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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1,801.00669 | E11, Brane Dynamics and Duality Symmetries | Following hep-th/0412336 we use the non-linear realisation of the semi-direct
product of E11 and its vector representation to construct brane dynamics. The
brane moves through a spacetime which arises in the non-linear realisation from
the vector representation and it contains the usual embedding coordinates as
well ... | hep-th | following hepth0412336 we use the nonlinear realisation of the semidirect product of e11 and its vector representation to construct brane dynamics the brane moves through a spacetime which arises in the nonlinear realisation from the vector representation and it contains the usual embedding coordinates as well as the w... | [['following', 'hepth0412336', 'we', 'use', 'the', 'nonlinear', 'realisation', 'of', 'the', 'semidirect', 'product', 'of', 'e11', 'and', 'its', 'vector', 'representation', 'to', 'construct', 'brane', 'dynamics', 'the', 'brane', 'moves', 'through', 'a', 'spacetime', 'which', 'arises', 'in', 'the', 'nonlinear', 'realisat... | [-0.12196346150063302, 0.11648370776801249, -0.05686649242416024, 0.10083964859722587, -0.12679143347119426, -0.10193522712620703, -0.03154533366652448, 0.29123462710691533, -0.24239832947597556, -0.25248373424958276, 0.1481555688933915, -0.2757437508472282, -0.17225831676598477, 0.08729349777264439, -0.065279277845326... |
1,801.0067 | Low-Rank Matrix Approximations Do Not Need a Singular Value Gap | This is a systematic investigation into the sensitivity of low-rank
approximations of real matrices. We show that the low-rank approximation
errors, in the two-norm, Frobenius norm and more generally, any Schatten
p-norm, are insensitive to additive rank-preserving perturbations in the
projector basis; and to matrix ... | math.NA | this is a systematic investigation into the sensitivity of lowrank approximations of real matrices we show that the lowrank approximation errors in the twonorm frobenius norm and more generally any schatten pnorm are insensitive to additive rankpreserving perturbations in the projector basis and to matrix perturbations... | [['this', 'is', 'a', 'systematic', 'investigation', 'into', 'the', 'sensitivity', 'of', 'lowrank', 'approximations', 'of', 'real', 'matrices', 'we', 'show', 'that', 'the', 'lowrank', 'approximation', 'errors', 'in', 'the', 'twonorm', 'frobenius', 'norm', 'and', 'more', 'generally', 'any', 'schatten', 'pnorm', 'are', 'i... | [-0.14948936854359798, 0.0784577093940849, -0.0452102912825972, 0.10156272119428549, -0.07045245375484228, -0.11390326996333897, 0.004116555624124076, 0.38906524061328834, -0.328444745288127, -0.22345700399018825, 0.16476258610297614, -0.26721753728472525, -0.19296099040915982, 0.08838665213099578, -0.09788215610509117... |
1,801.00671 | A Spectroscopic Survey of the Youngest Field Stars in the Solar
Neighborhood. II. The optically faint sample | Star formation in the solar neighborhood is mainly traced by young stars in
open clusters, associations and in the field, which can be identified by their
X-ray emission. The determination of stellar parameters for the counterparts of
X-ray sources is crucial for their study. This work extends the spectroscopic
study... | astro-ph.SR | star formation in the solar neighborhood is mainly traced by young stars in open clusters associations and in the field which can be identified by their xray emission the determination of stellar parameters for the counterparts of xray sources is crucial for their study this work extends the spectroscopic study of the ... | [['star', 'formation', 'in', 'the', 'solar', 'neighborhood', 'is', 'mainly', 'traced', 'by', 'young', 'stars', 'in', 'open', 'clusters', 'associations', 'and', 'in', 'the', 'field', 'which', 'can', 'be', 'identified', 'by', 'their', 'xray', 'emission', 'the', 'determination', 'of', 'stellar', 'parameters', 'for', 'the'... | [-0.05803531926252924, 0.12607195872970553, -0.04271665398951575, 0.09054968441204433, -0.11427689248688488, -0.040265228210323786, 0.12073647399268386, 0.4316387132640524, -0.16332518089895537, -0.3895249824697922, 0.0439498084961964, -0.3023495561813554, -0.02177702681251229, 0.24125113564704256, -0.05564165722960269... |
1,801.00672 | Primordial Black Holes as Generators of Cosmic Structures | Primordial black holes (PBHs) could provide the dark matter in various mass
windows below $10^2 M_{\odot}$ and those of $30 M_{\odot}$ might explain the
LIGO events. PBHs much larger than this might have important consequences even
if they provide only a small fraction of the dark matter. In particular, they
could ge... | astro-ph.CO | primordial black holes pbhs could provide the dark matter in various mass windows below 102 m_odot and those of 30 m_odot might explain the ligo events pbhs much larger than this might have important consequences even if they provide only a small fraction of the dark matter in particular they could generate cosmologica... | [['primordial', 'black', 'holes', 'pbhs', 'could', 'provide', 'the', 'dark', 'matter', 'in', 'various', 'mass', 'windows', 'below', '102', 'm_odot', 'and', 'those', 'of', '30', 'm_odot', 'might', 'explain', 'the', 'ligo', 'events', 'pbhs', 'much', 'larger', 'than', 'this', 'might', 'have', 'important', 'consequences', ... | [-0.12456265329393137, 0.196315207495612, -0.06996842891563375, 0.1940526907923651, -0.12643588144373433, -0.06242065335906853, -0.002428169509608157, 0.305229064667566, -0.17088156281911496, -0.3646590621642894, 0.053445147319484645, -0.3015165293927183, -0.049422665029068634, 0.2157367630783107, 0.0038116360004629766... |
1,801.00673 | CutIGA with Basis Function Removal | We consider a cut isogeometric method, where the boundary of the domain is
allowed to cut through the background mesh in an arbitrary fashion for a second
order elliptic model problem. In order to stabilize the method on the cut
boundary we remove basis functions which have small intersection with the
computational d... | math.NA | we consider a cut isogeometric method where the boundary of the domain is allowed to cut through the background mesh in an arbitrary fashion for a second order elliptic model problem in order to stabilize the method on the cut boundary we remove basis functions which have small intersection with the computational domai... | [['we', 'consider', 'a', 'cut', 'isogeometric', 'method', 'where', 'the', 'boundary', 'of', 'the', 'domain', 'is', 'allowed', 'to', 'cut', 'through', 'the', 'background', 'mesh', 'in', 'an', 'arbitrary', 'fashion', 'for', 'a', 'second', 'order', 'elliptic', 'model', 'problem', 'in', 'order', 'to', 'stabilize', 'the', '... | [-0.09121150376790381, 0.024758955881283174, -0.10242328190206341, 0.03380201912752571, -0.08055499312467873, -0.06682468914090002, 0.047765661161046157, 0.34914004750193117, -0.2970149583242675, -0.28548101766748313, 0.14040701857772953, -0.2577844690828723, -0.07313445679585825, 0.12019481472027033, -0.08731355537918... |
1,801.00674 | A Three-Dimensional Mathematical Model of Collagen Contraction | In this paper, we introduce a three-dimensional mathematical model of
collagen contraction with microbuckling based on the two-dimensional model
previously developed by the authors. The model both qualitatively and
quantitatively replicates experimental data including lattice contraction over
a time course of 40 hour... | q-bio.CB | in this paper we introduce a threedimensional mathematical model of collagen contraction with microbuckling based on the twodimensional model previously developed by the authors the model both qualitatively and quantitatively replicates experimental data including lattice contraction over a time course of 40 hours for ... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'threedimensional', 'mathematical', 'model', 'of', 'collagen', 'contraction', 'with', 'microbuckling', 'based', 'on', 'the', 'twodimensional', 'model', 'previously', 'developed', 'by', 'the', 'authors', 'the', 'model', 'both', 'qualitatively', 'and', 'quantitatively', 'r... | [-0.08209849623875376, 0.16095480890637087, -0.03833889107237447, -0.002502310683924424, -0.02209410094216747, -0.10709501799955999, 0.05582673238032445, 0.43657415487610224, -0.24026575418000268, -0.2581476836974891, 0.07917942095851034, -0.22628348790337596, -0.18520023239741348, 0.14600796795357898, -0.0179569827950... |
1,801.00675 | Estimating decay rate of $X^{\pm}(5568)\to B_s\pi^{\pm}$ while assuming
them to be molecular states | Discovery of $X(5568)$ brings up a tremendous interest because it is very
special, i.e. made of four different flavors. The D0 collaboration claimed that
they observed this resonance through portal $X(5568)\to B_s\pi$, but
unfortunately, later the LHCb, CMS, CDF and ATLAS collaborations' reports
indicate that no such... | hep-ph hep-ex | discovery of x5568 brings up a tremendous interest because it is very special ie made of four different flavors the d0 collaboration claimed that they observed this resonance through portal x5568to b_spi but unfortunately later the lhcb cms cdf and atlas collaborations reports indicate that no such state was found almo... | [['discovery', 'of', 'x5568', 'brings', 'up', 'a', 'tremendous', 'interest', 'because', 'it', 'is', 'very', 'special', 'ie', 'made', 'of', 'four', 'different', 'flavors', 'the', 'd0', 'collaboration', 'claimed', 'that', 'they', 'observed', 'this', 'resonance', 'through', 'portal', 'x5568to', 'b_spi', 'but', 'unfortunat... | [-0.09700250034195615, 0.20242332062569762, -0.10028228508856367, 0.10872905902542114, -0.0665666463151126, -0.14298920211118252, 0.09730308326110643, 0.3257126623881672, -0.19483342959002697, -0.3102683116666933, 0.05073049805938879, -0.32100826217593714, -0.046342410746075334, 0.1526563066670442, 0.057217693069008466... |
1,801.00676 | The frame of fixed stars in Relational Mechanics | Relational mechanics is a gauge theory of classical mechanics whose laws do
not govern the motion of individual particles but the evolution of the
distances between particles. Its formulation gives a satisfactory answer to
Leibniz's and Mach's criticisms of Newton's mechanics: relational mechanics
does not rely on th... | physics.hist-ph astro-ph.CO gr-qc | relational mechanics is a gauge theory of classical mechanics whose laws do not govern the motion of individual particles but the evolution of the distances between particles its formulation gives a satisfactory answer to leibnizs and machs criticisms of newtons mechanics relational mechanics does not rely on the idea ... | [['relational', 'mechanics', 'is', 'a', 'gauge', 'theory', 'of', 'classical', 'mechanics', 'whose', 'laws', 'do', 'not', 'govern', 'the', 'motion', 'of', 'individual', 'particles', 'but', 'the', 'evolution', 'of', 'the', 'distances', 'between', 'particles', 'its', 'formulation', 'gives', 'a', 'satisfactory', 'answer', ... | [-0.07695562756772892, 0.16503860309816884, -0.16323846236728373, 0.08323167224017229, -0.13260756104237176, -0.1551309167206737, -0.028009751937071118, 0.2961326768031697, -0.2914288408315644, -0.3303644258096405, -0.009331389229969475, -0.29857084487468516, -0.09139346386046814, 0.1382120375708147, -0.144022332247475... |
1,801.00677 | Ultrastrong adhesion in the contact with thin elastic layers on a rigid
foundation | In the present short note, we generalize simple approximate
Johnson-Jaffar-Barber solutions for the indentation by a rigid punch of a thin
elastic layer on a rigid foundation to the case of adhesion. This could be an
interesting geometry for an adhesive system, a limit case of the more general
class of layered system... | cond-mat.mtrl-sci | in the present short note we generalize simple approximate johnsonjaffarbarber solutions for the indentation by a rigid punch of a thin elastic layer on a rigid foundation to the case of adhesion this could be an interesting geometry for an adhesive system a limit case of the more general class of layered systems or fg... | [['in', 'the', 'present', 'short', 'note', 'we', 'generalize', 'simple', 'approximate', 'johnsonjaffarbarber', 'solutions', 'for', 'the', 'indentation', 'by', 'a', 'rigid', 'punch', 'of', 'a', 'thin', 'elastic', 'layer', 'on', 'a', 'rigid', 'foundation', 'to', 'the', 'case', 'of', 'adhesion', 'this', 'could', 'be', 'an... | [-0.14000822730146414, 0.11365686079404101, -0.04516495079789535, 0.02677186705026192, -0.04752024673262095, -0.16960190391695373, 0.040301724403664606, 0.3781512867524681, -0.27203566116471606, -0.27618734794668853, 0.04758419146612623, -0.23051654895857335, -0.1740194698178535, 0.2193298713284466, -0.0664139923819127... |
1,801.00678 | Artificial vs Substantial Gauge Symmetries: a Criterion and an
Application to the Electroweak Model | To systematically answer the generalized Kretschmann objection, we propose a
mean to make operational a criterion widely recognized as allowing to decide if
the gauge symmetry of a theory is artificial or substantial. Our proposition is
based on the dressing field method of gauge symmetry reduction, a new simple
tool... | physics.hist-ph hep-th | to systematically answer the generalized kretschmann objection we propose a mean to make operational a criterion widely recognized as allowing to decide if the gauge symmetry of a theory is artificial or substantial our proposition is based on the dressing field method of gauge symmetry reduction a new simple tool from... | [['to', 'systematically', 'answer', 'the', 'generalized', 'kretschmann', 'objection', 'we', 'propose', 'a', 'mean', 'to', 'make', 'operational', 'a', 'criterion', 'widely', 'recognized', 'as', 'allowing', 'to', 'decide', 'if', 'the', 'gauge', 'symmetry', 'of', 'a', 'theory', 'is', 'artificial', 'or', 'substantial', 'ou... | [-0.07217030940004267, 0.10048671602527355, -0.14973464761707153, 0.13380046424988126, -0.14979151606170849, -0.15380515940078013, 0.06258881166909955, 0.32312684026188576, -0.265339710268673, -0.30730839189305736, 0.06565155656010445, -0.1771996124459822, -0.20081068011727388, 0.1333296178190222, -0.09861790685617662,... |
1,801.00679 | An Effective Photon Momentum in a Dielectric Medium: A Relativistic
Approach | We use a relativistic argument to define an effective photon that travels
through a transparent (non-absorbing) nondispersive dielectric medium of index
of refraction $n$. If $p$ is the momentum of the photon in a vacuum, then the
momentum of an effective photon inside the medium may be of the form $p_{\rm
eff}=pn^\a... | physics.class-ph physics.optics | we use a relativistic argument to define an effective photon that travels through a transparent nonabsorbing nondispersive dielectric medium of index of refraction n if p is the momentum of the photon in a vacuum then the momentum of an effective photon inside the medium may be of the form p_rm effpnalpha and still rep... | [['we', 'use', 'a', 'relativistic', 'argument', 'to', 'define', 'an', 'effective', 'photon', 'that', 'travels', 'through', 'a', 'transparent', 'nonabsorbing', 'nondispersive', 'dielectric', 'medium', 'of', 'index', 'of', 'refraction', 'n', 'if', 'p', 'is', 'the', 'momentum', 'of', 'the', 'photon', 'in', 'a', 'vacuum', ... | [-0.12268585253982468, 0.2416668302629408, -0.154112776756247, 0.05444323437466742, -0.0871824826184472, -0.10496725283186645, -0.0014102794576753327, 0.38961801456010087, -0.2355038617301653, -0.28792101952267135, -0.021089921267009638, -0.2949345346460951, -0.024474487429193066, 0.1579976677176285, -0.004960656156168... |
1,801.0068 | Sampling-Based Methods for Factored Task and Motion Planning | This paper presents a general-purpose formulation of a large class of
discrete-time planning problems, with hybrid state and control-spaces, as
factored transition systems. Factoring allows state transitions to be described
as the intersection of several constraints each affecting a subset of the state
and control va... | cs.RO | this paper presents a generalpurpose formulation of a large class of discretetime planning problems with hybrid state and controlspaces as factored transition systems factoring allows state transitions to be described as the intersection of several constraints each affecting a subset of the state and control variables ... | [['this', 'paper', 'presents', 'a', 'generalpurpose', 'formulation', 'of', 'a', 'large', 'class', 'of', 'discretetime', 'planning', 'problems', 'with', 'hybrid', 'state', 'and', 'controlspaces', 'as', 'factored', 'transition', 'systems', 'factoring', 'allows', 'state', 'transitions', 'to', 'be', 'described', 'as', 'the... | [-0.12319955847403206, 0.05659339421334465, -0.08306151342241128, 0.02470488868118746, -0.10184259883390934, -0.14929652419741168, 0.065170079956054, 0.3857678639891049, -0.28271715878366144, -0.3457119418829508, 0.12551922717151673, -0.21581447347036228, -0.13273851978564005, 0.2337388471168883, -0.0956600053761543, 0... |
1,801.00681 | A novel improved fuzzy support vector machine based stock price trend
forecast model | Application of fuzzy support vector machine in stock price forecast. Support
vector machine is a new type of machine learning method proposed in 1990s. It
can deal with classification and regression problems very successfully. Due to
the excellent learning performance of support vector machine, the technology
has bec... | stat.ML q-fin.ST | application of fuzzy support vector machine in stock price forecast support vector machine is a new type of machine learning method proposed in 1990s it can deal with classification and regression problems very successfully due to the excellent learning performance of support vector machine the technology has become a ... | [['application', 'of', 'fuzzy', 'support', 'vector', 'machine', 'in', 'stock', 'price', 'forecast', 'support', 'vector', 'machine', 'is', 'a', 'new', 'type', 'of', 'machine', 'learning', 'method', 'proposed', 'in', '1990s', 'it', 'can', 'deal', 'with', 'classification', 'and', 'regression', 'problems', 'very', 'success... | [-0.05099307542965228, 0.057951759344715505, -0.09531503177803648, 0.11612178320361002, -0.17377546972734081, -0.19279911922733428, 0.05742577489630129, 0.41329149564326795, -0.27635839065403073, -0.2693931552483726, 0.14803892465305735, -0.27345883426415984, -0.15953361779163228, 0.22304914719733868, -0.14047936437064... |
1,801.00682 | A Probabilistic Subspace Bound with Application to Active Subspaces | Given a real symmetric positive semi-definite matrix E, and an approximation
S that is a sum of n independent matrix-valued random variables, we present
bounds on the relative error in S due to randomization. The bounds do not
depend on the matrix dimensions but only on the numerical rank (intrinsic
dimension) of E. ... | math.NA | given a real symmetric positive semidefinite matrix e and an approximation s that is a sum of n independent matrixvalued random variables we present bounds on the relative error in s due to randomization the bounds do not depend on the matrix dimensions but only on the numerical rank intrinsic dimension of e our approa... | [['given', 'a', 'real', 'symmetric', 'positive', 'semidefinite', 'matrix', 'e', 'and', 'an', 'approximation', 's', 'that', 'is', 'a', 'sum', 'of', 'n', 'independent', 'matrixvalued', 'random', 'variables', 'we', 'present', 'bounds', 'on', 'the', 'relative', 'error', 'in', 's', 'due', 'to', 'randomization', 'the', 'boun... | [-0.10166782218102219, 0.11582194049157571, -0.07040939817539929, 0.06707824826347798, -0.05545711914192508, -0.14049021393228112, 0.09403365239987589, 0.3753336032517673, -0.24452747710713307, -0.2975037185700213, 0.09805011253848442, -0.2667697711071566, -0.1390732761728839, 0.1980937841940891, -0.05580864868681418, ... |
1,801.00683 | The sequential loss of allelic diversity | This paper gives a new flavor of what Peter Jagers and his co-authors call `the path to extinction'. In a neutral population with constant size $N$, we assume that each individual at time $0$ carries a distinct type, or allele. We consider the joint dynamics of these $N$ alleles, for example the dynamics of their respe... | math.PR q-bio.PE | this paper gives a new flavor of what peter jagers and his coauthors call the path to extinction in a neutral population with constant size n we assume that each individual at time 0 carries a distinct type or allele we consider the joint dynamics of these n alleles for example the dynamics of their respective frequenc... | [['this', 'paper', 'gives', 'a', 'new', 'flavor', 'of', 'what', 'peter', 'jagers', 'and', 'his', 'coauthors', 'call', 'the', 'path', 'to', 'extinction', 'in', 'a', 'neutral', 'population', 'with', 'constant', 'size', 'n', 'we', 'assume', 'that', 'each', 'individual', 'at', 'time', '0', 'carries', 'a', 'distinct', 'type... | [-0.08926261556490961, 0.14669947238525777, -0.057967878073147246, 0.0678982419060115, -0.02288088617454533, -0.12230594273622535, 0.13114744642956705, 0.37219206368686947, -0.3110524370653055, -0.23203116740531674, 0.06631583780285948, -0.250403177651872, -0.11806884905885587, 0.11460736541861169, -0.07326914802216357... |
1,801.00684 | Risk minimization in life-cycle oil production optimization | The geology of oil reservoirs is largely unknown. Consequently, the reservoir
models used for production optimization are subject to significant uncertainty.
