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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710.2253 | McKay's correspondence for cocompact discrete subgroups of SU(1,1) | The classical McKay correspondence establishes an explicit link from the
representation theory of a finite subgroup G of SU(2) and the geometry of the
minimal resolution of the quotient of the affine plane by G. In this paper we
discuss a possible generalization of the McKay correspondence to the case when
G is repla... | math.AG math.GT | the classical mckay correspondence establishes an explicit link from the representation theory of a finite subgroup g of su2 and the geometry of the minimal resolution of the quotient of the affine plane by g in this paper we discuss a possible generalization of the mckay correspondence to the case when g is replaced w... | [['the', 'classical', 'mckay', 'correspondence', 'establishes', 'an', 'explicit', 'link', 'from', 'the', 'representation', 'theory', 'of', 'a', 'finite', 'subgroup', 'g', 'of', 'su2', 'and', 'the', 'geometry', 'of', 'the', 'minimal', 'resolution', 'of', 'the', 'quotient', 'of', 'the', 'affine', 'plane', 'by', 'g', 'in'... | [-0.19283335916614824, 0.0729514585106829, -0.10577635040135647, 0.026143009837791657, -0.1357313427184376, -0.12422446717391722, 0.039663759536259544, 0.35326930312190336, -0.34794519691994147, -0.22962234066134052, 0.07829311273755073, -0.22495042671965035, -0.16002400766592473, 0.1902971218015799, -0.183957336349911... |
710.2254 | Adding inverses to diagrams II: Invertible homotopy theories are spaces | In previous work, we showed that there are appropriate model category
structures on the category of simplicial categories and on the category of
Segal precategories, and that they are Quillen equivalent to one another and to
Rezk's complete Segal space model structure on the category of simplicial
spaces. Here, we sh... | math.AT math.CT | in previous work we showed that there are appropriate model category structures on the category of simplicial categories and on the category of segal precategories and that they are quillen equivalent to one another and to rezks complete segal space model structure on the category of simplicial spaces here we show that... | [['in', 'previous', 'work', 'we', 'showed', 'that', 'there', 'are', 'appropriate', 'model', 'category', 'structures', 'on', 'the', 'category', 'of', 'simplicial', 'categories', 'and', 'on', 'the', 'category', 'of', 'segal', 'precategories', 'and', 'that', 'they', 'are', 'quillen', 'equivalent', 'to', 'one', 'another', ... | [-0.0640928581405174, 0.023213782616698278, -0.04718087443375382, 0.1865684623249951, -0.11326375278917238, -0.12607450161032893, -0.024237169338197542, 0.5004517059644749, -0.3642285937636063, -0.19208407785004838, 0.0738748875677441, -0.22863181547165431, -0.17709229682002153, 0.14472356419970184, -0.2586347643117388... |
710.2255 | A phase-space study of jet formation in planetary-scale fluids | The interaction between planetary waves and an arbitrary zonal flow is
studied from a phase-space viewpoint. Using the Wigner distribution, a
planetary wave Vlasov equation is derived that includes the contribution of the
mean flow to the zonal potential vorticity gradient. This equation is applied
to the problem of ... | physics.flu-dyn physics.ao-ph | the interaction between planetary waves and an arbitrary zonal flow is studied from a phasespace viewpoint using the wigner distribution a planetary wave vlasov equation is derived that includes the contribution of the mean flow to the zonal potential vorticity gradient this equation is applied to the problem of planet... | [['the', 'interaction', 'between', 'planetary', 'waves', 'and', 'an', 'arbitrary', 'zonal', 'flow', 'is', 'studied', 'from', 'a', 'phasespace', 'viewpoint', 'using', 'the', 'wigner', 'distribution', 'a', 'planetary', 'wave', 'vlasov', 'equation', 'is', 'derived', 'that', 'includes', 'the', 'contribution', 'of', 'the', ... | [-0.16370359067852147, 0.1406828428391071, -0.15904957259243185, 0.09461327736392956, -0.14210049095775254, -0.05053002727829447, -0.06635598298820733, 0.28053472067124796, -0.28585175722084866, -0.2170888146366736, 0.044054682153709834, -0.23790664406436862, -0.13503815215363196, 0.19555012955603124, 0.019049894186959... |
710.2256 | Integral transformation solution of free-space cylindrical vector beams
and prediction of modified-Bessel-Gaussian vector beams | A unified description of the free-space cylindrical vector beams is
presented, which is an integral transformation solution to the vector Helmholtz
equation and the transversality condition. The amplitude 2-form of the angular
spectrum involved in this solution can be arbitrarily chosen. When one of the
two elements ... | physics.optics | a unified description of the freespace cylindrical vector beams is presented which is an integral transformation solution to the vector helmholtz equation and the transversality condition the amplitude 2form of the angular spectrum involved in this solution can be arbitrarily chosen when one of the two elements is zero... | [['a', 'unified', 'description', 'of', 'the', 'freespace', 'cylindrical', 'vector', 'beams', 'is', 'presented', 'which', 'is', 'an', 'integral', 'transformation', 'solution', 'to', 'the', 'vector', 'helmholtz', 'equation', 'and', 'the', 'transversality', 'condition', 'the', 'amplitude', '2form', 'of', 'the', 'angular',... | [-0.212699381180458, 0.18720334529139604, -0.07580899241112984, 0.049761940214533985, -0.12984095873440257, -0.17242068561752982, -0.05349579104913933, 0.39395408622809863, -0.2813267859095468, -0.21109058135327433, 0.0482339320432321, -0.2522143344625388, -0.06984613429395353, 0.1643964151718128, 0.02904206722234791, ... |
710.2257 | Finite Unified Theories confronted with low-energy phenomenology | Finite Unified Theories (FUTs) are N=1 supersymmetric Grand Unified Theories
that can be made all-loop finite. The requirement of all-loop finiteness leads
to a severe reduction of the free parameters of the theory and, in turn, to a
large number of predictions. Here SU(5) FUTs are investigated in the context of
low-... | hep-ph | finite unified theories futs are n1 supersymmetric grand unified theories that can be made allloop finite the requirement of allloop finiteness leads to a severe reduction of the free parameters of the theory and in turn to a large number of predictions here su5 futs are investigated in the context of lowenergy phenome... | [['finite', 'unified', 'theories', 'futs', 'are', 'n1', 'supersymmetric', 'grand', 'unified', 'theories', 'that', 'can', 'be', 'made', 'allloop', 'finite', 'the', 'requirement', 'of', 'allloop', 'finiteness', 'leads', 'to', 'a', 'severe', 'reduction', 'of', 'the', 'free', 'parameters', 'of', 'the', 'theory', 'and', 'in... | [-0.08439018981816777, 0.2383693360798333, -0.09937983452186097, 0.16437654038143418, -0.08592126633713607, -0.14847864225391216, 0.050719000754306895, 0.2717851323507264, -0.1954858334476713, -0.35470890060719784, 0.03919753680569901, -0.2492900149009605, -0.019706200216862844, 0.1357659522306351, 0.01459661647541462,... |
710.2258 | Control of generalized error rates in multiple testing | Consider the problem of testing $s$ hypotheses simultaneously. The usual
approach restricts attention to procedures that control the probability of even
one false rejection, the familywise error rate (FWER). If $s$ is large, one
might be willing to tolerate more than one false rejection, thereby increasing
the abilit... | math.ST stat.TH | consider the problem of testing s hypotheses simultaneously the usual approach restricts attention to procedures that control the probability of even one false rejection the familywise error rate fwer if s is large one might be willing to tolerate more than one false rejection thereby increasing the ability of the proc... | [['consider', 'the', 'problem', 'of', 'testing', 's', 'hypotheses', 'simultaneously', 'the', 'usual', 'approach', 'restricts', 'attention', 'to', 'procedures', 'that', 'control', 'the', 'probability', 'of', 'even', 'one', 'false', 'rejection', 'the', 'familywise', 'error', 'rate', 'fwer', 'if', 's', 'is', 'large', 'one... | [-0.06375823215500065, 0.060985614375739884, -0.03508960967529502, 0.04816620038292132, -0.06259150791840905, -0.221801322132091, 0.14854184614425223, 0.29439147917779535, -0.19240675790697914, -0.3683125783714491, 0.08647640319021947, -0.2694297103939666, -0.1417050182448096, 0.1834161267277621, -0.1615091601195525, 0... |
710.2259 | Sub-THz electrodynamics of the graphene-like superconductor CaAlSi | We report the first optical study of CaAlSi, a superconductor which displays
both the crystal structure of MgB2 and the electronic band structure of
intercalated graphites. The reflectivity of a CaAlSi single crystal was
measured down to sub-THz frequencies and to 3.3 K, with the use of Coherent
Synchrotron Radiation... | cond-mat.supr-con cond-mat.str-el | we report the first optical study of caalsi a superconductor which displays both the crystal structure of mgb2 and the electronic band structure of intercalated graphites the reflectivity of a caalsi single crystal was measured down to subthz frequencies and to 33 k with the use of coherent synchrotron radiation a supe... | [['we', 'report', 'the', 'first', 'optical', 'study', 'of', 'caalsi', 'a', 'superconductor', 'which', 'displays', 'both', 'the', 'crystal', 'structure', 'of', 'mgb2', 'and', 'the', 'electronic', 'band', 'structure', 'of', 'intercalated', 'graphites', 'the', 'reflectivity', 'of', 'a', 'caalsi', 'single', 'crystal', 'was... | [-0.15734320392154835, 0.17141934952153612, -0.047467162493955, -0.022861433297459207, -0.04842418056531725, -0.09963995692140254, 0.10969448050441728, 0.4559636303562332, -0.26975125081794843, -0.30693434026430955, 0.016816147665270943, -0.3156805920668624, -0.06792172107485715, 0.18489371793640946, 0.0886156745202077... |
710.226 | Nonisospectral integrable nonlinear equations with external potentials
and their GBDT solutions | Auxiliary systems for matrix nonisospectral equations, including coupled NLS
with external potential and KdV with variable coefficients, were introduced.
Explicit solutions of nonisospectral equations were constructed using the GBDT
version of the B\"acklund-Darboux transformation.
| nlin.SI | auxiliary systems for matrix nonisospectral equations including coupled nls with external potential and kdv with variable coefficients were introduced explicit solutions of nonisospectral equations were constructed using the gbdt version of the backlunddarboux transformation | [['auxiliary', 'systems', 'for', 'matrix', 'nonisospectral', 'equations', 'including', 'coupled', 'nls', 'with', 'external', 'potential', 'and', 'kdv', 'with', 'variable', 'coefficients', 'were', 'introduced', 'explicit', 'solutions', 'of', 'nonisospectral', 'equations', 'were', 'constructed', 'using', 'the', 'gbdt', '... | [-0.1204552416525343, 0.05328889681464609, -0.01900432666982798, 0.02452600100899444, -0.14256949991206913, -0.25246871536707177, -0.10849579018266763, 0.291902082890053, -0.2716713157646796, -0.2726983659188537, 0.17592647233430078, -0.3219847088159226, -0.20704376807107644, 0.14439641777426004, 0.011659723158706637, ... |
710.2261 | Comparison of work fluctuation relations | We compare two predictions regarding the microscopic fluctuations of a system
that is driven away from equilibrium: one due to Crooks [J. Stat. Phys. 90,
1481 (1998)] which has gained recent attention in the context of nonequilibrium
work and fluctuation theorems, and an earlier, analogous result obtained by
Bochkov ... | cond-mat.stat-mech | we compare two predictions regarding the microscopic fluctuations of a system that is driven away from equilibrium one due to crooks j stat phys 90 1481 1998 which has gained recent attention in the context of nonequilibrium work and fluctuation theorems and an earlier analogous result obtained by bochkov and kuzovlev ... | [['we', 'compare', 'two', 'predictions', 'regarding', 'the', 'microscopic', 'fluctuations', 'of', 'a', 'system', 'that', 'is', 'driven', 'away', 'from', 'equilibrium', 'one', 'due', 'to', 'crooks', 'j', 'stat', 'phys', '90', '1481', '1998', 'which', 'has', 'gained', 'recent', 'attention', 'in', 'the', 'context', 'of', ... | [-0.08186522086239043, 0.11350213531202187, -0.1113144813193562, 0.0785332806162596, -0.007824319580764938, -0.12975920738992155, 0.0886477110545604, 0.28970540428181757, -0.22118784104335448, -0.3230573997763615, 0.0492906943765922, -0.29327104938675874, -0.14320742335749437, 0.21789104312758995, -0.0647263916907832, ... |
710.2262 | A Method for Weak Lensing Flexion Analysis by the HOLICs Moment Approach | We have developed a method for measuring higher-order weak lensing
distortions of faint background galaxies, namely the weak gravitational
flexion, by fully extending the Kaiser, Squires & Broadhurst method to include
higher-order lensing image characteristics (HOLICs) introduced by Okura,
Umetsu, & Futamase. We take... | astro-ph | we have developed a method for measuring higherorder weak lensing distortions of faint background galaxies namely the weak gravitational flexion by fully extending the kaiser squires broadhurst method to include higherorder lensing image characteristics holics introduced by okura umetsu futamase we take into account ex... | [['we', 'have', 'developed', 'a', 'method', 'for', 'measuring', 'higherorder', 'weak', 'lensing', 'distortions', 'of', 'faint', 'background', 'galaxies', 'namely', 'the', 'weak', 'gravitational', 'flexion', 'by', 'fully', 'extending', 'the', 'kaiser', 'squires', 'broadhurst', 'method', 'to', 'include', 'higherorder', '... | [-0.07486804794188183, 0.00879502025753315, -0.10362653505969976, 0.12050574907392153, -0.09797584552705141, -0.05960987193284022, -0.022133982152502875, 0.37423392347438206, -0.18436818140761185, -0.3300054072319428, 0.022221855870877407, -0.2969456226473454, -0.08835384693679095, 0.21334999612080727, 0.01391853144741... |
710.2263 | Efficient Stochastic Simulations of Complex Reaction Networks on
Surfaces | Surfaces serve as highly efficient catalysts for a vast variety of chemical
reactions. Typically, such surface reactions involve billions of molecules
which diffuse and react over macroscopic areas. Therefore, stochastic
fluctuations are negligible and the reaction rates can be evaluated using rate
equations, which a... | cond-mat.stat-mech | surfaces serve as highly efficient catalysts for a vast variety of chemical reactions typically such surface reactions involve billions of molecules which diffuse and react over macroscopic areas therefore stochastic fluctuations are negligible and the reaction rates can be evaluated using rate equations which are base... | [['surfaces', 'serve', 'as', 'highly', 'efficient', 'catalysts', 'for', 'a', 'vast', 'variety', 'of', 'chemical', 'reactions', 'typically', 'such', 'surface', 'reactions', 'involve', 'billions', 'of', 'molecules', 'which', 'diffuse', 'and', 'react', 'over', 'macroscopic', 'areas', 'therefore', 'stochastic', 'fluctuatio... | [-0.10545612025663069, 0.1352330088989505, -0.05324494671970353, 0.06465062031241828, -0.03301133676607427, -0.12104181726911264, 0.026255291648195456, 0.3206528393789409, -0.2949390777359448, -0.28291179663716, 0.062330967762262005, -0.26374650238691655, -0.1612918219318668, 0.22804879907627734, -0.029171936258782775,... |
710.2264 | Evaluation of the Multiplane Method for Efficient Simulations of
Reaction Networks | Reaction networks in the bulk and on surfaces are widespread in physical,
chemical and biological systems. In macroscopic systems, which include large
populations of reactive species, stochastic fluctuations are negligible and the
reaction rates can be evaluated using rate equations. However, many physical
systems ar... | cond-mat.stat-mech cond-mat.other | reaction networks in the bulk and on surfaces are widespread in physical chemical and biological systems in macroscopic systems which include large populations of reactive species stochastic fluctuations are negligible and the reaction rates can be evaluated using rate equations however many physical systems are partit... | [['reaction', 'networks', 'in', 'the', 'bulk', 'and', 'on', 'surfaces', 'are', 'widespread', 'in', 'physical', 'chemical', 'and', 'biological', 'systems', 'in', 'macroscopic', 'systems', 'which', 'include', 'large', 'populations', 'of', 'reactive', 'species', 'stochastic', 'fluctuations', 'are', 'negligible', 'and', 't... | [-0.14327518804742384, 0.08123876499966202, -0.022871310065496683, 0.024039690878482595, -0.02968492798015265, -0.10404968577166719, 0.031003910528529705, 0.3144703259083232, -0.25435462576757756, -0.2939916956050682, 0.062217097441222696, -0.26435663852645386, -0.16437002660747949, 0.21856140349465872, -0.038406214536... |
710.2265 | Controlling spatiotemporal chaos and spiral turbulence in excitable
media: A review | Excitable media are a generic class of models used to simulate a wide variety
of natural systems including cardiac tissue. Propagation of excitation waves in
this medium results in the formation of characteristic patterns such as
rotating spiral waves. Instabilities in these structures may lead to
spatiotemporal chao... | nlin.CD q-bio.TO | excitable media are a generic class of models used to simulate a wide variety of natural systems including cardiac tissue propagation of excitation waves in this medium results in the formation of characteristic patterns such as rotating spiral waves instabilities in these structures may lead to spatiotemporal chaos th... | [['excitable', 'media', 'are', 'a', 'generic', 'class', 'of', 'models', 'used', 'to', 'simulate', 'a', 'wide', 'variety', 'of', 'natural', 'systems', 'including', 'cardiac', 'tissue', 'propagation', 'of', 'excitation', 'waves', 'in', 'this', 'medium', 'results', 'in', 'the', 'formation', 'of', 'characteristic', 'patter... | [-0.1159041170968855, 0.10191519990255185, -0.06269473527564848, 0.07536488421941377, -0.0778852922778255, -0.12597679699563402, -0.05159352460068738, 0.3847569949429134, -0.2697998717320051, -0.25222051980496524, 0.13233755810208042, -0.22228766176782602, -0.20864417253015227, 0.23469910956249176, -0.04135043419589349... |
710.2266 | Bihermitian metrics on Hopf surfaces | Inspired by a construction due to Hitchin, we produce strongly bihermitian
metrics on certain Hopf complex surfaces, which integrate the locally
conformally Kaehler metrics found by Gauduchon and Ornea. We also show that the
Inoue complex surfaces with zero second Betti number do not admit bihermitian
metrics. This c... | math.DG math-ph math.MP | inspired by a construction due to hitchin we produce strongly bihermitian metrics on certain hopf complex surfaces which integrate the locally conformally kaehler metrics found by gauduchon and ornea we also show that the inoue complex surfaces with zero second betti number do not admit bihermitian metrics this complet... | [['inspired', 'by', 'a', 'construction', 'due', 'to', 'hitchin', 'we', 'produce', 'strongly', 'bihermitian', 'metrics', 'on', 'certain', 'hopf', 'complex', 'surfaces', 'which', 'integrate', 'the', 'locally', 'conformally', 'kaehler', 'metrics', 'found', 'by', 'gauduchon', 'and', 'ornea', 'we', 'also', 'show', 'that', '... | [-0.21835241081813972, 0.08404001640155911, -0.035716314272334175, 0.10537092209754823, -0.18486233617489536, -0.19112707630265505, -0.0975759752560407, 0.37523408493337534, -0.18869868790109953, -0.22431067892660697, 0.08222659740907451, -0.23220979881783327, -0.3030724725996455, 0.22361022952827625, -0.20791092260430... |
710.2267 | A Note on the Effective Non-vanishing Conjecture | We give a reduction of the irregular case for the effective non-vanishing
conjecture by virtue of the Fourier-Mukai transform. As a consequence, we
reprove that the effective non-vanishing conjecture holds on algebraic
surfaces.
