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 |
|---|---|---|---|---|---|---|
1,801.00969 | Towards platform-independent verification of the standard mathematical
functions: the square root function | The paper presents (human-oriented) specification and (pen-and-paper)
verification of the square root function. The function implements Newton method
and uses a look-up table for initial approximations. Specification is done in
terms of total correctness assertions with use of precise arithmetic and the
mathematical ... | cs.LO | the paper presents humanoriented specification and penandpaper verification of the square root function the function implements newton method and uses a lookup table for initial approximations specification is done in terms of total correctness assertions with use of precise arithmetic and the mathematical square root ... | [['the', 'paper', 'presents', 'humanoriented', 'specification', 'and', 'penandpaper', 'verification', 'of', 'the', 'square', 'root', 'function', 'the', 'function', 'implements', 'newton', 'method', 'and', 'uses', 'a', 'lookup', 'table', 'for', 'initial', 'approximations', 'specification', 'is', 'done', 'in', 'terms', '... | [-0.10039020153462998, -0.02333943225774851, -0.10620659485585608, 0.06601737547365917, -0.11405835982601521, -0.15117597666971574, 0.05775681843535217, 0.377654464512874, -0.23095476900592893, -0.34033711434547176, 0.1511251558589165, -0.21861380782625559, -0.14063581069773537, 0.2395853518934573, -0.13894649012945592... |
1,801.0097 | Intertwining for semi-direct product operads | This paper shows that the semi-direct product construction for $G$-operads
and the levelwise Borel construction for $G$-cooperads are intertwined by the
topological operadic bar construction. En route we give a generalization of the
bar construction of M. Ching from reduced to certain non-reduced topological
operads.... | math.AT math.QA | this paper shows that the semidirect product construction for goperads and the levelwise borel construction for gcooperads are intertwined by the topological operadic bar construction en route we give a generalization of the bar construction of m ching from reduced to certain nonreduced topological operads | [['this', 'paper', 'shows', 'that', 'the', 'semidirect', 'product', 'construction', 'for', 'goperads', 'and', 'the', 'levelwise', 'borel', 'construction', 'for', 'gcooperads', 'are', 'intertwined', 'by', 'the', 'topological', 'operadic', 'bar', 'construction', 'en', 'route', 'we', 'give', 'a', 'generalization', 'of', '... | [-0.17049831888356873, 0.12054991551003484, -0.1068254702746175, 0.04024150112892912, -0.11134225457127012, -0.10891077363170511, 0.006486710596851311, 0.27105395140689476, -0.3344498989280573, -0.21332890954041897, 0.05430013867268382, -0.18163655992857244, -0.2234201489644515, 0.1956412006158728, -0.17119275702726702... |
1,801.00971 | Strong spin-orbit interaction and magnetotransport in semiconductor
Bi$_2$O$_2$Se nanoplates | Semiconductor Bi$_2$O$_2$Se nanolayers of high crystal quality have been
realized via epitaxial growth. These two-dimensional (2D) materials possess
excellent electron transport properties with potential application in
nanoelectronics. It is also strongly expected that the 2D Bi$_2$O$_2$Se
nanolayers could be of an e... | cond-mat.mes-hall | semiconductor bi_2o_2se nanolayers of high crystal quality have been realized via epitaxial growth these twodimensional 2d materials possess excellent electron transport properties with potential application in nanoelectronics it is also strongly expected that the 2d bi_2o_2se nanolayers could be of an excellent materi... | [['semiconductor', 'bi_2o_2se', 'nanolayers', 'of', 'high', 'crystal', 'quality', 'have', 'been', 'realized', 'via', 'epitaxial', 'growth', 'these', 'twodimensional', '2d', 'materials', 'possess', 'excellent', 'electron', 'transport', 'properties', 'with', 'potential', 'application', 'in', 'nanoelectronics', 'it', 'is'... | [-0.19341141328320136, 0.20699136241767388, -0.03983008469055806, -0.03850187584567739, -0.005150797753119651, -0.1955734790678193, 0.02206606127271828, 0.4281062549621589, -0.2709349202115697, -0.310768305095939, -0.008687047240899267, -0.3257625047497603, -0.1342941542757124, 0.2527700634898941, 0.06623645801790895, ... |
1,801.00972 | Plasma flow around and charge distribution of a dust cluster in a rf
discharge | We employ a particle-in-cell Monte Carlo collision/particle-particle
particle-mesh (PIC-MCC/PPPM) simulation to study the plasma flow around and the
charge distribution of a three-dimensional dust cluster in the sheath of a
low-pressure rf argon discharge. The geometry of the cluster and its position
in the sheath ar... | physics.plasm-ph | we employ a particleincell monte carlo collisionparticleparticle particlemesh picmccpppm simulation to study the plasma flow around and the charge distribution of a threedimensional dust cluster in the sheath of a lowpressure rf argon discharge the geometry of the cluster and its position in the sheath are fixed to the... | [['we', 'employ', 'a', 'particleincell', 'monte', 'carlo', 'collisionparticleparticle', 'particlemesh', 'picmccpppm', 'simulation', 'to', 'study', 'the', 'plasma', 'flow', 'around', 'and', 'the', 'charge', 'distribution', 'of', 'a', 'threedimensional', 'dust', 'cluster', 'in', 'the', 'sheath', 'of', 'a', 'lowpressure',... | [-0.10551185748168354, 0.19420758464317667, -0.056733960211989495, 0.035969447768853136, 0.019106874987991945, -0.06354068601732982, 0.023476208105958143, 0.3736171917325074, -0.24060489398635965, -0.29690150471526333, 0.04365946693012562, -0.2823405707855531, 0.0010092593602266141, 0.16262273345386885, 0.0118539987088... |
1,801.00973 | A New Wald Test for Hypothesis Testing Based on MCMC outputs | In this paper, a new and convenient $\chi^2$ wald test based on MCMC outputs
is proposed for hypothesis testing. The new statistic can be explained as MCMC
version of Wald test and has several important advantages that make it very
convenient in practical applications. First, it is well-defined under improper
prior d... | econ.EM stat.ME | in this paper a new and convenient chi2 wald test based on mcmc outputs is proposed for hypothesis testing the new statistic can be explained as mcmc version of wald test and has several important advantages that make it very convenient in practical applications first it is welldefined under improper prior distribution... | [['in', 'this', 'paper', 'a', 'new', 'and', 'convenient', 'chi2', 'wald', 'test', 'based', 'on', 'mcmc', 'outputs', 'is', 'proposed', 'for', 'hypothesis', 'testing', 'the', 'new', 'statistic', 'can', 'be', 'explained', 'as', 'mcmc', 'version', 'of', 'wald', 'test', 'and', 'has', 'several', 'important', 'advantages', 't... | [0.019690769250571196, 0.04131023017162945, -0.1684820667751843, 0.14779723949322943, -0.109705200806881, -0.15654807347926267, 0.06369523163275084, 0.40460088184391635, -0.2638085562066408, -0.3317154871432909, 0.12595079019055924, -0.2242583526198619, -0.10724344779737294, 0.24182224635955035, -0.09183243689282487, 0... |
1,801.00974 | Optimal Learning from the Doob-Dynkin lemma | The Doob-Dynkin Lemma gives conditions on two functions $X$ and $Y$ that
ensure existence of a function ${\phi}$ so that $X = {\phi} \circ Y$. This
communication proves different versions of the Doob-Dynkin Lemma, and shows how
it is related to optimal statistical learning algorithms.
Keywords and phrases: Improper... | math.ST math.PR stat.TH | the doobdynkin lemma gives conditions on two functions x and y that ensure existence of a function phi so that x phi circ y this communication proves different versions of the doobdynkin lemma and shows how it is related to optimal statistical learning algorithms keywords and phrases improper prior descriptive set theo... | [['the', 'doobdynkin', 'lemma', 'gives', 'conditions', 'on', 'two', 'functions', 'x', 'and', 'y', 'that', 'ensure', 'existence', 'of', 'a', 'function', 'phi', 'so', 'that', 'x', 'phi', 'circ', 'y', 'this', 'communication', 'proves', 'different', 'versions', 'of', 'the', 'doobdynkin', 'lemma', 'and', 'shows', 'how', 'it... | [-0.09840550012725952, 0.04814552249997083, -0.16129476013432803, 0.1558842738961865, -0.08483403429372943, -0.17070280361503107, 0.10799397698980917, 0.40514197913480215, -0.33710713135399695, -0.27112675573805284, 0.015456070986993867, -0.2731188868959274, -0.15561978650632605, 0.19911924996493577, -0.132767570124746... |
1,801.00975 | Nonlinear waves and polarization in diffusive directed particle flow | We consider a system of two reaction-diffusion-advection equations describing
the one dimensional directed motion of particles with superimposed diffusion
and mutual alignment. For this system we show the existence of traveling wave
solutions for weak diffusion by singular perturbation techniques and provide
evidence... | math.AP physics.flu-dyn | we consider a system of two reactiondiffusionadvection equations describing the one dimensional directed motion of particles with superimposed diffusion and mutual alignment for this system we show the existence of traveling wave solutions for weak diffusion by singular perturbation techniques and provide evidence for ... | [['we', 'consider', 'a', 'system', 'of', 'two', 'reactiondiffusionadvection', 'equations', 'describing', 'the', 'one', 'dimensional', 'directed', 'motion', 'of', 'particles', 'with', 'superimposed', 'diffusion', 'and', 'mutual', 'alignment', 'for', 'this', 'system', 'we', 'show', 'the', 'existence', 'of', 'traveling', ... | [-0.1863688429611489, 0.12287096597586127, -0.05666353341309761, 0.08286362845348944, -0.058471788031359516, -0.09231449180314767, -0.010807526137294441, 0.3502140925747567, -0.2840010587918176, -0.25034741559547596, 0.10962692752009494, -0.2653675214869195, -0.17933324516761576, 0.1881918212179437, 0.06746152238170991... |
1,801.00976 | Asymptotic mean value properties for fractional anisotropic operators | We obtain an asymptotic representation formula for harmonic functions with
respect to a linear anisotropic nonlocal operator. Furthermore we get a
Bourgain-Brezis-Mironescu type limit formula for a related class of anisotropic
nonlocal norms.
| math.AP | we obtain an asymptotic representation formula for harmonic functions with respect to a linear anisotropic nonlocal operator furthermore we get a bourgainbrezismironescu type limit formula for a related class of anisotropic nonlocal norms | [['we', 'obtain', 'an', 'asymptotic', 'representation', 'formula', 'for', 'harmonic', 'functions', 'with', 'respect', 'to', 'a', 'linear', 'anisotropic', 'nonlocal', 'operator', 'furthermore', 'we', 'get', 'a', 'bourgainbrezismironescu', 'type', 'limit', 'formula', 'for', 'a', 'related', 'class', 'of', 'anisotropic', '... | [-0.07591576781123877, 0.05111142898826846, -0.11797693865655949, 0.12946061321505994, -0.1258455008607019, -0.15998744099598491, -0.019835439369534, 0.32932926285447495, -0.276880989020521, -0.1577391858639506, 0.07794172801500694, -0.2916367668094057, -0.17888003079728645, 0.22462424703619696, -0.043971799977236624, ... |
1,801.00977 | Integrated quantile functions: properties and applications | In this paper we provide a systematic exposition of basic properties of
integrated distribution and quantile functions. We define these transforms in
such a way that they characterize any probability distribution on the real line
and are Fenchel conjugates of each other. We show that uniform integrability,
weak conve... | math.PR | in this paper we provide a systematic exposition of basic properties of integrated distribution and quantile functions we define these transforms in such a way that they characterize any probability distribution on the real line and are fenchel conjugates of each other we show that uniform integrability weak convergenc... | [['in', 'this', 'paper', 'we', 'provide', 'a', 'systematic', 'exposition', 'of', 'basic', 'properties', 'of', 'integrated', 'distribution', 'and', 'quantile', 'functions', 'we', 'define', 'these', 'transforms', 'in', 'such', 'a', 'way', 'that', 'they', 'characterize', 'any', 'probability', 'distribution', 'on', 'the', ... | [-0.068106917549146, 0.012384022235793135, -0.12974819055029957, 0.11967994907460554, -0.0631535531823883, -0.055411971473863515, 0.040060289291720286, 0.4285533701687461, -0.2776028858036688, -0.23625904888071414, 0.11788287730242061, -0.2581420171969008, -0.2012927561334454, 0.22380885649656895, -0.10009878818268454,... |
1,801.00978 | A quadratic finite element wavelet Riesz basis | In this paper, continuous piecewise quadratic finite element wavelets are
constructed on general polygons in $\mathbb{R}^2$. The wavelets are stable in
$H^s$ for $|s|<\frac{3}{2}$ and have two vanishing moments. Each wavelet is a
linear combination of 11 or 13 nodal basis functions. Numerically computed
condition num... | math.NA | in this paper continuous piecewise quadratic finite element wavelets are constructed on general polygons in mathbbr2 the wavelets are stable in hs for sfrac32 and have two vanishing moments each wavelet is a linear combination of 11 or 13 nodal basis functions numerically computed condition numbers for s in 101 are pro... | [['in', 'this', 'paper', 'continuous', 'piecewise', 'quadratic', 'finite', 'element', 'wavelets', 'are', 'constructed', 'on', 'general', 'polygons', 'in', 'mathbbr2', 'the', 'wavelets', 'are', 'stable', 'in', 'hs', 'for', 'sfrac32', 'and', 'have', 'two', 'vanishing', 'moments', 'each', 'wavelet', 'is', 'a', 'linear', '... | [-0.155326352513969, 0.14339369393253168, -0.012911545337244337, 0.06714940290631992, -0.027920506528711746, -0.13055555667961016, -0.039784982415897376, 0.39651172659068834, -0.2759891609395189, -0.16445473075145856, 0.17994536701423516, -0.28402816470978515, -0.1117728825400783, 0.2100917884423065, -0.023840715110834... |
1,801.00979 | Counting rational points on quadric surfaces | We give an upper bound for the number of rational points of height at most
$B$, lying on a surface defined by a quadratic form $Q$. The bound shows an
explicit dependence on $Q$. It is optimal with respect to $B$, and is also
optimal for typical forms $Q$.
| math.NT | we give an upper bound for the number of rational points of height at most b lying on a surface defined by a quadratic form q the bound shows an explicit dependence on q it is optimal with respect to b and is also optimal for typical forms q | [['we', 'give', 'an', 'upper', 'bound', 'for', 'the', 'number', 'of', 'rational', 'points', 'of', 'height', 'at', 'most', 'b', 'lying', 'on', 'a', 'surface', 'defined', 'by', 'a', 'quadratic', 'form', 'q', 'the', 'bound', 'shows', 'an', 'explicit', 'dependence', 'on', 'q', 'it', 'is', 'optimal', 'with', 'respect', 'to'... | [-0.19227189557360752, 0.09945745274426929, -0.07644629324501266, 0.031586827886081775, -0.05129966960877788, -0.1524986867811911, 0.10498809276566821, 0.301141148718188, -0.23528681483775454, -0.31577333290609816, 0.049587910814324815, -0.2734743295978679, -0.13139928979989218, 0.28616670446888526, -0.0293982212754840... |
1,801.0098 | Simple Explicit Formula for Near-Optimal Stochastic Lifestyling | In life-cycle economics the Samuelson paradigm (Samuelson, 1969) states that
the optimal investment is in constant proportions out of lifetime wealth
composed of current savings and the present value of future income. It is well
known that in the presence of credit constraints this paradigm no longer
applies. Instead... | q-fin.PM | in lifecycle economics the samuelson paradigm samuelson 1969 states that the optimal investment is in constant proportions out of lifetime wealth composed of current savings and the present value of future income it is well known that in the presence of credit constraints this paradigm no longer applies instead optimal... | [['in', 'lifecycle', 'economics', 'the', 'samuelson', 'paradigm', 'samuelson', '1969', 'states', 'that', 'the', 'optimal', 'investment', 'is', 'in', 'constant', 'proportions', 'out', 'of', 'lifetime', 'wealth', 'composed', 'of', 'current', 'savings', 'and', 'the', 'present', 'value', 'of', 'future', 'income', 'it', 'is... | [-0.09635060055066563, 0.060335204349703166, -0.060662551916982624, 0.08127464090110352, -0.11154997445661537, -0.13302376366552118, 0.13104490129905433, 0.3529110876460598, -0.2621867576437007, -0.31298554248227545, 0.1011802756605504, -0.2549635215872924, -0.13422439084388316, 0.1835552280041555, -0.18219901353426993... |
1,801.00981 | A Model-Free Selection Criterion For The Mixing Coefficient Of Spatial
Max-Mixture Models | One of the main concerns in extreme value theory is to quantify the
dependence between joint tails. Using stochastic processes that lack
flexibility in the joint tail may lead to severe under-or over-estimation of
probabilities associated to simultaneous extreme events. Following recent
advances in the literature, a ... | math.ST math.PR stat.TH | one of the main concerns in extreme value theory is to quantify the dependence between joint tails using stochastic processes that lack flexibility in the joint tail may lead to severe underor overestimation of probabilities associated to simultaneous extreme events following recent advances in the literature a flexibl... | [['one', 'of', 'the', 'main', 'concerns', 'in', 'extreme', 'value', 'theory', 'is', 'to', 'quantify', 'the', 'dependence', 'between', 'joint', 'tails', 'using', 'stochastic', 'processes', 'that', 'lack', 'flexibility', 'in', 'the', 'joint', 'tail', 'may', 'lead', 'to', 'severe', 'underor', 'overestimation', 'of', 'prob... | [-0.05600689953743396, 0.025710596371385636, -0.12931374425181386, 0.10500845512389347, -0.08917466606098143, -0.10575093436195995, 0.04348848597146571, 0.3774341490881687, -0.2493832288239377, -0.2842636278117866, 0.09875448928902518, -0.24913465868766335, -0.17606474270172784, 0.17845175207758351, -0.1264663579252859... |
1,801.00982 | Thick distribution tails in models of cancer secondary tumors | Recent progress in microdissection and in DNA sequencing has enabled
subsampling of multi-focal cancers in organs such as the liver in several
hundred spots, helping to determine the pattern of mutations in each of these
spots. This has led to the construction of genealogies of the primary,
secondary, tertiary and so... | q-bio.PE | recent progress in microdissection and in dna sequencing has enabled subsampling of multifocal cancers in organs such as the liver in several hundred spots helping to determine the pattern of mutations in each of these spots this has led to the construction of genealogies of the primary secondary tertiary and so forth ... | [['recent', 'progress', 'in', 'microdissection', 'and', 'in', 'dna', 'sequencing', 'has', 'enabled', 'subsampling', 'of', 'multifocal', 'cancers', 'in', 'organs', 'such', 'as', 'the', 'liver', 'in', 'several', 'hundred', 'spots', 'helping', 'to', 'determine', 'the', 'pattern', 'of', 'mutations', 'in', 'each', 'of', 'th... | [-0.06089663463552777, 0.08982058309675746, -0.09756081316031907, 0.03832653396355837, -0.03683721601325823, -0.08248033357637101, 0.05423512543723183, 0.35060900137269574, -0.20006002534769082, -0.2758718317307189, 0.08749693464487791, -0.26628550845443416, -0.19104609456722085, 0.1865464608074705, -0.1135178695408333... |
1,801.00983 | Stabilisation of wave equations on the torus with rough dampings | For the damped wave equation on a compact manifold with {\em continuous}
dampings, the geometric control condition is necessary and sufficient for
{uniform} stabilisation. In this article, on the two dimensional torus, in the
special case where $a(x) = \sum\_{j=1}^N a\_j 1\_{x\in R\_j}$ ($R\_j$ are
polygons), we give... | math.AP | for the damped wave equation on a compact manifold with em continuous dampings the geometric control condition is necessary and sufficient for uniform stabilisation in this article on the two dimensional torus in the special case where ax sum_j1n a_j 1_xin r_j r_j are polygons we give a very simple necessary and suffic... | [['for', 'the', 'damped', 'wave', 'equation', 'on', 'a', 'compact', 'manifold', 'with', 'em', 'continuous', 'dampings', 'the', 'geometric', 'control', 'condition', 'is', 'necessary', 'and', 'sufficient', 'for', 'uniform', 'stabilisation', 'in', 'this', 'article', 'on', 'the', 'two', 'dimensional', 'torus', 'in', 'the',... | [-0.17599222940459316, 0.11103042632540953, -0.041962575339961665, 0.06853532043273194, -0.1354849454073701, -0.16953986609171676, -0.001139642165591275, 0.3788405063429049, -0.22637756973771112, -0.16506037939897006, 0.17213279114418714, -0.16185735976614524, -0.16661181171158596, 0.2167275380675814, -0.15556171868645... |
1,801.00984 | Sentence Object Notation: Multilingual sentence notation based on
Wordnet | The representation of sentences is a very important task. It can be used as a
way to exchange data inter-applications. One main characteristic, that a
notation must have, is a minimal size and a representative form. This can
reduce the transfer time, and hopefully the processing time as well.
