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 |
|---|---|---|---|---|---|---|
1,801.09869 | Assessment of interaction-strength interpolation formulas for gold and
silver clusters | The performance of functionals based on the idea of interpolating between the
weak and the strong-interaction limits the global adiabatic-connection
integrand is carefully studied for the challenging case of noble-metal
clusters. Different interpolation formulas are considered and various features
of this approach ar... | physics.chem-ph cond-mat.other physics.atm-clus | the performance of functionals based on the idea of interpolating between the weak and the stronginteraction limits the global adiabaticconnection integrand is carefully studied for the challenging case of noblemetal clusters different interpolation formulas are considered and various features of this approach are anal... | [['the', 'performance', 'of', 'functionals', 'based', 'on', 'the', 'idea', 'of', 'interpolating', 'between', 'the', 'weak', 'and', 'the', 'stronginteraction', 'limits', 'the', 'global', 'adiabaticconnection', 'integrand', 'is', 'carefully', 'studied', 'for', 'the', 'challenging', 'case', 'of', 'noblemetal', 'clusters',... | [-0.0703456553139834, 0.06847002429346885, -0.09853573864506136, 0.15450973089243616, 0.010940374879126427, -0.11957947242884867, 0.005691994757701953, 0.3968763787259338, -0.2220747704787921, -0.30534475029856767, 0.08137604161616295, -0.261303855717102, -0.12319963462450491, 0.24948479382381325, 0.0021391814251953576... |
1,801.0987 | Fast Power system security analysis with Guided Dropout | We propose a new method to efficiently compute load-flows (the steady-state
of the power-grid for given productions, consumptions and grid topology),
substituting conventional simulators based on differential equation solvers. We
use a deep feed-forward neural network trained with load-flows precomputed by
simulation... | stat.ML cs.LG | we propose a new method to efficiently compute loadflows the steadystate of the powergrid for given productions consumptions and grid topology substituting conventional simulators based on differential equation solvers we use a deep feedforward neural network trained with loadflows precomputed by simulation our archite... | [['we', 'propose', 'a', 'new', 'method', 'to', 'efficiently', 'compute', 'loadflows', 'the', 'steadystate', 'of', 'the', 'powergrid', 'for', 'given', 'productions', 'consumptions', 'and', 'grid', 'topology', 'substituting', 'conventional', 'simulators', 'based', 'on', 'differential', 'equation', 'solvers', 'we', 'use',... | [-0.07584458389222466, 0.001253240909136366, -0.061346218533193074, 0.06810868716759917, -0.1355752234424775, -0.2059003386287562, 0.09016401261518088, 0.42870412262467045, -0.2886171213003763, -0.31109706650992547, 0.06642305886756124, -0.2248157232035434, -0.21536066927365027, 0.18297040043701904, -0.0740713568326706... |
1,801.09871 | An infinite family of subcubic graphs with unbounded packing chromatic
number | Recently, Balogh, Kostochka and Liu in [Packing chromatic number of cubic
graphs, Discrete Math.~341 (2018) 474--483] answered in negative the question
that was posed in several earlier papers whether the packing chromatic number
is bounded in the class of graphs with maximum degree $3$. In this note, we
present an e... | math.CO | recently balogh kostochka and liu in packing chromatic number of cubic graphs discrete math341 2018 474483 answered in negative the question that was posed in several earlier papers whether the packing chromatic number is bounded in the class of graphs with maximum degree 3 in this note we present an explicit infinite ... | [['recently', 'balogh', 'kostochka', 'and', 'liu', 'in', 'packing', 'chromatic', 'number', 'of', 'cubic', 'graphs', 'discrete', 'math341', '2018', '474483', 'answered', 'in', 'negative', 'the', 'question', 'that', 'was', 'posed', 'in', 'several', 'earlier', 'papers', 'whether', 'the', 'packing', 'chromatic', 'number', ... | [-0.19641131328387282, 0.18500099265854214, 0.0048720433645076675, 0.007199689319704549, -0.15413878012006565, -0.11099326485862672, 0.03184937339639133, 0.34467536343608873, -0.2266279823951802, -0.4420233117890055, 0.09160602536502342, -0.30366391926151465, -0.18789897679146064, 0.10771632047717349, -0.19166925617383... |
1,801.09872 | A State-of-the-Art of Semantic Change Computation | This paper reviews the state-of-the-art of semantic change computation, one
emerging research field in computational linguistics, proposing a framework
that summarizes the literature by identifying and expounding five essential
components in the field: diachronic corpus, diachronic word sense
characterization, change... | cs.CL | this paper reviews the stateoftheart of semantic change computation one emerging research field in computational linguistics proposing a framework that summarizes the literature by identifying and expounding five essential components in the field diachronic corpus diachronic word sense characterization change modelling... | [['this', 'paper', 'reviews', 'the', 'stateoftheart', 'of', 'semantic', 'change', 'computation', 'one', 'emerging', 'research', 'field', 'in', 'computational', 'linguistics', 'proposing', 'a', 'framework', 'that', 'summarizes', 'the', 'literature', 'by', 'identifying', 'and', 'expounding', 'five', 'essential', 'compone... | [-0.07361059642921225, 0.0021863454921531075, -0.061346532287811784, 0.08846059982653144, -0.16608133231203595, -0.09000293287925985, 0.06914964888906185, 0.38941239477956996, -0.23566842860221363, -0.3595840542131111, 0.08811473158582411, -0.2864179634606513, -0.12853811705531945, 0.2352885318716534, -0.08730605566661... |
1,801.09873 | Condition for confinement in non-Abelian gauge theories | We show that a criterion for confinement, based on the BRST invariance, holds
in four dimensions, by solving a non-Abelian gauge theory with a set of exact
solutions. The confinement condition we consider was obtained by Kugo and Ojima
some decades ago. The current understanding of gauge theories permits us to
apply ... | hep-th hep-ph math-ph math.MP | we show that a criterion for confinement based on the brst invariance holds in four dimensions by solving a nonabelian gauge theory with a set of exact solutions the confinement condition we consider was obtained by kugo and ojima some decades ago the current understanding of gauge theories permits us to apply the tech... | [['we', 'show', 'that', 'a', 'criterion', 'for', 'confinement', 'based', 'on', 'the', 'brst', 'invariance', 'holds', 'in', 'four', 'dimensions', 'by', 'solving', 'a', 'nonabelian', 'gauge', 'theory', 'with', 'a', 'set', 'of', 'exact', 'solutions', 'the', 'confinement', 'condition', 'we', 'consider', 'was', 'obtained', ... | [-0.13078173939588436, 0.15841603932362472, -0.14823363301217218, 0.0954188422977247, -0.08798364756247876, -0.13615144855363973, 0.02977073450826786, 0.35896949260495603, -0.17756782454142178, -0.27323787983782083, 0.08112959666389295, -0.1718566048128361, -0.18396405486220663, 0.11745573014063253, -0.0837617024292492... |
1,801.09874 | Change point analysis in non-stationary processes - a mass excess
approach | This paper considers the problem of testing if a sequence of means
$(\mu_t)_{t =1,\ldots ,n }$ of a non-stationary time series $(X_t)_{t =1,\ldots
,n }$ is stable in the sense that the difference of the means $\mu_1$ and
$\mu_t$ between the initial time $t=1$ and any other time is smaller than a
given level, that is ... | stat.ME math.ST stat.TH | this paper considers the problem of testing if a sequence of means mu_t_t 1ldots n of a nonstationary time series x_t_t 1ldots n is stable in the sense that the difference of the means mu_1 and mu_t between the initial time t1 and any other time is smaller than a given level that is mu_1 mu_t leq c for all t 1ldots n a... | [['this', 'paper', 'considers', 'the', 'problem', 'of', 'testing', 'if', 'a', 'sequence', 'of', 'means', 'mu_t_t', '1ldots', 'n', 'of', 'a', 'nonstationary', 'time', 'series', 'x_t_t', '1ldots', 'n', 'is', 'stable', 'in', 'the', 'sense', 'that', 'the', 'difference', 'of', 'the', 'means', 'mu_1', 'and', 'mu_t', 'between... | [-0.12690031462705564, 0.10744804212363707, -0.0995892840232583, 0.09153660277633946, -0.012850133245283703, -0.13608826466970755, 0.05587429918916954, 0.3198090293356832, -0.2520041937277939, -0.23996679285839903, 0.12334695873041081, -0.2803337278090558, -0.10962955290949522, 0.20799378202876673, -0.03974404030789932... |
1,801.09875 | Boundary effect in competition processes | This paper studies the long-term behaviour of a continuous time Markov chain
formed by two non-negative integer valued components that evolve subject to a
competitive interaction. In the absence of interaction the Markov chain is just
a pair of independent linear birth processes with immigration. Interactions of
inte... | math.PR | this paper studies the longterm behaviour of a continuous time markov chain formed by two nonnegative integer valued components that evolve subject to a competitive interaction in the absence of interaction the markov chain is just a pair of independent linear birth processes with immigration interactions of interest i... | [['this', 'paper', 'studies', 'the', 'longterm', 'behaviour', 'of', 'a', 'continuous', 'time', 'markov', 'chain', 'formed', 'by', 'two', 'nonnegative', 'integer', 'valued', 'components', 'that', 'evolve', 'subject', 'to', 'a', 'competitive', 'interaction', 'in', 'the', 'absence', 'of', 'interaction', 'the', 'markov', '... | [-0.13492011984993443, 0.173831881370446, -0.032221853258336326, 0.05269018205636399, -0.05982925109450751, -0.19547475178985566, 0.026538219235142785, 0.35016844413991344, -0.30179868490419914, -0.2233331347519883, 0.11324646126681207, -0.29568684852842364, -0.10815734581899691, 0.10915028694711748, -0.014973944091222... |
1,801.09876 | Cavity-assisted mesoscopic transport of fermions: Coherent and
dissipative dynamics | We study the interplay between charge transport and light-matter interactions
in a confined geometry, by considering an open, mesoscopic chain of two-orbital
systems resonantly coupled to a single bosonic mode close to its vacuum state.
We introduce and benchmark different methods based on self-consistent solutions
o... | quant-ph cond-mat.mes-hall | we study the interplay between charge transport and lightmatter interactions in a confined geometry by considering an open mesoscopic chain of twoorbital systems resonantly coupled to a single bosonic mode close to its vacuum state we introduce and benchmark different methods based on selfconsistent solutions of nonequ... | [['we', 'study', 'the', 'interplay', 'between', 'charge', 'transport', 'and', 'lightmatter', 'interactions', 'in', 'a', 'confined', 'geometry', 'by', 'considering', 'an', 'open', 'mesoscopic', 'chain', 'of', 'twoorbital', 'systems', 'resonantly', 'coupled', 'to', 'a', 'single', 'bosonic', 'mode', 'close', 'to', 'its', ... | [-0.17465164537558545, 0.17129371574333163, -0.044089701713346585, 0.027008732773538213, -0.017175388133182423, -0.14917139401465343, 0.09112396831066387, 0.34716307727406576, -0.25946463196669356, -0.26999465840829845, 0.03415655127294789, -0.2795612557480733, -0.09663389926815096, 0.22218150881841817, 0.0447424170997... |
1,801.09877 | On the Use of the Observability Gramian for Partially Observed Robotic
Path Planning Problems | Optimizing measures of the observability Gramian as a surrogate for the
estimation performance may provide irrelevant or misleading trajectories for
planning under observation uncertainty.
| cs.RO cs.SY | optimizing measures of the observability gramian as a surrogate for the estimation performance may provide irrelevant or misleading trajectories for planning under observation uncertainty | [['optimizing', 'measures', 'of', 'the', 'observability', 'gramian', 'as', 'a', 'surrogate', 'for', 'the', 'estimation', 'performance', 'may', 'provide', 'irrelevant', 'or', 'misleading', 'trajectories', 'for', 'planning', 'under', 'observation', 'uncertainty']] | [-0.11866651529756685, 0.010599154513329268, -0.10911547784538318, 0.15273975923870844, -0.060361202845039465, -0.15690579604900753, 0.062474114393504955, 0.3543352415629973, -0.2337654901202768, -0.3103244323283434, 0.19587605741495887, -0.2579115619882941, -0.10559223496238701, 0.21399886018480174, -0.167403228309315... |
1,801.09878 | Critical behavior of two-dimensional intrinsically ferromagnetic
semiconductor CrI3 | CrI3, which belongs to a rare category of two-dimensional (2D) ferromagnetic
semiconductors, is of great interest for spintronic device applications. Unlike
CrCl3 whose magnetism presents a 2D-Heisenberg behavior, CrI3 exhibits a larger
van der Waals gap, smaller cleavage energy, and stronger magnetic anisotropy
whic... | cond-mat.mtrl-sci | cri3 which belongs to a rare category of twodimensional 2d ferromagnetic semiconductors is of great interest for spintronic device applications unlike crcl3 whose magnetism presents a 2dheisenberg behavior cri3 exhibits a larger van der waals gap smaller cleavage energy and stronger magnetic anisotropy which could lead... | [['cri3', 'which', 'belongs', 'to', 'a', 'rare', 'category', 'of', 'twodimensional', '2d', 'ferromagnetic', 'semiconductors', 'is', 'of', 'great', 'interest', 'for', 'spintronic', 'device', 'applications', 'unlike', 'crcl3', 'whose', 'magnetism', 'presents', 'a', '2dheisenberg', 'behavior', 'cri3', 'exhibits', 'a', 'la... | [-0.18134248901433866, 0.15196779170058924, -0.05724488568833426, 0.032212878799991414, -0.0542238923228996, -0.19102227521486254, 0.07893657102469215, 0.3385924538904977, -0.25559915396320465, -0.28451871877512747, -0.02775557117050502, -0.34179986446638994, -0.17517788988668412, 0.20818082208499172, 0.076405384421125... |
1,801.09879 | Chiral Lagrangians with decuplet baryons to one loop | We construct the relativistic chiral Lagrangians with decuplet baryons up to
the order $\mathcal{O}(p^4)$ (one loop). For the meson-decuplet-decuplet
couplings, there are 1, 13, 55, and 548 terms in the
$\mathcal{O}(p^1)$-$\mathcal{O}(p^4)$ order Lagrangians, respectively. For the
meson-octet-decuplet Lagrangians, th... | hep-ph nucl-th | we construct the relativistic chiral lagrangians with decuplet baryons up to the order mathcalop4 one loop for the mesondecupletdecuplet couplings there are 1 13 55 and 548 terms in the mathcalop1mathcalop4 order lagrangians respectively for the mesonoctetdecuplet lagrangians the number of independent terms from mathca... | [['we', 'construct', 'the', 'relativistic', 'chiral', 'lagrangians', 'with', 'decuplet', 'baryons', 'up', 'to', 'the', 'order', 'mathcalop4', 'one', 'loop', 'for', 'the', 'mesondecupletdecuplet', 'couplings', 'there', 'are', '1', '13', '55', 'and', '548', 'terms', 'in', 'the', 'mathcalop1mathcalop4', 'order', 'lagrangi... | [-0.16062911446317144, 0.1787667545999977, 0.001775996582139106, 0.07439264200539106, -0.05168815103492567, -0.10993537343373257, 0.017398005894695718, 0.328960593346329, -0.18541578394139097, -0.34272829630035195, 0.021424444496265745, -0.3657800469192721, -0.06904576182742381, 0.12297749443955365, 0.05239882987613479... |
1,801.0988 | An application of collapsing levels to the representation theory of
affine vertex algebras | We discover a large class of simple affine vertex algebras $V_{k} (\mathfrak
g)$, associated to basic Lie superalgebras $\mathfrak g$ at non-admissible
collapsing levels $k$, having exactly one irreducible $\mathfrak g$-locally
finite module in the category ${\mathcal O}$. In the case when $\mathfrak g$ is
a Lie alge... | math.RT math-ph math.MP math.QA | we discover a large class of simple affine vertex algebras v_k mathfrak g associated to basic lie superalgebras mathfrak g at nonadmissible collapsing levels k having exactly one irreducible mathfrak glocally finite module in the category mathcal o in the case when mathfrak g is a lie algebra we prove a complete reduci... | [['we', 'discover', 'a', 'large', 'class', 'of', 'simple', 'affine', 'vertex', 'algebras', 'v_k', 'mathfrak', 'g', 'associated', 'to', 'basic', 'lie', 'superalgebras', 'mathfrak', 'g', 'at', 'nonadmissible', 'collapsing', 'levels', 'k', 'having', 'exactly', 'one', 'irreducible', 'mathfrak', 'glocally', 'finite', 'modul... | [-0.20780000489173553, 0.0917820139854438, 0.006945104247464215, 0.037140266745848485, -0.17005499337910343, -0.23762806272528814, -0.03325242126780815, 0.3668602099800009, -0.36622259462788953, -0.15612893276926826, 0.042985916767127305, -0.25841819668599103, -0.08457990828543897, 0.1203602018008419, -0.12093257280540... |
1,801.09881 | Do the contact angle and line tension of surface-attached droplets
depend on the radius of curvature? | Results from Monte Carlo simulations of wall-attached droplets in the
three-dimensional Ising lattice gas model and in a symmetric binary
Lennard-Jones fluid, confined by antisymmetric walls, are analyzed, with the
aim to estimate the dependence of the contact angle $(\Theta)$ on the droplet
radius $(R)$ of curvature... | cond-mat.soft cond-mat.stat-mech | results from monte carlo simulations of wallattached droplets in the threedimensional ising lattice gas model and in a symmetric binary lennardjones fluid confined by antisymmetric walls are analyzed with the aim to estimate the dependence of the contact angle theta on the droplet radius r of curvature spherecap shape ... | [['results', 'from', 'monte', 'carlo', 'simulations', 'of', 'wallattached', 'droplets', 'in', 'the', 'threedimensional', 'ising', 'lattice', 'gas', 'model', 'and', 'in', 'a', 'symmetric', 'binary', 'lennardjones', 'fluid', 'confined', 'by', 'antisymmetric', 'walls', 'are', 'analyzed', 'with', 'the', 'aim', 'to', 'estim... | [-0.09182890338320249, 0.14440264559385696, -0.10629307386443543, 0.05408337759581627, -0.053582844831908005, -0.12963218319237058, 0.045142066930566216, 0.37452128134464147, -0.24643358156572504, -0.3158464087136963, 0.06987235912083634, -0.29629784700955497, -0.09109927922668248, 0.15418594169250355, -0.0332278293662... |
1,801.09882 | Hamming weight and tight constraints of multi-qubit entanglement in
terms of unified entropy | We establish a characterization of multi-qubit entanglement constraints in
terms of non-negative power of entanglement measures based on unified-$(q,s)$
entropy. Using the Hamming weight of the binary vector related with the
distribution of subsystems, we establish a class of tight monogamy inequalities
of multi-qubi... | quant-ph | we establish a characterization of multiqubit entanglement constraints in terms of nonnegative power of entanglement measures based on unifiedqs entropy using the hamming weight of the binary vector related with the distribution of subsystems we establish a class of tight monogamy inequalities of multiqubit entanglemen... | [['we', 'establish', 'a', 'characterization', 'of', 'multiqubit', 'entanglement', 'constraints', 'in', 'terms', 'of', 'nonnegative', 'power', 'of', 'entanglement', 'measures', 'based', 'on', 'unifiedqs', 'entropy', 'using', 'the', 'hamming', 'weight', 'of', 'the', 'binary', 'vector', 'related', 'with', 'the', 'distribu... | [-0.16910183327455147, 0.15268957775140948, -0.030503655016860542, 0.05558596992883466, 0.060776879371819546, -0.2473337679927913, 0.06765220678575776, 0.28537133203673304, -0.2186010581459485, -0.2329003557781963, 0.0442966453105613, -0.28052895188368127, -0.08026230119753118, 0.2193307338611168, -0.05726837672238402,... |
1,801.09883 | Comparison of robustness of statistical procedures for network structure
analysis | Different network structures are compiared with respect to degree of
robustnes of identification statistical procedures. It is shown that threshold
(market) graph, cliques and independent sets in the threshold (market) graphs
are preferable network structure from this point of view.