| math.AG | we give a reduction of the irregular case for the effective nonvanishing conjecture by virtue of the fouriermukai transform as a consequence we reprove that the effective nonvanishing conjecture holds on algebraic surfaces | [['we', 'give', 'a', 'reduction', 'of', 'the', 'irregular', 'case', 'for', 'the', 'effective', 'nonvanishing', 'conjecture', 'by', 'virtue', 'of', 'the', 'fouriermukai', 'transform', 'as', 'a', 'consequence', 'we', 'reprove', 'that', 'the', 'effective', 'nonvanishing', 'conjecture', 'holds', 'on', 'algebraic', 'surface... | [-0.2127469755765615, 0.0707473520253023, -0.16977847051439862, 0.1590490017199155, -0.08733076963460806, -0.15494372467087072, 0.019648806728196865, 0.24253716997124933, -0.2454416412069942, -0.2517074059243455, 0.09901176246278214, -0.1900294542623063, -0.2257539521564137, 0.22337556472330383, -0.13621638370960049, -... |
710.2268 | Complexity of some Path Problems in DAGs and Linear Orders | We investigate here the computational complexity of three natural problems in
directed acyclic graphs. We prove their NP Completeness and consider their
restrictions to linear orders.
| math.CO cs.IT math.IT | we investigate here the computational complexity of three natural problems in directed acyclic graphs we prove their np completeness and consider their restrictions to linear orders | [['we', 'investigate', 'here', 'the', 'computational', 'complexity', 'of', 'three', 'natural', 'problems', 'in', 'directed', 'acyclic', 'graphs', 'we', 'prove', 'their', 'np', 'completeness', 'and', 'consider', 'their', 'restrictions', 'to', 'linear', 'orders']] | [-0.1691875307319256, 0.08735841691780549, 0.027895663721630208, 0.1576145701826765, -0.14744955953210592, -0.07450958839259468, 0.06883489978141509, 0.43101553403987336, -0.3988984093929713, -0.33616081145233834, 0.08554974905340575, -0.22679068413204873, -0.12536003082417524, 0.0997053522330064, -0.11184367170342459,... |
710.2269 | On the Farrell-Jones and related Conjectures | These extended notes are based on a series of six lectures presented at the
summer school ``Cohomology of groups and algebraic $K$-theory'' which took
place in Hangzhou, China from July 1 until July 12 in 2007. They give an
introduction to the Farrell-Jones and the Baum-Connes Conjecture.
| math.KT | these extended notes are based on a series of six lectures presented at the summer school cohomology of groups and algebraic ktheory which took place in hangzhou china from july 1 until july 12 in 2007 they give an introduction to the farrelljones and the baumconnes conjecture | [['these', 'extended', 'notes', 'are', 'based', 'on', 'a', 'series', 'of', 'six', 'lectures', 'presented', 'at', 'the', 'summer', 'school', 'cohomology', 'of', 'groups', 'and', 'algebraic', 'ktheory', 'which', 'took', 'place', 'in', 'hangzhou', 'china', 'from', 'july', '1', 'until', 'july', '12', 'in', '2007', 'they', ... | [-0.08791233642779767, 0.1188210212415644, -0.19998731207538475, 0.07522989752048508, -0.07501150414030602, -0.12450573193107514, -0.03567769220891468, 0.2680126847897438, -0.2126308842661216, -0.40609346680897984, 0.2349146711293291, -0.2633596798764205, -0.1481427792756957, 0.21012771298038832, -0.1760940177445399, -... |
710.227 | On the low-energy density of states in disordered d-wave superconductor | We study the low-energy density of states of Dirac fermions in disordered
d-wave superconductor. At zero energy, a finite density of states is obtained
via the mechanism of dynamical mass generation in an effective
(1+1)-dimensional relativistic field theory.
| cond-mat.supr-con cond-mat.str-el | we study the lowenergy density of states of dirac fermions in disordered dwave superconductor at zero energy a finite density of states is obtained via the mechanism of dynamical mass generation in an effective 11dimensional relativistic field theory | [['we', 'study', 'the', 'lowenergy', 'density', 'of', 'states', 'of', 'dirac', 'fermions', 'in', 'disordered', 'dwave', 'superconductor', 'at', 'zero', 'energy', 'a', 'finite', 'density', 'of', 'states', 'is', 'obtained', 'via', 'the', 'mechanism', 'of', 'dynamical', 'mass', 'generation', 'in', 'an', 'effective', '11di... | [-0.22405106754434345, 0.3286330027564729, -0.10848671104758978, 0.07526920433462549, 0.0182343387584153, -0.1232432739986842, 0.052929219700959755, 0.2621941308883068, -0.18758468374021744, -0.2586762464458221, -0.06912990321870893, -0.3190326660773472, -0.06442313657240256, 0.08068640990868996, 0.09570666414832599, 0... |
710.2271 | Support of generalized parton distributions in Bethe-Salpeter models of
hadrons | The proper support of generalized parton distributions from relativistic
constituent quark models with pointlike constituents is studied. The correct
support is guaranteed when the vertex function does not depend on the relative
minus-momentum. We show that including quark interactions in models with
pointlike consti... | hep-ph | the proper support of generalized parton distributions from relativistic constituent quark models with pointlike constituents is studied the correct support is guaranteed when the vertex function does not depend on the relative minusmomentum we show that including quark interactions in models with pointlike constituent... | [['the', 'proper', 'support', 'of', 'generalized', 'parton', 'distributions', 'from', 'relativistic', 'constituent', 'quark', 'models', 'with', 'pointlike', 'constituents', 'is', 'studied', 'the', 'correct', 'support', 'is', 'guaranteed', 'when', 'the', 'vertex', 'function', 'does', 'not', 'depend', 'on', 'the', 'relat... | [-0.05547285607248983, 0.2064533911727588, -0.13089029168152003, 0.12097355743753724, -0.10212794064051088, -0.08819150894551593, 0.02753802708706216, 0.3708271194687661, -0.18389054968514862, -0.25685610775561896, -0.028801060141310755, -0.2783594769288731, -0.024962886017473304, 0.0844719427439165, -0.005729989346839... |
710.2272 | Single-Particle Dynamics in the Vicinity of the Mott-Hubbard
Metal-to-Insulator Transition | The single-particle dynamics close to a metal-to-insulator transition induced
by strong repulsive interaction between the electrons is investigated. The
system is described by a half-filled Hubbard model which is treated by dynamic
mean-field theory evaluated by high-resolution dynamic density-matrix
renormalization.... | cond-mat.str-el | the singleparticle dynamics close to a metaltoinsulator transition induced by strong repulsive interaction between the electrons is investigated the system is described by a halffilled hubbard model which is treated by dynamic meanfield theory evaluated by highresolution dynamic densitymatrix renormalization we provide... | [['the', 'singleparticle', 'dynamics', 'close', 'to', 'a', 'metaltoinsulator', 'transition', 'induced', 'by', 'strong', 'repulsive', 'interaction', 'between', 'the', 'electrons', 'is', 'investigated', 'the', 'system', 'is', 'described', 'by', 'a', 'halffilled', 'hubbard', 'model', 'which', 'is', 'treated', 'by', 'dynam... | [-0.11168597249693617, 0.18546847692966736, -0.08586917735670728, 0.09562831283848802, -0.0022777352283743246, -0.17695638364939778, 0.06121836559355466, 0.40561093341697146, -0.25754784558106353, -0.28476594712723186, -0.05831203653684093, -0.3201230307006174, -0.11472436942643037, 0.0943293423452242, 0.09458325730843... |
710.2273 | Constituent and current quark masses at low chiral energies | Light constituent quark masses and the corresponding dynamical quark masses
are determined by data, the Quark-Level Linear $\sigma$ Model, and infrared
QCD. This allows to define effective nonstrange and strange current quark
masses which reproduce the experimental pion and kaon masses very accurately,
by simple addi... | hep-ph | light constituent quark masses and the corresponding dynamical quark masses are determined by data the quarklevel linear sigma model and infrared qcd this allows to define effective nonstrange and strange current quark masses which reproduce the experimental pion and kaon masses very accurately by simple additivity mor... | [['light', 'constituent', 'quark', 'masses', 'and', 'the', 'corresponding', 'dynamical', 'quark', 'masses', 'are', 'determined', 'by', 'data', 'the', 'quarklevel', 'linear', 'sigma', 'model', 'and', 'infrared', 'qcd', 'this', 'allows', 'to', 'define', 'effective', 'nonstrange', 'and', 'strange', 'current', 'quark', 'ma... | [0.009898717217939966, 0.35522241616111366, -0.12597950222961446, 0.2049735038419888, -0.09419206764915601, -0.12428791696289951, 0.10752159878586795, 0.29659859742969275, -0.10965991171790247, -0.25158858068406265, -0.06945482334444061, -0.2792130088697725, 0.03348096888634671, 0.08348359633856355, 0.05831738370173472... |
710.2274 | Phase diagram of the one-dimensional Hubbard model with
next-nearest-neighbor hopping | We study the one-dimensional Hubbard model with nearest-neighbor and
next-nearest-neighbor hopping integrals by using the density-matrix
renormalization group (DMRG) method and Hartree-Fock approximation. Based on
the calculated results for the spin gap, total-spin quantum number, and
Tomonaga-Luttinger-liquid parame... | cond-mat.str-el | we study the onedimensional hubbard model with nearestneighbor and nextnearestneighbor hopping integrals by using the densitymatrix renormalization group dmrg method and hartreefock approximation based on the calculated results for the spin gap totalspin quantum number and tomonagaluttingerliquid parameter we determine... | [['we', 'study', 'the', 'onedimensional', 'hubbard', 'model', 'with', 'nearestneighbor', 'and', 'nextnearestneighbor', 'hopping', 'integrals', 'by', 'using', 'the', 'densitymatrix', 'renormalization', 'group', 'dmrg', 'method', 'and', 'hartreefock', 'approximation', 'based', 'on', 'the', 'calculated', 'results', 'for',... | [-0.17758676682569785, 0.22778071961693058, -0.04723891841240402, 0.04054622301737254, 0.014051273403310915, -0.1526523525826633, 0.13825704120426963, 0.38356398686300963, -0.23476430901428103, -0.23403777564817574, 0.017708014937852568, -0.30805721229990013, -0.13496615966505487, 0.13760483987908856, 0.090555469513901... |
710.2275 | Pion structure in QCD: From theory to lattice to experimental data | We describe the present status of the pion distribution amplitude (DA) as it
originates from several sources: (i) a nonperturbative approach based on QCD
sum rules with nonlocal condensates, (ii) an $O(\alpha_s)$ QCD analysis of the
CLEO data on F^{\gamma\gamma^*\pi}(Q^2) with asymptotic and renormalon models
for hig... | hep-ph | we describe the present status of the pion distribution amplitude da as it originates from several sources i a nonperturbative approach based on qcd sum rules with nonlocal condensates ii an oalpha_s qcd analysis of the cleo data on fgammagammapiq2 with asymptotic and renormalon models for higher twists and iii recent ... | [['we', 'describe', 'the', 'present', 'status', 'of', 'the', 'pion', 'distribution', 'amplitude', 'da', 'as', 'it', 'originates', 'from', 'several', 'sources', 'i', 'a', 'nonperturbative', 'approach', 'based', 'on', 'qcd', 'sum', 'rules', 'with', 'nonlocal', 'condensates', 'ii', 'an', 'oalpha_s', 'qcd', 'analysis', 'of... | [-0.051224442342282746, 0.1584252140688688, -0.11106062996997565, 0.11765487641701654, -0.04863442445470803, -0.04330417760512859, 0.06849405262239641, 0.36397569849952194, -0.1490728480849361, -0.1787870294292984, 0.006455024556708994, -0.34230663745488593, -0.05141879489267434, 0.13152592194914495, 0.0735261427049619... |
710.2276 | Optical coupling of fundamental whispering gallery modes in bi-spheres | What will happen if two identical microspheres, with fundamental whispering
gallery modes excited in each of them, become optically coupled? Conventional
wisdom based on coupled-mode arguments says that two new modes, bonding and
anti-bonding, with two split frequencies would be formed. In this paper we
demonstrate, ... | physics.optics | what will happen if two identical microspheres with fundamental whispering gallery modes excited in each of them become optically coupled conventional wisdom based on coupledmode arguments says that two new modes bonding and antibonding with two split frequencies would be formed in this paper we demonstrate using exact... | [['what', 'will', 'happen', 'if', 'two', 'identical', 'microspheres', 'with', 'fundamental', 'whispering', 'gallery', 'modes', 'excited', 'in', 'each', 'of', 'them', 'become', 'optically', 'coupled', 'conventional', 'wisdom', 'based', 'on', 'coupledmode', 'arguments', 'says', 'that', 'two', 'new', 'modes', 'bonding', '... | [-0.11329499999599824, 0.21768672953528795, -0.1245268637942801, 0.00025542676645185213, -0.10533016637326723, -0.1989974817204996, -0.0015131873190851815, 0.392650044410972, -0.21141574923397907, -0.26201392658593425, -0.0024850293432912194, -0.2769838554717331, -0.1983617561285844, 0.1703069992812283, -0.025526496761... |
710.2277 | Renormalization of Polyakov loops in fundamental and higher
representations | We compare two renormalization procedures, one based on the short distance
behavior of heavy quark-antiquark free energies and the other by using bare
Polyakov loops at different temporal extent of the lattice and find that both
prescriptions are equivalent, resulting in renormalization constants that
depend on the b... | hep-lat hep-ph | we compare two renormalization procedures one based on the short distance behavior of heavy quarkantiquark free energies and the other by using bare polyakov loops at different temporal extent of the lattice and find that both prescriptions are equivalent resulting in renormalization constants that depend on the bare c... | [['we', 'compare', 'two', 'renormalization', 'procedures', 'one', 'based', 'on', 'the', 'short', 'distance', 'behavior', 'of', 'heavy', 'quarkantiquark', 'free', 'energies', 'and', 'the', 'other', 'by', 'using', 'bare', 'polyakov', 'loops', 'at', 'different', 'temporal', 'extent', 'of', 'the', 'lattice', 'and', 'find',... | [-0.1299298322470023, 0.2677695812502255, -0.08078805452738053, 0.11959340640654166, -0.03132535560199848, -0.13870657983427057, 0.03809939599327313, 0.409997964468904, -0.19787535004807302, -0.2393227558932267, 0.019763909135527242, -0.29833414653937024, -0.089731006152504, 0.13729189999270228, 0.028165416726364922, 0... |
710.2278 | Exploiting B Site Disorder for Phase Control in the Manganites | Disorder on the active d element site is usually very disruptive for
conduction and long range order in perovskite transition metal oxides. However,
in the background of phase competition such `B site' dopants also act to
promote one ordered phase at the expense of another. This occurs either through
valence change o... | cond-mat.str-el | disorder on the active d element site is usually very disruptive for conduction and long range order in perovskite transition metal oxides however in the background of phase competition such b site dopants also act to promote one ordered phase at the expense of another this occurs either through valence change of the t... | [['disorder', 'on', 'the', 'active', 'd', 'element', 'site', 'is', 'usually', 'very', 'disruptive', 'for', 'conduction', 'and', 'long', 'range', 'order', 'in', 'perovskite', 'transition', 'metal', 'oxides', 'however', 'in', 'the', 'background', 'of', 'phase', 'competition', 'such', 'b', 'site', 'dopants', 'also', 'act'... | [-0.12228797851823085, 0.23172312451541915, 0.004798633425519609, 0.0414609736108706, -8.828122522835889e-05, -0.18025441370011608, 0.1235396881811013, 0.38181225510606587, -0.2853512860341998, -0.3020436766919149, 0.04964624740826043, -0.30372443381881664, -0.11872486946988882, 0.12013104071211424, 0.02957300691334299... |
710.2279 | Unit Rectangle Visibility Graphs | Over the past twenty years, rectangle visibility graphs have generated
considerable interest, in part due to their applicability to VLSI chip design.