To minimize the associated risk, the oil literature has mainly used
ensemble-based methods to optimize sample estimated risk measures of net
present value (NPV)... | math.OC | the geology of oil reservoirs is largely unknown consequently the reservoir models used for production optimization are subject to significant uncertainty to minimize the associated risk the oil literature has mainly used ensemblebased methods to optimize sample estimated risk measures of net present value npv however ... | [['the', 'geology', 'of', 'oil', 'reservoirs', 'is', 'largely', 'unknown', 'consequently', 'the', 'reservoir', 'models', 'used', 'for', 'production', 'optimization', 'are', 'subject', 'to', 'significant', 'uncertainty', 'to', 'minimize', 'the', 'associated', 'risk', 'the', 'oil', 'literature', 'has', 'mainly', 'used', ... | [-0.062012753025042104, 0.027965095995339737, -0.06591290129768086, 0.14057905833549683, -0.03863573918485204, -0.14199422282621776, 0.11926112516973353, 0.41785123770814814, -0.2426294879774556, -0.2982716678172076, 0.09366265531337842, -0.2897424552383484, -0.12803051043266275, 0.20521878067693736, -0.212579057059599... |
1,801.00685 | Broadband Spectral Fitting of Blazars using XSPEC | The broadband spectral energy distribution(SED) of blazars is generally
interpreted as radiation arising from synchrotron and inverse Compton
mechanisms.Traditionally, the underlying source parameters responsible for
these emission processes,like particle energy density, magnetic field, etc.,
are obtained through sim... | astro-ph.HE | the broadband spectral energy distributionsed of blazars is generally interpreted as radiation arising from synchrotron and inverse compton mechanismstraditionally the underlying source parameters responsible for these emission processeslike particle energy density magnetic field etc are obtained through simple visual ... | [['the', 'broadband', 'spectral', 'energy', 'distributionsed', 'of', 'blazars', 'is', 'generally', 'interpreted', 'as', 'radiation', 'arising', 'from', 'synchrotron', 'and', 'inverse', 'compton', 'mechanismstraditionally', 'the', 'underlying', 'source', 'parameters', 'responsible', 'for', 'these', 'emission', 'processe... | [-0.018523388288071603, 0.0792540136711149, -0.092705948149093, 0.12504896514254246, -0.09463757791444269, -0.10862664817174146, 0.03215000369824976, 0.43891076421296876, -0.24399627576928332, -0.3884186143474897, 0.07756353285973062, -0.202590694275553, -0.06352270418456243, 0.24570574965730252, -0.027804271120539042,... |
1,801.00686 | Fermionic Minimal Dark Matter in 5D Gauge-Higgs Unification | We propose a Minimal Dark Matter (MDM) scenario in the context of a simple
gauge-Higgs Unification (GHU) model based on the gauge group SU(3) x U(1)' in
5-dimensional Minkowski space with a compactification of the 5th dimension on
S^1/Z_2 orbifold. A pair of vector-like SU(3) multiplet fermions in a
higher-dimensiona... | hep-ph | we propose a minimal dark matter mdm scenario in the context of a simple gaugehiggs unification ghu model based on the gauge group su3 x u1 in 5dimensional minkowski space with a compactification of the 5th dimension on s1z_2 orbifold a pair of vectorlike su3 multiplet fermions in a higherdimensional representation is ... | [['we', 'propose', 'a', 'minimal', 'dark', 'matter', 'mdm', 'scenario', 'in', 'the', 'context', 'of', 'a', 'simple', 'gaugehiggs', 'unification', 'ghu', 'model', 'based', 'on', 'the', 'gauge', 'group', 'su3', 'x', 'u1', 'in', '5dimensional', 'minkowski', 'space', 'with', 'a', 'compactification', 'of', 'the', '5th', 'di... | [-0.14381267686868893, 0.21590950268225165, -0.04015661252148971, 0.12823996879112495, -0.10015552659871617, -0.17419838634081983, -0.027718813735857575, 0.3093836114812765, -0.16420756608493042, -0.31432073538042143, 0.037090156430957276, -0.2635581706930335, -0.050048191217163536, 0.0828209970943599, 0.02360526871100... |
1,801.00687 | Scilla: a Smart Contract Intermediate-Level LAnguage | This paper outlines key design principles of Scilla---an intermediate-level
language for verified smart contracts.
Scilla provides a clean separation between the communication aspect of smart
contracts on a blockchain, allowing for the rich interaction patterns, and a
programming component, which enjoys principled ... | cs.PL | this paper outlines key design principles of scillaan intermediatelevel language for verified smart contracts scilla provides a clean separation between the communication aspect of smart contracts on a blockchain allowing for the rich interaction patterns and a programming component which enjoys principled semantics an... | [['this', 'paper', 'outlines', 'key', 'design', 'principles', 'of', 'scillaan', 'intermediatelevel', 'language', 'for', 'verified', 'smart', 'contracts', 'scilla', 'provides', 'a', 'clean', 'separation', 'between', 'the', 'communication', 'aspect', 'of', 'smart', 'contracts', 'on', 'a', 'blockchain', 'allowing', 'for',... | [-0.0984605828494144, -0.039633953407246736, -0.1292672341784055, 0.08087864425768505, -0.1653457952197641, -0.17345292772321652, 0.08356090886809397, 0.38707971991971135, -0.3398506993427873, -0.3112012722917522, 0.13476088067109232, -0.22269778183544986, -0.09953138129785657, 0.200725511291724, -0.11067353464507808, ... |
1,801.00688 | Learning audio and image representations with bio-inspired trainable
feature extractors | Recent advancements in pattern recognition and signal processing concern the
automatic learning of data representations from labeled training samples.
Typical approaches are based on deep learning and convolutional neural
networks, which require large amount of labeled training samples. In this work,
we propose novel... | cs.CV cs.AI cs.SD eess.AS eess.IV | recent advancements in pattern recognition and signal processing concern the automatic learning of data representations from labeled training samples typical approaches are based on deep learning and convolutional neural networks which require large amount of labeled training samples in this work we propose novel featu... | [['recent', 'advancements', 'in', 'pattern', 'recognition', 'and', 'signal', 'processing', 'concern', 'the', 'automatic', 'learning', 'of', 'data', 'representations', 'from', 'labeled', 'training', 'samples', 'typical', 'approaches', 'are', 'based', 'on', 'deep', 'learning', 'and', 'convolutional', 'neural', 'networks'... | [-0.013247112410941295, -0.0152020930197198, -0.046486489776898884, 0.015688189756582732, -0.11066528763400302, -0.14714679195146477, 0.0015413058683320525, 0.4993886450482976, -0.29591939102725257, -0.3584553762727107, 0.07327806649707436, -0.2864304670088348, -0.21050430215629085, 0.21155168918804043, -0.191095790160... |
1,801.00689 | Can decaying vacuum elucidate the late-time dynamics of the Universe ? | We examine the decay vacuum model with a parameter $\epsilon$ that indicates
the vacuum energy decay rate. By constraining this model with cosmic microwave
background radiation, baryon acoustic oscillation, type Ia supernovae and 30
H(z) cosmic chronometer data points, we find that $\epsilon=-0.0003\pm0.00024$
with t... | astro-ph.CO | we examine the decay vacuum model with a parameter epsilon that indicates the vacuum energy decay rate by constraining this model with cosmic microwave background radiation baryon acoustic oscillation type ia supernovae and 30 hz cosmic chronometer data points we find that epsilon00003pm000024 with the best fitted chi2... | [['we', 'examine', 'the', 'decay', 'vacuum', 'model', 'with', 'a', 'parameter', 'epsilon', 'that', 'indicates', 'the', 'vacuum', 'energy', 'decay', 'rate', 'by', 'constraining', 'this', 'model', 'with', 'cosmic', 'microwave', 'background', 'radiation', 'baryon', 'acoustic', 'oscillation', 'type', 'ia', 'supernovae', 'a... | [-0.09071186130417377, 0.17816065454306745, -0.05608528622542508, 0.1172617303122284, -0.1106256632379622, -0.1135009961144533, 0.054155691560091715, 0.28409985319428543, -0.23075819416304252, -0.3598344220746575, 0.021242450079755924, -0.29111422632455025, -0.012592413096821733, 0.1903968758332277, 0.06077172212820057... |
1,801.0069 | DeepMind Control Suite | The DeepMind Control Suite is a set of continuous control tasks with a
standardised structure and interpretable rewards, intended to serve as
performance benchmarks for reinforcement learning agents. The tasks are written
in Python and powered by the MuJoCo physics engine, making them easy to use and
modify. We inclu... | cs.AI | the deepmind control suite is a set of continuous control tasks with a standardised structure and interpretable rewards intended to serve as performance benchmarks for reinforcement learning agents the tasks are written in python and powered by the mujoco physics engine making them easy to use and modify we include ben... | [['the', 'deepmind', 'control', 'suite', 'is', 'a', 'set', 'of', 'continuous', 'control', 'tasks', 'with', 'a', 'standardised', 'structure', 'and', 'interpretable', 'rewards', 'intended', 'to', 'serve', 'as', 'performance', 'benchmarks', 'for', 'reinforcement', 'learning', 'agents', 'the', 'tasks', 'are', 'written', 'i... | [-0.0372269647064763, -0.022511393963162537, -0.06039838314804078, 0.05428478579384498, -0.1853805170919169, -0.21753596381323648, 0.017437772746656983, 0.5026377769003452, -0.26779075890687676, -0.37397262789833713, 0.11327372596789362, -0.27197371151718036, -0.068308069908493, 0.31578990712132254, -0.0854617211521721... |
1,801.00691 | Energy-enstrophy conserving compatible finite element schemes for the
rotating shallow water equations with slip boundary conditions | We describe an energy-enstrophy conserving discretisation for the rotating
shallow water equations with slip boundary conditions. This relaxes the
assumption of boundary-free domains (periodic solutions or the surface of a
sphere, for example) in the energy-enstrophy conserving formulation of McRae
and Cotter (2014).... | math.NA physics.ao-ph | we describe an energyenstrophy conserving discretisation for the rotating shallow water equations with slip boundary conditions this relaxes the assumption of boundaryfree domains periodic solutions or the surface of a sphere for example in the energyenstrophy conserving formulation of mcrae and cotter 2014 this discre... | [['we', 'describe', 'an', 'energyenstrophy', 'conserving', 'discretisation', 'for', 'the', 'rotating', 'shallow', 'water', 'equations', 'with', 'slip', 'boundary', 'conditions', 'this', 'relaxes', 'the', 'assumption', 'of', 'boundaryfree', 'domains', 'periodic', 'solutions', 'or', 'the', 'surface', 'of', 'a', 'sphere',... | [-0.16526358666820357, 0.1033697358176472, -0.0821272096587251, 0.03284996000795879, -0.08281192338714997, -0.12829202018452412, 0.003169302059563272, 0.3072035077705302, -0.23147071539330286, -0.2521760269830173, 0.13596916305268128, -0.22454019180602497, -0.058490176536989485, 0.15354231689736775, -0.0889312447415608... |
1,801.00692 | Transverse-velocity scaling of femtoscopy in $\sqrt{s}=7$ TeV
proton-proton collisions | Although transverse-mass scaling of femtoscopic radii is found to hold to a
good approximation in heavy-ion collision experiments, it is seen to fail for
high-energy proton-proton collisions. It is shown that if invariant radius
parameters are plotted versus the transverse velocity instead, scaling with the
transvers... | hep-ph nucl-ex | although transversemass scaling of femtoscopic radii is found to hold to a good approximation in heavyion collision experiments it is seen to fail for highenergy protonproton collisions it is shown that if invariant radius parameters are plotted versus the transverse velocity instead scaling with the transverse velocit... | [['although', 'transversemass', 'scaling', 'of', 'femtoscopic', 'radii', 'is', 'found', 'to', 'hold', 'to', 'a', 'good', 'approximation', 'in', 'heavyion', 'collision', 'experiments', 'it', 'is', 'seen', 'to', 'fail', 'for', 'highenergy', 'protonproton', 'collisions', 'it', 'is', 'shown', 'that', 'if', 'invariant', 'ra... | [-0.07725829972690944, 0.2067741417228731, -0.201662371824704, 0.19664655796099287, -0.04189159154002346, -0.15570708218294738, -0.15559599770983654, 0.4291024120218718, -0.19462725221276728, -0.2767412031291803, -0.08440939778003341, -0.3239471606437617, 0.029256271219568208, 0.22076562841756464, 0.02672481221327586, ... |
1,801.00693 | Denoising Adversarial Autoencoders: Classifying Skin Lesions Using
Limited Labelled Training Data | We propose a novel deep learning model for classifying medical images in the
setting where there is a large amount of unlabelled medical data available, but
labelled data is in limited supply. We consider the specific case of
classifying skin lesions as either malignant or benign. In this setting, the
proposed approa... | cs.CV | we propose a novel deep learning model for classifying medical images in the setting where there is a large amount of unlabelled medical data available but labelled data is in limited supply we consider the specific case of classifying skin lesions as either malignant or benign in this setting the proposed approach the... | [['we', 'propose', 'a', 'novel', 'deep', 'learning', 'model', 'for', 'classifying', 'medical', 'images', 'in', 'the', 'setting', 'where', 'there', 'is', 'a', 'large', 'amount', 'of', 'unlabelled', 'medical', 'data', 'available', 'but', 'labelled', 'data', 'is', 'in', 'limited', 'supply', 'we', 'consider', 'the', 'speci... | [0.0024412710140380976, 0.012713120408950984, -0.0025346275074642245, 0.09678254739436157, -0.12472781078389086, -0.1521614249756544, 0.05838354607699674, 0.4014338463693544, -0.255003362267959, -0.33949703508606494, 0.07389647681696512, -0.32764237214412006, -0.15522648251865903, 0.14445554915259928, -0.21268704935063... |
1,801.00694 | The New Threats of Information Hiding: the Road Ahead | Compared to cryptography, steganography is a less discussed domain. However,
there is a recent trend of exploiting various information hiding techniques to
empower malware, for instance to bypass security frameworks of mobile devices
or to exfiltrate sensitive data. This is mostly due to the need to counteract
increa... | cs.CR | compared to cryptography steganography is a less discussed domain however there is a recent trend of exploiting various information hiding techniques to empower malware for instance to bypass security frameworks of mobile devices or to exfiltrate sensitive data this is mostly due to the need to counteract increasingly ... | [['compared', 'to', 'cryptography', 'steganography', 'is', 'a', 'less', 'discussed', 'domain', 'however', 'there', 'is', 'a', 'recent', 'trend', 'of', 'exploiting', 'various', 'information', 'hiding', 'techniques', 'to', 'empower', 'malware', 'for', 'instance', 'to', 'bypass', 'security', 'frameworks', 'of', 'mobile', ... | [-0.16046735072670731, 0.007967896586650926, -0.0830191398378123, 0.08989720958352061, -0.1575202177645582, -0.25098170098058425, 0.0909090364549422, 0.3489159325534164, -0.2580508121089114, -0.33681473137359275, 0.17252256297224172, -0.31593622118728515, -0.17554279660566174, 0.23694746732133243, -0.20907104823113928,... |
1,801.00695 | Hydrodynamic, Optically-Field-Ionized (HOFI) Plasma Channels | We present experiments and numerical simulations which demonstrate that
fully-ionized, low-density plasma channels could be formed by hydrodynamic
expansion of plasma columns produced by optical field ionization (OFI).
