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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1,802.0756 | Critical yield numbers and limiting yield surfaces of particle arrays
settling in a Bingham fluid | We consider the flow of multiple particles in a Bingham fluid in an
anti-plane shear flow configuration. The limiting situation in which the
internal and applied forces balance and the fluid and particles stop flowing,
that is, when the flow settles, is formulated as finding the optimal ratio
between the total variat... | math.OC | we consider the flow of multiple particles in a bingham fluid in an antiplane shear flow configuration the limiting situation in which the internal and applied forces balance and the fluid and particles stop flowing that is when the flow settles is formulated as finding the optimal ratio between the total variation fun... | [['we', 'consider', 'the', 'flow', 'of', 'multiple', 'particles', 'in', 'a', 'bingham', 'fluid', 'in', 'an', 'antiplane', 'shear', 'flow', 'configuration', 'the', 'limiting', 'situation', 'in', 'which', 'the', 'internal', 'and', 'applied', 'forces', 'balance', 'and', 'the', 'fluid', 'and', 'particles', 'stop', 'flowing... | [-0.1255977571944604, 0.11740856095578191, -0.11272225652772912, 0.06876022762059089, -0.058886211693846766, -0.11649609184850847, 0.01740564687602825, 0.33269633655974673, -0.3233273341158954, -0.26678464779727207, 0.12143999178936932, -0.23718108430052595, -0.15119792543610053, 0.1814624041876072, -0.0853276644211607... |
1,802.07561 | $L_p$ Minkowski Valuations on polytopes | For $1 \leq p < \infty$, Ludwig, Haberl and Parapatits classified $L_p$
Minkowski valuations intertwining the special linear group with additional
conditions such as homogeneity and continuity. In this paper,a complete
classification of $L_p$ Minkowski valuations intertwining the special linear
group on polytopes wit... | math.MG | for 1 leq p infty ludwig haberl and parapatits classified l_p minkowski valuations intertwining the special linear group with additional conditions such as homogeneity and continuity in this papera complete classification of l_p minkowski valuations intertwining the special linear group on polytopes without any additio... | [['for', '1', 'leq', 'p', 'infty', 'ludwig', 'haberl', 'and', 'parapatits', 'classified', 'l_p', 'minkowski', 'valuations', 'intertwining', 'the', 'special', 'linear', 'group', 'with', 'additional', 'conditions', 'such', 'as', 'homogeneity', 'and', 'continuity', 'in', 'this', 'papera', 'complete', 'classification', 'of... | [-0.1384649303436163, 0.09902756131486967, -0.03142756858142093, 0.12108535345760174, -0.07116086279711453, -0.23944778117584065, 0.0016977296472759917, 0.37004374276148155, -0.29655683404416777, -0.2021098673576489, 0.11079998649620393, -0.29222374353412306, -0.0625319077516906, 0.13822739068200462, -0.106366966465429... |
1,802.07562 | Early warning signals in plant disease outbreaks | Summary
1. Infectious disease outbreaks in plants threaten ecosystems, agricultural
crops and food trade. Currently, several fungal diseases are affecting forests
worldwide, posing a major risk to tree species, habitats and consequently
ecosystem decay. Prediction and control of disease spread are difficult, mainly... | q-bio.PE | summary 1 infectious disease outbreaks in plants threaten ecosystems agricultural crops and food trade currently several fungal diseases are affecting forests worldwide posing a major risk to tree species habitats and consequently ecosystem decay prediction and control of disease spread are difficult mainly due to the ... | [['summary', '1', 'infectious', 'disease', 'outbreaks', 'in', 'plants', 'threaten', 'ecosystems', 'agricultural', 'crops', 'and', 'food', 'trade', 'currently', 'several', 'fungal', 'diseases', 'are', 'affecting', 'forests', 'worldwide', 'posing', 'a', 'major', 'risk', 'to', 'tree', 'species', 'habitats', 'and', 'conseq... | [-0.11208126162058263, 0.14762392555912165, -0.06008488949072703, 0.1371641900124334, -0.015537934725262641, -0.1713656917040657, 0.09848693619969154, 0.3472869435873658, -0.22983597447566195, -0.27164027275964336, 0.12617698715713707, -0.29564941305014764, -0.23528417407092994, 0.1784264231573431, -0.06834619686593713... |
1,802.07563 | Laplace transforms and valuations | It is proved that the classical Laplace transform is a continuous valuation
which is positively GL$(n)$ covariant and logarithmic translation covariant.
Conversely, these properties turn out to be sufficient to characterize this
transform.
| math.MG math.FA | it is proved that the classical laplace transform is a continuous valuation which is positively gln covariant and logarithmic translation covariant conversely these properties turn out to be sufficient to characterize this transform | [['it', 'is', 'proved', 'that', 'the', 'classical', 'laplace', 'transform', 'is', 'a', 'continuous', 'valuation', 'which', 'is', 'positively', 'gln', 'covariant', 'and', 'logarithmic', 'translation', 'covariant', 'conversely', 'these', 'properties', 'turn', 'out', 'to', 'be', 'sufficient', 'to', 'characterize', 'this',... | [-0.08421459794044495, 0.09920225738350189, -0.20404847896178113, 0.15207662874352978, -0.18106354722245174, -0.16073253255506809, -0.04971695237944721, 0.3910664322249817, -0.3768593768278758, -0.12197557001402884, 0.10573919515732225, -0.20357448870852363, -0.1747844543195132, 0.17778696819688333, -0.1216140425848689... |
1,802.07564 | Clipped Action Policy Gradient | Many continuous control tasks have bounded action spaces. When policy
gradient methods are applied to such tasks, out-of-bound actions need to be
clipped before execution, while policies are usually optimized as if the
actions are not clipped. We propose a policy gradient estimator that exploits
the knowledge of acti... | cs.LG cs.AI stat.ML | many continuous control tasks have bounded action spaces when policy gradient methods are applied to such tasks outofbound actions need to be clipped before execution while policies are usually optimized as if the actions are not clipped we propose a policy gradient estimator that exploits the knowledge of actions bein... | [['many', 'continuous', 'control', 'tasks', 'have', 'bounded', 'action', 'spaces', 'when', 'policy', 'gradient', 'methods', 'are', 'applied', 'to', 'such', 'tasks', 'outofbound', 'actions', 'need', 'to', 'be', 'clipped', 'before', 'execution', 'while', 'policies', 'are', 'usually', 'optimized', 'as', 'if', 'the', 'acti... | [-0.050210281000049276, 0.03161366748284887, -0.15160987351343713, 0.07196929596406831, -0.133406944132664, -0.21055660873905502, 0.053124361008998346, 0.5375661875713955, -0.2702980153262615, -0.2766546459360556, 0.16432227892272006, -0.2639779188162224, -0.1751357546499507, 0.2427335444245149, -0.21537427849305624, 0... |
1,802.07565 | Fluctuation Analysis of the Atmospheric Energy Cycle | The atmosphere gains available potential energy by solar radiation and
dissipates kinetic energy mainly in the atmospheric boundary layer. We analyze
the fluctuations of the global mean energy cycle defined by Lorenz (1955) in a
simulation with a simplified hydrostatic model. The energy current densities
are well app... | physics.ao-ph | the atmosphere gains available potential energy by solar radiation and dissipates kinetic energy mainly in the atmospheric boundary layer we analyze the fluctuations of the global mean energy cycle defined by lorenz 1955 in a simulation with a simplified hydrostatic model the energy current densities are well approxima... | [['the', 'atmosphere', 'gains', 'available', 'potential', 'energy', 'by', 'solar', 'radiation', 'and', 'dissipates', 'kinetic', 'energy', 'mainly', 'in', 'the', 'atmospheric', 'boundary', 'layer', 'we', 'analyze', 'the', 'fluctuations', 'of', 'the', 'global', 'mean', 'energy', 'cycle', 'defined', 'by', 'lorenz', '1955'... | [-0.10645065873307791, 0.15553899101799307, -0.07914019459507095, 0.13218185619257813, -0.015598348939334447, -0.05832442275318756, 0.0606553784422225, 0.28359898959971824, -0.2679264178095421, -0.35971992218620935, 0.053511007403392555, -0.2691416396706734, -0.04620347674145311, 0.14411023379751603, -0.047456356705570... |
1,802.07566 | Electron-impact excitation of diatomic hydride cations II: OH$^+$ and
SH$^+$ | R-matrix calculations combined with the adiabatic-nuclei-rotation and
Coulomb-Born approximations are used to compute electron-impact rotational rate
coefficients for two open-shell diatomic cations of astrophysical interest: the
hydoxyl and sulphanyl ions, OH$^+$ and SH$^+$. Hyperfine resolved rate
coefficients are ... | astro-ph.SR astro-ph.GA | rmatrix calculations combined with the adiabaticnucleirotation and coulombborn approximations are used to compute electronimpact rotational rate coefficients for two openshell diatomic cations of astrophysical interest the hydoxyl and sulphanyl ions oh and sh hyperfine resolved rate coefficients are deduced using the i... | [['rmatrix', 'calculations', 'combined', 'with', 'the', 'adiabaticnucleirotation', 'and', 'coulombborn', 'approximations', 'are', 'used', 'to', 'compute', 'electronimpact', 'rotational', 'rate', 'coefficients', 'for', 'two', 'openshell', 'diatomic', 'cations', 'of', 'astrophysical', 'interest', 'the', 'hydoxyl', 'and',... | [-0.07363623864498464, 0.11723800748600383, 0.06252908760260018, 0.08117314690684478, 0.026238664431181155, -0.11276421607647724, 0.03840857319685385, 0.43196039369224376, -0.1865532651350324, -0.23186553237994886, -0.03946380195634018, -0.2889716578296052, -0.000245529519095314, 0.15159105920103239, 0.0901176765413388... |
1,802.07567 | Measurement of optical to electrical and electrical to optical delays
with ps-level uncertainty | We present a new measurement principle to determine the absolute time delay
of a waveform from an optical reference plane to an electrical reference plane
and vice versa. We demonstrate a method based on this principle with 2 ps
uncertainty. This method can be used to perform accurate time delay
determinations of opt... | physics.optics | we present a new measurement principle to determine the absolute time delay of a waveform from an optical reference plane to an electrical reference plane and vice versa we demonstrate a method based on this principle with 2 ps uncertainty this method can be used to perform accurate time delay determinations of optical... | [['we', 'present', 'a', 'new', 'measurement', 'principle', 'to', 'determine', 'the', 'absolute', 'time', 'delay', 'of', 'a', 'waveform', 'from', 'an', 'optical', 'reference', 'plane', 'to', 'an', 'electrical', 'reference', 'plane', 'and', 'vice', 'versa', 'we', 'demonstrate', 'a', 'method', 'based', 'on', 'this', 'prin... | [-0.09943145566581528, 0.05027258154466873, -0.11189885897869148, 0.019796648870471903, -0.10110351341517315, -0.14011579084200496, 0.11416841704235173, 0.44496849947368977, -0.28223608608943285, -0.3330909161607629, 0.10953018933501017, -0.21107726519178485, -0.08387352454658482, 0.2608732716324403, -0.092336215707713... |
1,802.07568 | CABS-flex 2.0: a web server for fast simulations of flexibility of
protein structures | Classical simulations of protein flexibility remain computationally
expensive, especially for large proteins. A few years ago, we developed a fast
method for predicting protein structure fluctuations that uses a single protein
model as the input. The method has been made available as the CABS-flex web
server and appl... | q-bio.BM | classical simulations of protein flexibility remain computationally expensive especially for large proteins a few years ago we developed a fast method for predicting protein structure fluctuations that uses a single protein model as the input the method has been made available as the cabsflex web server and applied in ... | [['classical', 'simulations', 'of', 'protein', 'flexibility', 'remain', 'computationally', 'expensive', 'especially', 'for', 'large', 'proteins', 'a', 'few', 'years', 'ago', 'we', 'developed', 'a', 'fast', 'method', 'for', 'predicting', 'protein', 'structure', 'fluctuations', 'that', 'uses', 'a', 'single', 'protein', '... | [-0.09565082037275155, 0.04900798942141522, -0.04830830528562029, 0.0867346658498998, -0.09076054639836702, -0.20244446123251691, 0.06786014719713981, 0.4207782440890486, -0.28026867346264994, -0.3370168710915515, 0.06868777858303823, -0.2572202904758832, -0.142292498342263, 0.2205913661141844, -0.005910210058433362, 0... |
1,802.07569 | Continual Lifelong Learning with Neural Networks: A Review | Humans and animals have the ability to continually acquire, fine-tune, and
transfer knowledge and skills throughout their lifespan. This ability, referred
to as lifelong learning, is mediated by a rich set of neurocognitive mechanisms
that together contribute to the development and specialization of our
sensorimotor ... | cs.LG q-bio.NC stat.ML | humans and animals have the ability to continually acquire finetune and transfer knowledge and skills throughout their lifespan this ability referred to as lifelong learning is mediated by a rich set of neurocognitive mechanisms that together contribute to the development and specialization of our sensorimotor skills a... | [['humans', 'and', 'animals', 'have', 'the', 'ability', 'to', 'continually', 'acquire', 'finetune', 'and', 'transfer', 'knowledge', 'and', 'skills', 'throughout', 'their', 'lifespan', 'this', 'ability', 'referred', 'to', 'as', 'lifelong', 'learning', 'is', 'mediated', 'by', 'a', 'rich', 'set', 'of', 'neurocognitive', '... | [-0.02110953065843349, 0.07976944435106609, -0.034192074286188964, 0.07859922534587913, -0.18025617705402194, -0.18055729485707045, 0.04699564928080573, 0.4309504451045748, -0.33153628067823476, -0.34728856914040473, 0.09112309321350796, -0.24090210858059327, -0.2280140006234685, 0.1727139955066089, -0.1840679883578847... |
1,802.0757 | Influence of chemical potential on the Casimir-Polder interaction
between an atom and gapped graphene or graphene-coated substrate | We present a formalism based on first principles of quantum electrodynamics
at nonzero temperature which permits to calculate the Casimir-Polder
interaction between an atom and a graphene sheet with arbitrary mass gap and
chemical potential, including graphene-coated substrates. The free energy and
force of the Casim... | cond-mat.mes-hall | we present a formalism based on first principles of quantum electrodynamics at nonzero temperature which permits to calculate the casimirpolder interaction between an atom and a graphene sheet with arbitrary mass gap and chemical potential including graphenecoated substrates the free energy and force of the casimirpold... | [['we', 'present', 'a', 'formalism', 'based', 'on', 'first', 'principles', 'of', 'quantum', 'electrodynamics', 'at', 'nonzero', 'temperature', 'which', 'permits', 'to', 'calculate', 'the', 'casimirpolder', 'interaction', 'between', 'an', 'atom', 'and', 'a', 'graphene', 'sheet', 'with', 'arbitrary', 'mass', 'gap', 'and'... | [-0.15754718889994782, 0.1797748976406096, -0.06467883141322914, 0.0032015185816045007, 0.008711558359501948, -0.13525182048757398, 0.04965056170096349, 0.3909361978346978, -0.22901435853473506, -0.30326023830297455, -0.02181234061671187, -0.32903963609378617, -0.12320980468142459, 0.16617852425081048, 0.08423353640839... |
1,802.07571 | Norm estimates and asymptotic faithfulness of the quantum $SU(n)$
representations of the mapping class groups | We give a direct proof for the asymptotic faithfulness of the quantum $SU(n)$
representations of the mapping class groups using peak sections in Kodaira
embedding. We give also estimates on the norm of the parallell transport of the
projective connection on the Verlinde bundle. The faithfulness has been proved
earlie... | math.DG math.RT | we give a direct proof for the asymptotic faithfulness of the quantum sun representations of the mapping class groups using peak sections in kodaira embedding we give also estimates on the norm of the parallell transport of the projective connection on the verlinde bundle the faithfulness has been proved earlier in 1 u... | [['we', 'give', 'a', 'direct', 'proof', 'for', 'the', 'asymptotic', 'faithfulness', 'of', 'the', 'quantum', 'sun', 'representations', 'of', 'the', 'mapping', 'class', 'groups', 'using', 'peak', 'sections', 'in', 'kodaira', 'embedding', 'we', 'give', 'also', 'estimates', 'on', 'the', 'norm', 'of', 'the', 'parallell', 't... | [-0.14231040957383811, 0.01586983066249209, -0.1185572575309869, 0.10431740453036932, -0.07136386366775976, -0.10793885506259707, -0.009010327304713428, 0.3544153601217728, -0.224597876604933, -0.2355962708305854, 0.11564174049999565, -0.25052977171905627, -0.1546639241851293, 0.21373223970429256, -0.1298327930414906, ... |
1,802.07572 | Information Theoretic Co-Training | This paper introduces an information theoretic co-training objective for
unsupervised learning. We consider the problem of predicting the future. Rather
than predict future sensations (image pixels or sound waves) we predict
"hypotheses" to be confirmed by future sensations. More formally, we assume a
population dist... | cs.LG stat.ML | this paper introduces an information theoretic cotraining objective for unsupervised learning we consider the problem of predicting the future rather than predict future sensations image pixels or sound waves we predict hypotheses to be confirmed by future sensations more formally we assume a population distribution on... | [['this', 'paper', 'introduces', 'an', 'information', 'theoretic', 'cotraining', 'objective', 'for', 'unsupervised', 'learning', 'we', 'consider', 'the', 'problem', 'of', 'predicting', 'the', 'future', 'rather', 'than', 'predict', 'future', 'sensations', 'image', 'pixels', 'or', 'sound', 'waves', 'we', 'predict', 'hypo... | [-0.08164825205732247, 0.04783399861437775, -0.09183703949811924, 0.11265795392134939, -0.07904033071142347, -0.1622635422685348, 0.08622536601512419, 0.3855836526435964, -0.28319457195260944, -0.30522868901162464, 0.08809189464732567, -0.32740200023879024, -0.12430510695968919, 0.15881086667205263, -0.0790670689880190... |
1,802.07573 | Asymmetric Cryptography with Physical Unclonable Keys | Secure communication is of paramount importance in modern society. Asymmetric
cryptography methods such as the widely used RSA method allow secure exchange
of information between parties who have not shared secret keys. However, the
existing asymmetric cryptographic schemes rely on unproven mathematical
assumptions f... | physics.optics quant-ph | secure communication is of paramount importance in modern society asymmetric cryptography methods such as the widely used rsa method allow secure exchange of information between parties who have not shared secret keys however the existing asymmetric cryptographic schemes rely on unproven mathematical assumptions for se... | [['secure', 'communication', 'is', 'of', 'paramount', 'importance', 'in', 'modern', 'society', 'asymmetric', 'cryptography', 'methods', 'such', 'as', 'the', 'widely', 'used', 'rsa', 'method', 'allow', 'secure', 'exchange', 'of', 'information', 'between', 'parties', 'who', 'have', 'not', 'shared', 'secret', 'keys', 'how... | [-0.19705315304557136, 0.057569878945501196, -0.10675214274841197, 0.07311965673323036, -0.07144514956128072, -0.3333101862226613, 0.09661887759541381, 0.43313392553725005, -0.3007957029895967, -0.28990207961075665, 0.12350144669899772, -0.23944418873596826, -0.13109885505914196, 0.23418765092569896, -0.144922797951628... |
