logical selfcontained networks ie network slices in this paper we propose and analyze onets an online network slicing solution that i builds on the budgeted lockup multiarmed b... | [['network', 'slicing', 'allows', 'mobile', 'network', 'operators', 'to', 'open', 'their', 'physical', 'network', 'infrastructure', 'platform', 'to', 'the', 'concurrent', 'deployment', 'of', 'multiple', 'logical', 'selfcontained', 'networks', 'ie', 'network', 'slices', 'in', 'this', 'paper', 'we', 'propose', 'and', 'an... | [-0.2082567579277298, -0.11220119706244898, -0.023598298270657073, -0.002699138301050327, -0.13693010148035326, -0.2359195769600132, 0.08154488008985222, 0.44245507247636423, -0.2705440548632075, -0.2679167790155785, 0.08349522880926802, -0.1964546195690762, -0.21504064860717192, 0.14115053668558852, -0.127267944696131... |
1,801.03485 | Search for $h_{c}\rightarrow\pi^+\pi^-J/\psi$ via $\psi(3686)\rightarrow
\pi^0\pi^+\pi^-J/\psi$ | Using a data sample of $448.1\times10^6$ $\psi(3686)$ events collected with
the BESIII detector operating at the BEPCII, we perform search for the hadronic
transition $h_c\rightarrow\pi^+\pi^-J/\psi$ via
$\psi(3686)\rightarrow\pi^0h_c$. No signals of the transition are observed, and
the upper limit on the product bra... | hep-ex | using a data sample of 4481times106 psi3686 events collected with the besiii detector operating at the bepcii we perform search for the hadronic transition h_crightarrowpipijpsi via psi3686rightarrowpi0h_c no signals of the transition are observed and the upper limit on the product branching fraction mathcalbpsi3686rig... | [['using', 'a', 'data', 'sample', 'of', '4481times106', 'psi3686', 'events', 'collected', 'with', 'the', 'besiii', 'detector', 'operating', 'at', 'the', 'bepcii', 'we', 'perform', 'search', 'for', 'the', 'hadronic', 'transition', 'h_crightarrowpipijpsi', 'via', 'psi3686rightarrowpi0h_c', 'no', 'signals', 'of', 'the', '... | [-0.10534858894393907, 0.15587678511530675, -0.0626672930646174, 0.07361580355389943, -0.04018778845282464, -0.04420161863050327, 0.16601664515147949, 0.2990156638853509, -0.12138129545351618, -0.35434715000206024, 0.1417258480355015, -0.41635611097745856, 0.05301638243816279, 0.21363771592812805, 0.10247382259895575, ... |
1,801.03486 | Evolution of Photospheric Flow and Magnetic Fields Associated with The
2015 June 22 M6.5 Flare | The evolution of photospheric flow and magnetic fields before and after
flares can provide important information regarding the flare triggering and
back reaction processes. However, such studies on the flow field are rare due
to the paucity of high-resolution observations covering the entire flaring
period. Here we s... | astro-ph.SR | the evolution of photospheric flow and magnetic fields before and after flares can provide important information regarding the flare triggering and back reaction processes however such studies on the flow field are rare due to the paucity of highresolution observations covering the entire flaring period here we study t... | [['the', 'evolution', 'of', 'photospheric', 'flow', 'and', 'magnetic', 'fields', 'before', 'and', 'after', 'flares', 'can', 'provide', 'important', 'information', 'regarding', 'the', 'flare', 'triggering', 'and', 'back', 'reaction', 'processes', 'however', 'such', 'studies', 'on', 'the', 'flow', 'field', 'are', 'rare',... | [-0.09889191987683936, 0.18075953572124784, -0.01209875908534741, 0.07552882901584398, -0.08570180870705255, -0.049360792165727266, 0.0015540442344049111, 0.4329258380720632, -0.22881167723737175, -0.38194452728625505, 0.11269399272597154, -0.2756911891272231, -0.13059132077896426, 0.22739271271500677, -0.0283259832269... |
1,801.03487 | Tachyon constant-roll inflation | The constant-roll inflation is studied where the inflaton is taken as a
tachyon field. Since in this approach the second slow-roll parameter is assumed
to be of order one instead of being small, then the perturbation parameters
will be considered again. The results are compared with observational data, and
it is conf... | hep-ph | the constantroll inflation is studied where the inflaton is taken as a tachyon field since in this approach the second slowroll parameter is assumed to be of order one instead of being small then the perturbation parameters will be considered again the results are compared with observational data and it is confirmed th... | [['the', 'constantroll', 'inflation', 'is', 'studied', 'where', 'the', 'inflaton', 'is', 'taken', 'as', 'a', 'tachyon', 'field', 'since', 'in', 'this', 'approach', 'the', 'second', 'slowroll', 'parameter', 'is', 'assumed', 'to', 'be', 'of', 'order', 'one', 'instead', 'of', 'being', 'small', 'then', 'the', 'perturbation... | [-0.11584299539644567, 0.167619748077991, -0.1318915560619817, 0.11416812321459431, -0.10995806214798774, -0.1719092588487362, -0.03175083264738085, 0.32016831827128217, -0.22472961480537104, -0.27971171414745705, 0.15772265879740377, -0.22721461596943082, -0.10268703123761548, 0.1842865143821294, -0.047683093386391796... |
1,801.03488 | Correcting finite squeezing errors in continuous-variable cluster states | We introduce an efficient scheme to correct errors due to the finite
squeezing effects in continuous-variable cluster states. Specifically, we
consider the typical situation where the class of algorithms consists of input
states that are known. By using the knowledge of the input states, we can
diagnose exactly what ... | quant-ph | we introduce an efficient scheme to correct errors due to the finite squeezing effects in continuousvariable cluster states specifically we consider the typical situation where the class of algorithms consists of input states that are known by using the knowledge of the input states we can diagnose exactly what errors ... | [['we', 'introduce', 'an', 'efficient', 'scheme', 'to', 'correct', 'errors', 'due', 'to', 'the', 'finite', 'squeezing', 'effects', 'in', 'continuousvariable', 'cluster', 'states', 'specifically', 'we', 'consider', 'the', 'typical', 'situation', 'where', 'the', 'class', 'of', 'algorithms', 'consists', 'of', 'input', 'st... | [-0.12249040274400613, 0.13976284930424754, -0.08196123429752333, 0.08360123228067096, 0.018285032416315516, -0.20554901873038034, 0.09511167766686413, 0.4295033263915684, -0.2494824512541527, -0.2703950138457003, 0.04365886997766211, -0.19367294064431917, -0.10308429550786968, 0.20423206838859187, -0.128861181299726, ... |
1,801.03489 | The effect of turbulence strength on meandering field lines and Solar
Energetic Particle event extents | Insights into the processes of Solar Energetic Particle (SEP) propagation are
essential for understanding how solar eruptions affect the radiation
environment of near-Earth space. SEP propagation is influenced by turbulent
magnetic fields in the solar wind, resulting in stochastic transport of SEPs to
Earth. Multi-sp... | astro-ph.SR physics.space-ph | insights into the processes of solar energetic particle sep propagation are essential for understanding how solar eruptions affect the radiation environment of nearearth space sep propagation is influenced by turbulent magnetic fields in the solar wind resulting in stochastic transport of seps to earth multispacecraft ... | [['insights', 'into', 'the', 'processes', 'of', 'solar', 'energetic', 'particle', 'sep', 'propagation', 'are', 'essential', 'for', 'understanding', 'how', 'solar', 'eruptions', 'affect', 'the', 'radiation', 'environment', 'of', 'nearearth', 'space', 'sep', 'propagation', 'is', 'influenced', 'by', 'turbulent', 'magnetic... | [-0.1294692188790068, 0.2599797418131493, -0.04214635007828474, 0.1011225966871716, -0.02724515804555267, -0.04311554474383593, -0.04408981042494997, 0.41176468366384505, -0.2679942155666649, -0.33360803448478693, -0.00022744663013145327, -0.24873479083739222, -0.09329682217538357, 0.2219111927463673, -0.00367596185368... |
1,801.0349 | Superconductivity in the presence of microwaves: Full phase diagram | We address the problem of non-equilibrium superconductivity in the presence
of microwave irradiation. We refine the old Eliashberg theory and generalize it
to arbitrary temperatures $T$ and frequencies $\omega$. Microwave radiation is
shown to stimulate superconductivity in a bounded region in the $(\omega,T)$
plane.... | cond-mat.supr-con | we address the problem of nonequilibrium superconductivity in the presence of microwave irradiation we refine the old eliashberg theory and generalize it to arbitrary temperatures t and frequencies omega microwave radiation is shown to stimulate superconductivity in a bounded region in the omegat plane in particular fo... | [['we', 'address', 'the', 'problem', 'of', 'nonequilibrium', 'superconductivity', 'in', 'the', 'presence', 'of', 'microwave', 'irradiation', 'we', 'refine', 'the', 'old', 'eliashberg', 'theory', 'and', 'generalize', 'it', 'to', 'arbitrary', 'temperatures', 't', 'and', 'frequencies', 'omega', 'microwave', 'radiation', '... | [-0.17110412848482015, 0.19790091687508932, -0.028478093165456533, 0.07330685397475743, -0.04239319384886095, -0.09863098089296657, 0.0995653403660981, 0.3408329125243024, -0.2482769525018879, -0.28306232508307755, 0.010627992337014383, -0.2841199007021854, -0.11566077232307109, 0.21721870006988936, -0.0268083514330590... |
1,801.03491 | Note on the absence of remainders in the Wiener-Ikehara theorem | We show that it is impossible to get a better remainder than the classical
one in the Wiener-Ikehara theorem even if one assumes analytic continuation of
the Mellin transform after subtraction of the pole to a half-plane. We also
prove a similar result for the Ingham-Karamata theorem.
| math.CA math.CV math.FA math.NT | we show that it is impossible to get a better remainder than the classical one in the wienerikehara theorem even if one assumes analytic continuation of the mellin transform after subtraction of the pole to a halfplane we also prove a similar result for the inghamkaramata theorem | [['we', 'show', 'that', 'it', 'is', 'impossible', 'to', 'get', 'a', 'better', 'remainder', 'than', 'the', 'classical', 'one', 'in', 'the', 'wienerikehara', 'theorem', 'even', 'if', 'one', 'assumes', 'analytic', 'continuation', 'of', 'the', 'mellin', 'transform', 'after', 'subtraction', 'of', 'the', 'pole', 'to', 'a', '... | [-0.09269516595193873, 0.006542832064239875, -0.2249105528158986, 0.20080638301568915, -0.09695797571507485, -0.11694094636882453, 0.06792415725067258, 0.31236265437758487, -0.2573562615915485, -0.17797651336244916, 0.1486063678343983, -0.25279880995335785, -0.16056212529783015, 0.2531156192695641, -0.07698625342353531... |
1,801.03492 | $B+L$ violation at colliders and new physics | Chiral electroweak anomalies predict fermion interactions that violate baryon
($B$) and lepton number ($L$), and can be dressed with large numbers of Higgs
and gauge bosons. The estimation of the total $B+L$ violating rate from an
initial two-particle state --potentially observable at colliders-- has been the
subject... | hep-ph hep-th | chiral electroweak anomalies predict fermion interactions that violate baryon b and lepton number l and can be dressed with large numbers of higgs and gauge bosons the estimation of the total bl violating rate from an initial twoparticle state potentially observable at colliders has been the subject of an intense discu... | [['chiral', 'electroweak', 'anomalies', 'predict', 'fermion', 'interactions', 'that', 'violate', 'baryon', 'b', 'and', 'lepton', 'number', 'l', 'and', 'can', 'be', 'dressed', 'with', 'large', 'numbers', 'of', 'higgs', 'and', 'gauge', 'bosons', 'the', 'estimation', 'of', 'the', 'total', 'bl', 'violating', 'rate', 'from'... | [-0.0925895285070373, 0.2548226656255147, -0.06447014513473097, 0.12257161849711631, -0.08879180345715584, -0.1352376797817327, 0.01784508982648252, 0.30723496980624654, -0.21604972984892146, -0.31741053654101264, 0.017149722035874122, -0.31055285610879463, -0.03270066409842462, 0.17156289855233564, 0.03781922218910549... |
1,801.03493 | Focus: Querying Large Video Datasets with Low Latency and Low Cost | Large volumes of videos are continuously recorded from cameras deployed for
traffic control and surveillance with the goal of answering "after the fact"
queries: identify video frames with objects of certain classes (cars, bags)
from many days of recorded video. While advancements in convolutional neural