| math.ST stat.TH | different network structures are compiared with respect to degree of robustnes of identification statistical procedures it is shown that threshold market graph cliques and independent sets in the threshold market graphs are preferable network structure from this point of view | [['different', 'network', 'structures', 'are', 'compiared', 'with', 'respect', 'to', 'degree', 'of', 'robustnes', 'of', 'identification', 'statistical', 'procedures', 'it', 'is', 'shown', 'that', 'threshold', 'market', 'graph', 'cliques', 'and', 'independent', 'sets', 'in', 'the', 'threshold', 'market', 'graphs', 'are'... | [-0.12965525698688762, 0.04670727108972833, -0.0800515375541229, 0.0722937640292864, -0.07004911619189538, -0.14148763081941165, 0.08365332256806524, 0.469981334711376, -0.31018184056799664, -0.2968457117508239, 0.10341218546167702, -0.2941197748050878, -0.1958890976874452, 0.14152779876205482, -0.10156689439655135, 0.... |
1,801.09884 | Estimation of conditional extreme risk measures from heavy-tailed
elliptical random vectors | In this work, we focus on some conditional extreme risk measures estimation
for elliptical random vectors. In a previous paper, we proposed a methodology
to approximate extreme quantiles, based on two extremal parameters. We thus
propose some estimators for these parameters, and study their asymptotic
properties in t... | math.ST stat.TH | in this work we focus on some conditional extreme risk measures estimation for elliptical random vectors in a previous paper we proposed a methodology to approximate extreme quantiles based on two extremal parameters we thus propose some estimators for these parameters and study their asymptotic properties in the case ... | [['in', 'this', 'work', 'we', 'focus', 'on', 'some', 'conditional', 'extreme', 'risk', 'measures', 'estimation', 'for', 'elliptical', 'random', 'vectors', 'in', 'a', 'previous', 'paper', 'we', 'proposed', 'a', 'methodology', 'to', 'approximate', 'extreme', 'quantiles', 'based', 'on', 'two', 'extremal', 'parameters', 'w... | [-0.03917662581767548, 0.011609585187397898, -0.1423400434411385, 0.17160558458100159, -0.0402970412153412, -0.08863381223213351, 0.10672211854147132, 0.4488097681240602, -0.17058223084207963, -0.2686785247938877, 0.15965019928037444, -0.291316273893145, -0.19146066912534562, 0.20998798528559168, -0.17097900755788115, ... |
1,801.09885 | Evaporation-triggered segregation of sessile binary droplets | Droplet evaporation of multicomponent droplets is essential for various
physiochemical applications, e.g. in inkjet printing, spray cooling and
microfabrication. In this work, we observe and study phase segregation of an
evaporating sessile binary droplet, consisting of a mixture of water and a
surfactant-like liquid... | physics.flu-dyn | droplet evaporation of multicomponent droplets is essential for various physiochemical applications eg in inkjet printing spray cooling and microfabrication in this work we observe and study phase segregation of an evaporating sessile binary droplet consisting of a mixture of water and a surfactantlike liquid 12hexaned... | [['droplet', 'evaporation', 'of', 'multicomponent', 'droplets', 'is', 'essential', 'for', 'various', 'physiochemical', 'applications', 'eg', 'in', 'inkjet', 'printing', 'spray', 'cooling', 'and', 'microfabrication', 'in', 'this', 'work', 'we', 'observe', 'and', 'study', 'phase', 'segregation', 'of', 'an', 'evaporating'... | [-0.06776216257455163, 0.23155116606382062, -0.12456555175380285, -0.021587624199724577, 0.009671023252923957, -0.10879143111056602, 0.02526133760454927, 0.30784065038591746, -0.25956375213324656, -0.30174002527892896, 0.12208923795374996, -0.2771448500103271, -0.12082266105629015, 0.16126510884219658, -0.0352025045545... |
1,801.09886 | Positivity preserving along a flow over projective bundle | In this paper, we introduce a flow over the projective bundle $p:P(E^*)\to
M$, which is a natural generalization of both Hermitian-Yang-Mills flow and
K\"ahler-Ricci flow. We prove that the semipositivity of curvature of the
hyperplane line bundle $\mathcal{O}_{P(E^*)}(1)$ is preserved along this flow
under the null ... | math.DG math.AP | in this paper we introduce a flow over the projective bundle ppeto m which is a natural generalization of both hermitianyangmills flow and kahlerricci flow we prove that the semipositivity of curvature of the hyperplane line bundle mathcalo_pe1 is preserved along this flow under the null eigenvector assumption as appli... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'flow', 'over', 'the', 'projective', 'bundle', 'ppeto', 'm', 'which', 'is', 'a', 'natural', 'generalization', 'of', 'both', 'hermitianyangmills', 'flow', 'and', 'kahlerricci', 'flow', 'we', 'prove', 'that', 'the', 'semipositivity', 'of', 'curvature', 'of', 'the', 'hyperp... | [-0.28197026290759747, 0.03701102032269142, -0.1496540417761675, 0.031077930115743026, -0.0885246936992115, -0.13160366819677305, -0.07761547581306943, 0.3835922914310073, -0.34423360825345223, -0.11739532697746265, 0.1481539480689894, -0.21737739841966908, -0.1819264357149297, 0.16257030845201592, -0.18156995099722123... |
1,801.09887 | Contribution of the Extreme Term in the Sum of Samples with Regularly
Varying Tail | For a sequence of random variables $(X_1, X_2, \ldots, X_n)$, $n \geq 1$,
that are independent and identically distributed with a regularly varying tail
with index $-\alpha$, $\alpha \geq 0$, we show that the contribution of the
maximum term $M_n \triangleq \max(X_1,\ldots,X_n)$ in the sum $S_n \triangleq
X_1 + \cdot... | math.PR cs.IT math.IT | for a sequence of random variables x_1 x_2 ldots x_n n geq 1 that are independent and identically distributed with a regularly varying tail with index alpha alpha geq 0 we show that the contribution of the maximum term m_n triangleq maxx_1ldotsx_n in the sum s_n triangleq x_1 cdots x_n as n to infty decreases monotonic... | [['for', 'a', 'sequence', 'of', 'random', 'variables', 'x_1', 'x_2', 'ldots', 'x_n', 'n', 'geq', '1', 'that', 'are', 'independent', 'and', 'identically', 'distributed', 'with', 'a', 'regularly', 'varying', 'tail', 'with', 'index', 'alpha', 'alpha', 'geq', '0', 'we', 'show', 'that', 'the', 'contribution', 'of', 'the', '... | [-0.23763848447286692, 0.3190389291276453, -0.005385843059811436, -0.0712859232635161, 0.057150785643302025, -0.21869170670321242, -0.021783132501114466, 0.40995613992458485, -0.3673813869474364, -0.17896804543303663, 0.021109457276608855, -0.4109348977198366, -0.05683893429069612, 0.0592837213981347, -0.04677404680090... |
1,801.09888 | SIR Coverage Analysis in Cellular Networks with Temporal Traffic: A
Stochastic Geometry Approach | The bloom in mobile applications not just bring in enjoyment to daily life,
but also imposes more complicated traffic situation on wireless network. A
complete understanding of the impact from traffic profile is thus essential for
network operators to respond adequately to the surge in data traffic. In this
paper, ba... | cs.IT math.IT | the bloom in mobile applications not just bring in enjoyment to daily life but also imposes more complicated traffic situation on wireless network a complete understanding of the impact from traffic profile is thus essential for network operators to respond adequately to the surge in data traffic in this paper based on... | [['the', 'bloom', 'in', 'mobile', 'applications', 'not', 'just', 'bring', 'in', 'enjoyment', 'to', 'daily', 'life', 'but', 'also', 'imposes', 'more', 'complicated', 'traffic', 'situation', 'on', 'wireless', 'network', 'a', 'complete', 'understanding', 'of', 'the', 'impact', 'from', 'traffic', 'profile', 'is', 'thus', '... | [-0.15728173349099003, 0.054105999076215376, -0.05085758842870741, 0.08373641164333963, -0.06133132084013329, -0.1964174924228359, 0.16361190119192967, 0.37560876647464525, -0.22807719919538655, -0.30808427311486997, 0.07558924235306236, -0.2728802682901385, -0.17510919351436532, 0.1465755048154654, -0.15682889130175, ... |
1,801.09889 | Variational and viscosity operators for the evolutive Hamilton-Jacobi
equation | We study the Cauchy problem for the first order evolutive Hamilton-Jacobi
equation with a Lipschitz initial condition. The Hamiltonian is not necessarily
convex in the momentum variable and not a priori compactly supported. We build
and study an operator giving a variational solution of this problem, and get
local Li... | math.SG math.AP math.DS math.OC | we study the cauchy problem for the first order evolutive hamiltonjacobi equation with a lipschitz initial condition the hamiltonian is not necessarily convex in the momentum variable and not a priori compactly supported we build and study an operator giving a variational solution of this problem and get local lipschit... | [['we', 'study', 'the', 'cauchy', 'problem', 'for', 'the', 'first', 'order', 'evolutive', 'hamiltonjacobi', 'equation', 'with', 'a', 'lipschitz', 'initial', 'condition', 'the', 'hamiltonian', 'is', 'not', 'necessarily', 'convex', 'in', 'the', 'momentum', 'variable', 'and', 'not', 'a', 'priori', 'compactly', 'supported'... | [-0.10857984873776634, 0.04375975919189538, -0.13460009214516808, 0.09001887552221888, -0.15314570858996981, -0.10214531535651379, 0.021147703228052706, 0.32380833690209937, -0.35081311798421666, -0.19005787485123923, 0.15245457642352753, -0.27416782405149814, -0.11708551778428955, 0.11729310861119302, -0.0975689486076... |
1,801.0989 | Almost cosymplectic statistical manifolds | This paper is a study of almost contact statistical manifolds. Especially
this study is focused on almost cosymplectic statistical manifolds. We obtained
basic properties of such manifolds. It is proved a characterization theorem and
a corollary for the almost cosymplectic statistical manifold with Kaehler
leaves. We... | math.DG | this paper is a study of almost contact statistical manifolds especially this study is focused on almost cosymplectic statistical manifolds we obtained basic properties of such manifolds it is proved a characterization theorem and a corollary for the almost cosymplectic statistical manifold with kaehler leaves we also ... | [['this', 'paper', 'is', 'a', 'study', 'of', 'almost', 'contact', 'statistical', 'manifolds', 'especially', 'this', 'study', 'is', 'focused', 'on', 'almost', 'cosymplectic', 'statistical', 'manifolds', 'we', 'obtained', 'basic', 'properties', 'of', 'such', 'manifolds', 'it', 'is', 'proved', 'a', 'characterization', 'th... | [-0.210644818469882, 0.024928020726899074, -0.10418263968701164, 0.14324785243758623, -0.07467194898442055, -0.1412069695458437, -0.05053943628251242, 0.4317862388988336, -0.23471829208234946, -0.23025738339250287, 0.15333154407174637, -0.29411852384606996, -0.24322367208078505, 0.22067613825201987, -0.1540261087395871... |
1,801.09891 | Some remarks on Bell non-locality and Einstein-Podolsky-Rosen steering
of bipartite states | Bell nonlocality and Einstein-Podolsky-Rosen (EPR) steering are every
important quantum correlations of a composite quantum system. Bell nonlocality
of a bipartite state is a quantum correlation demonstrated by some local
quantum measurements, while EPR steering is another form of quantum
correlations, observed first... | quant-ph | bell nonlocality and einsteinpodolskyrosen epr steering are every important quantum correlations of a composite quantum system bell nonlocality of a bipartite state is a quantum correlation demonstrated by some local quantum measurements while epr steering is another form of quantum correlations observed firstly by sch... | [['bell', 'nonlocality', 'and', 'einsteinpodolskyrosen', 'epr', 'steering', 'are', 'every', 'important', 'quantum', 'correlations', 'of', 'a', 'composite', 'quantum', 'system', 'bell', 'nonlocality', 'of', 'a', 'bipartite', 'state', 'is', 'a', 'quantum', 'correlation', 'demonstrated', 'by', 'some', 'local', 'quantum', ... | [-0.15303309976348076, 0.18605069156158074, -0.10975533523115105, 0.13151677093039074, 0.009179047080045888, -0.2963798772623955, 0.03132308868326022, 0.30198060546937433, -0.20389358483025088, -0.2517227064135709, 0.013731077648618997, -0.3342427831135112, -0.10361338691015182, 0.15323685898228773, -0.0237741855069481... |
1,801.09892 | AC Response of the Edge States in a Two-Dimensional Topological
Insulator Coupled to a Conducting Puddle | We calculate an AC response of the edge states of a two-dimensional
topological insulator, which can exchange electrons with a conducting puddle in
the bulk of the insulator. This exchange leads to finite corrections to the
response of isolated edge states both at low and high frequencies. By comparing
these correcti... | cond-mat.mes-hall | we calculate an ac response of the edge states of a twodimensional topological insulator which can exchange electrons with a conducting puddle in the bulk of the insulator this exchange leads to finite corrections to the response of isolated edge states both at low and high frequencies by comparing these corrections on... | [['we', 'calculate', 'an', 'ac', 'response', 'of', 'the', 'edge', 'states', 'of', 'a', 'twodimensional', 'topological', 'insulator', 'which', 'can', 'exchange', 'electrons', 'with', 'a', 'conducting', 'puddle', 'in', 'the', 'bulk', 'of', 'the', 'insulator', 'this', 'exchange', 'leads', 'to', 'finite', 'corrections', 't... | [-0.19259965868066933, 0.22564411873093576, -0.07467082249379511, 0.03335405411632826, 0.006971783000754856, -0.13662412648988984, 0.09739010874773928, 0.3062513925892822, -0.2574465110014051, -0.30937684655694636, 0.03430303653220693, -0.37266757326611016, -0.07479437299751503, 0.13077921890732597, 0.02627611511497427... |
1,801.09893 | An Attention-Based Word-Level Interaction Model: Relation Detection for
Knowledge Base Question Answering | Relation detection plays a crucial role in Knowledge Base Question Answering
(KBQA) because of the high variance of relation expression in the question.
