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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1,801.09169 | Understanding finite dimensional representations generically | We survey the development and status quo of a subject best described as
"generic representation theory of finite dimensional algebras", which started
taking shape in the early 1980s. Let $\Lambda$ be a finite dimensional algebra
over an algebraically closed field. Roughly, the theory aims at (a) pinning
down the irre... | math.RT math.RA | we survey the development and status quo of a subject best described as generic representation theory of finite dimensional algebras which started taking shape in the early 1980s let lambda be a finite dimensional algebra over an algebraically closed field roughly the theory aims at a pinning down the irreducible compo... | [['we', 'survey', 'the', 'development', 'and', 'status', 'quo', 'of', 'a', 'subject', 'best', 'described', 'as', 'generic', 'representation', 'theory', 'of', 'finite', 'dimensional', 'algebras', 'which', 'started', 'taking', 'shape', 'in', 'the', 'early', '1980s', 'let', 'lambda', 'be', 'a', 'finite', 'dimensional', 'a... | [-0.14098178761788702, 0.10947057399800897, -0.06311938721290995, 0.009428351946521253, -0.08654536036115172, -0.13726607241577146, -0.026534974958286085, 0.32746521197259426, -0.3200554566754572, -0.1981655129734262, 0.12202230203521759, -0.23911324612779822, -0.09622705581523808, 0.1737086506956051, -0.09255928841246... |
1,801.0917 | Generalized Littlewood-Richardson coefficients for branching rules of
GL(n) and extremal weight crystals | Following the methods used by Derksen-Weyman in \cite{DW11} and Chindris in
\cite{Chi08}, we use quiver theory to represent the generalized
Littlewood-Richardson coefficients for the branching rule for the diagonal
embedding of $\gl(n)$ as the dimension of a weight space of semi-invariants.
Using this, we prove their... | math.RT math.CO | following the methods used by derksenweyman in citedw11 and chindris in citechi08 we use quiver theory to represent the generalized littlewoodrichardson coefficients for the branching rule for the diagonal embedding of gln as the dimension of a weight space of semiinvariants using this we prove their saturation and inv... | [['following', 'the', 'methods', 'used', 'by', 'derksenweyman', 'in', 'citedw11', 'and', 'chindris', 'in', 'citechi08', 'we', 'use', 'quiver', 'theory', 'to', 'represent', 'the', 'generalized', 'littlewoodrichardson', 'coefficients', 'for', 'the', 'branching', 'rule', 'for', 'the', 'diagonal', 'embedding', 'of', 'gln',... | [-0.10278695003552667, 0.10098614566511689, -0.09684503332335645, 0.08931477974357012, -0.0875667796891111, -0.14466740835296849, 0.009131812744621689, 0.34450244103880745, -0.3351434606996078, -0.1660107389370051, 0.09826156207866286, -0.20629719241808814, -0.19576994739831066, 0.1879271721610656, -0.09088935430582541... |
1,801.09171 | Sparse Portfolio Selection via Non-convex Fraction Function | In this paper, a continuous and non-convex promoting sparsity fraction
function is studied in two sparse portfolio selection models with and without
short-selling constraints. Firstly, we study the properties of the optimal
solution to the problem $(FP_{a,\lambda,\eta})$ including the first-order and
the second optim... | math.OC | in this paper a continuous and nonconvex promoting sparsity fraction function is studied in two sparse portfolio selection models with and without shortselling constraints firstly we study the properties of the optimal solution to the problem fp_alambdaeta including the firstorder and the second optimality condition an... | [['in', 'this', 'paper', 'a', 'continuous', 'and', 'nonconvex', 'promoting', 'sparsity', 'fraction', 'function', 'is', 'studied', 'in', 'two', 'sparse', 'portfolio', 'selection', 'models', 'with', 'and', 'without', 'shortselling', 'constraints', 'firstly', 'we', 'study', 'the', 'properties', 'of', 'the', 'optimal', 'so... | [-0.09025206567442164, 0.01299511610689459, -0.10345522129531712, 0.07042884391031545, -0.1100376466180178, -0.14635753049267494, 0.08765902704784666, 0.3845493637243325, -0.31188345716354693, -0.2674312847369212, 0.16102607025668284, -0.24615027081776172, -0.18913368410876694, 0.1269476966996816, -0.08239808463382516,... |
1,801.09172 | Modified lp-norm regularization minimization for sparse signal recovery | In numerous substitution models for the $\l_{0}$-norm minimization problem
$(P_{0})$, the $\l_{p}$-norm minimization $(P_{p})$ with $0<p<1$ have been
considered as the most natural choice. However, the non-convex optimization
problem $(P_{p})$ are much more computational challenges, and are also NP-hard.
Meanwhile, t... | math.OC | in numerous substitution models for the l_0norm minimization problem p_0 the l_pnorm minimization p_p with 0p1 have been considered as the most natural choice however the nonconvex optimization problem p_p are much more computational challenges and are also nphard meanwhile the algorithms corresponding to the proximal ... | [['in', 'numerous', 'substitution', 'models', 'for', 'the', 'l_0norm', 'minimization', 'problem', 'p_0', 'the', 'l_pnorm', 'minimization', 'p_p', 'with', '0p1', 'have', 'been', 'considered', 'as', 'the', 'most', 'natural', 'choice', 'however', 'the', 'nonconvex', 'optimization', 'problem', 'p_p', 'are', 'much', 'more',... | [-0.049053396851851845, 0.0010662988181296817, -0.09034393636924822, 0.10482353617566254, -0.1072911762192076, -0.19975421894544168, 0.018995572233309402, 0.40610646124443284, -0.34486090206432296, -0.28790845609087823, 0.13085298233668058, -0.2741689013580427, -0.17512921577018342, 0.18877409304917345, -0.115780580282... |
1,801.09173 | Why the Cosmological Constant is so Small ? A String Theory Perspective | With no free parameter (except the string scale $M_S$), dynamical flux
compactification in Type IIB string theory determines both the cosmological
constant (vacuum energy density) $\Lambda$ and the Planck mass $M_P$ in terms
of $M_S$, thus yielding their relation. Following elementary probability
theory, we find that... | hep-th | with no free parameter except the string scale m_s dynamical flux compactification in type iib string theory determines both the cosmological constant vacuum energy density lambda and the planck mass m_p in terms of m_s thus yielding their relation following elementary probability theory we find that a good fraction of... | [['with', 'no', 'free', 'parameter', 'except', 'the', 'string', 'scale', 'm_s', 'dynamical', 'flux', 'compactification', 'in', 'type', 'iib', 'string', 'theory', 'determines', 'both', 'the', 'cosmological', 'constant', 'vacuum', 'energy', 'density', 'lambda', 'and', 'the', 'planck', 'mass', 'm_p', 'in', 'terms', 'of', ... | [-0.1409896272055518, 0.2734865180394151, -0.0573592627247891, 0.19654482369943976, -0.10812597603459533, -0.17757332766986786, 0.010964601534233691, 0.28668719210560456, -0.22069470974533126, -0.3214623092252833, 0.06549902858872277, -0.243177603237713, -0.06430207580687682, 0.12223896514534807, -0.032749420953526474,... |
1,801.09174 | Integrating Ultra-Fast Charging Stations within the Power Grids of Smart
Cities: A Review | Plug-In Electric Vehicles (PEV) have become a key factor driving towards
smart cities, which allow for higher energy efficiency and lower environmental
impact across urban sectors. Industry vision for future PEV includes the
ability to recharge a vehicle at a speed comparable to traditional gas
refueling, i.e., less ... | math.OC | plugin electric vehicles pev have become a key factor driving towards smart cities which allow for higher energy efficiency and lower environmental impact across urban sectors industry vision for future pev includes the ability to recharge a vehicle at a speed comparable to traditional gas refueling ie less than 3 minu... | [['plugin', 'electric', 'vehicles', 'pev', 'have', 'become', 'a', 'key', 'factor', 'driving', 'towards', 'smart', 'cities', 'which', 'allow', 'for', 'higher', 'energy', 'efficiency', 'and', 'lower', 'environmental', 'impact', 'across', 'urban', 'sectors', 'industry', 'vision', 'for', 'future', 'pev', 'includes', 'the',... | [-0.12831423032474304, 0.09121518185738066, 0.009596354480812787, 0.03661876489841429, -0.08679324810102743, -0.1520200034037673, 0.07516697476873355, 0.3959082392875546, -0.24556147783834448, -0.3711629390881787, 0.1232967606403925, -0.29663580154839864, -0.06790740176739912, 0.25127375237011573, -0.1631674073509183, ... |
1,801.09175 | Decay of Kadomtsev - Petviashvili lumps in dissipative media | The decay of Kadomtsev - Petviashvili lumps is considered for a few typical
dissipations - Rayleigh dissipation, Reynolds dissipation, Landau damping,
Chezy bottom friction, viscous dissipation in the laminar boundary layer, and
radiative losses caused by large-scale dispersion. It is shown that the
straight-line mot... | physics.flu-dyn | the decay of kadomtsev petviashvili lumps is considered for a few typical dissipations rayleigh dissipation reynolds dissipation landau damping chezy bottom friction viscous dissipation in the laminar boundary layer and radiative losses caused by largescale dispersion it is shown that the straightline motion of lumps i... | [['the', 'decay', 'of', 'kadomtsev', 'petviashvili', 'lumps', 'is', 'considered', 'for', 'a', 'few', 'typical', 'dissipations', 'rayleigh', 'dissipation', 'reynolds', 'dissipation', 'landau', 'damping', 'chezy', 'bottom', 'friction', 'viscous', 'dissipation', 'in', 'the', 'laminar', 'boundary', 'layer', 'and', 'radiati... | [-0.22333252266641634, 0.15825620884057676, -0.07914514930520966, 0.09543975510575708, -0.04068833049748418, -0.1065194740240435, -0.03359913123993077, 0.27687961020387114, -0.2442829249374731, -0.26790870491921615, 0.04990760914617426, -0.2668497795617723, -0.11745209613977706, 0.254981425769392, 0.022813278736401963,... |
1,801.09176 | Mitigating Pilot Contamination in Multi-cell Hybrid Millimeter Wave
Systems | In this paper, we investigate the system performance of a multi-cell
multi-user (MU) hybrid millimeter wave (mmWave) multiple-input multiple-output
(MIMO) network adopting the channel estimation algorithm proposed in [1] for
channel estimation. Due to the reuse of orthogonal pilot symbols among
different cells, the c... | eess.SP cs.IT math.IT | in this paper we investigate the system performance of a multicell multiuser mu hybrid millimeter wave mmwave multipleinput multipleoutput mimo network adopting the channel estimation algorithm proposed in 1 for channel estimation due to the reuse of orthogonal pilot symbols among different cells the channel estimation... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'system', 'performance', 'of', 'a', 'multicell', 'multiuser', 'mu', 'hybrid', 'millimeter', 'wave', 'mmwave', 'multipleinput', 'multipleoutput', 'mimo', 'network', 'adopting', 'the', 'channel', 'estimation', 'algorithm', 'proposed', 'in', '1', 'for', 'channel', 'esti... | [-0.2787021407359709, 0.009165488162915082, 0.018901462519639416, 0.01413080186887926, -0.030934163386231568, -0.1879220016937899, 0.11968311075026195, 0.35359391875221935, -0.2133733779421738, -0.26311634330838723, 0.09751523414007879, -0.2380877089637675, -0.2156932218563988, 0.1264038737725442, -0.11559394277681254,... |
1,801.09177 | A Comparison of SC-FDE and UW DFT-s-OFDM for Millimeter Wave
Communications | In this study, we compare the single-carrier (SC) waveform adopted in IEEE
802.11ad and unique word discrete Fourier transform spread orthogonal frequency
division multiplexing (UW DFT-s-OFDM) waveform. We provide equivalent
representations of up-sampling and down-sampling operations of the SC waveform
by using discr... | cs.IT math.IT | in this study we compare the singlecarrier sc waveform adopted in ieee 80211ad and unique word discrete fourier transform spread orthogonal frequency division multiplexing uw dftsofdm waveform we provide equivalent representations of upsampling and downsampling operations of the sc waveform by using discrete fourier tr... | [['in', 'this', 'study', 'we', 'compare', 'the', 'singlecarrier', 'sc', 'waveform', 'adopted', 'in', 'ieee', '80211ad', 'and', 'unique', 'word', 'discrete', 'fourier', 'transform', 'spread', 'orthogonal', 'frequency', 'division', 'multiplexing', 'uw', 'dftsofdm', 'waveform', 'we', 'provide', 'equivalent', 'representati... | [-0.2217170602317943, -0.01582102930293778, -0.04906681996949932, 0.012162031987082888, -0.08016771341439838, -0.2545547004004842, 0.08292484835705213, 0.4545822057938367, -0.2734037092423927, -0.21255526459116858, 0.08968284153359077, -0.24430413773740856, -0.22715717409900799, 0.18612011346274343, -0.1474178479603159... |
1,801.09178 | On the Dynamics of a Rolling Ball Actuated by Internal Point Masses | The motion of a rolling ball actuated by internal point masses that move
inside the ball's frame of reference is considered. The equations of motion are
derived by applying Euler-Poincar\'e's symmetry reduction method in concert
with Lagrange-d'Alembert's principle, which accounts for the presence of the
nonholonomic... | math.DS math-ph math.MP | the motion of a rolling ball actuated by internal point masses that move inside the balls frame of reference is considered the equations of motion are derived by applying eulerpoincares symmetry reduction method in concert with lagrangedalemberts principle which accounts for the presence of the nonholonomic rolling con... | [['the', 'motion', 'of', 'a', 'rolling', 'ball', 'actuated', 'by', 'internal', 'point', 'masses', 'that', 'move', 'inside', 'the', 'balls', 'frame', 'of', 'reference', 'is', 'considered', 'the', 'equations', 'of', 'motion', 'are', 'derived', 'by', 'applying', 'eulerpoincares', 'symmetry', 'reduction', 'method', 'in', '... | [-0.1470497480343578, 0.14173144689025693, -0.053602598282754974, -0.010132078625395865, -0.07293476958592433, -0.13627831948602187, -0.003609709815028874, 0.36168566979975203, -0.25849890387716706, -0.3299928293780855, 0.10647603266569876, -0.2533833849993951, -0.11377642219813708, 0.2246444082885966, -0.0708100528751... |
1,801.09179 | Hindman-like theorems with uncountably many colours and finite
monochromatic sets | A particular case of the Hindman--Galvin--Glazer theorem states that, for
every partition of an infinite abelian group $G$ into two cells, there will be
an infinite $X\subseteq G$ such that the set of its finite sums
$\{x_1+\cdots+x_n\big|n\in\mathbb N\wedge x_1,\ldots,x_n\in X\text{ are
distinct}\}$ is monochromatic... | math.LO math.CO | a particular case of the hindmangalvinglazer theorem states that for every partition of an infinite abelian group g into two cells there will be an infinite xsubseteq g such that the set of its finite sums x_1cdotsx_nbigninmathbb nwedge x_1ldotsx_nin xtext are distinct is monochromatic it is known that the same stateme... | [['a', 'particular', 'case', 'of', 'the', 'hindmangalvinglazer', 'theorem', 'states', 'that', 'for', 'every', 'partition', 'of', 'an', 'infinite', 'abelian', 'group', 'g', 'into', 'two', 'cells', 'there', 'will', 'be', 'an', 'infinite', 'xsubseteq', 'g', 'such', 'that', 'the', 'set', 'of', 'its', 'finite', 'sums', 'x_1... | [-0.14403861318181715, 0.16386362906127283, -0.08859265576479317, 0.07038867715941671, -0.07062819046821474, -0.12875736044108413, 0.05414465678418553, 0.35166466395363555, -0.2588335162682729, -0.21308861009932997, 0.09504274145668046, -0.2982717310380589, -0.13206835138035639, 0.2251889018256587, -0.10155990264442472... |
1,801.0918 | Modelling of Bose - Einstein condensation in a water tank | It is shown that surface waves propagating against the external current,
slowly varying in the horizontal direction in deep water, are governed by the
equation which is tantamount to the Gross - Pitaevskii equation modelling the
mean-field dynamics of Bose - Einstein condensate. The repulsive or attractive
sign of th... | physics.flu-dyn | it is shown that surface waves propagating against the external current slowly varying in the horizontal direction in deep water are governed by the equation which is tantamount to the gross pitaevskii equation modelling the meanfield dynamics of bose einstein condensate the repulsive or attractive sign of the cubic te... | [['it', 'is', 'shown', 'that', 'surface', 'waves', 'propagating', 'against', 'the', 'external', 'current', 'slowly', 'varying', 'in', 'the', 'horizontal', 'direction', 'in', 'deep', 'water', 'are', 'governed', 'by', 'the', 'equation', 'which', 'is', 'tantamount', 'to', 'the', 'gross', 'pitaevskii', 'equation', 'modelli... | [-0.14600979628359748, 0.17374972614695197, -0.0975358331438192, 0.06658717968539164, -0.04892813651679958, -0.13179119122784813, -0.015712217582218652, 0.3071423159170972, -0.26075092188025617, -0.2965887996691222, 0.06558532913973346, -0.2788306730941926, -0.13021086715874547, 0.17893649594696734, 0.01714816064115290... |
1,801.09181 | Generalized Lambert series, Raabe's integral and a two-parameter
generalization of Ramanujan's formula for $\zeta(2m+1)$ | A comprehensive study of the generalized Lambert series
$\displaystyle\sum_{n=1}^{\infty}\frac{n^{N-2h}\exp{(-an^{N}x)}}{1-\exp{(-n^{N}x)}},
0<a\leq 1,\ x>0$, $N\in\mathbb{N}$ and $h\in\mathbb{Z}$, is undertaken. Two of
the general transformations of this series that we obtain here lead to
