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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707.333 | Extended Air Shower Simulations Based on EPOS | We discuss air shower simulations based on the EPOS hadronic interaction
model.
A remarkable feature is the fact that the number of produced muons is
considerably larger compared to other interaction models. We show that this is
due to an improved treatment of baryon-antibaryon production.
| astro-ph hep-ph | we discuss air shower simulations based on the epos hadronic interaction model a remarkable feature is the fact that the number of produced muons is considerably larger compared to other interaction models we show that this is due to an improved treatment of baryonantibaryon production | [['we', 'discuss', 'air', 'shower', 'simulations', 'based', 'on', 'the', 'epos', 'hadronic', 'interaction', 'model', 'a', 'remarkable', 'feature', 'is', 'the', 'fact', 'that', 'the', 'number', 'of', 'produced', 'muons', 'is', 'considerably', 'larger', 'compared', 'to', 'other', 'interaction', 'models', 'we', 'show', 't... | [-0.07110803433073064, 0.19389706339150306, -0.11028824297504293, 0.11428559229502247, -0.02275157504611545, -0.05998927156130473, -0.05516069712660586, 0.39484725031587814, -0.1981540232896805, -0.31879305462870333, -0.026213582791388034, -0.3423227411798305, -0.07771615162491799, 0.1863319574907008, 0.012652073805737... |
707.3331 | On positivity of quantum measure and of effective action in area tensor
Regge calculus | Because of unboundedness of the general relativity action, Euclidean version
of the path integral in general relativity requires definition. Area tensor
Regge calculus is considered in the representation with independent area tensor
and finite rotation matrices. Being integrated over rotation matrices the path
integr... | hep-th gr-qc | because of unboundedness of the general relativity action euclidean version of the path integral in general relativity requires definition area tensor regge calculus is considered in the representation with independent area tensor and finite rotation matrices being integrated over rotation matrices the path integral me... | [['because', 'of', 'unboundedness', 'of', 'the', 'general', 'relativity', 'action', 'euclidean', 'version', 'of', 'the', 'path', 'integral', 'in', 'general', 'relativity', 'requires', 'definition', 'area', 'tensor', 'regge', 'calculus', 'is', 'considered', 'in', 'the', 'representation', 'with', 'independent', 'area', '... | [-0.13426022115403535, 0.10939821023878056, -0.11287803024284004, 0.07831592206151906, -0.12865763537816166, -0.09594494271447364, -0.06260053496045713, 0.3432075453480494, -0.27939951837125243, -0.2754201500714977, 0.12019515107505829, -0.2597358291968703, -0.1711722401921282, 0.14919104737220043, -0.11447242415538922... |
707.3332 | Elliptic flow of deuterons in relativistic heavy-ion collisions | Using a dynamical model based on the $NN \to d\pi$, $NNN \to dN$, and $NN\pi
\to d\pi$ reactions and measured proton and pion transverse momentum spectra
and elliptic flows, we study the production of deuterons and their elliptic
flow in heavy ion collisions at RHIC. The results are compared with those from
the coale... | nucl-th hep-ph | using a dynamical model based on the nn to dpi nnn to dn and nnpi to dpi reactions and measured proton and pion transverse momentum spectra and elliptic flows we study the production of deuterons and their elliptic flow in heavy ion collisions at rhic the results are compared with those from the coalescence model the d... | [['using', 'a', 'dynamical', 'model', 'based', 'on', 'the', 'nn', 'to', 'dpi', 'nnn', 'to', 'dn', 'and', 'nnpi', 'to', 'dpi', 'reactions', 'and', 'measured', 'proton', 'and', 'pion', 'transverse', 'momentum', 'spectra', 'and', 'elliptic', 'flows', 'we', 'study', 'the', 'production', 'of', 'deuterons', 'and', 'their', '... | [-0.05119296143327475, 0.2116908289330161, -0.12616059068165233, 0.10140690685290357, 0.001608812675365935, -0.08566903583414387, 0.008368707849117725, 0.3330215584770169, -0.24170218808981386, -0.2602292254931577, -0.029690994743166655, -0.4239146895909115, 0.022181406758887613, 0.17004863484813224, 0.0830125041893157... |
707.3333 | Hamiltonian Dynamics of Linearly Polarized Gowdy Models Coupled to
Massless Scalar Fields | The purpose of this paper is to analyze in detail the Hamiltonian formulation
for the compact Gowdy models coupled to massless scalar fields as a necessary
first step towards their quantization. We will pay special attention to the
coupling of matter and those features that arise for the three-handle and
three-sphere... | gr-qc | the purpose of this paper is to analyze in detail the hamiltonian formulation for the compact gowdy models coupled to massless scalar fields as a necessary first step towards their quantization we will pay special attention to the coupling of matter and those features that arise for the threehandle and threesphere topo... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'analyze', 'in', 'detail', 'the', 'hamiltonian', 'formulation', 'for', 'the', 'compact', 'gowdy', 'models', 'coupled', 'to', 'massless', 'scalar', 'fields', 'as', 'a', 'necessary', 'first', 'step', 'towards', 'their', 'quantization', 'we', 'will', 'pay', 'special',... | [-0.1271311091213912, 0.08537689027123863, -0.09125069408874764, 0.09823177798280439, -0.08237908317400053, -0.10612986033592482, -0.021870380406521117, 0.3615246155724219, -0.2176427313859023, -0.2784749061881917, 0.12020177491917954, -0.23601655095354518, -0.17907971298114117, 0.16794821663388929, -0.0536515173129885... |
707.3334 | Dark matter annihilation near a black hole: plateau vs. weak cusp | Dark matter annihilation in so-called ``spikes'' near black holes is believed
to be an important method of indirect dark matter detection. In the case of
circular particle orbits, the density profile of dark matter has a plateau at
small radii, the maximal density being limited by the annihilation
cross-section. Howe... | astro-ph | dark matter annihilation in socalled spikes near black holes is believed to be an important method of indirect dark matter detection in the case of circular particle orbits the density profile of dark matter has a plateau at small radii the maximal density being limited by the annihilation crosssection however in the g... | [['dark', 'matter', 'annihilation', 'in', 'socalled', 'spikes', 'near', 'black', 'holes', 'is', 'believed', 'to', 'be', 'an', 'important', 'method', 'of', 'indirect', 'dark', 'matter', 'detection', 'in', 'the', 'case', 'of', 'circular', 'particle', 'orbits', 'the', 'density', 'profile', 'of', 'dark', 'matter', 'has', '... | [-0.13119854791284197, 0.1606314348464366, -0.11766387177497256, 0.13600884681808756, -0.07119877058711144, -0.0924521505785771, -0.052307715270963076, 0.32199816602757936, -0.2104298032337813, -0.3141859149989143, 0.03483308962271582, -0.2843327160603065, -0.03041872400589448, 0.2140697635075399, 0.006570555072521398,... |
707.3335 | Molecular gas in QSO host galaxies at z>5 | We present observations with the IRAM Plateau de Bure Interferometer of three
QSOs at z>5 aimed at detecting molecular gas in their host galaxies as traced
by CO transitions. CO (5-4) is detected in SDSSJ033829.31+002156.3 at z=5.0267,
placing it amongst the most distant sources detected in CO. The CO emission is
unr... | astro-ph | we present observations with the iram plateau de bure interferometer of three qsos at z5 aimed at detecting molecular gas in their host galaxies as traced by co transitions co 54 is detected in sdssj033829310021563 at z50267 placing it amongst the most distant sources detected in co the co emission is unresolved with a... | [['we', 'present', 'observations', 'with', 'the', 'iram', 'plateau', 'de', 'bure', 'interferometer', 'of', 'three', 'qsos', 'at', 'z5', 'aimed', 'at', 'detecting', 'molecular', 'gas', 'in', 'their', 'host', 'galaxies', 'as', 'traced', 'by', 'co', 'transitions', 'co', '54', 'is', 'detected', 'in', 'sdssj033829310021563'... | [-0.06276383759541204, 0.09008578295078858, 0.006683301360515708, 0.11213546611631472, -0.039649884665391946, -0.07024227718956712, 0.07071184634873079, 0.4249402455153, -0.12457244510270274, -0.3359704181114494, 0.07136399371754096, -0.30374085247185023, 0.026591482170977433, 0.18810670660759293, 0.035106474770696935,... |
707.3336 | Statistical mechanical analysis of the linear vector channel in digital
communication | A statistical mechanical framework to analyze linear vector channel models in
digital wireless communication is proposed for a large system. The framework is
a generalization of that proposed for code-division multiple-access systems in
Europhys. Lett. 76 (2006) 1193 and enables the analysis of the system in which
th... | cs.IT cond-mat.dis-nn cond-mat.stat-mech math.IT | a statistical mechanical framework to analyze linear vector channel models in digital wireless communication is proposed for a large system the framework is a generalization of that proposed for codedivision multipleaccess systems in europhys lett 76 2006 1193 and enables the analysis of the system in which the element... | [['a', 'statistical', 'mechanical', 'framework', 'to', 'analyze', 'linear', 'vector', 'channel', 'models', 'in', 'digital', 'wireless', 'communication', 'is', 'proposed', 'for', 'a', 'large', 'system', 'the', 'framework', 'is', 'a', 'generalization', 'of', 'that', 'proposed', 'for', 'codedivision', 'multipleaccess', 's... | [-0.19414819392697585, -0.0066265610697388904, -0.02634954776752878, -0.043074815294038456, 0.008355133867834085, -0.2013220022558982, 0.04337462705537033, 0.3315219530766761, -0.22521489282155893, -0.2851377336860255, 0.05730301141307724, -0.254861652109496, -0.2125765440157718, 0.21289845585627595, -0.115072363907080... |
707.3337 | On The Capacity of Surfaces in Manifolds with Nonnegative Scalar
Curvature | Given a surface in an asymptotically flat 3-manifold with nonnegative scalar
curvature, we derive an upper bound for the capacity of the surface in terms of
the area of the surface and the Willmore functional of the surface. The
capacity of a surface is defined to be the energy of the harmonic function
which equals 0... | math.DG gr-qc | given a surface in an asymptotically flat 3manifold with nonnegative scalar curvature we derive an upper bound for the capacity of the surface in terms of the area of the surface and the willmore functional of the surface the capacity of a surface is defined to be the energy of the harmonic function which equals 0 on t... | [['given', 'a', 'surface', 'in', 'an', 'asymptotically', 'flat', '3manifold', 'with', 'nonnegative', 'scalar', 'curvature', 'we', 'derive', 'an', 'upper', 'bound', 'for', 'the', 'capacity', 'of', 'the', 'surface', 'in', 'terms', 'of', 'the', 'area', 'of', 'the', 'surface', 'and', 'the', 'willmore', 'functional', 'of', ... | [-0.14993843984460303, 0.10859266035477048, -0.08407005799623828, 0.08940335570077877, -0.04103991480078548, -0.12809060066550348, 0.0212558905860836, 0.28528330971021204, -0.21687417759676464, -0.2805521966637267, 0.10695230980636553, -0.288051914635192, -0.12307634149959389, 0.20604794107881996, -0.11497525768354536,... |
707.3338 | Phase coherence, inelastic scattering, and interaction corrections in
pumping through quantum dots | Adiabatic quantum pumping in noninteracting, phase coherent quantum dots is
elegantly described by Brouwer's formula. Interactions within the dot, while
suppressing phase coherence, make Brouwer's formalism inapplicable. In this
paper, we discuss the nature of the physical processes forcing a description of
pumping b... | cond-mat.mes-hall | adiabatic quantum pumping in noninteracting phase coherent quantum dots is elegantly described by brouwers formula interactions within the dot while suppressing phase coherence make brouwers formalism inapplicable in this paper we discuss the nature of the physical processes forcing a description of pumping beyond brou... | [['adiabatic', 'quantum', 'pumping', 'in', 'noninteracting', 'phase', 'coherent', 'quantum', 'dots', 'is', 'elegantly', 'described', 'by', 'brouwers', 'formula', 'interactions', 'within', 'the', 'dot', 'while', 'suppressing', 'phase', 'coherence', 'make', 'brouwers', 'formalism', 'inapplicable', 'in', 'this', 'paper', ... | [-0.18144512684643269, 0.17493733497709035, -0.11546240596938878, 0.08556740406900644, 0.013927239060401917, -0.14055478060618043, 0.10986786287475843, 0.2973084504697472, -0.25751705772802236, -0.24608223950490354, 0.006992613305337727, -0.25148519460111857, -0.11082624915242195, 0.16728033390641212, -0.00870428654551... |
707.3339 | Non-real zeros of linear differential polynomials | Lower bounds are given for the number of non-real zeros of a second order
linear differential polynomial with constant coefficients in a real entire
function with finitely many non-real zeros.