Traditional deep learning methods follow an encoding-comparing paradigm, where
the question and the candidate relation are represented as vectors to compare
their se... | cs.CL | relation detection plays a crucial role in knowledge base question answering kbqa because of the high variance of relation expression in the question traditional deep learning methods follow an encodingcomparing paradigm where the question and the candidate relation are represented as vectors to compare their semantic ... | [['relation', 'detection', 'plays', 'a', 'crucial', 'role', 'in', 'knowledge', 'base', 'question', 'answering', 'kbqa', 'because', 'of', 'the', 'high', 'variance', 'of', 'relation', 'expression', 'in', 'the', 'question', 'traditional', 'deep', 'learning', 'methods', 'follow', 'an', 'encodingcomparing', 'paradigm', 'whe... | [-0.0748931288000177, 0.04751249034160693, -0.03767049500620393, 0.10657090592678212, -0.10406188095963217, -0.1406753288923975, 0.057025165918978035, 0.43063398465089536, -0.3428045638518437, -0.3380353419771273, 0.04985299944899339, -0.31523850166427037, -0.17988763462602514, 0.15893561446917404, -0.07496863856569048... |
1,801.09894 | Bayesian inverse problems with unknown operators | We consider the Bayesian approach to linear inverse problems when the
underlying operator depends on an unknown parameter. Allowing for finite
dimensional as well as infinite dimensional parameters, the theory covers
several models with different levels of uncertainty in the operator. Using
product priors, we prove c... | math.ST stat.ME stat.TH | we consider the bayesian approach to linear inverse problems when the underlying operator depends on an unknown parameter allowing for finite dimensional as well as infinite dimensional parameters the theory covers several models with different levels of uncertainty in the operator using product priors we prove contrac... | [['we', 'consider', 'the', 'bayesian', 'approach', 'to', 'linear', 'inverse', 'problems', 'when', 'the', 'underlying', 'operator', 'depends', 'on', 'an', 'unknown', 'parameter', 'allowing', 'for', 'finite', 'dimensional', 'as', 'well', 'as', 'infinite', 'dimensional', 'parameters', 'the', 'theory', 'covers', 'several',... | [-0.014616906044962392, 0.05901607835370338, -0.06039425314785066, 0.10570187399703586, -0.08628639769317074, -0.10987573906525293, 0.06633917267192208, 0.40332676154900005, -0.3040335063441572, -0.272218675500798, 0.14292331608356273, -0.218522574943067, -0.14003217916681684, 0.218393035068981, -0.09383402545724741, 0... |
1,801.09895 | One of the Odd Zeta Values from $\zeta(5)$ to $\zeta(25)$ Is Irrational.
By Elementary Means | Available proofs of result of the type 'at least one of the odd zeta values
$\zeta(5),\zeta(7),\dots,\zeta(s)$ is irrational' make use of the saddle-point
method or of linear independence criteria, or both. These two remarkable
techniques are however counted as highly non-elementary, therefore leaving the
partial irr... | math.NT math.CA | available proofs of result of the type at least one of the odd zeta values zeta5zeta7dotszetas is irrational make use of the saddlepoint method or of linear independence criteria or both these two remarkable techniques are however counted as highly nonelementary therefore leaving the partial irrationality result inacce... | [['available', 'proofs', 'of', 'result', 'of', 'the', 'type', 'at', 'least', 'one', 'of', 'the', 'odd', 'zeta', 'values', 'zeta5zeta7dotszetas', 'is', 'irrational', 'make', 'use', 'of', 'the', 'saddlepoint', 'method', 'or', 'of', 'linear', 'independence', 'criteria', 'or', 'both', 'these', 'two', 'remarkable', 'techniq... | [-0.13741688736423385, 0.08697484197691666, -0.12361900599207729, 0.12645867379033007, -0.12369756463449448, -0.17835398142808118, 0.05217498861195054, 0.28173845244571566, -0.2679226356744766, -0.3014148634462617, 0.10377513692947105, -0.24568779438734054, -0.13524879647942725, 0.2493476388650015, -0.05947823240421712... |
1,801.09896 | Pilot study for the COST Action "Reassembling the Republic of Letters":
language-driven network analysis of letters from the Hartlib's Papers | The present report summarizes an exploratory study which we carried out in
the context of the COST Action IS1310 "Reassembling the Republic of Letters,
1500-1800", and which is relevant to the activities of Working Group 3 "Texts
and Topics" and Working Group 2 "People and Networks". In this study we
investigated the... | cs.CL | the present report summarizes an exploratory study which we carried out in the context of the cost action is1310 reassembling the republic of letters 15001800 and which is relevant to the activities of working group 3 texts and topics and working group 2 people and networks in this study we investigated the use of natu... | [['the', 'present', 'report', 'summarizes', 'an', 'exploratory', 'study', 'which', 'we', 'carried', 'out', 'in', 'the', 'context', 'of', 'the', 'cost', 'action', 'is1310', 'reassembling', 'the', 'republic', 'of', 'letters', '15001800', 'and', 'which', 'is', 'relevant', 'to', 'the', 'activities', 'of', 'working', 'group... | [-0.07717469756756604, 0.05039140678371599, -0.08118801384681605, 0.057147424327816415, -0.11905884051382759, -0.058881990999037764, 0.06922005613871517, 0.3722941347798944, -0.24453118771576343, -0.3463373251232135, 0.10602827548868546, -0.3562752012346946, -0.1370885875755853, 0.17343401653270651, -0.0727795187042291... |
1,801.09897 | Open Material Property Library With Native Simulation Tool Integrations
-- MASTO | Reliable material property data is crucial for trustworthy simulations
throughout different areas of engineering. Special care must be taken when
materials at extreme conditions are under study. Superconductors and devices
assembled from superconductors and other materials, like superconducting
magnets, are often ope... | cond-mat.mtrl-sci | reliable material property data is crucial for trustworthy simulations throughout different areas of engineering special care must be taken when materials at extreme conditions are under study superconductors and devices assembled from superconductors and other materials like superconducting magnets are often operated ... | [['reliable', 'material', 'property', 'data', 'is', 'crucial', 'for', 'trustworthy', 'simulations', 'throughout', 'different', 'areas', 'of', 'engineering', 'special', 'care', 'must', 'be', 'taken', 'when', 'materials', 'at', 'extreme', 'conditions', 'are', 'under', 'study', 'superconductors', 'and', 'devices', 'assemb... | [-0.09578785895663643, 0.08843773104350906, -0.06915422248812508, 0.06787506125662553, -0.12320977128767775, -0.17403064924002434, 0.026867934668347766, 0.4181404577923699, -0.2516366594270088, -0.336053560317892, 0.14384097741391216, -0.29107828262934454, -0.09334709220256703, 0.2575648700387538, -0.057422702538846564... |
1,801.09898 | Optical Network Models and their Application to Software-Defined Network
Management | Software-defined networking is finding its way into optical networks. Here,
it promises a simplification and unification of network management for optical
networks allowing automation of operational tasks despite the highly diverse
and vendor-specific commercial systems and the complexity and analog nature of
optical... | cs.NI | softwaredefined networking is finding its way into optical networks here it promises a simplification and unification of network management for optical networks allowing automation of operational tasks despite the highly diverse and vendorspecific commercial systems and the complexity and analog nature of optical trans... | [['softwaredefined', 'networking', 'is', 'finding', 'its', 'way', 'into', 'optical', 'networks', 'here', 'it', 'promises', 'a', 'simplification', 'and', 'unification', 'of', 'network', 'management', 'for', 'optical', 'networks', 'allowing', 'automation', 'of', 'operational', 'tasks', 'despite', 'the', 'highly', 'divers... | [-0.17695916694736927, 0.010128202242259954, -0.025551671780228057, 0.029340512551167094, -0.0959374244655613, -0.20659618970293936, 0.050057730889905276, 0.47643404356291014, -0.25945316231700755, -0.31257859521728254, 0.12523893245809198, -0.2416093757149772, -0.19089089291144126, 0.2534456763473104, -0.0710470636558... |
1,801.09899 | Time-Irreversibility is Hidden Within Newtonian Mechanics | We develop a bit-reversible implementation of Milne's Fourth-order Predictor
algorithm so as to generate precisely time-reversible simulations of
irreversible processes. We apply our algorithm to the collision of two
zero-temperature Morse-potential balls, which collide to form a warm liquid
oscillating drop. The osc... | cond-mat.stat-mech nlin.CD physics.class-ph physics.comp-ph | we develop a bitreversible implementation of milnes fourthorder predictor algorithm so as to generate precisely timereversible simulations of irreversible processes we apply our algorithm to the collision of two zerotemperature morsepotential balls which collide to form a warm liquid oscillating drop the oscillations a... | [['we', 'develop', 'a', 'bitreversible', 'implementation', 'of', 'milnes', 'fourthorder', 'predictor', 'algorithm', 'so', 'as', 'to', 'generate', 'precisely', 'timereversible', 'simulations', 'of', 'irreversible', 'processes', 'we', 'apply', 'our', 'algorithm', 'to', 'the', 'collision', 'of', 'two', 'zerotemperature', ... | [-0.1315011881539433, 0.18153137436631736, -0.1399635867122395, 0.04668767479118667, -0.015683868192607843, -0.13218618102984714, 0.01746903573268954, 0.3649743149054083, -0.271817225220177, -0.28403031976327675, 0.08033778900103762, -0.2643004334826447, -0.11855598404720614, 0.13690603804506385, -0.009664384082336969,... |
1,801.099 | Human Echolocation in Static Situations: Auditory Models of Detection
Thresholds for Distance, Pitch, Loudness and Timbre | We investigated, by using auditory models, how three perceptual parameters,
loudness, pitch and sharpness, determine human echolocation. We used acoustic
recordings from two previous studies, both from stationary situations, and
their resulting perceptual data as input to our analysis. An initial analysis
was on the ... | q-bio.NC | we investigated by using auditory models how three perceptual parameters loudness pitch and sharpness determine human echolocation we used acoustic recordings from two previous studies both from stationary situations and their resulting perceptual data as input to our analysis an initial analysis was on the room acoust... | [['we', 'investigated', 'by', 'using', 'auditory', 'models', 'how', 'three', 'perceptual', 'parameters', 'loudness', 'pitch', 'and', 'sharpness', 'determine', 'human', 'echolocation', 'we', 'used', 'acoustic', 'recordings', 'from', 'two', 'previous', 'studies', 'both', 'from', 'stationary', 'situations', 'and', 'their'... | [-0.03595488622613286, 0.1070521077286685, -0.090231366091812, 0.11584535129500097, -0.10266579233883125, -0.16544149738718877, 0.012496896877111691, 0.46405322584060005, -0.20813095535696396, -0.3529286124409651, 0.09334107651946329, -0.27500248745716405, -0.16487868637426423, 0.23005586454539367, -0.08905737873579744... |
1,801.09901 | Systematic few-body analysis of eta-d, eta-3He and eta-4He interaction
at low energies | The Alt-Grassberger-Sandhas N-body theory is used to study interaction of
eta-mesons with d, 3He, and 4He. Separable expansion of the subamplitudes is
adopted to convert the integral equations into the quasi-two-body form. The
resulting formalism is applied to fit the existing data for low-energy eta
production on fe... | nucl-th | the altgrassbergersandhas nbody theory is used to study interaction of etamesons with d 3he and 4he separable expansion of the subamplitudes is adopted to convert the integral equations into the quasitwobody form the resulting formalism is applied to fit the existing data for lowenergy eta production on fewnucleon targ... | [['the', 'altgrassbergersandhas', 'nbody', 'theory', 'is', 'used', 'to', 'study', 'interaction', 'of', 'etamesons', 'with', 'd', '3he', 'and', '4he', 'separable', 'expansion', 'of', 'the', 'subamplitudes', 'is', 'adopted', 'to', 'convert', 'the', 'integral', 'equations', 'into', 'the', 'quasitwobody', 'form', 'the', 'r... | [-0.07546185588912119, 0.172497921800123, -0.13446793805430585, 0.1140680996895638, -0.003404341921021667, -0.10437101764675183, 0.010209772197965863, 0.29114643169590565, -0.24284843129659944, -0.24734567704645893, -0.030237975288654052, -0.35428614860188357, -0.02863208455095492, 0.16504579619799234, 0.12105626561030... |
1,801.09902 | Kinetics of (2x4) -> (3x1(6)) structural changes on GaAs(001) surfaces
during the UHV annealing | The peculiarities of superstructural transition (2x4) -> (3x1(6)) on the
GaAs(001) surface were studied by the RHEED method in the conditions initiated
by a sharp change of the arsenic flux. The specular beam intensities RHEED
picture dependences on time were obtained during the transition. The
measurement results we... | cond-mat.mtrl-sci | the peculiarities of superstructural transition 2x4 3x16 on the gaas001 surface were studied by the rheed method in the conditions initiated by a sharp change of the arsenic flux the specular beam intensities rheed picture dependences on time were obtained during the transition the measurement results were analyzed wit... | [['the', 'peculiarities', 'of', 'superstructural', 'transition', '2x4', '3x16', 'on', 'the', 'gaas001', 'surface', 'were', 'studied', 'by', 'the', 'rheed', 'method', 'in', 'the', 'conditions', 'initiated', 'by', 'a', 'sharp', 'change', 'of', 'the', 'arsenic', 'flux', 'the', 'specular', 'beam', 'intensities', 'rheed', '... | [-0.0823303081254157, 0.1652523038635577, -0.09235731917182485, 0.017218429701299786, -0.006295445672108117, -0.08844048063644393, 0.05854815330417704, 0.38744430499106736, -0.2488866697322064, -0.330764552399873, 0.07724348970962142, -0.2525228999170313, -0.11545275241655191, 0.17914655004575022, 0.015806729595098802,... |
1,801.09903 | X-Ray and Optical Properties of Black Widows and Redbacks | Black widows and redbacks are binary systems consisting of a millisecond
pulsar in a close binary with a companion having matter driven off of its
surface by the pulsar wind. X-rays due to an intra-binary shock have been
observed from many of these systems, as well as orbital variations in the
optical emission from t... | astro-ph.HE | black widows and redbacks are binary systems consisting of a millisecond pulsar in a close binary with a companion having matter driven off of its surface by the pulsar wind xrays due to an intrabinary shock have been observed from many of these systems as well as orbital variations in the optical emission from the com... | [['black', 'widows', 'and', 'redbacks', 'are', 'binary', 'systems', 'consisting', 'of', 'a', 'millisecond', 'pulsar', 'in', 'a', 'close', 'binary', 'with', 'a', 'companion', 'having', 'matter', 'driven', 'off', 'of', 'its', 'surface', 'by', 'the', 'pulsar', 'wind', 'xrays', 'due', 'to', 'an', 'intrabinary', 'shock', 'h... | [-0.10749573070699206, 0.10929625458335906, -0.06689879695813243, 0.07156122954060826, -0.11105262943042013, -0.08119119848841085, 0.038415607689575366, 0.4551119386540869, -0.244217947537366, -0.34171282867184627, 0.1341183562819004, -0.3355095845539696, -0.09300040885304603, 0.3078461518475356, -0.054072417305388414,... |
1,801.09904 | Taylor series for generalized Lambert W functions | The Lambert W function gives the solutions of a simple exponential
polynomial. The generalized Lambert W function was defined by Mez\"{o} and
Baricz, and has found applications in delay differential equations and physics.