two-parameter generalizatio... | math.NT | a comprehensive study of the generalized lambert series displaystylesum_n1inftyfracnn2hexpannx1expnnx 0aleq 1 x0 ninmathbbn and hinmathbbz is undertaken two of the general transformations of this series that we obtain here lead to twoparameter generalizations of ramanujans famous formula for zeta2m1 m0 and the transfor... | [['a', 'comprehensive', 'study', 'of', 'the', 'generalized', 'lambert', 'series', 'displaystylesum_n1inftyfracnn2hexpannx1expnnx', '0aleq', '1', 'x0', 'ninmathbbn', 'and', 'hinmathbbz', 'is', 'undertaken', 'two', 'of', 'the', 'general', 'transformations', 'of', 'this', 'series', 'that', 'we', 'obtain', 'here', 'lead', ... | [-0.17288835443070402, 0.05589824107629956, -0.11242116673485092, 0.10636805390088779, -0.09748853927721148, -0.17946901698799236, 0.033933482488678036, 0.26420070219623004, -0.23886744054844197, -0.26335815986537414, 0.09264082166001848, -0.27139849068556465, -0.18214175614082942, 0.30646144522596963, -0.0488491322318... |
1,801.09182 | Theoretical bounds for the exponent in the empirical power-law
advance-time curve for surface flow | A fundamental and widely applied concept used to study surface flow processes
is the advance-time curve characterized by an empirical power law with an
exponent r and a numerical prefactor p (i.e., x = p*t^r). In the literature,
different values of r have been reported for various situations and types of
surface irri... | physics.flu-dyn cond-mat.soft | a fundamental and widely applied concept used to study surface flow processes is the advancetime curve characterized by an empirical power law with an exponent r and a numerical prefactor p ie x ptr in the literature different values of r have been reported for various situations and types of surface irrigation invokin... | [['a', 'fundamental', 'and', 'widely', 'applied', 'concept', 'used', 'to', 'study', 'surface', 'flow', 'processes', 'is', 'the', 'advancetime', 'curve', 'characterized', 'by', 'an', 'empirical', 'power', 'law', 'with', 'an', 'exponent', 'r', 'and', 'a', 'numerical', 'prefactor', 'p', 'ie', 'x', 'ptr', 'in', 'the', 'lit... | [-0.11205293745315896, 0.10731581270337277, -0.05299901359905608, 0.03525608919265393, 0.012896293215304375, -0.16735602896182966, 0.07127195937060513, 0.36698432995054203, -0.24036909624313316, -0.3102391720152436, 0.11999387030850929, -0.29382155525784653, -0.18190230801888108, 0.23944344444092935, -0.044375574730787... |
1,801.09183 | Toward an understanding of GRB prompt emission mechanism: II. Patterns
of peak energy evolution and their connection to spectral lags | The prompt emission phase of gamma-ray bursts (GRBs) exhibits two distinct
patterns of the peak-energy ($E_p$) evolution, i.e., time-resolved spectral
analyses of $\nu F_{\nu}$ spectra of broad pulses reveal (1) "hard-to-soft" and
(2) "flux-tracking" patterns of $E_p$ evolution in time, the physical origin of
which s... | astro-ph.HE | the prompt emission phase of gammaray bursts grbs exhibits two distinct patterns of the peakenergy e_p evolution ie timeresolved spectral analyses of nu f_nu spectra of broad pulses reveal 1 hardtosoft and 2 fluxtracking patterns of e_p evolution in time the physical origin of which still remains not well understood we... | [['the', 'prompt', 'emission', 'phase', 'of', 'gammaray', 'bursts', 'grbs', 'exhibits', 'two', 'distinct', 'patterns', 'of', 'the', 'peakenergy', 'e_p', 'evolution', 'ie', 'timeresolved', 'spectral', 'analyses', 'of', 'nu', 'f_nu', 'spectra', 'of', 'broad', 'pulses', 'reveal', '1', 'hardtosoft', 'and', '2', 'fluxtracki... | [-0.10783453480136104, 0.15715447418340595, -0.09723610919105206, 0.15171139872769213, -0.037559901759391875, -0.12521172192447433, 0.0203972813128153, 0.46310898855146837, -0.26358171384327295, -0.31680017418069084, 0.05182282720442589, -0.2842065050789132, -0.08689537393724228, 0.2026175733119045, 0.01488993128622518... |
1,801.09184 | Contextual Multi-Scale Region Convolutional 3D Network for Activity
Detection | Activity detection is a fundamental problem in computer vision. Detecting
activities of different temporal scales is particularly challenging. In this
paper, we propose the contextual multi-scale region convolutional 3D network
(CMS-RC3D) for activity detection. To deal with the inherent temporal scale
variability of... | cs.CV | activity detection is a fundamental problem in computer vision detecting activities of different temporal scales is particularly challenging in this paper we propose the contextual multiscale region convolutional 3d network cmsrc3d for activity detection to deal with the inherent temporal scale variability of activity ... | [['activity', 'detection', 'is', 'a', 'fundamental', 'problem', 'in', 'computer', 'vision', 'detecting', 'activities', 'of', 'different', 'temporal', 'scales', 'is', 'particularly', 'challenging', 'in', 'this', 'paper', 'we', 'propose', 'the', 'contextual', 'multiscale', 'region', 'convolutional', '3d', 'network', 'cms... | [-0.06490015354887141, 0.018900420975674372, -0.05019184342894108, 0.07629391101544403, -0.06867801384537442, -0.16772236578034225, -0.0425268570746477, 0.48508136069192687, -0.23227332575389972, -0.35472097237368483, 0.07747704830687471, -0.2996856873695182, -0.15883803703772598, 0.18169019652553628, -0.11196628099286... |
1,801.09185 | Marketing Analytics: Methods, Practice, Implementation, and Links to
Other Fields | Marketing analytics is a diverse field, with both academic researchers and
practitioners coming from a range of backgrounds including marketing, expert
systems, statistics, and operations research. This paper provides an
integrative review at the boundary of these areas. The aim is to give
researchers in the intellig... | stat.ML | marketing analytics is a diverse field with both academic researchers and practitioners coming from a range of backgrounds including marketing expert systems statistics and operations research this paper provides an integrative review at the boundary of these areas the aim is to give researchers in the intelligent and ... | [['marketing', 'analytics', 'is', 'a', 'diverse', 'field', 'with', 'both', 'academic', 'researchers', 'and', 'practitioners', 'coming', 'from', 'a', 'range', 'of', 'backgrounds', 'including', 'marketing', 'expert', 'systems', 'statistics', 'and', 'operations', 'research', 'this', 'paper', 'provides', 'an', 'integrative... | [-0.07421740593219345, 0.0541067988347381, -0.06414904585596617, 0.039213049693612737, -0.16033272975339338, -0.1621673249320446, 0.052810032864205436, 0.3848028771572753, -0.24471977784565382, -0.3375333956201802, 0.14149221196002165, -0.3465492841689945, -0.14632609750997352, 0.25160144223877184, -0.09317575419204427... |
1,801.09186 | Is interacting vacuum viable? | We study the asymptotic dynamics of dark energy as a mixture of pressureless
matter and an interacting vacuum component. We find that the only dynamics
compatible with current observational data favors an asymptotically vanishing
matter-vacuum energy interaction in a model where dark energy is simulated by a
generali... | gr-qc | we study the asymptotic dynamics of dark energy as a mixture of pressureless matter and an interacting vacuum component we find that the only dynamics compatible with current observational data favors an asymptotically vanishing mattervacuum energy interaction in a model where dark energy is simulated by a generalized ... | [['we', 'study', 'the', 'asymptotic', 'dynamics', 'of', 'dark', 'energy', 'as', 'a', 'mixture', 'of', 'pressureless', 'matter', 'and', 'an', 'interacting', 'vacuum', 'component', 'we', 'find', 'that', 'the', 'only', 'dynamics', 'compatible', 'with', 'current', 'observational', 'data', 'favors', 'an', 'asymptotically', ... | [-0.171336998004585, 0.16649497897585616, -0.14518132251596041, 0.12861080494408003, -0.048161270452992004, -0.14511113375534906, -0.061594200886639895, 0.2786371451528633, -0.2110989071136596, -0.3174742738917178, 0.021854749933232134, -0.2588917790711218, -0.011286799312003102, 0.10732308657858156, 0.0390103710997922... |
1,801.09187 | A model of Josephson Junctions on Boson Systems - Currents and Entropy
Production Rate - | Non-equilibrium steady states (NESS), in the sense of D. Ruelle, of Boson
systems with Bose--Einstein condensation (BEC) are investigated with the aid of
the C^*-algebraic method. The model consists of a quantum particle and several
bosonic reservoirs. We show that the mean entropy production rate is strictly
positiv... | math-ph math.MP | nonequilibrium steady states ness in the sense of d ruelle of boson systems with boseeinstein condensation bec are investigated with the aid of the calgebraic method the model consists of a quantum particle and several bosonic reservoirs we show that the mean entropy production rate is strictly positive independent of ... | [['nonequilibrium', 'steady', 'states', 'ness', 'in', 'the', 'sense', 'of', 'd', 'ruelle', 'of', 'boson', 'systems', 'with', 'boseeinstein', 'condensation', 'bec', 'are', 'investigated', 'with', 'the', 'aid', 'of', 'the', 'calgebraic', 'method', 'the', 'model', 'consists', 'of', 'a', 'quantum', 'particle', 'and', 'seve... | [-0.17344476169588544, 0.265450142289898, -0.08638950808700628, 0.03711523986336344, 0.09052745774161161, -0.1864449776788583, 0.04499798231167582, 0.317531392977732, -0.21373698864949914, -0.20294360743790138, -0.0006740258611943118, -0.32704863866518546, -0.06095319606006009, 0.18006136269087153, 0.030284927442397285... |
1,801.09188 | On the quasisymmetric minimality of homogeneous perfect sets | Z. Wen and J. Wu introduced the notion of homogeneous perfect sets as a
generalization of Cantor type sets and determined their exact Hausdorff
dimension based on the length of their fundamental intervals and the gaps
between them. In this paper, we considered the minimality of the homogeneous
perfect sets with Hausd... | math.MG | z wen and j wu introduced the notion of homogeneous perfect sets as a generalization of cantor type sets and determined their exact hausdorff dimension based on the length of their fundamental intervals and the gaps between them in this paper we considered the minimality of the homogeneous perfect sets with hausdorff d... | [['z', 'wen', 'and', 'j', 'wu', 'introduced', 'the', 'notion', 'of', 'homogeneous', 'perfect', 'sets', 'as', 'a', 'generalization', 'of', 'cantor', 'type', 'sets', 'and', 'determined', 'their', 'exact', 'hausdorff', 'dimension', 'based', 'on', 'the', 'length', 'of', 'their', 'fundamental', 'intervals', 'and', 'the', 'g... | [-0.15407014412630815, 0.11866296028892975, -0.025311058794613928, 0.10774735767881793, -0.02539289365449804, -0.1267922776969499, 0.0814894097729848, 0.336391325959994, -0.28494551006588154, -0.19937672353262315, 0.09121250219141075, -0.2684281956171617, -0.11971071086736629, 0.1826081025064923, -0.1176578549639089, 0... |
1,801.09189 | Generalized Points-to Graphs: A New Abstraction of Memory in the
Presence of Pointers | Flow- and context-sensitive points-to analysis is difficult to scale; for
top-down approaches, the problem centers on repeated analysis of the same
procedure; for bottom-up approaches, the abstractions used to represent
procedure summaries have not scaled while preserving precision.
We propose a novel abstraction c... | cs.PL | flow and contextsensitive pointsto analysis is difficult to scale for topdown approaches the problem centers on repeated analysis of the same procedure for bottomup approaches the abstractions used to represent procedure summaries have not scaled while preserving precision we propose a novel abstraction called the gene... | [['flow', 'and', 'contextsensitive', 'pointsto', 'analysis', 'is', 'difficult', 'to', 'scale', 'for', 'topdown', 'approaches', 'the', 'problem', 'centers', 'on', 'repeated', 'analysis', 'of', 'the', 'same', 'procedure', 'for', 'bottomup', 'approaches', 'the', 'abstractions', 'used', 'to', 'represent', 'procedure', 'sum... | [-0.1101997122168541, 0.047249675251268705, -0.09640095437796725, 0.06627615067399809, -0.1307464074190767, -0.14356390908971184, 0.10965497804219743, 0.3683214193461921, -0.3053845097673446, -0.3727033497883984, 0.11897948530424371, -0.24919481816537942, -0.08851225004000894, 0.18005495889161974, -0.117520917898815, 0... |
1,801.0919 | A Stable Weak Galerkin Finite Element Method for Stokes Problem | We study the weak Galerkin finite element method for Stokes problem. A new
weak Galerkin finite element velocity-pressure space pair is presented which
satisfies the discrete inf-sup condition. Based on this space pair, we
establish a stable weak Galerkin approximation scheme without adding any
stability term or pena... | math.NA | we study the weak galerkin finite element method for stokes problem a new weak galerkin finite element velocitypressure space pair is presented which satisfies the discrete infsup condition based on this space pair we establish a stable weak galerkin approximation scheme without adding any stability term or penalty ter... | [['we', 'study', 'the', 'weak', 'galerkin', 'finite', 'element', 'method', 'for', 'stokes', 'problem', 'a', 'new', 'weak', 'galerkin', 'finite', 'element', 'velocitypressure', 'space', 'pair', 'is', 'presented', 'which', 'satisfies', 'the', 'discrete', 'infsup', 'condition', 'based', 'on', 'this', 'space', 'pair', 'we'... | [-0.13154390534489518, 0.025462836479871638, -0.11634397416168617, 0.08154244905906832, -0.12246536919459079, -0.1650503972131345, 0.08802320337336925, 0.3736064110319906, -0.332482464039155, -0.19404577559584546, 0.14172644797427994, -0.22516440221160236, -0.06946986591922016, 0.16019918027126956, -0.04899950656625959... |
1,801.09191 | On projective varieties with strictly nef tangent bundles | In this paper, we study smooth complex projective varieties $X$ such that
some exterior power $\bigwedge^r T_X$ of the tangent bundle is strictly nef. We
prove that such varieties are rationally connected. We also classify the
following two cases. If $T_X$ is strictly nef, then $X$ isomorphic to the
projective space ... | math.AG math.DG | in this paper we study smooth complex projective varieties x such that some exterior power bigwedger t_x of the tangent bundle is strictly nef we prove that such varieties are rationally connected we also classify the following two cases if t_x is strictly nef then x isomorphic to the projective space mathrmpn if bigwe... | [['in', 'this', 'paper', 'we', 'study', 'smooth', 'complex', 'projective', 'varieties', 'x', 'such', 'that', 'some', 'exterior', 'power', 'bigwedger', 't_x', 'of', 'the', 'tangent', 'bundle', 'is', 'strictly', 'nef', 'we', 'prove', 'that', 'such', 'varieties', 'are', 'rationally', 'connected', 'we', 'also', 'classify',... | [-0.1920880584123855, 0.09147891653184262, -0.048130608532422535, 0.05953685467183176, -0.11385700191345273, -0.23709376499755308, -0.04525371017290228, 0.4501697499718931, -0.36744758249389836, -0.03321873797621164, 0.1319392232415137, -0.33088375753464383, -0.17688330917735584, 0.17162597349831937, -0.185493179933271... |
1,801.09192 | Bloch Oscillations in Chains of Artificial Atoms Dressed with Photons | We present the model of one-dimensional chain of two-level artificial atoms
driven with dc field and quantum light simultaneously in strong coupling
regime. The interaction of atoms with light leads to entanglement of electron
and photon states (dressing of the atoms). The driving via dc field leads to
the Bloch osci... | quant-ph | we present the model of onedimensional chain of twolevel artificial atoms driven with dc field and quantum light simultaneously in strong coupling regime the interaction of atoms with light leads to entanglement of electron and photon states dressing of the atoms the driving via dc field leads to the bloch oscillations... | [['we', 'present', 'the', 'model', 'of', 'onedimensional', 'chain', 'of', 'twolevel', 'artificial', 'atoms', 'driven', 'with', 'dc', 'field', 'and', 'quantum', 'light', 'simultaneously', 'in', 'strong', 'coupling', 'regime', 'the', 'interaction', 'of', 'atoms', 'with', 'light', 'leads', 'to', 'entanglement', 'of', 'ele... | [-0.15215069670979944, 0.2248107487152299, -0.04507170742677556, 0.026109628345308257, -0.014012907414649755, -0.17513412367394668, 0.07628529653065617, 0.38483421439778503, -0.2487638225715797, -0.28999773196218004, -0.003610463221004959, -0.28026437369062784, -0.1078165256659011, 0.25140624914527476, 0.03715659957181... |
1,801.09193 | A statistical inference approach to structural reconstruction of complex
networks from binary time series | Complex networks hosting binary-state dynamics arise in a variety of
contexts. In spite of previous works, to fully reconstruct the network
structure from observed binary data remains to be challenging. We articulate a
statistical inference based approach to this problem. In particular, exploiting