Here we study unit rectangle visibility graphs, with fixed dimension
restrictions more closely modeling the constrained dimensions of gates and
other circuit components... | math.CO | over the past twenty years rectangle visibility graphs have generated considerable interest in part due to their applicability to vlsi chip design here we study unit rectangle visibility graphs with fixed dimension restrictions more closely modeling the constrained dimensions of gates and other circuit components in co... | [['over', 'the', 'past', 'twenty', 'years', 'rectangle', 'visibility', 'graphs', 'have', 'generated', 'considerable', 'interest', 'in', 'part', 'due', 'to', 'their', 'applicability', 'to', 'vlsi', 'chip', 'design', 'here', 'we', 'study', 'unit', 'rectangle', 'visibility', 'graphs', 'with', 'fixed', 'dimension', 'restri... | [-0.1511235537162079, 0.1182055325133598, 0.022142788430054686, -0.023945095051321707, -0.10283588694820878, -0.15861891643748482, 0.04308926580182298, 0.4606190833426614, -0.26215328449625097, -0.31868371255127076, 0.14766578028646818, -0.2985561758933859, -0.1355343214253973, 0.17478012070166415, -0.10533095418319163... |
710.228 | Hydrodynamical modeling of the deconfinement phase transition and
explosive hadronization | Dynamics of relativistic heavy-ion collisions is investigated on the basis of
a simple (1+1)-dimensional hydrodynamical model in light-cone coordinates. The
main emphasis is put on studying sensitivity of the dynamics and observables to
the equation of state and initial conditions. Low sensitivity of pion rapidity
sp... | hep-ph nucl-th | dynamics of relativistic heavyion collisions is investigated on the basis of a simple 11dimensional hydrodynamical model in lightcone coordinates the main emphasis is put on studying sensitivity of the dynamics and observables to the equation of state and initial conditions low sensitivity of pion rapidity spectra to t... | [['dynamics', 'of', 'relativistic', 'heavyion', 'collisions', 'is', 'investigated', 'on', 'the', 'basis', 'of', 'a', 'simple', '11dimensional', 'hydrodynamical', 'model', 'in', 'lightcone', 'coordinates', 'the', 'main', 'emphasis', 'is', 'put', 'on', 'studying', 'sensitivity', 'of', 'the', 'dynamics', 'and', 'observabl... | [-0.1396573981633637, 0.24682098032816263, -0.17187463343559908, 0.0917901738898874, -0.013433725550407317, -0.08039921200625992, 0.014542861088232054, 0.33163650818471985, -0.21754356148099996, -0.22358220262922407, 0.03836919682486573, -0.29626659377349346, -0.03895957382183855, 0.13066256786242308, 0.013935401187679... |
710.2281 | Non-linear Lie conformal algebras with three generators | We classify certain non-linear Lie conformal algebras with three generators,
which can be viewed as deformations of the current Lie conformal algebra of
sl_2. In doing so we discover an interesting 1-parameter family of non-linear
Lie conformal algebras R_{-1}^d and the corresponding freely generated vertex
algebras ... | math-ph math.MP math.QA | we classify certain nonlinear lie conformal algebras with three generators which can be viewed as deformations of the current lie conformal algebra of sl_2 in doing so we discover an interesting 1parameter family of nonlinear lie conformal algebras r_1d and the corresponding freely generated vertex algebras v_1d which ... | [['we', 'classify', 'certain', 'nonlinear', 'lie', 'conformal', 'algebras', 'with', 'three', 'generators', 'which', 'can', 'be', 'viewed', 'as', 'deformations', 'of', 'the', 'current', 'lie', 'conformal', 'algebra', 'of', 'sl_2', 'in', 'doing', 'so', 'we', 'discover', 'an', 'interesting', '1parameter', 'family', 'of', ... | [-0.18190280770820177, 0.09488216121017205, -0.006876891970718175, 0.034242496229289626, -0.1847172147133963, -0.17710793475630912, -0.0776616766881407, 0.3377130151297269, -0.3673820818991536, -0.17988245526140326, 0.13065482282440774, -0.24768703610876971, -0.15457527118661765, 0.1633775940981139, -0.0929065258817726... |
710.2282 | On crossed product rings with twisted involutions, their module
categories and L-theory | We study the Farrell-Jones Conjecture with coefficients in an additive
G-category with involution. This is a variant of the L-theoretic Farrell-Jones
Conjecture which originally deals with group rings with the standard
involution. We show that this formulation of the conjecture can be applied to
crossed product rings... | math.KT | we study the farrelljones conjecture with coefficients in an additive gcategory with involution this is a variant of the ltheoretic farrelljones conjecture which originally deals with group rings with the standard involution we show that this formulation of the conjecture can be applied to crossed product rings rg equi... | [['we', 'study', 'the', 'farrelljones', 'conjecture', 'with', 'coefficients', 'in', 'an', 'additive', 'gcategory', 'with', 'involution', 'this', 'is', 'a', 'variant', 'of', 'the', 'ltheoretic', 'farrelljones', 'conjecture', 'which', 'originally', 'deals', 'with', 'group', 'rings', 'with', 'the', 'standard', 'involution... | [-0.21969393687886035, 0.07047692484493676, -0.12792908180234652, 0.032760359277392945, -0.11663450778371864, -0.18431394614820037, -0.06124383781946475, 0.3414923105869562, -0.3397133869509543, -0.25627281797689294, 0.09706540845311998, -0.21870700626318612, -0.1750372893762805, 0.1865125403649384, -0.2172861606363327... |
710.2283 | Phenomenological study of the electronic transport coefficients of
graphene | Using a semi-classical approach and input from experiments on the
conductivity of graphene, we determine the electronic density dependence of the
electronic transport coefficients -- conductivity, thermal conductivity and
thermopower -- of doped graphene. Also the electronic density dependence of the
optical conducti... | cond-mat.mes-hall | using a semiclassical approach and input from experiments on the conductivity of graphene we determine the electronic density dependence of the electronic transport coefficients conductivity thermal conductivity and thermopower of doped graphene also the electronic density dependence of the optical conductivity is obta... | [['using', 'a', 'semiclassical', 'approach', 'and', 'input', 'from', 'experiments', 'on', 'the', 'conductivity', 'of', 'graphene', 'we', 'determine', 'the', 'electronic', 'density', 'dependence', 'of', 'the', 'electronic', 'transport', 'coefficients', 'conductivity', 'thermal', 'conductivity', 'and', 'thermopower', 'of... | [-0.11957444711070922, 0.1577848966842816, -0.08786967332348411, -0.02641623710098182, -0.025149996165347136, -0.10016437078377714, 0.04240594816647102, 0.3599448449403783, -0.29917686556776363, -0.24629396200180054, 0.034689541825633725, -0.3276442883099303, -0.15555139137776913, 0.22622835875868244, 0.037536514816621... |
710.2284 | Symmetric and Synchronous Communication in Peer-to-Peer Networks | Motivated by distributed implementations of game-theoretical algorithms, we
study symmetric process systems and the problem of attaining common knowledge
between processes. We formalize our setting by defining a notion of
peer-to-peer networks(*) and appropriate symmetry concepts in the context of
Communicating Seque... | cs.DC cs.GT | motivated by distributed implementations of gametheoretical algorithms we study symmetric process systems and the problem of attaining common knowledge between processes we formalize our setting by defining a notion of peertopeer networks and appropriate symmetry concepts in the context of communicating sequential proc... | [['motivated', 'by', 'distributed', 'implementations', 'of', 'gametheoretical', 'algorithms', 'we', 'study', 'symmetric', 'process', 'systems', 'and', 'the', 'problem', 'of', 'attaining', 'common', 'knowledge', 'between', 'processes', 'we', 'formalize', 'our', 'setting', 'by', 'defining', 'a', 'notion', 'of', 'peertope... | [-0.15290413669965885, 0.051422068101668696, -0.026383193037300197, 0.07470226337044787, -0.13601925999736758, -0.20034286972756188, 0.10330675875561104, 0.39008165430277586, -0.3154981974305378, -0.28663244804160465, 0.09235318091059863, -0.2263662287723963, -0.17122435568555913, 0.11704708871914557, -0.14418779610466... |
710.2285 | Comment on "Modified Coulomb Law in a Strongly Magnetized Vacuum" | This is a comment on Phys. Rev. Lett. 98, 180403 (2007) [arXiv:0704.2162].
| astro-ph hep-ph hep-th | this is a comment on phys rev lett 98 180403 2007 arxiv07042162 | [['this', 'is', 'a', 'comment', 'on', 'phys', 'rev', 'lett', '98', '180403', '2007', 'arxiv07042162']] | [-0.05500625996765765, 0.046946324238722976, 0.051162081050940535, -0.42028665813532745, -0.1693514505909248, 0.015884691383689642, 0.27155211161483417, 0.2563641710545529, 0.30784489485350525, -0.40682548318396916, -0.22220526898110454, -0.28843371400778944, -0.3361802107908509, 0.23292416605082425, -0.459697099148549... |
710.2286 | BCS theory for finite size superconductors | We study finite size effects in superconducting metallic grains and determine
the BCS order parameter and the low energy excitation spectrum in terms of
size, and shape of the grain. Our approach combines the BCS self-consistency
condition, a semiclassical expansion for the spectral density and interaction
matrix ele... | cond-mat.supr-con cond-mat.dis-nn cond-mat.mes-hall | we study finite size effects in superconducting metallic grains and determine the bcs order parameter and the low energy excitation spectrum in terms of size and shape of the grain our approach combines the bcs selfconsistency condition a semiclassical expansion for the spectral density and interaction matrix elements ... | [['we', 'study', 'finite', 'size', 'effects', 'in', 'superconducting', 'metallic', 'grains', 'and', 'determine', 'the', 'bcs', 'order', 'parameter', 'and', 'the', 'low', 'energy', 'excitation', 'spectrum', 'in', 'terms', 'of', 'size', 'and', 'shape', 'of', 'the', 'grain', 'our', 'approach', 'combines', 'the', 'bcs', 's... | [-0.1316682409200043, 0.17581290318423162, -0.08357619531544866, 0.08424019945859171, -0.010761538068625596, -0.06528546797148514, 0.05278382852493721, 0.2972262705316638, -0.2488147358197977, -0.2962344424374918, 0.013011192794575696, -0.2992735704646842, -0.06421265348165046, 0.08783609452334666, -0.00771741010479186... |
710.2287 | Gravitino Dark Matter with Broken R-parity | Scenarios with gravitino dark matter face potential cosmological problems
induced by the presence of the Next-to-Lightest Supersymmetric Particle (NLSP)
at the time of Big Bang Nucleosynthesis (BBN). A very simple, albeit radical,
solution to avoid all these problems consists on assuming that R-parity is
slightly vio... | hep-ph | scenarios with gravitino dark matter face potential cosmological problems induced by the presence of the nexttolightest supersymmetric particle nlsp at the time of big bang nucleosynthesis bbn a very simple albeit radical solution to avoid all these problems consists on assuming that rparity is slightly violated since ... | [['scenarios', 'with', 'gravitino', 'dark', 'matter', 'face', 'potential', 'cosmological', 'problems', 'induced', 'by', 'the', 'presence', 'of', 'the', 'nexttolightest', 'supersymmetric', 'particle', 'nlsp', 'at', 'the', 'time', 'of', 'big', 'bang', 'nucleosynthesis', 'bbn', 'a', 'very', 'simple', 'albeit', 'radical', ... | [-0.12268644276385506, 0.21166127341954658, -0.061344649691212304, 0.16265548976702526, -0.0861725643885115, -0.18023489121373537, 0.006427461925896851, 0.3065378907631384, -0.23445359779806393, -0.30856058918612284, 0.07574213187763235, -0.2684271849995841, -0.014410517792890055, 0.16110989116956867, -0.00151714866741... |
710.2288 | VERITAS Data Acquisition | VERITAS employs a multi-stage data acquisition chain that extends from the
VME readout of custom 500 MS/s flash ADC electronics to the construction of
telescope events and ultimately the compilation of information from each
telescope into array level data. These systems provide access to the
programming of the channe... | astro-ph | veritas employs a multistage data acquisition chain that extends from the vme readout of custom 500 mss flash adc electronics to the construction of telescope events and ultimately the compilation of information from each telescope into array level data these systems provide access to the programming of the channel lev... | [['veritas', 'employs', 'a', 'multistage', 'data', 'acquisition', 'chain', 'that', 'extends', 'from', 'the', 'vme', 'readout', 'of', 'custom', '500', 'mss', 'flash', 'adc', 'electronics', 'to', 'the', 'construction', 'of', 'telescope', 'events', 'and', 'ultimately', 'the', 'compilation', 'of', 'information', 'from', 'e... | [-0.15101472359094628, 0.05182376472433483, -0.044592946892100055, 0.023189642532252447, -0.07158914599147506, -0.16810408775818086, 0.08089820455840292, 0.3856981838668199, -0.251924822331035, -0.3692596235095446, 0.1806433980022312, -0.2739087510066233, -0.07388676994277123, 0.23635107491697585, -0.06261145427500955,... |
710.2289 | Decoherence induced by Smith-Purcell radiation | The interaction between charged particles and the vacuum fluctuations of the
electromagnetic field induces decoherence, and therefore affects the contrast
of fringes in an interference experiment. In this article we show that if a
double slit experiment is performed near a conducting grating, the fringe
visibility is... | quant-ph | the interaction between charged particles and the vacuum fluctuations of the electromagnetic field induces decoherence and therefore affects the contrast of fringes in an interference experiment in this article we show that if a double slit experiment is performed near a conducting grating the fringe visibility is redu... | [['the', 'interaction', 'between', 'charged', 'particles', 'and', 'the', 'vacuum', 'fluctuations', 'of', 'the', 'electromagnetic', 'field', 'induces', 'decoherence', 'and', 'therefore', 'affects', 'the', 'contrast', 'of', 'fringes', 'in', 'an', 'interference', 'experiment', 'in', 'this', 'article', 'we', 'show', 'that'... | [-0.1531983547565509, 0.21374254938179066, -0.09192502523507631, 0.04944016511652473, -0.011923384948578827, -0.07220672979932644, -0.001126019464458759, 0.35602959311183763, -0.2480625964646392, -0.3308987945099087, 0.02913220578179165, -0.280039718703312, -0.14498415296696418, 0.19126261198178718, -0.0515917072668397... |
710.229 | Estimates of multipolar coefficients to search for cosmic ray
anisotropies with non-uniform or partial sky coverage | We study the possibility to extract the multipolar moments of an underlying
distribution from a set of cosmic rays observed with non-uniform or even
partial sky coverage. We show that if the degree is assumed to be upper bounded
by $L$, each multipolar moment can be recovered whatever the coverage, but with
a varianc... | astro-ph | we study the possibility to extract the multipolar moments of an underlying distribution from a set of cosmic rays observed with nonuniform or even partial sky coverage we show that if the degree is assumed to be upper bounded by l each multipolar moment can be recovered whatever the coverage but with a variance increa... | [['we', 'study', 'the', 'possibility', 'to', 'extract', 'the', 'multipolar', 'moments', 'of', 'an', 'underlying', 'distribution', 'from', 'a', 'set', 'of', 'cosmic', 'rays', 'observed', 'with', 'nonuniform', 'or', 'even', 'partial', 'sky', 'coverage', 'we', 'show', 'that', 'if', 'the', 'degree', 'is', 'assumed', 'to', ... | [-0.10627796445954014, 0.13430553073448742, -0.06137532306854258, 0.06879749101677853, -0.0808252857796387, -0.06937323369988307, 0.06983355070001052, 0.35453949940688523, -0.2902349073094191, -0.3222764419756599, 0.09701832382910952, -0.2770101289989753, -0.0910576810951095, 0.1356849658456583, -0.02349067325751806, -... |
710.2291 | Rotating Black Holes in Higher Dimensions | The properties of higher-dimensional black holes can differ significantly
from those of black holes in four dimensions, since neither the uniqueness
theorem, nor the staticity theorem or the topological censorship theorem
generalize to higher dimensions. We first discuss black holes of
Einstein-Maxwell theory and Ein... | hep-th | the properties of higherdimensional black holes can differ significantly from those of black holes in four dimensions since neither the uniqueness theorem nor the staticity theorem or the topological censorship theorem generalize to higher dimensions we first discuss black holes of einsteinmaxwell theory and einsteinma... | [['the', 'properties', 'of', 'higherdimensional', 'black', 'holes', 'can', 'differ', 'significantly', 'from', 'those', 'of', 'black', 'holes', 'in', 'four', 'dimensions', 'since', 'neither', 'the', 'uniqueness', 'theorem', 'nor', 'the', 'staticity', 'theorem', 'or', 'the', 'topological', 'censorship', 'theorem', 'gener... | [-0.15773406214508656, 0.13423428070303556, -0.053034373225543545, 0.1948128143149252, -0.08675705470346115, -0.1667531525552575, 0.026328591560642864, 0.2560185153490385, -0.14612092192259593, -0.29595298253352176, 0.13488604518981348, -0.3188154754744893, -0.13767292383567406, 0.16546761868458643, -0.1120474102939919... |
