id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,801.08369 | First-principles calculations of Raman vibrational modes in the
fingerprint region for connective tissue | Vibrational spectroscopy has been widely employed to unravel
physical-chemical properties of biological systems. Due to its high sensitivity
to monitor real time "in situ" changes, Raman spectroscopy has been
successfully employed, e.g., in biomedicine, metabolomics, and biomedical
engineering. The grounds of interpr... | cond-mat.soft physics.bio-ph | vibrational spectroscopy has been widely employed to unravel physicalchemical properties of biological systems due to its high sensitivity to monitor real time in situ changes raman spectroscopy has been successfully employed eg in biomedicine metabolomics and biomedical engineering the grounds of interpretation of ram... | [['vibrational', 'spectroscopy', 'has', 'been', 'widely', 'employed', 'to', 'unravel', 'physicalchemical', 'properties', 'of', 'biological', 'systems', 'due', 'to', 'its', 'high', 'sensitivity', 'to', 'monitor', 'real', 'time', 'in', 'situ', 'changes', 'raman', 'spectroscopy', 'has', 'been', 'successfully', 'employed',... | [-0.06280919453215941, 0.08815282879770381, -0.08064488351550415, 0.07611012926993324, -0.03873847357593246, -0.11013606605293541, 0.042900128759333855, 0.41262646262412483, -0.24544885454259946, -0.30529312038597484, 0.034948455853827345, -0.27785954554131403, -0.1668312259565067, 0.1510618942766595, -0.01890578875151... |
1,801.0837 | On the abundance of silting modules | Silting modules are abundant. Indeed, they parametrise the definable torsion
classes over a noetherian ring, and the hereditary torsion pairs of finite type
over a commutative ring. Also the universal localisations of a hereditary ring,
or of a finite dimensional algebra of finite representation type, can be
parametr... | math.RT math.RA | silting modules are abundant indeed they parametrise the definable torsion classes over a noetherian ring and the hereditary torsion pairs of finite type over a commutative ring also the universal localisations of a hereditary ring or of a finite dimensional algebra of finite representation type can be parametrised by ... | [['silting', 'modules', 'are', 'abundant', 'indeed', 'they', 'parametrise', 'the', 'definable', 'torsion', 'classes', 'over', 'a', 'noetherian', 'ring', 'and', 'the', 'hereditary', 'torsion', 'pairs', 'of', 'finite', 'type', 'over', 'a', 'commutative', 'ring', 'also', 'the', 'universal', 'localisations', 'of', 'a', 'he... | [-0.18148091643468126, 0.08276856674316835, -0.06650261116492284, 0.11600215050887752, -0.1355878922350511, -0.17726510437205434, -0.06477903574705124, 0.36146197903465915, -0.40528115673692194, -0.1593995112200062, 0.0783418137504562, -0.1788576523495185, -0.09776831252875363, 0.2063504546705343, -0.18762769999417972,... |
1,801.08371 | Numerical construction of multipartite entanglement witnesses | Entanglement in multipartite systems is a key resource for quantum
information and communication protocols, making its verification in complex
systems a necessity. Because an exact calculation of arbitrary entanglement
probes is impossible, we derive and implement a numerical method to construct
multipartite witnesse... | quant-ph | entanglement in multipartite systems is a key resource for quantum information and communication protocols making its verification in complex systems a necessity because an exact calculation of arbitrary entanglement probes is impossible we derive and implement a numerical method to construct multipartite witnesses to ... | [['entanglement', 'in', 'multipartite', 'systems', 'is', 'a', 'key', 'resource', 'for', 'quantum', 'information', 'and', 'communication', 'protocols', 'making', 'its', 'verification', 'in', 'complex', 'systems', 'a', 'necessity', 'because', 'an', 'exact', 'calculation', 'of', 'arbitrary', 'entanglement', 'probes', 'is'... | [-0.11815611580534587, 0.019867825953244593, -0.128553298473846, 0.08516291001467921, -0.029929905331560543, -0.21639072767547554, 0.05440612027647033, 0.3272686639859799, -0.20707106043858128, -0.28099616302458186, 0.10549759762527953, -0.23736597652665326, -0.16829993630508108, 0.2682356030683935, -0.0418736209708546... |
1,801.08372 | decryst: an efficient software suite for structure determination from
powder diffraction | Presented here is decryst, a software suite for structure determination from
powder diffraction, which uses the direct space method, and is able to apply
anti-bump constraints automatically and efficiently during the procedure of
global optimisation using the crystallographic collision detection algorithm in
arXiv:17... | cond-mat.mtrl-sci | presented here is decryst a software suite for structure determination from powder diffraction which uses the direct space method and is able to apply antibump constraints automatically and efficiently during the procedure of global optimisation using the crystallographic collision detection algorithm in arxiv170803180... | [['presented', 'here', 'is', 'decryst', 'a', 'software', 'suite', 'for', 'structure', 'determination', 'from', 'powder', 'diffraction', 'which', 'uses', 'the', 'direct', 'space', 'method', 'and', 'is', 'able', 'to', 'apply', 'antibump', 'constraints', 'automatically', 'and', 'efficiently', 'during', 'the', 'procedure',... | [-0.05889101810480661, 0.04249050594480322, -0.12783431473213272, 0.024413846873653097, -0.11927896833701714, -0.15072670064631616, 0.043505680539670424, 0.4511544809148118, -0.2889593451132847, -0.35856821819686807, 0.11929374463176606, -0.18518803758664173, -0.1431180191234694, 0.25851484010549813, -0.063316848871312... |
1,801.08373 | On the subtelties of nonrelativistic reduction and applications | Various subtleties and problems associated with nonrelativistic (NR)
reduction of a scalar field theory to the Schroedinger theory are discussed.
Contrary to the usual approaches that discuss the mapping among the equations
of motion or the actions, we highlight the mapping among the space time
generators. Using a nu... | gr-qc hep-th | various subtleties and problems associated with nonrelativistic nr reduction of a scalar field theory to the schroedinger theory are discussed contrary to the usual approaches that discuss the mapping among the equations of motion or the actions we highlight the mapping among the space time generators using a null redu... | [['various', 'subtleties', 'and', 'problems', 'associated', 'with', 'nonrelativistic', 'nr', 'reduction', 'of', 'a', 'scalar', 'field', 'theory', 'to', 'the', 'schroedinger', 'theory', 'are', 'discussed', 'contrary', 'to', 'the', 'usual', 'approaches', 'that', 'discuss', 'the', 'mapping', 'among', 'the', 'equations', '... | [-0.14051199872763112, 0.10081080072380316, -0.07871625589009804, 0.09320671114591488, -0.09935411853411306, -0.12828905812393016, -0.05097850995550219, 0.303498960332945, -0.22063387650996447, -0.24806882681038517, 0.07337224896092756, -0.3029845066082019, -0.19834087086313118, 0.14638023493730892, -0.0338782345195515... |
1,801.08374 | Maximal subgroups of ${}^2E_6(2)$ and its automorphism groups | We give a new computer-assisted proof of the classification of maximal
subgroups of the simple group ${}^2E_6(2)$ and its extensions by any subgroup
of the outer automorphism group $S_3$. This is not a new result, but no earlier
proof exists in the literature. A large part of the proof consists of a
computational ana... | math.GR | we give a new computerassisted proof of the classification of maximal subgroups of the simple group 2e_62 and its extensions by any subgroup of the outer automorphism group s_3 this is not a new result but no earlier proof exists in the literature a large part of the proof consists of a computational analysis of subgro... | [['we', 'give', 'a', 'new', 'computerassisted', 'proof', 'of', 'the', 'classification', 'of', 'maximal', 'subgroups', 'of', 'the', 'simple', 'group', '2e_62', 'and', 'its', 'extensions', 'by', 'any', 'subgroup', 'of', 'the', 'outer', 'automorphism', 'group', 's_3', 'this', 'is', 'not', 'a', 'new', 'result', 'but', 'no'... | [-0.12539861063767027, 0.047685238912909926, -0.1582970418035984, 0.025475312410363632, -0.1067515026189779, -0.07792701515320101, 0.07432949727793273, 0.33237166659612405, -0.23938682720457252, -0.31131560324054014, 0.17612243067154562, -0.23969383238765754, -0.11749589418698299, 0.23060982986108253, -0.10821908112419... |
1,801.08375 | Theory of high-resolution tunneling spin transport on a magnetic
skyrmion | Tunneling spin transport characteristics of a magnetic skyrmion are described
theoretically in magnetic scanning tunneling microscopy (STM). The
spin-polarized charge current in STM (SP-STM) and tunneling spin transport
vector quantities, the longitudinal spin current and the spin transfer torque,
are calculated in h... | cond-mat.mtrl-sci | tunneling spin transport characteristics of a magnetic skyrmion are described theoretically in magnetic scanning tunneling microscopy stm the spinpolarized charge current in stm spstm and tunneling spin transport vector quantities the longitudinal spin current and the spin transfer torque are calculated in high spatial... | [['tunneling', 'spin', 'transport', 'characteristics', 'of', 'a', 'magnetic', 'skyrmion', 'are', 'described', 'theoretically', 'in', 'magnetic', 'scanning', 'tunneling', 'microscopy', 'stm', 'the', 'spinpolarized', 'charge', 'current', 'in', 'stm', 'spstm', 'and', 'tunneling', 'spin', 'transport', 'vector', 'quantities... | [-0.18973383735429844, 0.1932046211813744, -0.05012432698549019, 0.049946112746687726, -0.034739574504573996, -0.12014904958380239, 0.01620357845643562, 0.41819093179413314, -0.3179366875627487, -0.29190840218350184, -0.05278075486505337, -0.30086443537725605, -0.12014291347205477, 0.24456379735480538, 0.04794063164999... |
1,801.08376 | Persistent Betti numbers of random \v{C}ech complexes | We study the persistent homology of random \v{C}ech complexes. Generalizing a
method of Penrose for studying random geometric graphs, we first describe an
appropriate theoretical framework in which we can state and address our main
questions. Then we define the kth persistent Betti number of a random \v{C}ech
complex... | math.AT cs.CG math.MG | we study the persistent homology of random vcech complexes generalizing a method of penrose for studying random geometric graphs we first describe an appropriate theoretical framework in which we can state and address our main questions then we define the kth persistent betti number of a random vcech complex and determ... | [['we', 'study', 'the', 'persistent', 'homology', 'of', 'random', 'vcech', 'complexes', 'generalizing', 'a', 'method', 'of', 'penrose', 'for', 'studying', 'random', 'geometric', 'graphs', 'we', 'first', 'describe', 'an', 'appropriate', 'theoretical', 'framework', 'in', 'which', 'we', 'can', 'state', 'and', 'address', '... | [-0.1862747368897185, 0.07928485709208748, -0.0761449405302604, 0.12728459007296436, -0.058802920382147954, -0.04775251395264526, 0.0369569323439565, 0.2974205759733363, -0.3178062301910954, -0.24771894565151062, 0.09581643133999113, -0.23085088570268802, -0.21422995170463383, 0.15552572892219932, -0.13132819575315088,... |
1,801.08377 | Asteroseismology of red giant stars | If appropriately excited, a star will oscillate like a giant spherical
instrument. In most stars, including the Sun, surface convection provides the
excitation mechanism (Goldreich and Keeley, 1977). With turbulent velocities
reaching speeds comparable to the local sound speed near the surface of the
star, the vigoro... | astro-ph.SR | if appropriately excited a star will oscillate like a giant spherical instrument in most stars including the sun surface convection provides the excitation mechanism goldreich and keeley 1977 with turbulent velocities reaching speeds comparable to the local sound speed near the surface of the star the vigorous convecti... | [['if', 'appropriately', 'excited', 'a', 'star', 'will', 'oscillate', 'like', 'a', 'giant', 'spherical', 'instrument', 'in', 'most', 'stars', 'including', 'the', 'sun', 'surface', 'convection', 'provides', 'the', 'excitation', 'mechanism', 'goldreich', 'and', 'keeley', '1977', 'with', 'turbulent', 'velocities', 'reachi... | [-0.09885623187891733, 0.29033360078396037, -0.05767552274526247, 0.079176586654987, -0.14104985082890875, -0.052657318900864905, 0.04006153365624792, 0.34426255387226395, -0.2322383023306294, -0.3354574192948132, 0.07298788739227699, -0.26048898229105766, -0.05436682776607905, 0.210049527382598, -0.05140962344991956, ... |
1,801.08378 | On the local integrability condition for generalised
translation-invariant systems | This paper considers the local integrability condition for generalised
translation-invariant systems and its relation to the Calder\'on integrability
condition, the temperateness condition and the uniform counting estimate. It is
shown that sufficient and necessary conditions for satisfying the local
integrability co... | math.FA | this paper considers the local integrability condition for generalised translationinvariant systems and its relation to the calderon integrability condition the temperateness condition and the uniform counting estimate it is shown that sufficient and necessary conditions for satisfying the local integrability condition... | [['this', 'paper', 'considers', 'the', 'local', 'integrability', 'condition', 'for', 'generalised', 'translationinvariant', 'systems', 'and', 'its', 'relation', 'to', 'the', 'calderon', 'integrability', 'condition', 'the', 'temperateness', 'condition', 'and', 'the', 'uniform', 'counting', 'estimate', 'it', 'is', 'shown... | [-0.15725754655979793, 0.10230791027630295, -0.059022553951089164, 0.11857237444971414, -0.07150052875444732, -0.11864334512501955, 0.03541161416180651, 0.3073521024273599, -0.25137496825088473, -0.26987199371625836, 0.15925036733970047, -0.24039041325449945, -0.14940170234630762, 0.22677418190766782, -0.07669479124905... |
1,801.08379 | DeepWriting: Making Digital Ink Editable via Deep Generative Modeling | Digital ink promises to combine the flexibility and aesthetics of handwriting
and the ability to process, search and edit digital text. Character recognition
converts handwritten text into a digital representation, albeit at the cost of
losing personalized appearance due to the technical difficulties of separating
th... | cs.HC cs.LG | digital ink promises to combine the flexibility and aesthetics of handwriting and the ability to process search and edit digital text character recognition converts handwritten text into a digital representation albeit at the cost of losing personalized appearance due to the technical difficulties of separating the int... | [['digital', 'ink', 'promises', 'to', 'combine', 'the', 'flexibility', 'and', 'aesthetics', 'of', 'handwriting', 'and', 'the', 'ability', 'to', 'process', 'search', 'and', 'edit', 'digital', 'text', 'character', 'recognition', 'converts', 'handwritten', 'text', 'into', 'a', 'digital', 'representation', 'albeit', 'at', ... | [-0.015104123150406736, -0.011967237616872434, -0.06047410851195384, 0.03803849221518024, -0.16990356786457234, -0.17224011685354762, 0.08757955194147916, 0.41035563840645634, -0.30404384858421474, -0.3603420881682063, 0.06036702844183509, -0.3088643758283443, -0.1591141013131949, 0.19343284978084777, -0.16450125579594... |
1,801.0838 | Hardness of Approximation for Morse Matching | Discrete Morse theory has emerged as a powerful tool for a wide range of
problems, including the computation of (persistent) homology. In this context,
discrete Morse theory is used to reduce the problem of computing a topological
invariant of an input simplicial complex to computing the same topological
invariant of... | math.AT cs.CC cs.CG math.CO | discrete morse theory has emerged as a powerful tool for a wide range of problems including the computation of persistent homology in this context discrete morse theory is used to reduce the problem of computing a topological invariant of an input simplicial complex to computing the same topological invariant of a sign... | [['discrete', 'morse', 'theory', 'has', 'emerged', 'as', 'a', 'powerful', 'tool', 'for', 'a', 'wide', 'range', 'of', 'problems', 'including', 'the', 'computation', 'of', 'persistent', 'homology', 'in', 'this', 'context', 'discrete', 'morse', 'theory', 'is', 'used', 'to', 'reduce', 'the', 'problem', 'of', 'computing', '... | [-0.1271868631702402, 0.05512740837605859, -0.044119724332709186, 0.08987794634358734, -0.07728658327594018, -0.13367069149429664, 0.04062934872509243, 0.3858244774592483, -0.32199912631295174, -0.3152027752998675, 0.11325379905816263, -0.21804695169075242, -0.1719542240911028, 0.17928695826866847, -0.09585780081621263... |
1,801.08381 | Stability and Invariant Random Subgroups | Consider $\operatorname{Sym}(n)$, endowed with the normalized Hamming metric
$d_n$. A finitely-generated group $\Gamma$ is \emph{P-stable} if every almost
homomorphism $\rho_{n_k}\colon \Gamma\rightarrow\operatorname{Sym}(n_k)$ (i.e.,
for every $g,h\in\Gamma$, $\lim_{k\rightarrow\infty}d_{n_k}(
\rho_{n_k}(gh),\rho_{n... | math.GR | consider operatornamesymn endowed with the normalized hamming metric d_n a finitelygenerated group gamma is emphpstable if every almost homomorphism rho_n_kcolon gammarightarrowoperatornamesymn_k ie for every ghingamma lim_krightarrowinftyd_n_k rho_n_kghrho_n_kgrho_n_kh0 is close to an actual homomorphism varphi_n_k co... | [['consider', 'operatornamesymn', 'endowed', 'with', 'the', 'normalized', 'hamming', 'metric', 'd_n', 'a', 'finitelygenerated', 'group', 'gamma', 'is', 'emphpstable', 'if', 'every', 'almost', 'homomorphism', 'rho_n_kcolon', 'gammarightarrowoperatornamesymn_k', 'ie', 'for', 'every', 'ghingamma', 'lim_krightarrowinftyd_n... | [-0.1255616787037268, 0.12491225117790435, -0.12131124298724502, 0.09776819338630147, -0.08299237170883704, -0.15505625980694104, 0.030089164460492826, 0.4016572949430435, -0.31216759271550887, -0.2380824993908553, 0.12726257321664527, -0.26218286168180627, -0.1211846393560714, 0.23718943165633644, -0.1473647843444683,... |
1,801.08382 | Stationary solutions to the boundary value problem for relativistic BGK
model in a slab | In this paper, we are concerned with the boundary value problem in a slab for
the stationary relativistic BGK model of Marle type, which is a relaxation
model of the relativistic Boltzmann equation. In the case of fixed inflow
boundary conditions, we establish the existence of unique stationary solutions.