Usually, sentence repr... | cs.CL cs.AI | the representation of sentences is a very important task it can be used as a way to exchange data interapplications one main characteristic that a notation must have is a minimal size and a representative form this can reduce the transfer time and hopefully the processing time as well usually sentence representation is... | [['the', 'representation', 'of', 'sentences', 'is', 'a', 'very', 'important', 'task', 'it', 'can', 'be', 'used', 'as', 'a', 'way', 'to', 'exchange', 'data', 'interapplications', 'one', 'main', 'characteristic', 'that', 'a', 'notation', 'must', 'have', 'is', 'a', 'minimal', 'size', 'and', 'a', 'representative', 'form', ... | [-0.036679327658821266, 0.07327055865239208, -0.0951104044479312, 0.15283037424477242, -0.23100999255700622, -0.14380690243790653, 0.057453454466128935, 0.43608778631794287, -0.31404848276665476, -0.32162609367627376, 0.07665353521300967, -0.28720495643703986, -0.13973417584664416, 0.20145469124462903, -0.1306314581581... |
1,801.00985 | The GALEX Ultraviolet Virgo Cluster Survey (GUViCS). VII.: BCG UV upturn
and the FUV-NUV color up to redshift 0.35 | CONTEXT:At low redshift, early-type galaxies often exhibit a rising flux with
decreasing wavelength in the 1000-2500 \AA{} range, called "UV upturn". The
origin of this phenomenon is debated, and its evolution with redshift is poorly
constrained. The observed GALEX FUV-NUV color can be used to probe the UV
upturn app... | astro-ph.GA | contextat low redshift earlytype galaxies often exhibit a rising flux with decreasing wavelength in the 10002500 aa range called uv upturn the origin of this phenomenon is debated and its evolution with redshift is poorly constrained the observed galex fuvnuv color can be used to probe the uv upturn approximately to re... | [['contextat', 'low', 'redshift', 'earlytype', 'galaxies', 'often', 'exhibit', 'a', 'rising', 'flux', 'with', 'decreasing', 'wavelength', 'in', 'the', '10002500', 'aa', 'range', 'called', 'uv', 'upturn', 'the', 'origin', 'of', 'this', 'phenomenon', 'is', 'debated', 'and', 'its', 'evolution', 'with', 'redshift', 'is', '... | [-0.016732410850429518, 0.0958229094285212, -0.06725565096975342, 0.11953355206869247, -0.1126067197439513, -0.04222338708010015, 0.0904906738838618, 0.47774034394253895, -0.12633986613756912, -0.3947584808330028, 0.04092723539894252, -0.34296389280176226, -0.03252615632585146, 0.18564397216810666, -0.06552123735046908... |
1,801.00986 | Maximal lexicographic spectra and ranks for states with fixed uniform
margins | We find the spectrum in maximal lexicographic order for quantum states
$\rho_{AB}\in\mathcal{H}_A\otimes \mathcal{H}_B$ with margins
$\rho_A=\frac{1}{n}I_n$ and $\rho_B=\frac{1}{m}I_m$ and discuss the
construction of $\rho_{AB}$. By nonzero rectangular Kronecker coefficients, we
give counterexamples for Klyachko's co... | math.RT | we find the spectrum in maximal lexicographic order for quantum states rho_abinmathcalh_aotimes mathcalh_b with margins rho_afrac1ni_n and rho_bfrac1mi_m and discuss the construction of rho_ab by nonzero rectangular kronecker coefficients we give counterexamples for klyachkos conjecture which says that a quantum state ... | [['we', 'find', 'the', 'spectrum', 'in', 'maximal', 'lexicographic', 'order', 'for', 'quantum', 'states', 'rho_abinmathcalh_aotimes', 'mathcalh_b', 'with', 'margins', 'rho_afrac1ni_n', 'and', 'rho_bfrac1mi_m', 'and', 'discuss', 'the', 'construction', 'of', 'rho_ab', 'by', 'nonzero', 'rectangular', 'kronecker', 'coeffic... | [-0.16000879770861223, 0.1809798212793584, -0.029147691014581003, 0.023342353804036976, -0.028837869703196562, -0.17077520245399613, 0.033464854762244686, 0.35301141324094854, -0.25948813420433836, -0.22397584820596073, 0.09686362963492194, -0.3158980414092254, -0.12744564594557653, 0.17993619533685537, -0.075958272026... |
1,801.00987 | Probing quasi-integrability of the Gross-Pitaevskii equation in a
harmonic-oscillator potential | Previous simulations of the one-dimensional Gross-Pitaevskii equation (GPE)
with repulsive nonlinearity and a harmonic-oscillator trapping potential hint
towards the emergence of quasi-integrable dynamics -- in the sense of
quasi-periodic evolution of a moving dark soliton without any signs of
ergodicity -- although ... | cond-mat.quant-gas | previous simulations of the onedimensional grosspitaevskii equation gpe with repulsive nonlinearity and a harmonicoscillator trapping potential hint towards the emergence of quasiintegrable dynamics in the sense of quasiperiodic evolution of a moving dark soliton without any signs of ergodicity although this model does... | [['previous', 'simulations', 'of', 'the', 'onedimensional', 'grosspitaevskii', 'equation', 'gpe', 'with', 'repulsive', 'nonlinearity', 'and', 'a', 'harmonicoscillator', 'trapping', 'potential', 'hint', 'towards', 'the', 'emergence', 'of', 'quasiintegrable', 'dynamics', 'in', 'the', 'sense', 'of', 'quasiperiodic', 'evol... | [-0.13412172645834422, 0.07617469873677203, -0.11547916690767857, 0.08755550221341275, -0.06315617055047258, -0.1460920122697688, -0.0033477303366497638, 0.32468873057968733, -0.25931777038168524, -0.221205876524015, 0.07938539101060753, -0.2542641222102159, -0.13538989221404601, 0.14804689101619284, 0.0054268208563393... |
1,801.00988 | Joint Uplink and Downlink Resource Configuration for Ultra-reliable and
Low-latency Communications | Supporting ultra-reliable and low-latency communications (URLLC) is one of
the major goals for the fifth-generation cellular networks. Since spectrum
usage efficiency is always a concern, and large bandwidth is required for
ensuring stringent quality-of-service (QoS), we minimize the total bandwidth
under the QoS con... | cs.IT math.IT | supporting ultrareliable and lowlatency communications urllc is one of the major goals for the fifthgeneration cellular networks since spectrum usage efficiency is always a concern and large bandwidth is required for ensuring stringent qualityofservice qos we minimize the total bandwidth under the qos constraints of ur... | [['supporting', 'ultrareliable', 'and', 'lowlatency', 'communications', 'urllc', 'is', 'one', 'of', 'the', 'major', 'goals', 'for', 'the', 'fifthgeneration', 'cellular', 'networks', 'since', 'spectrum', 'usage', 'efficiency', 'is', 'always', 'a', 'concern', 'and', 'large', 'bandwidth', 'is', 'required', 'for', 'ensurin... | [-0.3526968670587168, 0.007822215613172784, 0.05013538636657268, 0.018370531428683334, -0.09353358441651725, -0.26612994242069454, 0.2041366970323816, 0.4431196939570741, -0.2611494738150251, -0.2868152331921677, 0.06429086780694865, -0.24370758557516634, -0.13618083157288935, 0.1149201582171296, -0.18170857674525123, ... |
1,801.00989 | On the invariance equation for two-variable weighted nonsymmetric
Bajraktarevi\'c means | The purpose of this paper is to investigate the invariance of the arithmetic
mean with respect to two weighted Bajraktarevi\'c means, i.e., to solve the
functional equation $$
\bigg(\frac{f}{g}\bigg)^{\!\!-1}\!\!\bigg(\frac{tf(x)+sf(y)}{tg(x)+sg(y)}\bigg)
+\bigg(\frac{h}{k}\bigg)^{\!\!-1}\!\!\bigg(\frac{sh(x)+th(... | math.CA | the purpose of this paper is to investigate the invariance of the arithmetic mean with respect to two weighted bajraktarevic means ie to solve the functional equation biggfracfgbigg1biggfractfxsfytgxsgybigg biggfrachkbigg1biggfracshxthyskxtkybiggxy qquadxyin i where fghkitomathbbr are unknown continuous functions such ... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'investigate', 'the', 'invariance', 'of', 'the', 'arithmetic', 'mean', 'with', 'respect', 'to', 'two', 'weighted', 'bajraktarevic', 'means', 'ie', 'to', 'solve', 'the', 'functional', 'equation', 'biggfracfgbigg1biggfractfxsfytgxsgybigg', 'biggfrachkbigg1biggfracshx... | [-0.12212525663171703, 0.11238685754798548, -0.03509416743660363, 0.04957898040780815, -0.04822993147944179, -0.09450250108526131, -0.015814390205386504, 0.37412565654126284, -0.3123637700331545, -0.24247041300959693, 0.12587597145629334, -0.2880357238257339, -0.1574381181217347, 0.17392065717020533, -0.075804420219185... |
1,801.0099 | A two-stage fourth order time-accurate discretization for Lax--Wendroff
type flow solvers II. High order numerical boundary conditions | This paper serves to treat boundary conditions numerically with high order
accuracy in order to match the two-stage fourth-order finite volume schemes for
hyperbolic problems developed in [{\em J. Li and Z. Du, A two-stage fourth
order time-accurate discretization {L}ax--{W}endroff type flow solvers, {I}.