networks (CN... | cs.DB cs.CV cs.DC | large volumes of videos are continuously recorded from cameras deployed for traffic control and surveillance with the goal of answering after the fact queries identify video frames with objects of certain classes cars bags from many days of recorded video while advancements in convolutional neural networks cnns have en... | [['large', 'volumes', 'of', 'videos', 'are', 'continuously', 'recorded', 'from', 'cameras', 'deployed', 'for', 'traffic', 'control', 'and', 'surveillance', 'with', 'the', 'goal', 'of', 'answering', 'after', 'the', 'fact', 'queries', 'identify', 'video', 'frames', 'with', 'objects', 'of', 'certain', 'classes', 'cars', '... | [-0.12762002872740738, 0.05694529167320355, -0.01957081178068576, 0.048259212784833805, -0.09885752713868776, -0.2068469426959349, 0.06278571259533336, 0.4668769790308483, -0.23539163294551244, -0.37719298327756845, 0.10752557088580285, -0.31234608460722646, -0.12266225345623512, 0.2428642748462328, -0.1930118545536400... |
1,801.03494 | Secure Retrospective Interference Alignment | In this paper, the $K$-user interference channel with secrecy constraints is
considered with delayed channel state information at transmitters (CSIT). We
propose a novel secure retrospective interference alignment scheme in which the
transmitters carefully mix information symbols with artificial noises to ensure
conf... | cs.IT cs.CR math.IT | in this paper the kuser interference channel with secrecy constraints is considered with delayed channel state information at transmitters csit we propose a novel secure retrospective interference alignment scheme in which the transmitters carefully mix information symbols with artificial noises to ensure confidentiali... | [['in', 'this', 'paper', 'the', 'kuser', 'interference', 'channel', 'with', 'secrecy', 'constraints', 'is', 'considered', 'with', 'delayed', 'channel', 'state', 'information', 'at', 'transmitters', 'csit', 'we', 'propose', 'a', 'novel', 'secure', 'retrospective', 'interference', 'alignment', 'scheme', 'in', 'which', 't... | [-0.33214530712459234, 0.060790784596581944, 0.003528717951849103, -0.03552800617995672, -0.07138061644136906, -0.33384184683859347, 0.13677559636952355, 0.37581350581347944, -0.2746831311360002, -0.25653444446611684, 0.0735228236638941, -0.28192857646755876, -0.1451733356034383, 0.028727938268333673, -0.10821063163317... |
1,801.03495 | Collisionless Transport Close to a Fermionic Quantum Critical Point in
Dirac Materials | Quantum transport close to a critical point is a fundamental, but enigmatic
problem due to fluctuations, persisting at all length scales. We report the
scaling of optical conductivity (OC) in the \emph{collisionless} regime ($\hbar
\omega \gg k_B T$) in the vicinity of a relativistic quantum critical point,
separatin... | cond-mat.mes-hall cond-mat.str-el hep-th | quantum transport close to a critical point is a fundamental but enigmatic problem due to fluctuations persisting at all length scales we report the scaling of optical conductivity oc in the emphcollisionless regime hbar omega gg k_b t in the vicinity of a relativistic quantum critical point separating twodimensional d... | [['quantum', 'transport', 'close', 'to', 'a', 'critical', 'point', 'is', 'a', 'fundamental', 'but', 'enigmatic', 'problem', 'due', 'to', 'fluctuations', 'persisting', 'at', 'all', 'length', 'scales', 'we', 'report', 'the', 'scaling', 'of', 'optical', 'conductivity', 'oc', 'in', 'the', 'emphcollisionless', 'regime', 'hb... | [-0.16449028522953207, 0.2502547260484532, -0.06391343429821766, 0.056199626505740584, -0.03397287847759899, -0.21807178529550783, 0.09749538582846796, 0.29208593652155135, -0.2529071727967564, -0.24984795396199072, 0.026305971712165404, -0.3560231894574648, -0.11637323589401286, 0.15167057919501686, 0.0370334685562989... |
1,801.03496 | Investigating the electronic structure of MSi (M = Cr, Mn, Fe $\&$ Co)
and calculating $\textit{$U_{eff}$}$ $\&$ $\textit{J}$ by using cDFT | We have investigated electronic energy band structures and partial density of
states of intermetallic compounds $\textit{viz.}$ CrSi, MnSi, FeSi and CoSi, by
using density functional theory (DFT). CrSi \& MnSi, FeSi and CoSi have
metallic, indirect band gap semiconducting (band gap $ \sim$ 90 meV) and
semi-metallic g... | cond-mat.str-el physics.comp-ph | we have investigated electronic energy band structures and partial density of states of intermetallic compounds textitviz crsi mnsi fesi and cosi by using density functional theory dft crsi mnsi fesi and cosi have metallic indirect band gap semiconducting band gap sim 90 mev and semimetallic ground state respectively o... | [['we', 'have', 'investigated', 'electronic', 'energy', 'band', 'structures', 'and', 'partial', 'density', 'of', 'states', 'of', 'intermetallic', 'compounds', 'textitviz', 'crsi', 'mnsi', 'fesi', 'and', 'cosi', 'by', 'using', 'density', 'functional', 'theory', 'dft', 'crsi', 'mnsi', 'fesi', 'and', 'cosi', 'have', 'meta... | [-0.09236320980091063, 0.2404637457083415, 0.0567060378559989, 0.05713452325979959, 0.02859310287711922, -0.15707960339710755, 0.13127190890660023, 0.3720877686907166, -0.20708982327547276, -0.40335221696133394, -0.017664254222329017, -0.41158294261237327, -0.00891463763716075, 0.1545673106110539, 0.09191207008440319, ... |
1,801.03497 | Tidal Disruptions of Main Sequence Stars of Varying Mass and Age:
Inferences from the Composition of the Fallback Material | We use a simple framework to calculate the time evolution of the composition
of the fallback material onto a supermassive black hole arising from the tidal
disruption of main sequence stars. We study stars with masses between 0.8 and
3.0 $M_\odot$, at evolutionary stages from zero-age main sequence to
terminal-age ma... | astro-ph.HE astro-ph.SR | we use a simple framework to calculate the time evolution of the composition of the fallback material onto a supermassive black hole arising from the tidal disruption of main sequence stars we study stars with masses between 08 and 30 m_odot at evolutionary stages from zeroage main sequence to terminalage main sequence... | [['we', 'use', 'a', 'simple', 'framework', 'to', 'calculate', 'the', 'time', 'evolution', 'of', 'the', 'composition', 'of', 'the', 'fallback', 'material', 'onto', 'a', 'supermassive', 'black', 'hole', 'arising', 'from', 'the', 'tidal', 'disruption', 'of', 'main', 'sequence', 'stars', 'we', 'study', 'stars', 'with', 'ma... | [-0.0667684070049219, 0.1325879553897311, -0.06514165959887061, 0.12444086705617534, -0.07096513610095809, -0.05283270403377566, 0.06034845485141976, 0.39044512596675285, -0.21435344763517872, -0.37376027944154366, 0.06626568548518288, -0.2798113792769465, -0.05793746244162321, 0.22508724293872423, -0.05075041656291076... |
1,801.03498 | Topological magnon nodal-lines and absence of magnon spin Nernst effect
in layered collinear antiferromagnets | We propose the existence of a symmetry-protected topological Dirac nodal line
(DNL) magnonic phase in layered honeycomb collinear antiferromagnets even in
the presence of spin-orbit Dzyaloshinskii-Moriya interaction. We show that the
magnon spin Nernst effect, predicted to occur in strictly two-dimensional (2D)
honey... | cond-mat.str-el | we propose the existence of a symmetryprotected topological dirac nodal line dnl magnonic phase in layered honeycomb collinear antiferromagnets even in the presence of spinorbit dzyaloshinskiimoriya interaction we show that the magnon spin nernst effect predicted to occur in strictly twodimensional 2d honeycomb colline... | [['we', 'propose', 'the', 'existence', 'of', 'a', 'symmetryprotected', 'topological', 'dirac', 'nodal', 'line', 'dnl', 'magnonic', 'phase', 'in', 'layered', 'honeycomb', 'collinear', 'antiferromagnets', 'even', 'in', 'the', 'presence', 'of', 'spinorbit', 'dzyaloshinskiimoriya', 'interaction', 'we', 'show', 'that', 'the... | [-0.3303838313383656, 0.2656922903466481, 0.017840980267883534, 0.015971622671903413, -0.13944350035026945, -0.15876851259999297, 0.06461162981077274, 0.41297781123833993, -0.2692091139204846, -0.18009361239618685, -0.03420250288473636, -0.3300736618851043, -0.20637303645054073, 0.10599751643689372, 0.0685629441097173,... |
1,801.03499 | Floquet Weyl Magnons | In three-dimensional (3D) quantum magnets, magnonic Weyl points (WPs)
featuring linear band crossing of two non-degenerate magnon branches can emerge
in certain lattice geometry when time-reversal symmetry is broken
macroscopically. Unfortunately, there are very limited 3D quantum magnets that
host magnonic WPs, and ... | cond-mat.str-el | in threedimensional 3d quantum magnets magnonic weyl points wps featuring linear band crossing of two nondegenerate magnon branches can emerge in certain lattice geometry when timereversal symmetry is broken macroscopically unfortunately there are very limited 3d quantum magnets that host magnonic wps and they are yet ... | [['in', 'threedimensional', '3d', 'quantum', 'magnets', 'magnonic', 'weyl', 'points', 'wps', 'featuring', 'linear', 'band', 'crossing', 'of', 'two', 'nondegenerate', 'magnon', 'branches', 'can', 'emerge', 'in', 'certain', 'lattice', 'geometry', 'when', 'timereversal', 'symmetry', 'is', 'broken', 'macroscopically', 'unf... | [-0.2305836239443101, 0.26980857918201645, -0.0612730804645719, 0.03443041470152541, -0.15130302070234067, -0.21677317522609463, 0.02500976547360038, 0.41036497757602963, -0.29606748622579454, -0.2837677132815887, -0.009978738013440026, -0.2764247702530179, -0.1668004229426002, 0.18707519590090482, 0.023228948877360194... |
1,801.035 | Chemical pre-processing of cluster galaxies over the past 10 billion
years in the IllustrisTNG simulations | We use the IllustrisTNG simulations to investigate the evolution of the
mass-metallicity relation (MZR) for star-forming cluster galaxies as a function
of the formation history of their cluster host. The simulations predict an
enhancement in the gas-phase metallicities of star-forming cluster galaxies
(10^9< M_star<1... | astro-ph.GA | we use the illustristng simulations to investigate the evolution of the massmetallicity relation mzr for starforming cluster galaxies as a function of the formation history of their cluster host the simulations predict an enhancement in the gasphase metallicities of starforming cluster galaxies 109 m_star1010 m_sun at ... | [['we', 'use', 'the', 'illustristng', 'simulations', 'to', 'investigate', 'the', 'evolution', 'of', 'the', 'massmetallicity', 'relation', 'mzr', 'for', 'starforming', 'cluster', 'galaxies', 'as', 'a', 'function', 'of', 'the', 'formation', 'history', 'of', 'their', 'cluster', 'host', 'the', 'simulations', 'predict', 'an... | [-0.060715858278930876, 0.07054170926582484, -0.09661072480345242, 0.11319481421470348, -0.05018229504042354, 0.02270984953195837, 0.06989614861576181, 0.43361573683980265, -0.12316992753430417, -0.33435526247822533, -0.009749840952970676, -0.262567398322158, -0.00210102760282002, 0.1791221095151023, 0.0016618236629782... |
1,801.03501 | Probing star formation and ISM properties using galaxy disk inclination
I: Evolution in disk opacity since $z\sim0.7$ | Disk galaxies at intermediate redshift ($z\sim0.7$) have been found in
previous work to display more optically thick behaviour than their local
counterparts in the rest-frame B-band surface brightness, suggesting an
evolution in dust properties over the past $\sim$6 Gyr. We compare the measured
luminosities of face-o... | astro-ph.GA | disk galaxies at intermediate redshift zsim07 have been found in previous work to display more optically thick behaviour than their local counterparts in the restframe bband surface brightness suggesting an evolution in dust properties over the past sim6 gyr we compare the measured luminosities of faceon and edgeon sta... | [['disk', 'galaxies', 'at', 'intermediate', 'redshift', 'zsim07', 'have', 'been', 'found', 'in', 'previous', 'work', 'to', 'display', 'more', 'optically', 'thick', 'behaviour', 'than', 'their', 'local', 'counterparts', 'in', 'the', 'restframe', 'bband', 'surface', 'brightness', 'suggesting', 'an', 'evolution', 'in', 'd... | [0.005194723561071112, 0.07407161690000016, -0.08567521489347538, 0.1122732958245424, -0.06360806242617614, -0.031214738174076127, 0.04210078917924163, 0.5505040316459011, -0.12602179908595043, -0.3199268977128273, 0.02950621090778803, -0.3118209414672932, 0.009266352926789703, 0.20918840717216658, 0.003802951890382625... |
1,801.03502 | An ultra-short period rocky super-Earth with a secondary eclipse and a
Neptune-like companion around K2-141 | Ultra-short period (USP) planets are a class of low mass planets with periods
shorter than one day. Their origin is still unknown, with photo-evaporation of
mini-Neptunes and in-situ formation being the most credited hypotheses.