| math.AP | in this paper we are concerned with the boundary value problem in a slab for the stationary relativistic bgk model of marle type which is a relaxation model of the relativistic boltzmann equation in the case of fixed inflow boundary conditions we establish the existence of unique stationary solutions | [['in', 'this', 'paper', 'we', 'are', 'concerned', 'with', 'the', 'boundary', 'value', 'problem', 'in', 'a', 'slab', 'for', 'the', 'stationary', 'relativistic', 'bgk', 'model', 'of', 'marle', 'type', 'which', 'is', 'a', 'relaxation', 'model', 'of', 'the', 'relativistic', 'boltzmann', 'equation', 'in', 'the', 'case', 'o... | [-0.16087163007837169, 0.05455536770691373, -0.10423702870172505, 0.04471411863912125, -0.07241198279875882, -0.14779694007747635, -0.026304075625078867, 0.29229274624008306, -0.28506898857196983, -0.191862018512828, 0.1137665248848973, -0.25158616583034094, -0.06384500617883643, 0.12950834570148465, -0.021492346094883... |
1,801.08383 | Data-Driven Impulse Response Regularization via Deep Learning | We consider the problem of impulse response estimation of stable linear
single-input single-output systems. It is a well-studied problem where flexible
non-parametric models recently offered a leap in performance compared to the
classical finite-dimensional model structures. Inspired by this development and
the succe... | cs.SY cs.LG stat.ML | we consider the problem of impulse response estimation of stable linear singleinput singleoutput systems it is a wellstudied problem where flexible nonparametric models recently offered a leap in performance compared to the classical finitedimensional model structures inspired by this development and the success of dee... | [['we', 'consider', 'the', 'problem', 'of', 'impulse', 'response', 'estimation', 'of', 'stable', 'linear', 'singleinput', 'singleoutput', 'systems', 'it', 'is', 'a', 'wellstudied', 'problem', 'where', 'flexible', 'nonparametric', 'models', 'recently', 'offered', 'a', 'leap', 'in', 'performance', 'compared', 'to', 'the'... | [-0.0815392769690805, 0.002265670841716858, -0.06544247349297785, 0.05395923328799117, -0.0949299237915281, -0.19969315327008266, 0.025712807222370463, 0.3755417109343661, -0.28336742525942715, -0.2645057467407132, 0.098347163797042, -0.2242298050817237, -0.23508389794312598, 0.219371282655454, -0.11746892004262612, 0.... |
1,801.08384 | Numerical investigation of transient, low-power metal vapour discharges
occurring in near limit ignitions of flammable gas | This article presents an investigation of a transient (30 {\mu}s - 5 ms)
electrical discharge in metal vapour with low voltage (< 50 V) and current (< 1
A), drawn between two separating electrodes. Discharges of this type are rarely
studied, but are important in electrical explosion safety, as they can ignite
flammab... | physics.app-ph | this article presents an investigation of a transient 30 mus 5 ms electrical discharge in metal vapour with low voltage 50 v and current 1 a drawn between two separating electrodes discharges of this type are rarely studied but are important in electrical explosion safety as they can ignite flammable gasses an empirica... | [['this', 'article', 'presents', 'an', 'investigation', 'of', 'a', 'transient', '30', 'mus', '5', 'ms', 'electrical', 'discharge', 'in', 'metal', 'vapour', 'with', 'low', 'voltage', '50', 'v', 'and', 'current', '1', 'a', 'drawn', 'between', 'two', 'separating', 'electrodes', 'discharges', 'of', 'this', 'type', 'are', '... | [-0.08660873483031352, 0.09837152948617883, -0.043955910420496666, 0.037998620642239835, 0.01671367674372254, -0.16695653899496762, 0.07233761196833684, 0.39199731038047037, -0.2379187251303383, -0.31902639055862186, 0.08651486909158328, -0.2788592323682233, -0.09941732929069169, 0.2363157468344256, -0.0337453125500861... |
1,801.08385 | Role of Coherence in Excitation Transfer Efficiency to the Reaction
Center in Photosynthetic Bacteria Chlorobium Tepidum | We investigate the effect of coherence to the excitation transfer efficiency
(ETE) in photosynthetic bacteria Chlorobium Tepidum. We have modeled the
monomer of Fenna-Matthews-Olson (FMO) complex as consisting of eight
bacteriochlorophyll-a sites, while explicitly consider reaction center core
complex (RCC) as an add... | physics.bio-ph | we investigate the effect of coherence to the excitation transfer efficiency ete in photosynthetic bacteria chlorobium tepidum we have modeled the monomer of fennamatthewsolson fmo complex as consisting of eight bacteriochlorophylla sites while explicitly consider reaction center core complex rcc as an additional site ... | [['we', 'investigate', 'the', 'effect', 'of', 'coherence', 'to', 'the', 'excitation', 'transfer', 'efficiency', 'ete', 'in', 'photosynthetic', 'bacteria', 'chlorobium', 'tepidum', 'we', 'have', 'modeled', 'the', 'monomer', 'of', 'fennamatthewsolson', 'fmo', 'complex', 'as', 'consisting', 'of', 'eight', 'bacteriochlorop... | [-0.09533025981858373, 0.10080981786595658, -0.04461636448488571, 0.06175074188411236, 0.050444352952763435, -0.1262767429985106, 0.01142280232347548, 0.36648025092110037, -0.24747279120981694, -0.2704284861907363, 0.033577864238061014, -0.2888932665064931, -0.12473318842798471, 0.1431297944318503, 0.01239512336999178,... |
1,801.08386 | Conserved energies for the one dimensional Gross-Pitaevskii equation | We prove the global-in-time well-posedness of the one dimensional
Gross-Pitaevskii equation in the energy space, which is a complete metric space
equipped with a newly introduced metric and with the energy norm describing the
$H^s$ regularities of the solutions. We establish a family of conserved
energies for the one... | math.AP | we prove the globalintime wellposedness of the one dimensional grosspitaevskii equation in the energy space which is a complete metric space equipped with a newly introduced metric and with the energy norm describing the hs regularities of the solutions we establish a family of conserved energies for the one dimensiona... | [['we', 'prove', 'the', 'globalintime', 'wellposedness', 'of', 'the', 'one', 'dimensional', 'grosspitaevskii', 'equation', 'in', 'the', 'energy', 'space', 'which', 'is', 'a', 'complete', 'metric', 'space', 'equipped', 'with', 'a', 'newly', 'introduced', 'metric', 'and', 'with', 'the', 'energy', 'norm', 'describing', 't... | [-0.16019053883331863, 0.10347997086547032, -0.05372835966630226, 0.11709935337900408, -0.046020256402560425, -0.09460178565210368, -0.09055871859522938, 0.2673923008238213, -0.2913795087981639, -0.21270337907149445, 0.09649871542896557, -0.3056066668344827, -0.1131113199163464, 0.1269198865924455, -0.00235946045575451... |
1,801.08387 | The $(2,5)$ minimal model on genus two surfaces | In the $(2,5)$ minimal model, the partition function for genus $g=2$ Riemann
surfaces is given by a $5$-tuple of functions with appropriate transformation
under the mapping class group. These functions generalise the two
Rogers-Ramanujan functions for the torus. Their expansions around a locus of
surfaces with conica... | hep-th math.QA | in the 25 minimal model the partition function for genus g2 riemann surfaces is given by a 5tuple of functions with appropriate transformation under the mapping class group these functions generalise the two rogersramanujan functions for the torus their expansions around a locus of surfaces with conical singularities i... | [['in', 'the', '25', 'minimal', 'model', 'the', 'partition', 'function', 'for', 'genus', 'g2', 'riemann', 'surfaces', 'is', 'given', 'by', 'a', '5tuple', 'of', 'functions', 'with', 'appropriate', 'transformation', 'under', 'the', 'mapping', 'class', 'group', 'these', 'functions', 'generalise', 'the', 'two', 'rogersrama... | [-0.15516376004181184, 0.07593714734709002, -0.0999402035095587, 0.08547581091988832, -0.108968237683251, -0.09009517754569946, -0.00468430043019305, 0.3037400339631401, -0.23384814486925226, -0.25246516265675106, 0.10151070558052781, -0.2532211781960499, -0.16268054410099786, 0.21965298985457973, -0.06886105092600087,... |
1,801.08388 | A Benchmark and Evaluation of Non-Rigid Structure from Motion | Non-Rigid structure from motion (NRSfM), is a long standing and central
problem in computer vision and its solution is necessary for obtaining 3D
information from multiple images when the scene is dynamic. A main issue
regarding the further development of this important computer vision topic, is
the lack of high qual... | cs.CV | nonrigid structure from motion nrsfm is a long standing and central problem in computer vision and its solution is necessary for obtaining 3d information from multiple images when the scene is dynamic a main issue regarding the further development of this important computer vision topic is the lack of high quality data... | [['nonrigid', 'structure', 'from', 'motion', 'nrsfm', 'is', 'a', 'long', 'standing', 'and', 'central', 'problem', 'in', 'computer', 'vision', 'and', 'its', 'solution', 'is', 'necessary', 'for', 'obtaining', '3d', 'information', 'from', 'multiple', 'images', 'when', 'the', 'scene', 'is', 'dynamic', 'a', 'main', 'issue',... | [-0.07891093357171439, -0.0030471546466932396, -0.06829314620405011, 0.02805813145602735, -0.09082464695483729, -0.0882943374859287, 0.023261313860104244, 0.3771863389948878, -0.25858624331370184, -0.3515715488568656, 0.1561668088071673, -0.2473018944287036, -0.10424001799023981, 0.23877888915565196, -0.086824069549683... |
1,801.08389 | Sodium storage via single epoxy group on graphene - The role of surface
doping | Due to its unique physical and chemical properties, graphene is being
considered as a promising material for energy conversion and storage
applications. Introduction of functional groups and dopants on/in graphene is a
useful strategy for tuning its properties. In order to fully exploit its
potential, atomic-level un... | cond-mat.mtrl-sci | due to its unique physical and chemical properties graphene is being considered as a promising material for energy conversion and storage applications introduction of functional groups and dopants onin graphene is a useful strategy for tuning its properties in order to fully exploit its potential atomiclevel understand... | [['due', 'to', 'its', 'unique', 'physical', 'and', 'chemical', 'properties', 'graphene', 'is', 'being', 'considered', 'as', 'a', 'promising', 'material', 'for', 'energy', 'conversion', 'and', 'storage', 'applications', 'introduction', 'of', 'functional', 'groups', 'and', 'dopants', 'onin', 'graphene', 'is', 'a', 'usefu... | [-0.07602237614932968, 0.14174542759090317, 0.010808848727191256, -0.017928998944076145, 0.016815145435028298, -0.20334603323676992, 0.09914089376675399, 0.44035485365189786, -0.24449859364066534, -0.3017870440949188, 0.01633886557693734, -0.3474007293630695, -0.14488712967330114, 0.15764363335857037, -0.03616897905814... |
1,801.0839 | Global and Local Consistent Age Generative Adversarial Networks | Age progression/regression is a challenging task due to the complicated and
non-linear transformation in human aging process. Many researches have shown
that both global and local facial features are essential for face
representation, but previous GAN based methods mainly focused on the global
feature in age synthesi... | cs.CV | age progressionregression is a challenging task due to the complicated and nonlinear transformation in human aging process many researches have shown that both global and local facial features are essential for face representation but previous gan based methods mainly focused on the global feature in age synthesis to u... | [['age', 'progressionregression', 'is', 'a', 'challenging', 'task', 'due', 'to', 'the', 'complicated', 'and', 'nonlinear', 'transformation', 'in', 'human', 'aging', 'process', 'many', 'researches', 'have', 'shown', 'that', 'both', 'global', 'and', 'local', 'facial', 'features', 'are', 'essential', 'for', 'face', 'repre... | [-0.013416587904974166, -0.05147744022415094, -0.06977630228034615, 0.07314353704561616, -0.07691031814428027, -0.15378474843653506, -0.0314726212095546, 0.46359612546937984, -0.25575108274867875, -0.3333775073616314, 0.10681888493397225, -0.29048204287579377, -0.2069335494672918, 0.15338872069344117, -0.18239455338814... |
1,801.08391 | Understanding Human Behaviors in Crowds by Imitating the Decision-Making
Process | Crowd behavior understanding is crucial yet challenging across a wide range
of applications, since crowd behavior is inherently determined by a sequential
decision-making process based on various factors, such as the pedestrians' own
destinations, interaction with nearby pedestrians and anticipation of upcoming
event... | cs.CV | crowd behavior understanding is crucial yet challenging across a wide range of applications since crowd behavior is inherently determined by a sequential decisionmaking process based on various factors such as the pedestrians own destinations interaction with nearby pedestrians and anticipation of upcoming events in th... | [['crowd', 'behavior', 'understanding', 'is', 'crucial', 'yet', 'challenging', 'across', 'a', 'wide', 'range', 'of', 'applications', 'since', 'crowd', 'behavior', 'is', 'inherently', 'determined', 'by', 'a', 'sequential', 'decisionmaking', 'process', 'based', 'on', 'various', 'factors', 'such', 'as', 'the', 'pedestrian... | [-0.06734222346414806, 0.08464452570251846, -0.09358361480321656, 0.09292452092760727, -0.14638780335506016, -0.15876057542239627, 0.06529868657763466, 0.4732394218709029, -0.28469127348577933, -0.3280096421817463, -9.519888950075875e-05, -0.2523052016230208, -0.2381978042106679, 0.12404267881594017, -0.163071242593730... |
1,801.08392 | Preliminary Planck constant measurements via UME oscillating - magnet
Kibble balance | The UME Kibble balance project was initiated at the second half of 2014.
