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 |
|---|---|---|---|---|---|---|
707.453 | Stabilization of a Bose-Einstein droplet by hyperfine Rabi oscillations | A self-trapped Bose-Einstein condensate is shown to be stabilized in
two-dimensional free space by Rabi oscillations between two hyperfine states
which make an effective interatomic interaction oscillate in time. The
stabilization mechanism is elucidated by using a two-component Gross-Pitaevskii
equation combined wit... | cond-mat.other | a selftrapped boseeinstein condensate is shown to be stabilized in twodimensional free space by rabi oscillations between two hyperfine states which make an effective interatomic interaction oscillate in time the stabilization mechanism is elucidated by using a twocomponent grosspitaevskii equation combined with a vari... | [['a', 'selftrapped', 'boseeinstein', 'condensate', 'is', 'shown', 'to', 'be', 'stabilized', 'in', 'twodimensional', 'free', 'space', 'by', 'rabi', 'oscillations', 'between', 'two', 'hyperfine', 'states', 'which', 'make', 'an', 'effective', 'interatomic', 'interaction', 'oscillate', 'in', 'time', 'the', 'stabilization'... | [-0.20042813681916763, 0.26370032747133965, -0.08161548246873561, 0.09697920030941112, -0.0286474683895134, -0.1894987054222908, 0.005561431395248151, 0.35140817891806364, -0.2636264250255548, -0.22086152638523623, -0.0015605403101429916, -0.20839226584380063, -0.0960330507503106, 0.15842285108430168, 0.088840734338960... |
707.4531 | Algebraic structure of the Feynman propagator and a new correspondence
for canonical transformations | We investigate the algebraic structure of the Feynman propagator with a
general time-dependent quadratic Hamiltonian system. Using the Lie-algebraic
technique we obtain a normal-ordered form of the time-evolution operator, and
then the propagator is easily derived by a simple ``Integration Within Ordered
Product" (IW... | quant-ph | we investigate the algebraic structure of the feynman propagator with a general timedependent quadratic hamiltonian system using the liealgebraic technique we obtain a normalordered form of the timeevolution operator and then the propagator is easily derived by a simple integration within ordered product iwop technique... | [['we', 'investigate', 'the', 'algebraic', 'structure', 'of', 'the', 'feynman', 'propagator', 'with', 'a', 'general', 'timedependent', 'quadratic', 'hamiltonian', 'system', 'using', 'the', 'liealgebraic', 'technique', 'we', 'obtain', 'a', 'normalordered', 'form', 'of', 'the', 'timeevolution', 'operator', 'and', 'then',... | [-0.14343807710974943, 0.11469754907284369, -0.17382574343355373, 0.10577669352096564, -0.08978094271151349, -0.09536714817659231, 0.026796285517775686, 0.3118504462472629, -0.2807064659864409, -0.23264941842353437, 0.026917691608105088, -0.22558726438728627, -0.2353069971795776, 0.16789972838159883, 0.0046823690317978... |
707.4532 | Determination of the Superconductor-Insulator Phase Diagram for
One-Dimensional Wires | We establish the superconductor-insulator phase diagram for quasi-one
dimensional wires by measuring a large set of MoGe nanowires. This diagram is
consistent with the Chakravarty-Schmid-Bulgadaev phase boundary, namely with
the critical resistance being equal to R_Q = h/4e^2. We find that transport
properties of ins... | cond-mat.supr-con | we establish the superconductorinsulator phase diagram for quasione dimensional wires by measuring a large set of moge nanowires this diagram is consistent with the chakravartyschmidbulgadaev phase boundary namely with the critical resistance being equal to r_q h4e2 we find that transport properties of insulating nanow... | [['we', 'establish', 'the', 'superconductorinsulator', 'phase', 'diagram', 'for', 'quasione', 'dimensional', 'wires', 'by', 'measuring', 'a', 'large', 'set', 'of', 'moge', 'nanowires', 'this', 'diagram', 'is', 'consistent', 'with', 'the', 'chakravartyschmidbulgadaev', 'phase', 'boundary', 'namely', 'with', 'the', 'crit... | [-0.24191297709941864, 0.24974382687360047, -0.05250081757083535, -0.0011997727863490581, -0.00636048536747694, -0.2395955909229815, 0.09988443337380887, 0.3731120877340436, -0.20473691023886204, -0.2357604201324284, 0.008779893824830652, -0.34202519606798887, -0.1441039526835084, 0.16328389175236224, 0.007196257342584... |
707.4533 | Cascade of Complexity in Evolving Predator-Prey Dynamics | We simulate an individual-based model that represents both the phenotype and
genome of digital organisms with predator-prey interactions. We show how
open-ended growth of complexity arises from the invariance of genetic evolution
operators with respect to changes in the complexity, and that the dynamics
which emerges... | q-bio.PE | we simulate an individualbased model that represents both the phenotype and genome of digital organisms with predatorprey interactions we show how openended growth of complexity arises from the invariance of genetic evolution operators with respect to changes in the complexity and that the dynamics which emerges is con... | [['we', 'simulate', 'an', 'individualbased', 'model', 'that', 'represents', 'both', 'the', 'phenotype', 'and', 'genome', 'of', 'digital', 'organisms', 'with', 'predatorprey', 'interactions', 'we', 'show', 'how', 'openended', 'growth', 'of', 'complexity', 'arises', 'from', 'the', 'invariance', 'of', 'genetic', 'evolutio... | [-0.1273757875755881, 0.16940667304041915, -0.0949950338470058, 0.08153707956344905, -0.021913619094641144, -0.08786927377381785, 0.006046854513415107, 0.31327741828069766, -0.330217623054826, -0.25855997898774646, 0.04586214631104447, -0.25126543776555493, -0.24773876924618063, 0.14282481328259702, -0.0657592117645298... |
707.4534 | Intramolecular vibrational energy redistribution from a high frequency
mode in the presence of an internal rotor: Classical thick-layer diffusion
and quantum localization | We study the effect of an internal rotor on the classical and quantum
intramolecular vibrational energy redistribution (IVR) dynamics of a model
system with three degrees of freedom. The system is based on a Hamiltonian
proposed by Martens and Reinhardt (J. Chem. Phys. {\bf 93}, 5621 (1990).) to
study IVR in the exci... | physics.chem-ph nlin.CD | we study the effect of an internal rotor on the classical and quantum intramolecular vibrational energy redistribution ivr dynamics of a model system with three degrees of freedom the system is based on a hamiltonian proposed by martens and reinhardt j chem phys bf 93 5621 1990 to study ivr in the excited electronic st... | [['we', 'study', 'the', 'effect', 'of', 'an', 'internal', 'rotor', 'on', 'the', 'classical', 'and', 'quantum', 'intramolecular', 'vibrational', 'energy', 'redistribution', 'ivr', 'dynamics', 'of', 'a', 'model', 'system', 'with', 'three', 'degrees', 'of', 'freedom', 'the', 'system', 'is', 'based', 'on', 'a', 'hamiltonia... | [-0.17238369778609805, 0.16430179189797678, -0.06497063841755246, -0.01788293158601699, -0.023300350048474125, -0.10054688746083318, 0.08689003484699154, 0.3216696486981105, -0.2375940441214029, -0.2845261483453214, 0.03246910948655568, -0.24630713819586222, -0.13759949909252744, 0.14122557060064508, -0.017201804052737... |
707.4535 | Quantum phase transition in the two-band Hubbard model | The interaction between itinerant and Mott localized electronic states in
strongly correlated materials is studied within dynamical mean field theory in
combination with the numerical renormalization group method. A novel
nonmagnetic zero temperature quantum phase transition is found in the
bad-metallic orbital-selec... | cond-mat.str-el | the interaction between itinerant and mott localized electronic states in strongly correlated materials is studied within dynamical mean field theory in combination with the numerical renormalization group method a novel nonmagnetic zero temperature quantum phase transition is found in the badmetallic orbitalselective ... | [['the', 'interaction', 'between', 'itinerant', 'and', 'mott', 'localized', 'electronic', 'states', 'in', 'strongly', 'correlated', 'materials', 'is', 'studied', 'within', 'dynamical', 'mean', 'field', 'theory', 'in', 'combination', 'with', 'the', 'numerical', 'renormalization', 'group', 'method', 'a', 'novel', 'nonmag... | [-0.1824784705069818, 0.2905902190222627, -0.03315288089363584, 0.0809613307679279, -0.0017650461800041654, -0.2244477064943769, 0.12296998172458852, 0.3898223964645276, -0.25171766124133554, -0.22652761859168846, -0.05106341755867655, -0.36246406230779865, -0.16714314841443584, 0.08941508867659621, 0.09182486801023876... |
707.4536 | On the paper ``Weak convergence of some classes of martingales with
jumps'' | This note extends some results of Nishiyama [Ann. Probab. 28 (2000)
685--712]. A maximal inequality for stochastic integrals with respect to
integer-valued random measures which may have infinitely many jumps on compact
time intervals is given. By using it, a tightness criterion is obtained; if the
so-called quadrati... | math.PR | this note extends some results of nishiyama ann probab 28 2000 685712 a maximal inequality for stochastic integrals with respect to integervalued random measures which may have infinitely many jumps on compact time intervals is given by using it a tightness criterion is obtained if the socalled quadratic modulus is bou... | [['this', 'note', 'extends', 'some', 'results', 'of', 'nishiyama', 'ann', 'probab', '28', '2000', '685712', 'a', 'maximal', 'inequality', 'for', 'stochastic', 'integrals', 'with', 'respect', 'to', 'integervalued', 'random', 'measures', 'which', 'may', 'have', 'infinitely', 'many', 'jumps', 'on', 'compact', 'time', 'int... | [-0.10805830437623497, 0.11306048662767612, -0.1335950197119798, 0.08303546018543698, -0.051752317935184, -0.11652405431405419, 0.06167848485139465, 0.32415996259078383, -0.2640734225943951, -0.24259390995541166, 0.1481375605328053, -0.2769374192714514, -0.16858463273161933, 0.25913938603896114, -0.13400135050705148, 0... |
707.4537 | State-Relevant Maxwell's Equation from Kaluza-Klein Theory | We study a five-dimensional perfect fluid coupled with Kaluza-Klein (KK)
gravity. By dimensional reduction, a modified form of Maxwell's equation is
obtained, which is relevant to the equation of state of the source. Since the
relativistic magnetohydrodynamics (MHD) and the 3-dimensional formulation are
widely used t... | gr-qc astro-ph hep-th physics.flu-dyn physics.plasm-ph | we study a fivedimensional perfect fluid coupled with kaluzaklein kk gravity by dimensional reduction a modified form of maxwells equation is obtained which is relevant to the equation of state of the source since the relativistic magnetohydrodynamics mhd and the 3dimensional formulation are widely used to study space ... | [['we', 'study', 'a', 'fivedimensional', 'perfect', 'fluid', 'coupled', 'with', 'kaluzaklein', 'kk', 'gravity', 'by', 'dimensional', 'reduction', 'a', 'modified', 'form', 'of', 'maxwells', 'equation', 'is', 'obtained', 'which', 'is', 'relevant', 'to', 'the', 'equation', 'of', 'state', 'of', 'the', 'source', 'since', 't... | [-0.10813624143159613, 0.12981159673439774, -0.11303316111309973, 0.08633523063589131, -0.09386675063230586, -0.12481068515936371, -0.04170433349514258, 0.2540887233984397, -0.242415444923519, -0.33443245197814264, 0.06387706997434105, -0.23207863588000602, -0.08619437011371016, 0.17630444130417508, -0.0115990482125675... |
707.4538 | A Note on Polonyi Problem | We reinvestigate the cosmological Polonyi problem in the case where the
Polonyi mass is $\mathcal{O}(10) \rm{TeV}$. Such a large supersymmetry breaking
scale implies that the Polonyi field should be sequestered from the standard
model sector. Since the Polonyi field does not have a coupling to the gauge
multiplets at... | hep-ph | we reinvestigate the cosmological polonyi problem in the case where the polonyi mass is mathcalo10 rmtev such a large supersymmetry breaking scale implies that the polonyi field should be sequestered from the standard model sector since the polonyi field does not have a coupling to the gauge multiplets at tree level in... | [['we', 'reinvestigate', 'the', 'cosmological', 'polonyi', 'problem', 'in', 'the', 'case', 'where', 'the', 'polonyi', 'mass', 'is', 'mathcalo10', 'rmtev', 'such', 'a', 'large', 'supersymmetry', 'breaking', 'scale', 'implies', 'that', 'the', 'polonyi', 'field', 'should', 'be', 'sequestered', 'from', 'the', 'standard', '... | [-0.1316685640205698, 0.2734793277112422, -0.003363976499962586, 0.16557447891251217, -0.10240206840551562, -0.16556571303107948, -0.0005368711426854134, 0.290743919255005, -0.24150726391968352, -0.34128343900320707, 0.10780951621493808, -0.22029704973101616, -0.0060820300201023065, 0.10701934459567485, 0.0001079407522... |
707.4539 | Periodic relativity: the theory of gravity in flat space time | Periodic relativity (PR), uses a flat metric without weak field
approximation. PR satisfies Einstein's field equations. PR proposes a definite
connection between the proper time interval of an object and Doppler frequency
shift of its constituent particles. This is because fundamentally time is
periodic in nature. Pe... | physics.gen-ph | periodic relativity pr uses a flat metric without weak field approximation pr satisfies einsteins field equations pr proposes a definite connection between the proper time interval of an object and doppler frequency shift of its constituent particles this is because fundamentally time is periodic in nature periodic tim... | [['periodic', 'relativity', 'pr', 'uses', 'a', 'flat', 'metric', 'without', 'weak', 'field', 'approximation', 'pr', 'satisfies', 'einsteins', 'field', 'equations', 'pr', 'proposes', 'a', 'definite', 'connection', 'between', 'the', 'proper', 'time', 'interval', 'of', 'an', 'object', 'and', 'doppler', 'frequency', 'shift... | [-0.17682721720432207, 0.1752825785163315, -0.0948275936526253, 0.11068806266990028, -0.12413860503425017, -0.13611848975813165, 0.01775263122277897, 0.316676321170601, -0.21666350281837551, -0.30100297073836996, 0.0018335582999170845, -0.2558090268155198, -0.08486078935130935, 0.20746045766889099, -0.02913684219879051... |
707.454 | The first high-amplitude delta Scuti star in an eclipsing binary system | We report the discovery of the first high-amplitude delta Scuti star in an
eclipsing binary, which we have designated UNSW-V-500. The system is an
Algol-type semi-detached eclipsing binary of maximum brightness V = 12.52 mag.