| math.CV | lower bounds are given for the number of nonreal zeros of a second order linear differential polynomial with constant coefficients in a real entire function with finitely many nonreal zeros | [['lower', 'bounds', 'are', 'given', 'for', 'the', 'number', 'of', 'nonreal', 'zeros', 'of', 'a', 'second', 'order', 'linear', 'differential', 'polynomial', 'with', 'constant', 'coefficients', 'in', 'a', 'real', 'entire', 'function', 'with', 'finitely', 'many', 'nonreal', 'zeros']] | [-0.23763418352852264, 0.07843541440864404, -0.016702740848995746, 0.03155521669735511, -0.16245185397565365, -0.12569850146149594, -0.02601859870677193, 0.24411562051003177, -0.26590933625896773, -0.26830389311847586, 0.11189319101395086, -0.33364361214141053, -0.19219023995101453, 0.2887369399269422, 0.01942858180652... |
707.334 | On the irrelevant disorder regime of pinning models | Recent results have lead to substantial progress in understanding the role of
disorder in the (de)localization transition of polymer pinning models. Notably,
there is an understanding of the crucial issue of disorder relevance and
irrelevance that is now rigorous. In this work, we exploit interpolation and
replica co... | math.PR | recent results have lead to substantial progress in understanding the role of disorder in the delocalization transition of polymer pinning models notably there is an understanding of the crucial issue of disorder relevance and irrelevance that is now rigorous in this work we exploit interpolation and replica coupling m... | [['recent', 'results', 'have', 'lead', 'to', 'substantial', 'progress', 'in', 'understanding', 'the', 'role', 'of', 'disorder', 'in', 'the', 'delocalization', 'transition', 'of', 'polymer', 'pinning', 'models', 'notably', 'there', 'is', 'an', 'understanding', 'of', 'the', 'crucial', 'issue', 'of', 'disorder', 'relevanc... | [-0.11862317173991625, 0.1271712013255704, -0.0928534234805805, 0.08998167128784855, 0.0024965100285665293, -0.0950812066808661, 0.04686490747731224, 0.34576272636740013, -0.2594058740566053, -0.25207933195207904, 0.09707126869868328, -0.26932307513907733, -0.1902359695082939, 0.1470348832152057, -0.053920892158114325,... |
707.3341 | Quantum Information from Graviton-Matter Gas | We present basics of conceptually new-type way for explaining of the origin,
evolution and current physical properties of our Universe from the
graviton-matter gas viewpoint. Quantization method for the Friedmann-Lemaitre
Universe based on the canonical Hamilton equations of motion is proposed and
quantum information... | gr-qc cond-mat.stat-mech hep-th math-ph math.MP quant-ph | we present basics of conceptually newtype way for explaining of the origin evolution and current physical properties of our universe from the gravitonmatter gas viewpoint quantization method for the friedmannlemaitre universe based on the canonical hamilton equations of motion is proposed and quantum information theory... | [['we', 'present', 'basics', 'of', 'conceptually', 'newtype', 'way', 'for', 'explaining', 'of', 'the', 'origin', 'evolution', 'and', 'current', 'physical', 'properties', 'of', 'our', 'universe', 'from', 'the', 'gravitonmatter', 'gas', 'viewpoint', 'quantization', 'method', 'for', 'the', 'friedmannlemaitre', 'universe',... | [-0.0720646799714869, 0.08193429584868929, -0.1610595341771841, 0.07448601993471102, -0.09641139056872237, -0.06540478469634597, -0.014051901629886053, 0.28893239721373626, -0.24257847181323802, -0.2963610071350228, 0.03482226028184717, -0.25067618544298137, -0.14414279044351794, 0.1792818628195109, -0.0300206400482266... |
707.3342 | Automated calculations for multi-leg processes | The search for signals of new physics at the forthcoming LHC experiments
involves the analysis of final states characterised by a high number of
hadronic jets or identified particles. Precise theoretical predictions for
these processes require the computation of scattering amplitudes with a large
number of external p... | hep-ph | the search for signals of new physics at the forthcoming lhc experiments involves the analysis of final states characterised by a high number of hadronic jets or identified particles precise theoretical predictions for these processes require the computation of scattering amplitudes with a large number of external part... | [['the', 'search', 'for', 'signals', 'of', 'new', 'physics', 'at', 'the', 'forthcoming', 'lhc', 'experiments', 'involves', 'the', 'analysis', 'of', 'final', 'states', 'characterised', 'by', 'a', 'high', 'number', 'of', 'hadronic', 'jets', 'or', 'identified', 'particles', 'precise', 'theoretical', 'predictions', 'for', ... | [-0.13902318815720113, 0.22002656014228705, -0.04933785741256239, 0.07316206127992093, -0.045130448697212465, -0.09298720504739322, 0.041578836364351446, 0.29482956081240747, -0.19706950744390875, -0.38154545847404125, 0.07492569919728946, -0.3118989475866935, -0.050711193255362254, 0.17362833562704813, 0.0591328163430... |
707.3343 | The role of the $\Lambda(1405)$ in the $pp\to p K^+\Lambda(1405)$
reaction | We report a theoretical study of the $pp\to p K^+\Lambda(1405)$ reaction,
which was recently investigated at COSY-J\"{u}lich by using a 3.65 GeV/c
circulating proton beam incident on an internal hydrogen target. The reaction
is driven by single kaon exchange, single pion exchange, and single rho
exchange terms which ... | hep-ph | we report a theoretical study of the ppto p klambda1405 reaction which was recently investigated at cosyjulich by using a 365 gevc circulating proton beam incident on an internal hydrogen target the reaction is driven by single kaon exchange single pion exchange and single rho exchange terms which have very different s... | [['we', 'report', 'a', 'theoretical', 'study', 'of', 'the', 'ppto', 'p', 'klambda1405', 'reaction', 'which', 'was', 'recently', 'investigated', 'at', 'cosyjulich', 'by', 'using', 'a', '365', 'gevc', 'circulating', 'proton', 'beam', 'incident', 'on', 'an', 'internal', 'hydrogen', 'target', 'the', 'reaction', 'is', 'driv... | [-0.07643823160318483, 0.17592558757725316, -0.04954656538044075, 0.05094598529348611, -0.006081756116767036, -0.07008650999615375, 0.053537639026244234, 0.3500196545357161, -0.20732663306269314, -0.31034578135845686, -0.03512971190329973, -0.3463041503812269, -0.030433458105504217, 0.132747621524452, 0.081276707238250... |
707.3344 | CP Violation in the General Two-Higgs-Doublet Model: a Geometric View | We discuss the CP properties of the potential in the general
Two-Higgs-Doublet Model (THDM). This is done in a concise way using real gauge
invariant functions built from the scalar products of the doublet fields. The
space of these invariant functions, parametrising the gauge orbits of the Higgs
fields, is isomorphi... | hep-ph | we discuss the cp properties of the potential in the general twohiggsdoublet model thdm this is done in a concise way using real gauge invariant functions built from the scalar products of the doublet fields the space of these invariant functions parametrising the gauge orbits of the higgs fields is isomorphic to the f... | [['we', 'discuss', 'the', 'cp', 'properties', 'of', 'the', 'potential', 'in', 'the', 'general', 'twohiggsdoublet', 'model', 'thdm', 'this', 'is', 'done', 'in', 'a', 'concise', 'way', 'using', 'real', 'gauge', 'invariant', 'functions', 'built', 'from', 'the', 'scalar', 'products', 'of', 'the', 'doublet', 'fields', 'the'... | [-0.144549442717305, 0.19085669431987465, -0.06909062630072439, 0.12914101994433283, -0.11741356377261786, -0.1579590801143271, 0.031418442160689404, 0.3369929097009962, -0.24209619826101855, -0.22402982232572677, 0.08692740024143487, -0.19642827842625327, -0.10150170205857884, 0.13391370613755163, 0.01349735572984835,... |
707.3345 | On the geometry of cohomogeneity one manifolds with positive curvature | This is a survey on cohomogeneity one manifolds with positive curvature. We
discuss the known examples of this type and their geometry and the functions
that describe the metric. We also describe the classification of cohomogeneity
one manifolds that can admit a metric with positive curvature due to
Grove-Wilking-Zil... | math.DG | this is a survey on cohomogeneity one manifolds with positive curvature we discuss the known examples of this type and their geometry and the functions that describe the metric we also describe the classification of cohomogeneity one manifolds that can admit a metric with positive curvature due to grovewilkingziller tw... | [['this', 'is', 'a', 'survey', 'on', 'cohomogeneity', 'one', 'manifolds', 'with', 'positive', 'curvature', 'we', 'discuss', 'the', 'known', 'examples', 'of', 'this', 'type', 'and', 'their', 'geometry', 'and', 'the', 'functions', 'that', 'describe', 'the', 'metric', 'we', 'also', 'describe', 'the', 'classification', 'of... | [-0.15470287374362512, 0.046763649589949004, -0.0679716679227093, 0.10846035033666893, -0.15160606210322483, -0.17015442543703577, -0.07674850317973482, 0.37348839369319053, -0.2295170510997591, -0.25363751867300144, 0.15689055851797332, -0.30145157744055207, -0.2314851957616275, 0.17927432813398217, -0.141249372927553... |
707.3346 | Spin-locking effect in the nanoscale ordered perovskite cobaltite
LaBaCo2O6 | A new nanoscale ordered perovskite cobaltite, which consists of 90 degree
ordered domains of the layered-112 LaBaCo2O6 has been evidenced by high
resolution- transmission electron microscopy. This new form, like the
disordered La0.5Ba0.5CoO3 and ordered LaBaCo2O6, exhibits a ferromagnetic
transition at TC around 179 ... | cond-mat.mtrl-sci cond-mat.other | a new nanoscale ordered perovskite cobaltite which consists of 90 degree ordered domains of the layered112 labaco2o6 has been evidenced by high resolution transmission electron microscopy this new form like the disordered la05ba05coo3 and ordered labaco2o6 exhibits a ferromagnetic transition at tc around 179 k however ... | [['a', 'new', 'nanoscale', 'ordered', 'perovskite', 'cobaltite', 'which', 'consists', 'of', '90', 'degree', 'ordered', 'domains', 'of', 'the', 'layered112', 'labaco2o6', 'has', 'been', 'evidenced', 'by', 'high', 'resolution', 'transmission', 'electron', 'microscopy', 'this', 'new', 'form', 'like', 'the', 'disordered', ... | [-0.18028313961202422, 0.24579566779833, -0.017037407163745508, -0.05818731776469996, -0.02713721234109611, -0.13764623900015766, 0.09980200458476947, 0.36629528742140305, -0.2549396731819098, -0.3343468600561699, 0.02634998957980245, -0.3454048574472276, -0.08312887989450246, 0.16433862812566355, 0.042080498076617144,... |
707.3347 | 3D spectral synthesis and rotational line broadening | Spectral synthesis calculations based on three-dimensional stellar atmosphere
models are limited by the affordable angular resolution of the radiation field.
This hampers an accurate treatment of rotational line broadening. We aim to
find a treatment of rotational broadening of a spherical star when the
radiation fie... | astro-ph | spectral synthesis calculations based on threedimensional stellar atmosphere models are limited by the affordable angular resolution of the radiation field this hampers an accurate treatment of rotational line broadening we aim to find a treatment of rotational broadening of a spherical star when the radiation field is... | [['spectral', 'synthesis', 'calculations', 'based', 'on', 'threedimensional', 'stellar', 'atmosphere', 'models', 'are', 'limited', 'by', 'the', 'affordable', 'angular', 'resolution', 'of', 'the', 'radiation', 'field', 'this', 'hampers', 'an', 'accurate', 'treatment', 'of', 'rotational', 'line', 'broadening', 'we', 'aim... | [-0.042475869155853135, 0.0773322560911189, -0.08477278269172098, 0.09266420793071597, -0.12126121131500395, -0.10435043648807424, 0.026706558818200436, 0.42343953410440155, -0.19397150740801994, -0.3601528707716503, 0.09812778103197602, -0.19110703823331854, -0.09449851745278529, 0.2443121604063539, -0.077909675662493... |
707.3348 | Spin gap and Luttinger liquid description of the NMR relaxation in
carbon nanotubes | Recent NMR experiments by Singer et al. [Singer et al. Phys. Rev. Lett. 95,
236403 (2005).] showed a deviation from Fermi-liquid behavior in carbon
nanotubes with an energy gap evident at low temperatures. Here, a comprehensive
theory for the magnetic field and temperature dependent NMR 13C spin-lattice
relaxation is... | cond-mat.str-el cond-mat.mes-hall | recent nmr experiments by singer et al singer et al phys rev lett 95 236403 2005 showed a deviation from fermiliquid behavior in carbon nanotubes with an energy gap evident at low temperatures here a comprehensive theory for the magnetic field and temperature dependent nmr 13c spinlattice relaxation is given in the fra... | [['recent', 'nmr', 'experiments', 'by', 'singer', 'et', 'al', 'singer', 'et', 'al', 'phys', 'rev', 'lett', '95', '236403', '2005', 'showed', 'a', 'deviation', 'from', 'fermiliquid', 'behavior', 'in', 'carbon', 'nanotubes', 'with', 'an', 'energy', 'gap', 'evident', 'at', 'low', 'temperatures', 'here', 'a', 'comprehensiv... | [-0.08515451834093601, 0.2395323216126902, -0.058197903424678815, -0.09435715399255666, -0.041744836123793254, -0.14620434884203687, 0.10361034325961511, 0.3304460089365464, -0.2110217445574346, -0.35908226012474015, -0.05668851715191046, -0.331292542185457, -0.11898883766428169, 0.1905326626313451, -0.0499576937540301... |
707.3349 | A comment on the superconductivity of Sr2CuO3+delta | We have revisited data in the literature and find compelling reasons for
believing that enhanced superconductivity occurs in Sr2CuO3+delta when about
one third of the oxygen sites in the CuO2 layers are vacant, contrary to the
almost universally accepted assumption that superconducting interactions in the
high Tc cup... | cond-mat.supr-con | we have revisited data in the literature and find compelling reasons for believing that enhanced superconductivity occurs in sr2cuo3delta when about one third of the oxygen sites in the cuo2 layers are vacant contrary to the almost universally accepted assumption that superconducting interactions in the high tc cuprate... | [['we', 'have', 'revisited', 'data', 'in', 'the', 'literature', 'and', 'find', 'compelling', 'reasons', 'for', 'believing', 'that', 'enhanced', 'superconductivity', 'occurs', 'in', 'sr2cuo3delta', 'when', 'about', 'one', 'third', 'of', 'the', 'oxygen', 'sites', 'in', 'the', 'cuo2', 'layers', 'are', 'vacant', 'contrary'... | [-0.1815555992249686, 0.20295144064136997, 0.06330482025357644, 0.10175653657643124, 0.004889582140514484, -0.18587138405284628, 0.17689213941160303, 0.3851941889868333, -0.22842659593488163, -0.2493812253412146, -0.012562620213989599, -0.39235961723786134, -0.10569952936986318, 0.10423471021707743, -0.0054402431974617... |
707.335 | New developments on embedding inflation in gauge theory and particle
physics | In this brief review we will discuss how a well motivated particle theory
beyond the eletroweak Standard Model provides ingredients and conditions for a
successful inflation. We will mainly focus on a low energy supersymmetric
Standard Model which provides plenty of scalars. In particular, these scalars
span a multid... | hep-ph astro-ph gr-qc hep-th | in this brief review we will discuss how a well motivated particle theory beyond the eletroweak standard model provides ingredients and conditions for a successful inflation we will mainly focus on a low energy supersymmetric standard model which provides plenty of scalars in particular these scalars span a multidimens... | [['in', 'this', 'brief', 'review', 'we', 'will', 'discuss', 'how', 'a', 'well', 'motivated', 'particle', 'theory', 'beyond', 'the', 'eletroweak', 'standard', 'model', 'provides', 'ingredients', 'and', 'conditions', 'for', 'a', 'successful', 'inflation', 'we', 'will', 'mainly', 'focus', 'on', 'a', 'low', 'energy', 'supe... | [-0.09609487715197053, 0.21652007655505626, -0.10196785081395919, 0.1479811402473678, -0.08962413913723914, -0.15466992576988017, -0.007383550716033998, 0.31954519657735175, -0.2322680764123203, -0.2775621944245823, 0.11758718996846236, -0.2311563790214503, -0.136223601645473, 0.18275738063211394, -0.04223669463634848,... |
707.3351 | Reflections and Thoughts on Tired Light | The position of the various tired light theories is reviewed briefly and it
is noted that one of the biggest objections to them concerns the mechanism by
which light might lose energy as it travels through space. Here some new work
relating to the constancy of the speed of light is highlighted as providing a
possible... | physics.gen-ph | the position of the various tired light theories is reviewed briefly and it is noted that one of the biggest objections to them concerns the mechanism by which light might lose energy as it travels through space here some new work relating to the constancy of the speed of light is highlighted as providing a possible so... | [['the', 'position', 'of', 'the', 'various', 'tired', 'light', 'theories', 'is', 'reviewed', 'briefly', 'and', 'it', 'is', 'noted', 'that', 'one', 'of', 'the', 'biggest', 'objections', 'to', 'them', 'concerns', 'the', 'mechanism', 'by', 'which', 'light', 'might', 'lose', 'energy', 'as', 'it', 'travels', 'through', 'spa... | [-0.106524907326481, 0.16263653241097928, -0.11545338142042359, 0.10544263079452018, -0.13721640050411224, -0.16316259569798908, 0.0858980822741675, 0.3314213749890526, -0.28905135735248527, -0.31779746726155284, 0.12267649831871191, -0.27222784634679553, -0.16943668807701517, 0.22380337511499723, -0.08728840384011467,... |
707.3352 | Wavepacket Solutions of the Klein-Gordon Equation | We find dispersion-free wavepacket solutions to the Klein-Gordon equation,
with the only free parameter being the wavepacket velocity $ {\bf v} $. These
wavefunctions are eigenvectors of a velocity operator with commuting components
which is symmetric in a certain scalar product space. We show that this
velocity oper... | quant-ph hep-th math-ph math.MP | we find dispersionfree wavepacket solutions to the kleingordon equation with the only free parameter being the wavepacket velocity bf v these wavefunctions are eigenvectors of a velocity operator with commuting components which is symmetric in a certain scalar product space we show that this velocity operator correspon... | [['we', 'find', 'dispersionfree', 'wavepacket', 'solutions', 'to', 'the', 'kleingordon', 'equation', 'with', 'the', 'only', 'free', 'parameter', 'being', 'the', 'wavepacket', 'velocity', 'bf', 'v', 'these', 'wavefunctions', 'are', 'eigenvectors', 'of', 'a', 'velocity', 'operator', 'with', 'commuting', 'components', 'wh... | [-0.1750966765685007, 0.1756961284481804, -0.08613176827930147, -0.014026422257302329, -0.1045963914366439, -0.12881696812110022, -0.035793929138890235, 0.3586665799666662, -0.2803265746915713, -0.18683350895298645, 0.031619137385860085, -0.27118338881700765, -0.11851362454763148, 0.12996917919372208, -0.01041417455417... |
707.3353 | The multiple effects of gradient coupling on network synchronization | Recent studies have shown that synchronizability of complex networks can be
significantly improved by asymmetric couplings, and increase of coupling
gradient is always in favor of network synchronization. Here we argue and
demonstrate that, for typical complex networks, there usually exists an optimal
coupling gradie... | nlin.AO nlin.PS | recent studies have shown that synchronizability of complex networks can be significantly improved by asymmetric couplings and increase of coupling gradient is always in favor of network synchronization here we argue and demonstrate that for typical complex networks there usually exists an optimal coupling gradient und... | [['recent', 'studies', 'have', 'shown', 'that', 'synchronizability', 'of', 'complex', 'networks', 'can', 'be', 'significantly', 'improved', 'by', 'asymmetric', 'couplings', 'and', 'increase', 'of', 'coupling', 'gradient', 'is', 'always', 'in', 'favor', 'of', 'network', 'synchronization', 'here', 'we', 'argue', 'and', '... | [-0.20780846498370514, 0.10597381261170023, -0.007371640110685795, 0.008090931062289208, -0.04002341545116501, -0.16732021520587326, 0.03601835665739134, 0.45205368345775526, -0.26386670746347485, -0.28714236656219516, 0.09812901611831196, -0.22641954772925676, -0.24820697944642617, 0.1589311109855771, -0.0321947157484... |
707.3354 | Indications of a Four-Quark Structure for the X(3872) and X(3876)
Particles from Recent Belle and BABAR Data | Recent results by BELLE and BaBar point to the existence of a second X
particle decaying in D^0 D^0bar pi^0, a few MeV above the X(3872). We identify
the two X states with the neutral particles predicted by the 4-quark model and
show that production and decays are consistent with this assignement. We
consider the yet... | hep-ph | recent results by belle and babar point to the existence of a second x particle decaying in d0 d0bar pi0 a few mev above the x3872 we identify the two x states with the neutral particles predicted by the 4quark model and show that production and decays are consistent with this assignement we consider the yettobeobserve... | [['recent', 'results', 'by', 'belle', 'and', 'babar', 'point', 'to', 'the', 'existence', 'of', 'a', 'second', 'x', 'particle', 'decaying', 'in', 'd0', 'd0bar', 'pi0', 'a', 'few', 'mev', 'above', 'the', 'x3872', 'we', 'identify', 'the', 'two', 'x', 'states', 'with', 'the', 'neutral', 'particles', 'predicted', 'by', 'the... | [-0.06398861695414604, 0.24347762271428286, -0.0547371829595806, 0.11028051711862157, -0.025492295809177015, -0.183638622442177, 0.10090530273998018, 0.2983504466768076, -0.18223632927705993, -0.24507098168885308, -0.03840164286119224, -0.3979685493369601, -0.02757283892315715, 0.11140816217225824, 0.07965756595523944,... |
707.3355 | Three-Family Models from a Heterotic Orbifold on the E_6 Root Lattice | We classify N=1 orbifolds on the E_6 root lattice and investigate explicit
model constructions on the Z_3xZ_3 orbifold in heterotic string theory.