1,802.07574 | Higher Hochschild homology and exponential functors | We study higher Hochschild homology evaluated on wedges of circles, viewed as
a functor on the category of free groups. The main results use coefficients
arising from square-zero extensions; this is motivated by work of Turchin and
Willwacher in relation to hairy graph cohomology. The functorial point of view
allows ... | math.AT | we study higher hochschild homology evaluated on wedges of circles viewed as a functor on the category of free groups the main results use coefficients arising from squarezero extensions this is motivated by work of turchin and willwacher in relation to hairy graph cohomology the functorial point of view allows us to e... | [['we', 'study', 'higher', 'hochschild', 'homology', 'evaluated', 'on', 'wedges', 'of', 'circles', 'viewed', 'as', 'a', 'functor', 'on', 'the', 'category', 'of', 'free', 'groups', 'the', 'main', 'results', 'use', 'coefficients', 'arising', 'from', 'squarezero', 'extensions', 'this', 'is', 'motivated', 'by', 'work', 'of... | [-0.17584505163646047, 0.001326660375934148, -0.11387952489346481, 0.10235714353621006, -0.12773190768084663, -0.09531337599796445, -0.02610280433335625, 0.34067982720022183, -0.39801332030607306, -0.2384524582716488, 0.08431586243323577, -0.16827812466310232, -0.16565002517629604, 0.18609250211359366, -0.1947129851281... |
1,802.07575 | Emulating dynamic non-linear simulators using Gaussian processes | The dynamic emulation of non-linear deterministic computer codes where the
output is a time series, possibly multivariate, is examined. Such computer
models simulate the evolution of some real-world phenomenon over time, for
example models of the climate or the functioning of the human brain. The models
we are intere... | stat.ML math.DS stat.AP | the dynamic emulation of nonlinear deterministic computer codes where the output is a time series possibly multivariate is examined such computer models simulate the evolution of some realworld phenomenon over time for example models of the climate or the functioning of the human brain the models we are interested in a... | [['the', 'dynamic', 'emulation', 'of', 'nonlinear', 'deterministic', 'computer', 'codes', 'where', 'the', 'output', 'is', 'a', 'time', 'series', 'possibly', 'multivariate', 'is', 'examined', 'such', 'computer', 'models', 'simulate', 'the', 'evolution', 'of', 'some', 'realworld', 'phenomenon', 'over', 'time', 'for', 'ex... | [-0.1154122315962219, 0.07541204049788199, -0.0943899963167496, 0.07386277080600197, -0.02134854038122971, -0.1433119944495562, 0.009843131181353456, 0.36301667345490063, -0.29457329364519846, -0.3134383728570098, 0.12974628495012097, -0.24842730048002745, -0.18143095541965076, 0.25198747067248783, -0.05618106054344197... |
1,802.07576 | A note on $\mathfrak{gl}_2$-invariant Bethe vectors | We consider $\mathfrak{gl}_2$-invariant quantum integrable models solvable by
the algebraic Bethe ansatz. We show that the form of on-shell Bethe vectors is
preserved under certain twist transformations of the monodromy matrix. We also
derive the actions of the twisted monodromy matrix entries onto twisted
off-shell ... | math-ph hep-th math.MP | we consider mathfrakgl_2invariant quantum integrable models solvable by the algebraic bethe ansatz we show that the form of onshell bethe vectors is preserved under certain twist transformations of the monodromy matrix we also derive the actions of the twisted monodromy matrix entries onto twisted offshell bethe vector... | [['we', 'consider', 'mathfrakgl_2invariant', 'quantum', 'integrable', 'models', 'solvable', 'by', 'the', 'algebraic', 'bethe', 'ansatz', 'we', 'show', 'that', 'the', 'form', 'of', 'onshell', 'bethe', 'vectors', 'is', 'preserved', 'under', 'certain', 'twist', 'transformations', 'of', 'the', 'monodromy', 'matrix', 'we', ... | [-0.25109810600786103, 0.2061267729808131, -0.03954858917985921, 0.10533872246995325, -0.11558187485713026, -0.14181605797595062, -0.006099677184070258, 0.36725187965709233, -0.3256142826133367, -0.09800040191444366, 0.09214575407500177, -0.23824688946099384, -0.22713752003872525, 0.07100496623847309, 0.000533394066619... |
1,802.07577 | Complex Cellular Structures | We introduce the notion of a complex cell, a complexification of the
cells/cylinders used in real tame geometry. For $\delta\in(0,1)$ and a complex
cell $\mathcal{C}$ we define its holomorphic extension
$\mathcal{C}\subset\mathcal{C}^\delta$, which is again a complex cell. The
hyperbolic geometry of $\mathcal{C}$ wit... | math.CV math.AG math.DS math.LO math.NT | we introduce the notion of a complex cell a complexification of the cellscylinders used in real tame geometry for deltain01 and a complex cell mathcalc we define its holomorphic extension mathcalcsubsetmathcalcdelta which is again a complex cell the hyperbolic geometry of mathcalc within mathcalcdelta provides the clas... | [['we', 'introduce', 'the', 'notion', 'of', 'a', 'complex', 'cell', 'a', 'complexification', 'of', 'the', 'cellscylinders', 'used', 'in', 'real', 'tame', 'geometry', 'for', 'deltain01', 'and', 'a', 'complex', 'cell', 'mathcalc', 'we', 'define', 'its', 'holomorphic', 'extension', 'mathcalcsubsetmathcalcdelta', 'which', ... | [-0.1423141313293807, 0.025465931903051655, -0.1171774020334738, 0.10224773284413603, -0.07225117679350207, -0.0799504270854448, 0.04774182655368803, 0.28672885422105016, -0.2931932979376155, -0.2261229684644066, 0.09502720506015881, -0.2289069694036676, -0.18741949710344, 0.22760830488810024, -0.15769938888692114, 0.0... |
1,802.07578 | Improving Recommender Systems Beyond the Algorithm | Recommender systems rely heavily on the predictive accuracy of the learning
algorithm. Most work on improving accuracy has focused on the learning
algorithm itself. We argue that this algorithmic focus is myopic. In
particular, since learning algorithms generally improve with more and better
data, we propose shaping ... | cs.HC cs.IR | recommender systems rely heavily on the predictive accuracy of the learning algorithm most work on improving accuracy has focused on the learning algorithm itself we argue that this algorithmic focus is myopic in particular since learning algorithms generally improve with more and better data we propose shaping the fee... | [['recommender', 'systems', 'rely', 'heavily', 'on', 'the', 'predictive', 'accuracy', 'of', 'the', 'learning', 'algorithm', 'most', 'work', 'on', 'improving', 'accuracy', 'has', 'focused', 'on', 'the', 'learning', 'algorithm', 'itself', 'we', 'argue', 'that', 'this', 'algorithmic', 'focus', 'is', 'myopic', 'in', 'parti... | [-0.08449100098790184, 0.02730981555645198, -0.09028383274562657, 0.047778806799322796, -0.16207152995354446, -0.1643766711747862, 0.10096358687013363, 0.45316442282331226, -0.25787298020517674, -0.36729206541885534, 0.09806527522682461, -0.27076729880890954, -0.1871724207119673, 0.1950798740144819, -0.1257378721248211... |
1,802.07579 | Spin Hartree-Fock approach to quantum Heisenberg antiferromagnets in low
dimensions | We construct a new mean-field theory for quantum (spin-1/2) Heisenberg
antiferromagnet in one (1D) and two (2D) dimensions using a Hartree-Fock
decoupling of the four-point correlation functions. We show that the solution
to the self-consistency equations based on two-point correlation functions does
not produce any ... | cond-mat.mes-hall cond-mat.str-el | we construct a new meanfield theory for quantum spin12 heisenberg antiferromagnet in one 1d and two 2d dimensions using a hartreefock decoupling of the fourpoint correlation functions we show that the solution to the selfconsistency equations based on twopoint correlation functions does not produce any unphysical finit... | [['we', 'construct', 'a', 'new', 'meanfield', 'theory', 'for', 'quantum', 'spin12', 'heisenberg', 'antiferromagnet', 'in', 'one', '1d', 'and', 'two', '2d', 'dimensions', 'using', 'a', 'hartreefock', 'decoupling', 'of', 'the', 'fourpoint', 'correlation', 'functions', 'we', 'show', 'that', 'the', 'solution', 'to', 'the',... | [-0.1275023343985887, 0.13162791229079485, -0.08742658047636863, 0.1000134085819542, -0.018104783751044448, -0.13968852424173506, 0.04686151321414025, 0.3276859588816866, -0.21209903622788567, -0.21207022494180583, 0.029350313104011795, -0.31817788211303155, -0.11412787687675938, 0.16435246037358378, 0.1011988517479853... |
1,802.0758 | Numerical Investigation on Local Non-equilibrium Flows Using a Diatomic
Nonlinear Constitutive Model | The linear Navier-Stokes-Fourier (NSF) constitutive relations are capable of
simulating the near-continuum flows, but fail in description of those flows
which are removed far away from local equilibrium. In this paper, a diatomic
nonlinear model named as nonlinear coupled constitutive relations (NCCR),
derived from E... | physics.flu-dyn physics.comp-ph | the linear navierstokesfourier nsf constitutive relations are capable of simulating the nearcontinuum flows but fail in description of those flows which are removed far away from local equilibrium in this paper a diatomic nonlinear model named as nonlinear coupled constitutive relations nccr derived from eus generalize... | [['the', 'linear', 'navierstokesfourier', 'nsf', 'constitutive', 'relations', 'are', 'capable', 'of', 'simulating', 'the', 'nearcontinuum', 'flows', 'but', 'fail', 'in', 'description', 'of', 'those', 'flows', 'which', 'are', 'removed', 'far', 'away', 'from', 'local', 'equilibrium', 'in', 'this', 'paper', 'a', 'diatomic... | [-0.08761930111180065, 0.062363334133668256, -0.10140133149279172, 0.052444879813436714, -0.034009601589272784, -0.18709462950571748, -0.011334476267330163, 0.34768773267699005, -0.2385951954291168, -0.28665893981190577, 0.09299414793543849, -0.290187050876115, -0.1305478042069608, 0.2153654562099715, -0.01440668255392... |
1,802.07581 | Universal Hypothesis Testing with Kernels: Asymptotically Optimal Tests
for Goodness of Fit | We characterize the asymptotic performance of nonparametric goodness of fit
testing. The exponential decay rate of the type-II error probability is used as
the asymptotic performance metric, and a test is optimal if it achieves the
maximum rate subject to a constant level constraint on the type-I error
probability. W... | stat.ML cs.IT cs.LG math.IT | we characterize the asymptotic performance of nonparametric goodness of fit testing the exponential decay rate of the typeii error probability is used as the asymptotic performance metric and a test is optimal if it achieves the maximum rate subject to a constant level constraint on the typei error probability we show ... | [['we', 'characterize', 'the', 'asymptotic', 'performance', 'of', 'nonparametric', 'goodness', 'of', 'fit', 'testing', 'the', 'exponential', 'decay', 'rate', 'of', 'the', 'typeii', 'error', 'probability', 'is', 'used', 'as', 'the', 'asymptotic', 'performance', 'metric', 'and', 'a', 'test', 'is', 'optimal', 'if', 'it', ... | [-0.06972900618088813, 0.010652887129070733, -0.11651815666663025, 0.16527020130323233, -0.059956083884931725, -0.17446645219616003, 0.11084519558261223, 0.36714787763818135, -0.2618582929558248, -0.2584238836019159, 0.10971530517161214, -0.23269302641852296, -0.11086432706135854, 0.22265041196088997, -0.11150507894914... |
1,802.07582 | Axisymmetric inertial modes in a spherical shell at low Ekman numbers | We investigate the asymptotic properties of axisymmetric inertial modes
propagating in a spherical shell when viscosity tends to zero. We identify
three kinds of eigenmodes whose eigenvalues follow very different laws as the
Ekman number $E$ becomes very small. First are modes associated with attractors
of characteri... | physics.flu-dyn astro-ph.EP astro-ph.SR | we investigate the asymptotic properties of axisymmetric inertial modes propagating in a spherical shell when viscosity tends to zero we identify three kinds of eigenmodes whose eigenvalues follow very different laws as the ekman number e becomes very small first are modes associated with attractors of characteristics ... | [['we', 'investigate', 'the', 'asymptotic', 'properties', 'of', 'axisymmetric', 'inertial', 'modes', 'propagating', 'in', 'a', 'spherical', 'shell', 'when', 'viscosity', 'tends', 'to', 'zero', 'we', 'identify', 'three', 'kinds', 'of', 'eigenmodes', 'whose', 'eigenvalues', 'follow', 'very', 'different', 'laws', 'as', 't... | [-0.20067228609902074, 0.17472122743203194, -0.09149043590279318, 0.032231923839205104, -0.05810629303383732, -0.10557316217480837, -0.015842325739208116, 0.3188070692245609, -0.2829973908286517, -0.22212464261833018, 0.08828472242272352, -0.2750395186538025, -0.13665627647784695, 0.1699493478116192, -0.015320813888838... |
1,802.07583 | Time-series analysis of fissure-fed multi-vent activity: a snapshot from
the July 2014 eruption of Etna volcano (Italy) | On 5 July 2014, an eruptive fissure opened on the eastern flank of Etna
volcano (Italy) at ~3.000 m a.s.l. Strombolian activity and lava effusion
occurred simultaneously at two neighbouring vents. In the following weeks,
eruptive activity led to the build-up of two cones, tens of meters high, here
named Crater N and ... | physics.geo-ph | on 5 july 2014 an eruptive fissure opened on the eastern flank of etna volcano italy at 3000 m asl strombolian activity and lava effusion occurred simultaneously at two neighbouring vents in the following weeks eruptive activity led to the buildup of two cones tens of meters high here named crater n and crater s to cha... | [['on', '5', 'july', '2014', 'an', 'eruptive', 'fissure', 'opened', 'on', 'the', 'eastern', 'flank', 'of', 'etna', 'volcano', 'italy', 'at', '3000', 'm', 'asl', 'strombolian', 'activity', 'and', 'lava', 'effusion', 'occurred', 'simultaneously', 'at', 'two', 'neighbouring', 'vents', 'in', 'the', 'following', 'weeks', 'e... | [-0.09663350345979804, 0.16854152589627372, -0.049020302887053765, 0.05175044193431618, -0.05358259381951906, -0.11688245326017485, 0.06933398600333608, 0.36714492405601884, -0.20284110642818215, -0.38602140472341545, 0.10509433176651943, -0.3064450529809089, -0.10860939133657047, 0.21063022961372285, -0.09196078790573... |
1,802.07584 | DeepASL: Enabling Ubiquitous and Non-Intrusive Word and Sentence-Level
Sign Language Translation | There is an undeniable communication barrier between deaf people and people
with normal hearing ability. Although innovations in sign language translation
technology aim to tear down this communication barrier, the majority of
existing sign language translation systems are either intrusive or constrained
by resolutio... | cs.CV | there is an undeniable communication barrier between deaf people and people with normal hearing ability although innovations in sign language translation technology aim to tear down this communication barrier the majority of existing sign language translation systems are either intrusive or constrained by resolution or... | [['there', 'is', 'an', 'undeniable', 'communication', 'barrier', 'between', 'deaf', 'people', 'and', 'people', 'with', 'normal', 'hearing', 'ability', 'although', 'innovations', 'in', 'sign', 'language', 'translation', 'technology', 'aim', 'to', 'tear', 'down', 'this', 'communication', 'barrier', 'the', 'majority', 'of... | [-0.10212883183015259, 0.044278330695256905, -0.021042443581422588, 0.1158811511481831, -0.17131752828828287, -0.20124380020970092, 0.11907878686539694, 0.4607789773191955, -0.273470315192868, -0.36746053740189216, 0.03337075428561064, -0.2956541793018177, -0.14949753980135527, 0.19126623496963843, -0.1862447320707295,... |
1,802.07585 | Maximising Bernoulli measures and dimension gaps for countable branched
systems | Kifer, Peres, and Weiss proved that there exists $c_0>0,$ such that $\dim
\mu\leq 1-c_0$ for any probability measure $\mu$ which makes the digits of the
continued fraction expansion i.i.d. random variables. In this paper we prove
that amongst this class of measures, there exists one whose dimension is
maximal. Our re... | math.DS | kifer peres and weiss proved that there exists c_00 such that dim muleq 1c_0 for any probability measure mu which makes the digits of the continued fraction expansion iid random variables in this paper we prove that amongst this class of measures there exists one whose dimension is maximal our results also apply in the... | [['kifer', 'peres', 'and', 'weiss', 'proved', 'that', 'there', 'exists', 'c_00', 'such', 'that', 'dim', 'muleq', '1c_0', 'for', 'any', 'probability', 'measure', 'mu', 'which', 'makes', 'the', 'digits', 'of', 'the', 'continued', 'fraction', 'expansion', 'iid', 'random', 'variables', 'in', 'this', 'paper', 'we', 'prove',... | [-0.14456619927468786, 0.15886748734037162, -0.06254358130094946, 0.07010135688765555, -0.02888190478361288, -0.15588168885375633, 0.10350158806035265, 0.3400694346208064, -0.2523875698508298, -0.13676414399820028, 0.09212164407534922, -0.30673989233728804, -0.19422279218723235, 0.20848850630410778, -0.1340114753311652... |
1,802.07586 | Global Spherical Tropicalization via Toric Embeddings | The first steps in defining tropicalization for spherical varieties have been
taken in the last few years. There are two parts to this theory: tropicalizing
subvarieties of homogeneous spaces and tropicalizing their closures in
spherical embeddings. In this paper, we obtain a new description of spherical
tropicalizat... | math.AG | the first steps in defining tropicalization for spherical varieties have been taken in the last few years there are two parts to this theory tropicalizing subvarieties of homogeneous spaces and tropicalizing their closures in spherical embeddings in this paper we obtain a new description of spherical tropicalization th... | [['the', 'first', 'steps', 'in', 'defining', 'tropicalization', 'for', 'spherical', 'varieties', 'have', 'been', 'taken', 'in', 'the', 'last', 'few', 'years', 'there', 'are', 'two', 'parts', 'to', 'this', 'theory', 'tropicalizing', 'subvarieties', 'of', 'homogeneous', 'spaces', 'and', 'tropicalizing', 'their', 'closure... | [-0.09159625358023178, 0.04282068385175247, -0.11580002964099591, 0.06393925086782452, -0.060965462405791225, -0.09140530656273851, -0.048579934140099965, 0.37891749774330646, -0.32646849914721543, -0.186879626180891, 0.08791650773224088, -0.22961563355792527, -0.1668277527566935, 0.19017769567582798, -0.17710736333713... |
1,802.07587 | Attaining the ultimate precision limit in quantum state estimation | We derive a bound on the precision of state estimation for finite dimensional
quantum systems and prove its attainability in the generic case where the
spectrum is non-degenerate. Our results hold under an assumption called local
asymptotic covariance, which is weaker than unbiasedness or local unbiasedness.
