id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,712.09901 | Remarks on multisymplectic reduction | The problem of reduction of multisymplectic manifolds by the action of Lie
groups is stated and discussed, as a previous step to give a fully covariant
scheme of reduction for classical field theories with symmetries.
| math-ph math.MP | the problem of reduction of multisymplectic manifolds by the action of lie groups is stated and discussed as a previous step to give a fully covariant scheme of reduction for classical field theories with symmetries | [['the', 'problem', 'of', 'reduction', 'of', 'multisymplectic', 'manifolds', 'by', 'the', 'action', 'of', 'lie', 'groups', 'is', 'stated', 'and', 'discussed', 'as', 'a', 'previous', 'step', 'to', 'give', 'a', 'fully', 'covariant', 'scheme', 'of', 'reduction', 'for', 'classical', 'field', 'theories', 'with', 'symmetries... | [-0.1786771803029946, 0.05742182247340679, -0.09602889389331852, 0.043609743156204264, -0.10904748971973147, -0.11746912003561322, 0.0018409752420016697, 0.3209192405853953, -0.245516423029559, -0.3117192479116576, 0.11302588772627392, -0.16839840324329478, -0.15634870012290775, 0.16483962096806085, -0.1291390114064727... |
1,712.09902 | Dynamics of open quantum systems by interpolation of von Neumann and
classical master equations, and its application to quantum annealing | We propose a method to interpolate dynamics of von Neumann and classical
master equations with an arbitrary mixing parameter to investigate the thermal
effects in quantum dynamics. The two dynamics are mixed by intervening to
continuously modify their solutions, thus coupling them indirectly instead of
directly intro... | quant-ph cond-mat.dis-nn | we propose a method to interpolate dynamics of von neumann and classical master equations with an arbitrary mixing parameter to investigate the thermal effects in quantum dynamics the two dynamics are mixed by intervening to continuously modify their solutions thus coupling them indirectly instead of directly introduci... | [['we', 'propose', 'a', 'method', 'to', 'interpolate', 'dynamics', 'of', 'von', 'neumann', 'and', 'classical', 'master', 'equations', 'with', 'an', 'arbitrary', 'mixing', 'parameter', 'to', 'investigate', 'the', 'thermal', 'effects', 'in', 'quantum', 'dynamics', 'the', 'two', 'dynamics', 'are', 'mixed', 'by', 'interven... | [-0.12830098444860571, 0.17163425366735516, -0.1254093238926121, 0.03254193464507822, -0.049559809969829734, -0.14013550534610295, 0.04613947904225989, 0.3373620727562595, -0.31991893008778816, -0.29078727389324477, 0.09018715027569604, -0.24634348823755084, -0.1366839548318438, 0.17713377547267153, 0.00101917319361100... |
1,712.09903 | Unimodular quantum gravity and the cosmological constant | It is shown that the one-loop effective action of unimodular gravity is the
same as that of ordinary gravity, restricted to unimodular metrics. The only
difference is in the treatment of the global scale degree of freedom and of the
cosmological term. A constant vacuum energy does not gravitate, addressing one
aspect... | gr-qc | it is shown that the oneloop effective action of unimodular gravity is the same as that of ordinary gravity restricted to unimodular metrics the only difference is in the treatment of the global scale degree of freedom and of the cosmological term a constant vacuum energy does not gravitate addressing one aspect of the... | [['it', 'is', 'shown', 'that', 'the', 'oneloop', 'effective', 'action', 'of', 'unimodular', 'gravity', 'is', 'the', 'same', 'as', 'that', 'of', 'ordinary', 'gravity', 'restricted', 'to', 'unimodular', 'metrics', 'the', 'only', 'difference', 'is', 'in', 'the', 'treatment', 'of', 'the', 'global', 'scale', 'degree', 'of',... | [-0.1896477625929963, 0.15064137009903789, -0.0850915270857513, 0.09699257305341266, -0.12041510651378255, -0.16317724978567608, -0.041174454103926554, 0.2677203399178229, -0.2552251344579354, -0.29674505749553964, 0.0817751458564185, -0.23428489042347983, -0.12519827400121772, 0.1144934581723391, -0.04812822675561173,... |
1,712.09904 | Analytic ground state wavefunctions of mean-field $p_x + ip_y$
superconductors with vortices and boundaries | We study Read and Green's mean-field model of the spinless $p_x+ip_y$
superconductor [N.Read and D.Green, Phys. Rev. B 61, 10267 (2000)] at a special
set of parameters where we find the analytic expressions for the topologically
degenerate ground states and the Majorana modes, including in finite systems
with edges a... | cond-mat.supr-con | we study read and greens meanfield model of the spinless p_xip_y superconductor nread and dgreen phys rev b 61 10267 2000 at a special set of parameters where we find the analytic expressions for the topologically degenerate ground states and the majorana modes including in finite systems with edges and in the presence... | [['we', 'study', 'read', 'and', 'greens', 'meanfield', 'model', 'of', 'the', 'spinless', 'p_xip_y', 'superconductor', 'nread', 'and', 'dgreen', 'phys', 'rev', 'b', '61', '10267', '2000', 'at', 'a', 'special', 'set', 'of', 'parameters', 'where', 'we', 'find', 'the', 'analytic', 'expressions', 'for', 'the', 'topologicall... | [-0.15007719517756335, 0.20823286238856267, -0.06931659186501866, 0.07045631201332941, -0.021567247747399328, -0.15696712989238618, 0.060027615546815745, 0.3018714465332501, -0.18034216440434608, -0.2811013536082338, 0.01882257575799367, -0.3009834016455621, -0.13270405332972904, 0.17538905038647656, 0.0372783364879939... |
1,712.09905 | Mean-field transport of a Bose-Einstein condensate | The expansion of an initially confined Bose-Einstein condensate into either
free space or a tilted optical lattice is investigated in a mean-field
approach. The effect of the interactions is to enhance or suppress the
transport depending on the sign and strength of the interactions. These effects
are discusses in det... | cond-mat.quant-gas | the expansion of an initially confined boseeinstein condensate into either free space or a tilted optical lattice is investigated in a meanfield approach the effect of the interactions is to enhance or suppress the transport depending on the sign and strength of the interactions these effects are discusses in detail in... | [['the', 'expansion', 'of', 'an', 'initially', 'confined', 'boseeinstein', 'condensate', 'into', 'either', 'free', 'space', 'or', 'a', 'tilted', 'optical', 'lattice', 'is', 'investigated', 'in', 'a', 'meanfield', 'approach', 'the', 'effect', 'of', 'the', 'interactions', 'is', 'to', 'enhance', 'or', 'suppress', 'the', '... | [-0.1731795853214158, 0.25273434387641064, -0.06977297989238475, 0.025485463541812234, 0.0005811773721248873, -0.11892336754188422, 0.014618454865300126, 0.35376607912081864, -0.28478514664475957, -0.23698206239890668, 0.03791479435336265, -0.3045352241475015, -0.09827566595988409, 0.1498299836211147, 0.058470231330683... |
1,712.09906 | Mode cooperation in two-dimensional plasmonic distributed-feedback laser | Plasmonic distributed-feedback lasers based on a two-dimensional periodic
array of metallic nanostructures are the main candidate for nanoscale sources
of coherent electromagnetic field. Strong localization of the electromagnetic
field and the large radiation surface are good opportunities for achieving an
ultrashort... | physics.optics | plasmonic distributedfeedback lasers based on a twodimensional periodic array of metallic nanostructures are the main candidate for nanoscale sources of coherent electromagnetic field strong localization of the electromagnetic field and the large radiation surface are good opportunities for achieving an ultrashort resp... | [['plasmonic', 'distributedfeedback', 'lasers', 'based', 'on', 'a', 'twodimensional', 'periodic', 'array', 'of', 'metallic', 'nanostructures', 'are', 'the', 'main', 'candidate', 'for', 'nanoscale', 'sources', 'of', 'coherent', 'electromagnetic', 'field', 'strong', 'localization', 'of', 'the', 'electromagnetic', 'field'... | [-0.19438398920227679, 0.16675839318300786, -0.043798917265399834, -0.0004323896416225376, -0.044030710194754054, -0.09590629818944299, 0.061943758028435845, 0.4118927216908077, -0.2600699909867681, -0.29939993008572074, 0.058250197553318186, -0.2623693626682863, -0.1615343347443648, 0.21743582987834756, 0.018430243810... |
1,712.09907 | Out-of-equilibrium dynamics driven by localized time-dependent
perturbations at quantum phase transitions | We investigate the quantum dynamics of many-body systems subject to local,
i.e. restricted to a limited space region, time-dependent perturbations. If the
perturbation drives the system across a quantum transition, an off-equilibrium
behavior is observed, even when the perturbation is very slow. We show that,
close t... | cond-mat.stat-mech | we investigate the quantum dynamics of manybody systems subject to local ie restricted to a limited space region timedependent perturbations if the perturbation drives the system across a quantum transition an offequilibrium behavior is observed even when the perturbation is very slow we show that close to the transiti... | [['we', 'investigate', 'the', 'quantum', 'dynamics', 'of', 'manybody', 'systems', 'subject', 'to', 'local', 'ie', 'restricted', 'to', 'a', 'limited', 'space', 'region', 'timedependent', 'perturbations', 'if', 'the', 'perturbation', 'drives', 'the', 'system', 'across', 'a', 'quantum', 'transition', 'an', 'offequilibrium... | [-0.15350920398180423, 0.2148137447035416, -0.11242141442683835, 0.0780018450888364, 0.0018462111577064845, -0.17249822745655188, 0.04483059636447905, 0.29661378688934636, -0.3027861275170979, -0.22645528206046214, 0.06439615428558011, -0.29594176034688163, -0.167195125109222, 0.16937907206776895, 0.022978743471628007,... |
1,712.09908 | Search for Deeply Bound Kaonic Nuclear States with AMADEUS | We briefly report on the search for Deeply Bound Kaonic Nuclear States with
AMADEUS in the Sigma0 p channel following K- absorption on 12C and outline
future perspectives for this work.
| nucl-ex | we briefly report on the search for deeply bound kaonic nuclear states with amadeus in the sigma0 p channel following k absorption on 12c and outline future perspectives for this work | [['we', 'briefly', 'report', 'on', 'the', 'search', 'for', 'deeply', 'bound', 'kaonic', 'nuclear', 'states', 'with', 'amadeus', 'in', 'the', 'sigma0', 'p', 'channel', 'following', 'k', 'absorption', 'on', '12c', 'and', 'outline', 'future', 'perspectives', 'for', 'this', 'work']] | [-0.04384171698362597, 0.20706431977751275, -0.07342948998144318, 0.03977379285084504, 0.004176625275924321, -0.1531317226228214, 0.13172904414034659, 0.36280842834422666, -0.1937970302608465, -0.26284443642643673, 0.024801122321326648, -0.33475477909368856, -0.05744009633218088, 0.17696195371418952, 0.1018031979760816... |
1,712.09909 | Properties of perturbations in beyond Horndeski theories | We study whether the approach of Deffayet et al. (DPSV) can be adopted for
obtaining a derivative part of quadratic action for scalar perturbations in
beyond Horndeski theories about homogeneous and isotropic backgrounds. We find
that even though the method does remove the second and higher derivatives of
metric pert... | hep-th | we study whether the approach of deffayet et al dpsv can be adopted for obtaining a derivative part of quadratic action for scalar perturbations in beyond horndeski theories about homogeneous and isotropic backgrounds we find that even though the method does remove the second and higher derivatives of metric perturbati... | [['we', 'study', 'whether', 'the', 'approach', 'of', 'deffayet', 'et', 'al', 'dpsv', 'can', 'be', 'adopted', 'for', 'obtaining', 'a', 'derivative', 'part', 'of', 'quadratic', 'action', 'for', 'scalar', 'perturbations', 'in', 'beyond', 'horndeski', 'theories', 'about', 'homogeneous', 'and', 'isotropic', 'backgrounds', '... | [-0.09880769192587902, 0.06195352158380395, -0.12018229743896766, 0.11197743137203593, -0.1293086983124785, -0.12205523901936063, 0.0027950161218425217, 0.2960536773514716, -0.22555626338308163, -0.2980898616617506, 0.04544943788688273, -0.2421011702415157, -0.23898877768202664, 0.16361299472764393, -0.0709404166901801... |
1,712.0991 | Surgery, Polygons and $SU(N)$-Floer Homology | Surgery exact triangles in various 3-manifold Floer homology theories provide
an important tool in studying and computing the relevant Floer homology groups.