Interestingly some of the twisted sectors from the Z_3xZ_3 orbifold on the E_6
root lattice have just three fixed tori respectively, and generate three
degenerate massless... | hep-th hep-ph | we classify n1 orbifolds on the e_6 root lattice and investigate explicit model constructions on the z_3xz_3 orbifold in heterotic string theory interestingly some of the twisted sectors from the z_3xz_3 orbifold on the e_6 root lattice have just three fixed tori respectively and generate three degenerate massless stat... | [['we', 'classify', 'n1', 'orbifolds', 'on', 'the', 'e_6', 'root', 'lattice', 'and', 'investigate', 'explicit', 'model', 'constructions', 'on', 'the', 'z_3xz_3', 'orbifold', 'in', 'heterotic', 'string', 'theory', 'interestingly', 'some', 'of', 'the', 'twisted', 'sectors', 'from', 'the', 'z_3xz_3', 'orbifold', 'on', 'th... | [-0.11938097893774587, 0.23895329492127834, -0.011455665298854, 0.17283170953548202, -0.04761193199374247, -0.22766102863048823, 0.026624543952493696, 0.3594619977423766, -0.18622353559476323, -0.28525781732363004, 0.113531211965892, -0.29239975634360843, -0.12534949835632384, 0.08039066734636435, -0.030252181430114433... |
707.3356 | Measuring the kinetic power of AGN in the radio mode | (Abridged) We have studied the relationship among nuclear radio and X-ray
power, Bondi rate and the kinetic luminosity of sub-Eddington active galactic
nuclear (AGN) jets. Besides the recently discovered correlation between jet
kinetic and Bondi power, we show that a clear correlation exists also between
Eddington-sc... | astro-ph | abridged we have studied the relationship among nuclear radio and xray power bondi rate and the kinetic luminosity of subeddington active galactic nuclear agn jets besides the recently discovered correlation between jet kinetic and bondi power we show that a clear correlation exists also between eddingtonscaled kinetic... | [['abridged', 'we', 'have', 'studied', 'the', 'relationship', 'among', 'nuclear', 'radio', 'and', 'xray', 'power', 'bondi', 'rate', 'and', 'the', 'kinetic', 'luminosity', 'of', 'subeddington', 'active', 'galactic', 'nuclear', 'agn', 'jets', 'besides', 'the', 'recently', 'discovered', 'correlation', 'between', 'jet', 'k... | [-0.05381504801583951, 0.0935241968850791, -0.06970174176480752, 0.16261720315486208, -0.09603679511362709, -0.08247014424122204, 0.045735096970232425, 0.43686348920985185, -0.170807194201061, -0.33131865286068984, 0.0644042526497705, -0.32270490955054065, 0.0010797610433485923, 0.2443632319359406, 0.003051605506804418... |
707.3357 | Quantum mechanics on manifolds and topological effects | A unique classification of the topological effects associated to quantum
mechanics on manifolds is obtained on the basis of the invariance under
diffeomorphisms and the realization of the Lie-Rinehart relations between the
generators of the diffeomorphism group and the algebra of infinitely
differentiable functions o... | math-ph hep-th math.MP | a unique classification of the topological effects associated to quantum mechanics on manifolds is obtained on the basis of the invariance under diffeomorphisms and the realization of the lierinehart relations between the generators of the diffeomorphism group and the algebra of infinitely differentiable functions on t... | [['a', 'unique', 'classification', 'of', 'the', 'topological', 'effects', 'associated', 'to', 'quantum', 'mechanics', 'on', 'manifolds', 'is', 'obtained', 'on', 'the', 'basis', 'of', 'the', 'invariance', 'under', 'diffeomorphisms', 'and', 'the', 'realization', 'of', 'the', 'lierinehart', 'relations', 'between', 'the', ... | [-0.19937657902063383, 0.09676881980251621, -0.10257045875999841, 0.039170978985189855, -0.10368385525034354, -0.09856140652570773, -0.018227311731148343, 0.3357921991967135, -0.3338680795586861, -0.2380739864935209, 0.11611643926605482, -0.254310220682381, -0.13801902987331421, 0.17072201272690887, -0.0821178784963112... |
707.3358 | New Angle on the Strong CP and Chiral Symmetry Problems from a Rotating
Mass Matrix | It is shown that when the mass matrix changes in orientation (rotates) in
generation space for changing energy scale, then the masses of the lower
generations are not given just by its eigenvalues. In particular, these masses
need not be zero even when the eigenvalues are zero. In that case, the strong
CP problem can... | hep-ph hep-th | it is shown that when the mass matrix changes in orientation rotates in generation space for changing energy scale then the masses of the lower generations are not given just by its eigenvalues in particular these masses need not be zero even when the eigenvalues are zero in that case the strong cp problem can be avoid... | [['it', 'is', 'shown', 'that', 'when', 'the', 'mass', 'matrix', 'changes', 'in', 'orientation', 'rotates', 'in', 'generation', 'space', 'for', 'changing', 'energy', 'scale', 'then', 'the', 'masses', 'of', 'the', 'lower', 'generations', 'are', 'not', 'given', 'just', 'by', 'its', 'eigenvalues', 'in', 'particular', 'thes... | [-0.12406860693590716, 0.2917346801379666, -0.04128524277817517, 0.1070554097421423, -0.09506781192289458, -0.14536170709863425, 0.04528173466678709, 0.3654274642171841, -0.2201624745650897, -0.33988937065337915, 0.097627738795598, -0.24773659642475346, -0.0986007015583002, 0.1332938535109399, -0.02238711037687839, 0.0... |
707.3359 | On the superstrings-induced four-dimensional gravity, and its
applications to cosmology | We review the status of the fourth-order (quartic in the spacetime curvature)
terms induced by superstrings/M-theory (compactified on a warped torus) in the
leading order with respect to the Regge slope parameter, and study their
(non-perturbative) impact on the evolution of the Hubble scale in the context
of the fou... | hep-th gr-qc | we review the status of the fourthorder quartic in the spacetime curvature terms induced by superstringsmtheory compactified on a warped torus in the leading order with respect to the regge slope parameter and study their nonperturbative impact on the evolution of the hubble scale in the context of the fourdimensional ... | [['we', 'review', 'the', 'status', 'of', 'the', 'fourthorder', 'quartic', 'in', 'the', 'spacetime', 'curvature', 'terms', 'induced', 'by', 'superstringsmtheory', 'compactified', 'on', 'a', 'warped', 'torus', 'in', 'the', 'leading', 'order', 'with', 'respect', 'to', 'the', 'regge', 'slope', 'parameter', 'and', 'study', ... | [-0.16044723074038014, 0.12699263931685828, -0.09687521507682866, 0.12876686117969044, -0.12728338631201688, -0.09611060067194782, -0.05099510115233237, 0.27177435465313315, -0.17368718748035114, -0.25905845261837535, 0.08126421262388922, -0.24227948277257383, -0.13561544794436187, 0.11158538658701343, -0.0377844108447... |
707.336 | Some constructions of almost para-hyperhermitian structures on manifolds
and tangent bundles | In this paper we give some examples of almost para-hyperhermitian structures
on the tangent bundle of an almost product manifold, on the product manifold
$M\times\mathbb{R}$, where $M$ is a manifold endowed with a mixed 3-structure
and on the circle bundle over a manifold with a mixed 3-structure.
| math.DG | in this paper we give some examples of almost parahyperhermitian structures on the tangent bundle of an almost product manifold on the product manifold mtimesmathbbr where m is a manifold endowed with a mixed 3structure and on the circle bundle over a manifold with a mixed 3structure | [['in', 'this', 'paper', 'we', 'give', 'some', 'examples', 'of', 'almost', 'parahyperhermitian', 'structures', 'on', 'the', 'tangent', 'bundle', 'of', 'an', 'almost', 'product', 'manifold', 'on', 'the', 'product', 'manifold', 'mtimesmathbbr', 'where', 'm', 'is', 'a', 'manifold', 'endowed', 'with', 'a', 'mixed', '3struc... | [-0.23129714389351455, 0.034613946901369305, -0.059208800951811545, -0.00894832409957939, -0.08145089955762663, -0.11783245241546884, -0.023688587218899517, 0.4076008653228587, -0.24157340983127026, -0.1885540548147277, 0.16686783706957592, -0.26163995416557534, -0.1824932994439881, 0.16381418958127975, -0.155201014289... |
707.3361 | Reply to `Extended Rejoinder to "Extended Comment on "One-Range Addition
Theorems for Coulomb Interaction Potential and Its Derivatives" by I. I.
Guseinov (Chem. Phys. Vol. 309 (2005), pp. 209 - 211)", arXiv:0706.0975v2" | In the years from 2001 to 2006, Guseinov and his coworkers published 40
articles on the derivation and application of one-range addition theorems. In
E. J. Weniger, Extended Comment on ``One-Range Addition Theorems for Coulomb
Interaction Potential and Its Derivatives'' by I. I. Guseinov (Chem. Phys. Vol.
309 (2005),... | math-ph math.MP | in the years from 2001 to 2006 guseinov and his coworkers published 40 articles on the derivation and application of onerange addition theorems in e j weniger extended comment on onerange addition theorems for coulomb interaction potential and its derivatives by i i guseinov chem phys vol 309 2005 pp 209 213 arxiv07041... | [['in', 'the', 'years', 'from', '2001', 'to', '2006', 'guseinov', 'and', 'his', 'coworkers', 'published', '40', 'articles', 'on', 'the', 'derivation', 'and', 'application', 'of', 'onerange', 'addition', 'theorems', 'in', 'e', 'j', 'weniger', 'extended', 'comment', 'on', 'onerange', 'addition', 'theorems', 'for', 'coulo... | [-0.02476262349126384, 0.013119928538799286, -0.07181737818863503, 0.0365992953816732, -0.06078202069498772, -0.15060798735484163, 0.10616415158877972, 0.3159515118161433, -0.09497642982570642, -0.3260359467952981, 0.03902690372020981, -0.3243735678306268, -0.16116390652348137, 0.13759333591604994, -0.17162890028742742... |
707.3362 | Gibbs measures with double stochastic integrals on a path space | We investigate Gibbs measures relative to Brownian motion in the case when
the interaction energy is given by a double stochastic integral. In the case
when the double stochastic integral is originating from the Pauli-Fierz model
in nonrelativistic quantum electrodynamics, we prove the existence of its
infinite volum... | math-ph math.MP | we investigate gibbs measures relative to brownian motion in the case when the interaction energy is given by a double stochastic integral in the case when the double stochastic integral is originating from the paulifierz model in nonrelativistic quantum electrodynamics we prove the existence of its infinite volume lim... | [['we', 'investigate', 'gibbs', 'measures', 'relative', 'to', 'brownian', 'motion', 'in', 'the', 'case', 'when', 'the', 'interaction', 'energy', 'is', 'given', 'by', 'a', 'double', 'stochastic', 'integral', 'in', 'the', 'case', 'when', 'the', 'double', 'stochastic', 'integral', 'is', 'originating', 'from', 'the', 'paul... | [-0.12505920535447645, 0.14808999308936147, -0.0810787364821501, 0.11515654620182302, -0.00971870645120436, -0.08035652919159252, 0.015447349168778378, 0.29934921723847485, -0.3171709496147779, -0.23400075140656257, 0.052376149870854406, -0.3072570717076258, -0.11793514538784416, 0.16998992327657736, -0.072866352113457... |
707.3363 | Very deep X-ray observations of the Anomalous X-ray Pulsar 4U 0142+614 | We report on two new XMM-Newton observations of the Anomalous X-ray Pulsar
(AXP) 4U 0142+614 performed in March and July 2004, collecting the most
accurate spectrum for this source to date. Furthermore, we analyse two short
archival observations performed in February 2002 and January 2003 (the latter
already reported... | astro-ph | we report on two new xmmnewton observations of the anomalous xray pulsar axp 4u 0142614 performed in march and july 2004 collecting the most accurate spectrum for this source to date furthermore we analyse two short archival observations performed in february 2002 and january 2003 the latter already reported by gohler ... | [['we', 'report', 'on', 'two', 'new', 'xmmnewton', 'observations', 'of', 'the', 'anomalous', 'xray', 'pulsar', 'axp', '4u', '0142614', 'performed', 'in', 'march', 'and', 'july', '2004', 'collecting', 'the', 'most', 'accurate', 'spectrum', 'for', 'this', 'source', 'to', 'date', 'furthermore', 'we', 'analyse', 'two', 'sh... | [-0.07455524720323546, 0.09192761636321131, -0.0637472324559222, 0.09246576369564602, -0.08809918905119074, -0.12243353261877805, 0.0770919467120067, 0.43021789148611866, -0.1533945877805739, -0.42867491482689546, 0.08400231764026454, -0.3327527673192916, -0.043447156004823635, 0.21761029762112433, -0.02787661863319971... |
707.3364 | On the base locus of the linear system of generalized theta functions | Let $\cM_r$ denote the moduli space of semi-stable rank-$r$ vector bundles
with trivial determinant over a smooth projective curve $C$ of genus $g$. In
this paper we study the base locus $\cB_r \subset \cM_r$ of the linear system
of the determinant line bundle $\cL$ over $\cM_r$, i.e., the set of semi-stable
rank-$r$... | math.AG | let cm_r denote the moduli space of semistable rankr vector bundles with trivial determinant over a smooth projective curve c of genus g in this paper we study the base locus cb_r subset cm_r of the linear system of the determinant line bundle cl over cm_r ie the set of semistable rankr vector bundles without theta div... | [['let', 'cm_r', 'denote', 'the', 'moduli', 'space', 'of', 'semistable', 'rankr', 'vector', 'bundles', 'with', 'trivial', 'determinant', 'over', 'a', 'smooth', 'projective', 'curve', 'c', 'of', 'genus', 'g', 'in', 'this', 'paper', 'we', 'study', 'the', 'base', 'locus', 'cb_r', 'subset', 'cm_r', 'of', 'the', 'linear', '... | [-0.3248687507329534, -0.011248975719503854, -0.06010480559341712, -0.07626927380086472, -0.1135482101458801, -0.19003060602340593, 0.10241747174367359, 0.3393249367299962, -0.3127008122073053, -0.11443453904700605, 0.04361280881359612, -0.22387731923683457, -0.13668531876006354, 0.2111889926895295, -0.1442264566079981... |
707.3365 | Generalized Wick's theorem for multiquasiparticle overlaps as a limit of
Gaudin's theorem | We are able to rederive in a very simple way the standard generalized Wick's
theorem for overlaps of mean field wave functions by using the extension of the
statistical Wick's theorem (Gaudin's theorem) in the appropriate limits.