In this article we describe an even more general function, the inverse of a
product of powers of... | math.CA | the lambert w function gives the solutions of a simple exponential polynomial the generalized lambert w function was defined by mezo and baricz and has found applications in delay differential equations and physics in this article we describe an even more general function the inverse of a product of powers of linear fu... | [['the', 'lambert', 'w', 'function', 'gives', 'the', 'solutions', 'of', 'a', 'simple', 'exponential', 'polynomial', 'the', 'generalized', 'lambert', 'w', 'function', 'was', 'defined', 'by', 'mezo', 'and', 'baricz', 'and', 'has', 'found', 'applications', 'in', 'delay', 'differential', 'equations', 'and', 'physics', 'in'... | [-0.132758180832975, 0.05097394866755408, -0.13619381935592284, 0.07517890537476014, -0.06740650181107376, -0.09103105527025704, 0.00435049225319633, 0.2849943906981118, -0.31762680973933666, -0.2331594015823259, 0.08204670012833512, -0.23475489321364357, -0.20354333183519085, 0.2318809035291173, -0.049869591246682166,... |
1,801.09905 | Tuning Rashba spin-orbit coupling in homogeneous semiconductor nanowires | We use $\vec{k}\cdot\vec{p}$ theory to estimate the Rashba spin-orbit
coupling (SOC) in large semiconductor nanowires. We specifically investigate
GaAs- and InSb-based devices with different gate configurations to control
symmetry and localization of the electron charge density. We explore
gate-controlled SOC for wir... | cond-mat.mes-hall | we use veckcdotvecp theory to estimate the rashba spinorbit coupling soc in large semiconductor nanowires we specifically investigate gaas and insbbased devices with different gate configurations to control symmetry and localization of the electron charge density we explore gatecontrolled soc for wires of different siz... | [['we', 'use', 'veckcdotvecp', 'theory', 'to', 'estimate', 'the', 'rashba', 'spinorbit', 'coupling', 'soc', 'in', 'large', 'semiconductor', 'nanowires', 'we', 'specifically', 'investigate', 'gaas', 'and', 'insbbased', 'devices', 'with', 'different', 'gate', 'configurations', 'to', 'control', 'symmetry', 'and', 'localiz... | [-0.1791714091869553, 0.14715608497599847, 0.02753260566507755, -0.0156971619701302, 0.01115396361123642, -0.16984374458692839, 0.07047656484466078, 0.4131840382028243, -0.16067194378260394, -0.3821692016489547, -0.04423217121451483, -0.2932002909666184, -0.161195152941469, 0.1894764490766804, -0.04781431661003494, 0.0... |
1,801.09906 | Ito's Formula for Gaussian Processes with Stochastic Discontinuities | We introduce a Skorokhod type integral and prove an Ito formula for a wide
class of Gaussian processes which may exhibit stochastic discontinuities. Our
Ito formula unifies and extends the classical one for general (i.e., possibly
discontinuous) Gaussian martingales in the sense of Ito integration and the one
for sto... | math.PR | we introduce a skorokhod type integral and prove an ito formula for a wide class of gaussian processes which may exhibit stochastic discontinuities our ito formula unifies and extends the classical one for general ie possibly discontinuous gaussian martingales in the sense of ito integration and the one for stochastica... | [['we', 'introduce', 'a', 'skorokhod', 'type', 'integral', 'and', 'prove', 'an', 'ito', 'formula', 'for', 'a', 'wide', 'class', 'of', 'gaussian', 'processes', 'which', 'may', 'exhibit', 'stochastic', 'discontinuities', 'our', 'ito', 'formula', 'unifies', 'and', 'extends', 'the', 'classical', 'one', 'for', 'general', 'i... | [-0.01801084233995746, 0.03895855887287111, -0.0723812392406056, 0.056160973111057985, -0.09092314986457281, -0.11343701153750504, 0.024483234448673424, 0.3326629365739577, -0.3048572999438928, -0.2369235462974757, 0.06433670289869256, -0.19757799444007962, -0.23046275041997433, 0.23305138904491768, -0.2080910459472387... |
1,801.09907 | Approximate ground states of the random-field Potts model from graph
cuts | While the ground-state problem for the random-field Ising model is
polynomial, and can be solved using a number of well-known algorithms for
maximum flow or graph cut, the analogue random-field Potts model corresponds to
a multi-terminal flow problem that is known to be NP hard. Hence an efficient
exact algorithm is ... | cond-mat.dis-nn cond-mat.stat-mech physics.comp-ph | while the groundstate problem for the randomfield ising model is polynomial and can be solved using a number of wellknown algorithms for maximum flow or graph cut the analogue randomfield potts model corresponds to a multiterminal flow problem that is known to be np hard hence an efficient exact algorithm is very unlik... | [['while', 'the', 'groundstate', 'problem', 'for', 'the', 'randomfield', 'ising', 'model', 'is', 'polynomial', 'and', 'can', 'be', 'solved', 'using', 'a', 'number', 'of', 'wellknown', 'algorithms', 'for', 'maximum', 'flow', 'or', 'graph', 'cut', 'the', 'analogue', 'randomfield', 'potts', 'model', 'corresponds', 'to', '... | [-0.11071585477705324, 0.08403927057534606, -0.06793302957178844, 0.08828823638764481, -0.06450741361646402, -0.17692856727949074, 0.04230886036980777, 0.37442297003562414, -0.2823519919488219, -0.3247310942729875, 0.08072368453647341, -0.24325596178551354, -0.11679311219993378, 0.1765565814480426, 0.007480625054168124... |
1,801.09908 | Topological classification of Chern-type insulators with the photonic
Green function | The Chern topological numbers of a material system are traditionally written
in terms of the Berry curvature which depends explicitly on the material band
structure and on the Bloch eigenwaves. Here, we demonstrate that it is possible
to calculate the gap Chern numbers of a photonic platform without having any
detail... | physics.optics | the chern topological numbers of a material system are traditionally written in terms of the berry curvature which depends explicitly on the material band structure and on the bloch eigenwaves here we demonstrate that it is possible to calculate the gap chern numbers of a photonic platform without having any detailed k... | [['the', 'chern', 'topological', 'numbers', 'of', 'a', 'material', 'system', 'are', 'traditionally', 'written', 'in', 'terms', 'of', 'the', 'berry', 'curvature', 'which', 'depends', 'explicitly', 'on', 'the', 'material', 'band', 'structure', 'and', 'on', 'the', 'bloch', 'eigenwaves', 'here', 'we', 'demonstrate', 'that'... | [-0.22769638622754856, 0.11483033924833617, -0.05177875458724609, 0.013682143245197582, -0.13258467972701213, -0.09230105450744701, 0.049919784439829404, 0.4246342045513271, -0.25605278318168734, -0.29036149988342236, 0.06299156628200832, -0.24309784066745965, -0.1980193261988461, 0.2194358445860508, 0.0208323949188807... |
1,801.09909 | Properties of additive functionals of Brownian motion with resetting | We study the distribution of additive functionals of reset Brownian motion, a
variation of normal Brownian motion in which the path is interrupted at a given
rate and placed back to a given reset position. Our goal is two-fold: (1) For
general functionals, we derive a large deviation principle in the presence of
rese... | math.PR cond-mat.stat-mech | we study the distribution of additive functionals of reset brownian motion a variation of normal brownian motion in which the path is interrupted at a given rate and placed back to a given reset position our goal is twofold 1 for general functionals we derive a large deviation principle in the presence of resetting and... | [['we', 'study', 'the', 'distribution', 'of', 'additive', 'functionals', 'of', 'reset', 'brownian', 'motion', 'a', 'variation', 'of', 'normal', 'brownian', 'motion', 'in', 'which', 'the', 'path', 'is', 'interrupted', 'at', 'a', 'given', 'rate', 'and', 'placed', 'back', 'to', 'a', 'given', 'reset', 'position', 'our', 'g... | [-0.14840560448110887, 0.11623306463782986, -0.0703556895166178, 0.07843781428681196, -0.014668829436822418, -0.10264655545746025, 0.12395094432296198, 0.32326568321635324, -0.2941106114712168, -0.3092267247439738, 0.061551876542803814, -0.2843031592732459, -0.10846447879285143, 0.20631383581029808, -0.0951527587317845... |
1,801.0991 | Edge State Quantization: Vector Fields in Rindler | We present a detailed discussion of the entanglement structure of vector
fields through canonical quantization. We quantize Maxwell theory in Rindler
space in Lorenz gauge, discuss the Hilbert space structure and analyze the
Unruh effect. As a warm-up, in 1+1 dimensions, we compute the spectrum and
prove that the the... | hep-th | we present a detailed discussion of the entanglement structure of vector fields through canonical quantization we quantize maxwell theory in rindler space in lorenz gauge discuss the hilbert space structure and analyze the unruh effect as a warmup in 11 dimensions we compute the spectrum and prove that the theory is th... | [['we', 'present', 'a', 'detailed', 'discussion', 'of', 'the', 'entanglement', 'structure', 'of', 'vector', 'fields', 'through', 'canonical', 'quantization', 'we', 'quantize', 'maxwell', 'theory', 'in', 'rindler', 'space', 'in', 'lorenz', 'gauge', 'discuss', 'the', 'hilbert', 'space', 'structure', 'and', 'analyze', 'th... | [-0.19002556105260737, 0.21412232965230943, -0.05796882937877224, 0.0892691626947803, -0.06380746979982807, -0.13919531795052956, -0.007444288489372971, 0.31803839747579055, -0.19748763684899762, -0.25189645314732423, 0.09547124113081597, -0.2720238013407932, -0.16476155885745986, 0.07753348582818244, -0.04888260808701... |
1,801.09911 | A Dynamic Process Interpretation of the Sparse ERGM Reference Model | Exponential family random graph models (ERGMs) can be understood in terms of
a set of structural biases that act on an underlying reference distribution.
This distribution determines many aspects of the behavior and interpretation of
the ERGM families incorporating it. One important innovation in this area has
been t... | math.ST stat.ME stat.TH | exponential family random graph models ergms can be understood in terms of a set of structural biases that act on an underlying reference distribution this distribution determines many aspects of the behavior and interpretation of the ergm families incorporating it one important innovation in this area has been the dev... | [['exponential', 'family', 'random', 'graph', 'models', 'ergms', 'can', 'be', 'understood', 'in', 'terms', 'of', 'a', 'set', 'of', 'structural', 'biases', 'that', 'act', 'on', 'an', 'underlying', 'reference', 'distribution', 'this', 'distribution', 'determines', 'many', 'aspects', 'of', 'the', 'behavior', 'and', 'inter... | [-0.09289652393504855, 0.1021710522036301, -0.13522352840079635, 0.06752338015995206, -0.09381392655978132, -0.13584666999179076, 0.03633941437373488, 0.37880210231867484, -0.3089516153482751, -0.3119381922526193, 0.04958321797550793, -0.20797166542043208, -0.20090415736385545, 0.1613986395527494, -0.09208644220994816,... |
1,801.09912 | Infinite Lattices of Vortex Molecules in Rabi-Coupled Condensates | Vortex molecules can form in a two component superfluid when a Rabi field
drives transitions between the two components. We study the ground state of an
infinite system of vortex molecules in 2D, using a numerical scheme which makes
no use of the lowest Landau level approximation. We find the ground state
lattice geo... | cond-mat.quant-gas | vortex molecules can form in a two component superfluid when a rabi field drives transitions between the two components we study the ground state of an infinite system of vortex molecules in 2d using a numerical scheme which makes no use of the lowest landau level approximation we find the ground state lattice geometry... | [['vortex', 'molecules', 'can', 'form', 'in', 'a', 'two', 'component', 'superfluid', 'when', 'a', 'rabi', 'field', 'drives', 'transitions', 'between', 'the', 'two', 'components', 'we', 'study', 'the', 'ground', 'state', 'of', 'an', 'infinite', 'system', 'of', 'vortex', 'molecules', 'in', '2d', 'using', 'a', 'numerical'... | [-0.20104411630991767, 0.1594855788965976, -0.06471872490725192, 0.03442832044989085, -0.02192556175986211, -0.08409136914306407, 0.04166425953002767, 0.3422553057266439, -0.2236716480416467, -0.27707941871699243, 0.0302598268436871, -0.24043001151292354, -0.09522594104809083, 0.17436804616381582, 0.05598151168229876, ... |
1,801.09913 | Dynamical Networks of Influence in Small Group Discussions | In many domains of life, business and management, numerous problems are
addressed by small groups of individuals engaged in face-to-face discussions.
While research in social psychology has a long history of studying the
determinants of small group performances, the internal dynamics that govern a
group discussion is... | physics.soc-ph cs.SI | in many domains of life business and management numerous problems are addressed by small groups of individuals engaged in facetoface discussions while research in social psychology has a long history of studying the determinants of small group performances the internal dynamics that govern a group discussion is not yet... | [['in', 'many', 'domains', 'of', 'life', 'business', 'and', 'management', 'numerous', 'problems', 'are', 'addressed', 'by', 'small', 'groups', 'of', 'individuals', 'engaged', 'in', 'facetoface', 'discussions', 'while', 'research', 'in', 'social', 'psychology', 'has', 'a', 'long', 'history', 'of', 'studying', 'the', 'de... | [-0.11655670734940142, 0.09006383304757176, -0.08989980465972647, 0.08190640177234497, -0.13118135305776757, -0.13641185269817607, 0.08964090900437238, 0.42175452623724, -0.2585952198084197, -0.31155479145609494, 0.09722315504918205, -0.26469010723112246, -0.2066987046768292, 0.16102035918483149, -0.07888419050230602, ... |
1,801.09914 | Stochastic band structure for waves propagating in periodic media or
along waveguides | We introduce the stochastic band structure, a method giving the dispersion
relation for waves propagating in periodic media or along waveguides, and
subject to material loss or radiation damping. Instead of considering an
explicit or implicit functional relation between frequency $\omega$ and
wavenumber $k$, as is us... | physics.comp-ph physics.optics | we introduce the stochastic band structure a method giving the dispersion relation for waves propagating in periodic media or along waveguides and subject to material loss or radiation damping instead of considering an explicit or implicit functional relation between frequency omega and wavenumber k as is usually done ... | [['we', 'introduce', 'the', 'stochastic', 'band', 'structure', 'a', 'method', 'giving', 'the', 'dispersion', 'relation', 'for', 'waves', 'propagating', 'in', 'periodic', 'media', 'or', 'along', 'waveguides', 'and', 'subject', 'to', 'material', 'loss', 'or', 'radiation', 'damping', 'instead', 'of', 'considering', 'an', ... | [-0.1868529293593789, 0.10845916443670357, -0.056804956006240255, 0.044415402197286735, -0.13452007358100973, -0.11155269959602844, 0.043018926929851826, 0.44423826694611673, -0.300281678772847, -0.25696131523144394, 0.07515980105814409, -0.2822161630942863, -0.12815843406133354, 0.20961143432785412, 0.0388935487255577... |
1,801.09915 | Possible relation between pulsar rotation and evolution of magnetic
inclination | The pulsar timing is observed to be different from predicted by a simple
magnetic dipole radiation. We choose eight pulsars whose braking index was
reliably determined. Assuming the smaller values of braking index are dominated
by the secular evolution of the magnetic inclination, we calculate the
increasing rate of ... | astro-ph.HE | the pulsar timing is observed to be different from predicted by a simple magnetic dipole radiation we choose eight pulsars whose braking index was reliably determined assuming the smaller values of braking index are dominated by the secular evolution of the magnetic inclination we calculate the increasing rate of the m... | [['the', 'pulsar', 'timing', 'is', 'observed', 'to', 'be', 'different', 'from', 'predicted', 'by', 'a', 'simple', 'magnetic', 'dipole', 'radiation', 'we', 'choose', 'eight', 'pulsars', 'whose', 'braking', 'index', 'was', 'reliably', 'determined', 'assuming', 'the', 'smaller', 'values', 'of', 'braking', 'index', 'are', ... | [-0.15186589645578988, 0.21031243391154172, -0.020034886356352748, 0.11633460413782125, -0.1490461441588778, -0.08906966158487264, 0.035291134534647814, 0.3775822401625439, -0.23801140651757857, -0.39935345365439806, 0.04499226786847253, -0.21855794356285946, -0.04869537766190987, 0.24827242902145513, -0.00425358702546... |
1,801.09916 | Input / Output Stability of a Damped String Equation coupled with
Ordinary Differential System | The input/output stability of an interconnected system composed of an
ordinary differential equation and a damped string equation is studied. Issued
from the literature on time-delay systems, an exact stability result is firstly
derived using pole locations. Then, based on the Small-Gain theorem and on the
Quadratic ... | math.OC | the inputoutput stability of an interconnected system composed of an ordinary differential equation and a damped string equation is studied issued from the literature on timedelay systems an exact stability result is firstly derived using pole locations then based on the smallgain theorem and on the quadratic separatio... | [['the', 'inputoutput', 'stability', 'of', 'an', 'interconnected', 'system', 'composed', 'of', 'an', 'ordinary', 'differential', 'equation', 'and', 'a', 'damped', 'string', 'equation', 'is', 'studied', 'issued', 'from', 'the', 'literature', 'on', 'timedelay', 'systems', 'an', 'exact', 'stability', 'result', 'is', 'firs... | [-0.1604472225868797, 0.0025153169414632894, -0.10228046982430239, 0.039748279995810085, -0.05421164564471295, -0.10881744868102226, 0.00860809539494283, 0.30394952033864375, -0.2613527559021369, -0.23135458076362836, 0.16101125776247577, -0.2950551650150025, -0.15791411834590613, 0.25738384295254946, -0.04906389504631... |
1,801.09917 | Calculated effects of disorder on the Mo core levels in purple bronze
Li$_2$Mo$_{12}$O$_{34}$ | The band structures of ordered and thermally disordered
Li$_2$Mo$_{12}$O$_{34}$ are calculated by use of ab-initio DFT-LMTO method with
focus on the behavior of the Mo 3d-core levels. It is shown that thermal
disorder and zero-point motion lead to substantial core level broadening, and
the broadening at room temperat... | cond-mat.mtrl-sci | the band structures of ordered and thermally disordered li_2mo_12o_34 are calculated by use of abinitio dftlmto method with focus on the behavior of the mo 3dcore levels it is shown that thermal disorder and zeropoint motion lead to substantial core level broadening and the broadening at room temperature is predicted t... | [['the', 'band', 'structures', 'of', 'ordered', 'and', 'thermally', 'disordered', 'li_2mo_12o_34', 'are', 'calculated', 'by', 'use', 'of', 'abinitio', 'dftlmto', 'method', 'with', 'focus', 'on', 'the', 'behavior', 'of', 'the', 'mo', '3dcore', 'levels', 'it', 'is', 'shown', 'that', 'thermal', 'disorder', 'and', 'zeropoi... | [-0.08490929197003023, 0.2377946752933171, -0.05241310614799186, 0.05852827773975781, -0.021282058885673017, -0.14159770524789264, 0.05087911228715317, 0.41423213235505923, -0.21770317430468641, -0.3163145468391544, 0.043295441805861715, -0.3301808898755181, -0.09949880209934758, 0.19342470552596286, 0.0124289105154984... |
1,801.09918 | Microresonator Isolators and Circulators Based on the Intrinsic
Nonreciprocity of the Kerr Effect | Nonreciprocal light propagation is important in many applications, ranging
from optical telecommunications to integrated photonics. A simple way to
achieve optical nonreciprocity is to use the nonlinear interaction between
counterpropagating light in a Kerr medium. Within a ring resonator, this leads
to spontaneous s... | physics.optics physics.app-ph | nonreciprocal light propagation is important in many applications ranging from optical telecommunications to integrated photonics a simple way to achieve optical nonreciprocity is to use the nonlinear interaction between counterpropagating light in a kerr medium within a ring resonator this leads to spontaneous symmetr... | [['nonreciprocal', 'light', 'propagation', 'is', 'important', 'in', 'many', 'applications', 'ranging', 'from', 'optical', 'telecommunications', 'to', 'integrated', 'photonics', 'a', 'simple', 'way', 'to', 'achieve', 'optical', 'nonreciprocity', 'is', 'to', 'use', 'the', 'nonlinear', 'interaction', 'between', 'counterpr... | [-0.1477256989413449, 0.14396636782383376, -0.07751817345957865, -0.04398405622500418, -0.11627514949915084, -0.17748353663323954, 0.034823635420550336, 0.47949831855314023, -0.2600267748560079, -0.27776813629845326, 0.05818113500400531, -0.24420657173137772, -0.15856701903553172, 0.27498301283498716, -0.04981796609460... |
1,801.09919 | E2E-MLT - an Unconstrained End-to-End Method for Multi-Language Scene
Text | An end-to-end trainable (fully differentiable) method for multi-language
scene text localization and recognition is proposed. The approach is based on a
single fully convolutional network (FCN) with shared layers for both tasks.