A best-fitting solution to the binary light curve and two radial velocity
curves is derived ... | astro-ph | we report the discovery of the first highamplitude delta scuti star in an eclipsing binary which we have designated unswv500 the system is an algoltype semidetached eclipsing binary of maximum brightness v 1252 mag a bestfitting solution to the binary light curve and two radial velocity curves is derived using the wils... | [['we', 'report', 'the', 'discovery', 'of', 'the', 'first', 'highamplitude', 'delta', 'scuti', 'star', 'in', 'an', 'eclipsing', 'binary', 'which', 'we', 'have', 'designated', 'unswv500', 'the', 'system', 'is', 'an', 'algoltype', 'semidetached', 'eclipsing', 'binary', 'of', 'maximum', 'brightness', 'v', '1252', 'mag', '... | [-0.1558797923633844, 0.09459290585700907, -0.12986644002566344, 0.033619731747594, -0.1360132616938524, -0.12793042483127803, 0.0969729906243266, 0.358027627241183, -0.19911716027593154, -0.30384347903134384, 0.06923245546313649, -0.28015911906616753, -0.0756831222877296, 0.2095395561514629, -0.06165657857177304, 0.02... |
707.4541 | GAW - An Imaging Atmospheric Cherenkov Telescope with Large Field of
View | GAW, acronym for Gamma Air Watch, is a Research and Development experiment in
the TeV range, whose main goal is to explore the feasibility of large field of
view Imaging Atmospheric Cherenkov Telescopes. GAW is an array of three
relatively small telescopes (2.13 m diameter) which differs from the existing
and present... | astro-ph | gaw acronym for gamma air watch is a research and development experiment in the tev range whose main goal is to explore the feasibility of large field of view imaging atmospheric cherenkov telescopes gaw is an array of three relatively small telescopes 213 m diameter which differs from the existing and presently planne... | [['gaw', 'acronym', 'for', 'gamma', 'air', 'watch', 'is', 'a', 'research', 'and', 'development', 'experiment', 'in', 'the', 'tev', 'range', 'whose', 'main', 'goal', 'is', 'to', 'explore', 'the', 'feasibility', 'of', 'large', 'field', 'of', 'view', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'gaw', 'is', 'an', ... | [-0.12468298640842626, 0.16103399093836976, -0.07973720035798812, 0.03450078293210394, -0.08383435164094785, -0.08731402266933455, -0.002978080704228067, 0.3412736638199762, -0.16196983403785795, -0.4077412226323873, 0.1177715006153369, -0.3360345730090627, -0.08334573776629127, 0.23520338064431126, -0.0837417508035267... |
707.4542 | Structural properties of proportional fairness: stability and
insensitivity | In this article we provide a novel characterization of the proportionally
fair bandwidth allocation of network capacities, in terms of the
Fenchel--Legendre transform of the network capacity region. We use this
characterization to prove stability (i.e., ergodicity) of network dynamics
under proportionally fair sharin... | math.PR | in this article we provide a novel characterization of the proportionally fair bandwidth allocation of network capacities in terms of the fenchellegendre transform of the network capacity region we use this characterization to prove stability ie ergodicity of network dynamics under proportionally fair sharing by exhibi... | [['in', 'this', 'article', 'we', 'provide', 'a', 'novel', 'characterization', 'of', 'the', 'proportionally', 'fair', 'bandwidth', 'allocation', 'of', 'network', 'capacities', 'in', 'terms', 'of', 'the', 'fenchellegendre', 'transform', 'of', 'the', 'network', 'capacity', 'region', 'we', 'use', 'this', 'characterization'... | [-0.1601773411932213, 0.04949369259711169, -0.11654783417664778, 0.07053513873446111, -0.07075176576645822, -0.18419659496950253, 0.09466933607334449, 0.38704578417708124, -0.2732973285019398, -0.24719352417603313, 0.07515457096797902, -0.21416183795303195, -0.15872627293962674, 0.15376932372843535, -0.1418025390589069... |
707.4543 | Electroweak phase transition in the MNMSSM with explicit CP violation | In explicit CP violation scenario of the minimal non-minimal supersymmetric
standard model (MNMSSM), the possibility of a strongly first-order electroweak
phase transition (EWPT) is investigated at the one-loop level, where the
radiative corrections from the loops of the top and stop quarks are taken into
account. As... | hep-ph | in explicit cp violation scenario of the minimal nonminimal supersymmetric standard model mnmssm the possibility of a strongly firstorder electroweak phase transition ewpt is investigated at the oneloop level where the radiative corrections from the loops of the top and stop quarks are taken into account assuming that ... | [['in', 'explicit', 'cp', 'violation', 'scenario', 'of', 'the', 'minimal', 'nonminimal', 'supersymmetric', 'standard', 'model', 'mnmssm', 'the', 'possibility', 'of', 'a', 'strongly', 'firstorder', 'electroweak', 'phase', 'transition', 'ewpt', 'is', 'investigated', 'at', 'the', 'oneloop', 'level', 'where', 'the', 'radia... | [-0.10026633587101993, 0.3286971347343151, -0.002021032870195958, 0.1748922087305992, -0.09126725696901582, -0.1612743690299491, 0.11243592709505638, 0.28662851083941354, -0.22029736799941885, -0.2696115224032986, 0.06151944440219323, -0.24949594688456075, -0.009455722674321966, 0.09119531126901964, 0.08345294865101677... |
707.4544 | Orbital period derivative of a binary system using an exact orbital
energy equation | It is proposed that the equations of motion in periodic relativity which
yielded major predictions of general relativity are exact in nature and can be
applied to pulsars and inspiraling compact binaries for analyzing orbital
period derivative and two polarization gravitational wave forms. Exactness of
these equation... | physics.gen-ph | it is proposed that the equations of motion in periodic relativity which yielded major predictions of general relativity are exact in nature and can be applied to pulsars and inspiraling compact binaries for analyzing orbital period derivative and two polarization gravitational wave forms exactness of these equations e... | [['it', 'is', 'proposed', 'that', 'the', 'equations', 'of', 'motion', 'in', 'periodic', 'relativity', 'which', 'yielded', 'major', 'predictions', 'of', 'general', 'relativity', 'are', 'exact', 'in', 'nature', 'and', 'can', 'be', 'applied', 'to', 'pulsars', 'and', 'inspiraling', 'compact', 'binaries', 'for', 'analyzing'... | [-0.18529272068638442, 0.12943597451978645, -0.08899122381415002, 0.12476170644824675, -0.14883060807492152, -0.07564231217297357, -0.03216298633569115, 0.2894557029940188, -0.21889160091577228, -0.32047585434778486, 0.06585816161566262, -0.25477935525393763, -0.08986771718847977, 0.21016376686477384, -0.02114387921908... |
707.4545 | Constraints on New Physics from Long Baseline Neutrino Oscillation
Experiments | New physics beyond the Standard Model can lead to extra matter effects on
neutrino oscillation if the new interactions distinguish among the three
flavors of neutrino. In a previous paper, we argued that a long-baseline
neutrino oscillation experiment in which the Fermilab-NUMI beam in its
high-energy mode is aimed a... | hep-ph | new physics beyond the standard model can lead to extra matter effects on neutrino oscillation if the new interactions distinguish among the three flavors of neutrino in a previous paper we argued that a longbaseline neutrino oscillation experiment in which the fermilabnumi beam in its highenergy mode is aimed at the p... | [['new', 'physics', 'beyond', 'the', 'standard', 'model', 'can', 'lead', 'to', 'extra', 'matter', 'effects', 'on', 'neutrino', 'oscillation', 'if', 'the', 'new', 'interactions', 'distinguish', 'among', 'the', 'three', 'flavors', 'of', 'neutrino', 'in', 'a', 'previous', 'paper', 'we', 'argued', 'that', 'a', 'longbaselin... | [-0.07752427575426137, 0.23713022902449396, -0.06208156007051002, 0.16734275820310862, -0.08256627445556892, -0.1711774287507572, 0.01955643117257073, 0.29730182202493255, -0.21320560259962493, -0.3382645079251775, 0.08850826801821352, -0.302876223938817, -0.063620886414936, 0.1942066427046542, 0.016605437037217965, 0.... |
707.4546 | Good rough path sequences and applications to anticipating stochastic
calculus | We consider anticipative Stratonovich stochastic differential equations
driven by some stochastic process lifted to a rough path. Neither adaptedness
of initial point and vector fields nor commuting conditions between vector
field is assumed. Under a simple condition on the stochastic process, we show
that the unique... | math.PR | we consider anticipative stratonovich stochastic differential equations driven by some stochastic process lifted to a rough path neither adaptedness of initial point and vector fields nor commuting conditions between vector field is assumed under a simple condition on the stochastic process we show that the unique solu... | [['we', 'consider', 'anticipative', 'stratonovich', 'stochastic', 'differential', 'equations', 'driven', 'by', 'some', 'stochastic', 'process', 'lifted', 'to', 'a', 'rough', 'path', 'neither', 'adaptedness', 'of', 'initial', 'point', 'and', 'vector', 'fields', 'nor', 'commuting', 'conditions', 'between', 'vector', 'fie... | [-0.1323549933902441, 0.10746748061047508, -0.08296069949694457, 0.09756765719049919, -0.1314057669486987, -0.11745289812684742, 0.03255743425715407, 0.38025150842827943, -0.3524225819001504, -0.19640845285062122, 0.12986015459819517, -0.229834370212544, -0.2015029382934674, 0.22404276870923767, -0.16632494200960896, 0... |
707.4547 | Bichromatically driven double well: Parametric perspective of the
control landscape | We numerically construct and study the control landscape of a
$(\omega,2\omega)$ bichromatically driven double well in the presence of strong
fields. The control landscape is obtained by correlating the overlap
intensities between the floquet states and an initial phase space coherent
state with the parametric motion... | nlin.CD physics.chem-ph | we numerically construct and study the control landscape of a omega2omega bichromatically driven double well in the presence of strong fields the control landscape is obtained by correlating the overlap intensities between the floquet states and an initial phase space coherent state with the parametric motion of the qu... | [['we', 'numerically', 'construct', 'and', 'study', 'the', 'control', 'landscape', 'of', 'a', 'omega2omega', 'bichromatically', 'driven', 'double', 'well', 'in', 'the', 'presence', 'of', 'strong', 'fields', 'the', 'control', 'landscape', 'is', 'obtained', 'by', 'correlating', 'the', 'overlap', 'intensities', 'between',... | [-0.19512128257533398, 0.21991943921939974, -0.07856299204925052, 0.06068699405579714, 0.0247030648255221, -0.09687828224311333, 0.04622429936397367, 0.38129534445157864, -0.29061056734857765, -0.2795076535151499, 0.07326883854764718, -0.21852168796311428, -0.14025118934251823, 0.19693780060085217, -0.01689892346692476... |
707.4548 | Comparison of the LUNA 3He(alpha,gamma)7Be activation results with
earlier measurements and model calculations | Recently, the LUNA collaboration has carried out a high precision measurement
on the 3He(alpha,gamma)7Be reaction cross section with both activation and
on-line gamma-detection methods at unprecedented low energies. In this paper
the results obtained with the activation method are summarized. The results are
compared... | nucl-ex | recently the luna collaboration has carried out a high precision measurement on the 3healphagamma7be reaction cross section with both activation and online gammadetection methods at unprecedented low energies in this paper the results obtained with the activation method are summarized the results are compared with prev... | [['recently', 'the', 'luna', 'collaboration', 'has', 'carried', 'out', 'a', 'high', 'precision', 'measurement', 'on', 'the', '3healphagamma7be', 'reaction', 'cross', 'section', 'with', 'both', 'activation', 'and', 'online', 'gammadetection', 'methods', 'at', 'unprecedented', 'low', 'energies', 'in', 'this', 'paper', 't... | [-0.02478336919190698, 0.1223047284073517, -0.0632701088702039, 0.026031178895567286, 0.019769069521123023, -0.11585878754859089, 0.045383629070396427, 0.39018259624965856, -0.19181107267828995, -0.35967786794864254, 0.04323247527573868, -0.34506327634463546, -0.05030517487740908, 0.25111219556200637, 0.059187748774763... |
707.4549 | Central limit theorem and almost sure central limit theorem for the
product of some partial sums | In this paper, we give the central limit theorem and almost sure central
limit theorem for products of some partial sums of independent identically
distributed random variables.
| math.PR | in this paper we give the central limit theorem and almost sure central limit theorem for products of some partial sums of independent identically distributed random variables | [['in', 'this', 'paper', 'we', 'give', 'the', 'central', 'limit', 'theorem', 'and', 'almost', 'sure', 'central', 'limit', 'theorem', 'for', 'products', 'of', 'some', 'partial', 'sums', 'of', 'independent', 'identically', 'distributed', 'random', 'variables']] | [-0.19161707845826945, 0.12414528363970695, -0.10146711207926273, 0.023900326181858503, 0.053216570919310605, -0.07708444253162101, 0.15754909986302396, 0.29004238214757705, -0.28156853936336657, -0.15110004306943328, 0.19579963478759896, -0.2625504758346964, -0.06034302436401723, 0.16799650920761955, -0.16226417529914... |
707.455 | The flow rate of granular materials through an orifice | The flow rate of grains through large orifices is known to be dependent on
its diameter to a 5/2 power law. This relationship has been checked for big
outlet sizes, whereas an empirical fitting parameter is needed to reproduce the
behavior for small openings.
In this work, we provide experimental data and numerical... | cond-mat.soft cond-mat.stat-mech | the flow rate of grains through large orifices is known to be dependent on its diameter to a 52 power law this relationship has been checked for big outlet sizes whereas an empirical fitting parameter is needed to reproduce the behavior for small openings in this work we provide experimental data and numerical simulati... | [['the', 'flow', 'rate', 'of', 'grains', 'through', 'large', 'orifices', 'is', 'known', 'to', 'be', 'dependent', 'on', 'its', 'diameter', 'to', 'a', '52', 'power', 'law', 'this', 'relationship', 'has', 'been', 'checked', 'for', 'big', 'outlet', 'sizes', 'whereas', 'an', 'empirical', 'fitting', 'parameter', 'is', 'neede... | [-0.0955485816672539, 0.12605341796006542, -0.09648701363069014, 0.04457335112752711, -0.057448745165701684, -0.12113513703253574, 0.019009365886165874, 0.3622278229871053, -0.23236781532490036, -0.33495151963296943, 0.12787194881868374, -0.2611523013905295, -0.06303858615315332, 0.24099428129450576, -0.061032482922622... |
707.4551 | Preon Model and Family Replicated E_6 Unification | Previously we suggested a new preon model of composite quark-leptons and
bosons with the 'flipped' $E_6\times \widetilde{E_6}$ gauge symmetry group. We
assumed that preons are dyons having both hyper-electric $g$ and hyper-magnetic
$\tilde g$ charges, and these preons-dyons are confined by hyper-magnetic
strings whic... | hep-ph hep-th | previously we suggested a new preon model of composite quarkleptons and bosons with the flipped e_6times widetildee_6 gauge symmetry group we assumed that preons are dyons having both hyperelectric g and hypermagnetic tilde g charges and these preonsdyons are confined by hypermagnetic strings which are an bf n1 supersy... | [['previously', 'we', 'suggested', 'a', 'new', 'preon', 'model', 'of', 'composite', 'quarkleptons', 'and', 'bosons', 'with', 'the', 'flipped', 'e_6times', 'widetildee_6', 'gauge', 'symmetry', 'group', 'we', 'assumed', 'that', 'preons', 'are', 'dyons', 'having', 'both', 'hyperelectric', 'g', 'and', 'hypermagnetic', 'til... | [-0.1733324008695538, 0.2872874147291607, -0.022612004479989897, 0.07641123026667249, -0.02835236486120551, -0.14681034408254073, 0.01139095237286871, 0.345166740208572, -0.18841409543529153, -0.3465949619201079, 0.06834607160000779, -0.25625307902425914, -0.053274421732769243, 0.08388000468303468, 0.024119217313972173... |
707.4552 | Wormhole and C-field: Revisited | Recently, Rahaman et al [ Nuovo.Cim 119B, 1115(2004)] have shown that the
static spherically symmetric solutions in presence of C-field give rise to
wormhole geometry. We highlight some of the characteristics of this wormhole,
which have not been considered in the previous study.