These exact triangles relate the invariants of 3-manifolds, obtained by three
different Dehn surgeries on a fixed knot. In this paper, the behavior of
$SU(N)$-i... | math.GT math.DG | surgery exact triangles in various 3manifold floer homology theories provide an important tool in studying and computing the relevant floer homology groups these exact triangles relate the invariants of 3manifolds obtained by three different dehn surgeries on a fixed knot in this paper the behavior of suninstanton floe... | [['surgery', 'exact', 'triangles', 'in', 'various', '3manifold', 'floer', 'homology', 'theories', 'provide', 'an', 'important', 'tool', 'in', 'studying', 'and', 'computing', 'the', 'relevant', 'floer', 'homology', 'groups', 'these', 'exact', 'triangles', 'relate', 'the', 'invariants', 'of', '3manifolds', 'obtained', 'b... | [-0.259687272803756, 0.07950743543596796, -0.12809645303951603, 0.12789246043526858, -0.07194818786250251, -0.21278378015968705, -0.08462209697986144, 0.3576753843222221, -0.22491922466097958, -0.2834366160520543, 0.11963319140537404, -0.2666367501237967, -0.23698980935397185, 0.15159444407607517, -0.19368591510357647,... |
1,712.09911 | Membrane Stretching Elasticity of Lipid Vesicle and Thermal Shape
Fluctuations | One of the most widely used methods for determination of the bending
elasticity modulus of model lipid membranes is the analysis of the shape
fluctuations of nearly spherical lipid vesicles. The theoretical basis of this
analysis is given by Milner and Safran. In their theory the stretching effects
are not considered... | cond-mat.soft | one of the most widely used methods for determination of the bending elasticity modulus of model lipid membranes is the analysis of the shape fluctuations of nearly spherical lipid vesicles the theoretical basis of this analysis is given by milner and safran in their theory the stretching effects are not considered in ... | [['one', 'of', 'the', 'most', 'widely', 'used', 'methods', 'for', 'determination', 'of', 'the', 'bending', 'elasticity', 'modulus', 'of', 'model', 'lipid', 'membranes', 'is', 'the', 'analysis', 'of', 'the', 'shape', 'fluctuations', 'of', 'nearly', 'spherical', 'lipid', 'vesicles', 'the', 'theoretical', 'basis', 'of', '... | [-0.09556042262637574, 0.09306665062083791, -0.12834298061594987, 0.026381269254165493, 0.012959070296751128, -0.0806406583223078, -0.022945894094947208, 0.32561570902665454, -0.27287230786330635, -0.25119492983342046, 0.08083378944300218, -0.2388894885726687, -0.20150477023950467, 0.18689388088144673, -0.0435818250674... |
1,712.09912 | Optimal Covariance Change Point Localization in High Dimension | We study the problem of change point detection for covariance matrices in
high dimensions. We assume that we observe a sequence {X_i}_{i=1,...,n} of
independent and centered p-dimensional sub-Gaussian random vectors whose
covariance matrices are piecewise constant. Our task is to recover with high
accuracy the number... | math.ST stat.TH | we study the problem of change point detection for covariance matrices in high dimensions we assume that we observe a sequence x_i_i1n of independent and centered pdimensional subgaussian random vectors whose covariance matrices are piecewise constant our task is to recover with high accuracy the number and locations o... | [['we', 'study', 'the', 'problem', 'of', 'change', 'point', 'detection', 'for', 'covariance', 'matrices', 'in', 'high', 'dimensions', 'we', 'assume', 'that', 'we', 'observe', 'a', 'sequence', 'x_i_i1n', 'of', 'independent', 'and', 'centered', 'pdimensional', 'subgaussian', 'random', 'vectors', 'whose', 'covariance', 'm... | [-0.08612226318098559, 0.05933670222057927, -0.0488815334068681, 0.03492133104975754, -0.05807945324741455, -0.1330851576395186, 0.07981317840810669, 0.3692259551214454, -0.2708659945866508, -0.3061977724982086, 0.13725559224340658, -0.2559581590290978, -0.17178256762768274, 0.16761976215886593, -0.09632188869689248, 0... |
1,712.09913 | Visualizing the Loss Landscape of Neural Nets | Neural network training relies on our ability to find "good" minimizers of
highly non-convex loss functions. It is well-known that certain network
architecture designs (e.g., skip connections) produce loss functions that train
easier, and well-chosen training parameters (batch size, learning rate,
optimizer) produce ... | cs.LG cs.CV stat.ML | neural network training relies on our ability to find good minimizers of highly nonconvex loss functions it is wellknown that certain network architecture designs eg skip connections produce loss functions that train easier and wellchosen training parameters batch size learning rate optimizer produce minimizers that ge... | [['neural', 'network', 'training', 'relies', 'on', 'our', 'ability', 'to', 'find', 'good', 'minimizers', 'of', 'highly', 'nonconvex', 'loss', 'functions', 'it', 'is', 'wellknown', 'that', 'certain', 'network', 'architecture', 'designs', 'eg', 'skip', 'connections', 'produce', 'loss', 'functions', 'that', 'train', 'easi... | [-0.034269394380224014, 0.009591058332534222, -0.10097213703663135, 0.17504859471652848, -0.13656815663523916, -0.14994857012613738, 0.05583789785661102, 0.48924316835664483, -0.30810082943117534, -0.3261331944882761, 0.016506769207482952, -0.23951826178652308, -0.2897554802144096, 0.17251250201523521, -0.1195919991803... |
1,712.09914 | The quantum fate of black hole horizons | The presence of a horizon is the principal marker for black holes as they
appear in the classical theory of gravity. In General Relativity (GR), horizons
have several defining properties. First, there exists a static spherically
symmetric solution to vacuum Einstein equations which possesses a horizon
defined as a nu... | hep-th gr-qc | the presence of a horizon is the principal marker for black holes as they appear in the classical theory of gravity in general relativity gr horizons have several defining properties first there exists a static spherically symmetric solution to vacuum einstein equations which possesses a horizon defined as a nullsurfac... | [['the', 'presence', 'of', 'a', 'horizon', 'is', 'the', 'principal', 'marker', 'for', 'black', 'holes', 'as', 'they', 'appear', 'in', 'the', 'classical', 'theory', 'of', 'gravity', 'in', 'general', 'relativity', 'gr', 'horizons', 'have', 'several', 'defining', 'properties', 'first', 'there', 'exists', 'a', 'static', 's... | [-0.17666943939100882, 0.12624921217798987, -0.1104065013455477, 0.12174129141753333, -0.08012292547910302, -0.15372342771712552, -0.015805738734046892, 0.29099797774623665, -0.19701127770736263, -0.21556743887356586, 0.11715079700138799, -0.2897625434384854, -0.14790197349739848, 0.1925997053760242, -0.071320998660047... |
1,712.09915 | Field Studies with Multimedia Big Data: Opportunities and Challenges
(Extended Version) | Social multimedia users are increasingly sharing all kinds of data about the
world. They do this for their own reasons, not to provide data for field
studies-but the trend presents a great opportunity for scientists. The Yahoo
Flickr Creative Commons 100 Million (YFCC100M) dataset comprises 99 million
images and near... | cs.MM | social multimedia users are increasingly sharing all kinds of data about the world they do this for their own reasons not to provide data for field studiesbut the trend presents a great opportunity for scientists the yahoo flickr creative commons 100 million yfcc100m dataset comprises 99 million images and nearly 800 t... | [['social', 'multimedia', 'users', 'are', 'increasingly', 'sharing', 'all', 'kinds', 'of', 'data', 'about', 'the', 'world', 'they', 'do', 'this', 'for', 'their', 'own', 'reasons', 'not', 'to', 'provide', 'data', 'for', 'field', 'studiesbut', 'the', 'trend', 'presents', 'a', 'great', 'opportunity', 'for', 'scientists', ... | [-0.06691387349860463, 0.044237558425450525, -0.06993791991249568, 0.09258239840321887, -0.16852728270311118, -0.15335156385965393, 0.0640383298737277, 0.40673514798063, -0.26904697931560695, -0.3946766894051623, 0.0965914576497328, -0.33468531851509686, -0.13044895087736413, 0.24053870506091848, -0.08834152947586114, ... |
1,712.09916 | A ReRAM Physically Unclonable Function (ReRAM PUF)-based Approach to
Enhance Authentication Security in Software Defined Wireless Networks | The exponentially increasing number of ubiquitous wireless devices connected
to the Internet in Internet of Things (IoT) networks highlights the need for a
new paradigm of data flow management in such large-scale networks under
software defined wireless networking (SDWN). The limited power and computation
capability ... | cs.CR cs.NI | the exponentially increasing number of ubiquitous wireless devices connected to the internet in internet of things iot networks highlights the need for a new paradigm of data flow management in such largescale networks under software defined wireless networking sdwn the limited power and computation capability availabl... | [['the', 'exponentially', 'increasing', 'number', 'of', 'ubiquitous', 'wireless', 'devices', 'connected', 'to', 'the', 'internet', 'in', 'internet', 'of', 'things', 'iot', 'networks', 'highlights', 'the', 'need', 'for', 'a', 'new', 'paradigm', 'of', 'data', 'flow', 'management', 'in', 'such', 'largescale', 'networks', ... | [-0.22881138810683324, -0.014184245996699301, -0.015539145728601425, 0.03642547052401245, -0.043080447523882896, -0.225677077677877, 0.070653516135115, 0.37534702470469655, -0.2718993909220444, -0.29039630972582736, 0.12358253743017981, -0.2325162718748977, -0.17477743651463903, 0.2396966529089365, -0.17111823125378578... |
1,712.09917 | Cosmic Microwave Background Dipole Asymmetry could be explained by Axion
Monodromy Cosmic Strings | Observations by the Wilkinson Microwave Anisotropy Probe and the Planck
mission suggest a hemispherical power amplitude asymmetry in the cosmic
microwave background, with a correlation length on the order of the size of the
observable Universe. We find that this anomaly can be naturally explained by an
axion-like par... | astro-ph.CO gr-qc hep-ph hep-th | observations by the wilkinson microwave anisotropy probe and the planck mission suggest a hemispherical power amplitude asymmetry in the cosmic microwave background with a correlation length on the order of the size of the observable universe we find that this anomaly can be naturally explained by an axionlike particle... | [['observations', 'by', 'the', 'wilkinson', 'microwave', 'anisotropy', 'probe', 'and', 'the', 'planck', 'mission', 'suggest', 'a', 'hemispherical', 'power', 'amplitude', 'asymmetry', 'in', 'the', 'cosmic', 'microwave', 'background', 'with', 'a', 'correlation', 'length', 'on', 'the', 'order', 'of', 'the', 'size', 'of', ... | [-0.13167028323254618, 0.25066865783939785, -0.08918182727325638, 0.1419492113901387, -0.08923301551383266, -0.09392004146833312, -0.01086142339430026, 0.3044653503303147, -0.2639951886309018, -0.35643025910989806, 0.06430373728238739, -0.254678295657793, -0.03840757390457275, 0.15324993984877663, 0.02312243629385494, ... |
1,712.09918 | Effective description of domain wall strings | The analysis of domain wall dynamics is often simplified to one dimensional
physics. For domain walls in thin films, more realistic approaches require the
description as two dimensional objects. This includes the study of vortices and
curvatures along the domain walls as well as the influence of boundary effects.
Her... | cond-mat.mes-hall | the analysis of domain wall dynamics is often simplified to one dimensional physics for domain walls in thin films more realistic approaches require the description as two dimensional objects this includes the study of vortices and curvatures along the domain walls as well as the influence of boundary effects here we p... | [['the', 'analysis', 'of', 'domain', 'wall', 'dynamics', 'is', 'often', 'simplified', 'to', 'one', 'dimensional', 'physics', 'for', 'domain', 'walls', 'in', 'thin', 'films', 'more', 'realistic', 'approaches', 'require', 'the', 'description', 'as', 'two', 'dimensional', 'objects', 'this', 'includes', 'the', 'study', 'of... | [-0.12175285746259075, 0.11155781628611663, -0.10696564315129882, 0.06571851816514264, -0.11002190323357565, -0.08434900002000664, 0.015220316668526957, 0.39195112947482563, -0.2288211581699611, -0.3046402105440696, 0.12485632010350894, -0.22795829575509255, -0.13076997562851486, 0.1998479899569023, 0.01735837183609281... |
1,712.09919 | Dynamical Dark Matter from Thermal Freeze-Out | In the Dynamical Dark Matter (DDM) framework, the dark sector comprises a
large number of constituent dark particles whose individual masses, lifetimes,
and cosmological abundances obey specific scaling relations with respect to
each other. In particular, the most natural versions of this framework tend to
require a ... | hep-ph astro-ph.CO | in the dynamical dark matter ddm framework the dark sector comprises a large number of constituent dark particles whose individual masses lifetimes and cosmological abundances obey specific scaling relations with respect to each other in particular the most natural versions of this framework tend to require a spectrum ... | [['in', 'the', 'dynamical', 'dark', 'matter', 'ddm', 'framework', 'the', 'dark', 'sector', 'comprises', 'a', 'large', 'number', 'of', 'constituent', 'dark', 'particles', 'whose', 'individual', 'masses', 'lifetimes', 'and', 'cosmological', 'abundances', 'obey', 'specific', 'scaling', 'relations', 'with', 'respect', 'to'... | [-0.041759146147847384, 0.21722978885669295, -0.09393589564866421, 0.07237364969828546, -0.08392072198330425, -0.10141696696896192, -0.011459156676546964, 0.34958029272793617, -0.21856131214762745, -0.37476533661619116, 0.02328288438729942, -0.24675059127535118, -0.029993502166622353, 0.1674826945160964, 0.004825822146... |
1,712.0992 | Quantification of coarse-graining error in Langevin and overdamped
Langevin dynamics | In molecular dynamics and sampling of high dimensional Gibbs measures
coarse-graining is an important technique to reduce the dimensionality of the
problem. We will study and quantify the coarse-graining error between the
coarse-grained dynamics and an effective dynamics. The effective dynamics is a
Markov process on... | math.AP | in molecular dynamics and sampling of high dimensional gibbs measures coarsegraining is an important technique to reduce the dimensionality of the problem we will study and quantify the coarsegraining error between the coarsegrained dynamics and an effective dynamics the effective dynamics is a markov process on the co... | [['in', 'molecular', 'dynamics', 'and', 'sampling', 'of', 'high', 'dimensional', 'gibbs', 'measures', 'coarsegraining', 'is', 'an', 'important', 'technique', 'to', 'reduce', 'the', 'dimensionality', 'of', 'the', 'problem', 'we', 'will', 'study', 'and', 'quantify', 'the', 'coarsegraining', 'error', 'between', 'the', 'co... | [-0.08794784874865605, 0.11598940781949486, -0.1572209896009055, 0.12085977033954012, 0.012065155331173071, -0.08752844030705971, 0.03149942035276082, 0.3272323204925464, -0.3271571291280129, -0.2761598268463727, 0.044899994286806175, -0.24662231351448421, -0.1252257088800111, 0.16527230575710775, -0.05758662564649938,... |
1,712.09921 | Holographic CBK Relation | The Crewther-Broadhurst-Kataev (CBK) relation connects the Bjorken function
for deep-inelastic sum rules (or the Gross - Llewellyn Smith function) with the
Adler function for electron-positron annihilation in QCD; it has been checked
to hold up to four loops in perturbation theory. Here we study non-perturbative
term... | hep-th hep-ph | the crewtherbroadhurstkataev cbk relation connects the bjorken function for deepinelastic sum rules or the gross llewellyn smith function with the adler function for electronpositron annihilation in qcd it has been checked to hold up to four loops in perturbation theory here we study nonperturbative terms in the cbk re... | [['the', 'crewtherbroadhurstkataev', 'cbk', 'relation', 'connects', 'the', 'bjorken', 'function', 'for', 'deepinelastic', 'sum', 'rules', 'or', 'the', 'gross', 'llewellyn', 'smith', 'function', 'with', 'the', 'adler', 'function', 'for', 'electronpositron', 'annihilation', 'in', 'qcd', 'it', 'has', 'been', 'checked', 't... | [-0.10107754977975636, 0.12558344781837533, -0.14781470967167126, 0.1889740094530764, -0.0698646751287229, -0.05291071396023661, 0.02748718229905084, 0.32627616783588376, -0.203966524581104, -0.20855640867400227, 0.013631839508644673, -0.3090074773517852, -0.11070069394606565, 0.1436559173783303, 0.043359572686129756, ... |
1,712.09922 | Low-Scale Seesaw and the CP Violation in Neutrino Oscillations | We consider a version of the low-scale type I seesaw mechanism for generating
small neutrino masses, as an alternative to the standard seesaw scenario. It
involves two right-handed (RH) neutrinos $\nu_{1R}$ and $\nu_{2R}$ having a
Majorana mass term with mass $M$, which conserves the lepton charge $L$. The RH
neutrin... | hep-ph | we consider a version of the lowscale type i seesaw mechanism for generating small neutrino masses as an alternative to the standard seesaw scenario it involves two righthanded rh neutrinos nu_1r and nu_2r having a majorana mass term with mass m which conserves the lepton charge l the rh neutrino nu_2r has leptoncharge... | [['we', 'consider', 'a', 'version', 'of', 'the', 'lowscale', 'type', 'i', 'seesaw', 'mechanism', 'for', 'generating', 'small', 'neutrino', 'masses', 'as', 'an', 'alternative', 'to', 'the', 'standard', 'seesaw', 'scenario', 'it', 'involves', 'two', 'righthanded', 'rh', 'neutrinos', 'nu_1r', 'and', 'nu_2r', 'having', 'a'... | [-0.15624343347008107, 0.3091069480380139, 0.07066819411529987, 0.19445438270836515, -0.0936209787851786, -0.2123980771478576, 0.03258949413861113, 0.28759589271309477, -0.20652654264941467, -0.3524657927811387, 0.03231590873285852, -0.26834256135798235, -0.0027063658096637853, 0.09997319659817515, 0.04868654999396919,... |
1,712.09923 | What do we need to build explainable AI systems for the medical domain? | Artificial intelligence (AI) generally and machine learning (ML) specifically
demonstrate impressive practical success in many different application domains,
e.g. in autonomous driving, speech recognition, or recommender systems. Deep
learning approaches, trained on extremely large data sets or using
reinforcement le... | cs.AI stat.ML | artificial intelligence ai generally and machine learning ml specifically demonstrate impressive practical success in many different application domains eg in autonomous driving speech recognition or recommender systems deep learning approaches trained on extremely large data sets or using reinforcement learning method... | [['artificial', 'intelligence', 'ai', 'generally', 'and', 'machine', 'learning', 'ml', 'specifically', 'demonstrate', 'impressive', 'practical', 'success', 'in', 'many', 'different', 'application', 'domains', 'eg', 'in', 'autonomous', 'driving', 'speech', 'recognition', 'or', 'recommender', 'systems', 'deep', 'learning... | [-0.058587194749686336, 0.035466685735757765, -0.060878071514889595, 0.10119271424212327, -0.15534795928979292, -0.1552668033217612, 0.05013419066921675, 0.4349913633357833, -0.2504703068989329, -0.3222416715174664, 0.14099071729412702, -0.27214867509236296, -0.18631601874450487, 0.23327346667314747, -0.176657202468985... |
1,712.09924 | Superluminal plasmons with resonant gain in population inverted bilayer
graphene | AB-stacked bilayer graphene with a tunable electronic bandgap in excess of
the optical phonon energy presents an interesting active medium, and we
consider such theoretical possibility in this work. We argue the possibility of
a highly resonant optical gain in the vicinity of the asymmetry gap. Associated
with this r... | cond-mat.mes-hall | abstacked bilayer graphene with a tunable electronic bandgap in excess of the optical phonon energy presents an interesting active medium and we consider such theoretical possibility in this work we argue the possibility of a highly resonant optical gain in the vicinity of the asymmetry gap associated with this resonan... | [['abstacked', 'bilayer', 'graphene', 'with', 'a', 'tunable', 'electronic', 'bandgap', 'in', 'excess', 'of', 'the', 'optical', 'phonon', 'energy', 'presents', 'an', 'interesting', 'active', 'medium', 'and', 'we', 'consider', 'such', 'theoretical', 'possibility', 'in', 'this', 'work', 'we', 'argue', 'the', 'possibility'... | [-0.19619472721672576, 0.19964094741790442, -0.01335296530843429, 0.005902588040149514, -0.09453987959853333, -0.14889599899828865, 0.08067757484262246, 0.47557042398746463, -0.27002096650582075, -0.28974314522592054, -0.04125978175948873, -0.3262695522196051, -0.2012196100195465, 0.1832816050104473, 0.0165054011158645... |
1,712.09925 | Fourier transform on high-dimensional unitary groups with applications
to random tilings | A combination of direct and inverse Fourier transforms on the unitary group
$U(N)$ identifies normalized characters with probability measures on $N$-tuples
of integers. We develop the $N\to\infty$ version of this correspondence by
matching the asymptotics of partial derivatives at the identity of logarithm of
charact... | math.PR math-ph math.FA math.MP math.RT | a combination of direct and inverse fourier transforms on the unitary group un identifies normalized characters with probability measures on ntuples of integers we develop the ntoinfty version of this correspondence by matching the asymptotics of partial derivatives at the identity of logarithm of characters with law o... | [['a', 'combination', 'of', 'direct', 'and', 'inverse', 'fourier', 'transforms', 'on', 'the', 'unitary', 'group', 'un', 'identifies', 'normalized', 'characters', 'with', 'probability', 'measures', 'on', 'ntuples', 'of', 'integers', 'we', 'develop', 'the', 'ntoinfty', 'version', 'of', 'this', 'correspondence', 'by', 'ma... | [-0.160099451494452, 0.09985832421596334, -0.10433013142732482, 0.0727829841038798, -0.03707081396057601, -0.08226307474767729, 0.06885768248016134, 0.29085852922270855, -0.26903285379070907, -0.22481269468252937, 0.125644425334852, -0.30390532143346427, -0.15353844574682654, 0.14585150187955268, -0.08276027400279418, ... |
1,712.09926 | Rapid Adaptation with Conditionally Shifted Neurons | We describe a mechanism by which artificial neural networks can learn rapid
adaptation - the ability to adapt on the fly, with little data, to new tasks -
that we call conditionally shifted neurons. We apply this mechanism in the
framework of metalearning, where the aim is to replicate some of the
flexibility of huma... | cs.LG cs.NE stat.ML | we describe a mechanism by which artificial neural networks can learn rapid adaptation the ability to adapt on the fly with little data to new tasks that we call conditionally shifted neurons we apply this mechanism in the framework of metalearning where the aim is to replicate some of the flexibility of human learning... | [['we', 'describe', 'a', 'mechanism', 'by', 'which', 'artificial', 'neural', 'networks', 'can', 'learn', 'rapid', 'adaptation', 'the', 'ability', 'to', 'adapt', 'on', 'the', 'fly', 'with', 'little', 'data', 'to', 'new', 'tasks', 'that', 'we', 'call', 'conditionally', 'shifted', 'neurons', 'we', 'apply', 'this', 'mechan... | [-0.01699635935341464, 0.10248604471015992, -0.05975961172953248, 0.04753600473768715, -0.172335596674369, -0.21041583795366542, 0.08273524015058516, 0.46974294225932384, -0.29490156589570093, -0.29267237930824713, 0.027359364601802463, -0.21562882325593002, -0.23239005775171884, 0.21388977787538185, -0.167064854685141... |
1,712.09927 | Fujita's Freeness Conjecture for $T$-Varieties of Complexity One | We prove Fujita's freeness conjecture for Gorenstein complexity-one
$T$-varieties with rational singularities.