During this period we have studied the theoretical aspects of Kibble balances
in which an oscillating magnet generates AC Faraday voltage in a stationary
coil and constructed a trial version to implement this idea. The remarkable
feature of this... | physics.ins-det | the ume kibble balance project was initiated at the second half of 2014 during this period we have studied the theoretical aspects of kibble balances in which an oscillating magnet generates ac faraday voltage in a stationary coil and constructed a trial version to implement this idea the remarkable feature of this app... | [['the', 'ume', 'kibble', 'balance', 'project', 'was', 'initiated', 'at', 'the', 'second', 'half', 'of', '2014', 'during', 'this', 'period', 'we', 'have', 'studied', 'the', 'theoretical', 'aspects', 'of', 'kibble', 'balances', 'in', 'which', 'an', 'oscillating', 'magnet', 'generates', 'ac', 'faraday', 'voltage', 'in', ... | [-0.12442276194612954, 0.15633663406005724, -0.08936588434358193, 0.02765918680889742, -0.06737133211777611, -0.1276855778853363, 0.06042662819496579, 0.3131611498374439, -0.24759945687985468, -0.344726924541813, 0.06236168556325269, -0.23467158555040057, -0.11525633641802312, 0.20833363038697608, -0.0664842759806689, ... |
1,801.08393 | Critique of Feynman Propagator, the $\E \cdot x$ gauge | Consider M\o{}ller scattering. Electrons with momentum $p$ and $-p$ scatter
by exchange of photon say in $z$ direction to $p+q$ and $-(p+q)$. The
scattering amplitude is well known, given as Feynman propagator $ \M = \frac{(e
\hbar c)^2}{\epsilon_0 V} \frac{\bar{u}(p+q) \gamma^{\mu} u(p) \
\bar{u}(-(p+q)) \gamma_{\mu... | quant-ph hep-th | consider moller scattering electrons with momentum p and p scatter by exchange of photon say in z direction to pq and pq the scattering amplitude is well known given as feynman propagator m frace hbar c2epsilon_0 v fracbarupq gammamu up barupq gamma_mu upq2 where v is the volume of the scattering electrons e elementary... | [['consider', 'moller', 'scattering', 'electrons', 'with', 'momentum', 'p', 'and', 'p', 'scatter', 'by', 'exchange', 'of', 'photon', 'say', 'in', 'z', 'direction', 'to', 'pq', 'and', 'pq', 'the', 'scattering', 'amplitude', 'is', 'well', 'known', 'given', 'as', 'feynman', 'propagator', 'm', 'frace', 'hbar', 'c2epsilon_0... | [-0.19032677541249593, 0.2802798742460785, -0.022810171520100137, 0.07301462095077545, -0.07662153688284594, -0.2015469289550191, 0.02647997947831361, 0.3809634521392329, -0.25848820100944764, -0.2357215836798569, -0.055194695308915985, -0.33520454687559004, -0.01732560001789236, 0.13286876737213835, 0.0363111977778288... |
1,801.08394 | Multiphoton Photoelectron Circular Dichroism of Limonene with
Independent Polarization State Control of the Bound-Bound and Bound-Continuum
Transitions | Photoionization of randomly oriented chiral molecules with circularly
polarized light leads to a strong forward/backward asymmetry in the
photoelectron angular distribution. This chiroptical effect, referred to as
Photoelectron Circular Dichroism (PECD), was shown to take place in all
ionization regimes, from single ... | physics.chem-ph | photoionization of randomly oriented chiral molecules with circularly polarized light leads to a strong forwardbackward asymmetry in the photoelectron angular distribution this chiroptical effect referred to as photoelectron circular dichroism pecd was shown to take place in all ionization regimes from single photon to... | [['photoionization', 'of', 'randomly', 'oriented', 'chiral', 'molecules', 'with', 'circularly', 'polarized', 'light', 'leads', 'to', 'a', 'strong', 'forwardbackward', 'asymmetry', 'in', 'the', 'photoelectron', 'angular', 'distribution', 'this', 'chiroptical', 'effect', 'referred', 'to', 'as', 'photoelectron', 'circular... | [-0.0867133640109793, 0.20251781937642896, -0.07595595436615085, 0.012624297789203447, -0.005850253731891664, -0.10427000378329439, 0.032356443983351406, 0.45671035300202784, -0.21978055930821708, -0.28430247060283265, -0.03814263242771991, -0.2875903374846401, -0.047983275887173445, 0.17792086662053305, 0.033588077175... |
1,801.08395 | Effect of optical crosstalk on performance of ILD AHCAL | The design of the ILD AHCAL is optimized to make the best use of the PFA and
its active layers are composed of about eight million scintillator tiles
readout by SiPMs. If there is optical crosstalk between the tiles, the
calorimeter performance can be worsened. Simulation studies on the effect of
the optical crosstal... | physics.ins-det | the design of the ild ahcal is optimized to make the best use of the pfa and its active layers are composed of about eight million scintillator tiles readout by sipms if there is optical crosstalk between the tiles the calorimeter performance can be worsened simulation studies on the effect of the optical crosstalk on ... | [['the', 'design', 'of', 'the', 'ild', 'ahcal', 'is', 'optimized', 'to', 'make', 'the', 'best', 'use', 'of', 'the', 'pfa', 'and', 'its', 'active', 'layers', 'are', 'composed', 'of', 'about', 'eight', 'million', 'scintillator', 'tiles', 'readout', 'by', 'sipms', 'if', 'there', 'is', 'optical', 'crosstalk', 'between', 't... | [-0.10033699552919986, 0.12445919369549854, 0.009192747063934803, -0.038900156637005835, -0.0351500383078836, -0.14133683760124055, 0.02742129429310992, 0.4517221356863561, -0.20478007202779036, -0.3881814257660206, 0.09871610183019083, -0.3641375033657296, -0.07633153413948805, 0.19472387565326862, -0.0368290279816458... |
1,801.08396 | Dark Matter: The Problem of Motion | Equations of non-geodesic and non-geodesic deviations for different particles
are obtained, using a specific type of classes of the Bazanski Lagrangian. Such
type of paths has been found to describe the problem of variable mass in the
presence of Riemannian geometry. This may give rise to detect the effect of
dark ma... | gr-qc | equations of nongeodesic and nongeodesic deviations for different particles are obtained using a specific type of classes of the bazanski lagrangian such type of paths has been found to describe the problem of variable mass in the presence of riemannian geometry this may give rise to detect the effect of dark matter wh... | [['equations', 'of', 'nongeodesic', 'and', 'nongeodesic', 'deviations', 'for', 'different', 'particles', 'are', 'obtained', 'using', 'a', 'specific', 'type', 'of', 'classes', 'of', 'the', 'bazanski', 'lagrangian', 'such', 'type', 'of', 'paths', 'has', 'been', 'found', 'to', 'describe', 'the', 'problem', 'of', 'variable... | [-0.12766657496053838, 0.11364122829625808, -0.1448458762646749, 0.1064676336379422, -0.1365443424632152, -0.12726233308685236, -0.06331411423295437, 0.2839664719816854, -0.25323014360204893, -0.3615192140127404, 0.029386320896045273, -0.2361434391571273, -0.12473761016936523, 0.17288763885019648, -0.09482064651560852,... |
1,801.08397 | On the extraction of the boundary conditions and the boundary ports in
second-order field theories | In this paper we consider second-order field theories in a variational
setting. From the variational principle the Euler-Lagrange equations follow in
an unambiguous way, but it is well known that this is not true for the Cartan
form. This has also consequences on the derivation of the boundary conditions
when non tri... | math.OC math-ph math.DS math.MP | in this paper we consider secondorder field theories in a variational setting from the variational principle the eulerlagrange equations follow in an unambiguous way but it is well known that this is not true for the cartan form this has also consequences on the derivation of the boundary conditions when non trivial va... | [['in', 'this', 'paper', 'we', 'consider', 'secondorder', 'field', 'theories', 'in', 'a', 'variational', 'setting', 'from', 'the', 'variational', 'principle', 'the', 'eulerlagrange', 'equations', 'follow', 'in', 'an', 'unambiguous', 'way', 'but', 'it', 'is', 'well', 'known', 'that', 'this', 'is', 'not', 'true', 'for', ... | [-0.12011996891487797, 0.07222558630667208, -0.09985784385571606, 0.054600493247562554, -0.13179947195385466, -0.1314344063939643, 0.0026784812198457075, 0.3150309068223578, -0.2830441850510397, -0.27631096537515987, 0.12874308163645765, -0.2136761340079829, -0.16948492481242283, 0.18532685582067643, -0.107914427640935... |
1,801.08398 | Results on TOP physics from CMS | After the discovery of the top quark more than 20 years ago, top quark
production cross sections have been meticulously studied. The rich variety of
results from the LHC experiments are complemented with increasingly accurate
theoretical predictions of heavy quark production and decay. Measurements of
the top quark p... | hep-ex | after the discovery of the top quark more than 20 years ago top quark production cross sections have been meticulously studied the rich variety of results from the lhc experiments are complemented with increasingly accurate theoretical predictions of heavy quark production and decay measurements of the top quark produc... | [['after', 'the', 'discovery', 'of', 'the', 'top', 'quark', 'more', 'than', '20', 'years', 'ago', 'top', 'quark', 'production', 'cross', 'sections', 'have', 'been', 'meticulously', 'studied', 'the', 'rich', 'variety', 'of', 'results', 'from', 'the', 'lhc', 'experiments', 'are', 'complemented', 'with', 'increasingly', '... | [0.02090556826342122, 0.23260866663145735, -0.08756938579709045, 0.12285606788395069, -0.054705930386011584, -0.17230923341362384, 0.04898468838755748, 0.3096422277840561, -0.18757179809397023, -0.2865564659727609, 0.052866795194608254, -0.3642794350643867, 0.06803178049800597, 0.21896288532498775, 0.10012063136372458,... |
1,801.08399 | Optical frequency comb Faraday rotation spectroscopy | We demonstrate optical frequency comb Faraday rotation spectroscopy (OFC-FRS)
for broadband interference-free detection of paramagnetic species. The system
is based on a femtosecond doubly resonant optical parametric oscillator and a
fast-scanning Fourier transform spectrometer (FTS). The sample is placed in a
DC mag... | physics.optics | we demonstrate optical frequency comb faraday rotation spectroscopy ofcfrs for broadband interferencefree detection of paramagnetic species the system is based on a femtosecond doubly resonant optical parametric oscillator and a fastscanning fourier transform spectrometer fts the sample is placed in a dc magnetic field... | [['we', 'demonstrate', 'optical', 'frequency', 'comb', 'faraday', 'rotation', 'spectroscopy', 'ofcfrs', 'for', 'broadband', 'interferencefree', 'detection', 'of', 'paramagnetic', 'species', 'the', 'system', 'is', 'based', 'on', 'a', 'femtosecond', 'doubly', 'resonant', 'optical', 'parametric', 'oscillator', 'and', 'a',... | [-0.14349858672132046, 0.11874375868706231, -0.05605868707429075, -0.020390807750444967, -0.041941138011520926, -0.12435370626705654, 0.07339556494844146, 0.4901442782664039, -0.2464965838550147, -0.2864574127315173, 0.06705608195512221, -0.2593094003884104, -0.06671361050125464, 0.24391846999625486, -0.001102766904808... |
1,801.084 | Generation of semigroup for symmetric matrix Schr\"odinger operators in
$L^p$-spaces | In this paper we establish generation of analytic strongly continuous
semigroup in $L^p$--spaces for the symmetric matrix Schr\"odinger operator
$div(Q\nabla u)-Vu$, where, for every $x\in\mathbb{R}^d$, $V(x)=(v_{ij}(x))$ is
a semi-definite positive and symmetric matrix. The diffusion matrix $Q(\cdot)$
is supposed to... | math.AP | in this paper we establish generation of analytic strongly continuous semigroup in lpspaces for the symmetric matrix schrodinger operator divqnabla uvu where for every xinmathbbrd vxv_ijx is a semidefinite positive and symmetric matrix the diffusion matrix qcdot is supposed to be strongly elliptic and bounded and the p... | [['in', 'this', 'paper', 'we', 'establish', 'generation', 'of', 'analytic', 'strongly', 'continuous', 'semigroup', 'in', 'lpspaces', 'for', 'the', 'symmetric', 'matrix', 'schrodinger', 'operator', 'divqnabla', 'uvu', 'where', 'for', 'every', 'xinmathbbrd', 'vxv_ijx', 'is', 'a', 'semidefinite', 'positive', 'and', 'symme... | [-0.11881051391052704, 0.11996212875414075, -0.02022598271088844, 0.0714458868967609, -0.09168240395515706, -0.14902815425937826, -0.04263239830668846, 0.36436230707278644, -0.34698722861481435, -0.09073943100079443, 0.18667362134720228, -0.3155181586008632, -0.15710046334954147, 0.14654371456355986, -0.047572725875811... |
1,801.08401 | The SysCalc code: A tool to derive theoretical systematic uncertainties | Undisputedly, derivation of theoretical systematic uncertainties is an
inseparable ingredient of any robust analysis dealing with experimental data.
However, it is not uncommon, even for those analyses that use state of the art
methods and tools to suffer from insufficient statistics when it comes to the
simulated da... | hep-ph hep-ex physics.comp-ph | undisputedly derivation of theoretical systematic uncertainties is an inseparable ingredient of any robust analysis dealing with experimental data however it is not uncommon even for those analyses that use state of the art methods and tools to suffer from insufficient statistics when it comes to the simulated datasets... | [['undisputedly', 'derivation', 'of', 'theoretical', 'systematic', 'uncertainties', 'is', 'an', 'inseparable', 'ingredient', 'of', 'any', 'robust', 'analysis', 'dealing', 'with', 'experimental', 'data', 'however', 'it', 'is', 'not', 'uncommon', 'even', 'for', 'those', 'analyses', 'that', 'use', 'state', 'of', 'the', 'a... | [-0.055104135692714766, 0.0475125544568966, -0.08197912918238422, 0.12049449579349372, -0.07806334830269482, -0.08113062093943665, 0.06992701361074316, 0.3496661094987225, -0.25970657845303285, -0.34837947209150744, 0.12853045862501475, -0.26912958434088563, -0.0977910601309385, 0.24380583584600696, -0.0865764676389345... |
1,801.08402 | Dynamical System Analysis of a Five-Dimensional Cosmological Model | A five-dimensional cosmological model including a single perfect fluid is
studied in the framework of dynamical system analysis. All the critical points
of the system with their stability properties are listed and some
representative phase diagrams are explicitly shown. It is found that the
stabilization of the extra... | gr-qc astro-ph.CO | a fivedimensional cosmological model including a single perfect fluid is studied in the framework of dynamical system analysis all the critical points of the system with their stability properties are listed and some representative phase diagrams are explicitly shown it is found that the stabilization of the extra dime... | [['a', 'fivedimensional', 'cosmological', 'model', 'including', 'a', 'single', 'perfect', 'fluid', 'is', 'studied', 'in', 'the', 'framework', 'of', 'dynamical', 'system', 'analysis', 'all', 'the', 'critical', 'points', 'of', 'the', 'system', 'with', 'their', 'stability', 'properties', 'are', 'listed', 'and', 'some', 'r... | [-0.16106901460584905, 0.12807496673951957, -0.08563036312466686, 0.0709887868272665, -0.020243464833469067, -0.09717721417116779, -0.009665300762190403, 0.29740791910698694, -0.2433510449109147, -0.3202945908658134, 0.13333607219313318, -0.23316704453810036, -0.13259708508170998, 0.16801936907503862, 0.009887531901556... |
1,801.08403 | Al/Ti/Al phonon-mediated KIDs for UV-VIS light detection over large
areas | The development of wide-area cryogenic light detectors with baseline energy
resolution lower than 20 eV RMS is essential for next generation bolometric
experiments searching for rare interactions. Indeed the simultaneous readout of
the light and heat signals will enable background suppression through particle
identif... | physics.ins-det physics.app-ph | the development of widearea cryogenic light detectors with baseline energy resolution lower than 20 ev rms is essential for next generation bolometric experiments searching for rare interactions indeed the simultaneous readout of the light and heat signals will enable background suppression through particle identificat... | [['the', 'development', 'of', 'widearea', 'cryogenic', 'light', 'detectors', 'with', 'baseline', 'energy', 'resolution', 'lower', 'than', '20', 'ev', 'rms', 'is', 'essential', 'for', 'next', 'generation', 'bolometric', 'experiments', 'searching', 'for', 'rare', 'interactions', 'indeed', 'the', 'simultaneous', 'readout'... | [-0.11279383216859072, 0.126589233418167, -0.007464832387260221, 0.019575239407684627, -0.07241388839002408, -0.14931433645559225, 0.051785100164743976, 0.39937727979602333, -0.1639561536226501, -0.4068888780125912, 0.07054894350730015, -0.34918499440747375, -0.01647635505795611, 0.23160907908438552, 0.0159231404896085... |
1,801.08404 | Observation of ultrafast solid-density plasma dynamics using femtosecond
X-ray pulses from a free-electron laser | The complex physics of the interaction between short pulse high intensity
lasers and solids is so far hardly accessible by experiments. As a result of
missing experimental capabilities to probe the complex electron dynamics and
competing instabilities, this impedes the development of compact laser-based