| nucl-th | we are able to rederive in a very simple way the standard generalized wicks theorem for overlaps of mean field wave functions by using the extension of the statistical wicks theorem gaudins theorem in the appropriate limits | [['we', 'are', 'able', 'to', 'rederive', 'in', 'a', 'very', 'simple', 'way', 'the', 'standard', 'generalized', 'wicks', 'theorem', 'for', 'overlaps', 'of', 'mean', 'field', 'wave', 'functions', 'by', 'using', 'the', 'extension', 'of', 'the', 'statistical', 'wicks', 'theorem', 'gaudins', 'theorem', 'in', 'the', 'appropr... | [-0.06558992517356937, 0.07367275411112083, -0.17820999559921188, 0.20142147443383127, -0.055493463309028664, -0.06394226988777518, 0.08941641152911894, 0.2886893176347823, -0.24640340748167522, -0.26701234633455406, 0.06428973014919541, -0.18752517070419886, -0.1384178031537984, 0.24984393893061457, -0.075685527798644... |
707.3366 | The Pion-Photon Transition Distribution Amplitudes in the Nambu-Jona
Lasinio Model | We define the pion-photon Transition Distribution Amplitudes (TDA) in a field
theoretic formalism from a covariant Bethe-Salpeter approach for the
determination of the bound state. We apply our formalism to the Nambu - Jona
Lasinio model, as a realistic theory of the pion. The obtained vector and axial
TDAs satisfy a... | hep-ph | we define the pionphoton transition distribution amplitudes tda in a field theoretic formalism from a covariant bethesalpeter approach for the determination of the bound state we apply our formalism to the nambu jona lasinio model as a realistic theory of the pion the obtained vector and axial tdas satisfy all features... | [['we', 'define', 'the', 'pionphoton', 'transition', 'distribution', 'amplitudes', 'tda', 'in', 'a', 'field', 'theoretic', 'formalism', 'from', 'a', 'covariant', 'bethesalpeter', 'approach', 'for', 'the', 'determination', 'of', 'the', 'bound', 'state', 'we', 'apply', 'our', 'formalism', 'to', 'the', 'nambu', 'jona', 'l... | [-0.13936033010832033, 0.16001305227167906, -0.1455104808975011, 0.13988875607494264, -0.05905773043166846, -0.07986176094040275, 0.06813043463393115, 0.30057935499586164, -0.17068214433267712, -0.19987624858040362, 0.014564110551727936, -0.23042621162720026, -0.18315669118892403, 0.08926129311788827, 0.056336676138453... |
707.3367 | Magic Baseline Beta Beam | We study the physics reach of an experiment where neutrinos produced in a
beta-beam facility at CERN are observed in a large magnetized iron calorimeter
(ICAL) at the India-based Neutrino Observatory (INO). The CERN-INO distance is
close to the so-called "magic" baseline which helps evade some of the parameter
degene... | hep-ph hep-ex | we study the physics reach of an experiment where neutrinos produced in a betabeam facility at cern are observed in a large magnetized iron calorimeter ical at the indiabased neutrino observatory ino the cernino distance is close to the socalled magic baseline which helps evade some of the parameter degeneracies and al... | [['we', 'study', 'the', 'physics', 'reach', 'of', 'an', 'experiment', 'where', 'neutrinos', 'produced', 'in', 'a', 'betabeam', 'facility', 'at', 'cern', 'are', 'observed', 'in', 'a', 'large', 'magnetized', 'iron', 'calorimeter', 'ical', 'at', 'the', 'indiabased', 'neutrino', 'observatory', 'ino', 'the', 'cernino', 'dis... | [-0.0724024455693941, 0.27607664588539327, -0.02556123136873207, 0.18641982546954927, -0.07930398278028494, -0.12675577122718096, 0.04764047311618924, 0.2842013501832562, -0.20353083441694897, -0.3910500103487603, 0.04514228641581271, -0.3558271413768976, 0.04589004810118387, 0.2014063075184822, 0.05899766366177749, 0.... |
707.3368 | 30 GHz flux density measurements of the Caltech-Jodrell flat-spectrum
sources with OCRA-p | To measure the 30-GHz flux densities of the 293 sources in the
Caltech-Jodrell Bank flat-spectrum (CJF) sample. The measurements are part of
an ongoing programme to measure the spectral energy distributions of flat
spectrum radio sources and to correlate them with the milliarcsecond structures
from VLBI and other mea... | astro-ph | to measure the 30ghz flux densities of the 293 sources in the caltechjodrell bank flatspectrum cjf sample the measurements are part of an ongoing programme to measure the spectral energy distributions of flat spectrum radio sources and to correlate them with the milliarcsecond structures from vlbi and other measured as... | [['to', 'measure', 'the', '30ghz', 'flux', 'densities', 'of', 'the', '293', 'sources', 'in', 'the', 'caltechjodrell', 'bank', 'flatspectrum', 'cjf', 'sample', 'the', 'measurements', 'are', 'part', 'of', 'an', 'ongoing', 'programme', 'to', 'measure', 'the', 'spectral', 'energy', 'distributions', 'of', 'flat', 'spectrum'... | [-0.07972416646856194, 0.06287042461165887, -0.059186165504312764, 0.02946519412410756, -0.08299175182473846, -0.10184845773425574, 0.04442337586078793, 0.45000689577621716, -0.1415345026180148, -0.413802556572288, 0.14147290105950863, -0.3846032575083276, 0.05196442091449474, 0.2503855629513661, 0.010521185180793206, ... |
707.3369 | Collisional Velocities and Rates in Resonant Planetesimal Belts | We consider a belt of small bodies around a star, captured in one of the
external or 1:1 mean-motion resonances with a massive perturber. The objects in
the belt collide with each other. Combining methods of celestial mechanics and
statistical physics, we calculate mean collisional velocities and collisional
rates, a... | astro-ph | we consider a belt of small bodies around a star captured in one of the external or 11 meanmotion resonances with a massive perturber the objects in the belt collide with each other combining methods of celestial mechanics and statistical physics we calculate mean collisional velocities and collisional rates averaged o... | [['we', 'consider', 'a', 'belt', 'of', 'small', 'bodies', 'around', 'a', 'star', 'captured', 'in', 'one', 'of', 'the', 'external', 'or', '11', 'meanmotion', 'resonances', 'with', 'a', 'massive', 'perturber', 'the', 'objects', 'in', 'the', 'belt', 'collide', 'with', 'each', 'other', 'combining', 'methods', 'of', 'celest... | [-0.10551239924155449, 0.18182626021200513, -0.06370148523105572, 0.09283697999629724, -0.0037790637102904125, -0.035142833635337274, 0.006799075915609713, 0.33895687681049275, -0.19105351009763946, -0.32911051546176107, 0.035285868007810736, -0.2660037568049495, -0.04206372840766726, 0.24556810984330116, -0.0936832572... |
707.337 | Weighted Strichartz estimates for radial Schr\"odinger equation on
noncompact manifolds | We prove global weighted Strichartz estimates for radial solutions of linear
Schr\"odinger equation on a class of rotationally symmetric noncompact
manifolds, generalizing the known results on hyperbolic and Damek-Ricci spaces.
This yields classical Strichartz estimates with a larger class of exponents
than in the Eu... | math.AP | we prove global weighted strichartz estimates for radial solutions of linear schrodinger equation on a class of rotationally symmetric noncompact manifolds generalizing the known results on hyperbolic and damekricci spaces this yields classical strichartz estimates with a larger class of exponents than in the euclidian... | [['we', 'prove', 'global', 'weighted', 'strichartz', 'estimates', 'for', 'radial', 'solutions', 'of', 'linear', 'schrodinger', 'equation', 'on', 'a', 'class', 'of', 'rotationally', 'symmetric', 'noncompact', 'manifolds', 'generalizing', 'the', 'known', 'results', 'on', 'hyperbolic', 'and', 'damekricci', 'spaces', 'this... | [-0.11271857998575657, 0.10686919760460464, -0.08033632934988978, 0.11344362945080949, -0.07927789095466813, -0.14581753950064572, -0.03219925944084445, 0.31349528300522184, -0.2398123956285417, -0.18878360314724538, 0.1517495812373594, -0.33207137091085315, -0.12379481629647601, 0.2619667417423513, -0.0478312205272511... |
707.3371 | Approximation by Several Rationals | Following T. H. Chan, we consider the problem of approximation of a given
rational fraction a/q by sums of several rational fractions a_1/q_1, ...,
a_n/q_n with smaller denominators. We show that in the special cases of n=3 and
n=4 and certain admissible ranges for the denominators q_1,..., q_n, one can
improve a res... | math.NT | following t h chan we consider the problem of approximation of a given rational fraction aq by sums of several rational fractions a_1q_1 a_nq_n with smaller denominators we show that in the special cases of n3 and n4 and certain admissible ranges for the denominators q_1 q_n one can improve a result of t h chan by usin... | [['following', 't', 'h', 'chan', 'we', 'consider', 'the', 'problem', 'of', 'approximation', 'of', 'a', 'given', 'rational', 'fraction', 'aq', 'by', 'sums', 'of', 'several', 'rational', 'fractions', 'a_1q_1', 'a_nq_n', 'with', 'smaller', 'denominators', 'we', 'show', 'that', 'in', 'the', 'special', 'cases', 'of', 'n3', ... | [-0.18368734062207326, 0.1431746046863875, -0.02562751000652374, 0.007611263882747646, -0.008202181560760838, -0.14470048167474442, 0.10779349556413748, 0.31004030623678436, -0.2549868971819721, -0.28613242472253614, 0.04288759820313209, -0.25625770501555656, -0.12068090802532132, 0.18259485261672634, -0.06409166945870... |
707.3372 | Collins fragmentation function for pions and kaons in a spectator model | We calculate the Collins fragmentation function in the framework of a
spectator model with pseudoscalar pion-quark coupling and a Gaussian form
factor at the vertex. We determine the model parameters by fitting the
unpolarized fragmentation function for pions and kaons. We show that the
Collins function for the pions... | hep-ph | we calculate the collins fragmentation function in the framework of a spectator model with pseudoscalar pionquark coupling and a gaussian form factor at the vertex we determine the model parameters by fitting the unpolarized fragmentation function for pions and kaons we show that the collins function for the pions in t... | [['we', 'calculate', 'the', 'collins', 'fragmentation', 'function', 'in', 'the', 'framework', 'of', 'a', 'spectator', 'model', 'with', 'pseudoscalar', 'pionquark', 'coupling', 'and', 'a', 'gaussian', 'form', 'factor', 'at', 'the', 'vertex', 'we', 'determine', 'the', 'model', 'parameters', 'by', 'fitting', 'the', 'unpol... | [-0.014331387309357523, 0.1769581107175327, -0.13909972136025317, 0.13345852624624968, 0.006460209348006174, -0.06576832574501168, 0.010371353209484369, 0.3756410425528884, -0.17987275420455262, -0.2463161543942988, -0.08609889320214278, -0.3006823307834566, -0.05751658293884247, 0.12358934532094282, 0.0872986008762382... |
707.3373 | How Much Work Does It Take To Straighten a Plane Graph Out? | We prove that if one wants to make a plane graph drawing straight-line then
in the worst case one has to move almost all vertices.
| math.CO | we prove that if one wants to make a plane graph drawing straightline then in the worst case one has to move almost all vertices | [['we', 'prove', 'that', 'if', 'one', 'wants', 'to', 'make', 'a', 'plane', 'graph', 'drawing', 'straightline', 'then', 'in', 'the', 'worst', 'case', 'one', 'has', 'to', 'move', 'almost', 'all', 'vertices']] | [-0.12131377585232257, 0.05680107772350311, -0.09306853607296944, 0.0296027784794569, -0.1962508656643331, -0.24212376041337846, 0.07368834137916565, 0.4498267078399658, -0.3085841198638082, -0.22962498445063828, 0.04646840266417712, -0.43107242703437804, -0.1199424346536398, 0.08688843674957752, -0.11625493165105581, ... |
707.3374 | Decomposition driven interface evolution for layers of binary mixtures:
I. Model derivation and stratified base states | A dynamical model is proposed to describe the coupled decomposition and
profile evolution of a free surface film of a binary mixture. An example is a
thin film of a polymer blend on a solid substrate undergoing simultaneous phase
separation and dewetting. The model is based on model-H describing the coupled
transport... | physics.flu-dyn | a dynamical model is proposed to describe the coupled decomposition and profile evolution of a free surface film of a binary mixture an example is a thin film of a polymer blend on a solid substrate undergoing simultaneous phase separation and dewetting the model is based on modelh describing the coupled transport of t... | [['a', 'dynamical', 'model', 'is', 'proposed', 'to', 'describe', 'the', 'coupled', 'decomposition', 'and', 'profile', 'evolution', 'of', 'a', 'free', 'surface', 'film', 'of', 'a', 'binary', 'mixture', 'an', 'example', 'is', 'a', 'thin', 'film', 'of', 'a', 'polymer', 'blend', 'on', 'a', 'solid', 'substrate', 'undergoing... | [-0.12503101419059248, 0.1541041171335, -0.10088651769039948, 0.008733423328176684, -0.05747163803044734, -0.14951357055526826, -0.005763649287885123, 0.32828303619566623, -0.2746148353075459, -0.2669382851297226, 0.09024306158297253, -0.26454462051174066, -0.07851572973606089, 0.16757195690361254, 0.008912567124042634... |
707.3375 | Towards a nonlinear Schwarz's list | This is basically the text of a survey talk (entitled 'Painleve, Klein and
the icosahedron') given at Hitchin's 60th birthday conference. It discusses the
search for and construction of algebraic solutions of the sixth Painleve
differential equation, which may be viewed as a nonlinear analogue of the Gauss
hypergeome... | math.CA math.AG nlin.SI | this is basically the text of a survey talk entitled painleve klein and the icosahedron given at hitchins 60th birthday conference it discusses the search for and construction of algebraic solutions of the sixth painleve differential equation which may be viewed as a nonlinear analogue of the gauss hypergeometric equat... | [['this', 'is', 'basically', 'the', 'text', 'of', 'a', 'survey', 'talk', 'entitled', 'painleve', 'klein', 'and', 'the', 'icosahedron', 'given', 'at', 'hitchins', '60th', 'birthday', 'conference', 'it', 'discusses', 'the', 'search', 'for', 'and', 'construction', 'of', 'algebraic', 'solutions', 'of', 'the', 'sixth', 'pai... | [-0.18939858968410872, -0.005233107901186542, -0.1109873794587906, 0.09019850428624128, -0.22176311437073534, -0.17865673082147157, -0.0464365460036273, 0.19534170408362309, -0.31027431004738387, -0.27151260523339815, 0.13261624175408213, -0.3084783539777638, -0.20284313878215246, 0.21553709826728873, -0.08657620005635... |
707.3376 | On the onset of galactic winds in quiescent star forming galaxies | We studied the effect of supernovae feedback on a disk galaxy, taking into
account the impact of infalling gas on both the star formation history and the
corresponding outflow structure, the apparition of a supernovae-driven wind
being highly sensitive to the halo mass, the galaxy spin and the star formation
efficien... | astro-ph | we studied the effect of supernovae feedback on a disk galaxy taking into account the impact of infalling gas on both the star formation history and the corresponding outflow structure the apparition of a supernovaedriven wind being highly sensitive to the halo mass the galaxy spin and the star formation efficiency we ... | [['we', 'studied', 'the', 'effect', 'of', 'supernovae', 'feedback', 'on', 'a', 'disk', 'galaxy', 'taking', 'into', 'account', 'the', 'impact', 'of', 'infalling', 'gas', 'on', 'both', 'the', 'star', 'formation', 'history', 'and', 'the', 'corresponding', 'outflow', 'structure', 'the', 'apparition', 'of', 'a', 'supernovae... | [-0.08783028964787833, 0.10767235426970047, -0.07167040049119695, 0.12066481295562685, -0.13541808142326772, -0.06484242038137905, 0.019956063256985998, 0.39722620432167294, -0.19800809303460193, -0.3391160856013837, 0.05088245593698176, -0.2549975317930505, 0.006511550797489748, 0.21332464190933548, 0.0179132519216892... |
707.3377 | One-loop corrections to a scalar field during inflation | The leading quantum correction to the power spectrum of a
gravitationally-coupled light scalar field is calculated, assuming that it is
generated during a phase of single-field, slow-roll inflation.
| astro-ph gr-qc hep-th | the leading quantum correction to the power spectrum of a gravitationallycoupled light scalar field is calculated assuming that it is generated during a phase of singlefield slowroll inflation | [['the', 'leading', 'quantum', 'correction', 'to', 'the', 'power', 'spectrum', 'of', 'a', 'gravitationallycoupled', 'light', 'scalar', 'field', 'is', 'calculated', 'assuming', 'that', 'it', 'is', 'generated', 'during', 'a', 'phase', 'of', 'singlefield', 'slowroll', 'inflation']] | [-0.18318414277330572, 0.2385216706565448, -0.1740742830027427, 0.09179734156766374, -0.05534427134054048, -0.17895468380967422, -0.04950297270469101, 0.28626618321452824, -0.21075482919280017, -0.26060413496036616, 0.03139659549508776, -0.21247509813734464, -0.12452015719775643, 0.19710719691855566, -0.021018989849835... |
707.3378 | One-loop corrections to the curvature perturbation from inflation | An estimate of the one-loop correction to the power spectrum of the
primordial curvature perturbation is given, assuming it is generated during a
phase of single-field, slow-roll inflation. The loop correction splits into two
parts, which can be calculated separately: a purely quantum-mechanical
contribution which is... | astro-ph gr-qc hep-th | an estimate of the oneloop correction to the power spectrum of the primordial curvature perturbation is given assuming it is generated during a phase of singlefield slowroll inflation the loop correction splits into two parts which can be calculated separately a purely quantummechanical contribution which is generated ... | [['an', 'estimate', 'of', 'the', 'oneloop', 'correction', 'to', 'the', 'power', 'spectrum', 'of', 'the', 'primordial', 'curvature', 'perturbation', 'is', 'given', 'assuming', 'it', 'is', 'generated', 'during', 'a', 'phase', 'of', 'singlefield', 'slowroll', 'inflation', 'the', 'loop', 'correction', 'splits', 'into', 'tw... | [-0.13460904797391285, 0.18820522708454748, -0.13816211794296074, 0.09913718305058807, -0.06047667298347704, -0.10704498848183051, -0.038683104371312, 0.2521021794527769, -0.28920126151263953, -0.2706574178079054, 0.08115259483770748, -0.3033533668707287, -0.10295983753767649, 0.1805599600313202, 0.009125166846114018, ... |
707.3379 | The ratio of sigma_L/sigma_T in DIS at low x | Assuming helicity independence for q-qbar scattering in the color-dipole
picture, or, equivalently proportionality of sea quark and gluon distributions,
we find R(W^2,Q^2) = 0.5 (approximately) at large Q^2, where R(W^2,Q^2) denotes
the ratio of the longitudinal and transverse photoabsorption cross sections.