Formation scenarios differ radically in the predicted composition of USP
planets, it is t... | astro-ph.EP astro-ph.SR | ultrashort period usp planets are a class of low mass planets with periods shorter than one day their origin is still unknown with photoevaporation of minineptunes and insitu formation being the most credited hypotheses formation scenarios differ radically in the predicted composition of usp planets it is therefore ext... | [['ultrashort', 'period', 'usp', 'planets', 'are', 'a', 'class', 'of', 'low', 'mass', 'planets', 'with', 'periods', 'shorter', 'than', 'one', 'day', 'their', 'origin', 'is', 'still', 'unknown', 'with', 'photoevaporation', 'of', 'minineptunes', 'and', 'insitu', 'formation', 'being', 'the', 'most', 'credited', 'hypothese... | [-0.11932878102334332, 0.16881528907057952, -0.10902390414276508, 0.03450785791240555, -0.10511385310630611, -0.10494360145513756, 0.1039446664894873, 0.37431722190385663, -0.17250815468272232, -0.3894615807721229, 0.1275737394947806, -0.28201214284445275, -0.06693152775814085, 0.22109959776613752, -0.11555822904287409... |
1,801.03503 | TASI Lectures on Remnants from the String Landscape | Superstring theories are very promising theoretically, but the enormous
landscape of string vacua and the (likely) very large underlying string scale
imply that they may never be tested directly. Nevertheless, concrete
constructions consistent with the observed world frequently lead to observable
remnants, i.e., new ... | hep-th hep-ex hep-ph | superstring theories are very promising theoretically but the enormous landscape of string vacua and the likely very large underlying string scale imply that they may never be tested directly nevertheless concrete constructions consistent with the observed world frequently lead to observable remnants ie new particles o... | [['superstring', 'theories', 'are', 'very', 'promising', 'theoretically', 'but', 'the', 'enormous', 'landscape', 'of', 'string', 'vacua', 'and', 'the', 'likely', 'very', 'large', 'underlying', 'string', 'scale', 'imply', 'that', 'they', 'may', 'never', 'be', 'tested', 'directly', 'nevertheless', 'concrete', 'constructi... | [-0.09446949524160901, 0.21221933319738404, -0.1045580546068148, 0.217963873558453, -0.13076379128259175, -0.19037187356033838, 0.01639960328376486, 0.3468670231007521, -0.22703462949402592, -0.32738403660889287, 0.13354291120168768, -0.25856743924857223, -0.12969964372100706, 0.16995599306830256, -0.06797906920598792,... |
1,801.03504 | Prediction of new states from $D^{(*)}B^{(*)}\bar{B}^{(*)}$ three-body
interactions | We study three-body systems composed of $D^{(*)}$, $B^{(*)}$ and
$\bar{B}^{(*)}$ in order to look for possible bound states or resonances. In
order to solve the three-body problem, we use the fixed center approach for the
Faddeev equations considering that the $B^*\bar{B}^*(B\bar{B})$ are clusterized
systems, generat... | hep-ph | we study threebody systems composed of d b and barb in order to look for possible bound states or resonances in order to solve the threebody problem we use the fixed center approach for the faddeev equations considering that the bbarbbbarb are clusterized systems generated dynamically which interact with a third partic... | [['we', 'study', 'threebody', 'systems', 'composed', 'of', 'd', 'b', 'and', 'barb', 'in', 'order', 'to', 'look', 'for', 'possible', 'bound', 'states', 'or', 'resonances', 'in', 'order', 'to', 'solve', 'the', 'threebody', 'problem', 'we', 'use', 'the', 'fixed', 'center', 'approach', 'for', 'the', 'faddeev', 'equations',... | [-0.13083304806479995, 0.21855561744524252, -0.007872491562311802, 0.09530589265274653, -0.01097689940217122, -0.1741211873034887, 0.07697277608084056, 0.33343906220424613, -0.2159644658396922, -0.3473374495633083, -0.0019202652684233467, -0.3359241728252227, -0.015887963954026068, 0.1393768128654877, 0.097061841347075... |
1,801.03505 | Top-philic $Z'$ Forces at the LHC | Despite extensive searches for an additional neutral massive gauge boson at
the LHC, a $Z^\prime$ at the weak scale could still be present if its couplings
to the first two generations of quarks are suppressed, in which case the
production in hadron colliders relies on tree-level processes in association
with heavy f... | hep-ph hep-ex | despite extensive searches for an additional neutral massive gauge boson at the lhc a zprime at the weak scale could still be present if its couplings to the first two generations of quarks are suppressed in which case the production in hadron colliders relies on treelevel processes in association with heavy flavors or... | [['despite', 'extensive', 'searches', 'for', 'an', 'additional', 'neutral', 'massive', 'gauge', 'boson', 'at', 'the', 'lhc', 'a', 'zprime', 'at', 'the', 'weak', 'scale', 'could', 'still', 'be', 'present', 'if', 'its', 'couplings', 'to', 'the', 'first', 'two', 'generations', 'of', 'quarks', 'are', 'suppressed', 'in', 'w... | [-0.09371361551862008, 0.22639505185764827, -0.0632148072627783, 0.15542438253190916, -0.065828117779861, -0.15515379210979596, 0.08071722857762918, 0.3291481779938888, -0.21645551178422148, -0.26903849310727546, 0.04643150633605926, -0.2864671110216042, -0.03532616685539403, 0.1385315200301272, 0.04322905817737236, 0.... |
1,801.03506 | $r$-process nucleosynthesis in the early Universe through fast mergers
of compact binaries in triple systems | Surface abundance observations of halo stars hint at the occurrence of
$r$-process nucleosynthesis at low metallicity ($\rm{[Fe/H]< -3}$), possibly
within the first $10^8$ yr after the formation of the first stars. Possible
loci of early-Universe $r$-process nucleosynthesis are the ejecta of either
black hole--neutro... | astro-ph.HE astro-ph.CO gr-qc | surface abundance observations of halo stars hint at the occurrence of rprocess nucleosynthesis at low metallicity rmfeh 3 possibly within the first 108 yr after the formation of the first stars possible loci of earlyuniverse rprocess nucleosynthesis are the ejecta of either black holeneutron star or neutron starneutro... | [['surface', 'abundance', 'observations', 'of', 'halo', 'stars', 'hint', 'at', 'the', 'occurrence', 'of', 'rprocess', 'nucleosynthesis', 'at', 'low', 'metallicity', 'rmfeh', '3', 'possibly', 'within', 'the', 'first', '108', 'yr', 'after', 'the', 'formation', 'of', 'the', 'first', 'stars', 'possible', 'loci', 'of', 'ear... | [-0.1396708130982006, 0.18610053511569277, -0.041478164556901904, 0.11328471002198057, -0.11186512596847024, -0.0485019624105189, 0.07233861096086912, 0.3458171412907541, -0.1519163558940636, -0.3425447110366076, 0.05973363939963747, -0.2929448121646419, 0.0008124147914350033, 0.23591176344431006, -0.04383419750025496,... |
1,801.03507 | On the Schrodinger-Poisson--Vlasov-Poisson correspondence | The Schr\"odinger-Poisson equations describe the behavior of a superfluid
Bose-Einstein condensate under self-gravity with a 3D wave function. As
$\hbar/m\to 0$, $m$ being the boson mass, the equations have been postulated to
approximate the collisionless Vlasov-Poisson equations also known as the
collisionless Boltz... | astro-ph.CO | the schrodingerpoisson equations describe the behavior of a superfluid boseeinstein condensate under selfgravity with a 3d wave function as hbarmto 0 m being the boson mass the equations have been postulated to approximate the collisionless vlasovpoisson equations also known as the collisionless boltzmannpoisson equati... | [['the', 'schrodingerpoisson', 'equations', 'describe', 'the', 'behavior', 'of', 'a', 'superfluid', 'boseeinstein', 'condensate', 'under', 'selfgravity', 'with', 'a', '3d', 'wave', 'function', 'as', 'hbarmto', '0', 'm', 'being', 'the', 'boson', 'mass', 'the', 'equations', 'have', 'been', 'postulated', 'to', 'approximat... | [-0.12598657180997222, 0.13545076000238104, -0.10825614108004465, 0.10555663993979122, -0.07733685279067623, -0.11754149753677612, -0.04353963266972298, 0.23707544980012737, -0.26879196038495423, -0.29837296832103954, 0.039913016413274105, -0.26381449396013873, -0.11662512324017597, 0.14977015113814257, 0.0297886668307... |
1,801.03508 | Locally Maximally Entangled States of Multipart Quantum Systems | For a multipart quantum system, a locally maximally entangled (LME) state is
one where each elementary subsystem is maximally entangled with its complement.
This paper is a sequel to arXiv:1708.01645, which gives necessary and
sufficient conditions for a system to admit LME states in terms of its
subsystem dimensions... | quant-ph hep-th | for a multipart quantum system a locally maximally entangled lme state is one where each elementary subsystem is maximally entangled with its complement this paper is a sequel to arxiv170801645 which gives necessary and sufficient conditions for a system to admit lme states in terms of its subsystem dimensions d_1 d_2 ... | [['for', 'a', 'multipart', 'quantum', 'system', 'a', 'locally', 'maximally', 'entangled', 'lme', 'state', 'is', 'one', 'where', 'each', 'elementary', 'subsystem', 'is', 'maximally', 'entangled', 'with', 'its', 'complement', 'this', 'paper', 'is', 'a', 'sequel', 'to', 'arxiv170801645', 'which', 'gives', 'necessary', 'an... | [-0.13663244781934697, 0.14150798114997745, -0.03428784558540525, 0.04736983432189296, 0.01083149555688139, -0.21133901022716564, 0.026510276260857744, 0.3018553425796366, -0.21556815964390258, -0.2102293661741567, 0.09204041267686708, -0.23880650587087487, -0.1139509420111384, 0.18348743641807513, -0.09391371114516928... |
1,801.03509 | micrOMEGAs5.0 : freeze-in | We present a major upgrade of the micrOMEGAs dark matter code to compute the
abundance of feebly interacting dark matter candidates through the freeze-in
mechanism in generic extensions of the Standard Model of particle physics. We
develop the necessary formalism in order to solve the freeze-in Boltzmann
equations wh... | hep-ph | we present a major upgrade of the micromegas dark matter code to compute the abundance of feebly interacting dark matter candidates through the freezein mechanism in generic extensions of the standard model of particle physics we develop the necessary formalism in order to solve the freezein boltzmann equations while m... | [['we', 'present', 'a', 'major', 'upgrade', 'of', 'the', 'micromegas', 'dark', 'matter', 'code', 'to', 'compute', 'the', 'abundance', 'of', 'feebly', 'interacting', 'dark', 'matter', 'candidates', 'through', 'the', 'freezein', 'mechanism', 'in', 'generic', 'extensions', 'of', 'the', 'standard', 'model', 'of', 'particle... | [-0.07284448910106704, 0.13632014770756323, -0.1131618264237348, 0.12789237141339382, -0.08286224517387727, -0.1327909978277557, 0.017122732784858423, 0.3065949419595867, -0.25754394234287775, -0.3936533104925626, 0.030590111902573065, -0.2209851393958552, -0.06687037247863799, 0.19225750033687683, 0.019017270518631876... |
1,801.0351 | Protoplanetary Disc Response to Distant Tidal Encounters in Stellar
Clusters | The majority of stars form in a clustered environment. This has an impact on
the evolution of surrounding protoplanetary discs (PPDs) due to either
photoevaporation or tidal truncation. Consequently, the development of planets
depends on formation environment. Here we present the first thorough
investigation of tidal... | astro-ph.EP astro-ph.GA astro-ph.SR | the majority of stars form in a clustered environment this has an impact on the evolution of surrounding protoplanetary discs ppds due to either photoevaporation or tidal truncation consequently the development of planets depends on formation environment here we present the first thorough investigation of tidally induc... | [['the', 'majority', 'of', 'stars', 'form', 'in', 'a', 'clustered', 'environment', 'this', 'has', 'an', 'impact', 'on', 'the', 'evolution', 'of', 'surrounding', 'protoplanetary', 'discs', 'ppds', 'due', 'to', 'either', 'photoevaporation', 'or', 'tidal', 'truncation', 'consequently', 'the', 'development', 'of', 'planets... | [-0.1406765530695904, 0.09851604681024269, -0.07818689062421508, 0.07138137522049859, -0.06484903775922515, -0.026719354046117357, 0.035271827908508684, 0.352201977075555, -0.2024466679881507, -0.3260463625681782, 0.036295715198038196, -0.2812849158878994, -0.09328170926721, 0.17230412077712395, -0.06359164210275098, 0... |
1,801.03511 | Parity-controlled $2\pi$ Josephson effect mediated by Majorana Kramers
pairs | We study a time-reversal-invariant topological superconductor island hosting
spatially separated Majorana Kramers pairs, with weak tunnel couplings to two
s-wave superconducting leads. When the topological superconductor island is in
the Coulomb blockade regime, we predict that a Josephson current flows between
the t... | cond-mat.mes-hall | we study a timereversalinvariant topological superconductor island hosting spatially separated majorana kramers pairs with weak tunnel couplings to two swave superconducting leads when the topological superconductor island is in the coulomb blockade regime we predict that a josephson current flows between the two leads... | [['we', 'study', 'a', 'timereversalinvariant', 'topological', 'superconductor', 'island', 'hosting', 'spatially', 'separated', 'majorana', 'kramers', 'pairs', 'with', 'weak', 'tunnel', 'couplings', 'to', 'two', 'swave', 'superconducting', 'leads', 'when', 'the', 'topological', 'superconductor', 'island', 'is', 'in', 't... | [-0.2905336914759852, 0.2748583262520177, -0.01145802324457208, 0.0977622115422083, -0.030429835217453693, -0.2621994393792155, 0.11037866123571839, 0.28367417978540976, -0.18520355028841567, -0.3058002253908816, -0.0882056950263641, -0.3184702183756673, -0.07051094295457006, 0.19720070866620815, 0.040432679267334085, ... |
1,801.03512 | Critical O(N) model to order $\epsilon^4$ from analytic bootstrap | We compute, using the method of large spin perturbation theory, the anomalous
dimensions and OPE coefficients of all leading twist operators in the critical
$ O(N) $ model, to fourth order in the $ \epsilon $-expansion. This is done
fully within a bootstrap framework, and generalizes a recent result for the
CFT-data ... | hep-th | we compute using the method of large spin perturbation theory the anomalous dimensions and ope coefficients of all leading twist operators in the critical on model to fourth order in the epsilon expansion this is done fully within a bootstrap framework and generalizes a recent result for the cftdata of the wilsonfisher... | [['we', 'compute', 'using', 'the', 'method', 'of', 'large', 'spin', 'perturbation', 'theory', 'the', 'anomalous', 'dimensions', 'and', 'ope', 'coefficients', 'of', 'all', 'leading', 'twist', 'operators', 'in', 'the', 'critical', 'on', 'model', 'to', 'fourth', 'order', 'in', 'the', 'epsilon', 'expansion', 'this', 'is', ... | [-0.07584128055154093, 0.10798586939387517, -0.021089198928178343, 0.03857904625131397, -0.0031810613420008627, -0.1285589663990286, -0.010999553600196658, 0.3122181078690468, -0.19114712409101525, -0.2715601846082321, 0.11263954717147824, -0.3307278288392634, -0.13137917724801906, 0.19800727657930592, 0.02646537352438... |
1,801.03513 | Proceedings of the Workshop on High Performance Energy Efficient
Embedded Systems (HIP3ES) 2018 | Proceedings of the Workshop on High Performance Energy Efficient Embedded
Systems (HIP3ES) 2018. Manchester, United Kingdom, January 22nd. Collocated
with HIPEAC 2018 Conference.