Simulations of the hydrodynamic expansion of plasma columns formed in hydrogen
by an axicon lens sh... | physics.plasm-ph physics.acc-ph | we present experiments and numerical simulations which demonstrate that fullyionized lowdensity plasma channels could be formed by hydrodynamic expansion of plasma columns produced by optical field ionization ofi simulations of the hydrodynamic expansion of plasma columns formed in hydrogen by an axicon lens show the g... | [['we', 'present', 'experiments', 'and', 'numerical', 'simulations', 'which', 'demonstrate', 'that', 'fullyionized', 'lowdensity', 'plasma', 'channels', 'could', 'be', 'formed', 'by', 'hydrodynamic', 'expansion', 'of', 'plasma', 'columns', 'produced', 'by', 'optical', 'field', 'ionization', 'ofi', 'simulations', 'of', ... | [-0.15733601224080773, 0.26966322675003646, 0.024276754019520938, 0.007305030229020935, 0.06802131481183941, -0.12129570860905087, -0.010676582198542584, 0.397677902594968, -0.1782374287285148, -0.3510182229861332, 0.0650048318117335, -0.2428320501145023, 0.02854224478019176, 0.18446816104482028, 0.04852914236223468, 0... |
1,801.00696 | On pairs of interacting electrons in a quantum wire | In this paper we consider pairs of interacting electrons moving in a simple
quantum wire, namely the half-line. In particular, we extend the results
obtained in [arXiv:1708.03753] by allowing for contact interactions of the
Lieb-Liniger type between the two electrons constituting the pair. We construct
the associated... | math-ph math.MP | in this paper we consider pairs of interacting electrons moving in a simple quantum wire namely the halfline in particular we extend the results obtained in arxiv170803753 by allowing for contact interactions of the liebliniger type between the two electrons constituting the pair we construct the associated hamiltonian... | [['in', 'this', 'paper', 'we', 'consider', 'pairs', 'of', 'interacting', 'electrons', 'moving', 'in', 'a', 'simple', 'quantum', 'wire', 'namely', 'the', 'halfline', 'in', 'particular', 'we', 'extend', 'the', 'results', 'obtained', 'in', 'arxiv170803753', 'by', 'allowing', 'for', 'contact', 'interactions', 'of', 'the', ... | [-0.17529848597657222, 0.15574999015450805, -0.05847507013790924, 0.09053915921230238, 0.0009101252813547195, -0.15832633380829306, 0.013843957006938981, 0.34521421923169066, -0.2309406564409773, -0.23911047618385856, 0.009178380858009825, -0.28626755538529586, -0.13390451566838138, 0.15859503337376557, 0.0323115400458... |
1,801.00697 | Weakly Interacting Topological Insulators: Quantum Criticality and
Renormalization Group Approach | For D-dimensional weakly interacting topological insulators in certain
symmetry classes, the topological invariant can be calculated from a D- or
(D+1)-dimensional integration over a certain curvature function that is
expressed in terms of single-particle Green's functions. Based on the
divergence of curvature functi... | cond-mat.str-el | for ddimensional weakly interacting topological insulators in certain symmetry classes the topological invariant can be calculated from a d or d1dimensional integration over a certain curvature function that is expressed in terms of singleparticle greens functions based on the divergence of curvature function at the to... | [['for', 'ddimensional', 'weakly', 'interacting', 'topological', 'insulators', 'in', 'certain', 'symmetry', 'classes', 'the', 'topological', 'invariant', 'can', 'be', 'calculated', 'from', 'a', 'd', 'or', 'd1dimensional', 'integration', 'over', 'a', 'certain', 'curvature', 'function', 'that', 'is', 'expressed', 'in', '... | [-0.17241209153844803, 0.2056824804375661, -0.09510280001825182, 0.08928152782135401, -0.05524080842273471, -0.15864368720428534, 0.055229528824350345, 0.32539228060035563, -0.2695240792185988, -0.26939668340815437, 0.027855109572870497, -0.2994491894942145, -0.22570061813005143, 0.16625540510084433, 0.0381300671350923... |
1,801.00698 | Nanophotonics with 2D Transition Metal Dichalcogenides | Two-dimensional transition metal dichalcogenides (TMDCs) have recently become
attractive semiconductor materials for several optoelectronic applications,
such as photodetection, light harvesting, phototransistors, light-emitting
diodes, and lasers. They are particularly appealing because their bandgap lies
in the vis... | physics.optics cond-mat.mes-hall | twodimensional transition metal dichalcogenides tmdcs have recently become attractive semiconductor materials for several optoelectronic applications such as photodetection light harvesting phototransistors lightemitting diodes and lasers they are particularly appealing because their bandgap lies in the visible and nea... | [['twodimensional', 'transition', 'metal', 'dichalcogenides', 'tmdcs', 'have', 'recently', 'become', 'attractive', 'semiconductor', 'materials', 'for', 'several', 'optoelectronic', 'applications', 'such', 'as', 'photodetection', 'light', 'harvesting', 'phototransistors', 'lightemitting', 'diodes', 'and', 'lasers', 'the... | [-0.14067071202243825, 0.15738799486425706, 0.01733307552676706, 0.0018316270877221541, -0.07251093190861865, -0.24680589615018106, 0.05777346954055247, 0.5880000306584406, -0.22462851274758577, -0.25466184208053166, -0.02990199447303894, -0.31566211174213094, -0.23517942947219125, 0.2515096202929271, 0.037838796009600... |
1,801.00699 | Sandwich classification for $O_{2n+1}(R)$ and $U_{2n+1}(R,\Delta)$
revisited | In a recent paper, the author proved that if $n\geq 3$ is a natural number,
$R$ a commutative ring and $\sigma\in GL_n(R)$, then $t_{kl}(\sigma_{ij})$
where $i\neq j$ and $k\neq l$ can be expressed as a product of $8$ matrices of
the form $^{\epsilon}\sigma^{\pm 1}$ where $\epsilon\in E_n(R)$. In this
article we prov... | math.KT | in a recent paper the author proved that if ngeq 3 is a natural number r a commutative ring and sigmain gl_nr then t_klsigma_ij where ineq j and kneq l can be expressed as a product of 8 matrices of the form epsilonsigmapm 1 where epsilonin e_nr in this article we prove similar results for the odddimensional orthogonal... | [['in', 'a', 'recent', 'paper', 'the', 'author', 'proved', 'that', 'if', 'ngeq', '3', 'is', 'a', 'natural', 'number', 'r', 'a', 'commutative', 'ring', 'and', 'sigmain', 'gl_nr', 'then', 't_klsigma_ij', 'where', 'ineq', 'j', 'and', 'kneq', 'l', 'can', 'be', 'expressed', 'as', 'a', 'product', 'of', '8', 'matrices', 'of',... | [-0.19081819621108784, 0.10588306325694753, -0.0578120126000916, 0.0379746913495991, -0.021660035538176695, -0.1967210612984167, -0.03385646642677279, 0.3341826152884298, -0.26541154637104936, -0.20160167936960027, 0.13502101900004265, -0.24980589468032122, -0.13658499952612652, 0.17133003849950101, -0.1194126036328574... |
1,801.007 | Nests, and their Role in the Orderability Problem | This chapter is divided into two parts. The first part is a survey of some
recent results on nests and the orderability problem. The second part consists
of results, partial results and open questions, all viewed in the light of
nests. From connected LOTS, to products of LOTS and function spaces, up to an
order relat... | math.GN | this chapter is divided into two parts the first part is a survey of some recent results on nests and the orderability problem the second part consists of results partial results and open questions all viewed in the light of nests from connected lots to products of lots and function spaces up to an order relation in th... | [['this', 'chapter', 'is', 'divided', 'into', 'two', 'parts', 'the', 'first', 'part', 'is', 'a', 'survey', 'of', 'some', 'recent', 'results', 'on', 'nests', 'and', 'the', 'orderability', 'problem', 'the', 'second', 'part', 'consists', 'of', 'results', 'partial', 'results', 'and', 'open', 'questions', 'all', 'viewed', '... | [-0.11998348140356238, 0.059295696452819194, -0.013517277070977649, 0.017430552626868375, -0.06283841018763478, -0.014065155904495814, 0.0032478636741393903, 0.3263296124632241, -0.29760434002172753, -0.2744368504366425, 0.15796260752135002, -0.34589079590361627, -0.15779107990751012, 0.2761946837799471, -0.09835047767... |
1,801.00701 | Temperature effect on the electronic structure of the polaronic
excitations within the three-band p-d-Holstein model | In this work we investigate temperature dependence of electronic structure of
system with strong electronic correlations and strong electron-phonon
interaction modeling cuprates in the frameworks of the three-band p-d-Holstein
model by a polaronic version of the generalized tight binding (GTB) method.
Within this app... | cond-mat.str-el | in this work we investigate temperature dependence of electronic structure of system with strong electronic correlations and strong electronphonon interaction modeling cuprates in the frameworks of the threeband pdholstein model by a polaronic version of the generalized tight binding gtb method within this approach the... | [['in', 'this', 'work', 'we', 'investigate', 'temperature', 'dependence', 'of', 'electronic', 'structure', 'of', 'system', 'with', 'strong', 'electronic', 'correlations', 'and', 'strong', 'electronphonon', 'interaction', 'modeling', 'cuprates', 'in', 'the', 'frameworks', 'of', 'the', 'threeband', 'pdholstein', 'model',... | [-0.1451840712772017, 0.19065712618352595, -0.08176145970979373, 0.1107781043299058, 0.023663638799916953, -0.09102247126949285, 0.10875227078317298, 0.3685562989474939, -0.25792320112148964, -0.306027545660202, -0.09756310315216458, -0.31991278648742344, -0.0898471691107261, 0.10674638157070149, 0.08553971292609017, -... |
1,801.00702 | A total uncertainty measure for D numbers based on belief intervals | As a generalization of Dempster-Shafer theory, the theory of D numbers is a
new theoretical framework for uncertainty reasoning. Measuring the uncertainty
of knowledge or information represented by D numbers is an unsolved issue in
that theory. In this paper, inspired by distance based uncertainty measures for
Dempst... | cs.AI | as a generalization of dempstershafer theory the theory of d numbers is a new theoretical framework for uncertainty reasoning measuring the uncertainty of knowledge or information represented by d numbers is an unsolved issue in that theory in this paper inspired by distance based uncertainty measures for dempstershafe... | [['as', 'a', 'generalization', 'of', 'dempstershafer', 'theory', 'the', 'theory', 'of', 'd', 'numbers', 'is', 'a', 'new', 'theoretical', 'framework', 'for', 'uncertainty', 'reasoning', 'measuring', 'the', 'uncertainty', 'of', 'knowledge', 'or', 'information', 'represented', 'by', 'd', 'numbers', 'is', 'an', 'unsolved',... | [-0.1157216090106904, 0.0939191959463495, -0.09548835330313504, 0.13063219650248725, -0.0626727481551393, -0.09096426260422426, 0.09234467752376628, 0.3013399682487502, -0.28340096449046726, -0.3627263912084428, 0.0707954196506321, -0.26228018153948013, -0.1446395085000367, 0.17588868551661796, -0.13769547231589455, 0.... |
1,801.00703 | Variational nonadiabatic dynamics in the moving crude adiabatic
representation: Further merging of nuclear dynamics and electronic structure | A new methodology of simulating nonadiabatic dynamics using frozen-width
Gaussian wavepackets within the moving crude adiabatic representation with the
on-the-fly evaluation of electronic structure is presented. The main feature of
the new approach is elimination of any global or local model representation of
electro... | physics.chem-ph | a new methodology of simulating nonadiabatic dynamics using frozenwidth gaussian wavepackets within the moving crude adiabatic representation with the onthefly evaluation of electronic structure is presented the main feature of the new approach is elimination of any global or local model representation of electronic po... | [['a', 'new', 'methodology', 'of', 'simulating', 'nonadiabatic', 'dynamics', 'using', 'frozenwidth', 'gaussian', 'wavepackets', 'within', 'the', 'moving', 'crude', 'adiabatic', 'representation', 'with', 'the', 'onthefly', 'evaluation', 'of', 'electronic', 'structure', 'is', 'presented', 'the', 'main', 'feature', 'of', ... | [-0.13756346259709004, 0.09556731687927085, -0.11731967351796639, 0.06429130885460238, -0.046132778279952234, -0.12297398900251731, 0.04691416219139791, 0.35181718603610157, -0.2655024025458973, -0.30863770046043437, 0.045057950617901826, -0.2177044851119285, -0.13461903031016667, 0.1434403195899058, 0.0022355377107493... |
1,801.00704 | The role of lattice mismatch on the emergence of surface states in 2D
hybrid perovskite quantum wells | Surface states are ubiquitous to semiconductors and significantly impact the
physical properties and consequently the performance of optoelectronic devices.