The fort... | hep-ph | assuming helicity independence for qqbar scattering in the colordipole picture or equivalently proportionality of sea quark and gluon distributions we find rw2q2 05 approximately at large q2 where rw2q2 denotes the ratio of the longitudinal and transverse photoabsorption cross sections the forthcoming direct measuremen... | [['assuming', 'helicity', 'independence', 'for', 'qqbar', 'scattering', 'in', 'the', 'colordipole', 'picture', 'or', 'equivalently', 'proportionality', 'of', 'sea', 'quark', 'and', 'gluon', 'distributions', 'we', 'find', 'rw2q2', '05', 'approximately', 'at', 'large', 'q2', 'where', 'rw2q2', 'denotes', 'the', 'ratio', '... | [-0.09098701088640944, 0.23372345619817386, -0.07633758024400417, 0.16220897049555238, -0.013502892317636957, -0.07101434311073906, 0.03391495586113723, 0.306572722306229, -0.18784725929628004, -0.2632470908662621, -0.056163564906455576, -0.31462403636355446, 0.05749803870687929, 0.11047133505959415, 0.1081196258969183... |
707.338 | The Fifth Data Release of the Sloan Digital Sky Survey | This paper describes the Fifth Data Release (DR5) of the Sloan Digital Sky
Survey (SDSS). DR5 includes all survey quality data taken through June 2005 and
represents the completion of the SDSS-I project (whose successor, SDSS-II will
continue through mid-2008). It includes five-band photometric data for 217
million o... | astro-ph | this paper describes the fifth data release dr5 of the sloan digital sky survey sdss dr5 includes all survey quality data taken through june 2005 and represents the completion of the sdssi project whose successor sdssii will continue through mid2008 it includes fiveband photometric data for 217 million objects selected... | [['this', 'paper', 'describes', 'the', 'fifth', 'data', 'release', 'dr5', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'dr5', 'includes', 'all', 'survey', 'quality', 'data', 'taken', 'through', 'june', '2005', 'and', 'represents', 'the', 'completion', 'of', 'the', 'sdssi', 'project', 'whose', 'successor', ... | [-0.0495238081115043, 0.002938924176493587, -0.04241970643874612, 0.05667857465909159, -0.15301680723569414, 0.027270344803018712, 0.07010150891689677, 0.36806213839094065, -0.17232862621800735, -0.39048740300011703, 0.10666869907033781, -0.4079600579011665, -0.0010513864817259073, 0.24293371205941341, -0.0173528135023... |
707.3381 | X-ray scattering from stepped and kinked surfaces: An approach with the
paracrystal model | A general formalism of X-ray scattering from different kinds of surface
morphologies is described. Based on a description of the surface morphology at
the atomic scale through the use of the paracrystal model and discrete
distributions of distances, the scattered intensity by non-periodic surfaces is
calculated over ... | cond-mat.mtrl-sci | a general formalism of xray scattering from different kinds of surface morphologies is described based on a description of the surface morphology at the atomic scale through the use of the paracrystal model and discrete distributions of distances the scattered intensity by nonperiodic surfaces is calculated over the wh... | [['a', 'general', 'formalism', 'of', 'xray', 'scattering', 'from', 'different', 'kinds', 'of', 'surface', 'morphologies', 'is', 'described', 'based', 'on', 'a', 'description', 'of', 'the', 'surface', 'morphology', 'at', 'the', 'atomic', 'scale', 'through', 'the', 'use', 'of', 'the', 'paracrystal', 'model', 'and', 'disc... | [-0.08238143807819197, 0.1611545654882524, -0.11121117229983489, 0.027464693230611563, -0.008490729788596283, -0.10463783594105504, 0.02353796675634473, 0.4046135720199169, -0.26177751652743503, -0.2687754598168184, 0.050226066558649626, -0.23723030843035275, -0.13686668332805163, 0.18248423126547028, -0.01039264040543... |
707.3382 | Generalized-Ensemble Algorithms for Protein Folding Simulations | Conventional simulations of complex systems in the canonical ensemble suffer
from the quasi-ergodicity problem. A simulation in generalized ensemble
overcomes this difficulty by performing a random walk in potential energy space
and other parameter space. From only one simulation run, one can obtain
canonical-ensembl... | cond-mat.stat-mech cond-mat.soft | conventional simulations of complex systems in the canonical ensemble suffer from the quasiergodicity problem a simulation in generalized ensemble overcomes this difficulty by performing a random walk in potential energy space and other parameter space from only one simulation run one can obtain canonicalensemble avera... | [['conventional', 'simulations', 'of', 'complex', 'systems', 'in', 'the', 'canonical', 'ensemble', 'suffer', 'from', 'the', 'quasiergodicity', 'problem', 'a', 'simulation', 'in', 'generalized', 'ensemble', 'overcomes', 'this', 'difficulty', 'by', 'performing', 'a', 'random', 'walk', 'in', 'potential', 'energy', 'space'... | [-0.057282983722603494, 0.10618112754423682, -0.10008698813023739, 0.09155426425265842, 0.017452619883103992, -0.12153686777524211, 0.04239670207093963, 0.4022129536697678, -0.2867951994287033, -0.31551594541901173, 0.10658509156814498, -0.25395614557954316, -0.160053906307154, 0.23047299881228336, -0.00276170197563866... |
707.3383 | Relaxation to equilibrium driven via indirect control in Markovian
dynamics | We characterize to what extent it is possible to modify the stationary states
of a quantum dynamical semigroup, that describes the irreversible evolution of
a two-level system, by means of an auxiliary two-level system. We consider
systems that can be initially entangled or uncorrelated. We find that the
indirect con... | quant-ph | we characterize to what extent it is possible to modify the stationary states of a quantum dynamical semigroup that describes the irreversible evolution of a twolevel system by means of an auxiliary twolevel system we consider systems that can be initially entangled or uncorrelated we find that the indirect control of ... | [['we', 'characterize', 'to', 'what', 'extent', 'it', 'is', 'possible', 'to', 'modify', 'the', 'stationary', 'states', 'of', 'a', 'quantum', 'dynamical', 'semigroup', 'that', 'describes', 'the', 'irreversible', 'evolution', 'of', 'a', 'twolevel', 'system', 'by', 'means', 'of', 'an', 'auxiliary', 'twolevel', 'system', '... | [-0.17595787332945068, 0.21010790545929545, -0.10702332541007888, 0.09429773919635101, 0.008503895062445239, -0.15392567810312205, 0.024860155112533408, 0.35916237804022705, -0.30546949670783113, -0.23419331751957342, 0.09488171395277242, -0.2548967837960786, -0.14690786239376605, 0.16544822208861543, -0.02838283018874... |
707.3384 | On the fusion matrix of the N=1 Neveu-Schwarz blocks | We propose an exact form of the fusion matrix of the Neveu-Schwarz blocks
that appear in a correlation function of four super-primary fields.
Orthogonality relation satisfied by this matrix is equivalent to the bootstrap
equation for the four-point super-primary correlator in the N=1 supersymmetric
Liouville theory.
| hep-th | we propose an exact form of the fusion matrix of the neveuschwarz blocks that appear in a correlation function of four superprimary fields orthogonality relation satisfied by this matrix is equivalent to the bootstrap equation for the fourpoint superprimary correlator in the n1 supersymmetric liouville theory | [['we', 'propose', 'an', 'exact', 'form', 'of', 'the', 'fusion', 'matrix', 'of', 'the', 'neveuschwarz', 'blocks', 'that', 'appear', 'in', 'a', 'correlation', 'function', 'of', 'four', 'superprimary', 'fields', 'orthogonality', 'relation', 'satisfied', 'by', 'this', 'matrix', 'is', 'equivalent', 'to', 'the', 'bootstrap'... | [-0.1596799850281652, 0.12683155123712544, -0.06907027765460637, 0.12996354411639596, -0.010355690656148869, -0.13251443586879127, -0.033703199848431446, 0.30089274822207895, -0.20959288169346427, -0.18239263304428238, 0.08754851698430012, -0.27324299168084626, -0.22901101585518083, 0.06698613759616147, 0.0055220002845... |
707.3385 | DARWIN mission proposal to ESA | The discovery of extra-solar planets is one of the greatest achievements of
modern astronomy. There are now more than 200 such objects known, and the
recent detection of planets with masses approximately 5 times that of Earth
demonstrates that extra-solar planets of low mass exist. In addition to
providing a wealth o... | astro-ph | the discovery of extrasolar planets is one of the greatest achievements of modern astronomy there are now more than 200 such objects known and the recent detection of planets with masses approximately 5 times that of earth demonstrates that extrasolar planets of low mass exist in addition to providing a wealth of scien... | [['the', 'discovery', 'of', 'extrasolar', 'planets', 'is', 'one', 'of', 'the', 'greatest', 'achievements', 'of', 'modern', 'astronomy', 'there', 'are', 'now', 'more', 'than', '200', 'such', 'objects', 'known', 'and', 'the', 'recent', 'detection', 'of', 'planets', 'with', 'masses', 'approximately', '5', 'times', 'that',... | [-0.08066510007520725, 0.14970787482925976, -0.05051511274414915, 0.07138913103137637, -0.12783528154250234, -0.0198802388305599, 0.03209565655708525, 0.30762476514423664, -0.21123038396486848, -0.41742030370544314, 0.09544699949866656, -0.296700104717401, -0.1701962814601492, 0.2469244238513793, -0.0780578997174773, 0... |
707.3386 | Galilei invariant theories. III. Wave equations for massless fields | Galilei invariant equations for massless fields are obtained via contractions
of relativistic wave equations. It is shown that the collection of
non-equivalent Galilei-invariant wave equations for massless fields with spin
equal 1 and 0 is very broad and describes many physically consistent systems.
In particular, th... | math-ph math.MP quant-ph | galilei invariant equations for massless fields are obtained via contractions of relativistic wave equations it is shown that the collection of nonequivalent galileiinvariant wave equations for massless fields with spin equal 1 and 0 is very broad and describes many physically consistent systems in particular there exi... | [['galilei', 'invariant', 'equations', 'for', 'massless', 'fields', 'are', 'obtained', 'via', 'contractions', 'of', 'relativistic', 'wave', 'equations', 'it', 'is', 'shown', 'that', 'the', 'collection', 'of', 'nonequivalent', 'galileiinvariant', 'wave', 'equations', 'for', 'massless', 'fields', 'with', 'spin', 'equal',... | [-0.20006275313351404, 0.2317612567942028, -0.027402546626758086, 0.0608986396093738, -0.07056543014127098, -0.13529459447663736, -0.12418772629781129, 0.30796352549366757, -0.20946863166069332, -0.26542038613394514, 0.06106819102559749, -0.3027076269053433, -0.12510993887912736, 0.22810634322566528, 0.0147389862877763... |
707.3387 | On the dynamics of the universe in $D$ spatial dimensions | In this paper we present the equations of the evolution of the universe in
$D$ spatial dimensions, as a generalization of the work of Lima \citep{lima}.
We discuss the Friedmann-Robertson-Walker cosmological equations in $D$ spatial
dimensions for a simple fluid with equation of state $p=\omega_{D}\rho$. It is
possib... | gr-qc | in this paper we present the equations of the evolution of the universe in d spatial dimensions as a generalization of the work of lima citeplima we discuss the friedmannrobertsonwalker cosmological equations in d spatial dimensions for a simple fluid with equation of state pomega_drho it is possible to reduce the mult... | [['in', 'this', 'paper', 'we', 'present', 'the', 'equations', 'of', 'the', 'evolution', 'of', 'the', 'universe', 'in', 'd', 'spatial', 'dimensions', 'as', 'a', 'generalization', 'of', 'the', 'work', 'of', 'lima', 'citeplima', 'we', 'discuss', 'the', 'friedmannrobertsonwalker', 'cosmological', 'equations', 'in', 'd', 's... | [-0.14887639572629244, 0.10812872605254223, -0.12124917823292897, 0.025914622655679995, -0.07933907000453654, -0.09300670573811529, -0.029844001828484793, 0.2660338171569512, -0.27274560980855467, -0.26885600900607753, 0.05952695267958606, -0.2412724167385951, -0.13499052531799263, 0.15273127726655691, -0.0387972757114... |
707.3388 | Complex Networks in and beyond Physics | Physicists study a wide variety of phenomena creating new interdisciplinary
research fields by applying theories and methods originally developed in
physics in order to solve problems in economics, social science, biology,
medicine, technology, etc. In their turn, these different branches of science
inspire the inven... | physics.pop-ph physics.soc-ph | physicists study a wide variety of phenomena creating new interdisciplinary research fields by applying theories and methods originally developed in physics in order to solve problems in economics social science biology medicine technology etc in their turn these different branches of science inspire the invention of n... | [['physicists', 'study', 'a', 'wide', 'variety', 'of', 'phenomena', 'creating', 'new', 'interdisciplinary', 'research', 'fields', 'by', 'applying', 'theories', 'and', 'methods', 'originally', 'developed', 'in', 'physics', 'in', 'order', 'to', 'solve', 'problems', 'in', 'economics', 'social', 'science', 'biology', 'medi... | [-0.05985048246765209, 0.0896412271675804, -0.05619001072500983, 0.12478008442257922, -0.13816029177978634, -0.13322330779365954, -0.007225812617839584, 0.29451454055886117, -0.29861983695938704, -0.3626584617646351, 0.1077001670360445, -0.2354151120574604, -0.2729763641127295, 0.2490860752502246, -0.1424500250317637, ... |
707.3389 | In-medium chiral SU(3) dynamics and hypernuclear structure | A previously introduced relativistic energy density functional, successfully
applied to ordinary nuclei, is extended to hypernuclei. The density-dependent
mean field and the spin-orbit potential are consistently calculated for a
$\Lambda$ hyperon in the nucleus using the SU(3) extension of in-medium chiral
perturbati... | nucl-th | a previously introduced relativistic energy density functional successfully applied to ordinary nuclei is extended to hypernuclei the densitydependent mean field and the spinorbit potential are consistently calculated for a lambda hyperon in the nucleus using the su3 extension of inmedium chiral perturbation theory the... | [['a', 'previously', 'introduced', 'relativistic', 'energy', 'density', 'functional', 'successfully', 'applied', 'to', 'ordinary', 'nuclei', 'is', 'extended', 'to', 'hypernuclei', 'the', 'densitydependent', 'mean', 'field', 'and', 'the', 'spinorbit', 'potential', 'are', 'consistently', 'calculated', 'for', 'a', 'lambda... | [-0.1146622688320349, 0.19599440425838566, -0.0786867783535854, 0.15068038245499338, -0.049395246714993846, -0.10681791673414409, 0.007849147878914664, 0.341387111635413, -0.2109001778298989, -0.28177414064703044, -0.06269955129118898, -0.3038013088007574, -0.058563771681292565, 0.06774804046108329, 0.07575899330731772... |
707.339 | Consistency of the group Lasso and multiple kernel learning | We consider the least-square regression problem with regularization by a
block 1-norm, i.e., a sum of Euclidean norms over spaces of dimensions larger
than one. This problem, referred to as the group Lasso, extends the usual
regularization by the 1-norm where all spaces have dimension one, where it is
commonly referr... | cs.LG | we consider the leastsquare regression problem with regularization by a block 1norm ie a sum of euclidean norms over spaces of dimensions larger than one this problem referred to as the group lasso extends the usual regularization by the 1norm where all spaces have dimension one where it is commonly referred to as the ... | [['we', 'consider', 'the', 'leastsquare', 'regression', 'problem', 'with', 'regularization', 'by', 'a', 'block', '1norm', 'ie', 'a', 'sum', 'of', 'euclidean', 'norms', 'over', 'spaces', 'of', 'dimensions', 'larger', 'than', 'one', 'this', 'problem', 'referred', 'to', 'as', 'the', 'group', 'lasso', 'extends', 'the', 'us... | [-0.024448219888976642, 0.026122059772273394, -0.07778817522206477, 0.13311154655912624, -0.09630693503389401, -0.1772435708849558, 0.01132288623135537, 0.3796408810360091, -0.29601162583567203, -0.23967430670878717, 0.19031086514105222, -0.2384288747395788, -0.18216484245877446, 0.15062574927029865, -0.127149265735144... |
707.3391 | Hadronic single inclusive kt distributions inside one jet beyond MLLA | The hadronic kt-spectrum inside one jet is determined including corrections
of relative magnitude sqrt{alpha_s} with respect to the Modified Leading
Logarithmic Approximation (MLLA), at and beyond the limiting spectrum (assuming
an infrared cut-off Q_0 = Lambda_QCD and Q_0 not = Lambda_QCD). The agreement
between our... | hep-ph hep-ex | the hadronic ktspectrum inside one jet is determined including corrections of relative magnitude sqrtalpha_s with respect to the modified leading logarithmic approximation mlla at and beyond the limiting spectrum assuming an infrared cutoff q_0 lambda_qcd and q_0 not lambda_qcd the agreement between our results and pre... | [['the', 'hadronic', 'ktspectrum', 'inside', 'one', 'jet', 'is', 'determined', 'including', 'corrections', 'of', 'relative', 'magnitude', 'sqrtalpha_s', 'with', 'respect', 'to', 'the', 'modified', 'leading', 'logarithmic', 'approximation', 'mlla', 'at', 'and', 'beyond', 'the', 'limiting', 'spectrum', 'assuming', 'an', ... | [-0.04129480493899721, 0.13415262591868388, -0.13456241835195284, 0.1256372046047965, -0.05217317084853466, -0.09366752052536377, 0.02987178678203446, 0.3463784968623748, -0.1649832008119959, -0.328113740894836, -0.00481207797733637, -0.3506671088246199, 0.022073211237931482, 0.17830779381597844, 0.019412300248558705, ... |
707.3392 | Neon Atoms Oscillating Inside Carbon and Boron-Nitride Nanotubes: A
Fully Atomistic Molecular Dynamics Investigation | In the present work we discuss based on extensive fully atomistic molecular
dynamics simulations the dynamics of Neon atoms oscillating inside
(5,5)single-walled carbon nanotubes (CNTs) and boron-nitride (BNNT) ones. Our
results show that sustained high frequency oscillatory regimes are possible for
a large range of ... | cond-mat.mtrl-sci | in the present work we discuss based on extensive fully atomistic molecular dynamics simulations the dynamics of neon atoms oscillating inside 55singlewalled carbon nanotubes cnts and boronnitride bnnt ones our results show that sustained high frequency oscillatory regimes are possible for a large range of temperatures... | [['in', 'the', 'present', 'work', 'we', 'discuss', 'based', 'on', 'extensive', 'fully', 'atomistic', 'molecular', 'dynamics', 'simulations', 'the', 'dynamics', 'of', 'neon', 'atoms', 'oscillating', 'inside', '55singlewalled', 'carbon', 'nanotubes', 'cnts', 'and', 'boronnitride', 'bnnt', 'ones', 'our', 'results', 'show'... | [-0.11320441772779787, 0.16207574252936854, -0.03991683078256537, 0.0036314767056021347, 0.008178005129637489, -0.10931906295401683, 0.054864233429824195, 0.4797597657664713, -0.20774992862828526, -0.2900245129523507, 0.046852100434354005, -0.2693132322957649, -0.18598407111972212, 0.19467399164428373, -0.0059670633243... |
707.3393 | Predicting C-H/$\pi$ interactions with nonlocal density functional
theory | We examine the performance of a recently developed nonlocal density
functional in predicting a model noncovalent interaction, the weak bond between
an aromatic $\pi$ system and an aliphatic C-H group. The new functional is a
significant improvement over traditional density functionals, providing results
which compare... | cond-mat.mtrl-sci | we examine the performance of a recently developed nonlocal density functional in predicting a model noncovalent interaction the weak bond between an aromatic pi system and an aliphatic ch group the new functional is a significant improvement over traditional density functionals providing results which compare favorabl... | [['we', 'examine', 'the', 'performance', 'of', 'a', 'recently', 'developed', 'nonlocal', 'density', 'functional', 'in', 'predicting', 'a', 'model', 'noncovalent', 'interaction', 'the', 'weak', 'bond', 'between', 'an', 'aromatic', 'pi', 'system', 'and', 'an', 'aliphatic', 'ch', 'group', 'the', 'new', 'functional', 'is',... | [-0.08373922498215028, 0.05341494833053205, -0.09067978550555165, 0.11962480532586306, 0.02840615109031655, -0.14223454532107896, 0.05987214304737209, 0.4081603908508094, -0.23961789391877264, -0.33910448241441216, -0.05884954361149024, -0.32498074337340815, -0.12535042688250542, 0.1574005510864453, 0.00331249350073420... |
707.3394 | Turan's theorem inverted | Turan's theorem implies that every graph of order n with more edges than the
r-partite Turan graph contains a complete graph of order r+1. We show that the
same premise implies the existence of much larger graphs. We also prove
corresponding stability theorems. These results complete work started by Erdos
in 1963.