The deri... | quant-ph math-ph math.MP | we derive a bound on the precision of state estimation for finite dimensional quantum systems and prove its attainability in the generic case where the spectrum is nondegenerate our results hold under an assumption called local asymptotic covariance which is weaker than unbiasedness or local unbiasedness the derivation... | [['we', 'derive', 'a', 'bound', 'on', 'the', 'precision', 'of', 'state', 'estimation', 'for', 'finite', 'dimensional', 'quantum', 'systems', 'and', 'prove', 'its', 'attainability', 'in', 'the', 'generic', 'case', 'where', 'the', 'spectrum', 'is', 'nondegenerate', 'our', 'results', 'hold', 'under', 'an', 'assumption', '... | [-0.10549013103049544, 0.0736550921870316, -0.095787067408904, 0.06157317562466764, -0.027550988535553513, -0.13647218771961214, 0.05261945819406134, 0.31158795761921915, -0.22813648053117577, -0.2563322149401549, 0.13752443704951214, -0.2195153109519512, -0.11664271441813891, 0.20735691133702155, -0.09166987454530202,... |
1,802.07588 | W-Types with Reductions and the Small Object Argument | We define a simple kind of higher inductive type generalising dependent
$W$-types, which we refer to as $W$-types with reductions. Just as dependent
$W$-types can be characterised as initial algebras of certain endofunctors
(referred to as polynomial endofunctors), we will define our generalisation as
initial algebra... | math.CT math.LO | we define a simple kind of higher inductive type generalising dependent wtypes which we refer to as wtypes with reductions just as dependent wtypes can be characterised as initial algebras of certain endofunctors referred to as polynomial endofunctors we will define our generalisation as initial algebras of certain poi... | [['we', 'define', 'a', 'simple', 'kind', 'of', 'higher', 'inductive', 'type', 'generalising', 'dependent', 'wtypes', 'which', 'we', 'refer', 'to', 'as', 'wtypes', 'with', 'reductions', 'just', 'as', 'dependent', 'wtypes', 'can', 'be', 'characterised', 'as', 'initial', 'algebras', 'of', 'certain', 'endofunctors', 'refer... | [-0.13451221395683075, 0.10073403260737125, -0.07928718042066543, 0.13994406366241274, -0.14249021699652076, -0.14957468157600878, -0.024117443909441743, 0.3757413027231537, -0.34246263597604065, -0.2521875230307896, 0.09054425721738621, -0.1965136769382904, -0.14350890345494485, 0.20474794781434216, -0.177668322066199... |
1,802.07589 | Collaboratively Weighting Deep and Classic Representation via L2
Regularization for Image Classification | Deep convolutional neural networks provide a powerful feature learning
capability for image classification. The deep image features can be utilized to
deal with many image understanding tasks like image classification and object
recognition. However, the robustness obtained in one dataset can be hardly
reproduced in ... | cs.CV | deep convolutional neural networks provide a powerful feature learning capability for image classification the deep image features can be utilized to deal with many image understanding tasks like image classification and object recognition however the robustness obtained in one dataset can be hardly reproduced in the o... | [['deep', 'convolutional', 'neural', 'networks', 'provide', 'a', 'powerful', 'feature', 'learning', 'capability', 'for', 'image', 'classification', 'the', 'deep', 'image', 'features', 'can', 'be', 'utilized', 'to', 'deal', 'with', 'many', 'image', 'understanding', 'tasks', 'like', 'image', 'classification', 'and', 'obj... | [-0.008046883368804892, -0.06281755432078147, -0.10108540849735273, 0.07420724278028287, -0.133027767319292, -0.205183932582915, -0.018905440053434416, 0.46795069874528256, -0.31023298082424994, -0.3207931759154653, 0.0824906577419659, -0.28610864388358026, -0.18653014833655426, 0.22152674595830354, -0.1241645516658371... |
1,802.0759 | Batch Normalization and the impact of batch structure on the behavior of
deep convolution networks | Batch normalization was introduced in 2015 to speed up training of deep
convolution networks by normalizing the activations across the current batch to
have zero mean and unity variance. The results presented here show an
interesting aspect of batch normalization, where controlling the shape of the
training batches c... | cs.CV | batch normalization was introduced in 2015 to speed up training of deep convolution networks by normalizing the activations across the current batch to have zero mean and unity variance the results presented here show an interesting aspect of batch normalization where controlling the shape of the training batches can i... | [['batch', 'normalization', 'was', 'introduced', 'in', '2015', 'to', 'speed', 'up', 'training', 'of', 'deep', 'convolution', 'networks', 'by', 'normalizing', 'the', 'activations', 'across', 'the', 'current', 'batch', 'to', 'have', 'zero', 'mean', 'and', 'unity', 'variance', 'the', 'results', 'presented', 'here', 'show'... | [-0.04122247414921436, 0.07935256284002429, -0.04351819186798624, 0.08256572793628014, -0.09955587626208325, -0.17143608675262814, 0.0766253411612549, 0.4389725658539179, -0.29294906842547497, -0.34955494577518187, 0.09745795618981828, -0.2543946754690763, -0.09905304409613883, 0.20616585732613865, -0.11767692881686663... |
1,802.07591 | Least Square Error Method Robustness of Computation: What is not usually
considered and taught | There are many practical applications based on the Least Square Error (LSE)
approximation. It is based on a square error minimization 'on a vertical' axis.
The LSE method is simple and easy also for analytical purposes. However, if
data span is large over several magnitudes or non-linear LSE is used, severe
numerical... | cs.GR cs.CV | there are many practical applications based on the least square error lse approximation it is based on a square error minimization on a vertical axis the lse method is simple and easy also for analytical purposes however if data span is large over several magnitudes or nonlinear lse is used severe numerical instability... | [['there', 'are', 'many', 'practical', 'applications', 'based', 'on', 'the', 'least', 'square', 'error', 'lse', 'approximation', 'it', 'is', 'based', 'on', 'a', 'square', 'error', 'minimization', 'on', 'a', 'vertical', 'axis', 'the', 'lse', 'method', 'is', 'simple', 'and', 'easy', 'also', 'for', 'analytical', 'purposes... | [-0.06573238628586446, 0.013465052303733436, -0.09048604001850256, 0.10326820742943889, -0.1031044884566511, -0.14218400069604092, -0.002879456682937352, 0.43807296014911545, -0.2683271381446696, -0.22762646287034347, 0.23228130492062754, -0.25571250153900726, -0.16361331480085908, 0.26501363017009644, -0.0508540809467... |
1,802.07592 | "How to squash a mathematical tomato", Rubic's cube-like surfaces and
their connection to reversible computation | Here we show how reversible computation processes, like Margolus diffusion,
can be envisioned as physical turning operations on a 2-dimensional rigid
surface that is cut by a regular pattern of intersecting circles. We then
briefly explore the design-space of these patterns, and report on the discovery
of an interest... | cs.GR | here we show how reversible computation processes like margolus diffusion can be envisioned as physical turning operations on a 2dimensional rigid surface that is cut by a regular pattern of intersecting circles we then briefly explore the designspace of these patterns and report on the discovery of an interesting frac... | [['here', 'we', 'show', 'how', 'reversible', 'computation', 'processes', 'like', 'margolus', 'diffusion', 'can', 'be', 'envisioned', 'as', 'physical', 'turning', 'operations', 'on', 'a', '2dimensional', 'rigid', 'surface', 'that', 'is', 'cut', 'by', 'a', 'regular', 'pattern', 'of', 'intersecting', 'circles', 'we', 'the... | [-0.14837224912198801, 0.15706828837573994, -0.12645094251881042, 0.08399627402534969, -0.09351128283687817, -0.12725495777383286, 0.03792994575554966, 0.38586156358641965, -0.3120338853889255, -0.27775376724700135, 0.1365339716455789, -0.24546848178430591, -0.26417894076596027, 0.22352419940814858, -0.0669637447249980... |
1,802.07593 | From Hamiltonian to zero curvature formulation for classical integrable
boundary conditions | We reconcile the Hamiltonian formalism and the zero curvature representation
in the approach to integrable boundary conditions for a classical integrable
system in 1+1 space-time dimensions. We start from an ultralocal Poisson
algebra involving a Lax matrix and two (dynamical) boundary matrices.
Sklyanin's formula fo... | math-ph hep-th math.MP nlin.SI | we reconcile the hamiltonian formalism and the zero curvature representation in the approach to integrable boundary conditions for a classical integrable system in 11 spacetime dimensions we start from an ultralocal poisson algebra involving a lax matrix and two dynamical boundary matrices sklyanins formula for the dou... | [['we', 'reconcile', 'the', 'hamiltonian', 'formalism', 'and', 'the', 'zero', 'curvature', 'representation', 'in', 'the', 'approach', 'to', 'integrable', 'boundary', 'conditions', 'for', 'a', 'classical', 'integrable', 'system', 'in', '11', 'spacetime', 'dimensions', 'we', 'start', 'from', 'an', 'ultralocal', 'poisson'... | [-0.14542179252542278, 0.08786705237782452, -0.060745237735725606, 0.09277106791911925, -0.06817447684302147, -0.1633729597939345, -0.04096996050272415, 0.2850484633266599, -0.2793793942007834, -0.2212222566960185, 0.10748249109410472, -0.2426734037815468, -0.1738748107115919, 0.14250475459092699, -0.03351060668729357,... |
1,802.07594 | Constructions of Unextendible Maximally Entangled Bases in \(\mathbb
{C}^{d}\otimes \mathbb {C}^{d^{\prime}}\) | We study unextendible maximally entangled bases (UMEBs) in \(\mathbb
{C}^{d}\otimes \mathbb {C}^{d^{\prime}}\) ($d<d'$). An operational method to
construct UMEBs containing $d(d^{\prime}-1)$ maximally entangled vectors is
established, and two UMEBs in \(\mathbb {C}^{5}\otimes \mathbb {C}^{6}\) and
\(\mathbb {C}^{5}\o... | quant-ph | we study unextendible maximally entangled bases umebs in mathbb cdotimes mathbb cdprime dd an operational method to construct umebs containing ddprime1 maximally entangled vectors is established and two umebs in mathbb c5otimes mathbb c6 and mathbb c5otimes mathbb c12 are given as examples furthermore a systematic way ... | [['we', 'study', 'unextendible', 'maximally', 'entangled', 'bases', 'umebs', 'in', 'mathbb', 'cdotimes', 'mathbb', 'cdprime', 'dd', 'an', 'operational', 'method', 'to', 'construct', 'umebs', 'containing', 'ddprime1', 'maximally', 'entangled', 'vectors', 'is', 'established', 'and', 'two', 'umebs', 'in', 'mathbb', 'c5oti... | [-0.20397954938166282, 0.15901966226781095, 0.07433896056061391, -0.028645604961853036, 0.07533600707949303, -0.21497998113559066, -0.10255244280458153, 0.39385994501850186, -0.22487005536608837, -0.05712642211823121, 0.09366287881344118, -0.3581042297951439, -0.03348643660052296, 0.17007225855965824, -0.11000148765742... |
1,802.07595 | Smooth Loss Functions for Deep Top-k Classification | The top-k error is a common measure of performance in machine learning and
computer vision. In practice, top-k classification is typically performed with
deep neural networks trained with the cross-entropy loss. Theoretical results
indeed suggest that cross-entropy is an optimal learning objective for such a
task in ... | cs.LG | the topk error is a common measure of performance in machine learning and computer vision in practice topk classification is typically performed with deep neural networks trained with the crossentropy loss theoretical results indeed suggest that crossentropy is an optimal learning objective for such a task in the limit... | [['the', 'topk', 'error', 'is', 'a', 'common', 'measure', 'of', 'performance', 'in', 'machine', 'learning', 'and', 'computer', 'vision', 'in', 'practice', 'topk', 'classification', 'is', 'typically', 'performed', 'with', 'deep', 'neural', 'networks', 'trained', 'with', 'the', 'crossentropy', 'loss', 'theoretical', 'res... | [-0.06441542121353856, -0.008212779959579534, -0.09138117095534788, 0.10571008389815688, -0.09085281129847182, -0.15172706443340855, 0.07079369024611376, 0.45062573745529705, -0.2723759676607207, -0.3180335212954657, 0.08096340005087885, -0.263250623614666, -0.20666128706504056, 0.21857441309492717, -0.1468413434625464... |
1,802.07596 | Maximal depth property of finitely generated modules | Let $(R,\mathfrak{m})$ be a Noetherian local ring and $M$ a finitely
generated $R$-module. We say $M$ has maximal depth if there is an associated
prime $\mathfrak{p}$ of $M$ such that depth $M=\dim R/\mathfrak{p}$. In this
paper, we study finitely generated modules with maximal depth. It is shown that
the maximal dep... | math.AC | let rmathfrakm be a noetherian local ring and m a finitely generated rmodule we say m has maximal depth if there is an associated prime mathfrakp of m such that depth mdim rmathfrakp in this paper we study finitely generated modules with maximal depth it is shown that the maximal depth property is preserved under some ... | [['let', 'rmathfrakm', 'be', 'a', 'noetherian', 'local', 'ring', 'and', 'm', 'a', 'finitely', 'generated', 'rmodule', 'we', 'say', 'm', 'has', 'maximal', 'depth', 'if', 'there', 'is', 'an', 'associated', 'prime', 'mathfrakp', 'of', 'm', 'such', 'that', 'depth', 'mdim', 'rmathfrakp', 'in', 'this', 'paper', 'we', 'study'... | [-0.2203929126737517, 0.12348286838345016, -0.055175066165822115, 0.0009601193780422603, -0.024897360083598056, -0.24086611476530762, -0.14265810911341473, 0.4023903389951508, -0.4163557815757629, -0.14774642971851312, 0.11644960363168809, -0.25132151244600354, -0.10024877588607763, 0.2210588172249692, -0.1759705805115... |
1,802.07597 | On a problem of S\'ark\"ozy and S\'os for multivariate linear forms | We prove that for pairwise co-prime numbers $k_1,\dots,k_d \geq 2$ there does
not exist any infinite set of positive integers $A$ such that the
representation function $r_A (n) = \{ (a_1, \dots, a_d) \in A^d : k_1 a_1 +
\dots + k_d a_d = n \}$ becomes constant for $n$ large enough. This result is a
particular case of... | math.CO | we prove that for pairwise coprime numbers k_1dotsk_d geq 2 there does not exist any infinite set of positive integers a such that the representation function r_a n a_1 dots a_d in ad k_1 a_1 dots k_d a_d n becomes constant for n large enough this result is a particular case of our main theorem which poses a further st... | [['we', 'prove', 'that', 'for', 'pairwise', 'coprime', 'numbers', 'k_1dotsk_d', 'geq', '2', 'there', 'does', 'not', 'exist', 'any', 'infinite', 'set', 'of', 'positive', 'integers', 'a', 'such', 'that', 'the', 'representation', 'function', 'r_a', 'n', 'a_1', 'dots', 'a_d', 'in', 'ad', 'k_1', 'a_1', 'dots', 'k_d', 'a_d',... | [-0.20728002073542204, 0.13910265317054488, -0.023330222240384713, 0.02240784910082081, -0.037114936858415604, -0.22200721375253282, 0.017659222465698367, 0.31357086288892194, -0.2692264366613264, -0.22827241833057302, 0.05935793336521098, -0.28633984842878063, -0.14849220015637485, 0.19168680093975532, -0.042572730409... |
1,802.07598 | Design of Irregular SC-LDPC Codes With Non-Uniform Degree Distributions
by Linear Programing | In this paper, we propose a new design method of irregular spatially-coupled
low-density parity-check (SC-LDPC) codes with non-uniform degree distributions
by linear programming (LP). In general, irregular SC-LDPC codes with
non-uniform degree distributions is difficult to design with low complexity
because their den... | cs.IT math.IT | in this paper we propose a new design method of irregular spatiallycoupled lowdensity paritycheck scldpc codes with nonuniform degree distributions by linear programming lp in general irregular scldpc codes with nonuniform degree distributions is difficult to design with low complexity because their density evolution e... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'new', 'design', 'method', 'of', 'irregular', 'spatiallycoupled', 'lowdensity', 'paritycheck', 'scldpc', 'codes', 'with', 'nonuniform', 'degree', 'distributions', 'by', 'linear', 'programming', 'lp', 'in', 'general', 'irregular', 'scldpc', 'codes', 'with', 'nonuniform', 'd... | [-0.1595927043199732, 0.02229297567191052, -0.10757834621030708, 0.07524393777812606, -0.026605489933542135, -0.23188865955854798, 0.01906824135783546, 0.4107697217307728, -0.31761692141921355, -0.27714143008644015, 0.10498763352455892, -0.18450113875341825, -0.2169910347346088, 0.18214343620528434, -0.1336315977740390... |
1,802.07599 | Graphene-enabled, directed nanomaterial placement from solution for
large-scale device integration | Controlled placement of nanomaterials at predefined locations with nanoscale
precision remains among the most challenging problems that inhibit their
large-scale integration in the field of semiconductor process technology.