710.2292 | Gap generation for Dirac fermions on Lobachevsky plane in a magnetic
field | We study symmetry breaking and gap generation for fermions in the 2D space of
constant negative curvature (the Lobachevsky plane) in an external covariantly
constant magnetic field in a four-fermion model. It is shown that due to the
magnetic and negative curvature catalysis phenomena the critical coupling
constant i... | hep-ph cond-mat.mes-hall | we study symmetry breaking and gap generation for fermions in the 2d space of constant negative curvature the lobachevsky plane in an external covariantly constant magnetic field in a fourfermion model it is shown that due to the magnetic and negative curvature catalysis phenomena the critical coupling constant is zero... | [['we', 'study', 'symmetry', 'breaking', 'and', 'gap', 'generation', 'for', 'fermions', 'in', 'the', '2d', 'space', 'of', 'constant', 'negative', 'curvature', 'the', 'lobachevsky', 'plane', 'in', 'an', 'external', 'covariantly', 'constant', 'magnetic', 'field', 'in', 'a', 'fourfermion', 'model', 'it', 'is', 'shown', 't... | [-0.220940344008169, 0.23710993558669766, -0.02670729959401179, 0.07939750542051492, -0.05863253222251276, -0.12348247559758711, 0.021055622293200908, 0.34945682206032974, -0.24361719998952774, -0.26584278149881735, 0.052382431597062296, -0.2795127988265792, -0.15999304181193266, 0.1284521837468382, 0.04507490935875982... |
710.2293 | Trends in multiparticle production and some "predictions" for pp and
PbPb collisions at LHC | Based on trends seen at lower energies we "predict" the multiplicities and
pseudorapidity distributions of particle density and elliptic flow that will be
seen in PbPb and pp collisions at the LHC. We argue that, if these predictions
turn out to be correct, either these quantities are insensitive to the state of
matt... | nucl-ex | based on trends seen at lower energies we predict the multiplicities and pseudorapidity distributions of particle density and elliptic flow that will be seen in pbpb and pp collisions at the lhc we argue that if these predictions turn out to be correct either these quantities are insensitive to the state of matter crea... | [['based', 'on', 'trends', 'seen', 'at', 'lower', 'energies', 'we', 'predict', 'the', 'multiplicities', 'and', 'pseudorapidity', 'distributions', 'of', 'particle', 'density', 'and', 'elliptic', 'flow', 'that', 'will', 'be', 'seen', 'in', 'pbpb', 'and', 'pp', 'collisions', 'at', 'the', 'lhc', 'we', 'argue', 'that', 'if'... | [-0.03417792764303976, 0.21935628580578256, -0.18492414313237696, 0.15840520558020707, -0.033988085784687753, -0.1309978432084821, -0.030614561317593193, 0.3473671963830803, -0.2558110554786294, -0.3434752714140027, 0.03056212158591141, -0.3158717346246867, 0.030406476683872804, 0.15040662139719563, -0.0081248667530631... |
710.2294 | Strong coupling expansion of Baxter equation in N=4 SYM | The anomalous dimensions of single-trace local Wilson operators with
covariant derivatives in maximally supersymmetric gauge theory are believed to
be generated from a deformed noncompact sl(2) Baxter equation. We perform a
systematic expansion of this equation at strong coupling in the
single-logarithmic limit of la... | hep-th | the anomalous dimensions of singletrace local wilson operators with covariant derivatives in maximally supersymmetric gauge theory are believed to be generated from a deformed noncompact sl2 baxter equation we perform a systematic expansion of this equation at strong coupling in the singlelogarithmic limit of large con... | [['the', 'anomalous', 'dimensions', 'of', 'singletrace', 'local', 'wilson', 'operators', 'with', 'covariant', 'derivatives', 'in', 'maximally', 'supersymmetric', 'gauge', 'theory', 'are', 'believed', 'to', 'be', 'generated', 'from', 'a', 'deformed', 'noncompact', 'sl2', 'baxter', 'equation', 'we', 'perform', 'a', 'syst... | [-0.17274072987380104, 0.1522721553354714, -0.047074522655818934, 0.09451493112713967, -0.08478729057270419, -0.07658324858119477, -0.031059335208570276, 0.28848250966193606, -0.25436275555453836, -0.22004368692609363, 0.0666035822088586, -0.3117107333597338, -0.11776970867610094, 0.09295451800221378, 0.022491900659464... |
710.2295 | Solar Neutrinos: Models, Observations, and New Opportunities | I discuss the development and resolution of the solar neutrino problem, as
well as opportunities now open to us to extend our knowledge of main-sequence
stellar evolution and neutrino astrophysics.
| nucl-th astro-ph | i discuss the development and resolution of the solar neutrino problem as well as opportunities now open to us to extend our knowledge of mainsequence stellar evolution and neutrino astrophysics | [['i', 'discuss', 'the', 'development', 'and', 'resolution', 'of', 'the', 'solar', 'neutrino', 'problem', 'as', 'well', 'as', 'opportunities', 'now', 'open', 'to', 'us', 'to', 'extend', 'our', 'knowledge', 'of', 'mainsequence', 'stellar', 'evolution', 'and', 'neutrino', 'astrophysics']] | [0.054644382651895286, 0.15088617894798517, 0.025003150633225838, 0.17643963685259223, -0.18299824135998885, -0.03568808541943629, 0.04522135766843955, 0.33845172040164473, -0.26334501085802914, -0.4297066015501817, 0.12239883582418164, -0.22730086517209808, -0.07104734356204669, 0.25856604278087614, -0.054078258760273... |
710.2296 | Vertex Percolation on Expander Graphs | We say that a graph $G=(V,E)$ on $n$ vertices is a $\beta$-expander for some
constant $\beta>0$ if every $U\subseteq V$ of cardinality $|U|\leq \frac{n}{2}$
satisfies $|N_G(U)|\geq \beta|U|$ where $N_G(U)$ denotes the neighborhood of
$U$. In this work we explore the process of deleting vertices of a
$\beta$-expander ... | math.CO cs.DM math.PR | we say that a graph gve on n vertices is a betaexpander for some constant beta0 if every usubseteq v of cardinality uleq fracn2 satisfies n_gugeq betau where n_gu denotes the neighborhood of u in this work we explore the process of deleting vertices of a betaexpander independently at random with probability nalpha for ... | [['we', 'say', 'that', 'a', 'graph', 'gve', 'on', 'n', 'vertices', 'is', 'a', 'betaexpander', 'for', 'some', 'constant', 'beta0', 'if', 'every', 'usubseteq', 'v', 'of', 'cardinality', 'uleq', 'fracn2', 'satisfies', 'n_gugeq', 'betau', 'where', 'n_gu', 'denotes', 'the', 'neighborhood', 'of', 'u', 'in', 'this', 'work', '... | [-0.15733036014430804, 0.15316034128170672, -0.03593246814352079, -0.007555628578652655, -0.07605896847127921, -0.14735186057829405, 0.10008809262348461, 0.3781521305543004, -0.2541120847835984, -0.27917369854286767, 0.08623620096191413, -0.33604141047270203, -0.13364626089832363, 0.10599775087244839, -0.10219314879333... |
710.2297 | Electrically Tunable Spin Polarization in a Carbon-Nanotube Spin Diode | We have studied the current through a carbon nanotube quantum dot with one
ferromagnetic and one normal-metal lead. For the values of gate voltage at
which the normal lead is resonant with the single available non-degenerate
energy level on the dot, we observe a pronounced decrease in the current for
one bias directi... | cond-mat.mes-hall | we have studied the current through a carbon nanotube quantum dot with one ferromagnetic and one normalmetal lead for the values of gate voltage at which the normal lead is resonant with the single available nondegenerate energy level on the dot we observe a pronounced decrease in the current for one bias direction we ... | [['we', 'have', 'studied', 'the', 'current', 'through', 'a', 'carbon', 'nanotube', 'quantum', 'dot', 'with', 'one', 'ferromagnetic', 'and', 'one', 'normalmetal', 'lead', 'for', 'the', 'values', 'of', 'gate', 'voltage', 'at', 'which', 'the', 'normal', 'lead', 'is', 'resonant', 'with', 'the', 'single', 'available', 'nond... | [-0.15376546680123257, 0.16048134781969645, -0.014962316979821637, -0.0052854807682254975, -0.020230148841874847, -0.20160466052337195, 0.05937785056768079, 0.4180428882350596, -0.273466308701703, -0.30066990279492073, 0.040603929721053506, -0.265459522015328, -0.10415061946670197, 0.28031552203582505, -0.0047295892597... |
710.2298 | Constant curvature foliations on asymptotically hyperbolic spaces | Let $(M,g)$ be an asymptotically hyperbolic manifold with a smooth conformal
compactification. We establish a general correspondence between semilinear
elliptic equations of scalar curvature type on $\del M$ and Weingarten
foliations in some neighbourhood of infinity in $M$. We focus mostly on
foliations where each l... | math.DG | let mg be an asymptotically hyperbolic manifold with a smooth conformal compactification we establish a general correspondence between semilinear elliptic equations of scalar curvature type on del m and weingarten foliations in some neighbourhood of infinity in m we focus mostly on foliations where each leaf has consta... | [['let', 'mg', 'be', 'an', 'asymptotically', 'hyperbolic', 'manifold', 'with', 'a', 'smooth', 'conformal', 'compactification', 'we', 'establish', 'a', 'general', 'correspondence', 'between', 'semilinear', 'elliptic', 'equations', 'of', 'scalar', 'curvature', 'type', 'on', 'del', 'm', 'and', 'weingarten', 'foliations', ... | [-0.20794245611776002, 0.097128727086177, -0.08812400533093347, 0.07097175452185588, -0.11563236174535835, -0.17875280512897815, -0.05833297584184846, 0.33996807545837426, -0.21190932899480686, -0.23559192812374224, 0.10080468038318537, -0.2926316163243933, -0.1607195560120292, 0.1800377638145518, -0.15557460121474126,... |
710.2299 | On Boltzmann's genius and thermodynamics | A recent essay [1] reminds us of how richly Boltzmann deserves to be
admiringly commemorated for the originality of his ideas on the occasion of his
150th birthday. Without any doubt, the scientific community owes Boltzmann a
great debt of gratitude for his ingenious and pathfinding contributions.
However, the essay ... | physics.hist-ph | a recent essay 1 reminds us of how richly boltzmann deserves to be admiringly commemorated for the originality of his ideas on the occasion of his 150th birthday without any doubt the scientific community owes boltzmann a great debt of gratitude for his ingenious and pathfinding contributions however the essay chooses ... | [['a', 'recent', 'essay', '1', 'reminds', 'us', 'of', 'how', 'richly', 'boltzmann', 'deserves', 'to', 'be', 'admiringly', 'commemorated', 'for', 'the', 'originality', 'of', 'his', 'ideas', 'on', 'the', 'occasion', 'of', 'his', '150th', 'birthday', 'without', 'any', 'doubt', 'the', 'scientific', 'community', 'owes', 'bo... | [-0.03582612457995613, 0.04865731635441383, -0.163118606377393, 0.10332843535579742, -0.25348424702882766, -0.18894198026508094, 0.11442208285133044, 0.2571090222646793, -0.2078016674766938, -0.2963435370475054, 0.13841740873176606, -0.32149137537926437, -0.1548962300705413, 0.17240398161113263, -0.20411477877448003, -... |
710.23 | Scattering of single spikes | We apply the dressing method to a string solution given by a static string
wrapped around the equator of a three-sphere and find that the result is the
single spike solution recently discussed in the literature. Further application
of the method allows the construction of solutions with multiple spikes. In
particular... | hep-th | we apply the dressing method to a string solution given by a static string wrapped around the equator of a threesphere and find that the result is the single spike solution recently discussed in the literature further application of the method allows the construction of solutions with multiple spikes in particular we c... | [['we', 'apply', 'the', 'dressing', 'method', 'to', 'a', 'string', 'solution', 'given', 'by', 'a', 'static', 'string', 'wrapped', 'around', 'the', 'equator', 'of', 'a', 'threesphere', 'and', 'find', 'that', 'the', 'result', 'is', 'the', 'single', 'spike', 'solution', 'recently', 'discussed', 'in', 'the', 'literature', ... | [-0.13298602153736283, 0.12289331998829311, -0.07224546191798709, 0.08555215873366251, -0.06912424196343636, -0.09592720657383325, 0.017553192828017927, 0.3218890325006214, -0.2719962920382386, -0.26635649238050974, 0.1026900441484031, -0.2840065920628376, -0.1805232158912986, 0.18385056225088192, -0.018061212827888085... |
710.2301 | Auto and crosscorrelograms for the spike response of LIF neurons with
slow synapses | An analytical description of the response properties of simple but realistic
neuron models in the presence of noise is still lacking. We determine
completely up to the second order the firing statistics of a single and a pair
of leaky integrate-and-fire neurons (LIFs) receiving some common slowly
filtered white noise... | q-bio.NC physics.bio-ph | an analytical description of the response properties of simple but realistic neuron models in the presence of noise is still lacking we determine completely up to the second order the firing statistics of a single and a pair of leaky integrateandfire neurons lifs receiving some common slowly filtered white noise in par... | [['an', 'analytical', 'description', 'of', 'the', 'response', 'properties', 'of', 'simple', 'but', 'realistic', 'neuron', 'models', 'in', 'the', 'presence', 'of', 'noise', 'is', 'still', 'lacking', 'we', 'determine', 'completely', 'up', 'to', 'the', 'second', 'order', 'the', 'firing', 'statistics', 'of', 'a', 'single',... | [-0.11759902638316687, 0.11106094211721271, 0.0027157955574898087, 0.08451871182033031, -0.016961366140131592, -0.15198867267225774, 0.0598815880259689, 0.4049563635121651, -0.2523104788174815, -0.25818177164361183, 0.022734266113043213, -0.282050390875119, -0.2545282244468488, 0.17921797060692796, -0.08649013259885263... |
710.2302 | Freeness of equivariant cohomology and mutants of compactified
representations | We survey generalisations of the Chang-Skjelbred Lemma for integral
coefficients. Moreover, we construct examples of manifolds with actions of tori
of rank > 2 whose equivariant cohomology is torsion-free, but not free. This
answers a question of Allday's. The "mutants" we construct are obtained from
compactified rep... | math.AT math.GT | we survey generalisations of the changskjelbred lemma for integral coefficients moreover we construct examples of manifolds with actions of tori of rank 2 whose equivariant cohomology is torsionfree but not free this answers a question of alldays the mutants we construct are obtained from compactified representations a... | [['we', 'survey', 'generalisations', 'of', 'the', 'changskjelbred', 'lemma', 'for', 'integral', 'coefficients', 'moreover', 'we', 'construct', 'examples', 'of', 'manifolds', 'with', 'actions', 'of', 'tori', 'of', 'rank', '2', 'whose', 'equivariant', 'cohomology', 'is', 'torsionfree', 'but', 'not', 'free', 'this', 'answ... | [-0.1710258729114496, 0.059821862897633596, -0.08913662458137381, 0.10765643836051789, -0.12275052765595182, -0.18343869008053587, -0.006463120996793908, 0.3661216481738144, -0.29156533660331985, -0.2247578538954258, 0.15533203309849958, -0.23370547397150043, -0.21276895578880356, 0.22835184076695508, -0.18651389622322... |
710.2303 | Phase Transitions and Quantum Stabilization in Quantum Anharmonic
Crystals | A unified theory of phase transitions and quantum effects in quantum
anharmonic crystals is presented. In its framework, the relationship between
these two phenomena is analyzed. The theory is based on the representation of
the model Gibbs states in terms of path measures (Euclidean Gibbs measures). It
covers the cas... | math-ph math.MP | a unified theory of phase transitions and quantum effects in quantum anharmonic crystals is presented in its framework the relationship between these two phenomena is analyzed the theory is based on the representation of the model gibbs states in terms of path measures euclidean gibbs measures it covers the case of cry... | [['a', 'unified', 'theory', 'of', 'phase', 'transitions', 'and', 'quantum', 'effects', 'in', 'quantum', 'anharmonic', 'crystals', 'is', 'presented', 'in', 'its', 'framework', 'the', 'relationship', 'between', 'these', 'two', 'phenomena', 'is', 'analyzed', 'the', 'theory', 'is', 'based', 'on', 'the', 'representation', '... | [-0.09571311201900244, 0.17054267522258063, -0.10543692936499914, 0.09679391046209881, 0.005545132880409559, -0.11628677967935801, 0.03719090077094734, 0.37640022672712803, -0.24651644088327884, -0.258633248458306, 0.05395886781315009, -0.33321255854020515, -0.18187402993440627, 0.20265193399973214, -0.0391432409361004... |
710.2304 | Comment on the article arXiv 0710.0349 by Chapoton et al. titled ``An
operational calculus for the Mould operad'' | This paper has been withdrawn.