| math.AG | we prove fujitas freeness conjecture for gorenstein complexityone tvarieties with rational singularities | [['we', 'prove', 'fujitas', 'freeness', 'conjecture', 'for', 'gorenstein', 'complexityone', 'tvarieties', 'with', 'rational', 'singularities']] | [-0.30799300968647003, -0.20645409643960497, -0.18876160743335882, 0.2184682252506415, -0.055961826195319496, -0.41797566289703053, -0.16073762873808542, 0.3403876672188441, -0.3686641063541174, -0.016378908573339384, 0.038793160230852664, -0.2532500748638995, -0.21148483796666065, 0.11825213953852654, -0.3986149582390... |
1,712.09928 | Critical loci for Higgs bundles | The paper studies the locus in the rank 2 Higgs bundle moduli space
corresponding to points which are critical for d of the Poisson commuting
functions. These correspond to the Higgs field vanishing on a divisor of degree
D. The degree D critical locus has an induced integrable system related to
K(-D)-twisted Higgs b... | math.DG math.AG | the paper studies the locus in the rank 2 higgs bundle moduli space corresponding to points which are critical for d of the poisson commuting functions these correspond to the higgs field vanishing on a divisor of degree d the degree d critical locus has an induced integrable system related to kdtwisted higgs bundles t... | [['the', 'paper', 'studies', 'the', 'locus', 'in', 'the', 'rank', '2', 'higgs', 'bundle', 'moduli', 'space', 'corresponding', 'to', 'points', 'which', 'are', 'critical', 'for', 'd', 'of', 'the', 'poisson', 'commuting', 'functions', 'these', 'correspond', 'to', 'the', 'higgs', 'field', 'vanishing', 'on', 'a', 'divisor',... | [-0.24519803348396504, 0.11909207480978996, -0.04952756937829748, 0.07406187582287997, -0.07432665842925272, -0.18917746538118946, 0.01381241750629944, 0.2911856195165051, -0.2875237758567054, -0.1618161669503602, 0.059766417212178194, -0.2694571576569052, -0.17069387669482874, 0.14770077519296182, -0.09205979723778981... |
1,712.09929 | On the Challenges of Detecting Rude Conversational Behaviour | In this study, we aim to identify moments of rudeness between two
individuals. In particular, we segment all occurrences of rudeness in
conversations into three broad, distinct categories and try to identify each.
We show how machine learning algorithms can be used to identify rudeness based
on acoustic and semantic ... | cs.HC cs.CL | in this study we aim to identify moments of rudeness between two individuals in particular we segment all occurrences of rudeness in conversations into three broad distinct categories and try to identify each we show how machine learning algorithms can be used to identify rudeness based on acoustic and semantic signals... | [['in', 'this', 'study', 'we', 'aim', 'to', 'identify', 'moments', 'of', 'rudeness', 'between', 'two', 'individuals', 'in', 'particular', 'we', 'segment', 'all', 'occurrences', 'of', 'rudeness', 'in', 'conversations', 'into', 'three', 'broad', 'distinct', 'categories', 'and', 'try', 'to', 'identify', 'each', 'we', 'sho... | [-0.07825269644263755, 0.03494953062762035, -0.06234696348919795, 0.11007063497993258, -0.1189333529923153, -0.12524922719497358, 0.07659461674688572, 0.4670145769048943, -0.2673078085808607, -0.3078906334559904, 0.05681918137392887, -0.28625956305375927, -0.20579606890966173, 0.152522106968871, -0.13374000199379796, 0... |
1,712.0993 | On the regularity of solutions to the Moore-Gibson-Thompson equation: a
perspective via wave equations with memory | We undertake a regularity analysis of the solutions to initial/boundary value
problems for the (third-order in time) Moore-Gibson-Thompson (MGT) equation.
The key to the present investigation is that the MGT equation falls within a
large class of systems with memory, with affine term depending on a parameter.
For thi... | math.AP | we undertake a regularity analysis of the solutions to initialboundary value problems for the thirdorder in time mooregibsonthompson mgt equation the key to the present investigation is that the mgt equation falls within a large class of systems with memory with affine term depending on a parameter for this model equat... | [['we', 'undertake', 'a', 'regularity', 'analysis', 'of', 'the', 'solutions', 'to', 'initialboundary', 'value', 'problems', 'for', 'the', 'thirdorder', 'in', 'time', 'mooregibsonthompson', 'mgt', 'equation', 'the', 'key', 'to', 'the', 'present', 'investigation', 'is', 'that', 'the', 'mgt', 'equation', 'falls', 'within'... | [-0.12903783118253517, 0.044612619926391, -0.1038208690634223, 0.04449900552686868, -0.10630752622206328, -0.11326397782699628, 0.0007743656473008521, 0.29339842829063084, -0.29162349021344475, -0.2508961392312565, 0.1726694227721909, -0.2679456206885251, -0.13793070317725792, 0.20012689976614306, -0.03981411297466945,... |
1,712.09931 | Top and Higgs: Recent Theory developments | I review recent theory developments in the computation of Higgs production in
association with top quarks, as well as the modelling of the corresponding
backgrounds. In addition to progress within the Standard model I discuss
higher-order corrections for the $t\bar{t}H$ process in the presence of new
interactions.
| hep-ph | i review recent theory developments in the computation of higgs production in association with top quarks as well as the modelling of the corresponding backgrounds in addition to progress within the standard model i discuss higherorder corrections for the tbarth process in the presence of new interactions | [['i', 'review', 'recent', 'theory', 'developments', 'in', 'the', 'computation', 'of', 'higgs', 'production', 'in', 'association', 'with', 'top', 'quarks', 'as', 'well', 'as', 'the', 'modelling', 'of', 'the', 'corresponding', 'backgrounds', 'in', 'addition', 'to', 'progress', 'within', 'the', 'standard', 'model', 'i', ... | [-0.024922009720962417, 0.12226295394654524, -0.014573355479056927, 0.09044454895360723, -0.02051535697574628, -0.09476046377119232, 0.03032344667627377, 0.30424306466382867, -0.23776721146869215, -0.2863623152011411, 0.06686200699868038, -0.30882484186440706, -0.09476941023418244, 0.12115464358035713, -0.0026844156889... |
1,712.09932 | Equivariant D-modules on binary cubic forms | We consider the space X = Sym^3(C^2) of binary cubic forms, equipped with the
natural action of the group GL_2 of invertible linear transformations of C^2.
We describe explicitly the category of GL_2-equivariant coherent D_X-modules as
the category of representations of a quiver with relations. We show moreover
that ... | math.AC math.AG math.RT | we consider the space x sym3c2 of binary cubic forms equipped with the natural action of the group gl_2 of invertible linear transformations of c2 we describe explicitly the category of gl_2equivariant coherent d_xmodules as the category of representations of a quiver with relations we show moreover that this quiver is... | [['we', 'consider', 'the', 'space', 'x', 'sym3c2', 'of', 'binary', 'cubic', 'forms', 'equipped', 'with', 'the', 'natural', 'action', 'of', 'the', 'group', 'gl_2', 'of', 'invertible', 'linear', 'transformations', 'of', 'c2', 'we', 'describe', 'explicitly', 'the', 'category', 'of', 'gl_2equivariant', 'coherent', 'd_xmodu... | [-0.17883071738897877, 0.07191149425617528, -0.08144473281058975, 0.055541110969166835, -0.10717232883268711, -0.10082881129118522, 0.003454286796862588, 0.3775286264261048, -0.3426243596911138, -0.21521928357690864, 0.09254046226395111, -0.20720871506423197, -0.20090061888457092, 0.17753228598146462, -0.12262320834341... |
1,712.09933 | The Hyperbolic Asymptotics of Elliptic Hypergeometric Integrals Arising
in Supersymmetric Gauge Theory | The purpose of this article is to demonstrate that i) the framework of
elliptic hypergeometric integrals (EHIs) can be extended by input from
supersymmetric gauge theory, and ii) analyzing the hyperbolic limit of the EHIs
in the extended framework leads to a rich structure containing sharp
mathematical problems of in... | math-ph math.CA math.MP math.QA | the purpose of this article is to demonstrate that i the framework of elliptic hypergeometric integrals ehis can be extended by input from supersymmetric gauge theory and ii analyzing the hyperbolic limit of the ehis in the extended framework leads to a rich structure containing sharp mathematical problems of interest ... | [['the', 'purpose', 'of', 'this', 'article', 'is', 'to', 'demonstrate', 'that', 'i', 'the', 'framework', 'of', 'elliptic', 'hypergeometric', 'integrals', 'ehis', 'can', 'be', 'extended', 'by', 'input', 'from', 'supersymmetric', 'gauge', 'theory', 'and', 'ii', 'analyzing', 'the', 'hyperbolic', 'limit', 'of', 'the', 'ehi... | [-0.06752666394390604, 0.09972416507182917, -0.09330245716332951, 0.07606392071842599, -0.12671262629686253, -0.14484122545622727, 0.00434893749667989, 0.31814804721404527, -0.20591063033583956, -0.2969816459726323, 0.08547641674817628, -0.2744491954388864, -0.18363402444532873, 0.15206562080968392, -0.1518348278943449... |
1,712.09934 | Improving the theoretical prediction for the $B_s-\bar{B}_s$ width
difference: matrix elements of next-to-leading order $\Delta B=2$ operators | We present lattice QCD results for the matrix elements of $R_2$ and other
dimension-7, $\Delta B = 2$ operators relevant for calculations of $\Delta
\Gamma_s$, the $B_s-\bar{B}_s$ width difference. We have computed correlation
functions using 5 ensembles of the MILC Collaboration's 2+1+1-flavour gauge
field configura... | hep-lat hep-ph | we present lattice qcd results for the matrix elements of r_2 and other dimension7 delta b 2 operators relevant for calculations of delta gamma_s the b_sbarb_s width difference we have computed correlation functions using 5 ensembles of the milc collaborations 211flavour gauge field configurations spanning 3 lattice sp... | [['we', 'present', 'lattice', 'qcd', 'results', 'for', 'the', 'matrix', 'elements', 'of', 'r_2', 'and', 'other', 'dimension7', 'delta', 'b', '2', 'operators', 'relevant', 'for', 'calculations', 'of', 'delta', 'gamma_s', 'the', 'b_sbarb_s', 'width', 'difference', 'we', 'have', 'computed', 'correlation', 'functions', 'us... | [-0.06333410601160422, 0.3141360825129314, -0.08405027577183065, 0.12626801530912174, 0.00973040535421946, -0.10355754528847552, 0.11654879057482269, 0.39650509641841825, -0.1851352518904455, -0.25175518240088346, 0.0408573768644104, -0.3560081905704568, -0.0008368278114297955, 0.10003405981265086, 0.04810833255490336,... |
1,712.09935 | Recurrence of singularities for second order isotropic
pseudodifferential operators | Let $H$ be a self-adjoint isotropic elliptic pseudodifferential operator of
order $2$. Denote by $u(t)$ the solution of the Schr\"odinger equation
$(i\partial_t - H)u = 0$ with initial data $u(0) = u_0$. If $u_0$ is compactly
supported the solution $u(t)$ is smooth for small $t > 0$, but not for all $t$.
We determine... | math.AP math-ph math.MP | let h be a selfadjoint isotropic elliptic pseudodifferential operator of order 2 denote by ut the solution of the schrodinger equation ipartial_t hu 0 with initial data u0 u_0 if u_0 is compactly supported the solution ut is smooth for small t 0 but not for all t we determine the wavefront set of ut in terms of the wav... | [['let', 'h', 'be', 'a', 'selfadjoint', 'isotropic', 'elliptic', 'pseudodifferential', 'operator', 'of', 'order', '2', 'denote', 'by', 'ut', 'the', 'solution', 'of', 'the', 'schrodinger', 'equation', 'ipartial_t', 'hu', '0', 'with', 'initial', 'data', 'u0', 'u_0', 'if', 'u_0', 'is', 'compactly', 'supported', 'the', 'so... | [-0.20273978101469997, 0.10499776346267949, -0.006053540924511535, -0.04687361156528579, -0.07454191428333731, -0.18988313083208994, -0.092657792873838, 0.3033607098942911, -0.34800698198902774, -0.16821940434755575, 0.15891584629212624, -0.3720046713108748, -0.04448634278501423, 0.1579656604756142, -0.0399212606093833... |
1,712.09936 | Gradient Regularization Improves Accuracy of Discriminative Models | Regularizing the gradient norm of the output of a neural network with respect
to its inputs is a powerful technique, rediscovered several times. This paper
presents evidence that gradient regularization can consistently improve
classification accuracy on vision tasks, using modern deep neural networks,
especially whe... | cs.LG | regularizing the gradient norm of the output of a neural network with respect to its inputs is a powerful technique rediscovered several times this paper presents evidence that gradient regularization can consistently improve classification accuracy on vision tasks using modern deep neural networks especially when the ... | [['regularizing', 'the', 'gradient', 'norm', 'of', 'the', 'output', 'of', 'a', 'neural', 'network', 'with', 'respect', 'to', 'its', 'inputs', 'is', 'a', 'powerful', 'technique', 'rediscovered', 'several', 'times', 'this', 'paper', 'presents', 'evidence', 'that', 'gradient', 'regularization', 'can', 'consistently', 'imp... | [-0.03270549606784935, -0.006248652636397468, -0.07424973598561178, 0.08337195657909631, -0.09790028279657355, -0.12815320839771352, 0.02889128948268278, 0.44944383216130995, -0.28794043721712154, -0.31558741952872166, 0.09863507083197043, -0.2581274159981505, -0.23048575843036498, 0.22503282826231874, -0.1704379593163... |
1,712.09937 | On the Supersymmetrization of Galileon Theories in Four Dimensions | We use on-shell amplitude techniques to study the possible $\mathcal{N}=1$
supersymmetrizations of Galileon theories in 3+1 dimensions, both in the limit
of decoupling from DBI and without. Our results are that (1) the quartic
Galileon has a supersymmetrization compatible with Galileon shift symmetry
($\phi \to \phi ... | hep-th | we use onshell amplitude techniques to study the possible mathcaln1 supersymmetrizations of galileon theories in 31 dimensions both in the limit of decoupling from dbi and without our results are that 1 the quartic galileon has a supersymmetrization compatible with galileon shift symmetry phi to phi c b_mu xmu for the ... | [['we', 'use', 'onshell', 'amplitude', 'techniques', 'to', 'study', 'the', 'possible', 'mathcaln1', 'supersymmetrizations', 'of', 'galileon', 'theories', 'in', '31', 'dimensions', 'both', 'in', 'the', 'limit', 'of', 'decoupling', 'from', 'dbi', 'and', 'without', 'our', 'results', 'are', 'that', '1', 'the', 'quartic', '... | [-0.185802820562615, 0.16282609947854695, -0.0417821475500126, 0.10803386423432118, -0.17815968163173507, -0.21087776697930638, -0.06678555612768518, 0.3126007038065129, -0.16403163342311242, -0.2485213267536443, 0.05509521230088006, -0.29423348919666703, -0.17569841923663554, 0.09874275258460577, 0.01365084819967088, ... |
1,712.09938 | Homological invariants of determinantal thickenings | The study of homological invariants such as Tor, Ext and local cohomology
modules constitutes an important direction in commutative algebra. Explicit
descriptions of these invariants are notoriously difficult to find and often
involve combining an array of techniques from other fields of mathematics. In
recent years ... | math.AC math.AG | the study of homological invariants such as tor ext and local cohomology modules constitutes an important direction in commutative algebra explicit descriptions of these invariants are notoriously difficult to find and often involve combining an array of techniques from other fields of mathematics in recent years tools... | [['the', 'study', 'of', 'homological', 'invariants', 'such', 'as', 'tor', 'ext', 'and', 'local', 'cohomology', 'modules', 'constitutes', 'an', 'important', 'direction', 'in', 'commutative', 'algebra', 'explicit', 'descriptions', 'of', 'these', 'invariants', 'are', 'notoriously', 'difficult', 'to', 'find', 'and', 'often... | [-0.11983593494391465, 0.00439869519719981, -0.12481314964554828, 0.1075617577128037, -0.11718242491990553, -0.1186271518412413, -0.05096933202032527, 0.35866036708231525, -0.3228304452366299, -0.3078187403052744, 0.15981000213592192, -0.2552980016023297, -0.20051841462275596, 0.24251928804160067, -0.14860606556193848,... |
1,712.09939 | Solving an Integral Equation Eigenvalue Problem via a New Domain
Decomposition Method and Hierarchical Matrices | In this paper the author introduces a new domain decomposition method for the
solution of discretised integral equation eigenvalue problems. The new domain
decomposition method is motivated by the so-called automated multi-level
substructuring (short AMLS) method. The AMLS method is a domain decomposition