| gr-qc | recently rahaman et al nuovocim 119b 11152004 have shown that the static spherically symmetric solutions in presence of cfield give rise to wormhole geometry we highlight some of the characteristics of this wormhole which have not been considered in the previous study | [['recently', 'rahaman', 'et', 'al', 'nuovocim', '119b', '11152004', 'have', 'shown', 'that', 'the', 'static', 'spherically', 'symmetric', 'solutions', 'in', 'presence', 'of', 'cfield', 'give', 'rise', 'to', 'wormhole', 'geometry', 'we', 'highlight', 'some', 'of', 'the', 'characteristics', 'of', 'this', 'wormhole', 'wh... | [-0.13406826402597988, -0.013176523889295565, -0.10932688292068167, 0.0073812645830166265, -0.09513462939036962, -0.12573880917177752, -0.08357091816381002, 0.3496672080304378, -0.11256878109027942, -0.3269713271695834, 0.06564781801082575, -0.23103245003865316, -0.21046078137050456, 0.12902694988327149, -0.11296068437... |
707.4553 | Stationary distributions of a model of sympatric speciation | This paper deals with a model of sympatric speciation, that is, speciation in
the absence of geographical separation, originally proposed by U. Dieckmann and
M. Doebeli in 1999. We modify their original model to obtain a Fleming--Viot
type model and study its stationary distribution. We show that speciation may
occur... | math.PR | this paper deals with a model of sympatric speciation that is speciation in the absence of geographical separation originally proposed by u dieckmann and m doebeli in 1999 we modify their original model to obtain a flemingviot type model and study its stationary distribution we show that speciation may occur that is th... | [['this', 'paper', 'deals', 'with', 'a', 'model', 'of', 'sympatric', 'speciation', 'that', 'is', 'speciation', 'in', 'the', 'absence', 'of', 'geographical', 'separation', 'originally', 'proposed', 'by', 'u', 'dieckmann', 'and', 'm', 'doebeli', 'in', '1999', 'we', 'modify', 'their', 'original', 'model', 'to', 'obtain', ... | [-0.1155853361217645, 0.1658062058344592, -0.08336551606410393, 0.08735571098326957, -0.0714487911059256, -0.15376362901684032, 0.10637283224330359, 0.37119907522778006, -0.24128055629442807, -0.24551227308782567, 0.07710353622763642, -0.26869098928478297, -0.163671072631952, 0.1229338062056986, -0.08930590829003031, -... |
707.4554 | Exact Solutions and the Attractor Mechanism in Non-BPS Black Holes | The attractor mechanism for the four-dimensional ${\cal N}=2$ supergravity
black hole solution is analyzed in the case of the D0-D4 system. Our analyses
are based on newly derived exact solutions, which exhibit explicitly the
attractor mechanism for extremal non-BPS black holes. Our solutions account for
the moduli a... | hep-th | the attractor mechanism for the fourdimensional cal n2 supergravity black hole solution is analyzed in the case of the d0d4 system our analyses are based on newly derived exact solutions which exhibit explicitly the attractor mechanism for extremal nonbps black holes our solutions account for the moduli as general comp... | [['the', 'attractor', 'mechanism', 'for', 'the', 'fourdimensional', 'cal', 'n2', 'supergravity', 'black', 'hole', 'solution', 'is', 'analyzed', 'in', 'the', 'case', 'of', 'the', 'd0d4', 'system', 'our', 'analyses', 'are', 'based', 'on', 'newly', 'derived', 'exact', 'solutions', 'which', 'exhibit', 'explicitly', 'the', ... | [-0.1531801738604469, 0.08837267961502822, -0.0677324978688967, 0.1260956469459857, -0.061359308406855294, -0.14642307085428133, 0.007806883754154432, 0.2719248710064561, -0.1806690272088479, -0.21758014052310615, 0.15025340839858772, -0.3180729757307224, -0.1718773254310911, 0.2009030382818027, -0.03332029620312082, 0... |
707.4555 | Mechanical properties of Pt monatomic chains | The mechanical properties of platinum monatomic chains were investigated by
simultaneous measurement of an effective stiffness and the conductance using
our newly developed mechanically controllable break junction (MCBJ) technique
with a tuning fork as a force sensor. When stretching a monatomic contact
(two-atom cha... | cond-mat.mes-hall | the mechanical properties of platinum monatomic chains were investigated by simultaneous measurement of an effective stiffness and the conductance using our newly developed mechanically controllable break junction mcbj technique with a tuning fork as a force sensor when stretching a monatomic contact twoatom chain the ... | [['the', 'mechanical', 'properties', 'of', 'platinum', 'monatomic', 'chains', 'were', 'investigated', 'by', 'simultaneous', 'measurement', 'of', 'an', 'effective', 'stiffness', 'and', 'the', 'conductance', 'using', 'our', 'newly', 'developed', 'mechanically', 'controllable', 'break', 'junction', 'mcbj', 'technique', 'w... | [-0.1607949547469616, 0.20590854098226108, -0.07755201332451354, -0.01472851520464305, 0.005737501490981348, -0.1703853829403318, 0.06118402709553559, 0.3977952470221827, -0.2956795200375059, -0.27591380219185546, 0.07978807231110911, -0.28754730649562854, -0.08050390295684337, 0.139632884977806, 0.05390906260018387, 0... |
707.4556 | Photometric monitoring of the blazar 3C 345 for the period 1996 - 2006 | We present the results of the blazar 3C 345 monitoring in Johnson-Cousins
BVRI bands for the period 1996 - 2006. We have collected 29 V and 43 R data
points for this period; the BI light curves contain a few measurements only.
The accuracy of our photometry is not better than 0.03 mag in the VR bands. The
total ampli... | astro-ph | we present the results of the blazar 3c 345 monitoring in johnsoncousins bvri bands for the period 1996 2006 we have collected 29 v and 43 r data points for this period the bi light curves contain a few measurements only the accuracy of our photometry is not better than 003 mag in the vr bands the total amplitude of th... | [['we', 'present', 'the', 'results', 'of', 'the', 'blazar', '3c', '345', 'monitoring', 'in', 'johnsoncousins', 'bvri', 'bands', 'for', 'the', 'period', '1996', '2006', 'we', 'have', 'collected', '29', 'v', 'and', '43', 'r', 'data', 'points', 'for', 'this', 'period', 'the', 'bi', 'light', 'curves', 'contain', 'a', 'few'... | [-0.09435344269881264, 0.10516609419973041, -0.07817817386239767, 0.0513336005477378, -0.0536775292446598, -0.1132050056488086, 0.10149288304532185, 0.4909464062501987, -0.1280057284819822, -0.4041095877448336, 0.10597895946867095, -0.31798962328227787, -0.045736834176260836, 0.2200922553988699, -0.13786938950801508, -... |
707.4557 | Majorana neutrino. Is double neutrinoless beta decay possible in the
framework of the weak interactions? How to prove that neutrino is Majorana
particle | Usually it is supposed that Majorana neutrino produced in the superposition
state $\chi_L = \nu_L + (\nu_L)^c$ and then follows the neutrinoless double
beta decay. But since weak interactions are chiral invariant then the neutrino
at production has definite helicity (i.e., $\nu_L$ and $(\nu_L)^c$ neutrinos
are separa... | hep-ph | usually it is supposed that majorana neutrino produced in the superposition state chi_l nu_l nu_lc and then follows the neutrinoless double beta decay but since weak interactions are chiral invariant then the neutrino at production has definite helicity ie nu_l and nu_lc neutrinos are separately produced and then neutr... | [['usually', 'it', 'is', 'supposed', 'that', 'majorana', 'neutrino', 'produced', 'in', 'the', 'superposition', 'state', 'chi_l', 'nu_l', 'nu_lc', 'and', 'then', 'follows', 'the', 'neutrinoless', 'double', 'beta', 'decay', 'but', 'since', 'weak', 'interactions', 'are', 'chiral', 'invariant', 'then', 'the', 'neutrino', '... | [-0.08909541029259091, 0.43667982607089645, -0.009997317040651517, 0.20593895351210656, -0.08756664104736116, -0.21740701336036378, 0.057306440382064144, 0.32130210302605094, -0.21437267904004814, -0.23003699964714014, -0.0056030507887642874, -0.31494235107675195, -0.030271339743056253, 0.1549572653882795, 0.0859374603... |
707.4558 | Open Problems in Algebraic Statistics | Algebraic statistics is concerned with the study of probabilistic models and
techniques for statistical inference using methods from algebra and geometry.
This article presents a list of open mathematical problems in this emerging
field, with main emphasis on graphical models with hidden variables, maximum
likelihood... | math.ST math.AG stat.CO stat.TH | algebraic statistics is concerned with the study of probabilistic models and techniques for statistical inference using methods from algebra and geometry this article presents a list of open mathematical problems in this emerging field with main emphasis on graphical models with hidden variables maximum likelihood esti... | [['algebraic', 'statistics', 'is', 'concerned', 'with', 'the', 'study', 'of', 'probabilistic', 'models', 'and', 'techniques', 'for', 'statistical', 'inference', 'using', 'methods', 'from', 'algebra', 'and', 'geometry', 'this', 'article', 'presents', 'a', 'list', 'of', 'open', 'mathematical', 'problems', 'in', 'this', '... | [-0.06357143118899937, -0.00705374314242767, -0.12594208894814882, 0.08186835939543219, -0.0991730085030819, -0.14290052213861296, 0.03146628964330173, 0.32729436391188454, -0.26214977336995715, -0.32402749959793353, 0.18838210777418377, -0.2334301568658298, -0.17783739228939843, 0.21581106517826104, -0.145075273447825... |
707.4559 | Information-Disturbance theorem and Uncertainty Relation | It has been shown that Information-Disturbance theorem can play an important
role in security proof of quantum cryptography. The theorem is by itself
interesting since it can be regarded as an information theoretic version of
uncertainty principle. It, however, has been able to treat restricted
situations. In this pa... | quant-ph | it has been shown that informationdisturbance theorem can play an important role in security proof of quantum cryptography the theorem is by itself interesting since it can be regarded as an information theoretic version of uncertainty principle it however has been able to treat restricted situations in this paper the ... | [['it', 'has', 'been', 'shown', 'that', 'informationdisturbance', 'theorem', 'can', 'play', 'an', 'important', 'role', 'in', 'security', 'proof', 'of', 'quantum', 'cryptography', 'the', 'theorem', 'is', 'by', 'itself', 'interesting', 'since', 'it', 'can', 'be', 'regarded', 'as', 'an', 'information', 'theoretic', 'versi... | [-0.07676329349322865, 0.04927523880304458, -0.21157652484873932, 0.13753474803330998, -0.08127266389628252, -0.22557887764647602, 0.020693313589630027, 0.3061803893496593, -0.2856321434925, -0.3041122414916754, 0.14277151545354475, -0.22650654102365175, -0.17357205828030906, 0.24285362541675568, -0.21411077183981736, ... |
707.456 | Masses and semileptonic decays of doubly heavy baryons in a
nonrelativistic quark model | We evaluate masses and semileptonic decay widths for the ground state of
doubly heavy $\Xi$ and $\Omega$ baryons in the framework of a nonrelativistic
quark model. We solve the three-body problem by means of a variational ansatz
made possible by heavy-quark spin symmetry constraints. Our masses are
comparable to the ... | nucl-th | we evaluate masses and semileptonic decay widths for the ground state of doubly heavy xi and omega baryons in the framework of a nonrelativistic quark model we solve the threebody problem by means of a variational ansatz made possible by heavyquark spin symmetry constraints our masses are comparable to the ones obtaine... | [['we', 'evaluate', 'masses', 'and', 'semileptonic', 'decay', 'widths', 'for', 'the', 'ground', 'state', 'of', 'doubly', 'heavy', 'xi', 'and', 'omega', 'baryons', 'in', 'the', 'framework', 'of', 'a', 'nonrelativistic', 'quark', 'model', 'we', 'solve', 'the', 'threebody', 'problem', 'by', 'means', 'of', 'a', 'variationa... | [-0.07657488162799235, 0.1903770421368761, -0.06546969846221468, 0.16669033905735328, -0.04542895473329531, -0.11702099813884424, 0.07570527419316463, 0.36442565689644507, -0.1746047259188227, -0.24335337934204407, -0.022791988150622215, -0.342876895360889, 0.017614705458043084, 0.12835786756758968, 0.1077673253133863,... |
707.4561 | Observation of B-meson decays to b_1 pi and b_1 K | We present the results of searches for decays of B mesons to final states
with a b_1 meson and a charged pion or kaon. The data, collected with the BaBar
detector at the Stanford Linear Accelerator Center, represent 382 million
B-Bbar pairs produced in e+e- annihilation. The results for the branching
fractions are, i... | hep-ex | we present the results of searches for decays of b mesons to final states with a b_1 meson and a charged pion or kaon the data collected with the babar detector at the stanford linear accelerator center represent 382 million bbbar pairs produced in ee annihilation the results for the branching fractions are in units of... | [['we', 'present', 'the', 'results', 'of', 'searches', 'for', 'decays', 'of', 'b', 'mesons', 'to', 'final', 'states', 'with', 'a', 'b_1', 'meson', 'and', 'a', 'charged', 'pion', 'or', 'kaon', 'the', 'data', 'collected', 'with', 'the', 'babar', 'detector', 'at', 'the', 'stanford', 'linear', 'accelerator', 'center', 'rep... | [-0.11983132950565475, 0.23901923535567068, 0.004669752044530658, 0.06162137224175665, 0.03533965393949252, -0.12821519435398498, 0.19745908045835867, 0.2720974398801079, -0.14818643514284646, -0.3432778144472992, -0.0210153458779073, -0.4763245755661424, 0.13004819365889558, 0.11149761794881846, 0.04149646978211505, 0... |
707.4562 | Warped Kaluza-Klein Towers Revisited | Inspired by the warped Randall Sundrum scenario proposed to solve the mass
scale hierarchy problem with a compactified fifth extra dimension, a similar
model with no metric singularities has been elaborated. In this framework, the