Methods based on surface functionalization have a drawback where undesired
chemical modificati... | physics.app-ph cond-mat.mes-hall | controlled placement of nanomaterials at predefined locations with nanoscale precision remains among the most challenging problems that inhibit their largescale integration in the field of semiconductor process technology methods based on surface functionalization have a drawback where undesired chemical modifications ... | [['controlled', 'placement', 'of', 'nanomaterials', 'at', 'predefined', 'locations', 'with', 'nanoscale', 'precision', 'remains', 'among', 'the', 'most', 'challenging', 'problems', 'that', 'inhibit', 'their', 'largescale', 'integration', 'in', 'the', 'field', 'of', 'semiconductor', 'process', 'technology', 'methods', '... | [-0.10753989533926578, 0.12979656993720615, -0.009731491940781243, -0.07899714937915057, -0.04133623977700837, -0.2011123151202334, 0.07179871008736251, 0.48107284409780576, -0.2677558641235339, -0.3480801236926737, 0.0753674517166101, -0.2520091473287782, -0.11675641328154296, 0.24276611609312035, -0.01727417992051555... |
1,802.076 | Randomized sliding window algorithms for regular languages | A sliding window algorithm receives a stream of symbols and has to output at
each time instant a certain value which only depends on the last $n$ symbols.
If the algorithm is randomized, then at each time instant it produces an
incorrect output with probability at most $\epsilon$, which is a constant error
bound. Thi... | cs.FL cs.DS | a sliding window algorithm receives a stream of symbols and has to output at each time instant a certain value which only depends on the last n symbols if the algorithm is randomized then at each time instant it produces an incorrect output with probability at most epsilon which is a constant error bound this work prop... | [['a', 'sliding', 'window', 'algorithm', 'receives', 'a', 'stream', 'of', 'symbols', 'and', 'has', 'to', 'output', 'at', 'each', 'time', 'instant', 'a', 'certain', 'value', 'which', 'only', 'depends', 'on', 'the', 'last', 'n', 'symbols', 'if', 'the', 'algorithm', 'is', 'randomized', 'then', 'at', 'each', 'time', 'insta... | [-0.1506905162698896, 0.10109293910373955, -0.08666831381199074, 0.023108247555846166, -0.08203756682994652, -0.19448165782334315, 0.11879767576179391, 0.3456055287357872, -0.28781671531503816, -0.28934652816418105, 0.09186780831919218, -0.22290393276236994, -0.12934438364292264, 0.19378692681653523, -0.107944706890925... |
1,802.07601 | Coupling non-conforming discretizations of PDEs by spectral
approximation of the Lagrange multiplier space | This work focuses on the development of a non-conforming domain decomposition
method for the approximation of PDEs based on weakly imposed transmission
conditions: the continuity of the global solution is enforced by a discrete
number of Lagrange multipliers defined over the interfaces of adjacent
subdomains. The met... | math.NA cs.CE cs.NA | this work focuses on the development of a nonconforming domain decomposition method for the approximation of pdes based on weakly imposed transmission conditions the continuity of the global solution is enforced by a discrete number of lagrange multipliers defined over the interfaces of adjacent subdomains the method f... | [['this', 'work', 'focuses', 'on', 'the', 'development', 'of', 'a', 'nonconforming', 'domain', 'decomposition', 'method', 'for', 'the', 'approximation', 'of', 'pdes', 'based', 'on', 'weakly', 'imposed', 'transmission', 'conditions', 'the', 'continuity', 'of', 'the', 'global', 'solution', 'is', 'enforced', 'by', 'a', 'd... | [-0.08475598137368236, 0.03709667746783697, -0.11984158019203017, -0.0035003691771113973, -0.06651378533944531, -0.11101086708384822, 0.028506854762818817, 0.36867881551036363, -0.327824465355874, -0.259932674867869, 0.1417718307436471, -0.229343048596417, -0.11420245207464921, 0.18103985022481162, -0.02966976843022725... |
1,802.07602 | Wake of inertial waves of a horizontal cylinder in horizontal
translation | We analyze theoretically and experimentally the wake behind a horizontal
cylinder of diameter $d$ horizontally translated at constant velocity $U$ in a
fluid rotating about the vertical axis at a rate $\Omega$. Using particle image
velocimetry measurements in the rotating frame, we show that the wake is
stabilized by... | physics.flu-dyn physics.geo-ph | we analyze theoretically and experimentally the wake behind a horizontal cylinder of diameter d horizontally translated at constant velocity u in a fluid rotating about the vertical axis at a rate omega using particle image velocimetry measurements in the rotating frame we show that the wake is stabilized by rotation f... | [['we', 'analyze', 'theoretically', 'and', 'experimentally', 'the', 'wake', 'behind', 'a', 'horizontal', 'cylinder', 'of', 'diameter', 'd', 'horizontally', 'translated', 'at', 'constant', 'velocity', 'u', 'in', 'a', 'fluid', 'rotating', 'about', 'the', 'vertical', 'axis', 'at', 'a', 'rate', 'omega', 'using', 'particle'... | [-0.18026227537383785, 0.2040770818933486, -0.05735736432531419, 0.029274248688422804, -0.035155951686006055, -0.10498046675538172, 0.012147466877415296, 0.30206269409490344, -0.26138786561486704, -0.3071046925282904, 0.07858445397942984, -0.24155212017441435, -0.047655587710122564, 0.20609313952371752, -0.037321753149... |
1,802.07603 | RichMol: A general variational approach for rovibrational molecular
dynamics in external electric fields | A general variational approach for computing the rovibrational dynamics of
polyatomic molecules in the presence of external electric fields is presented.
Highly accurate, full-dimensional variational calculations provide a basis of
field-free rovibrational states for evaluating the rovibrational matrix
elements of hi... | physics.chem-ph | a general variational approach for computing the rovibrational dynamics of polyatomic molecules in the presence of external electric fields is presented highly accurate fulldimensional variational calculations provide a basis of fieldfree rovibrational states for evaluating the rovibrational matrix elements of highrank... | [['a', 'general', 'variational', 'approach', 'for', 'computing', 'the', 'rovibrational', 'dynamics', 'of', 'polyatomic', 'molecules', 'in', 'the', 'presence', 'of', 'external', 'electric', 'fields', 'is', 'presented', 'highly', 'accurate', 'fulldimensional', 'variational', 'calculations', 'provide', 'a', 'basis', 'of',... | [-0.1434929342392613, 0.12619038329749788, -0.03547059479678253, 0.03527567647162731, -0.03624828376400308, -0.09342925239182195, -0.0117360529653188, 0.4229127884756367, -0.22513166684344285, -0.2838421607499613, 0.02478337780368992, -0.20041116699772035, -0.07898078896613996, 0.15820507772908615, 0.0974057393164194, ... |
1,802.07604 | Long gaps in sieved sets | For each prime $p$, let $I_p \subset \mathbb{Z}/p\mathbb{Z}$ denote a
collection of residue classes modulo $p$ such that the cardinalities $|I_p|$
are bounded and about $1$ on average. We show that for sufficiently large $x$,
the sifted set $\{ n \in \mathbb{Z}: n \pmod{p} \not \in I_p \hbox{ for all }p
\leq x\}$ con... | math.NT | for each prime p let i_p subset mathbbzpmathbbz denote a collection of residue classes modulo p such that the cardinalities i_p are bounded and about 1 on average we show that for sufficiently large x the sifted set n in mathbbz n pmodp not in i_p hbox for all p leq x contains gaps of size at least x log xdelta where d... | [['for', 'each', 'prime', 'p', 'let', 'i_p', 'subset', 'mathbbzpmathbbz', 'denote', 'a', 'collection', 'of', 'residue', 'classes', 'modulo', 'p', 'such', 'that', 'the', 'cardinalities', 'i_p', 'are', 'bounded', 'and', 'about', '1', 'on', 'average', 'we', 'show', 'that', 'for', 'sufficiently', 'large', 'x', 'the', 'sift... | [-0.25538480255818286, 0.1556587442247519, 0.008089057777397102, -0.017138736800006882, 0.01938714505013195, -0.22773025016795145, 0.044666126334050205, 0.29450094274943694, -0.287284869227733, -0.22988313620953704, 0.007985321955857216, -0.36332714529999066, -0.0034912777118734084, 0.19550741623243084, -0.049330016761... |
1,802.07605 | Accelerating crystal structure prediction by machine-learning
interatomic potentials with active learning | In this letter we propose a new methodology for crystal structure prediction,
which is based on the evolutionary algorithm USPEX and the machine-learning
interatomic potentials actively learning on-the-fly. Our methodology allows for
an automated construction of an interatomic interaction model from scratch
replacing... | cond-mat.mtrl-sci | in this letter we propose a new methodology for crystal structure prediction which is based on the evolutionary algorithm uspex and the machinelearning interatomic potentials actively learning onthefly our methodology allows for an automated construction of an interatomic interaction model from scratch replacing the ex... | [['in', 'this', 'letter', 'we', 'propose', 'a', 'new', 'methodology', 'for', 'crystal', 'structure', 'prediction', 'which', 'is', 'based', 'on', 'the', 'evolutionary', 'algorithm', 'uspex', 'and', 'the', 'machinelearning', 'interatomic', 'potentials', 'actively', 'learning', 'onthefly', 'our', 'methodology', 'allows', ... | [-0.031071374795399606, 0.056493659950094297, -0.09084635874070227, 0.024410510286688804, -0.02628976881422568, -0.15394948979467155, 0.07573478785902261, 0.45828965765237806, -0.23900954972207547, -0.3298055467233062, 0.023109562030062078, -0.2584871224035742, -0.18255977695062756, 0.197511833390221, -0.00860215698927... |
1,802.07606 | Ordered Preference Elicitation Strategies for Supporting Multi-Objective
Decision Making | In multi-objective decision planning and learning, much attention is paid to
producing optimal solution sets that contain an optimal policy for every
possible user preference profile. We argue that the step that follows, i.e,
determining which policy to execute by maximising the user's intrinsic utility
function over... | cs.LG cs.AI stat.ML | in multiobjective decision planning and learning much attention is paid to producing optimal solution sets that contain an optimal policy for every possible user preference profile we argue that the step that follows ie determining which policy to execute by maximising the users intrinsic utility function over this pos... | [['in', 'multiobjective', 'decision', 'planning', 'and', 'learning', 'much', 'attention', 'is', 'paid', 'to', 'producing', 'optimal', 'solution', 'sets', 'that', 'contain', 'an', 'optimal', 'policy', 'for', 'every', 'possible', 'user', 'preference', 'profile', 'we', 'argue', 'that', 'the', 'step', 'that', 'follows', 'i... | [-0.056601111460581756, -0.007408459187358398, -0.08604733519036364, 0.08559312257559949, -0.14071768480405378, -0.1347423590970843, 0.1404071990969549, 0.46006354528447885, -0.23203690021018905, -0.3085648820740746, 0.08394727450233015, -0.2918630416552128, -0.19136169466995792, 0.17327724768665065, -0.095739745463668... |
1,802.07607 | Regularity of minimal surfaces with lower dimensional obstacles | We study the Plateau problem with a lower dimensional obstacle in
$\mathbb{R}^n$. Intuitively, in $\mathbb{R}^3$ this corresponds to a soap film
(spanning a given contour) that is pushed from below by a "vertical" 2D
half-space (or some smooth deformation of it). We establish almost optimal
$C^{1,1/2-}$ estimates for... | math.AP | we study the plateau problem with a lower dimensional obstacle in mathbbrn intuitively in mathbbr3 this corresponds to a soap film spanning a given contour that is pushed from below by a vertical 2d halfspace or some smooth deformation of it we establish almost optimal c112 estimates for the solutions near points on th... | [['we', 'study', 'the', 'plateau', 'problem', 'with', 'a', 'lower', 'dimensional', 'obstacle', 'in', 'mathbbrn', 'intuitively', 'in', 'mathbbr3', 'this', 'corresponds', 'to', 'a', 'soap', 'film', 'spanning', 'a', 'given', 'contour', 'that', 'is', 'pushed', 'from', 'below', 'by', 'a', 'vertical', '2d', 'halfspace', 'or'... | [-0.12889616970418008, 0.06660075925384669, -0.09379831398105097, 0.04715256153169504, -0.05990369685591673, -0.14966999150156599, 0.03646374340959877, 0.35640422028120394, -0.26921633618104757, -0.2590291829415123, 0.12398606987374267, -0.2763550871479436, -0.13383467681266648, 0.22852841267836685, -0.1265132353471229... |
1,802.07608 | Learning to Synthesize | In many scenarios we need to find the most likely program under a local
context, where the local context can be an incomplete program, a partial
specification, natural language description, etc. We call such problem program
estimation. In this paper we propose an abstract framework, learning to
synthesis, or L2S in s... | cs.SE | in many scenarios we need to find the most likely program under a local context where the local context can be an incomplete program a partial specification natural language description etc we call such problem program estimation in this paper we propose an abstract framework learning to synthesis or l2s in short to ad... | [['in', 'many', 'scenarios', 'we', 'need', 'to', 'find', 'the', 'most', 'likely', 'program', 'under', 'a', 'local', 'context', 'where', 'the', 'local', 'context', 'can', 'be', 'an', 'incomplete', 'program', 'a', 'partial', 'specification', 'natural', 'language', 'description', 'etc', 'we', 'call', 'such', 'problem', 'p... | [-0.07016737343842425, -0.004471474529959931, -0.08490089525059226, 0.09897096999577845, -0.13375122522809296, -0.14497344513032315, 0.0733238019005301, 0.38619847342502417, -0.27907478414388187, -0.36244516669894045, 0.14411053055495807, -0.2424117255380044, -0.12349446003037338, 0.2007830333603537, -0.082855209903926... |
1,802.07609 | Distribution of Large Gaps Between Primes | We survey some past conditional results on the distribution of large
differences between consecutive primes and examine how the Hardy-Littlewood
prime k-tuples conjecture can be applied to this question.