| cs.DC | proceedings of the workshop on high performance energy efficient embedded systems hip3es 2018 manchester united kingdom january 22nd collocated with hipeac 2018 conference | [['proceedings', 'of', 'the', 'workshop', 'on', 'high', 'performance', 'energy', 'efficient', 'embedded', 'systems', 'hip3es', '2018', 'manchester', 'united', 'kingdom', 'january', '22nd', 'collocated', 'with', 'hipeac', '2018', 'conference']] | [-0.11667182037363881, 0.08856725822324338, -0.059888032973622496, -0.0599835276927637, -0.08269825310486814, -0.06508728732233462, -0.0215225445875979, 0.20434061652454344, 0.027786116540917883, -0.5550592787887739, 0.22941569643823997, -0.41648957068505493, -0.16918310166701025, 0.18592990949021085, -0.24267647504482... |
1,801.03514 | ALMA observations of AGN fuelling: the case of PKS B1718-649 | We present ALMA observations of the $^{12}$CO (2--1) line of the newly born
($t_\mathrm{radio}\sim10^2$ years) active galactic nucleus (AGN), PKS
B1718-649. These observations reveal that the carbon monoxide in the innermost
15 kpc of the galaxy is distributed in a complex warped disk. In the outer
parts of this disk... | astro-ph.GA | we present alma observations of the 12co 21 line of the newly born t_mathrmradiosim102 years active galactic nucleus agn pks b1718649 these observations reveal that the carbon monoxide in the innermost 15 kpc of the galaxy is distributed in a complex warped disk in the outer parts of this disk the co gas follows the ro... | [['we', 'present', 'alma', 'observations', 'of', 'the', '12co', '21', 'line', 'of', 'the', 'newly', 'born', 't_mathrmradiosim102', 'years', 'active', 'galactic', 'nucleus', 'agn', 'pks', 'b1718649', 'these', 'observations', 'reveal', 'that', 'the', 'carbon', 'monoxide', 'in', 'the', 'innermost', '15', 'kpc', 'of', 'the... | [-0.08909924209115358, 0.06173113207244213, -0.027437174018553417, 0.04523767750044657, -0.06269621290468975, -0.06734289346647489, 0.01007756962157462, 0.44657733876906014, -0.17121565982537426, -0.2771775414430759, 0.07872071896993514, -0.29810942497266374, 0.03538345693124701, 0.16512303724328217, -0.000907656182663... |
1,801.03515 | Formation of Globular Cluster Systems: From Dwarf Galaxies to Giants | Globular cluster (GC) systems around galaxies of a vast mass range show
remarkably simple scaling relations. The combined mass of all GCs is a constant
fraction of the total galaxy mass and the mean metallicity and metallicity
dispersion of the GC system scale up weakly with galaxy mass. The metallicity
of massive, m... | astro-ph.GA | globular cluster gc systems around galaxies of a vast mass range show remarkably simple scaling relations the combined mass of all gcs is a constant fraction of the total galaxy mass and the mean metallicity and metallicity dispersion of the gc system scale up weakly with galaxy mass the metallicity of massive metalpoo... | [['globular', 'cluster', 'gc', 'systems', 'around', 'galaxies', 'of', 'a', 'vast', 'mass', 'range', 'show', 'remarkably', 'simple', 'scaling', 'relations', 'the', 'combined', 'mass', 'of', 'all', 'gcs', 'is', 'a', 'constant', 'fraction', 'of', 'the', 'total', 'galaxy', 'mass', 'and', 'the', 'mean', 'metallicity', 'and'... | [-0.06525561641643031, 0.12870375383356744, -0.08159365973825383, 0.13154327365048388, -0.08614500447248037, -0.04893252910930727, 0.06751426703368242, 0.4357273457949965, -0.1245342810343728, -0.3872194153646755, -0.04626888488110903, -0.28771553789942056, -0.03550196622605794, 0.20606159554465084, -0.0472325391293320... |
1,801.03516 | Parseval's Identity and Optimal Transport Maps | Recent findings for optimal transport maps between distribution functions
sharing the same copula show that componentwise the solution is the optimal map
between marginal distributions. This is an important discovery since in the
multivariate setting optimal maps are difficult to find and only known in a few
special ... | math.PR | recent findings for optimal transport maps between distribution functions sharing the same copula show that componentwise the solution is the optimal map between marginal distributions this is an important discovery since in the multivariate setting optimal maps are difficult to find and only known in a few special cas... | [['recent', 'findings', 'for', 'optimal', 'transport', 'maps', 'between', 'distribution', 'functions', 'sharing', 'the', 'same', 'copula', 'show', 'that', 'componentwise', 'the', 'solution', 'is', 'the', 'optimal', 'map', 'between', 'marginal', 'distributions', 'this', 'is', 'an', 'important', 'discovery', 'since', 'in... | [-0.08835834741314992, 0.02870645898811029, -0.0930377564769476, 0.12429578988094557, -0.03813892308662229, -0.13252607569782102, 0.088201610907724, 0.414995660648701, -0.31328959238438053, -0.25383282312132577, 0.10270485025954414, -0.2550172736457093, -0.19763336515925983, 0.1718603301733891, -0.1077538177945671, 0.0... |
1,801.03517 | Comments on Entanglement Entropy in String Theory | Entanglement entropy for spatial subregions is difficult to define in string
theory because of the extended nature of strings. Here we propose a definition
for Bosonic open strings using the framework of string field theory. The key
difference (compared to ordinary quantum field theory) is that the subregion is
chose... | hep-th | entanglement entropy for spatial subregions is difficult to define in string theory because of the extended nature of strings here we propose a definition for bosonic open strings using the framework of string field theory the key difference compared to ordinary quantum field theory is that the subregion is chosen insi... | [['entanglement', 'entropy', 'for', 'spatial', 'subregions', 'is', 'difficult', 'to', 'define', 'in', 'string', 'theory', 'because', 'of', 'the', 'extended', 'nature', 'of', 'strings', 'here', 'we', 'propose', 'a', 'definition', 'for', 'bosonic', 'open', 'strings', 'using', 'the', 'framework', 'of', 'string', 'field', ... | [-0.13629443294135854, 0.18287988724143361, -0.1424928657070268, 0.13216153871850111, -0.02539357513654977, -0.09972386293869931, 0.03234143927984405, 0.291167500494048, -0.2650856163585559, -0.2166732949204743, 0.04644224737188779, -0.2591744671110064, -0.12593438631611206, 0.10517542187590152, -0.07636962239921559, 0... |
1,801.03518 | First Results from the $Herschel$ and ALMA Spectroscopic Surveys of the
SMC: The Relationship Between [CII]-bright Gas and CO-bright Gas at Low
Metallicity | The Small Magellanic Cloud (SMC) provides the only laboratory to study the
structure of molecular gas at high resolution and low metallicity. We present
results from the Herschel Spectroscopic Survey of the SMC (HS$^{3}$), which
mapped the key far-IR cooling lines [CII], [OI], [NII], and [OIII] in five
star-forming r... | astro-ph.GA | the small magellanic cloud smc provides the only laboratory to study the structure of molecular gas at high resolution and low metallicity we present results from the herschel spectroscopic survey of the smc hs3 which mapped the key farir cooling lines cii oi nii and oiii in five starforming regions and new alma 7marra... | [['the', 'small', 'magellanic', 'cloud', 'smc', 'provides', 'the', 'only', 'laboratory', 'to', 'study', 'the', 'structure', 'of', 'molecular', 'gas', 'at', 'high', 'resolution', 'and', 'low', 'metallicity', 'we', 'present', 'results', 'from', 'the', 'herschel', 'spectroscopic', 'survey', 'of', 'the', 'smc', 'hs3', 'whi... | [0.001382454237507891, 0.026354200560675282, 0.031560323970596785, 0.06149594003156706, -5.137336410097475e-05, -0.04056589713517001, 0.09035919476617545, 0.4961456982418895, -0.18568487194550368, -0.3187750717123395, 0.00017174748122707252, -0.2823795617739784, 0.034765164116331244, 0.11349882756651387, 0.035282367433... |
1,801.03519 | Radio-emitting narrow-line Seyfert 1 galaxies in the JVLA perspective | We report the first results of a survey on 74 narrow-line Seyfert 1 galaxies
(NLS1s) carried out in 2015 with the Karl G. Jansky Very Large Array (JVLA) at
5 GHz in A-configuration. So far, this is the largest survey aimed to image the
radio continuum of NLS1s. We produced radio maps in order to compare the
general p... | astro-ph.GA | we report the first results of a survey on 74 narrowline seyfert 1 galaxies nls1s carried out in 2015 with the karl g jansky very large array jvla at 5 ghz in aconfiguration so far this is the largest survey aimed to image the radio continuum of nls1s we produced radio maps in order to compare the general properties of... | [['we', 'report', 'the', 'first', 'results', 'of', 'a', 'survey', 'on', '74', 'narrowline', 'seyfert', '1', 'galaxies', 'nls1s', 'carried', 'out', 'in', '2015', 'with', 'the', 'karl', 'g', 'jansky', 'very', 'large', 'array', 'jvla', 'at', '5', 'ghz', 'in', 'aconfiguration', 'so', 'far', 'this', 'is', 'the', 'largest', ... | [-0.05463536331859666, 0.0807407000954722, -0.015473646751250809, 0.16297545712310033, -0.14471672012956, -0.09128899995604871, 0.01588559104129672, 0.5169198664666061, -0.06631075702837183, -0.34076006852195295, 0.05911819688552781, -0.32010832451231463, -0.0261096486093765, 0.20933701542311045, -0.010472512449806844,... |
1,801.0352 | Communication-Constrained Expansion Planning for Resilient Distribution
Systems | Distributed generation and remotely controlled switches have emerged as
important technologies to improve the resiliency of distribution grids against
extreme weather-related disturbances. Therefore it becomes impor- tant to study
how best to place them on the grid in order to meet a resiliency criteria,
while minimi... | math.OC | distributed generation and remotely controlled switches have emerged as important technologies to improve the resiliency of distribution grids against extreme weatherrelated disturbances therefore it becomes impor tant to study how best to place them on the grid in order to meet a resiliency criteria while minimizing c... | [['distributed', 'generation', 'and', 'remotely', 'controlled', 'switches', 'have', 'emerged', 'as', 'important', 'technologies', 'to', 'improve', 'the', 'resiliency', 'of', 'distribution', 'grids', 'against', 'extreme', 'weatherrelated', 'disturbances', 'therefore', 'it', 'becomes', 'impor', 'tant', 'to', 'study', 'ho... | [-0.15941223111775718, 0.03127420194263973, -0.04152286325344922, 0.0663745347742194, -0.044507423492988155, -0.1513790202790321, 0.08010872753838878, 0.35145859649511046, -0.2751992317169924, -0.34980200742578876, 0.13354083153460214, -0.24095750110552025, -0.1719544915207348, 0.18295718503602024, -0.11790825850378549... |
1,801.03521 | Interaction between a pulsating jet and a surrounding disk wind. A
hydrodynamical perspective | The molecular richness of fast protostellar jets within 20-100 au of their
source, despite strong ultraviolet irradiation, remains a challenge for the
models investigated so far. We aim to investigate the effect of interaction
between a time-variable jet and a surrounding steady disk wind, to assess the
possibility o... | astro-ph.SR astro-ph.HE | the molecular richness of fast protostellar jets within 20100 au of their source despite strong ultraviolet irradiation remains a challenge for the models investigated so far we aim to investigate the effect of interaction between a timevariable jet and a surrounding steady disk wind to assess the possibility of jet ch... | [['the', 'molecular', 'richness', 'of', 'fast', 'protostellar', 'jets', 'within', '20100', 'au', 'of', 'their', 'source', 'despite', 'strong', 'ultraviolet', 'irradiation', 'remains', 'a', 'challenge', 'for', 'the', 'models', 'investigated', 'so', 'far', 'we', 'aim', 'to', 'investigate', 'the', 'effect', 'of', 'interac... | [-0.10964016273419475, 0.09833561894731702, -0.07072667610668759, 0.07601324483812277, -0.08690724402913474, -0.05758462947414955, 0.0246231255996463, 0.44681647334073205, -0.2785833373291098, -0.29920861582286307, 0.05712939799423111, -0.23858866938371648, -0.024973034566073693, 0.18809417729369216, 0.0322401019511744... |
1,801.03522 | Zeeman-Induced Gapless Superconductivity with Partial Fermi Surface | We show that an in-plane magnetic field can drive two-dimensional
spin-orbit-coupled systems under superconducting proximity effect into a
gapless phase where parts of the normal state Fermi surface are gapped, and the
ungapped parts are reconstructed into a small Fermi surface of Bogoliubov
quasiparticles at zero en... | cond-mat.supr-con | we show that an inplane magnetic field can drive twodimensional spinorbitcoupled systems under superconducting proximity effect into a gapless phase where parts of the normal state fermi surface are gapped and the ungapped parts are reconstructed into a small fermi surface of bogoliubov quasiparticles at zero energy ch... | [['we', 'show', 'that', 'an', 'inplane', 'magnetic', 'field', 'can', 'drive', 'twodimensional', 'spinorbitcoupled', 'systems', 'under', 'superconducting', 'proximity', 'effect', 'into', 'a', 'gapless', 'phase', 'where', 'parts', 'of', 'the', 'normal', 'state', 'fermi', 'surface', 'are', 'gapped', 'and', 'the', 'ungappe... | [-0.2506477653847209, 0.2930672595628753, -0.0699385550405298, 0.03531359149409192, -0.0400810261589608, -0.14434324176316815, 0.03195465348128761, 0.36838162916579414, -0.2505680086091161, -0.2606768013909459, -0.011639987797077212, -0.34037478447758723, -0.09903374143343951, 0.19442204960754939, 0.042834194942510555,... |
1,801.03523 | Generative Models for Stochastic Processes Using Convolutional Neural
Networks | The present paper aims to demonstrate the usage of Convolutional Neural
Networks as a generative model for stochastic processes, enabling researchers
from a wide range of fields (such as quantitative finance and physics) to
develop a general tool for forecasts and simulations without the need to
identify/assume a spe... | stat.ML cs.NE physics.comp-ph q-fin.CP | the present paper aims to demonstrate the usage of convolutional neural networks as a generative model for stochastic processes enabling researchers from a wide range of fields such as quantitative finance and physics to develop a general tool for forecasts and simulations without the need to identifyassume a specific ... | [['the', 'present', 'paper', 'aims', 'to', 'demonstrate', 'the', 'usage', 'of', 'convolutional', 'neural', 'networks', 'as', 'a', 'generative', 'model', 'for', 'stochastic', 'processes', 'enabling', 'researchers', 'from', 'a', 'wide', 'range', 'of', 'fields', 'such', 'as', 'quantitative', 'finance', 'and', 'physics', '... | [-0.010632289211369224, 0.015107511542737484, -0.06593375635781774, 0.10263374968673344, -0.12038310179141937, -0.13741420205096128, 0.058387829264608664, 0.37571282836574094, -0.29982206835928893, -0.3745454829186201, 0.10434662433410133, -0.21550383326528524, -0.2123848621019904, 0.23960314303878005, -0.0498710253741... |
1,801.03524 | Application of fermionic marginal constraints to hybrid quantum
algorithms | Many quantum algorithms, including recently proposed hybrid classical/quantum
algorithms, make use of restricted tomography of the quantum state that
measures the reduced density matrices, or marginals, of the full state. The
most straightforward approach to this algorithmic step estimates each component
of the margi... | quant-ph physics.chem-ph | many quantum algorithms including recently proposed hybrid classicalquantum algorithms make use of restricted tomography of the quantum state that measures the reduced density matrices or marginals of the full state the most straightforward approach to this algorithmic step estimates each component of the marginal inde... | [['many', 'quantum', 'algorithms', 'including', 'recently', 'proposed', 'hybrid', 'classicalquantum', 'algorithms', 'make', 'use', 'of', 'restricted', 'tomography', 'of', 'the', 'quantum', 'state', 'that', 'measures', 'the', 'reduced', 'density', 'matrices', 'or', 'marginals', 'of', 'the', 'full', 'state', 'the', 'most... | [-0.09496693781812257, 0.09315166027746662, -0.06966578074355553, 0.0525824791309008, -0.02810698667005398, -0.13565658853503362, 0.06918691537385731, 0.36684837220806854, -0.25297843002208165, -0.3079847297179798, 0.09461678172478319, -0.22413763325965527, -0.13009592405358825, 0.23239882817677204, -0.0602226255695295... |
1,801.03525 | Accelerated Cardiac Diffusion Tensor Imaging Using Joint Low-Rank and
Sparsity Constraints | Objective: The purpose of this manuscript is to accelerate cardiac diffusion
tensor imaging (CDTI) by integrating low-rankness and compressed sensing.