the expectation-max... | physics.soc-ph | complex networks hosting binarystate dynamics arise in a variety of contexts in spite of previous works to fully reconstruct the network structure from observed binary data remains to be challenging we articulate a statistical inference based approach to this problem in particular exploiting the expectationmaximization... | [['complex', 'networks', 'hosting', 'binarystate', 'dynamics', 'arise', 'in', 'a', 'variety', 'of', 'contexts', 'in', 'spite', 'of', 'previous', 'works', 'to', 'fully', 'reconstruct', 'the', 'network', 'structure', 'from', 'observed', 'binary', 'data', 'remains', 'to', 'be', 'challenging', 'we', 'articulate', 'a', 'sta... | [-0.12409040381813921, 0.024085195092896066, -0.08510277209258298, 0.07135389158913934, -0.10392514155132741, -0.12086124721710093, 0.07008098735496765, 0.37445000897093517, -0.2860666513761006, -0.33942784219525934, 0.09607304295967901, -0.21395029188701656, -0.19863066658400363, 0.1884799710872424, -0.048229044180636... |
1,801.09194 | A Gale-Berlekamp permutation-switching problem in higher dimensions | Let an $n\times n$ array $\left( a_{ij}\right) $ of lights be given, each
either on (when $a_{ij}=1$) or off (when $a_{ij}=-1$). For each row and each
column there is a switch so that if the switch is pulled ($x_{i}=-1$ for row
$i$ and $y_{j}=-1$ for column $j$) all of the lights in that line are switched:
on to off ... | math.CO | let an ntimes n array left a_ijright of lights be given each either on when a_ij1 or off when a_ij1 for each row and each column there is a switch so that if the switch is pulled x_i1 for row i and y_j1 for column j all of the lights in that line are switched on to off or off to on the unbalancing lights problem galebe... | [['let', 'an', 'ntimes', 'n', 'array', 'left', 'a_ijright', 'of', 'lights', 'be', 'given', 'each', 'either', 'on', 'when', 'a_ij1', 'or', 'off', 'when', 'a_ij1', 'for', 'each', 'row', 'and', 'each', 'column', 'there', 'is', 'a', 'switch', 'so', 'that', 'if', 'the', 'switch', 'is', 'pulled', 'x_i1', 'for', 'row', 'i', '... | [-0.12128537912119894, 0.16603995132042676, -0.02465506585592285, -0.021068124048550553, -0.04301689531000212, -0.22487842928657822, 0.1255340129335193, 0.4210951081774336, -0.2716590954743801, -0.2293704819092725, 0.13199164566430363, -0.328807657426025, -0.08816356309739119, 0.15967659300014853, -0.06184849649311063,... |
1,801.09195 | Improved Training of Generative Adversarial Networks Using
Representative Features | Despite the success of generative adversarial networks (GANs) for image
generation, the trade-off between visual quality and image diversity remains a
significant issue. This paper achieves both aims simultaneously by improving
the stability of training GANs. The key idea of the proposed approach is to
implicitly reg... | cs.CV | despite the success of generative adversarial networks gans for image generation the tradeoff between visual quality and image diversity remains a significant issue this paper achieves both aims simultaneously by improving the stability of training gans the key idea of the proposed approach is to implicitly regularize ... | [['despite', 'the', 'success', 'of', 'generative', 'adversarial', 'networks', 'gans', 'for', 'image', 'generation', 'the', 'tradeoff', 'between', 'visual', 'quality', 'and', 'image', 'diversity', 'remains', 'a', 'significant', 'issue', 'this', 'paper', 'achieves', 'both', 'aims', 'simultaneously', 'by', 'improving', 't... | [0.010924751304132356, -0.040538488520365776, -0.08008191359201164, 0.11723309369302694, -0.09661638117077845, -0.13823796784731024, 0.031635288276998894, 0.44425381396925356, -0.3091397956295898, -0.32216439867448626, 0.003692927823232656, -0.30075391379509575, -0.19847799795609194, 0.13068116383598835, -0.18084580515... |
1,801.09196 | Photon-added and photon-subtracted coherent states on a sphere | In this paper, we construct the $m$-photon-added and $m$-photon-subtracted
coherent states on a sphere. These states are shown to satisfy the usual
conditions of continuity in the label, normalizability and the resolution of
identity. The preparation of the constructed states, as the states of radiation
field is cons... | quant-ph | in this paper we construct the mphotonadded and mphotonsubtracted coherent states on a sphere these states are shown to satisfy the usual conditions of continuity in the label normalizability and the resolution of identity the preparation of the constructed states as the states of radiation field is considered we exami... | [['in', 'this', 'paper', 'we', 'construct', 'the', 'mphotonadded', 'and', 'mphotonsubtracted', 'coherent', 'states', 'on', 'a', 'sphere', 'these', 'states', 'are', 'shown', 'to', 'satisfy', 'the', 'usual', 'conditions', 'of', 'continuity', 'in', 'the', 'label', 'normalizability', 'and', 'the', 'resolution', 'of', 'iden... | [-0.14523130437616297, 0.2271702372266494, -0.07903461264747118, 0.07830761422155774, 0.034605681209844384, -0.09996097170126934, 0.04087938303443176, 0.33830183383543044, -0.23721215405870075, -0.2635636865646423, 0.06836698170930806, -0.2756705736974254, -0.0887987092670907, 0.18770906008770302, -0.062385842572742455... |
1,801.09197 | Algorithmic Linearly Constrained Gaussian Processes | We algorithmically construct multi-output Gaussian process priors which
satisfy linear differential equations. Our approach attempts to parametrize all
solutions of the equations using Gr\"obner bases. If successful, a push forward
Gaussian process along the paramerization is the desired prior. We consider
several ex... | stat.ML cs.LG cs.SC math.AC | we algorithmically construct multioutput gaussian process priors which satisfy linear differential equations our approach attempts to parametrize all solutions of the equations using grobner bases if successful a push forward gaussian process along the paramerization is the desired prior we consider several examples fr... | [['we', 'algorithmically', 'construct', 'multioutput', 'gaussian', 'process', 'priors', 'which', 'satisfy', 'linear', 'differential', 'equations', 'our', 'approach', 'attempts', 'to', 'parametrize', 'all', 'solutions', 'of', 'the', 'equations', 'using', 'grobner', 'bases', 'if', 'successful', 'a', 'push', 'forward', 'g... | [-0.07700835565725962, 0.02336859281330059, -0.10599220980579654, 0.049700081333139676, -0.17506730708604057, -0.19289105076342822, 0.019095122156043847, 0.34568250705798464, -0.351062621542563, -0.2652652805298567, 0.10051478661441554, -0.24873628485326965, -0.1821637651976198, 0.19021537059297164, -0.0760572664191325... |
1,801.09198 | Flow equivalence of topological Markov shifts and Ruelle algebras | We study discrete flow equivalence of two-sided topological Markov shifts by
using extended Ruelle algebras. We characterize flow equivalence of two-sided
topological Markov shifts in terms of conjugacy of certain actions weighted by
ceiling functions of two-dimensional torus on the stabilized extended Ruelle
algebra... | math.OA math.DS | we study discrete flow equivalence of twosided topological markov shifts by using extended ruelle algebras we characterize flow equivalence of twosided topological markov shifts in terms of conjugacy of certain actions weighted by ceiling functions of twodimensional torus on the stabilized extended ruelle algebras for ... | [['we', 'study', 'discrete', 'flow', 'equivalence', 'of', 'twosided', 'topological', 'markov', 'shifts', 'by', 'using', 'extended', 'ruelle', 'algebras', 'we', 'characterize', 'flow', 'equivalence', 'of', 'twosided', 'topological', 'markov', 'shifts', 'in', 'terms', 'of', 'conjugacy', 'of', 'certain', 'actions', 'weigh... | [-0.14735039341030642, 0.21677175571676344, -0.04052469906552384, 0.15275481409238031, -0.07295979303307831, -0.1276940218716239, 0.056557512221237026, 0.4285329480965932, -0.3770248219758893, -0.12922132100599507, 0.1455593314288611, -0.1943874201485111, -0.11938766048600276, 0.1811718557146378, -0.12364721352544923, ... |
1,801.09199 | Photoelectron angular distribution from the high-order above-threshold
ionization process in IR+XUV two-color laser fields | High-order above-threshold ionization (HATI) spectrum in IR+XUV two-color
laser fields has been investigated. We found that the quantum features
corresponding to the absorption of the XUV photon is well illustrated by a
peculiar dip structure in the second plateau of the HATI spectrum. By the
channel analysis, we sho... | physics.atom-ph | highorder abovethreshold ionization hati spectrum in irxuv twocolor laser fields has been investigated we found that the quantum features corresponding to the absorption of the xuv photon is well illustrated by a peculiar dip structure in the second plateau of the hati spectrum by the channel analysis we show that the ... | [['highorder', 'abovethreshold', 'ionization', 'hati', 'spectrum', 'in', 'irxuv', 'twocolor', 'laser', 'fields', 'has', 'been', 'investigated', 'we', 'found', 'that', 'the', 'quantum', 'features', 'corresponding', 'to', 'the', 'absorption', 'of', 'the', 'xuv', 'photon', 'is', 'well', 'illustrated', 'by', 'a', 'peculiar... | [-0.10489447287129447, 0.15589395674371365, -0.10312830473366069, 0.07256911131452383, 0.005633597688022304, -0.0868676263729439, 0.02074302460644693, 0.3969709998492231, -0.2724448857943522, -0.29574536482858305, 0.00857856581647467, -0.29562959225380164, -0.06003049216457309, 0.16530118863730825, -0.00679317828800708... |
1,801.092 | Noise-induced Mixing and Multimodality in Reaction Networks | We analyze a class of chemical reaction networks under mass-action kinetics
and involving multiple time-scales, whose deterministic and stochastic models
display qualitative differences. The networks are inspired by gene-regulatory
networks, and consist of a slow-subnetwork, describing conversions among the
different... | q-bio.MN | we analyze a class of chemical reaction networks under massaction kinetics and involving multiple timescales whose deterministic and stochastic models display qualitative differences the networks are inspired by generegulatory networks and consist of a slowsubnetwork describing conversions among the different gene stat... | [['we', 'analyze', 'a', 'class', 'of', 'chemical', 'reaction', 'networks', 'under', 'massaction', 'kinetics', 'and', 'involving', 'multiple', 'timescales', 'whose', 'deterministic', 'and', 'stochastic', 'models', 'display', 'qualitative', 'differences', 'the', 'networks', 'are', 'inspired', 'by', 'generegulatory', 'net... | [-0.1299472543413349, 0.15216684050232887, -0.060220902106901696, 0.11788784201760866, 0.013283931334464722, -0.10873211738541849, 0.038501189729001066, 0.32392340343547604, -0.3132415991156898, -0.26086138660241276, 0.05538541308567502, -0.26971398441963, -0.24858711594843294, 0.18582716219331305, -0.02712166310811881... |
1,801.09201 | Quantum criticality at the superconductor insulator transition probed by
the Nernst effect | The superconductor-insulator transition (SIT) is an excellent example for a
quantum phase transition at zero temperature, dominated by quantum
fluctuations. These are expected to be very prominent close to the quantum
critical point. So far most of the experimental study of the SIT has
concentrated on transport prope... | cond-mat.supr-con | the superconductorinsulator transition sit is an excellent example for a quantum phase transition at zero temperature dominated by quantum fluctuations these are expected to be very prominent close to the quantum critical point so far most of the experimental study of the sit has concentrated on transport properties an... | [['the', 'superconductorinsulator', 'transition', 'sit', 'is', 'an', 'excellent', 'example', 'for', 'a', 'quantum', 'phase', 'transition', 'at', 'zero', 'temperature', 'dominated', 'by', 'quantum', 'fluctuations', 'these', 'are', 'expected', 'to', 'be', 'very', 'prominent', 'close', 'to', 'the', 'quantum', 'critical', ... | [-0.1240541532493786, 0.21109217033496253, -0.08952963851204902, 0.027646900280709406, -0.005612197161249861, -0.18316520144060783, 0.07809668492399068, 0.3198331730452658, -0.2533143456321287, -0.2502278924407162, 0.062278694352658585, -0.3840004217055951, -0.14429521787713265, 0.19578072817075842, 0.05124156370196910... |
1,801.09202 | Nucleon Properties in the Polyakov Quark Meson Model | We study the nucleon as a nontopological soliton in a quark medium as well as
in a nucleon medium in terms of the Polyakov quark meson (PQM) model with two
flavors at finite temperature and density. The constituent quark masses
evolving with the temperature at various baryon chemical potentials are
calculated and the... | hep-ph | we study the nucleon as a nontopological soliton in a quark medium as well as in a nucleon medium in terms of the polyakov quark meson pqm model with two flavors at finite temperature and density the constituent quark masses evolving with the temperature at various baryon chemical potentials are calculated and the equa... | [['we', 'study', 'the', 'nucleon', 'as', 'a', 'nontopological', 'soliton', 'in', 'a', 'quark', 'medium', 'as', 'well', 'as', 'in', 'a', 'nucleon', 'medium', 'in', 'terms', 'of', 'the', 'polyakov', 'quark', 'meson', 'pqm', 'model', 'with', 'two', 'flavors', 'at', 'finite', 'temperature', 'and', 'density', 'the', 'consti... | [-0.0912553029649182, 0.2879247029509383, -0.09997484728054547, 0.07526710867245834, 0.0023324189016095073, -0.058909252831545564, 0.0798742770505791, 0.354240989618337, -0.17131489988611037, -0.24191894450350038, -0.008227986371346207, -0.30803375844079167, -0.011896224711576838, 0.03696782378577141, 0.073470697838573... |
1,801.09203 | Fixed points of Sturmian morphisms and their derivated words | Any infinite uniformly recurrent word ${\bf u}$ can be written as
concatenation of a finite number of return words to a chosen prefix $w$ of
${\bf u}$. Ordering of the return words to $w$ in this concatenation is coded
by derivated word $d_{\bf u}(w)$. In 1998, Durand proved that a fixed point
${\bf u}$ of a primitiv... | math.CO | any infinite uniformly recurrent word bf u can be written as concatenation of a finite number of return words to a chosen prefix w of bf u ordering of the return words to w in this concatenation is coded by derivated word d_bf uw in 1998 durand proved that a fixed point bf u of a primitive morphism has only finitely ma... | [['any', 'infinite', 'uniformly', 'recurrent', 'word', 'bf', 'u', 'can', 'be', 'written', 'as', 'concatenation', 'of', 'a', 'finite', 'number', 'of', 'return', 'words', 'to', 'a', 'chosen', 'prefix', 'w', 'of', 'bf', 'u', 'ordering', 'of', 'the', 'return', 'words', 'to', 'w', 'in', 'this', 'concatenation', 'is', 'coded... | [-0.19228927365038545, 0.12127925130066265, -0.03511939860271433, 0.04056908639523989, -0.09814550511789723, -0.19308828967981614, 0.1526004715822637, 0.3697445119301287, -0.42502423248325405, -0.16501872571400153, 0.016107545740221843, -0.3238818242859382, -0.07982247809951122, 0.16303155018921153, -0.1443725191952231... |
1,801.09204 | Fast Standing Modes in Transversely Nonuniform Solar Coronal Slabs:
Effects of a Finite Plasma Beta | We examine the dispersive properties of linear fast standing modes in
transversely nonuniform solar coronal slabs with finite gas pressure, or,
equivalently, finite plasma beta. We derive a generic dispersion relation
governing fast waves in coronal slabs for which the continuous transverse
distributions of the physi... | astro-ph.SR | we examine the dispersive properties of linear fast standing modes in transversely nonuniform solar coronal slabs with finite gas pressure or equivalently finite plasma beta we derive a generic dispersion relation governing fast waves in coronal slabs for which the continuous transverse distributions of the physical pa... | [['we', 'examine', 'the', 'dispersive', 'properties', 'of', 'linear', 'fast', 'standing', 'modes', 'in', 'transversely', 'nonuniform', 'solar', 'coronal', 'slabs', 'with', 'finite', 'gas', 'pressure', 'or', 'equivalently', 'finite', 'plasma', 'beta', 'we', 'derive', 'a', 'generic', 'dispersion', 'relation', 'governing'... | [-0.1362685174174463, 0.25585053119623385, -0.029508431052872493, 0.07697005881128638, -0.0617233173856836, -0.11836340227882512, -0.010340392971249177, 0.4074506216372053, -0.25698700670931324, -0.25118796573025154, 0.059962006422762865, -0.25177151327144787, -0.047587105904738254, 0.2304384590251677, 0.05144481453117... |
1,801.09205 | Nobeyama 45m Cygnus-X CO survey I: photodissociation of molecules
revealed by the unbiased large-scale CN and C$^{18}$O maps | We present an unbiased large-scale (9 deg$^2$) CN ($N$=1-0) and C$^{18}$O
($J$=1-0) survey of Cygnus-X conducted with the Nobeyama 45m Cygnus-X CO
survey. CN and C$^{18}$O are detected in various objects towards the Cygnus-X
North and South (e.g., DR17, DR18, DR21, DR22, DR23, and W75N). We find that
CN/C$^{18}$O int... | astro-ph.GA | we present an unbiased largescale 9 deg2 cn n10 and c18o j10 survey of cygnusx conducted with the nobeyama 45m cygnusx co survey cn and c18o are detected in various objects towards the cygnusx north and south eg dr17 dr18 dr21 dr22 dr23 and w75n we find that cnc18o integrated intensity ratios are systematically differe... | [['we', 'present', 'an', 'unbiased', 'largescale', '9', 'deg2', 'cn', 'n10', 'and', 'c18o', 'j10', 'survey', 'of', 'cygnusx', 'conducted', 'with', 'the', 'nobeyama', '45m', 'cygnusx', 'co', 'survey', 'cn', 'and', 'c18o', 'are', 'detected', 'in', 'various', 'objects', 'towards', 'the', 'cygnusx', 'north', 'and', 'south'... | [-0.061841304492592425, 0.11158694661685035, 0.021395805775635428, 0.057370147627004264, -0.008582831618932451, -0.03199825151944412, 0.03290465489701162, 0.502054272001827, -0.1475050737385868, -0.3112741406740887, 0.034077290548374516, -0.2880130894009671, -0.08934862702153623, 0.12588354109411504, -0.002312352389436... |