| math.QA math.CO | this paper has been withdrawn | [['this', 'paper', 'has', 'been', 'withdrawn']] | [-0.14966976195573806, -0.11479587350040674, -0.26925536394119265, -0.2174653896363452, -0.24278417900204657, -0.06483052410185337, -0.18645338097121567, 0.4360402226448059, -0.2831330731511116, -0.34362963438034055, 0.12004837393760681, -0.3683081828057766, -0.1602430183440447, -0.10558439195156097, -0.497941048443317... |
710.2305 | The number of cliques in graphs of given order and size | Let k_r(n,m) denote the minimum number of r-cliques in graphs with n vertices
and m edges. For r=3,4 we give a lower bound on k_r(n,m) that approximates
k_r(n,m) with an error smaller than n^r/(n^2-2m). The solution is based on a
constraint minimization of certain multilinear forms. In our proof, a
combinatorial stra... | math.CO | let k_rnm denote the minimum number of rcliques in graphs with n vertices and m edges for r34 we give a lower bound on k_rnm that approximates k_rnm with an error smaller than nrn22m the solution is based on a constraint minimization of certain multilinear forms in our proof a combinatorial strategy is coupled with ext... | [['let', 'k_rnm', 'denote', 'the', 'minimum', 'number', 'of', 'rcliques', 'in', 'graphs', 'with', 'n', 'vertices', 'and', 'm', 'edges', 'for', 'r34', 'we', 'give', 'a', 'lower', 'bound', 'on', 'k_rnm', 'that', 'approximates', 'k_rnm', 'with', 'an', 'error', 'smaller', 'than', 'nrn22m', 'the', 'solution', 'is', 'based',... | [-0.1785722858223476, 0.0811818848027574, -0.0931909203594714, 0.0038636768637061642, -0.10674460054162824, -0.16880974047735595, 0.07674159462514676, 0.28919497004448713, -0.18406433167687633, -0.355513706443864, 0.08409505810899039, -0.3296454979531598, -0.13546324504759946, 0.18276753253303468, -0.08423356703694976,... |
710.2306 | Umbral Deformations on Discrete Spacetime | Given a minimum measurable length underlying spacetime, the latter may be
effectively regarded as discrete, at scales of order the Planck length. A
systematic discretization of continuum physics may be effected most efficiently
through the umbral deformation. General functionals yielding such deformations
at the leve... | hep-th gr-qc math-ph math.MP | given a minimum measurable length underlying spacetime the latter may be effectively regarded as discrete at scales of order the planck length a systematic discretization of continuum physics may be effected most efficiently through the umbral deformation general functionals yielding such deformations at the level of s... | [['given', 'a', 'minimum', 'measurable', 'length', 'underlying', 'spacetime', 'the', 'latter', 'may', 'be', 'effectively', 'regarded', 'as', 'discrete', 'at', 'scales', 'of', 'order', 'the', 'planck', 'length', 'a', 'systematic', 'discretization', 'of', 'continuum', 'physics', 'may', 'be', 'effected', 'most', 'efficien... | [-0.13207030751472038, 0.2005277150761216, -0.07940966874781635, 0.1303169542713271, -0.0817187941002269, -0.10105454973546008, -0.03459476191745771, 0.3307973228267304, -0.3514483090313602, -0.2777960251175588, 0.13655969441958493, -0.25245874752140335, -0.11335657915521052, 0.20509848788741133, 1.2183944965081831e-05... |
710.2307 | A stability version of H\"older's inequality | We present a stability version of H\"older's inequality, incorporating an
extra term that measures the deviation from equality. Applications are given.
| math.CA math.AP | we present a stability version of holders inequality incorporating an extra term that measures the deviation from equality applications are given | [['we', 'present', 'a', 'stability', 'version', 'of', 'holders', 'inequality', 'incorporating', 'an', 'extra', 'term', 'that', 'measures', 'the', 'deviation', 'from', 'equality', 'applications', 'are', 'given']] | [-0.1308609947917007, 0.03198771159389123, -0.13051582340683257, 0.1573127124103762, -0.06419986850094228, -0.1755023798461826, 0.04362706222482735, 0.26247756741940975, -0.3170111860547747, -0.2819220449420668, 0.18345538231854638, -0.3733899439019816, -0.12633240861552103, 0.1895333936526662, -0.15112112582262074, -0... |
710.2308 | Entanglement on demand through time reordering | Entangled photons can be generated "on demand" in a novel scheme involving
unitary time reordering of the photons emitted in a radiative decay cascade.
The scheme yields polarization entangled photon pairs, even though prior to
reordering the emitted photons carry significant "which path information" and
their polari... | quant-ph cond-mat.mes-hall | entangled photons can be generated on demand in a novel scheme involving unitary time reordering of the photons emitted in a radiative decay cascade the scheme yields polarization entangled photon pairs even though prior to reordering the emitted photons carry significant which path information and their polarizations ... | [['entangled', 'photons', 'can', 'be', 'generated', 'on', 'demand', 'in', 'a', 'novel', 'scheme', 'involving', 'unitary', 'time', 'reordering', 'of', 'the', 'photons', 'emitted', 'in', 'a', 'radiative', 'decay', 'cascade', 'the', 'scheme', 'yields', 'polarization', 'entangled', 'photon', 'pairs', 'even', 'though', 'pri... | [-0.12840586967474546, 0.28201165577643605, -0.11530335537012083, 0.05396733909539587, 0.013777083633130932, -0.20842130716149526, 0.03807677229703685, 0.4628083916627858, -0.2967051109186856, -0.27512815958225584, -0.023677126940687646, -0.26869562503892974, -0.025407472569271023, 0.23229959326605482, 0.00072205294462... |
710.2309 | Glueballs in Flatland | The pure gauge theory in 2+1 dimensions is explored, through both a
phenomenological model and a lattice calculation. The Isgur-Paton model is
extended to include a curvature term and various mixing mechanisms. The method
of inferential statistics is used to extract the parameters of best fit and to
compare the likel... | hep-lat | the pure gauge theory in 21 dimensions is explored through both a phenomenological model and a lattice calculation the isgurpaton model is extended to include a curvature term and various mixing mechanisms the method of inferential statistics is used to extract the parameters of best fit and to compare the likelihoods ... | [['the', 'pure', 'gauge', 'theory', 'in', '21', 'dimensions', 'is', 'explored', 'through', 'both', 'a', 'phenomenological', 'model', 'and', 'a', 'lattice', 'calculation', 'the', 'isgurpaton', 'model', 'is', 'extended', 'to', 'include', 'a', 'curvature', 'term', 'and', 'various', 'mixing', 'mechanisms', 'the', 'method',... | [-0.06930025436726588, 0.13873033994691564, -0.06279613214408185, 0.10420760830988053, -0.05210667244367093, -0.13707611069955922, 0.04486051478693457, 0.3494040420917156, -0.23909997621590232, -0.2962597814108525, 0.09674089841082223, -0.2825545374746923, -0.09548924603154296, 0.12733056715696112, 0.03406896079415, 0.... |
710.231 | Integrability of Rough Almost Complex Structures | We extend the Newlander-Nirenberg theorem to manifolds with almost complex
structures that have somewhat less than Lipschitz regularity. We also discuss
the regularity of local holomorphic coordinates in the integrable case, with
particular attention to Lipschitz almost complex structures.
| math.DG math.AP math.CV | we extend the newlandernirenberg theorem to manifolds with almost complex structures that have somewhat less than lipschitz regularity we also discuss the regularity of local holomorphic coordinates in the integrable case with particular attention to lipschitz almost complex structures | [['we', 'extend', 'the', 'newlandernirenberg', 'theorem', 'to', 'manifolds', 'with', 'almost', 'complex', 'structures', 'that', 'have', 'somewhat', 'less', 'than', 'lipschitz', 'regularity', 'we', 'also', 'discuss', 'the', 'regularity', 'of', 'local', 'holomorphic', 'coordinates', 'in', 'the', 'integrable', 'case', 'wi... | [-0.138671523031707, 0.028251171541901734, -0.05579321048198602, 0.13597806590871933, -0.1506649835082965, -0.12099642588351017, -0.0688322836246628, 0.4446640350879767, -0.28002451479626006, -0.167329543389571, 0.13022996039571574, -0.24680477435676715, -0.19225124680461028, 0.1971163059083315, -0.13452629544414008, 0... |
710.2311 | Testing Benson's Regularity Conjecture | D. J. Benson conjectures that the Castelnuovo-Mumford regularity of a group
cohomology ring is always zero. More generally he conjectures that the
cohomology ring always has a system of parameters satisfying a property he
calls very strong quasi-regular. Using computer calculations we find that the
more general conje... | math.GR | d j benson conjectures that the castelnuovomumford regularity of a group cohomology ring is always zero more generally he conjectures that the cohomology ring always has a system of parameters satisfying a property he calls very strong quasiregular using computer calculations we find that the more general conjecture ho... | [['d', 'j', 'benson', 'conjectures', 'that', 'the', 'castelnuovomumford', 'regularity', 'of', 'a', 'group', 'cohomology', 'ring', 'is', 'always', 'zero', 'more', 'generally', 'he', 'conjectures', 'that', 'the', 'cohomology', 'ring', 'always', 'has', 'a', 'system', 'of', 'parameters', 'satisfying', 'a', 'property', 'he'... | [-0.21881585775286352, 0.04868728082561702, -0.14175195848209815, 0.08101257753125474, -0.07841895578690526, -0.2564495412485772, -0.01201887000678924, 0.3223888729086244, -0.22978295428318934, -0.22664470477193072, 0.08588626293726918, -0.24432071768515334, -0.1125743502032077, 0.2203788083299929, -0.09663873780191991... |
710.2312 | Supercriticality of a Class of Critical String Cosmological Solutions | For a class of Friedmann-Robertson-Walker type string solutions with compact
hyperbolic spatial slices formulated in critical dimension, we find the world
sheet conformal field theory which involves the linear dilaton and
Wess-Zumino-Witten type model with the compact hyperbolic target space. By
analyzing the infrare... | hep-th | for a class of friedmannrobertsonwalker type string solutions with compact hyperbolic spatial slices formulated in critical dimension we find the world sheet conformal field theory which involves the linear dilaton and wesszuminowitten type model with the compact hyperbolic target space by analyzing the infrared spectr... | [['for', 'a', 'class', 'of', 'friedmannrobertsonwalker', 'type', 'string', 'solutions', 'with', 'compact', 'hyperbolic', 'spatial', 'slices', 'formulated', 'in', 'critical', 'dimension', 'we', 'find', 'the', 'world', 'sheet', 'conformal', 'field', 'theory', 'which', 'involves', 'the', 'linear', 'dilaton', 'and', 'wessz... | [-0.13853141325328253, 0.13187491342003616, -0.07575860707405603, 0.13474969963657335, -0.12029645490934546, -0.17087480201790073, -0.01513008269336391, 0.3236481185194175, -0.21232105388288508, -0.23184629937827164, 0.09537531130174, -0.23560506842573578, -0.18113204285080703, 0.15905374392673796, -0.04084895834115878... |
710.2313 | Super-Reflection in Fluid Discs: Corotation Amplifier, Corotation
Resonance, Rossby Waves, and Overstable Modes | In differentially rotating discs with no self-gravity, density waves cannot
propagate around the corotation, where the wave pattern rotation speed equals
the fluid rotation rate. Waves incident upon the corotation barrier may be
super-reflected (commonly referred to as corotation amplifier), but the
reflection can be... | astro-ph | in differentially rotating discs with no selfgravity density waves cannot propagate around the corotation where the wave pattern rotation speed equals the fluid rotation rate waves incident upon the corotation barrier may be superreflected commonly referred to as corotation amplifier but the reflection can be strongly ... | [['in', 'differentially', 'rotating', 'discs', 'with', 'no', 'selfgravity', 'density', 'waves', 'can', 'not', 'propagate', 'around', 'the', 'corotation', 'where', 'the', 'wave', 'pattern', 'rotation', 'speed', 'equals', 'the', 'fluid', 'rotation', 'rate', 'waves', 'incident', 'upon', 'the', 'corotation', 'barrier', 'ma... | [-0.19245712022921987, 0.11786979951997109, -0.05044233445271155, 0.0757756906053669, -0.1262942133869474, -0.0877432913948912, -0.008352233791830008, 0.34390703129818556, -0.2867850308183465, -0.26045460319339536, 0.09243965816353521, -0.23749599199732427, -0.09198510027466429, 0.19483691168957454, -0.0065914186084440... |
710.2314 | A Flattened Protostellar Envelope in Absorption around L1157 | Deep Spitzer IRAC images of L1157 reveal many of the details of the outflow
and the circumstellar environment of this Class 0 protostar. In IRAC band 4, 8
microns, there is a flattened structure seen in absorption against the
background emission. The structure is perpendicular to the outflow and is
extended to a diam... | astro-ph | deep spitzer irac images of l1157 reveal many of the details of the outflow and the circumstellar environment of this class 0 protostar in irac band 4 8 microns there is a flattened structure seen in absorption against the background emission the structure is perpendicular to the outflow and is extended to a diameter o... | [['deep', 'spitzer', 'irac', 'images', 'of', 'l1157', 'reveal', 'many', 'of', 'the', 'details', 'of', 'the', 'outflow', 'and', 'the', 'circumstellar', 'environment', 'of', 'this', 'class', '0', 'protostar', 'in', 'irac', 'band', '4', '8', 'microns', 'there', 'is', 'a', 'flattened', 'structure', 'seen', 'in', 'absorptio... | [-0.09664493316858677, 0.06652476613237769, -0.07378701794999692, 0.07627407492517568, -0.1019190272060841, -0.10019797639482432, -0.05489362863642452, 0.4856692387071331, -0.2296744208183836, -0.3026676615288036, 0.05247271551124224, -0.23165268096578331, -0.0953099087119696, 0.0957036820926448, -0.019255443929439096,... |
710.2315 | Universal Mandelbrot Set as a Model of Phase Transition Theory | The study of Mandelbrot Sets (MS) is a promising new approach to the phase
transition theory. We suggest two improvements which drastically simplify the
construction of MS. They could be used to modify the existing computer programs
so that they start building MS properly not only for the simplest families.