method for ... | math.NA | in this paper the author introduces a new domain decomposition method for the solution of discretised integral equation eigenvalue problems the new domain decomposition method is motivated by the socalled automated multilevel substructuring short amls method the amls method is a domain decomposition method for the solu... | [['in', 'this', 'paper', 'the', 'author', 'introduces', 'a', 'new', 'domain', 'decomposition', 'method', 'for', 'the', 'solution', 'of', 'discretised', 'integral', 'equation', 'eigenvalue', 'problems', 'the', 'new', 'domain', 'decomposition', 'method', 'is', 'motivated', 'by', 'the', 'socalled', 'automated', 'multileve... | [-0.09402017219718725, 0.022608169112880355, -0.11175243070817008, 0.029622131386650322, -0.13964651521308807, -0.12079224178954455, -0.035501232368484646, 0.3283208959920395, -0.33165675362095165, -0.2546738703838653, 0.16390431312796916, -0.23476460550862235, -0.16322964072510923, 0.1818799532652981, -0.0694427168500... |
1,712.0994 | On rank range of interval matrices | An interval matrix is a matrix whose entries are intervals in the set of real
numbers. Let $p , q $ be nonzero natural numbers and let $\mu =( [m_{i,j},
M_{i,j}])_{i,j}$ be a $p \times q$ interval matrix; given a $p \times q$ matrix
$A$ with entries in the set of real numbers, we say that $ A \in \mu $ if
$a_{i,j} \i... | math.RA | an interval matrix is a matrix whose entries are intervals in the set of real numbers let p q be nonzero natural numbers and let mu m_ij m_ij_ij be a p times q interval matrix given a p times q matrix a with entries in the set of real numbers we say that a in mu if a_ij in m_ij m_ij for any ij we establish a criterion ... | [['an', 'interval', 'matrix', 'is', 'a', 'matrix', 'whose', 'entries', 'are', 'intervals', 'in', 'the', 'set', 'of', 'real', 'numbers', 'let', 'p', 'q', 'be', 'nonzero', 'natural', 'numbers', 'and', 'let', 'mu', 'm_ij', 'm_ij_ij', 'be', 'a', 'p', 'times', 'q', 'interval', 'matrix', 'given', 'a', 'p', 'times', 'q', 'mat... | [-0.17536274637038843, 0.17364838022745321, -0.019585372849814292, 0.009094892714240747, 0.002467383206556968, -0.1398623808423375, 0.07523865960595175, 0.35357098493391903, -0.2744300933327617, -0.20691146219397205, 0.10308804029288392, -0.301838224125284, -0.1040950274715821, 0.11423614333436741, -0.04381981857946309... |
1,712.09941 | Sorted Concave Penalized Regression | The Lasso is biased. Concave penalized least squares estimation (PLSE) takes
advantage of signal strength to reduce this bias, leading to sharper error
bounds in prediction, coefficient estimation and variable selection. For
prediction and estimation, the bias of the Lasso can be also reduced by taking
a smaller pena... | math.ST stat.TH | the lasso is biased concave penalized least squares estimation plse takes advantage of signal strength to reduce this bias leading to sharper error bounds in prediction coefficient estimation and variable selection for prediction and estimation the bias of the lasso can be also reduced by taking a smaller penalty level... | [['the', 'lasso', 'is', 'biased', 'concave', 'penalized', 'least', 'squares', 'estimation', 'plse', 'takes', 'advantage', 'of', 'signal', 'strength', 'to', 'reduce', 'this', 'bias', 'leading', 'to', 'sharper', 'error', 'bounds', 'in', 'prediction', 'coefficient', 'estimation', 'and', 'variable', 'selection', 'for', 'pr... | [-0.04453940354373858, 0.0247325019570309, -0.09045567871243865, 0.10073314044986748, -0.13852319081952036, -0.20896455727051944, 0.09720811880435105, 0.3884747551400559, -0.29233847034888133, -0.30978975575762213, 0.13019314140978236, -0.2591661458472825, -0.1300656118111133, 0.12069576074481356, -0.1373218201737877, ... |
1,712.09942 | Intersecting non-uniform families containing subfamilies | A family of sets is said to be intersecting if every pair of sets in the
family have non-empty intersection. In this paper, we initiate the study of
intersecting non-uniform families of sets of one of two sizes containing given
subfamilies. For a set $X$ and integer $r$, let $\binom{X}{r}$ denote the
family $\{A \sub... | math.CO | a family of sets is said to be intersecting if every pair of sets in the family have nonempty intersection in this paper we initiate the study of intersecting nonuniform families of sets of one of two sizes containing given subfamilies for a set x and integer r let binomxr denote the family a subseteq x x r let a b and... | [['a', 'family', 'of', 'sets', 'is', 'said', 'to', 'be', 'intersecting', 'if', 'every', 'pair', 'of', 'sets', 'in', 'the', 'family', 'have', 'nonempty', 'intersection', 'in', 'this', 'paper', 'we', 'initiate', 'the', 'study', 'of', 'intersecting', 'nonuniform', 'families', 'of', 'sets', 'of', 'one', 'of', 'two', 'sizes... | [-0.19321705993908128, 0.10863716875411496, -0.011460539861414716, -0.030430130947122883, -0.009860810163772578, -0.14212244547059316, 0.028635194783916417, 0.294920467697888, -0.28843513505010726, -0.21161868282855092, 0.07729516262707817, -0.35394231189819547, -0.09104480958717923, 0.14867832483690258, -0.09962922132... |
1,712.09943 | Toward Continual Learning for Conversational Agents | While end-to-end neural conversation models have led to promising advances in
reducing hand-crafted features and errors induced by the traditional complex
system architecture, they typically require an enormous amount of data due to
the lack of modularity. Previous studies adopted a hybrid approach with
knowledge-bas... | cs.CL cs.AI cs.HC | while endtoend neural conversation models have led to promising advances in reducing handcrafted features and errors induced by the traditional complex system architecture they typically require an enormous amount of data due to the lack of modularity previous studies adopted a hybrid approach with knowledgebased compo... | [['while', 'endtoend', 'neural', 'conversation', 'models', 'have', 'led', 'to', 'promising', 'advances', 'in', 'reducing', 'handcrafted', 'features', 'and', 'errors', 'induced', 'by', 'the', 'traditional', 'complex', 'system', 'architecture', 'they', 'typically', 'require', 'an', 'enormous', 'amount', 'of', 'data', 'du... | [-0.04681804376791975, 0.011440600200542307, -0.07825362745309307, 0.05958478393837804, -0.19001673121567605, -0.14958661482171537, 0.0713571039732815, 0.44694356076747366, -0.26049061539530194, -0.34447586329056407, 0.024564852923412556, -0.2641788947136242, -0.21712082984956838, 0.20548605968818395, -0.14580839739397... |
1,712.09944 | Rare $B$ decays at CMS | The Flavor Changing Neutral Current mediated decays $B \rightarrow
\mu^{+}\mu^{-}$ and $B^{0} \rightarrow K^{*0}\mu^{+}\mu^{-}$ provide high
sensitivity to new physics contributions. Sensitive observables include the
branching fraction, the muon forward-backward asymmetry, the fraction of
$K^{*0}$ longitudinal polari... | hep-ex | the flavor changing neutral current mediated decays b rightarrow mumu and b0 rightarrow k0mumu provide high sensitivity to new physics contributions sensitive observables include the branching fraction the muon forwardbackward asymmetry the fraction of k0 longitudinal polarisation and the differential branching fractio... | [['the', 'flavor', 'changing', 'neutral', 'current', 'mediated', 'decays', 'b', 'rightarrow', 'mumu', 'and', 'b0', 'rightarrow', 'k0mumu', 'provide', 'high', 'sensitivity', 'to', 'new', 'physics', 'contributions', 'sensitive', 'observables', 'include', 'the', 'branching', 'fraction', 'the', 'muon', 'forwardbackward', '... | [-0.07270131576849424, 0.2918661545392954, 0.031120261858665833, 0.058927526197361725, -0.08395398525452172, -0.11163314430181075, 0.11617023144909008, 0.23144268043580707, -0.248679099932175, -0.22772407655914625, -0.03458066283363021, -0.39239468860129517, 0.05840353064101051, 0.1277136130741349, 0.11524348440407603,... |
1,712.09945 | Inverse Boundary Value Problem for Non-linear Hyperbolic Partial
Differential Equations | In this article we are concerned with an inverse boundary value problem for a
non-linear wave equation of divergence form with space dimension $n\geq 3$. In
particular the so called the interior determination problem. This non-linear
wave equation has a trivial solution, i.e. zero solution. By linearizing this
equati... | math.AP | in this article we are concerned with an inverse boundary value problem for a nonlinear wave equation of divergence form with space dimension ngeq 3 in particular the so called the interior determination problem this nonlinear wave equation has a trivial solution ie zero solution by linearizing this equation at the tri... | [['in', 'this', 'article', 'we', 'are', 'concerned', 'with', 'an', 'inverse', 'boundary', 'value', 'problem', 'for', 'a', 'nonlinear', 'wave', 'equation', 'of', 'divergence', 'form', 'with', 'space', 'dimension', 'ngeq', '3', 'in', 'particular', 'the', 'so', 'called', 'the', 'interior', 'determination', 'problem', 'thi... | [-0.15401193136508398, 0.10830379510090486, -0.04766778643127323, -0.005221670648221922, -0.12048272043177337, -0.12096646501862021, -0.035133300336824026, 0.3303319728161029, -0.33138891277105914, -0.1953903480255051, 0.1547877091534077, -0.33005331626150364, -0.12030566662480557, 0.15360946789013674, -0.0155930291125... |
1,712.09946 | Slice-Polynomial Functions and Twistor Geometry of Ruled Surfaces in
$\mathbb{CP}^3$ | In the present paper we introduce the class of slice-polynomial functions:
slice regular functions {defined over the quaternions, outside the real axis,}
whose restriction to any complex half-plane is a polynomial. These functions
naturally emerge in the twistor interpretation of slice regularity introduced
in \cite{... | math.CV math.DG | in the present paper we introduce the class of slicepolynomial functions slice regular functions defined over the quaternions outside the real axis whose restriction to any complex halfplane is a polynomial these functions naturally emerge in the twistor interpretation of slice regularity introduced in citegensalsto an... | [['in', 'the', 'present', 'paper', 'we', 'introduce', 'the', 'class', 'of', 'slicepolynomial', 'functions', 'slice', 'regular', 'functions', 'defined', 'over', 'the', 'quaternions', 'outside', 'the', 'real', 'axis', 'whose', 'restriction', 'to', 'any', 'complex', 'halfplane', 'is', 'a', 'polynomial', 'these', 'function... | [-0.16395911765905719, 0.08056869537569583, -0.09942025244235993, 0.07463929332327097, -0.13321660762031873, -0.09053005577996373, -0.0003066831834924718, 0.34994452610611915, -0.32387310397500796, -0.2006327995417329, 0.05147877811221406, -0.2198675775186469, -0.22092235174030064, 0.17422777325846256, -0.0810083109062... |
1,712.09947 | Large intrinsic anomalous Hall effect in half-metallic ferromagnet
Co3Sn2S2 with magnetic Weyl fermions | The origin of anomalous Hall effect (AHE) in magnetic materials is one of the
most intriguing aspect in condensed matter physics and has been controversial
for a long time. Recent studies indicate that the intrinsic AHE is closely
related to the Berry curvature of occupied electronic states. In a magnetic
Weyl semime... | cond-mat.str-el cond-mat.mtrl-sci | the origin of anomalous hall effect ahe in magnetic materials is one of the most intriguing aspect in condensed matter physics and has been controversial for a long time recent studies indicate that the intrinsic ahe is closely related to the berry curvature of occupied electronic states in a magnetic weyl semimetal wi... | [['the', 'origin', 'of', 'anomalous', 'hall', 'effect', 'ahe', 'in', 'magnetic', 'materials', 'is', 'one', 'of', 'the', 'most', 'intriguing', 'aspect', 'in', 'condensed', 'matter', 'physics', 'and', 'has', 'been', 'controversial', 'for', 'a', 'long', 'time', 'recent', 'studies', 'indicate', 'that', 'the', 'intrinsic', ... | [-0.2109300465680475, 0.2347594258034418, -0.0740239995696318, 0.04718838414114992, -0.12627121916657288, -0.14644671968368053, 0.04443339370584614, 0.3520203042040828, -0.2805951737551163, -0.30013508083705437, 0.004535668982114171, -0.33707601401272796, -0.18470010429646977, 0.15991043891679024, -0.006551940248242881... |
1,712.09948 | Minimizing Polarization and Disagreement in Social Networks | The rise of social media and online social networks has been a disruptive
force in society. Opinions are increasingly shaped by interactions on online
social media, and social phenomena including disagreement and polarization are
now tightly woven into everyday life. In this work we initiate the study of the
followin... | cs.SI cs.DS cs.LG | the rise of social media and online social networks has been a disruptive force in society opinions are increasingly shaped by interactions on online social media and social phenomena including disagreement and polarization are now tightly woven into everyday life in this work we initiate the study of the following que... | [['the', 'rise', 'of', 'social', 'media', 'and', 'online', 'social', 'networks', 'has', 'been', 'a', 'disruptive', 'force', 'in', 'society', 'opinions', 'are', 'increasingly', 'shaped', 'by', 'interactions', 'on', 'online', 'social', 'media', 'and', 'social', 'phenomena', 'including', 'disagreement', 'and', 'polarizati... | [-0.11197308378263295, 0.04040086560695165, -0.06940344113429413, 0.08400873666601803, -0.12197019933527746, -0.12724858660401558, 0.08170388768314082, 0.4436088813270223, -0.2630002080233466, -0.3266224145344869, 0.05428110360833885, -0.33299263395362205, -0.21891336155514343, 0.13897325115634457, -0.0733386213747401,... |
1,712.09949 | Almost formality of quasi-Sasakian and Vaisman manifolds with
applications to nilmanifolds | We provide models that are as close as possible to being formal for a large
class of compact manifolds that admit a transversely Kaehler structure,
including Vaisman and quasi-Sasakian manifolds. As an application we are able
to classify the corresponding nilmanifolds.
| math.DG math.AT math.SG | we provide models that are as close as possible to being formal for a large class of compact manifolds that admit a transversely kaehler structure including vaisman and quasisasakian manifolds as an application we are able to classify the corresponding nilmanifolds | [['we', 'provide', 'models', 'that', 'are', 'as', 'close', 'as', 'possible', 'to', 'being', 'formal', 'for', 'a', 'large', 'class', 'of', 'compact', 'manifolds', 'that', 'admit', 'a', 'transversely', 'kaehler', 'structure', 'including', 'vaisman', 'and', 'quasisasakian', 'manifolds', 'as', 'an', 'application', 'we', 'a... | [-0.12318865019010335, 0.044144890634925105, -0.05025039808597506, 0.14963162935725072, -0.17602101421528837, -0.1615611646415257, -0.08721899284367882, 0.45846082288317563, -0.21185806630145212, -0.25237007543626355, 0.17244350945963183, -0.2625609474574647, -0.19227369888344917, 0.25632618681141517, -0.10799165522089... |
1,712.0995 | Helical liquid in carbon nanotubes wrapped with DNA molecules | The measured electric resistance of carbon nanotubes wrapped with DNA
molecules depends strongly on the spin of the injected electrons. Motivated by
these experiments, we study the effect of helix-shaped potentials on the
electronic spectrum of carbon nanotubes. We find that in combination with the
curvature-induced ... | cond-mat.mes-hall | the measured electric resistance of carbon nanotubes wrapped with dna molecules depends strongly on the spin of the injected electrons motivated by these experiments we study the effect of helixshaped potentials on the electronic spectrum of carbon nanotubes we find that in combination with the curvatureinduced spinorb... | [['the', 'measured', 'electric', 'resistance', 'of', 'carbon', 'nanotubes', 'wrapped', 'with', 'dna', 'molecules', 'depends', 'strongly', 'on', 'the', 'spin', 'of', 'the', 'injected', 'electrons', 'motivated', 'by', 'these', 'experiments', 'we', 'study', 'the', 'effect', 'of', 'helixshaped', 'potentials', 'on', 'the', ... | [-0.16523834026580217, 0.2142874003057203, -0.022019360172770806, 0.00012626656185168384, -0.01698687357251157, -0.1302452854631441, 0.062433110515295126, 0.4504789511687053, -0.2740246191509624, -0.2756786882015529, -0.02023371792773702, -0.3026668774867569, -0.14335790958773317, 0.1727763486595185, 0.0250698673667441... |
1,712.09951 | Large-scale exact diagonalizations reveal low-momentum scales of nuclei | Ab initio methods aim to solve the nuclear many-body problem with controlled
approximations. Virtually exact numerical solutions for realistic interactions
can only be obtained for certain special cases such as few-nucleon systems.