{H}yperboli... | math.NA | this paper serves to treat boundary conditions numerically with high order accuracy in order to match the twostage fourthorder finite volume schemes for hyperbolic problems developed in em j li and z du a twostage fourth order timeaccurate discretization laxwendroff type flow solvers i hyperbolic conservation laws siam... | [['this', 'paper', 'serves', 'to', 'treat', 'boundary', 'conditions', 'numerically', 'with', 'high', 'order', 'accuracy', 'in', 'order', 'to', 'match', 'the', 'twostage', 'fourthorder', 'finite', 'volume', 'schemes', 'for', 'hyperbolic', 'problems', 'developed', 'in', 'em', 'j', 'li', 'and', 'z', 'du', 'a', 'twostage',... | [-0.08751016573697191, 0.07042287120999005, -0.05941941748343168, 0.045155596191359657, -0.1032309448990267, -0.14866851916223386, 0.0037373821106245785, 0.36232939533930064, -0.29025544592260905, -0.30182487166525307, 0.1513563173250102, -0.2338511262406608, -0.1402635686056611, 0.17254331564500688, -0.118432810521751... |
1,801.00991 | Reconciling Magma-Ocean Crystallization Models with the present-day
Structure of the Earth's mantle | Terrestrial planets are thought to experience episode(s) of large-scale
melting early in their history. Fractionation during magma-ocean freezing leads
to unstable stratification within the related cumulate layers due to
progressive iron enrichment upward, but the effects of incremental cumulate
overturns during MO c... | astro-ph.EP | terrestrial planets are thought to experience episodes of largescale melting early in their history fractionation during magmaocean freezing leads to unstable stratification within the related cumulate layers due to progressive iron enrichment upward but the effects of incremental cumulate overturns during mo crystalli... | [['terrestrial', 'planets', 'are', 'thought', 'to', 'experience', 'episodes', 'of', 'largescale', 'melting', 'early', 'in', 'their', 'history', 'fractionation', 'during', 'magmaocean', 'freezing', 'leads', 'to', 'unstable', 'stratification', 'within', 'the', 'related', 'cumulate', 'layers', 'due', 'to', 'progressive', ... | [-0.05650346476738, 0.24894136341902232, -0.06500902727004462, 0.04519385189372607, -0.04937552743779715, -0.06604677062610362, 0.06303364478810729, 0.3418075097127339, -0.2736843790357594, -0.30746333967379436, 0.1344869601094482, -0.24099329297267075, -0.11845727581000788, 0.14305846976320735, -0.05650660012587451, -... |
1,801.00992 | The Capacity on Degraded Relay Broadcast Channel | The relay broadcast channel (RBC) is considered, in which a transmitter
communicates with two receivers with the assistance of a relay. Based on
different degradation orders among the relay and the receivers' outputs, three
types of physically degraded RBCs (PDRBCs) are introduced. Inner bounds and
outer bounds are d... | cs.IT math.IT | the relay broadcast channel rbc is considered in which a transmitter communicates with two receivers with the assistance of a relay based on different degradation orders among the relay and the receivers outputs three types of physically degraded rbcs pdrbcs are introduced inner bounds and outer bounds are derived on t... | [['the', 'relay', 'broadcast', 'channel', 'rbc', 'is', 'considered', 'in', 'which', 'a', 'transmitter', 'communicates', 'with', 'two', 'receivers', 'with', 'the', 'assistance', 'of', 'a', 'relay', 'based', 'on', 'different', 'degradation', 'orders', 'among', 'the', 'relay', 'and', 'the', 'receivers', 'outputs', 'three'... | [-0.2592754217568697, 0.07359943747901776, 0.010344454593311144, 0.02125348292353497, -0.07201709444671282, -0.33303717182450526, 0.08017536151538214, 0.34630156669208384, -0.24002597434812878, -0.25661926064640284, 0.11697814926343757, -0.3040966812198556, -0.08119549915766505, 0.13729675553416407, -0.0907422183186923... |
1,801.00993 | Continuum Percolation of Polydisperse Rods in Quadrupole Fields: Theory
and Simulations | We investigate percolation in mixtures of nanorods in the presence of
external fields that align or disalign the particles with the field axis. Such
conditions are found in the formulation and processing of nanocomposites, where
the field may be electric, magnetic, or due to elongational flow. Our focus is
on the eff... | cond-mat.soft | we investigate percolation in mixtures of nanorods in the presence of external fields that align or disalign the particles with the field axis such conditions are found in the formulation and processing of nanocomposites where the field may be electric magnetic or due to elongational flow our focus is on the effect of ... | [['we', 'investigate', 'percolation', 'in', 'mixtures', 'of', 'nanorods', 'in', 'the', 'presence', 'of', 'external', 'fields', 'that', 'align', 'or', 'disalign', 'the', 'particles', 'with', 'the', 'field', 'axis', 'such', 'conditions', 'are', 'found', 'in', 'the', 'formulation', 'and', 'processing', 'of', 'nanocomposit... | [-0.11427534457166182, 0.18645917590122757, -0.07583598012660536, 0.039716987997878254, -0.03258755290113722, -0.09644491678417855, 0.011374635602953995, 0.37052016080061134, -0.23851887013965337, -0.28722246001337387, 0.08116858280642868, -0.2525471404317564, -0.1574782253199712, 0.17425472104322715, 0.009051963788919... |
1,801.00994 | Quantum uncertainty relation based on the mean deviation | Traditional forms of quantum uncertainty relations are invariably based on
the standard deviation. This can be understood in the historical context of
simultaneous development of quantum theory and mathematical statistics. Here,
we present alternative forms of uncertainty relations, in both state dependent
and state ... | quant-ph | traditional forms of quantum uncertainty relations are invariably based on the standard deviation this can be understood in the historical context of simultaneous development of quantum theory and mathematical statistics here we present alternative forms of uncertainty relations in both state dependent and state indepe... | [['traditional', 'forms', 'of', 'quantum', 'uncertainty', 'relations', 'are', 'invariably', 'based', 'on', 'the', 'standard', 'deviation', 'this', 'can', 'be', 'understood', 'in', 'the', 'historical', 'context', 'of', 'simultaneous', 'development', 'of', 'quantum', 'theory', 'and', 'mathematical', 'statistics', 'here',... | [-0.05361466277972795, 0.09329882691055537, -0.1320804508626461, 0.15505944117996842, -0.08513307155296207, -0.11167959352582693, 0.0932868713485077, 0.31000584054738284, -0.2630510376729071, -0.32346238278225065, 0.0974479630291462, -0.27259119037166235, -0.15154002493899316, 0.22659079850791022, -0.09584890982136131,... |
1,801.00995 | Tight-binding Piezoelectric Theory and Electromechanical Coupling
Correlations for Transition Metal Dichalcogenide Monolayers | The lack of inversion symmetry in semiconducting transition metal
dichalcogenide monolayers (TMDMs) enables a considerable molecular-level
intrinsic piezoelectricity, which opens prospects for atomically-thin
piezotronics and optoelectronics. Here, based on the tight-binding (TB)
approach and Berry phase polarization... | cond-mat.mes-hall | the lack of inversion symmetry in semiconducting transition metal dichalcogenide monolayers tmdms enables a considerable molecularlevel intrinsic piezoelectricity which opens prospects for atomicallythin piezotronics and optoelectronics here based on the tightbinding tb approach and berry phase polarization theory we e... | [['the', 'lack', 'of', 'inversion', 'symmetry', 'in', 'semiconducting', 'transition', 'metal', 'dichalcogenide', 'monolayers', 'tmdms', 'enables', 'a', 'considerable', 'molecularlevel', 'intrinsic', 'piezoelectricity', 'which', 'opens', 'prospects', 'for', 'atomicallythin', 'piezotronics', 'and', 'optoelectronics', 'he... | [-0.14924982062075287, 0.16571148367972152, -0.04166998805255086, 0.032079234037276666, -0.08379163520488267, -0.17388572190344956, 0.08738556605821941, 0.42635769097444914, -0.29403389187840123, -0.2542682261749481, -0.06743694836234984, -0.2777773781058689, -0.2656723771292794, 0.17661054180546973, 0.0944451893252941... |
1,801.00996 | Non-Hermitian gauged topological laser arrays | Stable and phase-locked emission in an extended topological supermode of
coupled laser arrays, based on concepts of non-Hermitian and topological
photonics, is theoretically suggested. We consider a non-Hermitian
Su-Schrieffer-Heeger chain of coupled microring resonators and show that
application of a synthetic imagi... | physics.optics quant-ph | stable and phaselocked emission in an extended topological supermode of coupled laser arrays based on concepts of nonhermitian and topological photonics is theoretically suggested we consider a nonhermitian suschriefferheeger chain of coupled microring resonators and show that application of a synthetic imaginary gauge... | [['stable', 'and', 'phaselocked', 'emission', 'in', 'an', 'extended', 'topological', 'supermode', 'of', 'coupled', 'laser', 'arrays', 'based', 'on', 'concepts', 'of', 'nonhermitian', 'and', 'topological', 'photonics', 'is', 'theoretically', 'suggested', 'we', 'consider', 'a', 'nonhermitian', 'suschriefferheeger', 'chai... | [-0.20889584539639475, 0.22912692757175548, -0.02775478793387466, 0.006610786654590835, -0.05533955398683263, -0.2512650440150328, -0.0005811105504945184, 0.44414423338541414, -0.21152466659607216, -0.22367448450387578, 0.049243016961747696, -0.26056271451896273, -0.1596050097368064, 0.2071663182768641, 0.0192786624085... |
1,801.00997 | Expectations of the Cosmic Antideuteron Flux | The cosmic antideuteron is a promising probe for the dark matter annihilation
signature. In order to determine the DM signature, the background astrophysical
antideuteron flux should be carefully studied. In this work we provide a new
calculation of the secondary antideuteron flux, and pay special attention to
the un... | astro-ph.HE hep-ph | the cosmic antideuteron is a promising probe for the dark matter annihilation signature in order to determine the dm signature the background astrophysical antideuteron flux should be carefully studied in this work we provide a new calculation of the secondary antideuteron flux and pay special attention to the uncertai... | [['the', 'cosmic', 'antideuteron', 'is', 'a', 'promising', 'probe', 'for', 'the', 'dark', 'matter', 'annihilation', 'signature', 'in', 'order', 'to', 'determine', 'the', 'dm', 'signature', 'the', 'background', 'astrophysical', 'antideuteron', 'flux', 'should', 'be', 'carefully', 'studied', 'in', 'this', 'work', 'we', '... | [-0.10105882579468618, 0.16761054240755344, -0.07223569860163712, 0.20608361558577298, -0.08286675368260621, -0.06368820002316532, -0.003107208427728007, 0.3571468715492944, -0.2254997911666961, -0.39462915374162166, 0.02016167641666375, -0.31184056549879224, 0.003273497391632177, 0.21515427272122606, 0.049393708103851... |
1,801.00998 | Perspectives on scaling and multiscaling in passive scalar turbulence | We revisit the well-known problem of multiscaling in substances passively
advected by homogeneous and isotropic turbulent flows or passive scalar
turbulence. To that end we propose a two-parameter continuum hydrodynamic model
for an advected substance concentration $\theta$, parametrised jointly by $y$
and $\overline... | cond-mat.stat-mech | we revisit the wellknown problem of multiscaling in substances passively advected by homogeneous and isotropic turbulent flows or passive scalar turbulence to that end we propose a twoparameter continuum hydrodynamic model for an advected substance concentration theta parametrised jointly by y and overline y that chara... | [['we', 'revisit', 'the', 'wellknown', 'problem', 'of', 'multiscaling', 'in', 'substances', 'passively', 'advected', 'by', 'homogeneous', 'and', 'isotropic', 'turbulent', 'flows', 'or', 'passive', 'scalar', 'turbulence', 'to', 'that', 'end', 'we', 'propose', 'a', 'twoparameter', 'continuum', 'hydrodynamic', 'model', 'f... | [-0.11446767973575334, 0.15461976027381752, -0.12763109546439308, 0.09877931035589427, -0.06006197467730898, -0.12842141643502852, 0.008825406946319466, 0.32603828819588265, -0.30798076468959656, -0.2564245337853208, 0.02005601816442019, -0.23522107779151863, -0.17659736715399454, 0.1865288471841874, -0.012313496513848... |
1,801.00999 | Unitary $n$-designs via random quenches in atomic Hubbard and Spin
models: Application to the measurement of R\'enyi entropies | We present a general framework for the generation of random unitaries based
on random quenches in atomic Hubbard and spin models, forming approximate
unitary $n$-designs, and their application to the measurement of R\'enyi
entropies. We generalize our protocol presented in [Elben2017:
arXiv:1709.05060, to appear in P... | quant-ph cond-mat.quant-gas | we present a general framework for the generation of random unitaries based on random quenches in atomic hubbard and spin models forming approximate unitary ndesigns and their application to the measurement of renyi entropies we generalize our protocol presented in elben2017 arxiv170905060 to appear in phys rev lett to... | [['we', 'present', 'a', 'general', 'framework', 'for', 'the', 'generation', 'of', 'random', 'unitaries', 'based', 'on', 'random', 'quenches', 'in', 'atomic', 'hubbard', 'and', 'spin', 'models', 'forming', 'approximate', 'unitary', 'ndesigns', 'and', 'their', 'application', 'to', 'the', 'measurement', 'of', 'renyi', 'en... | [-0.09494570948402671, 0.12710098834205008, -0.06530018981327029, -0.011886703305165558, 0.011875698540140601, -0.130418770793168, 0.10346732358448207, 0.3849786884973154, -0.19348165300839087, -0.25311665945850753, 0.021817197271294015, -0.2663164238609812, -0.18077821997268234, 0.20864593927365016, -0.062955277029644... |
1,801.01 | ViZDoom: DRQN with Prioritized Experience Replay, Double-Q Learning, &
Snapshot Ensembling | ViZDoom is a robust, first-person shooter reinforcement learning environment,
characterized by a significant degree of latent state information. In this
paper, double-Q learning and prioritized experience replay methods are tested
under a certain ViZDoom combat scenario using a competitive deep recurrent
Q-network (D... | cs.AI | vizdoom is a robust firstperson shooter reinforcement learning environment characterized by a significant degree of latent state information in this paper doubleq learning and prioritized experience replay methods are tested under a certain vizdoom combat scenario using a competitive deep recurrent qnetwork drqn archit... | [['vizdoom', 'is', 'a', 'robust', 'firstperson', 'shooter', 'reinforcement', 'learning', 'environment', 'characterized', 'by', 'a', 'significant', 'degree', 'of', 'latent', 'state', 'information', 'in', 'this', 'paper', 'doubleq', 'learning', 'and', 'prioritized', 'experience', 'replay', 'methods', 'are', 'tested', 'un... | [-0.06789248029358293, 0.04823925622660777, -0.0692813277425318, 0.08061865698607443, -0.06487628361577855, -0.19452707948359219, 0.08366767682049325, 0.45272725570554795, -0.228967045860267, -0.3203362507598573, 0.08876337151894786, -0.24474591206220028, -0.18951150240180523, 0.18209176481652417, -0.15100512364355573,... |
1,801.01001 | A Quinone Based Single-Molecule Switch as Building Block for Molecular
Electronics | Azophenine has previously been identified as a controllable molecular switch
when deposited on a Cu(110) surface, where it can be in two symmetry-equivalent
states. Each of the two states can be set as well as read by means of a
scanning tunneling microscope (STM). We propose a family of molecules based on
the same q... | physics.atm-clus physics.app-ph physics.chem-ph | azophenine has previously been identified as a controllable molecular switch when deposited on a cu110 surface where it can be in two symmetryequivalent states each of the two states can be set as well as read by means of a scanning tunneling microscope stm we propose a family of molecules based on the same quinone cor... | [['azophenine', 'has', 'previously', 'been', 'identified', 'as', 'a', 'controllable', 'molecular', 'switch', 'when', 'deposited', 'on', 'a', 'cu110', 'surface', 'where', 'it', 'can', 'be', 'in', 'two', 'symmetryequivalent', 'states', 'each', 'of', 'the', 'two', 'states', 'can', 'be', 'set', 'as', 'well', 'as', 'read', ... | [-0.11993184794035366, 0.14871339894068755, -0.09550599510720396, 0.019980640559968708, -0.03126997019347475, -0.17438138584743756, 0.06995218785930059, 0.4248139450296027, -0.2741770335152501, -0.3282017547209732, 0.05037783249090502, -0.24867996754369043, -0.1580177149296448, 0.21573195114663085, 0.003466550753161799... |
1,801.01002 | Collective motion of Active Brownian Particles with polar alignment | We present a comprehensive computational study of the collective behavior
emerging from the competition between self-propulsion, excluded volume
interactions and velocity-alignment in a two-dimensionnal model of active
particles. We consider an extension of the Active Brownian Particles model
where the self-propulsio... | cond-mat.soft | we present a comprehensive computational study of the collective behavior emerging from the competition between selfpropulsion excluded volume interactions and velocityalignment in a twodimensionnal model of active particles we consider an extension of the active brownian particles model where the selfpropulsion direct... | [['we', 'present', 'a', 'comprehensive', 'computational', 'study', 'of', 'the', 'collective', 'behavior', 'emerging', 'from', 'the', 'competition', 'between', 'selfpropulsion', 'excluded', 'volume', 'interactions', 'and', 'velocityalignment', 'in', 'a', 'twodimensionnal', 'model', 'of', 'active', 'particles', 'we', 'co... | [-0.1971337105967461, 0.22120304041752106, -0.07176484358825601, 0.04896205748249242, -0.041879861652360933, -0.1118511750238043, 0.05085872444792085, 0.3282643316901828, -0.2666407547140289, -0.31748891306336985, 0.022094833944772668, -0.26461637735591853, -0.1808698323374819, 0.09050919973618979, 0.012133127868255716... |
1,801.01003 | An Information Analysis on Modeling Interaction Effects in Logistic
Regression | The Akaike information criterion (AIC) is commonly used to select a logistic
regression model for optimal prediction of a binary response by a specified
family of models. It however lacks a convincing method of prescribing a proper
family of models using the desired predictors and their interaction effects.