next generati... | physics.plasm-ph | the complex physics of the interaction between short pulse high intensity lasers and solids is so far hardly accessible by experiments as a result of missing experimental capabilities to probe the complex electron dynamics and competing instabilities this impedes the development of compact laserbased next generation se... | [['the', 'complex', 'physics', 'of', 'the', 'interaction', 'between', 'short', 'pulse', 'high', 'intensity', 'lasers', 'and', 'solids', 'is', 'so', 'far', 'hardly', 'accessible', 'by', 'experiments', 'as', 'a', 'result', 'of', 'missing', 'experimental', 'capabilities', 'to', 'probe', 'the', 'complex', 'electron', 'dyna... | [-0.08832514159482821, 0.2544461324550056, -0.0858534240039379, 0.041228413315015006, -0.03897265944685234, -0.11577749339918984, 0.007002735854527627, 0.4796462177787677, -0.2643619410380707, -0.30492522308745856, 0.03921093926984024, -0.2561106206423466, -0.06604232169494106, 0.2522239628793109, 0.0395808980551244, 0... |
1,801.08405 | A smaller cover for closed unit curves | Forty years ago Schaer and Wetzel showed that a $\frac{1}{\pi}\times\frac
{1}{2\pi}\sqrt{\pi^{2}-4}$ rectangle, whose area is about $0.122\,74,$ is the
smallest rectangle that is a cover for the family of all closed unit arcs. More
recently F\"{u}redi and Wetzel showed that one corner of this rectangle can be
clipped... | cs.CG | forty years ago schaer and wetzel showed that a frac1pitimesfrac 12pisqrtpi24 rectangle whose area is about 012274 is the smallest rectangle that is a cover for the family of all closed unit arcs more recently furedi and wetzel showed that one corner of this rectangle can be clipped to form a pentagonal cover having ar... | [['forty', 'years', 'ago', 'schaer', 'and', 'wetzel', 'showed', 'that', 'a', 'frac1pitimesfrac', '12pisqrtpi24', 'rectangle', 'whose', 'area', 'is', 'about', '012274', 'is', 'the', 'smallest', 'rectangle', 'that', 'is', 'a', 'cover', 'for', 'the', 'family', 'of', 'all', 'closed', 'unit', 'arcs', 'more', 'recently', 'fu... | [-0.13220740319105817, 0.07645138289700164, -0.052637991416168976, 0.02325922374965306, -0.09129217877845339, -0.1257167807284822, 0.026229732279774754, 0.3845615590664935, -0.25554487489639444, -0.28384748096280593, 0.1550340506562745, -0.33168778277220246, -0.16237848409837943, 0.2320790598713892, -0.1363071088847565... |
1,801.08406 | C2MSNet: A Novel approach for single image haze removal | Degradation of image quality due to the presence of haze is a very common
phenomenon. Existing DehazeNet [3], MSCNN [11] tackled the drawbacks of hand
crafted haze relevant features. However, these methods have the problem of
color distortion in gloomy (poor illumination) environment. In this paper, a
cardinal (red, ... | cs.CV | degradation of image quality due to the presence of haze is a very common phenomenon existing dehazenet 3 mscnn 11 tackled the drawbacks of hand crafted haze relevant features however these methods have the problem of color distortion in gloomy poor illumination environment in this paper a cardinal red green and blue c... | [['degradation', 'of', 'image', 'quality', 'due', 'to', 'the', 'presence', 'of', 'haze', 'is', 'a', 'very', 'common', 'phenomenon', 'existing', 'dehazenet', '3', 'mscnn', '11', 'tackled', 'the', 'drawbacks', 'of', 'hand', 'crafted', 'haze', 'relevant', 'features', 'however', 'these', 'methods', 'have', 'the', 'problem'... | [-0.05679303607903421, -0.07166142741079966, -0.07905094145098701, 0.06739194029651116, -0.04349341193387772, -0.18388160965259887, -0.00731584565655794, 0.478141844732454, -0.24265621671329426, -0.3361463712353725, 0.09142557312152348, -0.28578125865315085, -0.19172675528679975, 0.14346129217592535, -0.175693474842410... |
1,801.08407 | Algebraic Geometric codes on minimal Hirzebruch surfaces | We define a linear code $C_\eta(\delta_T,\delta_X)$ by evaluating polynomials
of bidegree $(\delta_T,\delta_X)$ in the Cox ring on $\mathbb{F}_q$-rational
points of the Hirzebruch surface of parameter $\eta$ on the finite field
$\mathbb{F}_q$. We give explicit parameters of the code, notably using
Gr\"obner bases. Th... | cs.IT math.AC math.AG math.IT | we define a linear code c_etadelta_tdelta_x by evaluating polynomials of bidegree delta_tdelta_x in the cox ring on mathbbf_qrational points of the hirzebruch surface of parameter eta on the finite field mathbbf_q we give explicit parameters of the code notably using grobner bases the minimum distance provides an upper... | [['we', 'define', 'a', 'linear', 'code', 'c_etadelta_tdelta_x', 'by', 'evaluating', 'polynomials', 'of', 'bidegree', 'delta_tdelta_x', 'in', 'the', 'cox', 'ring', 'on', 'mathbbf_qrational', 'points', 'of', 'the', 'hirzebruch', 'surface', 'of', 'parameter', 'eta', 'on', 'the', 'finite', 'field', 'mathbbf_q', 'we', 'give... | [-0.26008008576196723, 0.022873592725430127, -0.1192504087325613, 0.04594016869811982, -0.03483546161108085, -0.14145151499017586, 0.09060210169705211, 0.24843821361218196, -0.2729425623280103, -0.2366528032561306, 0.04253599564277674, -0.24735262273184833, -0.11154290645948199, 0.2662351592672897, -0.0976415645086863,... |
1,801.08408 | Cyber-Induced Risk Modeling for Microprocessor-Based Relays in
Substations | Once critical substations are compromised, attack agents can coordinate among
their peers to plot for maximizing disruption using local control devices. For
defenders, it is critical to enumerate and identify all digital relays to
determine the systemic risks. Any combination of disruptive switching via the
compromis... | eess.SP | once critical substations are compromised attack agents can coordinate among their peers to plot for maximizing disruption using local control devices for defenders it is critical to enumerate and identify all digital relays to determine the systemic risks any combination of disruptive switching via the compromised rel... | [['once', 'critical', 'substations', 'are', 'compromised', 'attack', 'agents', 'can', 'coordinate', 'among', 'their', 'peers', 'to', 'plot', 'for', 'maximizing', 'disruption', 'using', 'local', 'control', 'devices', 'for', 'defenders', 'it', 'is', 'critical', 'to', 'enumerate', 'and', 'identify', 'all', 'digital', 'rel... | [-0.22586307407662098, 0.023529127563214212, -0.034194645342349214, 0.0451803993555526, -0.06800567372917932, -0.22507670919244357, 0.15069467964387862, 0.34476385634108786, -0.24300435012120086, -0.2985264332718308, 0.10804562177663261, -0.3008914169707391, -0.15664301231805705, 0.15964757957085596, -0.128096872814221... |
1,801.08409 | Computation of the State Bias and Initial States for Stochastic State
Space Systems in the General 2-D Roesser Model Form | Recently \cite{Ramos2017a} presented a subspace system identification
algorithm for 2-D purely stochastic state space models in the general Roesser
form. However, since the exact problem requires an oblique projection of
$Y_f^h$ projected onto $W_p^h$ along $\widehat{X}_f^{vh}$, where $W_p^h=
\begin{bmatrix}\widehat{... | math.NA cs.SY | recently citeramos2017a presented a subspace system identification algorithm for 2d purely stochastic state space models in the general roesser form however since the exact problem requires an oblique projection of y_fh projected onto w_ph along widehatx_fvh where w_ph beginbmatrixwidehatx_pvh y_ph endbmatrix this pres... | [['recently', 'citeramos2017a', 'presented', 'a', 'subspace', 'system', 'identification', 'algorithm', 'for', '2d', 'purely', 'stochastic', 'state', 'space', 'models', 'in', 'the', 'general', 'roesser', 'form', 'however', 'since', 'the', 'exact', 'problem', 'requires', 'an', 'oblique', 'projection', 'of', 'y_fh', 'proj... | [-0.10692228644904567, 0.07460467833308673, -0.062248088304725724, 0.03924511814626252, -0.06059459553372751, -0.1184213706292212, 0.032721384012185765, 0.3703568719100298, -0.2694512581407297, -0.27368943932261774, 0.13289022982438525, -0.24456458947189696, -0.1257743696602652, 0.17457839232960307, -0.0706868918016325... |
1,801.0841 | Relaxed Conditions for Secrecy in a Role-Based Specification | In this paper, we look at the property of secrecy through the growth of the
protocol. Intuitively, an increasing protocol preserves the secret. For that,
we need functions to estimate the security of messages. Here, we give relaxed
conditions on the functions and on the protocol and we prove that an increasing
protoc... | cs.CR | in this paper we look at the property of secrecy through the growth of the protocol intuitively an increasing protocol preserves the secret for that we need functions to estimate the security of messages here we give relaxed conditions on the functions and on the protocol and we prove that an increasing protocol is cor... | [['in', 'this', 'paper', 'we', 'look', 'at', 'the', 'property', 'of', 'secrecy', 'through', 'the', 'growth', 'of', 'the', 'protocol', 'intuitively', 'an', 'increasing', 'protocol', 'preserves', 'the', 'secret', 'for', 'that', 'we', 'need', 'functions', 'to', 'estimate', 'the', 'security', 'of', 'messages', 'here', 'we'... | [-0.17392373065804206, 0.07332353789538573, -0.1204236939564229, 0.046944203003058356, 0.004604369291060027, -0.18535586773225712, 0.10596220477831565, 0.4005950908620088, -0.27874792603746296, -0.238786184694618, 0.09599924617306521, -0.2557312755121125, -0.14992862095453938, 0.19569391263501038, -0.11389990992814539,... |
1,801.08411 | Global existence of solutions to 2-D Navier-Stokes flow with
non-decaying initial data in half-plane | We investigate the Navier-Stokes initial boundary value problem in the
half-plane $R^2_+$ with initial data $u_0 \in L^\infty(R^2_+)\cap J_0^2(R^2_+)$
or with non decaying initial data $u_0\in L^\infty(R^2_+) \cap J_0^p(R^2_+), p
> 2$ . We introduce a technique that allows to solve the two-dimesional
problem, further... | math.AP | we investigate the navierstokes initial boundary value problem in the halfplane r2_ with initial data u_0 in linftyr2_cap j_02r2_ or with non decaying initial data u_0in linftyr2_ cap j_0pr2_ p 2 we introduce a technique that allows to solve the twodimesional problem further but not least it can be also employed to obt... | [['we', 'investigate', 'the', 'navierstokes', 'initial', 'boundary', 'value', 'problem', 'in', 'the', 'halfplane', 'r2_', 'with', 'initial', 'data', 'u_0', 'in', 'linftyr2_cap', 'j_02r2_', 'or', 'with', 'non', 'decaying', 'initial', 'data', 'u_0in', 'linftyr2_', 'cap', 'j_0pr2_', 'p', '2', 'we', 'introduce', 'a', 'tech... | [-0.12715177169108452, 0.057631356738662966, -0.10880884081901361, 0.07232119880306224, -0.09752448988082404, -0.16434718130363357, -0.03690202997919793, 0.30318865004099077, -0.33414340391755104, -0.24819164038894492, 0.18959765350640131, -0.27473965696299274, -0.040618224784136854, 0.15541310143695833, -0.04265640544... |
1,801.08412 | Onset of fast "ideal" tearing in thin current sheets: dependence on the
equilibrium current profile | In this paper we study the scaling relations for the triggering of the fast,
or "ideal", tearing instability starting from equilibrium configurations
relevant to astrophysical as well as laboratory plasmas that differ from the
simple Harris current sheet configuration. We present the linear tearing
instability analys... | physics.plasm-ph astro-ph.SR physics.space-ph | in this paper we study the scaling relations for the triggering of the fast or ideal tearing instability starting from equilibrium configurations relevant to astrophysical as well as laboratory plasmas that differ from the simple harris current sheet configuration we present the linear tearing instability analysis for ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'scaling', 'relations', 'for', 'the', 'triggering', 'of', 'the', 'fast', 'or', 'ideal', 'tearing', 'instability', 'starting', 'from', 'equilibrium', 'configurations', 'relevant', 'to', 'astrophysical', 'as', 'well', 'as', 'laboratory', 'plasmas', 'that', 'differ', 'from', ... | [-0.16600648639229776, 0.179087343442282, -0.0367807869841768, 0.07058984041213989, -0.028679433160207487, -0.13970829863665682, 0.04472299560579951, 0.260078460742917, -0.22828883250159296, -0.28475944082619564, 0.096333826885728, -0.24496002506577608, -0.07444405439874213, 0.2135056896375097, 0.042765951503745535, 0.... |
1,801.08413 | Mean-field risk sensitive control and zero-sum games for Markov chains | We establish existence of controlled Markov chain of mean-field type with
unbounded jump intensities by means of a fixed point argument using the
Wasserstein distance. Using a Markov chain entropic backward SDE approach, we
further suggest conditions for existence of an optimal control and a
saddle-point for respecti... | math.PR math.OC | we establish existence of controlled markov chain of meanfield type with unbounded jump intensities by means of a fixed point argument using the wasserstein distance using a markov chain entropic backward sde approach we further suggest conditions for existence of an optimal control and a saddlepoint for respectively a... | [['we', 'establish', 'existence', 'of', 'controlled', 'markov', 'chain', 'of', 'meanfield', 'type', 'with', 'unbounded', 'jump', 'intensities', 'by', 'means', 'of', 'a', 'fixed', 'point', 'argument', 'using', 'the', 'wasserstein', 'distance', 'using', 'a', 'markov', 'chain', 'entropic', 'backward', 'sde', 'approach', '... | [-0.1273738751174488, 0.06772948584649174, -0.11419953933128944, 0.1396574850767278, -0.04981942954831398, -0.20191811404119317, 0.14724656804196107, 0.39031612666753623, -0.35014152088417455, -0.21548764997949968, 0.11944985032941287, -0.24362682810483072, -0.12740780489089398, 0.15192566271871327, -0.0805527610990863... |
1,801.08414 | First-order differential equations for a particle with spin $S = 1$ | A system of first-order differential equations for a particle with nonzero
mass and spin $S = 1$ is constructed. As distinct from the Proca-Duffin-Kemmer
(PDK) equations, the system has the form of the dynamical equation
$i\hbar\partial_t\hat{\Psi}=\hat{\mathrm{H}}\hat{\Psi}$ (with constraints) with
a Hamiltonian lin... | quant-ph | a system of firstorder differential equations for a particle with nonzero mass and spin s 1 is constructed as distinct from the procaduffinkemmer pdk equations the system has the form of the dynamical equation ihbarpartial_thatpsihatmathrmhhatpsi with constraints with a hamiltonian linear in momentum the sixcomponent w... | [['a', 'system', 'of', 'firstorder', 'differential', 'equations', 'for', 'a', 'particle', 'with', 'nonzero', 'mass', 'and', 'spin', 's', '1', 'is', 'constructed', 'as', 'distinct', 'from', 'the', 'procaduffinkemmer', 'pdk', 'equations', 'the', 'system', 'has', 'the', 'form', 'of', 'the', 'dynamical', 'equation', 'ihbar... | [-0.1861608316978583, 0.13261488557148438, -0.09854535715511212, -0.012933930788690654, -0.04155137514552245, -0.1295523015370306, -0.06248683386410658, 0.21007306868067155, -0.24565434652165724, -0.29522032166043155, 0.04517254429296232, -0.32687276154756545, -0.11422291561029851, 0.14597744450438768, 0.05372237386898... |
1,801.08415 | Convective evaporation of vertical films | Motivated by the evaporation of soap films, which has a significant effect on
their lifetime, we performed an experimental study on the evaporation of
vertical surfaces with model systems based on hydrogels. From the analogy
between heat and mass transfer, we adopt a model describing the natural
convection in the gas... | cond-mat.soft physics.flu-dyn | motivated by the evaporation of soap films which has a significant effect on their lifetime we performed an experimental study on the evaporation of vertical surfaces with model systems based on hydrogels from the analogy between heat and mass transfer we adopt a model describing the natural convection in the gas phase... | [['motivated', 'by', 'the', 'evaporation', 'of', 'soap', 'films', 'which', 'has', 'a', 'significant', 'effect', 'on', 'their', 'lifetime', 'we', 'performed', 'an', 'experimental', 'study', 'on', 'the', 'evaporation', 'of', 'vertical', 'surfaces', 'with', 'model', 'systems', 'based', 'on', 'hydrogels', 'from', 'the', 'a... | [-0.08372461508261039, 0.1450298853862332, -0.07646109678596258, 0.03122039275150746, 0.007789629263803363, -0.07222987891361117, 0.06397375377081335, 0.3381820659674704, -0.21761909839510918, -0.35744392141699793, 0.08838187171984464, -0.29978115573339165, -0.12131659907102585, 0.2090617133472115, -0.05849163164012134... |
1,801.08416 | Differential symbolic entropy in nonlinear dynamics complexity analysis | Differential symbolic entropy, a measure for nonlinear dynamics complexity,
is proposed in our contribution. With flexible controlling parameter, the
chaotic deterministic measure takes advantage of local nonlinear dynamical
information among three adjacent elements to extract nonlinear complexity. In
nonlinear compl... | physics.data-an | differential symbolic entropy a measure for nonlinear dynamics complexity is proposed in our contribution with flexible controlling parameter the chaotic deterministic measure takes advantage of local nonlinear dynamical information among three adjacent elements to extract nonlinear complexity in nonlinear complexity d... | [['differential', 'symbolic', 'entropy', 'a', 'measure', 'for', 'nonlinear', 'dynamics', 'complexity', 'is', 'proposed', 'in', 'our', 'contribution', 'with', 'flexible', 'controlling', 'parameter', 'the', 'chaotic', 'deterministic', 'measure', 'takes', 'advantage', 'of', 'local', 'nonlinear', 'dynamical', 'information'... | [-0.10430201682706934, 0.09116729527267492, -0.06493089073198612, 0.08885894769997295, -0.10649357050824076, -0.19659166202842215, 0.007120866784582665, 0.29780810083081916, -0.30245002861649023, -0.22059916031074278, 0.10777631195508805, -0.30461371294570283, -0.21368745171270376, 0.25054163108805694, -0.1555570927309... |
