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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709.4535 | Prospects of a Search for a New Massless Neutral Gauge Boson at the ILC | Prospects to search for a new massless neutral gauge boson, the paraphoton,
in e+ e- collisions at center-of-mass energies of 0.5 and 1 TeV are studied.
The paraphoton naturally appears in models with abelian kinetic mixing. A
possible realistic model independent lowest order effective Lagrangian contains
magnetic in... | hep-ph | prospects to search for a new massless neutral gauge boson the paraphoton in e e collisions at centerofmass energies of 05 and 1 tev are studied the paraphoton naturally appears in models with abelian kinetic mixing a possible realistic model independent lowest order effective lagrangian contains magnetic interactions ... | [['prospects', 'to', 'search', 'for', 'a', 'new', 'massless', 'neutral', 'gauge', 'boson', 'the', 'paraphoton', 'in', 'e', 'e', 'collisions', 'at', 'centerofmass', 'energies', 'of', '05', 'and', '1', 'tev', 'are', 'studied', 'the', 'paraphoton', 'naturally', 'appears', 'in', 'models', 'with', 'abelian', 'kinetic', 'mix... | [-0.11913116517259026, 0.25380524046614755, -0.04149358803119099, 0.16566945562581994, -0.08335686924522621, -0.1627807485562592, 0.009033380959231358, 0.33513623793071207, -0.21885522582277947, -0.3670212863944471, 0.01259204589341489, -0.3143754100681029, 0.01947500966731217, 0.13396389896651828, 0.08972761962054805,... |
709.4536 | Approximately Independent Features of Languages | To facilitate the testing of models for the evolution of languages, the
present note offers a set of linguistic features that are approximately
independent of each other. To find these features, the adjusted Rand index R'
is used to estimate the degree of pairwise relationship among 130 linguistic
features in a large... | physics.soc-ph | to facilitate the testing of models for the evolution of languages the present note offers a set of linguistic features that are approximately independent of each other to find these features the adjusted rand index r is used to estimate the degree of pairwise relationship among 130 linguistic features in a large publi... | [['to', 'facilitate', 'the', 'testing', 'of', 'models', 'for', 'the', 'evolution', 'of', 'languages', 'the', 'present', 'note', 'offers', 'a', 'set', 'of', 'linguistic', 'features', 'that', 'are', 'approximately', 'independent', 'of', 'each', 'other', 'to', 'find', 'these', 'features', 'the', 'adjusted', 'rand', 'index... | [-0.07914975564750476, 0.047206236344833875, -0.09449091618363228, 0.04504094018149331, -0.05582469082766711, -0.1499281264982666, 0.04420465052908644, 0.3587132528273746, -0.26948181039305646, -0.36556182993632375, 0.06916221320121126, -0.3268035773300763, -0.07818814548440371, 0.2071004734572136, -0.03761187965294929... |
709.4537 | On Polar Legendre Polynomials | We introduce a new class of polynomials $\{P_{n}\}$, that we call polar
Legendre polynomials, they appear as solutions of an inverse Gauss problem of
equilibrium position of a field of forces with $n+1$ unit masses. We study
algebraic, differential and asymptotic properties of this class of polynomials,
that are simu... | math.CA math.AP | we introduce a new class of polynomials p_n that we call polar legendre polynomials they appear as solutions of an inverse gauss problem of equilibrium position of a field of forces with n1 unit masses we study algebraic differential and asymptotic properties of this class of polynomials that are simultaneously orthogo... | [['we', 'introduce', 'a', 'new', 'class', 'of', 'polynomials', 'p_n', 'that', 'we', 'call', 'polar', 'legendre', 'polynomials', 'they', 'appear', 'as', 'solutions', 'of', 'an', 'inverse', 'gauss', 'problem', 'of', 'equilibrium', 'position', 'of', 'a', 'field', 'of', 'forces', 'with', 'n1', 'unit', 'masses', 'we', 'stud... | [-0.19854151205800008, 0.08594430114521856, -0.08680615550838411, 0.044718932314935955, -0.11822926315653604, -0.10986605654761661, -0.013192411774070933, 0.35320584881992545, -0.3443867020541802, -0.20224447271630197, 0.11030193968326785, -0.2474097276572138, -0.15930641465820372, 0.1628855592571199, -0.10324508661869... |
709.4538 | Gravitational Collapse in Higher Dimensional Husain Space-Time | We investigate exact solution in higher dimensional Husain model for a null
fluid source with pressure $p$ and density $\rho$ are related by the following
relations (i) $p=k\rho$, (ii) $p=k\rho-\frac{B(v)}{\rho^{\alpha}}$ (variable
modified Chaplygin) and (iii) $p=k\rho^{\alpha}$ (polytropic). We have studied
the nat... | gr-qc | we investigate exact solution in higher dimensional husain model for a null fluid source with pressure p and density rho are related by the following relations i pkrho ii pkrhofracbvrhoalpha variable modified chaplygin and iii pkrhoalpha polytropic we have studied the nature of singularity in gravitational collapse for... | [['we', 'investigate', 'exact', 'solution', 'in', 'higher', 'dimensional', 'husain', 'model', 'for', 'a', 'null', 'fluid', 'source', 'with', 'pressure', 'p', 'and', 'density', 'rho', 'are', 'related', 'by', 'the', 'following', 'relations', 'i', 'pkrho', 'ii', 'pkrhofracbvrhoalpha', 'variable', 'modified', 'chaplygin', ... | [-0.1328046398259052, 0.11256691455146518, -0.08156484170516921, 0.042196582954463754, -0.07769528674593164, -0.24414124900782955, -0.026815654007496977, 0.2930421752468446, -0.2308184366310173, -0.282622223909376, 0.04628872851371544, -0.2365698040052617, -0.07575008243724893, 0.10827062038460084, 0.005491946721291643... |
709.4539 | Distributed Quantum Computation Based-on Small Quantum Registers | We describe and analyze an efficient register-based hybrid quantum
computation scheme. Our scheme is based on probabilistic, heralded optical
connection among local five-qubit quantum registers. We assume high fidelity
local unitary operations within each register, but the error probability for
initialization, measur... | quant-ph | we describe and analyze an efficient registerbased hybrid quantum computation scheme our scheme is based on probabilistic heralded optical connection among local fivequbit quantum registers we assume high fidelity local unitary operations within each register but the error probability for initialization measurement and... | [['we', 'describe', 'and', 'analyze', 'an', 'efficient', 'registerbased', 'hybrid', 'quantum', 'computation', 'scheme', 'our', 'scheme', 'is', 'based', 'on', 'probabilistic', 'heralded', 'optical', 'connection', 'among', 'local', 'fivequbit', 'quantum', 'registers', 'we', 'assume', 'high', 'fidelity', 'local', 'unitary... | [-0.14549331212244024, 0.13430712696563887, -0.03624926075323167, 0.029105261202826402, 0.02251420659955182, -0.26313770118820873, 0.14274754432821377, 0.4514020103422893, -0.25060091397133377, -0.30571224060275654, 0.07347801702858804, -0.18033175547257324, -0.09750385987579101, 0.21944471558211426, -0.101720143004752... |
709.454 | Factorized domain wall partition functions in trigonometric vertex
models | We obtain factorized domain wall partition functions for two sets of
trigonometric vertex models: 1. The N-state Deguchi-Akutsu models, for N = {2,
3, 4} (and conjecture the result for all N >= 5), and 2. The sl(r+1|s+1)
Perk-Schultz models, for {r, s = \N}, where (given the symmetries of these
models) the result is ... | math-ph hep-th math.MP | we obtain factorized domain wall partition functions for two sets of trigonometric vertex models 1 the nstate deguchiakutsu models for n 2 3 4 and conjecture the result for all n 5 and 2 the slr1s1 perkschultz models for r s n where given the symmetries of these models the result is independent of r s | [['we', 'obtain', 'factorized', 'domain', 'wall', 'partition', 'functions', 'for', 'two', 'sets', 'of', 'trigonometric', 'vertex', 'models', '1', 'the', 'nstate', 'deguchiakutsu', 'models', 'for', 'n', '2', '3', '4', 'and', 'conjecture', 'the', 'result', 'for', 'all', 'n', '5', 'and', '2', 'the', 'slr1s1', 'perkschultz... | [-0.1469409768384966, 0.1218480455223471, -0.0028737005015665833, 0.04775187619750134, 0.049287718856199224, -0.2255753749304197, 0.012187367677688599, 0.3059977288273248, -0.24664255897091195, -0.3103068277155134, 0.10313178528608247, -0.29857938878492196, -0.07163818440061401, 0.13725157380527395, 0.04825693609362298... |
709.4541 | Quasi-Spherical Gravitational Collapse in higher dimension and the
effect of equation of state | Gravitational collapse in (n+2) dimensional quasi-spherical space-time is
studied for a fluid with non vanishing radial pressure. An exact analytic
solution is obtained (ignoring the arbitrary integration function) for the
equation of state $p_{r}=(\gamma-1)\rho.$ The singularity is studied locally by
comparing the t... | gr-qc | gravitational collapse in n2 dimensional quasispherical spacetime is studied for a fluid with non vanishing radial pressure an exact analytic solution is obtained ignoring the arbitrary integration function for the equation of state p_rgamma1rho the singularity is studied locally by comparing the time of formation of a... | [['gravitational', 'collapse', 'in', 'n2', 'dimensional', 'quasispherical', 'spacetime', 'is', 'studied', 'for', 'a', 'fluid', 'with', 'non', 'vanishing', 'radial', 'pressure', 'an', 'exact', 'analytic', 'solution', 'is', 'obtained', 'ignoring', 'the', 'arbitrary', 'integration', 'function', 'for', 'the', 'equation', '... | [-0.17561383772235695, 0.11412623142814932, -0.10087862863472782, 0.04713371646069543, -0.03381976543805829, -0.136925502634137, -0.04988583287980297, 0.27209739859151366, -0.1967139715642327, -0.22966701000707573, 0.12199221679475158, -0.25944359104453335, -0.03727132347089672, 0.10731143259102165, 0.04677720828959257... |
709.4542 | Real-time observation of polyelectrolyte-induced binding of charged
bilayers | We present real-time observations by confocal microscopy of the dynamic
behavior of multilamellar vesicles (MLVs), composed of charged synthetic
lipids, when put in contact with oppositely charged polyelectrolyte (PE)
molecules. We find that the MLVs exhibit astonishing morphological transitions,
which result from th... | cond-mat.soft | we present realtime observations by confocal microscopy of the dynamic behavior of multilamellar vesicles mlvs composed of charged synthetic lipids when put in contact with oppositely charged polyelectrolyte pe molecules we find that the mlvs exhibit astonishing morphological transitions which result from the discrete ... | [['we', 'present', 'realtime', 'observations', 'by', 'confocal', 'microscopy', 'of', 'the', 'dynamic', 'behavior', 'of', 'multilamellar', 'vesicles', 'mlvs', 'composed', 'of', 'charged', 'synthetic', 'lipids', 'when', 'put', 'in', 'contact', 'with', 'oppositely', 'charged', 'polyelectrolyte', 'pe', 'molecules', 'we', '... | [-0.09602178006051955, 0.2138832411305471, -0.04850037588991902, -0.012798361073840749, 0.02097339623353698, -0.17466074874709275, -0.002175883277298205, 0.4052605513144623, -0.22108583549376237, -0.3071341747089966, -0.0173534306073138, -0.31363924326036463, -0.14635536128083582, 0.12926796756854111, -0.00702186729441... |
709.4543 | Piecewise linear density estimation for sampled data | Nonparametric density estimation is considered for a discretely observed
stationary continuous-time process. For each of three given time sampling
procedures either random or deterministic, we establish that histograms and
frequency polygons can reach the same optimal $L_{2}$-rates as in the
independent and identical... | math.ST stat.TH | nonparametric density estimation is considered for a discretely observed stationary continuoustime process for each of three given time sampling procedures either random or deterministic we establish that histograms and frequency polygons can reach the same optimal l_2rates as in the independent and identically distrib... | [['nonparametric', 'density', 'estimation', 'is', 'considered', 'for', 'a', 'discretely', 'observed', 'stationary', 'continuoustime', 'process', 'for', 'each', 'of', 'three', 'given', 'time', 'sampling', 'procedures', 'either', 'random', 'or', 'deterministic', 'we', 'establish', 'that', 'histograms', 'and', 'frequency'... | [-0.12832272530231678, 0.15460680371386484, -0.06919972915989413, 0.04566452412593566, -0.044597118240322024, -0.17567026706307498, 0.11840477346403289, 0.44663302915197023, -0.2843654675828949, -0.25653036365049403, 0.18049081513153153, -0.17848962908741875, -0.05361287433549132, 0.20350381814297552, -0.09020884236661... |
709.4544 | A class of finite simple Bol loops of exponent 2 | In this paper we give an infinite class of finite simple right Bol loops of
exponent 2. The right multiplication group of these loops is an extension of an
elementary Abelian 2-group by $S_5$. The construction uses the description of
the structure of such loops given by M. Aschbacher. These results answer some
questi... | math.GR | in this paper we give an infinite class of finite simple right bol loops of exponent 2 the right multiplication group of these loops is an extension of an elementary abelian 2group by s_5 the construction uses the description of the structure of such loops given by m aschbacher these results answer some questions of m ... | [['in', 'this', 'paper', 'we', 'give', 'an', 'infinite', 'class', 'of', 'finite', 'simple', 'right', 'bol', 'loops', 'of', 'exponent', '2', 'the', 'right', 'multiplication', 'group', 'of', 'these', 'loops', 'is', 'an', 'extension', 'of', 'an', 'elementary', 'abelian', '2group', 'by', 's_5', 'the', 'construction', 'uses... | [-0.1909012378503879, 0.17294174204697924, -0.024174104934852374, 0.06952775880825102, -0.11517156296707853, -0.13039722391649297, 0.01760362046811599, 0.362223335002598, -0.27738306748582736, -0.26565767350819025, 0.10963081036849569, -0.2477355697720716, -0.14303140273713916, 0.20001099089552699, -0.11776596077783197... |
709.4545 | Post common envelope binaries from SDSS. II: Identification of 9 close
binaries with VLT/FORS2 | The Sloan Digital Sky Survey turned out to be very efficient in identifying
white dwarf/main sequence binaries (WDMS). The population of WDMS systems
consists of wide systems whose stellar components evolve like single stars and
- more interesting in the context of close binary evolution - PCEBs. We pursue
a large-sc... | astro-ph | the sloan digital sky survey turned out to be very efficient in identifying white dwarfmain sequence binaries wdms the population of wdms systems consists of wide systems whose stellar components evolve like single stars and more interesting in the context of close binary evolution pcebs we pursue a largescale followup... | [['the', 'sloan', 'digital', 'sky', 'survey', 'turned', 'out', 'to', 'be', 'very', 'efficient', 'in', 'identifying', 'white', 'dwarfmain', 'sequence', 'binaries', 'wdms', 'the', 'population', 'of', 'wdms', 'systems', 'consists', 'of', 'wide', 'systems', 'whose', 'stellar', 'components', 'evolve', 'like', 'single', 'sta... | [-0.08997819419703197, 0.07570281407603895, -0.07460977149352374, 0.09953847054733347, -0.11470115871012268, -0.08530618401443343, 0.12048110669080651, 0.40692395526020014, -0.15331561433674346, -0.39028605646702624, 0.049892476164888705, -0.33029644810432435, -0.06765138617301722, 0.23481527782038195, -0.0535762143971... |
709.4546 | On harmonic quasiconformal quasi-isometries | The purpose of this paper is to explore conditions which guarantee
Lipschitz-continuity of harmonic maps w.r.t. quasihyperbolic metrics. For
instance, we prove that harmonic quasiconformal maps are Lipschitz w.r.t.
quasihyperbolic metrics.
| math.CV math.CA | the purpose of this paper is to explore conditions which guarantee lipschitzcontinuity of harmonic maps wrt quasihyperbolic metrics for instance we prove that harmonic quasiconformal maps are lipschitz wrt quasihyperbolic metrics | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'explore', 'conditions', 'which', 'guarantee', 'lipschitzcontinuity', 'of', 'harmonic', 'maps', 'wrt', 'quasihyperbolic', 'metrics', 'for', 'instance', 'we', 'prove', 'that', 'harmonic', 'quasiconformal', 'maps', 'are', 'lipschitz', 'wrt', 'quasihyperbolic', 'metri... | [-0.1537789471462489, -0.012446549540806201, -0.050680505111813545, 0.11289857904757222, -0.07544440859478087, -0.12340642385665447, -0.06920870816740658, 0.46542551404526156, -0.3061648598842083, -0.12522356170079402, 0.1330168479602904, -0.2831590349425472, -0.19820324583880364, 0.20988917350769043, -0.23568884763986... |
709.4547 | Probe into the interior of compact stars | The interior of neutron stars contains nuclear matter at very high density
for numerous subatomic particles compete with each other. Therefore, confirming
the components and properties there is our significant task. Here we summarize
the possible methods especial the way of r-mode instability to probe into the
neutro... | astro-ph | the interior of neutron stars contains nuclear matter at very high density for numerous subatomic particles compete with each other therefore confirming the components and properties there is our significant task here we summarize the possible methods especial the way of rmode instability to probe into the neutron star... | [['the', 'interior', 'of', 'neutron', 'stars', 'contains', 'nuclear', 'matter', 'at', 'very', 'high', 'density', 'for', 'numerous', 'subatomic', 'particles', 'compete', 'with', 'each', 'other', 'therefore', 'confirming', 'the', 'components', 'and', 'properties', 'there', 'is', 'our', 'significant', 'task', 'here', 'we'... | [-0.08441074625230753, 0.17155117445105975, -0.09146768073909557, 0.09713641543550273, -0.15103299801166242, -0.07388306960033683, 0.05624889032198833, 0.340798069572506, -0.19515398663397018, -0.3145500766256681, 0.07754108980118941, -0.31269964529917793, -0.05371192520341048, 0.25993289002933756, -0.03006119857757137... |
709.4548 | Three episodes of jet activity in the FRII radio galaxy B0925+420 | We present Very Large Array images of a "Double-Double Radio Galaxy", a class
of objects in which two pairs of lobes are aligned either side of the nucleus.