For an al... | stat.ME | the akaike information criterion aic is commonly used to select a logistic regression model for optimal prediction of a binary response by a specified family of models it however lacks a convincing method of prescribing a proper family of models using the desired predictors and their interaction effects for an alternat... | [['the', 'akaike', 'information', 'criterion', 'aic', 'is', 'commonly', 'used', 'to', 'select', 'a', 'logistic', 'regression', 'model', 'for', 'optimal', 'prediction', 'of', 'a', 'binary', 'response', 'by', 'a', 'specified', 'family', 'of', 'models', 'it', 'however', 'lacks', 'a', 'convincing', 'method', 'of', 'prescri... | [-0.05041883845579313, -0.015836599279260063, -0.11297105588276007, 0.13693029651321195, -0.10256606528101249, -0.20777792946944024, 0.10514306546720259, 0.35977039822560103, -0.26296535186666675, -0.2966202145579494, 0.09316528450977629, -0.264679693251254, -0.19077042785638865, 0.1714995620340863, -0.0417170504599444... |
1,801.01004 | Structures and magnetic properties of iron silicide from adaptive
genetic algorithm and first-principles calculations | We performed a systematic search for low-energy structures of binary iron
silicide over a wide range of compositions using the crystal structure
prediction method based on adaptive genetic algorithm. 36 structures with
formation energies within 50 meV/atom (11 of them are within 20 meV) above the
convex hull formed b... | cond-mat.mes-hall cond-mat.mtrl-sci | we performed a systematic search for lowenergy structures of binary iron silicide over a wide range of compositions using the crystal structure prediction method based on adaptive genetic algorithm 36 structures with formation energies within 50 mevatom 11 of them are within 20 mev above the convex hull formed by exper... | [['we', 'performed', 'a', 'systematic', 'search', 'for', 'lowenergy', 'structures', 'of', 'binary', 'iron', 'silicide', 'over', 'a', 'wide', 'range', 'of', 'compositions', 'using', 'the', 'crystal', 'structure', 'prediction', 'method', 'based', 'on', 'adaptive', 'genetic', 'algorithm', '36', 'structures', 'with', 'form... | [-0.11315191255294178, 0.17118437338228287, -0.004376895544976976, 0.07608349603144329, -0.031069105826885022, -0.0928533001263675, 0.07175244148943181, 0.47249873609919296, -0.2690142173202108, -0.3904177894521701, 0.057765378806691026, -0.2402871345954114, -0.11836826143247124, 0.2301924194938405, 0.0830276957284169,... |
1,801.01005 | An interacting galaxy pair at the origin of a light echo | In a low-density region of the Shapley supercluster we identified an
interacting galaxy pair at redshift z=0.04865 in which the Seyfert-2 nucleus of
the main galaxy (ShaSS 073) is exciting an extended emission line region (EELR,
~170 kpc^2) in the disk of the less massive companion (ShaSS 622). New
integral-field spe... | astro-ph.GA | in a lowdensity region of the shapley supercluster we identified an interacting galaxy pair at redshift z004865 in which the seyfert2 nucleus of the main galaxy shass 073 is exciting an extended emission line region eelr 170 kpc2 in the disk of the less massive companion shass 622 new integralfield spectroscopy and the... | [['in', 'a', 'lowdensity', 'region', 'of', 'the', 'shapley', 'supercluster', 'we', 'identified', 'an', 'interacting', 'galaxy', 'pair', 'at', 'redshift', 'z004865', 'in', 'which', 'the', 'seyfert2', 'nucleus', 'of', 'the', 'main', 'galaxy', 'shass', '073', 'is', 'exciting', 'an', 'extended', 'emission', 'line', 'region... | [-0.09730737216304988, 0.059725809125811796, -0.07631738800508901, 0.09141710179392248, -0.05430017465073615, -0.07871145734004677, 0.06389482348505407, 0.43308287505060433, -0.1472437015118776, -0.3052150968444767, 0.04052667170669883, -0.27817421447485685, -0.023856973154470325, 0.1906103361621499, 0.0024917915632249... |
1,801.01006 | The risk model with stochastic premiums, dependence and a threshold
dividend strategy | The paper deals with a generalization of the risk model with stochastic
premiums where dependence structures between claim sizes and inter-claim times
as well as premium sizes and inter-premium times are modeled by
Farlie--Gumbel--Morgenstern copulas. In addition, dividends are paid to its
shareholders according to a... | math.PR | the paper deals with a generalization of the risk model with stochastic premiums where dependence structures between claim sizes and interclaim times as well as premium sizes and interpremium times are modeled by farliegumbelmorgenstern copulas in addition dividends are paid to its shareholders according to a threshold... | [['the', 'paper', 'deals', 'with', 'a', 'generalization', 'of', 'the', 'risk', 'model', 'with', 'stochastic', 'premiums', 'where', 'dependence', 'structures', 'between', 'claim', 'sizes', 'and', 'interclaim', 'times', 'as', 'well', 'as', 'premium', 'sizes', 'and', 'interpremium', 'times', 'are', 'modeled', 'by', 'farli... | [-0.05246855647888996, 0.05742661715034516, -0.04698213889083314, 0.15405534967900283, -0.07449824536865156, -0.12636004453299626, 0.14345150438772003, 0.4141193725348961, -0.24721775919334182, -0.26293184622866855, 0.19163497925206507, -0.310971160392998, -0.10886229479858171, 0.1339727063595708, -0.12018917017790486,... |
1,801.01007 | A Comprehensive Bayesian Treatment of the Universal Kriging model with
Mat\'ern correlation kernels | The Gibbs reference posterior distribution provides an objective
full-Bayesian solution to the problem of prediction of a stationary Gaussian
process with Mat\'ern anisotropic kernel. A full-Bayesian approach is possible,
because the posterior distribution is expressed as the invariant distribution
of a uniformly erg... | math.ST stat.TH | the gibbs reference posterior distribution provides an objective fullbayesian solution to the problem of prediction of a stationary gaussian process with matern anisotropic kernel a fullbayesian approach is possible because the posterior distribution is expressed as the invariant distribution of a uniformly ergodic mar... | [['the', 'gibbs', 'reference', 'posterior', 'distribution', 'provides', 'an', 'objective', 'fullbayesian', 'solution', 'to', 'the', 'problem', 'of', 'prediction', 'of', 'a', 'stationary', 'gaussian', 'process', 'with', 'matern', 'anisotropic', 'kernel', 'a', 'fullbayesian', 'approach', 'is', 'possible', 'because', 'the... | [-0.04484901971802229, 0.041052251246749806, -0.1506128966886522, 0.12388753696653716, -0.054227669959717235, -0.10768162990913137, 0.06027743610720513, 0.4219047640030848, -0.2678927557137688, -0.24221587423164084, 0.08161365102358048, -0.21093693365278932, -0.14912704544724853, 0.18405732522071658, -0.090517238459642... |
1,801.01008 | Structural and Chemical Orders in Ni64.5Zr35.5 Metallic Glass by
Molecular Dynamics Simulation | The atomic structure of Ni64.5Zr35.5 metallic glass has been investigated by
molecular dynamics (MD) simulations. The calculated structure factors from the
MD glassy sample at room temperature agree well with the X-ray diffraction
(XRD) and neutron diffraction (ND) experimental data. Using the pairwise
cluster alignm... | cond-mat.mes-hall cond-mat.mtrl-sci | the atomic structure of ni645zr355 metallic glass has been investigated by molecular dynamics md simulations the calculated structure factors from the md glassy sample at room temperature agree well with the xray diffraction xrd and neutron diffraction nd experimental data using the pairwise cluster alignment and cliqu... | [['the', 'atomic', 'structure', 'of', 'ni645zr355', 'metallic', 'glass', 'has', 'been', 'investigated', 'by', 'molecular', 'dynamics', 'md', 'simulations', 'the', 'calculated', 'structure', 'factors', 'from', 'the', 'md', 'glassy', 'sample', 'at', 'room', 'temperature', 'agree', 'well', 'with', 'the', 'xray', 'diffract... | [-0.07519294989354436, 0.15460725311589027, -0.09370339842557553, 0.021241418906443175, 0.021765701230689292, -0.07423535185969538, 0.07055005861357563, 0.4279867098149326, -0.24391479357071813, -0.30069448169882573, 0.02751217610184251, -0.3544991813149185, -0.13687837437545466, 0.10193544993406191, 0.1054215043799818... |
1,801.01009 | Origin and Control of Polyacrylonitrile Alignments on Carbon Nanotube
and Graphene Nanoribbon | While one of the most promising applications of carbon nanotubes (CNTs) is to
enhance polymer orientation and crystallization to achieve advanced carbon
fibers, the successful realization of this goal has been hindered by the
insufficient atomistic understanding of polymer-CNT interfaces. We herein
theoretically stud... | cond-mat.mtrl-sci | while one of the most promising applications of carbon nanotubes cnts is to enhance polymer orientation and crystallization to achieve advanced carbon fibers the successful realization of this goal has been hindered by the insufficient atomistic understanding of polymercnt interfaces we herein theoretically study polya... | [['while', 'one', 'of', 'the', 'most', 'promising', 'applications', 'of', 'carbon', 'nanotubes', 'cnts', 'is', 'to', 'enhance', 'polymer', 'orientation', 'and', 'crystallization', 'to', 'achieve', 'advanced', 'carbon', 'fibers', 'the', 'successful', 'realization', 'of', 'this', 'goal', 'has', 'been', 'hindered', 'by', ... | [-0.12723414990668014, 0.09829935770248995, -0.04038095735871282, 0.031729235090345975, -0.038776572357471055, -0.12262767534703016, 0.026485345521819238, 0.4410924798858009, -0.23816799754093057, -0.2998989702634342, 0.054414432310486996, -0.24119488237407302, -0.1787650599285323, 0.17268973537598198, -0.0017227503152... |
1,801.0101 | Ion-exchange synthesis and superconductivity at 8.6 K of Na2Cr3As3 with
quasi-one-dimensional crystal structure | A new Cr-based quasi-one-dimensional superconductor Na2Cr3As3 was synthesized
by an ion-exchange method in sodium naphthalenide solution. The crystals are
thread-like and the structure was analyzed by X-ray diffraction with a
noncentrosymmetric hexagonal space group P-6m2 (No. 187), in which the
(Cr3As3)2- linear cha... | cond-mat.supr-con cond-mat.mtrl-sci cond-mat.str-el | a new crbased quasionedimensional superconductor na2cr3as3 was synthesized by an ionexchange method in sodium naphthalenide solution the crystals are threadlike and the structure was analyzed by xray diffraction with a noncentrosymmetric hexagonal space group p6m2 no 187 in which the cr3as32 linear chains are separated... | [['a', 'new', 'crbased', 'quasionedimensional', 'superconductor', 'na2cr3as3', 'was', 'synthesized', 'by', 'an', 'ionexchange', 'method', 'in', 'sodium', 'naphthalenide', 'solution', 'the', 'crystals', 'are', 'threadlike', 'and', 'the', 'structure', 'was', 'analyzed', 'by', 'xray', 'diffraction', 'with', 'a', 'noncentr... | [-0.1663758106152998, 0.23388290390378164, 0.023928622385549745, -0.03722905342498522, -0.040690368161735574, -0.20668991778590037, 0.11529116868303063, 0.4173432587949413, -0.20820580710646477, -0.2726956641699156, 0.028501486371721278, -0.3858669458710578, -0.07180700750676182, 0.18807548183026943, 0.095293894117133,... |
1,801.01011 | Connections between a system of Forward-Backward SDEs and Backward
Stochastic PDEs related to the utility maximization problem | Connections between a system of Forward-Backward SDEs and Backward Stochastic
PDEs related to the utility maximiza- tion problem is established. Besides, we
derive another version of FBSDE of the same problem and prove an existence of a
solution
| math.PR | connections between a system of forwardbackward sdes and backward stochastic pdes related to the utility maximiza tion problem is established besides we derive another version of fbsde of the same problem and prove an existence of a solution | [['connections', 'between', 'a', 'system', 'of', 'forwardbackward', 'sdes', 'and', 'backward', 'stochastic', 'pdes', 'related', 'to', 'the', 'utility', 'maximiza', 'tion', 'problem', 'is', 'established', 'besides', 'we', 'derive', 'another', 'version', 'of', 'fbsde', 'of', 'the', 'same', 'problem', 'and', 'prove', 'an'... | [-0.1890203253793958, -0.05690353834093863, -0.09664286038762815, 0.12758457873683623, -0.10170150296510877, -0.15643676518890504, 0.03547903985993282, 0.2720552266550225, -0.4060901128498183, -0.23095658602746758, 0.14319892780150514, -0.29759428227269974, -0.15789622612096169, 0.19274052781858356, -0.1179947898899381... |
1,801.01012 | Graph Pattern Matching for Dynamic Team Formation | Finding a list of k teams of experts, referred to as top-k team formation,
with the required skills and high collaboration compatibility has been
extensively studied. However, existing methods have not considered the specific
collaboration relationships among different team members, i.e., structural
constraints, whic... | cs.DB | finding a list of k teams of experts referred to as topk team formation with the required skills and high collaboration compatibility has been extensively studied however existing methods have not considered the specific collaboration relationships among different team members ie structural constraints which are typica... | [['finding', 'a', 'list', 'of', 'k', 'teams', 'of', 'experts', 'referred', 'to', 'as', 'topk', 'team', 'formation', 'with', 'the', 'required', 'skills', 'and', 'high', 'collaboration', 'compatibility', 'has', 'been', 'extensively', 'studied', 'however', 'existing', 'methods', 'have', 'not', 'considered', 'the', 'specif... | [-0.09189028016291559, 0.003550303539086599, -0.07444241311090688, 0.04795541345297048, -0.16181130633999904, -0.11991505997876327, 0.09840954537813862, 0.4458200037617159, -0.2579100584642341, -0.423505387318631, 0.11039278431252265, -0.24648397548124193, -0.17406144126163176, 0.1015929114073515, -0.0716660719869348, ... |
1,801.01013 | Instrumental variables estimation with competing risk data | Time-to-event analyses are often plagued by both -- possibly unmeasured --
confounding and competing risks. To deal with the former, the use of
instrumental variables for effect estimation is rapidly gaining ground. We show
how to make use of such variables in competing risk analyses. In particular, we
show how to in... | stat.ME | timetoevent analyses are often plagued by both possibly unmeasured confounding and competing risks to deal with the former the use of instrumental variables for effect estimation is rapidly gaining ground we show how to make use of such variables in competing risk analyses in particular we show how to infer the effect ... | [['timetoevent', 'analyses', 'are', 'often', 'plagued', 'by', 'both', 'possibly', 'unmeasured', 'confounding', 'and', 'competing', 'risks', 'to', 'deal', 'with', 'the', 'former', 'the', 'use', 'of', 'instrumental', 'variables', 'for', 'effect', 'estimation', 'is', 'rapidly', 'gaining', 'ground', 'we', 'show', 'how', 't... | [-0.04738196375503212, 0.054177035933187144, -0.08895815669075775, 0.14384972978964505, -0.10698637852263182, -0.1269607085916669, 0.07991280263864008, 0.41048302315525653, -0.21099482571419076, -0.28732973779726745, 0.12317921413822953, -0.28114845014800477, -0.15699922814755177, 0.21185433199888276, -0.13786003560430... |
1,801.01014 | Finite asymptotic clusters of metric spaces | Let $(X, d)$ be an unbounded metric space and let $\tilde
r=(r_n)_{n\in\mathbb N}$ be a sequence of positive real numbers tending to
infinity. A pretangent space $\Omega_{\infty, \tilde r}^{X}$ to $(X, d)$ at
infinity is a limit of the rescaling sequence $\left(X, \frac{1}{r_n}d\right).$
The set of all pretangent spa... | math.MG | let x d be an unbounded metric space and let tilde rr_n_ninmathbb n be a sequence of positive real numbers tending to infinity a pretangent space omega_infty tilde rx to x d at infinity is a limit of the rescaling sequence leftx frac1r_ndright the set of all pretangent spaces omega_infty tilde rx is called an asymptoti... | [['let', 'x', 'd', 'be', 'an', 'unbounded', 'metric', 'space', 'and', 'let', 'tilde', 'rr_n_ninmathbb', 'n', 'be', 'a', 'sequence', 'of', 'positive', 'real', 'numbers', 'tending', 'to', 'infinity', 'a', 'pretangent', 'space', 'omega_infty', 'tilde', 'rx', 'to', 'x', 'd', 'at', 'infinity', 'is', 'a', 'limit', 'of', 'the... | [-0.20571326040583898, 0.14525053435290367, -0.09234288003753428, 0.06204913509763004, -0.08822108456722887, -0.16859868445465245, 0.02234699608170096, 0.3654363835072618, -0.3117348815046124, -0.16986973264838678, 0.12148369937914155, -0.3340625132323574, -0.06725425173931013, 0.1279166295366772, -0.07688915231501904,... |
1,801.01015 | An accurate centroid algorithm for PSF reconstruction | In this work, we present a novel centroiding method based on Fourier space
Phase Fitting(FPF) for Point Spread Function(PSF) reconstruction. We generate
two sets of simulations to test our method. The first set is generated by
GalSim with elliptical Moffat profile and strong anisotropy which shifts the
center of the ... | astro-ph.IM | in this work we present a novel centroiding method based on fourier space phase fittingfpf for point spread functionpsf reconstruction we generate two sets of simulations to test our method the first set is generated by galsim with elliptical moffat profile and strong anisotropy which shifts the center of the psf the s... | [['in', 'this', 'work', 'we', 'present', 'a', 'novel', 'centroiding', 'method', 'based', 'on', 'fourier', 'space', 'phase', 'fittingfpf', 'for', 'point', 'spread', 'functionpsf', 'reconstruction', 'we', 'generate', 'two', 'sets', 'of', 'simulations', 'to', 'test', 'our', 'method', 'the', 'first', 'set', 'is', 'generate... | [-0.014207444508972857, 0.03849220104616366, -0.10958585801976013, 0.06295689870363351, -0.0877763396501061, -0.09261696422280571, 0.026217039933154534, 0.4399336373635097, -0.23256153071097568, -0.3698779314050701, 0.06362770547245428, -0.3183642790734422, -0.11767535737071176, 0.22731337900160686, -0.0453064456034797... |
1,801.01016 | Double barrier reflected BSDEs with stochastic Lipschitz coefficient | This paper proves the existence and uniqueness of a solution to doubly
reflected backward stochastic differential equations where the coefficient is
stochastic Lipschitz, by means of the penalization method.
| math.PR | this paper proves the existence and uniqueness of a solution to doubly reflected backward stochastic differential equations where the coefficient is stochastic lipschitz by means of the penalization method | [['this', 'paper', 'proves', 'the', 'existence', 'and', 'uniqueness', 'of', 'a', 'solution', 'to', 'doubly', 'reflected', 'backward', 'stochastic', 'differential', 'equations', 'where', 'the', 'coefficient', 'is', 'stochastic', 'lipschitz', 'by', 'means', 'of', 'the', 'penalization', 'method']] | [-0.1361453160934616, -0.005573949310928583, -0.07565496701361804, 0.05211354294342214, -0.12669139360238252, -0.1255246642174135, 0.009871720629423085, 0.24738765784121794, -0.4463391599470171, -0.19595635309815407, 0.14282952846381172, -0.29495975002646446, -0.17654748723424715, 0.13539538404037213, -0.09022309537976... |
1,801.01017 | Particle Clustering Machine: A Dynamical System Based Approach | Identification of the clusters from an unlabeled data set is one of the most
important problems in Unsupervised Machine Learning. The state of the art
clustering algorithms are based on either the statistical properties or the
geometric properties of the data set. In this work, we propose a novel method
to cluster th... | cs.LG math.OC | identification of the clusters from an unlabeled data set is one of the most important problems in unsupervised machine learning the state of the art clustering algorithms are based on either the statistical properties or the geometric properties of the data set in this work we propose a novel method to cluster the dat... | [['identification', 'of', 'the', 'clusters', 'from', 'an', 'unlabeled', 'data', 'set', 'is', 'one', 'of', 'the', 'most', 'important', 'problems', 'in', 'unsupervised', 'machine', 'learning', 'the', 'state', 'of', 'the', 'art', 'clustering', 'algorithms', 'are', 'based', 'on', 'either', 'the', 'statistical', 'properties... | [-0.08835570983743916, 0.019195517268912977, -0.1334349582662228, 0.027377374854939723, -0.07160385429120526, -0.10547033827096203, 0.038758891106759806, 0.36328163827587473, -0.2911188485697661, -0.3245888380654927, 0.12483370960047789, -0.28111670383027404, -0.13961794905648192, 0.21035645482124996, -0.06330391603532... |
1,801.01018 | Pierre Auger Observatory and Telescope Array: Joint Contributions to the
35th International Cosmic Ray Conference (ICRC 2017) | Joint contributions of the Telescope Array Collaboration and the Pierre Auger
Collaboration to the 35th International Cosmic Ray Conference (ICRC 2017),
12-20 July 2017, Bexco, Busan, Korea.