Kaluza-Klein reduction equations for a real massless scalar field propagating
in the bu... | hep-th | inspired by the warped randall sundrum scenario proposed to solve the mass scale hierarchy problem with a compactified fifth extra dimension a similar model with no metric singularities has been elaborated in this framework the kaluzaklein reduction equations for a real massless scalar field propagating in the bulk hav... | [['inspired', 'by', 'the', 'warped', 'randall', 'sundrum', 'scenario', 'proposed', 'to', 'solve', 'the', 'mass', 'scale', 'hierarchy', 'problem', 'with', 'a', 'compactified', 'fifth', 'extra', 'dimension', 'a', 'similar', 'model', 'with', 'no', 'metric', 'singularities', 'has', 'been', 'elaborated', 'in', 'this', 'fram... | [-0.12283243841871068, 0.13487432839573119, -0.06231363670969451, 0.11493549139532089, -0.08658793080011727, -0.15504355168797904, -0.0064640713131262195, 0.2955070674126209, -0.1672221766853774, -0.3234073471415926, 0.1087370048397807, -0.2370015950942481, -0.12408412642501018, 0.1477421824199458, -0.03738999300532870... |
707.4563 | Origin of lower velocity dispersions of ultra-compact dwarf galaxy
populations in clusters of galaxies | Recent observations have revealed that velocity dispersions of
``ultra-compact dwarf'' (UCD) galaxies are significantly smaller than those of
other galaxy populations in the Fornax and the Virgo clusters of galaxies. In
order to understand the origin of the observed lower velocity dispersions of
UCDs, we numerically ... | astro-ph | recent observations have revealed that velocity dispersions of ultracompact dwarf ucd galaxies are significantly smaller than those of other galaxy populations in the fornax and the virgo clusters of galaxies in order to understand the origin of the observed lower velocity dispersions of ucds we numerically investigate... | [['recent', 'observations', 'have', 'revealed', 'that', 'velocity', 'dispersions', 'of', 'ultracompact', 'dwarf', 'ucd', 'galaxies', 'are', 'significantly', 'smaller', 'than', 'those', 'of', 'other', 'galaxy', 'populations', 'in', 'the', 'fornax', 'and', 'the', 'virgo', 'clusters', 'of', 'galaxies', 'in', 'order', 'to'... | [-0.0934456614943096, 0.12755548735351666, -0.10560126468288922, 0.11290613873751297, -0.06729291490529454, -0.021580444866047783, 0.010265110406367543, 0.44898669570389943, -0.08914356405033248, -0.37707889959098323, -0.053154964256744555, -0.29747219278252585, -0.006617323837791507, 0.22324849857204215, -0.0160644450... |
707.4564 | Characterisation of pulsed Carbon fiber illuminators for FIR instrument
calibration | We manufactured pulsed illuminators emitting in the far infrared for the
Planck-HFI bolometric instrument ground calibrations. Specific measurements
have been conducted on these light sources, based on Carbon fibers, to
understand and predict their properties. We present a modelisation of the
temperature dependence o... | astro-ph | we manufactured pulsed illuminators emitting in the far infrared for the planckhfi bolometric instrument ground calibrations specific measurements have been conducted on these light sources based on carbon fibers to understand and predict their properties we present a modelisation of the temperature dependence of the t... | [['we', 'manufactured', 'pulsed', 'illuminators', 'emitting', 'in', 'the', 'far', 'infrared', 'for', 'the', 'planckhfi', 'bolometric', 'instrument', 'ground', 'calibrations', 'specific', 'measurements', 'have', 'been', 'conducted', 'on', 'these', 'light', 'sources', 'based', 'on', 'carbon', 'fibers', 'to', 'understand'... | [-0.0730061371747676, 0.08617603014378498, -0.10981859561191716, 0.04013423839084377, -0.048256224050419405, -0.10283445037081644, 0.05768758118938422, 0.48801500885747373, -0.17643763349042274, -0.3185788821380508, 0.12052678731803705, -0.31754661806917284, -0.04624210186496688, 0.26248878896876704, -0.013667309273538... |
707.4565 | On the Complexity of the Interlace Polynomial | We consider the two-variable interlace polynomial introduced by Arratia,
Bollobas and Sorkin (2004). We develop graph transformations which allow us to
derive point-to-point reductions for the interlace polynomial. Exploiting these
reductions we obtain new results concerning the computational complexity of
evaluating... | cs.CC math.CO | we consider the twovariable interlace polynomial introduced by arratia bollobas and sorkin 2004 we develop graph transformations which allow us to derive pointtopoint reductions for the interlace polynomial exploiting these reductions we obtain new results concerning the computational complexity of evaluating the inter... | [['we', 'consider', 'the', 'twovariable', 'interlace', 'polynomial', 'introduced', 'by', 'arratia', 'bollobas', 'and', 'sorkin', '2004', 'we', 'develop', 'graph', 'transformations', 'which', 'allow', 'us', 'to', 'derive', 'pointtopoint', 'reductions', 'for', 'the', 'interlace', 'polynomial', 'exploiting', 'these', 'red... | [-0.14399161539350946, 0.013901546774432063, -0.06839255856970947, 0.08215878588069851, -0.09532799259293824, -0.17688886598994336, 0.06294572648281853, 0.3181582723309596, -0.34248705514861894, -0.2781335458283623, 0.11154435676444943, -0.24670630109806854, -0.15696146519854665, 0.19696368379052728, -0.068301056629667... |
707.4566 | Evolution of the Small Magellanic Cloud | Based on the results of N-body simulations on the last 2.5 Gyr evolution of
the Large and Small Magellanic Clouds (LMC and SMC, respectively) interacting
with the Galaxy, we firstly show when and where the leading arms (LAs) of the
Magellanic stream (MS) can pass through the Galactic plane after the MS
formation. We ... | astro-ph | based on the results of nbody simulations on the last 25 gyr evolution of the large and small magellanic clouds lmc and smc respectively interacting with the galaxy we firstly show when and where the leading arms las of the magellanic stream ms can pass through the galactic plane after the ms formation we secondly show... | [['based', 'on', 'the', 'results', 'of', 'nbody', 'simulations', 'on', 'the', 'last', '25', 'gyr', 'evolution', 'of', 'the', 'large', 'and', 'small', 'magellanic', 'clouds', 'lmc', 'and', 'smc', 'respectively', 'interacting', 'with', 'the', 'galaxy', 'we', 'firstly', 'show', 'when', 'and', 'where', 'the', 'leading', 'a... | [-0.061821241021600096, 0.11743505323780763, -0.08858628662984003, 0.08413660547839816, -0.061507152441901546, 0.025405763276546395, 0.07300034957006574, 0.4093915499471778, -0.2204121401746001, -0.3832073863595724, 0.0009064305731526657, -0.2800613100321701, -0.045685452305955575, 0.16980891774764797, -0.0386555851530... |
707.4567 | A boundedness result for toric log Del Pezzo surfaces | In this paper we give an upper bound for the Picard number of the rational
surfaces which resolve minimally the singularities of toric log Del Pezzo
surfaces of given index $\ell$. This upper bound turns out to be a quadratic
polynomial in the variable $\ell$.
| math.AG math.CO | in this paper we give an upper bound for the picard number of the rational surfaces which resolve minimally the singularities of toric log del pezzo surfaces of given index ell this upper bound turns out to be a quadratic polynomial in the variable ell | [['in', 'this', 'paper', 'we', 'give', 'an', 'upper', 'bound', 'for', 'the', 'picard', 'number', 'of', 'the', 'rational', 'surfaces', 'which', 'resolve', 'minimally', 'the', 'singularities', 'of', 'toric', 'log', 'del', 'pezzo', 'surfaces', 'of', 'given', 'index', 'ell', 'this', 'upper', 'bound', 'turns', 'out', 'to', ... | [-0.23338679602990547, 0.05950723871258864, -0.13245322135173612, 0.09978183910975026, -0.06429898080726465, -0.24181874985289242, 0.0698142002776472, 0.18971635355717606, -0.27426431230786774, -0.33980934747184316, 0.03946632072846923, -0.2630737160642942, -0.13110238718282846, 0.20358371064066888, -0.1484086512898405... |
707.4568 | Emergent Quantum Mechanics and Emergent Symmetries | Quantum mechanics is 'emergent' if a statistical treatment of large scale
phenomena in a locally deterministic theory requires the use of quantum
operators. These quantum operators may allow for symmetry transformations that
are not present in the underlying deterministic system. Such theories allow for
a natural exp... | hep-th | quantum mechanics is emergent if a statistical treatment of large scale phenomena in a locally deterministic theory requires the use of quantum operators these quantum operators may allow for symmetry transformations that are not present in the underlying deterministic system such theories allow for a natural explanati... | [['quantum', 'mechanics', 'is', 'emergent', 'if', 'a', 'statistical', 'treatment', 'of', 'large', 'scale', 'phenomena', 'in', 'a', 'locally', 'deterministic', 'theory', 'requires', 'the', 'use', 'of', 'quantum', 'operators', 'these', 'quantum', 'operators', 'may', 'allow', 'for', 'symmetry', 'transformations', 'that', ... | [-0.15182969586053136, 0.20700471418525052, -0.11994108108236738, 0.11469569480370569, -0.11886200888345586, -0.16433780520658373, -0.011318034109021739, 0.31290779619113257, -0.28709281897982175, -0.2829960584640503, 0.07233911718788516, -0.19228549442841145, -0.16118684181255166, 0.14023621730587404, -0.0666743833514... |
707.4569 | Selective amplification of scars in a chaotic optical fiber | In this letter we propose an original mechanism to select scar modes through
coherent gain amplification in a multimode D-shaped fiber. More precisely, we
numerically demonstrate how scar modes can be amplified by positioning a gain
region in the vicinity of specific points of a short periodic orbit known to
give ris... | nlin.CD nlin.PS physics.optics | in this letter we propose an original mechanism to select scar modes through coherent gain amplification in a multimode dshaped fiber more precisely we numerically demonstrate how scar modes can be amplified by positioning a gain region in the vicinity of specific points of a short periodic orbit known to give rise to ... | [['in', 'this', 'letter', 'we', 'propose', 'an', 'original', 'mechanism', 'to', 'select', 'scar', 'modes', 'through', 'coherent', 'gain', 'amplification', 'in', 'a', 'multimode', 'dshaped', 'fiber', 'more', 'precisely', 'we', 'numerically', 'demonstrate', 'how', 'scar', 'modes', 'can', 'be', 'amplified', 'by', 'positio... | [-0.18554159378082577, 0.15132973576202693, -0.10064377398653464, 0.03952561598906124, -0.07030578956685284, -0.13588820908387952, 0.08044637885706668, 0.41337829327041453, -0.27353152002800596, -0.21472511416809126, 0.05236904079687189, -0.19526436887681484, -0.21431513388895176, 0.21742937019602818, -0.12660347837584... |
707.457 | A necessary condition for existence of S-matrix outside perturbation
theory | Using the Maslov--Shvedov method of complex germ, we show that quantum field
theory S-matrix can exist outside perturbation theory in the principal order of
quasiclassical approximation only under the condition that the tangent
symplectic transformation to the evolution operator of non-linear classical
field equation... | hep-th math-ph math.MP | using the maslovshvedov method of complex germ we show that quantum field theory smatrix can exist outside perturbation theory in the principal order of quasiclassical approximation only under the condition that the tangent symplectic transformation to the evolution operator of nonlinear classical field equation is uni... | [['using', 'the', 'maslovshvedov', 'method', 'of', 'complex', 'germ', 'we', 'show', 'that', 'quantum', 'field', 'theory', 'smatrix', 'can', 'exist', 'outside', 'perturbation', 'theory', 'in', 'the', 'principal', 'order', 'of', 'quasiclassical', 'approximation', 'only', 'under', 'the', 'condition', 'that', 'the', 'tange... | [-0.17302045752368275, 0.12231707462804421, -0.16326047009271052, 0.06623799616049621, -0.07581535605565896, -0.1197213978166618, -0.04580523908167841, 0.3321405234377062, -0.2868607852253176, -0.1836030576969423, 0.0645149191157774, -0.20760219681653239, -0.22688653745821544, 0.1726480925137857, -0.07666472321937955, ... |
707.4571 | Photon-assisted spin transport in a two-dimensional electron gas | We study spin-dependent transport in a two-dimensional electron gas subject
to an external step-like potential $V(x)$ and irradiated by an electromagnetic
field (EF). In the absence of EF the electronic spectrum splits into spin
sub-bands originating from the "Rashba" spin-orbit coupling. We show that the
resonant in... | cond-mat.mes-hall | we study spindependent transport in a twodimensional electron gas subject to an external steplike potential vx and irradiated by an electromagnetic field ef in the absence of ef the electronic spectrum splits into spin subbands originating from the rashba spinorbit coupling we show that the resonant interaction of prop... | [['we', 'study', 'spindependent', 'transport', 'in', 'a', 'twodimensional', 'electron', 'gas', 'subject', 'to', 'an', 'external', 'steplike', 'potential', 'vx', 'and', 'irradiated', 'by', 'an', 'electromagnetic', 'field', 'ef', 'in', 'the', 'absence', 'of', 'ef', 'the', 'electronic', 'spectrum', 'splits', 'into', 'spin... | [-0.24759800226013062, 0.2088806996733893, -0.020094921009811927, 0.022114001179484997, -0.0377036379877387, -0.14409896283887508, 0.05153219282203089, 0.39924067260349183, -0.31140534305657314, -0.284401992547924, -0.06761658989362479, -0.29833991462137643, -0.10159087222357227, 0.20357091012278314, 0.0623849240080567... |
707.4572 | The Grand View of Physics | Abdus Salam was known for his `grand views', grand views of science as well
as grand views of society. In this talk the grand view of theoretical physics
is put in perspective.