1,801.08417 | Electromagnetic form factors of $\Lambda_c$ in the Bethe-Salpeter
equation approach | We study the electromagnetic form factors (EMFFs) of $\Lambda_c$ and the
quark and diquark current contributes to the EMFFs of $\Lambda_c$ in the
space-like (SL) region in the Bethe-Salpeter equation approach. In this
picture, the heavy baryon $\Lambda_c $ is regarded as composed of a heavy quark
and a scalar diquark... | hep-ph | we study the electromagnetic form factors emffs of lambda_c and the quark and diquark current contributes to the emffs of lambda_c in the spacelike sl region in the bethesalpeter equation approach in this picture the heavy baryon lambda_c is regarded as composed of a heavy quark and a scalar diquark we find that for di... | [['we', 'study', 'the', 'electromagnetic', 'form', 'factors', 'emffs', 'of', 'lambda_c', 'and', 'the', 'quark', 'and', 'diquark', 'current', 'contributes', 'to', 'the', 'emffs', 'of', 'lambda_c', 'in', 'the', 'spacelike', 'sl', 'region', 'in', 'the', 'bethesalpeter', 'equation', 'approach', 'in', 'this', 'picture', 'th... | [-0.10432512824237347, 0.2462452130462043, -0.08789365892857313, 0.08652471866738051, -0.04031659854575992, -0.10392315995460376, 0.05330753389745951, 0.3011935029774904, -0.18750230979919433, -0.23456918421387674, -0.08914930002298206, -0.3373614434301853, 0.02200560802221298, 0.0805860303407535, 0.10775692837475799, ... |
1,801.08418 | Unexpected cyclic behavior in cosmic ray protons observed by PAMELA at 1
AU | Protons detected by the PAMELA experiment in the period 2006-2014 have been
analyzed in the energy range between 0.40-50 GV to explore possible
periodicities besides the well known solar undecennial modulation. An
unexpected clear and regular feature has been found at rigidities below 15 GV,
with a quasi-periodicity ... | physics.space-ph astro-ph.EP astro-ph.SR | protons detected by the pamela experiment in the period 20062014 have been analyzed in the energy range between 04050 gv to explore possible periodicities besides the well known solar undecennial modulation an unexpected clear and regular feature has been found at rigidities below 15 gv with a quasiperiodicity of sim45... | [['protons', 'detected', 'by', 'the', 'pamela', 'experiment', 'in', 'the', 'period', '20062014', 'have', 'been', 'analyzed', 'in', 'the', 'energy', 'range', 'between', '04050', 'gv', 'to', 'explore', 'possible', 'periodicities', 'besides', 'the', 'well', 'known', 'solar', 'undecennial', 'modulation', 'an', 'unexpected'... | [-0.1206667461480141, 0.20490243196085925, -0.07222274042644793, 0.141965175125568, -0.08793082181364298, -0.11703165513145822, 0.03132021941498599, 0.39885726201729005, -0.23793355805967373, -0.3936308557167649, 0.027693201990173708, -0.27611689685462887, -0.07718074338679964, 0.22064537108367818, -0.04980490843511440... |
1,801.08419 | Analysis of the triply-charmed pentaquark states with QCD sum rules | In this article, we construct the scalar-diquark-scalar-diquark-antiquark
type current to study the ground state triply charmed pentaquark states with
the QCD sum rules. We separate the contributions of the negative-parity and
positive parity triply charmed pentaquark states explicitly, and take the
energy scale form... | hep-ph | in this article we construct the scalardiquarkscalardiquarkantiquark type current to study the ground state triply charmed pentaquark states with the qcd sum rules we separate the contributions of the negativeparity and positive parity triply charmed pentaquark states explicitly and take the energy scale formula musqrt... | [['in', 'this', 'article', 'we', 'construct', 'the', 'scalardiquarkscalardiquarkantiquark', 'type', 'current', 'to', 'study', 'the', 'ground', 'state', 'triply', 'charmed', 'pentaquark', 'states', 'with', 'the', 'qcd', 'sum', 'rules', 'we', 'separate', 'the', 'contributions', 'of', 'the', 'negativeparity', 'and', 'posi... | [-0.12022785172946211, 0.21225826168243866, -0.08193287106932721, 0.18499850129971848, -0.0591684353362391, -0.09672529524043742, 0.12273766143598418, 0.30367325732241507, -0.21539594384207242, -0.24344098711372825, 0.013939662070512988, -0.34165533606057474, 0.010252876153242762, 0.015418300648098406, 0.10676400101595... |
1,801.0842 | Numerical modeling of laser-driven ion acceleration from near-critical
gas targets | In the past two decades, laser-accelerated ion sources and their applications
have been intensely researched. Recently, it has been shown through experiments
that proton beams with characteristics comparable to those obtained with solid
targets can be obtained from gaseous targets. By means of Particle-In-Cell
simula... | physics.plasm-ph | in the past two decades laseraccelerated ion sources and their applications have been intensely researched recently it has been shown through experiments that proton beams with characteristics comparable to those obtained with solid targets can be obtained from gaseous targets by means of particleincell simulations thi... | [['in', 'the', 'past', 'two', 'decades', 'laseraccelerated', 'ion', 'sources', 'and', 'their', 'applications', 'have', 'been', 'intensely', 'researched', 'recently', 'it', 'has', 'been', 'shown', 'through', 'experiments', 'that', 'proton', 'beams', 'with', 'characteristics', 'comparable', 'to', 'those', 'obtained', 'wi... | [-0.04374888632377778, 0.18328614620121533, -0.10339417680089663, 0.04240643050737943, 0.01993516669058659, -0.08831559841504584, -0.02327522700175819, 0.4591086671694996, -0.2041042163595924, -0.33879181411205317, 0.037637879574253394, -0.32146990921084334, 0.0029179796532500446, 0.20696140835281668, 0.025393158754729... |
1,801.08421 | Differential proteomics highlights macrophage-specific responses to
amorphous silica nanoparticles | The technological and economic benefits of engineered nanomaterials may be
offset by their adverse effects on living organisms. One of the highly produced
nanomaterials under such scrutiny is amorphous silica nanoparticles, which are
known to have an appreciable, although reversible, inflammatory potential. This
is d... | q-bio.GN | the technological and economic benefits of engineered nanomaterials may be offset by their adverse effects on living organisms one of the highly produced nanomaterials under such scrutiny is amorphous silica nanoparticles which are known to have an appreciable although reversible inflammatory potential this is due to t... | [['the', 'technological', 'and', 'economic', 'benefits', 'of', 'engineered', 'nanomaterials', 'may', 'be', 'offset', 'by', 'their', 'adverse', 'effects', 'on', 'living', 'organisms', 'one', 'of', 'the', 'highly', 'produced', 'nanomaterials', 'under', 'such', 'scrutiny', 'is', 'amorphous', 'silica', 'nanoparticles', 'wh... | [-0.049778237712084, 0.188748806985553, -0.012084533085637703, 0.023755399096422124, -0.044649989023327646, -0.15428085243840498, 0.09466364752095216, 0.42760111657028066, -0.23176907846227107, -0.26639786912923363, 0.07369600565360132, -0.2790559633981391, -0.22519201212619408, 0.1552760476784542, -0.11776158793846418... |
1,801.08422 | Multi-peak semiclassical bound states for Fractional Schr\"{o}dinger
Equations with fast decaying potentials | We study the following fractional Schr\"{o}dinger equation
\begin{equation*}\label{eq0.1} \varepsilon^{2s}(-\Delta)^s u + V(x)u = f(u),
\,\,x\in\mathbb{R}^N, \end{equation*}
where $s\in(0,1)$. Under some conditions on $f(u)$, we show that the problem
has a family of solutions concentrating at any finite given local... | math.AP | we study the following fractional schrodinger equation beginequationlabeleq01 varepsilon2sdeltas u vxu fu xinmathbbrn endequation where sin01 under some conditions on fu we show that the problem has a family of solutions concentrating at any finite given local minima of v provided that vin crn0infty all decay rates of ... | [['we', 'study', 'the', 'following', 'fractional', 'schrodinger', 'equation', 'beginequationlabeleq01', 'varepsilon2sdeltas', 'u', 'vxu', 'fu', 'xinmathbbrn', 'endequation', 'where', 'sin01', 'under', 'some', 'conditions', 'on', 'fu', 'we', 'show', 'that', 'the', 'problem', 'has', 'a', 'family', 'of', 'solutions', 'con... | [-0.16459208832765443, 0.02935877087126885, -0.029160215118012967, 0.016883413299607734, -0.08347599605719248, -0.17840315205089394, -0.00874637980790188, 0.3628567000762338, -0.30548453251166, -0.20769073917929615, 0.10602024960154224, -0.3696563101684054, -0.1301135758935873, 0.1816747576996152, -0.04699415595137647,... |
1,801.08423 | Average radio spectral energy distribution of highly star-forming
galaxies | The infrared-radio correlation (IRRC) offers a way to assess star formation
from radio emission. Multiple studies found the IRRC to decrease with
increasing redshift. This may in part be due to the lack of knowledge about the
possible radio spectral energy distributions (SEDs) of star-forming galaxies.
We constrain t... | astro-ph.GA | the infraredradio correlation irrc offers a way to assess star formation from radio emission multiple studies found the irrc to decrease with increasing redshift this may in part be due to the lack of knowledge about the possible radio spectral energy distributions seds of starforming galaxies we constrain the radio se... | [['the', 'infraredradio', 'correlation', 'irrc', 'offers', 'a', 'way', 'to', 'assess', 'star', 'formation', 'from', 'radio', 'emission', 'multiple', 'studies', 'found', 'the', 'irrc', 'to', 'decrease', 'with', 'increasing', 'redshift', 'this', 'may', 'in', 'part', 'be', 'due', 'to', 'the', 'lack', 'of', 'knowledge', 'a... | [-0.020352665564295516, 0.04726409213964952, -0.1222746038163053, 0.11678628698547384, -0.149939401469666, -0.04168489492679043, 0.08040996981478894, 0.4755759975636628, -0.13645052359050222, -0.35425817119930664, 0.02501458931738622, -0.28309088486677675, -0.026408993625585964, 0.1834075218857155, -0.03111713100745996... |
1,801.08424 | Coronal Elemental Abundances in Solar Emerging Flux Regions | The chemical composition of solar and stellar atmospheres differs from that
of their photospheres. Abundances of elements with low first ionization
potential (FIP) are enhanced in the corona relative to high FIP elements with
respect to the photosphere. This is known as the FIP effect and it is important
for understa... | astro-ph.SR | the chemical composition of solar and stellar atmospheres differs from that of their photospheres abundances of elements with low first ionization potential fip are enhanced in the corona relative to high fip elements with respect to the photosphere this is known as the fip effect and it is important for understanding ... | [['the', 'chemical', 'composition', 'of', 'solar', 'and', 'stellar', 'atmospheres', 'differs', 'from', 'that', 'of', 'their', 'photospheres', 'abundances', 'of', 'elements', 'with', 'low', 'first', 'ionization', 'potential', 'fip', 'are', 'enhanced', 'in', 'the', 'corona', 'relative', 'to', 'high', 'fip', 'elements', '... | [-0.05881695647646363, 0.24849576877182006, 0.010881117735975533, 0.09208842812804505, -0.03543477945606269, -0.023257012696315846, 0.03372545039192552, 0.3998417635891764, -0.21306919897241253, -0.3736980022588146, 0.05623992359642649, -0.2681167898677467, -0.054760171016234725, 0.2160192585905038, -0.0347349628151971... |
1,801.08425 | On Sidorenko's conjecture for determinants and Gaussian Markov random
fields | We study a class of determinant inequalities that are closely related to
Sidorenko's famous conjecture (Also conjectured by Erd\H os and Simonovits in a
different form). Our main result can also be interpreted as an entropy
inequality for Gaussian Markov random fields (GMRF). We call a GMRF on a finite
graph $G$ homo... | math.CO | we study a class of determinant inequalities that are closely related to sidorenkos famous conjecture also conjectured by erdh os and simonovits in a different form our main result can also be interpreted as an entropy inequality for gaussian markov random fields gmrf we call a gmrf on a finite graph g homogeneous if t... | [['we', 'study', 'a', 'class', 'of', 'determinant', 'inequalities', 'that', 'are', 'closely', 'related', 'to', 'sidorenkos', 'famous', 'conjecture', 'also', 'conjectured', 'by', 'erdh', 'os', 'and', 'simonovits', 'in', 'a', 'different', 'form', 'our', 'main', 'result', 'can', 'also', 'be', 'interpreted', 'as', 'an', 'e... | [-0.14018029232509435, 0.13592107868617556, -0.09092693814765274, 0.08825588405442734, -0.048761722908044855, -0.14257865804247558, 0.025627183761292447, 0.3626450750728448, -0.26880804674699904, -0.27271848030388357, 0.09899561937122295, -0.30490930162680646, -0.17065672860480846, 0.1656579251649479, -0.08619783736610... |
1,801.08426 | Synthetic spin-orbit coupling and topological polaritons in
Janeys-Cummings lattices | The interaction between a photon and a qubit in the Janeys-Cummings (JC)
model generates a kind of quasiparticle called polariton. While they are widely
used in quantum optics, difficulties in engineering controllable coupling of
them severely limit their applications to simulate spinful quantum systems.
Here we show... | quant-ph cond-mat.mes-hall | the interaction between a photon and a qubit in the janeyscummings jc model generates a kind of quasiparticle called polariton while they are widely used in quantum optics difficulties in engineering controllable coupling of them severely limit their applications to simulate spinful quantum systems here we show that in... | [['the', 'interaction', 'between', 'a', 'photon', 'and', 'a', 'qubit', 'in', 'the', 'janeyscummings', 'jc', 'model', 'generates', 'a', 'kind', 'of', 'quasiparticle', 'called', 'polariton', 'while', 'they', 'are', 'widely', 'used', 'in', 'quantum', 'optics', 'difficulties', 'in', 'engineering', 'controllable', 'coupling... | [-0.2107614483635025, 0.24262766084182888, -0.031345377153859884, 0.0052176391275934675, -0.06795595377368271, -0.24594404345634516, 0.061926919696532266, 0.39393035955628547, -0.23581626914471152, -0.28357285006272376, -0.010096882638107572, -0.2549330990702387, -0.16200577507347422, 0.25269339182266287, 0.01198218505... |
1,801.08427 | Search for dark matter in events with energetic, hadronically decaying
top quarks and missing transverse momentum at $\sqrt{s}=$ 13 TeV | A search for dark matter is conducted in events with large missing transverse
momentum and a hadronically decaying, Lorentz-boosted top quark. This study is
performed using proton-proton collisions at a center-of-mass energy of 13 TeV,
in data recorded by the CMS detector in 2016 at the LHC, corresponding to an
integ... | hep-ex | a search for dark matter is conducted in events with large missing transverse momentum and a hadronically decaying lorentzboosted top quark this study is performed using protonproton collisions at a centerofmass energy of 13 tev in data recorded by the cms detector in 2016 at the lhc corresponding to an integrated lumi... | [['a', 'search', 'for', 'dark', 'matter', 'is', 'conducted', 'in', 'events', 'with', 'large', 'missing', 'transverse', 'momentum', 'and', 'a', 'hadronically', 'decaying', 'lorentzboosted', 'top', 'quark', 'this', 'study', 'is', 'performed', 'using', 'protonproton', 'collisions', 'at', 'a', 'centerofmass', 'energy', 'of... | [-0.07426517873421817, 0.28689912721569677, -0.08077384594161018, 0.20320569506607788, -0.06052365509022809, -0.14781136515860757, 0.0324811142578974, 0.30539718088636425, -0.15806938810159027, -0.4084332258452052, -0.02326243981089512, -0.3447248175234338, 0.15031284456756425, 0.13406618389324, 0.12145655379159215, 0.... |
1,801.08428 | Discrete projective minimal surfaces | We propose a natural discretisation scheme for classical projective minimal
surfaces. We follow the classical geometric characterisation and classification
of projective minimal surfaces and introduce at each step canonical discrete
models of the associated geometric notions and objects. Thus, we introduce
discrete a... | math.DG | we propose a natural discretisation scheme for classical projective minimal surfaces we follow the classical geometric characterisation and classification of projective minimal surfaces and introduce at each step canonical discrete models of the associated geometric notions and objects thus we introduce discrete analog... | [['we', 'propose', 'a', 'natural', 'discretisation', 'scheme', 'for', 'classical', 'projective', 'minimal', 'surfaces', 'we', 'follow', 'the', 'classical', 'geometric', 'characterisation', 'and', 'classification', 'of', 'projective', 'minimal', 'surfaces', 'and', 'introduce', 'at', 'each', 'step', 'canonical', 'discret... | [-0.12787246835564184, 0.08160344192560358, -0.11370870630762124, 0.08577868180161223, -0.1003548650732363, -0.15126122096850675, 0.04162355073160452, 0.34743739272210195, -0.2961461652476499, -0.24354064352612229, 0.10353606042732048, -0.20660476143313375, -0.16515730198552, 0.18730712969703203, -0.17140336902663508, ... |
1,801.08429 | Moderate deviations for stochastic models of two-dimensional second
grade fluids driven by L'evy noise | In this paper, we establish a moderate deviation principle for stochastic
models of two-dimensional second grade fluids driven by L\'evy noise. We will
adopt the weak convergence approach. Because of the appearance of jumps, this
result is significantly different from that in Gaussian case.