| astro-ph.HE astro-ph.CO astro-ph.IM | joint contributions of the telescope array collaboration and the pierre auger collaboration to the 35th international cosmic ray conference icrc 2017 1220 july 2017 bexco busan korea | [['joint', 'contributions', 'of', 'the', 'telescope', 'array', 'collaboration', 'and', 'the', 'pierre', 'auger', 'collaboration', 'to', 'the', '35th', 'international', 'cosmic', 'ray', 'conference', 'icrc', '2017', '1220', 'july', '2017', 'bexco', 'busan', 'korea']] | [-0.07578055555414823, 0.2625836564434899, -0.02526791483439781, 0.10798053471026597, -0.16480087192246207, 0.09180352657481476, -0.058593852928391206, 0.2588379714913942, -0.06393709640811991, -0.5744622523585955, 0.05852150330664935, -0.5494755267820977, -0.14120561229409995, 0.21615631381670633, 0.014456753446548074... |
1,801.01019 | Proteomics Analysis of FLT3-ITD Mutation in Acute Myeloid Leukemia Using
Deep Learning Neural Network | Deep Learning can significantly benefit cancer proteomics and genomics. In
this study, we attempt to determine a set of critical proteins that are
associated with the FLT3-ITD mutation in newly-diagnosed acute myeloid leukemia
patients. A Deep Learning network consisting of autoencoders forming a
hierarchical model f... | q-bio.QM cs.LG stat.ML | deep learning can significantly benefit cancer proteomics and genomics in this study we attempt to determine a set of critical proteins that are associated with the flt3itd mutation in newlydiagnosed acute myeloid leukemia patients a deep learning network consisting of autoencoders forming a hierarchical model from whi... | [['deep', 'learning', 'can', 'significantly', 'benefit', 'cancer', 'proteomics', 'and', 'genomics', 'in', 'this', 'study', 'we', 'attempt', 'to', 'determine', 'a', 'set', 'of', 'critical', 'proteins', 'that', 'are', 'associated', 'with', 'the', 'flt3itd', 'mutation', 'in', 'newlydiagnosed', 'acute', 'myeloid', 'leukemi... | [-0.018103388248668084, 0.04363182194303996, 0.003448755527250201, 0.0897678957578706, -0.03566484308044473, -0.18024564795062054, 0.09800483964269699, 0.38405402351787193, -0.24290826138617344, -0.32683578012980147, 0.01905276446700391, -0.30439030451418686, -0.23140325155712183, 0.17445383908012682, -0.09921447604412... |
1,801.0102 | Top Quark Pair Production: theory overview | In this talk we present the current status of the theoretical description of
the production of top-quark pairs at the LHC, detailing recent progress for
predictions at the stable-top level as well as for predictions that include the
decay of the top quarks.
| hep-ph hep-ex | in this talk we present the current status of the theoretical description of the production of topquark pairs at the lhc detailing recent progress for predictions at the stabletop level as well as for predictions that include the decay of the top quarks | [['in', 'this', 'talk', 'we', 'present', 'the', 'current', 'status', 'of', 'the', 'theoretical', 'description', 'of', 'the', 'production', 'of', 'topquark', 'pairs', 'at', 'the', 'lhc', 'detailing', 'recent', 'progress', 'for', 'predictions', 'at', 'the', 'stabletop', 'level', 'as', 'well', 'as', 'for', 'predictions', ... | [-0.01247961534785905, 0.16092453921391142, -0.04731303391357263, 0.07906042845154714, -0.018632675166286174, -0.06188104683089824, 0.05412721759750552, 0.2890437949626219, -0.18119277841677622, -0.29655084058287595, 0.06324531308962919, -0.3306950953389917, -0.006624698505869934, 0.174839966098911, 0.05596121844081651... |
1,801.01021 | The Unified Astronomy Thesaurus: Semantic Metadata for Astronomy and
Astrophysics | Several different controlled vocabularies have been developed and used by the
astronomical community, each designed to serve a specific need and a specific
group. The Unified Astronomy Thesaurus (UAT) attempts to provide a highly
structured controlled vocabulary that will be relevant and useful across the
entire disc... | astro-ph.IM cs.DL | several different controlled vocabularies have been developed and used by the astronomical community each designed to serve a specific need and a specific group the unified astronomy thesaurus uat attempts to provide a highly structured controlled vocabulary that will be relevant and useful across the entire discipline... | [['several', 'different', 'controlled', 'vocabularies', 'have', 'been', 'developed', 'and', 'used', 'by', 'the', 'astronomical', 'community', 'each', 'designed', 'to', 'serve', 'a', 'specific', 'need', 'and', 'a', 'specific', 'group', 'the', 'unified', 'astronomy', 'thesaurus', 'uat', 'attempts', 'to', 'provide', 'a', ... | [-0.01212774933471034, 0.06285202329357466, -0.04782411028993212, 0.09857563083577488, -0.15438896618369552, -0.1452295986780276, 0.05012166416272521, 0.3985322075585524, -0.2303897993483891, -0.373182924464345, 0.134292257813892, -0.2436733726463798, -0.11997758652238796, 0.24592744264906893, -0.05651183452250229, 0.0... |
1,801.01022 | Shannon Capacity is Achievable for Binary Interactive First-Order
Markovian Protocols | We address the problem of simulating an arbitrary binary interactive
first-order Markovian protocol over a pair of binary symmetric channels with
crossover probability $\varepsilon$. We are interested in the achievable rates
of reliable simulation, i.e., in characterizing the smallest possible blowup in
communication... | cs.IT math.IT | we address the problem of simulating an arbitrary binary interactive firstorder markovian protocol over a pair of binary symmetric channels with crossover probability varepsilon we are interested in the achievable rates of reliable simulation ie in characterizing the smallest possible blowup in communications such that... | [['we', 'address', 'the', 'problem', 'of', 'simulating', 'an', 'arbitrary', 'binary', 'interactive', 'firstorder', 'markovian', 'protocol', 'over', 'a', 'pair', 'of', 'binary', 'symmetric', 'channels', 'with', 'crossover', 'probability', 'varepsilon', 'we', 'are', 'interested', 'in', 'the', 'achievable', 'rates', 'of',... | [-0.177677417843483, 0.10315665356858573, -0.06343113502273735, 0.04613877787976797, -0.019704380127010642, -0.2165891527096788, 0.1139577144638233, 0.3647792931385193, -0.2781131793926053, -0.26170584161182436, 0.09789991843267724, -0.2060238424333443, -0.12520587288843402, 0.2053015033699978, -0.09595096247145682, 0.... |
1,801.01023 | Calder\'on-Zygmund operators on Zygmund spaces on domains | Given a bounded Lipschitz domain $D\subset \mathbb{R}^d$ and a
Calder\'on-Zygmund operator $T$, we study the relations between smoothness
properties of $\partial D$ and the boundedness of $T$ on the Zydmund space
$\mathcal{C}_{\omega}(D)$ defined for a general growth function $\omega$. In
the proof we obtain a T(P) t... | math.FA | given a bounded lipschitz domain dsubset mathbbrd and a calderonzygmund operator t we study the relations between smoothness properties of partial d and the boundedness of t on the zydmund space mathcalc_omegad defined for a general growth function omega in the proof we obtain a tp theorem for the zygmund spaces when o... | [['given', 'a', 'bounded', 'lipschitz', 'domain', 'dsubset', 'mathbbrd', 'and', 'a', 'calderonzygmund', 'operator', 't', 'we', 'study', 'the', 'relations', 'between', 'smoothness', 'properties', 'of', 'partial', 'd', 'and', 'the', 'boundedness', 'of', 't', 'on', 'the', 'zydmund', 'space', 'mathcalc_omegad', 'defined', ... | [-0.16798424737432718, 0.0799733755305748, -0.07646096906286072, 0.10120482398964338, -0.14078545210808938, -0.11046612642663108, 0.05444168224295771, 0.30113945821490645, -0.3428370230407877, -0.1502422140434977, 0.15364808758816004, -0.24876390066294168, -0.0919586565797462, 0.182821785373645, -0.09888467511204495, 0... |
1,801.01024 | Relativistic quantum motion of spin-0 particles under the influence of
non-inertial effects in the cosmic string space-time | We study solutions for the Klein-Gordon equation with vector and scalar
potentials of the Coulomb types under the influence of non-inertial effects in
the space-time of topological defects. We also investigate a quantum particle
described by the Klein-Gordon oscillator in the background space-time generated
by a stri... | hep-th | we study solutions for the kleingordon equation with vector and scalar potentials of the coulomb types under the influence of noninertial effects in the spacetime of topological defects we also investigate a quantum particle described by the kleingordon oscillator in the background spacetime generated by a string an im... | [['we', 'study', 'solutions', 'for', 'the', 'kleingordon', 'equation', 'with', 'vector', 'and', 'scalar', 'potentials', 'of', 'the', 'coulomb', 'types', 'under', 'the', 'influence', 'of', 'noninertial', 'effects', 'in', 'the', 'spacetime', 'of', 'topological', 'defects', 'we', 'also', 'investigate', 'a', 'quantum', 'pa... | [-0.14469663089571091, 0.190775221261192, -0.08530652745125386, 0.08380307738188204, -0.03259819778255545, -0.1140357284489405, -0.03977711465219957, 0.2892678004003816, -0.22177888229898698, -0.2536597900747598, 0.011381461540912534, -0.28173871934004535, -0.1753501400535742, 0.15918086679744442, -0.005167601080317111... |
1,801.01025 | A Study of Bug Resolution Characteristics in Popular Programming
Languages | This paper presents a large-scale study that investigates the bug resolution
characteristics among popular Github projects written in different programming
languages. We explore correlations but, of course, we cannot infer causation.
Specifically, we analyse bug resolution data from approximately 70 million
Source Li... | cs.SE | this paper presents a largescale study that investigates the bug resolution characteristics among popular github projects written in different programming languages we explore correlations but of course we cannot infer causation specifically we analyse bug resolution data from approximately 70 million source line of co... | [['this', 'paper', 'presents', 'a', 'largescale', 'study', 'that', 'investigates', 'the', 'bug', 'resolution', 'characteristics', 'among', 'popular', 'github', 'projects', 'written', 'in', 'different', 'programming', 'languages', 'we', 'explore', 'correlations', 'but', 'of', 'course', 'we', 'can', 'not', 'infer', 'caus... | [-0.0990858868820942, 0.02216520378133282, -0.07541204199194908, 0.11770112739584875, -0.1282278285943903, -0.16524087727768347, 0.09517294444289291, 0.44323098219931123, -0.25617278889287265, -0.38192078911699356, 0.11704169543343595, -0.3107886514085112, -0.052998785816598684, 0.2033864611131139, -0.08805549350567161... |
1,801.01026 | A remark on the Sibony function | We present an effective formula for the Sibony function for all Reinhardt
domains.
| math.CV | we present an effective formula for the sibony function for all reinhardt domains | [['we', 'present', 'an', 'effective', 'formula', 'for', 'the', 'sibony', 'function', 'for', 'all', 'reinhardt', 'domains']] | [-0.1442488464885033, -0.0058476070486134495, -0.07234254364783947, 0.12290501902596308, -0.09595108214909068, -0.052313995762513235, 0.028840368524050482, 0.3707710693661983, -0.189582121773408, -0.219431666800609, 0.11233553326187226, -0.265736900556546, -0.20438913585474858, 0.27352137634387386, -0.095422552468685, ... |
1,801.01027 | Optimal density for values of generic polynomial maps | We establish that the optimal bound for the size of the smallest integral
solution of the Oppenheim Diophantine approximation problem $\abs{Q(x)-\xi}<
\epsilon$ for a generic ternary form $Q$ is $\abs{x}\ll \epsilon^{-1}$. We also
establish an optimal rate of density for the values of polynomials maps in a
number of ... | math.NT | we establish that the optimal bound for the size of the smallest integral solution of the oppenheim diophantine approximation problem absqxxi epsilon for a generic ternary form q is absxll epsilon1 we also establish an optimal rate of density for the values of polynomials maps in a number of other natural problems incl... | [['we', 'establish', 'that', 'the', 'optimal', 'bound', 'for', 'the', 'size', 'of', 'the', 'smallest', 'integral', 'solution', 'of', 'the', 'oppenheim', 'diophantine', 'approximation', 'problem', 'absqxxi', 'epsilon', 'for', 'a', 'generic', 'ternary', 'form', 'q', 'is', 'absxll', 'epsilon1', 'we', 'also', 'establish', ... | [-0.18945087467519833, 0.0643466289036691, -0.07306337662739679, 0.06322015831704318, -0.0792969394791206, -0.10944142189109698, 0.0480109955649823, 0.3121087558600785, -0.2972356492986104, -0.2537144006379614, 0.11844893908128143, -0.21189159118470602, -0.14977292884141208, 0.2340227710997819, -0.08391497263302361, 0.... |
1,801.01028 | Existence of $C^\alpha$ solutions to integro-PDEs | This paper is concerned with existence of a $C^{\alpha}$ viscosity solution
of a second order non-translation invariant integro-PDE. We first obtain a weak
Harnack inequality for such integro-PDE. We then use the weak Harnack
inequality to prove H\"older regularity and existence of solutions of the
integro-PDEs.
| math.AP | this paper is concerned with existence of a calpha viscosity solution of a second order nontranslation invariant integropde we first obtain a weak harnack inequality for such integropde we then use the weak harnack inequality to prove holder regularity and existence of solutions of the integropdes | [['this', 'paper', 'is', 'concerned', 'with', 'existence', 'of', 'a', 'calpha', 'viscosity', 'solution', 'of', 'a', 'second', 'order', 'nontranslation', 'invariant', 'integropde', 'we', 'first', 'obtain', 'a', 'weak', 'harnack', 'inequality', 'for', 'such', 'integropde', 'we', 'then', 'use', 'the', 'weak', 'harnack', '... | [-0.1872119133106687, 0.0005931407001546838, -0.08823723595758731, 0.09461174090392888, -0.10551545172083107, -0.17361941274297846, -0.014933865980393339, 0.25603186353956436, -0.3605150736191056, -0.17400662795725194, 0.19507967454211955, -0.2939526478505947, -0.09415014308284629, 0.15257084572857077, -0.0908061644083... |
1,801.01029 | Bulk viscous embedded hybrid dark energy models | In this paper, we have constructed the cosmological model of the universe in
a two fluids environment with a newly developed mathematical formalism. In
order to construct the model Binachi type V (BV) space time is considered with
a time varying deceleration parameter. Both the fluids, the viscous fluid and
the dark ... | gr-qc | in this paper we have constructed the cosmological model of the universe in a two fluids environment with a newly developed mathematical formalism in order to construct the model binachi type v bv space time is considered with a time varying deceleration parameter both the fluids the viscous fluid and the dark energy d... | [['in', 'this', 'paper', 'we', 'have', 'constructed', 'the', 'cosmological', 'model', 'of', 'the', 'universe', 'in', 'a', 'two', 'fluids', 'environment', 'with', 'a', 'newly', 'developed', 'mathematical', 'formalism', 'in', 'order', 'to', 'construct', 'the', 'model', 'binachi', 'type', 'v', 'bv', 'space', 'time', 'is',... | [-0.10899669395572781, 0.12860327238925326, -0.13749386005195408, 0.06035866066534728, -0.06074255353502247, -0.0838596905634122, -0.024527541774121756, 0.30193526602783044, -0.25036072085650873, -0.3459547036458594, 0.06143994413604829, -0.20344461509826736, -0.0896218805459105, 0.1449122051446056, 0.03942694432453849... |
1,801.0103 | Dissipative measure valued solutions for general conservation laws | In the last years measure-valued solutions started to be considered as a
relevant notion of solutions if they satisfy the so-called measure-valued --
strong uniqueness principle. This means that they coincide with a strong
solution emanating from the same initial data if this strong solution exists.