E2E-MLT is the first published multi-language OCR for scene text. While
trained in mult... | cs.CV | an endtoend trainable fully differentiable method for multilanguage scene text localization and recognition is proposed the approach is based on a single fully convolutional network fcn with shared layers for both tasks e2emlt is the first published multilanguage ocr for scene text while trained in multilanguage setup ... | [['an', 'endtoend', 'trainable', 'fully', 'differentiable', 'method', 'for', 'multilanguage', 'scene', 'text', 'localization', 'and', 'recognition', 'is', 'proposed', 'the', 'approach', 'is', 'based', 'on', 'a', 'single', 'fully', 'convolutional', 'network', 'fcn', 'with', 'shared', 'layers', 'for', 'both', 'tasks', 'e... | [-0.018413681268998203, -0.07711646213233694, -0.02396214261733965, 0.04952319532836953, -0.1230491448882712, -0.2506136921145124, -0.023929547386129117, 0.507140529482332, -0.2511754782538708, -0.3032442074881433, 0.02519538761786351, -0.286007683700244, -0.16198575318063776, 0.23889068383978654, -0.1784122796244409, ... |
1,801.0992 | The black hole at the Galactic Center: observations and models | One of the most interesting astronomical objects is the Galactic Center. We
concentrate our discussion on a theoretical analysis of observational data of
bright stars in the IR-band obtained with large telescopes. We also discuss the
importance of VLBI observations of bright structures which could characterize
the sh... | gr-qc astro-ph.CO astro-ph.GA | one of the most interesting astronomical objects is the galactic center we concentrate our discussion on a theoretical analysis of observational data of bright stars in the irband obtained with large telescopes we also discuss the importance of vlbi observations of bright structures which could characterize the shadow ... | [['one', 'of', 'the', 'most', 'interesting', 'astronomical', 'objects', 'is', 'the', 'galactic', 'center', 'we', 'concentrate', 'our', 'discussion', 'on', 'a', 'theoretical', 'analysis', 'of', 'observational', 'data', 'of', 'bright', 'stars', 'in', 'the', 'irband', 'obtained', 'with', 'large', 'telescopes', 'we', 'also... | [-0.11035334504174314, 0.12131241220554759, -0.06542789185033092, 0.12356128244274207, -0.10801148973581082, -0.1033002709517396, 0.012328207410239387, 0.32974529545402753, -0.1340512291866548, -0.3571409794027513, 0.13109504229933866, -0.3029537639721244, -0.07779149807866592, 0.2186635676437532, -0.028339138171934293... |
1,801.09921 | On the properties of the $(p,\nu)$-extension of the Whittaker function
$M_{\kappa,\mu}(z)$ | In this paper, we obtain a $(p,\nu)$-extension of the Whittaker function
$M_{\kappa,\mu}(z)$ by using the extended confluent hypergeometric function of
the first kind $\Phi_{p,\nu}(b;c;z)$ introduced in Parmar et al. [J. Classical
Anal. 11 (2017) 81--106]. Also, we derive some of the main properties of this
function,... | math.CA | in this paper we obtain a pnuextension of the whittaker function m_kappamuz by using the extended confluent hypergeometric function of the first kind phi_pnubcz introduced in parmar et al j classical anal 11 2017 81106 also we derive some of the main properties of this function namely several integral representations a... | [['in', 'this', 'paper', 'we', 'obtain', 'a', 'pnuextension', 'of', 'the', 'whittaker', 'function', 'm_kappamuz', 'by', 'using', 'the', 'extended', 'confluent', 'hypergeometric', 'function', 'of', 'the', 'first', 'kind', 'phi_pnubcz', 'introduced', 'in', 'parmar', 'et', 'al', 'j', 'classical', 'anal', '11', '2017', '81... | [-0.0955337753208975, -0.03198795294839797, -0.1719357747951466, 0.08327034685520851, -0.11693137150370714, -0.037312855259656455, 0.0350754802471563, 0.249570112506097, -0.2828768946505575, -0.28067271442463, 0.08490609740803132, -0.2392606587628975, -0.2919314688805378, 0.2187260755401274, -0.09040767390450294, 0.069... |
1,801.09922 | Modern Regularization Methods for Inverse Problems | Regularization methods are a key tool in the solution of inverse problems.
They are used to introduce prior knowledge and make the approximation of
ill-posed (pseudo-)inverses feasible. In the last two decades interest has
shifted from linear towards nonlinear regularization methods even for linear
inverse problems. ... | math.NA | regularization methods are a key tool in the solution of inverse problems they are used to introduce prior knowledge and make the approximation of illposed pseudoinverses feasible in the last two decades interest has shifted from linear towards nonlinear regularization methods even for linear inverse problems the aim o... | [['regularization', 'methods', 'are', 'a', 'key', 'tool', 'in', 'the', 'solution', 'of', 'inverse', 'problems', 'they', 'are', 'used', 'to', 'introduce', 'prior', 'knowledge', 'and', 'make', 'the', 'approximation', 'of', 'illposed', 'pseudoinverses', 'feasible', 'in', 'the', 'last', 'two', 'decades', 'interest', 'has',... | [-0.019803304690867662, 0.006354567645935387, -0.08872345594946689, 0.07939474608624218, -0.12356861966200233, -0.14024992602900033, -0.02180663501177498, 0.43263539104018267, -0.3381689236522084, -0.27921458599876947, 0.20868078925139535, -0.261891116308639, -0.1998085077034264, 0.24613725577624954, -0.109902181638868... |
1,801.09923 | Analytical modeling and analysis of interleaving on correlated wireless
channels | Interleaving is a mechanism universally used in wireless access technologies
to alleviate the effect of channel correlation. In spite of its wide adoption,
to the best of our knowledge, there are no analytical models proposed so far.
In this paper we fill this void proposing three different models of
interleaving. Tw... | cs.IT cs.NI eess.SP math.IT | interleaving is a mechanism universally used in wireless access technologies to alleviate the effect of channel correlation in spite of its wide adoption to the best of our knowledge there are no analytical models proposed so far in this paper we fill this void proposing three different models of interleaving two of th... | [['interleaving', 'is', 'a', 'mechanism', 'universally', 'used', 'in', 'wireless', 'access', 'technologies', 'to', 'alleviate', 'the', 'effect', 'of', 'channel', 'correlation', 'in', 'spite', 'of', 'its', 'wide', 'adoption', 'to', 'the', 'best', 'of', 'our', 'knowledge', 'there', 'are', 'no', 'analytical', 'models', 'p... | [-0.1378858443395253, 0.020477468215212152, -0.04578592980796398, 0.09510605038211033, -0.041716456775069605, -0.1818394956667451, 0.10281933770702202, 0.4196598642989628, -0.2644765096780497, -0.3274969997377518, 0.08746102230061832, -0.2468342807067743, -0.16018469603823535, 0.19834940890124178, -0.09765705695562978,... |
1,801.09924 | Toda hierarchies and their applications | The 2D Toda hierarchy occupies a central position in the family of integrable
hierarchies of the Toda type. The 1D Toda hierarchy and the Ablowitz-Ladik (aka
relativistic Toda) hierarchy can be derived from the 2D Toda hierarchy as
reductions. These integrable hierarchies have been applied to various problems
of math... | math-ph hep-th math.MP nlin.SI | the 2d toda hierarchy occupies a central position in the family of integrable hierarchies of the toda type the 1d toda hierarchy and the ablowitzladik aka relativistic toda hierarchy can be derived from the 2d toda hierarchy as reductions these integrable hierarchies have been applied to various problems of mathematics... | [['the', '2d', 'toda', 'hierarchy', 'occupies', 'a', 'central', 'position', 'in', 'the', 'family', 'of', 'integrable', 'hierarchies', 'of', 'the', 'toda', 'type', 'the', '1d', 'toda', 'hierarchy', 'and', 'the', 'ablowitzladik', 'aka', 'relativistic', 'toda', 'hierarchy', 'can', 'be', 'derived', 'from', 'the', '2d', 'to... | [-0.10295366603356079, 0.10009259108654005, -0.057288702452342785, 0.13266497557192117, -0.08882089331746101, -0.1913476089771912, -0.05207499955943317, 0.28814689526896947, -0.3382789990645927, -0.2629328271086584, 0.1279872810028981, -0.2523409088889149, -0.19138514845563262, 0.15998048920828173, 0.005011590578962092... |
1,801.09925 | Multiplicity results for $(p,\, q)$ fractional elliptic equations
involving critical nonlinearities | In this paper we prove the existence of infinitely many nontrivial solutions
for the class of $(p,\, q)$ fractional elliptic equations involving
concave-critical nonlinearities in bounded domains in $\mathbb{R}^N$. Further,
when the nonlinearity is of convex-critical type, we establish the multiplicity
of nonnegative... | math.AP | in this paper we prove the existence of infinitely many nontrivial solutions for the class of p q fractional elliptic equations involving concavecritical nonlinearities in bounded domains in mathbbrn further when the nonlinearity is of convexcritical type we establish the multiplicity of nonnegative solutions using var... | [['in', 'this', 'paper', 'we', 'prove', 'the', 'existence', 'of', 'infinitely', 'many', 'nontrivial', 'solutions', 'for', 'the', 'class', 'of', 'p', 'q', 'fractional', 'elliptic', 'equations', 'involving', 'concavecritical', 'nonlinearities', 'in', 'bounded', 'domains', 'in', 'mathbbrn', 'further', 'when', 'the', 'nonl... | [-0.19314500830867992, 0.022314862847062095, -0.05306766661981653, 0.0293251966691709, -0.05190832249354571, -0.12811378545926086, -0.06209041881499745, 0.2826027929383729, -0.3181002611360912, -0.2016215628079538, 0.13285889304825105, -0.3283092591778508, -0.1577104837301054, 0.18708525589733785, -0.06672593902788192,... |
1,801.09926 | SY Mus - search for physical parameters | This is a preliminary analysis of the orbital parameters of the well known
eclipsing symbiotic binary, SY Muscae. It is a system composed of a white dwarf
(WD) and a red giant (RG), located in the southern sky. With the use of
photometric data in the infrared (IR) bands and radial velocities (RV) for the
RG, we deter... | astro-ph.SR | this is a preliminary analysis of the orbital parameters of the well known eclipsing symbiotic binary sy muscae it is a system composed of a white dwarf wd and a red giant rg located in the southern sky with the use of photometric data in the infrared ir bands and radial velocities rv for the rg we determine physical p... | [['this', 'is', 'a', 'preliminary', 'analysis', 'of', 'the', 'orbital', 'parameters', 'of', 'the', 'well', 'known', 'eclipsing', 'symbiotic', 'binary', 'sy', 'muscae', 'it', 'is', 'a', 'system', 'composed', 'of', 'a', 'white', 'dwarf', 'wd', 'and', 'a', 'red', 'giant', 'rg', 'located', 'in', 'the', 'southern', 'sky', '... | [-0.10597015215785473, 0.07225692246937762, -0.10217734138396653, 0.05683537751327378, -0.1296635848687744, -0.07489529859226246, 0.09484809477414403, 0.3715075438285803, -0.17664550034353485, -0.3089579799418132, 0.12107625997068917, -0.3314377229854271, -0.10824309580947285, 0.21752978014675053, -0.08827646674781844,... |
1,801.09927 | Diagnose like a Radiologist: Attention Guided Convolutional Neural
Network for Thorax Disease Classification | This paper considers the task of thorax disease classification on chest X-ray
images. Existing methods generally use the global image as input for network
learning. Such a strategy is limited in two aspects. 1) A thorax disease
usually happens in (small) localized areas which are disease specific. Training
CNNs using... | cs.CV | this paper considers the task of thorax disease classification on chest xray images existing methods generally use the global image as input for network learning such a strategy is limited in two aspects 1 a thorax disease usually happens in small localized areas which are disease specific training cnns using global im... | [['this', 'paper', 'considers', 'the', 'task', 'of', 'thorax', 'disease', 'classification', 'on', 'chest', 'xray', 'images', 'existing', 'methods', 'generally', 'use', 'the', 'global', 'image', 'as', 'input', 'for', 'network', 'learning', 'such', 'a', 'strategy', 'is', 'limited', 'in', 'two', 'aspects', '1', 'a', 'thor... | [-0.052766079635252594, -0.010843491356986899, -0.06013566274803294, 0.08449241780471646, -0.09222403194549633, -0.14611643003925623, 0.05698176288679095, 0.4077666740084119, -0.27385557385892223, -0.29794495139388816, 0.10856526548304253, -0.26997698807404213, -0.1897938631828359, 0.14368545694512283, -0.1626392350895... |
1,801.09928 | Invariable generation of permutation and linear groups | A subset $\left\{x_{1},x_{2},\hdots,x_{d}\right\}$ of a group $G$
\emph{invariably generates} $G$ if
$\left\{x_{1}^{g_{1}},x_{2}^{g_{2}},\hdots,x_{d}^{g_{d}}\right\}$ generates $G$
for every $d$-tuple $(g_{1},g_{2}\hdots,g_{d})\in G^{d}$. We prove that a
finite completely reducible linear group of dimension $n$ can b... | math.GR | a subset leftx_1x_2hdotsx_dright of a group g emphinvariably generates g if leftx_1g_1x_2g_2hdotsx_dg_dright generates g for every dtuple g_1g_2hdotsg_din gd we prove that a finite completely reducible linear group of dimension n can be invariably generated by leftlfloor frac3n2rightrfloor elements we also prove tighte... | [['a', 'subset', 'leftx_1x_2hdotsx_dright', 'of', 'a', 'group', 'g', 'emphinvariably', 'generates', 'g', 'if', 'leftx_1g_1x_2g_2hdotsx_dg_dright', 'generates', 'g', 'for', 'every', 'dtuple', 'g_1g_2hdotsg_din', 'gd', 'we', 'prove', 'that', 'a', 'finite', 'completely', 'reducible', 'linear', 'group', 'of', 'dimension', ... | [-0.1944129324377808, 0.240273723582903, -0.037313076909886646, -0.009420333251561204, -0.06357003020581929, -0.17934140764585096, 0.006857882649318812, 0.3796925047629398, -0.32378240169523514, -0.22563672281342417, 0.11223888476155953, -0.3138657475579275, -0.16191100445894957, 0.17871608177825093, -0.090790761886674... |
1,801.09929 | Discovery of three new millisecond pulsars in Terzan 5 | We report on the discovery of three new millisecond pulsars (namely
J1748-2446aj, J1748-2446ak and J1748-2446al) in the inner regions of the dense
stellar system Terzan 5. These pulsars have been discovered thanks to a method,
alternative to the classical search routines, that exploited the large set of
archival obse... | astro-ph.HE | we report on the discovery of three new millisecond pulsars namely j17482446aj j17482446ak and j17482446al in the inner regions of the dense stellar system terzan 5 these pulsars have been discovered thanks to a method alternative to the classical search routines that exploited the large set of archival observations of... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'three', 'new', 'millisecond', 'pulsars', 'namely', 'j17482446aj', 'j17482446ak', 'and', 'j17482446al', 'in', 'the', 'inner', 'regions', 'of', 'the', 'dense', 'stellar', 'system', 'terzan', '5', 'these', 'pulsars', 'have', 'been', 'discovered', 'thanks', 'to', 'a', 'met... | [-0.09921988931882973, 0.1118090793096758, -0.03985560395633058, 0.0742873841819843, -0.08365173498438623, -0.05889669038144123, 0.09461869685862635, 0.3768583335001598, -0.1902271183519672, -0.41536716806711915, 0.11225151573487836, -0.28962075885519695, -0.041910265263928506, 0.29263798527770013, -0.00899259416271269... |
1,801.0993 | Trace class groups: the case of semi-direct products | In this paper we continue the study of groups of trace class and consider in
particular the case of semi-direct products. One of the highlights is the
theorem saying that the semi-direct product of a semisimple Lie group G and its
Lie algebra is a trace class group if and only if G is compact.
| math.RT math.FA | in this paper we continue the study of groups of trace class and consider in particular the case of semidirect products one of the highlights is the theorem saying that the semidirect product of a semisimple lie group g and its lie algebra is a trace class group if and only if g is compact | [['in', 'this', 'paper', 'we', 'continue', 'the', 'study', 'of', 'groups', 'of', 'trace', 'class', 'and', 'consider', 'in', 'particular', 'the', 'case', 'of', 'semidirect', 'products', 'one', 'of', 'the', 'highlights', 'is', 'the', 'theorem', 'saying', 'that', 'the', 'semidirect', 'product', 'of', 'a', 'semisimple', 'l... | [-0.19759030110118064, 0.07658982681618495, -0.07257791124284267, -0.00454662382518026, -0.15560627921738407, -0.04785215593027797, -0.00030177858954464845, 0.3824156506495042, -0.324796215173873, -0.20005818673155523, 0.1738792419052598, -0.22292166955091736, -0.15254850927740335, 0.1901379270479083, -0.12330184506083... |
1,801.09931 | $ \mu-\tau $ Reflection Symmetry Embedded in Minimal Seesaw | We embed $\mu-\tau$ reflection symmetry into the minimal seesaw formalism,
where two right-handed neutrinos are added to the Standard Model of particle
physics. Assuming that both the left- and right-handed neutrino fields
transform under $\mu-\tau$ reflection symmetry, we obtain the required forms of
the neutrino Di... | hep-ph | we embed mutau reflection symmetry into the minimal seesaw formalism where two righthanded neutrinos are added to the standard model of particle physics assuming that both the left and righthanded neutrino fields transform under mutau reflection symmetry we obtain the required forms of the neutrino dirac mass matrix an... | [['we', 'embed', 'mutau', 'reflection', 'symmetry', 'into', 'the', 'minimal', 'seesaw', 'formalism', 'where', 'two', 'righthanded', 'neutrinos', 'are', 'added', 'to', 'the', 'standard', 'model', 'of', 'particle', 'physics', 'assuming', 'that', 'both', 'the', 'left', 'and', 'righthanded', 'neutrino', 'fields', 'transfor... | [-0.12319437563419341, 0.2971159741380497, 0.014205889217555523, 0.19023571907493628, -0.11718863825019644, -0.18532959710022337, 0.02996955086526118, 0.34455512188080895, -0.26353258869953844, -0.3043300620133155, 0.0554441263592851, -0.25716316461269006, -0.03687671363647831, 0.04353555205008505, 0.07193622218542978,... |
1,801.09932 | EUPRAXIA@SPARC_LAB: Beam Dynamics studies for the X-band Linac | In the framework of the Eupraxia Design Study an advanced accelerator
facility EUPRAXIA@SPARC_LAB has been proposed to be realized at Frascati
(Italy) Laboratories of INFN. Two advanced acceleration schemes will be
applied, namely an ultimate high gradient 1 GeV X-band linac together with a
plasma acceleration stage ... | physics.acc-ph | in the framework of the eupraxia design study an advanced accelerator facility eupraxiasparc_lab has been proposed to be realized at frascati italy laboratories of infn two advanced acceleration schemes will be applied namely an ultimate high gradient 1 gev xband linac together with a plasma acceleration stage to provi... | [['in', 'the', 'framework', 'of', 'the', 'eupraxia', 'design', 'study', 'an', 'advanced', 'accelerator', 'facility', 'eupraxiasparc_lab', 'has', 'been', 'proposed', 'to', 'be', 'realized', 'at', 'frascati', 'italy', 'laboratories', 'of', 'infn', 'two', 'advanced', 'acceleration', 'schemes', 'will', 'be', 'applied', 'na... | [-0.06752556002271982, 0.21957981080655978, -0.09845602289230253, 0.04835868267788707, -0.01939899263282617, -0.19108111165308703, -0.062447707888592656, 0.4585441511745254, -0.1990316973727507, -0.30773845113192994, 0.054512890682478124, -0.30094823471736165, 0.08900054191083957, 0.3020138350004951, 0.0306457718776073... |
1,801.09933 | Nonlinear stability of 2-solitons of the Sine-Gordon equation in the
energy space | In this article we prove that 2-soliton solutions of the sine-Gordon equation
(SG) are orbitally stable in the natural energy space of the problem. The
solutions that we study are the {\it 2-kink, kink-antikink and breather} of SG.