Methods: Diffusion-weighted images exhibit both transform sparsity and
low-rankness. These properties can jointly be exploited to accelerate CDTI,
especially when a ph... | eess.SP | objective the purpose of this manuscript is to accelerate cardiac diffusion tensor imaging cdti by integrating lowrankness and compressed sensing methods diffusionweighted images exhibit both transform sparsity and lowrankness these properties can jointly be exploited to accelerate cdti especially when a phase map is a... | [['objective', 'the', 'purpose', 'of', 'this', 'manuscript', 'is', 'to', 'accelerate', 'cardiac', 'diffusion', 'tensor', 'imaging', 'cdti', 'by', 'integrating', 'lowrankness', 'and', 'compressed', 'sensing', 'methods', 'diffusionweighted', 'images', 'exhibit', 'both', 'transform', 'sparsity', 'and', 'lowrankness', 'the... | [-0.013829152935662718, 0.033940493199293334, -0.06441255744736922, 0.061541833448529204, -0.09793449579662974, -0.16840019887964172, -0.0045330962015976825, 0.4578852243621343, -0.29216586911590187, -0.3065229382651347, 0.10400785777970688, -0.22675443819213298, -0.13957307167521488, 0.16859647345989542, -0.0825849444... |
1,801.03526 | Neural Program Synthesis with Priority Queue Training | We consider the task of program synthesis in the presence of a reward
function over the output of programs, where the goal is to find programs with
maximal rewards. We employ an iterative optimization scheme, where we train an
RNN on a dataset of K best programs from a priority queue of the generated
programs so far.... | cs.AI | we consider the task of program synthesis in the presence of a reward function over the output of programs where the goal is to find programs with maximal rewards we employ an iterative optimization scheme where we train an rnn on a dataset of k best programs from a priority queue of the generated programs so far then ... | [['we', 'consider', 'the', 'task', 'of', 'program', 'synthesis', 'in', 'the', 'presence', 'of', 'a', 'reward', 'function', 'over', 'the', 'output', 'of', 'programs', 'where', 'the', 'goal', 'is', 'to', 'find', 'programs', 'with', 'maximal', 'rewards', 'we', 'employ', 'an', 'iterative', 'optimization', 'scheme', 'where'... | [-0.08983655950686992, -0.0029787023170805994, -0.10167028614034904, 0.09434209847840161, -0.176675481687008, -0.20412865211255848, 0.12431791977984692, 0.4683311524064238, -0.3129642525854618, -0.32107569029165517, 0.06556825334494655, -0.2394404281486771, -0.14856112703382135, 0.18803942527225825, -0.1249033139337465... |
1,801.03527 | Multiplication of Distributions and Nonperturbative Calculations of
Transition Probabilities | In a mathematical context in which one can multiply distributions the
"`formal"' nonperturbative canonical Hamiltonian formalism in Quantum Field
Theory makes sense mathematically, which can be understood a priori from the
fact the so called "`infinite quantities"' make sense unambiguously (but are
not classical real... | math-ph math.FA math.MP | in a mathematical context in which one can multiply distributions the formal nonperturbative canonical hamiltonian formalism in quantum field theory makes sense mathematically which can be understood a priori from the fact the so called infinite quantities make sense unambiguously but are not classical real numbers the... | [['in', 'a', 'mathematical', 'context', 'in', 'which', 'one', 'can', 'multiply', 'distributions', 'the', 'formal', 'nonperturbative', 'canonical', 'hamiltonian', 'formalism', 'in', 'quantum', 'field', 'theory', 'makes', 'sense', 'mathematically', 'which', 'can', 'be', 'understood', 'a', 'priori', 'from', 'the', 'fact',... | [-0.07398479803901245, 0.14775215950061762, -0.11578268941214427, 0.14004668820622965, -0.10662800424520903, -0.16305313007047412, 0.02241283386090361, 0.3586455737802048, -0.2582885729056512, -0.28521787750382793, 0.06122236957373956, -0.24057917263530565, -0.1780596569870724, 0.17233929768533293, -0.07976983967138097... |
1,801.03528 | Applications of Blockchain Technology beyond Cryptocurrency | Blockchain (BC), the technology behind the Bitcoin crypto-currency system, is
considered to be both alluring and critical for ensuring enhanced security and
(in some implementations, non-traceable) privacy for diverse applications in
many other domains including in the Internet of Things (IoT) eco-system.
Intensive r... | cs.CR | blockchain bc the technology behind the bitcoin cryptocurrency system is considered to be both alluring and critical for ensuring enhanced security and in some implementations nontraceable privacy for diverse applications in many other domains including in the internet of things iot ecosystem intensive research is curr... | [['blockchain', 'bc', 'the', 'technology', 'behind', 'the', 'bitcoin', 'cryptocurrency', 'system', 'is', 'considered', 'to', 'be', 'both', 'alluring', 'and', 'critical', 'for', 'ensuring', 'enhanced', 'security', 'and', 'in', 'some', 'implementations', 'nontraceable', 'privacy', 'for', 'diverse', 'applications', 'in', ... | [-0.21392597611217448, -0.03588635658582489, -0.025226085017802137, 0.04088291179769757, -0.09722724379124967, -0.24646715980418252, 0.06610956150248196, 0.35799342209868357, -0.2793588964099234, -0.2987407515559233, 0.1694493210641667, -0.289027131552046, -0.11909027071387479, 0.20824399816549638, -0.16310689320336236... |
1,801.03529 | Autism Children's App using PECS | Since autistic children suffers from learning disabilities and communication
barriers, this research aim to design, develop and evaluate an Android based
mobile application (app) providing better learning environment with inclusion
of graphical representation in a cost effective manner. This research evaluate
various... | cs.CY | since autistic children suffers from learning disabilities and communication barriers this research aim to design develop and evaluate an android based mobile application app providing better learning environment with inclusion of graphical representation in a cost effective manner this research evaluate various suppor... | [['since', 'autistic', 'children', 'suffers', 'from', 'learning', 'disabilities', 'and', 'communication', 'barriers', 'this', 'research', 'aim', 'to', 'design', 'develop', 'and', 'evaluate', 'an', 'android', 'based', 'mobile', 'application', 'app', 'providing', 'better', 'learning', 'environment', 'with', 'inclusion', ... | [-0.07623198992067962, 0.070398650813838, -0.08351195197666192, 0.06756313203190603, -0.15460095287279318, -0.24961726351477603, 0.09874706176991169, 0.40783644860738333, -0.176807627316479, -0.3842930089227343, 0.07384867526285123, -0.3230725662171386, -0.20811938436680566, 0.1716670402839339, -0.15090606653465682, -0... |
1,801.0353 | Multi-Scale Attention with Dense Encoder for Handwritten Mathematical
Expression Recognition | Handwritten mathematical expression recognition is a challenging problem due
to the complicated two-dimensional structures, ambiguous handwriting input and
variant scales of handwritten math symbols. To settle this problem, we utilize
the attention based encoder-decoder model that recognizes mathematical
expression i... | cs.CV | handwritten mathematical expression recognition is a challenging problem due to the complicated twodimensional structures ambiguous handwriting input and variant scales of handwritten math symbols to settle this problem we utilize the attention based encoderdecoder model that recognizes mathematical expression images f... | [['handwritten', 'mathematical', 'expression', 'recognition', 'is', 'a', 'challenging', 'problem', 'due', 'to', 'the', 'complicated', 'twodimensional', 'structures', 'ambiguous', 'handwriting', 'input', 'and', 'variant', 'scales', 'of', 'handwritten', 'math', 'symbols', 'to', 'settle', 'this', 'problem', 'we', 'utilize... | [-0.038890271480162664, 0.00023859552153747632, -0.04466524732037011, 0.06297647622023168, -0.13375126488076952, -0.19027892753304393, 0.021378440928761032, 0.4158089418172628, -0.24405590204482938, -0.33840988183042386, 0.0815198945550743, -0.25422174474094195, -0.20346591787712348, 0.20536389025384105, -0.17193879876... |
1,801.03531 | The Binary Neutron Star event LIGO/VIRGO GW170817 a hundred and sixty
days after merger: synchrotron emission across the electromagnetic spectrum | We report deep Chandra, HST and VLA observations of the binary neutron star
event GW170817 at $t<160$ d after merger. These observations show that GW170817
has been steadily brightening with time and might have now reached its peak,
and constrain the emission process as non-thermal synchrotron emission where
the cool... | astro-ph.HE | we report deep chandra hst and vla observations of the binary neutron star event gw170817 at t160 d after merger these observations show that gw170817 has been steadily brightening with time and might have now reached its peak and constrain the emission process as nonthermal synchrotron emission where the cooling frequ... | [['we', 'report', 'deep', 'chandra', 'hst', 'and', 'vla', 'observations', 'of', 'the', 'binary', 'neutron', 'star', 'event', 'gw170817', 'at', 't160', 'd', 'after', 'merger', 'these', 'observations', 'show', 'that', 'gw170817', 'has', 'been', 'steadily', 'brightening', 'with', 'time', 'and', 'might', 'have', 'now', 're... | [-0.06773159236859026, 0.18283636444873275, -0.07238090251186924, 0.0878401187733065, -0.13307771892916626, -0.10197740770708465, 0.024268846801428705, 0.45581020058331184, -0.21523207745211367, -0.30024064962034586, 0.045243468685228314, -0.2937933871079786, 0.04379789364241735, 0.21682851111952794, 0.0519272154311603... |
1,801.03532 | Charge ordering and non-local correlations in the doped extended Hubbard
model | We study the extended Hubbard model away from half-filling on a
two-dimensional square lattice using cluster dynamical mean field theory on
clusters of size $8$. We show that the model exhibits metallic, compressible
charge ordered, and insulating charge ordered phases. We determine the location
of the charge orderin... | cond-mat.str-el | we study the extended hubbard model away from halffilling on a twodimensional square lattice using cluster dynamical mean field theory on clusters of size 8 we show that the model exhibits metallic compressible charge ordered and insulating charge ordered phases we determine the location of the charge ordering phase tr... | [['we', 'study', 'the', 'extended', 'hubbard', 'model', 'away', 'from', 'halffilling', 'on', 'a', 'twodimensional', 'square', 'lattice', 'using', 'cluster', 'dynamical', 'mean', 'field', 'theory', 'on', 'clusters', 'of', 'size', '8', 'we', 'show', 'that', 'the', 'model', 'exhibits', 'metallic', 'compressible', 'charge'... | [-0.15154950855536137, 0.2007053092821656, -0.05406555241154535, 0.04694276932738165, 0.019135363959471016, -0.08343349546350455, 0.1222870111484567, 0.37384563986795827, -0.27998953551373706, -0.2634519511249973, 0.03168234623770522, -0.34901542476475683, -0.11905270727323507, 0.048159135731437534, 0.1049353108783044,... |
1,801.03533 | Selection Problems in the Presence of Implicit Bias | Over the past two decades, the notion of implicit bias has come to serve as
an important component in our understanding of discrimination in activities
such as hiring, promotion, and school admissions. Research on implicit bias
posits that when people evaluate others -- for example, in a hiring context --
their uncon... | cs.CY cs.LG stat.ML | over the past two decades the notion of implicit bias has come to serve as an important component in our understanding of discrimination in activities such as hiring promotion and school admissions research on implicit bias posits that when people evaluate others for example in a hiring context their unconscious biases... | [['over', 'the', 'past', 'two', 'decades', 'the', 'notion', 'of', 'implicit', 'bias', 'has', 'come', 'to', 'serve', 'as', 'an', 'important', 'component', 'in', 'our', 'understanding', 'of', 'discrimination', 'in', 'activities', 'such', 'as', 'hiring', 'promotion', 'and', 'school', 'admissions', 'research', 'on', 'impli... | [-0.08019032430889057, 0.05970941477067569, -0.1245584007187247, 0.10594883440796327, -0.12803074581281998, -0.14919039922550428, 0.12794244564914456, 0.402091283341798, -0.2489868910068754, -0.35135571851118375, 0.09584542478272773, -0.26928851685311267, -0.13902065563994204, 0.1746256639978484, -0.11924837527550299, ... |
1,801.03534 | Mechanical Computing Systems Using Only Links and Rotary Joints | A new model for mechanical computing is demonstrated that requires only two
basic parts: links and rotary joints. These basic parts are combined into two
main higher level structures: locks and balances, which suffice to create all
necessary combinatorial and sequential logic required for a Turing-complete
computatio... | cs.ET cs.AR | a new model for mechanical computing is demonstrated that requires only two basic parts links and rotary joints these basic parts are combined into two main higher level structures locks and balances which suffice to create all necessary combinatorial and sequential logic required for a turingcomplete computational sys... | [['a', 'new', 'model', 'for', 'mechanical', 'computing', 'is', 'demonstrated', 'that', 'requires', 'only', 'two', 'basic', 'parts', 'links', 'and', 'rotary', 'joints', 'these', 'basic', 'parts', 'are', 'combined', 'into', 'two', 'main', 'higher', 'level', 'structures', 'locks', 'and', 'balances', 'which', 'suffice', 't... | [-0.13093178969398706, 0.09724794452859446, -0.08015550724748108, 0.06104311706836928, -0.13290918440172317, -0.23565303861643327, 0.02701502674343911, 0.4091820601336282, -0.25947326820607136, -0.33176143570906586, 0.09776801692975703, -0.19896508944973426, -0.15773696511645208, 0.2777277114072043, -0.0823418833597591... |
1,801.03535 | Measurement of the $\mathrm{Z}\gamma^{*} \to \tau\tau$ cross section in
pp collisions at $\sqrt{s} = $ 13 TeV and validation of $\tau$ lepton
analysis techniques | A measurement is presented of the $\mathrm{Z}/\gamma^{*} \to \tau\tau$ cross
section in pp collisions at $\sqrt{s} = $ 13 TeV, using data recorded by the
CMS experiment at the LHC, corresponding to an integrated luminosity of 2.3
fb$^{-1}$. The product of the inclusive cross section and branching fraction is
measured... | hep-ex | a measurement is presented of the mathrmzgamma to tautau cross section in pp collisions at sqrts 13 tev using data recorded by the cms experiment at the lhc corresponding to an integrated luminosity of 23 fb1 the product of the inclusive cross section and branching fraction is measured to be sigmamathrmpp to mathrmzgam... | [['a', 'measurement', 'is', 'presented', 'of', 'the', 'mathrmzgamma', 'to', 'tautau', 'cross', 'section', 'in', 'pp', 'collisions', 'at', 'sqrts', '13', 'tev', 'using', 'data', 'recorded', 'by', 'the', 'cms', 'experiment', 'at', 'the', 'lhc', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', '23', 'fb1', '... | [-0.010821270989747403, 0.15506786071723505, -0.06348684668083186, 0.08886267415196555, 0.028621289693608373, -0.10603751891126888, 0.01478163093245604, 0.31095532999350295, -0.1885500316936286, -0.3797896363480427, 0.0010370114528163636, -0.396940245687709, 0.1458824308967944, 0.17079634385743825, 0.053096707484100836... |
1,801.03536 | On B. Moss\'e's unilateral recognizability theorem | We complete statement and proof for B. Moss\'e's unilateral recognizability
theorem. We also provide an algorithm for deciding the unilateral
non-recognizability of a given primitive substitution.