This property has... | math.AP | in the last years measurevalued solutions started to be considered as a relevant notion of solutions if they satisfy the socalled measurevalued strong uniqueness principle this means that they coincide with a strong solution emanating from the same initial data if this strong solution exists this property has been exam... | [['in', 'the', 'last', 'years', 'measurevalued', 'solutions', 'started', 'to', 'be', 'considered', 'as', 'a', 'relevant', 'notion', 'of', 'solutions', 'if', 'they', 'satisfy', 'the', 'socalled', 'measurevalued', 'strong', 'uniqueness', 'principle', 'this', 'means', 'that', 'they', 'coincide', 'with', 'a', 'strong', 'so... | [-0.12666195217870183, 0.04560410420996167, -0.08316730013898303, 0.0884076602965398, -0.07925135609243185, -0.17165371100793803, -0.041243554543583624, 0.2777178007283158, -0.2699044062474352, -0.24857923821846564, 0.1676603204715291, -0.26940508528740237, -0.13198817604702087, 0.22125223900882468, -0.0748986902481485... |
1,801.01031 | On local stabilities of $p$-K\"ahler structures | By use of a natural extension map and a power series method, we obtain a
local stability theorem for p-K\"ahler structures with the $(p,p+1)$-th mild
$\partial\bar\partial$-lemma under small differentiable deformations.
| math.CV math.DG | by use of a natural extension map and a power series method we obtain a local stability theorem for pkahler structures with the pp1th mild partialbarpartiallemma under small differentiable deformations | [['by', 'use', 'of', 'a', 'natural', 'extension', 'map', 'and', 'a', 'power', 'series', 'method', 'we', 'obtain', 'a', 'local', 'stability', 'theorem', 'for', 'pkahler', 'structures', 'with', 'the', 'pp1th', 'mild', 'partialbarpartiallemma', 'under', 'small', 'differentiable', 'deformations']] | [-0.1398397285876603, -0.017020417666383857, -0.14118482692745224, 0.09269061588264745, -0.07025960550226014, -0.1127524580645921, 0.017790984635337674, 0.336058180907677, -0.3181871419836735, -0.22289812224435396, 0.14951633018088237, -0.16569241033947288, -0.21923358160360107, 0.22838755530016175, -0.1168019830907598... |
1,801.01032 | The $C^1$ property of convex carrying simplices for competitive maps | For a class of competitive maps there is an invariant one-codimensional
manifold (the carrying simplex) attracting all non-trivial orbits. In the
present paper it is shown that its convexity implies that it is a $C^1$
submanifold-with-corners, neatly embedded in the non-negative orthant. The
proof uses the characteri... | math.DS math.CA | for a class of competitive maps there is an invariant onecodimensional manifold the carrying simplex attracting all nontrivial orbits in the present paper it is shown that its convexity implies that it is a c1 submanifoldwithcorners neatly embedded in the nonnegative orthant the proof uses the characterization of neat ... | [['for', 'a', 'class', 'of', 'competitive', 'maps', 'there', 'is', 'an', 'invariant', 'onecodimensional', 'manifold', 'the', 'carrying', 'simplex', 'attracting', 'all', 'nontrivial', 'orbits', 'in', 'the', 'present', 'paper', 'it', 'is', 'shown', 'that', 'its', 'convexity', 'implies', 'that', 'it', 'is', 'a', 'c1', 'su... | [-0.19395160880041026, 0.08091319597556519, -0.11731141942647705, 0.05419130975454776, -0.01687217254758529, -0.15788635797123762, 0.023362747540333025, 0.31925950746855064, -0.24958672652533953, -0.14154067578172122, 0.1333009392998276, -0.29948847330566764, -0.1851695350546768, 0.20428689595554833, -0.118228202307785... |
1,801.01033 | Two-Loop master integrals for heavy-to-light form factors of two
different massive fermions | We calculate the full set of the two-loop master integrals for heavy-to-light
form factors of two different massive fermions for arbitrary momentum transfer
in NNLO QCD or QED corrections. These integrals allow to determine the two-loop
QCD or QED corrections to the amplitudes for heavy-to-light form factors of two
m... | hep-ph | we calculate the full set of the twoloop master integrals for heavytolight form factors of two different massive fermions for arbitrary momentum transfer in nnlo qcd or qed corrections these integrals allow to determine the twoloop qcd or qed corrections to the amplitudes for heavytolight form factors of two massive fe... | [['we', 'calculate', 'the', 'full', 'set', 'of', 'the', 'twoloop', 'master', 'integrals', 'for', 'heavytolight', 'form', 'factors', 'of', 'two', 'different', 'massive', 'fermions', 'for', 'arbitrary', 'momentum', 'transfer', 'in', 'nnlo', 'qcd', 'or', 'qed', 'corrections', 'these', 'integrals', 'allow', 'to', 'determin... | [-0.17921490676823365, 0.11785569404148394, -0.0852045209683252, 0.11680004036411493, -0.056900795045863796, -0.03645589499913081, 0.06845226119074857, 0.29973226025550054, -0.15098993194223653, -0.2402049274127366, 0.006303991577964314, -0.29494618474872725, -0.10964076562474172, 0.20946463265672627, 0.056525480698304... |
1,801.01034 | Computing rotation numbers in open books | We give explicit formulas and algorithms for the computation of the rotation
number of a nullhomologous Legendrian knot on a page of a contact open book. On
the way, we derive new formulas for the computation of the Thurston-Bennequin
invariant of such knots and the Euler class and the d3-invariant of the
underlying ... | math.GT math.SG | we give explicit formulas and algorithms for the computation of the rotation number of a nullhomologous legendrian knot on a page of a contact open book on the way we derive new formulas for the computation of the thurstonbennequin invariant of such knots and the euler class and the d3invariant of the underlying contac... | [['we', 'give', 'explicit', 'formulas', 'and', 'algorithms', 'for', 'the', 'computation', 'of', 'the', 'rotation', 'number', 'of', 'a', 'nullhomologous', 'legendrian', 'knot', 'on', 'a', 'page', 'of', 'a', 'contact', 'open', 'book', 'on', 'the', 'way', 'we', 'derive', 'new', 'formulas', 'for', 'the', 'computation', 'of... | [-0.25920150172034345, 0.01740891496754355, -0.10012163688359713, 0.1078649485759713, -0.11055567301809788, -0.1395716752115361, 0.09604324431469043, 0.3138221580259226, -0.25521091095396076, -0.3562405108715649, 0.09373174296881727, -0.1971614759941413, -0.16364586289489158, 0.24520337923550634, -0.08111452165165381, ... |
1,801.01035 | Local probabilities of randomly stopped sums of power law lattice random
variables | Let $X_1$ and $N\ge 0$ be integer valued power law random variables. For a
randomly stopped sum $S_N=X_1+\cdots+X_N$ of independent and identically
distributed copies of $X_1$ we establish a first order asymptotics of the local
probabilities $P(S_N=t)$ as $t\to+\infty$. Using this result we show the
$k^{-\delta}$, $0... | math.PR physics.soc-ph | let x_1 and nge 0 be integer valued power law random variables for a randomly stopped sum s_nx_1cdotsx_n of independent and identically distributed copies of x_1 we establish a first order asymptotics of the local probabilities ps_nt as ttoinfty using this result we show the kdelta 0le deltale 1 scaling of the local cl... | [['let', 'x_1', 'and', 'nge', '0', 'be', 'integer', 'valued', 'power', 'law', 'random', 'variables', 'for', 'a', 'randomly', 'stopped', 'sum', 's_nx_1cdotsx_n', 'of', 'independent', 'and', 'identically', 'distributed', 'copies', 'of', 'x_1', 'we', 'establish', 'a', 'first', 'order', 'asymptotics', 'of', 'the', 'local',... | [-0.20772088916205309, 0.16670489166041508, -0.07767040952218368, -0.05405237925108796, -0.017424419907483217, -0.1865938910666634, 0.08905073494979125, 0.32126478256438584, -0.33063765871338546, -0.207006493336795, 0.05159472515772316, -0.3363599852823159, -0.09213878962498925, 0.07375387799487833, -0.0390633953433922... |
1,801.01036 | Counter-streaming flows in a giant quiet-Sun filament observed in the
extreme ultraviolet | A giant solar filament was visible on the solar surface from 2011 Nov. 8-23.
The filament stretched over more than half a solar diameter. Multiwavelength
data from the SDO instrument AIA (171, 193, 304, and 211\AA) were used to
examine counter-streaming flows within the spine of the filament. H$\alpha$
images from th... | astro-ph.SR | a giant solar filament was visible on the solar surface from 2011 nov 823 the filament stretched over more than half a solar diameter multiwavelength data from the sdo instrument aia 171 193 304 and 211aa were used to examine counterstreaming flows within the spine of the filament halpha images from the kanzelhohe sola... | [['a', 'giant', 'solar', 'filament', 'was', 'visible', 'on', 'the', 'solar', 'surface', 'from', '2011', 'nov', '823', 'the', 'filament', 'stretched', 'over', 'more', 'than', 'half', 'a', 'solar', 'diameter', 'multiwavelength', 'data', 'from', 'the', 'sdo', 'instrument', 'aia', '171', '193', '304', 'and', '211aa', 'were... | [-0.10562471287262046, 0.16167952205001027, -0.04270877921419432, 0.07910799785234705, -0.03843559875862948, -0.06760252275672116, -0.02231769927884223, 0.4690157877067562, -0.22352734368798308, -0.3371396224350348, 0.09833987990211024, -0.2704429651511791, -0.0799428992897089, 0.21522281100347515, -0.0654127383337463,... |
1,801.01037 | Distributed Memory Techniques for Classical Simulation of Quantum
Circuits | In this paper we describe, implement, and test the performance of distributed
memory simulations of quantum circuits on the MSU Laconia Top500 supercomputer.
Using OpenMP and MPI hybrid parallelization, we first use a distributed
matrix-vector multiplication with one-dimensional partitioning and discuss the
shortcomi... | quant-ph cs.DC | in this paper we describe implement and test the performance of distributed memory simulations of quantum circuits on the msu laconia top500 supercomputer using openmp and mpi hybrid parallelization we first use a distributed matrixvector multiplication with onedimensional partitioning and discuss the shortcomings of t... | [['in', 'this', 'paper', 'we', 'describe', 'implement', 'and', 'test', 'the', 'performance', 'of', 'distributed', 'memory', 'simulations', 'of', 'quantum', 'circuits', 'on', 'the', 'msu', 'laconia', 'top500', 'supercomputer', 'using', 'openmp', 'and', 'mpi', 'hybrid', 'parallelization', 'we', 'first', 'use', 'a', 'dist... | [-0.19536795419382974, 0.08744838674653194, -0.012341071850299755, -0.0012780360278851224, -0.028398252116085623, -0.21356417032168998, 0.12754944724253608, 0.41897985909975344, -0.2638897582167579, -0.3391432820629048, 0.05189014844764124, -0.24756768989363892, -0.12448506079043352, 0.19160200315039425, -0.05808284817... |
1,801.01038 | Mechanical, optoelectronic and transport properties of single-layer Ca2N
and Sr2N electrides | Electride materials offer attractive physical properties due to their loosely
bound electrons. Ca2N, an electride in the two-dimensional (2D) form was
successfully recently synthesized. We conducted extensive first-principles
calculations to explore the mechanical, electronic, optical and transport
response of single... | physics.comp-ph cond-mat.mtrl-sci | electride materials offer attractive physical properties due to their loosely bound electrons ca2n an electride in the twodimensional 2d form was successfully recently synthesized we conducted extensive firstprinciples calculations to explore the mechanical electronic optical and transport response of singlelayer and f... | [['electride', 'materials', 'offer', 'attractive', 'physical', 'properties', 'due', 'to', 'their', 'loosely', 'bound', 'electrons', 'ca2n', 'an', 'electride', 'in', 'the', 'twodimensional', '2d', 'form', 'was', 'successfully', 'recently', 'synthesized', 'we', 'conducted', 'extensive', 'firstprinciples', 'calculations',... | [-0.15559902369283402, 0.163851862658127, -0.010457321137994828, -0.014758765530168786, -0.029276896639897878, -0.11613008361684168, 0.0468213224500399, 0.4587106489056918, -0.2839175218051702, -0.2692160217358202, 0.014872929043295657, -0.2898908937466916, -0.15914571330526928, 0.21081407519698556, 0.05068202827350428... |
1,801.01039 | Computing the Inverse Mellin Transform of Holonomic Sequences using
Kovacic's Algorithm | We describe how the extension of a solver for linear differential equations
by Kovacic's algorithm helps to improve a method to compute the inverse Mellin
transform of holonomic sequences. The method is implemented in the computer
algebra package HarmonicSums.
| cs.SC math-ph math.CO math.MP | we describe how the extension of a solver for linear differential equations by kovacics algorithm helps to improve a method to compute the inverse mellin transform of holonomic sequences the method is implemented in the computer algebra package harmonicsums | [['we', 'describe', 'how', 'the', 'extension', 'of', 'a', 'solver', 'for', 'linear', 'differential', 'equations', 'by', 'kovacics', 'algorithm', 'helps', 'to', 'improve', 'a', 'method', 'to', 'compute', 'the', 'inverse', 'mellin', 'transform', 'of', 'holonomic', 'sequences', 'the', 'method', 'is', 'implemented', 'in', ... | [-0.0719360842441137, -0.057712772311881565, -0.1735291799578147, 0.11155184558055435, -0.1445420645416165, -0.14453647451666304, -0.05221645204493633, 0.3336274083226155, -0.37745043807304823, -0.2970561430288049, 0.11012848237087616, -0.19750066636464533, -0.21581844374155387, 0.27457938350450534, -0.0768453125806095... |
1,801.0104 | Interpretation of increased energetic particle flux measurements by SEPT
aboard the STEREO spacecraft and contamination | Context. Interplanetary (IP) shocks are known to be accelerators of energetic
charged particles observed in-situ in the heliosphere. However, the
acceleration of near-relativistic electrons by shocks in the interplanetary
medium is often questioned. On 9 August 2011 a Corotating Interaction Region
(CIR) passed STEREO... | physics.space-ph astro-ph.SR | context interplanetary ip shocks are known to be accelerators of energetic charged particles observed insitu in the heliosphere however the acceleration of nearrelativistic electrons by shocks in the interplanetary medium is often questioned on 9 august 2011 a corotating interaction region cir passed stereo b stb that ... | [['context', 'interplanetary', 'ip', 'shocks', 'are', 'known', 'to', 'be', 'accelerators', 'of', 'energetic', 'charged', 'particles', 'observed', 'insitu', 'in', 'the', 'heliosphere', 'however', 'the', 'acceleration', 'of', 'nearrelativistic', 'electrons', 'by', 'shocks', 'in', 'the', 'interplanetary', 'medium', 'is', ... | [-0.06196933160789659, 0.23765453038849743, 0.0011738045575959673, 0.10312809568244587, 0.009850240986547814, -0.1277823793178185, 0.061992147751243114, 0.4173808812149275, -0.16245419556612026, -0.4206791322439155, -0.012362170278670898, -0.36171030961629363, 0.02656570245450225, 0.1949304669023245, -0.018379546867358... |
1,801.01041 | Almost h-conformal slant submersions from almost quaternionic Hermitian
manifolds | We introduce the notions of h-conformal slant submersions and almost
h-conformal slant submersions from almost quaternionic Hermitian manifolds onto
Riemannian manifolds as a generalization of Riemannian submersions,
horizontally conformal submersions, slant submersions, h-slant submersions,
almost h-slant submersion... | math.DG | we introduce the notions of hconformal slant submersions and almost hconformal slant submersions from almost quaternionic hermitian manifolds onto riemannian manifolds as a generalization of riemannian submersions horizontally conformal submersions slant submersions hslant submersions almost hslant submersion and confo... | [['we', 'introduce', 'the', 'notions', 'of', 'hconformal', 'slant', 'submersions', 'and', 'almost', 'hconformal', 'slant', 'submersions', 'from', 'almost', 'quaternionic', 'hermitian', 'manifolds', 'onto', 'riemannian', 'manifolds', 'as', 'a', 'generalization', 'of', 'riemannian', 'submersions', 'horizontally', 'confor... | [-0.22520385722856265, 0.06457852436279929, -0.05855140526703483, 0.20055290755840974, -0.15641737454633758, -0.14728393757438943, -0.18214737718320778, 0.4762380022454906, -0.3146262173415036, -0.14646930533864005, 0.13935386450533327, -0.3827290020732058, -0.2848412412646654, 0.16425177269942454, -0.24218500961826459... |
1,801.01042 | Highly anisotropic strain dependencies in PrIr$_2$Zn$_{20}$ | We report thermal expansion and magnetostriction of the cubic non-Kramers
system PrIr$_2$Zn$_{20}$ with a non-magnetic $\varGamma_{3}$ ground state
doublet. In previous experiments, antiferroquadrupolar order at
\hbox{$T_{\mathrm{Q}}=0.11$\,K} and a Fermi liquid state around
$B_{\mathrm{c}}\approx5$\,T for \hbox{$\bo... | cond-mat.str-el | we report thermal expansion and magnetostriction of the cubic nonkramers system prir_2zn_20 with a nonmagnetic vargamma_3 ground state doublet in previous experiments antiferroquadrupolar order at hboxt_mathrmq011k and a fermi liquid state around b_mathrmcapprox5t for hboxboldsymbolbparallel001 indicative of possible f... | [['we', 'report', 'thermal', 'expansion', 'and', 'magnetostriction', 'of', 'the', 'cubic', 'nonkramers', 'system', 'prir_2zn_20', 'with', 'a', 'nonmagnetic', 'vargamma_3', 'ground', 'state', 'doublet', 'in', 'previous', 'experiments', 'antiferroquadrupolar', 'order', 'at', 'hboxt_mathrmq011k', 'and', 'a', 'fermi', 'liq... | [-0.1749872621186378, 0.25392921174681116, -0.02388000756224257, 0.029560377658438688, -0.040923700016367456, -0.11370105448088819, 0.08746277178673359, 0.34979884546144957, -0.24774741398681316, -0.3027775040076625, 0.04286024159274905, -0.30635532177984715, -0.06372608374353618, 0.14612552042179291, 0.042926781149881... |
1,801.01043 | A and F stars as probes of outer Galactic disc kinematics | Previous studies of the rotation law in the outer Galactic disc have mainly
used gas tracers or clump giants. Here, we explore A and F stars as
alternatives: these provide a much denser sampling in the outer disc than gas
tracers and have experienced significantly less velocity scattering than older
clump giants. Thi... | astro-ph.GA astro-ph.SR | previous studies of the rotation law in the outer galactic disc have mainly used gas tracers or clump giants here we explore a and f stars as alternatives these provide a much denser sampling in the outer disc than gas tracers and have experienced significantly less velocity scattering than older clump giants this firs... | [['previous', 'studies', 'of', 'the', 'rotation', 'law', 'in', 'the', 'outer', 'galactic', 'disc', 'have', 'mainly', 'used', 'gas', 'tracers', 'or', 'clump', 'giants', 'here', 'we', 'explore', 'a', 'and', 'f', 'stars', 'as', 'alternatives', 'these', 'provide', 'a', 'much', 'denser', 'sampling', 'in', 'the', 'outer', 'd... | [-0.06598779394557573, 0.12987029923472154, -0.07132632540782544, 0.05250978696293626, -0.09522236968618562, -0.05604607606589605, 0.05325915487993996, 0.4277022267585691, -0.16912838734709953, -0.344907663402517, 0.02107399313529867, -0.2937920902961794, -0.024112816246713704, 0.20204968959729694, -0.07115860918022492... |
1,801.01044 | Opposing effects of stacking faults and antisite domain boundaries on
the conduction band edge in kesterite quaternary semiconductors | We investigated stability and the electronic structure of extended defects
including anti-site domain boundaries and stacking faults in the
kesterite-structured semiconductors, Cu$_2$ZnSnS$_4$ (CZTS) and
Cu$_2$ZnSnSe$_4$ (CZTSe). Our hybrid density functional theory calculations
show that stacking faults in CZTS and ... | cond-mat.mtrl-sci | we investigated stability and the electronic structure of extended defects including antisite domain boundaries and stacking faults in the kesteritestructured semiconductors cu_2znsns_4 czts and cu_2znsnse_4 cztse our hybrid density functional theory calculations show that stacking faults in czts and cztse induce a hig... | [['we', 'investigated', 'stability', 'and', 'the', 'electronic', 'structure', 'of', 'extended', 'defects', 'including', 'antisite', 'domain', 'boundaries', 'and', 'stacking', 'faults', 'in', 'the', 'kesteritestructured', 'semiconductors', 'cu_2znsns_4', 'czts', 'and', 'cu_2znsnse_4', 'cztse', 'our', 'hybrid', 'density'... | [-0.1637257196394225, 0.11254920924441719, 0.029397502447514292, 0.06409599545300947, -0.006874863776969365, -0.10468195719519056, 0.09492845824234582, 0.4334072126254726, -0.258505535697063, -0.3061103224396132, 0.036707128424985476, -0.32852598490605417, -0.1484311434391062, 0.08780581089936626, 0.03321150726137253, ... |
1,801.01045 | The effect of metallicity on the atmospheres of exoplanets with fully
coupled 3D hydrodynamics, equilibrium chemistry, and radiative transfer | In this work we have performed a series of simulations of the atmosphere of
GJ~1214b assuming different metallicities using the Met Office Unified Model
(UM). The UM is a general circulation model (GCM) that solves the deep,
non-hydrostatic equations of motion and uses a flexible and accurate radiative
transfer schem... | astro-ph.EP | in this work we have performed a series of simulations of the atmosphere of gj1214b assuming different metallicities using the met office unified model um the um is a general circulation model gcm that solves the deep nonhydrostatic equations of motion and uses a flexible and accurate radiative transfer scheme based on... | [['in', 'this', 'work', 'we', 'have', 'performed', 'a', 'series', 'of', 'simulations', 'of', 'the', 'atmosphere', 'of', 'gj1214b', 'assuming', 'different', 'metallicities', 'using', 'the', 'met', 'office', 'unified', 'model', 'um', 'the', 'um', 'is', 'a', 'general', 'circulation', 'model', 'gcm', 'that', 'solves', 'the... | [-0.05476203343138245, 0.1013915559329698, -0.06633136748322492, 0.08064522437024127, -0.021266697179938992, -0.06923265929111358, 0.0599593530005312, 0.3858853933571154, -0.2472849298461244, -0.3307867306903959, 0.03663126513272469, -0.23526043046192435, -0.10309905241693146, 0.1750950191971121, -0.03657294722650145, ... |
1,801.01046 | Grinberg-Kazhdan theorem and Newton groupoids | We first prove the Grinberg-Kazhdan formal arc theorem without any
assumptions on the characteristic. This part of the article is equivalent to
arXiv:math-AG/0203263.