Moreover, surface effects are strongly amplified in lower dimensional systems
such as quantum wells and nanostructures. Layered halide perovskites (LHPs) are
2D ... | cond-mat.mtrl-sci | surface states are ubiquitous to semiconductors and significantly impact the physical properties and consequently the performance of optoelectronic devices moreover surface effects are strongly amplified in lower dimensional systems such as quantum wells and nanostructures layered halide perovskites lhps are 2d solutio... | [['surface', 'states', 'are', 'ubiquitous', 'to', 'semiconductors', 'and', 'significantly', 'impact', 'the', 'physical', 'properties', 'and', 'consequently', 'the', 'performance', 'of', 'optoelectronic', 'devices', 'moreover', 'surface', 'effects', 'are', 'strongly', 'amplified', 'in', 'lower', 'dimensional', 'systems'... | [-0.1471549973196391, 0.2047947079247836, 0.006106596041775349, 0.00778838962831962, -0.013486446490593301, -0.15872564278367274, 0.03355361424670584, 0.4303612464968607, -0.30869522157751916, -0.29414045179274473, 0.05369233527827024, -0.28384376720835763, -0.21191943125248705, 0.23335924917545006, -0.0068644200460458... |
1,801.00705 | Non-chiral bosonization of strongly inhomogeneous Luttinger liquids | Non-chiral bosonization (NCBT) is a non-trivial modification of the standard
Fermi-Bose correspondence in one spatial dimensions made in order to facilitate
the study of strongly inhomogeneous Luttinger liquids (LL) where the properties
of free fermions plus the source of inhomogeneities are reproduced exactly. The
f... | cond-mat.str-el | nonchiral bosonization ncbt is a nontrivial modification of the standard fermibose correspondence in one spatial dimensions made in order to facilitate the study of strongly inhomogeneous luttinger liquids ll where the properties of free fermions plus the source of inhomogeneities are reproduced exactly the formalism o... | [['nonchiral', 'bosonization', 'ncbt', 'is', 'a', 'nontrivial', 'modification', 'of', 'the', 'standard', 'fermibose', 'correspondence', 'in', 'one', 'spatial', 'dimensions', 'made', 'in', 'order', 'to', 'facilitate', 'the', 'study', 'of', 'strongly', 'inhomogeneous', 'luttinger', 'liquids', 'll', 'where', 'the', 'prope... | [-0.11243111267377505, 0.1264705429468859, -0.10125633386821048, 0.11928077888850813, -0.04510809431956551, -0.15525766046615996, 2.8059184890462468e-05, 0.333186656187307, -0.21683829954350428, -0.23017475248271266, 0.07315538864619783, -0.3061978950085032, -0.15057708746414408, 0.16518821552749885, 0.0676636818275225... |
1,801.00706 | A new representation of Hankel operators and its spectral consequences | We describe a new representation of Hankel operators $H$ as
pseudo-differential operators $A$ in the space of functions defined on the
whole axis. The amplitudes of such operators $A$ have a very special structure:
they are products of functions of a one variable only. This representation has
numerous spectral conseq... | math.SP math.FA | we describe a new representation of hankel operators h as pseudodifferential operators a in the space of functions defined on the whole axis the amplitudes of such operators a have a very special structure they are products of functions of a one variable only this representation has numerous spectral consequences both ... | [['we', 'describe', 'a', 'new', 'representation', 'of', 'hankel', 'operators', 'h', 'as', 'pseudodifferential', 'operators', 'a', 'in', 'the', 'space', 'of', 'functions', 'defined', 'on', 'the', 'whole', 'axis', 'the', 'amplitudes', 'of', 'such', 'operators', 'a', 'have', 'a', 'very', 'special', 'structure', 'they', 'a... | [-0.14515789096514065, 0.11193492684152818, -0.0792913191553746, 0.11901865381890187, -0.08281539505602972, -0.053241450365843074, -0.0034729955237238637, 0.3884064640489317, -0.26376954213746134, -0.1719444139650272, 0.20336243927651534, -0.28656594288880904, -0.1590528714680864, 0.20088210216753424, -0.02890770295785... |
1,801.00707 | Preliminary RF design of an X-band linac for the EuPRAXIA@SPARC_LAB
project | In the framework of the upgrade of the SPARC_LAB facility at INFN-LNF, named
EuPRAXIA@SPARC_LAB, a high gradient linac is foreseen. One of the most suitable
options is to realize it in X-band. A preliminary design study of both
accelerating structures and power distribution system has been performed. It is
based on 0... | physics.acc-ph | in the framework of the upgrade of the sparc_lab facility at infnlnf named eupraxiasparc_lab a high gradient linac is foreseen one of the most suitable options is to realize it in xband a preliminary design study of both accelerating structures and power distribution system has been performed it is based on 05 m long t... | [['in', 'the', 'framework', 'of', 'the', 'upgrade', 'of', 'the', 'sparc_lab', 'facility', 'at', 'infnlnf', 'named', 'eupraxiasparc_lab', 'a', 'high', 'gradient', 'linac', 'is', 'foreseen', 'one', 'of', 'the', 'most', 'suitable', 'options', 'is', 'to', 'realize', 'it', 'in', 'xband', 'a', 'preliminary', 'design', 'study... | [-0.15385439226255668, 0.1240358704552901, -0.08430270286044106, -0.0007689168308967386, -0.043361456683752214, -0.17734973683995617, -0.04303255374014208, 0.43245376959781756, -0.22716028429170942, -0.28710781543684954, 0.13461073200266005, -0.2332609610404523, -0.016973411897197366, 0.2616053439480972, 0.003773153166... |
1,801.00708 | Restricted Deformable Convolution based Road Scene Semantic Segmentation
Using Surround View Cameras | Understanding the surrounding environment of the vehicle is still one of the
challenges for autonomous driving. This paper addresses 360-degree road scene
semantic segmentation using surround view cameras, which are widely equipped in
existing production cars. First, in order to address large distortion problem
in th... | cs.CV | understanding the surrounding environment of the vehicle is still one of the challenges for autonomous driving this paper addresses 360degree road scene semantic segmentation using surround view cameras which are widely equipped in existing production cars first in order to address large distortion problem in the fishe... | [['understanding', 'the', 'surrounding', 'environment', 'of', 'the', 'vehicle', 'is', 'still', 'one', 'of', 'the', 'challenges', 'for', 'autonomous', 'driving', 'this', 'paper', 'addresses', '360degree', 'road', 'scene', 'semantic', 'segmentation', 'using', 'surround', 'view', 'cameras', 'which', 'are', 'widely', 'equi... | [-0.03553145453417506, -0.03970041497069213, -0.06358942574916218, 0.02333915977485054, -0.11659201004815672, -0.15185157004409208, -0.03881009190111884, 0.455774649927493, -0.29681472707829787, -0.35663529154482093, 0.05628519232662305, -0.2934894170650437, -0.19129800957677787, 0.18841409940177764, -0.206594977796936... |
1,801.00709 | Cluster algebras arising from cluster tubes I: integer vectors | We study cluster algebras arising from cluster tubes. We obtain categorical
interpretations for $g$-vectors, $c$-vectors and denominator vectors for
cluster algebras of type $\mathrm{C}$ with respect to arbitrary initial seeds.
In particular, a denominator theorem has been proved, which enables us to
establish the li... | math.RA math.RT | we study cluster algebras arising from cluster tubes we obtain categorical interpretations for gvectors cvectors and denominator vectors for cluster algebras of type mathrmc with respect to arbitrary initial seeds in particular a denominator theorem has been proved which enables us to establish the linearly independenc... | [['we', 'study', 'cluster', 'algebras', 'arising', 'from', 'cluster', 'tubes', 'we', 'obtain', 'categorical', 'interpretations', 'for', 'gvectors', 'cvectors', 'and', 'denominator', 'vectors', 'for', 'cluster', 'algebras', 'of', 'type', 'mathrmc', 'with', 'respect', 'to', 'arbitrary', 'initial', 'seeds', 'in', 'particu... | [-0.12846846765605732, 0.068282554281177, -0.09743533174041659, 0.06709929379721871, -0.10800157044432127, -0.1092413061138359, 0.06571719111889252, 0.33658388012554497, -0.3184529622667469, -0.2265989721090591, 0.08057632178388303, -0.20117265566568676, -0.08260791490465635, 0.1733874583092984, -0.11086999407270923, -... |
1,801.0071 | Basins of convergence of equilibrium points in the generalized Hill
problem | The Newton-Raphson basins of attraction, associated with the libration points
(attractors), are revealed in the generalized Hill problem. The parametric
variation of the position and the linear stability of the equilibrium points is
determined, when the value of the perturbation parameter $\epsilon$ varies. The
multi... | nlin.CD | the newtonraphson basins of attraction associated with the libration points attractors are revealed in the generalized hill problem the parametric variation of the position and the linear stability of the equilibrium points is determined when the value of the perturbation parameter epsilon varies the multivariate newto... | [['the', 'newtonraphson', 'basins', 'of', 'attraction', 'associated', 'with', 'the', 'libration', 'points', 'attractors', 'are', 'revealed', 'in', 'the', 'generalized', 'hill', 'problem', 'the', 'parametric', 'variation', 'of', 'the', 'position', 'and', 'the', 'linear', 'stability', 'of', 'the', 'equilibrium', 'points'... | [-0.17803838189324214, 0.05344094630905655, -0.10824564146897654, 0.08135663590098248, -0.0014566838652928815, -0.051906760283201986, 0.06789736632584002, 0.28728374913606763, -0.29014953765610274, -0.267678504048364, 0.1339433713625763, -0.29741023645403175, -0.15754252356769394, 0.20001250660951067, -0.02750659158902... |
1,801.00711 | Network-Scale Traffic Modeling and Forecasting with Graphical Lasso and
Neural Networks | Traffic flow forecasting, especially the short-term case, is an important
topic in intelligent transportation systems (ITS). This paper does a lot of
research on network-scale modeling and forecasting of short-term traffic flows.
Firstly, we propose the concepts of single-link and multi-link models of
traffic flow fo... | cs.LG stat.ML | traffic flow forecasting especially the shortterm case is an important topic in intelligent transportation systems its this paper does a lot of research on networkscale modeling and forecasting of shortterm traffic flows firstly we propose the concepts of singlelink and multilink models of traffic flow forecasting seco... | [['traffic', 'flow', 'forecasting', 'especially', 'the', 'shortterm', 'case', 'is', 'an', 'important', 'topic', 'in', 'intelligent', 'transportation', 'systems', 'its', 'this', 'paper', 'does', 'a', 'lot', 'of', 'research', 'on', 'networkscale', 'modeling', 'and', 'forecasting', 'of', 'shortterm', 'traffic', 'flows', '... | [-0.05508841133420598, -0.0025152582807095314, -0.08262703966950842, 0.059641690182966535, -0.1125900692071203, -0.20764690502013158, 0.028815872599807335, 0.4363341418744919, -0.2676730739767663, -0.2763551232953129, 0.12292064996472618, -0.26373735989424557, -0.25057406373040675, 0.21747847747125584, -0.1518477979892... |
1,801.00712 | Multi-Objective Vehicle Routing Problem Applied to Large Scale Post
Office Deliveries | The number of optimization techniques in the combinatorial domain is large
and diversified. Nevertheless, real-world based benchmarks for testing
algorithms are few. This work creates an extensible real-world mail delivery
benchmark to the Vehicle Routing Problem (VRP) in a planar graph embedded in
the 2D Euclidean s... | cs.AI cs.CC | the number of optimization techniques in the combinatorial domain is large and diversified nevertheless realworld based benchmarks for testing algorithms are few this work creates an extensible realworld mail delivery benchmark to the vehicle routing problem vrp in a planar graph embedded in the 2d euclidean space such... | [['the', 'number', 'of', 'optimization', 'techniques', 'in', 'the', 'combinatorial', 'domain', 'is', 'large', 'and', 'diversified', 'nevertheless', 'realworld', 'based', 'benchmarks', 'for', 'testing', 'algorithms', 'are', 'few', 'this', 'work', 'creates', 'an', 'extensible', 'realworld', 'mail', 'delivery', 'benchmark... | [-0.13422582202881414, 0.0008204180050343375, -0.012216409723404594, 0.04263242217586927, -0.09449039635959491, -0.21121401120207564, 0.05288856599720255, 0.4320778623724016, -0.27346179633831946, -0.41819089969560025, 0.14489959920030487, -0.2914742445823566, -0.12568439817636884, 0.25844705945271396, -0.1281340649621... |
1,801.00713 | Nonlinear Parity Readout with a Microwave Photodetector | Robust high-fidelity parity measurment is an important operation in many
applications of quantum computing. In this work we show how in a circuit-QED
architecture, one can measure parity in a single shot at very high contrast by
taking advantage of the nonlinear behavior of a strongly driven microwave
cavity coupled ... | quant-ph | robust highfidelity parity measurment is an important operation in many applications of quantum computing in this work we show how in a circuitqed architecture one can measure parity in a single shot at very high contrast by taking advantage of the nonlinear behavior of a strongly driven microwave cavity coupled to one... | [['robust', 'highfidelity', 'parity', 'measurment', 'is', 'an', 'important', 'operation', 'in', 'many', 'applications', 'of', 'quantum', 'computing', 'in', 'this', 'work', 'we', 'show', 'how', 'in', 'a', 'circuitqed', 'architecture', 'one', 'can', 'measure', 'parity', 'in', 'a', 'single', 'shot', 'at', 'very', 'high', ... | [-0.15628867883765307, 0.1404164879505578, -0.03657831304630487, 0.005911913423640829, -0.03419519309979518, -0.19284599265025096, 0.032474241824967075, 0.39319736084098333, -0.23694532121525808, -0.3063060758670546, 0.06488539574451088, -0.2529554299471326, -0.13712713903595208, 0.23817274372573685, -0.061114300428977... |
1,801.00714 | Exact Exponent for Soft Covering | This work establishes the exact exponents for the soft-covering phenomenon of
a memoryless channel under the total variation metric when random (i.i.d. and
constant-composition) channel codes are used. The exponents, established
herein, are strict improvements in both directions on bounds found in the
literature. Thi... | cs.IT math.IT | this work establishes the exact exponents for the softcovering phenomenon of a memoryless channel under the total variation metric when random iid and constantcomposition channel codes are used the exponents established herein are strict improvements in both directions on bounds found in the literature this complements... | [['this', 'work', 'establishes', 'the', 'exact', 'exponents', 'for', 'the', 'softcovering', 'phenomenon', 'of', 'a', 'memoryless', 'channel', 'under', 'the', 'total', 'variation', 'metric', 'when', 'random', 'iid', 'and', 'constantcomposition', 'channel', 'codes', 'are', 'used', 'the', 'exponents', 'established', 'here... | [-0.16969156995737733, 0.07100671581558396, -0.10054332759910237, 0.1202066730660012, -0.03492447976392877, -0.22614891209561272, 0.1302161133264966, 0.31112436060227944, -0.2471618358280823, -0.2526707748455979, 0.1408297674932787, -0.2434250817364343, -0.15501567285843018, 0.2648627708549611, -0.10831948645656632, 0.... |
1,801.00715 | Charge-based superconducting digital logic family using quantum
phase-slip junctions | Superconducting digital computing systems, primarily involving Josephson
junctions are actively being pursued as high performance and low energy
dissipating alternatives to CMOS-based technologies for petascale and exascale
computers, although several challenges still exist in overcoming barriers to
practically imple... | physics.app-ph cond-mat.supr-con cs.ET | superconducting digital computing systems primarily involving josephson junctions are actively being pursued as high performance and low energy dissipating alternatives to cmosbased technologies for petascale and exascale computers although several challenges still exist in overcoming barriers to practically implement ... | [['superconducting', 'digital', 'computing', 'systems', 'primarily', 'involving', 'josephson', 'junctions', 'are', 'actively', 'being', 'pursued', 'as', 'high', 'performance', 'and', 'low', 'energy', 'dissipating', 'alternatives', 'to', 'cmosbased', 'technologies', 'for', 'petascale', 'and', 'exascale', 'computers', 'a... | [-0.1996990214842795, 0.10743429850900253, 0.015102278765742525, 0.029297027857865032, -0.06293894957475872, -0.25679702906177915, 0.031538482852876325, 0.4213710310868919, -0.2328706221429236, -0.3182640712739984, 0.07911058381344474, -0.23493521670443993, -0.1615557894198873, 0.30306648162800365, -0.06859910469784429... |
1,801.00716 | Computing Hitting Set Kernels By AC^0-Circuits | Given a hypergraph $H = (V,E)$, what is the smallest subset $X \subseteq V$
such that $e \cap X \neq \emptyset$ holds for all $e \in E$? This problem,
known as the hitting set problem, is a basic problem in parameterized
complexity theory. There are well-known kernelization algorithms for it, which
get a hypergraph $... | cs.CC cs.DS | given a hypergraph h ve what is the smallest subset x subseteq v such that e cap x neq emptyset holds for all e in e this problem known as the hitting set problem is a basic problem in parameterized complexity theory there are wellknown kernelization algorithms for it which get a hypergraph h and a number k as input an... | [['given', 'a', 'hypergraph', 'h', 've', 'what', 'is', 'the', 'smallest', 'subset', 'x', 'subseteq', 'v', 'such', 'that', 'e', 'cap', 'x', 'neq', 'emptyset', 'holds', 'for', 'all', 'e', 'in', 'e', 'this', 'problem', 'known', 'as', 'the', 'hitting', 'set', 'problem', 'is', 'a', 'basic', 'problem', 'in', 'parameterized',... | [-0.12030518377392058, 0.1191368389212114, -0.06018233032368902, 0.04131664939697331, -0.0811165593441724, -0.18619630828068884, 0.051960397972169316, 0.39042489296196037, -0.3336383534956779, -0.3043200177168335, 0.07809278234000785, -0.25414236555853625, -0.10570705617866039, 0.16331497952573706, -0.06793637876051353... |
1,801.00717 | Some further validations and comparison of the Bearing Area Model (BAM)
for adhesion of rough surfaces | In the present short note, we attempt further validations and comparisons of
a recent simple model for the estimate for adhesion between elastic (hard)
rough solids with Gaussian multiple scales of roughness, BAM (Bearing Area
Model) belonging to a DMT class of models. In one case, we use the GJP
(Generalized Johnson... | cond-mat.mtrl-sci | in the present short note we attempt further validations and comparisons of a recent simple model for the estimate for adhesion between elastic hard rough solids with gaussian multiple scales of roughness bam bearing area model belonging to a dmt class of models in one case we use the gjp generalized johnson parameter ... | [['in', 'the', 'present', 'short', 'note', 'we', 'attempt', 'further', 'validations', 'and', 'comparisons', 'of', 'a', 'recent', 'simple', 'model', 'for', 'the', 'estimate', 'for', 'adhesion', 'between', 'elastic', 'hard', 'rough', 'solids', 'with', 'gaussian', 'multiple', 'scales', 'of', 'roughness', 'bam', 'bearing',... | [-0.059695523135706335, 0.031494217675152376, -0.09401366217599179, 0.0759956315647349, -0.0591815491923346, -0.17431671255562678, 0.07829916410040684, 0.3774700297010887, -0.22919667830280802, -0.30835887125860423, 0.07732986690154156, -0.287856367090319, -0.1873707396747409, 0.22128780815814042, -0.0755546920431348, ... |
1,801.00718 | Selective review of offline change point detection methods | This article presents a selective survey of algorithms for the offline
detection of multiple change points in multivariate time series. A general yet
structuring methodological strategy is adopted to organize this vast body of
work. More precisely, detection algorithms considered in this review are
characterized by t... | cs.CE stat.CO stat.ME | this article presents a selective survey of algorithms for the offline detection of multiple change points in multivariate time series a general yet structuring methodological strategy is adopted to organize this vast body of work more precisely detection algorithms considered in this review are characterized by three ... | [['this', 'article', 'presents', 'a', 'selective', 'survey', 'of', 'algorithms', 'for', 'the', 'offline', 'detection', 'of', 'multiple', 'change', 'points', 'in', 'multivariate', 'time', 'series', 'a', 'general', 'yet', 'structuring', 'methodological', 'strategy', 'is', 'adopted', 'to', 'organize', 'this', 'vast', 'bod... | [-0.13495183843475755, 0.04847450125334638, -0.06933225317219838, 0.04438330412821405, -0.059770599258749675, -0.1345733805360754, 0.04432432855782884, 0.37913693516421015, -0.25331097019292165, -0.29420778613663123, 0.10371568145131002, -0.22349623392932536, -0.1793934819864088, 0.1974991241841462, -0.0887586703194368... |
1,801.00719 | Lattice model constructions for gapless domain walls between topological
phases | Domain walls between different topological phases are one of the most
interesting phenomena that reveal the non-trivial bulk properties of
topological phases. Very recently, gapped domain walls between different
topological phases have been intensively studied. In this paper, we
systematically construct a large class... | cond-mat.str-el | domain walls between different topological phases are one of the most interesting phenomena that reveal the nontrivial bulk properties of topological phases very recently gapped domain walls between different topological phases have been intensively studied in this paper we systematically construct a large class of lat... | [['domain', 'walls', 'between', 'different', 'topological', 'phases', 'are', 'one', 'of', 'the', 'most', 'interesting', 'phenomena', 'that', 'reveal', 'the', 'nontrivial', 'bulk', 'properties', 'of', 'topological', 'phases', 'very', 'recently', 'gapped', 'domain', 'walls', 'between', 'different', 'topological', 'phases... | [-0.17058806896520157, 0.19797409156958262, -0.1046682701818645, 0.048394301598115516, -0.13121604940543571, -0.16323539371602236, 0.025099973687902094, 0.4127366794149081, -0.25566708914081876, -0.2789684147760272, 0.09315367473289371, -0.20537939883458117, -0.19230873619671912, 0.1359270254150033, -0.0187087612055862... |
1,801.0072 | Non-grey dimming events of KIC 8462852 from GTC spectrophotometry | We report ground-based spectrophotometry of KIC 8462852, during its first
dimming events since the end of the Kepler mission. The dimmings show a clear
colour-signature, and are deeper in visual blue wavelengths than in red ones.