| math.NT | we survey some past conditional results on the distribution of large differences between consecutive primes and examine how the hardylittlewood prime ktuples conjecture can be applied to this question | [['we', 'survey', 'some', 'past', 'conditional', 'results', 'on', 'the', 'distribution', 'of', 'large', 'differences', 'between', 'consecutive', 'primes', 'and', 'examine', 'how', 'the', 'hardylittlewood', 'prime', 'ktuples', 'conjecture', 'can', 'be', 'applied', 'to', 'this', 'question']] | [-0.1687838600563078, 0.10434979982352977, -0.1590483171287282, 0.18357879878423208, -0.08237935435669176, -0.05228587246403612, 0.025953439289125902, 0.3690231391710454, -0.32782280804782077, -0.3345307432885828, 0.05283738908775408, -0.3125591681354904, -0.12331217363605211, 0.2038016606941177, -0.1534568483716455, 0... |
1,802.0761 | Homotopy Theory of Bicomplexes | We define two model structures on the category of bicomplexes concentrated in
the right half plane. The first model structure has weak equivalences detected
by the totalisation functor. The second model structure's weak equivalences are
detected by the $E^2$-term of the spectral sequence associated to the
filtration ... | math.AT math.KT | we define two model structures on the category of bicomplexes concentrated in the right half plane the first model structure has weak equivalences detected by the totalisation functor the second model structures weak equivalences are detected by the e2term of the spectral sequence associated to the filtration of the to... | [['we', 'define', 'two', 'model', 'structures', 'on', 'the', 'category', 'of', 'bicomplexes', 'concentrated', 'in', 'the', 'right', 'half', 'plane', 'the', 'first', 'model', 'structure', 'has', 'weak', 'equivalences', 'detected', 'by', 'the', 'totalisation', 'functor', 'the', 'second', 'model', 'structures', 'weak', 'e... | [-0.16004923926365952, 0.0725137030315255, -0.027539648806616183, 0.09545390074133812, -0.05172536564209769, -0.05863144501082359, -0.014488524139573376, 0.3981982680908855, -0.38770229093760494, -0.2540916879961808, 0.08369788011318192, -0.22174087239733536, -0.1340219743790165, 0.11554699661135073, -0.056807610882265... |
1,802.07611 | H.E.S.S. discovery of very high energy gamma-ray emission from PKS
0625-354 | PKS 0625-354 (z=0.055) was observed with the four H.E.S.S. telescopes in 2012
during 5.5 hours. The source was detected above an energy threshold of 200 GeV
at a significance level of 6.1$\sigma$. No significant variability is found in
these observations. The source is well described with a power-law spectrum with
ph... | astro-ph.HE | pks 0625354 z0055 was observed with the four hess telescopes in 2012 during 55 hours the source was detected above an energy threshold of 200 gev at a significance level of 61sigma no significant variability is found in these observations the source is well described with a powerlaw spectrum with photon index gamma 284... | [['pks', '0625354', 'z0055', 'was', 'observed', 'with', 'the', 'four', 'hess', 'telescopes', 'in', '2012', 'during', '55', 'hours', 'the', 'source', 'was', 'detected', 'above', 'an', 'energy', 'threshold', 'of', '200', 'gev', 'at', 'a', 'significance', 'level', 'of', '61sigma', 'no', 'significant', 'variability', 'is',... | [-0.04943660957300488, 0.09973703790601576, -0.05724271332899875, 0.13800952822339776, -0.09154367021367173, -0.13834836560520616, 0.06598475503680461, 0.48538184082683394, -0.13496662632781356, -0.4102523234727628, 0.05469429502606063, -0.34900299680028934, 0.02708033889751224, 0.23720072470468415, -0.0002985092746230... |
1,802.07612 | WQO dichotomy for 3-graphs | We investigate data-enriched models, like Petri nets with data, where
executability of a transition is conditioned by a relation between data values
involved. Decidability status of various decision problems in such models may
depend on the structure of data domain. According to the WQO Dichotomy
Conjecture, if a dat... | cs.LO | we investigate dataenriched models like petri nets with data where executability of a transition is conditioned by a relation between data values involved decidability status of various decision problems in such models may depend on the structure of data domain according to the wqo dichotomy conjecture if a data domain... | [['we', 'investigate', 'dataenriched', 'models', 'like', 'petri', 'nets', 'with', 'data', 'where', 'executability', 'of', 'a', 'transition', 'is', 'conditioned', 'by', 'a', 'relation', 'between', 'data', 'values', 'involved', 'decidability', 'status', 'of', 'various', 'decision', 'problems', 'in', 'such', 'models', 'ma... | [-0.09754102593203923, 0.07264861539174039, -0.04553931859229599, 0.10374335970872224, -0.12449159361589868, -0.1381377139682504, 0.0879896533851688, 0.3846229960521062, -0.2959506247393988, -0.28284609211222816, 0.18032725698834806, -0.2998800683926019, -0.11748899598312271, 0.19134414095960156, -0.10965420799497683, ... |
1,802.07613 | About Kendall's regression | Conditional Kendall's tau is a measure of dependence between two random
variables, conditionally on some covariates. We assume a regression-type
relationship between conditional Kendall's tau and some covariates, in a
parametric setting with a large number of transformations of a small number of
regressors. This mode... | math.ST stat.ME stat.TH | conditional kendalls tau is a measure of dependence between two random variables conditionally on some covariates we assume a regressiontype relationship between conditional kendalls tau and some covariates in a parametric setting with a large number of transformations of a small number of regressors this model may be ... | [['conditional', 'kendalls', 'tau', 'is', 'a', 'measure', 'of', 'dependence', 'between', 'two', 'random', 'variables', 'conditionally', 'on', 'some', 'covariates', 'we', 'assume', 'a', 'regressiontype', 'relationship', 'between', 'conditional', 'kendalls', 'tau', 'and', 'some', 'covariates', 'in', 'a', 'parametric', 's... | [-0.1013886974057338, 0.10674819798199071, -0.12638262957140492, 0.13223235631812713, -0.10833992840101321, -0.180683240032522, 0.1137622079756208, 0.3891228954695786, -0.2754641436113161, -0.26982696260286804, 0.12270995955987019, -0.2507586277934024, -0.164082539898421, 0.17359806066087913, -0.09374176753044594, 0.10... |
1,802.07614 | Light Scattering by Cholesteric Skyrmions | We study the light scattering by localized quasi planar excitations of a
Cholesteric Liquid Crystal known as spherulites. Due to the anisotropic optical
properties of the medium and the peculiar shape of the excitations, we
quantitatively evaluate the cross section of the axis-rotation of polarized
light. Because of ... | cond-mat.soft | we study the light scattering by localized quasi planar excitations of a cholesteric liquid crystal known as spherulites due to the anisotropic optical properties of the medium and the peculiar shape of the excitations we quantitatively evaluate the cross section of the axisrotation of polarized light because of the co... | [['we', 'study', 'the', 'light', 'scattering', 'by', 'localized', 'quasi', 'planar', 'excitations', 'of', 'a', 'cholesteric', 'liquid', 'crystal', 'known', 'as', 'spherulites', 'due', 'to', 'the', 'anisotropic', 'optical', 'properties', 'of', 'the', 'medium', 'and', 'the', 'peculiar', 'shape', 'of', 'the', 'excitations... | [-0.14342282782093174, 0.1362966863132358, -0.08765926402648566, 0.06559987705959766, -0.04866101445319752, -0.08438857667648268, 0.048470693097139396, 0.3644660893586223, -0.24021546144676567, -0.29626923835301705, 0.06444092782503166, -0.2517406178476112, -0.14189157037590458, 0.17667050073052654, 0.01792193027385683... |
1,802.07615 | Resonant optical pulses on a continuous wave background in two-level
active media | We present exact N-soliton optical pulses riding on a continuous-wave (c.w.)
beam that propagate through and interact with a two-level active optical
medium. Their representation is derived via an appropriate generalization of
the inverse scattering transform for the corresponding Maxwell-Bloch equations.
We describe... | nlin.PS nlin.SI | we present exact nsoliton optical pulses riding on a continuouswave cw beam that propagate through and interact with a twolevel active optical medium their representation is derived via an appropriate generalization of the inverse scattering transform for the corresponding maxwellbloch equations we describe the singles... | [['we', 'present', 'exact', 'nsoliton', 'optical', 'pulses', 'riding', 'on', 'a', 'continuouswave', 'cw', 'beam', 'that', 'propagate', 'through', 'and', 'interact', 'with', 'a', 'twolevel', 'active', 'optical', 'medium', 'their', 'representation', 'is', 'derived', 'via', 'an', 'appropriate', 'generalization', 'of', 'th... | [-0.1652790772631158, 0.10468361107192577, -0.07527647360206344, 0.06059830562958797, -0.07956225928207931, -0.13931243295976242, -0.01260678941120444, 0.40887581662440947, -0.2671498922818853, -0.23578057270641475, 0.11151070652219157, -0.29149374087131763, -0.1329555663229652, 0.22605106933042407, 0.02855100670861903... |
1,802.07616 | Constraining the Higgs self couplings at $e^+e^-$ colliders | We study the sensitivity to the shape of the Higgs potential of single,
double, and triple Higgs production at future $e^+e^-$ colliders. Physics
beyond the Standard Model is parameterised through the inclusion of
higher-dimensional operators $(\Phi^\dagger \Phi- v^2/2)^n/\Lambda^{(2n-4)}$
with $n=3,4$, which allows ... | hep-ph | we study the sensitivity to the shape of the higgs potential of single double and triple higgs production at future ee colliders physics beyond the standard model is parameterised through the inclusion of higherdimensional operators phidagger phi v22nlambda2n4 with n34 which allows a consistent treatment of independent... | [['we', 'study', 'the', 'sensitivity', 'to', 'the', 'shape', 'of', 'the', 'higgs', 'potential', 'of', 'single', 'double', 'and', 'triple', 'higgs', 'production', 'at', 'future', 'ee', 'colliders', 'physics', 'beyond', 'the', 'standard', 'model', 'is', 'parameterised', 'through', 'the', 'inclusion', 'of', 'higherdimensi... | [-0.08705193611998034, 0.19024840516185088, -0.018425586144536488, 0.11231439941730814, -0.04821048635232003, -0.1934724216179389, 0.03905659575397883, 0.3072581784026813, -0.24559161050971676, -0.26272401119934014, 0.02255594324372724, -0.31320929313876766, -0.04805935982661128, 0.19179485934106363, 0.0629415066716651... |
1,802.07617 | Convergence rates for smooth k-means change-point detection | In this paper, we consider the estimation of a change-point for possibly
high-dimensional data in a Gaussian model, using a k-means method. We prove
that, up to a logarithmic term, this change-point estimator has a minimax rate
of convergence. Then, considering the case of sparse data, with a Sobolev
regularity, we p... | math.ST stat.TH | in this paper we consider the estimation of a changepoint for possibly highdimensional data in a gaussian model using a kmeans method we prove that up to a logarithmic term this changepoint estimator has a minimax rate of convergence then considering the case of sparse data with a sobolev regularity we propose a smooth... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'estimation', 'of', 'a', 'changepoint', 'for', 'possibly', 'highdimensional', 'data', 'in', 'a', 'gaussian', 'model', 'using', 'a', 'kmeans', 'method', 'we', 'prove', 'that', 'up', 'to', 'a', 'logarithmic', 'term', 'this', 'changepoint', 'estimator', 'has', 'a', 'minima... | [-0.07405877923592925, -0.04475532276424929, -0.13806248577311636, 0.08851972126518376, -0.06403075356036425, -0.16867135206703096, 0.098923696896818, 0.4058976363763213, -0.26020232735201715, -0.24469102963339537, 0.1905172278522514, -0.22701461985241622, -0.19302753374911844, 0.23124733036151157, -0.14604922898113729... |
1,802.07618 | On the l^{q,p} cohomology of Carnot groups | We study the simplicial {\ell} q,p cohomology of Carnot groups G. We show
vanishing and non-vanishing results depending of the range of the (p, q) gap
with respect to the weight gaps in the Lie algebra cohomology of G.
| math.FA math.DG | we study the simplicial ell qp cohomology of carnot groups g we show vanishing and nonvanishing results depending of the range of the p q gap with respect to the weight gaps in the lie algebra cohomology of g | [['we', 'study', 'the', 'simplicial', 'ell', 'qp', 'cohomology', 'of', 'carnot', 'groups', 'g', 'we', 'show', 'vanishing', 'and', 'nonvanishing', 'results', 'depending', 'of', 'the', 'range', 'of', 'the', 'p', 'q', 'gap', 'with', 'respect', 'to', 'the', 'weight', 'gaps', 'in', 'the', 'lie', 'algebra', 'cohomology', 'of... | [-0.27690412598447156, 0.09895524121403025, -0.07718184165274486, -0.0019397636254628499, -0.10533640001757213, -0.09916387331218292, 0.04277921919949735, 0.3450183052665148, -0.37056916503187937, -0.30469256507692477, 0.0003744617719442034, -0.2380965750139111, -0.08380402021635419, 0.15127093753275964, -0.11741841178... |
1,802.07619 | On the local cohomology of modular invariants | We compute some numerical invariants of local cohomology of the ring of
invariants by a finite group, mainly in the modular case. Also, we present some
applications. In particular, we study Cohen-Macaulay property of modular
invariants from the viewpoints of depth, Serre's condition and the relevant
generalizations (... | math.AC | we compute some numerical invariants of local cohomology of the ring of invariants by a finite group mainly in the modular case also we present some applications in particular we study cohenmacaulay property of modular invariants from the viewpoints of depth serres condition and the relevant generalizations eg the buch... | [['we', 'compute', 'some', 'numerical', 'invariants', 'of', 'local', 'cohomology', 'of', 'the', 'ring', 'of', 'invariants', 'by', 'a', 'finite', 'group', 'mainly', 'in', 'the', 'modular', 'case', 'also', 'we', 'present', 'some', 'applications', 'in', 'particular', 'we', 'study', 'cohenmacaulay', 'property', 'of', 'modu... | [-0.20145421659981366, 0.03293065566685982, -0.10370343519025482, 0.08230157936668547, -0.06252820663212333, -0.10979906241846038, -0.042956355693604564, 0.29936284295399673, -0.3664446252514608, -0.21845022498746403, 0.14380204324879742, -0.24474252050276846, -0.2085215289698681, 0.1901786828530021, -0.134246916320989... |
1,802.0762 | Angular and polarization trails from effective interactions of Majorana
neutrinos at the LHeC | We study the possibility of the LHeC facility to disentangle different new
physics contributions to the production of heavy sterile Majorana neutrinos in
the lepton number violating channel $e^{-}p\rightarrow l_{j}^{+} + 3 jets$
($l_j\equiv e ,\mu $). This is done investigating the angular and polarization
trails of ... | hep-ph | we study the possibility of the lhec facility to disentangle different new physics contributions to the production of heavy sterile majorana neutrinos in the lepton number violating channel eprightarrow l_j 3 jets l_jequiv e mu this is done investigating the angular and polarization trails of effective operators with d... | [['we', 'study', 'the', 'possibility', 'of', 'the', 'lhec', 'facility', 'to', 'disentangle', 'different', 'new', 'physics', 'contributions', 'to', 'the', 'production', 'of', 'heavy', 'sterile', 'majorana', 'neutrinos', 'in', 'the', 'lepton', 'number', 'violating', 'channel', 'eprightarrow', 'l_j', '3', 'jets', 'l_jequi... | [-0.13521672140008636, 0.265554472867405, -0.05730250328612913, 0.1692771931844098, -0.06535065361032528, -0.1217505979462571, 0.0267703199138244, 0.26155328425977914, -0.24693973990423337, -0.35067559773368495, -0.03444634703697548, -0.3325542564193408, 0.005983092972920054, 0.11993619559244031, 0.10050003825731221, 0... |
1,802.07621 | An exact extremal result for tournaments and 4-uniform hypergraphs | In this paper, we address the following problem due to Frankl and F\"uredi
(1984). What is the maximum number of hyperedges in an $r$-uniform hypergraph
with $n$ vertices, such that every set of $r+1$ vertices contains $0$ or
exactly $2$ hyperedges? They solved this problem for $r=3$. For $r=4$, a
partial solution is... | math.CO | in this paper we address the following problem due to frankl and furedi 1984 what is the maximum number of hyperedges in an runiform hypergraph with n vertices such that every set of r1 vertices contains 0 or exactly 2 hyperedges they solved this problem for r3 for r4 a partial solution is given by gunderson and semera... | [['in', 'this', 'paper', 'we', 'address', 'the', 'following', 'problem', 'due', 'to', 'frankl', 'and', 'furedi', '1984', 'what', 'is', 'the', 'maximum', 'number', 'of', 'hyperedges', 'in', 'an', 'runiform', 'hypergraph', 'with', 'n', 'vertices', 'such', 'that', 'every', 'set', 'of', 'r1', 'vertices', 'contains', '0', '... | [-0.1745298345854809, 0.09259686968103187, 0.01775970755058319, 0.012986638631974889, -0.05394184418824003, -0.1852075266868396, 0.015105030533240372, 0.2998242814007194, -0.2479880332708532, -0.333199983370642, 0.10158406036938432, -0.3523307031150474, -0.1366332512792893, 0.09156494121998549, -0.12982232384058798, 0.... |