Then we try to clarify the geometric ideas behind the proof by introducing
the notion of Newton groupoid (which is related to Newton's method for fin... | math.AG math.RT | we first prove the grinbergkazhdan formal arc theorem without any assumptions on the characteristic this part of the article is equivalent to arxivmathag0203263 then we try to clarify the geometric ideas behind the proof by introducing the notion of newton groupoid which is related to newtons method for finding roots n... | [['we', 'first', 'prove', 'the', 'grinbergkazhdan', 'formal', 'arc', 'theorem', 'without', 'any', 'assumptions', 'on', 'the', 'characteristic', 'this', 'part', 'of', 'the', 'article', 'is', 'equivalent', 'to', 'arxivmathag0203263', 'then', 'we', 'try', 'to', 'clarify', 'the', 'geometric', 'ideas', 'behind', 'the', 'pro... | [-0.14490100432646602, 0.005372282870317975, -0.1566063238288697, 0.09207303904488122, -0.18762788893527363, -0.12761203333582372, 0.029967717060895814, 0.3341882241609162, -0.4080719589319539, -0.21330286180345367, 0.10159345270191919, -0.2003267859682849, -0.15337533952846918, 0.20937429258140594, -0.2321806958021774... |
1,801.01047 | On the exact maximum induced density of almost all graphs and their
inducibility | Let $H$ be a graph on $h$ vertices. The number of induced copies of $H$ in a
graph $G$ is denoted by $i_H(G)$. Let $i_H(n)$ denote the maximum of $i_H(G)$
taken over all graphs $G$ with $n$ vertices.
Let $f(n,h) = \Pi_{i}^h a_i$ where $\sum_{i=1}^h a_i = n$ and the $a_i$ are
as equal as possible. Let $g(n,h) = f(n,... | math.CO | let h be a graph on h vertices the number of induced copies of h in a graph g is denoted by i_hg let i_hn denote the maximum of i_hg taken over all graphs g with n vertices let fnh pi_ih a_i where sum_i1h a_i n and the a_i are as equal as possible let gnh fnh sum_i1h ga_ih it is proved that for almost all graphs h on h... | [['let', 'h', 'be', 'a', 'graph', 'on', 'h', 'vertices', 'the', 'number', 'of', 'induced', 'copies', 'of', 'h', 'in', 'a', 'graph', 'g', 'is', 'denoted', 'by', 'i_hg', 'let', 'i_hn', 'denote', 'the', 'maximum', 'of', 'i_hg', 'taken', 'over', 'all', 'graphs', 'g', 'with', 'n', 'vertices', 'let', 'fnh', 'pi_ih', 'a_i', '... | [-0.16732561449300676, 0.19577747200953513, -0.01097804850260178, -0.015117467875189786, -0.06422812824735345, -0.19615018667396988, 0.018137350906190914, 0.3644509014640996, -0.2357412842407367, -0.2677994125754487, 0.057936949271090554, -0.355055857244391, -0.1022579573276839, 0.10769222683820255, -0.0575207808465741... |
1,801.01048 | Impact Assessment of Hypothesized Cyberattacks on Interconnected Bulk
Power Systems | The first-ever Ukraine cyberattack on power grid has proven its devastation
by hacking into their critical cyber assets. With administrative privileges
accessing substation networks/local control centers, one intelligent way of
coordinated cyberattacks is to execute a series of disruptive switching
executions on mult... | cs.CR cs.SY | the firstever ukraine cyberattack on power grid has proven its devastation by hacking into their critical cyber assets with administrative privileges accessing substation networkslocal control centers one intelligent way of coordinated cyberattacks is to execute a series of disruptive switching executions on multiple s... | [['the', 'firstever', 'ukraine', 'cyberattack', 'on', 'power', 'grid', 'has', 'proven', 'its', 'devastation', 'by', 'hacking', 'into', 'their', 'critical', 'cyber', 'assets', 'with', 'administrative', 'privileges', 'accessing', 'substation', 'networkslocal', 'control', 'centers', 'one', 'intelligent', 'way', 'of', 'coo... | [-0.20487948977563064, 0.04694407465700351, -0.052081763879104986, 0.037855006799218244, -0.10146084845880977, -0.14110767902748195, 0.0927961969212629, 0.3232722379779443, -0.25677920758556866, -0.3190193822752917, 0.18964041511004326, -0.2888229638244957, -0.12871274372562766, 0.18929445318703075, -0.1377580364933237... |
1,801.01049 | Orbital Period Increase in ES Ceti | We report a long-term study of the eclipse times in the 10-minute helium
binary ES Ceti. The binary period increases rapidly, with P/P-dot = 6.2x10^6
yr. This is consistent with the assumption that gravitational radiation (GR)
drives the mass transfer, and appears to be the first dynamical evidence that
GR is indeed ... | astro-ph.SR | we report a longterm study of the eclipse times in the 10minute helium binary es ceti the binary period increases rapidly with ppdot 62x106 yr this is consistent with the assumption that gravitational radiation gr drives the mass transfer and appears to be the first dynamical evidence that gr is indeed the driver of ev... | [['we', 'report', 'a', 'longterm', 'study', 'of', 'the', 'eclipse', 'times', 'in', 'the', '10minute', 'helium', 'binary', 'es', 'ceti', 'the', 'binary', 'period', 'increases', 'rapidly', 'with', 'ppdot', '62x106', 'yr', 'this', 'is', 'consistent', 'with', 'the', 'assumption', 'that', 'gravitational', 'radiation', 'gr',... | [-0.1339463561724649, 0.1852986933107474, -0.09286377113312483, 0.08558481915005997, -0.08393717432783833, -0.09663685706075725, 0.05640182232678826, 0.34393875801296375, -0.19482380308822464, -0.2992241849650198, 0.07361799971645337, -0.2685357759404344, -0.11632532114163041, 0.19753392869189604, -0.09960297468716084,... |
1,801.0105 | Information Bottleneck on General Alphabets | We prove rigorously a source coding theorem that can probably be considered
folklore, a generalization to arbitrary alphabets of a problem motivated by the
Information Bottleneck method. For general random variables $(Y, X)$, we show
essentially that for some $n \in \mathbb{N}$, a function $f$ with rate limit
$\log|f... | cs.IT math.IT | we prove rigorously a source coding theorem that can probably be considered folklore a generalization to arbitrary alphabets of a problem motivated by the information bottleneck method for general random variables y x we show essentially that for some n in mathbbn a function f with rate limit logf le nr and iyn fxn ge ... | [['we', 'prove', 'rigorously', 'a', 'source', 'coding', 'theorem', 'that', 'can', 'probably', 'be', 'considered', 'folklore', 'a', 'generalization', 'to', 'arbitrary', 'alphabets', 'of', 'a', 'problem', 'motivated', 'by', 'the', 'information', 'bottleneck', 'method', 'for', 'general', 'random', 'variables', 'y', 'x', '... | [-0.16632436437286297, 0.11856738257744648, -0.06996727129883783, 0.07931886508485372, -0.004929707578892978, -0.2476192726050767, 0.12082839699216047, 0.35608204956746325, -0.3258002519888698, -0.19684801951823933, 0.08708827624883819, -0.2606752481496067, -0.10146111135265597, 0.1935041393373021, -0.09698272439352465... |
1,801.01051 | Spot the Difference by Object Detection | In this paper, we propose a simple yet effective solution to a change
detection task that detects the difference between two images, which we call
"spot the difference". Our approach uses CNN-based object detection by stacking
two aligned images as input and considering the differences between the two
images as objec... | cs.CV | in this paper we propose a simple yet effective solution to a change detection task that detects the difference between two images which we call spot the difference our approach uses cnnbased object detection by stacking two aligned images as input and considering the differences between the two images as objects to de... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'simple', 'yet', 'effective', 'solution', 'to', 'a', 'change', 'detection', 'task', 'that', 'detects', 'the', 'difference', 'between', 'two', 'images', 'which', 'we', 'call', 'spot', 'the', 'difference', 'our', 'approach', 'uses', 'cnnbased', 'object', 'detection', 'by', '... | [-0.04869376233298776, -0.039211244936298205, -0.06821569827464379, 0.04988215933325609, -0.10950215554071797, -0.16580253685794138, 0.05199743611388079, 0.45565177999996864, -0.2163164648988278, -0.3888200859423556, 0.10497131624359492, -0.279030535090106, -0.15877271553705405, 0.21631640561984158, -0.1357314808676901... |
1,801.01052 | Monolithic quantum-dot distributed feedback laser array on silicon | Electrically-pumped lasers directly grown on silicon are key devices
interfacing silicon microelectronics and photonics. We report here, for the
first time, an electrically-pumped, room-temperature, continuous-wave (CW) and
single-mode distributed feedback (DFB) laser array fabricated in InAs/GaAs
quantum-dot (QD) ga... | physics.optics physics.app-ph | electricallypumped lasers directly grown on silicon are key devices interfacing silicon microelectronics and photonics we report here for the first time an electricallypumped roomtemperature continuouswave cw and singlemode distributed feedback dfb laser array fabricated in inasgaas quantumdot qd gain material epitaxia... | [['electricallypumped', 'lasers', 'directly', 'grown', 'on', 'silicon', 'are', 'key', 'devices', 'interfacing', 'silicon', 'microelectronics', 'and', 'photonics', 'we', 'report', 'here', 'for', 'the', 'first', 'time', 'an', 'electricallypumped', 'roomtemperature', 'continuouswave', 'cw', 'and', 'singlemode', 'distribut... | [-0.15245482475490224, 0.16625963133218588, 0.011411723449614877, -0.1189485745213873, 0.053236371885443515, -0.24092304578764326, 0.06929194779260785, 0.5351435493691065, -0.2056599698683366, -0.32695948310090717, 0.09597538863820625, -0.26529200191106744, -0.04024938139189299, 0.3077715248173327, -0.02049050710976440... |
1,801.01053 | Low-depth circuit ansatz for preparing correlated fermionic states on a
quantum computer | Quantum simulations are bound to be one of the main applications of near-term
quantum computers. Quantum chemistry and condensed matter physics are expected
to benefit from these technological developments. Several quantum simulation
methods are known to prepare a state on a quantum computer and measure the
desired o... | quant-ph | quantum simulations are bound to be one of the main applications of nearterm quantum computers quantum chemistry and condensed matter physics are expected to benefit from these technological developments several quantum simulation methods are known to prepare a state on a quantum computer and measure the desired observ... | [['quantum', 'simulations', 'are', 'bound', 'to', 'be', 'one', 'of', 'the', 'main', 'applications', 'of', 'nearterm', 'quantum', 'computers', 'quantum', 'chemistry', 'and', 'condensed', 'matter', 'physics', 'are', 'expected', 'to', 'benefit', 'from', 'these', 'technological', 'developments', 'several', 'quantum', 'simu... | [-0.08855523976744015, 0.1724357746587173, -0.11640759487866913, 0.05206039459167952, -0.021167145842584865, -0.1842586915100934, 0.04203108368478346, 0.33888780972044363, -0.262239549849021, -0.3149916002628311, 0.0420465417711138, -0.2709533339965683, -0.11470600237405978, 0.20680925807002748, 0.00011455248995213816,... |
1,801.01054 | Computational complexity lower bounds of certain discrete Radon
transform approximations | For the computational model where only additions are allowed, the
$\Omega(n^2\log n)$ lower bound on operations count with respect to image size
$n\times n$ is obtained for two types of the discrete Radon transform
implementations: the fast Hough transform and a generic strip pattern class
which includes the classica... | cs.CC cs.CV | for the computational model where only additions are allowed the omegan2log n lower bound on operations count with respect to image size ntimes n is obtained for two types of the discrete radon transform implementations the fast hough transform and a generic strip pattern class which includes the classical hough transf... | [['for', 'the', 'computational', 'model', 'where', 'only', 'additions', 'are', 'allowed', 'the', 'omegan2log', 'n', 'lower', 'bound', 'on', 'operations', 'count', 'with', 'respect', 'to', 'image', 'size', 'ntimes', 'n', 'is', 'obtained', 'for', 'two', 'types', 'of', 'the', 'discrete', 'radon', 'transform', 'implementat... | [-0.07294790776255208, 0.0784714152770383, -0.05009792354844865, 0.0733412159343494, -0.0856226378375487, -0.19215316281077408, 0.07748660126318489, 0.3548265930952593, -0.2754366298516591, -0.26370919287174255, 0.16017965196737177, -0.25516432277592166, -0.1695313643375855, 0.2677082112973689, -0.07427151586549978, 0.... |
1,801.01055 | Gaps between prime numbers and tensor rank of multiplication in finite
fields | We present effective upper bounds on the symmetric bilinear complexity of
multiplication in extensions of a base finite field Fp2 of prime square order,
obtained by combining estimates on gaps between prime numbers together with an
optimal construction of auxiliary divisors for multiplication algorithms by
evaluation... | math.NT cs.CC | we present effective upper bounds on the symmetric bilinear complexity of multiplication in extensions of a base finite field fp2 of prime square order obtained by combining estimates on gaps between prime numbers together with an optimal construction of auxiliary divisors for multiplication algorithms by evaluationint... | [['we', 'present', 'effective', 'upper', 'bounds', 'on', 'the', 'symmetric', 'bilinear', 'complexity', 'of', 'multiplication', 'in', 'extensions', 'of', 'a', 'base', 'finite', 'field', 'fp2', 'of', 'prime', 'square', 'order', 'obtained', 'by', 'combining', 'estimates', 'on', 'gaps', 'between', 'prime', 'numbers', 'toge... | [-0.13754458502587635, 0.0756687294793444, -0.06880707098664998, 0.07164844132035575, -0.10259767448896485, -0.11526143794639432, 0.08697752588231003, 0.3374752196003542, -0.26089805149152223, -0.32859515046672616, 0.12545694359560552, -0.25168125877462444, -0.12820105957198943, 0.2724165827032376, -0.10152047828799396... |
1,801.01056 | A New HDG Method for Dirichlet Boundary Control of Convection Diffusion
PDEs II: Low Regularity | In the first part of this work, we analyzed a Dirichlet boundary control
problem for an elliptic convection diffusion PDE and proposed a new
hybridizable discontinuous Galerkin (HDG) method to approximate the solution.