| math.CO | turans theorem implies that every graph of order n with more edges than the rpartite turan graph contains a complete graph of order r1 we show that the same premise implies the existence of much larger graphs we also prove corresponding stability theorems these results complete work started by erdos in 1963 | [['turans', 'theorem', 'implies', 'that', 'every', 'graph', 'of', 'order', 'n', 'with', 'more', 'edges', 'than', 'the', 'rpartite', 'turan', 'graph', 'contains', 'a', 'complete', 'graph', 'of', 'order', 'r1', 'we', 'show', 'that', 'the', 'same', 'premise', 'implies', 'the', 'existence', 'of', 'much', 'larger', 'graphs'... | [-0.15844245955948003, 0.08903362090775492, -0.09645585912781265, 0.09422595554720968, -0.09861307393293828, -0.11235546343064365, 0.04623115098533722, 0.30668478964183193, -0.17951335918265754, -0.31618703566849804, 0.074941009988274, -0.33612007898493457, -0.18211400942303813, 0.12026034510479523, -0.1534796307364908... |
707.3395 | Classical Spinning Branes in Curved Backgrounds | The dynamics of a classical branelike object in a curved background is
derived from the covariant stress-energy conservation of the brane matter. The
world sheet equations and boundary conditions are obtained in the pole-dipole
approximation, where nontrivial brane thickness gives rise to its intrinsic
angular moment... | gr-qc hep-th | the dynamics of a classical branelike object in a curved background is derived from the covariant stressenergy conservation of the brane matter the world sheet equations and boundary conditions are obtained in the poledipole approximation where nontrivial brane thickness gives rise to its intrinsic angular momentum it ... | [['the', 'dynamics', 'of', 'a', 'classical', 'branelike', 'object', 'in', 'a', 'curved', 'background', 'is', 'derived', 'from', 'the', 'covariant', 'stressenergy', 'conservation', 'of', 'the', 'brane', 'matter', 'the', 'world', 'sheet', 'equations', 'and', 'boundary', 'conditions', 'are', 'obtained', 'in', 'the', 'pole... | [-0.17859141624140892, 0.16847995495689766, -0.09164091018730745, 0.09956489433626836, -0.12302287511475798, -0.12890184730927032, -0.06826703803288559, 0.327431736141628, -0.18866437886442458, -0.28381231240789584, 0.038189322210013095, -0.28515712703977314, -0.10493976466121181, 0.10160104132124356, -0.08138924724762... |
707.3396 | Self-force of a point charge in the space-time of a symmetric wormhole | We consider the self-energy and the self-force for an electrically charged
particle at rest in the wormhole space-time. We develop general approach and
apply it to two specific profiles of the wormhole throat with singular and with
smooth curvature. The self-force for these two profiles is found in manifest
form; it ... | gr-qc | we consider the selfenergy and the selfforce for an electrically charged particle at rest in the wormhole spacetime we develop general approach and apply it to two specific profiles of the wormhole throat with singular and with smooth curvature the selfforce for these two profiles is found in manifest form it is an att... | [['we', 'consider', 'the', 'selfenergy', 'and', 'the', 'selfforce', 'for', 'an', 'electrically', 'charged', 'particle', 'at', 'rest', 'in', 'the', 'wormhole', 'spacetime', 'we', 'develop', 'general', 'approach', 'and', 'apply', 'it', 'to', 'two', 'specific', 'profiles', 'of', 'the', 'wormhole', 'throat', 'with', 'singu... | [-0.15800275620713364, 0.05157931670455582, -0.12147191567928531, 0.08580861156078753, -0.07899732841469813, -0.20030737725319342, -0.08488794008735567, 0.35717117618769406, -0.15706035611219704, -0.2518014854809735, 0.037764446112851145, -0.32429936901899054, -0.14281319612055085, 0.15180697292817058, -0.0180972805304... |
707.3397 | Mixing of 1/2^- Octets under SU(3) Symmetry | We investigate the J^p=1/2^- baryons in the octets based on flavor SU(3)
symmetry. Since baryons with same quantum numbers can mix with each other, we
consider the mixing between two octets before their mixing with the singlet.
Most predicted decay widths are consistent with the experimental data, and
meanwhile we pr... | hep-ph | we investigate the jp12 baryons in the octets based on flavor su3 symmetry since baryons with same quantum numbers can mix with each other we consider the mixing between two octets before their mixing with the singlet most predicted decay widths are consistent with the experimental data and meanwhile we predict two pos... | [['we', 'investigate', 'the', 'jp12', 'baryons', 'in', 'the', 'octets', 'based', 'on', 'flavor', 'su3', 'symmetry', 'since', 'baryons', 'with', 'same', 'quantum', 'numbers', 'can', 'mix', 'with', 'each', 'other', 'we', 'consider', 'the', 'mixing', 'between', 'two', 'octets', 'before', 'their', 'mixing', 'with', 'the', ... | [-0.11914796485410382, 0.3129275700543076, -0.023316223965957762, 0.1504335208175083, -0.04524494243475298, -0.17662029541097582, 0.05427436461905018, 0.40750279985368254, -0.17695412198275637, -0.2942832881584764, -0.0011994292940168331, -0.3258540387265384, 0.024969895603135228, 0.054518882169698676, 0.10350334091732... |
707.3398 | Efficient coupling of photons to a single molecule and the observation
of its resonance fluorescence | Single dye molecules at cryogenic temperatures display many spectroscopic
phenomena known from free atoms and are thus promising candidates for
fundamental quantum optical studies. However, the existing techniques for the
detection of single molecules have either sacrificed the information on the
coherence of the exc... | quant-ph | single dye molecules at cryogenic temperatures display many spectroscopic phenomena known from free atoms and are thus promising candidates for fundamental quantum optical studies however the existing techniques for the detection of single molecules have either sacrificed the information on the coherence of the excited... | [['single', 'dye', 'molecules', 'at', 'cryogenic', 'temperatures', 'display', 'many', 'spectroscopic', 'phenomena', 'known', 'from', 'free', 'atoms', 'and', 'are', 'thus', 'promising', 'candidates', 'for', 'fundamental', 'quantum', 'optical', 'studies', 'however', 'the', 'existing', 'techniques', 'for', 'the', 'detecti... | [-0.09001337845394439, 0.14450317411457356, -0.038201505173551475, 0.008396157720739752, -0.01670357503777219, -0.1599339067250037, 0.06414843576400213, 0.42774614003310735, -0.2507111214740812, -0.32325214940135844, 0.04337842723062086, -0.30521419022802176, -0.05708594316761387, 0.2364186085870716, 0.0422000418631698... |
707.3399 | Nonlinear analysis of a simple model of temperature evolution in a
satellite | We analyse a simple model of the heat transfer to and from a small satellite
orbiting round a solar system planet. Our approach considers the satellite
isothermal, with external heat input from the environment and from internal
energy dissipation, and output to the environment as black-body radiation. The
resulting n... | physics.space-ph math-ph math.MP nlin.CD | we analyse a simple model of the heat transfer to and from a small satellite orbiting round a solar system planet our approach considers the satellite isothermal with external heat input from the environment and from internal energy dissipation and output to the environment as blackbody radiation the resulting nonlinea... | [['we', 'analyse', 'a', 'simple', 'model', 'of', 'the', 'heat', 'transfer', 'to', 'and', 'from', 'a', 'small', 'satellite', 'orbiting', 'round', 'a', 'solar', 'system', 'planet', 'our', 'approach', 'considers', 'the', 'satellite', 'isothermal', 'with', 'external', 'heat', 'input', 'from', 'the', 'environment', 'and', '... | [-0.12954406206630018, 0.1275006388929036, -0.08926347554151019, 0.05561417098275118, -0.024136437294519926, -0.09299193959912821, 0.08174876688679757, 0.3376014547371497, -0.25696861266783655, -0.30567761214628614, 0.10270588170284124, -0.2726585648201202, -0.09830814027482618, 0.24205479409054484, -0.0349603766145725... |
707.34 | The Physics of Maxwell's demon and information | Maxwell's demon was born in 1867 and still thrives in modern physics. He
plays important roles in clarifying the connections between two theories:
thermodynamics and information. Here, we present the history of the demon and a
variety of interesting consequences of the second law of thermodynamics, mainly
in quantum ... | physics.hist-ph quant-ph | maxwells demon was born in 1867 and still thrives in modern physics he plays important roles in clarifying the connections between two theories thermodynamics and information here we present the history of the demon and a variety of interesting consequences of the second law of thermodynamics mainly in quantum mechanic... | [['maxwells', 'demon', 'was', 'born', 'in', '1867', 'and', 'still', 'thrives', 'in', 'modern', 'physics', 'he', 'plays', 'important', 'roles', 'in', 'clarifying', 'the', 'connections', 'between', 'two', 'theories', 'thermodynamics', 'and', 'information', 'here', 'we', 'present', 'the', 'history', 'of', 'the', 'demon', ... | [-0.1217386006667256, 0.11909949023094846, -0.13408885724138378, 0.07311264897991972, -0.06364207493748925, -0.13069294585005903, 0.03200867905554066, 0.26691289133642143, -0.2600536520149922, -0.3328388479152104, 0.05176167064289585, -0.30183072251881043, -0.234470026244863, 0.20106794321682395, -0.10049393284134567, ... |
707.3401 | Limit laws for boolean convolutions | We study the distributional behavior for products, and for sums of boolean
independent random variables in an infinitesimal triangular array. We show that
the limit laws of boolean convolutions are determined by the limit laws of free
convolutions, and vice versa. We further use these results to show several
connecti... | math.OA math.PR | we study the distributional behavior for products and for sums of boolean independent random variables in an infinitesimal triangular array we show that the limit laws of boolean convolutions are determined by the limit laws of free convolutions and vice versa we further use these results to show several connections be... | [['we', 'study', 'the', 'distributional', 'behavior', 'for', 'products', 'and', 'for', 'sums', 'of', 'boolean', 'independent', 'random', 'variables', 'in', 'an', 'infinitesimal', 'triangular', 'array', 'we', 'show', 'that', 'the', 'limit', 'laws', 'of', 'boolean', 'convolutions', 'are', 'determined', 'by', 'the', 'limi... | [-0.08074105329190691, 0.11499362615200553, -0.08565328784215336, 0.06886857271176548, -0.04425914124705088, -0.05409290327523381, 0.07009094506979753, 0.3760669566690922, -0.31950809276447845, -0.18955141465919903, 0.13686423922459093, -0.27944616424158597, -0.20503346626766217, 0.23923206555609328, -0.054645747352295... |
707.3402 | Synchronized Collective Behavior via Low-cost Communication | An important natural phenomenon surfaces that satisfactory synchronization of
self-driven particles can be achieved via sharply reduced communication cost,
especially for high density particle groups with low external noise.