| math.PR | in this paper we establish a moderate deviation principle for stochastic models of twodimensional second grade fluids driven by levy noise we will adopt the weak convergence approach because of the appearance of jumps this result is significantly different from that in gaussian case | [['in', 'this', 'paper', 'we', 'establish', 'a', 'moderate', 'deviation', 'principle', 'for', 'stochastic', 'models', 'of', 'twodimensional', 'second', 'grade', 'fluids', 'driven', 'by', 'levy', 'noise', 'we', 'will', 'adopt', 'the', 'weak', 'convergence', 'approach', 'because', 'of', 'the', 'appearance', 'of', 'jumps'... | [-0.07635113872079687, 0.1170124920212071, -0.08325379892904618, 0.05725447928522375, -0.018082549435679208, -0.14020806583787568, 0.04226024531685239, 0.32158127903345635, -0.3024283265694976, -0.25803553442132066, 0.08098564271031963, -0.22005795010111548, -0.19461768984117292, 0.1739435189572925, -0.1394652214366942... |
1,801.0843 | An example of the geometry of a 5th-order ODE: the metric on the space
of conics in ${\mathbb{CP}}^2$ | As an application of the method of [4], we find the metric and connection on
the space of conics in $\mathbb{CP}^2$ determined as the solution space of the
ODE eqn(1). These calculations underpin the twistor construction of the Radon
transform on conics in $\mathbb{CP}^2$ described in [5]. Two further examples
of the... | math.DG | as an application of the method of 4 we find the metric and connection on the space of conics in mathbbcp2 determined as the solution space of the ode eqn1 these calculations underpin the twistor construction of the radon transform on conics in mathbbcp2 described in 5 two further examples of the method are provided | [['as', 'an', 'application', 'of', 'the', 'method', 'of', '4', 'we', 'find', 'the', 'metric', 'and', 'connection', 'on', 'the', 'space', 'of', 'conics', 'in', 'mathbbcp2', 'determined', 'as', 'the', 'solution', 'space', 'of', 'the', 'ode', 'eqn1', 'these', 'calculations', 'underpin', 'the', 'twistor', 'construction', '... | [-0.10918129232056716, 0.016334246316142123, -0.06604921096866881, 0.08850743104186323, -0.010694864262067885, -0.04036735020646894, 0.011676511537559607, 0.3648695998514692, -0.25697156809339367, -0.2798260925337672, 0.14010553770155335, -0.29742128909048104, -0.22136530517255543, 0.2525301514779804, -0.07210204348451... |
1,801.08431 | Mag2Pol: A program for the analysis of spherical neutron polarimetry,
flipping ratio and integrated intensity data | Mag2Pol is a graphical user interface program which is devoted to the
analysis of data from polarized neutron diffractometers with spherical
polarization analysis. Nuclear and magnetic structure models can be introduced
using space group symbols and individual symmetry operators, respectively, and
viewed in an OpenGL... | cond-mat.str-el | mag2pol is a graphical user interface program which is devoted to the analysis of data from polarized neutron diffractometers with spherical polarization analysis nuclear and magnetic structure models can be introduced using space group symbols and individual symmetry operators respectively and viewed in an opengl widg... | [['mag2pol', 'is', 'a', 'graphical', 'user', 'interface', 'program', 'which', 'is', 'devoted', 'to', 'the', 'analysis', 'of', 'data', 'from', 'polarized', 'neutron', 'diffractometers', 'with', 'spherical', 'polarization', 'analysis', 'nuclear', 'and', 'magnetic', 'structure', 'models', 'can', 'be', 'introduced', 'using... | [-0.10323137716456715, 0.10368844499067303, -0.09029363758995064, 0.0690901719183395, -0.09390721095426541, -0.08170208381156303, 0.015860188780685087, 0.42978755509746924, -0.2936189674739061, -0.3481625966095765, 0.08947106833054153, -0.2576454779598862, -0.06130629449783425, 0.17243788820092698, 0.033767251044212444... |
1,801.08432 | BIGSTICK: A flexible configuration-interaction shell-model code (updated) | We present BIGSTICK, a flexible configuration-interaction open-source shell-model code for the many-fermion problem. Written mostly in Fortran 90 with some later extensions, BIGSTICK utilizes a factorized on-the-fly algorithm for computing many-body matrix elements, and has both MPI (distributed memory) and OpenMP (sha... | physics.comp-ph nucl-th | we present bigstick a flexible configurationinteraction opensource shellmodel code for the manyfermion problem written mostly in fortran 90 with some later extensions bigstick utilizes a factorized onthefly algorithm for computing manybody matrix elements and has both mpi distributed memory and openmp shared memory par... | [['we', 'present', 'bigstick', 'a', 'flexible', 'configurationinteraction', 'opensource', 'shellmodel', 'code', 'for', 'the', 'manyfermion', 'problem', 'written', 'mostly', 'in', 'fortran', '90', 'with', 'some', 'later', 'extensions', 'bigstick', 'utilizes', 'a', 'factorized', 'onthefly', 'algorithm', 'for', 'computing... | [-0.08809310928691269, 0.08113582741977397, -0.07942999881641122, 0.09671358599131587, -0.08035176991990473, -0.1865002467586636, 0.03612060702928319, 0.4073103315043604, -0.2608628080165434, -0.3565535417803359, 0.049328326124118686, -0.2607659635917715, -0.05998925914953849, 0.14964383940223785, 0.034176952625829274,... |
1,801.08433 | The $(\mathfrak{gl}_m,\mathfrak{gl}_n$) duality in the quantum toroidal
setting | On a Fock space constructed from $mn$ free bosons and lattice ${\Bbb
{Z}}^{mn}$, we give a level $n$ action of the quantum toroidal algebra
$\mathscr {E}_m$ associated to $\mathfrak{gl}_m$, together with a level $m$
action of the quantum toroidal algebra ${\mathscr E}_n$ associated to
${\mathfrak {gl}}_n$. We prove t... | math.QA | on a fock space constructed from mn free bosons and lattice bbb zmn we give a level n action of the quantum toroidal algebra mathscr e_m associated to mathfrakgl_m together with a level m action of the quantum toroidal algebra mathscr e_n associated to mathfrak gl_n we prove that the mathscr e_m transfer matrices commu... | [['on', 'a', 'fock', 'space', 'constructed', 'from', 'mn', 'free', 'bosons', 'and', 'lattice', 'bbb', 'zmn', 'we', 'give', 'a', 'level', 'n', 'action', 'of', 'the', 'quantum', 'toroidal', 'algebra', 'mathscr', 'e_m', 'associated', 'to', 'mathfrakgl_m', 'together', 'with', 'a', 'level', 'm', 'action', 'of', 'the', 'quan... | [-0.21297202240536683, 0.21022231107488198, 0.025463276021460545, 0.0408654308863985, -0.0273506839189734, -0.1567704159168721, -0.034918262755303686, 0.3674343617549583, -0.3442464585958132, -0.16667861237065562, 0.0032798830183473097, -0.2681844526790638, -0.06807155015099961, 0.1347242541743248, -0.09295855893461562... |
1,801.08434 | Pauli-Zeldovich cancellation of the vacuum energy divergences, auxiliary
fields and supersymmetry | We have considered the Pauli-Zeldovich mechanism for the cancellation of the
ultraviolet divergences in vacuum energy. This mechanism arises because bosons
and fermions give contributions of the opposite signs. In contrast with the
preceding papers devoted to this topic wherein mainly free fields were studied,
here w... | hep-th gr-qc | we have considered the paulizeldovich mechanism for the cancellation of the ultraviolet divergences in vacuum energy this mechanism arises because bosons and fermions give contributions of the opposite signs in contrast with the preceding papers devoted to this topic wherein mainly free fields were studied here we have... | [['we', 'have', 'considered', 'the', 'paulizeldovich', 'mechanism', 'for', 'the', 'cancellation', 'of', 'the', 'ultraviolet', 'divergences', 'in', 'vacuum', 'energy', 'this', 'mechanism', 'arises', 'because', 'bosons', 'and', 'fermions', 'give', 'contributions', 'of', 'the', 'opposite', 'signs', 'in', 'contrast', 'with... | [-0.128617472904311, 0.23106817503205754, -0.07057972619209481, 0.09135411849869839, -0.035238900110760536, -0.12839783169329166, -0.008013434254363265, 0.3688146604902365, -0.20084386981431057, -0.3135348552710969, 0.05704808112667789, -0.30247365054674447, -0.09528995361919938, 0.08309380525977096, 0.0060793073710308... |
1,801.08435 | Fermionic properties of two interacting bosons in a two-dimensional
harmonic trap | The system of two interacting bosons in a two-dimensional harmonic trap is
compared with the system consisting of two noninteracting fermions in the same
potential. In particular, we discuss how the properties of the ground state of
the system, e.g., the different contributions to the total energy, change as we
vary ... | cond-mat.quant-gas | the system of two interacting bosons in a twodimensional harmonic trap is compared with the system consisting of two noninteracting fermions in the same potential in particular we discuss how the properties of the ground state of the system eg the different contributions to the total energy change as we vary both the s... | [['the', 'system', 'of', 'two', 'interacting', 'bosons', 'in', 'a', 'twodimensional', 'harmonic', 'trap', 'is', 'compared', 'with', 'the', 'system', 'consisting', 'of', 'two', 'noninteracting', 'fermions', 'in', 'the', 'same', 'potential', 'in', 'particular', 'we', 'discuss', 'how', 'the', 'properties', 'of', 'the', 'g... | [-0.17853145784338134, 0.16749112950009123, -0.05173624099239054, 0.0755119794847131, 0.061790099831461144, -0.11076351035943757, 0.010717743667807892, 0.3338716811072217, -0.23697374453836115, -0.28363428363426973, 0.012765477528714025, -0.3413053596133951, -0.11551005212440543, 0.1473900925531222, 0.07424114651665309... |
1,801.08436 | Dual Free Adaptive Minibatch SDCA for Empirical Risk Minimization | In this paper we develop an adaptive dual free Stochastic Dual Coordinate
Ascent (adfSDCA) algorithm for regularized empirical risk minimization
problems. This is motivated by the recent work on dual free SDCA of
Shalev-Shwartz (2016). The novelty of our approach is that the coordinates to
update at each iteration ar... | math.OC | in this paper we develop an adaptive dual free stochastic dual coordinate ascent adfsdca algorithm for regularized empirical risk minimization problems this is motivated by the recent work on dual free sdca of shalevshwartz 2016 the novelty of our approach is that the coordinates to update at each iteration are selecte... | [['in', 'this', 'paper', 'we', 'develop', 'an', 'adaptive', 'dual', 'free', 'stochastic', 'dual', 'coordinate', 'ascent', 'adfsdca', 'algorithm', 'for', 'regularized', 'empirical', 'risk', 'minimization', 'problems', 'this', 'is', 'motivated', 'by', 'the', 'recent', 'work', 'on', 'dual', 'free', 'sdca', 'of', 'shalevsh... | [-0.06223731173096693, 0.018998377157523057, -0.10731687015665273, 0.03697023265980801, -0.09115746805438646, -0.131955144372683, 0.08243972241972784, 0.39603430192711897, -0.281229134857586, -0.2595224426130827, 0.09110963316005798, -0.22588999154891795, -0.18385118463196637, 0.1733365788587306, -0.1352804797427283, 0... |
1,801.08437 | Fast Algorithm for Calculating the Minimal Annihilating Polynomials of
Matrices via Pseudo Annihilating Polynomials | Minimal annihilating polynomials are very useful in a wide variety of
algorithms in exact linear algebra. A new efficient method is proposed for
calculating the minimal annihilating polynomials for all the unit vectors, for
a square matrix over a field of characteristic zero. Key ideas of the proposed
method are the ... | math.AC cs.SC | minimal annihilating polynomials are very useful in a wide variety of algorithms in exact linear algebra a new efficient method is proposed for calculating the minimal annihilating polynomials for all the unit vectors for a square matrix over a field of characteristic zero key ideas of the proposed method are the conce... | [['minimal', 'annihilating', 'polynomials', 'are', 'very', 'useful', 'in', 'a', 'wide', 'variety', 'of', 'algorithms', 'in', 'exact', 'linear', 'algebra', 'a', 'new', 'efficient', 'method', 'is', 'proposed', 'for', 'calculating', 'the', 'minimal', 'annihilating', 'polynomials', 'for', 'all', 'the', 'unit', 'vectors', '... | [-0.14848651656104872, 0.071383222391208, -0.09437076923747857, 0.07882788933813573, -0.0897120740202566, -0.1300009057368152, -0.006852312848592798, 0.32882145314166944, -0.31726160558561484, -0.2628697152870397, 0.0949007894936949, -0.19079472621281943, -0.15917539363106092, 0.28631359804421663, -0.012197164669632912... |
1,801.08438 | A near-infrared, optical and ultraviolet polarimetric and timing
investigation of complex equatorial dusty structures | Context. From stars to active galactic nuclei, many astrophysical systems are
surrounded by an equatorial distribution of dusty material that are, in a
number of cases, spatially unresolved even with cutting edge facilities. Aims.
In this paper, we investigate if and how one can determine the unresolved and
heterogen... | astro-ph.HE astro-ph.GA astro-ph.SR | context from stars to active galactic nuclei many astrophysical systems are surrounded by an equatorial distribution of dusty material that are in a number of cases spatially unresolved even with cutting edge facilities aims in this paper we investigate if and how one can determine the unresolved and heterogeneous morp... | [['context', 'from', 'stars', 'to', 'active', 'galactic', 'nuclei', 'many', 'astrophysical', 'systems', 'are', 'surrounded', 'by', 'an', 'equatorial', 'distribution', 'of', 'dusty', 'material', 'that', 'are', 'in', 'a', 'number', 'of', 'cases', 'spatially', 'unresolved', 'even', 'with', 'cutting', 'edge', 'facilities',... | [-0.06803885460738504, 0.13211010158041633, -0.05785934858650497, 0.10021375972788937, -0.07478212795953836, -0.10323958529522066, 0.03128964630850854, 0.4910121063487522, -0.20267697089002468, -0.3213800065728333, 0.10139781742694631, -0.300816549070641, -0.07342042381240599, 0.20054461786227787, -0.04072134252905483,... |
1,801.08439 | Analyzing Similarity in Mathematical Content To Enhance the Detection of
Academic Plagiarism | Despite the effort put into the detection of academic plagiarism, it
continues to be a ubiquitous problem spanning all disciplines. Various tools
have been developed to assist human inspectors by automatically identifying
suspicious documents. However, to our knowledge currently none of these tools
use mathematical c... | cs.IR | despite the effort put into the detection of academic plagiarism it continues to be a ubiquitous problem spanning all disciplines various tools have been developed to assist human inspectors by automatically identifying suspicious documents however to our knowledge currently none of these tools use mathematical content... | [['despite', 'the', 'effort', 'put', 'into', 'the', 'detection', 'of', 'academic', 'plagiarism', 'it', 'continues', 'to', 'be', 'a', 'ubiquitous', 'problem', 'spanning', 'all', 'disciplines', 'various', 'tools', 'have', 'been', 'developed', 'to', 'assist', 'human', 'inspectors', 'by', 'automatically', 'identifying', 's... | [-0.0407622416264839, -0.002410717729736663, -0.03849755093977867, 0.10825790440027888, -0.17142974568596236, -0.148411099851654, 0.07764613310694779, 0.3458015801873884, -0.24699528997224582, -0.3580594965893084, 0.1291036566216878, -0.28167599324364534, -0.15089286154987316, 0.2189512200257425, -0.13100297131145802, ... |
1,801.0844 | Transient charge and energy flow in the wide-band limit | The wide-band limit is a commonly used approximation to analyze transport
through nanoscale devices. In this work we investigate its applicability to the
study of charge and heat transport through molecular break junctions exposed to
voltage biases and temperature gradients. We find that while this approximation
fait... | cond-mat.mes-hall | the wideband limit is a commonly used approximation to analyze transport through nanoscale devices in this work we investigate its applicability to the study of charge and heat transport through molecular break junctions exposed to voltage biases and temperature gradients we find that while this approximation faithfull... | [['the', 'wideband', 'limit', 'is', 'a', 'commonly', 'used', 'approximation', 'to', 'analyze', 'transport', 'through', 'nanoscale', 'devices', 'in', 'this', 'work', 'we', 'investigate', 'its', 'applicability', 'to', 'the', 'study', 'of', 'charge', 'and', 'heat', 'transport', 'through', 'molecular', 'break', 'junctions'... | [-0.16627344772648883, 0.08259093439846765, -0.08618541903267721, 0.04890569203216867, -0.04148362654453243, -0.14035442869271372, 0.0830313063347499, 0.3883223880850177, -0.29396469410124965, -0.26139143589201547, 0.07665559851905715, -0.27932379343582475, -0.13464420738111016, 0.19885633311426368, -0.0477069641449239... |
1,801.08441 | Finitary-based Domain Theory in Coq: An Early Report | In domain theory every finite computable object can be represented by a
single mathematical object instead of a set of objects, using the notion of
finitary-basis. In this article we report on our effort to formalize domain
theory in Coq in terms of finitary-basis.