For the case of a 2D polygonal domain, we also proved an optimal superlinear
convergence rate for t... | math.NA | in the first part of this work we analyzed a dirichlet boundary control problem for an elliptic convection diffusion pde and proposed a new hybridizable discontinuous galerkin hdg method to approximate the solution for the case of a 2d polygonal domain we also proved an optimal superlinear convergence rate for the cont... | [['in', 'the', 'first', 'part', 'of', 'this', 'work', 'we', 'analyzed', 'a', 'dirichlet', 'boundary', 'control', 'problem', 'for', 'an', 'elliptic', 'convection', 'diffusion', 'pde', 'and', 'proposed', 'a', 'new', 'hybridizable', 'discontinuous', 'galerkin', 'hdg', 'method', 'to', 'approximate', 'the', 'solution', 'for... | [-0.09841709762572422, -0.041938237361679356, -0.10896440017797532, 0.044977313517421964, -0.06970101539600948, -0.09322160867752012, 0.059697630833364476, 0.3658167192319391, -0.30995705228196374, -0.22308998450705217, 0.18815227058062484, -0.2313631289262632, -0.14546411117931846, 0.2016692685760096, -0.1190833769943... |
1,801.01057 | Full configuration interaction quantum Monte Carlo benchmark and
multireference coupled cluster studies of tetramethyleneethane diradical | We have performed a FCI-quality benchmark calculation for the
tetramethyleneethane molecule in cc-pVTZ basis set employing a subset of
CASPT2(6,6) natural orbitals for the FCIQMC calculation. The results are in an
excellent agreement with the previous large scale diffusion Monte Carlo
calculations by Pozun et al. and... | physics.chem-ph cond-mat.str-el | we have performed a fciquality benchmark calculation for the tetramethyleneethane molecule in ccpvtz basis set employing a subset of caspt266 natural orbitals for the fciqmc calculation the results are in an excellent agreement with the previous large scale diffusion monte carlo calculations by pozun et al and availabl... | [['we', 'have', 'performed', 'a', 'fciquality', 'benchmark', 'calculation', 'for', 'the', 'tetramethyleneethane', 'molecule', 'in', 'ccpvtz', 'basis', 'set', 'employing', 'a', 'subset', 'of', 'caspt266', 'natural', 'orbitals', 'for', 'the', 'fciqmc', 'calculation', 'the', 'results', 'are', 'in', 'an', 'excellent', 'agr... | [-0.07391502933593534, 0.08337708087781787, -0.051728907380679465, 0.08876595352509856, -0.012454758079845953, -0.10973334794791123, 0.050706875173891164, 0.39506197651197394, -0.19799850446856523, -0.37388126032584046, 0.007825896880275244, -0.2865963816833514, -0.059073707997709154, 0.1819740033102592, 0.025285873879... |
1,801.01058 | Polynomial-based rotation invariant features | One of basic difficulties of machine learning is handling unknown rotations
of objects, for example in image recognition. A related problem is evaluation
of similarity of shapes, for example of two chemical molecules, for which
direct approach requires costly pairwise rotation alignment and comparison.
Rotation invar... | cs.LG | one of basic difficulties of machine learning is handling unknown rotations of objects for example in image recognition a related problem is evaluation of similarity of shapes for example of two chemical molecules for which direct approach requires costly pairwise rotation alignment and comparison rotation invariants a... | [['one', 'of', 'basic', 'difficulties', 'of', 'machine', 'learning', 'is', 'handling', 'unknown', 'rotations', 'of', 'objects', 'for', 'example', 'in', 'image', 'recognition', 'a', 'related', 'problem', 'is', 'evaluation', 'of', 'similarity', 'of', 'shapes', 'for', 'example', 'of', 'two', 'chemical', 'molecules', 'for'... | [-0.09588864321206493, 0.09074443040738225, -0.06918825799411985, 0.08562795361263324, -0.10475983306526222, -0.20654075681466047, -0.0005493212072438867, 0.3901964942794605, -0.27647158859412096, -0.3381138214342005, 0.10985811371694439, -0.21072758570074118, -0.12536915109945493, 0.24699628379653785, -0.0712494721335... |
1,801.01059 | Slowing Down Top Trees for Better Worst-Case Bounds | We consider the top tree compression scheme introduced by Bille et al. [ICALP
2013] and construct an infinite family of trees on $n$ nodes labeled from an
alphabet of size $\sigma$, for which the size of the top DAG is
$\Theta(\frac{n}{\log_\sigma n}\log\log_\sigma n)$. Our construction matches a
previously known upp... | cs.DS | we consider the top tree compression scheme introduced by bille et al icalp 2013 and construct an infinite family of trees on n nodes labeled from an alphabet of size sigma for which the size of the top dag is thetafracnlog_sigma nloglog_sigma n our construction matches a previously known upper bound and exhibits a wea... | [['we', 'consider', 'the', 'top', 'tree', 'compression', 'scheme', 'introduced', 'by', 'bille', 'et', 'al', 'icalp', '2013', 'and', 'construct', 'an', 'infinite', 'family', 'of', 'trees', 'on', 'n', 'nodes', 'labeled', 'from', 'an', 'alphabet', 'of', 'size', 'sigma', 'for', 'which', 'the', 'size', 'of', 'the', 'top', '... | [-0.11191008192743512, 0.11783921818425659, -0.06706615981807851, 0.052377363536135715, -0.07928070855205474, -0.15139686488681406, 0.10742183757163044, 0.3129213664451263, -0.244816232121725, -0.3772194336009873, 0.09568848501784606, -0.23062746903683612, -0.14898414904946813, 0.17887942742326876, -0.14157587528714669... |
1,801.0106 | A strictly commutative model for the cochain algebra of a space | The commutative differential graded algebra $A_{\mathrm{PL}}(X)$ of
polynomial forms on a simplicial set $X$ is a crucial tool in rational homotopy
theory. In this note, we construct an integral version $A^{\mathcal{I}}(X)$ of
$A_{\mathrm{PL}}(X)$. Our approach uses diagrams of chain complexes indexed by
the category... | math.AT | the commutative differential graded algebra a_mathrmplx of polynomial forms on a simplicial set x is a crucial tool in rational homotopy theory in this note we construct an integral version amathcalix of a_mathrmplx our approach uses diagrams of chain complexes indexed by the category of finite sets and injections math... | [['the', 'commutative', 'differential', 'graded', 'algebra', 'a_mathrmplx', 'of', 'polynomial', 'forms', 'on', 'a', 'simplicial', 'set', 'x', 'is', 'a', 'crucial', 'tool', 'in', 'rational', 'homotopy', 'theory', 'in', 'this', 'note', 'we', 'construct', 'an', 'integral', 'version', 'amathcalix', 'of', 'a_mathrmplx', 'ou... | [-0.17521129049168066, 0.03561566662904405, -0.11022495474537898, 0.08053710627498041, -0.12233634686161732, -0.14676376126449683, -0.04153425065110084, 0.3150978378309258, -0.43975363062887357, -0.1653765333976982, 0.053766745165921746, -0.21661237719075369, -0.13419544839075415, 0.2018243037533529, -0.209207566467852... |
1,801.01061 | Intrinsic Gaussian processes on complex constrained domains | We propose a class of intrinsic Gaussian processes (in-GPs) for
interpolation, regression and classification on manifolds with a primary focus
on complex constrained domains or irregular shaped spaces arising as subsets or
submanifolds of R, R2, R3 and beyond. For example, in-GPs can accommodate
spatial domains arisi... | stat.ML cs.LG | we propose a class of intrinsic gaussian processes ingps for interpolation regression and classification on manifolds with a primary focus on complex constrained domains or irregular shaped spaces arising as subsets or submanifolds of r r2 r3 and beyond for example ingps can accommodate spatial domains arising as compl... | [['we', 'propose', 'a', 'class', 'of', 'intrinsic', 'gaussian', 'processes', 'ingps', 'for', 'interpolation', 'regression', 'and', 'classification', 'on', 'manifolds', 'with', 'a', 'primary', 'focus', 'on', 'complex', 'constrained', 'domains', 'or', 'irregular', 'shaped', 'spaces', 'arising', 'as', 'subsets', 'or', 'su... | [-0.07056104054453073, 0.016226275184133148, -0.013058480435422251, 0.11232068027952569, -0.10301282579059733, -0.14655340910999926, -0.0005363271005086966, 0.4059540655633265, -0.27353486968074125, -0.26150063904681264, 0.16726051783189178, -0.23898533311789738, -0.15269942419974694, 0.23366650835597902, -0.1179981471... |
1,801.01062 | Construction of Algorithms for Parallel Addition | An algebraic number $\beta \in \mathbb{C}$ with no conjugate of modulus 1 can
serve as the base of a numeration system $(\beta, \mathcal{A})$ with parallel
addition, i.e., the sum of two operands represented in base $\beta$ with digits
from $\mathcal{A}$ is calculated in constant time, irrespective of the length
of t... | math.NT | an algebraic number beta in mathbbc with no conjugate of modulus 1 can serve as the base of a numeration system beta mathcala with parallel addition ie the sum of two operands represented in base beta with digits from mathcala is calculated in constant time irrespective of the length of the operands in order to allow p... | [['an', 'algebraic', 'number', 'beta', 'in', 'mathbbc', 'with', 'no', 'conjugate', 'of', 'modulus', '1', 'can', 'serve', 'as', 'the', 'base', 'of', 'a', 'numeration', 'system', 'beta', 'mathcala', 'with', 'parallel', 'addition', 'ie', 'the', 'sum', 'of', 'two', 'operands', 'represented', 'in', 'base', 'beta', 'with', '... | [-0.1418526997322361, 0.11876272843393318, -0.03971802388451911, 0.043976760661827465, -0.07300371434659839, -0.17118151945223503, 0.06575790966467458, 0.37233215902083144, -0.28259414076337735, -0.2677622823237108, 0.0963331578641776, -0.2025241737092443, -0.11887782380221983, 0.21607908717445976, -0.08521460470523534... |
1,801.01063 | The Effects of Barycentric and Asymmetric Transverse Velocities on
Eclipse and Transit Times | It has long been recognized that the finite speed of light can affect the
observed time of an event. For example, as a source moves radially toward or
away from an observer, the path length and therefore the light travel time to
the observer decreases or increases, causing the event to appear earlier or
later than ot... | astro-ph.SR astro-ph.EP | it has long been recognized that the finite speed of light can affect the observed time of an event for example as a source moves radially toward or away from an observer the path length and therefore the light travel time to the observer decreases or increases causing the event to appear earlier or later than otherwis... | [['it', 'has', 'long', 'been', 'recognized', 'that', 'the', 'finite', 'speed', 'of', 'light', 'can', 'affect', 'the', 'observed', 'time', 'of', 'an', 'event', 'for', 'example', 'as', 'a', 'source', 'moves', 'radially', 'toward', 'or', 'away', 'from', 'an', 'observer', 'the', 'path', 'length', 'and', 'therefore', 'the',... | [-0.17622397463157893, 0.16603877217769727, -0.09014502127168451, 0.054664904871476655, -0.09465763218859248, -0.12238420456127538, 0.04398097827472547, 0.4014620422781539, -0.27841911387256524, -0.342942648895296, 0.101209605359642, -0.28754830366445455, -0.08828069950922426, 0.20885067851836925, -0.08766916645728504,... |
1,801.01064 | Revealing the nature of excitons in liquid exfoliated monolayer WS2 | Transition metal dichalcogenides hold promise for applications in novel
optoelectronic devices. There is therefore a need for materials that can be
obtained in large quantities and with well understood optical properties. In
this report, we present a thorough photoluminescence (PL) investigations of
monolayer tungste... | cond-mat.mes-hall | transition metal dichalcogenides hold promise for applications in novel optoelectronic devices there is therefore a need for materials that can be obtained in large quantities and with well understood optical properties in this report we present a thorough photoluminescence pl investigations of monolayer tungsten disul... | [['transition', 'metal', 'dichalcogenides', 'hold', 'promise', 'for', 'applications', 'in', 'novel', 'optoelectronic', 'devices', 'there', 'is', 'therefore', 'a', 'need', 'for', 'materials', 'that', 'can', 'be', 'obtained', 'in', 'large', 'quantities', 'and', 'with', 'well', 'understood', 'optical', 'properties', 'in',... | [-0.08867869201989378, 0.2044546457526303, -0.033073338340618645, -0.008889967102441006, 0.03116705219144933, -0.14823048494639807, 0.08201056445686845, 0.4735907878354192, -0.24177497637923806, -0.2943933206656948, 0.010211640693596565, -0.33998778567183763, -0.12799680435680785, 0.21439332659327193, 0.024763979637064... |
1,801.01065 | Negative spin-Hall angle and anisotropic spin-orbit torques in epitaxial
IrMn | A spin-torque ferromagnetic resonance study is performed in epitaxial
$\mathrm{Fe / Ir_{15}Mn_{85}}$ bilayers with different Fe thicknesses. We
measure a negative spin-Hall angle of a few percent in the antiferromagnetic
IrMn in contrast to previously reported positive values. A large spin-orbit
field with Rashba sym... | cond-mat.mes-hall | a spintorque ferromagnetic resonance study is performed in epitaxial mathrmfe ir_15mn_85 bilayers with different fe thicknesses we measure a negative spinhall angle of a few percent in the antiferromagnetic irmn in contrast to previously reported positive values a large spinorbit field with rashba symmetry opposing the... | [['a', 'spintorque', 'ferromagnetic', 'resonance', 'study', 'is', 'performed', 'in', 'epitaxial', 'mathrmfe', 'ir_15mn_85', 'bilayers', 'with', 'different', 'fe', 'thicknesses', 'we', 'measure', 'a', 'negative', 'spinhall', 'angle', 'of', 'a', 'few', 'percent', 'in', 'the', 'antiferromagnetic', 'irmn', 'in', 'contrast'... | [-0.2281089491509604, 0.20918261955650347, 0.043083612565478345, 0.009133116704552382, -0.09355789493277387, -0.11746628196769447, 0.009772227795900038, 0.4606604699950384, -0.25788831156414915, -0.32390654169655636, -0.03497860369487789, -0.3118480246268072, -0.08359633720005458, 0.2065413749407766, 0.0816297767165486... |
1,801.01066 | Detection of additional Be+sdO systems from IUE spectroscopy | There is growing evidence that some Be stars were spun up through mass
transfer in a close binary system, leaving the former mass donor star as a hot,
stripped-down object. There are five known cases of Be stars with hot subdwarf
(sdO) companions that were discovered through International Ultraviolet
Explorer (IUE) s... | astro-ph.SR | there is growing evidence that some be stars were spun up through mass transfer in a close binary system leaving the former mass donor star as a hot strippeddown object there are five known cases of be stars with hot subdwarf sdo companions that were discovered through international ultraviolet explorer iue spectroscop... | [['there', 'is', 'growing', 'evidence', 'that', 'some', 'be', 'stars', 'were', 'spun', 'up', 'through', 'mass', 'transfer', 'in', 'a', 'close', 'binary', 'system', 'leaving', 'the', 'former', 'mass', 'donor', 'star', 'as', 'a', 'hot', 'strippeddown', 'object', 'there', 'are', 'five', 'known', 'cases', 'of', 'be', 'star... | [-0.06361362538221081, 0.13370202302890408, -0.07863102756461805, 0.08025169430170949, -0.11658963601803407, -0.11930586441039023, 0.07598528091330081, 0.42737438230869884, -0.14689555150405134, -0.37467337465337053, 0.08554578506498894, -0.3710154599182054, -0.06665856507606804, 0.23395173248983073, -0.053122469179801... |
1,801.01067 | Remnant radio-loud AGN in the Herschel-ATLAS field | Only a small fraction of observed Active Galactic Nuclei display large-scale
radio emission associated with jets, yet these radio-loud AGN have become
increasingly important in models of galaxy evolution. In determining the
dynamics and energetics of the radio sources over cosmic time, a key question
concerns what ha... | astro-ph.GA astro-ph.HE | only a small fraction of observed active galactic nuclei display largescale radio emission associated with jets yet these radioloud agn have become increasingly important in models of galaxy evolution in determining the dynamics and energetics of the radio sources over cosmic time a key question concerns what happens w... | [['only', 'a', 'small', 'fraction', 'of', 'observed', 'active', 'galactic', 'nuclei', 'display', 'largescale', 'radio', 'emission', 'associated', 'with', 'jets', 'yet', 'these', 'radioloud', 'agn', 'have', 'become', 'increasingly', 'important', 'in', 'models', 'of', 'galaxy', 'evolution', 'in', 'determining', 'the', 'd... | [-0.05930743037549523, 0.12450450498784217, -0.0521417833093152, 0.1384611701337146, -0.10828374918463513, -0.07865527311714329, 0.10076462913575061, 0.4658568672808435, -0.14152883527961369, -0.33636249847625677, 0.08940347899767279, -0.2923805923905913, -0.028936532292944177, 0.21099369563921308, -0.00431295573392109... |
1,801.01068 | Importance of charge capture in inter-phase regions during readout of
charge-coupled devices | The current understanding of charge transfer dynamics in Charge-Coupled
Devices (CCDs) is that charge is moved so quickly from one phase to the next in
a clocking sequence and with a density so low that trapping of charge in the
inter-phase regions is negligible. However, new simulation capabilities
developed at the ... | astro-ph.IM | the current understanding of charge transfer dynamics in chargecoupled devices ccds is that charge is moved so quickly from one phase to the next in a clocking sequence and with a density so low that trapping of charge in the interphase regions is negligible however new simulation capabilities developed at the centre f... | [['the', 'current', 'understanding', 'of', 'charge', 'transfer', 'dynamics', 'in', 'chargecoupled', 'devices', 'ccds', 'is', 'that', 'charge', 'is', 'moved', 'so', 'quickly', 'from', 'one', 'phase', 'to', 'the', 'next', 'in', 'a', 'clocking', 'sequence', 'and', 'with', 'a', 'density', 'so', 'low', 'that', 'trapping', '... | [-0.07578499187669642, 0.1350456448786098, -0.10760886420672931, 0.023366305481448222, -0.021968091430965286, -0.13274633787012446, 0.04847507517173475, 0.4075937769918537, -0.2514791702030318, -0.3311832626950156, 0.09944120831887575, -0.28700167356356066, -0.10185697854730798, 0.1997594003668455, -0.04221025469250109... |
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