In order to prove this result, we will use B\"acklund transformations
implemented by t... | math.AP math-ph math.MP nlin.SI | in this article we prove that 2soliton solutions of the sinegordon equation sg are orbitally stable in the natural energy space of the problem the solutions that we study are the it 2kink kinkantikink and breather of sg in order to prove this result we will use backlund transformations implemented by the implicit funct... | [['in', 'this', 'article', 'we', 'prove', 'that', '2soliton', 'solutions', 'of', 'the', 'sinegordon', 'equation', 'sg', 'are', 'orbitally', 'stable', 'in', 'the', 'natural', 'energy', 'space', 'of', 'the', 'problem', 'the', 'solutions', 'that', 'we', 'study', 'are', 'the', 'it', '2kink', 'kinkantikink', 'and', 'breathe... | [-0.13772827459742193, 0.06264528016006385, -0.0975655411467955, 0.0724335388108359, -0.0940688689989274, -0.07296474046492274, -0.001967323334901121, 0.30013044488926727, -0.24665775413935384, -0.2662358459598128, 0.11638503558877847, -0.26429455960844306, -0.18517035632596715, 0.18273890532040293, -0.0682577350703270... |
1,801.09934 | The Necklace Process: A Generating Function Approach | The "necklace process", a procedure constructing necklaces of black and white
beads by randomly choosing positions to insert new beads (whose color is
uniquely determined based on the chosen location), is revisited. This article
illustrates how, after deriving the corresponding bivariate probability
generating functi... | math.PR math.CO | the necklace process a procedure constructing necklaces of black and white beads by randomly choosing positions to insert new beads whose color is uniquely determined based on the chosen location is revisited this article illustrates how after deriving the corresponding bivariate probability generating function the cha... | [['the', 'necklace', 'process', 'a', 'procedure', 'constructing', 'necklaces', 'of', 'black', 'and', 'white', 'beads', 'by', 'randomly', 'choosing', 'positions', 'to', 'insert', 'new', 'beads', 'whose', 'color', 'is', 'uniquely', 'determined', 'based', 'on', 'the', 'chosen', 'location', 'is', 'revisited', 'this', 'arti... | [-0.07438421396738185, 0.13397161967753032, -0.12513476026444031, 0.06209165762507577, -0.065324683217997, -0.10463821136924838, 0.11447712114646233, 0.3500061911929931, -0.24268353184951202, -0.30973345138398667, 0.06404882062093488, -0.21967910384493214, -0.150945839099586, 0.14110571456008725, -0.11648214363958687, ... |
1,801.09935 | On series of translates of positive functions III | Suppose $\Lambda$ is a discrete infinite set of nonnegative real numbers. We
say that $ {\Lambda}$ is of type 1 if the series
$s(x)=\sum_{\lambda\in\Lambda}f(x+\lambda)$ satisfies a zero-one law. This
means that for any non-negative measurable $f: { {\mathbb R}}\to [0,+
{\infty})$ either the convergence set $C(f, {\L... | math.CA | suppose lambda is a discrete infinite set of nonnegative real numbers we say that lambda is of type 1 if the series sxsum_lambdainlambdafxlambda satisfies a zeroone law this means that for any nonnegative measurable f mathbb rto 0 infty either the convergence set cf lambdax sx infty mathbb r modulo sets of lebesgue zer... | [['suppose', 'lambda', 'is', 'a', 'discrete', 'infinite', 'set', 'of', 'nonnegative', 'real', 'numbers', 'we', 'say', 'that', 'lambda', 'is', 'of', 'type', '1', 'if', 'the', 'series', 'sxsum_lambdainlambdafxlambda', 'satisfies', 'a', 'zeroone', 'law', 'this', 'means', 'that', 'for', 'any', 'nonnegative', 'measurable', ... | [-0.19433282737013105, 0.10015617582241947, -0.05567768602342592, 0.04059802383279144, -0.06787047141868263, -0.2335140986662716, 0.03247542783623235, 0.3201181064530849, -0.35597552915266845, -0.12208361618877205, 0.05054215611600564, -0.34647923674287096, -0.07667293187262396, 0.14029198377077484, -0.0651461202217171... |
1,801.09936 | PEYMA: A Tagged Corpus for Persian Named Entities | The goal in the NER task is to classify proper nouns of a text into classes
such as person, location, and organization. This is an important preprocessing
step in many NLP tasks such as question-answering and summarization. Although
many research studies have been conducted in this area in English and the
state-of-th... | cs.CL | the goal in the ner task is to classify proper nouns of a text into classes such as person location and organization this is an important preprocessing step in many nlp tasks such as questionanswering and summarization although many research studies have been conducted in this area in english and the stateoftheart ner ... | [['the', 'goal', 'in', 'the', 'ner', 'task', 'is', 'to', 'classify', 'proper', 'nouns', 'of', 'a', 'text', 'into', 'classes', 'such', 'as', 'person', 'location', 'and', 'organization', 'this', 'is', 'an', 'important', 'preprocessing', 'step', 'in', 'many', 'nlp', 'tasks', 'such', 'as', 'questionanswering', 'and', 'summ... | [-0.042637315052096975, 0.013767689991594795, -0.03252869615457115, 0.1022893228336482, -0.1315407321407375, -0.13939722607646024, 0.03713984786053047, 0.4428548752471353, -0.19910444663084967, -0.3668909764594652, 0.07635258398291589, -0.3523387916743605, -0.09355115399500731, 0.2539872791749811, -0.09993355065311371,... |
1,801.09937 | Binary Compressive Sensing via Smoothed $\ell_0$ Gradient Descent | We present a Compressive Sensing algorithm for reconstructing binary signals
from its linear measurements. The proposed algorithm minimizes a non-convex
cost function expressed as a weighted sum of smoothed $\ell_0$ norms which
takes into account the binariness of signals. We show that for binary signals
the proposed... | eess.SP cs.LG | we present a compressive sensing algorithm for reconstructing binary signals from its linear measurements the proposed algorithm minimizes a nonconvex cost function expressed as a weighted sum of smoothed ell_0 norms which takes into account the binariness of signals we show that for binary signals the proposed algorit... | [['we', 'present', 'a', 'compressive', 'sensing', 'algorithm', 'for', 'reconstructing', 'binary', 'signals', 'from', 'its', 'linear', 'measurements', 'the', 'proposed', 'algorithm', 'minimizes', 'a', 'nonconvex', 'cost', 'function', 'expressed', 'as', 'a', 'weighted', 'sum', 'of', 'smoothed', 'ell_0', 'norms', 'which',... | [-0.14155065027686456, -0.0007544735368962089, -0.10777112767876436, 0.042580441245809196, -0.05773415891453624, -0.1714304394631957, 0.04256388954430198, 0.3916013184313973, -0.33080854114765923, -0.28435153343404335, 0.11034235425565081, -0.24405374073733885, -0.19958928319780778, 0.19932276176599165, -0.052190325284... |
1,801.09938 | Volume and Topological Invariants of Quantum Many-body Systems | A gapped many-body system is described by path integral on a space-time
lattice $C^{d+1}$, which gives rise to a partition function $Z(C^{d+1})$ if
$\partial C^{d+1} =\emptyset$, and gives rise to a vector $|\Psi\rangle$ on the
boundary of space-time if $\partial C^{d+1} \neq\emptyset$. We show that $V =
\text{log} \... | cond-mat.str-el hep-th | a gapped manybody system is described by path integral on a spacetime lattice cd1 which gives rise to a partition function zcd1 if partial cd1 emptyset and gives rise to a vector psirangle on the boundary of spacetime if partial cd1 neqemptyset we show that v textlog sqrtlanglepsipsirangle satisfies the inclusionexclus... | [['a', 'gapped', 'manybody', 'system', 'is', 'described', 'by', 'path', 'integral', 'on', 'a', 'spacetime', 'lattice', 'cd1', 'which', 'gives', 'rise', 'to', 'a', 'partition', 'function', 'zcd1', 'if', 'partial', 'cd1', 'emptyset', 'and', 'gives', 'rise', 'to', 'a', 'vector', 'psirangle', 'on', 'the', 'boundary', 'of',... | [-0.18665404886219197, 0.16167821738593005, -0.1431602485990398, 0.06595560591901953, -0.111622541834891, -0.14747335560738095, 0.04547876923002559, 0.28953533596236003, -0.28571248176709685, -0.19148276100014017, 0.06733271627620395, -0.2954908931558883, -0.17489609942603954, 0.14428593088237066, -0.07469325653269947,... |
1,801.09939 | Macdonald Polynomials of Type $C_n$ with One-Column Diagrams and
Deformed Catalan Numbers | We present an explicit formula for the transition matrix $\mathcal{C}$ from
the type $C_n$ degeneration of the Koornwinder polynomials
$P_{(1^r)}(x\,|\,a,-a,c,-c\,|\,q,t)$ with one column diagrams, to the type
$C_n$ monomial symmetric polynomials $m_{(1^{r})}(x)$. The entries of the
matrix $\mathcal{C}$ enjoy a set o... | math.QA math.CO math.RT | we present an explicit formula for the transition matrix mathcalc from the type c_n degeneration of the koornwinder polynomials p_1rxaaccqt with one column diagrams to the type c_n monomial symmetric polynomials m_1rx the entries of the matrix mathcalc enjoy a set of three term recursion relations which can be regarded... | [['we', 'present', 'an', 'explicit', 'formula', 'for', 'the', 'transition', 'matrix', 'mathcalc', 'from', 'the', 'type', 'c_n', 'degeneration', 'of', 'the', 'koornwinder', 'polynomials', 'p_1rxaaccqt', 'with', 'one', 'column', 'diagrams', 'to', 'the', 'type', 'c_n', 'monomial', 'symmetric', 'polynomials', 'm_1rx', 'the... | [-0.1777189373768087, 0.12427598888625281, -0.044846857346746385, 0.07981425120788674, -0.08892910969348586, -0.17242503930560352, 0.011255159446665523, 0.2705545368775421, -0.370355842749075, -0.17627668206351904, 0.12322142515307749, -0.2872282607452374, -0.20191816515431796, 0.13499816508051388, -0.06204241924748129... |
1,801.0994 | Embedded Clusters | The past decade has seen an increase of star formation studies made at the
molecular cloud scale, motivated mostly by the deployment of a wealth of
sensitive infrared telescopes and instruments. Embedded clusters, long
recognised as the basic units of coherent star formation in molecular clouds,
are now seen to inhab... | astro-ph.GA astro-ph.SR | the past decade has seen an increase of star formation studies made at the molecular cloud scale motivated mostly by the deployment of a wealth of sensitive infrared telescopes and instruments embedded clusters long recognised as the basic units of coherent star formation in molecular clouds are now seen to inhabit pre... | [['the', 'past', 'decade', 'has', 'seen', 'an', 'increase', 'of', 'star', 'formation', 'studies', 'made', 'at', 'the', 'molecular', 'cloud', 'scale', 'motivated', 'mostly', 'by', 'the', 'deployment', 'of', 'a', 'wealth', 'of', 'sensitive', 'infrared', 'telescopes', 'and', 'instruments', 'embedded', 'clusters', 'long', ... | [-0.12621899383306942, 0.10910250520371882, -0.03678324184033508, 0.08011573773150946, -0.02976818584754844, 0.007286045264324867, 0.0033379733247463315, 0.4199270794131592, -0.27006188204840703, -0.34775006070769593, 0.11023111632048134, -0.23520223306966762, -0.05044567282311618, 0.19628172493585402, -0.0026339521272... |
1,801.09941 | Large Deviations in Renewal Theory and Renewal Models of Statistical
Mechanics | We present and establish large deviations principles for general multivariate
renewal-reward processes associated with a classical discrete-time renewal
process. A renewal-reward process describes a cumulative reward over time,
supposing that a broad-sense multivariate reward is obtained at each occurrence
of the eve... | math-ph cond-mat.stat-mech math.MP math.PR | we present and establish large deviations principles for general multivariate renewalreward processes associated with a classical discretetime renewal process a renewalreward process describes a cumulative reward over time supposing that a broadsense multivariate reward is obtained at each occurrence of the event that ... | [['we', 'present', 'and', 'establish', 'large', 'deviations', 'principles', 'for', 'general', 'multivariate', 'renewalreward', 'processes', 'associated', 'with', 'a', 'classical', 'discretetime', 'renewal', 'process', 'a', 'renewalreward', 'process', 'describes', 'a', 'cumulative', 'reward', 'over', 'time', 'supposing'... | [-0.08354021583547383, 0.10524833825963074, -0.10282559868776137, 0.1018067829021344, -0.03111693836075978, -0.13807265392993812, 0.09473086217702884, 0.359505931705688, -0.3072757733741192, -0.241869261104971, 0.11057022551363899, -0.23665339916690506, -0.15106444053276621, 0.1607487582345258, -0.0724067191165317, 0.0... |
1,801.09942 | The MAPLE package TDDS for computing Thomas decompositions of systems of
nonlinear PDEs | We present the Maple package TDDS (Thomas Decomposition of Differential
Systems). Given a polynomially nonlinear differential system, which in addition
to equations may contain inequations, this package computes a decomposition of
it into a finite set of differentially triangular and algebraically simple
subsystems w... | physics.comp-ph math.AC math.AP | we present the maple package tdds thomas decomposition of differential systems given a polynomially nonlinear differential system which in addition to equations may contain inequations this package computes a decomposition of it into a finite set of differentially triangular and algebraically simple subsystems whose su... | [['we', 'present', 'the', 'maple', 'package', 'tdds', 'thomas', 'decomposition', 'of', 'differential', 'systems', 'given', 'a', 'polynomially', 'nonlinear', 'differential', 'system', 'which', 'in', 'addition', 'to', 'equations', 'may', 'contain', 'inequations', 'this', 'package', 'computes', 'a', 'decomposition', 'of',... | [-0.16266120820060617, 0.029392942119866948, -0.10393874641190601, 0.06300731465427696, -0.11904522659292874, -0.17272359295236459, -0.004648461321926584, 0.2693223305926709, -0.33712786629509467, -0.27660996748062855, 0.143580363642496, -0.2658446464147246, -0.1253260397608136, 0.18512156506191815, -0.0447045939937387... |
1,801.09943 | Assisted Vacuum Decay by Time Dependent Electric Fields | We consider the vacuum decay by electron-positron pair production in
spatially homogeneous, time dependent electric fields by means of quantum
kinetic equations. Our focus is on the impact of various pulse shapes as
envelopes of oscillating fields and the assistance effects in multi-scale
fields, which are also seen ... | hep-ph | we consider the vacuum decay by electronpositron pair production in spatially homogeneous time dependent electric fields by means of quantum kinetic equations our focus is on the impact of various pulse shapes as envelopes of oscillating fields and the assistance effects in multiscale fields which are also seen in phot... | [['we', 'consider', 'the', 'vacuum', 'decay', 'by', 'electronpositron', 'pair', 'production', 'in', 'spatially', 'homogeneous', 'time', 'dependent', 'electric', 'fields', 'by', 'means', 'of', 'quantum', 'kinetic', 'equations', 'our', 'focus', 'is', 'on', 'the', 'impact', 'of', 'various', 'pulse', 'shapes', 'as', 'envel... | [-0.155931579580698, 0.25117312017174664, -0.052798516198731306, 0.071240650941291, -0.023202870453691536, -0.044736158200784734, -0.06326428701561924, 0.38395678271588524, -0.239194447893584, -0.2910541812644193, 0.030652111034693296, -0.24493872717823506, -0.050839607816254885, 0.21721389974679864, 0.0562465890604806... |
1,801.09944 | Collisional relaxation and dynamical scaling in multiparticle collisions
dynamics | We present the Multi-Particle-Collision (MPC) dynamics approach to simulate
properties of low-dimensional systems. In particular, we illustrate the method
for a simple model: a one-dimensional gas of point particles interacting
through stochastic collisions and admitting three conservation laws (density,
momentum and... | physics.plasm-ph | we present the multiparticlecollision mpc dynamics approach to simulate properties of lowdimensional systems in particular we illustrate the method for a simple model a onedimensional gas of point particles interacting through stochastic collisions and admitting three conservation laws density momentum and energy motiv... | [['we', 'present', 'the', 'multiparticlecollision', 'mpc', 'dynamics', 'approach', 'to', 'simulate', 'properties', 'of', 'lowdimensional', 'systems', 'in', 'particular', 'we', 'illustrate', 'the', 'method', 'for', 'a', 'simple', 'model', 'a', 'onedimensional', 'gas', 'of', 'point', 'particles', 'interacting', 'through'... | [-0.09663565741387904, 0.1510533344340396, -0.11569540796089839, 0.09666374842734667, 0.010877352932625463, -0.11879855502006585, -0.0070450156746747, 0.3257520239813332, -0.26914861127176704, -0.2714158115928179, 0.006955991433539861, -0.30782425371457783, -0.09555713252433326, 0.16375286959465857, 0.05507133520555905... |
1,801.09945 | Edge on-site potential effects in a honeycomb topological magnon
insulator | The difference between the edge on-site potential and the bulk values in a
magnonic topological honeycomb lattice leads to the formation of edge states in
a bearded boundary, and the same difference is found to be the responsible for
the absence of edge states in a zig-zag termination. In a finite lattice, the
intrin... | cond-mat.mes-hall | the difference between the edge onsite potential and the bulk values in a magnonic topological honeycomb lattice leads to the formation of edge states in a bearded boundary and the same difference is found to be the responsible for the absence of edge states in a zigzag termination in a finite lattice the intrinsic ons... | [['the', 'difference', 'between', 'the', 'edge', 'onsite', 'potential', 'and', 'the', 'bulk', 'values', 'in', 'a', 'magnonic', 'topological', 'honeycomb', 'lattice', 'leads', 'to', 'the', 'formation', 'of', 'edge', 'states', 'in', 'a', 'bearded', 'boundary', 'and', 'the', 'same', 'difference', 'is', 'found', 'to', 'be'... | [-0.2366263276399595, 0.23933632352619216, -0.062364220332679465, 0.05708462302773741, -0.031374483227786, -0.16456748740667285, 0.08527032878141497, 0.41208871060596974, -0.2974442525060269, -0.2609284373064493, 0.04941093685518918, -0.31163205507468306, -0.12273218975892163, 0.06784186171014504, 0.044132823056284465,... |
1,801.09946 | "23andMe confirms: I'm super white" -- Analyzing Twitter Discourse On
Genetic Testing | Recent progress in genomics is bringing genetic testing to the masses.