| hep-th | abdus salam was known for his grand views grand views of science as well as grand views of society in this talk the grand view of theoretical physics is put in perspective | [['abdus', 'salam', 'was', 'known', 'for', 'his', 'grand', 'views', 'grand', 'views', 'of', 'science', 'as', 'well', 'as', 'grand', 'views', 'of', 'society', 'in', 'this', 'talk', 'the', 'grand', 'view', 'of', 'theoretical', 'physics', 'is', 'put', 'in', 'perspective']] | [-0.02571653236373095, 0.09147536364616826, -0.13884035765659064, 0.1821174322431034, -0.03080522862728685, -0.11181434101308696, 0.03489791648462415, 0.2673086766153574, -0.19300137436948717, -0.4114744523540139, 0.0605910130252596, -0.20321792899630964, -0.1994484272727277, 0.0780221666500438, -0.21001847024308518, -... |
707.4573 | Fronts Propagation at the Onset of Plastic Yielding | The existence of a finite threshold, the yield stress, for the onset of
plastic yielding is a universal feature of plasticity. This jamming-unjamming
transition is naturally accounted for by the dynamics of a bistable internal
state field. We show, within the athermal Shear Transformation Zones (STZ)
theory of amorph... | cond-mat.mtrl-sci cond-mat.stat-mech | the existence of a finite threshold the yield stress for the onset of plastic yielding is a universal feature of plasticity this jammingunjamming transition is naturally accounted for by the dynamics of a bistable internal state field we show within the athermal shear transformation zones stz theory of amorphous plasti... | [['the', 'existence', 'of', 'a', 'finite', 'threshold', 'the', 'yield', 'stress', 'for', 'the', 'onset', 'of', 'plastic', 'yielding', 'is', 'a', 'universal', 'feature', 'of', 'plasticity', 'this', 'jammingunjamming', 'transition', 'is', 'naturally', 'accounted', 'for', 'by', 'the', 'dynamics', 'of', 'a', 'bistable', 'i... | [-0.12711520530442652, 0.20390170839782823, -0.12497921238661322, 0.03423192896721009, -0.03074140840361261, -0.06038001218699237, 0.029498162924144894, 0.3275147505267722, -0.311549703984593, -0.21749709576814094, 0.04663944245379768, -0.2306303543985909, -0.21517210499120829, 0.13256146178509182, 0.004496175887333786... |
707.4574 | Ground-state fidelity in one-dimensional gapless model | A general relation between quantum phase transitions and the second
derivative of the fidelity (or the "fidelity susceptibility") is proposed. The
validity and the limitation of the fidelity susceptibility in characterizing
quantum phase transitions is thus established. Moreover, based on the
bosonization method, gen... | quant-ph cond-mat.stat-mech | a general relation between quantum phase transitions and the second derivative of the fidelity or the fidelity susceptibility is proposed the validity and the limitation of the fidelity susceptibility in characterizing quantum phase transitions is thus established moreover based on the bosonization method general formu... | [['a', 'general', 'relation', 'between', 'quantum', 'phase', 'transitions', 'and', 'the', 'second', 'derivative', 'of', 'the', 'fidelity', 'or', 'the', 'fidelity', 'susceptibility', 'is', 'proposed', 'the', 'validity', 'and', 'the', 'limitation', 'of', 'the', 'fidelity', 'susceptibility', 'in', 'characterizing', 'quant... | [-0.1672693260166774, 0.19096783823483893, -0.025760096912172133, 0.0486957535963826, -0.006480560407683414, -0.18511039445236807, 0.10536419779753252, 0.3204939234200665, -0.21422313016548913, -0.24277826639703445, 0.11149553328336928, -0.2872081595442949, -0.15992210826696326, 0.21221127264421955, 0.02963722264049925... |
707.4575 | Strong covalent bonding between two graphene layers | We show that two graphene layers stacked directly on top of each other (AA
stacking) form strong chemical bonds when the distance between planes is 0.156
nm. Simultaneously, C-C in-plane bonds are considerably weakened from partial
double-bond (0.141 nm) to single bond (0.154 nm). This polymorphic form of
graphene bi... | cond-mat.mtrl-sci | we show that two graphene layers stacked directly on top of each other aa stacking form strong chemical bonds when the distance between planes is 0156 nm simultaneously cc inplane bonds are considerably weakened from partial doublebond 0141 nm to single bond 0154 nm this polymorphic form of graphene bilayer is metastab... | [['we', 'show', 'that', 'two', 'graphene', 'layers', 'stacked', 'directly', 'on', 'top', 'of', 'each', 'other', 'aa', 'stacking', 'form', 'strong', 'chemical', 'bonds', 'when', 'the', 'distance', 'between', 'planes', 'is', '0156', 'nm', 'simultaneously', 'cc', 'inplane', 'bonds', 'are', 'considerably', 'weakened', 'fro... | [-0.15227885662898188, 0.20371560363685148, -0.00888113992914441, -0.0062823123544148984, 0.010145485437533353, -0.22954317050243844, 0.08920547954403446, 0.41680948545945284, -0.34814083050878253, -0.3110877401759353, -0.08660846344901074, -0.3394713072266313, -0.07600294640269567, 0.1290966264105009, 0.08005303253503... |
707.4576 | Heat kernel estimates for the Grusin operator | We study the geometry associated to the Grusin operator
G=\Delta_{x}+|x|^{2}\partial_{u}^{2} on \mathbb{R}_{x}^{n}\times\mathbb{R}_{u},
to obtain heat kernel estimates for this operator. The main work is to find the
shortest geodesics connecting two given points in $\mathbb{R}^{n+1}$. This
gives the Carnot-Caratheodo... | math.AP math.DG | we study the geometry associated to the grusin operator gdelta_xx2partial_u2 on mathbbr_xntimesmathbbr_u to obtain heat kernel estimates for this operator the main work is to find the shortest geodesics connecting two given points in mathbbrn1 this gives the carnotcaratheodory distance d_cc associated to this operator ... | [['we', 'study', 'the', 'geometry', 'associated', 'to', 'the', 'grusin', 'operator', 'gdelta_xx2partial_u2', 'on', 'mathbbr_xntimesmathbbr_u', 'to', 'obtain', 'heat', 'kernel', 'estimates', 'for', 'this', 'operator', 'the', 'main', 'work', 'is', 'to', 'find', 'the', 'shortest', 'geodesics', 'connecting', 'two', 'given'... | [-0.11282555300254966, 0.06178947746161824, -0.05331586856638717, 0.05368983079940429, -0.07741693707148188, -0.07175403870816265, 0.009922875052265754, 0.3489776481569649, -0.2732028717079383, -0.21215577994551615, 0.10534563088880974, -0.3100344388806653, -0.12130946998438737, 0.21260033490867397, -0.1009198014241443... |
707.4577 | The influence of self-citation corrections on Egghe's g index | The g index was introduced by Leo Egghe as an improvement of Hirsch's index h
for measuring the overall citation record of a set of articles. It better takes
into account the highly skewed frequency distribution of citations than the h
index. I propose to sharpen this g index by excluding the self-citations. I
have w... | physics.soc-ph | the g index was introduced by leo egghe as an improvement of hirschs index h for measuring the overall citation record of a set of articles it better takes into account the highly skewed frequency distribution of citations than the h index i propose to sharpen this g index by excluding the selfcitations i have worked o... | [['the', 'g', 'index', 'was', 'introduced', 'by', 'leo', 'egghe', 'as', 'an', 'improvement', 'of', 'hirschs', 'index', 'h', 'for', 'measuring', 'the', 'overall', 'citation', 'record', 'of', 'a', 'set', 'of', 'articles', 'it', 'better', 'takes', 'into', 'account', 'the', 'highly', 'skewed', 'frequency', 'distribution', ... | [-0.06869951272185645, 0.10534910511190868, -0.07259110783947245, 0.06154106628865812, -0.08641687371188177, -0.13448146226780736, 0.0799426187284484, 0.3818622762513048, -0.17891606942855948, -0.4071972288261607, 0.03554296522853755, -0.290183095604111, -0.07738254806202538, 0.19520273224784518, -0.08916920009684169, ... |
707.4578 | Update on Counting Valence Quarks at RHIC | We update our former analysis of the Nuclear Modification Factors (NMF) for
different hadron species at RHIC and LHC. This update is motivated by the new
experimental data from STAR which presents differences with the preliminary
data used to fix some of the parameters in our model. The main change is the
use of AKK ... | hep-ph | we update our former analysis of the nuclear modification factors nmf for different hadron species at rhic and lhc this update is motivated by the new experimental data from star which presents differences with the preliminary data used to fix some of the parameters in our model the main change is the use of akk fragme... | [['we', 'update', 'our', 'former', 'analysis', 'of', 'the', 'nuclear', 'modification', 'factors', 'nmf', 'for', 'different', 'hadron', 'species', 'at', 'rhic', 'and', 'lhc', 'this', 'update', 'is', 'motivated', 'by', 'the', 'new', 'experimental', 'data', 'from', 'star', 'which', 'presents', 'differences', 'with', 'the'... | [-0.03438913380313251, 0.11676505321843757, -0.17134897196148005, 0.08193227272713557, -0.08292225447690321, -0.061339017329737545, 0.05000920355733898, 0.3594380851628052, -0.2463256818552812, -0.28197709801024756, 0.07453204117482529, -0.2836369592489468, -0.057552232220768926, 0.148263012449671, -0.00737006014419926... |
707.4579 | Magnetic Field Structures of BL Lac Objects on Decaparsec Scales | Relatively few Very Long Baseline Interferometry (VLBI) polarization
observations have been carried out at 18 cm. The importance of such
observations lies in their ability to reveal information about the jet magnetic
({\bf B}) field structure and the environment of the jet on scales intermediate
between those probed ... | astro-ph | relatively few very long baseline interferometry vlbi polarization observations have been carried out at 18 cm the importance of such observations lies in their ability to reveal information about the jet magnetic bf b field structure and the environment of the jet on scales intermediate between those probed by higherf... | [['relatively', 'few', 'very', 'long', 'baseline', 'interferometry', 'vlbi', 'polarization', 'observations', 'have', 'been', 'carried', 'out', 'at', '18', 'cm', 'the', 'importance', 'of', 'such', 'observations', 'lies', 'in', 'their', 'ability', 'to', 'reveal', 'information', 'about', 'the', 'jet', 'magnetic', 'bf', 'b... | [-0.12900437978521784, 0.1256405111423104, -0.05079151509326131, 0.07862115476096078, -0.0928080604378569, -0.09401238819130409, -0.0027510634059710474, 0.4605248833670834, -0.23224950095444805, -0.3498308740906077, 0.10439728305150334, -0.24828954821282306, -0.012748636255693164, 0.19290395898196072, 0.042612614042671... |
707.458 | Note on edge-colored graphs and digraphs without properly colored cycles | We study the following two functions: d(n,c) and $\vec{d}(n,c)$; d(n,c)
($\vec{d}(n,c)$) is the minimum number k such that every c-edge-colored
undirected (directed) graph of order n and minimum monochromatic degree
(out-degree) at least k has a properly colored cycle. Abouelaoualim et al.
(2007) stated a conjecture ... | cs.DM | we study the following two functions dnc and vecdnc dnc vecdnc is the minimum number k such that every cedgecolored undirected directed graph of order n and minimum monochromatic degree outdegree at least k has a properly colored cycle abouelaoualim et al 2007 stated a conjecture which implies that dnc1 using a recursi... | [['we', 'study', 'the', 'following', 'two', 'functions', 'dnc', 'and', 'vecdnc', 'dnc', 'vecdnc', 'is', 'the', 'minimum', 'number', 'k', 'such', 'that', 'every', 'cedgecolored', 'undirected', 'directed', 'graph', 'of', 'order', 'n', 'and', 'minimum', 'monochromatic', 'degree', 'outdegree', 'at', 'least', 'k', 'has', 'a... | [-0.169959098270904, 0.15487216690415015, -0.059618511492566716, 0.020654497753267966, -0.04489453487418672, -0.16131070400438002, 0.07008999095408507, 0.3597632685641167, -0.1935149136109538, -0.37734851117936835, 0.02844415984356836, -0.26697246130976465, -0.17594233458931807, 0.12612734404542753, -0.1152721987686730... |
707.4581 | Physical conditions in CaFe interstellar clouds | Interstellar clouds that exhibit strong Ca I and Fe I lines were called CaFe
clouds. The ionisation equilibrium equations were used to model the column
densities of Ca II, Ca I, K I, Na I, Fe I and Ti II in CaFe clouds. The
chemical composition of CaFe clouds is that of the Solar System and no
depletion of elements o... | astro-ph | interstellar clouds that exhibit strong ca i and fe i lines were called cafe clouds the ionisation equilibrium equations were used to model the column densities of ca ii ca i k i na i fe i and ti ii in cafe clouds the chemical composition of cafe clouds is that of the solar system and no depletion of elements onto dust... | [['interstellar', 'clouds', 'that', 'exhibit', 'strong', 'ca', 'i', 'and', 'fe', 'i', 'lines', 'were', 'called', 'cafe', 'clouds', 'the', 'ionisation', 'equilibrium', 'equations', 'were', 'used', 'to', 'model', 'the', 'column', 'densities', 'of', 'ca', 'ii', 'ca', 'i', 'k', 'i', 'na', 'i', 'fe', 'i', 'and', 'ti', 'ii',... | [-0.043016261519754635, 0.15862407067461926, 0.04590686263845247, 0.013718194298117476, 0.07119019581552814, -0.17019598159719915, 0.07161607156808981, 0.4849912706543418, -0.17821543557459818, -0.28164136884186197, -0.06449138090041849, -0.3249507173238432, 0.028467901072957935, 0.003718660045963, -0.02247844830922344... |
707.4582 | Hall Effect in Granular Metals: Weak Localization Corrections | We study the effects of localization on the Hall transport in a granular
system at large tunneling conductance $g_{T}\gg 1$ corresponding to the
metallic regime. We show that the first-order in 1/g_T weak localization
correction to Hall resistivity of a two- or three-dimensional granular array
vanishes identically, $... | cond-mat.mes-hall cond-mat.str-el | we study the effects of localization on the hall transport in a granular system at large tunneling conductance g_tgg 1 corresponding to the metallic regime we show that the firstorder in 1g_t weak localization correction to hall resistivity of a two or threedimensional granular array vanishes identically de rho_xywl0 t... | [['we', 'study', 'the', 'effects', 'of', 'localization', 'on', 'the', 'hall', 'transport', 'in', 'a', 'granular', 'system', 'at', 'large', 'tunneling', 'conductance', 'g_tgg', '1', 'corresponding', 'to', 'the', 'metallic', 'regime', 'we', 'show', 'that', 'the', 'firstorder', 'in', '1g_t', 'weak', 'localization', 'corre... | [-0.18188524168898473, 0.22039248562708413, -0.020645426388583937, 0.011413728545929463, 0.013002749005297446, -0.16913787851039813, 0.01674672564544346, 0.3231415512075402, -0.2544026856644536, -0.2849067241603614, 0.04246306621781463, -0.29950713817873653, -0.11318562606147509, 0.18797434815908518, 0.0120128459771567... |
707.4583 | Warping and F-term uplifting | We analyse the effective supergravity model of a warped compactification with
matter on D3 and D7-branes. We find that the main effect of the warp factor is
to modify the F-terms while leaving the D-terms invariant. Hence warped models
with moduli stabilisation and a small positive cosmological constant resulting