The flux loss' wavelength dependency can be described with an \AA ngstr\"om
absorption c... | astro-ph.SR astro-ph.EP | we report groundbased spectrophotometry of kic 8462852 during its first dimming events since the end of the kepler mission the dimmings show a clear coloursignature and are deeper in visual blue wavelengths than in red ones the flux loss wavelength dependency can be described with an aa ngstrom absorption coefficient o... | [['we', 'report', 'groundbased', 'spectrophotometry', 'of', 'kic', '8462852', 'during', 'its', 'first', 'dimming', 'events', 'since', 'the', 'end', 'of', 'the', 'kepler', 'mission', 'the', 'dimmings', 'show', 'a', 'clear', 'coloursignature', 'and', 'are', 'deeper', 'in', 'visual', 'blue', 'wavelengths', 'than', 'in', '... | [-0.03366304748396942, 0.23349551250350942, -0.0846108565092436, 0.08522800553691923, -0.09500279507483356, -0.10231354558345629, 0.0139939518776373, 0.47411506598291453, -0.17086272587562235, -0.3434658903206582, 0.06780324678857141, -0.34661301848245785, -0.04440770768269431, 0.20733954936895316, -0.13644561445107684... |
1,801.00721 | A crossing lemma for multigraphs | Let $G$ be a drawing of a graph with $n$ vertices and $e>4n$ edges, in which
no two adjacent edges cross and any pair of independent edges cross at most
once. According to the celebrated Crossing Lemma of Ajtai, Chv\'atal, Newborn,
Szemer\'edi and Leighton, the number of crossings in $G$ is at least
$c{e^3\over n^2}$... | math.CO | let g be a drawing of a graph with n vertices and e4n edges in which no two adjacent edges cross and any pair of independent edges cross at most once according to the celebrated crossing lemma of ajtai chvatal newborn szemeredi and leighton the number of crossings in g is at least ce3over n2 for a suitable constant c0 ... | [['let', 'g', 'be', 'a', 'drawing', 'of', 'a', 'graph', 'with', 'n', 'vertices', 'and', 'e4n', 'edges', 'in', 'which', 'no', 'two', 'adjacent', 'edges', 'cross', 'and', 'any', 'pair', 'of', 'independent', 'edges', 'cross', 'at', 'most', 'once', 'according', 'to', 'the', 'celebrated', 'crossing', 'lemma', 'of', 'ajtai',... | [-0.1946143373284194, 0.13042571789825003, -0.060684616509958995, 0.003481384400251529, -0.06432143281542248, -0.17094534633868783, 0.07335948369804127, 0.2881364597195237, -0.2161034412167819, -0.3516960602602084, 0.03827456042351429, -0.3477282386236295, -0.08996757794767886, 0.10914024750521178, -0.09261903042315418... |
1,801.00722 | Bases for Kumjian-Pask algebras over standard $k$-graphs | For any Kumjian-Pask algebra $KP_R(\Lambda)$ defined over a $k$-graph
$\Lambda$ of a special kind (a "standard $k$-graph"), we obtain an $R$-basis.
| math.KT | for any kumjianpask algebra kp_rlambda defined over a kgraph lambda of a special kind a standard kgraph we obtain an rbasis | [['for', 'any', 'kumjianpask', 'algebra', 'kp_rlambda', 'defined', 'over', 'a', 'kgraph', 'lambda', 'of', 'a', 'special', 'kind', 'a', 'standard', 'kgraph', 'we', 'obtain', 'an', 'rbasis']] | [-0.20207267294504813, 0.04133910919231961, -0.04323828056277264, 0.05560009350024518, -0.1699876726738044, -0.15131094255706384, -0.041844524398800875, 0.3820361463086946, -0.3548243839648508, -0.13674929203642977, 0.0653883800398381, -0.19065203696178892, -0.08764008592282023, 0.21050891133823565, -0.1310272498411082... |
1,801.00723 | Deep Learning for Identifying Potential Conceptual Shifts for
Co-creative Drawing | We present a system for identifying conceptual shifts between visual
categories, which will form the basis for a co-creative drawing system to help
users draw more creative sketches. The system recognizes human sketches and
matches them to structurally similar sketches from categories to which they do
not belong. Thi... | cs.LG cs.AI stat.ML | we present a system for identifying conceptual shifts between visual categories which will form the basis for a cocreative drawing system to help users draw more creative sketches the system recognizes human sketches and matches them to structurally similar sketches from categories to which they do not belong this woul... | [['we', 'present', 'a', 'system', 'for', 'identifying', 'conceptual', 'shifts', 'between', 'visual', 'categories', 'which', 'will', 'form', 'the', 'basis', 'for', 'a', 'cocreative', 'drawing', 'system', 'to', 'help', 'users', 'draw', 'more', 'creative', 'sketches', 'the', 'system', 'recognizes', 'human', 'sketches', 'a... | [-0.042993203967908455, 0.012805216303880143, -0.15435366500451259, 0.09989316869971597, -0.17056579707246838, -0.2097731720035275, 0.05911549200325019, 0.43336309481299284, -0.2648953094260033, -0.30935335111324536, 0.02494802663921181, -0.3103188316648205, -0.18032713488421656, 0.19133377528333134, -0.213798947223095... |
1,801.00724 | Subdifferential formulae for the supremum of an arbitrary family of
functions | This work provides calculus for the Fr\'echet and limiting subdifferential of
the pointwise supremum given by an arbitrary family of lower semicontinuous
functions. We start our study showing fuzzy results about the Fr\'echet
subdifferential of the supremum function. Posteriorly, we study in finite- and
infinite-dime... | math.OC | this work provides calculus for the frechet and limiting subdifferential of the pointwise supremum given by an arbitrary family of lower semicontinuous functions we start our study showing fuzzy results about the frechet subdifferential of the supremum function posteriorly we study in finite and infinitedimensional set... | [['this', 'work', 'provides', 'calculus', 'for', 'the', 'frechet', 'and', 'limiting', 'subdifferential', 'of', 'the', 'pointwise', 'supremum', 'given', 'by', 'an', 'arbitrary', 'family', 'of', 'lower', 'semicontinuous', 'functions', 'we', 'start', 'our', 'study', 'showing', 'fuzzy', 'results', 'about', 'the', 'frechet'... | [-0.058503912505693735, -0.004527538602178538, -0.0801783840666758, 0.12194118755141972, -0.09187811154406518, -0.005276424973271787, 0.07059092149720528, 0.3732780137099326, -0.30320125505677425, -0.1572701835364569, 0.11344363016978605, -0.27752267067553477, -0.17793889426393433, 0.20935284391744063, -0.1617127554112... |
1,801.00725 | Semantic Modeling with Foundries | We analyze challenges for the development of the Human Activities and
Infrastructures Foundry. We explore a rich semantic modeling approach to
describe two Korean ceramic water droppers used to mix ink for calligraphy, how
they were produced and the reasons for their differing aesthetic. Our modeling
supports schema ... | cs.DL | we analyze challenges for the development of the human activities and infrastructures foundry we explore a rich semantic modeling approach to describe two korean ceramic water droppers used to mix ink for calligraphy how they were produced and the reasons for their differing aesthetic our modeling supports schema and a... | [['we', 'analyze', 'challenges', 'for', 'the', 'development', 'of', 'the', 'human', 'activities', 'and', 'infrastructures', 'foundry', 'we', 'explore', 'a', 'rich', 'semantic', 'modeling', 'approach', 'to', 'describe', 'two', 'korean', 'ceramic', 'water', 'droppers', 'used', 'to', 'mix', 'ink', 'for', 'calligraphy', 'h... | [-0.04759001838309424, 0.03946737224211941, -0.09485316085447738, 0.10121974551539215, -0.13669328352847657, -0.1256115354912041, 0.05859507241758046, 0.4614690070512233, -0.2457879614689714, -0.3607197094031356, 0.06173593723275638, -0.31145771956029683, -0.17131356285376984, 0.17253285133077267, -0.07574425358929998,... |
1,801.00726 | Forcing Brushes | We give short and simple proofs of the inequalities $B(G)\leq Z(L(G))$ and
$Z(G)\leq Z(L(G))$ first established by Erzurumluo\u{g}lu, Meagher, and Pike,
where $G$ is a graph without isolated vertices, $B(G)$ is the brushing number
of $G$, $Z(G)$ is the zero forcing number of $G$, and $L(G)$ is the line graph
of $G$.
| math.CO | we give short and simple proofs of the inequalities bgleq zlg and zgleq zlg first established by erzurumluouglu meagher and pike where g is a graph without isolated vertices bg is the brushing number of g zg is the zero forcing number of g and lg is the line graph of g | [['we', 'give', 'short', 'and', 'simple', 'proofs', 'of', 'the', 'inequalities', 'bgleq', 'zlg', 'and', 'zgleq', 'zlg', 'first', 'established', 'by', 'erzurumluouglu', 'meagher', 'and', 'pike', 'where', 'g', 'is', 'a', 'graph', 'without', 'isolated', 'vertices', 'bg', 'is', 'the', 'brushing', 'number', 'of', 'g', 'zg',... | [-0.22073698928922086, 0.12642726848157598, -0.07566085227938625, 0.006216831687910884, -0.14860356545221864, -0.15563332664725535, 0.046623621688352206, 0.3369857015124723, -0.19240776737969295, -0.3298098735292168, 0.06566945219631581, -0.28514663997453216, -0.10254883853828206, 0.13995136214675857, -0.11548762686331... |
1,801.00727 | Accounting for hidden common causes when inferring cause and effect from
observational data | Identifying causal relationships from observation data is difficult, in large
part, due to the presence of hidden common causes. In some cases, where just
the right patterns of conditional independence and dependence lie in the
data---for example, Y-structures---it is possible to identify cause and effect.
In other c... | cs.AI stat.AP | identifying causal relationships from observation data is difficult in large part due to the presence of hidden common causes in some cases where just the right patterns of conditional independence and dependence lie in the datafor example ystructuresit is possible to identify cause and effect in other cases the analys... | [['identifying', 'causal', 'relationships', 'from', 'observation', 'data', 'is', 'difficult', 'in', 'large', 'part', 'due', 'to', 'the', 'presence', 'of', 'hidden', 'common', 'causes', 'in', 'some', 'cases', 'where', 'just', 'the', 'right', 'patterns', 'of', 'conditional', 'independence', 'and', 'dependence', 'lie', 'i... | [-0.10495480933187014, 0.11777599953115606, -0.04299912718620072, 0.14964377526392011, -0.17310391857903054, -0.1715607459538002, 0.07739392628687672, 0.36146336673025753, -0.2979114650837839, -0.3255201748255244, 0.12695405804898907, -0.28986763452833636, -0.19349832281945867, 0.1403380681418794, -0.0952407982933553, ... |
1,801.00728 | Integration of quadratic Lie algebroids to Riemannian Cartan-Lie
groupoids | Cartan-Lie algebroids, i.e. Lie algebroids equipped with a compatible
connection, permit the definition of an adjoint representation, on the fiber as
well as on the tangent of the base. We call (positive) quadratic Lie
algebroids, Cartan-Lie algebroids with ad-invariant (Riemannian) metrics on
their fibers and base $... | math.DG | cartanlie algebroids ie lie algebroids equipped with a compatible connection permit the definition of an adjoint representation on the fiber as well as on the tangent of the base we call positive quadratic lie algebroids cartanlie algebroids with adinvariant riemannian metrics on their fibers and base kappa and g respe... | [['cartanlie', 'algebroids', 'ie', 'lie', 'algebroids', 'equipped', 'with', 'a', 'compatible', 'connection', 'permit', 'the', 'definition', 'of', 'an', 'adjoint', 'representation', 'on', 'the', 'fiber', 'as', 'well', 'as', 'on', 'the', 'tangent', 'of', 'the', 'base', 'we', 'call', 'positive', 'quadratic', 'lie', 'algeb... | [-0.23452193432304763, 0.03148444628065004, -0.05830928068782124, 0.07844842238804307, -0.24644546764119415, -0.1608940629314666, 0.010270418061779063, 0.44860653008256, -0.320116308532986, -0.19316530194586126, 0.08925328773193966, -0.2467443915171044, -0.2011651791910702, 0.1778156038528204, -0.1742288791694217, -0.0... |
1,801.00729 | Surface plasmons in a semi-bounded massless Dirac plasma | The collective excitation of surface plasmons in a massless Dirac plasma
(e.g., graphene) half-space (bounded by air) is investigated using a
relativistic quantum fluid model. The unique features of such surface waves are
discussed and compared with those in a Fermi plasma. It is found that in
contrast to Fermi plasm... | physics.plasm-ph | the collective excitation of surface plasmons in a massless dirac plasma eg graphene halfspace bounded by air is investigated using a relativistic quantum fluid model the unique features of such surface waves are discussed and compared with those in a fermi plasma it is found that in contrast to fermi plasmas the longw... | [['the', 'collective', 'excitation', 'of', 'surface', 'plasmons', 'in', 'a', 'massless', 'dirac', 'plasma', 'eg', 'graphene', 'halfspace', 'bounded', 'by', 'air', 'is', 'investigated', 'using', 'a', 'relativistic', 'quantum', 'fluid', 'model', 'the', 'unique', 'features', 'of', 'such', 'surface', 'waves', 'are', 'discu... | [-0.1474333364828253, 0.2804148812932199, -0.05812516610406465, 0.10107277337288073, -0.039371130159282584, -0.14554811745755752, -0.02272945626686185, 0.36688653084496825, -0.1922400329356729, -0.24989237313521867, -0.047542034871817046, -0.33397164502796733, -0.1551129338923463, 0.23948974912627047, 0.016221826964144... |
1,801.0073 | Mass deformations of 5d SCFTs via holography | Using six-dimensional Euclidean $F(4)$ gauged supergravity we construct a
holographic renormalization group flow for a CFT on $S^5$. Numerical solutions
to the BPS equations are obtained and the free energy of the theory on $S^5$ is
determined holographically by calculation of the renormalized on-shell
supergravity a... | hep-th | using sixdimensional euclidean f4 gauged supergravity we construct a holographic renormalization group flow for a cft on s5 numerical solutions to the bps equations are obtained and the free energy of the theory on s5 is determined holographically by calculation of the renormalized onshell supergravity action in the pr... | [['using', 'sixdimensional', 'euclidean', 'f4', 'gauged', 'supergravity', 'we', 'construct', 'a', 'holographic', 'renormalization', 'group', 'flow', 'for', 'a', 'cft', 'on', 's5', 'numerical', 'solutions', 'to', 'the', 'bps', 'equations', 'are', 'obtained', 'and', 'the', 'free', 'energy', 'of', 'the', 'theory', 'on', '... | [-0.11251883305875318, 0.15327911170066466, -0.10346374478789845, 0.08785532312183153, -0.061890782903563896, -0.12400022930399116, -0.014522248827519693, 0.3092499381396919, -0.17265163674684508, -0.25653216882741875, 0.07479811882949434, -0.2785295356065035, -0.14715809574616806, 0.09347197323305799, -0.0759637214941... |
1,801.00731 | Tuning Nanocrystal Surface Depletion by Controlling Dopant Distribution
as a Route Toward Enhanced Film Conductivity | Electron conduction through bare metal oxide nanocrystal (NC) films is
hindered by surface depletion regions resulting from the presence of surface
states. We control the radial dopant distribution in tin-doped indium oxide
(ITO) NCs as a means to manipulate the NC depletion width. We find in films of
ITO NCs of equa... | cond-mat.mes-hall cond-mat.mtrl-sci | electron conduction through bare metal oxide nanocrystal nc films is hindered by surface depletion regions resulting from the presence of surface states we control the radial dopant distribution in tindoped indium oxide ito ncs as a means to manipulate the nc depletion width we find in films of ito ncs of equal overall... | [['electron', 'conduction', 'through', 'bare', 'metal', 'oxide', 'nanocrystal', 'nc', 'films', 'is', 'hindered', 'by', 'surface', 'depletion', 'regions', 'resulting', 'from', 'the', 'presence', 'of', 'surface', 'states', 'we', 'control', 'the', 'radial', 'dopant', 'distribution', 'in', 'tindoped', 'indium', 'oxide', 'i... | [-0.07705734694524924, 0.23932281319272294, 0.017521703866140177, -0.015207163042887065, 0.07619689162620293, -0.17903982863388454, 0.09366396756001538, 0.4617295386369831, -0.21517709435855029, -0.3306489156418911, -0.03798923712653754, -0.3616380329439116, -0.05258729431267467, 0.14962212606182984, -0.042199932033307... |
1,801.00732 | The First Post-Kepler Brightness Dips of KIC 8462852 | We present a photometric detection of the first brightness dips of the unique
variable star KIC 8462852 since the end of the Kepler space mission in 2013
May. Our regular photometric surveillance started in October 2015, and a
sequence of dipping began in 2017 May continuing on through the end of 2017,
when the star ... | astro-ph.SR astro-ph.EP | we present a photometric detection of the first brightness dips of the unique variable star kic 8462852 since the end of the kepler space mission in 2013 may our regular photometric surveillance started in october 2015 and a sequence of dipping began in 2017 may continuing on through the end of 2017 when the star was n... | [['we', 'present', 'a', 'photometric', 'detection', 'of', 'the', 'first', 'brightness', 'dips', 'of', 'the', 'unique', 'variable', 'star', 'kic', '8462852', 'since', 'the', 'end', 'of', 'the', 'kepler', 'space', 'mission', 'in', '2013', 'may', 'our', 'regular', 'photometric', 'surveillance', 'started', 'in', 'october',... | [-0.06569961843483929, 0.1503477287569242, -0.12338214514392488, 0.06286654558786736, -0.10984594976548012, -0.11289851388439943, 0.04690556560523706, 0.41814704922338325, -0.2125934603037915, -0.35934585281439235, 0.14015348087700863, -0.2877979813681091, -0.09273506808242371, 0.214494776826894, -0.1343329763955052, -... |
1,801.00733 | The bicanonical map of the Cartwright-Steger surface | We prove that the bicanonical map of the Cartwright-Steger surface is an
embedding. We also discuss two minimal surfaces of general type, both covered
by the Cartwright-Steger surface. One has $K^2=2$, $p_g=1$, $\pi_1=\{1\}$ and
the other has $K^2=1$, $p_g=0$, $\pi_1=\mathbb{Z}/2\mathbb{Z}$.