In this object, B0925+420, we discover a third pair of lobes, close to the core
and again in alignment with the other lobes. This first-known "Triple-Double"
obj... | astro-ph | we present very large array images of a doubledouble radio galaxy a class of objects in which two pairs of lobes are aligned either side of the nucleus in this object b0925420 we discover a third pair of lobes close to the core and again in alignment with the other lobes this firstknown tripledouble object strongly inc... | [['we', 'present', 'very', 'large', 'array', 'images', 'of', 'a', 'doubledouble', 'radio', 'galaxy', 'a', 'class', 'of', 'objects', 'in', 'which', 'two', 'pairs', 'of', 'lobes', 'are', 'aligned', 'either', 'side', 'of', 'the', 'nucleus', 'in', 'this', 'object', 'b0925420', 'we', 'discover', 'a', 'third', 'pair', 'of', ... | [-0.1365621012685951, 0.10288682567110659, -0.08222962781241175, 0.09072734946221896, -0.0819304443118726, -0.0662197857497521, -0.0033592740689244146, 0.4604500038608624, -0.2410995000765724, -0.2989097116018236, 0.07733042654507218, -0.24378026510547302, -0.07061085800505332, 0.15071435971482164, -0.01595923269114154... |
709.4549 | Higgs mechanism in five-dimensional gauge theories | Lattice simulations of five-dimensional gauge theories on an orbifold
revealed that there is spontaneous symmetry breaking. Some of the
extra-dimensional components of the gauge field play the role of a Higgs field
and some of the four-dimensional components become massive gauge bosons. The
effect is confirmed by com... | hep-lat hep-ph | lattice simulations of fivedimensional gauge theories on an orbifold revealed that there is spontaneous symmetry breaking some of the extradimensional components of the gauge field play the role of a higgs field and some of the fourdimensional components become massive gauge bosons the effect is confirmed by computing ... | [['lattice', 'simulations', 'of', 'fivedimensional', 'gauge', 'theories', 'on', 'an', 'orbifold', 'revealed', 'that', 'there', 'is', 'spontaneous', 'symmetry', 'breaking', 'some', 'of', 'the', 'extradimensional', 'components', 'of', 'the', 'gauge', 'field', 'play', 'the', 'role', 'of', 'a', 'higgs', 'field', 'and', 'so... | [-0.2066432614166003, 0.21436406828378005, -0.0798626734660222, 0.08269172593987045, -0.08567315781345734, -0.12071513701230288, -0.02101235863251182, 0.34339699051701106, -0.15323877832494104, -0.23867233553184913, 0.08707712151898214, -0.2547232879182467, -0.14590779633189624, 0.10721587316634563, 0.02807165091328967... |
709.455 | Strong coupling analysis of QED$_3$ for excitation spectrum broadening
in undoped high-temperature superconductor | Theory of quantum electrodynamics in three spatial-time dimension is applied
to the two-dimensional $S=1/2$ quantum Heisenberg antiferromagnet in order to
investigate a doped hole in high-temperature superconductors. Strong coupling
analysis of the U(1) gauge field interaction is carried out to describe
spectral broa... | cond-mat.str-el | theory of quantum electrodynamics in three spatialtime dimension is applied to the twodimensional s12 quantum heisenberg antiferromagnet in order to investigate a doped hole in hightemperature superconductors strong coupling analysis of the u1 gauge field interaction is carried out to describe spectral broadening obser... | [['theory', 'of', 'quantum', 'electrodynamics', 'in', 'three', 'spatialtime', 'dimension', 'is', 'applied', 'to', 'the', 'twodimensional', 's12', 'quantum', 'heisenberg', 'antiferromagnet', 'in', 'order', 'to', 'investigate', 'a', 'doped', 'hole', 'in', 'hightemperature', 'superconductors', 'strong', 'coupling', 'analy... | [-0.19505031590693092, 0.20746367861998774, -0.03865843875693124, 0.06706694161147696, -0.04065172856657259, -0.13362654700074672, 0.014775826562024457, 0.3702084503152914, -0.21205380123941914, -0.26128572438845593, -0.0061488012168474755, -0.33986367991096095, -0.061810302311195095, 0.11369492131154657, 0.07650688025... |
709.4551 | A Near-Infrared Stellar Spectral Library: III. J-Band Spectra | This paper is the third in the series of papers published on near-infrared
(NIR) stellar spectral library by Ranade et al. (2004 & 2007). The observations
were carried out with 1.2 meter Gurushikhar Infrared Telescope (GIRT), at Mt.
Abu, India using a NICMOS3 HgCdTe $256 \times 256$ NIR array based
spectrometer. In p... | astro-ph | this paper is the third in the series of papers published on nearinfrared nir stellar spectral library by ranade et al 2004 2007 the observations were carried out with 12 meter gurushikhar infrared telescope girt at mt abu india using a nicmos3 hgcdte 256 times 256 nir array based spectrometer in paper i ranade et al 2... | [['this', 'paper', 'is', 'the', 'third', 'in', 'the', 'series', 'of', 'papers', 'published', 'on', 'nearinfrared', 'nir', 'stellar', 'spectral', 'library', 'by', 'ranade', 'et', 'al', '2004', '2007', 'the', 'observations', 'were', 'carried', 'out', 'with', '12', 'meter', 'gurushikhar', 'infrared', 'telescope', 'girt', ... | [-0.005391515890991538, 0.06405408982972398, -0.04616050168420862, -0.018686243973572814, -0.0820482636965905, -0.09967954515087062, 0.06635358229201908, 0.4390158821717373, -0.1205444341502006, -0.4421139332178816, 0.07260640302772557, -0.31400577781821526, -0.015190321732453018, 0.20112944810662958, -0.09549060658955... |
709.4552 | Distributed N-body Simulation on the Grid Using Dedicated Hardware | We present performance measurements of direct gravitational N -body
simulation on the grid, with and without specialized (GRAPE-6) hardware. Our
inter-continental virtual organization consists of three sites, one in Tokyo,
one in Philadelphia and one in Amsterdam. We run simulations with up to 196608
particles for a ... | astro-ph cs.DC | we present performance measurements of direct gravitational n body simulation on the grid with and without specialized grape6 hardware our intercontinental virtual organization consists of three sites one in tokyo one in philadelphia and one in amsterdam we run simulations with up to 196608 particles for a variety of t... | [['we', 'present', 'performance', 'measurements', 'of', 'direct', 'gravitational', 'n', 'body', 'simulation', 'on', 'the', 'grid', 'with', 'and', 'without', 'specialized', 'grape6', 'hardware', 'our', 'intercontinental', 'virtual', 'organization', 'consists', 'of', 'three', 'sites', 'one', 'in', 'tokyo', 'one', 'in', '... | [-0.1377801274050622, 0.06060964522727263, -0.024274595211021096, -0.007812403672720983, -0.013313254977805607, -0.11753214855132264, 0.066795384711269, 0.38563569923814056, -0.2062686169739442, -0.3975093424300717, 0.10575668835471243, -0.27238181609835926, -0.08717485313932777, 0.2648462960865295, -0.0386751040557877... |
709.4553 | Microwave power generated by a spin-torque oscillator in the presence of
noise | An expression for the microwave power generated by a spin-torque oscillator
in the presence of thermal noise is derived. This expression, when used in a
subcritical regime, demonstrates that generated power is determined by the
noise level and provides a simple way to experimentally determine the threshold
current fo... | cond-mat.mtrl-sci | an expression for the microwave power generated by a spintorque oscillator in the presence of thermal noise is derived this expression when used in a subcritical regime demonstrates that generated power is determined by the noise level and provides a simple way to experimentally determine the threshold current for micr... | [['an', 'expression', 'for', 'the', 'microwave', 'power', 'generated', 'by', 'a', 'spintorque', 'oscillator', 'in', 'the', 'presence', 'of', 'thermal', 'noise', 'is', 'derived', 'this', 'expression', 'when', 'used', 'in', 'a', 'subcritical', 'regime', 'demonstrates', 'that', 'generated', 'power', 'is', 'determined', 'b... | [-0.15628876106491613, 0.11458827129347439, -0.024799215319899866, 0.05100150005230795, -0.023833007586223108, -0.10064583783969283, 0.056918577699243654, 0.31545371622031115, -0.24997880922078533, -0.30064722318432213, 0.02395651348216896, -0.22638351375949972, -0.12213023162711366, 0.31006373545545857, -0.01776202960... |
709.4554 | Feshbach resonances in mixtures of ultracold $^6$Li and $^{87}$Rb gases | We report on the observation of two Feshbach resonances in collisions between
ultracold $^6$Li and $^{87}$Rb atoms in their respective hyperfine ground
states $|F,m_F>=|1/2,1/2>$ and $|1,1>$. The resonances show up as trap losses
for the $^6$Li cloud induced by inelastic Li-Rb-Rb three-body collisions. The
magnetic f... | cond-mat.other cond-mat.soft | we report on the observation of two feshbach resonances in collisions between ultracold 6li and 87rb atoms in their respective hyperfine ground states fm_f1212 and 11 the resonances show up as trap losses for the 6li cloud induced by inelastic lirbrb threebody collisions the magnetic field values where they occur repre... | [['we', 'report', 'on', 'the', 'observation', 'of', 'two', 'feshbach', 'resonances', 'in', 'collisions', 'between', 'ultracold', '6li', 'and', '87rb', 'atoms', 'in', 'their', 'respective', 'hyperfine', 'ground', 'states', 'fm_f1212', 'and', '11', 'the', 'resonances', 'show', 'up', 'as', 'trap', 'losses', 'for', 'the', ... | [-0.16937418882811411, 0.24646019052867263, -0.004154105094398876, 0.039292783091860045, 0.07351378431986468, -0.1441564271608215, 0.0773182809562804, 0.384202278417642, -0.18000946098511092, -0.27670058154607896, -0.10871152451918384, -0.3028771088718147, 0.021847897059413927, 0.15154264420347258, 0.12286600457565462,... |
709.4555 | Branching Fractions and Direct CP Asymmetries of Charmless B Decay Modes
at CDF | We present new CDF results on the branching fractions and time-integrated
direct CP asymmetries for $B^0$ and $B^0_s$ decay modes into pairs of charmless
charged hadrons (pions or kaons). The data-set for this update amounts to 1
$\mathrm{fb}^{-1}$ of $p\bar p$ collisions at a center of mass energy 1.96
$\mathrm{TeV}... | hep-ex | we present new cdf results on the branching fractions and timeintegrated direct cp asymmetries for b0 and b0_s decay modes into pairs of charmless charged hadrons pions or kaons the dataset for this update amounts to 1 mathrmfb1 of pbar p collisions at a center of mass energy 196 mathrmtev we report the first observati... | [['we', 'present', 'new', 'cdf', 'results', 'on', 'the', 'branching', 'fractions', 'and', 'timeintegrated', 'direct', 'cp', 'asymmetries', 'for', 'b0', 'and', 'b0_s', 'decay', 'modes', 'into', 'pairs', 'of', 'charmless', 'charged', 'hadrons', 'pions', 'or', 'kaons', 'the', 'dataset', 'for', 'this', 'update', 'amounts',... | [-0.10537509095181873, 0.24717906951074206, -0.09753774201153251, 0.05872226390435927, -0.05838142181069681, -0.07105253908641475, 0.13242575829550016, 0.2596976192992019, -0.21892551955281067, -0.24207609580100878, -0.08026901736055785, -0.42418462316424627, 0.09252851084633933, 0.09591524385715551, 0.1490883053604351... |
709.4556 | Charge-to-spin conversion of electron entanglement states and
spin-interaction-free solid-state quantum computation | Without resorting to spin-spin coupling, we propose a scalable spin quantum
computing scheme assisted with a semiconductor multiple-quantum-dot structure.
The techniques of single electron transitions and the nanostructure of
quantum-dot cellular automata (QCA) are used to generate charge entangled
states of two elec... | cond-mat.mes-hall | without resorting to spinspin coupling we propose a scalable spin quantum computing scheme assisted with a semiconductor multiplequantumdot structure the techniques of single electron transitions and the nanostructure of quantumdot cellular automata qca are used to generate charge entangled states of two electrons whic... | [['without', 'resorting', 'to', 'spinspin', 'coupling', 'we', 'propose', 'a', 'scalable', 'spin', 'quantum', 'computing', 'scheme', 'assisted', 'with', 'a', 'semiconductor', 'multiplequantumdot', 'structure', 'the', 'techniques', 'of', 'single', 'electron', 'transitions', 'and', 'the', 'nanostructure', 'of', 'quantumdo... | [-0.16569429982308914, 0.24846209006980785, -0.02995526503084354, 0.024274591813135207, 0.03220572121366768, -0.3011600149171517, 0.08127012693332238, 0.435018938541123, -0.2729086902476305, -0.2515633302894466, -0.009811954949168688, -0.22767692559751349, -0.08309709636474173, 0.2421303008619732, 0.04520466175038838, ... |
709.4557 | A diffusion Monte Carlo study of small para-Hydrogen clusters | Ground state energies and chemical potentials of parahydrogen clusters are
calculated from 3 to 40 molecules using the diffusion Monte Carlo technique
with two different pH2-pH2 interactions. This calculation improves a previous
one by the inclusion of three-body correlations in the importance sampling, by
the time s... | physics.atm-clus | ground state energies and chemical potentials of parahydrogen clusters are calculated from 3 to 40 molecules using the diffusion monte carlo technique with two different ph2ph2 interactions this calculation improves a previous one by the inclusion of threebody correlations in the importance sampling by the time step ad... | [['ground', 'state', 'energies', 'and', 'chemical', 'potentials', 'of', 'parahydrogen', 'clusters', 'are', 'calculated', 'from', '3', 'to', '40', 'molecules', 'using', 'the', 'diffusion', 'monte', 'carlo', 'technique', 'with', 'two', 'different', 'ph2ph2', 'interactions', 'this', 'calculation', 'improves', 'a', 'previo... | [-0.04372497211367666, 0.1743663142362682, -0.08018765336449875, 0.0853362043400283, 0.045351218305189504, -0.0912271830655465, 0.07684965827199933, 0.41175166159481197, -0.23737832057809868, -0.39201485359581645, 0.04177538126211178, -0.3368787663904103, -0.0336621508286516, 0.1694343358447606, 0.08749356610071543, 0.... |
709.4558 | Practical Multiwriter Lock-Free Queues for "Hard Real-Time" Systems
without CAS | FIFO queues with a single reader and writer can be insufficient for "hard
real-time" systems where interrupt handlers require wait-free guarantees when
writing to message queues. We present an algorithm which elegantly and
practically solves this problem on small processors that are often found in
embedded systems. T... | cs.OS cs.DC | fifo queues with a single reader and writer can be insufficient for hard realtime systems where interrupt handlers require waitfree guarantees when writing to message queues we present an algorithm which elegantly and practically solves this problem on small processors that are often found in embedded systems the algor... | [['fifo', 'queues', 'with', 'a', 'single', 'reader', 'and', 'writer', 'can', 'be', 'insufficient', 'for', 'hard', 'realtime', 'systems', 'where', 'interrupt', 'handlers', 'require', 'waitfree', 'guarantees', 'when', 'writing', 'to', 'message', 'queues', 'we', 'present', 'an', 'algorithm', 'which', 'elegantly', 'and', '... | [-0.1807487784247439, 0.059558697415923234, -0.061675364261164385, 0.06225887879012518, -0.12030420527455635, -0.3069276820055629, 0.09022872843186133, 0.4265911971383235, -0.2626398713784475, -0.33680429947494034, 0.13832444354193285, -0.23208334337344722, -0.10394002205701362, 0.2033558357278725, -0.16448466152445795... |
709.4559 | A model for the orbifold Chow ring of weighted projective spaces | We construct an isomorphism of graded Frobenius algebras between the orbifold
Chow ring of weighted projective spaces and graded algebras of groups of roots
of the unity.