| math.DS cs.FL | we complete statement and proof for b mosses unilateral recognizability theorem we also provide an algorithm for deciding the unilateral nonrecognizability of a given primitive substitution | [['we', 'complete', 'statement', 'and', 'proof', 'for', 'b', 'mosses', 'unilateral', 'recognizability', 'theorem', 'we', 'also', 'provide', 'an', 'algorithm', 'for', 'deciding', 'the', 'unilateral', 'nonrecognizability', 'of', 'a', 'given', 'primitive', 'substitution']] | [-0.14039796035736798, 0.0026574016228551045, -0.10495139434933662, 0.09695991314947605, -0.1507754872739315, -0.21338400600478052, 0.1954743917658925, 0.3363243418931961, -0.3217705890536308, -0.19549691505730152, 0.05995164565742016, -0.27210308983922005, -0.19756776150316, 0.19398701436817645, -0.1578530665114522, 0... |
1,801.03537 | The JCMT Transient Survey: Stochastic and Secular Variability of
Protostars and Disks In the Sub-Millimeter Observed Over Eighteen Months | We analyze results from the first eighteen months of monthly sub-mm
monitoring of eight star-forming regions in the JCMT Transient Survey. In our
search for stochastic variability in 1643 bright peaks, only the previously
identified source, EC53, shows behavior well above the expected measurement
uncertainty. Another... | astro-ph.SR astro-ph.GA | we analyze results from the first eighteen months of monthly submm monitoring of eight starforming regions in the jcmt transient survey in our search for stochastic variability in 1643 bright peaks only the previously identified source ec53 shows behavior well above the expected measurement uncertainty another four sou... | [['we', 'analyze', 'results', 'from', 'the', 'first', 'eighteen', 'months', 'of', 'monthly', 'submm', 'monitoring', 'of', 'eight', 'starforming', 'regions', 'in', 'the', 'jcmt', 'transient', 'survey', 'in', 'our', 'search', 'for', 'stochastic', 'variability', 'in', '1643', 'bright', 'peaks', 'only', 'the', 'previously'... | [-0.07292353305808215, 0.11501863620878049, -0.08222352957818657, 0.10543353911098016, -0.03755289884894842, -0.06846477354201107, 0.032621782455310895, 0.40794584988692745, -0.1892154108581217, -0.3667520670779431, 0.10674892089350653, -0.3225734746999672, -0.04853703865979905, 0.20795657411675716, -0.0584555200003392... |
1,801.03538 | On Monotonous Separately Continuous Functions | Let ${\mathbb T}=({\bf T},\leq)$ and ${\mathbb T}_{1}=({\bf T}_{1},\leq_{1})$
be linearly ordered sets and $\mathscr{X}$ be a topological space. The main
result of the paper is the following:
If function $\boldsymbol{f}(t,x):{\bf T}\times\mathscr{X}\mapsto{\bf T}_{1}$
is continuous in each variable ("$t$"and "$x$")... | math.GM | let mathbb tbf tleq and mathbb t_1bf t_1leq_1 be linearly ordered sets and mathscrx be a topological space the main result of the paper is the following if function boldsymbolftxbf ttimesmathscrxmapstobf t_1 is continuous in each variable tand x separately and function boldsymbolf_xtboldsymbolftx is monotonous on bf t ... | [['let', 'mathbb', 'tbf', 'tleq', 'and', 'mathbb', 't_1bf', 't_1leq_1', 'be', 'linearly', 'ordered', 'sets', 'and', 'mathscrx', 'be', 'a', 'topological', 'space', 'the', 'main', 'result', 'of', 'the', 'paper', 'is', 'the', 'following', 'if', 'function', 'boldsymbolftxbf', 'ttimesmathscrxmapstobf', 't_1', 'is', 'continu... | [-0.18434726983389776, 0.2298848740098512, -0.01141237816773355, -0.02044541352686634, -0.052050977155728186, -0.10900178447912406, 0.01223285468016832, 0.3935624553376566, -0.3406518646718367, -0.12851894277390902, 0.09877889194783916, -0.25395915078242187, -0.09751372173954935, 0.1674667943937137, -0.0841330202073668... |
1,801.03539 | Strong Sure Screening of Ultra-high Dimensional Categorical Data | Feature screening for ultra high dimensional feature spaces plays a critical
role in the analysis of data sets whose predictors exponentially exceed the
number of observations. Such data sets are becoming increasingly prevalent in
areas such as bioinformatics, medical imaging, and social network analysis.
Frequently,... | stat.ME | feature screening for ultra high dimensional feature spaces plays a critical role in the analysis of data sets whose predictors exponentially exceed the number of observations such data sets are becoming increasingly prevalent in areas such as bioinformatics medical imaging and social network analysis frequently these ... | [['feature', 'screening', 'for', 'ultra', 'high', 'dimensional', 'feature', 'spaces', 'plays', 'a', 'critical', 'role', 'in', 'the', 'analysis', 'of', 'data', 'sets', 'whose', 'predictors', 'exponentially', 'exceed', 'the', 'number', 'of', 'observations', 'such', 'data', 'sets', 'are', 'becoming', 'increasingly', 'prev... | [-0.04139326116189274, 0.026579760744637096, -0.0884653078798248, 0.10912181996688962, -0.07598592570934141, -0.1232228429803928, 0.05661322317356217, 0.3922179857875372, -0.2509575367818565, -0.29415611424050186, 0.13972489453031856, -0.300553677579321, -0.2014850643246846, 0.20463132311936555, -0.062451796668451715, ... |
1,801.0354 | Structured illumination fluorescence microscopy using Talbot
self-imaging effect for high-throughput visualization | We report a novel extension to structured illumination (SI) microscopy that
utilizes the Talbot self-imaging effect to generate a SI pattern on a sample
with field-of-view (FOV) and resolution unconstrained by the numerical aperture
(NA) of the microscope objective. This enables high-resolution SI pattern
generation ... | physics.optics | we report a novel extension to structured illumination si microscopy that utilizes the talbot selfimaging effect to generate a si pattern on a sample with fieldofview fov and resolution unconstrained by the numerical aperture na of the microscope objective this enables highresolution si pattern generation up to the fre... | [['we', 'report', 'a', 'novel', 'extension', 'to', 'structured', 'illumination', 'si', 'microscopy', 'that', 'utilizes', 'the', 'talbot', 'selfimaging', 'effect', 'to', 'generate', 'a', 'si', 'pattern', 'on', 'a', 'sample', 'with', 'fieldofview', 'fov', 'and', 'resolution', 'unconstrained', 'by', 'the', 'numerical', 'a... | [-0.04594735369812795, 0.08428622907369229, -0.05984958873193769, 0.0038505646531806566, -0.05509560342136946, -0.1542105192650129, 0.03897610536949582, 0.4654574677621195, -0.2993348320209816, -0.34778524177997366, 0.05171173678513577, -0.2873707513169645, -0.10939919234055986, 0.19998165167970533, -0.0791923011731141... |
1,801.03541 | A New Solution to the Plasma Starved Event Horizon Magnetosphere:
Application to the Forked Jet in M87 | Very Long Baseline Interferometry observations at 86 GHz reveal an almost
hollow jet in M87 with a forked morphology. The detailed analysis presented
here indicates that the spectral luminosity of the central spine of the jet in
M87 is a few percent of that of the surrounding hollow jet $200 -400
\mu\rm{as}$ from the... | astro-ph.HE astro-ph.CO | very long baseline interferometry observations at 86 ghz reveal an almost hollow jet in m87 with a forked morphology the detailed analysis presented here indicates that the spectral luminosity of the central spine of the jet in m87 is a few percent of that of the surrounding hollow jet 200 400 murmas from the central b... | [['very', 'long', 'baseline', 'interferometry', 'observations', 'at', '86', 'ghz', 'reveal', 'an', 'almost', 'hollow', 'jet', 'in', 'm87', 'with', 'a', 'forked', 'morphology', 'the', 'detailed', 'analysis', 'presented', 'here', 'indicates', 'that', 'the', 'spectral', 'luminosity', 'of', 'the', 'central', 'spine', 'of',... | [-0.1095362488181365, 0.11815032019077981, -0.047717338498426735, 0.13078537216232278, -0.10030573439041415, -0.09461492022665612, -0.046093162043402705, 0.40813148230086255, -0.20501353298226965, -0.32832261588795425, 0.06204530541375434, -0.24051024412728567, 0.03213140173308953, 0.23099756904363755, -0.0247390809810... |
1,801.03542 | Oddities of quantum colorings | We study quantum analogs of graph colorings and chromatic number. Initially
defined via an interactive protocol, quantum colorings can also be viewed as a
natural operator relaxation of graph coloring. Since there is no known
algorithm for producing nontrivial quantum colorings, the existing examples
rely on ad hoc c... | quant-ph math.CO | we study quantum analogs of graph colorings and chromatic number initially defined via an interactive protocol quantum colorings can also be viewed as a natural operator relaxation of graph coloring since there is no known algorithm for producing nontrivial quantum colorings the existing examples rely on ad hoc constru... | [['we', 'study', 'quantum', 'analogs', 'of', 'graph', 'colorings', 'and', 'chromatic', 'number', 'initially', 'defined', 'via', 'an', 'interactive', 'protocol', 'quantum', 'colorings', 'can', 'also', 'be', 'viewed', 'as', 'a', 'natural', 'operator', 'relaxation', 'of', 'graph', 'coloring', 'since', 'there', 'is', 'no',... | [-0.16718771848711186, 0.14758066608235823, -0.07182437508832663, 0.046642248262651266, -0.1326012606988661, -0.16496645237552002, 0.029106232468038798, 0.38711937932414003, -0.26754062760912345, -0.3308627782948315, 0.09079064749355893, -0.2635131539264694, -0.22312356307171285, 0.1941001206403598, -0.1206613790476694... |
1,801.03543 | Quantum current algebras associated with rational $R$-matrix | We study quantum current algebra $\textrm{A}(\overline{R})$ associated with
the rational $R$-matrix of $\mathfrak{gl}_N$ and we give explicit formulae for
the elements of its center at the critical level. Due to Etingof--Kazhdan's
construction, the level $c$ vacuum module $\mathcal{V}_c(\overline{R})$ for the
algebra... | math.QA math-ph math.MP math.RT | we study quantum current algebra textrmaoverliner associated with the rational rmatrix of mathfrakgl_n and we give explicit formulae for the elements of its center at the critical level due to etingofkazhdans construction the level c vacuum module mathcalv_coverliner for the algebra textrmaoverliner possesses a quantum... | [['we', 'study', 'quantum', 'current', 'algebra', 'textrmaoverliner', 'associated', 'with', 'the', 'rational', 'rmatrix', 'of', 'mathfrakgl_n', 'and', 'we', 'give', 'explicit', 'formulae', 'for', 'the', 'elements', 'of', 'its', 'center', 'at', 'the', 'critical', 'level', 'due', 'to', 'etingofkazhdans', 'construction', ... | [-0.1554610732590384, 0.08296197030443318, -0.030182745307683945, 0.025849773339633765, -0.09965563539976943, -0.1961024161747159, 0.03216345891777477, 0.3341753535285235, -0.3402271728375799, -0.20296077029651974, 0.10049408513491284, -0.23218093101215892, -0.14084470180207737, 0.17492186645530675, -0.0538962404817751... |
1,801.03544 | PHENIX results on three-particle Bose-Einstein correlations in
$\sqrt{S_{NN}} = 200$ GeV Au+Au collisions | Bose-Einstein correlations of identical hadrons reveal information about
hadron creation from the strongly interacting matter formed in
ultrarelativistic heavy ion collisions. The measurement of three-particle
correlations may in particular shed light on hadron creation mechanisms beyond
thermal/chaotic emission. In ... | nucl-ex hep-ex nucl-th | boseeinstein correlations of identical hadrons reveal information about hadron creation from the strongly interacting matter formed in ultrarelativistic heavy ion collisions the measurement of threeparticle correlations may in particular shed light on hadron creation mechanisms beyond thermalchaotic emission in this pa... | [['boseeinstein', 'correlations', 'of', 'identical', 'hadrons', 'reveal', 'information', 'about', 'hadron', 'creation', 'from', 'the', 'strongly', 'interacting', 'matter', 'formed', 'in', 'ultrarelativistic', 'heavy', 'ion', 'collisions', 'the', 'measurement', 'of', 'threeparticle', 'correlations', 'may', 'in', 'partic... | [-0.12178418579576321, 0.223741893086207, -0.16138348306796346, 0.14903348429370383, 0.00910860799657282, -0.09969105147720539, -0.009180692641913724, 0.3441934342416682, -0.21617629366038843, -0.2518903842852848, -0.04595372943178743, -0.37005966722012257, -0.02604648028680867, 0.11612171895887527, 0.09633924413198071... |
1,801.03545 | Labyrinthine domains in ferroelectric nanoparticles: a manifestation of
gradient-driven morphological transition | In the framework of the Landau-Ginzburg-Devonshire (LGD) approach we studied
finite size effects of the phase diagram and domain structure evolution in
spherical nanoparticles of uniaxial ferroelectric. The particle surface is
covered by a layer of screening charge characterized by finite screening
length. The phase ... | cond-mat.mtrl-sci | in the framework of the landauginzburgdevonshire lgd approach we studied finite size effects of the phase diagram and domain structure evolution in spherical nanoparticles of uniaxial ferroelectric the particle surface is covered by a layer of screening charge characterized by finite screening length the phase diagram ... | [['in', 'the', 'framework', 'of', 'the', 'landauginzburgdevonshire', 'lgd', 'approach', 'we', 'studied', 'finite', 'size', 'effects', 'of', 'the', 'phase', 'diagram', 'and', 'domain', 'structure', 'evolution', 'in', 'spherical', 'nanoparticles', 'of', 'uniaxial', 'ferroelectric', 'the', 'particle', 'surface', 'is', 'co... | [-0.1741190886470177, 0.224506913603558, -0.07094027450754024, 0.006454257107463617, -0.060231554599188136, -0.08254091000464352, 0.061602445225086, 0.42067423114025526, -0.2695143954758398, -0.26239981407547275, 0.036829012776509656, -0.2669844834963021, -0.1394191118700139, 0.11791055744400819, 0.04481358593800832, 0... |
1,801.03546 | Segment-based Methods for Facial Attribute Detection from Partial Faces | State-of-the-art methods of attribute detection from faces almost always
assume the presence of a full, unoccluded face. Hence, their performance
degrades for partially visible and occluded faces. In this paper, we introduce
SPLITFACE, a deep convolutional neural network-based method that is explicitly
designed to pe... | cs.CV | stateoftheart methods of attribute detection from faces almost always assume the presence of a full unoccluded face hence their performance degrades for partially visible and occluded faces in this paper we introduce splitface a deep convolutional neural networkbased method that is explicitly designed to perform attrib... | [['stateoftheart', 'methods', 'of', 'attribute', 'detection', 'from', 'faces', 'almost', 'always', 'assume', 'the', 'presence', 'of', 'a', 'full', 'unoccluded', 'face', 'hence', 'their', 'performance', 'degrades', 'for', 'partially', 'visible', 'and', 'occluded', 'faces', 'in', 'this', 'paper', 'we', 'introduce', 'spli... | [-0.056073410058009664, -0.037644972574374456, -0.035024736764171394, 0.010594653516212324, -0.09361724038050549, -0.16345541965226099, 0.022507369718975195, 0.4475397678713004, -0.2498624931637702, -0.3136610921743947, 0.09130062417989393, -0.29883921768616045, -0.18773761103996853, 0.17462410275038565, -0.16771366971... |
1,801.03547 | CALLISTO Spectrometer at IISER-Pune | A CALLISTO spectrometer to monitor solar radio transient emissions from
$\approx 0.8-1.6~R_{\odot}$ (above photosphere) is installed at IISER, Pune,
India (longitude $73^{\circ} 55'$ E and latitude $18^{\circ}31'$ N). In this
paper, we illustrate the instrumental details (log-periodic dipole antenna and
the receiver ... | astro-ph.IM | a callisto spectrometer to monitor solar radio transient emissions from approx 0816r_odot above photosphere is installed at iiser pune india longitude 73circ 55 e and latitude 18circ31 n in this paper we illustrate the instrumental details logperiodic dipole antenna and the receiver system along with the recorded solar... | [['a', 'callisto', 'spectrometer', 'to', 'monitor', 'solar', 'radio', 'transient', 'emissions', 'from', 'approx', '0816r_odot', 'above', 'photosphere', 'is', 'installed', 'at', 'iiser', 'pune', 'india', 'longitude', '73circ', '55', 'e', 'and', 'latitude', '18circ31', 'n', 'in', 'this', 'paper', 'we', 'illustrate', 'the... | [-0.13739230220516524, 0.16089572629580895, 0.014895649719983339, 0.047918663832048576, -0.10018793088694414, -0.1280437550220328, 0.040731965565743544, 0.4367791353724897, -0.18482268812755745, -0.35420246499590574, 0.07960418376450737, -0.28144665957738957, -0.10156746740452945, 0.25963333951930206, -0.03890594641367... |
1,801.03548 | On strong $L^2$ convergence of time numerical schemes for the stochastic
2D Navier-Stokes equations | We prove that some discretization schemes for the 2D Navier-Stokes equations
subject to a random perturbation converge in $L^2(\Omega)$. This refines
previous results which only established the convergence in probability of these
numerical approximations. Using exponential moment estimates of the solution of
the stoc... | math.PR | we prove that some discretization schemes for the 2d navierstokes equations subject to a random perturbation converge in l2omega this refines previous results which only established the convergence in probability of these numerical approximations using exponential moment estimates of the solution of the stochastic ns e... | [['we', 'prove', 'that', 'some', 'discretization', 'schemes', 'for', 'the', '2d', 'navierstokes', 'equations', 'subject', 'to', 'a', 'random', 'perturbation', 'converge', 'in', 'l2omega', 'this', 'refines', 'previous', 'results', 'which', 'only', 'established', 'the', 'convergence', 'in', 'probability', 'of', 'these', ... | [-0.15263405002631425, 0.037285927577786857, -0.12259807343417335, 0.034663685210814164, -0.027828084615369637, -0.11130541839659036, 0.03828274047381932, 0.3155190299619876, -0.3036115344259001, -0.20487397551048725, 0.13265906379369663, -0.2212016977386416, -0.08907713998840856, 0.17898985630433475, -0.05227589514106... |
1,801.03549 | $E_{2}$ Structures and Derived Koszul Duality in String Topology | We construct an equivalence of $E_{2}$ algebras between two models for the
Thom spectrum of the free loop space that are related by derived Koszul
duality. To do this, we describe the functoriality and invariance properties of
topological Hochschild cohomology.