| math.AG | we prove that the bicanonical map of the cartwrightsteger surface is an embedding we also discuss two minimal surfaces of general type both covered by the cartwrightsteger surface one has k22 p_g1 pi_11 and the other has k21 p_g0 pi_1mathbbz2mathbbz | [['we', 'prove', 'that', 'the', 'bicanonical', 'map', 'of', 'the', 'cartwrightsteger', 'surface', 'is', 'an', 'embedding', 'we', 'also', 'discuss', 'two', 'minimal', 'surfaces', 'of', 'general', 'type', 'both', 'covered', 'by', 'the', 'cartwrightsteger', 'surface', 'one', 'has', 'k22', 'p_g1', 'pi_11', 'and', 'the', 'o... | [-0.15917860451154411, 0.05406551388186927, -0.06644527031457984, 0.08013516605424229, -0.06641011931933463, -0.21733410339802503, -0.049240079754963514, 0.35253863750258463, -0.25187425505137073, -0.19033709302020724, 0.12876031163614243, -0.33864655762445184, -0.19021327188238502, 0.23377636652439832, -0.170080746524... |
1,801.00734 | Complexity Theory, Game Theory, and Economics: The Barbados Lectures | This document collects the lecture notes from my mini-course "Complexity
Theory, Game Theory, and Economics," taught at the Bellairs Research Institute
of McGill University, Holetown, Barbados, February 19--23, 2017, as the 29th
McGill Invitational Workshop on Computational Complexity.
The goal of this mini-course ... | cs.CC cs.GT econ.EM | this document collects the lecture notes from my minicourse complexity theory game theory and economics taught at the bellairs research institute of mcgill university holetown barbados february 1923 2017 as the 29th mcgill invitational workshop on computational complexity the goal of this minicourse is twofold i to exp... | [['this', 'document', 'collects', 'the', 'lecture', 'notes', 'from', 'my', 'minicourse', 'complexity', 'theory', 'game', 'theory', 'and', 'economics', 'taught', 'at', 'the', 'bellairs', 'research', 'institute', 'of', 'mcgill', 'university', 'holetown', 'barbados', 'february', '1923', '2017', 'as', 'the', '29th', 'mcgil... | [-0.03132346028289875, 0.08278155255624477, -0.14559861215050607, 0.08257539554679093, -0.1002038207703403, -0.13887817270568564, 0.025450941312181598, 0.25524584942951234, -0.216069635520337, -0.3956001838121344, 0.12233733755493333, -0.32098903816913354, -0.23609325565992534, 0.16254384946391112, -0.2298485336770468,... |
1,801.00735 | Filtered finiteness of the image of the unstable Hurewicz homomorphism
with applications to bordism of immersions | After recent work of Hill, Hopkins, and Ravenel on the Kervaire invariant one
problem, as well as Adams' solution of the Hopf invariant one problem, an
immediate consequence of Curtis conjecture is that the set of spherical classes
in $H_*Q_0S^0$ is finite. Similarly, Eccles conjecture, when specialised to
$X=S^n$ wi... | math.AT | after recent work of hill hopkins and ravenel on the kervaire invariant one problem as well as adams solution of the hopf invariant one problem an immediate consequence of curtis conjecture is that the set of spherical classes in h_q_0s0 is finite similarly eccles conjecture when specialised to xsn with n0 together wit... | [['after', 'recent', 'work', 'of', 'hill', 'hopkins', 'and', 'ravenel', 'on', 'the', 'kervaire', 'invariant', 'one', 'problem', 'as', 'well', 'as', 'adams', 'solution', 'of', 'the', 'hopf', 'invariant', 'one', 'problem', 'an', 'immediate', 'consequence', 'of', 'curtis', 'conjecture', 'is', 'that', 'the', 'set', 'of', '... | [-0.16166551241174584, 0.1021373978973926, -0.09255240229723599, 0.043792446769179316, -0.06138632012784761, -0.14155422070417817, -0.0096016482858888, 0.35358390863547584, -0.2780531452632041, -0.2470999914038371, 0.12167252585654773, -0.2553766069719524, -0.13183930568602548, 0.17958499385183896, -0.12183545890019358... |
1,801.00736 | Variable selection in Functional Additive Regression Models | This paper considers the problem of variable selection in regression models
in the case of functional variables that may be mixed with other type of
variables (scalar, multivariate, directional, etc.). Our proposal begins with a
simple null model and sequentially selects a new variable to be incorporated
into the mod... | stat.ME stat.AP stat.CO | this paper considers the problem of variable selection in regression models in the case of functional variables that may be mixed with other type of variables scalar multivariate directional etc our proposal begins with a simple null model and sequentially selects a new variable to be incorporated into the model based ... | [['this', 'paper', 'considers', 'the', 'problem', 'of', 'variable', 'selection', 'in', 'regression', 'models', 'in', 'the', 'case', 'of', 'functional', 'variables', 'that', 'may', 'be', 'mixed', 'with', 'other', 'type', 'of', 'variables', 'scalar', 'multivariate', 'directional', 'etc', 'our', 'proposal', 'begins', 'wit... | [-0.05396929108376366, 0.027144462001592953, -0.10109348026320965, 0.04405104026306734, -0.1149186715760296, -0.1901284027568037, 0.05597713185096215, 0.3551041111165639, -0.27660996422614204, -0.2632081897717227, 0.09851346196984817, -0.2275882543129201, -0.1795993121433081, 0.19327096045847134, -0.08929207532823381, ... |
1,801.00737 | Even cycle creating paths | We say that two graphs $H_1,H_2$ on the same vertex set are $G$-creating
($G$-different in other papers, this difference is explained in the
introduction) if the union of the two graphs contains $G$ as a subgraph. Let
$H(n,k)$ be the maximal number of pairwise $C_k$-creating paths (of arbitrary
length) on $n$ vertice... | math.CO | we say that two graphs h_1h_2 on the same vertex set are gcreating gdifferent in other papers this difference is explained in the introduction if the union of the two graphs contains g as a subgraph let hnk be the maximal number of pairwise c_kcreating paths of arbitrary length on n vertices the behaviour of hn2k1 is m... | [['we', 'say', 'that', 'two', 'graphs', 'h_1h_2', 'on', 'the', 'same', 'vertex', 'set', 'are', 'gcreating', 'gdifferent', 'in', 'other', 'papers', 'this', 'difference', 'is', 'explained', 'in', 'the', 'introduction', 'if', 'the', 'union', 'of', 'the', 'two', 'graphs', 'contains', 'g', 'as', 'a', 'subgraph', 'let', 'hnk... | [-0.1517065937353417, 0.15885215173291223, -0.036380338324035734, 0.04483338929415542, -0.062411031777415665, -0.17787294314946345, 0.04142662594599545, 0.33805699019687885, -0.20447376547653742, -0.2978210565490101, 0.07201442982880102, -0.3306556883332458, -0.10360238351363768, 0.1900976144289474, -0.0760590921111523... |
1,801.00738 | The hidden depths of planetary atmospheres | Atmospheric regions below a refractive boundary are hidden in limb
observations. Refraction thus creates a gray continuum in the planet's
transmission spectrum which can hide spectral features associated with sources
of atmospheric opacity. We combine refractive theory with recent analytical
advances describing the e... | astro-ph.EP | atmospheric regions below a refractive boundary are hidden in limb observations refraction thus creates a gray continuum in the planets transmission spectrum which can hide spectral features associated with sources of atmospheric opacity we combine refractive theory with recent analytical advances describing the effect... | [['atmospheric', 'regions', 'below', 'a', 'refractive', 'boundary', 'are', 'hidden', 'in', 'limb', 'observations', 'refraction', 'thus', 'creates', 'a', 'gray', 'continuum', 'in', 'the', 'planets', 'transmission', 'spectrum', 'which', 'can', 'hide', 'spectral', 'features', 'associated', 'with', 'sources', 'of', 'atmosp... | [-0.06326730169984512, 0.16719173965416848, -0.05819695046171546, 0.0852134204916656, -0.10815478495135904, -0.07605050966423005, 0.05353402907121926, 0.3955525428876281, -0.2043917343020439, -0.3704217566549778, 0.09708005166286603, -0.28759351429069646, -0.11856499989656731, 0.18358315342571585, -0.07500071366131306,... |
1,801.00739 | Log canonical pairs over varieties with maximal Albanese dimension | Let $(X,B)$ be a log canonical pair over a normal variety $Z$ with maximal
Albanese dimension. If $K_X+B$ is relatively abundant over $Z$ (for example,
$K_X+B$ is relatively big over $Z$), then we prove that $K_X+B$ is abundant. In
particular, the subadditvity of Kodaira dimensions $\kappa(K_X+B) \geq
\kappa(K_F+B_F)... | math.AG | let xb be a log canonical pair over a normal variety z with maximal albanese dimension if k_xb is relatively abundant over z for example k_xb is relatively big over z then we prove that k_xb is abundant in particular the subadditvity of kodaira dimensions kappak_xb geq kappak_fb_f kappaz holds where f is a general fibe... | [['let', 'xb', 'be', 'a', 'log', 'canonical', 'pair', 'over', 'a', 'normal', 'variety', 'z', 'with', 'maximal', 'albanese', 'dimension', 'if', 'k_xb', 'is', 'relatively', 'abundant', 'over', 'z', 'for', 'example', 'k_xb', 'is', 'relatively', 'big', 'over', 'z', 'then', 'we', 'prove', 'that', 'k_xb', 'is', 'abundant', '... | [-0.16322414293972543, 0.08204094171726509, -0.05519989050884286, 0.09172847232168904, 0.0012383328107914524, -0.22314464881429044, -0.00020042161011825436, 0.3443844316061586, -0.24841556228373363, -0.17943711047384725, 0.05939356242837992, -0.28864850535857206, -0.1206923286764599, 0.2580544479980903, -0.096151192905... |
1,801.0074 | Halley's Wind: Reappraising a Centuries Old Theory for the Trade Winds | The astronomical work of Edmond Halley (1656-1742) during the latter half of
the Copernican Revolution contributed substantially to the scientific proof and
widespread acceptance of heliocentrism. Perhaps the most well-known example is
his prediction of the return of the comet named in his honor. Halley is also
known... | physics.hist-ph physics.ao-ph | the astronomical work of edmond halley 16561742 during the latter half of the copernican revolution contributed substantially to the scientific proof and widespread acceptance of heliocentrism perhaps the most wellknown example is his prediction of the return of the comet named in his honor halley is also known for off... | [['the', 'astronomical', 'work', 'of', 'edmond', 'halley', '16561742', 'during', 'the', 'latter', 'half', 'of', 'the', 'copernican', 'revolution', 'contributed', 'substantially', 'to', 'the', 'scientific', 'proof', 'and', 'widespread', 'acceptance', 'of', 'heliocentrism', 'perhaps', 'the', 'most', 'wellknown', 'example... | [-0.07496901371816904, 0.09468779576099787, -0.11759644961485616, 0.09980938021208549, -0.09612982955472425, -0.07856219072230868, 0.039851207103391614, 0.24631728946313827, -0.22662978177621984, -0.33632499295510826, 0.13491700557458414, -0.2618701346896447, -0.13187537287491596, 0.1978207682421478, -0.161993583863235... |
1,801.00741 | Mixed Boundary Value Problems for non-Divergence Type Elliptic Equations
in Unbounded Domain | We investigate the qualitative properties of solution to the Zaremba type
problem in unbounded domain for the non-divergence elliptic equation with
possible degeneration at infinity. The main result is Phragm\'en-Lindel\"of
type principle on growth/decay of a solution at infinity depending on both the
structure of th... | math.AP | we investigate the qualitative properties of solution to the zaremba type problem in unbounded domain for the nondivergence elliptic equation with possible degeneration at infinity the main result is phragmenlindelof type principle on growthdecay of a solution at infinity depending on both the structure of the neumann ... | [['we', 'investigate', 'the', 'qualitative', 'properties', 'of', 'solution', 'to', 'the', 'zaremba', 'type', 'problem', 'in', 'unbounded', 'domain', 'for', 'the', 'nondivergence', 'elliptic', 'equation', 'with', 'possible', 'degeneration', 'at', 'infinity', 'the', 'main', 'result', 'is', 'phragmenlindelof', 'type', 'pr... | [-0.15419408300270637, 0.027707578976535134, -0.0776833907287154, 0.013756273689472841, -0.12298045230822431, -0.092524218869706, 0.014966784656927403, 0.25538073955621154, -0.33357490019665825, -0.21822138525959517, 0.18283843028022803, -0.2741629866676198, -0.05873847644672626, 0.1590652058625387, -0.1131123405726005... |
1,801.00742 | Large Flocks of Small Birds: On the Minimal Size of Population Protocols | Population protocols are a well established model of distributed computation
by mobile finite-state agents with very limited storage. A classical result
establishes that population protocols compute exactly predicates definable in
Presburger arithmetic. We initiate the study of the minimal amount of memory
required t... | cs.DC cs.CC | population protocols are a well established model of distributed computation by mobile finitestate agents with very limited storage a classical result establishes that population protocols compute exactly predicates definable in presburger arithmetic we initiate the study of the minimal amount of memory required to com... | [['population', 'protocols', 'are', 'a', 'well', 'established', 'model', 'of', 'distributed', 'computation', 'by', 'mobile', 'finitestate', 'agents', 'with', 'very', 'limited', 'storage', 'a', 'classical', 'result', 'establishes', 'that', 'population', 'protocols', 'compute', 'exactly', 'predicates', 'definable', 'in',... | [-0.18404095484008795, 0.12217506821097647, -0.04503634122250847, 0.07915152539318615, -0.007658092976482802, -0.19748166424597707, 0.11992573075997282, 0.3607304785725509, -0.2845556202900502, -0.32050958786939465, 0.07121882507804954, -0.24668915120725946, -0.08825446059746855, 0.20983679896191687, -0.100921230235221... |
1,801.00743 | Um Sistema Multiagente no Combate ao Braqueamento de Capitais | Money laundering is a crime that makes it possible to finance other crimes,
for this reason, it is important for criminal organizations and their combat is
prioritized by nations around the world. The anti-money laundering process has
not evolved as expected because it has prioritized only the signaling of
suspicious... | cs.MA cs.AI | money laundering is a crime that makes it possible to finance other crimes for this reason it is important for criminal organizations and their combat is prioritized by nations around the world the antimoney laundering process has not evolved as expected because it has prioritized only the signaling of suspicious trans... | [['money', 'laundering', 'is', 'a', 'crime', 'that', 'makes', 'it', 'possible', 'to', 'finance', 'other', 'crimes', 'for', 'this', 'reason', 'it', 'is', 'important', 'for', 'criminal', 'organizations', 'and', 'their', 'combat', 'is', 'prioritized', 'by', 'nations', 'around', 'the', 'world', 'the', 'antimoney', 'launder... | [-0.09512859561427094, 0.02672313039216238, -0.09256914416894417, 0.10852240585274951, -0.15798109448892442, -0.1643138628616627, 0.1543182951486292, 0.34701398254145643, -0.22731086713099866, -0.32080849917366394, 0.12260502060667637, -0.3242499070443414, -0.1773009645297173, 0.13048179750960018, -0.16279245724876387,... |
1,801.00744 | Thermodynamics of non-Markovian reservoirs and heat engines | We show that non-Markovian effects of the reservoirs can be used as a
resource to extract work from an Otto cycle. The state transformation under
non-Markovian dynamics is achieved via a two-step process, namely an isothermal
process using a Markovian reservoir followed by an adiabatic process. From
second law of the... | quant-ph cond-mat.stat-mech | we show that nonmarkovian effects of the reservoirs can be used as a resource to extract work from an otto cycle the state transformation under nonmarkovian dynamics is achieved via a twostep process namely an isothermal process using a markovian reservoir followed by an adiabatic process from second law of thermodynam... | [['we', 'show', 'that', 'nonmarkovian', 'effects', 'of', 'the', 'reservoirs', 'can', 'be', 'used', 'as', 'a', 'resource', 'to', 'extract', 'work', 'from', 'an', 'otto', 'cycle', 'the', 'state', 'transformation', 'under', 'nonmarkovian', 'dynamics', 'is', 'achieved', 'via', 'a', 'twostep', 'process', 'namely', 'an', 'is... | [-0.08840174620204112, 0.14753603862447884, -0.16665221990688758, 0.002907215980175191, 0.01213280534481301, -0.12149955823140986, 0.09819679706740905, 0.32651334962643247, -0.3130042036118753, -0.2505972830688252, 0.062318736490081336, -0.23123716394800473, -0.1444166127099272, 0.24142524742603522, -0.0655523868661154... |
1,801.00745 | Key-Rate Bound of a Semi-Quantum Protocol Using an Entropic Uncertainty
Relation | In this paper we present a new proof technique for semi-quantum key
distribution protocols which makes use of a quantum entropic uncertainty
relation to bound an adversary's information. Our new technique provides a more
optimistic key-rate bound than previous work relying only on noise statistics
(as opposed to usin... | quant-ph | in this paper we present a new proof technique for semiquantum key distribution protocols which makes use of a quantum entropic uncertainty relation to bound an adversarys information our new technique provides a more optimistic keyrate bound than previous work relying only on noise statistics as opposed to using addit... | [['in', 'this', 'paper', 'we', 'present', 'a', 'new', 'proof', 'technique', 'for', 'semiquantum', 'key', 'distribution', 'protocols', 'which', 'makes', 'use', 'of', 'a', 'quantum', 'entropic', 'uncertainty', 'relation', 'to', 'bound', 'an', 'adversarys', 'information', 'our', 'new', 'technique', 'provides', 'a', 'more'... | [-0.15514792356958712, 0.05862460924254265, -0.14481346790041577, 0.047921141754149604, -0.05280086437338277, -0.2372785596324033, 0.168799707973621, 0.3102542207037148, -0.21449477558367347, -0.3656398229202942, 0.06989418021403253, -0.2244760522226754, -0.10680319634756368, 0.27712170205961323, -0.15753353629261255, ... |
1,801.00746 | Bridging the Gap Between Neural Networks and Neuromorphic Hardware with
A Neural Network Compiler | Different from developing neural networks (NNs) for general-purpose
processors, the development for NN chips usually faces with some
hardware-specific restrictions, such as limited precision of network signals
and parameters, constrained computation scale, and limited types of non-linear
functions.