| math.AG | we construct an isomorphism of graded frobenius algebras between the orbifold chow ring of weighted projective spaces and graded algebras of groups of roots of the unity | [['we', 'construct', 'an', 'isomorphism', 'of', 'graded', 'frobenius', 'algebras', 'between', 'the', 'orbifold', 'chow', 'ring', 'of', 'weighted', 'projective', 'spaces', 'and', 'graded', 'algebras', 'of', 'groups', 'of', 'roots', 'of', 'the', 'unity']] | [-0.28636911197531, -0.035816597626695444, -0.09671707958396938, 0.08285324447960765, -0.11949619474924272, -0.13000969823311875, -0.14017389149025636, 0.3302546540896098, -0.5069663963384099, -0.14613198826986332, 0.06900076345644063, -0.20490686516105025, -0.10718951674385203, 0.15192464920174745, -0.2500439733266830... |
709.456 | The distant galaxy cluster CL0016+16: X-ray analysis up to $R_{200}$ | To study the mass distribution of galaxy clusters up to their Virial radius,
CL0016+16 seems to be a good candidate,since it is a bright massive cluster,
previously considered as being dynamically relaxed. Using XMM-Newton
observations of CL0016+16, we performed a careful X-ray background analysis,
and we detected co... | astro-ph | to study the mass distribution of galaxy clusters up to their virial radius cl001616 seems to be a good candidatesince it is a bright massive cluster previously considered as being dynamically relaxed using xmmnewton observations of cl001616 we performed a careful xray background analysis and we detected convincingly i... | [['to', 'study', 'the', 'mass', 'distribution', 'of', 'galaxy', 'clusters', 'up', 'to', 'their', 'virial', 'radius', 'cl001616', 'seems', 'to', 'be', 'a', 'good', 'candidatesince', 'it', 'is', 'a', 'bright', 'massive', 'cluster', 'previously', 'considered', 'as', 'being', 'dynamically', 'relaxed', 'using', 'xmmnewton',... | [-0.05056290791566245, 0.08648755335227841, -0.1324909099797172, 0.08777614792930116, -0.05925894329181972, -0.06577794466885423, 0.05510935014099833, 0.4193906216104784, -0.2142985287494765, -0.36772144383804733, 0.09268358061359502, -0.29455406478921736, -0.05886795246359808, 0.1755433202421, 0.0017070379466576548, 0... |
709.4561 | Semi-Classical Dynamics in Quantum Spin Systems | We consider two limiting regimes, the large-spin and the mean-field limit,
for the dynamical evolution of quantum spin systems. We prove that, in these
limits, the time evolution of a class of quantum spin systems is determined by
a corresponding Hamiltonian dynamics of classical spins. This result can be
viewed as a... | math-ph math.MP | we consider two limiting regimes the largespin and the meanfield limit for the dynamical evolution of quantum spin systems we prove that in these limits the time evolution of a class of quantum spin systems is determined by a corresponding hamiltonian dynamics of classical spins this result can be viewed as a egorovtyp... | [['we', 'consider', 'two', 'limiting', 'regimes', 'the', 'largespin', 'and', 'the', 'meanfield', 'limit', 'for', 'the', 'dynamical', 'evolution', 'of', 'quantum', 'spin', 'systems', 'we', 'prove', 'that', 'in', 'these', 'limits', 'the', 'time', 'evolution', 'of', 'a', 'class', 'of', 'quantum', 'spin', 'systems', 'is', ... | [-0.17187142036422048, 0.1828459517713528, -0.09564700982598372, 0.07756661965923253, 0.046907491965739186, -0.06551905378271544, 0.05762429478534952, 0.3177217779854356, -0.27775343416561915, -0.23257720933923887, 0.11050189677544675, -0.2365454289369112, -0.11293098613684781, 0.21081603975793303, 0.016121034764922982... |
709.4562 | A hydrodynamic scheme for two-component winds from hot stars | We have developed a time-dependent two-component hydrodynamics code to
simulate radiatively-driven stellar winds from hot stars. We use a
time-explicit van Leer scheme to solve the hydrodynamic equations of a
two-component stellar wind. Dynamical friction due to Coulomb collisions
between the passive bulk plasma and ... | astro-ph | we have developed a timedependent twocomponent hydrodynamics code to simulate radiativelydriven stellar winds from hot stars we use a timeexplicit van leer scheme to solve the hydrodynamic equations of a twocomponent stellar wind dynamical friction due to coulomb collisions between the passive bulk plasma and the lines... | [['we', 'have', 'developed', 'a', 'timedependent', 'twocomponent', 'hydrodynamics', 'code', 'to', 'simulate', 'radiativelydriven', 'stellar', 'winds', 'from', 'hot', 'stars', 'we', 'use', 'a', 'timeexplicit', 'van', 'leer', 'scheme', 'to', 'solve', 'the', 'hydrodynamic', 'equations', 'of', 'a', 'twocomponent', 'stellar... | [-0.06519306816065822, 0.08590260626213556, -0.10183399408641788, 0.1067537815402762, -0.07665332297242626, -0.1305840888105902, -0.0008726645534840861, 0.33453889859460845, -0.22202944174339925, -0.30854095509534496, 0.016793126792267517, -0.25743296554450085, -0.06259348197319789, 0.20310838525485317, -0.036903215542... |
709.4563 | Systematic generation of entanglement measures for pure states | We propose a method to generate entanglement measures systematically by using
the irreducible decomposition of some copies of a state under the local unitary
(LU) transformations. It is applicable to general multipartite systems. We show
that there are entanglement monotones corresponding to singlet representations
o... | quant-ph | we propose a method to generate entanglement measures systematically by using the irreducible decomposition of some copies of a state under the local unitary lu transformations it is applicable to general multipartite systems we show that there are entanglement monotones corresponding to singlet representations of the ... | [['we', 'propose', 'a', 'method', 'to', 'generate', 'entanglement', 'measures', 'systematically', 'by', 'using', 'the', 'irreducible', 'decomposition', 'of', 'some', 'copies', 'of', 'a', 'state', 'under', 'the', 'local', 'unitary', 'lu', 'transformations', 'it', 'is', 'applicable', 'to', 'general', 'multipartite', 'sys... | [-0.09045745785973702, 0.13421333345100683, -0.15031246342366994, 0.06719472436728238, -0.016906846008931446, -0.14113018783091597, 0.014366734655329375, 0.3957507215214498, -0.28689801904156503, -0.23643263149065802, 0.06697386130455392, -0.2512671160088344, -0.14845660144481995, 0.2088280412641288, -0.090681579697764... |
709.4564 | Neutral mesons and disconnected diagrams in Twisted Mass QCD | We evaluate properties of neutral mesons in Nf=2 dynamical simulations of
TMQCD at maximal twist. The pion is explored - establishing the size of the
isospin splitting (an order a^2 effect). We investigate the eta' (the Nf=2
flavour singlet pseudoscalar meson) and neutral rho and scalar mesons. We show
that disconnec... | hep-lat | we evaluate properties of neutral mesons in nf2 dynamical simulations of tmqcd at maximal twist the pion is explored establishing the size of the isospin splitting an order a2 effect we investigate the eta the nf2 flavour singlet pseudoscalar meson and neutral rho and scalar mesons we show that disconnected diagrams ca... | [['we', 'evaluate', 'properties', 'of', 'neutral', 'mesons', 'in', 'nf2', 'dynamical', 'simulations', 'of', 'tmqcd', 'at', 'maximal', 'twist', 'the', 'pion', 'is', 'explored', 'establishing', 'the', 'size', 'of', 'the', 'isospin', 'splitting', 'an', 'order', 'a2', 'effect', 'we', 'investigate', 'the', 'eta', 'the', 'nf... | [-0.14481224265370157, 0.30623468018588496, -0.09420467210903523, 0.16948382060171194, 0.00048297690227627754, -0.10995208761361878, 0.060099148602720594, 0.37442979628160117, -0.15802322745683692, -0.1691900598966787, -0.040880163061252285, -0.30406223193952636, -0.05246178801697228, 0.054117413733394876, 0.0990178830... |
709.4565 | Topological Dynamics of 2D Cellular Automata | Topological dynamics of cellular automata (CA), inherited from classical
dynamical systems theory, has been essentially studied in dimension 1. This
paper focuses on 2D CA and aims at showing that the situation is different and
more complex. The main results are the existence of non sensitive CA without
equicontinuou... | cs.DM | topological dynamics of cellular automata ca inherited from classical dynamical systems theory has been essentially studied in dimension 1 this paper focuses on 2d ca and aims at showing that the situation is different and more complex the main results are the existence of non sensitive ca without equicontinuous points... | [['topological', 'dynamics', 'of', 'cellular', 'automata', 'ca', 'inherited', 'from', 'classical', 'dynamical', 'systems', 'theory', 'has', 'been', 'essentially', 'studied', 'in', 'dimension', '1', 'this', 'paper', 'focuses', 'on', '2d', 'ca', 'and', 'aims', 'at', 'showing', 'that', 'the', 'situation', 'is', 'different... | [-0.1244225576017542, 0.10438799442184207, -0.016222560743948348, 0.07242670700346168, -0.01283085582483756, -0.17171600755230573, 0.059254904272721, 0.35074372944471083, -0.27280412930014886, -0.21977734628476595, 0.10497554857651457, -0.2847153312967796, -0.1891650860442927, 0.21081132337843117, -0.07972657805994937,... |
709.4566 | Experimental proton-proton correlation function derived for the pp ->
ppeta reaction | Based on the high statistics data from the pp -> ppX reaction measured by the
COSY-11 collaboration [1] we have derived a two-proton correlation function for
the production of the ppeta and pp+pions systems. The measured correlation
function normalized to the value simulated for a point-like source was compared
with ... | hep-ph | based on the high statistics data from the pp ppx reaction measured by the cosy11 collaboration 1 we have derived a twoproton correlation function for the production of the ppeta and pppions systems the measured correlation function normalized to the value simulated for a pointlike source was compared with a theoretica... | [['based', 'on', 'the', 'high', 'statistics', 'data', 'from', 'the', 'pp', 'ppx', 'reaction', 'measured', 'by', 'the', 'cosy11', 'collaboration', '1', 'we', 'have', 'derived', 'a', 'twoproton', 'correlation', 'function', 'for', 'the', 'production', 'of', 'the', 'ppeta', 'and', 'pppions', 'systems', 'the', 'measured', '... | [-0.022220237492283267, 0.06612206586906987, -0.11577166042820129, 0.11324249535438514, 0.05977105609171333, -0.047022838768879735, 0.03740928017143761, 0.31343847198877484, -0.2044372714214748, -0.3362757072994305, 0.021012617513582472, -0.3918350963222404, -0.015770715418189103, 0.18302789404087008, 0.070485205584836... |
709.4567 | Structural and Nucleosynthetic Evolution of Metal-poor and Metal-free
Low and Intermediate Mass Stars | We report on an investigation into stellar evolution and nucleosynthesis in
the low and extremely low metallicity regime, including models of stars with a
pure Big Bang composition (i.e. Z=0). The metallicity range of the extremely
metal poor (EMP) models we have calculated is -6.5 < [Fe/H] < -3.0, whilst our
models ... | astro-ph | we report on an investigation into stellar evolution and nucleosynthesis in the low and extremely low metallicity regime including models of stars with a pure big bang composition ie z0 the metallicity range of the extremely metal poor emp models we have calculated is 65 feh 30 whilst our models are in the mass range 0... | [['we', 'report', 'on', 'an', 'investigation', 'into', 'stellar', 'evolution', 'and', 'nucleosynthesis', 'in', 'the', 'low', 'and', 'extremely', 'low', 'metallicity', 'regime', 'including', 'models', 'of', 'stars', 'with', 'a', 'pure', 'big', 'bang', 'composition', 'ie', 'z0', 'the', 'metallicity', 'range', 'of', 'the'... | [-0.042638982030249004, 0.15489021458446686, -0.057110037305392325, 0.08844978809708642, -0.027078618690310148, -0.031715892977261725, 0.04892171553901014, 0.40372675611428166, -0.1726011557517169, -0.38591163269742285, 0.0834341101870013, -0.2981088071404559, -0.056769141736043284, 0.19182122637727117, -0.072574307109... |
709.4568 | Gamma-Ray Burst high energy emission from Internal Shocks | In this paper we study synchrotron and synchrotron self Compton (SSC)
emission from internal shocks (IS) during the prompt and X-ray flare phases of
Gamma-Ray Bursts (GRBs). The aim is to test the IS model for the flare emission
and for whether GRBs can be GeV sources. We determine the parameters for which
the IS mod... | astro-ph | in this paper we study synchrotron and synchrotron self compton ssc emission from internal shocks is during the prompt and xray flare phases of gammaray bursts grbs the aim is to test the is model for the flare emission and for whether grbs can be gev sources we determine the parameters for which the is model can accou... | [['in', 'this', 'paper', 'we', 'study', 'synchrotron', 'and', 'synchrotron', 'self', 'compton', 'ssc', 'emission', 'from', 'internal', 'shocks', 'is', 'during', 'the', 'prompt', 'and', 'xray', 'flare', 'phases', 'of', 'gammaray', 'bursts', 'grbs', 'the', 'aim', 'is', 'to', 'test', 'the', 'is', 'model', 'for', 'the', 'f... | [-0.05079779110522384, 0.2089532541684028, -0.05665174611024113, 0.20752391803813022, -0.10325409379041943, -0.05916503143071965, 0.030152919844620346, 0.4804709246345013, -0.17530235432392632, -0.3527218124094564, 0.054485814815175636, -0.30355849140045416, -0.022789495814391283, 0.24223085147452975, -0.00063131802874... |
709.4569 | Diffusion-controlled death of $A$-particle and $B$-particle islands at
propagation of the sharp annihilation front $A + B \to 0$ | We consider the problem of diffusion-controlled evolution of the system
$A$-particle island - $B$-particle island at propagation of the sharp
annihilation front $A+B\to 0$. We show that this general problem, which
includes as particular cases the sea-sea and the island-sea problems,
demonstrates rich dynamical behavi... | cond-mat.stat-mech cond-mat.soft | we consider the problem of diffusioncontrolled evolution of the system aparticle island bparticle island at propagation of the sharp annihilation front abto 0 we show that this general problem which includes as particular cases the seasea and the islandsea problems demonstrates rich dynamical behavior from selfaccelera... | [['we', 'consider', 'the', 'problem', 'of', 'diffusioncontrolled', 'evolution', 'of', 'the', 'system', 'aparticle', 'island', 'bparticle', 'island', 'at', 'propagation', 'of', 'the', 'sharp', 'annihilation', 'front', 'abto', '0', 'we', 'show', 'that', 'this', 'general', 'problem', 'which', 'includes', 'as', 'particular... | [-0.1480010338326371, 0.0882808805625068, -0.10060679834767632, 0.10625300222366094, -0.01590479494259897, -0.07946925689381115, 0.06292492898589955, 0.2700647449847765, -0.2826566269007943, -0.2409985432083287, 0.08409388178800482, -0.2612100457091157, -0.1664418196987088, 0.1992611284481316, 0.030026834963525578, 0.0... |
709.457 | Gamma-Ray Emission from PWNe Interacting with Molecular Clouds | We consider a situation in which a pulsar (and its nebula) is formed inside
or close to a high density regions of a molecular cloud. We apply a recent
model for the gamma radiation of pulsar wind nebulae (PWN), which includes not
only radiation processes due to injected leptons but also processes due to
injection of ... | astro-ph | we consider a situation in which a pulsar and its nebula is formed inside or close to a high density regions of a molecular cloud we apply a recent model for the gamma radiation of pulsar wind nebulae pwn which includes not only radiation processes due to injected leptons but also processes due to injection of relativi... | [['we', 'consider', 'a', 'situation', 'in', 'which', 'a', 'pulsar', 'and', 'its', 'nebula', 'is', 'formed', 'inside', 'or', 'close', 'to', 'a', 'high', 'density', 'regions', 'of', 'a', 'molecular', 'cloud', 'we', 'apply', 'a', 'recent', 'model', 'for', 'the', 'gamma', 'radiation', 'of', 'pulsar', 'wind', 'nebulae', 'pw... | [-0.04607894509631608, 0.20816745822450944, -0.05085590985337538, 0.15908658339176326, -0.07885607029843543, -0.07363644135849816, 0.0016007501618670566, 0.43064910167029924, -0.22706218457913824, -0.34074230714834164, -0.0049287920398637655, -0.3088942845857569, 0.05008760228087859, 0.18524105962498913, 0.037501243004... |
709.4571 | Einstein's Lost Battles and Neglected Achievements | We analyze some of Einstein's failures to accomplish tasks which he posed to
himself, notably deterministic interpretation of Quantum mechanics and
formulation of the Unified theory of physical interactions, putting them into
broader ontological and epistemological context. We highlight, on the other
hand, a number o... | physics.hist-ph | we analyze some of einsteins failures to accomplish tasks which he posed to himself notably deterministic interpretation of quantum mechanics and formulation of the unified theory of physical interactions putting them into broader ontological and epistemological context we highlight on the other hand a number of his co... | [['we', 'analyze', 'some', 'of', 'einsteins', 'failures', 'to', 'accomplish', 'tasks', 'which', 'he', 'posed', 'to', 'himself', 'notably', 'deterministic', 'interpretation', 'of', 'quantum', 'mechanics', 'and', 'formulation', 'of', 'the', 'unified', 'theory', 'of', 'physical', 'interactions', 'putting', 'them', 'into',... | [-0.07856629025583795, 0.09001470340348511, -0.09777174196949408, 0.1212453161918906, -0.16282506854868078, -0.19268178048330437, 0.04406700749371021, 0.3129624341087169, -0.25440179757459697, -0.33159739582473974, 0.07197731881997133, -0.27391898188689523, -0.16872674498303109, 0.15356442009811347, -0.1344827225190553... |
709.4572 | Measurement of Heavy Quark cross-sections at CDF | The measurement of heavy quark cross-sections provides important tests of the
QCD theory. This paper reviews recent measurements of single b-quark and
correlated b-quark cross-sections at CDF. Two new measurements of the single
b-quark production at CDF agree with the first result from CDF Run II. This
clarifies the ... | hep-ex | the measurement of heavy quark crosssections provides important tests of the qcd theory this paper reviews recent measurements of single bquark and correlated bquark crosssections at cdf two new measurements of the single bquark production at cdf agree with the first result from cdf run ii this clarifies the experiment... | [['the', 'measurement', 'of', 'heavy', 'quark', 'crosssections', 'provides', 'important', 'tests', 'of', 'the', 'qcd', 'theory', 'this', 'paper', 'reviews', 'recent', 'measurements', 'of', 'single', 'bquark', 'and', 'correlated', 'bquark', 'crosssections', 'at', 'cdf', 'two', 'new', 'measurements', 'of', 'the', 'single... | [-0.034918638126577674, 0.14792010683895035, -0.09037190465503098, 0.07414123093978703, -0.01717874575315007, -0.1392207758857266, 0.0597937998450909, 0.3009005034086751, -0.1307001758558566, -0.30754646662549645, -0.04665664644847971, -0.39841233292484984, 0.039552219677716494, 0.1559224370227871, 0.006975432885262896... |
709.4573 | Pulsating B and Be stars in the Small Magellanic Cloud | Context: Stellar pulsations in main-sequence B-type stars are driven by the
kappa-mechanism due to the Fe-group opacity bump. The current models do not
predict the presence of instability strips in the B spectral domain at very low
metallicities. As the metallicity of the SMC is lower than Z=0.005, it
constitutes a v... | astro-ph | context stellar pulsations in mainsequence btype stars are driven by the kappamechanism due to the fegroup opacity bump the current models do not predict the presence of instability strips in the b spectral domain at very low metallicities as the metallicity of the smc is lower than z0005 it constitutes a very suitable... | [['context', 'stellar', 'pulsations', 'in', 'mainsequence', 'btype', 'stars', 'are', 'driven', 'by', 'the', 'kappamechanism', 'due', 'to', 'the', 'fegroup', 'opacity', 'bump', 'the', 'current', 'models', 'do', 'not', 'predict', 'the', 'presence', 'of', 'instability', 'strips', 'in', 'the', 'b', 'spectral', 'domain', 'a... | [-0.05178998295751797, 0.1579705639831865, -0.07963149691280628, 0.10303207336749126, -0.15488185392126078, -0.09664602440430203, 0.1172543623186713, 0.39518917798084185, -0.14063507806749076, -0.336458289894842, 0.06381494499265926, -0.31340694913992306, -0.0013159798676802587, 0.2285735827904859, -0.07739396295097208... |
709.4574 | Light quark masses and pseudoscalar decay constants from Nf=2 Lattice
QCD with twisted mass fermions | We present the results of a lattice QCD calculation of the average up-down
and strange quark masses and of the light meson pseudoscalar decay constants
with Nf=2 dynamical fermions. The simulation is carried out at a single value
of the lattice spacing with the twisted mass fermionic action at maximal twist,
which gu... | hep-lat hep-ph | we present the results of a lattice qcd calculation of the average updown and strange quark masses and of the light meson pseudoscalar decay constants with nf2 dynamical fermions the simulation is carried out at a single value of the lattice spacing with the twisted mass fermionic action at maximal twist which guarante... | [['we', 'present', 'the', 'results', 'of', 'a', 'lattice', 'qcd', 'calculation', 'of', 'the', 'average', 'updown', 'and', 'strange', 'quark', 'masses', 'and', 'of', 'the', 'light', 'meson', 'pseudoscalar', 'decay', 'constants', 'with', 'nf2', 'dynamical', 'fermions', 'the', 'simulation', 'is', 'carried', 'out', 'at', '... | [-0.0892899986260153, 0.312442631929599, -0.07017468803658568, 0.06861444563717292, -0.0057150461243321024, -0.12086458410826866, 0.16012759266485427, 0.33174356091125257, -0.13571205997582653, -0.31582775411420855, 0.02347084912230614, -0.3367303920845533, 0.055571044905207534, 0.1454312340549097, 0.09581092493177054,... |
709.4575 | Density profiles in the raise and peel model with and without a wall.