1,801.09206 | Finite Groups Having Nonnormal T.I. Subgroups | In the present paper, the structure of a finite group $G$ having a nonnormal
T.I. subgroup $H$ which is also a Hall $\pi$-subgroup is studied. As a
generalization of a result due to Gow, we prove that $H$ is a Frobenius
complement whenever $G$ is $\pi$-separable. This is achieved by obtaining the
fact that Hall T.I. ... | math.GR | in the present paper the structure of a finite group g having a nonnormal ti subgroup h which is also a hall pisubgroup is studied as a generalization of a result due to gow we prove that h is a frobenius complement whenever g is piseparable this is achieved by obtaining the fact that hall ti subgroups are conjugate in... | [['in', 'the', 'present', 'paper', 'the', 'structure', 'of', 'a', 'finite', 'group', 'g', 'having', 'a', 'nonnormal', 'ti', 'subgroup', 'h', 'which', 'is', 'also', 'a', 'hall', 'pisubgroup', 'is', 'studied', 'as', 'a', 'generalization', 'of', 'a', 'result', 'due', 'to', 'gow', 'we', 'prove', 'that', 'h', 'is', 'a', 'fr... | [-0.16662273937954178, 0.11225394621680054, -0.1314090604693452, 0.026484737585334085, -0.10136734845140312, -0.13360062126023106, 0.03756357170494061, 0.32097080731882327, -0.29605772192413105, -0.22791540938653523, 0.08426510824827783, -0.24089660198439525, -0.1521866405972197, 0.2134166507498373, -0.1574096066547156... |
1,801.09207 | Interaction of a hydrogenlike ion with a planar topological insulator | An electric charge near the surface of a topological insulator (TI) induces
an image magnetic monopole. Here we study the spectra of hydrogenlike ions near
the surface of a planar TI, taking into account the modifications which arise
due to the presence of the image monopole magnetic fields. In fact, the atom-TI
inte... | quant-ph cond-mat.other hep-th | an electric charge near the surface of a topological insulator ti induces an image magnetic monopole here we study the spectra of hydrogenlike ions near the surface of a planar ti taking into account the modifications which arise due to the presence of the image monopole magnetic fields in fact the atomti interaction p... | [['an', 'electric', 'charge', 'near', 'the', 'surface', 'of', 'a', 'topological', 'insulator', 'ti', 'induces', 'an', 'image', 'magnetic', 'monopole', 'here', 'we', 'study', 'the', 'spectra', 'of', 'hydrogenlike', 'ions', 'near', 'the', 'surface', 'of', 'a', 'planar', 'ti', 'taking', 'into', 'account', 'the', 'modifica... | [-0.17563281204167971, 0.2016958088382928, -0.028554078709224568, 0.06448995624668896, -0.024687825873329797, -0.09565931354813716, 0.03182329117895707, 0.37052133116213715, -0.2467547839260934, -0.31549756647471117, -0.03966677280156599, -0.30978914741974545, -0.0871664706590202, 0.1378853992339881, 0.0344642725033576... |
1,801.09208 | Constant-roll tachyon inflation and observational constraints | For the constant-roll tachyon inflation, we derive the analytical expressions
for the scalar and tensor power spectra, the scalar and tensor spectral tilts
and the tensor to scalar ratio up to the first order by using the method of
Bessel function approximation. The derived $n_s-r$ results for the
constant-roll infla... | gr-qc astro-ph.CO hep-th | for the constantroll tachyon inflation we derive the analytical expressions for the scalar and tensor power spectra the scalar and tensor spectral tilts and the tensor to scalar ratio up to the first order by using the method of bessel function approximation the derived n_sr results for the constantroll inflation are a... | [['for', 'the', 'constantroll', 'tachyon', 'inflation', 'we', 'derive', 'the', 'analytical', 'expressions', 'for', 'the', 'scalar', 'and', 'tensor', 'power', 'spectra', 'the', 'scalar', 'and', 'tensor', 'spectral', 'tilts', 'and', 'the', 'tensor', 'to', 'scalar', 'ratio', 'up', 'to', 'the', 'first', 'order', 'by', 'usi... | [-0.10439510426503863, 0.15617494463445025, -0.11958272765053714, 0.12825369773348397, -0.11195613273439255, -0.15892629077697687, -0.08297326693192442, 0.31189073144676205, -0.18941966035809527, -0.2732749420634292, 0.10077331910662829, -0.21969711279219134, -0.15775902472694028, 0.14051953135702283, 0.024187942303003... |
1,801.09209 | Nash inequality for Diffusion Processes Associated with Dirichlet
Distributions | For any $N\ge 2$ and $\alpha=(\alpha_1,\cdots, \alpha_{N+1})\in
(0,\infty)^{N+1}$, let $\mu^{(N)}_{\alpha}$ be the Dirichlet distribution with
parameter $\alpha$ on the set $\Delta^{ (N)}:= \{ x \in [0,1]^N:\ \sum_{1\le
i\le N}x_i \le 1 \}.$ The multivariate Dirichlet diffusion is associated with
the Dirichlet form
... | math.PR | for any nge 2 and alphaalpha_1cdots alpha_n1in 0inftyn1 let mun_alpha be the dirichlet distribution with parameter alpha on the set delta n x in 01n sum_1le ile nx_i le 1 the multivariate dirichlet diffusion is associated with the dirichlet form scr e_alphanff sum_n1n int_ deltan bigg1sum_1le ile nx_ibigg x_npartial_n ... | [['for', 'any', 'nge', '2', 'and', 'alphaalpha_1cdots', 'alpha_n1in', '0inftyn1', 'let', 'mun_alpha', 'be', 'the', 'dirichlet', 'distribution', 'with', 'parameter', 'alpha', 'on', 'the', 'set', 'delta', 'n', 'x', 'in', '01n', 'sum_1le', 'ile', 'nx_i', 'le', '1', 'the', 'multivariate', 'dirichlet', 'diffusion', 'is', 'a... | [-0.15430620623531646, 0.1201769727289427, 0.01947050203194784, 0.0012826237524837104, -0.0004959038708397408, -0.27591304057613786, 0.02402697811287242, 0.32951849848800097, -0.29767269540347696, -0.16954297088470655, 0.061111544252891746, -0.3706485808049281, -0.02649621548342336, 0.09469268662067726, -0.054190446929... |
1,801.0921 | Selective highly charged ions as the prospective optical clock
candidates with quality factors larger than $10^{15}$ | We propose here a few selective highly charged ions (HCIs), namely Ni$^{12+}$
and Cu$^{13+}$, Pd$^{12+}$ and Ag$^{13+}$, that not only promise to be very
high accurate optical clocks below $10^{-19}$ uncertainties, but also offer
quality factors larger than $10^{15}$ and yet possess simple atomic structures
for the e... | physics.atom-ph | we propose here a few selective highly charged ions hcis namely ni12 and cu13 pd12 and ag13 that not only promise to be very high accurate optical clocks below 1019 uncertainties but also offer quality factors larger than 1015 and yet possess simple atomic structures for the experimental setup moreover these ions have ... | [['we', 'propose', 'here', 'a', 'few', 'selective', 'highly', 'charged', 'ions', 'hcis', 'namely', 'ni12', 'and', 'cu13', 'pd12', 'and', 'ag13', 'that', 'not', 'only', 'promise', 'to', 'be', 'very', 'high', 'accurate', 'optical', 'clocks', 'below', '1019', 'uncertainties', 'but', 'also', 'offer', 'quality', 'factors', ... | [-0.06796750124000633, 0.21652074833509688, 0.03125806182118443, 0.07295876582308362, -0.007828800030983985, -0.1483723111334257, 0.05722956641111523, 0.45726245287805795, -0.20334137363824994, -0.3668387432117015, 0.04412166594023195, -0.2682173878109703, -0.05101564519573003, 0.2355286827990009, -0.000396989654594411... |
1,801.09211 | Exact expansions of Hankel transforms and related integrals | The Hankel transform H_n[f(x)](q) = int_0^infinity xf(x)J_n(qx)dx is studied
for integer n>=-1 and positive parameter q. It is proved that the Hankel
transform is given by uniformly and absolutely convergent series in reciprocal
powers of q, provided special conditions on the function f(x) and its
derivatives are imp... | math.CA | the hankel transform h_nfxq int_0infinity xfxj_nqxdx is studied for integer n1 and positive parameter q it is proved that the hankel transform is given by uniformly and absolutely convergent series in reciprocal powers of q provided special conditions on the function fx and its derivatives are imposed it is necessary t... | [['the', 'hankel', 'transform', 'h_nfxq', 'int_0infinity', 'xfxj_nqxdx', 'is', 'studied', 'for', 'integer', 'n1', 'and', 'positive', 'parameter', 'q', 'it', 'is', 'proved', 'that', 'the', 'hankel', 'transform', 'is', 'given', 'by', 'uniformly', 'and', 'absolutely', 'convergent', 'series', 'in', 'reciprocal', 'powers', ... | [-0.15645250156133747, 0.10591059402666159, -0.08836518908954329, 0.0955388302061086, -0.08899678725024893, -0.14588720196237168, -0.004490720089072258, 0.3394716871798866, -0.2608359729664193, -0.18153727129101754, 0.17341708708037104, -0.28654944818311684, -0.16539817312732338, 0.2238587550404999, -0.0504153070463669... |
1,801.09212 | BOPS, Not FLOPS! A New Metric and Roofline Performance Model For
Datacenter Computing | For emerging datacenter (in short, DC) workloads, such as online Internet
services or offline data analytics, how to evaluate the upper bound performance
and provide apple-to-apple comparisons are fundamental problems. To this end, a
unified computation-centric metric is an essential requirement. As the most
importan... | cs.PF | for emerging datacenter in short dc workloads such as online internet services or offline data analytics how to evaluate the upper bound performance and provide appletoapple comparisons are fundamental problems to this end a unified computationcentric metric is an essential requirement as the most important computation... | [['for', 'emerging', 'datacenter', 'in', 'short', 'dc', 'workloads', 'such', 'as', 'online', 'internet', 'services', 'or', 'offline', 'data', 'analytics', 'how', 'to', 'evaluate', 'the', 'upper', 'bound', 'performance', 'and', 'provide', 'appletoapple', 'comparisons', 'are', 'fundamental', 'problems', 'to', 'this', 'en... | [-0.17965088021018416, 0.010113829887872116, -0.06507292637726993, 0.04902093148507931, -0.051521405718018505, -0.149036488900331, 0.12183255394128092, 0.3969058949617563, -0.2140826795085875, -0.38172791235426323, 0.11932827690277738, -0.26268366337522653, -0.13103295032327983, 0.2867226429945783, -0.07735805854705784... |
1,801.09213 | Fr\'echet differentiability in Fr\'echet spaces, and differential
equations with unbounded variable delay | We introduce and discuss Fr\'echet differentiability for maps between
Fr\'echet spaces. For delay differential equations $x'(t)=f(x_t)$ we construct
a continuous semiflow of continuously differentiable solution operators
$x_0\mapsto x_t$, $t\ge0$, on submanifolds of the Fr\'echet space
$C^1((-\infty,0],\mathbb{R}^n)$... | math.DS | we introduce and discuss frechet differentiability for maps between frechet spaces for delay differential equations xtfx_t we construct a continuous semiflow of continuously differentiable solution operators x_0mapsto x_t tge0 on submanifolds of the frechet space c1infty0mathbbrn and establish local invariant manifolds... | [['we', 'introduce', 'and', 'discuss', 'frechet', 'differentiability', 'for', 'maps', 'between', 'frechet', 'spaces', 'for', 'delay', 'differential', 'equations', 'xtfx_t', 'we', 'construct', 'a', 'continuous', 'semiflow', 'of', 'continuously', 'differentiable', 'solution', 'operators', 'x_0mapsto', 'x_t', 'tge0', 'on'... | [-0.14414329973090897, 0.05469284317913955, -0.07544856946283983, 0.14870169659350382, -0.0732357705966964, -0.12606286269344263, 0.020763053700832996, 0.4321248280042309, -0.3724439039952674, -0.14956556100366733, 0.1453584739622676, -0.2727826919457954, -0.1491332724532586, 0.1917194325745232, -0.17315899295006262, 0... |
1,801.09214 | Delay differential equations with differentiable solution operators on
open domains in $C((-\infty,0],\mathbb{R}^n)$, and processes for Volterra
integro-differential equations | For autonomous delay differential equations $x'(t)=f(x_t)$ we construct a
continuous semiflow of continuously differentiable solution operators
$x_0\mapsto x_t$, $t\ge0$, on open subsets of the Fr\'echet space
$C((-\infty,0],\mathbb{R}^n)$. For nonautonomous equations this yields a
continuous process of differentiabl... | math.DS | for autonomous delay differential equations xtfx_t we construct a continuous semiflow of continuously differentiable solution operators x_0mapsto x_t tge0 on open subsets of the frechet space cinfty0mathbbrn for nonautonomous equations this yields a continuous process of differentiable solution operators as an applicat... | [['for', 'autonomous', 'delay', 'differential', 'equations', 'xtfx_t', 'we', 'construct', 'a', 'continuous', 'semiflow', 'of', 'continuously', 'differentiable', 'solution', 'operators', 'x_0mapsto', 'x_t', 'tge0', 'on', 'open', 'subsets', 'of', 'the', 'frechet', 'space', 'cinfty0mathbbrn', 'for', 'nonautonomous', 'equa... | [-0.17140896819531917, 0.030554720920335968, -0.0726705225277692, 0.08840011067124579, -0.11387855250388385, -0.12465197538957, -0.004380631670355797, 0.33341716051101683, -0.38090636737644673, -0.11537772353738546, 0.18496807796880602, -0.3026754034915939, -0.15127969531342386, 0.20936495993286372, -0.09637904625386, ... |
1,801.09215 | The kurtosis of net baryon number fluctuations from a realistic
Polyakov--Nambu--Jona-Lasinio model along the experimental freeze-out line | Firstly we qualitatively analyze the formation of the dip and peak structures
of the kurtosis $\kappa \sigma^2$ of net baryon number fluctuation along
imagined freeze-out lines and discuss the signature of the existence of the QCD
critical end point (CEP) in the Nambu--Jona-Lasinio (NJL) model, Polyakov-NJL
(PNJL) mo... | hep-ph hep-th | firstly we qualitatively analyze the formation of the dip and peak structures of the kurtosis kappa sigma2 of net baryon number fluctuation along imagined freezeout lines and discuss the signature of the existence of the qcd critical end point cep in the nambujonalasinio njl model polyakovnjl pnjl model as well as mude... | [['firstly', 'we', 'qualitatively', 'analyze', 'the', 'formation', 'of', 'the', 'dip', 'and', 'peak', 'structures', 'of', 'the', 'kurtosis', 'kappa', 'sigma2', 'of', 'net', 'baryon', 'number', 'fluctuation', 'along', 'imagined', 'freezeout', 'lines', 'and', 'discuss', 'the', 'signature', 'of', 'the', 'existence', 'of',... | [-0.08836426041230108, 0.15090864390745615, -0.13323387222816097, 0.08445582721126367, -0.04323914909062028, -0.13959265875456717, 0.06282797385736881, 0.3279905654893164, -0.21854218429365715, -0.25996065907002913, 0.047708751580343295, -0.3366992518636378, -0.03695120387488887, 0.12997572125113083, 0.0427044939161056... |
1,801.09216 | Cross-over between diffusion-limited and reaction-limited regimes in the
coagulation-diffusion process | The change from the diffusion-limited to the reaction-limited cooperative
behaviour in reaction-diffusion systems is analysed by comparing the universal
long-time behaviour of the coagulation-diffusion process on a chain and on the
Bethe lattice. On a chain, this model is exactly solvable through the
empty-interval m... | cond-mat.stat-mech math-ph math.MP physics.chem-ph | the change from the diffusionlimited to the reactionlimited cooperative behaviour in reactiondiffusion systems is analysed by comparing the universal longtime behaviour of the coagulationdiffusion process on a chain and on the bethe lattice on a chain this model is exactly solvable through the emptyinterval method this... | [['the', 'change', 'from', 'the', 'diffusionlimited', 'to', 'the', 'reactionlimited', 'cooperative', 'behaviour', 'in', 'reactiondiffusion', 'systems', 'is', 'analysed', 'by', 'comparing', 'the', 'universal', 'longtime', 'behaviour', 'of', 'the', 'coagulationdiffusion', 'process', 'on', 'a', 'chain', 'and', 'on', 'the'... | [-0.11919806471594901, 0.13881156934466934, -0.09465833599053657, 0.10452294471261707, 8.653195004965832e-05, -0.1328389611957011, 0.07050519718883261, 0.3278269444621835, -0.2742213137454784, -0.1964047250560304, 0.10673093428546841, -0.30276012061330587, -0.11711626051257906, 0.1735977101011146, 0.04728007106694268, ... |
1,801.09217 | Observations of excitation and damping of transversal oscillation in
coronal loops by AIA/SDO | The excitation and damping of transversal coronal loop oscillations and
quantitative relation between damping time, damping quality (damping time per
period), oscillation amplitude, dissipation mechanism and the wake phenomena
are investigated. The observed time series data with the \textit{Atmospheric
Imaging Assemb... | astro-ph.SR | the excitation and damping of transversal coronal loop oscillations and quantitative relation between damping time damping quality damping time per period oscillation amplitude dissipation mechanism and the wake phenomena are investigated the observed time series data with the textitatmospheric imaging assembly aia tel... | [['the', 'excitation', 'and', 'damping', 'of', 'transversal', 'coronal', 'loop', 'oscillations', 'and', 'quantitative', 'relation', 'between', 'damping', 'time', 'damping', 'quality', 'damping', 'time', 'per', 'period', 'oscillation', 'amplitude', 'dissipation', 'mechanism', 'and', 'the', 'wake', 'phenomena', 'are', 'i... | [-0.1921852011076192, 0.26921121947277615, 0.004318886034457979, 0.09484461006111276, -0.06882259647978504, -0.1002890119475692, 0.037757407042792894, 0.37767811498121806, -0.21648378746963484, -0.37535317098162424, 0.1108305707823968, -0.29908205945833255, -0.10367193430041273, 0.29144694504146984, 0.02838992535813573... |
1,801.09218 | Simulating Soft-Sphere Margination in Arterioles and Venules | In this paper, we deploy a Lattice Boltzmann - Particle Dynamics (LBPD)
method to dissect the transport properties within arterioles and venules.