| cs.LO cs.PL | in domain theory every finite computable object can be represented by a single mathematical object instead of a set of objects using the notion of finitarybasis in this article we report on our effort to formalize domain theory in coq in terms of finitarybasis | [['in', 'domain', 'theory', 'every', 'finite', 'computable', 'object', 'can', 'be', 'represented', 'by', 'a', 'single', 'mathematical', 'object', 'instead', 'of', 'a', 'set', 'of', 'objects', 'using', 'the', 'notion', 'of', 'finitarybasis', 'in', 'this', 'article', 'we', 'report', 'on', 'our', 'effort', 'to', 'formaliz... | [-0.0879422458820045, 0.046170629937911316, -0.12439839192111754, 0.011476060677696728, -0.10363698690863592, -0.03562816930934787, 0.09314034233379755, 0.3677591660414778, -0.29566887570988565, -0.29732177446463276, 0.07955007681933542, -0.2065158880958777, -0.1506855453231505, 0.18329028565702693, -0.1882640086668765... |
1,801.08442 | Limit Operators, Compactness and Essential Spectra on Bounded Symmetric
Domains | This paper is a follow-up to a recent article about the essential spectrum of
Toeplitz operators acting on the Bergman space over the unit ball. As mentioned
in the said article, some of the arguments can be carried over to the case of
bounded symmetric domains and some cannot. The aim of this paper is to close
the g... | math.FA math.OA math.SP | this paper is a followup to a recent article about the essential spectrum of toeplitz operators acting on the bergman space over the unit ball as mentioned in the said article some of the arguments can be carried over to the case of bounded symmetric domains and some cannot the aim of this paper is to close the gaps to... | [['this', 'paper', 'is', 'a', 'followup', 'to', 'a', 'recent', 'article', 'about', 'the', 'essential', 'spectrum', 'of', 'toeplitz', 'operators', 'acting', 'on', 'the', 'bergman', 'space', 'over', 'the', 'unit', 'ball', 'as', 'mentioned', 'in', 'the', 'said', 'article', 'some', 'of', 'the', 'arguments', 'can', 'be', 'c... | [-0.11262907816992429, 0.11566274596000203, -0.05312848827590989, 0.0868312336602858, -0.10726507659862927, -0.08598784220382749, -0.02341366116057283, 0.38477998599410057, -0.30942995473742485, -0.14809233713008108, 0.2001759172742909, -0.2874026208578254, -0.1939263612564121, 0.19879702449543402, -0.14339118247153237... |
1,801.08443 | A first determination of the unpolarized quark TMDs from a global
analysis | Transverse momentum dependent distribution and fragmentation functions of
unpolarized quarks inside unpolarized protons are extracted, for the first
time, through a simultaneous analysis of semi-inclusive deep-inelastic
scattering, Drell-Yan and $Z$ boson hadroproduction processes. This study is
performed at leading ... | hep-ph | transverse momentum dependent distribution and fragmentation functions of unpolarized quarks inside unpolarized protons are extracted for the first time through a simultaneous analysis of semiinclusive deepinelastic scattering drellyan and z boson hadroproduction processes this study is performed at leading order in pe... | [['transverse', 'momentum', 'dependent', 'distribution', 'and', 'fragmentation', 'functions', 'of', 'unpolarized', 'quarks', 'inside', 'unpolarized', 'protons', 'are', 'extracted', 'for', 'the', 'first', 'time', 'through', 'a', 'simultaneous', 'analysis', 'of', 'semiinclusive', 'deepinelastic', 'scattering', 'drellyan'... | [-0.08514029677078296, 0.23675566104899967, -0.11074890650473954, 0.16007486787975211, -0.051591356007612485, -0.059899755949782356, -0.02078146159778391, 0.42532382175075206, -0.17993008035622285, -0.2430493745513344, -0.024138383774003118, -0.3356176940410325, 0.11414612788874447, 0.10954529554269203, 0.1092254258767... |
1,801.08444 | Hardware implementation of auto-mutual information function for
condition monitoring | This study is aimed at showing applicability of mutual information, namely
auto-mutual information function for condition monitoring in electrical motors,
through age detection in accelerated motor aging. Vibration data collected in
artificial induction motor experiment is used for verification of both the
original a... | cs.OH eess.SP | this study is aimed at showing applicability of mutual information namely automutual information function for condition monitoring in electrical motors through age detection in accelerated motor aging vibration data collected in artificial induction motor experiment is used for verification of both the original automut... | [['this', 'study', 'is', 'aimed', 'at', 'showing', 'applicability', 'of', 'mutual', 'information', 'namely', 'automutual', 'information', 'function', 'for', 'condition', 'monitoring', 'in', 'electrical', 'motors', 'through', 'age', 'detection', 'in', 'accelerated', 'motor', 'aging', 'vibration', 'data', 'collected', 'i... | [-0.08848685621622983, 0.035809019593886514, -0.11077387807400603, 0.04592478440527134, -0.09903701444630299, -0.20084285140527705, -0.008155325676821042, 0.40983520690024944, -0.23939749398350454, -0.34728663471903193, 0.14668084452696667, -0.2316020914892617, -0.16827307515695952, 0.2672359150846636, -0.0904871302926... |
1,801.08445 | Multiset-Partition Distribution Matching | Distribution matching is a fixed-length invertible mapping from a uniformly
distributed bit sequence to shaped amplitudes and plays an important role in
the probabilistic amplitude shaping framework. With conventional
constantcomposition distribution matching (CCDM), all output sequences have
identical composition. I... | eess.SP | distribution matching is a fixedlength invertible mapping from a uniformly distributed bit sequence to shaped amplitudes and plays an important role in the probabilistic amplitude shaping framework with conventional constantcomposition distribution matching ccdm all output sequences have identical composition in this p... | [['distribution', 'matching', 'is', 'a', 'fixedlength', 'invertible', 'mapping', 'from', 'a', 'uniformly', 'distributed', 'bit', 'sequence', 'to', 'shaped', 'amplitudes', 'and', 'plays', 'an', 'important', 'role', 'in', 'the', 'probabilistic', 'amplitude', 'shaping', 'framework', 'with', 'conventional', 'constantcompos... | [-0.14332695939053033, 0.10499240953875717, -0.08013712574271874, 0.06176904783630258, -0.04385584638779013, -0.1317448198836549, 0.08945761186987511, 0.391254846782734, -0.3032888919333345, -0.29888502486088936, 0.061850550594802677, -0.243809873586315, -0.10012223266069971, 0.1631388129583987, -0.10894147410726873, 0... |
1,801.08446 | A Scalable Approach for Hardware Semiformal Verification | The current verification flow of complex systems uses different engines
synergistically: virtual prototyping, formal verification, simulation,
emulation and FPGA prototyping. However, none is able to verify a complete
architecture. Furthermore, hybrid approaches aiming at complete verification
use techniques that low... | cs.LO cs.SE | the current verification flow of complex systems uses different engines synergistically virtual prototyping formal verification simulation emulation and fpga prototyping however none is able to verify a complete architecture furthermore hybrid approaches aiming at complete verification use techniques that lower the ove... | [['the', 'current', 'verification', 'flow', 'of', 'complex', 'systems', 'uses', 'different', 'engines', 'synergistically', 'virtual', 'prototyping', 'formal', 'verification', 'simulation', 'emulation', 'and', 'fpga', 'prototyping', 'however', 'none', 'is', 'able', 'to', 'verify', 'a', 'complete', 'architecture', 'furth... | [-0.09786247804930265, -0.052654414176934304, -0.06999045614396561, 0.03215656427842491, -0.0800758307397535, -0.14532764079790053, 0.05180924078872935, 0.36617102998901496, -0.2090363677919165, -0.34800624032504857, 0.10903929271311923, -0.22244865540415049, -0.14481359519149092, 0.3057145380034027, -0.072871162450279... |
1,801.08447 | Loss-function learning for digital tissue deconvolution | The gene expression profile of a tissue averages the expression profiles of
all cells in this tissue. Digital tissue deconvolution (DTD) addresses the
following inverse problem: Given the expression profile $y$ of a tissue, what
is the cellular composition $c$ of that tissue? If $X$ is a matrix whose
columns are refe... | q-bio.QM | the gene expression profile of a tissue averages the expression profiles of all cells in this tissue digital tissue deconvolution dtd addresses the following inverse problem given the expression profile y of a tissue what is the cellular composition c of that tissue if x is a matrix whose columns are reference profiles... | [['the', 'gene', 'expression', 'profile', 'of', 'a', 'tissue', 'averages', 'the', 'expression', 'profiles', 'of', 'all', 'cells', 'in', 'this', 'tissue', 'digital', 'tissue', 'deconvolution', 'dtd', 'addresses', 'the', 'following', 'inverse', 'problem', 'given', 'the', 'expression', 'profile', 'y', 'of', 'a', 'tissue',... | [-0.0640930491470316, 0.0875230676146025, -0.006759675934254748, 0.07283705826878033, -0.028994430041046074, -0.1516800314369582, 0.08135883207945446, 0.38264295358046796, -0.29136239993532403, -0.28033140396593875, 0.04063153152248629, -0.2540593678220475, -0.17031290529606244, 0.14416185009612484, -0.1353109193432771... |
1,801.08448 | Symmetry breaking in planar and maximal outerplanar graphs | The distinguishing number (index) $D(G)$ ($D'(G)$) of a graph $G$ is the
least integer $d$ such that $G$ has a vertex (edge) labeling with $d$ labels
that is preserved only by a trivial automorphism. In this paper we consider the
maximal outerplanar graphs (MOP graphs) and show that MOP graphs, except $K_3$,
can be d... | math.CO | the distinguishing number index dg dg of a graph g is the least integer d such that g has a vertex edge labeling with d labels that is preserved only by a trivial automorphism in this paper we consider the maximal outerplanar graphs mop graphs and show that mop graphs except k_3 can be distinguished by at most two vert... | [['the', 'distinguishing', 'number', 'index', 'dg', 'dg', 'of', 'a', 'graph', 'g', 'is', 'the', 'least', 'integer', 'd', 'such', 'that', 'g', 'has', 'a', 'vertex', 'edge', 'labeling', 'with', 'd', 'labels', 'that', 'is', 'preserved', 'only', 'by', 'a', 'trivial', 'automorphism', 'in', 'this', 'paper', 'we', 'consider',... | [-0.2207283575099881, 0.14823340493943785, -0.02655270164106767, 0.016089325539416985, -0.13033325956868275, -0.22790562695908276, 0.022520758237314784, 0.40108666244845886, -0.30050588589820815, -0.3673109796333623, 0.08930080695313632, -0.333145995080084, -0.16342810410159556, 0.06473141874779355, -0.1260364636198266... |
1,801.08449 | Singular Cw-Expansive Flows | We study continuum-wise expansive flows with fixed points on metric spaces
and low dimensional manifolds. We give sufficient conditions for a surface flow
to be singular cw-expansive and examples showing that cw-expansivity does not
imply expansivity. We also construct a singular Axiom A vector field on a
three-manif... | math.DS | we study continuumwise expansive flows with fixed points on metric spaces and low dimensional manifolds we give sufficient conditions for a surface flow to be singular cwexpansive and examples showing that cwexpansivity does not imply expansivity we also construct a singular axiom a vector field on a threemanifold bein... | [['we', 'study', 'continuumwise', 'expansive', 'flows', 'with', 'fixed', 'points', 'on', 'metric', 'spaces', 'and', 'low', 'dimensional', 'manifolds', 'we', 'give', 'sufficient', 'conditions', 'for', 'a', 'surface', 'flow', 'to', 'be', 'singular', 'cwexpansive', 'and', 'examples', 'showing', 'that', 'cwexpansivity', 'd... | [-0.21728043024620367, 0.12440573453297099, -0.14093543113105828, 0.09144962354311867, -0.07861902272432214, -0.18848824918654467, 0.034142302800088176, 0.32861884576933725, -0.21673784526212822, -0.12893789255666355, 0.17508965370518761, -0.2899267787912062, -0.20937875953931656, 0.21341209463952554, -0.18050078704716... |
1,801.0845 | Reasoning about effects: from lists to cyber-physical agents | Theories for reasoning about programs with effects initially focused on basic
manipulation of lists and other mutable data. The next challenge was to
consider higher-order programming, adding functions as first class objects to
mutable data. Reasoning about actors added the challenge of dealing with
distributed open ... | cs.PL cs.LO | theories for reasoning about programs with effects initially focused on basic manipulation of lists and other mutable data the next challenge was to consider higherorder programming adding functions as first class objects to mutable data reasoning about actors added the challenge of dealing with distributed open system... | [['theories', 'for', 'reasoning', 'about', 'programs', 'with', 'effects', 'initially', 'focused', 'on', 'basic', 'manipulation', 'of', 'lists', 'and', 'other', 'mutable', 'data', 'the', 'next', 'challenge', 'was', 'to', 'consider', 'higherorder', 'programming', 'adding', 'functions', 'as', 'first', 'class', 'objects', ... | [-0.14802397318029156, 0.07277494569619497, 0.0005590907686079542, 0.06696026761686275, -0.18293951058682675, -0.20221709311784555, 0.05381934503190375, 0.34207333009690044, -0.26236439259179556, -0.39820546605600005, 0.10269451731049534, -0.30954840453341603, -0.13350302706627795, 0.18881733799547268, -0.1471059839939... |
1,801.08451 | Higher-dimensional automata modeling shared-variable systems | The purpose of this paper is to provide a construction to model
shared-variable systems using higher-dimensional automata which is
compositional in the sense that the parallel composition of completely
independent systems is modeled by the standard tensor product of HDAs and
nondeterministic choice is represented by ... | cs.LO cs.FL | the purpose of this paper is to provide a construction to model sharedvariable systems using higherdimensional automata which is compositional in the sense that the parallel composition of completely independent systems is modeled by the standard tensor product of hdas and nondeterministic choice is represented by the ... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'provide', 'a', 'construction', 'to', 'model', 'sharedvariable', 'systems', 'using', 'higherdimensional', 'automata', 'which', 'is', 'compositional', 'in', 'the', 'sense', 'that', 'the', 'parallel', 'composition', 'of', 'completely', 'independent', 'systems', 'is',... | [-0.12373088286646332, 0.13678973228282607, -0.05817204727403199, 0.02955052477530747, -0.061484420322813094, -0.12332229066911775, 0.009514372720635341, 0.32609862469447154, -0.33794888900592923, -0.2515224351081997, 0.0928619663536665, -0.17308549439379325, -0.16853186682177088, 0.15167841986112762, -0.09894584556847... |
1,801.08452 | Generic Dynamics on Compact Metric Spaces | We prove that generically and modulo a topological conjugacy there is only
one dynamical system.
| math.DS | we prove that generically and modulo a topological conjugacy there is only one dynamical system | [['we', 'prove', 'that', 'generically', 'and', 'modulo', 'a', 'topological', 'conjugacy', 'there', 'is', 'only', 'one', 'dynamical', 'system']] | [-0.3111875620981058, 0.17372959932933252, -0.13203312021990618, 0.09086396573887517, -0.028405876519779365, -0.2583968338323757, 0.030879626919825872, 0.2937975359459718, -0.36335541506608326, -0.1755052932848533, 0.11806426641220848, -0.293571533759435, -0.240589806670323, 0.215536222110192, -0.09441426123181978, 0.0... |
1,801.08453 | Failure of $L^2$ boundedness of gradients of single layer potentials for
measures with zero low density | Consider a totally irregular measure $\mu$ in $\mathbb{R}^{n+1}$, that is,
the upper density $\limsup_{r\to0}\frac{\mu(B(x,r))}{(2r)^n}$ is positive
$\mu$-a.e.\ in $\mathbb{R}^{n+1}$, and the lower density
$\liminf_{r\to0}\frac{\mu(B(x,r))}{(2r)^n}$ vanishes $\mu$-a.e. in
$\mathbb{R}^{n+1}$. We show that if $T_\mu f(... | math.CA | consider a totally irregular measure mu in mathbbrn1 that is the upper density limsup_rto0fracmubxr2rn is positive muae in mathbbrn1 and the lower density liminf_rto0fracmubxr2rn vanishes muae in mathbbrn1 we show that if t_mu fxint kxydmuy is an operator whose kernel kcdotcdot is the gradient of the fundamental soluti... | [['consider', 'a', 'totally', 'irregular', 'measure', 'mu', 'in', 'mathbbrn1', 'that', 'is', 'the', 'upper', 'density', 'limsup_rto0fracmubxr2rn', 'is', 'positive', 'muae', 'in', 'mathbbrn1', 'and', 'the', 'lower', 'density', 'liminf_rto0fracmubxr2rn', 'vanishes', 'muae', 'in', 'mathbbrn1', 'we', 'show', 'that', 'if', ... | [-0.1440084352867589, 0.13959559271201474, -0.0920127330436593, 0.04425213295949756, -0.07177431315981916, -0.11887675135706861, -0.043626073366751714, 0.3336444201857029, -0.2987375561192277, -0.08114268985532579, 0.14794239668879614, -0.3364278258578408, -0.13886204858620962, 0.1685344189782405, -0.12772580344850817,... |
1,801.08454 | A Distributed Framework for the Construction of Transport Maps | The need to reason about uncertainty in large, complex, and multi-modal
datasets has become increasingly common across modern scientific environments.
The ability to transform samples from one distribution $P$ to another
distribution $Q$ enables the solution to many problems in machine learning
(e.g. Bayesian inferen... | stat.ML | the need to reason about uncertainty in large complex and multimodal datasets has become increasingly common across modern scientific environments the ability to transform samples from one distribution p to another distribution q enables the solution to many problems in machine learning eg bayesian inference generative... | [['the', 'need', 'to', 'reason', 'about', 'uncertainty', 'in', 'large', 'complex', 'and', 'multimodal', 'datasets', 'has', 'become', 'increasingly', 'common', 'across', 'modern', 'scientific', 'environments', 'the', 'ability', 'to', 'transform', 'samples', 'from', 'one', 'distribution', 'p', 'to', 'another', 'distribut... | [-0.030516394493919876, 0.027169911149986407, -0.11793773637549809, 0.06876131625534272, -0.09441397826175474, -0.1616198261114532, 0.03664674264007895, 0.405073593994129, -0.3420127458748076, -0.34577825613974955, 0.09590419023287862, -0.2653656420692549, -0.17129504860756659, 0.21620431509642404, -0.11789300100053109... |
1,801.08455 | Constraints on Radial Migration in Spiral Galaxies - II. Angular
momentum distribution and preferential migration | The orbital angular momentum of individual stars in galactic discs can be
permanently changed through torques from transient spiral patterns.
Interactions at the corotation resonance dominate these changes and have the
further property of conserving orbital circularity. We derived in an earlier
paper an analytic crit... | astro-ph.GA | the orbital angular momentum of individual stars in galactic discs can be permanently changed through torques from transient spiral patterns interactions at the corotation resonance dominate these changes and have the further property of conserving orbital circularity we derived in an earlier paper an analytic criterio... | [['the', 'orbital', 'angular', 'momentum', 'of', 'individual', 'stars', 'in', 'galactic', 'discs', 'can', 'be', 'permanently', 'changed', 'through', 'torques', 'from', 'transient', 'spiral', 'patterns', 'interactions', 'at', 'the', 'corotation', 'resonance', 'dominate', 'these', 'changes', 'and', 'have', 'the', 'furthe... | [-0.14854179461265332, 0.1510104729843961, -0.10802296211823158, 0.05898149991765305, -0.06909074242420421, -0.02574016052381237, 0.024017953951866136, 0.38415296434765994, -0.242527136044337, -0.3072356913166148, 0.017465079312747583, -0.26591399663340043, -0.0651450133882463, 0.2035333181242689, -0.038068127280705154... |
1,801.08456 | Determining sets and determining numbers of finite groups | Let $G$ be a group. A subset $D$ of $G$ is a determining set of $G$, if every
automorphism of $G$ is uniquely determined by its action on $D$. The
determining number of $G$, denoted by $\alpha(G)$, is the cardinality of a
smallest determining set. A generating set of $G$ is a subset such that every
element of $G$ can... | math.GR | let g be a group a subset d of g is a determining set of g if every automorphism of g is uniquely determined by its action on d the determining number of g denoted by alphag is the cardinality of a smallest determining set a generating set of g is a subset such that every element of g can be expressed as the combinatio... | [['let', 'g', 'be', 'a', 'group', 'a', 'subset', 'd', 'of', 'g', 'is', 'a', 'determining', 'set', 'of', 'g', 'if', 'every', 'automorphism', 'of', 'g', 'is', 'uniquely', 'determined', 'by', 'its', 'action', 'on', 'd', 'the', 'determining', 'number', 'of', 'g', 'denoted', 'by', 'alphag', 'is', 'the', 'cardinality', 'of',... | [-0.23762122285092788, 0.17617634355502607, -0.060736186426181935, -0.029374889887893867, -0.11314969497830853, -0.10066465298694215, 0.035053821011005265, 0.3476696329828548, -0.31128903942084624, -0.2924017423812888, 0.11635055956920903, -0.29359445715733606, -0.09030063417249996, 0.19138955499266128, -0.075696687836... |
1,801.08457 | Giant magnetic quantum oscillations in the thermal conductivity of TaAs:
Indications of chiral zero sound | Charge transport of topological semimetals has been in the focus of intensive
investigations because of their non-trivial band topology. Heat transport of
these materials, on the other hand, is largely unexplored and remains elusive.