Physics and combinatorics | We consider the raise and peel model of a one-dimensional fluctuating
interface in the presence of an attractive wall. The model can also describe a
pair annihilation process in a disordered unquenched media with a source at one
end of the system. For the stationary states, several density profiles are
studied using ... | cond-mat.stat-mech cond-mat.soft | we consider the raise and peel model of a onedimensional fluctuating interface in the presence of an attractive wall the model can also describe a pair annihilation process in a disordered unquenched media with a source at one end of the system for the stationary states several density profiles are studied using monte ... | [['we', 'consider', 'the', 'raise', 'and', 'peel', 'model', 'of', 'a', 'onedimensional', 'fluctuating', 'interface', 'in', 'the', 'presence', 'of', 'an', 'attractive', 'wall', 'the', 'model', 'can', 'also', 'describe', 'a', 'pair', 'annihilation', 'process', 'in', 'a', 'disordered', 'unquenched', 'media', 'with', 'a', ... | [-0.15493413600898176, 0.10525776516329238, -0.08041958418088378, 0.1019834551499554, -0.04274040017173522, -0.14754802540496545, 0.038639787732002634, 0.38042455022826926, -0.2759176496899238, -0.2794107829634514, 0.12230388242320192, -0.30930509997048866, -0.16261800472383145, 0.17724174556701824, 0.01756127264212679... |
709.4576 | Confinement of Cosmic Rays in Dark Matter clumps | Some part of the relic Dark Matter is distributed in small-scale clumps which
survived structure formation in inflation cosmological scenario. The
annihilation of DM inside these clumps is a strong source of stable charged
particles which can have a substantial density near the clump core. The
streaming of the annihi... | astro-ph | some part of the relic dark matter is distributed in smallscale clumps which survived structure formation in inflation cosmological scenario the annihilation of dm inside these clumps is a strong source of stable charged particles which can have a substantial density near the clump core the streaming of the annihilatio... | [['some', 'part', 'of', 'the', 'relic', 'dark', 'matter', 'is', 'distributed', 'in', 'smallscale', 'clumps', 'which', 'survived', 'structure', 'formation', 'in', 'inflation', 'cosmological', 'scenario', 'the', 'annihilation', 'of', 'dm', 'inside', 'these', 'clumps', 'is', 'a', 'strong', 'source', 'of', 'stable', 'charg... | [-0.1747535355481025, 0.23305274808999935, -0.0999944070354104, 0.12245753228413186, -0.09219458515412714, 0.031242162770420117, -0.057738565821445695, 0.34853311049702923, -0.28474487675549953, -0.33272465730184003, 0.014737675989683913, -0.2434351312388715, -0.00302624153463464, 0.12715133066338144, 0.030327623366917... |
709.4577 | Sub-Kelvin Cooling of a Macroscopic Oscillator and femto-Newton Force
Measurement | Measuring very small forces, particularly those of a gravitational nature,
has always been of great interest, as fundamental tests of our understanding of
the physical laws. Ultra-long period mechanical oscillators, typically used in
such measurements, will have kT/2 of thermal energy associated with each degree
of f... | physics.ins-det physics.optics | measuring very small forces particularly those of a gravitational nature has always been of great interest as fundamental tests of our understanding of the physical laws ultralong period mechanical oscillators typically used in such measurements will have kt2 of thermal energy associated with each degree of freedom owi... | [['measuring', 'very', 'small', 'forces', 'particularly', 'those', 'of', 'a', 'gravitational', 'nature', 'has', 'always', 'been', 'of', 'great', 'interest', 'as', 'fundamental', 'tests', 'of', 'our', 'understanding', 'of', 'the', 'physical', 'laws', 'ultralong', 'period', 'mechanical', 'oscillators', 'typically', 'used... | [-0.14784003706084742, 0.20828462788688804, -0.06036281469857699, 0.014696194319608122, -0.04838696885680108, -0.13663004680983026, 0.05061197920540093, 0.3706656899766927, -0.2639433082996933, -0.3509445635223166, 0.05258598473648583, -0.23757281875094358, -0.12165722922282873, 0.2548046741282946, -0.02536869582553931... |
709.4578 | On the Nature of Precursors in the Radio Pulsar Profiles | In the average profiles of several radio pulsars, the main pulse is
accompanied by the preceding component. This so called precursor is known for
its distinctive polarization, spectral, and fluctuation properties. Recent
single-pulse observations hint that the sporadic activity at the extreme
leading edge of the puls... | astro-ph | in the average profiles of several radio pulsars the main pulse is accompanied by the preceding component this so called precursor is known for its distinctive polarization spectral and fluctuation properties recent singlepulse observations hint that the sporadic activity at the extreme leading edge of the pulse may be... | [['in', 'the', 'average', 'profiles', 'of', 'several', 'radio', 'pulsars', 'the', 'main', 'pulse', 'is', 'accompanied', 'by', 'the', 'preceding', 'component', 'this', 'so', 'called', 'precursor', 'is', 'known', 'for', 'its', 'distinctive', 'polarization', 'spectral', 'and', 'fluctuation', 'properties', 'recent', 'singl... | [-0.12515590189169967, 0.16834129395256578, -0.09364708961579765, 0.09359332650215768, -0.07894724368600657, -0.05653189914013593, 0.009034385875925238, 0.4292038902712204, -0.25899792011298334, -0.29403271303040746, 0.09283817459377863, -0.23579050893435416, -0.13338408092278298, 0.21938167873016892, -0.02537326833515... |
709.4579 | Classification problems of toric manifolds via topology | We propose some problems on the classification of toric manifolds from the
viewpoint of topology and survey related results.
| math.AT math.AG | we propose some problems on the classification of toric manifolds from the viewpoint of topology and survey related results | [['we', 'propose', 'some', 'problems', 'on', 'the', 'classification', 'of', 'toric', 'manifolds', 'from', 'the', 'viewpoint', 'of', 'topology', 'and', 'survey', 'related', 'results']] | [-0.11404437718814925, -0.058610162379122095, -0.07395469318879277, 0.08426855141787153, -0.10694877028857407, -0.1009008027613163, 0.018134277117879766, 0.3332871697647007, -0.3029590045150958, -0.2886383486421485, 0.19531025891927511, -0.3043538108468056, -0.2618809807065286, 0.2531477689350906, -0.2339879439065331, ... |
709.458 | Influence of mechanical properties on mixing and segregation of granular
material | Processes of mixing and segregation in a packed bed of granular material
stirred by a periodically moving rectangular bar are simulated by the discrete
element method (DEM). Influence of mechanical properties of the particle
material (dynamic friction coefficient, density, elastic modulus) on the
segregation intensit... | cond-mat.soft cond-mat.stat-mech | processes of mixing and segregation in a packed bed of granular material stirred by a periodically moving rectangular bar are simulated by the discrete element method dem influence of mechanical properties of the particle material dynamic friction coefficient density elastic modulus on the segregation intensity is rese... | [['processes', 'of', 'mixing', 'and', 'segregation', 'in', 'a', 'packed', 'bed', 'of', 'granular', 'material', 'stirred', 'by', 'a', 'periodically', 'moving', 'rectangular', 'bar', 'are', 'simulated', 'by', 'the', 'discrete', 'element', 'method', 'dem', 'influence', 'of', 'mechanical', 'properties', 'of', 'the', 'parti... | [-0.12026773821262102, 0.24417532657483412, -0.13256509202502428, -0.025282916483364157, -0.037291782562650984, -0.08905920410348524, -0.00465244192098673, 0.4098356700231952, -0.3204504393412912, -0.308772441119917, 0.05286569765866584, -0.28280837551480337, -0.1389845094132808, 0.13921513603136484, 0.0121551490569066... |
709.4581 | Detecting a Lorentz-Violating Field in Cosmology | We consider cosmology in the Einstein-aether theory (the generally covariant
theory of gravitation coupled to a dynamical timelike Lorentz-violating vector
field) with a linear aether-Lagrangian. The 3+1 spacetime splitting approach is
used to derive covariant and gauge invariant perturbation equations which are
vali... | astro-ph gr-qc hep-ph | we consider cosmology in the einsteinaether theory the generally covariant theory of gravitation coupled to a dynamical timelike lorentzviolating vector field with a linear aetherlagrangian the 31 spacetime splitting approach is used to derive covariant and gauge invariant perturbation equations which are valid for a g... | [['we', 'consider', 'cosmology', 'in', 'the', 'einsteinaether', 'theory', 'the', 'generally', 'covariant', 'theory', 'of', 'gravitation', 'coupled', 'to', 'a', 'dynamical', 'timelike', 'lorentzviolating', 'vector', 'field', 'with', 'a', 'linear', 'aetherlagrangian', 'the', '31', 'spacetime', 'splitting', 'approach', 'i... | [-0.11698082698800136, 0.17994252815144138, -0.10496570425573737, 0.12156943908135873, -0.10341458668932318, -0.1304699992534006, -0.08727120216703042, 0.31830451360845474, -0.21956178891123274, -0.3011356753288419, 0.06276229561364743, -0.2556903181760572, -0.12882809582166374, 0.16598106815479696, -0.0042073590098880... |
709.4582 | Dynamical Chirally Improved Quarks: First Results for Hadron Masses | We present first results for a study with two mass-degenerate dynamical
Chirally Improved (CI) fermions on lattices of spatial extent 2.4 fm. The CI
Dirac operator obeys the Ginsparg-Wilson condition in good approximation. The
pion mass we use is still large O(470 MeV) for the 16**3*32 lattices with
lattice spacing o... | hep-lat | we present first results for a study with two massdegenerate dynamical chirally improved ci fermions on lattices of spatial extent 24 fm the ci dirac operator obeys the ginspargwilson condition in good approximation the pion mass we use is still large o470 mev for the 16332 lattices with lattice spacing of 015 fm the h... | [['we', 'present', 'first', 'results', 'for', 'a', 'study', 'with', 'two', 'massdegenerate', 'dynamical', 'chirally', 'improved', 'ci', 'fermions', 'on', 'lattices', 'of', 'spatial', 'extent', '24', 'fm', 'the', 'ci', 'dirac', 'operator', 'obeys', 'the', 'ginspargwilson', 'condition', 'in', 'good', 'approximation', 'th... | [-0.09735992643525641, 0.22955103356427714, -0.0579105012812743, 0.08931928203445767, -0.012466274296885411, -0.12316915950870287, 0.08458250130791509, 0.4193079447483315, -0.10557182355984754, -0.2568119098386709, 0.028746165930950904, -0.3014616407454014, -0.04753714157085793, 0.10998920104512032, 0.07056009997990366... |
709.4583 | Chiral effective-field theory in the Delta(1232) region: II. radiative
pion photoproduction | We present a theoretical study of the radiative pion photoproduction on the
nucleon ($\gamma N \to \pi N \gamma'$) in the $\De$-resonance region, with the
aim to determine the magnetic dipole moment (MDM) of the $\Delta^+(1232)$. The
study is done within the framework of chiral effective-field theory where the
expans... | hep-ph nucl-ex nucl-th | we present a theoretical study of the radiative pion photoproduction on the nucleon gamma n to pi n gamma in the deresonance region with the aim to determine the magnetic dipole moment mdm of the delta1232 the study is done within the framework of chiral effectivefield theory where the expansion is performed to nexttol... | [['we', 'present', 'a', 'theoretical', 'study', 'of', 'the', 'radiative', 'pion', 'photoproduction', 'on', 'the', 'nucleon', 'gamma', 'n', 'to', 'pi', 'n', 'gamma', 'in', 'the', 'deresonance', 'region', 'with', 'the', 'aim', 'to', 'determine', 'the', 'magnetic', 'dipole', 'moment', 'mdm', 'of', 'the', 'delta1232', 'the... | [-0.1462441873383906, 0.13969985999464177, -0.10347716329322959, 0.07482434119094361, -0.07692622853033809, -0.035442231579288615, 0.044074443490403195, 0.3429820801794642, -0.20320231852890697, -0.27932613379688875, -0.02230386456270053, -0.30859007871229993, -0.06019254690600616, 0.132825452629759, 0.0958985008513660... |
709.4584 | New constraints on the Mid-IR EBL from the HESS discovery of VHE gamma
rays from 1ES 0229+200 | AIMS: To investigate the very high energy (VHE: >100 GeV) gamma-ray emission
from the high-frequency peaked BL Lac 1ES 0229+200.
METHODS: Observations of 1ES 0229+200 at energies above 580 GeV were
performed with the High Energy Stereoscopic System (HESS) in 2005 and 2006.
RESULTS: 1ES 0229+200 is discovered by H... | astro-ph | aims to investigate the very high energy vhe 100 gev gammaray emission from the highfrequency peaked bl lac 1es 0229200 methods observations of 1es 0229200 at energies above 580 gev were performed with the high energy stereoscopic system hess in 2005 and 2006 results 1es 0229200 is discovered by hess to be an emitter o... | [['aims', 'to', 'investigate', 'the', 'very', 'high', 'energy', 'vhe', '100', 'gev', 'gammaray', 'emission', 'from', 'the', 'highfrequency', 'peaked', 'bl', 'lac', '1es', '0229200', 'methods', 'observations', 'of', '1es', '0229200', 'at', 'energies', 'above', '580', 'gev', 'were', 'performed', 'with', 'the', 'high', 'e... | [-0.03626984328322818, 0.16900650703732917, -0.038089019181245146, 0.16974654170402342, -0.08836699937520082, -0.12326383444963505, 0.03925847966624462, 0.4512458933371698, -0.14041023861488458, -0.4726502208169473, 0.021245703655148957, -0.3496519450592682, 0.09515310748989997, 0.23269097805943018, -0.0314528534601829... |
709.4585 | Coulomb gauge studies of SU(3) Yang-Mills theory on the lattice | We study the infrared behaviour of lattice SU(3) Yang-Mills theory in Coulomb
gauge in terms of the ghost propagator, the Coulomb potential and the
transversal and the time-time component of the equal-time gluon propagator. In
particular, we focus on the Gribov problem and its impact on the observables.