Statistical numerical evidence illustrates that a highly efficient manner is to
distribute th... | physics.data-an physics.gen-ph | an important natural phenomenon surfaces that satisfactory synchronization of selfdriven particles can be achieved via sharply reduced communication cost especially for high density particle groups with low external noise statistical numerical evidence illustrates that a highly efficient manner is to distribute the com... | [['an', 'important', 'natural', 'phenomenon', 'surfaces', 'that', 'satisfactory', 'synchronization', 'of', 'selfdriven', 'particles', 'can', 'be', 'achieved', 'via', 'sharply', 'reduced', 'communication', 'cost', 'especially', 'for', 'high', 'density', 'particle', 'groups', 'with', 'low', 'external', 'noise', 'statisti... | [-0.2129100841934012, 0.21858412400326735, -0.06796210427145365, 0.07941705693012997, -0.052809717450359395, -0.22252688669644105, 0.10175501103239025, 0.38430125250563246, -0.26632517180405557, -0.317348867041908, 0.0983542092692326, -0.2515172158189885, -0.1868288733633509, 0.17039128756304683, -0.11168672266306684, ... |
707.3403 | On the noncommutative spin geometry of the standard Podles sphere and
index computations | The purpose of the paper is twofold: First, known results of the
noncommutative spin geometry of the standard Podles sphere are extended by
discussing Poincare duality and orientability. In the discussion of
orientability, Hochschild homology is replaced by a twisted version which
avoids the dimension drop. The twist... | math.QA math.KT | the purpose of the paper is twofold first known results of the noncommutative spin geometry of the standard podles sphere are extended by discussing poincare duality and orientability in the discussion of orientability hochschild homology is replaced by a twisted version which avoids the dimension drop the twisted hoch... | [['the', 'purpose', 'of', 'the', 'paper', 'is', 'twofold', 'first', 'known', 'results', 'of', 'the', 'noncommutative', 'spin', 'geometry', 'of', 'the', 'standard', 'podles', 'sphere', 'are', 'extended', 'by', 'discussing', 'poincare', 'duality', 'and', 'orientability', 'in', 'the', 'discussion', 'of', 'orientability', ... | [-0.23331812233540905, 0.10844995877583863, -0.08755869514717864, 0.0973018174516727, -0.09901259711909073, -0.13218778135284545, -0.0325981888460567, 0.30863379079493736, -0.35767472307715154, -0.21980150240084168, 0.08993817171853075, -0.2034654986068961, -0.17448864917630558, 0.1824684175022104, -0.1525407329044014,... |
707.3404 | Kouchnirenko type formulas for local invariants of plane analytic curves | Let f(x,y)=0 be an equation of plane analytic curve defined in the
neighborhood of the origin and let $\pi:M\to(\Cn^2,0)$ be a local toric
modification. We give a formula which connects a number of double points
\delta_0(f)$ with a sum $\sum_p \delta_p(\tilde f)$ which runs over all
intersection points of the proper ... | math.AG | let fxy0 be an equation of plane analytic curve defined in the neighborhood of the origin and let pimtocn20 be a local toric modification we give a formula which connects a number of double points delta_0f with a sum sum_p delta_ptilde f which runs over all intersection points of the proper preimage of f0 with the exce... | [['let', 'fxy0', 'be', 'an', 'equation', 'of', 'plane', 'analytic', 'curve', 'defined', 'in', 'the', 'neighborhood', 'of', 'the', 'origin', 'and', 'let', 'pimtocn20', 'be', 'a', 'local', 'toric', 'modification', 'we', 'give', 'a', 'formula', 'which', 'connects', 'a', 'number', 'of', 'double', 'points', 'delta_0f', 'wit... | [-0.24795523998750882, 0.011326648221107792, -0.1643193213099783, -0.02928850388323719, -0.08715598270805044, -0.14327275509184056, 0.07317614059217951, 0.24264570484784517, -0.3169942830773917, -0.20846106374678625, 0.045085463501428336, -0.27765335007147357, -0.09667454453354532, 0.2205652579665184, -0.07481532554057... |
707.3405 | Large scale ab initio calculations based on three levels of
parallelization | We suggest and implement a parallelization scheme based on an efficient
multiband eigenvalue solver, called the locally optimal block preconditioned
conjugate gradient LOBPCG method, and using an optimized three-dimensional (3D)
fast Fourier transform (FFT) in the ab initio}plane-wave code ABINIT. In
addition to the ... | cond-mat.mtrl-sci | we suggest and implement a parallelization scheme based on an efficient multiband eigenvalue solver called the locally optimal block preconditioned conjugate gradient lobpcg method and using an optimized threedimensional 3d fast fourier transform fft in the ab initioplanewave code abinit in addition to the standard dat... | [['we', 'suggest', 'and', 'implement', 'a', 'parallelization', 'scheme', 'based', 'on', 'an', 'efficient', 'multiband', 'eigenvalue', 'solver', 'called', 'the', 'locally', 'optimal', 'block', 'preconditioned', 'conjugate', 'gradient', 'lobpcg', 'method', 'and', 'using', 'an', 'optimized', 'threedimensional', '3d', 'fas... | [-0.12523845671271178, 0.010540205600179054, -0.05878182764089904, 0.008569608913931232, -0.07033208264934582, -0.15014632688025417, 0.07764528523870275, 0.4343335731707004, -0.29867117760575707, -0.30877225141377934, 0.10285337659622895, -0.23566677190525376, -0.08919825788980686, 0.26532552467936776, -0.0189620891198... |
707.3406 | On the gravitational stability of D1-D5-P black holes | We examine the stability of the nonextremal D1-D5-P black hole solutions. In
particular, we look for the appearance of a superradiant instability for the
spinning black holes but we find no evidence of such an instability. We compare
this situation with that for the smooth soliton geometries, which were recently
obse... | hep-th gr-qc | we examine the stability of the nonextremal d1d5p black hole solutions in particular we look for the appearance of a superradiant instability for the spinning black holes but we find no evidence of such an instability we compare this situation with that for the smooth soliton geometries which were recently observed to ... | [['we', 'examine', 'the', 'stability', 'of', 'the', 'nonextremal', 'd1d5p', 'black', 'hole', 'solutions', 'in', 'particular', 'we', 'look', 'for', 'the', 'appearance', 'of', 'a', 'superradiant', 'instability', 'for', 'the', 'spinning', 'black', 'holes', 'but', 'we', 'find', 'no', 'evidence', 'of', 'such', 'an', 'instab... | [-0.15336846309140897, 0.07396806911610139, -0.07625497701861744, 0.15506531772955964, -0.06729261786318742, -0.13209451712811224, -0.010037087061657355, 0.3029272802174091, -0.14386518753778477, -0.23280943982446423, 0.13270941099259428, -0.30655323622318414, -0.14473956174288805, 0.2009905715401356, -0.06831799150229... |
707.3407 | Faster subsequence recognition in compressed strings | Computation on compressed strings is one of the key approaches to processing
massive data sets. We consider local subsequence recognition problems on
strings compressed by straight-line programs (SLP), which is closely related to
Lempel--Ziv compression. For an SLP-compressed text of length $\bar m$, and an
uncompres... | cs.DS cs.CC cs.DM | computation on compressed strings is one of the key approaches to processing massive data sets we consider local subsequence recognition problems on strings compressed by straightline programs slp which is closely related to lempelziv compression for an slpcompressed text of length bar m and an uncompressed pattern of ... | [['computation', 'on', 'compressed', 'strings', 'is', 'one', 'of', 'the', 'key', 'approaches', 'to', 'processing', 'massive', 'data', 'sets', 'we', 'consider', 'local', 'subsequence', 'recognition', 'problems', 'on', 'strings', 'compressed', 'by', 'straightline', 'programs', 'slp', 'which', 'is', 'closely', 'related', ... | [-0.1391144087538123, 0.08706109337305752, -0.05760476104325055, 0.047554468940046335, -0.07035135784519649, -0.14380368985953407, 0.023774495668743456, 0.3873386739864262, -0.371718544542892, -0.2991185536855883, 0.10172988359662576, -0.29171737739730863, -0.08424979737968347, 0.16937373675739203, -0.11057015218309536... |
707.3408 | On a Gibbs characterization of normalized generalized Gamma processes | We show that a Gibbs characterization of normalized generalized Gamma
processes, recently obtained in Lijoi, Pr\"unster and Walker (2007), can
alternatively be derived by exploiting a characterization of exponentially
tilted Poisson-Kingman models stated in Pitman (2003). We also provide a
completion of this result i... | math.PR | we show that a gibbs characterization of normalized generalized gamma processes recently obtained in lijoi prunster and walker 2007 can alternatively be derived by exploiting a characterization of exponentially tilted poissonkingman models stated in pitman 2003 we also provide a completion of this result investigating ... | [['we', 'show', 'that', 'a', 'gibbs', 'characterization', 'of', 'normalized', 'generalized', 'gamma', 'processes', 'recently', 'obtained', 'in', 'lijoi', 'prunster', 'and', 'walker', '2007', 'can', 'alternatively', 'be', 'derived', 'by', 'exploiting', 'a', 'characterization', 'of', 'exponentially', 'tilted', 'poissonki... | [-0.09770847544012988, 0.17115389301487413, -0.14167631770575756, 0.09870493777485595, -0.0033939856593115407, -0.13959291165877805, 0.08678635148728481, 0.3529565167292708, -0.26526994117703595, -0.23594727697133347, 0.0650563089379308, -0.20761110718346765, -0.1513414862031331, 0.15010470549240099, -0.120787345987485... |
707.3409 | Faster exon assembly by sparse spliced alignment | Assembling a gene from candidate exons is an important problem in
computational biology. Among the most successful approaches to this problem is
\emph{spliced alignment}, proposed by Gelfand et al., which scores different
candidate exon chains within a DNA sequence of length $m$ by comparing them to
a known related g... | cs.DS cs.CC cs.CE q-bio.QM | assembling a gene from candidate exons is an important problem in computational biology among the most successful approaches to this problem is emphspliced alignment proposed by gelfand et al which scores different candidate exon chains within a dna sequence of length m by comparing them to a known related gene sequenc... | [['assembling', 'a', 'gene', 'from', 'candidate', 'exons', 'is', 'an', 'important', 'problem', 'in', 'computational', 'biology', 'among', 'the', 'most', 'successful', 'approaches', 'to', 'this', 'problem', 'is', 'emphspliced', 'alignment', 'proposed', 'by', 'gelfand', 'et', 'al', 'which', 'scores', 'different', 'candid... | [-0.10318333483835468, 0.038771879103046185, -0.019840111162086, 0.031296787830260506, -0.07226383104943289, -0.14595149913955419, 0.06769747743917415, 0.37700691632926464, -0.24972717807967917, -0.38845302592046926, 0.003191974655282302, -0.21439757046946248, -0.19299548453666637, 0.1855188904933204, -0.12548383596528... |
707.341 | Fubini-Griffiths-Harris rigidity and Lie algebra cohomology | We prove a general extrinsic rigidity theorem for homogeneous varieties in
$\mathbb{CP}^N$. The theorem is used to show that the adjoint variety of a
complex simple Lie algebra $\mathfrak{g}$ (the unique minimal G orbit in
$\mathbb{P}\mathfrak{g}$) is extrinsically rigid to third order.
In contrast, we show that th... | math.DG math.AG math.RT | we prove a general extrinsic rigidity theorem for homogeneous varieties in mathbbcpn the theorem is used to show that the adjoint variety of a complex simple lie algebra mathfrakg the unique minimal g orbit in mathbbpmathfrakg is extrinsically rigid to third order in contrast we show that the adjoint variety of sl_3mat... | [['we', 'prove', 'a', 'general', 'extrinsic', 'rigidity', 'theorem', 'for', 'homogeneous', 'varieties', 'in', 'mathbbcpn', 'the', 'theorem', 'is', 'used', 'to', 'show', 'that', 'the', 'adjoint', 'variety', 'of', 'a', 'complex', 'simple', 'lie', 'algebra', 'mathfrakg', 'the', 'unique', 'minimal', 'g', 'orbit', 'in', 'ma... | [-0.17601189994569338, 0.004848765679710825, -0.07561022793965005, 0.08741593921398062, -0.14601846285376366, -0.12373464939192058, -0.02812211762174843, 0.35400959539295335, -0.31842273720199377, -0.22614289283358713, 0.10986133079125916, -0.2187781328017392, -0.1845969358019955, 0.20461517186244813, -0.17020993495768... |
707.3411 | Thermotropic Biaxial Nematics: Spontaneous or Field-Stabilized? | An intermediate nematic phase is proposed for the interpretation of recent
experimental results on phase biaxiality in bent-core nematics. The phase is
macroscopically uniaxial but consists of microscopic biaxial, and possibly
polar, domains. On applying an electric field the phase exhibits substantial
macroscopic bi... | cond-mat.soft cond-mat.mtrl-sci | an intermediate nematic phase is proposed for the interpretation of recent experimental results on phase biaxiality in bentcore nematics the phase is macroscopically uniaxial but consists of microscopic biaxial and possibly polar domains on applying an electric field the phase exhibits substantial macroscopic biaxial o... | [['an', 'intermediate', 'nematic', 'phase', 'is', 'proposed', 'for', 'the', 'interpretation', 'of', 'recent', 'experimental', 'results', 'on', 'phase', 'biaxiality', 'in', 'bentcore', 'nematics', 'the', 'phase', 'is', 'macroscopically', 'uniaxial', 'but', 'consists', 'of', 'microscopic', 'biaxial', 'and', 'possibly', '... | [-0.2336644395105302, 0.2452786127616538, -0.09574988985565515, -0.07574492178630465, -0.06106037510415682, -0.06428403871802565, 0.01924694720387029, 0.404794989607464, -0.27133295595502627, -0.24665174352076763, 0.04850624367678299, -0.24708832742479175, -0.16403486259663716, 0.08444516332103656, 0.023850320557801005... |
707.3412 | Spectrophotometric investigations of Blue Compact Dwarf Galaxies:
Markarian 35 | We present results from a detailed spectrophotometric analysis of the blue
compact dwarf galaxy Mrk 35 (Haro 3), based on deep optical (B,V,R,I) and
near-IR (J,H,K) imaging, Halpha narrow-band observations and long-slit
spectroscopy. The optical emission of the galaxy is dominated by a central
young starburst, with a... | astro-ph | we present results from a detailed spectrophotometric analysis of the blue compact dwarf galaxy mrk 35 haro 3 based on deep optical bvri and nearir jhk imaging halpha narrowband observations and longslit spectroscopy the optical emission of the galaxy is dominated by a central young starburst with a barlike shape while... | [['we', 'present', 'results', 'from', 'a', 'detailed', 'spectrophotometric', 'analysis', 'of', 'the', 'blue', 'compact', 'dwarf', 'galaxy', 'mrk', '35', 'haro', '3', 'based', 'on', 'deep', 'optical', 'bvri', 'and', 'nearir', 'jhk', 'imaging', 'halpha', 'narrowband', 'observations', 'and', 'longslit', 'spectroscopy', 't... | [-0.003990622789962799, 0.07666898859356297, -0.09356184014678001, 0.10793673956999555, -0.09792434646934271, -0.08364054286852479, 0.029946943412534892, 0.49994405258074404, -0.13233531482890248, -0.3433386739343405, 0.030724824882112443, -0.29647836804110556, -0.02179793964876444, 0.18381364501547068, -0.065593647712... |
707.3413 | The Sixth Data Release of the Sloan Digital Sky Survey | With the Sixth Data Release of the Sloan Digital Sky Survey, the imaging of
the Northern Galactic Cap is now complete. The survey contains images and
parameters of roughly 287 million objects over 9583 deg^2, and 1.27 million
spectra of stars, galaxies, quasars and blank sky (for sky subtraction)
selected over 7425 d... | astro-ph | with the sixth data release of the sloan digital sky survey the imaging of the northern galactic cap is now complete the survey contains images and parameters of roughly 287 million objects over 9583 deg2 and 127 million spectra of stars galaxies quasars and blank sky for sky subtraction selected over 7425 deg2 this re... | [['with', 'the', 'sixth', 'data', 'release', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'the', 'imaging', 'of', 'the', 'northern', 'galactic', 'cap', 'is', 'now', 'complete', 'the', 'survey', 'contains', 'images', 'and', 'parameters', 'of', 'roughly', '287', 'million', 'objects', 'over', '9583', 'deg2', 'and', '... | [-0.03230009642417523, 0.08294338826423579, -0.04196482350137861, 0.07414996094485105, -0.10439247290438895, -0.0328513413927188, 0.05540704497252591, 0.44440226459604065, -0.12595765103469603, -0.4072375432830692, 0.08850260378615833, -0.36875454289111076, 0.050561241040365225, 0.2607893947812651, -0.07187597353185993... |
707.3414 | Probing the Two Greatest Mysteries of the Universe | The neutrinoless double beta decay and the direct dark matter detection
experiments probe the origins of the two greatest mysteries of the universe,
i.e. the baryon asymmetry and the invisible or dark matter. The underlying
theoretical ideas are briefly discussed along with the experimental prospects.
| hep-ph | the neutrinoless double beta decay and the direct dark matter detection experiments probe the origins of the two greatest mysteries of the universe ie the baryon asymmetry and the invisible or dark matter the underlying theoretical ideas are briefly discussed along with the experimental prospects | [['the', 'neutrinoless', 'double', 'beta', 'decay', 'and', 'the', 'direct', 'dark', 'matter', 'detection', 'experiments', 'probe', 'the', 'origins', 'of', 'the', 'two', 'greatest', 'mysteries', 'of', 'the', 'universe', 'ie', 'the', 'baryon', 'asymmetry', 'and', 'the', 'invisible', 'or', 'dark', 'matter', 'the', 'underl... | [-0.09723659963864419, 0.23933241408732203, -0.08115941513743666, 0.19338516737851832, -0.11823072861880064, -0.12076558214094904, 0.00817853667669826, 0.2463751001490487, -0.26940999833039114, -0.31175182398615614, 0.0693108475715336, -0.32554253544658424, -0.05070901697811981, 0.1805331298822744, 0.14539396072893093,... |
707.3415 | UV to IR SEDs of UV selected galaxies in the ELAIS fields: evolution of
dust attenuation and star formation activity from z=0.7 to z=0.2 | We study the ultraviolet to far-infrared (hereafter UV-to-IR) SEDs of a
sample of intermediate redshift (0.2 < z < 0.7) UV-selected galaxies from the
ELAIS-N1 and ELAIS-N2 fields by fitting a multi-wavelength dataset to a library
of GRASIL templates. Star formation related properties of the galaxies are
derived from ... | astro-ph | we study the ultraviolet to farinfrared hereafter uvtoir seds of a sample of intermediate redshift 02 z 07 uvselected galaxies from the elaisn1 and elaisn2 fields by fitting a multiwavelength dataset to a library of grasil templates star formation related properties of the galaxies are derived from the library of model... | [['we', 'study', 'the', 'ultraviolet', 'to', 'farinfrared', 'hereafter', 'uvtoir', 'seds', 'of', 'a', 'sample', 'of', 'intermediate', 'redshift', '02', 'z', '07', 'uvselected', 'galaxies', 'from', 'the', 'elaisn1', 'and', 'elaisn2', 'fields', 'by', 'fitting', 'a', 'multiwavelength', 'dataset', 'to', 'a', 'library', 'of... | [-0.024787348042831153, 0.1329823007040164, -0.04508217928164145, 0.11164959675207843, -0.08349027484312982, -0.04290541093887798, 0.06635721603536285, 0.4505111861645299, -0.09250358764456548, -0.38051250115876983, 0.012263191154559929, -0.28811087842811556, 0.020014586945192193, 0.17554300031727454, -0.05086608544076... |
707.3416 | Searching for statistical equilibrium in a dynamical multifragmentation
path | A method for identifying statistical equilibrium stages in dynamical
multifragmentation paths as provided by transport models, already successfully
tested for for the reaction ^{129}Xe+^{119}Sn at 32 MeV/u is applied here to a
higher energy reaction, ^{129}Xe+^{119}Sn at 50 MeV/u. The method evaluates
equilibrium fro... | nucl-th | a method for identifying statistical equilibrium stages in dynamical multifragmentation paths as provided by transport models already successfully tested for for the reaction 129xe119sn at 32 mevu is applied here to a higher energy reaction 129xe119sn at 50 mevu the method evaluates equilibrium from the point of view o... | [['a', 'method', 'for', 'identifying', 'statistical', 'equilibrium', 'stages', 'in', 'dynamical', 'multifragmentation', 'paths', 'as', 'provided', 'by', 'transport', 'models', 'already', 'successfully', 'tested', 'for', 'for', 'the', 'reaction', '129xe119sn', 'at', '32', 'mevu', 'is', 'applied', 'here', 'to', 'a', 'hig... | [-0.07838661534510971, 0.14166950238190268, -0.10561285115385201, 0.0724329782822206, 0.05350937546546182, -0.09160850475098586, 0.06364680691732197, 0.33412769873897863, -0.2637272006584566, -0.3234435057956872, 0.051738286670022386, -0.2896291193163653, -0.04434235918328283, 0.1657515917024685, 0.0366973015259746, 0.... |
707.3417 | When almost all sets are difference dominated | We investigate the relationship between the sizes of the sum and difference
sets attached to a subset of {0,1,...,N}, chosen randomly according to a
binomial model with parameter p(N), with N^{-1} = o(p(N)). We show that the
random subset is almost surely difference dominated, as N --> oo, for any
choice of p(N) tend... | math.NT math.PR | we investigate the relationship between the sizes of the sum and difference sets attached to a subset of 01n chosen randomly according to a binomial model with parameter pn with n1 opn we show that the random subset is almost surely difference dominated as n oo for any choice of pn tending to zero thus confirming a con... | [['we', 'investigate', 'the', 'relationship', 'between', 'the', 'sizes', 'of', 'the', 'sum', 'and', 'difference', 'sets', 'attached', 'to', 'a', 'subset', 'of', '01n', 'chosen', 'randomly', 'according', 'to', 'a', 'binomial', 'model', 'with', 'parameter', 'pn', 'with', 'n1', 'opn', 'we', 'show', 'that', 'the', 'random'... | [-0.11915106010265773, 0.1296636859180632, -0.049613327739086555, 0.049028027962880034, 0.007647966672930576, -0.12805285339296552, 0.08321033430563167, 0.3637330061987254, -0.29789243662624176, -0.26569052118847664, 0.07724854454616124, -0.33800941066575363, -0.11215905330048094, 0.18361337467654879, -0.03092954300983... |
707.3418 | Radio Frequency Spectra of 388 Bright 74 MHz Sources | As a service to the community, we have compiled radio frequency spectra from
the literature for all sources within the VLA Low Frequency Sky Survey (VLSS)
that are brighter than 15 Jy at 74 MHz. Over 160 references were used to
maximize the amount of spectral data used in the compilation of the spectra,
while also ta... | astro-ph | as a service to the community we have compiled radio frequency spectra from the literature for all sources within the vla low frequency sky survey vlss that are brighter than 15 jy at 74 mhz over 160 references were used to maximize the amount of spectral data used in the compilation of the spectra while also taking ca... | [['as', 'a', 'service', 'to', 'the', 'community', 'we', 'have', 'compiled', 'radio', 'frequency', 'spectra', 'from', 'the', 'literature', 'for', 'all', 'sources', 'within', 'the', 'vla', 'low', 'frequency', 'sky', 'survey', 'vlss', 'that', 'are', 'brighter', 'than', '15', 'jy', 'at', '74', 'mhz', 'over', '160', 'refere... | [-0.05012235645932078, 0.09435874072969266, -0.0131097851805965, 0.07198834537045992, -0.12023604365387336, -0.05227722215211768, 0.07414670623226821, 0.442467215518976, -0.1705206975523267, -0.39627782975745957, 0.13627927089002004, -0.32582511603064146, 0.020804527380081258, 0.26588274272321966, -0.025910131838508717... |
707.3419 | The Seesaw with Many Right-Handed Neutrinos | There are no upper limits on the possible number of massive, singlet
(right--handed) neutrinos that may participate in the seesaw mechanism, and
some string constructions motivate seesaw models with up to O(100)
right--handed neutrinos. In this case, the seesaw mass scale can be
significantly higher than that in the ... | hep-ph | there are no upper limits on the possible number of massive singlet righthanded neutrinos that may participate in the seesaw mechanism and some string constructions motivate seesaw models with up to o100 righthanded neutrinos in this case the seesaw mass scale can be significantly higher than that in the traditional sc... | [['there', 'are', 'no', 'upper', 'limits', 'on', 'the', 'possible', 'number', 'of', 'massive', 'singlet', 'righthanded', 'neutrinos', 'that', 'may', 'participate', 'in', 'the', 'seesaw', 'mechanism', 'and', 'some', 'string', 'constructions', 'motivate', 'seesaw', 'models', 'with', 'up', 'to', 'o100', 'righthanded', 'ne... | [-0.0980236125959946, 0.33050581909741134, 0.04629820267413587, 0.20625849126528747, -0.07870423605965587, -0.16178271182243956, 0.051682768716170585, 0.31530856926325435, -0.17956352265764203, -0.3354916969758002, 0.055981939455381775, -0.2893877031544111, -0.019384070680845505, 0.1797069741050469, 0.02776541177420908... |
707.342 | Free motion in deformed (quantum) four-dimensional space | It is shown that trajectories of free motion of the particles in deformed
("quantum") four dimensional space-time are quadratic curves.