Here we report on an observation of unprecedented, giant magnetic quantum
oscillatio... | cond-mat.mtrl-sci | charge transport of topological semimetals has been in the focus of intensive investigations because of their nontrivial band topology heat transport of these materials on the other hand is largely unexplored and remains elusive here we report on an observation of unprecedented giant magnetic quantum oscillations of th... | [['charge', 'transport', 'of', 'topological', 'semimetals', 'has', 'been', 'in', 'the', 'focus', 'of', 'intensive', 'investigations', 'because', 'of', 'their', 'nontrivial', 'band', 'topology', 'heat', 'transport', 'of', 'these', 'materials', 'on', 'the', 'other', 'hand', 'is', 'largely', 'unexplored', 'and', 'remains'... | [-0.22297464506859713, 0.22051487172751685, -0.06561618429277474, 0.035453193413920885, -0.12860018735670525, -0.14012718439588082, 0.08986739002411133, 0.36864286290932885, -0.22660316783148124, -0.2626848716855697, 0.0312309373496968, -0.3355986799535729, -0.14969171033391254, 0.21968551942361345, 0.02003000136349142... |
1,801.08458 | $p$-bases and differential operators on varieties defined over a
non-perfect field | Let $k$ be a possibly non-perfect field of characteristic $p > 0$. In this
work we prove the local existence of absolute $p$-bases for regular algebras of
finite type over $k$. Namely, consider a regular variety $Z$ over $k$. Kimura
and Niitsuma proved that, for every $\xi \in Z$, the local ring
$\mathcal{O}_{Z,\xi}$... | math.AC | let k be a possibly nonperfect field of characteristic p 0 in this work we prove the local existence of absolute pbases for regular algebras of finite type over k namely consider a regular variety z over k kimura and niitsuma proved that for every xi in z the local ring mathcalo_zxi has a pbasis over mathcalo_zxip here... | [['let', 'k', 'be', 'a', 'possibly', 'nonperfect', 'field', 'of', 'characteristic', 'p', '0', 'in', 'this', 'work', 'we', 'prove', 'the', 'local', 'existence', 'of', 'absolute', 'pbases', 'for', 'regular', 'algebras', 'of', 'finite', 'type', 'over', 'k', 'namely', 'consider', 'a', 'regular', 'variety', 'z', 'over', 'k'... | [-0.1923303046740245, 0.06380406276248111, -0.09556277908606801, -0.0014248447916416322, -0.045021694389085265, -0.13662257404499795, 0.02824007421407069, 0.3527838467785461, -0.3324322962326669, -0.16860094788361768, 0.07672888224032101, -0.23209834601026202, -0.10190787879130153, 0.21730244192186482, -0.0698549711703... |
1,801.08459 | Finding ReMO (Related Memory Object): A Simple Neural Architecture for
Text based Reasoning | To solve the text-based question and answering task that requires relational
reasoning, it is necessary to memorize a large amount of information and find
out the question relevant information from the memory. Most approaches were
based on external memory and four components proposed by Memory Network. The
distinctiv... | cs.AI | to solve the textbased question and answering task that requires relational reasoning it is necessary to memorize a large amount of information and find out the question relevant information from the memory most approaches were based on external memory and four components proposed by memory network the distinctive comp... | [['to', 'solve', 'the', 'textbased', 'question', 'and', 'answering', 'task', 'that', 'requires', 'relational', 'reasoning', 'it', 'is', 'necessary', 'to', 'memorize', 'a', 'large', 'amount', 'of', 'information', 'and', 'find', 'out', 'the', 'question', 'relevant', 'information', 'from', 'the', 'memory', 'most', 'approa... | [-0.07290776732763082, -0.011594793993722777, -0.04625395561793241, 0.09518904268083259, -0.15084951461035886, -0.2170586678649074, 0.053851953152053315, 0.4188476753389013, -0.2991790232320862, -0.3683853872377297, 0.05446783487508394, -0.25940246391912986, -0.2066974698276869, 0.20128493437479283, -0.1086240294421541... |
1,801.0846 | Frobenius linear translators giving rise to new infinite classes of
permutations and bent functions | We show the existence of many infinite classes of permutations over finite
fields and bent functions by extending the notion of linear translators,
introduced by Kyureghyan [12]. We call these translators Frobenius translators
since the derivatives of $f : F_{p^n} \rightarrow F_{p^k}$, where $n = rk$, are
of the form... | math.AC math.NT | we show the existence of many infinite classes of permutations over finite fields and bent functions by extending the notion of linear translators introduced by kyureghyan 12 we call these translators frobenius translators since the derivatives of f f_pn rightarrow f_pk where n rk are of the form fx uphi fx upib for a ... | [['we', 'show', 'the', 'existence', 'of', 'many', 'infinite', 'classes', 'of', 'permutations', 'over', 'finite', 'fields', 'and', 'bent', 'functions', 'by', 'extending', 'the', 'notion', 'of', 'linear', 'translators', 'introduced', 'by', 'kyureghyan', '12', 'we', 'call', 'these', 'translators', 'frobenius', 'translator... | [-0.17658583655732102, 0.11736975435128938, -0.007112758885377483, 0.05654892595577063, -0.05549291024989642, -0.1522284900622055, 0.021473752711622947, 0.35530620176197575, -0.3078914352803316, -0.2368780494261865, 0.08466399813100861, -0.2972143229724157, -0.12424022527405817, 0.21519758330086375, -0.0318042603090848... |
1,801.08461 | Rescaled expansivity and separating flows | In this article we give sufficient conditions for Komuro expansivity to imply
the rescaled expansivity recently introduced by Wen and Wen. Also, we show that
a flow on a compact metric space is expansive in the sense of Katok-Hasselblatt
if and only if it is separating in the sense of Gura and the set of fixed
points... | math.DS | in this article we give sufficient conditions for komuro expansivity to imply the rescaled expansivity recently introduced by wen and wen also we show that a flow on a compact metric space is expansive in the sense of katokhasselblatt if and only if it is separating in the sense of gura and the set of fixed points is o... | [['in', 'this', 'article', 'we', 'give', 'sufficient', 'conditions', 'for', 'komuro', 'expansivity', 'to', 'imply', 'the', 'rescaled', 'expansivity', 'recently', 'introduced', 'by', 'wen', 'and', 'wen', 'also', 'we', 'show', 'that', 'a', 'flow', 'on', 'a', 'compact', 'metric', 'space', 'is', 'expansive', 'in', 'the', '... | [-0.12098129763545697, 0.1476745363447423, -0.12410185873720861, 0.05284390375099815, -0.029644640538383994, -0.08657877622662406, 0.07149662402572862, 0.35384182448972734, -0.265754128822632, -0.20897825938861883, 0.13316757107161703, -0.2518705352323881, -0.20920685760415436, 0.19859530498976247, -0.14276228389261583... |
1,801.08462 | Weyl invariant $E_8$ Jacobi forms | We investigate the Jacobi forms for the root system $E_8$ invariant under the
Weyl group. This type of Jacobi forms has significance in Frobenius manifolds,
Gromov--Witten theory and string theory. In 1992, Wirthm\"{u}ller proved that
the space of Jacobi forms for any irreducible root system not of type $E_8$ is
a po... | math.NT hep-th math.AG | we investigate the jacobi forms for the root system e_8 invariant under the weyl group this type of jacobi forms has significance in frobenius manifolds gromovwitten theory and string theory in 1992 wirthmuller proved that the space of jacobi forms for any irreducible root system not of type e_8 is a polynomial algebra... | [['we', 'investigate', 'the', 'jacobi', 'forms', 'for', 'the', 'root', 'system', 'e_8', 'invariant', 'under', 'the', 'weyl', 'group', 'this', 'type', 'of', 'jacobi', 'forms', 'has', 'significance', 'in', 'frobenius', 'manifolds', 'gromovwitten', 'theory', 'and', 'string', 'theory', 'in', '1992', 'wirthmuller', 'proved'... | [-0.23627871139906348, 0.07955562548401456, -0.09734611939897554, 0.0767314658273891, -0.11232918287601529, -0.144470723082001, -0.06714221983565949, 0.2956903612862031, -0.3235302381113999, -0.20730912294497505, 0.10026104708667845, -0.2173652761641683, -0.21034001561088694, 0.2044146044438498, -0.09214031775093948, -... |
1,801.08463 | Symmetry-breaking supercollisions in Landau-quantized graphene | Recent pump-probe experiments performed on graphene in a perpendicular
magnetic field have revealed carrier relaxation times ranging from picoseconds
to nanoseconds depending on the quality of the sample. To explain this
surprising behavior, we propose a novel symmetry-breaking defect-assisted
relaxation channel. Thi... | cond-mat.mtrl-sci | recent pumpprobe experiments performed on graphene in a perpendicular magnetic field have revealed carrier relaxation times ranging from picoseconds to nanoseconds depending on the quality of the sample to explain this surprising behavior we propose a novel symmetrybreaking defectassisted relaxation channel this enable... | [['recent', 'pumpprobe', 'experiments', 'performed', 'on', 'graphene', 'in', 'a', 'perpendicular', 'magnetic', 'field', 'have', 'revealed', 'carrier', 'relaxation', 'times', 'ranging', 'from', 'picoseconds', 'to', 'nanoseconds', 'depending', 'on', 'the', 'quality', 'of', 'the', 'sample', 'to', 'explain', 'this', 'surpr... | [-0.13699601613629012, 0.18869847092018635, -0.07838355447453113, -0.031453192340394044, -0.04013265774550813, -0.12396206693036804, 0.11154348062880245, 0.4246873795169831, -0.31331971908609074, -0.31979969716458406, -0.006599222804293221, -0.25092934214590507, -0.09700931004467017, 0.21913828781265535, 0.023815857091... |
1,801.08464 | Algebraic multigrid preconditioners for two-phase flow in porous media
with phase transitions | Multiphase flow is a critical process in a wide range of applications,
including oil and gas recovery, carbon sequestration, and contaminant
remediation. Numerical simulation of multiphase flow requires solving of a
large, sparse linear system resulting from the discretization of the partial
differential equations mo... | math.NA physics.comp-ph physics.flu-dyn | multiphase flow is a critical process in a wide range of applications including oil and gas recovery carbon sequestration and contaminant remediation numerical simulation of multiphase flow requires solving of a large sparse linear system resulting from the discretization of the partial differential equations modeling ... | [['multiphase', 'flow', 'is', 'a', 'critical', 'process', 'in', 'a', 'wide', 'range', 'of', 'applications', 'including', 'oil', 'and', 'gas', 'recovery', 'carbon', 'sequestration', 'and', 'contaminant', 'remediation', 'numerical', 'simulation', 'of', 'multiphase', 'flow', 'requires', 'solving', 'of', 'a', 'large', 'spa... | [-0.10742235259749577, 0.05526609128379884, -0.0936483902032099, 0.01574046675066256, -0.07935689410757428, -0.14754541476722807, 0.019232164246689838, 0.34758661155744147, -0.3325661755477389, -0.29108139968399577, 0.14008844201016474, -0.24321634060858438, -0.16754319555135833, 0.20268907014202947, -0.061567524680867... |
1,801.08465 | Undulator-Based Positron Source at 250 GeV CM Energy with Different
Optical Matching Devices: Pulsed Flux Concentrator and Quarter Wave
Transformer | In the baseline design of the International Linear Collider (ILC) an
undulator-based source is foreseen for the positron source. In this study the
energy deposition in the pulsed flux concentrator (FC) of positron source is
calculated for the ILC at 250 GeV center-of-mass energy. The peak energy of 33
J/g deposited b... | physics.acc-ph | in the baseline design of the international linear collider ilc an undulatorbased source is foreseen for the positron source in this study the energy deposition in the pulsed flux concentrator fc of positron source is calculated for the ilc at 250 gev centerofmass energy the peak energy of 33 jg deposited by one beam p... | [['in', 'the', 'baseline', 'design', 'of', 'the', 'international', 'linear', 'collider', 'ilc', 'an', 'undulatorbased', 'source', 'is', 'foreseen', 'for', 'the', 'positron', 'source', 'in', 'this', 'study', 'the', 'energy', 'deposition', 'in', 'the', 'pulsed', 'flux', 'concentrator', 'fc', 'of', 'positron', 'source', '... | [-0.0430756085586515, 0.1397279227451637, -0.04460258799372241, 0.09375995634977966, -0.02797388190896634, -0.1376969797488795, 0.021123329619192246, 0.38390185242957053, -0.2547592602615409, -0.31263030585422014, 0.0585443717033794, -0.30257917353917624, 0.0535374832479112, 0.25970440595205324, -0.004648906750577118, ... |
1,801.08466 | Halo-independent comparison of direct detection experiments in the
effective theory of dark matter-nucleon interactions | The theoretical interpretation of dark matter direct detection experiments is
hindered by uncertainties of the microphysics governing the dark matter-nucleon
interaction, and of the dark matter density and velocity distribution inside
the Solar System. These uncertainties are especially relevant when confronting
a de... | hep-ph astro-ph.CO | the theoretical interpretation of dark matter direct detection experiments is hindered by uncertainties of the microphysics governing the dark matternucleon interaction and of the dark matter density and velocity distribution inside the solar system these uncertainties are especially relevant when confronting a detecti... | [['the', 'theoretical', 'interpretation', 'of', 'dark', 'matter', 'direct', 'detection', 'experiments', 'is', 'hindered', 'by', 'uncertainties', 'of', 'the', 'microphysics', 'governing', 'the', 'dark', 'matternucleon', 'interaction', 'and', 'of', 'the', 'dark', 'matter', 'density', 'and', 'velocity', 'distribution', 'i... | [-0.12297971733544721, 0.13318694683444718, -0.08425166950135486, 0.08617416757921195, -0.07792834251982629, -0.07534637425545675, 0.03737990593665226, 0.3172689230732952, -0.2226087954874109, -0.3953036123613833, 0.06672177715360478, -0.3017800166301287, -0.06926188798573842, 0.19099523466240592, 0.03286311338851406, ... |
1,801.08467 | Identifying Corresponding Patches in SAR and Optical Images with a
Pseudo-Siamese CNN | In this letter, we propose a pseudo-siamese convolutional neural network
(CNN) architecture that enables to solve the task of identifying corresponding
patches in very-high-resolution (VHR) optical and synthetic aperture radar
(SAR) remote sensing imagery. Using eight convolutional layers each in two
parallel network... | eess.IV cs.CV | in this letter we propose a pseudosiamese convolutional neural network cnn architecture that enables to solve the task of identifying corresponding patches in veryhighresolution vhr optical and synthetic aperture radar sar remote sensing imagery using eight convolutional layers each in two parallel network streams a fu... | [['in', 'this', 'letter', 'we', 'propose', 'a', 'pseudosiamese', 'convolutional', 'neural', 'network', 'cnn', 'architecture', 'that', 'enables', 'to', 'solve', 'the', 'task', 'of', 'identifying', 'corresponding', 'patches', 'in', 'veryhighresolution', 'vhr', 'optical', 'and', 'synthetic', 'aperture', 'radar', 'sar', 'r... | [-0.04815544200357094, -0.014943267007419351, -0.05623516665830735, 0.028810694361618035, -0.06693017325442896, -0.18850786459050758, 0.0037529150359135455, 0.49261325177928755, -0.2655750070273551, -0.321695580211266, 0.09320302126207265, -0.2647575343830915, -0.22470853317691575, 0.18454731678437422, -0.1338669163308... |
1,801.08468 | Convolutional Invasion and Expansion Networks for Tumor Growth
Prediction | Tumor growth is associated with cell invasion and mass-effect, which are
traditionally formulated by mathematical models, namely reaction-diffusion
equations and biomechanics. Such models can be personalized based on clinical
measurements to build the predictive models for tumor growth. In this paper, we
investigate ... | cs.CV | tumor growth is associated with cell invasion and masseffect which are traditionally formulated by mathematical models namely reactiondiffusion equations and biomechanics such models can be personalized based on clinical measurements to build the predictive models for tumor growth in this paper we investigate the possi... | [['tumor', 'growth', 'is', 'associated', 'with', 'cell', 'invasion', 'and', 'masseffect', 'which', 'are', 'traditionally', 'formulated', 'by', 'mathematical', 'models', 'namely', 'reactiondiffusion', 'equations', 'and', 'biomechanics', 'such', 'models', 'can', 'be', 'personalized', 'based', 'on', 'clinical', 'measureme... | [0.013037334988373764, 0.01750697887421, -0.04616796522468482, 0.06426758950182535, -0.07836399245263106, -0.15866722266871444, 0.038022493718542424, 0.3901919252537707, -0.2633381935020131, -0.27187944990438745, 0.09567712963963487, -0.28429690554507614, -0.23261248645823948, 0.16581919080741012, -0.11403797472378277,... |
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