We observe th... | hep-lat | we study the infrared behaviour of lattice su3 yangmills theory in coulomb gauge in terms of the ghost propagator the coulomb potential and the transversal and the timetime component of the equaltime gluon propagator in particular we focus on the gribov problem and its impact on the observables we observe that the simu... | [['we', 'study', 'the', 'infrared', 'behaviour', 'of', 'lattice', 'su3', 'yangmills', 'theory', 'in', 'coulomb', 'gauge', 'in', 'terms', 'of', 'the', 'ghost', 'propagator', 'the', 'coulomb', 'potential', 'and', 'the', 'transversal', 'and', 'the', 'timetime', 'component', 'of', 'the', 'equaltime', 'gluon', 'propagator',... | [-0.12770585070327928, 0.1974393419327471, -0.15307827970336477, 0.13433510779464494, -0.07705618054076226, -0.09793560810576746, 0.022796850017840768, 0.37135866019333863, -0.21385875326430726, -0.22794440779054237, 0.04510638258534255, -0.26866630251480345, -0.13038864094257901, 0.10788217101184774, 0.003338827231541... |
709.4586 | Scalar Curvature Estimates by Parallel Alternating Torsion | We generalize Llarull's scalar curvature comparison to Riemannian manifolds
admitting metric connections with parallel and alternating torsion and having a
nonnegative curvature operator on 2-vectors. As a byproduct, we show that Euler
number and signature of such manifolds are determined by their global holonomy
rep... | math.DG | we generalize llarulls scalar curvature comparison to riemannian manifolds admitting metric connections with parallel and alternating torsion and having a nonnegative curvature operator on 2vectors as a byproduct we show that euler number and signature of such manifolds are determined by their global holonomy represent... | [['we', 'generalize', 'llarulls', 'scalar', 'curvature', 'comparison', 'to', 'riemannian', 'manifolds', 'admitting', 'metric', 'connections', 'with', 'parallel', 'and', 'alternating', 'torsion', 'and', 'having', 'a', 'nonnegative', 'curvature', 'operator', 'on', '2vectors', 'as', 'a', 'byproduct', 'we', 'show', 'that',... | [-0.1930415895409309, 0.0913273664489866, -0.06555514791622184, 0.09674188874972363, -0.14882320338764635, -0.15535425081944618, -0.033186881767156035, 0.40240018564061475, -0.20847752752403417, -0.23582217886667842, 0.1078879554108239, -0.27950403296973747, -0.19275392214648235, 0.18640669101538757, -0.128284427080637... |
709.4587 | Quadratic equations and monodromy evolving deformations | We give a basic theory on monodromy evolving deformations. proposed by
Chakravarty and Ablowitz in 1996. We show that Halphen's second quadratic
system can be described by monodromy evolving deformations. Our result is a
generalization of the work on the DH-V system by Chakravarty and Ablowitz.
| math.CA math-ph math.MP | we give a basic theory on monodromy evolving deformations proposed by chakravarty and ablowitz in 1996 we show that halphens second quadratic system can be described by monodromy evolving deformations our result is a generalization of the work on the dhv system by chakravarty and ablowitz | [['we', 'give', 'a', 'basic', 'theory', 'on', 'monodromy', 'evolving', 'deformations', 'proposed', 'by', 'chakravarty', 'and', 'ablowitz', 'in', '1996', 'we', 'show', 'that', 'halphens', 'second', 'quadratic', 'system', 'can', 'be', 'described', 'by', 'monodromy', 'evolving', 'deformations', 'our', 'result', 'is', 'a',... | [-0.1450838624085817, 0.08052098188135359, -0.10822148260970911, 0.010201269157955216, -0.0421869543277555, -0.10486242831167247, -0.02068074277550396, 0.25900445897132157, -0.25074099276421796, -0.2977094949947463, 0.12233360453974455, -0.23992520852221383, -0.30354424570169714, 0.20538356560799811, -0.168377646100189... |
709.4588 | m-Mode Regularization Scheme for the Self Force in Kerr Spacetime | We present a new, simple method for calculating the scalar, electromagnetic,
and gravitational self forces acting on particles in orbit around a Kerr black
hole. The standard ``mode-sum regularization'' approach for self-force
calculations relies on a decomposition of the full (retarded) perturbation
field into multi... | gr-qc astro-ph | we present a new simple method for calculating the scalar electromagnetic and gravitational self forces acting on particles in orbit around a kerr black hole the standard modesum regularization approach for selfforce calculations relies on a decomposition of the full retarded perturbation field into multipole modes fol... | [['we', 'present', 'a', 'new', 'simple', 'method', 'for', 'calculating', 'the', 'scalar', 'electromagnetic', 'and', 'gravitational', 'self', 'forces', 'acting', 'on', 'particles', 'in', 'orbit', 'around', 'a', 'kerr', 'black', 'hole', 'the', 'standard', 'modesum', 'regularization', 'approach', 'for', 'selfforce', 'calc... | [-0.12733483453604408, 0.06740566122053719, -0.13424343210923026, 0.064766611515891, -0.09998317322096051, -0.11527932783130056, -0.007743576595406813, 0.3279583034897918, -0.18687561408741704, -0.26026562009173543, 0.05382776736028131, -0.24215997726336788, -0.14060941009622402, 0.23212423870590196, 0.0094060322118631... |
709.4589 | All-electric detectors of the polarization state of terahertz laser
radiation (extended version) | Two types of room temperature detectors of terahertz laser radiation have
been developed which allow in an all-electric manner to determine the plane of
polarization of linearly polarized radiation and the ellipticity of
elliptically polarized radiation, respectively. The operation of the detectors
is based on photog... | cond-mat.mes-hall | two types of room temperature detectors of terahertz laser radiation have been developed which allow in an allelectric manner to determine the plane of polarization of linearly polarized radiation and the ellipticity of elliptically polarized radiation respectively the operation of the detectors is based on photogalvan... | [['two', 'types', 'of', 'room', 'temperature', 'detectors', 'of', 'terahertz', 'laser', 'radiation', 'have', 'been', 'developed', 'which', 'allow', 'in', 'an', 'allelectric', 'manner', 'to', 'determine', 'the', 'plane', 'of', 'polarization', 'of', 'linearly', 'polarized', 'radiation', 'and', 'the', 'ellipticity', 'of',... | [-0.1669822079812487, 0.24384936306179347, -0.08462681890154879, -0.028987871462789673, -0.04212130820689102, -0.1220378492710491, -0.02114138373794655, 0.47940650577346483, -0.22911721261839071, -0.3202710601501167, 0.05396928772019843, -0.28671869861582916, -0.04452106410016616, 0.254750962095956, 0.04720355437447627... |
709.459 | Measurements of the CKM angle gamma at BABAR | We present a short review of the measurements of the CKM angle gamma
performed by the babar experiment. We focus on methods using charged B decays,
which give a direct access to gamma and provide the best constraints so far.
| hep-ex | we present a short review of the measurements of the ckm angle gamma performed by the babar experiment we focus on methods using charged b decays which give a direct access to gamma and provide the best constraints so far | [['we', 'present', 'a', 'short', 'review', 'of', 'the', 'measurements', 'of', 'the', 'ckm', 'angle', 'gamma', 'performed', 'by', 'the', 'babar', 'experiment', 'we', 'focus', 'on', 'methods', 'using', 'charged', 'b', 'decays', 'which', 'give', 'a', 'direct', 'access', 'to', 'gamma', 'and', 'provide', 'the', 'best', 'con... | [-0.10068277781247162, 0.13149073920212687, -0.0928307589609176, 0.043109439220279454, -0.12823932603932917, -0.16756281240377574, 0.15554854884685482, 0.33727543875575067, -0.20146662201732396, -0.259269426879473, 0.05599285594653338, -0.3076244191266596, -0.047884673322550954, 0.20080127487890423, 0.0822452814434655,... |
709.4591 | Theoretical study of molecular electronic excitations and optical
transitions of C60 | We report results on ab initio calculations of excited states of the
fullerene molecule by using configuration interaction (CI) approach with singly
excited determinants (SCI). We have used both the experimental geometry and the
one optimized by the density functional method and worked with basis sets at
the cc-pVTZ ... | cond-mat.str-el cond-mat.mtrl-sci | we report results on ab initio calculations of excited states of the fullerene molecule by using configuration interaction ci approach with singly excited determinants sci we have used both the experimental geometry and the one optimized by the density functional method and worked with basis sets at the ccpvtz and augc... | [['we', 'report', 'results', 'on', 'ab', 'initio', 'calculations', 'of', 'excited', 'states', 'of', 'the', 'fullerene', 'molecule', 'by', 'using', 'configuration', 'interaction', 'ci', 'approach', 'with', 'singly', 'excited', 'determinants', 'sci', 'we', 'have', 'used', 'both', 'the', 'experimental', 'geometry', 'and',... | [-0.06508995035997117, 0.16821400450656787, 0.03119550129609569, 0.0521240117835209, 0.05973395170957295, -0.15621923344244934, 0.10327291417114273, 0.4286705300258765, -0.19267192933673286, -0.3640509535581951, -0.009347944628775307, -0.3717485132375322, -0.048402264756706996, 0.0994011511302805, 0.0944078787165524, -... |
709.4592 | The isomorphism conjecture in L-theory: graphs of groups | We study the Fibered Isomorphism Conjecture of Farrell and Jones in L-theory
for groups acting on trees. In several cases we prove the conjecture. This
includes wreath products of abelian groups and free metabelian groups. We also
deduce the conjecture in pseudoisotopy theory for these groups. Finally in B of
Theorem... | math.KT math.GT | we study the fibered isomorphism conjecture of farrell and jones in ltheory for groups acting on trees in several cases we prove the conjecture this includes wreath products of abelian groups and free metabelian groups we also deduce the conjecture in pseudoisotopy theory for these groups finally in b of theorem 11 we ... | [['we', 'study', 'the', 'fibered', 'isomorphism', 'conjecture', 'of', 'farrell', 'and', 'jones', 'in', 'ltheory', 'for', 'groups', 'acting', 'on', 'trees', 'in', 'several', 'cases', 'we', 'prove', 'the', 'conjecture', 'this', 'includes', 'wreath', 'products', 'of', 'abelian', 'groups', 'and', 'free', 'metabelian', 'gro... | [-0.20268686464606006, 0.09850287092391585, -0.11910016530910965, 0.11774944103910726, -0.009009249981675968, -0.10897450736861249, 0.03369073319958798, 0.3641567703214337, -0.3084977502385002, -0.295889927776622, 0.10957213816019233, -0.23018550780052166, -0.1557826301174574, 0.24844796934210864, -0.1770634208004311, ... |
709.4593 | Gamma Ray Spectrum from Gravitino Dark Matter Decay | Gravitinos are very promising candidates for the cold dark matter of the
Universe. Interestingly, to achieve a sufficiently long gravitino lifetime,
R-parity conservation is not required, thus preventing any dangerous
cosmological influence of the next-to-lightest supersymmetric particle. When
R-parity is violated, g... | astro-ph hep-ph | gravitinos are very promising candidates for the cold dark matter of the universe interestingly to achieve a sufficiently long gravitino lifetime rparity conservation is not required thus preventing any dangerous cosmological influence of the nexttolightest supersymmetric particle when rparity is violated gravitinos de... | [['gravitinos', 'are', 'very', 'promising', 'candidates', 'for', 'the', 'cold', 'dark', 'matter', 'of', 'the', 'universe', 'interestingly', 'to', 'achieve', 'a', 'sufficiently', 'long', 'gravitino', 'lifetime', 'rparity', 'conservation', 'is', 'not', 'required', 'thus', 'preventing', 'any', 'dangerous', 'cosmological',... | [-0.0971742290650692, 0.3003592139034711, -0.0814303773492951, 0.20923832506047224, -0.11050899145240435, -0.17265918253064907, -0.014470095882478001, 0.32561957305579475, -0.21399905279542158, -0.35132370131428947, 0.0344680248785557, -0.30535424164863245, 0.06730543672474044, 0.19156914462471814, 0.01935719292272221,... |
709.4594 | Flows of Spin(7)-structures | We consider flows of Spin(7)-structures. We use local coordinates to describe
the torsion tensor of a Spin(7)-structure and derive the evolution equations
for a general flow of a Spin(7)-structure on an 8-manifold M. Specifically, we
compute the evolution of the metric and the torsion tensor. We also give an
explicit... | math.DG | we consider flows of spin7structures we use local coordinates to describe the torsion tensor of a spin7structure and derive the evolution equations for a general flow of a spin7structure on an 8manifold m specifically we compute the evolution of the metric and the torsion tensor we also give an explicit description of ... | [['we', 'consider', 'flows', 'of', 'spin7structures', 'we', 'use', 'local', 'coordinates', 'to', 'describe', 'the', 'torsion', 'tensor', 'of', 'a', 'spin7structure', 'and', 'derive', 'the', 'evolution', 'equations', 'for', 'a', 'general', 'flow', 'of', 'a', 'spin7structure', 'on', 'an', '8manifold', 'm', 'specifically'... | [-0.22096442396286875, 0.04555266138352939, -0.1152368468271258, 0.048567465878780545, -0.11790511038270779, -0.055881337980584554, -0.09046741188891853, 0.28458410570359166, -0.2604189821043595, -0.21553687863827994, 0.10879844236721208, -0.22714771532143155, -0.18702231262189647, 0.1376069462300317, -0.04961519189722... |
709.4595 | Worldline Approach to Chiral Fermions | We propose to apply ``worldline numerics'' to a numerical calculation of
quark determinants. The Gross-Neveu model with a U(1) chiral symmetry is
considered as a first test. The worldline approach allows for an analytic
renormalisation, and only finite parts of the determinant require a numerical
calculation. It is s... | hep-lat hep-ph hep-th | we propose to apply worldline numerics to a numerical calculation of quark determinants the grossneveu model with a u1 chiral symmetry is considered as a first test the worldline approach allows for an analytic renormalisation and only finite parts of the determinant require a numerical calculation it is shown that the... | [['we', 'propose', 'to', 'apply', 'worldline', 'numerics', 'to', 'a', 'numerical', 'calculation', 'of', 'quark', 'determinants', 'the', 'grossneveu', 'model', 'with', 'a', 'u1', 'chiral', 'symmetry', 'is', 'considered', 'as', 'a', 'first', 'test', 'the', 'worldline', 'approach', 'allows', 'for', 'an', 'analytic', 'reno... | [-0.1238440558191781, 0.12778948904888238, -0.10672607363054627, 0.06811372289238007, -0.09875020045591028, -0.1280728252212468, -0.010320014714900601, 0.3612759842096191, -0.13205834633523697, -0.2283782115941377, 0.07625623888973343, -0.2632176874917748, -0.15973961672892695, 0.14863902724249975, 0.022024048502115826... |
709.4596 | Ground state fidelity from tensor network representations | For any D-dimensional quantum lattice system, the fidelity between two ground
state many-body wave functions is mapped onto the partition function of a
D-dimensional classical statistical vertex lattice model with the same lattice
geometry. The fidelity per lattice site, analogous to the free energy per site,
is well... | cond-mat.stat-mech cond-mat.str-el | for any ddimensional quantum lattice system the fidelity between two ground state manybody wave functions is mapped onto the partition function of a ddimensional classical statistical vertex lattice model with the same lattice geometry the fidelity per lattice site analogous to the free energy per site is welldefined i... | [['for', 'any', 'ddimensional', 'quantum', 'lattice', 'system', 'the', 'fidelity', 'between', 'two', 'ground', 'state', 'manybody', 'wave', 'functions', 'is', 'mapped', 'onto', 'the', 'partition', 'function', 'of', 'a', 'ddimensional', 'classical', 'statistical', 'vertex', 'lattice', 'model', 'with', 'the', 'same', 'la... | [-0.11465278914985583, 0.16899996214623073, -0.031138891008557733, 0.06807233523529445, 0.019518265903917784, -0.14456462023357294, 0.0674472984848256, 0.3704144048034069, -0.279344276880327, -0.2555506728282294, 0.04460684874349456, -0.2722940349797766, -0.1109254731767878, 0.15071749417639346, 0.029231745389664603, 0... |
709.4597 | Some Aspects of Intermediate mass black holes | There is a lot of current astrophysical evidence and interest in intermediate
mass black holes, ranging from a few hundred to several thousand solar masses.