Participatory public initiatives are underway to sequence the genome of
millions of volunteers, and a new market is booming with a number of companies
like 23andMe and AncestryDNA offering affordable tests directly to consumers.
Consequently, news... | cs.SI cs.CY | recent progress in genomics is bringing genetic testing to the masses participatory public initiatives are underway to sequence the genome of millions of volunteers and a new market is booming with a number of companies like 23andme and ancestrydna offering affordable tests directly to consumers consequently news exper... | [['recent', 'progress', 'in', 'genomics', 'is', 'bringing', 'genetic', 'testing', 'to', 'the', 'masses', 'participatory', 'public', 'initiatives', 'are', 'underway', 'to', 'sequence', 'the', 'genome', 'of', 'millions', 'of', 'volunteers', 'and', 'a', 'new', 'market', 'is', 'booming', 'with', 'a', 'number', 'of', 'compa... | [-0.07757383217519745, 0.05786306228277818, -0.03276979411460178, 0.11869683820273252, -0.18518776114467742, -0.14396539898940697, 0.1282717414158572, 0.4223913664595698, -0.22070832235984644, -0.35752515999143414, 0.13609468938292987, -0.38021612525253146, -0.1975122304536613, 0.21252140443099943, -0.10099057468172726... |
1,801.09947 | Causality in Quantum Field Theory with Classical Sources - Quantum
Electrodynamics | In an exact quantum-mechanical framework, we show that expectation values of
the second-quantized electro-magnetic fields in the Coulomb gauge, and in the
presence of classical sources, automatically lead to causal and retarded
electro-magnetic field strengths. The classical $\hbar$-independent Maxwell's
equations na... | quant-ph gr-qc hep-th | in an exact quantummechanical framework we show that expectation values of the secondquantized electromagnetic fields in the coulomb gauge and in the presence of classical sources automatically lead to causal and retarded electromagnetic field strengths the classical hbarindependent maxwells equations naturally emerge ... | [['in', 'an', 'exact', 'quantummechanical', 'framework', 'we', 'show', 'that', 'expectation', 'values', 'of', 'the', 'secondquantized', 'electromagnetic', 'fields', 'in', 'the', 'coulomb', 'gauge', 'and', 'in', 'the', 'presence', 'of', 'classical', 'sources', 'automatically', 'lead', 'to', 'causal', 'and', 'retarded', ... | [-0.10365707092774167, 0.16300303042092784, -0.07653814008210222, 0.12378272136122408, -0.078369145229144, -0.101893871766843, 0.009085379757354376, 0.31713160681439906, -0.2461633030907251, -0.302415634895688, 0.006699726411836668, -0.23317635456972402, -0.18536126088928168, 0.1901664236022658, -0.033208693389151195, ... |
1,801.09948 | Playing with universality classes of Barkhausen avalanches | Many systems crackle, from earthquakes and financial market to Barkhausen
effect in ferromagnetic materials. Despite the diversity in essence, the noise
emitted in these dynamical systems consists of avalanche-like events with broad
range of sizes and durations, characterized by power-law avalanche
distributions and ... | cond-mat.dis-nn cond-mat.mtrl-sci cond-mat.stat-mech | many systems crackle from earthquakes and financial market to barkhausen effect in ferromagnetic materials despite the diversity in essence the noise emitted in these dynamical systems consists of avalanchelike events with broad range of sizes and durations characterized by powerlaw avalanche distributions and typical ... | [['many', 'systems', 'crackle', 'from', 'earthquakes', 'and', 'financial', 'market', 'to', 'barkhausen', 'effect', 'in', 'ferromagnetic', 'materials', 'despite', 'the', 'diversity', 'in', 'essence', 'the', 'noise', 'emitted', 'in', 'these', 'dynamical', 'systems', 'consists', 'of', 'avalanchelike', 'events', 'with', 'b... | [-0.10871357208816335, 0.20025894598937918, -0.07013999757141709, 0.05340056349222175, -0.006900565090946593, -0.090605193741625, 0.029085776665746126, 0.4069910690406348, -0.2638698881221285, -0.30310292325935567, 0.04348955295240875, -0.31253831876918325, -0.1561776586391335, 0.19507658825970667, 0.006976179234401951... |
1,801.09949 | Observational constraints on quantum decoherence during inflation | Since inflationary perturbations must generically couple to all degrees of
freedom present in the early Universe, it is more realistic to view these
fluctuations as an open quantum system interacting with an environment. Then,
on very general grounds, their evolution can be modelled with a Lindblad
equation. This mod... | astro-ph.CO gr-qc hep-th quant-ph | since inflationary perturbations must generically couple to all degrees of freedom present in the early universe it is more realistic to view these fluctuations as an open quantum system interacting with an environment then on very general grounds their evolution can be modelled with a lindblad equation this modified e... | [['since', 'inflationary', 'perturbations', 'must', 'generically', 'couple', 'to', 'all', 'degrees', 'of', 'freedom', 'present', 'in', 'the', 'early', 'universe', 'it', 'is', 'more', 'realistic', 'to', 'view', 'these', 'fluctuations', 'as', 'an', 'open', 'quantum', 'system', 'interacting', 'with', 'an', 'environment', ... | [-0.13280602069730363, 0.14400930272392792, -0.09552599176214162, 0.09084999177350916, -0.06788178234234113, -0.13720952157798985, -0.009669136977754534, 0.32485595865767786, -0.24033204674593767, -0.31751890196464955, 0.10222969106557271, -0.24479751222004945, -0.11968539855972102, 0.20676246235274118, -0.041999142621... |
1,801.0995 | Model Based Desgin Environment for Launcher Upper Stage GNC Development | The cost associated with developing flight control forms a significant part
of the overall development cost. The increased demand for greater functionality
and for extending the domain of applicability of future launchers leads to
higher complexity of the GNC algorithms. Furthermore, there is also a need for
a respon... | cs.SY | the cost associated with developing flight control forms a significant part of the overall development cost the increased demand for greater functionality and for extending the domain of applicability of future launchers leads to higher complexity of the gnc algorithms furthermore there is also a need for a responsive ... | [['the', 'cost', 'associated', 'with', 'developing', 'flight', 'control', 'forms', 'a', 'significant', 'part', 'of', 'the', 'overall', 'development', 'cost', 'the', 'increased', 'demand', 'for', 'greater', 'functionality', 'and', 'for', 'extending', 'the', 'domain', 'of', 'applicability', 'of', 'future', 'launchers', '... | [-0.1261078408324944, 0.05821815099481778, -0.06207890421807717, -0.00698189624516712, -0.07880702304751858, -0.13297095703034612, 0.02918778014655369, 0.3866566789557079, -0.24076713179697676, -0.33895198438978313, 0.14161046570408967, -0.19463224241840898, -0.16823345134770007, 0.23474163701145076, -0.077094594482332... |
1,801.09951 | Features in the diffraction of a scalar plane wave from doubly-periodic
Dirichlet and Neumann surfaces | The diffraction of a scalar plane wave from a doubly-periodic surface on
which either the Dirichlet or Neumann boundary condition is imposed is studied
by means of a rigorous numerical solution of the Rayleigh equation for the
amplitudes of the diffracted Bragg beams. From the results of these
calculations the diffra... | physics.optics | the diffraction of a scalar plane wave from a doublyperiodic surface on which either the dirichlet or neumann boundary condition is imposed is studied by means of a rigorous numerical solution of the rayleigh equation for the amplitudes of the diffracted bragg beams from the results of these calculations the diffractio... | [['the', 'diffraction', 'of', 'a', 'scalar', 'plane', 'wave', 'from', 'a', 'doublyperiodic', 'surface', 'on', 'which', 'either', 'the', 'dirichlet', 'or', 'neumann', 'boundary', 'condition', 'is', 'imposed', 'is', 'studied', 'by', 'means', 'of', 'a', 'rigorous', 'numerical', 'solution', 'of', 'the', 'rayleigh', 'equati... | [-0.16681173797375262, 0.13847710441641667, -0.11298626345880264, 0.044538159358113276, -0.051093073157997396, -0.06434962280758924, 0.020741779020160334, 0.3507757480191132, -0.24496371059400074, -0.27007855512722806, 0.10614866430796292, -0.30169147607004204, -0.13104602578747365, 0.2577864149995669, 0.02703997221117... |
1,801.09952 | Numerical Calibration of the HCN$-$Star Formation Correlation | HCN(1$-$0) emission traces dense gas and correlates very strongly with star
formation rates (SFRs) on scales from small Milky Way clouds to whole galaxies.
The observed correlation offers strong constraints on the efficiency of star
formation in dense gas, but quantitative interpretation of this constraint
requires a... | astro-ph.GA astro-ph.SR | hcn10 emission traces dense gas and correlates very strongly with star formation rates sfrs on scales from small milky way clouds to whole galaxies the observed correlation offers strong constraints on the efficiency of star formation in dense gas but quantitative interpretation of this constraint requires a mapping fr... | [['hcn10', 'emission', 'traces', 'dense', 'gas', 'and', 'correlates', 'very', 'strongly', 'with', 'star', 'formation', 'rates', 'sfrs', 'on', 'scales', 'from', 'small', 'milky', 'way', 'clouds', 'to', 'whole', 'galaxies', 'the', 'observed', 'correlation', 'offers', 'strong', 'constraints', 'on', 'the', 'efficiency', 'o... | [-0.08289746152864688, 0.09629856278650392, -0.00479754388190644, 0.09020503703859108, 0.014174483868333957, -0.00903300685889047, 0.07248187383242033, 0.4554391637606465, -0.16663138512926906, -0.33015247137164294, -0.002847372048595191, -0.26896169194141806, 0.01068402512565903, 0.14205269994943037, 0.020026895913052... |
1,801.09953 | Period variations of Algol-type eclipsing binaries AD And, TW Cas and IV
Cas | We present new analysis of O-C diagrams variations of three Algol-type
eclipsing binary stars AD And, TW Cas and IV Cas. We have used all published
minima times (including visual and photographic) as well as new determined ones
from our and SuperWasp observations. We determined orbital parameters of the
3rd bodies in... | astro-ph.SR | we present new analysis of oc diagrams variations of three algoltype eclipsing binary stars ad and tw cas and iv cas we have used all published minima times including visual and photographic as well as new determined ones from our and superwasp observations we determined orbital parameters of the 3rd bodies in the syst... | [['we', 'present', 'new', 'analysis', 'of', 'oc', 'diagrams', 'variations', 'of', 'three', 'algoltype', 'eclipsing', 'binary', 'stars', 'ad', 'and', 'tw', 'cas', 'and', 'iv', 'cas', 'we', 'have', 'used', 'all', 'published', 'minima', 'times', 'including', 'visual', 'and', 'photographic', 'as', 'well', 'as', 'new', 'det... | [-0.08974588030928767, 0.031400515349929804, -0.07777492270119242, 0.05135062851707686, -0.0798321052065508, -0.15288390322066434, 0.13751951929253453, 0.3967658812487191, -0.22010226056470975, -0.35585613978596836, 0.09256673758148451, -0.28567784207944685, -0.16498260276781007, 0.2553620924814962, -0.0489444465448076... |
1,801.09954 | Hill's Spherical Vortex in a Rotating Fluid | A popular model for a generic fat-cored vortex ring or eddy is Hill's
spherical vortex (Phil. Trans. Roy. Soc. A vol. 185, 1894, p. 213). Here we
find an exact solution for such a spherical vortex steadily propagating along
the axis of a rotating ideal fluid. The spherical vortex swirls in such a way
as to exactly ca... | physics.flu-dyn | a popular model for a generic fatcored vortex ring or eddy is hills spherical vortex phil trans roy soc a vol 185 1894 p 213 here we find an exact solution for such a spherical vortex steadily propagating along the axis of a rotating ideal fluid the spherical vortex swirls in such a way as to exactly cancel out the bac... | [['a', 'popular', 'model', 'for', 'a', 'generic', 'fatcored', 'vortex', 'ring', 'or', 'eddy', 'is', 'hills', 'spherical', 'vortex', 'phil', 'trans', 'roy', 'soc', 'a', 'vol', '185', '1894', 'p', '213', 'here', 'we', 'find', 'an', 'exact', 'solution', 'for', 'such', 'a', 'spherical', 'vortex', 'steadily', 'propagating',... | [-0.21019051651865805, 0.1299028936081745, -0.06271427969581314, 0.003415232394925422, -0.0745911742486651, -0.11170778599279445, -0.03478264474607487, 0.33389746909961104, -0.2690628126618408, -0.23101322615883194, 0.0892115173369853, -0.231268591247499, -0.09200309638103973, 0.17539496514539693, -0.026850210957548817... |
1,801.09955 | COBRA: A Fast and Simple Method for Active Clustering with Pairwise
Constraints | Clustering is inherently ill-posed: there often exist multiple valid
clusterings of a single dataset, and without any additional information a
clustering system has no way of knowing which clustering it should produce.