| math.AT | we construct an equivalence of e_2 algebras between two models for the thom spectrum of the free loop space that are related by derived koszul duality to do this we describe the functoriality and invariance properties of topological hochschild cohomology | [['we', 'construct', 'an', 'equivalence', 'of', 'e_2', 'algebras', 'between', 'two', 'models', 'for', 'the', 'thom', 'spectrum', 'of', 'the', 'free', 'loop', 'space', 'that', 'are', 'related', 'by', 'derived', 'koszul', 'duality', 'to', 'do', 'this', 'we', 'describe', 'the', 'functoriality', 'and', 'invariance', 'prope... | [-0.2183927745791152, 0.08513392991480942, -0.11489742008270695, 0.16713682432600763, -0.10018000439740718, -0.14870389276184143, -0.0833385530859232, 0.3877138704061508, -0.4465983768925071, -0.2222844551317394, 0.06147074304171838, -0.18305780549999326, -0.18274816107004882, 0.1476511179265799, -0.17020439505577087, ... |
1,801.0355 | Edge Modes of Scattering Chains with Aperiodic Order | We study the scattering resonances of one-dimensional deterministic aperiodic
chains of electric dipoles using the vectorial Green's matrix method, which
accounts for both short- and long-range electromagnetic interactions in open
scattering systems. We discover the existence of edge-localized scattering
states withi... | physics.optics | we study the scattering resonances of onedimensional deterministic aperiodic chains of electric dipoles using the vectorial greens matrix method which accounts for both short and longrange electromagnetic interactions in open scattering systems we discover the existence of edgelocalized scattering states within fractal... | [['we', 'study', 'the', 'scattering', 'resonances', 'of', 'onedimensional', 'deterministic', 'aperiodic', 'chains', 'of', 'electric', 'dipoles', 'using', 'the', 'vectorial', 'greens', 'matrix', 'method', 'which', 'accounts', 'for', 'both', 'short', 'and', 'longrange', 'electromagnetic', 'interactions', 'in', 'open', 's... | [-0.20893264360160435, 0.20043285670451172, -0.04468377879862341, 0.09843165590427816, -0.03282408243810226, -0.1576512531377375, 0.03532695077758815, 0.3973579237902803, -0.27655197705940476, -0.241576105609004, 0.03906601339913322, -0.3010716190561652, -0.21870083693980372, 0.19057508262506287, 0.05207507269269627, 0... |
1,801.03551 | From Superpixel to Human Shape Modelling for Carried Object Detection | Detecting carried objects is one of the requirements for developing systems
to reason about activities involving people and objects. We present an approach
to detect carried objects from a single video frame with a novel method that
incorporates features from multiple scales. Initially, a foreground mask in a
video f... | cs.CV | detecting carried objects is one of the requirements for developing systems to reason about activities involving people and objects we present an approach to detect carried objects from a single video frame with a novel method that incorporates features from multiple scales initially a foreground mask in a video frame ... | [['detecting', 'carried', 'objects', 'is', 'one', 'of', 'the', 'requirements', 'for', 'developing', 'systems', 'to', 'reason', 'about', 'activities', 'involving', 'people', 'and', 'objects', 'we', 'present', 'an', 'approach', 'to', 'detect', 'carried', 'objects', 'from', 'a', 'single', 'video', 'frame', 'with', 'a', 'n... | [-0.0555027060926895, 0.0018704709074046223, -0.13463159696107754, 0.05504206647920246, -0.08233923534548061, -0.13908729738732045, 0.0473957053036429, 0.448815190283632, -0.23160542959246683, -0.33029951952473335, 0.07479115087315566, -0.29959215851488047, -0.12803351836486696, 0.175059152765489, -0.10199912872977203,... |
1,801.03552 | An evolutionary algorithm for online, resource constrained,
multi-vehicle sensing mission planning | Mobile robotic platforms are an indispensable tool for various scientific and
industrial applications. Robots are used to undertake missions whose execution
is constrained by various factors, such as the allocated time or their
remaining energy. Existing solutions for resource constrained multi-robot
sensing mission ... | cs.RO | mobile robotic platforms are an indispensable tool for various scientific and industrial applications robots are used to undertake missions whose execution is constrained by various factors such as the allocated time or their remaining energy existing solutions for resource constrained multirobot sensing mission planni... | [['mobile', 'robotic', 'platforms', 'are', 'an', 'indispensable', 'tool', 'for', 'various', 'scientific', 'and', 'industrial', 'applications', 'robots', 'are', 'used', 'to', 'undertake', 'missions', 'whose', 'execution', 'is', 'constrained', 'by', 'various', 'factors', 'such', 'as', 'the', 'allocated', 'time', 'or', 't... | [-0.1272998915313344, 0.029946453101833217, -0.05407947873962777, 0.08602925961238465, -0.11602882530274136, -0.2140709744473653, 0.0795959762676752, 0.4116289608978799, -0.25268041226214594, -0.3781501994282007, 0.17072055433012012, -0.23097961129088487, -0.13181948076268393, 0.23560307077531303, -0.11482625165422047,... |
1,801.03553 | On the Noise-Information Separation of a Private Principal Component
Analysis Scheme | In a survey disclosure model, we consider an additive noise privacy mechanism
and study the trade-off between privacy guarantees and statistical utility.
Privacy is approached from two different but complementary viewpoints:
information and estimation theoretic. Motivated by the performance of principal
component ana... | cs.IT math.IT | in a survey disclosure model we consider an additive noise privacy mechanism and study the tradeoff between privacy guarantees and statistical utility privacy is approached from two different but complementary viewpoints information and estimation theoretic motivated by the performance of principal component analysis s... | [['in', 'a', 'survey', 'disclosure', 'model', 'we', 'consider', 'an', 'additive', 'noise', 'privacy', 'mechanism', 'and', 'study', 'the', 'tradeoff', 'between', 'privacy', 'guarantees', 'and', 'statistical', 'utility', 'privacy', 'is', 'approached', 'from', 'two', 'different', 'but', 'complementary', 'viewpoints', 'inf... | [-0.09528085907610755, -0.04971176987475764, -0.12012392953145264, 0.1117788119838391, -0.08703295778397513, -0.16258945476649136, 0.09757806988427652, 0.3700232258730236, -0.3414512588160819, -0.3078962336669023, 0.10731306073694737, -0.29278340015089377, -0.2215498023647708, 0.16317167845768746, -0.15422864416721224,... |
1,801.03554 | Rate equation analysis and non-Hermiticity in coupled semiconductor
laser arrays | Optically-coupled semiconductor laser arrays are described by coupled rate
equations. The coupled mode equations and carrier densities are included in the
analysis, which inherently incorporate the carrier-induced nonlinearities
including spatial hole burning and amplitude-phase coupling. We solve the
steady-state co... | physics.optics | opticallycoupled semiconductor laser arrays are described by coupled rate equations the coupled mode equations and carrier densities are included in the analysis which inherently incorporate the carrierinduced nonlinearities including spatial hole burning and amplitudephase coupling we solve the steadystate coupled rat... | [['opticallycoupled', 'semiconductor', 'laser', 'arrays', 'are', 'described', 'by', 'coupled', 'rate', 'equations', 'the', 'coupled', 'mode', 'equations', 'and', 'carrier', 'densities', 'are', 'included', 'in', 'the', 'analysis', 'which', 'inherently', 'incorporate', 'the', 'carrierinduced', 'nonlinearities', 'includin... | [-0.23864661863960981, 0.1968653823274213, 0.0045728790384994165, 0.006309157382143107, -0.02837220167212591, -0.2427079134708824, 0.04830681031327569, 0.44268606184679715, -0.24536593007301358, -0.2634613813857573, 0.08187962438937943, -0.2544827434058125, -0.10317438839607544, 0.16363085062570265, 0.00072172114517810... |
1,801.03555 | Galactic Reddening in 3D from Stellar Photometry - An Improved Map | We present a new 3D map of interstellar dust reddening, covering three
quarters of the sky (declinations greater than -30 degrees) out to a distance
of several kiloparsecs. The map is based on high-quality stellar photometry of
800 million stars from Pan-STARRS 1 and 2MASS. We divide the sky into
sightlines containin... | astro-ph.GA | we present a new 3d map of interstellar dust reddening covering three quarters of the sky declinations greater than 30 degrees out to a distance of several kiloparsecs the map is based on highquality stellar photometry of 800 million stars from panstarrs 1 and 2mass we divide the sky into sightlines containing a few hu... | [['we', 'present', 'a', 'new', '3d', 'map', 'of', 'interstellar', 'dust', 'reddening', 'covering', 'three', 'quarters', 'of', 'the', 'sky', 'declinations', 'greater', 'than', '30', 'degrees', 'out', 'to', 'a', 'distance', 'of', 'several', 'kiloparsecs', 'the', 'map', 'is', 'based', 'on', 'highquality', 'stellar', 'phot... | [-0.007314003019101537, 0.05547199400337955, -0.06881578726461157, 0.05339590377314545, -0.047796311116227036, -0.04951846265281678, 0.07162227792088577, 0.4262096015101468, -0.22426844952331687, -0.3584893380492841, 0.055798703514896755, -0.3706886923914267, -0.0032806090070649093, 0.22660656431716317, -0.051887822779... |
1,801.03556 | Lifshitz transitions induced by magnetic field | The Fermi surface can be changed by different external conditions like, e.g.,
pressure or doping. It can lead to a change in the Fermi surface topology,
called as the Lifshitz transition. Here, we briefly describe the Lifshitz
transitions induced by the external magnetic field in a one-dimensional optical
lattice and... | cond-mat.supr-con cond-mat.quant-gas | the fermi surface can be changed by different external conditions like eg pressure or doping it can lead to a change in the fermi surface topology called as the lifshitz transition here we briefly describe the lifshitz transitions induced by the external magnetic field in a onedimensional optical lattice and ironbased ... | [['the', 'fermi', 'surface', 'can', 'be', 'changed', 'by', 'different', 'external', 'conditions', 'like', 'eg', 'pressure', 'or', 'doping', 'it', 'can', 'lead', 'to', 'a', 'change', 'in', 'the', 'fermi', 'surface', 'topology', 'called', 'as', 'the', 'lifshitz', 'transition', 'here', 'we', 'briefly', 'describe', 'the', ... | [-0.1736082314651032, 0.2913162478352668, -0.038505362621584875, 0.09067555686428411, -0.0810004583537029, -0.16536031700060017, 0.11289795331626398, 0.39525121731347723, -0.2750479056820518, -0.29416859036952747, 0.047959011296176766, -0.27549291058580894, -0.20832761314880774, 0.16811295482330024, -0.0050876837483317... |
1,801.03557 | Rate Selection and Power Adaptation using Maximal Ratio Combining for
the Random Access Gaussian Channel | With the emergence of machine-driven communi- cation, there is a renewed
interest in the design of random multiple access schemes for networks with
large number of active devices. Many of the recently proposed access paradigms
are enhancements to slotted ALOHA. One of the popular schemes, irregular
repetition slotted... | cs.IT math.IT | with the emergence of machinedriven communi cation there is a renewed interest in the design of random multiple access schemes for networks with large number of active devices many of the recently proposed access paradigms are enhancements to slotted aloha one of the popular schemes irregular repetition slotted aloha i... | [['with', 'the', 'emergence', 'of', 'machinedriven', 'communi', 'cation', 'there', 'is', 'a', 'renewed', 'interest', 'in', 'the', 'design', 'of', 'random', 'multiple', 'access', 'schemes', 'for', 'networks', 'with', 'large', 'number', 'of', 'active', 'devices', 'many', 'of', 'the', 'recently', 'proposed', 'access', 'pa... | [-0.20640916452244373, 0.03748800288295803, -0.046049805850431814, 0.013651802752273859, -0.0660510824909281, -0.22554332149199774, 0.10738662467974294, 0.41438623888245046, -0.25416835993490194, -0.28051050516771653, 0.08598432275708358, -0.23319139604868946, -0.15072853149734233, 0.1951067648850931, -0.11612062612446... |
1,801.03558 | Inference Suboptimality in Variational Autoencoders | Amortized inference allows latent-variable models trained via variational
learning to scale to large datasets. The quality of approximate inference is
determined by two factors: a) the capacity of the variational distribution to
match the true posterior and b) the ability of the recognition network to
produce good va... | cs.LG stat.ML | amortized inference allows latentvariable models trained via variational learning to scale to large datasets the quality of approximate inference is determined by two factors a the capacity of the variational distribution to match the true posterior and b the ability of the recognition network to produce good variation... | [['amortized', 'inference', 'allows', 'latentvariable', 'models', 'trained', 'via', 'variational', 'learning', 'to', 'scale', 'to', 'large', 'datasets', 'the', 'quality', 'of', 'approximate', 'inference', 'is', 'determined', 'by', 'two', 'factors', 'a', 'the', 'capacity', 'of', 'the', 'variational', 'distribution', 'to... | [-0.03287334692422926, 0.018019138314107907, -0.06648190818386458, 0.1318268249343052, -0.1136467844949785, -0.10606894813262538, 0.08572186077875432, 0.3918307084562396, -0.2915093900163227, -0.3589924862191303, 0.05851077172060761, -0.2107580601353478, -0.1437161609507861, 0.15450564360440666, -0.11044864335667286, 0... |
1,801.03559 | Bound states induced by the ferromagnetic dimer in a triangular lattice | The ongoing efforts aiming at control and manipulation of novel topological
phases renewed the interest in bound states induced in superconducting
substrates by magnetic impurities. First described by Yu, Shiba and Rusinov,
those bound states are spin-polarized and exhibit a rather large spatial extent
in two dimensi... | cond-mat.supr-con cond-mat.mtrl-sci | the ongoing efforts aiming at control and manipulation of novel topological phases renewed the interest in bound states induced in superconducting substrates by magnetic impurities first described by yu shiba and rusinov those bound states are spinpolarized and exhibit a rather large spatial extent in two dimensional 2... | [['the', 'ongoing', 'efforts', 'aiming', 'at', 'control', 'and', 'manipulation', 'of', 'novel', 'topological', 'phases', 'renewed', 'the', 'interest', 'in', 'bound', 'states', 'induced', 'in', 'superconducting', 'substrates', 'by', 'magnetic', 'impurities', 'first', 'described', 'by', 'yu', 'shiba', 'and', 'rusinov', '... | [-0.1739412561318902, 0.2839102260910549, -0.021553065586864928, 0.03411434835559407, 0.003923837095499039, -0.16795548628799098, 0.1058383911284943, 0.36753687080602315, -0.21009901161630487, -0.3243560025381834, -0.010330688538636232, -0.30798334942935685, -0.15855982921324496, 0.15291853055363347, 0.0515356859203081... |
1,801.0356 | KKMC-hh: A Precision Event Generator for EW Radiative Corrections in
Hadron Scattering | KKMC-hh is a precision event-generator for Z production and decay in hadronic
collisions, which applies amplitude-level exponentiation to both initial and
final state photon radiation, including perturbative residuals through order
$\alpha^2 L$, together with electroweak matrix element corrections. We present
results... | hep-ph | kkmchh is a precision eventgenerator for z production and decay in hadronic collisions which applies amplitudelevel exponentiation to both initial and final state photon radiation including perturbative residuals through order alpha2 l together with electroweak matrix element corrections we present results showing the ... | [['kkmchh', 'is', 'a', 'precision', 'eventgenerator', 'for', 'z', 'production', 'and', 'decay', 'in', 'hadronic', 'collisions', 'which', 'applies', 'amplitudelevel', 'exponentiation', 'to', 'both', 'initial', 'and', 'final', 'state', 'photon', 'radiation', 'including', 'perturbative', 'residuals', 'through', 'order', '... | [-0.0489307022909066, 0.1978347160478645, -0.10673095292707042, 0.12193218982784168, -0.03377023678295678, -0.10674828510140864, 0.006362108181503306, 0.3470253932130773, -0.1562203781951855, -0.29304380265132685, 0.008000824721132564, -0.3509678413818886, 0.017605151481381278, 0.1596921347308813, 0.04123521777914792, ... |
1,801.03561 | Bivector Gauge Fields and Amplification of Radiation from Distant Cosmic
Sources | This paper describes in some detail the concept of bivector gauge fields and
then examines the possibility of confirming their existence by recording
certain patterns in variation of intensity of radiation from distant cosmic
sources versus radiation frequency and versus the estimated distance to the
source.