The active galaxy M82 and the globular cluster in M31, for example, are known
to host such objects. Here we discuss several aspects of intermediate mass
black ho... | astro-ph | there is a lot of current astrophysical evidence and interest in intermediate mass black holes ranging from a few hundred to several thousand solar masses the active galaxy m82 and the globular cluster in m31 for example are known to host such objects here we discuss several aspects of intermediate mass black holes suc... | [['there', 'is', 'a', 'lot', 'of', 'current', 'astrophysical', 'evidence', 'and', 'interest', 'in', 'intermediate', 'mass', 'black', 'holes', 'ranging', 'from', 'a', 'few', 'hundred', 'to', 'several', 'thousand', 'solar', 'masses', 'the', 'active', 'galaxy', 'm82', 'and', 'the', 'globular', 'cluster', 'in', 'm31', 'for... | [-0.10955975356535251, 0.138896395205794, -0.0039388523084901966, 0.2070814342513884, -0.07752745169676653, -0.055976097613862644, 0.025387260155016633, 0.37700472691119846, -0.1824181749321082, -0.3899855120029269, 0.11288026795906461, -0.3007400886492193, -0.07963324139411208, 0.2570524493216717, -0.00110064320532338... |
709.4598 | Upper Limits from HESS Observations of AGN in 2005-2007 | Very high energy (VHE; >100 GeV) observations of a sample of selected active
galactic nuclei (AGN) were performed between January 2005 and April 2007 with
the High Energy Stereoscopic System (HESS), an array of imaging
atmospheric-Cherenkov telescopes. Significant detections are reported elsewhere
for many of these o... | astro-ph | very high energy vhe 100 gev observations of a sample of selected active galactic nuclei agn were performed between january 2005 and april 2007 with the high energy stereoscopic system hess an array of imaging atmosphericcherenkov telescopes significant detections are reported elsewhere for many of these objects here i... | [['very', 'high', 'energy', 'vhe', '100', 'gev', 'observations', 'of', 'a', 'sample', 'of', 'selected', 'active', 'galactic', 'nuclei', 'agn', 'were', 'performed', 'between', 'january', '2005', 'and', 'april', '2007', 'with', 'the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'an', 'array', 'of', 'imaging', 'at... | [-0.04907249314531397, 0.15988023418503872, -0.0030315232042294857, 0.18208130876323245, -0.12728814198635519, -0.14633980286844933, 0.02344404611414155, 0.5392957100590977, -0.04601310599201287, -0.5287105143607522, 0.05718157064648739, -0.37359531411381725, 0.05918395689849813, 0.2850828380189621, -0.0272994649433083... |
709.4599 | Braided differential structure on Weyl groups, quadratic algebras and
elliptic functions | We discuss a class of generalized divided difference operators which give
rise to a representation of Nichols-Woronowicz algebras associated to Weyl
groups. For the root system of type $A,$ we also study the condition for the
deformations of the Fomin-Kirillov quadratic algebra, which is a quadratic lift
of the Nicho... | math.QA | we discuss a class of generalized divided difference operators which give rise to a representation of nicholsworonowicz algebras associated to weyl groups for the root system of type a we also study the condition for the deformations of the fominkirillov quadratic algebra which is a quadratic lift of the nicholsworonow... | [['we', 'discuss', 'a', 'class', 'of', 'generalized', 'divided', 'difference', 'operators', 'which', 'give', 'rise', 'to', 'a', 'representation', 'of', 'nicholsworonowicz', 'algebras', 'associated', 'to', 'weyl', 'groups', 'for', 'the', 'root', 'system', 'of', 'type', 'a', 'we', 'also', 'study', 'the', 'condition', 'fo... | [-0.1585704820287047, 0.12926522096750712, -0.056640290589344625, 0.06882602878201828, -0.11535433897127707, -0.11283753755398923, -0.03984211239436961, 0.2708133326918639, -0.3727869757949704, -0.17115166165038115, 0.09975440551014146, -0.2797111625585592, -0.1692918740269361, 0.16726007658724834, -0.10676990075018068... |
709.46 | Twisted Hopf symmetries of canonical noncommutative spacetimes and the
no-pure-boost principle | We study the twisted-Hopf-algebra symmetries of observer-independent
canonical spacetime noncommutativity, for which the commutators of the
spacetime coordinates take the form [x^{mu},x^{nu}]=i theta^{mu nu} with
observer-independent (and coordinate-independent) theta^{mu nu}. We find that
it is necessary to introduc... | hep-th | we study the twistedhopfalgebra symmetries of observerindependent canonical spacetime noncommutativity for which the commutators of the spacetime coordinates take the form xmuxnui thetamu nu with observerindependent and coordinateindependent thetamu nu we find that it is necessary to introduce nontrivial commutators be... | [['we', 'study', 'the', 'twistedhopfalgebra', 'symmetries', 'of', 'observerindependent', 'canonical', 'spacetime', 'noncommutativity', 'for', 'which', 'the', 'commutators', 'of', 'the', 'spacetime', 'coordinates', 'take', 'the', 'form', 'xmuxnui', 'thetamu', 'nu', 'with', 'observerindependent', 'and', 'coordinateindepe... | [-0.16357348708429767, 0.13550600327251136, -0.08499117171404098, 0.052510403959834216, -0.10242652385127976, -0.07692140327631741, 0.009275105406566965, 0.3241518073421168, -0.24122132816793104, -0.26773213222929226, 0.05489169424062742, -0.2558530105697604, -0.14989235868530446, 0.12752284252430973, -0.03502445262366... |
709.4601 | Multiple stellar populations in Globular Clusters: collection of
information from the Horizontal Branch | The majority of the inhomogeneities in the chemical composition of Globular
Cluster (GC) stars appear due to primordial enrichment by hot-CNO cycled
material processed in stars belonging to a first stellar generation. Either
massive AGB envelopes subject to hot bottom burning, or the envelopes of
massive fastly rotat... | astro-ph | the majority of the inhomogeneities in the chemical composition of globular cluster gc stars appear due to primordial enrichment by hotcno cycled material processed in stars belonging to a first stellar generation either massive agb envelopes subject to hot bottom burning or the envelopes of massive fastly rotating sta... | [['the', 'majority', 'of', 'the', 'inhomogeneities', 'in', 'the', 'chemical', 'composition', 'of', 'globular', 'cluster', 'gc', 'stars', 'appear', 'due', 'to', 'primordial', 'enrichment', 'by', 'hotcno', 'cycled', 'material', 'processed', 'in', 'stars', 'belonging', 'to', 'a', 'first', 'stellar', 'generation', 'either'... | [-0.05590196574549437, 0.16126204639024927, -0.06823446889746895, 0.10237671617852925, -0.08207290548569598, -0.03180992493057103, 0.06352747197702277, 0.39629692993663224, -0.1920961070897933, -0.357777905278566, 0.04586086129603493, -0.26396641278750094, -0.03791024969798569, 0.16993571457398773, -0.07539603260819645... |
709.4602 | Multi-wavelength Observations of PG 1553+113 with HESS | Very high energy (VHE; >100 GeV) gamma-ray observations of PG 1553+113 were
made with the High Energy Stereoscopic System (HESS) in 2005 and 2006. A strong
signal, ~10 standard deviations, is detected by HESS during the 2 years of
observations (24.8 hours live time). The time-averaged energy spectrum,
measured betwee... | astro-ph | very high energy vhe 100 gev gammaray observations of pg 1553113 were made with the high energy stereoscopic system hess in 2005 and 2006 a strong signal 10 standard deviations is detected by hess during the 2 years of observations 248 hours live time the timeaveraged energy spectrum measured between 225 gev to 13 tev ... | [['very', 'high', 'energy', 'vhe', '100', 'gev', 'gammaray', 'observations', 'of', 'pg', '1553113', 'were', 'made', 'with', 'the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'in', '2005', 'and', '2006', 'a', 'strong', 'signal', '10', 'standard', 'deviations', 'is', 'detected', 'by', 'hess', 'during', 'the', '2... | [-0.08387429449831223, 0.16778855014137217, -0.0596165910678105, 0.10807837763292005, -0.09253698455424403, -0.149443362757443, 0.024237396148629756, 0.4583542555999413, -0.12085710419509425, -0.482351306611471, 0.07627996940772123, -0.33451312882892736, 0.07094903950070253, 0.2228181592780065, -0.029319427114753924, -... |
709.4603 | Action Principle and Modification of the Faddeev-Popov Factor in Gauge
Theories | The quantum action (dynamical) principle is exploited to investigate the
nature and origin of the Faddeev-Popov (FP) factor in gauge theories without
recourse to path integrals. Gauge invariant as well as gauge non-invariant
interactions are considered to show that the FP factor needs to be modified in
more general c... | hep-th | the quantum action dynamical principle is exploited to investigate the nature and origin of the faddeevpopov fp factor in gauge theories without recourse to path integrals gauge invariant as well as gauge noninvariant interactions are considered to show that the fp factor needs to be modified in more general cases and ... | [['the', 'quantum', 'action', 'dynamical', 'principle', 'is', 'exploited', 'to', 'investigate', 'the', 'nature', 'and', 'origin', 'of', 'the', 'faddeevpopov', 'fp', 'factor', 'in', 'gauge', 'theories', 'without', 'recourse', 'to', 'path', 'integrals', 'gauge', 'invariant', 'as', 'well', 'as', 'gauge', 'noninvariant', '... | [-0.126766203913245, 0.16577102986539338, -0.10941872749758835, 0.15429070732985659, -0.13653938491623124, -0.13839921107449168, -0.007205070551279206, 0.3808047752585504, -0.24052520766975238, -0.2868485909632661, 0.03945419962318348, -0.1832045026534757, -0.19816764168344536, 0.14710084420278088, -0.09024156877988732... |
709.4604 | Relativistic analysis of an earth-satellite time transfer | Analytical treatment of time transfer problem for Earth-Satellite system is
presented. The development was made in a complete relativistic framework. In
accordance with modern clock precision and for low altitude orbits, we neglect
the other bodies and consider only the 1/c^2 Earth potential developed up to
the J_2 t... | gr-qc | analytical treatment of time transfer problem for earthsatellite system is presented the development was made in a complete relativistic framework in accordance with modern clock precision and for low altitude orbits we neglect the other bodies and consider only the 1c2 earth potential developed up to the j_2 term in s... | [['analytical', 'treatment', 'of', 'time', 'transfer', 'problem', 'for', 'earthsatellite', 'system', 'is', 'presented', 'the', 'development', 'was', 'made', 'in', 'a', 'complete', 'relativistic', 'framework', 'in', 'accordance', 'with', 'modern', 'clock', 'precision', 'and', 'for', 'low', 'altitude', 'orbits', 'we', 'n... | [-0.15488479666722318, 0.11762992842305525, -0.0266970972548805, 0.04591373076854164, -0.030806503792786422, -0.10461062865843083, -0.003888700084359038, 0.36715406723612665, -0.19949068538114137, -0.2967502818095918, 0.08688063770486955, -0.27617400658189084, -0.08110809555350273, 0.2137622652283194, -0.05877978839642... |
709.4605 | Superconformal spaces and implications for superstrings | We clarify some properties of projective superspace by using a manifestly
superconformal notation. In particular, we analyze the N=2 scalar multiplet in
detail, including its action, and the propagator and its super-Schwinger
parameters. The internal symmetry is taken to be noncompact (after Wick
rotation), allowing ... | hep-th | we clarify some properties of projective superspace by using a manifestly superconformal notation in particular we analyze the n2 scalar multiplet in detail including its action and the propagator and its superschwinger parameters the internal symmetry is taken to be noncompact after wick rotation allowing boundary con... | [['we', 'clarify', 'some', 'properties', 'of', 'projective', 'superspace', 'by', 'using', 'a', 'manifestly', 'superconformal', 'notation', 'in', 'particular', 'we', 'analyze', 'the', 'n2', 'scalar', 'multiplet', 'in', 'detail', 'including', 'its', 'action', 'and', 'the', 'propagator', 'and', 'its', 'superschwinger', 'p... | [-0.08918602665090153, 0.1658306952843803, -0.07787632967735972, 0.09919024445304286, -0.14354014056809847, -0.13952921899486212, -0.018604451820494666, 0.38892856645848484, -0.1733095699680909, -0.2089040015313414, 0.12242157856047514, -0.2439977568273823, -0.18332173326052725, 0.05460709812600286, -0.1003117013662572... |
709.4606 | A photometric study of Be stars located in the seismology fields of
COROT | Context: In preparation for the COROT mission, an exhaustive photometric
study of Be stars located in the seismology fields of the COROT mission has
been performed. The very precise and long-time-spanned photometric observations
gathered by the COROT satellite will give important clues of the origin of the
Be phenome... | astro-ph | context in preparation for the corot mission an exhaustive photometric study of be stars located in the seismology fields of the corot mission has been performed the very precise and longtimespanned photometric observations gathered by the corot satellite will give important clues of the origin of the be phenomenon aim... | [['context', 'in', 'preparation', 'for', 'the', 'corot', 'mission', 'an', 'exhaustive', 'photometric', 'study', 'of', 'be', 'stars', 'located', 'in', 'the', 'seismology', 'fields', 'of', 'the', 'corot', 'mission', 'has', 'been', 'performed', 'the', 'very', 'precise', 'and', 'longtimespanned', 'photometric', 'observatio... | [-0.06855531773131923, 0.13869269292057926, -0.14689623408654298, 0.0896694263008907, -0.14942708645307318, -0.054256782141207154, 0.05969761691300729, 0.39592063831758567, -0.15123909957610673, -0.3787089475019518, 0.11482706709242005, -0.30702163366985885, -0.07033531587341978, 0.2575071151017123, -0.1169028801989205... |
709.4607 | Motion of Spin 1/2 Massive Particle in a Curved Spacetime | Quasi-classical picture of motion of spin 1/2 massive particle in a curved
spacetime is built on base of simple Lagrangian model. The one is constructed
due to analogy with Lagrangian of massive vector particle. Equations of motion
and spin propagation coincide with Papapetrou equations describing dynamic of
classica... | gr-qc | quasiclassical picture of motion of spin 12 massive particle in a curved spacetime is built on base of simple lagrangian model the one is constructed due to analogy with lagrangian of massive vector particle equations of motion and spin propagation coincide with papapetrou equations describing dynamic of classical spin... | [['quasiclassical', 'picture', 'of', 'motion', 'of', 'spin', '12', 'massive', 'particle', 'in', 'a', 'curved', 'spacetime', 'is', 'built', 'on', 'base', 'of', 'simple', 'lagrangian', 'model', 'the', 'one', 'is', 'constructed', 'due', 'to', 'analogy', 'with', 'lagrangian', 'of', 'massive', 'vector', 'particle', 'equatio... | [-0.17113239863128574, 0.21947346667379694, -0.0693480939845796, 0.05425547279365775, -0.1347072326095292, -0.15174788355620372, -0.1082863572433039, 0.27232137767391074, -0.18925762416243, -0.28685577113733246, -0.012049828114902118, -0.23708272687400933, -0.12634201616876656, 0.12863613174650473, -0.03186493524764147... |
709.4608 | A Spectacular VHE Gamma-Ray Outburst from PKS 2155-304 in 2006 | Since 2002 the VHE (>100 GeV) gamma-ray flux of the high-frequency peaked BL
Lac PKS 2155-304 has been monitored with the High Energy Stereoscopic System
(HESS). An extreme gamma-ray outburst was detected in the early hours of July
28, 2006 (MJD 53944). The average flux above 200 GeV observed during this
outburst is ... | astro-ph | since 2002 the vhe 100 gev gammaray flux of the highfrequency peaked bl lac pks 2155304 has been monitored with the high energy stereoscopic system hess an extreme gammaray outburst was detected in the early hours of july 28 2006 mjd 53944 the average flux above 200 gev observed during this outburst is 7 times the flux... | [['since', '2002', 'the', 'vhe', '100', 'gev', 'gammaray', 'flux', 'of', 'the', 'highfrequency', 'peaked', 'bl', 'lac', 'pks', '2155304', 'has', 'been', 'monitored', 'with', 'the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'an', 'extreme', 'gammaray', 'outburst', 'was', 'detected', 'in', 'the', 'early', 'hour... | [-0.08207355326895292, 0.18834948294844556, -0.01958492511883378, 0.1620658876808981, -0.06784032589135071, -0.1093981062946841, 0.0033879378034422794, 0.44906229071319104, -0.13992855072254315, -0.47223927749941746, 0.08148585833841934, -0.320142811043188, 0.08313105791807175, 0.2405612344512095, -0.03653181775220825,... |
709.4609 | Super-Tonks-Girardeau regime in trapped one-dimensional dipolar gases | Possible signatures of a super-Tonks-Girardeau gas in bosonic systems of
trapped quasi-one-dimensional dipoles are discussed at zero temperature. We
provide estimation of the frequency of the lowest compressional mode and
compare it to analytical results derived using harmonic approach in the high
density regime. We ... | cond-mat.other | possible signatures of a supertonksgirardeau gas in bosonic systems of trapped quasionedimensional dipoles are discussed at zero temperature we provide estimation of the frequency of the lowest compressional mode and compare it to analytical results derived using harmonic approach in the high density regime we construc... | [['possible', 'signatures', 'of', 'a', 'supertonksgirardeau', 'gas', 'in', 'bosonic', 'systems', 'of', 'trapped', 'quasionedimensional', 'dipoles', 'are', 'discussed', 'at', 'zero', 'temperature', 'we', 'provide', 'estimation', 'of', 'the', 'frequency', 'of', 'the', 'lowest', 'compressional', 'mode', 'and', 'compare', ... | [-0.15485271085605123, 0.19209313761384691, -0.04403925724817734, 0.07451983259402607, 0.002714445883114087, -0.14950323637182775, 0.02845558663830161, 0.3793231395906524, -0.23716105646208713, -0.23868695499473497, 0.037715029091525236, -0.26392711692146564, -0.0799938215996678, 0.18362976063385997, 0.0773516145767644... |