First, the numerical approach is applied to study the transport of Red Blood
Cells (RBC) through plasma and validated by means of comparison with the
experimental data in t... | physics.comp-ph physics.bio-ph | in this paper we deploy a lattice boltzmann particle dynamics lbpd method to dissect the transport properties within arterioles and venules first the numerical approach is applied to study the transport of red blood cells rbc through plasma and validated by means of comparison with the experimental data in the seminal ... | [['in', 'this', 'paper', 'we', 'deploy', 'a', 'lattice', 'boltzmann', 'particle', 'dynamics', 'lbpd', 'method', 'to', 'dissect', 'the', 'transport', 'properties', 'within', 'arterioles', 'and', 'venules', 'first', 'the', 'numerical', 'approach', 'is', 'applied', 'to', 'study', 'the', 'transport', 'of', 'red', 'blood', ... | [-0.07612627941794926, 0.10596769377123565, -0.08151930949825328, -0.017191605994012208, -0.016856265254318714, -0.026132160662673414, 0.037712889938848096, 0.3430850449949503, -0.24741801663767546, -0.30418637393042447, 0.08728839605115354, -0.28529965493362397, -0.16156000300310552, 0.17415437833056785, -0.0400681279... |
1,801.09219 | The Zarankiewicz problem in 3-partite graphs | Let $F$ be a graph, $k \geq 2$ be an integer, and write $\mathrm{ex}_{ \chi
\leq k } (n , F)$ for the maximum number of edges in an $n$-vertex graph that
is $k$-partite and has no subgraph isomorphic to $F$. The function
$\mathrm{ex}_{ \chi \leq 2} ( n , F)$ has been studied by many researchers.
Finding $\mathrm{ex}_... | math.CO | let f be a graph k geq 2 be an integer and write mathrmex_ chi leq k n f for the maximum number of edges in an nvertex graph that is kpartite and has no subgraph isomorphic to f the function mathrmex_ chi leq 2 n f has been studied by many researchers finding mathrmex_ chi leq 2 n k_st is a special case of the zarankie... | [['let', 'f', 'be', 'a', 'graph', 'k', 'geq', '2', 'be', 'an', 'integer', 'and', 'write', 'mathrmex_', 'chi', 'leq', 'k', 'n', 'f', 'for', 'the', 'maximum', 'number', 'of', 'edges', 'in', 'an', 'nvertex', 'graph', 'that', 'is', 'kpartite', 'and', 'has', 'no', 'subgraph', 'isomorphic', 'to', 'f', 'the', 'function', 'mat... | [-0.21873869146471478, 0.2010867416646957, 0.008519044289748897, 0.03639893441583149, -0.01433279856299872, -0.25015714875760253, 0.05176745594065983, 0.3308672578018113, -0.2218291500523942, -0.3480998686236311, 0.04403752961832866, -0.38646018360946877, -0.09024264708882672, 0.13214950304245576, -0.01310387324009949,... |
1,801.0922 | The Methods of Layer Potentials for General Elliptic Homogenization
Problems in Lipschitz Domains | In terms of layer potential methods, this paper is devoted to study the $L^2$
boundary value problems for nonhomogeneous elliptic operators with rapidly
oscillating coefficients in a periodic setting. Under a low regularity
assumption on the coefficients, we establish the solvability for Dirichlet,
regular and Neuman... | math.AP | in terms of layer potential methods this paper is devoted to study the l2 boundary value problems for nonhomogeneous elliptic operators with rapidly oscillating coefficients in a periodic setting under a low regularity assumption on the coefficients we establish the solvability for dirichlet regular and neumann problem... | [['in', 'terms', 'of', 'layer', 'potential', 'methods', 'this', 'paper', 'is', 'devoted', 'to', 'study', 'the', 'l2', 'boundary', 'value', 'problems', 'for', 'nonhomogeneous', 'elliptic', 'operators', 'with', 'rapidly', 'oscillating', 'coefficients', 'in', 'a', 'periodic', 'setting', 'under', 'a', 'low', 'regularity', ... | [-0.12242697724410924, 0.060214669901608606, -0.05937787275136698, 0.09137198901394518, -0.10808654165281574, -0.10318246844122414, 0.0027913327900999474, 0.3385678982098087, -0.29430040442679367, -0.22825793014617818, 0.17823442391179525, -0.2599391955768735, -0.13785661244764924, 0.18594316730528457, -0.1169895446950... |
1,801.09221 | Renormalizability of pure $\mathcal{N}=1$ Super Yang-Mills in the
Wess-Zumino gauge in the presence of the local composite operators $A^{2}$
and $\bar{\lambda}\lambda$ | The $\mathcal{N}=1$ Super Yang-Mills theory in the presence of the local
composite operator $A^2$ is analyzed in the Wess-Zumino gauge by employing the
Landau gauge fixing condition. Due to the superymmetric structure of the
theory, two more composite operators, $A_\mu \gamma_\mu \lambda$ and
$\bar{\lambda}\lambda$, ... | hep-th | the mathcaln1 super yangmills theory in the presence of the local composite operator a2 is analyzed in the wesszumino gauge by employing the landau gauge fixing condition due to the superymmetric structure of the theory two more composite operators a_mu gamma_mu lambda and barlambdalambda related to the susy variations... | [['the', 'mathcaln1', 'super', 'yangmills', 'theory', 'in', 'the', 'presence', 'of', 'the', 'local', 'composite', 'operator', 'a2', 'is', 'analyzed', 'in', 'the', 'wesszumino', 'gauge', 'by', 'employing', 'the', 'landau', 'gauge', 'fixing', 'condition', 'due', 'to', 'the', 'superymmetric', 'structure', 'of', 'the', 'th... | [-0.1447069392008165, 0.2090163492159326, -0.0707120410817001, 0.08059528434813697, -0.06723414462437083, -0.11914453237189045, -0.03325795873513863, 0.28980908928246335, -0.22311464040379586, -0.2550961780181187, 0.07138851500248761, -0.24347147376854614, -0.17136051616599335, 0.07693546678035937, -0.04429456337098161... |
1,801.09222 | Analysis of a Failed Eclipse Plasma Ejection Using EUV Observations | The photometry of eclipse white-light (W-L) images showing a moving blob is
interpreted for the first time together with observations from space with the
PRoject for On Board Autonomy (PROBA-2) mission (ESA). An off-limb event seen
with great details in W-L was analyzed with the SWAP imager (Sun Watcher using
Active ... | astro-ph.SR | the photometry of eclipse whitelight wl images showing a moving blob is interpreted for the first time together with observations from space with the project for on board autonomy proba2 mission esa an offlimb event seen with great details in wl was analyzed with the swap imager sun watcher using active pixel system de... | [['the', 'photometry', 'of', 'eclipse', 'whitelight', 'wl', 'images', 'showing', 'a', 'moving', 'blob', 'is', 'interpreted', 'for', 'the', 'first', 'time', 'together', 'with', 'observations', 'from', 'space', 'with', 'the', 'project', 'for', 'on', 'board', 'autonomy', 'proba2', 'mission', 'esa', 'an', 'offlimb', 'event... | [-0.08653391703326059, 0.17275052508803926, -0.03868269812659843, 0.09280260703567285, -0.035200836823174826, -0.07412457322771253, 0.013614042145159226, 0.4366772952440538, -0.2013217588151364, -0.39083403484536366, 0.11168299491982907, -0.3007905194266258, -0.04070424307648321, 0.2188906522230817, -0.0496925815687670... |
1,801.09223 | Probability Mass Exclusions and the Directed Components of Pointwise
Mutual Information | This paper examines how an event from one random variable provides pointwise
mutual information about an event from another variable via probability mass
exclusions. We start by introducing probability mass diagrams, which provide a
visual representation of how a prior distribution is transformed to a posterior
distr... | cs.IT math.IT | this paper examines how an event from one random variable provides pointwise mutual information about an event from another variable via probability mass exclusions we start by introducing probability mass diagrams which provide a visual representation of how a prior distribution is transformed to a posterior distribut... | [['this', 'paper', 'examines', 'how', 'an', 'event', 'from', 'one', 'random', 'variable', 'provides', 'pointwise', 'mutual', 'information', 'about', 'an', 'event', 'from', 'another', 'variable', 'via', 'probability', 'mass', 'exclusions', 'we', 'start', 'by', 'introducing', 'probability', 'mass', 'diagrams', 'which', '... | [-0.09873980563750726, 0.10984631254208978, -0.12264415119706795, 0.1272014115423593, -0.11431448144949233, -0.10942775782950173, 0.09183422657923267, 0.32592835456799, -0.27463279025542814, -0.2805699341381524, 0.08312225427759182, -0.290063630530475, -0.13020488434773408, 0.11634114013355694, -0.09317249066461593, 0.... |
1,801.09224 | Securing On-Body IoT Devices By Exploiting Creeping Wave Propagation | On-body devices are an intrinsic part of the Internet-of-Things (IoT) vision
to provide human-centric services. These on-body IoT devices are largely
embedded devices that lack a sophisticated user interface to facilitate
traditional Pre-Shared Key based security protocols. Motivated by this
real-world security vulne... | cs.NI | onbody devices are an intrinsic part of the internetofthings iot vision to provide humancentric services these onbody iot devices are largely embedded devices that lack a sophisticated user interface to facilitate traditional preshared key based security protocols motivated by this realworld security vulnerability this... | [['onbody', 'devices', 'are', 'an', 'intrinsic', 'part', 'of', 'the', 'internetofthings', 'iot', 'vision', 'to', 'provide', 'humancentric', 'services', 'these', 'onbody', 'iot', 'devices', 'are', 'largely', 'embedded', 'devices', 'that', 'lack', 'a', 'sophisticated', 'user', 'interface', 'to', 'facilitate', 'traditiona... | [-0.24132412401073686, 0.017090625530398064, -0.04101368169545944, -0.003238891763469787, -0.10626915876290824, -0.2731839573964979, 0.10433696930802376, 0.38548054895220907, -0.22387637942779431, -0.3265679725017284, 0.10583470536515893, -0.3160482034247163, -0.20360239704590907, 0.23297575650668126, -0.19475604013819... |
1,801.09225 | Contextual Modal Type Theory with Polymorphic Contexts | Modal types -- types that are derived from proof systems of modal logic --
have been studied as theoretical foundations of metaprogramming, where program
code is manipulated as first-class values. In modal type systems, modality
corresponds to a type constructor for code types and controls free variables
and their ty... | cs.LO | modal types types that are derived from proof systems of modal logic have been studied as theoretical foundations of metaprogramming where program code is manipulated as firstclass values in modal type systems modality corresponds to a type constructor for code types and controls free variables and their types in code ... | [['modal', 'types', 'types', 'that', 'are', 'derived', 'from', 'proof', 'systems', 'of', 'modal', 'logic', 'have', 'been', 'studied', 'as', 'theoretical', 'foundations', 'of', 'metaprogramming', 'where', 'program', 'code', 'is', 'manipulated', 'as', 'firstclass', 'values', 'in', 'modal', 'type', 'systems', 'modality', ... | [-0.06255814523876345, 0.03839525886847259, -0.06324579266963598, 0.06524304575999293, -0.13062409074630976, -0.1661559343108999, 0.02147839758786897, 0.3675258671203272, -0.2952776520049881, -0.302301801382335, 0.06674504311070803, -0.2349115854200444, -0.1222512916726368, 0.20427744840195433, -0.14154025456293032, 0.... |
1,801.09226 | Bogoliubov de Gennes equation on metric graphs | We consider Bogoliubov de Gennes equation on metric graphs. The vertex
boundary conditions providing self-adjoint realization of the Bogoliubov de
Gennes operator on a metric star graph are derived. Secular equation providing
quantization of the energy and the vertex transmission matrix are also
obtained. Application... | quant-ph cond-mat.mes-hall cond-mat.supr-con | we consider bogoliubov de gennes equation on metric graphs the vertex boundary conditions providing selfadjoint realization of the bogoliubov de gennes operator on a metric star graph are derived secular equation providing quantization of the energy and the vertex transmission matrix are also obtained application of th... | [['we', 'consider', 'bogoliubov', 'de', 'gennes', 'equation', 'on', 'metric', 'graphs', 'the', 'vertex', 'boundary', 'conditions', 'providing', 'selfadjoint', 'realization', 'of', 'the', 'bogoliubov', 'de', 'gennes', 'operator', 'on', 'a', 'metric', 'star', 'graph', 'are', 'derived', 'secular', 'equation', 'providing',... | [-0.2430807708038224, 0.10906851530523488, -0.08074644524431615, 0.09647531711918957, -0.16533580611684118, -0.17956399385541402, -0.02597864634460873, 0.33015106804668903, -0.20113193481746647, -0.23029334363700063, 0.04528954168954105, -0.31042804829431353, -0.14533603274159962, 0.11685247884425162, -0.03499192351268... |
1,801.09227 | A Probabilistic Ant-based Heuristic for the Longest Simple Cycle Problem
in Complex Networks | We propose a new probabilistic ant-based heuristic (ANTH-LS) for the longest
simple cycle problem. This NP-hard problem has numerous real-world applications
in complex networks, including efficient construction of graph layouts,
analysis of social networks or bioinformatics. Our algorithm is based on
reinforcing the ... | cs.SI | we propose a new probabilistic antbased heuristic anthls for the longest simple cycle problem this nphard problem has numerous realworld applications in complex networks including efficient construction of graph layouts analysis of social networks or bioinformatics our algorithm is based on reinforcing the probability ... | [['we', 'propose', 'a', 'new', 'probabilistic', 'antbased', 'heuristic', 'anthls', 'for', 'the', 'longest', 'simple', 'cycle', 'problem', 'this', 'nphard', 'problem', 'has', 'numerous', 'realworld', 'applications', 'in', 'complex', 'networks', 'including', 'efficient', 'construction', 'of', 'graph', 'layouts', 'analysi... | [-0.14208546147339654, -0.0074961850434786415, -0.013024010828563146, 0.0577879042497703, -0.08981744218522644, -0.12350199706092173, 0.051058215279208154, 0.4598582849590754, -0.22893389711650658, -0.3461426972715678, 0.09906954982327487, -0.2671289504268112, -0.255622818873606, 0.2254050281872897, -0.0662968139905406... |
1,801.09228 | {\gamma} Doradus stars as test of angular momentum transport models | Helioseismology and asteroseismology of red giant stars have shown that the
distribution of angular momentum in stellar interiors, and its evolution with
time remains an open issue in stellar physics. Owing to the unprecedented
quality of Kepler photometry, we are able to seismically infer internal
rotation rates in ... | astro-ph.SR | helioseismology and asteroseismology of red giant stars have shown that the distribution of angular momentum in stellar interiors and its evolution with time remains an open issue in stellar physics owing to the unprecedented quality of kepler photometry we are able to seismically infer internal rotation rates in gamma... | [['helioseismology', 'and', 'asteroseismology', 'of', 'red', 'giant', 'stars', 'have', 'shown', 'that', 'the', 'distribution', 'of', 'angular', 'momentum', 'in', 'stellar', 'interiors', 'and', 'its', 'evolution', 'with', 'time', 'remains', 'an', 'open', 'issue', 'in', 'stellar', 'physics', 'owing', 'to', 'the', 'unprec... | [-0.0774803563579758, 0.17123308342309557, -0.10475086702222407, 0.10918658116114018, -0.09929881054660109, -0.02303207984969732, 0.0685450991316867, 0.3865995207617104, -0.2102389065817963, -0.3753489641084911, 0.03711861938217483, -0.22410293360236386, -0.025887041372952686, 0.21334601527893654, -0.07562597239955803,... |
1,801.09229 | GraphCombEx: A Software Tool for Exploration of Combinatorial
Optimisation Properties of Large Graphs | We present a prototype of a software tool for exploration of multiple
combinatorial optimisation problems in large real-world and synthetic complex
networks. Our tool, called GraphCombEx (an acronym of Graph Combinatorial
Explorer), provides a unified framework for scalable computation and
presentation of high-qualit... | cs.SI cs.MS | we present a prototype of a software tool for exploration of multiple combinatorial optimisation problems in large realworld and synthetic complex networks our tool called graphcombex an acronym of graph combinatorial explorer provides a unified framework for scalable computation and presentation of highquality subopti... | [['we', 'present', 'a', 'prototype', 'of', 'a', 'software', 'tool', 'for', 'exploration', 'of', 'multiple', 'combinatorial', 'optimisation', 'problems', 'in', 'large', 'realworld', 'and', 'synthetic', 'complex', 'networks', 'our', 'tool', 'called', 'graphcombex', 'an', 'acronym', 'of', 'graph', 'combinatorial', 'explor... | [-0.09243688045741891, -0.015153296663031153, -0.058512179335281696, 0.08454931499615598, -0.1592911070284362, -0.16385881867006244, 0.0466580887823834, 0.4093171021151604, -0.2820159547559961, -0.3721238985112124, 0.16261152903199438, -0.21383234963872189, -0.19148170091446004, 0.2583088132128472, -0.08144643518108649... |
1,801.0923 | Magnetotransport signatures of three-dimensional topological insulator
nanostructures | We study the magnetotransport properties of patterned 3D topological
insulator nanostructures with several leads, such as kinks or Y-junctions, near
the Dirac point with analytical as well as numerical techniques. The interplay
of the nanostructure geometry, the external magnetic field and the
spin-momentum locking o... | cond-mat.mes-hall | we study the magnetotransport properties of patterned 3d topological insulator nanostructures with several leads such as kinks or yjunctions near the dirac point with analytical as well as numerical techniques the interplay of the nanostructure geometry the external magnetic field and the spinmomentum locking of the to... | [['we', 'study', 'the', 'magnetotransport', 'properties', 'of', 'patterned', '3d', 'topological', 'insulator', 'nanostructures', 'with', 'several', 'leads', 'such', 'as', 'kinks', 'or', 'yjunctions', 'near', 'the', 'dirac', 'point', 'with', 'analytical', 'as', 'well', 'as', 'numerical', 'techniques', 'the', 'interplay'... | [-0.22713945969258265, 0.19422197261625232, -0.042733779362332754, 0.00546308613747799, -0.07829131414082342, -0.19854020076974105, 0.03148186062174719, 0.4240475104901419, -0.27327347638696353, -0.32595543385613507, 0.021204142482958793, -0.25956601779707655, -0.14281146311181125, 0.23327912999722625, 0.01229799577655... |
1,801.09231 | Monitoring of Wild Pseudomonas Biofilm Strain Conditions Using
Statistical Characterisation of Scanning Electron Microscopy Images | The present paper proposes a novel method of quantification of the variation
in biofilm architecture, in correlation with the alteration of growth
conditions that include, variations of substrate and conditioning layer. The
polymeric biomaterial serving as substrates are widely used in implants and
indwelling medical... | physics.bio-ph cond-mat.soft q-bio.QM stat.AP | the present paper proposes a novel method of quantification of the variation in biofilm architecture in correlation with the alteration of growth conditions that include variations of substrate and conditioning layer the polymeric biomaterial serving as substrates are widely used in implants and indwelling medical devi... | [['the', 'present', 'paper', 'proposes', 'a', 'novel', 'method', 'of', 'quantification', 'of', 'the', 'variation', 'in', 'biofilm', 'architecture', 'in', 'correlation', 'with', 'the', 'alteration', 'of', 'growth', 'conditions', 'that', 'include', 'variations', 'of', 'substrate', 'and', 'conditioning', 'layer', 'the', '... | [-0.04592105557775482, 0.08556765750580915, -0.07357530728814766, 0.013317637814288127, -0.016879121298614415, -0.16842350722885036, -0.008526599488562924, 0.38265526716775716, -0.22951566904320064, -0.30855883211590984, 0.11046625724238185, -0.282572403708671, -0.1869083556799872, 0.20894713536216977, -0.0745610785150... |
1,801.09232 | Multimodal Functional and Structural Brain Connectivity Analysis in
Autism: A Preliminary Integrated Approach with EEG, fMRI and DTI | This paper proposes a novel approach of integrating different neuroimaging
techniques to characterize an autistic brain. Different techniques like EEG,
fMRI and DTI have traditionally been used to find biomarkers for autism, but
there have been very few attempts for a combined or multimodal approach of EEG,
fMRI and ... | physics.med-ph stat.AP | this paper proposes a novel approach of integrating different neuroimaging techniques to characterize an autistic brain different techniques like eeg fmri and dti have traditionally been used to find biomarkers for autism but there have been very few attempts for a combined or multimodal approach of eeg fmri and dti to... | [['this', 'paper', 'proposes', 'a', 'novel', 'approach', 'of', 'integrating', 'different', 'neuroimaging', 'techniques', 'to', 'characterize', 'an', 'autistic', 'brain', 'different', 'techniques', 'like', 'eeg', 'fmri', 'and', 'dti', 'have', 'traditionally', 'been', 'used', 'to', 'find', 'biomarkers', 'for', 'autism', ... | [-0.03613464537425898, 0.05961938342727081, -0.09603226970764808, 0.0774312226451002, -0.09191538707353175, -0.1467242943053134, 0.0075706907222047445, 0.4281415726616979, -0.24658192056696862, -0.3179775949707255, 0.10322839537926484, -0.2680105256720708, -0.22972750026994618, 0.17389549926156178, -0.03447800079794433... |
1,801.09233 | Random matrix approach to plasmon resonances in the random impedance
network model of disordered nanocomposites | Random impedance networks are widely used as a model to describe plasmon
resonances in disordered metal-dielectric and other two-component
nanocomposites. In the present work, the spectral properties of resonances in
random networks are studied within the framework of the random matrix theory.