This motivates the use of constraints in clustering, as they allow users to
communicate their inter... | cs.AI cs.LG stat.ML | clustering is inherently illposed there often exist multiple valid clusterings of a single dataset and without any additional information a clustering system has no way of knowing which clustering it should produce this motivates the use of constraints in clustering as they allow users to communicate their interests to... | [['clustering', 'is', 'inherently', 'illposed', 'there', 'often', 'exist', 'multiple', 'valid', 'clusterings', 'of', 'a', 'single', 'dataset', 'and', 'without', 'any', 'additional', 'information', 'a', 'clustering', 'system', 'has', 'no', 'way', 'of', 'knowing', 'which', 'clustering', 'it', 'should', 'produce', 'this',... | [-0.10687435842701234, 0.044118865515429206, -0.1094667446683161, 0.07930894308810821, -0.15568701550218975, -0.1637561037990963, 0.07532444501121063, 0.3998066069325432, -0.26870936868872375, -0.4040333245298825, 0.08591347805049736, -0.27349900860572235, -0.0959415524484939, 0.16292717636169982, -0.04045454845763743,... |
1,801.09956 | Nonparametric Bayesian volatility estimation | Given discrete time observations over a fixed time interval, we study a
nonparametric Bayesian approach to estimation of the volatility coefficient of
a stochastic differential equation. We postulate a histogram-type prior on the
volatility with piecewise constant realisations on bins forming a partition of
the time ... | stat.ME math.ST q-fin.ST stat.TH | given discrete time observations over a fixed time interval we study a nonparametric bayesian approach to estimation of the volatility coefficient of a stochastic differential equation we postulate a histogramtype prior on the volatility with piecewise constant realisations on bins forming a partition of the time inter... | [['given', 'discrete', 'time', 'observations', 'over', 'a', 'fixed', 'time', 'interval', 'we', 'study', 'a', 'nonparametric', 'bayesian', 'approach', 'to', 'estimation', 'of', 'the', 'volatility', 'coefficient', 'of', 'a', 'stochastic', 'differential', 'equation', 'we', 'postulate', 'a', 'histogramtype', 'prior', 'on',... | [-0.03698996849739411, 0.034006824543792204, -0.11334304752810968, 0.10803744865684059, -0.10012327821184624, -0.11043287067138773, 0.11070160164156796, 0.47255123588513204, -0.27163569003666244, -0.2782793765645621, 0.12675031287206967, -0.23364212190343697, -0.08712008359336008, 0.20453707651440495, -0.06954205448108... |
1,801.09957 | Valley qubit in gated MoS$_2$ monolayer quantum dot | The aim of presented research is to design a nanodevice, based on a MoS$_2$
monolayer, performing operations on a well-defined valley qubit. We show how to
confine an electron in a gate induced quantum dot within the monolayer, and to
perform the NOT operation on its valley degree of freedom. The operations are
carri... | cond-mat.mes-hall | the aim of presented research is to design a nanodevice based on a mos_2 monolayer performing operations on a welldefined valley qubit we show how to confine an electron in a gate induced quantum dot within the monolayer and to perform the not operation on its valley degree of freedom the operations are carried out all... | [['the', 'aim', 'of', 'presented', 'research', 'is', 'to', 'design', 'a', 'nanodevice', 'based', 'on', 'a', 'mos_2', 'monolayer', 'performing', 'operations', 'on', 'a', 'welldefined', 'valley', 'qubit', 'we', 'show', 'how', 'to', 'confine', 'an', 'electron', 'in', 'a', 'gate', 'induced', 'quantum', 'dot', 'within', 'th... | [-0.1703349752719269, 0.1346063901890279, -0.03528567759770483, 0.0006460893009237847, -0.004095436364877969, -0.17601746467469065, 0.1045927292725537, 0.42614496437416066, -0.2325711182784289, -0.2887856643279328, 0.01116986942207931, -0.23522165026760808, -0.16428374792571718, 0.21990256084092452, 0.02598773664488506... |
1,801.09958 | Non-Reciprocal Transmission and Reflection of a Chirally-Coupled Quantum
Dot | We report strongly non-reciprocal behaviour for quantum dot exciton spins
coupled to nano-photonic waveguides under resonant laser excitation. A clear
dependence of the transmission spectrum on the propagation direction is found
for a chirally-coupled quantum dot, with spin up and spin down exciton spins
coupling to ... | quant-ph cond-mat.mes-hall | we report strongly nonreciprocal behaviour for quantum dot exciton spins coupled to nanophotonic waveguides under resonant laser excitation a clear dependence of the transmission spectrum on the propagation direction is found for a chirallycoupled quantum dot with spin up and spin down exciton spins coupling to the lef... | [['we', 'report', 'strongly', 'nonreciprocal', 'behaviour', 'for', 'quantum', 'dot', 'exciton', 'spins', 'coupled', 'to', 'nanophotonic', 'waveguides', 'under', 'resonant', 'laser', 'excitation', 'a', 'clear', 'dependence', 'of', 'the', 'transmission', 'spectrum', 'on', 'the', 'propagation', 'direction', 'is', 'found',... | [-0.20594312593549768, 0.1865415529917249, -0.02243142111105061, -0.04323129271370332, -0.04550772517153593, -0.22441677554623685, 0.027196865433078504, 0.4830447395427901, -0.2829058412046315, -0.2467069218746304, -0.00668174983763841, -0.3090041066371949, -0.10341732432983085, 0.2446536257118857, 0.0532889605334429, ... |
1,801.09959 | The effect of polarization on the propagation distance of leaky guided
modes | We show that transverse-magnetic (TM) leaky modes can propagate further than
transverse electric (TE) modes in real-index dielectric waveguides. We compute
the density of states and find that while the TE spectrum contains only
overlapping resonances, the TM spectrum typically contains several isolated
peaks. By tran... | physics.optics | we show that transversemagnetic tm leaky modes can propagate further than transverse electric te modes in realindex dielectric waveguides we compute the density of states and find that while the te spectrum contains only overlapping resonances the tm spectrum typically contains several isolated peaks by transforming th... | [['we', 'show', 'that', 'transversemagnetic', 'tm', 'leaky', 'modes', 'can', 'propagate', 'further', 'than', 'transverse', 'electric', 'te', 'modes', 'in', 'realindex', 'dielectric', 'waveguides', 'we', 'compute', 'the', 'density', 'of', 'states', 'and', 'find', 'that', 'while', 'the', 'te', 'spectrum', 'contains', 'on... | [-0.15481889938107796, 0.1739340914141697, -0.0529769158249514, 0.04645309404392416, -0.05685177898655335, -0.15398960575047466, -0.004496661787076543, 0.4344115661457181, -0.23625713522649475, -0.26913437648779814, -0.024311859275783516, -0.4015746991150081, -0.14366745820475949, 0.17459300466709668, 0.095073650813558... |
1,801.0996 | Dependence of the Substructure Abundance on the Orientation Coherence of
the Halo Tidal Field | A numerical evidence for the dependence of the substructure abundance of
cluster halos on the orientation coherence of the surrounding tidal fields is
presented. Applying the adapted minimal spanning tree (MST) algorithm to the
cluster halos with $M\ge 10^{14}\,h^{-1}\,M_{\odot}$ from the Big
MultiDark-Planck Simulat... | astro-ph.CO | a numerical evidence for the dependence of the substructure abundance of cluster halos on the orientation coherence of the surrounding tidal fields is presented applying the adapted minimal spanning tree mst algorithm to the cluster halos with mge 1014h1m_odot from the big multidarkplanck simulations we identify primar... | [['a', 'numerical', 'evidence', 'for', 'the', 'dependence', 'of', 'the', 'substructure', 'abundance', 'of', 'cluster', 'halos', 'on', 'the', 'orientation', 'coherence', 'of', 'the', 'surrounding', 'tidal', 'fields', 'is', 'presented', 'applying', 'the', 'adapted', 'minimal', 'spanning', 'tree', 'mst', 'algorithm', 'to'... | [-0.1338887004047153, 0.14865504734941173, -0.058470911344411125, 0.07329256936440143, -0.08116771250409133, 0.003671759765060768, -0.010602207044886134, 0.4086302454693376, -0.2300456218688674, -0.35420853521611995, 0.04897556642369064, -0.2535145682506735, -0.033156406902609875, 0.14705060090563155, 0.027206880276244... |
1,801.09961 | Modeling Influence with Semantics in Social Networks: a Survey | The discovery of influential entities in all kinds of networks (e.g. social,
digital, or computer) has always been an important field of study. In recent
years, Online Social Networks (OSNs) have been established as a basic means of
communication and often influencers and opinion makers promote politics,
events, bran... | cs.IR cs.SI | the discovery of influential entities in all kinds of networks eg social digital or computer has always been an important field of study in recent years online social networks osns have been established as a basic means of communication and often influencers and opinion makers promote politics events brands or products... | [['the', 'discovery', 'of', 'influential', 'entities', 'in', 'all', 'kinds', 'of', 'networks', 'eg', 'social', 'digital', 'or', 'computer', 'has', 'always', 'been', 'an', 'important', 'field', 'of', 'study', 'in', 'recent', 'years', 'online', 'social', 'networks', 'osns', 'have', 'been', 'established', 'as', 'a', 'basi... | [-0.08801047786970631, 0.03495973367473383, -0.05543624585241837, 0.09044024842234834, -0.12456463834949595, -0.1085465775794839, 0.06302537525790917, 0.4363862594305459, -0.24877477384772215, -0.32720806347640324, 0.12070910030802301, -0.3400061306370012, -0.2599207507643722, 0.14234906126610872, -0.0648654909657002, ... |
1,801.09962 | Symmetries and similarities of planar algebraic curves using harmonic
polynomials | We present novel, deterministic, efficient algorithms to compute the
symmetries of a planar algebraic curve, implicitly defined, and to check
whether or not two given implicit planar algebraic curves are similar, i.e.
equal up to a similarity transformation. Both algorithms are based on the fact,
well-known in Harmon... | math.AG cs.SC | we present novel deterministic efficient algorithms to compute the symmetries of a planar algebraic curve implicitly defined and to check whether or not two given implicit planar algebraic curves are similar ie equal up to a similarity transformation both algorithms are based on the fact wellknown in harmonic analysis ... | [['we', 'present', 'novel', 'deterministic', 'efficient', 'algorithms', 'to', 'compute', 'the', 'symmetries', 'of', 'a', 'planar', 'algebraic', 'curve', 'implicitly', 'defined', 'and', 'to', 'check', 'whether', 'or', 'not', 'two', 'given', 'implicit', 'planar', 'algebraic', 'curves', 'are', 'similar', 'ie', 'equal', 'u... | [-0.1237086110340897, 0.047146156549085085, -0.08216075054951943, 0.10716488643083721, -0.14138893461010107, -0.18681794459795734, 0.017865217123471666, 0.4141418811244269, -0.29309909587512567, -0.24075544745816538, 0.09332607078370832, -0.23795168053523716, -0.19134187247012355, 0.24001240656313408, -0.10181172194885... |
1,801.09963 | Order closed ideals in pre-Riesz spaces and their relationship to bands | In Archimedean vector lattices bands can be introduced via three different
coinciding notions. First, they are order closed ideals. Second, they are
precisely those ideals which equal their double disjoint complements. The third
concept is that of an ideal which contains the supremum of any of its bounded
subsets, pr... | math.FA | in archimedean vector lattices bands can be introduced via three different coinciding notions first they are order closed ideals second they are precisely those ideals which equal their double disjoint complements the third concept is that of an ideal which contains the supremum of any of its bounded subsets provided t... | [['in', 'archimedean', 'vector', 'lattices', 'bands', 'can', 'be', 'introduced', 'via', 'three', 'different', 'coinciding', 'notions', 'first', 'they', 'are', 'order', 'closed', 'ideals', 'second', 'they', 'are', 'precisely', 'those', 'ideals', 'which', 'equal', 'their', 'double', 'disjoint', 'complements', 'the', 'thi... | [-0.1744140786907993, 0.15484533024937264, -0.032928269935858456, 0.10023843440996093, -0.10758829425457259, -0.12025807230722506, -0.013121507341735238, 0.3805368411798723, -0.34298450545662323, -0.12088088297046894, 0.09443246944655859, -0.30152182894498974, -0.12015163628817645, 0.15542907814690193, -0.0960650389342... |
1,801.09964 | Statistical Equilibrium in Quantum Gravity: Gibbs states in Group Field
Theory | Gibbs states are known to play a crucial role in the statistical description
of a system with a large number of degrees of freedom. They are expected to be
vital also in a quantum gravitational system with many underlying fundamental
discrete degrees of freedom. However, due to the absence of well-defined
concepts of... | gr-qc cond-mat.stat-mech hep-th | gibbs states are known to play a crucial role in the statistical description of a system with a large number of degrees of freedom they are expected to be vital also in a quantum gravitational system with many underlying fundamental discrete degrees of freedom however due to the absence of welldefined concepts of time ... | [['gibbs', 'states', 'are', 'known', 'to', 'play', 'a', 'crucial', 'role', 'in', 'the', 'statistical', 'description', 'of', 'a', 'system', 'with', 'a', 'large', 'number', 'of', 'degrees', 'of', 'freedom', 'they', 'are', 'expected', 'to', 'be', 'vital', 'also', 'in', 'a', 'quantum', 'gravitational', 'system', 'with', 'm... | [-0.12271688446214112, 0.1666735509834148, -0.13179113631270797, 0.05886345476470163, -0.06659485367108643, -0.1339507527026105, 0.03221813154294507, 0.337308745997947, -0.2614738414107536, -0.2890247352401353, 0.08797663110417064, -0.2326913925244723, -0.12327093500571493, 0.1450741001502665, -0.0872907308745651, 0.05... |
1,801.09965 | Extremal and stationary discs for the Kobayashi $k$-metric | We generalize Lempert's and Poletsky's works on the description of extremal
discs for the Kobayashi metric to a higher order setting.
| math.CV | we generalize lemperts and poletskys works on the description of extremal discs for the kobayashi metric to a higher order setting | [['we', 'generalize', 'lemperts', 'and', 'poletskys', 'works', 'on', 'the', 'description', 'of', 'extremal', 'discs', 'for', 'the', 'kobayashi', 'metric', 'to', 'a', 'higher', 'order', 'setting']] | [-0.11209676627601896, 0.012168849807321316, -0.0822900759854487, 0.15144950417535646, -0.13213075635333857, -0.06585760048723646, 0.027702139291380132, 0.3285420128986949, -0.12153232640897234, -0.25938395463994574, 0.09042577452159353, -0.29213555840154487, -0.1484919243625232, 0.1955087280699185, -0.1892682029643938... |
1,801.09966 | On the propagation of regularity and decay of solutions to the Benjamin
equation | In this paper, we investigate some special regularities and decay properties
of solutions to the initial value problem(IVP) of the Benjamin equation. The
main result shows that: for initial datum $u_{0}\in H^{s}(\mathbb{R})$ with
$s>3/4,$ if the restriction of $u_{0}$ belongs to $H^{l}((x_{0}, \infty))$ for
some $l\i... | math.AP | in this paper we investigate some special regularities and decay properties of solutions to the initial value problemivp of the benjamin equation the main result shows that for initial datum u_0in hsmathbbr with s34 if the restriction of u_0 belongs to hlx_0 infty for some lin mathbbz and x_0in mathbbr then the restric... | [['in', 'this', 'paper', 'we', 'investigate', 'some', 'special', 'regularities', 'and', 'decay', 'properties', 'of', 'solutions', 'to', 'the', 'initial', 'value', 'problemivp', 'of', 'the', 'benjamin', 'equation', 'the', 'main', 'result', 'shows', 'that', 'for', 'initial', 'datum', 'u_0in', 'hsmathbbr', 'with', 's34', ... | [-0.12914760433227182, 0.09888118303925113, -0.06877343622541213, 0.008049456859905138, -0.09106302905984852, -0.17516900100240326, -0.01321888312063438, 0.3056159989392183, -0.3509412428296833, -0.13184180850140662, 0.15737844302448029, -0.3221308344677764, -0.03875388297061604, 0.1431490850679756, -0.0753924650061561... |
1,801.09967 | Secure and Robust Identification via Classical-Quantum Channels | We study the identification capacity of classical-quantum channels
("cq-channels"), under channel uncertainty and privacy constraints. To be
precise, we consider first compound memoryless cq-channels and determine their
identification capacity; then we add an eavesdropper, considering compound
memoryless wiretap cqq-... | quant-ph cs.IT math.IT | we study the identification capacity of classicalquantum channels cqchannels under channel uncertainty and privacy constraints to be precise we consider first compound memoryless cqchannels and determine their identification capacity then we add an eavesdropper considering compound memoryless wiretap cqqchannels and de... | [['we', 'study', 'the', 'identification', 'capacity', 'of', 'classicalquantum', 'channels', 'cqchannels', 'under', 'channel', 'uncertainty', 'and', 'privacy', 'constraints', 'to', 'be', 'precise', 'we', 'consider', 'first', 'compound', 'memoryless', 'cqchannels', 'and', 'determine', 'their', 'identification', 'capacity... | [-0.24665649118674857, 0.015525011958013491, -0.009008411349741374, 0.05086031075183708, -0.06963109895650323, -0.2955172803018521, 0.21103332116312923, 0.31948211152410627, -0.2935580714212946, -0.21955764189134447, 0.15033723060500992, -0.29759868224259134, -0.08469422988523888, 0.1233593864971455, -0.135138261205196... |
1,801.09968 | Chemical analysis of eight giant stars of the globular cluster NGC 6366 | The metal-rich Galactic globular cluster NGC 6366 is the fifth closest to the
Sun. Despite its interest, it has received scarce attention, and little is
known about its internal structure. Its kinematics suggests a link to the halo,
but its metallicity indicates otherwise. We present a detailed chemical
analysis of e... | astro-ph.GA | the metalrich galactic globular cluster ngc 6366 is the fifth closest to the sun despite its interest it has received scarce attention and little is known about its internal structure its kinematics suggests a link to the halo but its metallicity indicates otherwise we present a detailed chemical analysis of eight gian... | [['the', 'metalrich', 'galactic', 'globular', 'cluster', 'ngc', '6366', 'is', 'the', 'fifth', 'closest', 'to', 'the', 'sun', 'despite', 'its', 'interest', 'it', 'has', 'received', 'scarce', 'attention', 'and', 'little', 'is', 'known', 'about', 'its', 'internal', 'structure', 'its', 'kinematics', 'suggests', 'a', 'link'... | [-0.07706605409528466, 0.06397737706516496, -0.057206829444964746, 0.09797427522362737, -0.09895420939535586, -0.06762165575544687, 0.06199199193526185, 0.46058321393045465, -0.1452872144184323, -0.4032252847671437, 0.006090748383087705, -0.31586087712847094, -0.035353794056193336, 0.19205602489249862, -0.0595601894656... |
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