Here we extend the reach of exact diagonalization methods to handle model
spaces with ... | nucl-th | ab initio methods aim to solve the nuclear manybody problem with controlled approximations virtually exact numerical solutions for realistic interactions can only be obtained for certain special cases such as fewnucleon systems here we extend the reach of exact diagonalization methods to handle model spaces with dimens... | [['ab', 'initio', 'methods', 'aim', 'to', 'solve', 'the', 'nuclear', 'manybody', 'problem', 'with', 'controlled', 'approximations', 'virtually', 'exact', 'numerical', 'solutions', 'for', 'realistic', 'interactions', 'can', 'only', 'be', 'obtained', 'for', 'certain', 'special', 'cases', 'such', 'as', 'fewnucleon', 'syst... | [-0.025351307717742536, 0.07802708853467753, -0.09714360495989506, 0.14745085863453314, -0.02085230938476942, -0.11268268535822266, 0.06636655869007838, 0.4368300249572934, -0.21969332729080102, -0.2812279362753942, 0.050316813939092, -0.2773656825953101, -0.06506116198966416, 0.17018344214117928, 0.029015308922929008,... |
1,712.09952 | Spectral Methods in the Presence of Discontinuities | Spectral methods provide an elegant and efficient way of numerically solving
differential equations of all kinds. For smooth problems, truncation error for
spectral methods vanishes exponentially in the infinity norm and $L_2$-norm.
However, for non-smooth problems, convergence is significantly worse---the
$L_2$-norm... | cs.NA gr-qc physics.comp-ph | spectral methods provide an elegant and efficient way of numerically solving differential equations of all kinds for smooth problems truncation error for spectral methods vanishes exponentially in the infinity norm and l_2norm however for nonsmooth problems convergence is significantly worsethe l_2norm of the error for... | [['spectral', 'methods', 'provide', 'an', 'elegant', 'and', 'efficient', 'way', 'of', 'numerically', 'solving', 'differential', 'equations', 'of', 'all', 'kinds', 'for', 'smooth', 'problems', 'truncation', 'error', 'for', 'spectral', 'methods', 'vanishes', 'exponentially', 'in', 'the', 'infinity', 'norm', 'and', 'l_2no... | [-0.05728691561441673, 0.004439535582940535, -0.11690684678094265, 0.11597618848011879, -0.027760260767842593, -0.15230254449538494, 0.01113333689434895, 0.3735389933676312, -0.2998988762301834, -0.22184132290513892, 0.17429959477832246, -0.2589460926424516, -0.10852299323060403, 0.24010282898027646, -0.105513910213305... |
1,712.09953 | Probing the CP properties of top Yukawa coupling at an $e^+e^-$ collider | We study consequences of CP violation in the $ht\bar{t}$ Yukawa coupling
through the process $e^+e^- \to$ $h(125)t\bar{t}$. The helicity amplitudes are
calculated in the $t\bar{t}$ rest frame, where the initial $e^+e^-$ current and
the final Higgs boson have the same three-momentum. CP-violating asymmetries
appear no... | hep-ph | we study consequences of cp violation in the htbart yukawa coupling through the process ee to h125tbart the helicity amplitudes are calculated in the tbart rest frame where the initial ee current and the final higgs boson have the same threemomentum cpviolating asymmetries appear not only in the azimuthal angle between... | [['we', 'study', 'consequences', 'of', 'cp', 'violation', 'in', 'the', 'htbart', 'yukawa', 'coupling', 'through', 'the', 'process', 'ee', 'to', 'h125tbart', 'the', 'helicity', 'amplitudes', 'are', 'calculated', 'in', 'the', 'tbart', 'rest', 'frame', 'where', 'the', 'initial', 'ee', 'current', 'and', 'the', 'final', 'hi... | [-0.10514650979716027, 0.2624144935156821, -0.04981388539815524, 0.13471534833845655, -0.052408367569628016, -0.1365564480601322, 0.034049623014665124, 0.3207474084330254, -0.23657555957673257, -0.28606946984952203, -0.038311662049457226, -0.3167562271257685, 0.05210700723006814, 0.14195152966711086, 0.1271148078067570... |
1,712.09954 | Evolution of single-particle structure of silicon isotopes | New data on proton and neutron single-particle energies $E_{nlj}$ of Si
isotopes with neutron number $N$ from 12 to 28 as well as occupation
probabilities $N_{nlj}$ of single particle states of stable isotopes
$^{28,30}$Si near the Fermi energy were obtained by the joint evaluation of the
stripping and pick-up reacti... | nucl-th nucl-ex | new data on proton and neutron singleparticle energies e_nlj of si isotopes with neutron number n from 12 to 28 as well as occupation probabilities n_nlj of single particle states of stable isotopes 2830si near the fermi energy were obtained by the joint evaluation of the stripping and pickup reaction data and excited ... | [['new', 'data', 'on', 'proton', 'and', 'neutron', 'singleparticle', 'energies', 'e_nlj', 'of', 'si', 'isotopes', 'with', 'neutron', 'number', 'n', 'from', '12', 'to', '28', 'as', 'well', 'as', 'occupation', 'probabilities', 'n_nlj', 'of', 'single', 'particle', 'states', 'of', 'stable', 'isotopes', '2830si', 'near', 't... | [-0.06790275987821506, 0.21001062693713762, -0.007632597570469145, 0.08549355692925181, 0.05555421973703735, -0.11060195894644304, 0.08392718031919047, 0.31563590561498456, -0.21647820598445833, -0.36377765833219483, -0.03655954713780266, -0.3423222854625739, 0.007148167526752535, 0.13046445517102256, 0.087712020547226... |
1,712.09955 | Group constraint relations for five-point amplitudes in gauge theories
with SO(N) and Sp(2N) groups | In this paper,linear constraint relations among loop-order five-point
color-ordered amplitudes in $SO(N)$ and $Sp(2N)$ gauge theories are derived
with the group-theoretic method. These constrains are derived up to four-loop
order. It is found that in both theories, there are $n=6,22,34,44,50$ linear
constraint relati... | hep-th | in this paperlinear constraint relations among looporder fivepoint colorordered amplitudes in son and sp2n gauge theories are derived with the grouptheoretic method these constrains are derived up to fourloop order it is found that in both theories there are n622344450 linear constraint relations at l01234 loop orders ... | [['in', 'this', 'paperlinear', 'constraint', 'relations', 'among', 'looporder', 'fivepoint', 'colorordered', 'amplitudes', 'in', 'son', 'and', 'sp2n', 'gauge', 'theories', 'are', 'derived', 'with', 'the', 'grouptheoretic', 'method', 'these', 'constrains', 'are', 'derived', 'up', 'to', 'fourloop', 'order', 'it', 'is', '... | [-0.2068601240230314, 0.23329684624479988, -0.037823309837761575, 0.13427937698503167, -0.0705245134057635, -0.12219181307986127, 0.003573755062800848, 0.3403313311479859, -0.17374319043326175, -0.3201690259847348, 0.0663449451005702, -0.3026987195520078, -0.17096952829604684, 0.16706068649635478, 0.031911018825436045,... |
1,712.09956 | Estimation of non-femtoscopic effects in p+p and p+A collisions at RHIC
energies using PYTHIA and HIJING generators | The spatial extents of particle emission source in high-energy collisions can
be measured using two-particle femtoscopic correlations. In collisions with
small multipli cities, such as proton-proton collisions, correlation functions
can be distorted by non-femtos copic effects, for example due to the
correlations tha... | hep-ex nucl-ex | the spatial extents of particle emission source in highenergy collisions can be measured using twoparticle femtoscopic correlations in collisions with small multipli cities such as protonproton collisions correlation functions can be distorted by nonfemtos copic effects for example due to the correlations that caused b... | [['the', 'spatial', 'extents', 'of', 'particle', 'emission', 'source', 'in', 'highenergy', 'collisions', 'can', 'be', 'measured', 'using', 'twoparticle', 'femtoscopic', 'correlations', 'in', 'collisions', 'with', 'small', 'multipli', 'cities', 'such', 'as', 'protonproton', 'collisions', 'correlation', 'functions', 'can... | [-0.021387469917904623, 0.2523791832794057, -0.17723609378450725, 0.22703382784113435, 0.05526058340334509, -0.09385019460102857, -0.12211014505586412, 0.41811420457520626, -0.2029976032231704, -0.34878884563868, -0.07036604773078003, -0.43928514767696364, 0.11794699760704845, 0.14695173240667855, 0.1288120647394421, 0... |
1,712.09957 | Estimation and prediction of Gaussian processes using generalized Cauchy
covariance model under fixed domain asymptotics | We study estimation and prediction of Gaussian processes with covariance
model belonging to the generalized Cauchy (GC) family, under fixed domain
asymptotics. Gaussian processes with this kind of covariance function provide
separate characterization of fractal dimension and long range dependence, an
appealing featur... | stat.ME | we study estimation and prediction of gaussian processes with covariance model belonging to the generalized cauchy gc family under fixed domain asymptotics gaussian processes with this kind of covariance function provide separate characterization of fractal dimension and long range dependence an appealing feature in ma... | [['we', 'study', 'estimation', 'and', 'prediction', 'of', 'gaussian', 'processes', 'with', 'covariance', 'model', 'belonging', 'to', 'the', 'generalized', 'cauchy', 'gc', 'family', 'under', 'fixed', 'domain', 'asymptotics', 'gaussian', 'processes', 'with', 'this', 'kind', 'of', 'covariance', 'function', 'provide', 'sep... | [-0.05616504104171761, 0.030655226195501758, -0.09821376368430262, 0.12067640267232042, -0.050468655992031035, -0.11833425237842234, 0.0441325387707624, 0.3824312144721793, -0.23526395198318018, -0.2734269547073071, 0.1238096101480678, -0.26560233341368994, -0.1645888810375621, 0.15301130396417445, -0.04400744508384677... |
1,712.09958 | Object-Oriented Theorem Proving (OOTP): First Thoughts | Automatic (i.e., computer-assisted) theorem proving (ATP) can come in many
flavors. This document presents early steps in our effort towards defining
object-oriented theorem proving (OOTP) as a new style of ATP.
Traditional theorem proving (TTP) is the only well-known flavor of ATP so
far. OOTP is a generalization ... | cs.PL | automatic ie computerassisted theorem proving atp can come in many flavors this document presents early steps in our effort towards defining objectoriented theorem proving ootp as a new style of atp traditional theorem proving ttp is the only wellknown flavor of atp so far ootp is a generalization of ttp while ttp is s... | [['automatic', 'ie', 'computerassisted', 'theorem', 'proving', 'atp', 'can', 'come', 'in', 'many', 'flavors', 'this', 'document', 'presents', 'early', 'steps', 'in', 'our', 'effort', 'towards', 'defining', 'objectoriented', 'theorem', 'proving', 'ootp', 'as', 'a', 'new', 'style', 'of', 'atp', 'traditional', 'theorem', ... | [-0.08973165691801996, 0.05891031209341805, -0.12289480068203476, 0.12803931705150376, -0.17359320412982593, -0.22910630139004853, 0.08156842004620668, 0.32572881185045144, -0.23232596990360757, -0.3028152786345795, 0.09500603229418923, -0.24316730433980924, -0.124959129472075, 0.26470975382159456, -0.1393307175497312,... |
1,712.09959 | How not to establish the non-renormalizability of gravity | General relativity cannot be formulated as a perturbatively renormalizable
quantum field theory. An argument relying on the validity of the
Bekenstein-Hawking entropy formula aims at dismissing gravity as
non-renormalizable per se, against hopes (underlying programs such as
Asymptotic Safety) that d-dimensional GR co... | physics.hist-ph gr-qc | general relativity cannot be formulated as a perturbatively renormalizable quantum field theory an argument relying on the validity of the bekensteinhawking entropy formula aims at dismissing gravity as nonrenormalizable per se against hopes underlying programs such as asymptotic safety that ddimensional gr could turn ... | [['general', 'relativity', 'can', 'not', 'be', 'formulated', 'as', 'a', 'perturbatively', 'renormalizable', 'quantum', 'field', 'theory', 'an', 'argument', 'relying', 'on', 'the', 'validity', 'of', 'the', 'bekensteinhawking', 'entropy', 'formula', 'aims', 'at', 'dismissing', 'gravity', 'as', 'nonrenormalizable', 'per',... | [-0.13644861510950093, 0.11077973272576763, -0.139488395515152, 0.15635759415777606, -0.07473680416517185, -0.20039518154461425, 0.045592466197588076, 0.23390453344098094, -0.1961592888327861, -0.2527227898956173, 0.06677474449459238, -0.27054979844310445, -0.13987686586650935, 0.162537929874779, -0.14319671527247388, ... |
1,712.0996 | Social Bayesian Learning in the Wisdom of the Crowd | Being able to correctly aggregate the beliefs of many people into a single
belief is a problem fundamental to many important social, economic and
political processes such as policy making, market pricing and voting. Although
there exist many models and mechanisms for aggregation, there is a lack of
methods and litera... | cs.SI physics.soc-ph | being able to correctly aggregate the beliefs of many people into a single belief is a problem fundamental to many important social economic and political processes such as policy making market pricing and voting although there exist many models and mechanisms for aggregation there is a lack of methods and literature r... | [['being', 'able', 'to', 'correctly', 'aggregate', 'the', 'beliefs', 'of', 'many', 'people', 'into', 'a', 'single', 'belief', 'is', 'a', 'problem', 'fundamental', 'to', 'many', 'important', 'social', 'economic', 'and', 'political', 'processes', 'such', 'as', 'policy', 'making', 'market', 'pricing', 'and', 'voting', 'al... | [-0.02656428321212416, 0.05527030408610495, -0.09612422092100226, 0.13465421093979432, -0.13256017297829445, -0.16952044746068742, 0.08945092979559618, 0.4531689572281071, -0.29201724382155403, -0.31750488248374553, 0.08520223180898845, -0.30876477969316196, -0.2292510190674541, 0.1491309188125769, -0.11471377173201086... |
1,712.09961 | Multifield Reheating after Modular $j$-Inflation | In the inflationary framework of cosmology the initial phase of rapid
expansion has to be followed by a reheating stage, which is envisioned to end
in a radiation dominated big bang. Key parameters that characterize this big
bang state are the temperature at the end of the reheating stage and the baryon
asymmetry. Fo... | hep-ph astro-ph.CO hep-th | in the inflationary framework of cosmology the initial phase of rapid expansion has to be followed by a reheating stage which is envisioned to end in a radiation dominated big bang key parameters that characterize this big bang state are the temperature at the end of the reheating stage and the baryon asymmetry for gen... | [['in', 'the', 'inflationary', 'framework', 'of', 'cosmology', 'the', 'initial', 'phase', 'of', 'rapid', 'expansion', 'has', 'to', 'be', 'followed', 'by', 'a', 'reheating', 'stage', 'which', 'is', 'envisioned', 'to', 'end', 'in', 'a', 'radiation', 'dominated', 'big', 'bang', 'key', 'parameters', 'that', 'characterize',... | [-0.13205022546961637, 0.2259330754678948, -0.12949080963361276, 0.08653942215044351, -0.05067072183425937, -0.14618952121236362, -0.031102178640139755, 0.3000794547177585, -0.24964283904409967, -0.27428119181422517, 0.11355831677688652, -0.2014980949825258, -0.083540829795051, 0.1603235690397144, -0.029693998205142895... |
1,712.09962 | A new proof of scattering below the ground state for the non-radial
focusing NLS | We revisit the scattering result of Duyckaerts, Holmer, and Roudenko for the
non-radial $\dot H^{1/2}$-critical focusing NLS. By proving an interaction
Morawetz inequality, we give a simple proof of scattering below the ground
state in dimensions $d\geq 3$ that avoids the use of concentration compactness.
| math.AP | we revisit the scattering result of duyckaerts holmer and roudenko for the nonradial dot h12critical focusing nls by proving an interaction morawetz inequality we give a simple proof of scattering below the ground state in dimensions dgeq 3 that avoids the use of concentration compactness | [['we', 'revisit', 'the', 'scattering', 'result', 'of', 'duyckaerts', 'holmer', 'and', 'roudenko', 'for', 'the', 'nonradial', 'dot', 'h12critical', 'focusing', 'nls', 'by', 'proving', 'an', 'interaction', 'morawetz', 'inequality', 'we', 'give', 'a', 'simple', 'proof', 'of', 'scattering', 'below', 'the', 'ground', 'stat... | [-0.1479224378036128, 0.10854567361562253, -0.05344413388132428, 0.10062035140064028, -0.051639077812433244, -0.1755793856146435, 0.018616403225395414, 0.2679004162963894, -0.1970365766642822, -0.22900754722456138, 0.10482192180999038, -0.2960311430609889, -0.10282867117267516, 0.18843861816243992, -0.04702860640568866... |
1,712.09963 | Low-Energy Effective Field Theory of Lepton-Proton Bremsstrahlung | We calculate the cross section for the lepton-proton bremsstrahlung process
$l+p\to l^\prime +p+\gamma$ in effective field theory. This process corresponds
to an undetected background signal for the proposed MUSE experiment at PSI.