1,802.07622 | Cubic Halo Bias in Eulerian and Lagrangian Space | Predictions of the next-to-leading order, i.e. one-loop, halo power spectra
depend on local and non-local bias parameters up to cubic order. The linear
bias parameter can be estimated from the large scale limit of the halo-matter
power spectrum, and the second order bias parameters from the large scale,
tree-level, b... | astro-ph.CO | predictions of the nexttoleading order ie oneloop halo power spectra depend on local and nonlocal bias parameters up to cubic order the linear bias parameter can be estimated from the large scale limit of the halomatter power spectrum and the second order bias parameters from the large scale treelevel bispectrum cubic ... | [['predictions', 'of', 'the', 'nexttoleading', 'order', 'ie', 'oneloop', 'halo', 'power', 'spectra', 'depend', 'on', 'local', 'and', 'nonlocal', 'bias', 'parameters', 'up', 'to', 'cubic', 'order', 'the', 'linear', 'bias', 'parameter', 'can', 'be', 'estimated', 'from', 'the', 'large', 'scale', 'limit', 'of', 'the', 'hal... | [-0.11358561216479861, 0.07662288449836478, -0.05727656989583754, 0.09949020875009738, -0.13350098819118927, -0.07664862961920837, 0.006133058285936033, 0.34396029332733485, -0.23653622695495222, -0.36396463702275467, 0.051367961064823074, -0.2774514029329838, -0.11672524464785516, 0.1730514277441461, -0.01709525776786... |
1,802.07623 | Explanations based on the Missing: Towards Contrastive Explanations with
Pertinent Negatives | In this paper we propose a novel method that provides contrastive
explanations justifying the classification of an input by a black box
classifier such as a deep neural network. Given an input we find what should be
%necessarily and minimally and sufficiently present (viz. important object
pixels in an image) to just... | cs.AI cs.CV cs.LG | in this paper we propose a novel method that provides contrastive explanations justifying the classification of an input by a black box classifier such as a deep neural network given an input we find what should be necessarily and minimally and sufficiently present viz important object pixels in an image to justify its... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'novel', 'method', 'that', 'provides', 'contrastive', 'explanations', 'justifying', 'the', 'classification', 'of', 'an', 'input', 'by', 'a', 'black', 'box', 'classifier', 'such', 'as', 'a', 'deep', 'neural', 'network', 'given', 'an', 'input', 'we', 'find', 'what', 'should'... | [-0.030937023077610086, 0.028371130210217324, -0.05857144591262501, 0.12176345461806848, -0.11105685361943553, -0.1553911541541515, 0.0083992717142761, 0.42758648253433157, -0.20725579290478124, -0.33021495770663023, 0.10330744260029993, -0.28706402977237877, -0.22892047070605115, 0.22094858757812422, -0.14860069419236... |
1,802.07624 | Endoscopic transfer for unitary Lie algebras | We give another proof of the existence of the endoscopic transfer for unitary
Lie algebras and its compatibility with Fourier transforms. By the work of
Kazhdan and Vashavsky, this implies the corresponding endoscopic fundamental
lemma (theorem of Laumon--Ng\^o). We study the compatibility between Fourier
transforms ... | math.NT | we give another proof of the existence of the endoscopic transfer for unitary lie algebras and its compatibility with fourier transforms by the work of kazhdan and vashavsky this implies the corresponding endoscopic fundamental lemma theorem of laumonngo we study the compatibility between fourier transforms and transfe... | [['we', 'give', 'another', 'proof', 'of', 'the', 'existence', 'of', 'the', 'endoscopic', 'transfer', 'for', 'unitary', 'lie', 'algebras', 'and', 'its', 'compatibility', 'with', 'fourier', 'transforms', 'by', 'the', 'work', 'of', 'kazhdan', 'and', 'vashavsky', 'this', 'implies', 'the', 'corresponding', 'endoscopic', 'fu... | [-0.16325229254837792, 0.051599489766746186, -0.15926966031010334, 0.045356488018296656, -0.07710233069239901, -0.06217351433319541, 0.037727237650408196, 0.34800535566531693, -0.3374792690388858, -0.22621032826315898, 0.12629649027680548, -0.18266263143875852, -0.15742560792714358, 0.24830510980234696, -0.146707547456... |
1,802.07625 | Fast flow-based algorithm for creating density-equalizing map
projections | Cartograms are maps that rescale geographic regions (e.g., countries,
districts) such that their areas are proportional to quantitative demographic
data (e.g., population size, gross domestic product). Unlike conventional bar
or pie charts, cartograms can represent correctly which regions share common
borders, result... | cs.CG | cartograms are maps that rescale geographic regions eg countries districts such that their areas are proportional to quantitative demographic data eg population size gross domestic product unlike conventional bar or pie charts cartograms can represent correctly which regions share common borders resulting in insightful... | [['cartograms', 'are', 'maps', 'that', 'rescale', 'geographic', 'regions', 'eg', 'countries', 'districts', 'such', 'that', 'their', 'areas', 'are', 'proportional', 'to', 'quantitative', 'demographic', 'data', 'eg', 'population', 'size', 'gross', 'domestic', 'product', 'unlike', 'conventional', 'bar', 'or', 'pie', 'char... | [-0.05333480179789032, 0.03659222985737855, -0.10702932028474742, 0.0911505959128103, -0.08692283327285494, -0.13029273860233825, 0.03604265048262312, 0.3892639109138322, -0.25498355447055765, -0.3302227787101541, 0.12142909316904456, -0.30025268401622124, -0.1504021653822426, 0.22826168884105857, -0.10594380257315006,... |
1,802.07626 | Neumann Boundary Problem for Parabolic Partial Differential Equations
with Divergence Terms | We prove an existence and uniqueness result for Neumann boundary problem of a
parabolic partial differential equation (PDE for short) with a singular
nonlinear divergence term which can only be understood in a weak sense. A
probabilistic approach is applied by studying the backward stochastic
differential equations (... | math.PR | we prove an existence and uniqueness result for neumann boundary problem of a parabolic partial differential equation pde for short with a singular nonlinear divergence term which can only be understood in a weak sense a probabilistic approach is applied by studying the backward stochastic differential equations bsdes ... | [['we', 'prove', 'an', 'existence', 'and', 'uniqueness', 'result', 'for', 'neumann', 'boundary', 'problem', 'of', 'a', 'parabolic', 'partial', 'differential', 'equation', 'pde', 'for', 'short', 'with', 'a', 'singular', 'nonlinear', 'divergence', 'term', 'which', 'can', 'only', 'be', 'understood', 'in', 'a', 'weak', 'se... | [-0.14276803630621057, 0.0034743603895026043, -0.1236228227411231, 0.1169927036309972, -0.13459651100079287, -0.17591440871562045, -0.005686326333551272, 0.2624810806456443, -0.4095147963460178, -0.20859971608048025, 0.17284534557575792, -0.2536908610889765, -0.1252539847301294, 0.22480903644264638, -0.1155836158559645... |
1,802.07627 | Readout Of Singlet-Triplet Qubits At Large Magnetic Field Gradients | Visibility of singlet-triplet qubit readout is reduced to almost zero in
large magnetic field gradients due to relaxation processes. Here we present a
new readout technique that is robust against relaxation and allows for
measurement when previously studied methods fail. This technique maps the qubit
onto spin states... | cond-mat.mes-hall | visibility of singlettriplet qubit readout is reduced to almost zero in large magnetic field gradients due to relaxation processes here we present a new readout technique that is robust against relaxation and allows for measurement when previously studied methods fail this technique maps the qubit onto spin states that... | [['visibility', 'of', 'singlettriplet', 'qubit', 'readout', 'is', 'reduced', 'to', 'almost', 'zero', 'in', 'large', 'magnetic', 'field', 'gradients', 'due', 'to', 'relaxation', 'processes', 'here', 'we', 'present', 'a', 'new', 'readout', 'technique', 'that', 'is', 'robust', 'against', 'relaxation', 'and', 'allows', 'fo... | [-0.10558849507744641, 0.187253322571199, -0.06394761625399932, 0.035633596733551966, -0.012424780848495503, -0.19449897852052558, 0.039490130673004116, 0.42404523563194785, -0.26333313056842444, -0.30209901397849653, 0.050896281642750146, -0.21758935558426992, -0.10285079437109859, 0.2500991648449463, -0.0126791270102... |
1,802.07628 | On the fast quenching of young low-mass galaxies up to z $\sim$ 0.6: new
spotlight on the lead role of environment | We investigate the connection between environment and the different quenching
channels that galaxies are prone to follow in the rest-frame NUVrK colour
diagram, as identified by Moutard et al. (2016b). Namely, the fast quenching
channel followed by $young$ low-mass galaxies and the slow quenching channel
followed by ... | astro-ph.GA | we investigate the connection between environment and the different quenching channels that galaxies are prone to follow in the restframe nuvrk colour diagram as identified by moutard et al 2016b namely the fast quenching channel followed by young lowmass galaxies and the slow quenching channel followed by old highmass... | [['we', 'investigate', 'the', 'connection', 'between', 'environment', 'and', 'the', 'different', 'quenching', 'channels', 'that', 'galaxies', 'are', 'prone', 'to', 'follow', 'in', 'the', 'restframe', 'nuvrk', 'colour', 'diagram', 'as', 'identified', 'by', 'moutard', 'et', 'al', '2016b', 'namely', 'the', 'fast', 'quench... | [-0.06918239585625438, 0.18869456574141694, -0.0662781383179558, 0.1258859340558187, -0.047833515470847486, -0.06394992360415366, 0.08039021671597416, 0.4520081198416077, -0.08878502571292651, -0.38524886323139074, 0.025874136849933376, -0.2763506862482665, -0.002967128798795434, 0.16059727921652106, -0.046621971483378... |
1,802.07629 | Extreme cooperative swelling in topologically disordered fibre
entanglements | Entangled states are ubiquitous amongst fibrous materials, whether naturally
occurring (keratin, collagen, DNA) or synthetic (nanotube assemblies,
elastane). A key mechanical characteristic of these systems is their ability to
reorganise in response to external stimuli, as implicated in e.g.
hydration-induced swellin... | cond-mat.soft cond-mat.mtrl-sci | entangled states are ubiquitous amongst fibrous materials whether naturally occurring keratin collagen dna or synthetic nanotube assemblies elastane a key mechanical characteristic of these systems is their ability to reorganise in response to external stimuli as implicated in eg hydrationinduced swelling of keratin fi... | [['entangled', 'states', 'are', 'ubiquitous', 'amongst', 'fibrous', 'materials', 'whether', 'naturally', 'occurring', 'keratin', 'collagen', 'dna', 'or', 'synthetic', 'nanotube', 'assemblies', 'elastane', 'a', 'key', 'mechanical', 'characteristic', 'of', 'these', 'systems', 'is', 'their', 'ability', 'to', 'reorganise',... | [-0.1457373814101942, 0.23802915571272196, -0.06762896102518137, 0.055837107929051395, -0.06139609624591211, -0.17799952681537115, 0.039283441147295824, 0.40592248257150204, -0.28724748608122463, -0.2704668951776659, 0.07791444966422298, -0.26401972752101277, -0.24270149924941434, 0.15268724012393836, -0.07160677003633... |
1,802.0763 | Diffractive shear interferometry for extreme ultraviolet high-resolution
lensless imaging | We demonstrate a novel imaging approach and associated reconstruction
algorithm for far-field coherent diffractive imaging, based on the measurement
of a pair of laterally sheared diffraction patterns. The differential phase
profile retrieved from such a measurement leads to improved reconstruction
accuracy, increase... | physics.optics | we demonstrate a novel imaging approach and associated reconstruction algorithm for farfield coherent diffractive imaging based on the measurement of a pair of laterally sheared diffraction patterns the differential phase profile retrieved from such a measurement leads to improved reconstruction accuracy increased robu... | [['we', 'demonstrate', 'a', 'novel', 'imaging', 'approach', 'and', 'associated', 'reconstruction', 'algorithm', 'for', 'farfield', 'coherent', 'diffractive', 'imaging', 'based', 'on', 'the', 'measurement', 'of', 'a', 'pair', 'of', 'laterally', 'sheared', 'diffraction', 'patterns', 'the', 'differential', 'phase', 'profi... | [-0.0448575310439772, 0.11224261387814205, -0.11245211744476315, 0.051310867617408246, -0.001339920338468401, -0.14654695052285116, 0.049487763858441225, 0.5140332925941918, -0.29110886891382737, -0.31912830570241907, 0.06664370239333628, -0.31514634503368905, -0.1325346030253958, 0.25716451691414977, -0.04549133550928... |
1,802.07631 | Koll\'ar's injectivity theorem for globally $F$-regular varieties | We prove Koll\'ar's injectivity theorem for globally $F$-regular varieties.
| math.AG math.AC | we prove kollars injectivity theorem for globally fregular varieties | [['we', 'prove', 'kollars', 'injectivity', 'theorem', 'for', 'globally', 'fregular', 'varieties']] | [-0.32115849521425033, -0.11620748156888618, -0.16274521955185467, 0.2971620372393065, -0.036204440519213676, -0.3588213407331043, -0.050003132679396205, 0.28221047669649124, -0.37319893886645633, 0.024573464670942888, 0.18470423854887486, -0.17990144880281556, -0.15143034358819327, 0.3233218482799, -0.4448141290081872... |
1,802.07632 | Spanning Tree Congestion and Computation of Generalized
Gy\H{o}ri-Lov\'{a}sz Partition | We study a natural problem in graph sparsification, the Spanning Tree
Congestion (\STC) problem. Informally, the \STC problem seeks a spanning tree
with no tree-edge \emph{routing} too many of the original edges. The root of
this problem dates back to at least 30 years ago, motivated by applications in
network design... | cs.DS cs.CC cs.DM | we study a natural problem in graph sparsification the spanning tree congestion stc problem informally the stc problem seeks a spanning tree with no treeedge emphrouting too many of the original edges the root of this problem dates back to at least 30 years ago motivated by applications in network design parallel compu... | [['we', 'study', 'a', 'natural', 'problem', 'in', 'graph', 'sparsification', 'the', 'spanning', 'tree', 'congestion', 'stc', 'problem', 'informally', 'the', 'stc', 'problem', 'seeks', 'a', 'spanning', 'tree', 'with', 'no', 'treeedge', 'emphrouting', 'too', 'many', 'of', 'the', 'original', 'edges', 'the', 'root', 'of', ... | [-0.14357586705866526, 0.09582822138309986, -0.08819113298792275, 0.05030113618223246, -0.08909549181510908, -0.16393451159086636, 0.0937501352196046, 0.37420044210922765, -0.280949616402307, -0.3546118190801724, 0.11823267894604529, -0.22903249097078687, -0.19230043111924966, 0.16211913063605207, -0.09224329539391352,... |
1,802.07633 | G\^Ateaux-Differentiability of Convex Functions in Infinite Dimension | It is well known that in $R^n$ , G{\^a}teaux (hence Fr{\'e}chet)
differ-entiability of a convex continuous function at some point is equivalent
to the existence of the partial derivatives at this point. We prove that this
result extends naturally to certain infinite dimensional vector spaces, in
particular to Banach ... | math.FA | it is well known that in rn gateaux hence frechet differentiability of a convex continuous function at some point is equivalent to the existence of the partial derivatives at this point we prove that this result extends naturally to certain infinite dimensional vector spaces in particular to banach spaces having a scha... | [['it', 'is', 'well', 'known', 'that', 'in', 'rn', 'gateaux', 'hence', 'frechet', 'differentiability', 'of', 'a', 'convex', 'continuous', 'function', 'at', 'some', 'point', 'is', 'equivalent', 'to', 'the', 'existence', 'of', 'the', 'partial', 'derivatives', 'at', 'this', 'point', 'we', 'prove', 'that', 'this', 'result'... | [-0.0971856036768207, 0.06503699922863886, -0.08282208970730316, 0.12946358635881036, -0.11779839517372959, -0.059843040001139325, 0.031840627064120094, 0.40838439258711656, -0.37958988568411683, -0.09241410431821111, 0.1543453953378254, -0.26306245296771796, -0.14780243496709275, 0.13911155674536274, -0.16061137501097... |
1,802.07634 | Stochastic Model Predictive Control of Air Conditioning System for
Electric Vehicles: Sensitivity Study, Comparison and Improvement | A stochastic model predictive controller (SMPC) of air conditioning (AC)
system is proposed to improve the energy efficiency of electric vehicles (EV).