| hep-th | it is shown that trajectories of free motion of the particles in deformed quantum four dimensional spacetime are quadratic curves | [['it', 'is', 'shown', 'that', 'trajectories', 'of', 'free', 'motion', 'of', 'the', 'particles', 'in', 'deformed', 'quantum', 'four', 'dimensional', 'spacetime', 'are', 'quadratic', 'curves']] | [-0.16904321759357116, 0.27719018324278294, -0.14759396475274117, 0.061018933198647575, -0.01494346372783184, -0.15841355454176664, -0.14209613656857983, 0.36861104555428026, -0.24753873157314957, -0.22564192105783148, 0.0060029479151126, -0.3021511442027986, -0.18324068393558263, 0.24682804327458144, -0.09145436882972... |
707.3421 | The nature of electromagnetic energy | We study the nature and location of electromagetic energy for two cases. The energy density for electromagnetic radiation is shown to be $\frac{1}{8\pi}(E^2+B^2)$, with the energy contained in the electromagnet fields. For a static charge distribution, the electromagnet energy is contained in the charge, with an energy... | physics.gen-ph | we study the nature and location of electromagetic energy for two cases the energy density for electromagnetic radiation is shown to be frac18pie2b2 with the energy contained in the electromagnet fields for a static charge distribution the electromagnet energy is contained in the charge with an energy density frac12rho... | [['we', 'study', 'the', 'nature', 'and', 'location', 'of', 'electromagetic', 'energy', 'for', 'two', 'cases', 'the', 'energy', 'density', 'for', 'electromagnetic', 'radiation', 'is', 'shown', 'to', 'be', 'frac18pie2b2', 'with', 'the', 'energy', 'contained', 'in', 'the', 'electromagnet', 'fields', 'for', 'a', 'static', ... | [-0.1476560683650682, 0.15331323249780723, -0.04448005464463227, 0.08593378577317143, -0.008058679017141974, -0.024164542927802807, -0.025735644666456628, 0.3840945267557413, -0.2100085383334636, -0.3321168051882722, 0.04681197315154747, -0.2990436042691099, -0.017958138946272517, 0.1611578278685117, -0.016943906069915... |
707.3422 | CPT and Decoherence in Quantum Gravity | In this review, I first discuss briefly some theoretical motivations for
potential Lorentz Violation and deviation from ordinary quantum mechanical
behavior (decoherence) of field theoretic systems in the background of some
quantum gravity (QG) models. Both types of effects lead to CPT violation, but
they can be dise... | hep-ph gr-qc hep-th | in this review i first discuss briefly some theoretical motivations for potential lorentz violation and deviation from ordinary quantum mechanical behavior decoherence of field theoretic systems in the background of some quantum gravity qg models both types of effects lead to cpt violation but they can be disentangled ... | [['in', 'this', 'review', 'i', 'first', 'discuss', 'briefly', 'some', 'theoretical', 'motivations', 'for', 'potential', 'lorentz', 'violation', 'and', 'deviation', 'from', 'ordinary', 'quantum', 'mechanical', 'behavior', 'decoherence', 'of', 'field', 'theoretic', 'systems', 'in', 'the', 'background', 'of', 'some', 'qua... | [-0.09710106958670171, 0.20058284969470366, -0.09403906460487987, 0.10608410744689314, -0.06764411520992776, -0.18736711605944165, 0.026053627542167054, 0.290606336493984, -0.24788398137013237, -0.2715821597020982, 0.03451882368209204, -0.2876347034821302, -0.11736155412636878, 0.162088540516135, -0.02472852237855758, ... |
707.3423 | An improved Julia-Caratheodory theorem for Schur-Agler mappings of the
unit ball | We adapt Sarason's proof of the Julia-Caratheodory theorem to the class of
Schur-Agler mappings of the unit ball, obtaining a strengthened form of this
theorem. In particular those quantities which appear in the classical theorem
and depend only on the component of the mapping in the complex normal direction
have K-l... | math.CV math.FA | we adapt sarasons proof of the juliacaratheodory theorem to the class of schuragler mappings of the unit ball obtaining a strengthened form of this theorem in particular those quantities which appear in the classical theorem and depend only on the component of the mapping in the complex normal direction have klimits no... | [['we', 'adapt', 'sarasons', 'proof', 'of', 'the', 'juliacaratheodory', 'theorem', 'to', 'the', 'class', 'of', 'schuragler', 'mappings', 'of', 'the', 'unit', 'ball', 'obtaining', 'a', 'strengthened', 'form', 'of', 'this', 'theorem', 'in', 'particular', 'those', 'quantities', 'which', 'appear', 'in', 'the', 'classical',... | [-0.1113227955730898, 0.06000908653368242, -0.09905689799260083, 0.05517567580058572, -0.0816008758764448, -0.11274260850456942, 0.0636469659595085, 0.29477825820712106, -0.2968100383877754, -0.21494023212497787, 0.14656585182196327, -0.21959001956773655, -0.10579134941716413, 0.22945243379633343, -0.11412756020269756,... |
707.3424 | IR-Improved DGLAP Theory: Kernels, Parton Distributions, Reduced Cross
Sections | It is shown that exact, amplitude-based resummation allows IR-improvement of
the usual DGLAP theory. This results in a new set of kernels, parton
distributions and attendant reduced cross sections, so that the QCD
perturbative result for the respective hadron-hadron or lepton-hadron cross
section is unchanged order-b... | hep-ph | it is shown that exact amplitudebased resummation allows irimprovement of the usual dglap theory this results in a new set of kernels parton distributions and attendant reduced cross sections so that the qcd perturbative result for the respective hadronhadron or leptonhadron cross section is unchanged orderbyorder in a... | [['it', 'is', 'shown', 'that', 'exact', 'amplitudebased', 'resummation', 'allows', 'irimprovement', 'of', 'the', 'usual', 'dglap', 'theory', 'this', 'results', 'in', 'a', 'new', 'set', 'of', 'kernels', 'parton', 'distributions', 'and', 'attendant', 'reduced', 'cross', 'sections', 'so', 'that', 'the', 'qcd', 'perturbati... | [-0.046426983085966864, 0.11896646753644116, -0.14438004086345987, 0.1516774986471038, -0.048368529336136064, -0.0596986542639817, 0.0032077990285477335, 0.36711356860160094, -0.21079955173564363, -0.24150151614513662, 0.005179538972169897, -0.30906227072661335, -0.050267633611198376, 0.18532475057333983, -0.0156394102... |
707.3425 | Norms and spectral radii of linear fractional composition operators on
the ball | We give a new proof that every linear fractional map of the unit ball induces
a bounded composition operator on the standard scale of Hilbert function spaces
on the ball, and obtain norm bounds analogous to the standard one-variable
estimates. We also show that Cowen's one-variable spectral radius formula
extends to ... | math.FA | we give a new proof that every linear fractional map of the unit ball induces a bounded composition operator on the standard scale of hilbert function spaces on the ball and obtain norm bounds analogous to the standard onevariable estimates we also show that cowens onevariable spectral radius formula extends to these o... | [['we', 'give', 'a', 'new', 'proof', 'that', 'every', 'linear', 'fractional', 'map', 'of', 'the', 'unit', 'ball', 'induces', 'a', 'bounded', 'composition', 'operator', 'on', 'the', 'standard', 'scale', 'of', 'hilbert', 'function', 'spaces', 'on', 'the', 'ball', 'and', 'obtain', 'norm', 'bounds', 'analogous', 'to', 'the... | [-0.0826340024295735, 0.0638841219208114, -0.09329563612477178, 0.09163717053709425, -0.11262463677789353, -0.10712611735543262, 0.004346553848622596, 0.319679462593304, -0.3342810380591513, -0.17850428854102549, 0.13785212971461452, -0.2615359409469856, -0.16175499959045078, 0.2250586118013279, -0.12783291688418552, 0... |
707.3426 | Reproducing kernels, de Branges-Rovnyak spaces, and norms of weighted
composition operators | We prove that the norm of a weighted composition operator on the Hardy space
H^2 of the disk is controlled by the norm of the weight function in the de
Branges-Rovnyak space associated to the symbol of the composition operator. As
a corollary we obtain a new proof of the boundedness of composition operators
on H^2, a... | math.FA | we prove that the norm of a weighted composition operator on the hardy space h2 of the disk is controlled by the norm of the weight function in the de brangesrovnyak space associated to the symbol of the composition operator as a corollary we obtain a new proof of the boundedness of composition operators on h2 and reco... | [['we', 'prove', 'that', 'the', 'norm', 'of', 'a', 'weighted', 'composition', 'operator', 'on', 'the', 'hardy', 'space', 'h2', 'of', 'the', 'disk', 'is', 'controlled', 'by', 'the', 'norm', 'of', 'the', 'weight', 'function', 'in', 'the', 'de', 'brangesrovnyak', 'space', 'associated', 'to', 'the', 'symbol', 'of', 'the', ... | [-0.08308115004769807, 0.0728083916677578, -0.0784417511293443, 0.140938502774818, -0.06629641816354565, -0.00485830310533203, 0.026936171976487757, 0.32214999427675334, -0.3103693074465377, -0.17232646623590184, 0.15162050464412072, -0.24486810289033986, -0.13069682891109904, 0.19835538637724895, -0.1254824449769357, ... |
707.3427 | Weak values and the Leggett-Garg inequality in solid-state qubits | An implementation of weak values is investigated in solid-state qubits. We
demonstrate that a weak value can be non-classical if and only if a
Leggett-Garg inequality can also be violated. Generalized weak values are
described, where post-selection on a range of weak measurement results.
Imposing classical weak value... | cond-mat.mes-hall quant-ph | an implementation of weak values is investigated in solidstate qubits we demonstrate that a weak value can be nonclassical if and only if a leggettgarg inequality can also be violated generalized weak values are described where postselection on a range of weak measurement results imposing classical weak values permits ... | [['an', 'implementation', 'of', 'weak', 'values', 'is', 'investigated', 'in', 'solidstate', 'qubits', 'we', 'demonstrate', 'that', 'a', 'weak', 'value', 'can', 'be', 'nonclassical', 'if', 'and', 'only', 'if', 'a', 'leggettgarg', 'inequality', 'can', 'also', 'be', 'violated', 'generalized', 'weak', 'values', 'are', 'des... | [-0.1571918471615661, 0.18998042234031615, -0.02843158648072465, 0.051224690462412265, -0.047716727439389636, -0.26009513951233915, 0.046168437270082636, 0.3162519231791029, -0.22993878202160467, -0.24170934203760447, 0.04561433666605955, -0.26151796383153947, -0.060993465506849254, 0.3079622513111177, -0.0656706657940... |
707.3428 | Effects of noise and confidence thresholds in nominal and metric Axelrod
dynamics of social influence | We study the effects of bounded confidence thresholds and of interaction and
external noise on Axelrod's model of social influence. Our study is based on a
combination of numerical simulations and an integration of the mean-field
Master equation describing the system in the thermodynamic limit. We find that
interacti... | physics.soc-ph cond-mat.stat-mech | we study the effects of bounded confidence thresholds and of interaction and external noise on axelrods model of social influence our study is based on a combination of numerical simulations and an integration of the meanfield master equation describing the system in the thermodynamic limit we find that interaction thr... | [['we', 'study', 'the', 'effects', 'of', 'bounded', 'confidence', 'thresholds', 'and', 'of', 'interaction', 'and', 'external', 'noise', 'on', 'axelrods', 'model', 'of', 'social', 'influence', 'our', 'study', 'is', 'based', 'on', 'a', 'combination', 'of', 'numerical', 'simulations', 'and', 'an', 'integration', 'of', 'th... | [-0.1335024407587161, 0.10226466965702943, -0.10759161392941255, 0.08373141398873461, -0.028002110239730715, -0.11841658478258305, 0.0971501840546421, 0.37990158385507866, -0.2539824424694254, -0.28629141692582466, 0.06515944915367546, -0.31777478800448655, -0.2003917352054013, 0.13772752283903297, -0.018594693162874, ... |
707.3429 | The Hot Inner Disk of FU Ori | We have constructed a detailed radiative transfer disk model which reproduces
the main features of the spectrum of the outbursting young stellar object FU
Orionis from ~ 4000 angstrom, to ~ 8 micron. Using an estimated visual
extinction Av~1.5, a steady disk model with a central star mass ~0.3 Msun and a
mass accreti... | astro-ph | we have constructed a detailed radiative transfer disk model which reproduces the main features of the spectrum of the outbursting young stellar object fu orionis from 4000 angstrom to 8 micron using an estimated visual extinction av15 a steady disk model with a central star mass 03 msun and a mass accretion rate 2e4 m... | [['we', 'have', 'constructed', 'a', 'detailed', 'radiative', 'transfer', 'disk', 'model', 'which', 'reproduces', 'the', 'main', 'features', 'of', 'the', 'spectrum', 'of', 'the', 'outbursting', 'young', 'stellar', 'object', 'fu', 'orionis', 'from', '4000', 'angstrom', 'to', '8', 'micron', 'using', 'an', 'estimated', 'vi... | [-0.06108250775122865, 0.11665087769747075, -0.07232333730620842, 0.05634778999346083, -0.07480241159623068, -0.09004135760328462, -0.001979809325759209, 0.38544717292872166, -0.22236591562212257, -0.3317871060327537, 0.08222178725108895, -0.2723003897117451, 0.013247032482321364, 0.1858022670700936, -0.066254962095920... |
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