This allo... | nlin.CD cond-mat.stat-mech hep-th math.CV math.DS | the study of mandelbrot sets ms is a promising new approach to the phase transition theory we suggest two improvements which drastically simplify the construction of ms they could be used to modify the existing computer programs so that they start building ms properly not only for the simplest families this allows us t... | [['the', 'study', 'of', 'mandelbrot', 'sets', 'ms', 'is', 'a', 'promising', 'new', 'approach', 'to', 'the', 'phase', 'transition', 'theory', 'we', 'suggest', 'two', 'improvements', 'which', 'drastically', 'simplify', 'the', 'construction', 'of', 'ms', 'they', 'could', 'be', 'used', 'to', 'modify', 'the', 'existing', 'c... | [-0.08890288547074494, 0.1132676951079206, -0.14055194432980248, 0.0821515606170484, -0.15651319255786283, -0.13435837814535995, 0.09942617455902569, 0.35024777238632177, -0.2749581117570013, -0.3142734661928148, 0.0985174127128701, -0.21219579624212437, -0.15871886156692908, 0.22662917853562864, -0.085519180548462, -0... |
710.2316 | The Complex Frobenius Theorem for Rough Involutive Structures | We establish a version of the complex Frobenius theorem in the context of a
complex subbundle S of the complexified tangent bundle of a manifold, having
minimal regularity. If the subbundle S defines the structure of a Levi-flat
CR-manifold, it suffices that S be Lipschitz for our results to apply. A
principal tool i... | math.DG math.AP math.CV | we establish a version of the complex frobenius theorem in the context of a complex subbundle s of the complexified tangent bundle of a manifold having minimal regularity if the subbundle s defines the structure of a leviflat crmanifold it suffices that s be lipschitz for our results to apply a principal tool in the an... | [['we', 'establish', 'a', 'version', 'of', 'the', 'complex', 'frobenius', 'theorem', 'in', 'the', 'context', 'of', 'a', 'complex', 'subbundle', 's', 'of', 'the', 'complexified', 'tangent', 'bundle', 'of', 'a', 'manifold', 'having', 'minimal', 'regularity', 'if', 'the', 'subbundle', 's', 'defines', 'the', 'structure', '... | [-0.17147788728576108, -0.0032941616555473893, -0.10709216131503324, 0.04747778541515076, -0.1267618075776172, -0.12118518355874772, -0.012050788714943162, 0.30687795086842345, -0.2761143639526633, -0.20739963808355022, 0.10464423042385423, -0.23215386398832302, -0.1676165466926184, 0.19956929976518928, -0.108855887865... |
710.2317 | Numerical simulation of excitation of solar oscillation modes for
different turbulent models | The goal of this research is to investigate how well various turbulence
models can describe physical properties of the upper convective boundary layer
of the Sun. An accurate modeling of the turbulence motions is necessary for
understanding the excitation mechanisms of solar oscillation modes. We have
carried out rea... | astro-ph | the goal of this research is to investigate how well various turbulence models can describe physical properties of the upper convective boundary layer of the sun an accurate modeling of the turbulence motions is necessary for understanding the excitation mechanisms of solar oscillation modes we have carried out realist... | [['the', 'goal', 'of', 'this', 'research', 'is', 'to', 'investigate', 'how', 'well', 'various', 'turbulence', 'models', 'can', 'describe', 'physical', 'properties', 'of', 'the', 'upper', 'convective', 'boundary', 'layer', 'of', 'the', 'sun', 'an', 'accurate', 'modeling', 'of', 'the', 'turbulence', 'motions', 'is', 'nec... | [-0.10716207681743559, 0.1309826272076333, -0.07771500003184693, 0.08325979568478435, -0.05035621985836431, -0.04361367440609218, -0.008265318125648813, 0.3498808777685342, -0.242530609564964, -0.3451163096429217, 0.08193559567599698, -0.26054438644056316, -0.12447252594439454, 0.2242291135182821, 0.019730564516828242,... |
710.2318 | Planetesimal Formation with Particle Feedback | Proposed mechanisms for the formation of km-sized solid planetesimals face
long-standing difficulties. Robust sticking mechanisms that would produce
planetesimals by coagulation alone remain elusive. The gravitational collapse
of smaller solids into planetesimals is opposed by stirring from turbulent gas.
This procee... | astro-ph | proposed mechanisms for the formation of kmsized solid planetesimals face longstanding difficulties robust sticking mechanisms that would produce planetesimals by coagulation alone remain elusive the gravitational collapse of smaller solids into planetesimals is opposed by stirring from turbulent gas this proceeding de... | [['proposed', 'mechanisms', 'for', 'the', 'formation', 'of', 'kmsized', 'solid', 'planetesimals', 'face', 'longstanding', 'difficulties', 'robust', 'sticking', 'mechanisms', 'that', 'would', 'produce', 'planetesimals', 'by', 'coagulation', 'alone', 'remain', 'elusive', 'the', 'gravitational', 'collapse', 'of', 'smaller... | [-0.13402366623537795, 0.1960339509251137, -0.08709624489288657, 0.11434976924999407, -0.07292685486496456, -0.02112233101375281, -0.043407031840498315, 0.26008286982053713, -0.2353508278179253, -0.3018062912648724, 0.006913123720404392, -0.21468121031179063, -0.10258566065890444, 0.16022823073135148, -0.00817989640598... |
710.2319 | Weyl's law in the theory of automorphic forms | For a compact Riemannian manifold, Weyl's law describes the asymptotic
behavior of the counting function of the eigenvalues of the associated Laplace
operator. In this paper we discuss Weyl's law in the context of automorphic
forms. The underlying manifolds are locally symmetric spaces of finite volume.
In the non-co... | math.SP math.NT | for a compact riemannian manifold weyls law describes the asymptotic behavior of the counting function of the eigenvalues of the associated laplace operator in this paper we discuss weyls law in the context of automorphic forms the underlying manifolds are locally symmetric spaces of finite volume in the noncompact cas... | [['for', 'a', 'compact', 'riemannian', 'manifold', 'weyls', 'law', 'describes', 'the', 'asymptotic', 'behavior', 'of', 'the', 'counting', 'function', 'of', 'the', 'eigenvalues', 'of', 'the', 'associated', 'laplace', 'operator', 'in', 'this', 'paper', 'we', 'discuss', 'weyls', 'law', 'in', 'the', 'context', 'of', 'autom... | [-0.18767618829946195, 0.0798727605743186, -0.1510782747264741, 0.13457595317491464, -0.14641976297374756, -0.07561335775498597, -0.03638393598763893, 0.24880319387311972, -0.25964971132103415, -0.19917527669005924, 0.1325110093088052, -0.29962264378333375, -0.20503696003219202, 0.17793417668029193, -0.1614950952814921... |
710.232 | Random walk delayed on percolation clusters | We study a continuous time random walk on the $d$-dimensional lattice,
subject to a drift and an attraction to large clusters of a subcritical
Bernoulli site percolation. We find two distinct regimes: a ballistic one, and
a subballistic one taking place when the attraction is strong enough. We
identify the speed in t... | math.PR | we study a continuous time random walk on the ddimensional lattice subject to a drift and an attraction to large clusters of a subcritical bernoulli site percolation we find two distinct regimes a ballistic one and a subballistic one taking place when the attraction is strong enough we identify the speed in the former ... | [['we', 'study', 'a', 'continuous', 'time', 'random', 'walk', 'on', 'the', 'ddimensional', 'lattice', 'subject', 'to', 'a', 'drift', 'and', 'an', 'attraction', 'to', 'large', 'clusters', 'of', 'a', 'subcritical', 'bernoulli', 'site', 'percolation', 'we', 'find', 'two', 'distinct', 'regimes', 'a', 'ballistic', 'one', 'a... | [-0.1808246879139915, 0.17650936382869986, -0.06700584915815852, 0.07929001790034818, -0.020725889873574488, -0.14278393922722898, 0.09775998865370639, 0.3287694806640502, -0.295444921113085, -0.1399254351039417, 0.09033315731358016, -0.2819703057757579, -0.11608003317378461, 0.1513477323227562, 0.0026944700366584584, ... |
710.2321 | Acoustic Probing of the Jamming Transition in an Unconsolidated Granular
Medium | Experiments with acoustic waves guided along the mechanically free surface of
an unconsolidated granular packed structure provide information on the
elasticity of granular media at very low pressures that are naturally
controlled by the gravitational acceleration and the depth beneath the surface.
Comparison of the d... | physics.class-ph cond-mat.soft | experiments with acoustic waves guided along the mechanically free surface of an unconsolidated granular packed structure provide information on the elasticity of granular media at very low pressures that are naturally controlled by the gravitational acceleration and the depth beneath the surface comparison of the dete... | [['experiments', 'with', 'acoustic', 'waves', 'guided', 'along', 'the', 'mechanically', 'free', 'surface', 'of', 'an', 'unconsolidated', 'granular', 'packed', 'structure', 'provide', 'information', 'on', 'the', 'elasticity', 'of', 'granular', 'media', 'at', 'very', 'low', 'pressures', 'that', 'are', 'naturally', 'contr... | [-0.14623124019171183, 0.24421888331965488, -0.13293985419620116, -0.028540116018400744, -0.08956142501153339, -0.07264484077906952, 0.03377516149238755, 0.35017612722093383, -0.31570086639392403, -0.2711353740941447, 0.0454002972996722, -0.3062729526311159, -0.1539159734500572, 0.19435224343771831, 0.01666494300588965... |
710.2322 | Long-living superpartners in the MSSM | The parameter space of the Constrained Minimal supersymmetric Standard Model
is considered. It is shown that for the particular choice of parameters there
are some regions where long-living charged superparticles exist. Two regions of
interest are the co-annihilation region with light staus, and the region with
large... | hep-ph | the parameter space of the constrained minimal supersymmetric standard model is considered it is shown that for the particular choice of parameters there are some regions where longliving charged superparticles exist two regions of interest are the coannihilation region with light staus and the region with large negati... | [['the', 'parameter', 'space', 'of', 'the', 'constrained', 'minimal', 'supersymmetric', 'standard', 'model', 'is', 'considered', 'it', 'is', 'shown', 'that', 'for', 'the', 'particular', 'choice', 'of', 'parameters', 'there', 'are', 'some', 'regions', 'where', 'longliving', 'charged', 'superparticles', 'exist', 'two', '... | [-0.14562070267311356, 0.3221420061890967, 0.04093116463627666, 0.16685975077962212, -0.08101099741907092, -0.24113054118788568, -0.010234861285425723, 0.3332817634291132, -0.22145300032570958, -0.26460843681707047, 0.10738247551853419, -0.2793466591683682, -0.07811268922523595, 0.1713528760265035, -3.630971423262963e-... |
710.2323 | The role of spin noise in the detection of nanoscale ensembles of
nuclear spins | When probing nuclear spins in materials on the nanometer scale, random
fluctuations of the spin polarization will exceed the mean Boltzmann
polarization for sample volumes below about (100nm)^3. In this work, we use
magnetic resonance force microscopy to observe nuclear spin fluctuations in
real time. We show how rep... | cond-mat.mes-hall | when probing nuclear spins in materials on the nanometer scale random fluctuations of the spin polarization will exceed the mean boltzmann polarization for sample volumes below about 100nm3 in this work we use magnetic resonance force microscopy to observe nuclear spin fluctuations in real time we show how reproducible... | [['when', 'probing', 'nuclear', 'spins', 'in', 'materials', 'on', 'the', 'nanometer', 'scale', 'random', 'fluctuations', 'of', 'the', 'spin', 'polarization', 'will', 'exceed', 'the', 'mean', 'boltzmann', 'polarization', 'for', 'sample', 'volumes', 'below', 'about', '100nm3', 'in', 'this', 'work', 'we', 'use', 'magnetic... | [-0.1469937492895158, 0.2532855581759693, -0.036565396238732686, 0.043560662643706546, -0.0012755116764852342, -0.10177179233002615, 0.025267469870704325, 0.4140055459389027, -0.2716979229218386, -0.34109703792219465, 0.0481569151780469, -0.2702798928986204, -0.047069729266173026, 0.22351316428257825, 0.027741063326755... |
710.2324 | Study of $\psi(2S)$ decays into $\gamma K^+K^-$ and $\gamma \pi^+\pi^-$ | Radiative charmonium decays from the BESII sample of 14$\times10^{6}$
$\psi(2S)$-events into two different final states, $\gamma K^+K^-$ and
$\gamma\pi^+\pi^-$, are analyzed. Product branching fractions for
$\psi(2S)\to\gamma X\to \gamma\pi^+\pi^-$, $\gamma K^+K^-$ are given, where
$X=f_2(1270)$, $f_0(1500)$, and $f_... | hep-ex | radiative charmonium decays from the besii sample of 14times106 psi2sevents into two different final states gamma kk and gammapipi are analyzed product branching fractions for psi2stogamma xto gammapipi gamma kk are given where xf_21270 f_01500 and f_01710 in pipi and f_21270 f_21525 and f_01700 in kk an angular analys... | [['radiative', 'charmonium', 'decays', 'from', 'the', 'besii', 'sample', 'of', '14times106', 'psi2sevents', 'into', 'two', 'different', 'final', 'states', 'gamma', 'kk', 'and', 'gammapipi', 'are', 'analyzed', 'product', 'branching', 'fractions', 'for', 'psi2stogamma', 'xto', 'gammapipi', 'gamma', 'kk', 'are', 'given', ... | [-0.09775033414916834, 0.2957432008388423, -0.08148218890632311, 0.1368849392581199, -0.0032420551786864443, -0.09611293360857028, 0.046489075377134474, 0.28526670479082633, -0.17059697985782155, -0.17226438141161843, -0.10716448872075748, -0.37126554841441767, 0.0726231184255864, 0.14424636173394642, 0.137637967609667... |
710.2325 | SU(5) Completion of the Dark Scalar Doublet Model of Radiative Neutrino
Mass | Adding a second scalar doublet (eta^+,eta^0) and three neutral singlet
fermions N_{1,2,3} to the Standard Model of particle interactions with a new
Z_2 symmetry, it has been shown that eta^0_R or eta^0_I is a good dark-matter
candidate and seesaw neutrino masses are generated radiatively. A minimal
extension of this ... | hep-ph | adding a second scalar doublet etaeta0 and three neutral singlet fermions n_123 to the standard model of particle interactions with a new z_2 symmetry it has been shown that eta0_r or eta0_i is a good darkmatter candidate and seesaw neutrino masses are generated radiatively a minimal extension of this new idea is propo... | [['adding', 'a', 'second', 'scalar', 'doublet', 'etaeta0', 'and', 'three', 'neutral', 'singlet', 'fermions', 'n_123', 'to', 'the', 'standard', 'model', 'of', 'particle', 'interactions', 'with', 'a', 'new', 'z_2', 'symmetry', 'it', 'has', 'been', 'shown', 'that', 'eta0_r', 'or', 'eta0_i', 'is', 'a', 'good', 'darkmatter'... | [-0.08039876899675692, 0.2425348907834976, -0.017786247659682272, 0.19686109021721357, -0.14415408424227624, -0.24113804912760956, -0.02986990024864271, 0.35404652567907563, -0.18731621007837757, -0.3172504043936528, 0.05505764207211197, -0.2696511316320834, -0.04689857005330457, 0.08109686050620685, 0.0342555789031541... |
710.2326 | The resultant on compact Riemann surfaces | We introduce a notion of resultant of two meromorphic functions on a compact
Riemann surface and demonstrate its usefulness in several respects. For
example, we exhibit several integral formulas for the resultant, relate it to
potential theory and give explicit formulas for the algebraic dependence
between two meromo... | math.AG math.CV | we introduce a notion of resultant of two meromorphic functions on a compact riemann surface and demonstrate its usefulness in several respects for example we exhibit several integral formulas for the resultant relate it to potential theory and give explicit formulas for the algebraic dependence between two meromorphic... | [['we', 'introduce', 'a', 'notion', 'of', 'resultant', 'of', 'two', 'meromorphic', 'functions', 'on', 'a', 'compact', 'riemann', 'surface', 'and', 'demonstrate', 'its', 'usefulness', 'in', 'several', 'respects', 'for', 'example', 'we', 'exhibit', 'several', 'integral', 'formulas', 'for', 'the', 'resultant', 'relate', '... | [-0.1609557326401359, 0.008035856266987735, -0.11444660525597718, 0.12574236751293186, -0.10066212896771472, -0.05951917673536073, 0.0194731769031556, 0.34841369439301817, -0.2595274918338006, -0.21878173360708117, 0.1075917400818468, -0.22266871253585166, -0.22905669312110577, 0.3152638739938366, -0.021425719199977794... |
710.2327 | Theory of shot noise in single-walled metallic carbon nanotubes weakly
coupled to nonmagnetic and ferromagnetic leads | We present theoretical study of shot noise in single wall metallic carbon
nanotubes weakly coupled to either nonmagnetic or ferromagnetic leads. Using
the real-time diagrammatic technique, we calculate the current, Fano factor and
tunnel magnetoresistance in the sequential tunneling regime. It is shown that
the diffe... | cond-mat.mes-hall cond-mat.mtrl-sci | we present theoretical study of shot noise in single wall metallic carbon nanotubes weakly coupled to either nonmagnetic or ferromagnetic leads using the realtime diagrammatic technique we calculate the current fano factor and tunnel magnetoresistance in the sequential tunneling regime it is shown that the differential... | [['we', 'present', 'theoretical', 'study', 'of', 'shot', 'noise', 'in', 'single', 'wall', 'metallic', 'carbon', 'nanotubes', 'weakly', 'coupled', 'to', 'either', 'nonmagnetic', 'or', 'ferromagnetic', 'leads', 'using', 'the', 'realtime', 'diagrammatic', 'technique', 'we', 'calculate', 'the', 'current', 'fano', 'factor',... | [-0.21503204704495146, 0.08901495319894619, -0.0342267919331789, 0.033317688974137935, -0.011574755989325542, -0.20816022644543813, 0.08014398142824777, 0.40586316238881814, -0.2522435257004367, -0.29467873852699994, -0.03159478326948981, -0.3045975309974488, -0.1790175367276081, 0.21290585565535972, -0.024953423114493... |