MUSE is designed to measure elastic scattering of low-energy electrons and
muons off a... | nucl-th hep-ph | we calculate the cross section for the leptonproton bremsstrahlung process lpto lprime pgamma in effective field theory this process corresponds to an undetected background signal for the proposed muse experiment at psi muse is designed to measure elastic scattering of lowenergy electrons and muons off a proton target ... | [['we', 'calculate', 'the', 'cross', 'section', 'for', 'the', 'leptonproton', 'bremsstrahlung', 'process', 'lpto', 'lprime', 'pgamma', 'in', 'effective', 'field', 'theory', 'this', 'process', 'corresponds', 'to', 'an', 'undetected', 'background', 'signal', 'for', 'the', 'proposed', 'muse', 'experiment', 'at', 'psi', 'm... | [0.0031181888870086593, 0.135502511882668, -0.10444935117980009, 0.20045933965061608, -0.05580874697639132, -0.07841576829460396, -0.000891256239484855, 0.395458500039789, -0.22540947875306713, -0.2661907491010596, -0.02466865899458633, -0.34515179962552384, -0.021602433987559296, 0.18205468784490564, 0.039870912803310... |
1,712.09964 | Two-pion and two-kaon femtoscopic correlations in Au+Au collisions at
$\sqrt{s_{NN}}$=200 GeV from STAR | Measurement of femtoscopic correlations in heavy-ion collisions can provide
information about spatial and temporal parameters of the particle emission
region at kinetic freeze-out. In this work we present the measurement of
two-pion and two-kaon femtoscopic correlations in 200 GeV Au+Au collisions at
RHIC. The collis... | nucl-ex | measurement of femtoscopic correlations in heavyion collisions can provide information about spatial and temporal parameters of the particle emission region at kinetic freezeout in this work we present the measurement of twopion and twokaon femtoscopic correlations in 200 gev auau collisions at rhic the collision centr... | [['measurement', 'of', 'femtoscopic', 'correlations', 'in', 'heavyion', 'collisions', 'can', 'provide', 'information', 'about', 'spatial', 'and', 'temporal', 'parameters', 'of', 'the', 'particle', 'emission', 'region', 'at', 'kinetic', 'freezeout', 'in', 'this', 'work', 'we', 'present', 'the', 'measurement', 'of', 'two... | [-0.09909332899066309, 0.25391901906890174, -0.22273921157854298, 0.149771748483181, 0.04097695026236276, -0.07121242911865314, -0.1709049859122994, 0.37211408813794455, -0.18281071162006507, -0.3060584037254254, -0.11596631059073843, -0.3907536150732388, 0.1826124109948675, 0.09351745506476922, 0.1072593549300412, 0.1... |
1,712.09965 | Conductivity spectrum of ultracold atoms in an optical lattice | We measure the conductivity of neutral fermions in a cubic optical lattice.
Using in-situ fluorescence microscopy, we observe the alternating current
resultant from a single-frequency uniform force applied by displacement of a
weak harmonic trapping potential. In the linear response regime, a
neutral-particle analogu... | cond-mat.quant-gas | we measure the conductivity of neutral fermions in a cubic optical lattice using insitu fluorescence microscopy we observe the alternating current resultant from a singlefrequency uniform force applied by displacement of a weak harmonic trapping potential in the linear response regime a neutralparticle analogue of ohms... | [['we', 'measure', 'the', 'conductivity', 'of', 'neutral', 'fermions', 'in', 'a', 'cubic', 'optical', 'lattice', 'using', 'insitu', 'fluorescence', 'microscopy', 'we', 'observe', 'the', 'alternating', 'current', 'resultant', 'from', 'a', 'singlefrequency', 'uniform', 'force', 'applied', 'by', 'displacement', 'of', 'a',... | [-0.15227262386700735, 0.1738302143899806, -0.06114403039814448, -0.001853034226260435, -0.03782460200102449, -0.1149600707814566, 0.08491703752338968, 0.3788629301688956, -0.28822889167862303, -0.2478863847099315, 0.03751951986711484, -0.2852892461906439, -0.0913912132587401, 0.17095126606430272, 0.0453854058766679, 0... |
1,712.09966 | Low significance of evidence for black hole echoes in gravitational wave
data | Recent detections of merging black holes allow observational tests of the
nature of these objects. In some proposed models, non-trivial structure at or
near the black hole horizon could lead to echo signals in gravitational wave
data. Recently, Abedi et al. claimed tentative evidence for repeating damped
echo signals... | gr-qc astro-ph.IM | recent detections of merging black holes allow observational tests of the nature of these objects in some proposed models nontrivial structure at or near the black hole horizon could lead to echo signals in gravitational wave data recently abedi et al claimed tentative evidence for repeating damped echo signals followi... | [['recent', 'detections', 'of', 'merging', 'black', 'holes', 'allow', 'observational', 'tests', 'of', 'the', 'nature', 'of', 'these', 'objects', 'in', 'some', 'proposed', 'models', 'nontrivial', 'structure', 'at', 'or', 'near', 'the', 'black', 'hole', 'horizon', 'could', 'lead', 'to', 'echo', 'signals', 'in', 'gravitat... | [-0.1385579414426618, 0.05697178678124543, -0.09211428779108613, 0.1344652340830235, -0.10406911191874302, -0.0976124987218704, 0.07194423432861949, 0.3187263339457896, -0.14128444359587794, -0.3330404107152616, 0.10556573501784955, -0.33348999794997625, -0.1259346169922751, 0.22820153355054656, -0.04656013021333106, 0... |
1,712.09967 | A PSPACE Construction of a Hitting Set for the Closure of Small
Algebraic Circuits | In this paper we study the complexity of constructing a hitting set for the
closure of VP, the class of polynomials that can be infinitesimally
approximated by polynomials that are computed by polynomial sized algebraic
circuits, over the real or complex numbers. Specifically, we show that there is
a PSPACE algorithm... | cs.CC math.AG | in this paper we study the complexity of constructing a hitting set for the closure of vp the class of polynomials that can be infinitesimally approximated by polynomials that are computed by polynomial sized algebraic circuits over the real or complex numbers specifically we show that there is a pspace algorithm that ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'complexity', 'of', 'constructing', 'a', 'hitting', 'set', 'for', 'the', 'closure', 'of', 'vp', 'the', 'class', 'of', 'polynomials', 'that', 'can', 'be', 'infinitesimally', 'approximated', 'by', 'polynomials', 'that', 'are', 'computed', 'by', 'polynomial', 'sized', 'algebr... | [-0.13592043137196988, 0.08627473204415828, -0.0928183589188129, 0.0813282121412663, -0.08519861821867065, -0.13394469935832634, 0.0647760063808396, 0.29449119528280304, -0.32160927864067534, -0.2753348409566154, 0.1218407400907688, -0.23108610300895271, -0.14609758025935923, 0.23874626156429418, -0.10070019772989147, ... |
1,712.09968 | Transverse universal links | We show that there exists a transverse link in the standard contact
structures on the 3-sphere such that all contact 3-manifolds are contact
branched covers over this transverse link.
| math.GT math.SG | we show that there exists a transverse link in the standard contact structures on the 3sphere such that all contact 3manifolds are contact branched covers over this transverse link | [['we', 'show', 'that', 'there', 'exists', 'a', 'transverse', 'link', 'in', 'the', 'standard', 'contact', 'structures', 'on', 'the', '3sphere', 'such', 'that', 'all', 'contact', '3manifolds', 'are', 'contact', 'branched', 'covers', 'over', 'this', 'transverse', 'link']] | [-0.34165671297573835, 0.12024006584723448, -0.06158381327986717, 0.0967535295098185, -0.0676817353011976, -0.18003679996613284, 0.002131481502397821, 0.4696441724382598, -0.26779454978632516, -0.22915941913580073, 0.014904639968680668, -0.2874460807391282, -0.23948630866803358, 0.23674122006471815, -0.0756510661368996... |
1,712.09969 | De Facto Control: Applying Game Theory to the Law on Corporate
Nationality | One unexamined assumption in foreign ownership regulation is the notion that
majority voting rights translate to 'effective control'. This assumption is so
deeply entrenched in foreign investments law that possession of majority voting
rights can determine the nationality of a corporation and its capacity to
engage i... | q-fin.GN q-fin.EC | one unexamined assumption in foreign ownership regulation is the notion that majority voting rights translate to effective control this assumption is so deeply entrenched in foreign investments law that possession of majority voting rights can determine the nationality of a corporation and its capacity to engage in par... | [['one', 'unexamined', 'assumption', 'in', 'foreign', 'ownership', 'regulation', 'is', 'the', 'notion', 'that', 'majority', 'voting', 'rights', 'translate', 'to', 'effective', 'control', 'this', 'assumption', 'is', 'so', 'deeply', 'entrenched', 'in', 'foreign', 'investments', 'law', 'that', 'possession', 'of', 'majorit... | [-0.10724531385942751, 0.07307917522944954, -0.08067654714062317, 0.08024752550736834, -0.14225921841239594, -0.18916232456662846, 0.19689887597122296, 0.3494552511549154, -0.2647731178470992, -0.2949178512609064, 0.1012077314273411, -0.3063396012829925, -0.13098901421115394, 0.1362159508712195, -0.1992605561945612, -0... |
1,712.0997 | Cannonball model diagnosis of the short gamma ray burst 170817A | The rich and complex data obtained from multi-wavelength observations of
SHB170817A, the short hard gamma ray burst (SHB) associated with GW170817 --the
first neutron stars merger event detected in gravitational waves (GWs)-- are
analyzed in the framework of the cannonball model of SHBs. In this model a
highly relati... | astro-ph.HE hep-ph hep-th | the rich and complex data obtained from multiwavelength observations of shb170817a the short hard gamma ray burst shb associated with gw170817 the first neutron stars merger event detected in gravitational waves gws are analyzed in the framework of the cannonball model of shbs in this model a highly relativistic jet is... | [['the', 'rich', 'and', 'complex', 'data', 'obtained', 'from', 'multiwavelength', 'observations', 'of', 'shb170817a', 'the', 'short', 'hard', 'gamma', 'ray', 'burst', 'shb', 'associated', 'with', 'gw170817', 'the', 'first', 'neutron', 'stars', 'merger', 'event', 'detected', 'in', 'gravitational', 'waves', 'gws', 'are',... | [-0.0642600155202672, 0.2041244067510383, -0.11171605341757337, 0.1580654897985773, -0.16889952240356554, -0.068247940352497, 0.00695887119820529, 0.4426057263225731, -0.1995949369625628, -0.2921591852584647, 0.05387188401784644, -0.29674814302060337, 0.005178321710425532, 0.2369023368965524, 0.02255958982981004, -0.03... |
1,712.09971 | Chiral liquid crystal colloids | Colloidal particles disturb the alignment of rod-like molecules of liquid
crystals, giving rise to long-range interactions that minimize the free energy
of distorted regions. Particle shape and topology are known to guide this
self-assembly process. However, how chirality of colloidal inclusions affects
these long-ra... | cond-mat.soft cond-mat.mtrl-sci | colloidal particles disturb the alignment of rodlike molecules of liquid crystals giving rise to longrange interactions that minimize the free energy of distorted regions particle shape and topology are known to guide this selfassembly process however how chirality of colloidal inclusions affects these longrange intera... | [['colloidal', 'particles', 'disturb', 'the', 'alignment', 'of', 'rodlike', 'molecules', 'of', 'liquid', 'crystals', 'giving', 'rise', 'to', 'longrange', 'interactions', 'that', 'minimize', 'the', 'free', 'energy', 'of', 'distorted', 'regions', 'particle', 'shape', 'and', 'topology', 'are', 'known', 'to', 'guide', 'thi... | [-0.1511419540796204, 0.28251775735739193, -0.09005074254346498, -0.0020350326771918026, -0.06190782694158538, -0.13218833209834244, -0.03679186452630182, 0.4256807578065051, -0.2858340027273301, -0.3031517934511594, -0.019321833914552108, -0.2939690547313966, -0.19554572791992467, 0.06590744432361934, 0.00882246380440... |
1,712.09972 | Extrema of the two-dimensional Discrete Gaussian Free Field | These lecture notes offer a gentle introduction to the two-dimensional
Discrete Gaussian Free Field with particular attention paid to the scaling
limits of the level sets at heights proportional to the absolute maximum. The
bulk of the text is based on recent joint papers with O. Louidor and with J.
Ding and S. Goswa... | math.PR math-ph math.MP | these lecture notes offer a gentle introduction to the twodimensional discrete gaussian free field with particular attention paid to the scaling limits of the level sets at heights proportional to the absolute maximum the bulk of the text is based on recent joint papers with o louidor and with j ding and s goswami stil... | [['these', 'lecture', 'notes', 'offer', 'a', 'gentle', 'introduction', 'to', 'the', 'twodimensional', 'discrete', 'gaussian', 'free', 'field', 'with', 'particular', 'attention', 'paid', 'to', 'the', 'scaling', 'limits', 'of', 'the', 'level', 'sets', 'at', 'heights', 'proportional', 'to', 'the', 'absolute', 'maximum', '... | [-0.06129972401987573, 0.09139665920049836, -0.06146396097322606, 0.0485685760251745, -0.1160641915512958, -0.15995879816549896, 0.08609730117211137, 0.33242971737953747, -0.24149157912141145, -0.2735702787229622, 0.1310337932752163, -0.2963320845502871, -0.09511418067944245, 0.19394780222721625, -0.10664390248594562, ... |
1,712.09973 | Charge ordering and ferrimagnetism in the strongly correlated
$\beta$-V$_2$PO$_5$ single crystal | A combined study of transport, thermodynamic, neutron diffraction, nuclear
magnetic resonance measurements and first principles calculation were performed
for $\beta$-V$_2$PO$_5$ single crystal. It was shown to be a semiconductor with
a band gap of 0.48 eV, undergoing a charge ordering (unusual V$^{2+}$ and
V$^{3+}$)... | cond-mat.str-el | a combined study of transport thermodynamic neutron diffraction nuclear magnetic resonance measurements and first principles calculation were performed for betav_2po_5 single crystal it was shown to be a semiconductor with a band gap of 048 ev undergoing a charge ordering unusual v2 and v3 phase transition accompanied ... | [['a', 'combined', 'study', 'of', 'transport', 'thermodynamic', 'neutron', 'diffraction', 'nuclear', 'magnetic', 'resonance', 'measurements', 'and', 'first', 'principles', 'calculation', 'were', 'performed', 'for', 'betav_2po_5', 'single', 'crystal', 'it', 'was', 'shown', 'to', 'be', 'a', 'semiconductor', 'with', 'a', ... | [-0.19937478538127362, 0.25053149825583965, -0.03410588827323845, -0.019305286690599145, -0.0792553538842484, -0.11553826730073213, 0.11115462250675853, 0.43780617679992356, -0.2923040857844769, -0.2611722113207391, 0.019277837568390094, -0.32317717203691804, -0.07790310182353508, 0.09746467895097775, 0.147310098824537... |
1,712.09974 | Massive Nambu-Goldstone Fermions and Bosons for Non-relativistic
Superconformal Symmetry: Jackiw-Pi Vortices in a Trap | We discuss a supersymmetric extension of a non-relativistic Chern-Simons
matter theory, known as the SUSY Jackiw-Pi model, in a harmonic trap. We show
that the non-relativistic version of the superconformal symmetry, called the
super-Schr\"odinger symmetry, is not spoiled by an external field including the
harmonic p... | hep-th | we discuss a supersymmetric extension of a nonrelativistic chernsimons matter theory known as the susy jackiwpi model in a harmonic trap we show that the nonrelativistic version of the superconformal symmetry called the superschrodinger symmetry is not spoiled by an external field including the harmonic potential it su... | [['we', 'discuss', 'a', 'supersymmetric', 'extension', 'of', 'a', 'nonrelativistic', 'chernsimons', 'matter', 'theory', 'known', 'as', 'the', 'susy', 'jackiwpi', 'model', 'in', 'a', 'harmonic', 'trap', 'we', 'show', 'that', 'the', 'nonrelativistic', 'version', 'of', 'the', 'superconformal', 'symmetry', 'called', 'the',... | [-0.17136825343125506, 0.24921324732094727, -0.04392390030793132, 0.11946432211388928, -0.053633807199131585, -0.15352333579379732, -0.016306413192591983, 0.30051215168110984, -0.16499197630847465, -0.29096531511624596, 0.03867808646316121, -0.2574218604434839, -0.1349997665805597, 0.06551652884774445, 0.00532566898845... |