709.461 | Minisuperspace dynamics in a generalized uncertainty principle framework | The minisuperspace dynamics of the Friedmann-Robertson-Walker (FRW) and of
the Taub Universes in the context of a Generalized Uncertainty Principle is
analyzed in detail. In particular, the motion of the wave packets is
investigated and, in both the models, the classical singularity appear to be
probabilistic suppres... | gr-qc hep-th | the minisuperspace dynamics of the friedmannrobertsonwalker frw and of the taub universes in the context of a generalized uncertainty principle is analyzed in detail in particular the motion of the wave packets is investigated and in both the models the classical singularity appear to be probabilistic suppressed moreov... | [['the', 'minisuperspace', 'dynamics', 'of', 'the', 'friedmannrobertsonwalker', 'frw', 'and', 'of', 'the', 'taub', 'universes', 'in', 'the', 'context', 'of', 'a', 'generalized', 'uncertainty', 'principle', 'is', 'analyzed', 'in', 'detail', 'in', 'particular', 'the', 'motion', 'of', 'the', 'wave', 'packets', 'is', 'inve... | [-0.16900588291593724, 0.12465537999281272, -0.11798695432436135, 0.15613698127110384, -0.06238925821251339, -0.12328425095830527, -0.0254772909787587, 0.3109205622639921, -0.23405645608695017, -0.20005317797056502, 0.0684995310406925, -0.2675104386315474, -0.1035619020048115, 0.15957890657397608, -0.0107759704118103, ... |
709.4611 | Quantum and classical integrable sine-Gordon model with defect | Defects which are predominant in a realistic model, usually spoil its
integrability or solvability. We on the other hand show the exact integrability
of a known sine-Gordon field model with a defect (DSG), at the classical as
well as at the quantum level based on the Yang-Baxter equation. We find the
associated class... | hep-th cond-mat.stat-mech math-ph math.DS math.MP nlin.SI | defects which are predominant in a realistic model usually spoil its integrability or solvability we on the other hand show the exact integrability of a known sinegordon field model with a defect dsg at the classical as well as at the quantum level based on the yangbaxter equation we find the associated classical and q... | [['defects', 'which', 'are', 'predominant', 'in', 'a', 'realistic', 'model', 'usually', 'spoil', 'its', 'integrability', 'or', 'solvability', 'we', 'on', 'the', 'other', 'hand', 'show', 'the', 'exact', 'integrability', 'of', 'a', 'known', 'sinegordon', 'field', 'model', 'with', 'a', 'defect', 'dsg', 'at', 'the', 'class... | [-0.12541568421758711, 0.10260052160173655, -0.050858504571020605, 0.1056266395105049, -0.057434297166764736, -0.1771135120280087, 0.017922481067478655, 0.329616623416543, -0.2918631590064615, -0.23533637464046478, 0.11160112236533314, -0.27910034483671187, -0.1737224733605981, 0.14108444585371763, 0.017111033126711847... |
709.4612 | Wavelet transform modulus maxima based fractal correlation analysis | The wavelet transform modulus maxima (WTMM) used in the singularity analysis
of one fractal function is extended to study the fractal correlation of two
multifractal functions. The technique is developed in the framework of joint
partition function analysis (JPFA) proposed by Meneveau et al. [1] and is shown
to be eq... | physics.data-an | the wavelet transform modulus maxima wtmm used in the singularity analysis of one fractal function is extended to study the fractal correlation of two multifractal functions the technique is developed in the framework of joint partition function analysis jpfa proposed by meneveau et al 1 and is shown to be equally effe... | [['the', 'wavelet', 'transform', 'modulus', 'maxima', 'wtmm', 'used', 'in', 'the', 'singularity', 'analysis', 'of', 'one', 'fractal', 'function', 'is', 'extended', 'to', 'study', 'the', 'fractal', 'correlation', 'of', 'two', 'multifractal', 'functions', 'the', 'technique', 'is', 'developed', 'in', 'the', 'framework', '... | [-0.049099827172338135, 0.034380234177166846, -0.18245561019069068, 0.12851093972050068, -0.021530748425442496, -0.1120748239753331, -0.020629609003663063, 0.33195397821197536, -0.2574274509938227, -0.2583856998402395, 0.09006577514738626, -0.2537841202237034, -0.2453818043254109, 0.1920565964228669, -0.033609484316620... |
709.4613 | Asteroseismology and Interferometry | Asteroseismology provides us with a unique opportunity to improve our
understanding of stellar structure and evolution. Recent developments,
including the first systematic studies of solar-like pulsators, have boosted
the impact of this field of research within Astrophysics and have led to a
significant increase in t... | astro-ph | asteroseismology provides us with a unique opportunity to improve our understanding of stellar structure and evolution recent developments including the first systematic studies of solarlike pulsators have boosted the impact of this field of research within astrophysics and have led to a significant increase in the siz... | [['asteroseismology', 'provides', 'us', 'with', 'a', 'unique', 'opportunity', 'to', 'improve', 'our', 'understanding', 'of', 'stellar', 'structure', 'and', 'evolution', 'recent', 'developments', 'including', 'the', 'first', 'systematic', 'studies', 'of', 'solarlike', 'pulsators', 'have', 'boosted', 'the', 'impact', 'of... | [-0.06846282654789401, 0.09824795570910563, -0.08043412579251315, 0.025475107245170395, -0.16431908171383006, -0.04149960970682143, 0.07855611831929757, 0.3558095488048608, -0.17182102737674926, -0.35077385511017634, 0.11808111594523076, -0.2901630126500493, -0.14391515276566222, 0.27493487697196617, -0.091635902742368... |
709.4614 | Galaxy Bulges at Mid and High-Redshift | Bulges are a major galaxy component in the nearby universe, and are one of
the primary features that differentiates and defines galaxies. The origin of
bulges can be directly probed in part by examining distant galaxies to search
for high redshift bulges, and to study the properties of bulges in formation.
We review ... | astro-ph | bulges are a major galaxy component in the nearby universe and are one of the primary features that differentiates and defines galaxies the origin of bulges can be directly probed in part by examining distant galaxies to search for high redshift bulges and to study the properties of bulges in formation we review the ev... | [['bulges', 'are', 'a', 'major', 'galaxy', 'component', 'in', 'the', 'nearby', 'universe', 'and', 'are', 'one', 'of', 'the', 'primary', 'features', 'that', 'differentiates', 'and', 'defines', 'galaxies', 'the', 'origin', 'of', 'bulges', 'can', 'be', 'directly', 'probed', 'in', 'part', 'by', 'examining', 'distant', 'gal... | [-0.08592769514200174, 0.126779560050151, -0.07284860112316285, 0.14756337168353437, -0.06629312211233708, -0.05453951723304474, -0.009574274681896592, 0.4468939002085891, -0.1526969574268959, -0.3332946227863431, 0.09017398133033162, -0.2647562749890818, -0.10644688287284225, 0.20065150118168984, -0.009800747083500028... |
709.4615 | Comment on ``Passage Times for Unbiased Polymer Translocation through a
Narrow Pore'' | One of the most fundamental quantities associated with polymer translocation
through a nanopore is the translocation time $\tau$ and its dependence on the
chain length $N$. Our simulation results based on both the bond fluctuation
Monte Carlo and Molecular Dynamics methods confirm the original prediction
$\tau\sim N^... | cond-mat.soft cond-mat.stat-mech | one of the most fundamental quantities associated with polymer translocation through a nanopore is the translocation time tau and its dependence on the chain length n our simulation results based on both the bond fluctuation monte carlo and molecular dynamics methods confirm the original prediction tausim n2nu1 which s... | [['one', 'of', 'the', 'most', 'fundamental', 'quantities', 'associated', 'with', 'polymer', 'translocation', 'through', 'a', 'nanopore', 'is', 'the', 'translocation', 'time', 'tau', 'and', 'its', 'dependence', 'on', 'the', 'chain', 'length', 'n', 'our', 'simulation', 'results', 'based', 'on', 'both', 'the', 'bond', 'fl... | [-0.1256888812008713, 0.16188648262593364, -0.10923643540923617, 0.04617212847972821, 0.009391938203147479, -0.16652127069288067, 0.02807689093585525, 0.35753158325595513, -0.2879934346785636, -0.24776169962382744, 0.08121670283476955, -0.2767991101435785, -0.09365673008640962, 0.2176370654787336, 0.09779286521204215, ... |
709.4616 | Charm | New results on properties and decays of open charm and charmonium states are
reviewed. The emphasis is on examples that illustrate the various aspects
through which studies of charm physics impact the field.
| hep-ex | new results on properties and decays of open charm and charmonium states are reviewed the emphasis is on examples that illustrate the various aspects through which studies of charm physics impact the field | [['new', 'results', 'on', 'properties', 'and', 'decays', 'of', 'open', 'charm', 'and', 'charmonium', 'states', 'are', 'reviewed', 'the', 'emphasis', 'is', 'on', 'examples', 'that', 'illustrate', 'the', 'various', 'aspects', 'through', 'which', 'studies', 'of', 'charm', 'physics', 'impact', 'the', 'field']] | [-0.02165428786115213, 0.21873458298487644, -0.08846706713578015, 0.1507903661924612, -0.06088322739709507, -0.09983331949986292, 0.061650000558460524, 0.3097052288552125, -0.17582905450553604, -0.2158988073016658, 0.11615617415218642, -0.3616561710157178, -0.08967162476796092, 0.2751114381985231, 0.042538284013668694,... |
709.4617 | $C^*$-pseudo-Kac systems and duality for coactions of concrete Hopf
$C^*$-bimodules | We study coactions of concrete Hopf $C^{*}$-bimodules in the framework of
(weak) $C^{*}$-pseudo-Kac systems, define reduced crossed products and dual
coactions, and prove an analogue of Baaj-Skandalis duality.
| math.OA | we study coactions of concrete hopf cbimodules in the framework of weak cpseudokac systems define reduced crossed products and dual coactions and prove an analogue of baajskandalis duality | [['we', 'study', 'coactions', 'of', 'concrete', 'hopf', 'cbimodules', 'in', 'the', 'framework', 'of', 'weak', 'cpseudokac', 'systems', 'define', 'reduced', 'crossed', 'products', 'and', 'dual', 'coactions', 'and', 'prove', 'an', 'analogue', 'of', 'baajskandalis', 'duality']] | [-0.21610670930777603, 0.07469656764890086, -0.07279031874182132, 0.11040547404151696, -0.06908633559942245, -0.12474392297176215, -0.019480860147338647, 0.34235235317968404, -0.40064261423853725, -0.1346677549255009, 0.13180169753748208, -0.16397003170389396, -0.1849593093009809, 0.18742504286078307, -0.18580080117457... |
709.4618 | The deformation of the Whitham systems in the almost linear case | We consider the deformation of the Whitham systems in the case when the
initial system is close to linear one. It appears that the deformation
procedure should be modified in this special case to make all the constructions
stable in the linear limit. We suggest here the special deformation scheme
which gives the stab... | nlin.SI | we consider the deformation of the whitham systems in the case when the initial system is close to linear one it appears that the deformation procedure should be modified in this special case to make all the constructions stable in the linear limit we suggest here the special deformation scheme which gives the stable d... | [['we', 'consider', 'the', 'deformation', 'of', 'the', 'whitham', 'systems', 'in', 'the', 'case', 'when', 'the', 'initial', 'system', 'is', 'close', 'to', 'linear', 'one', 'it', 'appears', 'that', 'the', 'deformation', 'procedure', 'should', 'be', 'modified', 'in', 'this', 'special', 'case', 'to', 'make', 'all', 'the',... | [-0.17104225178750662, 0.08384588127239392, -0.0917375632848304, 0.05544579216780571, -0.021380613507846227, -0.14765878196519155, -0.02197185712866485, 0.30856120703885187, -0.33224416203223744, -0.19228122371893663, 0.12393193748743775, -0.19428868437759006, -0.20077305510640145, 0.21229516743467405, -0.0944335148025... |
709.4619 | Gauge-invariant coherent states for Loop Quantum Gravity I: Abelian
gauge groups | In this paper we investigate the properties of gauge-invariant coherent
states for Loop Quantum Gravity, for the gauge group U(1). This is done by
projecting the corresponding complexifier coherent states, which have been
applied in numerous occasions to investigate the semiclassical limit of the
kinematical sector, ... | gr-qc | in this paper we investigate the properties of gaugeinvariant coherent states for loop quantum gravity for the gauge group u1 this is done by projecting the corresponding complexifier coherent states which have been applied in numerous occasions to investigate the semiclassical limit of the kinematical sector to the ga... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'properties', 'of', 'gaugeinvariant', 'coherent', 'states', 'for', 'loop', 'quantum', 'gravity', 'for', 'the', 'gauge', 'group', 'u1', 'this', 'is', 'done', 'by', 'projecting', 'the', 'corresponding', 'complexifier', 'coherent', 'states', 'which', 'have', 'been', 'ap... | [-0.14878112025489318, 0.17776598309049227, -0.13469113675424846, 0.11844276042141577, -0.06935412878449136, -0.07626607019680544, 0.03312270810814557, 0.3279131549088476, -0.26506126403947855, -0.2438774480153676, 0.05708650800521337, -0.23453508337272036, -0.10659902449479658, 0.10971242025773102, -0.0388894450903008... |
709.462 | Mott transition in one dimension: Benchmarking dynamical cluster
approaches | The variational cluster approach (VCA) is applied to the one-dimensional
Hubbard model at zero temperature using clusters (chains) of up to ten sites
with full diagonalization and the Lanczos method as cluster solver. Within the
framework of the self-energy-functional theory (SFT), different cluster
reference systems... | cond-mat.str-el cond-mat.supr-con | the variational cluster approach vca is applied to the onedimensional hubbard model at zero temperature using clusters chains of up to ten sites with full diagonalization and the lanczos method as cluster solver within the framework of the selfenergyfunctional theory sft different cluster reference systems with and wit... | [['the', 'variational', 'cluster', 'approach', 'vca', 'is', 'applied', 'to', 'the', 'onedimensional', 'hubbard', 'model', 'at', 'zero', 'temperature', 'using', 'clusters', 'chains', 'of', 'up', 'to', 'ten', 'sites', 'with', 'full', 'diagonalization', 'and', 'the', 'lanczos', 'method', 'as', 'cluster', 'solver', 'within... | [-0.09112582299281406, 0.0925390954084068, -0.07915873130766955, 0.07261993732319864, -0.006244576880213829, -0.15063286202071663, 0.09864241658685217, 0.3703877738042347, -0.2477159706702604, -0.3039399953950526, 0.06846750622297909, -0.29348800023111093, -0.10988907818373425, 0.1575472009997257, 0.08310831028584853, ... |
709.4621 | H.E.S.S. observations of the supernova remnant RX J0852.0-4622 | The shell-type supernova remnant RX J0852.0-4622 was detected in 2004 and
re-observed between December 2004 and May 2005 with the High Energy
Stereoscopic System (H.E.S.S.), an array of four Imaging Cherenkov Telescopes
located in Namibia and dedicated to the observations of gamma-rays above 100
GeV. The angular reso... | astro-ph | the shelltype supernova remnant rx j085204622 was detected in 2004 and reobserved between december 2004 and may 2005 with the high energy stereoscopic system hess an array of four imaging cherenkov telescopes located in namibia and dedicated to the observations of gammarays above 100 gev the angular resolution of 01 de... | [['the', 'shelltype', 'supernova', 'remnant', 'rx', 'j085204622', 'was', 'detected', 'in', '2004', 'and', 'reobserved', 'between', 'december', '2004', 'and', 'may', '2005', 'with', 'the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'an', 'array', 'of', 'four', 'imaging', 'cherenkov', 'telescopes', 'located', 'i... | [-0.0694876337197217, 0.1678174039553644, -0.04647027160765566, 0.1314754597789081, -0.07163159670553317, -0.10155482628761092, -0.012557998961327891, 0.4299958963682385, -0.22116685102044262, -0.41199768054004954, 0.05862033872567975, -0.3099389010213168, 0.02898843653996377, 0.19883287196678698, 0.026889301033071734,... |
709.4622 | Dynamics and Hadronization at intermediate transverse momentum at RHIC | The ultra-relativistic heavy-ion program at RHIC has shown that at
intermediate transverse momenta ($p_T \simeq 2$-6 GeV) standard (independent)
parton fragmentation can neither describe the observed baryon-to-meson ratios
nor the empirical scaling of the hadronic elliptic flow ($v_2$) according to