This paper propo... | cs.NE cs.ET cs.LG | different from developing neural networks nns for generalpurpose processors the development for nn chips usually faces with some hardwarespecific restrictions such as limited precision of network signals and parameters constrained computation scale and limited types of nonlinear functions this paper proposes a general ... | [['different', 'from', 'developing', 'neural', 'networks', 'nns', 'for', 'generalpurpose', 'processors', 'the', 'development', 'for', 'nn', 'chips', 'usually', 'faces', 'with', 'some', 'hardwarespecific', 'restrictions', 'such', 'as', 'limited', 'precision', 'of', 'network', 'signals', 'and', 'parameters', 'constrained... | [-0.11879968096894261, 0.02187059186536843, -0.04125573437562899, 0.05387857539309679, -0.09223035505825752, -0.23685845082356152, 0.034524679690672966, 0.4432714792654703, -0.2831901222761524, -0.3319617606822009, 0.08993965201202388, -0.21822794755969785, -0.21221087552288448, 0.22172988040470762, -0.0780001048321872... |
1,801.00747 | Quantum theory of charged isolated horizons | We describe the quantum theory of isolated horizons with electromagnetic or
non-Abelian gauge charges in a setting in which both gauge and gravitational
field are quantized. We consider the distorted case, and its spherically
symmetric limit. We show that the gravitational horizon degrees of freedom give
rise to the ... | gr-qc hep-th | we describe the quantum theory of isolated horizons with electromagnetic or nonabelian gauge charges in a setting in which both gauge and gravitational field are quantized we consider the distorted case and its spherically symmetric limit we show that the gravitational horizon degrees of freedom give rise to the bekens... | [['we', 'describe', 'the', 'quantum', 'theory', 'of', 'isolated', 'horizons', 'with', 'electromagnetic', 'or', 'nonabelian', 'gauge', 'charges', 'in', 'a', 'setting', 'in', 'which', 'both', 'gauge', 'and', 'gravitational', 'field', 'are', 'quantized', 'we', 'consider', 'the', 'distorted', 'case', 'and', 'its', 'spheric... | [-0.1329623463700108, 0.1568247393809323, -0.08783801206275178, 0.10692019949281781, -0.07932983191908691, -0.11582081448607917, -0.020035579433044466, 0.2984800137627613, -0.19990232783562406, -0.3105296146863237, 0.06208101024646472, -0.33507917317208546, -0.14014500115620743, 0.17095608959287598, -0.0738273467667850... |
1,801.00748 | Habitability of Exoplanet Waterworlds | Many habitable zone exoplanets are expected to form with water mass fractions
higher than that of the Earth. For rocky exoplanets with 10-1000x Earth's H2O
but without H2, we model the multi-Gyr evolution of ocean temperature and
chemistry, taking into account C partitioning, high-pressure ice phases, and
atmosphere-... | astro-ph.EP | many habitable zone exoplanets are expected to form with water mass fractions higher than that of the earth for rocky exoplanets with 101000x earths h2o but without h2 we model the multigyr evolution of ocean temperature and chemistry taking into account c partitioning highpressure ice phases and atmospherelithosphere ... | [['many', 'habitable', 'zone', 'exoplanets', 'are', 'expected', 'to', 'form', 'with', 'water', 'mass', 'fractions', 'higher', 'than', 'that', 'of', 'the', 'earth', 'for', 'rocky', 'exoplanets', 'with', '101000x', 'earths', 'h2o', 'but', 'without', 'h2', 'we', 'model', 'the', 'multigyr', 'evolution', 'of', 'ocean', 'tem... | [-0.08624078585036268, 0.18807073260954707, -0.044627932976167455, 0.03739642597135309, -0.0706691606877665, -0.019336046242754753, 0.0805366712894246, 0.34752833671000316, -0.20681601234915833, -0.352922376915047, 0.10043888281995338, -0.23957362104830618, -0.0995011574553632, 0.20647577293558456, -0.06827465810474927... |
1,801.00749 | Simplicial faces of the set of correlation matrices | This paper concerns the facial geometry of the set of $n \times n$
correlation matrices. The main result states that almost every set of $r$
vertices generates a simplicial face, provided that $r \leq \sqrt{\mathrm{c}
n}$, where $\mathrm{c}$ is an absolute constant. This bound is qualitatively
sharp because the set o... | math.MG math.CO math.OC | this paper concerns the facial geometry of the set of n times n correlation matrices the main result states that almost every set of r vertices generates a simplicial face provided that r leq sqrtmathrmc n where mathrmc is an absolute constant this bound is qualitatively sharp because the set of correlation matrices ha... | [['this', 'paper', 'concerns', 'the', 'facial', 'geometry', 'of', 'the', 'set', 'of', 'n', 'times', 'n', 'correlation', 'matrices', 'the', 'main', 'result', 'states', 'that', 'almost', 'every', 'set', 'of', 'r', 'vertices', 'generates', 'a', 'simplicial', 'face', 'provided', 'that', 'r', 'leq', 'sqrtmathrmc', 'n', 'whe... | [-0.17814380454177398, 0.1120301734662198, -0.021901238198962905, 0.007205223424300071, 0.012132412491125925, -0.16941810656909742, -0.013244554819163656, 0.3386830521086531, -0.23937313883535324, -0.26374082817065136, 0.05227983593490095, -0.36883799566496767, -0.15015943154444797, 0.10994031142082906, -0.099707513548... |
1,801.0075 | Integrated RF-photonic Filters via Photonic-Phononic Emit-Receive
Operations | The creation of high-performance narrowband filters is of great interest for
many RF-signal processing applications. To this end, numerous schemes for
electronic, MEMS-based, and microwave photonic filters have been demonstrated.
Filtering schemes based on microwave photonic systems offer superior
flexibility and tun... | physics.app-ph physics.optics | the creation of highperformance narrowband filters is of great interest for many rfsignal processing applications to this end numerous schemes for electronic memsbased and microwave photonic filters have been demonstrated filtering schemes based on microwave photonic systems offer superior flexibility and tunability to... | [['the', 'creation', 'of', 'highperformance', 'narrowband', 'filters', 'is', 'of', 'great', 'interest', 'for', 'many', 'rfsignal', 'processing', 'applications', 'to', 'this', 'end', 'numerous', 'schemes', 'for', 'electronic', 'memsbased', 'and', 'microwave', 'photonic', 'filters', 'have', 'been', 'demonstrated', 'filte... | [-0.12751999618779328, 0.09004809150472827, -0.006534377656437491, -0.0453827164372206, -0.08482023645257665, -0.1911141824490765, 0.028243388671296863, 0.5063803613503577, -0.2539537393152888, -0.2759426738579962, 0.09523513449234104, -0.23963331573460006, -0.15010744563486672, 0.2954398591014792, -0.05752288127126537... |
1,801.00751 | A Modified Poisson--Nernst--Planck Model with Excluded Volume Effect:
Theory and Numerical Implementation | The Poisson--Nernst--Planck (PNP) equations have been widely applied to
describe ionic transport in ion channels, nanofluidic devices, and many
electrochemical systems. Despite their wide applications, the PNP equations
fail in predicting dynamics and equilibrium states of ionic concentrations in
confined environment... | cond-mat.stat-mech | the poissonnernstplanck pnp equations have been widely applied to describe ionic transport in ion channels nanofluidic devices and many electrochemical systems despite their wide applications the pnp equations fail in predicting dynamics and equilibrium states of ionic concentrations in confined environments due to the... | [['the', 'poissonnernstplanck', 'pnp', 'equations', 'have', 'been', 'widely', 'applied', 'to', 'describe', 'ionic', 'transport', 'in', 'ion', 'channels', 'nanofluidic', 'devices', 'and', 'many', 'electrochemical', 'systems', 'despite', 'their', 'wide', 'applications', 'the', 'pnp', 'equations', 'fail', 'in', 'predictin... | [-0.13162724205330775, 0.08858355124414499, -0.0760200948248931, 0.07104209179191717, -0.015318502962817343, -0.14764768130773184, 0.031782661383610446, 0.3293707070111924, -0.24061031268187325, -0.2894010969513685, 0.06321252854255846, -0.27152696272111215, -0.09861104042193262, 0.176833133068772, 0.007555431042018594... |
1,801.00752 | Analytic Neutrino Oscillation Probabilities in Matter: Revisited | We summarize our recent paper on neutrino oscillation probabilities in
matter, explaining the importance, relevance and need for simple, highly
accurate approximations to the neutrino oscillation probabilities in matter.
Simple expressions for the neutrino mixing angles and mass squared differences
in matter are give... | hep-ph hep-ex | we summarize our recent paper on neutrino oscillation probabilities in matter explaining the importance relevance and need for simple highly accurate approximations to the neutrino oscillation probabilities in matter simple expressions for the neutrino mixing angles and mass squared differences in matter are given in a... | [['we', 'summarize', 'our', 'recent', 'paper', 'on', 'neutrino', 'oscillation', 'probabilities', 'in', 'matter', 'explaining', 'the', 'importance', 'relevance', 'and', 'need', 'for', 'simple', 'highly', 'accurate', 'approximations', 'to', 'the', 'neutrino', 'oscillation', 'probabilities', 'in', 'matter', 'simple', 'exp... | [-0.08005601131067058, 0.22219901302858067, -0.028666733939578568, 0.1902417029267636, -0.056252563993136086, -0.03297000131367341, 0.0823199949581581, 0.3581780518634596, -0.17944892092297474, -0.30164422945159935, 0.028856269782409072, -0.2695329745934493, -0.10345537334248639, 0.2248759011913469, -0.0294781330756951... |
1,801.00753 | Probabilistic supervised learning | Predictive modelling and supervised learning are central to modern data
science. With predictions from an ever-expanding number of supervised black-box
strategies - e.g., kernel methods, random forests, deep learning aka neural
networks - being employed as a basis for decision making processes, it is
crucial to under... | stat.ML cs.LG math.ST stat.ME stat.TH | predictive modelling and supervised learning are central to modern data science with predictions from an everexpanding number of supervised blackbox strategies eg kernel methods random forests deep learning aka neural networks being employed as a basis for decision making processes it is crucial to understand the stati... | [['predictive', 'modelling', 'and', 'supervised', 'learning', 'are', 'central', 'to', 'modern', 'data', 'science', 'with', 'predictions', 'from', 'an', 'everexpanding', 'number', 'of', 'supervised', 'blackbox', 'strategies', 'eg', 'kernel', 'methods', 'random', 'forests', 'deep', 'learning', 'aka', 'neural', 'networks'... | [0.02825248213240411, -0.003050761686929036, -0.13031981179118157, 0.1069569703284651, -0.158605637001805, -0.23049918592721225, 0.09040130475297338, 0.41607881339639424, -0.29770268478617073, -0.33917068867385386, 0.07284428722562734, -0.22319096704298863, -0.16032298430800437, 0.20471225751470776, -0.1178569050524383... |
1,801.00754 | Fundamental Latency Limits for D2D-Aided Content Delivery in Fog
Wireless Networks | Device-to-Device (D2D) communication can support the operation of cellular
systems by reducing the traffic in the network infrastructure. In this paper,
the benefits of D2D communication are investigated in the context of a
Fog-Radio Access Network (F-RAN) that leverages edge caching and fronthaul
connectivity for th... | cs.IT math.IT | devicetodevice d2d communication can support the operation of cellular systems by reducing the traffic in the network infrastructure in this paper the benefits of d2d communication are investigated in the context of a fogradio access network fran that leverages edge caching and fronthaul connectivity for the purpose of... | [['devicetodevice', 'd2d', 'communication', 'can', 'support', 'the', 'operation', 'of', 'cellular', 'systems', 'by', 'reducing', 'the', 'traffic', 'in', 'the', 'network', 'infrastructure', 'in', 'this', 'paper', 'the', 'benefits', 'of', 'd2d', 'communication', 'are', 'investigated', 'in', 'the', 'context', 'of', 'a', '... | [-0.35973424223700057, -0.007232652612017571, -0.0009502258186263067, -0.019504119602411434, -0.04550676217509641, -0.26202465626238675, 0.20250077891008308, 0.4196031256130448, -0.2739704654448562, -0.25153176961121737, 0.04922667133225197, -0.25319475078679343, -0.2316519536043483, 0.08100739660396895, -0.15568461831... |
1,801.00755 | Graphene lattice-layer entanglement under non-Markovian phase noise | The evolution of single particle excitations of bilayer graphene under
effects of non-Markovian noise is described with focus on the decoherence
process of lattice-layer (LL) maximally entangled states. Once that the
noiseless dynamics of an arbitrary initial state is identified by the
correspondence between the tigh... | cond-mat.mes-hall hep-th quant-ph | the evolution of single particle excitations of bilayer graphene under effects of nonmarkovian noise is described with focus on the decoherence process of latticelayer ll maximally entangled states once that the noiseless dynamics of an arbitrary initial state is identified by the correspondence between the tightbindin... | [['the', 'evolution', 'of', 'single', 'particle', 'excitations', 'of', 'bilayer', 'graphene', 'under', 'effects', 'of', 'nonmarkovian', 'noise', 'is', 'described', 'with', 'focus', 'on', 'the', 'decoherence', 'process', 'of', 'latticelayer', 'll', 'maximally', 'entangled', 'states', 'once', 'that', 'the', 'noiseless', ... | [-0.17788692782115606, 0.21994746281497, -0.043465020452276806, 0.0812113510894758, 0.029865212078827124, -0.18910904388305627, 0.01793527980335057, 0.32463438645419146, -0.24771551061680333, -0.24911611947851878, 0.047114966979845324, -0.30093263727693637, -0.09055304810042597, 0.1746453873522114, -0.01263625437342044... |
1,801.00756 | Driven-Dissipative Supersolid in a Ring Cavity | Supersolids are characterized by the counter-intuitive coexistence of
superfluid and crystalline order. Here we study a supersolid phase emerging in
the steady state of a driven-dissipative system. We consider a transversely
pumped Bose-Einstein condensate trapped along the axis of a ring cavity and
coherently couple... | cond-mat.quant-gas quant-ph | supersolids are characterized by the counterintuitive coexistence of superfluid and crystalline order here we study a supersolid phase emerging in the steady state of a drivendissipative system we consider a transversely pumped boseeinstein condensate trapped along the axis of a ring cavity and coherently coupled to a ... | [['supersolids', 'are', 'characterized', 'by', 'the', 'counterintuitive', 'coexistence', 'of', 'superfluid', 'and', 'crystalline', 'order', 'here', 'we', 'study', 'a', 'supersolid', 'phase', 'emerging', 'in', 'the', 'steady', 'state', 'of', 'a', 'drivendissipative', 'system', 'we', 'consider', 'a', 'transversely', 'pum... | [-0.26756324469917325, 0.33878535870551146, -0.10006345470272307, -0.017868368581214267, -0.00034458652245686263, -0.17127596863035768, 0.0742992800762688, 0.363002387787895, -0.25593500442777734, -0.16200033337431582, 0.007400149376465108, -0.2698068945114878, -0.06837038018715542, 0.10700716815788198, 0.0440004304365... |
1,801.00757 | The second Weyl coefficient for a first order system | For a scalar elliptic self-adjoint operator on a compact manifold without
boundary we have two-term asymptotics for the number of eigenvalues between
zero and lambda when lambda tends to infinity, under an additional dynamical
condition. This is a well known result of J.J.Duistermaat and V.W.Guillemin
from 1975.