1,712.09975 | Generalized Chern-Simons higher-spin gravity theories in three
dimensions | The coupling of spin-3 gauge fields to three-dimensional Maxwell and
$AdS$-Lorentz gravity theories is presented. After showing how the usual spin-3
extensions of the $AdS$ and the Poincar\'e algebras in three dimensions can be
obtained as expansions of $\mathfrak{sl}\left( 3,\mathbb{R}\right)$ algebra,
the procedure... | hep-th math-ph math.MP | the coupling of spin3 gauge fields to threedimensional maxwell and adslorentz gravity theories is presented after showing how the usual spin3 extensions of the ads and the poincare algebras in three dimensions can be obtained as expansions of mathfrakslleft 3mathbbrright algebra the procedure is generalized so as to de... | [['the', 'coupling', 'of', 'spin3', 'gauge', 'fields', 'to', 'threedimensional', 'maxwell', 'and', 'adslorentz', 'gravity', 'theories', 'is', 'presented', 'after', 'showing', 'how', 'the', 'usual', 'spin3', 'extensions', 'of', 'the', 'ads', 'and', 'the', 'poincare', 'algebras', 'in', 'three', 'dimensions', 'can', 'be',... | [-0.14901963974014648, 0.1552020021153668, -0.07959219002282446, 0.0806703016057936, -0.15893663751702863, -0.16381642794760976, -0.09114871081869, 0.2524075825761968, -0.18824849976678787, -0.27881131391154007, 0.05452310573987808, -0.229209377068842, -0.1699733180400816, 0.12064686486976746, -0.050445022298818795, 0.... |
1,712.09976 | $p$-adic multiple zeta values at roots of unity and $p$-adic
pro-unipotent harmonic actions - IV-1 : $p$-adic multiple zeta values at
roots of unity extended to sequences of integers of any sign | This work is a study of $p$-adic multiple zeta values at roots of unity
($p$MZV$\mu_{N}$'s), the $p$-adic periods of the crystalline pro-unipotent
fundamental groupoid of $(\mathbb{P}^{1} - \{0,\mu_{N},\infty\})/
\mathbb{F}_{q}$. The main tool is new objects which we call $p$-adic
pro-unipotent harmonic actions. In t... | math.NT | this work is a study of padic multiple zeta values at roots of unity pmzvmu_ns the padic periods of the crystalline prounipotent fundamental groupoid of mathbbp1 0mu_ninfty mathbbf_q the main tool is new objects which we call padic prounipotent harmonic actions in this part iv we define and study padic analogues of som... | [['this', 'work', 'is', 'a', 'study', 'of', 'padic', 'multiple', 'zeta', 'values', 'at', 'roots', 'of', 'unity', 'pmzvmu_ns', 'the', 'padic', 'periods', 'of', 'the', 'crystalline', 'prounipotent', 'fundamental', 'groupoid', 'of', 'mathbbp1', '0mu_ninfty', 'mathbbf_q', 'the', 'main', 'tool', 'is', 'new', 'objects', 'whi... | [-0.22400500929727446, 0.11488819757759108, -0.13217582031520028, 0.08748624114951147, -0.08675782091979106, -0.09232860624395085, 0.009755510459371813, 0.31283216330815444, -0.32469993962017313, -0.20984637280784998, 0.06290342297253312, -0.2087795310911712, -0.19683317612604392, 0.22822380514557924, -0.11799420511251... |
1,712.09977 | Logarithmic corrections in the asymptotic expansion for the radiation
field along null infinity | We obtain the second-order asymptotics for the radiation field of spherically
symmetric solutions to the wave equation on spherically symmetric and
asymptotically flat backgrounds including the Schwarzschild and sub-extremal
Reissner-Nordstrom families of black holes. These terms appear as logarithmic
corrections to ... | gr-qc math.AP | we obtain the secondorder asymptotics for the radiation field of spherically symmetric solutions to the wave equation on spherically symmetric and asymptotically flat backgrounds including the schwarzschild and subextremal reissnernordstrom families of black holes these terms appear as logarithmic corrections to the le... | [['we', 'obtain', 'the', 'secondorder', 'asymptotics', 'for', 'the', 'radiation', 'field', 'of', 'spherically', 'symmetric', 'solutions', 'to', 'the', 'wave', 'equation', 'on', 'spherically', 'symmetric', 'and', 'asymptotically', 'flat', 'backgrounds', 'including', 'the', 'schwarzschild', 'and', 'subextremal', 'reissne... | [-0.1121121913831877, 0.0509567965728868, -0.08736880933825057, 0.1232286853534006, -0.07077468452125527, -0.10995665793470516, -0.018242530375126784, 0.27763351843806733, -0.16108402492184387, -0.2677804679934573, 0.10918394071785242, -0.2992106716254759, -0.11026630727901009, 0.19996624689124393, -0.01730593598627469... |
1,712.09978 | Why Long-Term Debt Instruments Cannot Be Deposit Substitutes | The definition of deposit substitutes in Philippine tax law fails to consider
the maturity of a debt instrument. This makes it possible for long-term bonds
to be considered as deposit substitutes if they meet the 20-lender rule,
taxable at 20% final tax. However, long-term debt instruments cannot
realistically functi... | q-fin.GN q-fin.PR | the definition of deposit substitutes in philippine tax law fails to consider the maturity of a debt instrument this makes it possible for longterm bonds to be considered as deposit substitutes if they meet the 20lender rule taxable at 20 final tax however longterm debt instruments cannot realistically function as depo... | [['the', 'definition', 'of', 'deposit', 'substitutes', 'in', 'philippine', 'tax', 'law', 'fails', 'to', 'consider', 'the', 'maturity', 'of', 'a', 'debt', 'instrument', 'this', 'makes', 'it', 'possible', 'for', 'longterm', 'bonds', 'to', 'be', 'considered', 'as', 'deposit', 'substitutes', 'if', 'they', 'meet', 'the', '2... | [-0.05167811006995854, 0.09031880683114987, -0.08081451726482353, 0.13181202617263604, -0.11801181740830308, -0.14557273195263137, 0.08646085412840841, 0.38664501102175564, -0.2827185176623364, -0.30041974239672226, 0.15684850426515806, -0.30001858517924257, -0.0765225979417597, 0.13637834809466126, -0.1794775443122489... |
1,712.09979 | Spin excitation spectrum of high-temperature cuprate superconductors
from finite cluster simulations | A cluster of spins $1/2$ of a finite size can be regarded as a basic building
block of a spin texture in high-temperature cuprate superconductors. If this
texture has the character of a network of weakly coupled spin clusters, then
spin excitation spectra of finite clusters are expected to capture the
principal featu... | cond-mat.supr-con | a cluster of spins 12 of a finite size can be regarded as a basic building block of a spin texture in hightemperature cuprate superconductors if this texture has the character of a network of weakly coupled spin clusters then spin excitation spectra of finite clusters are expected to capture the principal features of t... | [['a', 'cluster', 'of', 'spins', '12', 'of', 'a', 'finite', 'size', 'can', 'be', 'regarded', 'as', 'a', 'basic', 'building', 'block', 'of', 'a', 'spin', 'texture', 'in', 'hightemperature', 'cuprate', 'superconductors', 'if', 'this', 'texture', 'has', 'the', 'character', 'of', 'a', 'network', 'of', 'weakly', 'coupled', ... | [-0.15193499074553368, 0.22352380780346295, -0.036083380969138455, 0.05676120490534231, -0.022096344618491116, -0.11497357706070647, 0.021595131932431226, 0.35826344344184385, -0.2523456713450806, -0.3089534013302295, 0.02148600470338186, -0.32906825524791106, -0.04282544588355662, 0.1500206366725653, 0.076166897513238... |
1,712.0998 | Laughlin states on higher genus Riemann surfaces | Considering quantum Hall states on geometric backgrounds has proved over the
past few years to be a useful tool for uncovering their less evident
properties, such as gravitational and electromagnetic responses, topological
phases and novel geometric adiabatic transport coefficients. One of the
transport coefficients,... | cond-mat.str-el hep-th math-ph math.MP | considering quantum hall states on geometric backgrounds has proved over the past few years to be a useful tool for uncovering their less evident properties such as gravitational and electromagnetic responses topological phases and novel geometric adiabatic transport coefficients one of the transport coefficients the c... | [['considering', 'quantum', 'hall', 'states', 'on', 'geometric', 'backgrounds', 'has', 'proved', 'over', 'the', 'past', 'few', 'years', 'to', 'be', 'a', 'useful', 'tool', 'for', 'uncovering', 'their', 'less', 'evident', 'properties', 'such', 'as', 'gravitational', 'and', 'electromagnetic', 'responses', 'topological', '... | [-0.18652851311284122, 0.16074837561573277, -0.0930987864328183, 0.08778828192111207, -0.06130394172077762, -0.1174634810490791, 0.036775424796058824, 0.29329794611220983, -0.22797846576476788, -0.26157639259523946, 0.07578358209938922, -0.2500886857941829, -0.16299126099896244, 0.21939687641821184, -0.0357279716626688... |
1,712.09981 | Nonlinear quantile mixed models | In regression applications, the presence of nonlinearity and correlation
among observations offer computational challenges not only in traditional
settings such as least squares regression, but also (and especially) when the
objective function is non-smooth as in the case of quantile regression. In this
paper, we dev... | stat.ME | in regression applications the presence of nonlinearity and correlation among observations offer computational challenges not only in traditional settings such as least squares regression but also and especially when the objective function is nonsmooth as in the case of quantile regression in this paper we develop meth... | [['in', 'regression', 'applications', 'the', 'presence', 'of', 'nonlinearity', 'and', 'correlation', 'among', 'observations', 'offer', 'computational', 'challenges', 'not', 'only', 'in', 'traditional', 'settings', 'such', 'as', 'least', 'squares', 'regression', 'but', 'also', 'and', 'especially', 'when', 'the', 'object... | [-0.031071650404691585, -0.02257856413443597, -0.08895015952163446, 0.10184486379148439, -0.07018663451760146, -0.1863632892126412, -3.6565445314870394e-05, 0.3912020026977216, -0.2651680126515175, -0.2781499229830259, 0.15268103509217001, -0.27018820642451963, -0.21985528012737632, 0.1939232433475415, -0.1146204129952... |
1,712.09982 | Affinity-based measures of medical diagnostic test accuracy | We propose new summary measures of diagnostic test accuracy which can be used
as companions to existing diagnostic accuracy measures. Conceptually, our
summary measures are tantamount to the so-called Hellinger affinity and we show
that they can be regarded as measures of agreement constructed from similar
geometrica... | stat.ME | we propose new summary measures of diagnostic test accuracy which can be used as companions to existing diagnostic accuracy measures conceptually our summary measures are tantamount to the socalled hellinger affinity and we show that they can be regarded as measures of agreement constructed from similar geometrical pri... | [['we', 'propose', 'new', 'summary', 'measures', 'of', 'diagnostic', 'test', 'accuracy', 'which', 'can', 'be', 'used', 'as', 'companions', 'to', 'existing', 'diagnostic', 'accuracy', 'measures', 'conceptually', 'our', 'summary', 'measures', 'are', 'tantamount', 'to', 'the', 'socalled', 'hellinger', 'affinity', 'and', '... | [0.019929741558878392, -0.012250150575829273, -0.15177532614468306, 0.1607369011073358, -0.053718666099469924, -0.15657564698810095, 0.03774654638541282, 0.3994729872983804, -0.20290352669773531, -0.316612212727854, 0.10843338234899719, -0.2725994538088314, -0.15203262094530415, 0.2625757150664987, -0.13509262250125653... |
1,712.09983 | Random Feature-based Online Multi-kernel Learning in Environments with
Unknown Dynamics | Kernel-based methods exhibit well-documented performance in various nonlinear
learning tasks. Most of them rely on a preselected kernel, whose prudent choice
presumes task-specific prior information. Especially when the latter is not
available, multi-kernel learning has gained popularity thanks to its
flexibility in ... | stat.ML cs.LG | kernelbased methods exhibit welldocumented performance in various nonlinear learning tasks most of them rely on a preselected kernel whose prudent choice presumes taskspecific prior information especially when the latter is not available multikernel learning has gained popularity thanks to its flexibility in choosing k... | [['kernelbased', 'methods', 'exhibit', 'welldocumented', 'performance', 'in', 'various', 'nonlinear', 'learning', 'tasks', 'most', 'of', 'them', 'rely', 'on', 'a', 'preselected', 'kernel', 'whose', 'prudent', 'choice', 'presumes', 'taskspecific', 'prior', 'information', 'especially', 'when', 'the', 'latter', 'is', 'not... | [-0.05398303480530329, -0.013974861929566668, -0.09375248583422208, 0.04053316494764937, -0.14150736782488418, -0.18325638622216925, 0.01993022342369623, 0.46394583786283533, -0.25886037587859534, -0.285611364030582, 0.09092504851894305, -0.2081733438946261, -0.20126391769611088, 0.20847364000267596, -0.109704135271486... |
1,712.09984 | Low-luminosity gamma-ray bursts as the sources of ultrahigh-energy
cosmic ray nuclei | Recent results from the Pierre Auger Collaboration have shown that the
composition of ultrahigh-energy cosmic rays (UHECRs) becomes gradually heavier
with increasing energy. Although gamma-ray bursts (GRBs) have been promising
sources of UHECRs, it is still unclear whether they can account for the Auger
results becau... | astro-ph.HE astro-ph.SR hep-ph nucl-th | recent results from the pierre auger collaboration have shown that the composition of ultrahighenergy cosmic rays uhecrs becomes gradually heavier with increasing energy although gammaray bursts grbs have been promising sources of uhecrs it is still unclear whether they can account for the auger results because of thei... | [['recent', 'results', 'from', 'the', 'pierre', 'auger', 'collaboration', 'have', 'shown', 'that', 'the', 'composition', 'of', 'ultrahighenergy', 'cosmic', 'rays', 'uhecrs', 'becomes', 'gradually', 'heavier', 'with', 'increasing', 'energy', 'although', 'gammaray', 'bursts', 'grbs', 'have', 'been', 'promising', 'sources... | [-0.005302191879283169, 0.21180936821993426, -0.04055105852577368, 0.23135963994755132, -0.0889896385736174, -0.0585584204517118, 0.0247874116119478, 0.4648534970184434, -0.19286407227127222, -0.3176093210284072, -0.03177114325453691, -0.3456902147861578, -0.0028090045610476137, 0.22028660770976335, 0.03749377436526049... |
1,712.09985 | Two-sided infinite-bin models and analyticity for Barak-Erd\H{o}s graphs | In this article, we prove that for any probability distribution $\mu$ on
$\mathbb{N}$ one can construct a two-sided stationary version of the
infinite-bin model (an interacting particle system introduced by Foss and
Konstantopoulos) with move distribution $\mu$. Using this result, we obtain a
new formula for the spee... | math.PR math.CO | in this article we prove that for any probability distribution mu on mathbbn one can construct a twosided stationary version of the infinitebin model an interacting particle system introduced by foss and konstantopoulos with move distribution mu using this result we obtain a new formula for the speed of the front of in... | [['in', 'this', 'article', 'we', 'prove', 'that', 'for', 'any', 'probability', 'distribution', 'mu', 'on', 'mathbbn', 'one', 'can', 'construct', 'a', 'twosided', 'stationary', 'version', 'of', 'the', 'infinitebin', 'model', 'an', 'interacting', 'particle', 'system', 'introduced', 'by', 'foss', 'and', 'konstantopoulos',... | [-0.1372166155757973, 0.11697713605560527, -0.09855065684731505, 0.03345874018637782, -0.026528957901840528, -0.10890344105570055, 0.06871461777993274, 0.3093483719645386, -0.27017321928245264, -0.24092799971425316, 0.0844572726722307, -0.2454249805532305, -0.11451932857744396, 0.1870923505729723, -0.062050253766157276... |
1,712.09986 | Fragmentation function of gluon into spin-singlet $P$-wave quarkonium | Following the operator definition of the fragmentation function developed by
Collins and Soper, we compute the gluon-to-$h_c$ fragmentation function at the
lowest order in the velocity expansion in NRQCD factorization approach.