We have shown that the ... | cond-mat.dis-nn cond-mat.mes-hall physics.optics | random impedance networks are widely used as a model to describe plasmon resonances in disordered metaldielectric and other twocomponent nanocomposites in the present work the spectral properties of resonances in random networks are studied within the framework of the random matrix theory we have shown that the appropr... | [['random', 'impedance', 'networks', 'are', 'widely', 'used', 'as', 'a', 'model', 'to', 'describe', 'plasmon', 'resonances', 'in', 'disordered', 'metaldielectric', 'and', 'other', 'twocomponent', 'nanocomposites', 'in', 'the', 'present', 'work', 'the', 'spectral', 'properties', 'of', 'resonances', 'in', 'random', 'netw... | [-0.1198776793216194, 0.12432011872834454, -0.06301745482218954, 0.07203128000121349, 0.04050945777159471, -0.120576167676168, 0.006722625964007771, 0.4287378838321624, -0.20062880555185705, -0.262751512372723, 0.030534778844902084, -0.27842465210526895, -0.213213638545802, 0.16088903200803684, 0.022805043346194837, 0.... |
1,801.09234 | On $\sigma$-quasinormal subgroups of finite groups | Let $G$ be a finite group and $\sigma =\{\sigma_{i} | i\in I\}$ some
partition of the set of all primes $\Bbb{P}$, that is, $\sigma =\{\sigma_{i} |
i\in I \}$, where $\Bbb{P}=\bigcup_{i\in I} \sigma_{i}$ and $\sigma_{i}\cap
\sigma_{j}= \emptyset $ for all $i\ne j$. We say that $G$ is $\sigma$-primary
if $G$ is a $\si... | math.GR | let g be a finite group and sigma sigma_i iin i some partition of the set of all primes bbbp that is sigma sigma_i iin i where bbbpbigcup_iin i sigma_i and sigma_icap sigma_j emptyset for all ine j we say that g is sigmaprimary if g is a sigma _igroup for some i a subgroup a of g is said to be sigmasubnormal in g if th... | [['let', 'g', 'be', 'a', 'finite', 'group', 'and', 'sigma', 'sigma_i', 'iin', 'i', 'some', 'partition', 'of', 'the', 'set', 'of', 'all', 'primes', 'bbbp', 'that', 'is', 'sigma', 'sigma_i', 'iin', 'i', 'where', 'bbbpbigcup_iin', 'i', 'sigma_i', 'and', 'sigma_icap', 'sigma_j', 'emptyset', 'for', 'all', 'ine', 'j', 'we', ... | [-0.21688341659507113, 0.1957701897865794, -0.02946168395053399, -0.03174116600106546, -0.0598954232938757, -0.21206973001147, 0.020190728297618633, 0.43227758224714885, -0.29056666755790345, -0.13879295614585346, 0.03988482731363277, -0.3544063422891298, -0.04143138380239954, 0.13125205768325754, -0.05894003261959082,... |
1,801.09235 | On one generalization of finite nilpotent groups | Let $\sigma =\{\sigma_{i} | i\in I\}$ be a partition of the set $\Bbb{P}$ of
all primes and $G$ a finite group. A chief factor $H/K$ of $G$ is said to be
$\sigma$-central if the semidirect product $(H/K)\rtimes (G/C_{G}(H/K))$ is a
$\sigma_{i}$-group for some $i=i(H/K)$. $G$ is called $\sigma$-nilpotent if
every chie... | math.GR | let sigma sigma_i iin i be a partition of the set bbbp of all primes and g a finite group a chief factor hk of g is said to be sigmacentral if the semidirect product hkrtimes gc_ghk is a sigma_igroup for some iihk g is called sigmanilpotent if every chief factor of g is sigmacentral we say that g is semisigmanilpotent ... | [['let', 'sigma', 'sigma_i', 'iin', 'i', 'be', 'a', 'partition', 'of', 'the', 'set', 'bbbp', 'of', 'all', 'primes', 'and', 'g', 'a', 'finite', 'group', 'a', 'chief', 'factor', 'hk', 'of', 'g', 'is', 'said', 'to', 'be', 'sigmacentral', 'if', 'the', 'semidirect', 'product', 'hkrtimes', 'gc_ghk', 'is', 'a', 'sigma_igroup'... | [-0.19095890559053616, 0.1807659112306757, -0.08548463319185311, -0.014645251160760856, -0.11064409838645192, -0.14474756174984024, 0.005723041901111846, 0.3764210137660089, -0.28171829336687276, -0.14315334706581148, 0.07739698163071729, -0.3094731345772743, -0.11253769882529488, 0.14351081018052672, -0.12422108815213... |
1,801.09236 | Structure and Sensitivity in Differential Privacy: Comparing K-Norm
Mechanisms | Differential privacy (DP), provides a framework for provable privacy
protection against arbitrary adversaries, while allowing the release of summary
statistics and synthetic data. We address the problem of releasing a noisy
real-valued statistic vector $T$, a function of sensitive data under DP, via
the class of $K$-... | stat.ME | differential privacy dp provides a framework for provable privacy protection against arbitrary adversaries while allowing the release of summary statistics and synthetic data we address the problem of releasing a noisy realvalued statistic vector t a function of sensitive data under dp via the class of knorm mechanisms... | [['differential', 'privacy', 'dp', 'provides', 'a', 'framework', 'for', 'provable', 'privacy', 'protection', 'against', 'arbitrary', 'adversaries', 'while', 'allowing', 'the', 'release', 'of', 'summary', 'statistics', 'and', 'synthetic', 'data', 'we', 'address', 'the', 'problem', 'of', 'releasing', 'a', 'noisy', 'realv... | [-0.08714112991598158, 0.0028749147141802745, -0.06540455086971048, 0.10120032729180857, -0.06716450594655758, -0.13560663306870352, 0.12065813027675633, 0.33287039117410255, -0.31268891073931854, -0.29974163389395003, 0.09881554953239147, -0.2753737915550644, -0.1456720309949775, 0.1934594480144141, -0.097605573943577... |
1,801.09237 | A Balian-Low Theorem for Subspaces | We extend the Balian-Low theorem to Gabor subspaces of $L^2(\mathbb R)$ by
involving the concept of additional time-frequency shift invariance. We prove
that if a Gabor system on a lattice of rational density is a Riesz sequence
generating a subspace which is invariant under an additional time-frequency
shift, then i... | math.FA | we extend the balianlow theorem to gabor subspaces of l2mathbb r by involving the concept of additional timefrequency shift invariance we prove that if a gabor system on a lattice of rational density is a riesz sequence generating a subspace which is invariant under an additional timefrequency shift then its generator ... | [['we', 'extend', 'the', 'balianlow', 'theorem', 'to', 'gabor', 'subspaces', 'of', 'l2mathbb', 'r', 'by', 'involving', 'the', 'concept', 'of', 'additional', 'timefrequency', 'shift', 'invariance', 'we', 'prove', 'that', 'if', 'a', 'gabor', 'system', 'on', 'a', 'lattice', 'of', 'rational', 'density', 'is', 'a', 'riesz',... | [-0.16102886737013858, 0.15235073227498408, -0.1431919154090186, 0.06294449154908459, -0.09270581095479428, -0.1196309853810817, 0.02533759325936747, 0.4062019285435478, -0.35449379016645255, -0.10426529498460392, 0.12839864285391134, -0.22318941007057827, -0.15385918660710254, 0.18732255902141332, -0.10612354192417114... |
1,801.09238 | Performance Analysis of Robust Stable PID Controllers Using Dominant
Pole Placement for SOPTD Process Models | This paper derives new formulations for designing dominant pole placement
based proportional-integral-derivative (PID) controllers to handle second order
processes with time delays (SOPTD). Previously, similar attempts have been made
for pole placement in delay-free systems. The presence of the time delay term
manife... | cs.SY cs.CV stat.AP | this paper derives new formulations for designing dominant pole placement based proportionalintegralderivative pid controllers to handle second order processes with time delays soptd previously similar attempts have been made for pole placement in delayfree systems the presence of the time delay term manifests itself a... | [['this', 'paper', 'derives', 'new', 'formulations', 'for', 'designing', 'dominant', 'pole', 'placement', 'based', 'proportionalintegralderivative', 'pid', 'controllers', 'to', 'handle', 'second', 'order', 'processes', 'with', 'time', 'delays', 'soptd', 'previously', 'similar', 'attempts', 'have', 'been', 'made', 'for'... | [-0.17825215860125354, 0.07403686548013866, -0.058281237275878084, 0.06627921406496995, -0.0922818409417232, -0.1334278313224786, 0.07900316256973383, 0.37754232731094817, -0.24572408710628224, -0.31806866578699555, 0.12471014443428885, -0.22390093874491868, -0.13958357889805484, 0.18636347868869052, -0.000512084606384... |
1,801.09239 | Vector fields on $\mathfrak{osp}_{2m-1|2n}(\mathbb C)$-flag
supermanifolds | We compute the Lie superalgebras of holomorphic vector fields on isotropic
flag supermanifolds of maximal type corresponding to the Lie superalgebra
$\mathfrak{osp}_{2m-1|2n}(\mathbb C)$.
| math.RT math.AG math.CV | we compute the lie superalgebras of holomorphic vector fields on isotropic flag supermanifolds of maximal type corresponding to the lie superalgebra mathfrakosp_2m12nmathbb c | [['we', 'compute', 'the', 'lie', 'superalgebras', 'of', 'holomorphic', 'vector', 'fields', 'on', 'isotropic', 'flag', 'supermanifolds', 'of', 'maximal', 'type', 'corresponding', 'to', 'the', 'lie', 'superalgebra', 'mathfrakosp_2m12nmathbb', 'c']] | [-0.2566023747521368, 0.011034093728416006, 0.07028575910424645, 0.05614008441228758, -0.30117521348240023, -0.1582709071226418, -0.07848437028852376, 0.3897699149833484, -0.32524107938463037, -0.12392419534312053, 0.12547520029527898, -0.17200035957450216, -0.15951995839449493, 0.18677273324944757, -0.1003578012301163... |
1,801.0924 | Time Constrained Continuous Subgraph Search over Streaming Graphs | The growing popularity of dynamic applications such as social networks
provides a promising way to detect valuable information in real time. Efficient
analysis over high-speed data from dynamic applications is of great
significance. Data from these dynamic applications can be easily modeled as
streaming graph. In thi... | cs.DB | the growing popularity of dynamic applications such as social networks provides a promising way to detect valuable information in real time efficient analysis over highspeed data from dynamic applications is of great significance data from these dynamic applications can be easily modeled as streaming graph in this pape... | [['the', 'growing', 'popularity', 'of', 'dynamic', 'applications', 'such', 'as', 'social', 'networks', 'provides', 'a', 'promising', 'way', 'to', 'detect', 'valuable', 'information', 'in', 'real', 'time', 'efficient', 'analysis', 'over', 'highspeed', 'data', 'from', 'dynamic', 'applications', 'is', 'of', 'great', 'sign... | [-0.14795431888802948, -0.020641850078633676, -0.05599398531485349, 0.04535853769775713, -0.17003720495849847, -0.0910008826913933, 0.10222130475352363, 0.4147855670479961, -0.3305276825247953, -0.3966951540671289, 0.132988719517986, -0.29028293984010817, -0.20844974857755005, 0.20358277881750836, -0.09866207216012603,... |
1,801.09241 | Virtually abelian subgroups of $IA_n(Z/3)$ are abelian | When studying subgroups of $Out(F_n)$, one often replaces a given subgroup
$H$ with one of its finite index subgroups $H_0$ so that virtual properties of
$H$ become actual properties of $H_0$. In many cases, the finite index subgroup
is $H_0 = H \cap IA_n(Z/3)$. For which properties is this a good choice? Our
main th... | math.GR | when studying subgroups of outf_n one often replaces a given subgroup h with one of its finite index subgroups h_0 so that virtual properties of h become actual properties of h_0 in many cases the finite index subgroup is h_0 h cap ia_nz3 for which properties is this a good choice our main theorem states that being abe... | [['when', 'studying', 'subgroups', 'of', 'outf_n', 'one', 'often', 'replaces', 'a', 'given', 'subgroup', 'h', 'with', 'one', 'of', 'its', 'finite', 'index', 'subgroups', 'h_0', 'so', 'that', 'virtual', 'properties', 'of', 'h', 'become', 'actual', 'properties', 'of', 'h_0', 'in', 'many', 'cases', 'the', 'finite', 'index... | [-0.14943356783655676, 0.17325203277278636, -0.10523398186795521, 0.04468821462722954, -0.12628967317658057, -0.1539437219068624, 0.015585226290251898, 0.38853073344174505, -0.32466598287683684, -0.20844247294724852, 0.14390315955498026, -0.2758196470854075, -0.02947048385344122, 0.22782701245792533, -0.100999443967273... |
1,801.09242 | Joint Voxel and Coordinate Regression for Accurate 3D Facial Landmark
Localization | 3D face shape is more expressive and viewpoint-consistent than its 2D
counterpart. However, 3D facial landmark localization in a single image is
challenging due to the ambiguous nature of landmarks under 3D perspective.
Existing approaches typically adopt a suboptimal two-step strategy, performing
2D landmark localiz... | cs.CV | 3d face shape is more expressive and viewpointconsistent than its 2d counterpart however 3d facial landmark localization in a single image is challenging due to the ambiguous nature of landmarks under 3d perspective existing approaches typically adopt a suboptimal twostep strategy performing 2d landmark localization fo... | [['3d', 'face', 'shape', 'is', 'more', 'expressive', 'and', 'viewpointconsistent', 'than', 'its', '2d', 'counterpart', 'however', '3d', 'facial', 'landmark', 'localization', 'in', 'a', 'single', 'image', 'is', 'challenging', 'due', 'to', 'the', 'ambiguous', 'nature', 'of', 'landmarks', 'under', '3d', 'perspective', 'ex... | [-0.027042088263834734, -0.05749438328548589, -0.05757339141163932, 0.022483306425867107, -0.07791694949611748, -0.16607704610828686, -0.00033543156214280547, 0.45486724706486276, -0.2573535393222893, -0.3201773282644604, 0.06987178799431396, -0.23731221335324879, -0.22709618679620538, 0.15861119457024977, -0.166851688... |
1,801.09243 | Motivic Intersection Complex of Certain Shimura varieties | Using a version of weight conservativity we demonstrate that for certain
Shimura varieties (including all Shimura three-folds, most Shimura four-folds
and the Siegel sixfold) the construction of the motivic intersection complex
due to Wildeshaus compares with a motivic weight truncation in the sense of S.