| physics.gen-ph hep-th | this paper describes in some detail the concept of bivector gauge fields and then examines the possibility of confirming their existence by recording certain patterns in variation of intensity of radiation from distant cosmic sources versus radiation frequency and versus the estimated distance to the source | [['this', 'paper', 'describes', 'in', 'some', 'detail', 'the', 'concept', 'of', 'bivector', 'gauge', 'fields', 'and', 'then', 'examines', 'the', 'possibility', 'of', 'confirming', 'their', 'existence', 'by', 'recording', 'certain', 'patterns', 'in', 'variation', 'of', 'intensity', 'of', 'radiation', 'from', 'distant', ... | [-0.14557258906247822, 0.16769406311821355, -0.037512741547644786, 0.07838151811207038, -0.05794801309947734, -0.020024556504643482, 0.05515036331337836, 0.38223324574368156, -0.26747871931318357, -0.3422648580947324, 0.03933924620302961, -0.2799844038065361, -0.11442569521782191, 0.18658574909457695, -0.05655931027444... |
1,801.03562 | Discrete symbolic optimization and Boltzmann sampling by continuous
neural dynamics: Gradient Symbolic Computation | Gradient Symbolic Computation is proposed as a means of solving discrete
global optimization problems using a neurally plausible continuous stochastic
dynamical system. Gradient symbolic dynamics involves two free parameters that
must be adjusted as a function of time to obtain the global maximizer at the
end of the ... | cs.CL | gradient symbolic computation is proposed as a means of solving discrete global optimization problems using a neurally plausible continuous stochastic dynamical system gradient symbolic dynamics involves two free parameters that must be adjusted as a function of time to obtain the global maximizer at the end of the com... | [['gradient', 'symbolic', 'computation', 'is', 'proposed', 'as', 'a', 'means', 'of', 'solving', 'discrete', 'global', 'optimization', 'problems', 'using', 'a', 'neurally', 'plausible', 'continuous', 'stochastic', 'dynamical', 'system', 'gradient', 'symbolic', 'dynamics', 'involves', 'two', 'free', 'parameters', 'that',... | [-0.10514738881513346, 0.05978083593126769, -0.12717957937846255, 0.10116241571045194, -0.08707599498975639, -0.14930590324508566, 0.08215237930242981, 0.34459576257025804, -0.2713607984386106, -0.29379530370270257, 0.14201199932232778, -0.21654406080466357, -0.1410687560145961, 0.23804028837932883, -0.0458778993647641... |
1,801.03563 | Group Communication Analysis: A Computational Linguistics Approach for
Detecting Sociocognitive Roles in Multi-Party Interactions | Roles are one of the most important concepts in understanding human
sociocognitive behavior. During group interactions, members take on different
roles within the discussion. Roles have distinct patterns of behavioral
engagement (i.e., active or passive, leading or following), contribution
characteristics (i.e., prov... | cs.CL | roles are one of the most important concepts in understanding human sociocognitive behavior during group interactions members take on different roles within the discussion roles have distinct patterns of behavioral engagement ie active or passive leading or following contribution characteristics ie providing new inform... | [['roles', 'are', 'one', 'of', 'the', 'most', 'important', 'concepts', 'in', 'understanding', 'human', 'sociocognitive', 'behavior', 'during', 'group', 'interactions', 'members', 'take', 'on', 'different', 'roles', 'within', 'the', 'discussion', 'roles', 'have', 'distinct', 'patterns', 'of', 'behavioral', 'engagement',... | [-0.0960639301493788, 0.10881670819974809, -0.11044701972247728, 0.08244108347571455, -0.11845103840761144, -0.15290451248915032, 0.054823901333669524, 0.4059250435896282, -0.22828806419144304, -0.36107552800415854, 0.02826800267161914, -0.30082965797467703, -0.1984406165529749, 0.13670411481971628, -0.0541324658825425... |
1,801.03564 | Unsupervised Part-of-Speech Induction | Part-of-Speech (POS) tagging is an old and fundamental task in natural
language processing. While supervised POS taggers have shown promising
accuracy, it is not always feasible to use supervised methods due to lack of
labeled data. In this project, we attempt to unsurprisingly induce POS tags by
iteratively looking ... | cs.CL | partofspeech pos tagging is an old and fundamental task in natural language processing while supervised pos taggers have shown promising accuracy it is not always feasible to use supervised methods due to lack of labeled data in this project we attempt to unsurprisingly induce pos tags by iteratively looking for a recu... | [['partofspeech', 'pos', 'tagging', 'is', 'an', 'old', 'and', 'fundamental', 'task', 'in', 'natural', 'language', 'processing', 'while', 'supervised', 'pos', 'taggers', 'have', 'shown', 'promising', 'accuracy', 'it', 'is', 'not', 'always', 'feasible', 'to', 'use', 'supervised', 'methods', 'due', 'to', 'lack', 'of', 'la... | [0.03854100267814759, -0.027704535844513416, -0.09718349642860584, 0.1321541151989713, -0.18629149466944048, -0.16917345210766563, 0.08236030848601307, 0.4813271520229486, -0.319601414940105, -0.3851046969767851, -0.016134439773547154, -0.31438545318087563, -0.11693895694229585, 0.17173700300955738, -0.1108474283932875... |
1,801.03565 | Charge carrier transport asymmetry in monolayer graphene | The conductivity and Hall effect were measured in CVD-grown monolayer
graphene as a function of the gate voltage, $V_{g}$, at temperatures down to
$T$ = 2 K and in magnetic fields up to $B$ = 8 T. The minimal conductivity was
observed at positive $V_{g}$ which shows the position of the charge neutrality
point, $V_{NP... | cond-mat.mtrl-sci cond-mat.mes-hall | the conductivity and hall effect were measured in cvdgrown monolayer graphene as a function of the gate voltage v_g at temperatures down to t 2 k and in magnetic fields up to b 8 t the minimal conductivity was observed at positive v_g which shows the position of the charge neutrality point v_np with decreasing t v_np f... | [['the', 'conductivity', 'and', 'hall', 'effect', 'were', 'measured', 'in', 'cvdgrown', 'monolayer', 'graphene', 'as', 'a', 'function', 'of', 'the', 'gate', 'voltage', 'v_g', 'at', 'temperatures', 'down', 'to', 't', '2', 'k', 'and', 'in', 'magnetic', 'fields', 'up', 'to', 'b', '8', 't', 'the', 'minimal', 'conductivity'... | [-0.1720139190400242, 0.2759525731013602, -0.018259955608063257, -0.00041936295810560495, -0.015923168506402442, -0.19539443276944043, 0.07528607007090772, 0.33961489088276564, -0.2468287535112999, -0.3680226173879498, -0.017646290278365916, -0.37445007369387895, -0.08686135021802645, 0.19427331883723484, -0.0059751661... |
1,801.03566 | Another unWISE Update: The Deepest Ever Full-sky Maps at 3-5 microns | We have uniformly reprocessed ~140 terabytes of WISE and NEOWISE exposures to
create the deepest ever full-sky maps at 3.4 microns (W1) and 4.6 microns (W2).
Our coadds include ~4 years of observations and therefore feature ~4 times
greater integer frame coverage than the AllWISE Atlas stacks. Our new, publicly
avail... | astro-ph.IM | we have uniformly reprocessed 140 terabytes of wise and neowise exposures to create the deepest ever fullsky maps at 34 microns w1 and 46 microns w2 our coadds include 4 years of observations and therefore feature 4 times greater integer frame coverage than the allwise atlas stacks our new publicly available maps shoul... | [['we', 'have', 'uniformly', 'reprocessed', '140', 'terabytes', 'of', 'wise', 'and', 'neowise', 'exposures', 'to', 'create', 'the', 'deepest', 'ever', 'fullsky', 'maps', 'at', '34', 'microns', 'w1', 'and', '46', 'microns', 'w2', 'our', 'coadds', 'include', '4', 'years', 'of', 'observations', 'and', 'therefore', 'featur... | [-0.0034267577459104357, 0.06907644368475303, -0.05548978013321175, 0.07122499487595632, -0.1311640193744097, -0.09185831662616692, 0.03385272883460857, 0.448703276226297, -0.14613198694423774, -0.4068503356189467, 0.12475995329295983, -0.38459017892600966, 0.03546212335349992, 0.22327861001062957, -0.03852627641754225... |
1,801.03567 | SemiCompRisks: An R Package for Independent and Cluster-Correlated
Analyses of Semi-Competing Risks Data | Semi-competing risks refer to the setting where primary scientific interest
lies in estimation and inference with respect to a non-terminal event, the
occurrence of which is subject to a terminal event. In this paper, we present
the R package SemiCompRisks that provides functions to perform the analysis of
independen... | stat.CO | semicompeting risks refer to the setting where primary scientific interest lies in estimation and inference with respect to a nonterminal event the occurrence of which is subject to a terminal event in this paper we present the r package semicomprisks that provides functions to perform the analysis of independentcluste... | [['semicompeting', 'risks', 'refer', 'to', 'the', 'setting', 'where', 'primary', 'scientific', 'interest', 'lies', 'in', 'estimation', 'and', 'inference', 'with', 'respect', 'to', 'a', 'nonterminal', 'event', 'the', 'occurrence', 'of', 'which', 'is', 'subject', 'to', 'a', 'terminal', 'event', 'in', 'this', 'paper', 'we... | [-0.04878911046666632, -0.009714991609431118, -0.07554540468845516, 0.1088384864407616, -0.12144665085208162, -0.19226628466582807, 0.04993884269941574, 0.3728545410926209, -0.2454375857242236, -0.2916893051607124, 0.13946254155139046, -0.26742729538062504, -0.08027998815094561, 0.17186061347111767, -0.0929302302615006... |
1,801.03568 | Relation between boundary slip mechanisms and water-like fluid behavior | The slip of a fluid layer in contact with a solid confining surface is
investigated for different temperatures and densities using molecular dynamic
simulations. We show that for an anomalous water-like fluid the slip goes as
follows: for low levels of shear, the defect slip appears and is related with
the particle e... | cond-mat.soft | the slip of a fluid layer in contact with a solid confining surface is investigated for different temperatures and densities using molecular dynamic simulations we show that for an anomalous waterlike fluid the slip goes as follows for low levels of shear the defect slip appears and is related with the particle exchang... | [['the', 'slip', 'of', 'a', 'fluid', 'layer', 'in', 'contact', 'with', 'a', 'solid', 'confining', 'surface', 'is', 'investigated', 'for', 'different', 'temperatures', 'and', 'densities', 'using', 'molecular', 'dynamic', 'simulations', 'we', 'show', 'that', 'for', 'an', 'anomalous', 'waterlike', 'fluid', 'the', 'slip', ... | [-0.1588108108833829, 0.22008182722937716, -0.09749636797803557, -0.009704114407887337, 0.011417318530018546, -0.11719110450293455, -0.023308312505293912, 0.32840473142762977, -0.29966181666693753, -0.28937502089818873, 0.05980856835096212, -0.25956481001857257, -0.11409953106367202, 0.11384026869739129, -0.01156912481... |
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