the number of vale... | hep-ph | the ultrarelativistic heavyion program at rhic has shown that at intermediate transverse momenta p_t simeq 26 gev standard independent parton fragmentation can neither describe the observed baryontomeson ratios nor the empirical scaling of the hadronic elliptic flow v_2 according to the number of valence quarks both as... | [['the', 'ultrarelativistic', 'heavyion', 'program', 'at', 'rhic', 'has', 'shown', 'that', 'at', 'intermediate', 'transverse', 'momenta', 'p_t', 'simeq', '26', 'gev', 'standard', 'independent', 'parton', 'fragmentation', 'can', 'neither', 'describe', 'the', 'observed', 'baryontomeson', 'ratios', 'nor', 'the', 'empirica... | [-0.039271580115516964, 0.2700477417045892, -0.19700534727843166, 0.15112148536347328, -0.032367601961009955, -0.06630697129481791, -0.012774452485844193, 0.3545059098943368, -0.19370046405484212, -0.24391641288420698, -0.07557191206736102, -0.2941825355953168, 0.02456871618910524, 0.12634199211972996, 0.05766784823062... |
709.4623 | Low energy polarization sensitivity of the Gas Pixel Detector | An X-ray photoelectric polarimeter based on the Gas Pixel Detector has been
proposed to be included in many upcoming space missions to fill the gap of
about 30 years from the first (and to date only) positive measurement of
polarized X-ray emission from an astrophysical source. The estimated
sensitivity of the curren... | astro-ph | an xray photoelectric polarimeter based on the gas pixel detector has been proposed to be included in many upcoming space missions to fill the gap of about 30 years from the first and to date only positive measurement of polarized xray emission from an astrophysical source the estimated sensitivity of the current proto... | [['an', 'xray', 'photoelectric', 'polarimeter', 'based', 'on', 'the', 'gas', 'pixel', 'detector', 'has', 'been', 'proposed', 'to', 'be', 'included', 'in', 'many', 'upcoming', 'space', 'missions', 'to', 'fill', 'the', 'gap', 'of', 'about', '30', 'years', 'from', 'the', 'first', 'and', 'to', 'date', 'only', 'positive', '... | [-0.024236738814226923, 0.12236360980282616, -0.04870302231924594, 0.02559921637361566, -0.01856308148960879, -0.08506243256491053, 0.037480170949535485, 0.44830790047295566, -0.21030634421811895, -0.37357016156974443, 0.08810655350296924, -0.3518024265004481, 0.02190864456604531, 0.23192751667572387, -0.00355020876750... |
709.4624 | Leptogenesis with exclusively low-energy CP Violation in the Context of
Minimal Lepton Flavour Violation | We analyze lepton flavour violation (LFV) and the generation of the observed
baryon-antibaryon asymmetry of the Universe (BAU) within a generalized minimal
lepton flavour violation framework with three quasi-degenerate heavy Majorana
neutrinos. The BAU which is obtained through radiative resonant leptogenesis
can suc... | hep-ph | we analyze lepton flavour violation lfv and the generation of the observed baryonantibaryon asymmetry of the universe bau within a generalized minimal lepton flavour violation framework with three quasidegenerate heavy majorana neutrinos the bau which is obtained through radiative resonant leptogenesis can successfully... | [['we', 'analyze', 'lepton', 'flavour', 'violation', 'lfv', 'and', 'the', 'generation', 'of', 'the', 'observed', 'baryonantibaryon', 'asymmetry', 'of', 'the', 'universe', 'bau', 'within', 'a', 'generalized', 'minimal', 'lepton', 'flavour', 'violation', 'framework', 'with', 'three', 'quasidegenerate', 'heavy', 'majorana... | [-0.12386585118249059, 0.3011108208575752, 0.010289782057516277, 0.194284563283436, -0.07409408334642649, -0.1971142499265261, 0.06248106872255448, 0.2535510989278555, -0.23784416902810335, -0.2858401289000176, 0.024720847392454743, -0.25344303451944145, -0.0191901639662683, 0.1012811980699189, 0.07225702579831704, 0.0... |
709.4625 | Transversity Measurements at COMPASS | The measurement of transverse spin effects in semi-inclusive deep-inelastic
scattering is an important part of the COMPASS physics program. From the
analysis of the 2002-2004 data, new results for the transverse target spin
asymmetry of z-ordered identified pion and kaon pairs are presented. In
addition, a first resu... | hep-ex | the measurement of transverse spin effects in semiinclusive deepinelastic scattering is an important part of the compass physics program from the analysis of the 20022004 data new results for the transverse target spin asymmetry of zordered identified pion and kaon pairs are presented in addition a first result for the... | [['the', 'measurement', 'of', 'transverse', 'spin', 'effects', 'in', 'semiinclusive', 'deepinelastic', 'scattering', 'is', 'an', 'important', 'part', 'of', 'the', 'compass', 'physics', 'program', 'from', 'the', 'analysis', 'of', 'the', '20022004', 'data', 'new', 'results', 'for', 'the', 'transverse', 'target', 'spin', ... | [-0.08237145334437844, 0.24072456980952883, -0.12006029684747023, 0.14466584716657443, -0.032356971978313394, -0.03753870095880259, -0.04807726169625918, 0.3149467060371997, -0.1926659259091442, -0.2019731762804209, -0.054482582258060575, -0.3517960686650541, 0.03753887589961764, 0.19950003093404192, 0.1234703054651618... |
709.4626 | Global regularity for a Birkhoff-Rott-alpha approximation of the
dynamics of vortex sheets of the 2D Euler equations | We present an alpha-regularization of the Birkhoff-Rott equation, induced by
the two-dimensional Euler-alpha equations, for the vortex sheet dynamics. We
show that initially smooth self-avoiding vortex sheet remains smooth for all
times under the alpha-regularized dynamics, provided the initial density of
vorticity i... | math.AP | we present an alpharegularization of the birkhoffrott equation induced by the twodimensional euleralpha equations for the vortex sheet dynamics we show that initially smooth selfavoiding vortex sheet remains smooth for all times under the alpharegularized dynamics provided the initial density of vorticity is an integra... | [['we', 'present', 'an', 'alpharegularization', 'of', 'the', 'birkhoffrott', 'equation', 'induced', 'by', 'the', 'twodimensional', 'euleralpha', 'equations', 'for', 'the', 'vortex', 'sheet', 'dynamics', 'we', 'show', 'that', 'initially', 'smooth', 'selfavoiding', 'vortex', 'sheet', 'remains', 'smooth', 'for', 'all', 't... | [-0.19494378925724462, 0.12362682284755548, -0.08806785839525136, 0.0012834135040810163, -0.001028152411295609, -0.06930846842852506, -0.09103557801466775, 0.3577370699325746, -0.3017248698086901, -0.14928136704680087, 0.07928045329383829, -0.24642705299298873, -0.14174002552066337, 0.20546212607825345, -0.023408585482... |
709.4627 | Statistical analysis of neutrino events from SN1987A neutrino burst:
estimation of the electron antineutrino mass | The method of the statistical sample moments was used for the analysis of
neutrino events from SN1987A burst in Cherenkov detectors. In particular the
coefficients of correlation $Q(E,t)$ between the energies $E$ of electron
antineutrinos $\bar \nu_e$ emitted by star and the ejection instants $t$ of
$\bar \nu_e$ for ... | astro-ph | the method of the statistical sample moments was used for the analysis of neutrino events from sn1987a burst in cherenkov detectors in particular the coefficients of correlation qet between the energies e of electron antineutrinos bar nu_e emitted by star and the ejection instants t of bar nu_e for neutrino events reco... | [['the', 'method', 'of', 'the', 'statistical', 'sample', 'moments', 'was', 'used', 'for', 'the', 'analysis', 'of', 'neutrino', 'events', 'from', 'sn1987a', 'burst', 'in', 'cherenkov', 'detectors', 'in', 'particular', 'the', 'coefficients', 'of', 'correlation', 'qet', 'between', 'the', 'energies', 'e', 'of', 'electron',... | [-0.05696743958452273, 0.2192049050397708, -0.047777254483662546, 0.16857269438454145, 0.008236996487193253, -0.10024332648442526, 0.03736377453121046, 0.2996654373904069, -0.1696583584333504, -0.32165303867250694, -0.001002413716161668, -0.34382868999437916, 0.0002962378913209596, 0.18821631476471556, 0.02238510054857... |
709.4628 | Precision Lattice Calculation of D and Ds decay constants | We present a determination of the decay constants of the $D$ and $D_s$ mesons
from lattice QCD, each with a total error of about 2%, approximately a factor
of three better than previous calculations. We have been able to achieve this
through the use of a highly improved discretization of QCD for charm quarks,
coupled... | hep-lat | we present a determination of the decay constants of the d and d_s mesons from lattice qcd each with a total error of about 2 approximately a factor of three better than previous calculations we have been able to achieve this through the use of a highly improved discretization of qcd for charm quarks coupled to gauge c... | [['we', 'present', 'a', 'determination', 'of', 'the', 'decay', 'constants', 'of', 'the', 'd', 'and', 'd_s', 'mesons', 'from', 'lattice', 'qcd', 'each', 'with', 'a', 'total', 'error', 'of', 'about', '2', 'approximately', 'a', 'factor', 'of', 'three', 'better', 'than', 'previous', 'calculations', 'we', 'have', 'been', 'a... | [-0.036827279568902534, 0.2020349250843737, -0.09083659716785272, 0.05552831241327179, -0.038544432586626855, -0.1016706753516479, 0.13263564313784604, 0.3658743334718321, -0.1465562065699842, -0.2830474558627097, 0.041320576592314445, -0.3089636317738218, 0.00040322686006065184, 0.14398253019246068, 0.0603211650670301... |
709.4629 | Scanning tunneling spectroscopy with superconducting tips of Al | We present Scanning Tunneling Spectroscopy measurements at 0.1 K using tips
made of Al. At zero field, the atomic lattice and charge density wave of
2HNbSe2 are observed, and under magnetic fields the peculiar electronic surface
properties of vortices are precisely resolved. The tip density of states is
influenced by... | cond-mat.supr-con cond-mat.str-el | we present scanning tunneling spectroscopy measurements at 01 k using tips made of al at zero field the atomic lattice and charge density wave of 2hnbse2 are observed and under magnetic fields the peculiar electronic surface properties of vortices are precisely resolved the tip density of states is influenced by the lo... | [['we', 'present', 'scanning', 'tunneling', 'spectroscopy', 'measurements', 'at', '01', 'k', 'using', 'tips', 'made', 'of', 'al', 'at', 'zero', 'field', 'the', 'atomic', 'lattice', 'and', 'charge', 'density', 'wave', 'of', '2hnbse2', 'are', 'observed', 'and', 'under', 'magnetic', 'fields', 'the', 'peculiar', 'electroni... | [-0.1970087471620544, 0.23372430382701365, -0.0722666634719117, 0.002804940223923304, -0.011916189764936766, -0.09146055365251242, 0.04219911220159544, 0.39059872671529866, -0.257772596552968, -0.34033995069077483, 0.013563081912318434, -0.27780759739487065, -0.043212765503836716, 0.1782962266546404, 0.0895394092911611... |
709.463 | Domain-wall and overlap fermions at nonzero quark chemical potential | We have recently given a construction of the overlap Dirac operator at
nonzero quark chemical potential. Here, we introduce a quark chemical potential
in the domain-wall fermion formalism and show that our earlier result is
reproduced if the extent of the fifth dimension is taken to infinity and its
lattice spacing i... | hep-lat | we have recently given a construction of the overlap dirac operator at nonzero quark chemical potential here we introduce a quark chemical potential in the domainwall fermion formalism and show that our earlier result is reproduced if the extent of the fifth dimension is taken to infinity and its lattice spacing is tak... | [['we', 'have', 'recently', 'given', 'a', 'construction', 'of', 'the', 'overlap', 'dirac', 'operator', 'at', 'nonzero', 'quark', 'chemical', 'potential', 'here', 'we', 'introduce', 'a', 'quark', 'chemical', 'potential', 'in', 'the', 'domainwall', 'fermion', 'formalism', 'and', 'show', 'that', 'our', 'earlier', 'result'... | [-0.1198903573050092, 0.18385054459437156, -0.10674846585103435, 0.06733846655697562, -0.044587486078783586, -0.09010130988183217, 0.10695286154245529, 0.3601416793759339, -0.22203014488331974, -0.24658956156613734, 0.02928149736656521, -0.2681454734590191, -0.11915755872122155, 0.08342050975233388, -0.0085662135567802... |
709.4631 | Dynamics of the triple contact line on a non-isothermal heater at
partial wetting | The dynamics of the triple gas-liquid-solid contact line is analysed for the
case where the gas is the saturated vapour corresponding to the liquid, like in
the vapour bubble in boiling. It is shown that even small superheating (with
respect to the saturation temperature) causes evaporation of the adsorption
liquid f... | cond-mat.soft | the dynamics of the triple gasliquidsolid contact line is analysed for the case where the gas is the saturated vapour corresponding to the liquid like in the vapour bubble in boiling it is shown that even small superheating with respect to the saturation temperature causes evaporation of the adsorption liquid film and ... | [['the', 'dynamics', 'of', 'the', 'triple', 'gasliquidsolid', 'contact', 'line', 'is', 'analysed', 'for', 'the', 'case', 'where', 'the', 'gas', 'is', 'the', 'saturated', 'vapour', 'corresponding', 'to', 'the', 'liquid', 'like', 'in', 'the', 'vapour', 'bubble', 'in', 'boiling', 'it', 'is', 'shown', 'that', 'even', 'smal... | [-0.11675034025635493, 0.13380979499544038, -0.0596858450742383, 0.019753989916699494, -0.03932725283638796, -0.17428245222739255, 0.022873974596482834, 0.3592724926614513, -0.2586264849454719, -0.271834215993641, 0.12691129858458658, -0.26587835597317844, -0.10851670635470544, 0.17235962985155528, -0.03756226724796024... |
709.4632 | N=1 4D Supermembrane from 11D | The action of the 11D supermembrane with nontrivial central charges
compactified on a 7D toroidal manifold is obtained. It describes a
supermembrane evolving in a 4d Minkowski space-time. The action is invariant
under additional symmetries in comparison to the supermembrane on a Minkowski
target space. The hamiltonia... | hep-th | the action of the 11d supermembrane with nontrivial central charges compactified on a 7d toroidal manifold is obtained it describes a supermembrane evolving in a 4d minkowski spacetime the action is invariant under additional symmetries in comparison to the supermembrane on a minkowski target space the hamiltonian in t... | [['the', 'action', 'of', 'the', '11d', 'supermembrane', 'with', 'nontrivial', 'central', 'charges', 'compactified', 'on', 'a', '7d', 'toroidal', 'manifold', 'is', 'obtained', 'it', 'describes', 'a', 'supermembrane', 'evolving', 'in', 'a', '4d', 'minkowski', 'spacetime', 'the', 'action', 'is', 'invariant', 'under', 'add... | [-0.17938556655069754, 0.18075829004749633, -0.09259026448407601, 0.08302701474449056, -0.10744860310918622, -0.1331776119130213, -0.08423572657780061, 0.3399873514370542, -0.17569880636649265, -0.20966688339549658, 0.09602590992055353, -0.26236905423443646, -0.11188909007356532, 0.08201173127388521, -0.137757046320926... |
709.4633 | SUSY Associated Vector Coherent States and Generalized Landau Levels
Arising From 2-dimensional SUSY | We describe a method for constructing vector coherent states for quantum
supersymmetric partner Hamiltonians. The method is then applied to such partner
Hamiltonians arising from a generalization of the fractional quantum Hall
effect. Explicit examples are worked out.
| math-ph math.MP | we describe a method for constructing vector coherent states for quantum supersymmetric partner hamiltonians the method is then applied to such partner hamiltonians arising from a generalization of the fractional quantum hall effect explicit examples are worked out | [['we', 'describe', 'a', 'method', 'for', 'constructing', 'vector', 'coherent', 'states', 'for', 'quantum', 'supersymmetric', 'partner', 'hamiltonians', 'the', 'method', 'is', 'then', 'applied', 'to', 'such', 'partner', 'hamiltonians', 'arising', 'from', 'a', 'generalization', 'of', 'the', 'fractional', 'quantum', 'hal... | [-0.07282814059994723, 0.17074736876805363, -0.07236551035097555, 0.1472976372828462, -0.0883165167546586, -0.22780306237798773, 0.02028976264409721, 0.33531212801799964, -0.25597645018837956, -0.2429988086958857, 0.04692026219747372, -0.2763396456077891, -0.21985998973985643, 0.2639309446278371, -0.019529963304337702,... |
709.4634 | Lepton mass effects in weak CC single pion production | Different approaches to take into account nonzero lepton mass in the
Rein-Sehgal model are compared. Modification of the axial current due to pion
pole term are included and it is shown that they lead to large reduction of
antineutrino cross section and a change of the shape of $d\sigma/dQ^2$.
| hep-ph | different approaches to take into account nonzero lepton mass in the reinsehgal model are compared modification of the axial current due to pion pole term are included and it is shown that they lead to large reduction of antineutrino cross section and a change of the shape of dsigmadq2 | [['different', 'approaches', 'to', 'take', 'into', 'account', 'nonzero', 'lepton', 'mass', 'in', 'the', 'reinsehgal', 'model', 'are', 'compared', 'modification', 'of', 'the', 'axial', 'current', 'due', 'to', 'pion', 'pole', 'term', 'are', 'included', 'and', 'it', 'is', 'shown', 'that', 'they', 'lead', 'to', 'large', 'r... | [-0.06350273222481946, 0.15466518069104274, -0.07450266174820004, 0.13993853082813854, -0.04756064857451283, -0.11721306981290786, -0.011424939746835403, 0.33128954941520883, -0.19333077332347023, -0.28923200348354117, 0.003431684705808911, -0.31270918150774524, -0.040818478531983435, 0.15509991659022562, -0.0071641801... |
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