A Markov-chain based velocity predictor is adopted to provide a sense of the
future disturbances over the SMPC control horizon. The sensitivity of
electrified AC plan... | cs.SY math.OC | a stochastic model predictive controller smpc of air conditioning ac system is proposed to improve the energy efficiency of electric vehicles ev a markovchain based velocity predictor is adopted to provide a sense of the future disturbances over the smpc control horizon the sensitivity of electrified ac plant to solar ... | [['a', 'stochastic', 'model', 'predictive', 'controller', 'smpc', 'of', 'air', 'conditioning', 'ac', 'system', 'is', 'proposed', 'to', 'improve', 'the', 'energy', 'efficiency', 'of', 'electric', 'vehicles', 'ev', 'a', 'markovchain', 'based', 'velocity', 'predictor', 'is', 'adopted', 'to', 'provide', 'a', 'sense', 'of',... | [-0.08890198561168136, 0.061385968676559, -0.060060660088483514, 0.03627170399637905, -0.0694420655665834, -0.14990877082839218, 0.06906587329200085, 0.3649423160389358, -0.24781956374523492, -0.3527547273803137, 0.12187971242711487, -0.27603265442855024, -0.07440042748493356, 0.26549455657558746, -0.13333058141147583,... |
1,802.07635 | Matrix factorizations over elementary divisor domains | We study the homotopy category $\mathrm{hmf}(R,W)$ of matrix factorizations
of non-zero elements $W\in R^\times$, where $R$ is an elementary divisor
domain. When $R$ has prime elements and $W$ factors into a square-free element
$W_0$ and a finite product of primes of multiplicity greater than one and which
do not div... | math.AC hep-th math.AG | we study the homotopy category mathrmhmfrw of matrix factorizations of nonzero elements win rtimes where r is an elementary divisor domain when r has prime elements and w factors into a squarefree element w_0 and a finite product of primes of multiplicity greater than one and which do not divide w_0 we show that mathrm... | [['we', 'study', 'the', 'homotopy', 'category', 'mathrmhmfrw', 'of', 'matrix', 'factorizations', 'of', 'nonzero', 'elements', 'win', 'rtimes', 'where', 'r', 'is', 'an', 'elementary', 'divisor', 'domain', 'when', 'r', 'has', 'prime', 'elements', 'and', 'w', 'factors', 'into', 'a', 'squarefree', 'element', 'w_0', 'and', ... | [-0.18557779361435678, 0.0846508532979442, -0.07965507584594889, 0.05591939021451253, -0.043100533901451854, -0.18768269902284374, -0.039970031391931116, 0.3761567090987228, -0.3694456406374229, -0.17589842287793545, 0.07072607256122865, -0.26340475668985164, -0.08306274923688761, 0.13330187141491479, -0.12592929302809... |
1,802.07636 | The lower central and derived series of the braid groups of compact
surfaces | Let M be a compact surface, either orientable or non-orientable. We study the
lower central and derived series of the braid and pure braid groups of M in
order to determine the values of n for which B\_n(M) and P\_n(M) are residually
nilpotent or residually soluble. First, we solve this problem for the case
where M i... | math.GT math.GR | let m be a compact surface either orientable or nonorientable we study the lower central and derived series of the braid and pure braid groups of m in order to determine the values of n for which b_nm and p_nm are residually nilpotent or residually soluble first we solve this problem for the case where m is the 2torus ... | [['let', 'm', 'be', 'a', 'compact', 'surface', 'either', 'orientable', 'or', 'nonorientable', 'we', 'study', 'the', 'lower', 'central', 'and', 'derived', 'series', 'of', 'the', 'braid', 'and', 'pure', 'braid', 'groups', 'of', 'm', 'in', 'order', 'to', 'determine', 'the', 'values', 'of', 'n', 'for', 'which', 'b_nm', 'an... | [-0.12400610956862784, 0.14068356124820033, -0.05630134289031443, 0.05557020748813596, -0.09496581840220893, -0.15291037335249502, 0.004372694290013633, 0.34862146896404633, -0.2424921539909058, -0.2717956457948447, 0.12416275336316017, -0.25785931470591755, -0.08434664092635723, 0.2226676701557944, -0.1122542980508339... |
1,802.07637 | Non-Abelian extension of the aether term and the Gribov problem | In this paper, we treat the proper path integral quantization of the
Yang-Mills-aether (YM-aether) system by dealing with the extra gauge copies in
the Landau gauge. Within Gribov's prescription to get rid of such remaining
gauge copies, we explicitly derive the Gribov parameter dependence of the
coupling constant an... | hep-th | in this paper we treat the proper path integral quantization of the yangmillsaether ymaether system by dealing with the extra gauge copies in the landau gauge within gribovs prescription to get rid of such remaining gauge copies we explicitly derive the gribov parameter dependence of the coupling constant and of the lo... | [['in', 'this', 'paper', 'we', 'treat', 'the', 'proper', 'path', 'integral', 'quantization', 'of', 'the', 'yangmillsaether', 'ymaether', 'system', 'by', 'dealing', 'with', 'the', 'extra', 'gauge', 'copies', 'in', 'the', 'landau', 'gauge', 'within', 'gribovs', 'prescription', 'to', 'get', 'rid', 'of', 'such', 'remaining... | [-0.18134869201766218, 0.21231586184790907, -0.07976824652184458, 0.05114789425450213, -0.11431636162759627, -0.07866353600779001, 0.07676169626442168, 0.31553689309341065, -0.1997675480403225, -0.2923818968455581, 0.06924680283649222, -0.21963118181070862, -0.10940636832486181, 0.08198680016760002, -0.0991247964995529... |
1,802.07638 | Energy Harvesting and Magneto-Inductive Communications with Molecular
Magnets on Vibrating Graphene and Biomedical Applications in the Kilohertz to
Terahertz Band | Magneto-inductive (MI) Terahertz (THz) wireless channels provide significant
theoretical performances for MI communications (MIC) and wireless power
transmission (WPT) in nanoscale networks. Energy harvesting (EH) and signal
generation are critical for autonomous operation in challenging medium
including biomedical c... | physics.app-ph physics.med-ph | magnetoinductive mi terahertz thz wireless channels provide significant theoretical performances for mi communications mic and wireless power transmission wpt in nanoscale networks energy harvesting eh and signal generation are critical for autonomous operation in challenging medium including biomedical channels state ... | [['magnetoinductive', 'mi', 'terahertz', 'thz', 'wireless', 'channels', 'provide', 'significant', 'theoretical', 'performances', 'for', 'mi', 'communications', 'mic', 'and', 'wireless', 'power', 'transmission', 'wpt', 'in', 'nanoscale', 'networks', 'energy', 'harvesting', 'eh', 'and', 'signal', 'generation', 'are', 'cr... | [-0.2157530848200273, 0.09692545220340518, 0.07683979439657332, -0.053913469945205225, -0.07226234841550878, -0.24791138504180266, 0.037482870097102765, 0.4434831388520472, -0.2156085753437094, -0.29662319942791426, 0.04414844818059308, -0.27575653668662364, -0.15397231143457119, 0.2569349066306122, -0.0201465802266017... |
1,802.07639 | Notes On Open Book Decompositions For Engel Structures | We relate open book decompositions of a 4-manifold M with its Engel
structures. Our main result is, given an open book decomposition of M whose
binding is a collection of 2-tori and whose monodromy preserves a framing of a
page, the construction of an En-gel structure whose isotropic foliation is
transverse to the in... | math.SG | we relate open book decompositions of a 4manifold m with its engel structures our main result is given an open book decomposition of m whose binding is a collection of 2tori and whose monodromy preserves a framing of a page the construction of an engel structure whose isotropic foliation is transverse to the interior o... | [['we', 'relate', 'open', 'book', 'decompositions', 'of', 'a', '4manifold', 'm', 'with', 'its', 'engel', 'structures', 'our', 'main', 'result', 'is', 'given', 'an', 'open', 'book', 'decomposition', 'of', 'm', 'whose', 'binding', 'is', 'a', 'collection', 'of', '2tori', 'and', 'whose', 'monodromy', 'preserves', 'a', 'fra... | [-0.22460826421317098, 0.06352527982267804, -0.09679983124731044, 0.0659710400274168, -0.1319936879364581, -0.11059452870916896, -0.0031566007297630584, 0.39070618486609954, -0.29139698513558715, -0.26199943053632463, 0.07828298951338591, -0.2852260785775484, -0.16890927122259544, 0.17314491388970055, -0.14761897101034... |
1,802.0764 | Antenna Design and Implementation for the Future Space Ultra-Long
Wavelength Radio Telescope | In radio astronomy, the Ultra-Long Wavelengths (ULW) regime of longer than 10
m (frequencies below 30 MHz), remains the last virtually unexplored window of
the celestial electromagnetic spectrum. The strength of the science case for
extending radio astronomy into the ULW window is growing. However, the
opaqueness of ... | astro-ph.IM | in radio astronomy the ultralong wavelengths ulw regime of longer than 10 m frequencies below 30 mhz remains the last virtually unexplored window of the celestial electromagnetic spectrum the strength of the science case for extending radio astronomy into the ulw window is growing however the opaqueness of the earths i... | [['in', 'radio', 'astronomy', 'the', 'ultralong', 'wavelengths', 'ulw', 'regime', 'of', 'longer', 'than', '10', 'm', 'frequencies', 'below', '30', 'mhz', 'remains', 'the', 'last', 'virtually', 'unexplored', 'window', 'of', 'the', 'celestial', 'electromagnetic', 'spectrum', 'the', 'strength', 'of', 'the', 'science', 'ca... | [-0.2023965704492698, 0.13758074334185474, 0.0007758196696396108, 0.03287171113175725, -0.10409464108955074, -0.13548829261360326, 0.04587988970350758, 0.414486877353066, -0.19916832935743276, -0.2942107443852127, 0.15320427073469467, -0.2536573746929998, -0.08356192045966568, 0.2639711321560595, -0.020005946771403695,... |
1,802.07641 | The life cycles of Be viscous decretion discs: fundamental disc
parameters of 54 SMC Be stars | Be stars are main-sequence massive stars with emission features in their
spectrum, which originates in circumstellar gaseous discs. Even though the
viscous decretion disc (VDD) model can satisfactorily explain most
observations, two important physical ingredients, namely the magnitude of the
viscosity ($\alpha$) and ... | astro-ph.SR | be stars are mainsequence massive stars with emission features in their spectrum which originates in circumstellar gaseous discs even though the viscous decretion disc vdd model can satisfactorily explain most observations two important physical ingredients namely the magnitude of the viscosity alpha and the disk mass ... | [['be', 'stars', 'are', 'mainsequence', 'massive', 'stars', 'with', 'emission', 'features', 'in', 'their', 'spectrum', 'which', 'originates', 'in', 'circumstellar', 'gaseous', 'discs', 'even', 'though', 'the', 'viscous', 'decretion', 'disc', 'vdd', 'model', 'can', 'satisfactorily', 'explain', 'most', 'observations', 't... | [-0.08280863624442909, 0.12613572196317135, -0.05911649734880207, 0.0980001003872461, -0.06709345451641457, -0.055288623193748124, 0.03128111071730004, 0.3689649012508511, -0.19288340676875823, -0.383326098235779, 0.07606456721315288, -0.30159585821648477, -0.026046592129024725, 0.22069440071159113, -0.0503502074906332... |
1,802.07642 | Cofree Com-PreLie algebras | A Com-PreLie bialgebra is a commutative bialgebra with an extra preLie
product satisfying some compatibilities with the product and the coproduct. We
here give examples of cofree Com-PreLie bialgebras, including all the ones such
that the preLie product is homogeneous of degree $\ge$ --1. We also give a
graphical des... | math.RA | a comprelie bialgebra is a commutative bialgebra with an extra prelie product satisfying some compatibilities with the product and the coproduct we here give examples of cofree comprelie bialgebras including all the ones such that the prelie product is homogeneous of degree ge 1 we also give a graphical description of ... | [['a', 'comprelie', 'bialgebra', 'is', 'a', 'commutative', 'bialgebra', 'with', 'an', 'extra', 'prelie', 'product', 'satisfying', 'some', 'compatibilities', 'with', 'the', 'product', 'and', 'the', 'coproduct', 'we', 'here', 'give', 'examples', 'of', 'cofree', 'comprelie', 'bialgebras', 'including', 'all', 'the', 'ones'... | [-0.20453317123180143, 0.0843089501035212, -0.0261130523440257, 0.09436807279921688, -0.21936365742977632, -0.16094216692014313, -0.058446966905184854, 0.4003893688929324, -0.43041423676364426, -0.15970328146097612, 0.10328892193145442, -0.19572744864913427, -0.21910826478400552, 0.1507563925044117, -0.1619751832319651... |
1,802.07643 | Floating structures in shallow water: local well-posedness in the
axisymmetric case | The floating structure problem describes the interaction between surface
water waves and a floating body, generally a boat or a wave energy converter.
As shown by Lannes in [18] the equations for the fluid motion can be reduced to
a set of two evolution equations on the surface elevation and the horizontal
discharge.... | math.AP physics.ao-ph physics.flu-dyn | the floating structure problem describes the interaction between surface water waves and a floating body generally a boat or a wave energy converter as shown by lannes in 18 the equations for the fluid motion can be reduced to a set of two evolution equations on the surface elevation and the horizontal discharge the pr... | [['the', 'floating', 'structure', 'problem', 'describes', 'the', 'interaction', 'between', 'surface', 'water', 'waves', 'and', 'a', 'floating', 'body', 'generally', 'a', 'boat', 'or', 'a', 'wave', 'energy', 'converter', 'as', 'shown', 'by', 'lannes', 'in', '18', 'the', 'equations', 'for', 'the', 'fluid', 'motion', 'can... | [-0.1691813956429195, 0.08934846747710946, -0.08943175729031541, 0.031173349051858253, -0.06680696063891187, -0.08330575729598336, -0.020089361660731293, 0.2720046996525655, -0.30996322833622497, -0.3025947076080012, 0.148693084822125, -0.2598117589673382, -0.10889985370643747, 0.1640842525673742, -0.06168517378752031,... |
1,802.07644 | A gauge-invariant reversible cellular automaton | Gauge-invariance is a fundamental concept in physics---known to provide the
mathematical justification for all four fundamental forces. In this paper, we
provide discrete counterparts to the main gauge theoretical concepts, directly
in terms of Cellular Automata. More precisely, we describe a step-by-step
gauging pro... | cs.FL nlin.CG quant-ph | gaugeinvariance is a fundamental concept in physicsknown to provide the mathematical justification for all four fundamental forces in this paper we provide discrete counterparts to the main gauge theoretical concepts directly in terms of cellular automata more precisely we describe a stepbystep gauging procedure to enf... | [['gaugeinvariance', 'is', 'a', 'fundamental', 'concept', 'in', 'physicsknown', 'to', 'provide', 'the', 'mathematical', 'justification', 'for', 'all', 'four', 'fundamental', 'forces', 'in', 'this', 'paper', 'we', 'provide', 'discrete', 'counterparts', 'to', 'the', 'main', 'gauge', 'theoretical', 'concepts', 'directly',... | [-0.09079510151178158, 0.10519835752986219, -0.12360852349511518, 0.10799563582036265, -0.15785727740683575, -0.1854125006475999, 0.11663919405617314, 0.3538638196543467, -0.2874397312347986, -0.2371784977624383, 0.05842858577284924, -0.1717540019723986, -0.22340763432605723, 0.18676075923769753, -0.1177496489809175, 0... |
1,802.07645 | Limiting behavior of solutions for Euler equations of compressible fluid
flow | We study the limiting behavior of the solutions of Euler equations of
one-dimensional compressible fluid flow as the pressure like term vanishes.
This system can be thought of as an approximation for the one dimensional model
for large scale structure formation of universe. We show that the solutions of
former equati... | math.AP | we study the limiting behavior of the solutions of euler equations of onedimensional compressible fluid flow as the pressure like term vanishes this system can be thought of as an approximation for the one dimensional model for large scale structure formation of universe we show that the solutions of former equation co... | [['we', 'study', 'the', 'limiting', 'behavior', 'of', 'the', 'solutions', 'of', 'euler', 'equations', 'of', 'onedimensional', 'compressible', 'fluid', 'flow', 'as', 'the', 'pressure', 'like', 'term', 'vanishes', 'this', 'system', 'can', 'be', 'thought', 'of', 'as', 'an', 'approximation', 'for', 'the', 'one', 'dimension... | [-0.14395065427218612, 0.08834876055035765, -0.10655508882513172, 0.0755781359688722, -0.027543453959821676, -0.0964074480886522, -0.05741631172989544, 0.24756759836485512, -0.2904008029126807, -0.2599243982057822, 0.1394514205069036, -0.2560994452331215, -0.09846571817209845, 0.1674595416915652, 0.014659574377889695, ... |
1,802.07646 | Minimal cut-sets in the power graphs of certain finite non-cyclic groups | The power graph of a group is the simple graph with vertices as the group
elements, in which two distinct vertices are adjacent if and only if one of
them can be obtained as an integral power of the other. We study (minimal)
cut-sets of the power graph of a (finite) non-cyclic (nilpotent) group which
are associated w... | math.CO | the power graph of a group is the simple graph with vertices as the group elements in which two distinct vertices are adjacent if and only if one of them can be obtained as an integral power of the other we study minimal cutsets of the power graph of a finite noncyclic nilpotent group which are associated with its maxi... | [['the', 'power', 'graph', 'of', 'a', 'group', 'is', 'the', 'simple', 'graph', 'with', 'vertices', 'as', 'the', 'group', 'elements', 'in', 'which', 'two', 'distinct', 'vertices', 'are', 'adjacent', 'if', 'and', 'only', 'if', 'one', 'of', 'them', 'can', 'be', 'obtained', 'as', 'an', 'integral', 'power', 'of', 'the', 'ot... | [-0.21805198574561233, 0.19293369852570513, -0.10329531031464667, -0.004817861264056869, -0.1463032436180296, -0.17590815857616499, 1.3335635517968944e-06, 0.382867496210996, -0.32772786457989195, -0.24807931470844014, 0.12324008869396302, -0.28774377874000684, -0.09923855555366333, 0.1408657735446468, -0.1197886817022... |
1,802.07647 | MIS in the Congested Clique Model in $O(\log \log \Delta)$ Rounds | We give a maximal independent set (MIS) algorithm that runs in $O(\log \log
\Delta)$ rounds in the congested clique model, where $\Delta$ is the maximum
degree of the input graph. This improves upon the $O(\frac{\log(\Delta) \cdot
\log \log \Delta}{\sqrt{\log n}} + \log \log \Delta )$ rounds algorithm of
[Ghaffari, P... | cs.DC cs.DS | we give a maximal independent set mis algorithm that runs in olog log delta rounds in the congested clique model where delta is the maximum degree of the input graph this improves upon the ofraclogdelta cdot log log deltasqrtlog n log log delta rounds algorithm of ghaffari podc 17 where n is the number of vertices of t... | [['we', 'give', 'a', 'maximal', 'independent', 'set', 'mis', 'algorithm', 'that', 'runs', 'in', 'olog', 'log', 'delta', 'rounds', 'in', 'the', 'congested', 'clique', 'model', 'where', 'delta', 'is', 'the', 'maximum', 'degree', 'of', 'the', 'input', 'graph', 'this', 'improves', 'upon', 'the', 'ofraclogdelta', 'cdot', 'l... | [-0.2027628507332078, 0.09626005319545844, -0.007991373711930854, -0.027635909942910077, -0.020706950154687678, -0.18253538983408363, 0.17990228940200592, 0.3288057387606906, -0.25882368915315185, -0.4256586043031088, 0.03503341306017579, -0.28422449034239566, -0.14364315820525267, 0.06650875540217385, -0.1049660980701... |
1,802.07648 | Scalable and Robust Sparse Subspace Clustering Using Randomized
Clustering and Multilayer Graphs | Sparse subspace clustering (SSC) is one of the current state-of-the-art
methods for partitioning data points into the union of subspaces, with strong
theoretical guarantees. However, it is not practical for large data sets as it
requires solving a LASSO problem for each data point, where the number of
variables in ea... | cs.CV stat.ML | sparse subspace clustering ssc is one of the current stateoftheart methods for partitioning data points into the union of subspaces with strong theoretical guarantees however it is not practical for large data sets as it requires solving a lasso problem for each data point where the number of variables in each lasso pr... | [['sparse', 'subspace', 'clustering', 'ssc', 'is', 'one', 'of', 'the', 'current', 'stateoftheart', 'methods', 'for', 'partitioning', 'data', 'points', 'into', 'the', 'union', 'of', 'subspaces', 'with', 'strong', 'theoretical', 'guarantees', 'however', 'it', 'is', 'not', 'practical', 'for', 'large', 'data', 'sets', 'as'... | [-0.07657376557379977, 0.00281003839020276, -0.05801968538198131, 0.06236769308070589, -0.10333150224043773, -0.1631246035975484, 0.10833872744931557, 0.401205793954432, -0.3085306200675026, -0.2955189927573826, 0.11354470509525844, -0.29002792751228246, -0.1130040766691317, 0.18370636444269128, -0.0921574504097831, 0.... |
1,802.07649 | Harnack's Inequality for Parabolic Nonlocal Equations | The main result of this paper is a nonlocal version of Harnack's inequality
for a class of parabolic nonlocal equations. We additionally establish a weak
Harnack inequality as well as local boundedness of solutions. None of the
results require the solution to be globally positive.