Utilizing some modern technique developed in the area of multi-loop
calculation, we are ab... | hep-ph | following the operator definition of the fragmentation function developed by collins and soper we compute the gluontoh_c fragmentation function at the lowest order in the velocity expansion in nrqcd factorization approach utilizing some modern technique developed in the area of multiloop calculation we are able to anal... | [['following', 'the', 'operator', 'definition', 'of', 'the', 'fragmentation', 'function', 'developed', 'by', 'collins', 'and', 'soper', 'we', 'compute', 'the', 'gluontoh_c', 'fragmentation', 'function', 'at', 'the', 'lowest', 'order', 'in', 'the', 'velocity', 'expansion', 'in', 'nrqcd', 'factorization', 'approach', 'ut... | [-0.06377342782382454, 0.14608302378494825, -0.17079102275227862, 0.11027105168073571, -0.03846754808244961, -0.016192293838996973, -0.004724228009581566, 0.3476449297208871, -0.21844273379465448, -0.19716888948210648, 0.006498360928214555, -0.25177376941345364, -0.0804410906508565, 0.10852374966655459, 0.0705007242038... |
1,712.09987 | How Short Sales Circumvent the Capital Gains Tax System | Through a short sale, a person borrows a share of stock from a lender, sells
the borrowed share to a third person at the current price, and purchases an
identical share in the market at a future date and at a future price to replace
the borrowed share of stock. This only makes sense if the short seller
anticipates a ... | q-fin.GN q-fin.TR | through a short sale a person borrows a share of stock from a lender sells the borrowed share to a third person at the current price and purchases an identical share in the market at a future date and at a future price to replace the borrowed share of stock this only makes sense if the short seller anticipates a downwa... | [['through', 'a', 'short', 'sale', 'a', 'person', 'borrows', 'a', 'share', 'of', 'stock', 'from', 'a', 'lender', 'sells', 'the', 'borrowed', 'share', 'to', 'a', 'third', 'person', 'at', 'the', 'current', 'price', 'and', 'purchases', 'an', 'identical', 'share', 'in', 'the', 'market', 'at', 'a', 'future', 'date', 'and', ... | [-0.09931849927066806, 0.09261902133685579, -0.11412665496104733, 0.10103496828889276, -0.12697403896302778, -0.23531869335962025, 0.17887166193735965, 0.38576468932838676, -0.3414236290722174, -0.23068403263893375, 0.12041282886639237, -0.39634216928661387, -0.07217413732073606, 0.14107781550921303, -0.187192023028322... |
1,712.09988 | Estimation and Inference on Heterogeneous Treatment Effects in
High-Dimensional Dynamic Panels under Weak Dependence | This paper provides estimation and inference methods for a conditional
average treatment effects (CATE) characterized by a high-dimensional parameter
in both homogeneous cross-sectional and unit-heterogeneous dynamic panel data
settings. In our leading example, we model CATE by interacting the base
treatment variable... | stat.ML | this paper provides estimation and inference methods for a conditional average treatment effects cate characterized by a highdimensional parameter in both homogeneous crosssectional and unitheterogeneous dynamic panel data settings in our leading example we model cate by interacting the base treatment variable with exp... | [['this', 'paper', 'provides', 'estimation', 'and', 'inference', 'methods', 'for', 'a', 'conditional', 'average', 'treatment', 'effects', 'cate', 'characterized', 'by', 'a', 'highdimensional', 'parameter', 'in', 'both', 'homogeneous', 'crosssectional', 'and', 'unitheterogeneous', 'dynamic', 'panel', 'data', 'settings',... | [-0.03945580157853192, 0.048637876217968154, -0.08579097344110027, 0.05479386333977718, -0.10552601434880357, -0.16514512594603664, 0.08580043285984042, 0.40189674075069803, -0.2650779833506753, -0.2549289412054091, 0.1103721630384191, -0.27274924094848385, -0.18805314071937979, 0.18033429085992914, -0.0918331364305603... |
1,712.09989 | The genus of a random bipartite graph | Archdeacon and Grable (1995) proved that the genus of the random graph
$G\in\mathcal{G}_{n,p}$ is almost surely close to $pn^2/12$ if $p=p(n)\geq3(\ln
n)^2n^{-1/2}$. In this paper we prove an analogous result for random bipartite
graphs in $\mathcal{G}_{n_1,n_2,p}$. If $n_1\ge n_2 \gg 1$, phase transitions
occur for ... | math.CO | archdeacon and grable 1995 proved that the genus of the random graph ginmathcalg_np is almost surely close to pn212 if ppngeq3ln n2n12 in this paper we prove an analogous result for random bipartite graphs in mathcalg_n_1n_2p if n_1ge n_2 gg 1 phase transitions occur for every positive integer i when pthetan_1n_2fraci2... | [['archdeacon', 'and', 'grable', '1995', 'proved', 'that', 'the', 'genus', 'of', 'the', 'random', 'graph', 'ginmathcalg_np', 'is', 'almost', 'surely', 'close', 'to', 'pn212', 'if', 'ppngeq3ln', 'n2n12', 'in', 'this', 'paper', 'we', 'prove', 'an', 'analogous', 'result', 'for', 'random', 'bipartite', 'graphs', 'in', 'mat... | [-0.13641453552544627, 0.2532207953047138, -0.02902519491131175, 0.020965696609106986, 0.025966629991945746, -0.22260959611006387, 0.009996885524692703, 0.3691496824054685, -0.2525413247871481, -0.22224036614372306, 0.12134294534797385, -0.30583334806030743, -0.19228512923909377, 0.12255871325271996, -0.064303712051821... |
1,712.0999 | 4-particle Amplituhedron at 3-loop and its Mondrian Diagrammatic
Implication | This article provides a direct calculation of the 4-particle amplituhedron at
3-loop order, by introducing a set of practical tricks. After delicately
rearranging each piece of this calculation, we find a suggestive connection
between positivity conditions and Mondrian diagrams, which will be
quantitatively defined. ... | hep-th | this article provides a direct calculation of the 4particle amplituhedron at 3loop order by introducing a set of practical tricks after delicately rearranging each piece of this calculation we find a suggestive connection between positivity conditions and mondrian diagrams which will be quantitatively defined such a pa... | [['this', 'article', 'provides', 'a', 'direct', 'calculation', 'of', 'the', '4particle', 'amplituhedron', 'at', '3loop', 'order', 'by', 'introducing', 'a', 'set', 'of', 'practical', 'tricks', 'after', 'delicately', 'rearranging', 'each', 'piece', 'of', 'this', 'calculation', 'we', 'find', 'a', 'suggestive', 'connection... | [-0.12021648466868914, 0.17896714109290196, -0.09176244269014876, 0.07031458036324598, -0.08700614301242719, -0.08188025856170018, 0.05346908919072073, 0.3527052904185104, -0.22063993657081338, -0.28857572974735185, 0.06657862932249707, -0.2651777303115906, -0.2131501654971783, 0.1618981103804943, -0.019472231910760075... |
1,712.09991 | One-Loop Integrals from Spherical Projections of Planes and Quadrics | We initiate a systematic study of one-loop integrals by investigating the
connection between their singularity structures and geometric configurations in
the projective space associated to their Feynman parametrization. We analyze
these integrals by two recursive methods, which leads to two independent
algebraic algo... | hep-th hep-ph | we initiate a systematic study of oneloop integrals by investigating the connection between their singularity structures and geometric configurations in the projective space associated to their feynman parametrization we analyze these integrals by two recursive methods which leads to two independent algebraic algorithm... | [['we', 'initiate', 'a', 'systematic', 'study', 'of', 'oneloop', 'integrals', 'by', 'investigating', 'the', 'connection', 'between', 'their', 'singularity', 'structures', 'and', 'geometric', 'configurations', 'in', 'the', 'projective', 'space', 'associated', 'to', 'their', 'feynman', 'parametrization', 'we', 'analyze',... | [-0.17882669862987222, 0.13223306170933075, -0.11957517728580445, 0.11642675840994343, -0.0922106320070008, -0.08553921080873174, 0.04212667750218346, 0.34327495637965405, -0.27192003451193036, -0.23031979322165125, 0.06872757267447631, -0.2401913511685206, -0.17553848550276105, 0.17636831838763872, -0.0577293740715180... |
1,712.09992 | A three-dimensional magnetic topological phase | We use photoemission spectroscopy to discover the first topological magnet in
three dimensions, the material Co$_2$MnGa.
| cond-mat.mtrl-sci cond-mat.mes-hall | we use photoemission spectroscopy to discover the first topological magnet in three dimensions the material co_2mnga | [['we', 'use', 'photoemission', 'spectroscopy', 'to', 'discover', 'the', 'first', 'topological', 'magnet', 'in', 'three', 'dimensions', 'the', 'material', 'co_2mnga']] | [-0.1404354692203924, 0.1471848475630395, -0.06946078594774008, -0.0089498539455235, -0.09847192419692874, -0.1531298375921324, 0.06881145620718598, 0.43501141294837, -0.30359981348738074, -0.31388339726254344, 0.025012607096869033, -0.42910873237997293, -0.18374161329120398, 0.16878692200407386, 0.062382300675380975, ... |
1,712.09993 | First Data Release of the ESO-ARO Public Survey SAMPLING --- SMT
"All-sky" Mapping of PLanck Interstellar Nebulae in the Galaxy | We make the first data release (DR1) of the ongoing ESO Public Survey
SAMPLING (http://dx.doi.org/10.7910/DVN/0L8NHX). DR1 comprises of 124 fields
distributed in $70^\circ < l < 216^\circ$, $-35^\circ < b < 25^\circ$. The 12CO
and 13CO (2-1) cubes are gridded in $8"$ pixels, with an effective resolution
of $36"$. The... | astro-ph.GA | we make the first data release dr1 of the ongoing eso public survey sampling httpdxdoiorg107910dvn0l8nhx dr1 comprises of 124 fields distributed in 70circ l 216circ 35circ b 25circ the 12co and 13co 21 cubes are gridded in 8 pixels with an effective resolution of 36 the channel width is 033 kms and the rms noise is t_r... | [['we', 'make', 'the', 'first', 'data', 'release', 'dr1', 'of', 'the', 'ongoing', 'eso', 'public', 'survey', 'sampling', 'httpdxdoiorg107910dvn0l8nhx', 'dr1', 'comprises', 'of', '124', 'fields', 'distributed', 'in', '70circ', 'l', '216circ', '35circ', 'b', '25circ', 'the', '12co', 'and', '13co', '21', 'cubes', 'are', '... | [-0.12713362631836422, 0.10105385191118442, -0.023500544065034684, 0.0336798681664844, -0.09373037358975889, -0.05486155285810431, 0.038952851231083455, 0.43364345624950934, -0.22398474676833477, -0.33765221844760723, 0.11639436708337823, -0.3193836463270364, 0.05179280455707124, 0.12996492587765793, -0.019901692131419... |
1,712.09994 | All-loop Mondrian Diagrammatics and 4-particle Amplituhedron | Based on 1712.09990 which handles the 4-particle amplituhedron at 3-loop, we
have found an extremely simple pattern, yet far more non-trivial than one might
naturally expect: the all-loop Mondrian diagrammatics. By further simplifying
and rephrasing the key relation of positivity in the amplituhedron setting,
remarka... | hep-th | based on 171209990 which handles the 4particle amplituhedron at 3loop we have found an extremely simple pattern yet far more nontrivial than one might naturally expect the allloop mondrian diagrammatics by further simplifying and rephrasing the key relation of positivity in the amplituhedron setting remarkably we find ... | [['based', 'on', '171209990', 'which', 'handles', 'the', '4particle', 'amplituhedron', 'at', '3loop', 'we', 'have', 'found', 'an', 'extremely', 'simple', 'pattern', 'yet', 'far', 'more', 'nontrivial', 'than', 'one', 'might', 'naturally', 'expect', 'the', 'allloop', 'mondrian', 'diagrammatics', 'by', 'further', 'simplif... | [-0.1160169561863532, 0.12383883004254635, -0.09594464973601538, 0.13329458898838817, -0.12567093619964673, -0.12267553337021835, 0.07058347976007671, 0.36219458160318296, -0.2557433058835428, -0.26640222065012764, 0.09415152542534526, -0.2560009860820611, -0.17806734765051968, 0.16864595368927068, -0.03111437556713267... |
1,712.09995 | AdS backgrounds and induced gravity | In this paper we look for AdS solutions to generalised gravity theories in
the bulk in various spacetime dimensions. The bulk gravity action includes the
action of a non-minimally coupled scalar field with gravity, and a
higher-derivative action of gravity. The usual Einstein-Hilbert gravity is
induced when the scala... | hep-th gr-qc hep-ph | in this paper we look for ads solutions to generalised gravity theories in the bulk in various spacetime dimensions the bulk gravity action includes the action of a nonminimally coupled scalar field with gravity and a higherderivative action of gravity the usual einsteinhilbert gravity is induced when the scalar acquir... | [['in', 'this', 'paper', 'we', 'look', 'for', 'ads', 'solutions', 'to', 'generalised', 'gravity', 'theories', 'in', 'the', 'bulk', 'in', 'various', 'spacetime', 'dimensions', 'the', 'bulk', 'gravity', 'action', 'includes', 'the', 'action', 'of', 'a', 'nonminimally', 'coupled', 'scalar', 'field', 'with', 'gravity', 'and... | [-0.21948520971332178, 0.18063664477491795, -0.1024980167316836, 0.06123368883895319, -0.1099063151700119, -0.14457034378659067, -0.07641112093873278, 0.22582572379127838, -0.1821781948850447, -0.27233479109722686, 0.02576972831170573, -0.3032554395410211, -0.17191582676402273, 0.09583042472124446, -0.05521962316273603... |
1,712.09996 | Gauge-invariant screening masses and static quark free energies in $N_f
= 2+1$ QCD at non-zero baryon density | We discuss the extension of gauge-invariant electric and magnetic screening
masses in the Quark-Gluon Plasma to the case of a finite baryon density,
defining them in terms of a matrix of Polyakov loop correlators. We present
lattice results for $N_f=2+1$ QCD with physical quark masses, obtained using
the imaginary ch... | hep-lat hep-ph hep-th | we discuss the extension of gaugeinvariant electric and magnetic screening masses in the quarkgluon plasma to the case of a finite baryon density defining them in terms of a matrix of polyakov loop correlators we present lattice results for n_f21 qcd with physical quark masses obtained using the imaginary chemical pote... | [['we', 'discuss', 'the', 'extension', 'of', 'gaugeinvariant', 'electric', 'and', 'magnetic', 'screening', 'masses', 'in', 'the', 'quarkgluon', 'plasma', 'to', 'the', 'case', 'of', 'a', 'finite', 'baryon', 'density', 'defining', 'them', 'in', 'terms', 'of', 'a', 'matrix', 'of', 'polyakov', 'loop', 'correlators', 'we', ... | [-0.11345808016568688, 0.23019914864895066, -0.10345466348808259, 0.0812608725624159, -0.036436730746312866, -0.08169065336031574, 0.10457658665753634, 0.3470507101022771, -0.186231472509514, -0.2438832204323262, 0.027813422545191965, -0.29727190393023195, -0.07888476943065013, 0.10009075421174722, 0.0768777472831841, ... |
1,712.09997 | Noncommutative momentum and torsional regularization | We show that in the presence of the torsion tensor $S^k_{\phantom{k}ij}$, the
quantum commutation relation for the four-momentum, traced over spinor indices,
is given by $[p_i,p_j]=2i\hbar S^k_{\phantom{k}ij}p_k$. In the Einstein--Cartan
theory of gravity, in which torsion is coupled to spin of fermions, this
relatio... | gr-qc hep-th quant-ph | we show that in the presence of the torsion tensor sk_phantomkij the quantum commutation relation for the fourmomentum traced over spinor indices is given by p_ip_j2ihbar sk_phantomkijp_k in the einsteincartan theory of gravity in which torsion is coupled to spin of fermions this relation in a coordinate frame reduces ... | [['we', 'show', 'that', 'in', 'the', 'presence', 'of', 'the', 'torsion', 'tensor', 'sk_phantomkij', 'the', 'quantum', 'commutation', 'relation', 'for', 'the', 'fourmomentum', 'traced', 'over', 'spinor', 'indices', 'is', 'given', 'by', 'p_ip_j2ihbar', 'sk_phantomkijp_k', 'in', 'the', 'einsteincartan', 'theory', 'of', 'g... | [-0.18631515610857163, 0.20690740142628938, -0.09913375981678083, 0.07505357481857082, -0.09904307501745366, -0.0890199324047124, 0.027061929835807953, 0.33344942187919974, -0.23487634910270572, -0.24898765248951144, -0.006506123515979323, -0.261916103491944, -0.11576377730028181, 0.15011960931988336, -0.04476043504845... |
1,712.09998 | Revisiting non-Gaussianity from non-attractor inflation models | Non-attractor inflation is known as the only single field inflationary
scenario that can violate non-Gaussianity consistency relation with the
Bunch-Davies vacuum state and generate large local non-Gaussianity. However, it
is also known that the non-attractor inflation by itself is incomplete and
should be followed b... | astro-ph.CO gr-qc hep-ph hep-th | nonattractor inflation is known as the only single field inflationary scenario that can violate nongaussianity consistency relation with the bunchdavies vacuum state and generate large local nongaussianity however it is also known that the nonattractor inflation by itself is incomplete and should be followed by a phase... | [['nonattractor', 'inflation', 'is', 'known', 'as', 'the', 'only', 'single', 'field', 'inflationary', 'scenario', 'that', 'can', 'violate', 'nongaussianity', 'consistency', 'relation', 'with', 'the', 'bunchdavies', 'vacuum', 'state', 'and', 'generate', 'large', 'local', 'nongaussianity', 'however', 'it', 'is', 'also', ... | [-0.13373671644480395, 0.21811168192535157, -0.1275280183577073, 0.10376057278104553, -0.04434501508963464, -0.11953471186815907, -0.0080249588403979, 0.3088784696202469, -0.26473736898928335, -0.2760762056554498, 0.10759052810323262, -0.22815533109982064, -0.1481236950937387, 0.1108193932975895, -0.013264469883446149,... |
1,712.09999 | Parallel Active Subspace Decomposition for Scalable and Efficient Tensor
Robust Principal Component Analysis | Tensor robust principal component analysis (TRPCA) has received a substantial
amount of attention in various fields. Most existing methods, normally relying
on tensor nuclear norm minimization, need to pay an expensive computational
cost due to multiple singular value decompositions (SVDs) at each iteration. To
overc... | cs.NA cs.LG math.NA | tensor robust principal component analysis trpca has received a substantial amount of attention in various fields most existing methods normally relying on tensor nuclear norm minimization need to pay an expensive computational cost due to multiple singular value decompositions svds at each iteration to overcome the dr... | [['tensor', 'robust', 'principal', 'component', 'analysis', 'trpca', 'has', 'received', 'a', 'substantial', 'amount', 'of', 'attention', 'in', 'various', 'fields', 'most', 'existing', 'methods', 'normally', 'relying', 'on', 'tensor', 'nuclear', 'norm', 'minimization', 'need', 'to', 'pay', 'an', 'expensive', 'computatio... | [-0.0925331263076455, 0.013001842053107553, -0.07729112585421498, 0.051494604468056815, -0.12278768982549634, -0.15720574424714087, 0.0014131460847226973, 0.41026008671408964, -0.3114814169069787, -0.26878474558456034, 0.13780982058813585, -0.2511333372160981, -0.14531138705353464, 0.18253370073824365, -0.0763341774486... |
1,712.1 | Simplex-like Structures of Maximally Supersymmetric Scattering
Amplitudes | We elaborate the two-fold simplex-like structures of tree amplitudes in
planar maximally supersymmetric Yang-Mills (N=4 SYM), through its connection to
a mathematical structure known as the positive Grassmannian. Exploiting the
reduced Grassmannian geometry and the matrix form of on-shell recursion
relation in terms ... | hep-th | we elaborate the twofold simplexlike structures of tree amplitudes in planar maximally supersymmetric yangmills n4 sym through its connection to a mathematical structure known as the positive grassmannian exploiting the reduced grassmannian geometry and the matrix form of onshell recursion relation in terms of super mo... | [['we', 'elaborate', 'the', 'twofold', 'simplexlike', 'structures', 'of', 'tree', 'amplitudes', 'in', 'planar', 'maximally', 'supersymmetric', 'yangmills', 'n4', 'sym', 'through', 'its', 'connection', 'to', 'a', 'mathematical', 'structure', 'known', 'as', 'the', 'positive', 'grassmannian', 'exploiting', 'the', 'reduced... | [-0.15783756591796796, 0.22897736281962958, -0.04945553000046251, 0.09738771594129503, -0.09456052774961184, -0.10647724052250851, 0.030870984255064588, 0.31561756028289284, -0.24669940626093498, -0.2647464169810216, 0.06723918720672373, -0.2190764038823545, -0.2354843703263517, 0.11809391475981101, -0.0676433806177859... |
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