Morel. In p... | math.AG | using a version of weight conservativity we demonstrate that for certain shimura varieties including all shimura threefolds most shimura fourfolds and the siegel sixfold the construction of the motivic intersection complex due to wildeshaus compares with a motivic weight truncation in the sense of s morel in particular... | [['using', 'a', 'version', 'of', 'weight', 'conservativity', 'we', 'demonstrate', 'that', 'for', 'certain', 'shimura', 'varieties', 'including', 'all', 'shimura', 'threefolds', 'most', 'shimura', 'fourfolds', 'and', 'the', 'siegel', 'sixfold', 'the', 'construction', 'of', 'the', 'motivic', 'intersection', 'complex', 'd... | [-0.18210749477421975, -0.027189084402112606, -0.12948463868130655, 0.09216208604801282, -0.0897691654630334, -0.1251221217064406, 0.014717348253779003, 0.2639327759628513, -0.32451862509889695, -0.23286445342990406, 0.08823125926787992, -0.1913793024004382, -0.1597831019145601, 0.23307614022290662, -0.2460737355868332... |
1,801.09244 | A periodic solution of period two of a delay differential equation | In this paper we prove that the following delay differential equation \[
\frac{d}{dt}x(t)=rx(t)\left(1-\int_{0}^{1}x(t-s)ds\right), \] has a periodic
solution of period two for $r>\frac{\pi^{2}}{2}$ (when the steady state, $x=1$,
is unstable). In order to find the periodic solution, we study an integrable
system of o... | math.DS | in this paper we prove that the following delay differential equation fracddtxtrxtleft1int_01xtsdsright has a periodic solution of period two for rfracpi22 when the steady state x1 is unstable in order to find the periodic solution we study an integrable system of ordinary differential equations following the idea by k... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'following', 'delay', 'differential', 'equation', 'fracddtxtrxtleft1int_01xtsdsright', 'has', 'a', 'periodic', 'solution', 'of', 'period', 'two', 'for', 'rfracpi22', 'when', 'the', 'steady', 'state', 'x1', 'is', 'unstable', 'in', 'order', 'to', 'find', 'the', 'peri... | [-0.2340375563343529, 0.03948404131000136, -0.0983597728210028, 0.04290064698520315, -0.029212750937240045, -0.11136341375130855, -0.04356610442351428, 0.27788332684851086, -0.31679337355689924, -0.221692078426236, 0.14655373489186474, -0.31201158002873913, -0.1836097371443862, 0.18475437433016104, -0.09033000177596925... |
1,801.09245 | Wavelet Analysis of the Besov Regularity of L\'evy White Noises | We characterize the local smoothness and the asymptotic growth rate of the
L\'evy white noise. We do so by characterizing the weighted Besov spaces in
which it is located. We extend known results in two ways. First, we obtain new
bounds for the local smoothness via the Blumenthal-Getoor indices of the L\'evy
white no... | math.PR | we characterize the local smoothness and the asymptotic growth rate of the levy white noise we do so by characterizing the weighted besov spaces in which it is located we extend known results in two ways first we obtain new bounds for the local smoothness via the blumenthalgetoor indices of the levy white noise we also... | [['we', 'characterize', 'the', 'local', 'smoothness', 'and', 'the', 'asymptotic', 'growth', 'rate', 'of', 'the', 'levy', 'white', 'noise', 'we', 'do', 'so', 'by', 'characterizing', 'the', 'weighted', 'besov', 'spaces', 'in', 'which', 'it', 'is', 'located', 'we', 'extend', 'known', 'results', 'in', 'two', 'ways', 'first... | [-0.08556771115687342, 0.11311496814632398, -0.0953477182034633, 0.1404218597065968, -0.0659413930994493, -0.07720457884931455, 0.06796470672872354, 0.34176902949844523, -0.270838395609049, -0.22485428536023347, 0.16155446483178731, -0.257791878103658, -0.16015136386785242, 0.2251202866067121, -0.1638133330443115, 0.07... |
1,801.09246 | Topological properties of convolutor spaces via the short-time Fourier
transform | We discuss the structural and topological properties of a general class of
weighted $L^1$ convolutor spaces. Our theory simultaneously applies to weighted
$\mathcal{D}'_{L^1}$ spaces as well as to convolutor spaces of the
Gelfand-Shilov spaces $\mathcal{K}\{M_p\}$. In particular, we characterize the
sequences of weig... | math.FA | we discuss the structural and topological properties of a general class of weighted l1 convolutor spaces our theory simultaneously applies to weighted mathcald_l1 spaces as well as to convolutor spaces of the gelfandshilov spaces mathcalkm_p in particular we characterize the sequences of weight functions m_p_p in mathb... | [['we', 'discuss', 'the', 'structural', 'and', 'topological', 'properties', 'of', 'a', 'general', 'class', 'of', 'weighted', 'l1', 'convolutor', 'spaces', 'our', 'theory', 'simultaneously', 'applies', 'to', 'weighted', 'mathcald_l1', 'spaces', 'as', 'well', 'as', 'to', 'convolutor', 'spaces', 'of', 'the', 'gelfandshilo... | [-0.07860757580198262, 0.11165579226424639, -0.07738901826756439, 0.1383581448777247, -0.05684322116618184, -0.033914109563519215, 0.04284398550376425, 0.3468888659544032, -0.3129749784524413, -0.2182156229926937, 0.09906516623570873, -0.22328995266693763, -0.14371682443366995, 0.22788424989015893, -0.1298764752352546,... |
1,801.09247 | Stability, convergence, and sensitivity analysis of the Filament Based
Lamellipodium Model and the corresponding FEM | This paper focuses on the study of the Filament Based Lamellipodium Model
(FBLM) and the corresponding Finite Element Method (FEM) from a numerical point
of view. We study fundamental numerical properties of the FEM and justify the
further use of the FBLM. We exhibit that the FEM satisfies a timestep stability
condit... | q-bio.CB | this paper focuses on the study of the filament based lamellipodium model fblm and the corresponding finite element method fem from a numerical point of view we study fundamental numerical properties of the fem and justify the further use of the fblm we exhibit that the fem satisfies a timestep stability condition that... | [['this', 'paper', 'focuses', 'on', 'the', 'study', 'of', 'the', 'filament', 'based', 'lamellipodium', 'model', 'fblm', 'and', 'the', 'corresponding', 'finite', 'element', 'method', 'fem', 'from', 'a', 'numerical', 'point', 'of', 'view', 'we', 'study', 'fundamental', 'numerical', 'properties', 'of', 'the', 'fem', 'and'... | [-0.08864112965248783, 0.04855213065968891, -0.10071224319138404, -0.019363763576758834, -0.0480412770737091, -0.06186659989300473, 0.039986462609697904, 0.39344334370328177, -0.27052348258198594, -0.25491579530704445, 0.13193992582021347, -0.2377827737095027, -0.18005033616972124, 0.17568655801166233, -0.0375330465428... |
1,801.09248 | The point equivalence problem for ordinary differential equations of the
second order | We use E. Cartan's method to solve the problem of equivalence of the second
order ordinary differential equations with respect to the pseudogroup of point
transformations.
| math.DG math.CA | we use e cartans method to solve the problem of equivalence of the second order ordinary differential equations with respect to the pseudogroup of point transformations | [['we', 'use', 'e', 'cartans', 'method', 'to', 'solve', 'the', 'problem', 'of', 'equivalence', 'of', 'the', 'second', 'order', 'ordinary', 'differential', 'equations', 'with', 'respect', 'to', 'the', 'pseudogroup', 'of', 'point', 'transformations']] | [-0.13168488174247053, -0.02924884741122906, -0.09654438280715393, 0.03459534550067754, -0.1627301904731072, -0.09618612436147836, 0.003290451454141965, 0.2756622298620641, -0.40524706359093005, -0.3228953020006884, 0.05786365317180753, -0.3339793558877248, -0.12332265394238326, 0.11530357370009789, -0.0985240687687809... |
1,801.09249 | Polarity imbalance of the photospheric magnetic field | Polarity imbalance of the photospheric magnetic field was studied using
synoptic maps of NSO Kitt Peak (1976-2016). Imbalance of positive and negative
fluxes was considered for the fields with strength B>50 G in the sunspot zone
(5 deg - 40 deg) and for the fields with strength B<50 G at higher latitudes
(40 deg - 90... | astro-ph.SR | polarity imbalance of the photospheric magnetic field was studied using synoptic maps of nso kitt peak 19762016 imbalance of positive and negative fluxes was considered for the fields with strength b50 g in the sunspot zone 5 deg 40 deg and for the fields with strength b50 g at higher latitudes 40 deg 90 deg the 22year... | [['polarity', 'imbalance', 'of', 'the', 'photospheric', 'magnetic', 'field', 'was', 'studied', 'using', 'synoptic', 'maps', 'of', 'nso', 'kitt', 'peak', '19762016', 'imbalance', 'of', 'positive', 'and', 'negative', 'fluxes', 'was', 'considered', 'for', 'the', 'fields', 'with', 'strength', 'b50', 'g', 'in', 'the', 'suns... | [-0.18935912355905535, 0.2072301065410124, 0.041511381469757816, 0.09770678041003099, -0.06831369441820354, -0.0451514127721056, 0.037116620188476744, 0.36355078400271695, -0.19841302816369913, -0.38349225350269456, 0.05715694409545238, -0.2571746730711311, -0.0729458579063847, 0.19414218651335233, -0.00783652292973384... |
1,801.0925 | Virtual Breakpoints for x86/64 | Efficient, reliable trapping of execution in a program at the desired
location is a linchpin technique for dynamic malware analysis. The progression
of debuggers and malware is akin to a game of cat and mouse - each are
constantly in a state of trying to thwart one another. At the core of most
efficient debuggers tod... | cs.OS cs.CR | efficient reliable trapping of execution in a program at the desired location is a linchpin technique for dynamic malware analysis the progression of debuggers and malware is akin to a game of cat and mouse each are constantly in a state of trying to thwart one another at the core of most efficient debuggers today is a... | [['efficient', 'reliable', 'trapping', 'of', 'execution', 'in', 'a', 'program', 'at', 'the', 'desired', 'location', 'is', 'a', 'linchpin', 'technique', 'for', 'dynamic', 'malware', 'analysis', 'the', 'progression', 'of', 'debuggers', 'and', 'malware', 'is', 'akin', 'to', 'a', 'game', 'of', 'cat', 'and', 'mouse', 'each'... | [-0.11014883082226742, 0.038342046482232064, -0.1034803427182192, 0.04367490352023447, -0.12325766262179916, -0.19558378537792875, 0.10283340475913408, 0.37515237280909997, -0.27821289515544567, -0.3148097679849066, 0.09975574843153573, -0.24705031864426058, -0.14676827963684563, 0.20272104559547227, -0.120529684923130... |
1,801.09251 | Multi-Pointer Co-Attention Networks for Recommendation | Many recent state-of-the-art recommender systems such as D-ATT, TransNet and
DeepCoNN exploit reviews for representation learning. This paper proposes a new
neural architecture for recommendation with reviews. Our model operates on a
multi-hierarchical paradigm and is based on the intuition that not all reviews
are c... | cs.CL cs.AI cs.IR | many recent stateoftheart recommender systems such as datt transnet and deepconn exploit reviews for representation learning this paper proposes a new neural architecture for recommendation with reviews our model operates on a multihierarchical paradigm and is based on the intuition that not all reviews are created equ... | [['many', 'recent', 'stateoftheart', 'recommender', 'systems', 'such', 'as', 'datt', 'transnet', 'and', 'deepconn', 'exploit', 'reviews', 'for', 'representation', 'learning', 'this', 'paper', 'proposes', 'a', 'new', 'neural', 'architecture', 'for', 'recommendation', 'with', 'reviews', 'our', 'model', 'operates', 'on', ... | [-0.06154305448509218, 0.021842678458609457, -0.08159252598118497, 0.034789790712597655, -0.14245751708737603, -0.17477487554829024, 0.07158374503691317, 0.43257764237619634, -0.23806759263331387, -0.32749576083564036, 0.042120721742395034, -0.30353122653967946, -0.23701048089763474, 0.21151398363911583, -0.09201705427... |
1,801.09252 | End to End Performance Analysis of Relay Cooperative Communication Based
on Parked Cars | Parking lots (PLs) are usually full with cars. If these cars are formed into
a self-organizing vehicular network, they can be new kind of road side units
(RSUs) in urban area to provide communication data forwarding between mobile
terminals nearby and a base station. However cars in PLs can leave at any time,
which i... | cs.IT math.IT | parking lots pls are usually full with cars if these cars are formed into a selforganizing vehicular network they can be new kind of road side units rsus in urban area to provide communication data forwarding between mobile terminals nearby and a base station however cars in pls can leave at any time which is neglected... | [['parking', 'lots', 'pls', 'are', 'usually', 'full', 'with', 'cars', 'if', 'these', 'cars', 'are', 'formed', 'into', 'a', 'selforganizing', 'vehicular', 'network', 'they', 'can', 'be', 'new', 'kind', 'of', 'road', 'side', 'units', 'rsus', 'in', 'urban', 'area', 'to', 'provide', 'communication', 'data', 'forwarding', '... | [-0.2561355439138424, 0.07687495582285919, -0.070916987478995, 0.012026972833155014, -0.06675689518306172, -0.19901137066699448, 0.15697118264961318, 0.4017528282420244, -0.2417558667202684, -0.24559953709467663, 0.09233051488718047, -0.3166456490632754, -0.16518402640758723, 0.16732084177419893, -0.14139050612902793, ... |
1,801.09253 | Borosilicones and viscoelastic silicone rubbers: network liquids and
network solids | Borosilicones (e.g., Silly Putty) have been known for 70 years, but their
peculiar behaviors have remain unexplained. In this work, experiment and theory
are used to show that they are network liquids---dynamic macromolecules that
appear elastic on short timescales but exhibit flow on longer timescales. Each
borosili... | cond-mat.soft | borosilicones eg silly putty have been known for 70 years but their peculiar behaviors have remain unexplained in this work experiment and theory are used to show that they are network liquidsdynamic macromolecules that appear elastic on short timescales but exhibit flow on longer timescales each borosilicone is a vast... | [['borosilicones', 'eg', 'silly', 'putty', 'have', 'been', 'known', 'for', '70', 'years', 'but', 'their', 'peculiar', 'behaviors', 'have', 'remain', 'unexplained', 'in', 'this', 'work', 'experiment', 'and', 'theory', 'are', 'used', 'to', 'show', 'that', 'they', 'are', 'network', 'liquidsdynamic', 'macromolecules', 'tha... | [-0.15457183088323004, 0.18103187635005497, -0.09419048614484868, 0.03296452175468711, -0.05935490083761681, -0.1925632043468549, 0.018745129266701275, 0.37354674282189654, -0.2935928016239287, -0.2698795898533881, 0.06890721014294689, -0.2701271744935136, -0.19213826832522576, 0.13941468181415384, -0.02070113144730939... |
1,801.09254 | SEURAT: SPH scheme extended with ultraviolet line radiative transfer | We present a novel Lyman alpha (Ly$\alpha$) radiative transfer code, SEURAT,
where line scatterings are solved adaptively with the resolution of the
smoothed particle hydrodynamics (SPH). The radiative transfer method
implemented in SEURAT is based on a Monte Carlo algorithm in which the
scattering and absorption by ... | astro-ph.IM astro-ph.GA | we present a novel lyman alpha lyalpha radiative transfer code seurat where line scatterings are solved adaptively with the resolution of the smoothed particle hydrodynamics sph the radiative transfer method implemented in seurat is based on a monte carlo algorithm in which the scattering and absorption by dust are als... | [['we', 'present', 'a', 'novel', 'lyman', 'alpha', 'lyalpha', 'radiative', 'transfer', 'code', 'seurat', 'where', 'line', 'scatterings', 'are', 'solved', 'adaptively', 'with', 'the', 'resolution', 'of', 'the', 'smoothed', 'particle', 'hydrodynamics', 'sph', 'the', 'radiative', 'transfer', 'method', 'implemented', 'in',... | [-0.006495632175058343, 0.09249390629304609, -0.05757838816633773, 0.11484945923777644, -0.05947570892478621, -0.14307353971255293, -0.0109551930509042, 0.46392159139585876, -0.17582121840678155, -0.3216088306142537, -0.008738884168980254, -0.28030325376244564, -0.05776604136376273, 0.17262762537575327, 0.0513473311060... |
1,801.09255 | Zeeman Splitting and Inverted Polarization of Biexciton Emission in
Monolayer WS2 | We investigate the magnetic-field-induced splitting of biexcitons in
monolayer WS$_2$ using polarization-resolved photoluminescence spectroscopy in
out-of-plane magnetic fields up to 30 T. The observed $g$ factor of the
biexciton amounts to $-3.89$, closely matching the $g$ factor of the neutral
exciton. The biexcito... | cond-mat.mes-hall | we investigate the magneticfieldinduced splitting of biexcitons in monolayer ws_2 using polarizationresolved photoluminescence spectroscopy in outofplane magnetic fields up to 30 t the observed g factor of the biexciton amounts to 389 closely matching the g factor of the neutral exciton the biexciton emission shows an ... | [['we', 'investigate', 'the', 'magneticfieldinduced', 'splitting', 'of', 'biexcitons', 'in', 'monolayer', 'ws_2', 'using', 'polarizationresolved', 'photoluminescence', 'spectroscopy', 'in', 'outofplane', 'magnetic', 'fields', 'up', 'to', '30', 't', 'the', 'observed', 'g', 'factor', 'of', 'the', 'biexciton', 'amounts', ... | [-0.1570613731983704, 0.23270460520507186, -0.039594575306653966, 0.06744867540287992, -0.003970919213585417, -0.06503187689317942, 0.06381322595903098, 0.4609882992312864, -0.26887480853798074, -0.3357369286844645, -0.10644977009656874, -0.27348537500775244, -0.06421833593156878, 0.1775536038373873, 0.0990451813634502... |
1,801.09256 | Study on Energy Consumption and Coverage of Hierarchical Cooperation of
Small Cell Base Stations in Heterogeneous Networks | The demand for communication services in the era of intelligent terminals is
unprecedented and huge. To meet such development, modern wireless
communications must provide higher quality services with higher energy