| math.AP | the main result of this paper is a nonlocal version of harnacks inequality for a class of parabolic nonlocal equations we additionally establish a weak harnack inequality as well as local boundedness of solutions none of the results require the solution to be globally positive | [['the', 'main', 'result', 'of', 'this', 'paper', 'is', 'a', 'nonlocal', 'version', 'of', 'harnacks', 'inequality', 'for', 'a', 'class', 'of', 'parabolic', 'nonlocal', 'equations', 'we', 'additionally', 'establish', 'a', 'weak', 'harnack', 'inequality', 'as', 'well', 'as', 'local', 'boundedness', 'of', 'solutions', 'no... | [-0.1118327606883314, -0.02779257714541422, -0.07421222730643219, 0.08956959988507959, -0.09920439504914813, -0.18348586316116983, -0.025995533662434255, 0.2449564983861314, -0.3204025745391846, -0.2593295325628585, 0.18521818005893792, -0.27580361891951827, -0.14536166199379497, 0.23208847077977326, -0.102967763578312... |
1,802.0765 | Relativistic Entropy Inequality | In this paper we apply the entropy principle to the relativistic version of
the differential equations describing a standard fluid flow, that is, the
equations for mass, momentum, and a system for the energy matrix. These are the
second order equations which have been introduced in [3]. Since the principle
also says ... | math-ph math.MP | in this paper we apply the entropy principle to the relativistic version of the differential equations describing a standard fluid flow that is the equations for mass momentum and a system for the energy matrix these are the second order equations which have been introduced in 3 since the principle also says that the e... | [['in', 'this', 'paper', 'we', 'apply', 'the', 'entropy', 'principle', 'to', 'the', 'relativistic', 'version', 'of', 'the', 'differential', 'equations', 'describing', 'a', 'standard', 'fluid', 'flow', 'that', 'is', 'the', 'equations', 'for', 'mass', 'momentum', 'and', 'a', 'system', 'for', 'the', 'energy', 'matrix', 't... | [-0.10998275592033793, 0.0953960136116088, -0.13571618069047192, 0.07688821418848527, -0.027703826038821322, -0.09100968736802807, -0.02451479501145481, 0.2539327005260028, -0.2973675656358938, -0.2856251276937221, 0.09651273606357642, -0.2925403043438957, -0.10019773207940497, 0.170667630569959, -0.04015323200875574, ... |
1,802.07651 | Mixed perverse sheaves on flag varieties of Coxeter groups | In this paper we construct an abelian category of "mixed perverse sheaves"
attached to any realization of a Coxeter group, in terms of the associated
Elias-Williamson diagrammatic category. This construction extends previous work
of the first two authors, where we worked with parity complexes instead of
diagrams, and... | math.RT | in this paper we construct an abelian category of mixed perverse sheaves attached to any realization of a coxeter group in terms of the associated eliaswilliamson diagrammatic category this construction extends previous work of the first two authors where we worked with parity complexes instead of diagrams and we exten... | [['in', 'this', 'paper', 'we', 'construct', 'an', 'abelian', 'category', 'of', 'mixed', 'perverse', 'sheaves', 'attached', 'to', 'any', 'realization', 'of', 'a', 'coxeter', 'group', 'in', 'terms', 'of', 'the', 'associated', 'eliaswilliamson', 'diagrammatic', 'category', 'this', 'construction', 'extends', 'previous', 'w... | [-0.14472241630631216, 0.034474371342849135, -0.08454001340439564, 0.02685435546962335, -0.13495507646938054, -0.08664231733262037, -0.008986288962854345, 0.34354978879348613, -0.3350243176754794, -0.1888560623432813, 0.0717090824632016, -0.1970092559212379, -0.1660965181719721, 0.1697569117263964, -0.18698894778747907... |
1,802.07652 | Landmark Placement for Localization in a GPS-denied Environment | Path planning algorithms for unmanned aerial or ground vehicles, in many
surveillance applications, rely on Global Positioning System (GPS) information
for localization. However, disruption of GPS signals, by intention or
otherwise, can render these plans and algorithms ineffective. This article
provides a way of add... | math.OC | path planning algorithms for unmanned aerial or ground vehicles in many surveillance applications rely on global positioning system gps information for localization however disruption of gps signals by intention or otherwise can render these plans and algorithms ineffective this article provides a way of addressing thi... | [['path', 'planning', 'algorithms', 'for', 'unmanned', 'aerial', 'or', 'ground', 'vehicles', 'in', 'many', 'surveillance', 'applications', 'rely', 'on', 'global', 'positioning', 'system', 'gps', 'information', 'for', 'localization', 'however', 'disruption', 'of', 'gps', 'signals', 'by', 'intention', 'or', 'otherwise', ... | [-0.17916419646501833, 0.028999645733183213, -0.025925286977058825, 0.041793710627483535, -0.07229411241361032, -0.1407135181338983, 0.08383817760292075, 0.4231981552621423, -0.22555502915901005, -0.3695195483445537, 0.17150809223804733, -0.2500315884621266, -0.1915619065870951, 0.20851442825240904, -0.1699344633768002... |
1,802.07653 | Building Efficient ConvNets using Redundant Feature Pruning | This paper presents an efficient technique to prune deep and/or wide
convolutional neural network models by eliminating redundant features (or
filters). Previous studies have shown that over-sized deep neural network
models tend to produce a lot of redundant features that are either shifted
version of one another or ... | cs.CV | this paper presents an efficient technique to prune deep andor wide convolutional neural network models by eliminating redundant features or filters previous studies have shown that oversized deep neural network models tend to produce a lot of redundant features that are either shifted version of one another or are ver... | [['this', 'paper', 'presents', 'an', 'efficient', 'technique', 'to', 'prune', 'deep', 'andor', 'wide', 'convolutional', 'neural', 'network', 'models', 'by', 'eliminating', 'redundant', 'features', 'or', 'filters', 'previous', 'studies', 'have', 'shown', 'that', 'oversized', 'deep', 'neural', 'network', 'models', 'tend'... | [-0.04180648381316132, 0.045849836396087085, -0.05834343302922207, 0.05631192228884174, -0.11106672948881169, -0.19670894001956185, 0.0690963131355602, 0.4889333663045363, -0.2823272081222967, -0.3551755723747192, 0.10124833468125871, -0.2701824011091958, -0.18200813952216777, 0.17526316991825297, -0.12531862512332737,... |
1,802.07654 | Intersecting limit sets of Kleinian subgroups and Susskind's question | We construct a non-elementary Fuchsian group that admits two non-elementary
subgroups with trivial intersection and whose radial limit sets intersect
non-trivially. This negatively answers a question of Perry Susskind (1989) that
was stated as a conjecture by James W. Anderson (2014).
| math.DS | we construct a nonelementary fuchsian group that admits two nonelementary subgroups with trivial intersection and whose radial limit sets intersect nontrivially this negatively answers a question of perry susskind 1989 that was stated as a conjecture by james w anderson 2014 | [['we', 'construct', 'a', 'nonelementary', 'fuchsian', 'group', 'that', 'admits', 'two', 'nonelementary', 'subgroups', 'with', 'trivial', 'intersection', 'and', 'whose', 'radial', 'limit', 'sets', 'intersect', 'nontrivially', 'this', 'negatively', 'answers', 'a', 'question', 'of', 'perry', 'susskind', '1989', 'that', '... | [-0.1804722297436944, 0.17765399521194036, -0.12241872356886543, 0.07348871088825257, -0.12374362794727814, -0.22567089954845426, 0.10470699554411467, 0.3128049266411037, -0.2126692174593123, -0.24332923986153995, 0.07771526966471135, -0.2760806679668859, -0.1322375133451892, 0.1913759788816295, -0.22012535486052312, -... |
1,802.07655 | A Riemann-Hilbert problem for uncoupled BPS structures | We study the Riemann-Hilbert problem attached to an uncoupled BPS structure
proposed by Bridgeland in "Riemann-Hilbert problems from Donaldson-Thomas
theory". We show that it has "essentially" unique meromorphic solutions given
by a product of Gamma functions. We reconstruct the corresponding connection.
| math.AG hep-th | we study the riemannhilbert problem attached to an uncoupled bps structure proposed by bridgeland in riemannhilbert problems from donaldsonthomas theory we show that it has essentially unique meromorphic solutions given by a product of gamma functions we reconstruct the corresponding connection | [['we', 'study', 'the', 'riemannhilbert', 'problem', 'attached', 'to', 'an', 'uncoupled', 'bps', 'structure', 'proposed', 'by', 'bridgeland', 'in', 'riemannhilbert', 'problems', 'from', 'donaldsonthomas', 'theory', 'we', 'show', 'that', 'it', 'has', 'essentially', 'unique', 'meromorphic', 'solutions', 'given', 'by', 'a... | [-0.12284418934865332, -0.04805446454719924, -0.1387574356503603, 0.08693302068405034, -0.08173786516006036, -0.13253435343731104, -0.026148177129670797, 0.33332080098732214, -0.3617024105496523, -0.23909800695028247, 0.08058654984442244, -0.2352319099009037, -0.27457621689068107, 0.16252368674954262, -0.12223446007999... |
1,802.07656 | Effects of CO2 flushing on crystal textures and compositions:
experimental evidence from recent K trachybasalts erupted at Mt. Etna | Changes in magmatic assemblages and crystal stability as a response of CO2
flushing in basaltic systems have been never directly addressed experimentally,
making the role of CO2 in magma dynamics still controversial and object of
scientific debate. We conducted a series of experiments to understand the
response of ma... | physics.geo-ph | changes in magmatic assemblages and crystal stability as a response of co2 flushing in basaltic systems have been never directly addressed experimentally making the role of co2 in magma dynamics still controversial and object of scientific debate we conducted a series of experiments to understand the response of magmas... | [['changes', 'in', 'magmatic', 'assemblages', 'and', 'crystal', 'stability', 'as', 'a', 'response', 'of', 'co2', 'flushing', 'in', 'basaltic', 'systems', 'have', 'been', 'never', 'directly', 'addressed', 'experimentally', 'making', 'the', 'role', 'of', 'co2', 'in', 'magma', 'dynamics', 'still', 'controversial', 'and', ... | [-0.07015592207454042, 0.20879306839753536, -0.07972478957697621, -0.013818514070362024, -0.02656761716948264, -0.06387770853181314, 0.05102082625919876, 0.34572854108275836, -0.2894267296479706, -0.3300620469732493, 0.1443545440145369, -0.2939540565116889, -0.10086541420652441, 0.15432897485118824, -0.0424892378215622... |
1,802.07657 | DNA-Graphene Interactions During Translocation Through Nanogaps | We study how double-stranded DNA translocates through graphene nanogaps.
Nanogaps are fabricated with a novel capillary-force induced graphene nanogap
formation technique. DNA translocation signatures for nanogaps are
qualitatively different from those obtained with circular nanopores, owing to
the distinct shape of ... | cond-mat.mes-hall | we study how doublestranded dna translocates through graphene nanogaps nanogaps are fabricated with a novel capillaryforce induced graphene nanogap formation technique dna translocation signatures for nanogaps are qualitatively different from those obtained with circular nanopores owing to the distinct shape of the gap... | [['we', 'study', 'how', 'doublestranded', 'dna', 'translocates', 'through', 'graphene', 'nanogaps', 'nanogaps', 'are', 'fabricated', 'with', 'a', 'novel', 'capillaryforce', 'induced', 'graphene', 'nanogap', 'formation', 'technique', 'dna', 'translocation', 'signatures', 'for', 'nanogaps', 'are', 'qualitatively', 'diffe... | [-0.1433656914645563, 0.22808245601962604, -0.021957280011543925, 0.004571024355802523, -0.030981910981885765, -0.22031891512401078, 0.058312635312018836, 0.4738933715969324, -0.3135643478442469, -0.2934490189533276, -0.002519618863563823, -0.24128534933147222, -0.1839892477963788, 0.21487872737824268, -0.0080691802037... |
1,802.07658 | The local rotation curve of the Milky Way based on SEGUE and RAVE data | We construct the rotation curve of the Milky Way in the extended solar
neighbourhood using a sample of SEGUE (Sloan Extension for Galactic
Understanding and Exploration) G-dwarfs. We investigate the rotation curve
shape for the presence of any peculiarities just outside the solar radius as
has been reported by some a... | astro-ph.GA | we construct the rotation curve of the milky way in the extended solar neighbourhood using a sample of segue sloan extension for galactic understanding and exploration gdwarfs we investigate the rotation curve shape for the presence of any peculiarities just outside the solar radius as has been reported by some authors... | [['we', 'construct', 'the', 'rotation', 'curve', 'of', 'the', 'milky', 'way', 'in', 'the', 'extended', 'solar', 'neighbourhood', 'using', 'a', 'sample', 'of', 'segue', 'sloan', 'extension', 'for', 'galactic', 'understanding', 'and', 'exploration', 'gdwarfs', 'we', 'investigate', 'the', 'rotation', 'curve', 'shape', 'fo... | [-0.07804717816395203, 0.055668244155606735, -0.11219883933578483, 0.054703986632241006, -0.10483934562135902, -0.025266484636126227, 0.01878833112789801, 0.3849934492846606, -0.23985386553761567, -0.33865409297437443, 0.03567359432108114, -0.23035872887380215, -0.018907556327542773, 0.2352698207843652, -0.069699512297... |
1,802.07659 | 3D modelling of self-organized patterns of spots on anodes of DC glow
discharge | Self-organized patterns of spots on a at metallic anode in a cylindrical glow
dis- charge tube are simulated self-consistently. A standard model of a glow
discharge is used, comprising conservation and transport equations for a single
species of ion and electrons, written with the use of the drift-diffusion and
local... | physics.plasm-ph | selforganized patterns of spots on a at metallic anode in a cylindrical glow dis charge tube are simulated selfconsistently a standard model of a glow discharge is used comprising conservation and transport equations for a single species of ion and electrons written with the use of the driftdiffusion and localfield app... | [['selforganized', 'patterns', 'of', 'spots', 'on', 'a', 'at', 'metallic', 'anode', 'in', 'a', 'cylindrical', 'glow', 'dis', 'charge', 'tube', 'are', 'simulated', 'selfconsistently', 'a', 'standard', 'model', 'of', 'a', 'glow', 'discharge', 'is', 'used', 'comprising', 'conservation', 'and', 'transport', 'equations', 'f... | [-0.12876521623995638, 0.14350198242120826, -0.0349966218868175, 0.025211282910253756, 0.013195187848909065, -0.14550381089644268, 0.01578335279340629, 0.33826960913407117, -0.23215077343420723, -0.278266936301803, 0.08095916199351613, -0.3013640607181841, -0.06276464164674951, 0.17559145774486332, -0.01008019992094397... |
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