fro... | hep-th | we analyse the effective supergravity model of a warped compactification with matter on d3 and d7branes we find that the main effect of the warp factor is to modify the fterms while leaving the dterms invariant hence warped models with moduli stabilisation and a small positive cosmological constant resulting from a lar... | [['we', 'analyse', 'the', 'effective', 'supergravity', 'model', 'of', 'a', 'warped', 'compactification', 'with', 'matter', 'on', 'd3', 'and', 'd7branes', 'we', 'find', 'that', 'the', 'main', 'effect', 'of', 'the', 'warp', 'factor', 'is', 'to', 'modify', 'the', 'fterms', 'while', 'leaving', 'the', 'dterms', 'invariant',... | [-0.17280887141047666, 0.20864718163914706, -0.025939662508123244, 0.12678157735208515, -0.12540815459991184, -0.17769815453793852, 4.87651404303809e-05, 0.30070587920684677, -0.16790193715132773, -0.30259016242926007, 0.13898405783790319, -0.21915577265123526, -0.11680512800812722, 0.10806559469977704, -0.099602848477... |
707.4584 | Some new Strichartz estimates for the Schr\"odinger equation | We deal with fixed-time and Strichartz estimates for the Schr\"odinger
propagator as an operator on Wiener amalgam spaces. We discuss the sharpness of
the known estimates and we provide some new estimates which generalize the
classical ones. As an application, we present a result on the wellposedness of
the linear Sc... | math.AP math-ph math.MP | we deal with fixedtime and strichartz estimates for the schrodinger propagator as an operator on wiener amalgam spaces we discuss the sharpness of the known estimates and we provide some new estimates which generalize the classical ones as an application we present a result on the wellposedness of the linear schrodinge... | [['we', 'deal', 'with', 'fixedtime', 'and', 'strichartz', 'estimates', 'for', 'the', 'schrodinger', 'propagator', 'as', 'an', 'operator', 'on', 'wiener', 'amalgam', 'spaces', 'we', 'discuss', 'the', 'sharpness', 'of', 'the', 'known', 'estimates', 'and', 'we', 'provide', 'some', 'new', 'estimates', 'which', 'generalize'... | [-0.07613800568827267, 0.048018306482217984, -0.0963934620135817, 0.12236910637725017, -0.13078427576492058, -0.08708146941880214, 0.002522345788873218, 0.35170398003839215, -0.27364616722253887, -0.20439863100583697, 0.1985715146774651, -0.3060770963382875, -0.17810631384430775, 0.2432466097786252, -0.1093479119851414... |
707.4585 | Two-eigenfunction correlation in a multifractal metal and insulator | We consider the correlation of two single-particle probability densities
$|\Psi_{E}({\bf r})|^{2}$ at coinciding points ${\bf r}$ as a function of the
energy separation $\omega=|E-E'|$ for disordered tight-binding lattice models
(the Anderson models) and certain random matrix ensembles. We focus on the
models in the ... | cond-mat.mes-hall cond-mat.stat-mech | we consider the correlation of two singleparticle probability densities psi_ebf r2 at coinciding points bf r as a function of the energy separation omegaee for disordered tightbinding lattice models the anderson models and certain random matrix ensembles we focus on the models in the parameter range where they are clos... | [['we', 'consider', 'the', 'correlation', 'of', 'two', 'singleparticle', 'probability', 'densities', 'psi_ebf', 'r2', 'at', 'coinciding', 'points', 'bf', 'r', 'as', 'a', 'function', 'of', 'the', 'energy', 'separation', 'omegaee', 'for', 'disordered', 'tightbinding', 'lattice', 'models', 'the', 'anderson', 'models', 'an... | [-0.116893427791684, 0.15400963211133278, -0.05707485453390023, 0.11317580051466146, 0.03674375892362811, -0.15692391141721193, 0.04173220768598914, 0.35845692981691923, -0.2403275305044185, -0.23267582857752228, 0.059658915897642065, -0.3445519726016225, -0.1864396338276366, 0.14268777057538456, 0.04348893408080872, 0... |
707.4586 | Light Scalar Tetraquark Mesons in the QCD Sum Rule | We study the lowest-lying scalar mesons in the QCD sum rule by considering
them as tetraquark states. We find that there are five independent currents for
each state with a certain flavor structure. By forming linear combinations, we
find that some mixed currents give reliable QCD sum rules. Among various
tetraquark ... | hep-ph | we study the lowestlying scalar mesons in the qcd sum rule by considering them as tetraquark states we find that there are five independent currents for each state with a certain flavor structure by forming linear combinations we find that some mixed currents give reliable qcd sum rules among various tetraquark current... | [['we', 'study', 'the', 'lowestlying', 'scalar', 'mesons', 'in', 'the', 'qcd', 'sum', 'rule', 'by', 'considering', 'them', 'as', 'tetraquark', 'states', 'we', 'find', 'that', 'there', 'are', 'five', 'independent', 'currents', 'for', 'each', 'state', 'with', 'a', 'certain', 'flavor', 'structure', 'by', 'forming', 'linea... | [-0.15307466941410486, 0.2659509736279558, -0.03524019408552927, 0.1176131152909021, -0.05172066320190016, -0.12817894605615612, 0.08664957045254354, 0.3912638223787047, -0.1892985030058391, -0.1978524841976409, 0.03399453752517358, -0.2573662552298332, -0.09827665507565347, 0.06136389616496709, 0.12167681844867005, 0.... |
707.4587 | Observations on Gaussian bases for Schrodinger's equation | One of the few methods for generating efficient function spaces for multi-D
Schrodinger eigenproblems is given by Garashchuk and Light in J.Chem.Phys. 114
(2001) 3929. Their Gaussian basis functions are wider and sparser in high
potential regions, and narrower and denser in low ones. We suggest a
modification of thei... | physics.comp-ph physics.chem-ph | one of the few methods for generating efficient function spaces for multid schrodinger eigenproblems is given by garashchuk and light in jchemphys 114 2001 3929 their gaussian basis functions are wider and sparser in high potential regions and narrower and denser in low ones we suggest a modification of their approach ... | [['one', 'of', 'the', 'few', 'methods', 'for', 'generating', 'efficient', 'function', 'spaces', 'for', 'multid', 'schrodinger', 'eigenproblems', 'is', 'given', 'by', 'garashchuk', 'and', 'light', 'in', 'jchemphys', '114', '2001', '3929', 'their', 'gaussian', 'basis', 'functions', 'are', 'wider', 'and', 'sparser', 'in',... | [-0.051645438568308374, 0.05057115609614322, -0.11602328406073727, 0.10822590115265204, -0.05832904823160229, -0.14205573027093824, 0.061027094417323284, 0.4362083742395043, -0.21360630634455727, -0.29858606116702924, 0.10065042134195279, -0.24544249246470057, -0.13521636861483924, 0.24002069600213033, -0.0624264007505... |
707.4588 | Probabilistic validation of homology computations for nodal domains | Homology has long been accepted as an important computable tool for
quantifying complex structures. In many applications, these structures arise as
nodal domains of real-valued functions and are therefore amenable only to a
numerical study based on suitable discretizations. Such an approach immediately
raises the que... | math.PR | homology has long been accepted as an important computable tool for quantifying complex structures in many applications these structures arise as nodal domains of realvalued functions and are therefore amenable only to a numerical study based on suitable discretizations such an approach immediately raises the question ... | [['homology', 'has', 'long', 'been', 'accepted', 'as', 'an', 'important', 'computable', 'tool', 'for', 'quantifying', 'complex', 'structures', 'in', 'many', 'applications', 'these', 'structures', 'arise', 'as', 'nodal', 'domains', 'of', 'realvalued', 'functions', 'and', 'are', 'therefore', 'amenable', 'only', 'to', 'a'... | [-0.14191119610814396, 0.06688657386867153, -0.07874226931751042, 0.11807415192959377, -0.09379957438454972, -0.11427057064180304, 0.018481401519992533, 0.3759873513035845, -0.2847053837744301, -0.25142803423207355, 0.15425616885464102, -0.1949498996176329, -0.18852003512753024, 0.26913292075062656, -0.0839212417963321... |
707.4589 | Sum Rules for Total Cross-Sections of Hadron Photo-Production on
Pseudoscalar Mesons and Octet Baryons | Considering very high energy peripheral electron-hadron scattering with a
production of hadronic state X moving closely to the direction of initial
hadron the Weizs\"acker-Williams like expression, relating the difference of
q^2-dependent differential cross-sections of DIS processes to the convergent
integral over th... | hep-ph | considering very high energy peripheral electronhadron scattering with a production of hadronic state x moving closely to the direction of initial hadron the weizsackerwilliams like expression relating the difference of q2dependent differential crosssections of dis processes to the convergent integral over the differen... | [['considering', 'very', 'high', 'energy', 'peripheral', 'electronhadron', 'scattering', 'with', 'a', 'production', 'of', 'hadronic', 'state', 'x', 'moving', 'closely', 'to', 'the', 'direction', 'of', 'initial', 'hadron', 'the', 'weizsackerwilliams', 'like', 'expression', 'relating', 'the', 'difference', 'of', 'q2depen... | [-0.08033658865589541, 0.164389385578587, -0.14828311193696866, 0.1316069691565117, -0.08519204177866703, -0.0430701844819376, 0.01426415012552963, 0.3173598601496306, -0.24002951340398926, -0.18494542426281219, -0.036997572729782456, -0.3442150460205216, 0.022537224457018834, 0.18102249709224544, 0.09376967900122206, ... |
707.459 | Exciton condensate at a total filling factor of 1 in Corbino 2D electron
bilayers | Magneto-transport and drag measurements on a quasi-Corbino 2D electron
bilayer at the systems total filling factor 1 (v_tot=1) reveal a drag voltage
that is equal in magnitude to the drive voltage as soon as the two layers begin
to form the expected v_tot=1 exciton condensate. The identity of both voltages
remains pr... | cond-mat.mes-hall cond-mat.str-el | magnetotransport and drag measurements on a quasicorbino 2d electron bilayer at the systems total filling factor 1 v_tot1 reveal a drag voltage that is equal in magnitude to the drive voltage as soon as the two layers begin to form the expected v_tot1 exciton condensate the identity of both voltages remains present eve... | [['magnetotransport', 'and', 'drag', 'measurements', 'on', 'a', 'quasicorbino', '2d', 'electron', 'bilayer', 'at', 'the', 'systems', 'total', 'filling', 'factor', '1', 'v_tot1', 'reveal', 'a', 'drag', 'voltage', 'that', 'is', 'equal', 'in', 'magnitude', 'to', 'the', 'drive', 'voltage', 'as', 'soon', 'as', 'the', 'two',... | [-0.21571030411657624, 0.19459409960853175, 0.004954959578092464, -0.029413674046571196, 0.052386869824576104, -0.17075340510663492, 0.09764790899300185, 0.3438131657683037, -0.2779818387829106, -0.30911018705757504, 0.031649341162516394, -0.331208229996264, -0.06790341055867347, 0.1810882565650073, 0.0647298672225919,... |
707.4591 | Tachyon Vacuum in Cubic Superstring Field Theory | In this paper we give an exact analytic solution for tachyon condensation in
the modified (picture 0) cubic superstring field theory. We prove the absence
of cohomology and, crucially, reproduce the correct value for the D-brane
tension. The solution is surprising for two reasons: First, the existence of a
tachyon va... | hep-th | in this paper we give an exact analytic solution for tachyon condensation in the modified picture 0 cubic superstring field theory we prove the absence of cohomology and crucially reproduce the correct value for the dbrane tension the solution is surprising for two reasons first the existence of a tachyon vacuum in thi... | [['in', 'this', 'paper', 'we', 'give', 'an', 'exact', 'analytic', 'solution', 'for', 'tachyon', 'condensation', 'in', 'the', 'modified', 'picture', '0', 'cubic', 'superstring', 'field', 'theory', 'we', 'prove', 'the', 'absence', 'of', 'cohomology', 'and', 'crucially', 'reproduce', 'the', 'correct', 'value', 'for', 'the... | [-0.17232393686260497, 0.0917396172785846, -0.1275069617910222, 0.14897132373187646, -0.06822847792257865, -0.1472256169709865, 0.011741946272585275, 0.2757465655006291, -0.1937713540114817, -0.24355582405059112, 0.0944965923180072, -0.2332156789710834, -0.14637897512295153, 0.10758938013445697, -0.048028180575264354, ... |
707.4592 | One loop corrections to the mass of self-dual semi-local planar
topological solitons | A formula is derived that allows the computation of one-loop mass shifts for
self-dual semilocal topological solitons. These extended objects, which in
three spatial dimensions are called semi-local strings, arise in a generalized
Abelian Higgs model with a doublet of complex Higgs fields. Having a mixture of
global,... | hep-th | a formula is derived that allows the computation of oneloop mass shifts for selfdual semilocal topological solitons these extended objects which in three spatial dimensions are called semilocal strings arise in a generalized abelian higgs model with a doublet of complex higgs fields having a mixture of global su2 and l... | [['a', 'formula', 'is', 'derived', 'that', 'allows', 'the', 'computation', 'of', 'oneloop', 'mass', 'shifts', 'for', 'selfdual', 'semilocal', 'topological', 'solitons', 'these', 'extended', 'objects', 'which', 'in', 'three', 'spatial', 'dimensions', 'are', 'called', 'semilocal', 'strings', 'arise', 'in', 'a', 'generali... | [-0.1740122044463689, 0.21455752145677728, -0.09260315807404543, 0.16165414883289486, -0.09052453191969732, -0.18779120685513875, 0.004431244257527093, 0.33308144698314596, -0.20849426390810144, -0.25153020606611415, 0.04875729262777087, -0.22719967268619598, -0.12238087461652196, 0.10290360831740228, -0.03381932873456... |
707.4593 | nu_e Disappearance in MiniBooNE | The anomalous excess of low-energy nu_e events measured in the MiniBooNE
experiment is explained through a renormalization of the absolute neutrino flux
and a simultaneous disappearance of the nu_e's in the beam, which is compatible
with that indicated by the results of Gallium radioactive source experiments.
We pres... | hep-ph hep-ex physics.acc-ph | the anomalous excess of lowenergy nu_e events measured in the miniboone experiment is explained through a renormalization of the absolute neutrino flux and a simultaneous disappearance of the nu_es in the beam which is compatible with that indicated by the results of gallium radioactive source experiments we present th... | [['the', 'anomalous', 'excess', 'of', 'lowenergy', 'nu_e', 'events', 'measured', 'in', 'the', 'miniboone', 'experiment', 'is', 'explained', 'through', 'a', 'renormalization', 'of', 'the', 'absolute', 'neutrino', 'flux', 'and', 'a', 'simultaneous', 'disappearance', 'of', 'the', 'nu_es', 'in', 'the', 'beam', 'which', 'is... | [-0.04274787573816897, 0.16555986476060836, -0.06243936187478111, 0.08955723283511094, 0.00044195608337636757, -0.09239827720017932, 0.10987420314179436, 0.313804466997375, -0.1651630672555761, -0.3557500847803131, 0.023538574447244907, -0.4244034095215337, -0.010430046173297809, 0.22317943844099006, -0.027982667417210... |
707.4594 | Stability of steady states in kinetic Fokker-Planck equations for Bosons
and Fermions | We study a class of nonlinear kinetic Fokker-Planck type equations modeling
quantum particles which obey the Bose-Einstein and Fermi-Dirac statistics,
respectively. We establish the existence of classical solutions in the
perturbative regime and prove exponential convergence towards the equilibrium.