efficiency in terms of system capacity and quality of service (QoS), which
could be achieved by the high... | cs.IT math.IT | the demand for communication services in the era of intelligent terminals is unprecedented and huge to meet such development modern wireless communications must provide higher quality services with higher energy efficiency in terms of system capacity and quality of service qos which could be achieved by the highspeed d... | [['the', 'demand', 'for', 'communication', 'services', 'in', 'the', 'era', 'of', 'intelligent', 'terminals', 'is', 'unprecedented', 'and', 'huge', 'to', 'meet', 'such', 'development', 'modern', 'wireless', 'communications', 'must', 'provide', 'higher', 'quality', 'services', 'with', 'higher', 'energy', 'efficiency', 'i... | [-0.2246574743655679, 0.04480052442371923, -0.012222246906280982, 0.023813450365771247, -0.04144302712647254, -0.14016872419314605, 0.15116279906354402, 0.34870814856677435, -0.24704298087024162, -0.34829550055507086, 0.07382229661540046, -0.2445836241496968, -0.12383990416935418, 0.17204321885766183, -0.11518141502572... |
1,801.09257 | Volume entropy and information flow in a brain graph | Entropy is a classical measure to quantify the amount of information or
complexity of a system. Various entropy-based measures such as functional and
spectral entropies have been proposed in brain network analysis. However, they
are less widely used than traditional graph theoretic measures such as global
and local e... | q-bio.NC q-bio.QM | entropy is a classical measure to quantify the amount of information or complexity of a system various entropybased measures such as functional and spectral entropies have been proposed in brain network analysis however they are less widely used than traditional graph theoretic measures such as global and local efficie... | [['entropy', 'is', 'a', 'classical', 'measure', 'to', 'quantify', 'the', 'amount', 'of', 'information', 'or', 'complexity', 'of', 'a', 'system', 'various', 'entropybased', 'measures', 'such', 'as', 'functional', 'and', 'spectral', 'entropies', 'have', 'been', 'proposed', 'in', 'brain', 'network', 'analysis', 'however',... | [-0.0846706061220543, 0.0809412305375282, -0.13504545289178488, 0.1149677156597029, -0.08860290837417609, -0.09611190164552225, 0.04386758330176294, 0.35107715741207124, -0.3003653334566818, -0.27968203303920713, 0.11996693714042968, -0.31233865768848523, -0.18127708529006228, 0.1458787740941578, -0.11083111314759081, ... |
1,801.09258 | Toward a Phenomenology of Computational Thinking in STEM Education | In this chapter, we argue for an epistemological shift from viewing coding
and computational thinking as mastery over computational logic and symbolic
forms, to viewing them as a more complex form of experience. Rather than
viewing computing as regurgitation and production of a set of axiomatic
computational abstract... | physics.ed-ph | in this chapter we argue for an epistemological shift from viewing coding and computational thinking as mastery over computational logic and symbolic forms to viewing them as a more complex form of experience rather than viewing computing as regurgitation and production of a set of axiomatic computational abstractions ... | [['in', 'this', 'chapter', 'we', 'argue', 'for', 'an', 'epistemological', 'shift', 'from', 'viewing', 'coding', 'and', 'computational', 'thinking', 'as', 'mastery', 'over', 'computational', 'logic', 'and', 'symbolic', 'forms', 'to', 'viewing', 'them', 'as', 'a', 'more', 'complex', 'form', 'of', 'experience', 'rather', ... | [-0.05021951130229833, 0.09756724882993838, -0.1033233400207552, 0.0818238217118625, -0.12648054543196371, -0.1607703469405686, 0.06765905891140726, 0.3758633950921266, -0.2665799771509084, -0.3475019413836938, 0.08490284889596392, -0.23721311551727062, -0.21501124258104123, 0.23213443868046038, -0.13571386775737138, -... |
1,801.09259 | Nonlinear refractive index of electric field aligned gold nanorods
measured with a Hartmann-Shack wavefront aberrometer | The capability to dynamically control the nonlinear refractive index of
plasmonic suspensions may enable innovative nonlinear sensing and signaling
nanotechnologies. Here, we experimentally determine the effective nonlinear
refractive index for gold nanorods suspended in an index matching oil aligned
using electric f... | physics.optics | the capability to dynamically control the nonlinear refractive index of plasmonic suspensions may enable innovative nonlinear sensing and signaling nanotechnologies here we experimentally determine the effective nonlinear refractive index for gold nanorods suspended in an index matching oil aligned using electric field... | [['the', 'capability', 'to', 'dynamically', 'control', 'the', 'nonlinear', 'refractive', 'index', 'of', 'plasmonic', 'suspensions', 'may', 'enable', 'innovative', 'nonlinear', 'sensing', 'and', 'signaling', 'nanotechnologies', 'here', 'we', 'experimentally', 'determine', 'the', 'effective', 'nonlinear', 'refractive', '... | [-0.09928479709028118, 0.2355438827389794, -0.05846806332482484, -0.04582954694489962, -0.04591475721732106, -0.1303796330045072, -0.02158135044189386, 0.49781433698059857, -0.2774338640333356, -0.31710152194727265, 0.05231855360899067, -0.2723895655843713, -0.1766858780014234, 0.21276468622280567, -0.0198315374141532,... |
1,801.0926 | Transition to turbulence in shear flows | Pipe flow and many other shear flows show a transition to turbulence at flow
rates for which the laminar profile is stable against infinitesimal
perturbations. In this brief review the recent progress in the understanding of
this transition will be summarized, with a focus on the linear and nonlinear
states that driv... | physics.flu-dyn nlin.CD | pipe flow and many other shear flows show a transition to turbulence at flow rates for which the laminar profile is stable against infinitesimal perturbations in this brief review the recent progress in the understanding of this transition will be summarized with a focus on the linear and nonlinear states that drive th... | [['pipe', 'flow', 'and', 'many', 'other', 'shear', 'flows', 'show', 'a', 'transition', 'to', 'turbulence', 'at', 'flow', 'rates', 'for', 'which', 'the', 'laminar', 'profile', 'is', 'stable', 'against', 'infinitesimal', 'perturbations', 'in', 'this', 'brief', 'review', 'the', 'recent', 'progress', 'in', 'the', 'understa... | [-0.1341489721218952, 0.2071026669970403, -0.09355755091463733, 0.04151608697429765, -0.027269235398206446, -0.0957967062972279, -0.015583754032074163, 0.35073333973398096, -0.30338234742844683, -0.2205219834124566, 0.1563480650301143, -0.2594840966695402, -0.18022369282941023, 0.1658657586344311, -0.003896047406467712... |
1,801.09261 | Inverse Uncertainty Quantification using the Modular Bayesian Approach
based on Gaussian Process, Part 2: Application to TRACE | Inverse Uncertainty Quantification (UQ) is a process to quantify the
uncertainties in random input parameters while achieving consistency between
code simulations and physical observations. In this paper, we performed inverse
UQ using an improved modular Bayesian approach based on Gaussian Process (GP)
for TRACE phys... | stat.AP | inverse uncertainty quantification uq is a process to quantify the uncertainties in random input parameters while achieving consistency between code simulations and physical observations in this paper we performed inverse uq using an improved modular bayesian approach based on gaussian process gp for trace physical mod... | [['inverse', 'uncertainty', 'quantification', 'uq', 'is', 'a', 'process', 'to', 'quantify', 'the', 'uncertainties', 'in', 'random', 'input', 'parameters', 'while', 'achieving', 'consistency', 'between', 'code', 'simulations', 'and', 'physical', 'observations', 'in', 'this', 'paper', 'we', 'performed', 'inverse', 'uq', ... | [-0.018318044156250025, 0.0256375422869934, -0.06892962816809477, 0.10173321664167613, -0.09495966209064204, -0.13977603957712376, 0.0802866056440743, 0.4011544389512252, -0.2555372193735955, -0.35220805208405687, 0.1226285583628514, -0.23922571240303417, -0.06823191766765106, 0.20971659957345024, -0.04198463848033161,... |
1,801.09262 | Cell-less Communications in 5G Vehicular Networks Based on
Vehicle-Installed Access Points | The development of intelligent transportation systems raises many
requirements to the current vehicular networks. For instance, to ensure secure
communications between vehicles, low latency, high connectivity and high data
rate are required for vehicular networks. To meet such requirements, the 5G
communication syste... | cs.NI | the development of intelligent transportation systems raises many requirements to the current vehicular networks for instance to ensure secure communications between vehicles low latency high connectivity and high data rate are required for vehicular networks to meet such requirements the 5g communication systems for v... | [['the', 'development', 'of', 'intelligent', 'transportation', 'systems', 'raises', 'many', 'requirements', 'to', 'the', 'current', 'vehicular', 'networks', 'for', 'instance', 'to', 'ensure', 'secure', 'communications', 'between', 'vehicles', 'low', 'latency', 'high', 'connectivity', 'and', 'high', 'data', 'rate', 'are... | [-0.3028405544212131, 0.02501194745388334, 0.021652576065423087, -0.006694391015863229, -0.08114391509470438, -0.2569673178782094, 0.13241201909033534, 0.41156448388332234, -0.25354984555005855, -0.29882838166819486, 0.07669963833951321, -0.2535354132263388, -0.16276280739010887, 0.16460269526309318, -0.170023428260031... |
1,801.09263 | Fast hybrid density-functional computations using plane-wave basis sets | A new, very fast, implementation of the exact (Fock) exchange operator for
electronic structure calculations within the plane-wave pseudopotential method
is described in detail for both molecular and periodic systems, and carefully
validated. Our method combines the recently proposed Adaptively Compressed
Exchange ap... | cond-mat.mtrl-sci physics.chem-ph physics.comp-ph | a new very fast implementation of the exact fock exchange operator for electronic structure calculations within the planewave pseudopotential method is described in detail for both molecular and periodic systems and carefully validated our method combines the recently proposed adaptively compressed exchange approach to... | [['a', 'new', 'very', 'fast', 'implementation', 'of', 'the', 'exact', 'fock', 'exchange', 'operator', 'for', 'electronic', 'structure', 'calculations', 'within', 'the', 'planewave', 'pseudopotential', 'method', 'is', 'described', 'in', 'detail', 'for', 'both', 'molecular', 'and', 'periodic', 'systems', 'and', 'carefull... | [-0.11111379760716643, 0.08150604808179196, -0.079284124197184, 0.05673743535651035, -0.009365036340132981, -0.11638196992116566, 0.054325347601929135, 0.37443876340828774, -0.2387068334090359, -0.32252470535390515, 0.06321297269784101, -0.24966013904645287, -0.10951386844473225, 0.24168438823236263, 0.0198980539023657... |
1,801.09264 | An Energy Stable One-Field Fictitious Domain Method for Fluid-Structure
Interactions | In this article, the energy stability of a one-field fictitious domain method
is proved and validated by numerical tests in two and three dimensions. The
distinguishing feature of this method is that it only solves for one velocity
field for the whole fluid-structure domain; the interactions remain decoupled
until so... | cs.CE physics.comp-ph | in this article the energy stability of a onefield fictitious domain method is proved and validated by numerical tests in two and three dimensions the distinguishing feature of this method is that it only solves for one velocity field for the whole fluidstructure domain the interactions remain decoupled until solving t... | [['in', 'this', 'article', 'the', 'energy', 'stability', 'of', 'a', 'onefield', 'fictitious', 'domain', 'method', 'is', 'proved', 'and', 'validated', 'by', 'numerical', 'tests', 'in', 'two', 'and', 'three', 'dimensions', 'the', 'distinguishing', 'feature', 'of', 'this', 'method', 'is', 'that', 'it', 'only', 'solves', '... | [-0.11181107472016741, 0.0851459147136245, -0.08828888883216501, 0.0251038213844286, -0.02723628809369767, -0.11790442802081469, -0.01970386114353731, 0.35529088288017396, -0.3010696124619068, -0.2747399859728097, 0.14632804047510917, -0.2513846141710155, -0.09362769946881654, 0.19064403983500244, -0.017756225000858418... |
1,801.09265 | The weakly dependent strong law of large numbers revisited | We give a short, self-contained, and elementary proof of the strong law of
large numbers under a power law decay hypothesis for joint second moments. The
result is related to the classical one by Lyons. However, we also provide a
rate of convergence. Our proof does not use maximal inequalities and is instead
inspired... | math.PR math.CA | we give a short selfcontained and elementary proof of the strong law of large numbers under a power law decay hypothesis for joint second moments the result is related to the classical one by lyons however we also provide a rate of convergence our proof does not use maximal inequalities and is instead inspired by the m... | [['we', 'give', 'a', 'short', 'selfcontained', 'and', 'elementary', 'proof', 'of', 'the', 'strong', 'law', 'of', 'large', 'numbers', 'under', 'a', 'power', 'law', 'decay', 'hypothesis', 'for', 'joint', 'second', 'moments', 'the', 'result', 'is', 'related', 'to', 'the', 'classical', 'one', 'by', 'lyons', 'however', 'we'... | [-0.1078131279665167, 0.11724554301927918, -0.12956548663045186, 0.10848347984753764, -0.10271655673674052, -0.13648489512422163, 0.06674596319899664, 0.24585814521634491, -0.2717842266395472, -0.2789920569950904, 0.09523852509311467, -0.21750021472141362, -0.1443211489459972, 0.24037919406765612, -0.11611341365167628,... |
1,801.09266 | Reducible subgroups of exceptional algebraic groups | Let $G$ be a simple algebraic group over an algebraically closed field. A
closed subgroup $H$ of $G$ is called $G$-completely reducible ($G$-cr) if,
whenever $H$ is contained in a parabolic subgroup $P$ of $G$, it is contained
in a Levi factor of $P$. In this paper we complete the classification of
connected $G$-cr s... | math.GR math.RT | let g be a simple algebraic group over an algebraically closed field a closed subgroup h of g is called gcompletely reducible gcr if whenever h is contained in a parabolic subgroup p of g it is contained in a levi factor of p in this paper we complete the classification of connected gcr subgroups when g has exceptional... | [['let', 'g', 'be', 'a', 'simple', 'algebraic', 'group', 'over', 'an', 'algebraically', 'closed', 'field', 'a', 'closed', 'subgroup', 'h', 'of', 'g', 'is', 'called', 'gcompletely', 'reducible', 'gcr', 'if', 'whenever', 'h', 'is', 'contained', 'in', 'a', 'parabolic', 'subgroup', 'p', 'of', 'g', 'it', 'is', 'contained', ... | [-0.2129559579961857, 0.0958738441192106, -0.09018607302492515, 0.0009549723071672144, -0.16713437640688336, -0.1295331899672136, 0.002215979701923359, 0.3807570052134698, -0.2887342967451779, -0.2096854156325953, 0.0623088848460313, -0.2378776078494113, -0.10518621849626127, 0.21425587641930238, -0.1703138266552667, -... |
1,801.09267 | Clean Os(0001) electronic surface states: a first-principle fully
relativistic investigation | We analyze the electronic structure of the Os(0001) surface by means of
first-principle calculations based on Fully Relativistic (FR) Density
Functional Theory (DFT) and a Projector Augmented-Wave (PAW) approach. We
investigate surface states and resonances analyzing their spin-orbit induced
energy splitting and thei... | cond-mat.mtrl-sci | we analyze the electronic structure of the os0001 surface by means of firstprinciple calculations based on fully relativistic fr density functional theory dft and a projector augmentedwave paw approach we investigate surface states and resonances analyzing their spinorbit induced energy splitting and their spin polariz... | [['we', 'analyze', 'the', 'electronic', 'structure', 'of', 'the', 'os0001', 'surface', 'by', 'means', 'of', 'firstprinciple', 'calculations', 'based', 'on', 'fully', 'relativistic', 'fr', 'density', 'functional', 'theory', 'dft', 'and', 'a', 'projector', 'augmentedwave', 'paw', 'approach', 'we', 'investigate', 'surface... | [-0.16374279992554588, 0.14280202767373626, -0.08026910617053018, 0.0728618888556651, -0.03705238635149343, -0.11230494249244466, 0.03590934817284027, 0.43277471925524114, -0.2446416593616289, -0.3038208611806591, -0.018405147034699393, -0.2847570574621817, -0.13762796827971838, 0.16772577482640227, 0.03782347975433559... |
1,801.09268 | A Finite Soluble Quotient Algorithm | An algorithm for computing power conjugate presentations for finite soluble
quotients of predetermined structure of finitely presented groups is described.
Practical aspects of an implementation are discussed.
| math.GR | an algorithm for computing power conjugate presentations for finite soluble quotients of predetermined structure of finitely presented groups is described practical aspects of an implementation are discussed | [['an', 'algorithm', 'for', 'computing', 'power', 'conjugate', 'presentations', 'for', 'finite', 'soluble', 'quotients', 'of', 'predetermined', 'structure', 'of', 'finitely', 'presented', 'groups', 'is', 'described', 'practical', 'aspects', 'of', 'an', 'implementation', 'are', 'discussed']] | [-0.16565700034024539, 0.11735255061756578, -0.04718559069765939, 0.04599230702431804, -0.06998345131675403, -0.18943994575076634, -0.058366842895608256, 0.4368258894041733, -0.3383534674843152, -0.19108905091329856, 0.09573934447986109, -0.2443801541640251, -0.09861200923720996, 0.3094079619687464, -0.1393241036545347... |
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