In... | math.SP | for a scalar elliptic selfadjoint operator on a compact manifold without boundary we have twoterm asymptotics for the number of eigenvalues between zero and lambda when lambda tends to infinity under an additional dynamical condition this is a well known result of jjduistermaat and vwguillemin from 1975 in the case of ... | [['for', 'a', 'scalar', 'elliptic', 'selfadjoint', 'operator', 'on', 'a', 'compact', 'manifold', 'without', 'boundary', 'we', 'have', 'twoterm', 'asymptotics', 'for', 'the', 'number', 'of', 'eigenvalues', 'between', 'zero', 'and', 'lambda', 'when', 'lambda', 'tends', 'to', 'infinity', 'under', 'an', 'additional', 'dyna... | [-0.13662770195210824, 0.05267823859549704, -0.1038963565908706, 0.07030255114051527, -0.09421033846777377, -0.09250135944353473, -0.017953619966457196, 0.296893515874312, -0.22654798177918836, -0.25843282181547206, 0.1365075159006502, -0.28073432795189096, -0.15623599559124282, 0.18828072273102936, -0.0371354810453503... |
1,801.00758 | Global Dirac bispinor entanglement under Lorentz boosts | The effects of Lorentz boosts on the quantum entanglement encoded by a pair
of massive spin one-half particles are described according to the Lorentz
covariant structure described by Dirac bispinors. The quantum system considered
incorporates four degrees of freedom -- two of them related to the bispinor
intrinsic pa... | quant-ph hep-th | the effects of lorentz boosts on the quantum entanglement encoded by a pair of massive spin onehalf particles are described according to the lorentz covariant structure described by dirac bispinors the quantum system considered incorporates four degrees of freedom two of them related to the bispinor intrinsic parity an... | [['the', 'effects', 'of', 'lorentz', 'boosts', 'on', 'the', 'quantum', 'entanglement', 'encoded', 'by', 'a', 'pair', 'of', 'massive', 'spin', 'onehalf', 'particles', 'are', 'described', 'according', 'to', 'the', 'lorentz', 'covariant', 'structure', 'described', 'by', 'dirac', 'bispinors', 'the', 'quantum', 'system', 'c... | [-0.16956406269726587, 0.24927304485853471, -0.0666212038409973, 0.08038146089247057, -0.034526756165540115, -0.15391790053752946, -0.04663124240966496, 0.3270709475737463, -0.2520060607557664, -0.25764516723405534, 0.006807990005981286, -0.2596262867327382, -0.12125454765509416, 0.15181602840368338, 0.0257906315286499... |
1,801.00759 | On the clustering properties of produced particles in high-energy $pp$
collisions | Minijets provide useful information on parton interactions in the low
transverse-momentum (low-$p_T$) region. Because minijets produce clusters, we
study the clustering properties of produced particles in high-energy $pp$
collisions as a first step to identify minijets. We develop an algorithm to
find clusters by usi... | hep-ph hep-ex nucl-ex nucl-th | minijets provide useful information on parton interactions in the low transversemomentum lowp_t region because minijets produce clusters we study the clustering properties of produced particles in highenergy pp collisions as a first step to identify minijets we develop an algorithm to find clusters by using the kmeans ... | [['minijets', 'provide', 'useful', 'information', 'on', 'parton', 'interactions', 'in', 'the', 'low', 'transversemomentum', 'lowp_t', 'region', 'because', 'minijets', 'produce', 'clusters', 'we', 'study', 'the', 'clustering', 'properties', 'of', 'produced', 'particles', 'in', 'highenergy', 'pp', 'collisions', 'as', 'a'... | [-0.07478613708353339, 0.192012311942306, -0.18832420311231637, 0.19381696154521658, -0.010736746362780627, -0.05351722721332827, -0.028562989497843843, 0.4108835717704959, -0.2349452120669855, -0.34877784437953663, -0.07127254294643465, -0.3075539122413223, -0.02078690078222933, 0.1286610763770743, 0.05610525270588905... |
1,801.0076 | The cover time of a biased random walk on a random cubic graph | We study a random walk that prefers tou se unvisited edges in the context of
random cubic graphs. We establish asymptotically correct estimates for the
vertex and edge cover times, these being $\approx n\log n$ and $\approx
\frac32n\log n$ respectively.
| math.CO cs.DS | we study a random walk that prefers tou se unvisited edges in the context of random cubic graphs we establish asymptotically correct estimates for the vertex and edge cover times these being approx nlog n and approx frac32nlog n respectively | [['we', 'study', 'a', 'random', 'walk', 'that', 'prefers', 'tou', 'se', 'unvisited', 'edges', 'in', 'the', 'context', 'of', 'random', 'cubic', 'graphs', 'we', 'establish', 'asymptotically', 'correct', 'estimates', 'for', 'the', 'vertex', 'and', 'edge', 'cover', 'times', 'these', 'being', 'approx', 'nlog', 'n', 'and', '... | [-0.15801149007315055, 0.19034842430399015, 0.009834120241113199, 0.04639662730579193, -0.037105763665376566, -0.22040733920696837, 0.14972619836529097, 0.4298836682469417, -0.18996587476860255, -0.29904240837846047, 0.1018584422999993, -0.39078678467716926, -0.11432349451411611, 0.04374822305563169, -0.049462086359898... |
1,801.00761 | Ornstein-Uhlenbeck processes with singular drifts: integral estimates
and Girsanov densities | We consider a perturbation of a Hilbert space-valued Ornstein--Uhlenbeck
process by a class of singular nonlinear non-autonomous maximal monotone
time-dependent drifts. The only further assumption on the drift is that it is
bounded on balls in the Hilbert space uniformly in time. First we introduce a
new notion of ge... | math.PR | we consider a perturbation of a hilbert spacevalued ornsteinuhlenbeck process by a class of singular nonlinear nonautonomous maximal monotone timedependent drifts the only further assumption on the drift is that it is bounded on balls in the hilbert space uniformly in time first we introduce a new notion of generalized... | [['we', 'consider', 'a', 'perturbation', 'of', 'a', 'hilbert', 'spacevalued', 'ornsteinuhlenbeck', 'process', 'by', 'a', 'class', 'of', 'singular', 'nonlinear', 'nonautonomous', 'maximal', 'monotone', 'timedependent', 'drifts', 'the', 'only', 'further', 'assumption', 'on', 'the', 'drift', 'is', 'that', 'it', 'is', 'bou... | [-0.10640944601105087, 0.10795399606200483, -0.09129249251803712, 0.08101266524031683, -0.05980653197655235, -0.10810834810356884, 0.007775627651854473, 0.3653391136048252, -0.3046765249934705, -0.17455084916924962, 0.16919219155576737, -0.28148184928988274, -0.1761701517217957, 0.20518702389466958, -0.1303984658169450... |
1,801.00762 | All bipartitions of arbitrary Dicke states | By exploiting the permutation symmetry of Dick states, we derive closed
analytical expressions of Schmidt decompositions for {\it all} possible
bipartitions of a system described by this kind of state. This allows us to
exhaustively compute the entropy of entanglement of the bipartitions and, thus,
compare the their ... | quant-ph | by exploiting the permutation symmetry of dick states we derive closed analytical expressions of schmidt decompositions for it all possible bipartitions of a system described by this kind of state this allows us to exhaustively compute the entropy of entanglement of the bipartitions and thus compare the their entanglem... | [['by', 'exploiting', 'the', 'permutation', 'symmetry', 'of', 'dick', 'states', 'we', 'derive', 'closed', 'analytical', 'expressions', 'of', 'schmidt', 'decompositions', 'for', 'it', 'all', 'possible', 'bipartitions', 'of', 'a', 'system', 'described', 'by', 'this', 'kind', 'of', 'state', 'this', 'allows', 'us', 'to', '... | [-0.16123981275579777, 0.19716993214766662, -0.05312537381502047, 0.06932599369232377, 0.032219179846946, -0.14814188250991173, 0.104154135813388, 0.3105796945013412, -0.24375063545638312, -0.2725925255719929, 0.06286781738362314, -0.2883749868967355, -0.09575987362369819, 0.15775484909552265, -0.06543201574264731, 0.0... |
1,801.00763 | Koszul almost complete intersections | Let $R = S/I$ be a quotient of a standard graded polynomial ring $S$ by an
ideal $I$ generated by quadrics. If $R$ is Koszul, a question of Avramov,
Conca, and Iyengar asks whether the Betti numbers of $R$ over $S$ can be
bounded above by binomial coefficients on the minimal number of generators of
$I$. Motivated by ... | math.AC | let r si be a quotient of a standard graded polynomial ring s by an ideal i generated by quadrics if r is koszul a question of avramov conca and iyengar asks whether the betti numbers of r over s can be bounded above by binomial coefficients on the minimal number of generators of i motivated by previous results for kos... | [['let', 'r', 'si', 'be', 'a', 'quotient', 'of', 'a', 'standard', 'graded', 'polynomial', 'ring', 's', 'by', 'an', 'ideal', 'i', 'generated', 'by', 'quadrics', 'if', 'r', 'is', 'koszul', 'a', 'question', 'of', 'avramov', 'conca', 'and', 'iyengar', 'asks', 'whether', 'the', 'betti', 'numbers', 'of', 'r', 'over', 's', 'c... | [-0.17663110346582375, 0.03509966991627344, -0.00800594687461853, 0.03860141865269198, -0.0584042001368576, -0.18775836111683594, -0.03671407520182823, 0.30926245482834547, -0.38132814863010456, -0.22308297951852804, 0.09487074702659523, -0.24385335921849075, -0.10586132879895893, 0.20315498214607175, -0.16998294113007... |
1,801.00764 | Modeling solid-state dewetting of a single-crystal binary alloy thin
films | Dewetting of a binary alloy thin film is studied using a continuum
many-parameter model that accounts for the surface and bulk diffusion, the bulk
phase separation, the surface segregation and the particles formation.
Analytical solution is found for the quasistatic equilibrium concentration of a
surface-segregated a... | cond-mat.mtrl-sci cond-mat.mes-hall math.AP nlin.PS | dewetting of a binary alloy thin film is studied using a continuum manyparameter model that accounts for the surface and bulk diffusion the bulk phase separation the surface segregation and the particles formation analytical solution is found for the quasistatic equilibrium concentration of a surfacesegregated atomic s... | [['dewetting', 'of', 'a', 'binary', 'alloy', 'thin', 'film', 'is', 'studied', 'using', 'a', 'continuum', 'manyparameter', 'model', 'that', 'accounts', 'for', 'the', 'surface', 'and', 'bulk', 'diffusion', 'the', 'bulk', 'phase', 'separation', 'the', 'surface', 'segregation', 'and', 'the', 'particles', 'formation', 'anal... | [-0.1160242920663395, 0.209758783263992, -0.08072288700655186, 0.0008979975759681293, 0.016967954153101372, -0.0914302898711374, 0.01749010457704104, 0.3568874997601912, -0.25678979637499316, -0.3097598612995938, 0.07038177587625222, -0.2925055643918211, -0.10235457202841075, 0.11045646675675067, 0.028621804041985693, ... |
1,801.00765 | Localized all-optical control of single semiconductor quantum dots
through plasmon-polariton-induced screening | Due to their ability to strongly modify the local electromagnetic (EM) field
through the excitation of surface plasmon polaritons (SPPs), plasmonic
nanostructures have been often used to reshape the emission direction and
enhance the radiative decay rate of quantum emitters, such as semiconductor
quantum dots (QDs). ... | cond-mat.mes-hall | due to their ability to strongly modify the local electromagnetic em field through the excitation of surface plasmon polaritons spps plasmonic nanostructures have been often used to reshape the emission direction and enhance the radiative decay rate of quantum emitters such as semiconductor quantum dots qds these featu... | [['due', 'to', 'their', 'ability', 'to', 'strongly', 'modify', 'the', 'local', 'electromagnetic', 'em', 'field', 'through', 'the', 'excitation', 'of', 'surface', 'plasmon', 'polaritons', 'spps', 'plasmonic', 'nanostructures', 'have', 'been', 'often', 'used', 'to', 'reshape', 'the', 'emission', 'direction', 'and', 'enha... | [-0.10922123204262432, 0.15787934318267374, -0.04837362130196129, 0.026230667909324358, -0.07405734478932204, -0.1800569258807109, 0.05268871803514518, 0.47964012369372044, -0.30637370242701867, -0.34223947380787306, 0.013467441215710361, -0.25490361820210855, -0.1544683352856944, 0.21369276753379196, 0.014967639370573... |
1,801.00766 | Fluctuating chemohydrodynamics and the stochastic motion of
self-diffusiophoretic particles | The propulsion of active particles by self-diffusiophoresis is driven by
asymmetric catalytic reactions on the particle surface that generate a
mechanochemical coupling between the fluid velocity and the concentration
fields of fuel and product in the surrounding solution. Because of thermal and
molecular fluctuation... | cond-mat.stat-mech cond-mat.soft | the propulsion of active particles by selfdiffusiophoresis is driven by asymmetric catalytic reactions on the particle surface that generate a mechanochemical coupling between the fluid velocity and the concentration fields of fuel and product in the surrounding solution because of thermal and molecular fluctuations in... | [['the', 'propulsion', 'of', 'active', 'particles', 'by', 'selfdiffusiophoresis', 'is', 'driven', 'by', 'asymmetric', 'catalytic', 'reactions', 'on', 'the', 'particle', 'surface', 'that', 'generate', 'a', 'mechanochemical', 'coupling', 'between', 'the', 'fluid', 'velocity', 'and', 'the', 'concentration', 'fields', 'of'... | [-0.1275139689957338, 0.2700068723017827, -0.06813725966730247, 0.00028116671822595696, -0.0007732958351993117, -0.1152731560647857, 0.002885670857196135, 0.3129430660085121, -0.27353196169349775, -0.32198176354416147, 0.03082070621846567, -0.29141982583221326, -0.10266289212894895, 0.14543691302903675, 0.0273433940692... |
1,801.00767 | The local-triviality dimension of actions of compact quantum groups | We define the local-triviality dimension for actions of compact quantum
groups on unital C*-algebras. The resulting compact quantum principal bundle is
said to be locally trivial when this dimension is finite. For commutative
C*-algebras, this notion recovers the standard definition of local triviality
of compact pri... | math.OA math.QA | we define the localtriviality dimension for actions of compact quantum groups on unital calgebras the resulting compact quantum principal bundle is said to be locally trivial when this dimension is finite for commutative calgebras this notion recovers the standard definition of local triviality of compact principal bun... | [['we', 'define', 'the', 'localtriviality', 'dimension', 'for', 'actions', 'of', 'compact', 'quantum', 'groups', 'on', 'unital', 'calgebras', 'the', 'resulting', 'compact', 'quantum', 'principal', 'bundle', 'is', 'said', 'to', 'be', 'locally', 'trivial', 'when', 'this', 'dimension', 'is', 'finite', 'for', 'commutative'... | [-0.17443215367026055, 0.16060483638788214, -0.1355235548913837, 0.05674156828116303, -0.14335800807636517, -0.17885840725816357, -0.038343987583245434, 0.34652314184663385, -0.32501118511964494, -0.10073396152942084, 0.10599331270406345, -0.20973614193812515, -0.1304676959497066, 0.17424171908686942, -0.19209111986744... |
1,801.00768 | Emergent de Sitter epoch of the quantum Cosmos | The quantum nature of the Big Bang is reexamined in the framework of Loop
Quantum Cosmology. The strict application of a regularization procedure to the
Hamiltonian, originally developed for the Hamiltonian in loop quantum gravity,
leads to a qualitative modification of the bounce paradigm. Quantum gravity
effects st... | gr-qc | the quantum nature of the big bang is reexamined in the framework of loop quantum cosmology the strict application of a regularization procedure to the hamiltonian originally developed for the hamiltonian in loop quantum gravity leads to a qualitative modification of the bounce paradigm quantum gravity effects still le... | [['the', 'quantum', 'nature', 'of', 'the', 'big', 'bang', 'is', 'reexamined', 'in', 'the', 'framework', 'of', 'loop', 'quantum', 'cosmology', 'the', 'strict', 'application', 'of', 'a', 'regularization', 'procedure', 'to', 'the', 'hamiltonian', 'originally', 'developed', 'for', 'the', 'hamiltonian', 'in', 'loop', 'quant... | [-0.16174990379150553, 0.1856301093855536, -0.19207286496972104, 0.12005035018868161, -0.10063993457300835, -0.19278558325134668, -0.021958656049423278, 0.24180132827261486, -0.22790560238512167, -0.2805247343221051, 0.03736260928724141, -0.21452216485358147, -0.08968664662553424, 0.1484797548850527, -0.050971582666578... |
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