710.2328 | An approach to the finitistic dimension conjecture | Let $R$ be a finite dimensional $k$-algebra over an algebraically closed
field $k$ and $\mathrm{mod} R$ be the category of all finitely generated left
$R$-modules. For a given full subcategory $\mathcal{X}$ of $\mathrm{mod} R,$ we
denote by $\pfd \mathcal{X}$ the projective finitistic dimension of
$\mathcal{X}.$ That... | math.RT | let r be a finite dimensional kalgebra over an algebraically closed field k and mathrmmod r be the category of all finitely generated left rmodules for a given full subcategory mathcalx of mathrmmod r we denote by pfd mathcalx the projective finitistic dimension of mathcalx that is pfd mathcalxmathrmsup pd x xinmathcal... | [['let', 'r', 'be', 'a', 'finite', 'dimensional', 'kalgebra', 'over', 'an', 'algebraically', 'closed', 'field', 'k', 'and', 'mathrmmod', 'r', 'be', 'the', 'category', 'of', 'all', 'finitely', 'generated', 'left', 'rmodules', 'for', 'a', 'given', 'full', 'subcategory', 'mathcalx', 'of', 'mathrmmod', 'r', 'we', 'denote',... | [-0.16831969950779727, 0.046100967476466, -0.08186699017859632, 0.021613115507956002, -0.04992956202193277, -0.21940183403288446, -0.06546377668032287, 0.3459678533282585, -0.3530605667719345, -0.15114390632569244, 0.0820531064762291, -0.22586158266228556, -0.04910970921202267, 0.1874914714759897, -0.13115145016189028,... |
710.2329 | Magnetic Moment of Vector Mesons in the Background Field Method | We report some results for the magnetic moments of vector mesons extracted
from mass shifts in the presence of static external magnetic fields. The
calculations are done on $24^4$ quenched lattices using standard Wilson
actions, with $\beta$=6.0 and pion mass down to 500 MeV. The results are
compared to those from th... | hep-lat | we report some results for the magnetic moments of vector mesons extracted from mass shifts in the presence of static external magnetic fields the calculations are done on 244 quenched lattices using standard wilson actions with beta60 and pion mass down to 500 mev the results are compared to those from the form factor... | [['we', 'report', 'some', 'results', 'for', 'the', 'magnetic', 'moments', 'of', 'vector', 'mesons', 'extracted', 'from', 'mass', 'shifts', 'in', 'the', 'presence', 'of', 'static', 'external', 'magnetic', 'fields', 'the', 'calculations', 'are', 'done', 'on', '244', 'quenched', 'lattices', 'using', 'standard', 'wilson', ... | [-0.08071696199476719, 0.23502503389661963, -0.013903528265655041, 0.08032262203368273, -0.020273543596373532, -0.03488258278336037, 0.09374761320650578, 0.4483345102180134, -0.15848450772464276, -0.33555922928181564, 0.04431962936227633, -0.33849437988617204, -0.007049313077533787, 0.20425034566274422, 0.0780287355692... |
710.233 | On NIP and invariant measures | We study forking, Lascar strong types, Keisler measures and definable groups,
under an assumption of $NIP$ (not the independence property), continuing
aspects of math.LO/0607442. Among key results are: (i) if $p = tp(b/A)$ does
not fork over $A$ then the Lascar strong type of $b$ over $A$ coincides with
the compact s... | math.LO | we study forking lascar strong types keisler measures and definable groups under an assumption of nip not the independence property continuing aspects of mathlo0607442 among key results are i if p tpba does not fork over a then the lascar strong type of b over a coincides with the compact strong type of b over a and an... | [['we', 'study', 'forking', 'lascar', 'strong', 'types', 'keisler', 'measures', 'and', 'definable', 'groups', 'under', 'an', 'assumption', 'of', 'nip', 'not', 'the', 'independence', 'property', 'continuing', 'aspects', 'of', 'mathlo0607442', 'among', 'key', 'results', 'are', 'i', 'if', 'p', 'tpba', 'does', 'not', 'fork... | [-0.18929082262911834, 0.0984431110365449, -0.1024812348314299, 0.10223533575572219, -0.12119342527876142, -0.14412316615926102, 0.04799213073283681, 0.37585102109005675, -0.28731657651951537, -0.16705541688861558, 0.07615366594018269, -0.22489205630517972, -0.07039028343933751, 0.22999013065418694, -0.1428028222780994... |
710.2331 | On the energy growth of some periodically driven quantum systems with
shrinking gaps in the spectrum | We consider quantum Hamiltonians of the form H(t)=H+V(t) where the spectrum
of H is semibounded and discrete, and the eigenvalues behave as E_n~n^\alpha,
with 0<\alpha<1. In particular, the gaps between successive eigenvalues decay
as n^{\alpha-1}. V(t) is supposed to be periodic, bounded, continuously
differentiable... | math-ph math.MP | we consider quantum hamiltonians of the form hthvt where the spectrum of h is semibounded and discrete and the eigenvalues behave as e_nnalpha with 0alpha1 in particular the gaps between successive eigenvalues decay as nalpha1 vt is supposed to be periodic bounded continuously differentiable in the strong sense and suc... | [['we', 'consider', 'quantum', 'hamiltonians', 'of', 'the', 'form', 'hthvt', 'where', 'the', 'spectrum', 'of', 'h', 'is', 'semibounded', 'and', 'discrete', 'and', 'the', 'eigenvalues', 'behave', 'as', 'e_nnalpha', 'with', '0alpha1', 'in', 'particular', 'the', 'gaps', 'between', 'successive', 'eigenvalues', 'decay', 'as... | [-0.11232726362575177, 0.18572158831645333, -0.030504303312139405, 0.05289711491223575, -0.03266528638332308, -0.15911812984174298, -0.016335732333602443, 0.3548233914339254, -0.29513426448008223, -0.2575061084508273, 0.12002616848011742, -0.28846551613946025, -0.13025210460135336, 0.167418003608022, -0.041353894608384... |
710.2332 | Application of the RMF mass model to the r-process and the influence of
mass uncertainties | A new mass table calculated by the relativistic mean field approach with the
state-dependent BCS method for the pairing correlation is applied for the first
time to study r-process nucleosynthesis. The solar r-process abundance is well
reproduced within a waiting-point approximation approach. Using an exponential
fit... | astro-ph nucl-th | a new mass table calculated by the relativistic mean field approach with the statedependent bcs method for the pairing correlation is applied for the first time to study rprocess nucleosynthesis the solar rprocess abundance is well reproduced within a waitingpoint approximation approach using an exponential fitting pro... | [['a', 'new', 'mass', 'table', 'calculated', 'by', 'the', 'relativistic', 'mean', 'field', 'approach', 'with', 'the', 'statedependent', 'bcs', 'method', 'for', 'the', 'pairing', 'correlation', 'is', 'applied', 'for', 'the', 'first', 'time', 'to', 'study', 'rprocess', 'nucleosynthesis', 'the', 'solar', 'rprocess', 'abun... | [-0.029170360721120264, 0.11786133613124741, -0.09264148832752114, 0.18013907060340312, 0.0036744710739982206, -0.0675741655224588, 0.031133517989707468, 0.3839320729989394, -0.2051974318888599, -0.33589502415759903, 0.009716374432849409, -0.2366856694205013, -0.04132792778906569, 0.2134293031660362, 0.0291551975121276... |
710.2333 | Time delay and magnification centroid due to gravitational lensing by
black holes and naked singularities | We model the massive dark object at the center of the Galaxy as a
Schwarzschild black hole as well as Janis-Newman-Winicour naked singularities,
characterized by the mass and scalar charge parameters, and study gravitational
lensing (particularly time delay, magnification centroid, and total
magnification) by them. W... | gr-qc astro-ph hep-th physics.class-ph | we model the massive dark object at the center of the galaxy as a schwarzschild black hole as well as janisnewmanwinicour naked singularities characterized by the mass and scalar charge parameters and study gravitational lensing particularly time delay magnification centroid and total magnification by them we find that... | [['we', 'model', 'the', 'massive', 'dark', 'object', 'at', 'the', 'center', 'of', 'the', 'galaxy', 'as', 'a', 'schwarzschild', 'black', 'hole', 'as', 'well', 'as', 'janisnewmanwinicour', 'naked', 'singularities', 'characterized', 'by', 'the', 'mass', 'and', 'scalar', 'charge', 'parameters', 'and', 'study', 'gravitation... | [-0.14610297989923293, 0.06551221714726764, -0.08228450671518467, 0.17788593004776262, -0.11419732450393208, -0.19324585489863366, -0.08367273189523666, 0.3489497394480726, -0.171721509563851, -0.3132767153560723, 0.07333402220147515, -0.35117995147715864, -0.10810033921989727, 0.2130475941383721, -0.05674528342001794,... |
710.2334 | Off-center impurity in alkali halides: reorientation, electric
polarization and pairing to F center. III. Numerical calculations | We carried out numerical calculations by an extended-Hueckel program in order
to check the analytical results reported in the preceding Part I and Part II.
We typically consider alkali halide clusters composed of some tens of
constituent atoms to calculate electronic energies under static conditions or
versus the dis... | physics.chem-ph physics.comp-ph | we carried out numerical calculations by an extendedhueckel program in order to check the analytical results reported in the preceding part i and part ii we typically consider alkali halide clusters composed of some tens of constituent atoms to calculate electronic energies under static conditions or versus the displac... | [['we', 'carried', 'out', 'numerical', 'calculations', 'by', 'an', 'extendedhueckel', 'program', 'in', 'order', 'to', 'check', 'the', 'analytical', 'results', 'reported', 'in', 'the', 'preceding', 'part', 'i', 'and', 'part', 'ii', 'we', 'typically', 'consider', 'alkali', 'halide', 'clusters', 'composed', 'of', 'some', ... | [-0.10795150075956614, 0.12842602330083883, 0.02813672474762307, 0.025468783691831972, 0.024312466082363565, -0.13106746603793737, 0.08757073166957006, 0.43052581980635846, -0.21886481495745055, -0.28884419904951053, 0.001745745473352697, -0.3490426228676416, -0.0774781080375461, 0.13460172923234634, 0.0347628043316116... |
710.2335 | A template bank for gravitational waveforms from coalescing binary black
holes: non-spinning binaries | Gravitational waveforms from the inspiral and ring-down stages of the binary
black hole coalescences can be modelled accurately by
approximation/perturbation techniques in general relativity. Recent progress in
numerical relativity has enabled us to model also the non-perturbative merger
phase of the binary black-hol... | gr-qc astro-ph | gravitational waveforms from the inspiral and ringdown stages of the binary black hole coalescences can be modelled accurately by approximationperturbation techniques in general relativity recent progress in numerical relativity has enabled us to model also the nonperturbative merger phase of the binary blackhole coale... | [['gravitational', 'waveforms', 'from', 'the', 'inspiral', 'and', 'ringdown', 'stages', 'of', 'the', 'binary', 'black', 'hole', 'coalescences', 'can', 'be', 'modelled', 'accurately', 'by', 'approximationperturbation', 'techniques', 'in', 'general', 'relativity', 'recent', 'progress', 'in', 'numerical', 'relativity', 'h... | [-0.10703420963872733, 0.07485097480449612, -0.08556223740095543, 0.08111551679703632, -0.09953745061096772, -0.09654340507782634, 0.010044858285271059, 0.3305542536042959, -0.1452787552656614, -0.3224980303882273, 0.07353960451391005, -0.27966902838273194, -0.1336799151959546, 0.2655363716708193, -0.002848880609604099... |
710.2336 | Constraints on mSUGRA through entropy and abundance criteria | We derive an expression for the entropy of a present dark matter halo
described by a Navarro-Frenk-White modified model with a central core. The
comparison of this entropy with the one of the halo at the freeze-out era
allows us to obtain an expression for the relic abundance of neutralinos, which
in turn is used to ... | astro-ph | we derive an expression for the entropy of a present dark matter halo described by a navarrofrenkwhite modified model with a central core the comparison of this entropy with the one of the halo at the freezeout era allows us to obtain an expression for the relic abundance of neutralinos which in turn is used to constra... | [['we', 'derive', 'an', 'expression', 'for', 'the', 'entropy', 'of', 'a', 'present', 'dark', 'matter', 'halo', 'described', 'by', 'a', 'navarrofrenkwhite', 'modified', 'model', 'with', 'a', 'central', 'core', 'the', 'comparison', 'of', 'this', 'entropy', 'with', 'the', 'one', 'of', 'the', 'halo', 'at', 'the', 'freezeou... | [-0.04831723078128932, 0.13505863557269235, -0.07697204616015588, 0.13089084831027392, -0.07366539219054143, -0.15232954452561584, 0.07335624790438144, 0.30905786121520634, -0.16146859317365475, -0.36290225088819417, 0.06283867732945182, -0.257296290208375, -0.0031662248298079667, 0.21478280412384537, 0.008239452994824... |
710.2337 | Instanton representation of Plebanski gravity. Euclidean signature
minisuperspace solution | Using the action for the instanton representation of Plebanski gravity
(IRPG), we construct minisuperspace solutions restricted to diagonal variables.
We have treated the Euclidean signature case with zero cosmological constant,
depicting a gravitational analogy to free particle motion. This paper provides
a testing ... | gr-qc | using the action for the instanton representation of plebanski gravity irpg we construct minisuperspace solutions restricted to diagonal variables we have treated the euclidean signature case with zero cosmological constant depicting a gravitational analogy to free particle motion this paper provides a testing ground f... | [['using', 'the', 'action', 'for', 'the', 'instanton', 'representation', 'of', 'plebanski', 'gravity', 'irpg', 'we', 'construct', 'minisuperspace', 'solutions', 'restricted', 'to', 'diagonal', 'variables', 'we', 'have', 'treated', 'the', 'euclidean', 'signature', 'case', 'with', 'zero', 'cosmological', 'constant', 'dep... | [-0.12911946238619426, 0.10381380198222975, -0.11890540143565065, 0.10731190129656405, -0.14148687701972743, -0.1479028893048845, -0.015141334001635831, 0.3011693138809454, -0.22419653303410497, -0.2361706984604919, 0.06747142134437097, -0.23553457014044868, -0.16158001109837525, 0.1258563180247532, -0.0589067681857775... |
710.2338 | Constraining Cosmic Evolution of Type Ia Supernovae | We present the first large-scale effort of creating composite spectra of
high-redshift type Ia supernovae (SNe Ia) and comparing them to low-redshift
counterparts. Through the ESSENCE project, we have obtained 107 spectra of 88
high-redshift SNe Ia with excellent light-curve information. In addition, we
have obtained... | astro-ph | we present the first largescale effort of creating composite spectra of highredshift type ia supernovae sne ia and comparing them to lowredshift counterparts through the essence project we have obtained 107 spectra of 88 highredshift sne ia with excellent lightcurve information in addition we have obtained 397 spectra ... | [['we', 'present', 'the', 'first', 'largescale', 'effort', 'of', 'creating', 'composite', 'spectra', 'of', 'highredshift', 'type', 'ia', 'supernovae', 'sne', 'ia', 'and', 'comparing', 'them', 'to', 'lowredshift', 'counterparts', 'through', 'the', 'essence', 'project', 'we', 'have', 'obtained', '107', 'spectra', 'of', '... | [0.018978445801200432, 0.06681458072497283, -0.07424617291012452, 0.11140128188115013, -0.09125369124598162, -0.1051577326138164, 0.058824447821026325, 0.4613224047768507, -0.14824895629491416, -0.35932774844183685, 0.041000613249746416, -0.36754644992282914, -0.015993700547107845, 0.21118588092519058, -0.0362555226920... |
710.2339 | Recombination of H3+ Ions in the Afterglow of a He-Ar-H2 Plasma | Recombination of H3+ with electrons was studied in a low temperature plasma
in helium. The plasma recombination rate is driven by two body, H3+ + e, and
three-body, H3+ + e + He, processes with the rate coefficients 7.5x10^{-8}cm3/s
and 2.8x10^{-25}cm6/s correspondingly at 260K. The two-body rate coefficient is
in ex... | physics.atom-ph physics.plasm-ph | recombination of h3 with electrons was studied in a low temperature plasma in helium the plasma recombination rate is driven by two body h3 e and threebody h3 e he processes with the rate coefficients 75x108cm3s and 28x1025cm6s correspondingly at 260k the twobody rate coefficient is in excellent agreement with results ... | [['recombination', 'of', 'h3', 'with', 'electrons', 'was', 'studied', 'in', 'a', 'low', 'temperature', 'plasma', 'in', 'helium', 'the', 'plasma', 'recombination', 'rate', 'is', 'driven', 'by', 'two', 'body', 'h3', 'e', 'and', 'threebody', 'h3', 'e', 'he', 'processes', 'with', 'the', 'rate', 'coefficients', '75x108cm3s'... | [-0.1090530621189497, 0.21229509853864412, 0.03383279062109068, 0.0001893314845140346, 0.10734074447166429, -0.14984937259842726, 0.020451132324524224, 0.39145753500898456, -0.19587114183443852, -0.26615402972410346, -0.025148552835823713, -0.32775287571447814, 0.030024850166889584, 0.16434292227760042, 0.0692774858643... |
710.234 | On ground fields of arithmetic hyperbolic reflection groups. III | This paper continues arXiv.org:math.AG/0609256, arXiv:0708.3991 and
arXiv:0710.0162 .