| math.AP math-ph math.MP | we study a class of nonlinear kinetic fokkerplanck type equations modeling quantum particles which obey the boseeinstein and fermidirac statistics respectively we establish the existence of classical solutions in the perturbative regime and prove exponential convergence towards the equilibrium | [['we', 'study', 'a', 'class', 'of', 'nonlinear', 'kinetic', 'fokkerplanck', 'type', 'equations', 'modeling', 'quantum', 'particles', 'which', 'obey', 'the', 'boseeinstein', 'and', 'fermidirac', 'statistics', 'respectively', 'we', 'establish', 'the', 'existence', 'of', 'classical', 'solutions', 'in', 'the', 'perturbati... | [-0.12234726388198443, 0.1283569740346418, -0.153741719869849, 0.12936702019009644, -0.028628367835130446, -0.15667760772152972, 0.010781635619843235, 0.2227415265276646, -0.2633842920215848, -0.20841863674995226, 0.018368481485268626, -0.28657792499050116, -0.0913526412481681, 0.1403218281503098, 0.039511050600758144,... |
707.4595 | Einstein solvmanifolds with a simple Einstein derivation | The structure of a solvable Lie groups admitting an Einstein left-invariant
metric is, in a sense, completely determined by the nilradical of its Lie
algebra. We give an easy-to-check necessary and sufficient condition for a
nilpotent algebra to be an Einstein nilradical whose Einstein derivation has
simple eigenvalu... | math.DG | the structure of a solvable lie groups admitting an einstein leftinvariant metric is in a sense completely determined by the nilradical of its lie algebra we give an easytocheck necessary and sufficient condition for a nilpotent algebra to be an einstein nilradical whose einstein derivation has simple eigenvalues as an... | [['the', 'structure', 'of', 'a', 'solvable', 'lie', 'groups', 'admitting', 'an', 'einstein', 'leftinvariant', 'metric', 'is', 'in', 'a', 'sense', 'completely', 'determined', 'by', 'the', 'nilradical', 'of', 'its', 'lie', 'algebra', 'we', 'give', 'an', 'easytocheck', 'necessary', 'and', 'sufficient', 'condition', 'for',... | [-0.2194560741289304, -0.007617680172328479, -0.042432006649099865, 0.04831527658702376, -0.2608326321467757, -0.19417500877036498, -0.1395950982454591, 0.41170003726505316, -0.292092658751286, -0.19051257483661174, 0.16923766794363754, -0.20296423630072521, -0.15374716816541667, 0.18612306272754303, -0.190847053364492... |
707.4596 | Uniform convergence of exact large deviations for renewal reward
processes | Let (X_n,Y_n) be i.i.d. random vectors. Let W(x) be the partial sum of Y_n
just before that of X_n exceeds x>0. Motivated by stochastic models for neural
activity, uniform convergence of the form $\sup_{c\in I}|a(c,x)\operatorname
{Pr}\{W(x)\gecx\}-1|=o(1)$, $x\to\infty$, is established for probabilities of
large dev... | math.PR | let x_ny_n be iid random vectors let wx be the partial sum of y_n just before that of x_n exceeds x0 motivated by stochastic models for neural activity uniform convergence of the form sup_cin iacxoperatorname prwxgecx1o1 xtoinfty is established for probabilities of large deviations with acx a deterministic function and... | [['let', 'x_ny_n', 'be', 'iid', 'random', 'vectors', 'let', 'wx', 'be', 'the', 'partial', 'sum', 'of', 'y_n', 'just', 'before', 'that', 'of', 'x_n', 'exceeds', 'x0', 'motivated', 'by', 'stochastic', 'models', 'for', 'neural', 'activity', 'uniform', 'convergence', 'of', 'the', 'form', 'sup_cin', 'iacxoperatorname', 'prw... | [-0.1265937470127153, 0.1333584577462348, -0.08840547891276825, 0.05787383872066546, -0.02951323037313027, -0.13367810915801887, 0.05597112447473057, 0.3589011617431431, -0.33487072938569745, -0.1560713531812013, 0.10728384222024838, -0.27795442753251043, -0.07703393512629399, 0.150478694150722, -0.06547423289512917, 0... |
707.4597 | Side-information Scalable Source Coding | The problem of side-information scalable (SI-scalable) source coding is
considered in this work, where the encoder constructs a progressive
description, such that the receiver with high quality side information will be
able to truncate the bitstream and reconstruct in the rate distortion sense,
while the receiver wit... | cs.IT math.IT | the problem of sideinformation scalable siscalable source coding is considered in this work where the encoder constructs a progressive description such that the receiver with high quality side information will be able to truncate the bitstream and reconstruct in the rate distortion sense while the receiver with low qua... | [['the', 'problem', 'of', 'sideinformation', 'scalable', 'siscalable', 'source', 'coding', 'is', 'considered', 'in', 'this', 'work', 'where', 'the', 'encoder', 'constructs', 'a', 'progressive', 'description', 'such', 'that', 'the', 'receiver', 'with', 'high', 'quality', 'side', 'information', 'will', 'be', 'able', 'to'... | [-0.1268496670818422, 0.061634397795680376, -0.05756608367171454, 0.06884534998157582, -0.09620591077038039, -0.23501810566837883, 0.048512591608460616, 0.38530292183602766, -0.30168462689902825, -0.25365446971816213, 0.17726444859369422, -0.24603987029966726, -0.12198560781331962, 0.17448592919982592, -0.1168351084927... |
707.4598 | On the fraction of intermediate-mass close binaries that explode as
type-Ia supernovae | Type-Ia supernovae (SNe-Ia) are thought to result from a thermonuclear
runaway in white dwarfs (WDs) that approach the Chandrasekhar limit, either
through accretion from a companion or a merger with another WD. I compile
observational estimates of the fraction eta of intermediate-mass stars that
eventually explode as... | astro-ph | typeia supernovae sneia are thought to result from a thermonuclear runaway in white dwarfs wds that approach the chandrasekhar limit either through accretion from a companion or a merger with another wd i compile observational estimates of the fraction eta of intermediatemass stars that eventually explode as sneia supp... | [['typeia', 'supernovae', 'sneia', 'are', 'thought', 'to', 'result', 'from', 'a', 'thermonuclear', 'runaway', 'in', 'white', 'dwarfs', 'wds', 'that', 'approach', 'the', 'chandrasekhar', 'limit', 'either', 'through', 'accretion', 'from', 'a', 'companion', 'or', 'a', 'merger', 'with', 'another', 'wd', 'i', 'compile', 'ob... | [-0.04977914172811684, 0.14303763039852582, -0.01709241047501564, 0.16064151689246067, -0.10447653899191418, -0.09343479480059154, 0.12921347750539952, 0.37207473935095514, -0.16365797221446518, -0.31488556690715697, 0.06060014883773508, -0.3233039363312367, 0.024532684900216272, 0.2593316925373785, -0.0414786759658970... |
707.4599 | Near-Infrared Surface Photometry of a Sample of Barred Galaxies | We have obtained deep J and Ks images of a sample of nine barred galaxies in
order to collect a reliable and homogeneous set of images to which N-body
simulations of barred galaxies will be compared. The observations were
performed using the new near-infrared camera available at the 2.1-m telescope
of the Observatori... | astro-ph | we have obtained deep j and ks images of a sample of nine barred galaxies in order to collect a reliable and homogeneous set of images to which nbody simulations of barred galaxies will be compared the observations were performed using the new nearinfrared camera available at the 21m telescope of the observatorio astro... | [['we', 'have', 'obtained', 'deep', 'j', 'and', 'ks', 'images', 'of', 'a', 'sample', 'of', 'nine', 'barred', 'galaxies', 'in', 'order', 'to', 'collect', 'a', 'reliable', 'and', 'homogeneous', 'set', 'of', 'images', 'to', 'which', 'nbody', 'simulations', 'of', 'barred', 'galaxies', 'will', 'be', 'compared', 'the', 'obse... | [-0.06516659920410049, 0.04287394191909809, -0.12603307473082237, 0.0834765673551943, -0.055834657096709234, -0.04910108278939174, -0.016210838123260223, 0.4451135986178886, -0.18598281754045712, -0.3378660640313169, 0.07826599574342143, -0.28023421546828203, -0.10622651191145707, 0.20142990808208822, -0.06206884419630... |
707.46 | Heavy traffic limit for a processor sharing queue with soft deadlines | This paper considers a GI/GI/1 processor sharing queue in which jobs have
soft deadlines. At each point in time, the collection of residual service times
and deadlines is modeled using a random counting measure on the right
half-plane. The limit of this measure valued process is obtained under
diffusion scaling and h... | math.PR | this paper considers a gigi1 processor sharing queue in which jobs have soft deadlines at each point in time the collection of residual service times and deadlines is modeled using a random counting measure on the right halfplane the limit of this measure valued process is obtained under diffusion scaling and heavy tra... | [['this', 'paper', 'considers', 'a', 'gigi1', 'processor', 'sharing', 'queue', 'in', 'which', 'jobs', 'have', 'soft', 'deadlines', 'at', 'each', 'point', 'in', 'time', 'the', 'collection', 'of', 'residual', 'service', 'times', 'and', 'deadlines', 'is', 'modeled', 'using', 'a', 'random', 'counting', 'measure', 'on', 'th... | [-0.16479352495976185, 0.09820841931198773, -0.09189117727801203, 0.04165146137410806, 0.014010048797354102, -0.1846154942520355, 0.12423526283329059, 0.3898711586076962, -0.2709408678653601, -0.23452745903479424, 0.1526173934083138, -0.28267859246238675, -0.027369548409785095, 0.16288068431282515, -0.08835536186142187... |
707.4601 | Violation of the isotropic-$\ell$ approximation in overdoped
La_{2-x}Sr_xCuO_4 | Magnetotransport measurements on the overdoped cuprate La_{1.7}Sr_{0.3}CuO_4
are fitted using the Ong construction and band parameters inferred from
angle-resolved photoemission. Within a band picture, the low temperature Hall
data can only be fitted satisfactorily by invoking strong basal-plane
anisotropy in the mea... | cond-mat.supr-con cond-mat.str-el | magnetotransport measurements on the overdoped cuprate la_17sr_03cuo_4 are fitted using the ong construction and band parameters inferred from angleresolved photoemission within a band picture the low temperature hall data can only be fitted satisfactorily by invoking strong basalplane anisotropy in the meanfreepath el... | [['magnetotransport', 'measurements', 'on', 'the', 'overdoped', 'cuprate', 'la_17sr_03cuo_4', 'are', 'fitted', 'using', 'the', 'ong', 'construction', 'and', 'band', 'parameters', 'inferred', 'from', 'angleresolved', 'photoemission', 'within', 'a', 'band', 'picture', 'the', 'low', 'temperature', 'hall', 'data', 'can', '... | [-0.15372883116102054, 0.2213609324199044, -0.056861004347188604, 0.04126734167932429, -0.071188929467462, -0.16829738209748435, 0.1103663760677187, 0.4058192966712846, -0.3008134198271566, -0.29103461217859555, -0.07629419160592887, -0.3704985196495222, -0.07898249801041352, 0.1976740530692041, 0.0544059917718793, 0.0... |
707.4602 | Geometry of the theta divisor of a compactified jacobian | We study the theta divisor of the compactified jacobian of a nodal, possibly
reducible, curve. We compute its irreducible components and give it a geometric
interpretation consistent with the classical Brill-Noether theory of smooth
curves. Some applications on hyperelliptic stable curves are appended.
| math.AG | we study the theta divisor of the compactified jacobian of a nodal possibly reducible curve we compute its irreducible components and give it a geometric interpretation consistent with the classical brillnoether theory of smooth curves some applications on hyperelliptic stable curves are appended | [['we', 'study', 'the', 'theta', 'divisor', 'of', 'the', 'compactified', 'jacobian', 'of', 'a', 'nodal', 'possibly', 'reducible', 'curve', 'we', 'compute', 'its', 'irreducible', 'components', 'and', 'give', 'it', 'a', 'geometric', 'interpretation', 'consistent', 'with', 'the', 'classical', 'brillnoether', 'theory', 'of... | [-0.268585326095913, 0.04711898135259574, -0.20110364258289337, 0.10498209670186043, -0.1428569395874822, -0.23677663659936812, 0.017788005589377567, 0.31914637003602936, -0.2979944216650586, -0.15144913750808947, 0.12022816588246632, -0.2601419793506868, -0.18867328661212393, 0.2504950957156198, -0.1918900243634748, 0... |
707.4603 | Improved Laboratory Transition Probabilities for Neutral Chromium and
Re-determination of the Chromium Abundance for the Sun and Three Stars | Branching fraction measurements from Fourier transform spectra in conjunction
with published radiative lifetimes are used to determine transition
probabilities for 263 lines of neutral chromium. These laboratory values are
employed to derive a new photospheric abundance for the Sun: log $\epsilon$(Cr
I)$_{\odot}$ = 5... | astro-ph | branching fraction measurements from fourier transform spectra in conjunction with published radiative lifetimes are used to determine transition probabilities for 263 lines of neutral chromium these laboratory values are employed to derive a new photospheric abundance for the sun log epsiloncr i_odot 564pm001 sigma 00... | [['branching', 'fraction', 'measurements', 'from', 'fourier', 'transform', 'spectra', 'in', 'conjunction', 'with', 'published', 'radiative', 'lifetimes', 'are', 'used', 'to', 'determine', 'transition', 'probabilities', 'for', '263', 'lines', 'of', 'neutral', 'chromium', 'these', 'laboratory', 'values', 'are', 'employed... | [-0.03730502265883444, 0.14250131903299168, 0.03239287181838323, 0.0872870784696217, -0.046029092523920005, -0.15980340707855784, 0.0773233770263662, 0.4435904977256305, -0.1273093620452341, -0.3472154563382963, -0.026113451183422738, -0.33846517058395564, -0.00937200875431363, 0.14971164154919017, -0.0370814904940557,... |
707.4604 | Electronic and Vibrational Properties of gamma-AlH3 | Aluminum hydride (alane) AlH_3 is an important material in hydrogen storage
applications. It is known that AlH_3 exists in multiply forms of polymorphs,
where $\alpha$-AlH_3 is found to be the most stable with a hexagonal structure.
Recent experimental studies on $\gamma$-AlH_3 reported an orthorhombic
structure with... | cond-mat.mtrl-sci | aluminum hydride alane alh_3 is an important material in hydrogen storage applications it is known that alh_3 exists in multiply forms of polymorphs where alphaalh_3 is found to be the most stable with a hexagonal structure recent experimental studies on gammaalh_3 reported an orthorhombic structure with a unique doubl... | [['aluminum', 'hydride', 'alane', 'alh_3', 'is', 'an', 'important', 'material', 'in', 'hydrogen', 'storage', 'applications', 'it', 'is', 'known', 'that', 'alh_3', 'exists', 'in', 'multiply', 'forms', 'of', 'polymorphs', 'where', 'alphaalh_3', 'is', 'found', 'to', 'be', 'the', 'most', 'stable', 'with', 'a', 'hexagonal',... | [-0.10108768306442617, 0.14860285425513414, -0.03934210297266412, 0.019257374557689475, -0.018930151250880257, -0.12146309670348318, 0.03753008466985732, 0.41434919365026335, -0.24134437279721124, -0.2731329961622387, 0.018725768190860335, -0.33345288905763515, -0.13506577405101264, 0.15625528396067015, 0.0368200332360... |
707.4605 | Teaching the Kepler laws for freshmen | We present a natural proof of Kepler's law of ellipses in the spirit of
Euclidean geometry. Moreover we discuss two existing Euclidean geometric
proofs, one by Feynman in hist Lost Lecture from 1964 and the other by Newton
in the Principia of 1687.