Using authors's methods of 1980, 1981, some explicit finite sets of number
fields containing all ground fields of arithmetic hyperbolic reflection groups
in dimension at least 3 are defined, and explicit bounds of their degrees (o... | math.AG math.GT | this paper continues arxivorgmathag0609256 arxiv07083991 and arxiv07100162 using authorss methods of 1980 1981 some explicit finite sets of number fields containing all ground fields of arithmetic hyperbolic reflection groups in dimension at least 3 are defined and explicit bounds of their degrees over q are obtained t... | [['this', 'paper', 'continues', 'arxivorgmathag0609256', 'arxiv07083991', 'and', 'arxiv07100162', 'using', 'authorss', 'methods', 'of', '1980', '1981', 'some', 'explicit', 'finite', 'sets', 'of', 'number', 'fields', 'containing', 'all', 'ground', 'fields', 'of', 'arithmetic', 'hyperbolic', 'reflection', 'groups', 'in',... | [-0.19176837448712167, 0.17325370771265247, -0.060657049887018595, 0.07368406657947273, -0.06976351137670529, -0.11482539336855818, 0.04484210919912496, 0.35306794199774544, -0.22162663452781556, -0.3136295794293557, 0.13575755741742507, -0.24546342447013936, -0.1096361603917236, 0.2493746064762335, -0.0995542208732264... |
710.2341 | Extended Higgs Models and a Transition to Exact Susy | String landscape ideas and the observation of a positive vacuum energy in the
current universe suggest that there could be a future transition to an exactly
supersymmetric world. Atomic and molecular binding in this susy background
probably require that electroweak symmetry breaking survives the transition.
Among sev... | hep-ph | string landscape ideas and the observation of a positive vacuum energy in the current universe suggest that there could be a future transition to an exactly supersymmetric world atomic and molecular binding in this susy background probably require that electroweak symmetry breaking survives the transition among several... | [['string', 'landscape', 'ideas', 'and', 'the', 'observation', 'of', 'a', 'positive', 'vacuum', 'energy', 'in', 'the', 'current', 'universe', 'suggest', 'that', 'there', 'could', 'be', 'a', 'future', 'transition', 'to', 'an', 'exactly', 'supersymmetric', 'world', 'atomic', 'and', 'molecular', 'binding', 'in', 'this', '... | [-0.11944094351069494, 0.22067631591281414, -0.0914975942895663, 0.15592715543012178, -0.08363815365274521, -0.1553833430939862, -0.010159245628694242, 0.3554785613986579, -0.2163095265118913, -0.26592984760645777, 0.07004375462367368, -0.2518369099019434, -0.09381991363294549, 0.12977945182303136, 0.02279164124576544,... |
710.2342 | Theory of input spike auto- and cross-correlations and their effect on
the response of spiking neurons | Spike correlations between neurons are ubiquitous in the cortex, but their
role is at present not understood. Here we describe the firing response of a
leaky integrate-and-fire neuron (LIF) when it receives a temporarily correlated
input generated by presynaptic correlated neuronal populations. Input
correlations are... | q-bio.NC physics.bio-ph | spike correlations between neurons are ubiquitous in the cortex but their role is at present not understood here we describe the firing response of a leaky integrateandfire neuron lif when it receives a temporarily correlated input generated by presynaptic correlated neuronal populations input correlations are characte... | [['spike', 'correlations', 'between', 'neurons', 'are', 'ubiquitous', 'in', 'the', 'cortex', 'but', 'their', 'role', 'is', 'at', 'present', 'not', 'understood', 'here', 'we', 'describe', 'the', 'firing', 'response', 'of', 'a', 'leaky', 'integrateandfire', 'neuron', 'lif', 'when', 'it', 'receives', 'a', 'temporarily', '... | [-0.13324799715740226, 0.19212630345911078, 0.0068638278035790595, 0.12647468130309736, 0.017928071342661833, -0.17971751065834343, 0.019859008472955342, 0.4535276183442583, -0.28935762360981365, -0.23259030505833986, 0.02706190770677318, -0.2786826780970091, -0.2905577583672497, 0.1523972755355661, -0.0615791027135785... |
710.2343 | The radio properties of optically obscured Spitzer sources | This paper analyses the radio properties of a subsample of optically obscured
(R>25.5) galaxies observed at 24um by the Spitzer Space Telescope within the
First Look Survey. 96 F[24um]>0.35 mJy objects out of 510 are found to have a
radio counterpart at 1.4 GHz, 610 MHz or at both frequencies respectively down
to ~40... | astro-ph | this paper analyses the radio properties of a subsample of optically obscured r255 galaxies observed at 24um by the spitzer space telescope within the first look survey 96 f24um035 mjy objects out of 510 are found to have a radio counterpart at 14 ghz 610 mhz or at both frequencies respectively down to 40ujy and 200ujy... | [['this', 'paper', 'analyses', 'the', 'radio', 'properties', 'of', 'a', 'subsample', 'of', 'optically', 'obscured', 'r255', 'galaxies', 'observed', 'at', '24um', 'by', 'the', 'spitzer', 'space', 'telescope', 'within', 'the', 'first', 'look', 'survey', '96', 'f24um035', 'mjy', 'objects', 'out', 'of', '510', 'are', 'foun... | [-0.06408776026681236, 0.11303203340531158, -0.02259616085633863, 0.11043716712813924, -0.09181329149944807, -0.08362913987855249, 0.11993794568204712, 0.4805178828537464, -0.09688686464294677, -0.372454916873506, 0.06787885419491417, -0.29918736973445276, -0.029273950901835134, 0.2011711866564192, -0.00276378675573683... |
710.2344 | Measurement of Upsilon Production for p+p and p+d Interactions at 800
GeV | We report a high statistics measurement of Upsilon production with an 800
GeV/c proton beam on hydrogen and deuterium targets. The dominance of the
gluon-gluon fusion process for Upsilon production at this energy implies that
the cross section ratio, $\sigma (p + d \to \Upsilon) / 2\sigma (p + p\to
\Upsilon)$, is sen... | hep-ex | we report a high statistics measurement of upsilon production with an 800 gevc proton beam on hydrogen and deuterium targets the dominance of the gluongluon fusion process for upsilon production at this energy implies that the cross section ratio sigma p d to upsilon 2sigma p pto upsilon is sensitive to the gluon conte... | [['we', 'report', 'a', 'high', 'statistics', 'measurement', 'of', 'upsilon', 'production', 'with', 'an', '800', 'gevc', 'proton', 'beam', 'on', 'hydrogen', 'and', 'deuterium', 'targets', 'the', 'dominance', 'of', 'the', 'gluongluon', 'fusion', 'process', 'for', 'upsilon', 'production', 'at', 'this', 'energy', 'implies'... | [-0.038834032405453224, 0.20190549216474005, -0.10929039878124792, 0.10479852074770186, 0.04093109373559033, -0.07376798889045828, 0.01945140932859372, 0.35377694861662967, -0.19578182271441386, -0.24473545871554844, -0.1056296695925055, -0.35310246507006304, 0.07755073332302873, 0.15371282799770275, 0.0445208987425318... |
710.2345 | Visual Observability of the Cassiopeia A Supernova | It is generally believed that the explosion which gave birth to the
Cassiopeia A supernova remmant resulted from core collapse of a
hydrogen-deficient star. A progenitor that has lost all its hydrogen envelope
and part of its helium envelope would lead to an explosion with the optical
properties of a Type Ic supernov... | astro-ph | it is generally believed that the explosion which gave birth to the cassiopeia a supernova remmant resulted from core collapse of a hydrogendeficient star a progenitor that has lost all its hydrogen envelope and part of its helium envelope would lead to an explosion with the optical properties of a type ic supernova th... | [['it', 'is', 'generally', 'believed', 'that', 'the', 'explosion', 'which', 'gave', 'birth', 'to', 'the', 'cassiopeia', 'a', 'supernova', 'remmant', 'resulted', 'from', 'core', 'collapse', 'of', 'a', 'hydrogendeficient', 'star', 'a', 'progenitor', 'that', 'has', 'lost', 'all', 'its', 'hydrogen', 'envelope', 'and', 'par... | [-0.055463223949237896, 0.1016619514933546, -0.1269413595985159, 0.08199409687684264, -0.11730011771891918, -0.11070188716475438, 0.06940071828948864, 0.3986149097616057, -0.185069277610657, -0.32391198373732777, 0.15072114597564143, -0.27589190028009625, -0.04598758349970092, 0.2139700995146358, -0.05373212605388495, ... |
710.2346 | Hilbert Functions of Filtered Modules | In this presentation we shall deal with some aspects of the theory of Hilbert
functions of modules over local rings, and we intend to guide the reader along
one of the possible routes through the last three decades of progress in this
area of dynamic mathematical activity. Motivated by the ever increasing
interest in... | math.AC math.AG | in this presentation we shall deal with some aspects of the theory of hilbert functions of modules over local rings and we intend to guide the reader along one of the possible routes through the last three decades of progress in this area of dynamic mathematical activity motivated by the ever increasing interest in thi... | [['in', 'this', 'presentation', 'we', 'shall', 'deal', 'with', 'some', 'aspects', 'of', 'the', 'theory', 'of', 'hilbert', 'functions', 'of', 'modules', 'over', 'local', 'rings', 'and', 'we', 'intend', 'to', 'guide', 'the', 'reader', 'along', 'one', 'of', 'the', 'possible', 'routes', 'through', 'the', 'last', 'three', '... | [-0.09304057051587147, 0.06524062435732875, -0.0975714722757429, 0.03383797288901299, -0.08417747116514615, -0.09821755379001736, -9.620139262751563e-05, 0.36131440102030615, -0.3012362244686507, -0.2549055813856068, 0.1277199675501307, -0.25487192140059756, -0.17629101846879688, 0.22154914917067825, -0.126431877793907... |
710.2347 | Ramsey degrees of finite ultrametric spaces, ultrametric Urysohn spaces
and dynamics of their isometry groups | We study Ramsey-theoretic properties of several natural classes of finite
ultrametric spaces, describe the corresponding Urysohn spaces and compute a
dynamical invariant attached to their isometry groups.
| math.CO math.LO | we study ramseytheoretic properties of several natural classes of finite ultrametric spaces describe the corresponding urysohn spaces and compute a dynamical invariant attached to their isometry groups | [['we', 'study', 'ramseytheoretic', 'properties', 'of', 'several', 'natural', 'classes', 'of', 'finite', 'ultrametric', 'spaces', 'describe', 'the', 'corresponding', 'urysohn', 'spaces', 'and', 'compute', 'a', 'dynamical', 'invariant', 'attached', 'to', 'their', 'isometry', 'groups']] | [-0.14325157759918106, 0.14642180538201635, -0.15421845884648738, 0.2241648224837802, -0.11899514432513604, -0.04717603236592064, -0.018681014439573995, 0.3959967044216615, -0.3810887179440922, -0.19575866008246387, 0.14541470381879695, -0.2500817745372101, -0.15673336392716952, 0.17445272452163477, -0.1381492432965724... |
710.2348 | Memory Effects in Spin Chain Channels for Information Transmission | We investigate the multiple use of a ferromagnetic spin chain for quantum and
classical communications without resetting. We find that the memory of the
state transmitted during the first use makes the spin chain a qualitatively
different quantum channel during the second transmission, for which we find the
relevant ... | quant-ph | we investigate the multiple use of a ferromagnetic spin chain for quantum and classical communications without resetting we find that the memory of the state transmitted during the first use makes the spin chain a qualitatively different quantum channel during the second transmission for which we find the relevant krau... | [['we', 'investigate', 'the', 'multiple', 'use', 'of', 'a', 'ferromagnetic', 'spin', 'chain', 'for', 'quantum', 'and', 'classical', 'communications', 'without', 'resetting', 'we', 'find', 'that', 'the', 'memory', 'of', 'the', 'state', 'transmitted', 'during', 'the', 'first', 'use', 'makes', 'the', 'spin', 'chain', 'a',... | [-0.15885416941474315, 0.150775892238902, -0.0320544758244701, 0.04950203568796101, -0.028310682667095376, -0.1633048329623821, 0.10978633459535954, 0.3622133680173884, -0.30887301234204484, -0.25866146199405193, 0.11083158273249864, -0.22694855043474768, -0.12817349103886796, 0.19352201886637055, -0.0485189319304798, ... |
710.2349 | 2D Multipartite Valence Bond States in Quantum Antiferromagnets | A quantum anti-ferromagnetic spin-1 model is characterised on a 2D lattice
with the following requirements: i) The Hamiltonian is made out of nearest
neighbour interactions. ii) It is homogeneous, translational and rotational
invariant. iii) The ground state is a real singlet state of SU(2) (non-chiral).
iv) It has a... | cond-mat.str-el cond-mat.stat-mech hep-th quant-ph | a quantum antiferromagnetic spin1 model is characterised on a 2d lattice with the following requirements i the hamiltonian is made out of nearest neighbour interactions ii it is homogeneous translational and rotational invariant iii the ground state is a real singlet state of su2 nonchiral iv it has a local spin1 repre... | [['a', 'quantum', 'antiferromagnetic', 'spin1', 'model', 'is', 'characterised', 'on', 'a', '2d', 'lattice', 'with', 'the', 'following', 'requirements', 'i', 'the', 'hamiltonian', 'is', 'made', 'out', 'of', 'nearest', 'neighbour', 'interactions', 'ii', 'it', 'is', 'homogeneous', 'translational', 'and', 'rotational', 'in... | [-0.1487680994797238, 0.19611033721458773, -0.02541711100520631, 0.08641430522385594, -0.060385996846720406, -0.2247470376449962, 0.0058571421839080234, 0.3827459145294026, -0.249573947823888, -0.21918610312304523, 0.06686250269304701, -0.3062007382057261, -0.13017641744836297, 0.0832618418701946, 0.0693899326021025, 0... |
710.235 | A Search for Prompt Very High Energy Emission from Satellite-detected
Gamma-ray Bursts using Milagro | Gamma-ray bursts (GRBs) have been detected up to GeV energies and are
predicted by many models to emit in the very high energy (VHE, > 100 GeV)
regime too. Detection of such emission would allow us to constrain GRB models.
Since its launch, in late 2004, the Swift satellite has been locating GRBs at a
rate of approxi... | astro-ph | gammaray bursts grbs have been detected up to gev energies and are predicted by many models to emit in the very high energy vhe 100 gev regime too detection of such emission would allow us to constrain grb models since its launch in late 2004 the swift satellite has been locating grbs at a rate of approximately 100 per... | [['gammaray', 'bursts', 'grbs', 'have', 'been', 'detected', 'up', 'to', 'gev', 'energies', 'and', 'are', 'predicted', 'by', 'many', 'models', 'to', 'emit', 'in', 'the', 'very', 'high', 'energy', 'vhe', '100', 'gev', 'regime', 'too', 'detection', 'of', 'such', 'emission', 'would', 'allow', 'us', 'to', 'constrain', 'grb'... | [-0.05174706634244616, 0.18735985451913828, -0.018538485104270155, 0.16750262238608163, -0.10378747598876834, -0.10039023277948106, 0.042157740926619766, 0.46534641903913554, -0.17778253540469532, -0.4330587698843892, 0.07323814858227198, -0.35518189737125816, 0.0176914542778161, 0.3003185192063222, -0.0066064885900714... |
710.2351 | The Red-Sequence Luminosity Function in Galaxy Clusters since z~1 | We use a statistical sample of ~500 rich clusters taken from 72 square
degrees of the Red-Sequence Cluster Survey (RCS-1) to study the evolution of
~30,000 red-sequence galaxies in clusters over the redshift range 0.35<z<0.95.
We construct red-sequence luminosity functions (RSLFs) for a well-defined,
homogeneously se... | astro-ph | we use a statistical sample of 500 rich clusters taken from 72 square degrees of the redsequence cluster survey rcs1 to study the evolution of 30000 redsequence galaxies in clusters over the redshift range 035z095 we construct redsequence luminosity functions rslfs for a welldefined homogeneously selected richness limi... | [['we', 'use', 'a', 'statistical', 'sample', 'of', '500', 'rich', 'clusters', 'taken', 'from', '72', 'square', 'degrees', 'of', 'the', 'redsequence', 'cluster', 'survey', 'rcs1', 'to', 'study', 'the', 'evolution', 'of', '30000', 'redsequence', 'galaxies', 'in', 'clusters', 'over', 'the', 'redshift', 'range', '035z095',... | [-0.03838696437613929, 0.1216760260507757, -0.08284482332885641, 0.1330753458928828, -0.10793107156759175, -0.009072204525465099, 0.06675609820933245, 0.47324690218827054, -0.05355981196141841, -0.35051603041620566, 0.005512902378143759, -0.30273001526771975, -0.029657184339065824, 0.1805643896884455, -0.05599347599696... |
710.2352 | Big Ramsey degrees and divisibility in classes of ultrametric spaces | Given a countable set S of positive reals, we study finite-dimensional
Ramsey-theoretic properties of the countable ultrametric Urysohn space with
distances in S.
| math.CO math.LO | given a countable set s of positive reals we study finitedimensional ramseytheoretic properties of the countable ultrametric urysohn space with distances in s | [['given', 'a', 'countable', 'set', 's', 'of', 'positive', 'reals', 'we', 'study', 'finitedimensional', 'ramseytheoretic', 'properties', 'of', 'the', 'countable', 'ultrametric', 'urysohn', 'space', 'with', 'distances', 'in', 's']] | [-0.19691943822671537, 0.17781219756959574, -0.047665920918402466, 0.09954264083796222, -0.14651464290269042, -0.06771459857649777, 0.1294544303546781, 0.35859309333255107, -0.3946499108620312, -0.08184251642745474, 0.04328264649856188, -0.31530566136960103, -0.038864384850730065, 0.14384138576544658, -0.08555773220470... |
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