| math.SG math.HO | we present a natural proof of keplers law of ellipses in the spirit of euclidean geometry moreover we discuss two existing euclidean geometric proofs one by feynman in hist lost lecture from 1964 and the other by newton in the principia of 1687 | [['we', 'present', 'a', 'natural', 'proof', 'of', 'keplers', 'law', 'of', 'ellipses', 'in', 'the', 'spirit', 'of', 'euclidean', 'geometry', 'moreover', 'we', 'discuss', 'two', 'existing', 'euclidean', 'geometric', 'proofs', 'one', 'by', 'feynman', 'in', 'hist', 'lost', 'lecture', 'from', '1964', 'and', 'the', 'other', ... | [-0.09527306548227708, 0.0593771500036467, -0.15569427119957846, 0.07709373499071875, -0.12323607915882455, -0.12482003584980618, 0.03922643677634729, 0.2297270103942516, -0.25318287711503895, -0.3030012068880159, 0.11286005934667882, -0.28953365879783105, -0.19592574860380832, 0.20055891694717629, -0.20142771396785975... |
707.4606 | LDA+Gutzwiller Method for Correlated Electron Systems | Combining the density functional theory (DFT) and the Gutzwiller variational
approach, a LDA+Gutzwiller method is developed to treat the correlated electron
systems from {\it ab-initio}. All variational parameters are self-consistently
determined from total energy minimization. The method is computationally
cheaper, ... | cond-mat.str-el cond-mat.mtrl-sci | combining the density functional theory dft and the gutzwiller variational approach a ldagutzwiller method is developed to treat the correlated electron systems from it abinitio all variational parameters are selfconsistently determined from total energy minimization the method is computationally cheaper yet the quasip... | [['combining', 'the', 'density', 'functional', 'theory', 'dft', 'and', 'the', 'gutzwiller', 'variational', 'approach', 'a', 'ldagutzwiller', 'method', 'is', 'developed', 'to', 'treat', 'the', 'correlated', 'electron', 'systems', 'from', 'it', 'abinitio', 'all', 'variational', 'parameters', 'are', 'selfconsistently', 'd... | [-0.02972789921696825, 0.11241180054192622, -0.08467645716505597, 0.15985725177536123, 0.002428921315459961, -0.15665860357974848, 0.0647379258066887, 0.4360095956643303, -0.3047366991578826, -0.3267771022686039, -0.04330364632678319, -0.34808690767421063, -0.13990421441595102, 0.18842947319239736, 0.06384042717224683,... |
707.4607 | LBB Stability of a Mixed Discontinuous/Continuous Galerkin Finite
Element Pair | We introduce a new mixed discontinuous/continuous Galerkin finite element for
solving the 2- and 3-dimensional wave equations and equations of incompressible
flow. The element, which we refer to as P1dg-P2, uses discontinuous piecewise
linear functions for velocity and continuous piecewise quadratic functions for
pre... | math.NA | we introduce a new mixed discontinuouscontinuous galerkin finite element for solving the 2 and 3dimensional wave equations and equations of incompressible flow the element which we refer to as p1dgp2 uses discontinuous piecewise linear functions for velocity and continuous piecewise quadratic functions for pressure the... | [['we', 'introduce', 'a', 'new', 'mixed', 'discontinuouscontinuous', 'galerkin', 'finite', 'element', 'for', 'solving', 'the', '2', 'and', '3dimensional', 'wave', 'equations', 'and', 'equations', 'of', 'incompressible', 'flow', 'the', 'element', 'which', 'we', 'refer', 'to', 'as', 'p1dgp2', 'uses', 'discontinuous', 'pi... | [-0.13332337610747502, 0.10269834517169764, -0.10176672092841371, 0.017552302773717953, -0.10205817047263617, -0.1368777895062838, -0.0339152544008001, 0.31794649676581765, -0.3062791208534137, -0.19172764645140294, 0.13369730312235492, -0.2449059713469899, -0.13559363273822744, 0.15491523952425823, -0.0087498377360727... |
707.4608 | Event-by-event transverse momentum fluctuations in nuclear collisions at
CERN SPS | The latest NA49 results on event-by-event transverse momentum fluctuations
are presented for central Pb+Pb interactions over the whole SPS energy range
(20A - 158A GeV). Two different methods are applied: evaluating the
$\Phi_{p_{T}}$ fluctuation measure and studying two-particle transverse
momentum correlations. The... | nucl-ex | the latest na49 results on eventbyevent transverse momentum fluctuations are presented for central pbpb interactions over the whole sps energy range 20a 158a gev two different methods are applied evaluating the phi_p_t fluctuation measure and studying twoparticle transverse momentum correlations the obtained results ar... | [['the', 'latest', 'na49', 'results', 'on', 'eventbyevent', 'transverse', 'momentum', 'fluctuations', 'are', 'presented', 'for', 'central', 'pbpb', 'interactions', 'over', 'the', 'whole', 'sps', 'energy', 'range', '20a', '158a', 'gev', 'two', 'different', 'methods', 'are', 'applied', 'evaluating', 'the', 'phi_p_t', 'fl... | [-0.09502897989260396, 0.20606681892489334, -0.17658742213488285, 0.1922803092251032, 0.017302481224760413, -0.06791085136554591, -0.08063905531676804, 0.35264882209097465, -0.16751776661769283, -0.29871003002655216, -0.019513738296199137, -0.39848795219710686, 0.10562075268499917, 0.2531681280872762, 0.085005266467682... |
707.4609 | Study of the radiative decay phi to a0(980) gamma with the KLOE detector | A sample of 1.25x10^9 phi decays, collected with the KLOE detector at the
Frascati phi-factory DAFNE at center of mass energy ~ Mphi, has been used to
study the radiative decay phi to eta pi0 gamma. This decay is dominated by phi
to a0(980) gamma. Two decay chains, corresponding to eta to gamma gamma and eta
to pi+ p... | hep-ex | a sample of 125x109 phi decays collected with the kloe detector at the frascati phifactory dafne at center of mass energy mphi has been used to study the radiative decay phi to eta pi0 gamma this decay is dominated by phi to a0980 gamma two decay chains corresponding to eta to gamma gamma and eta to pi pi pi0 have been... | [['a', 'sample', 'of', '125x109', 'phi', 'decays', 'collected', 'with', 'the', 'kloe', 'detector', 'at', 'the', 'frascati', 'phifactory', 'dafne', 'at', 'center', 'of', 'mass', 'energy', 'mphi', 'has', 'been', 'used', 'to', 'study', 'the', 'radiative', 'decay', 'phi', 'to', 'eta', 'pi0', 'gamma', 'this', 'decay', 'is',... | [-0.06635625793608607, 0.25567734160745936, -0.14555806522908551, 0.07495096346403482, -0.021258225579375543, -0.1754380611212103, 0.05788092323834257, 0.3170707687405088, -0.1880022781971161, -0.29568708827531326, -0.10022428315207962, -0.43816855818193445, 0.13443310091632507, 0.17529681777851958, 0.10130564038271225... |
707.461 | Estimates for the maximal singular integral in terms of the singular
integral:the case of even kernels | The purpose of this paper is to describe the smooth homogeneous
Calderon-Zygmund operators for which the maximal singular integral T*f may be
controlled by the singular integral Tf. We consider two types of control. The
first is the L2 estimate of T*f by Tf, namely the estimate of the L2 norm of
T*f by a constant tim... | math.CA math.AP | the purpose of this paper is to describe the smooth homogeneous calderonzygmund operators for which the maximal singular integral tf may be controlled by the singular integral tf we consider two types of control the first is the l2 estimate of tf by tf namely the estimate of the l2 norm of tf by a constant times the l2... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'describe', 'the', 'smooth', 'homogeneous', 'calderonzygmund', 'operators', 'for', 'which', 'the', 'maximal', 'singular', 'integral', 'tf', 'may', 'be', 'controlled', 'by', 'the', 'singular', 'integral', 'tf', 'we', 'consider', 'two', 'types', 'of', 'control', 'the... | [-0.1136709312927358, 0.10072967406464456, -0.0735568959257236, 0.11184964632396871, -0.06350957785676024, -0.11163577331280729, -0.001777586502618581, 0.2765690788664684, -0.29157255013428984, -0.18234992995034574, 0.16122992014430057, -0.27071586276917736, -0.10797830865849886, 0.19627665142452685, -0.096455915144020... |
707.4611 | Theory of swimming filaments in viscoelastic media | Motivated by the swimming of sperm in the non-Newtonian fluids of the female
mammalian reproductive tract, we examine the swimming of filaments in the
nonlinear viscoelastic Upper Convected Maxwell model. We obtain the swimming
velocity and hydrodynamic force exerted on an infinitely long cylinder with
prescribed bea... | cond-mat.soft | motivated by the swimming of sperm in the nonnewtonian fluids of the female mammalian reproductive tract we examine the swimming of filaments in the nonlinear viscoelastic upper convected maxwell model we obtain the swimming velocity and hydrodynamic force exerted on an infinitely long cylinder with prescribed beating ... | [['motivated', 'by', 'the', 'swimming', 'of', 'sperm', 'in', 'the', 'nonnewtonian', 'fluids', 'of', 'the', 'female', 'mammalian', 'reproductive', 'tract', 'we', 'examine', 'the', 'swimming', 'of', 'filaments', 'in', 'the', 'nonlinear', 'viscoelastic', 'upper', 'convected', 'maxwell', 'model', 'we', 'obtain', 'the', 'sw... | [-0.18033734144620508, 0.21142569886599752, -0.0773246573026191, -0.0019604654573128523, -0.1177424240116793, -0.1342751954917807, -0.02117077193043408, 0.3339997631194721, -0.301458067356059, -0.25604100170803357, -0.007426983375293034, -0.2327861037913216, -0.24052846414901047, 0.1745741467821939, -0.1521289444651948... |
707.4612 | Hartree-Fock theory for pseudorelativistic atoms | We study the Hartree-Fock model for pseudorelativistic atoms, that is, atoms
where the kinetic energy of the electrons is given by the pseudorelativistic
operator \sqrt{(pc)^2+(mc^2)^2}-mc^2. We prove the existence of a Hartree-Fock
minimizer, and prove regularity away from the nucleus and pointwise exponential
decay... | math-ph math.MP | we study the hartreefock model for pseudorelativistic atoms that is atoms where the kinetic energy of the electrons is given by the pseudorelativistic operator sqrtpc2mc22mc2 we prove the existence of a hartreefock minimizer and prove regularity away from the nucleus and pointwise exponential decay of the corresponding... | [['we', 'study', 'the', 'hartreefock', 'model', 'for', 'pseudorelativistic', 'atoms', 'that', 'is', 'atoms', 'where', 'the', 'kinetic', 'energy', 'of', 'the', 'electrons', 'is', 'given', 'by', 'the', 'pseudorelativistic', 'operator', 'sqrtpc2mc22mc2', 'we', 'prove', 'the', 'existence', 'of', 'a', 'hartreefock', 'minimi... | [-0.07780458801921378, 0.12058534526434589, -0.04720716556890848, 0.13239937935995452, 0.041468885013873275, -0.10655718614803032, 0.07029118226405154, 0.29724946836049254, -0.28466728186987816, -0.19005970078262877, -0.01032308421216588, -0.36244686233236434, -0.03382889411233841, 0.0713971911067579, 0.059823788643041... |
707.4613 | Correlation Effects in Wave Function Mapping of Molecular Beam Epitaxy
Grown Quantum Dots | We investigate correlation effects in the regime of a few electrons in
uncapped InAs quantum dots by tunneling spectroscopy and wave function (WF)
mapping at high tunneling currents where electron-electron interactions become
relevant. Four clearly resolved states are found, whose approximate symmetries
are roughly s... | cond-mat.mes-hall cond-mat.str-el | we investigate correlation effects in the regime of a few electrons in uncapped inas quantum dots by tunneling spectroscopy and wave function wf mapping at high tunneling currents where electronelectron interactions become relevant four clearly resolved states are found whose approximate symmetries are roughly s and p ... | [['we', 'investigate', 'correlation', 'effects', 'in', 'the', 'regime', 'of', 'a', 'few', 'electrons', 'in', 'uncapped', 'inas', 'quantum', 'dots', 'by', 'tunneling', 'spectroscopy', 'and', 'wave', 'function', 'wf', 'mapping', 'at', 'high', 'tunneling', 'currents', 'where', 'electronelectron', 'interactions', 'become',... | [-0.16119772018619666, 0.19426315706468333, -0.02260932988597472, 0.11040806057740395, 0.08528429738883125, -0.15965642416849732, 0.010220719882483152, 0.36521675682773713, -0.25128292451171497, -0.30083286089724615, -0.00939700481923003, -0.3693814624493059, -0.0947667240214191, 0.1550969475518765, 0.08191467352015408... |
707.4614 | Thermal conductivity of ions in a neutron star envelope | We analyze the thermal conductivity of ions (equivalent to the conductivity
of phonons in crystalline matter) in a neutron star envelope.
We calculate the ion/phonon thermal conductivity in a crystal of atomic
nuclei using variational formalism and performing momentum-space integration by
Monte Carlo method. We tak... | astro-ph cond-mat.stat-mech physics.plasm-ph | we analyze the thermal conductivity of ions equivalent to the conductivity of phonons in crystalline matter in a neutron star envelope we calculate the ionphonon thermal conductivity in a crystal of atomic nuclei using variational formalism and performing momentumspace integration by monte carlo method we take into acc... | [['we', 'analyze', 'the', 'thermal', 'conductivity', 'of', 'ions', 'equivalent', 'to', 'the', 'conductivity', 'of', 'phonons', 'in', 'crystalline', 'matter', 'in', 'a', 'neutron', 'star', 'envelope', 'we', 'calculate', 'the', 'ionphonon', 'thermal', 'conductivity', 'in', 'a', 'crystal', 'of', 'atomic', 'nuclei', 'using... | [-0.08918215267400438, 0.2560619598751917, -0.039360989066796546, 0.045038696632023256, -0.04879688837867796, -0.08052569136745175, 0.050960344991388275, 0.41046077453077856, -0.23238870023666877, -0.2806663485835136, -0.0020451238598303955, -0.3048817175306399, 0.009712224403220712, 0.22675552430711393, 0.037983897356... |
707.4615 | New nuclear three-body clusters \phi{NN} | Binding energies of three-body systems of the type \phi+2N are estimated. Due
to the strong attraction between \phi-meson and nucleon, suggested in different
approaches, bound states can appear in systems like \phi+np (singlet and
triplet) and \phi+pp. This indicates the principal possibility of the formation
of new ... | nucl-th | binding energies of threebody systems of the type phi2n are estimated due to the strong attraction between phimeson and nucleon suggested in different approaches bound states can appear in systems like phinp singlet and triplet and phipp this indicates the principal possibility of the formation of new nuclear clusters | [['binding', 'energies', 'of', 'threebody', 'systems', 'of', 'the', 'type', 'phi2n', 'are', 'estimated', 'due', 'to', 'the', 'strong', 'attraction', 'between', 'phimeson', 'and', 'nucleon', 'suggested', 'in', 'different', 'approaches', 'bound', 'states', 'can', 'appear', 'in', 'systems', 'like', 'phinp', 'singlet', 'an... | [-0.11383315720983471, 0.1835272149182856, -0.07498673361260444, 0.14646834149364926, 0.02415454470307547, -0.1202619637188036, 0.03323601207618291, 0.3098546930317146, -0.22910927776198756, -0.31156149205829325, -0.05897516604454722, -0.2880000891940047, -0.06110638448202129, 0.11566051908691104, 0.0606859260199902, 0... |
707.4616 | Measurement of the eta mass at KLOE | An integrated luminosity of 410 pb^(-1), corresponding to ~ 17 million of eta
events, has been analyzed to measure the eta mass using the decay eta to gamma
gamma. The measurement is insensitive to the calorimeter energy calibration and
the systematic error on the measurement is dominated by the uniformity of the
det... | hep-ex | an integrated luminosity of 410 pb1 corresponding to 17 million of eta events has been analyzed to measure the eta mass using the decay eta to gamma gamma the measurement is insensitive to the calorimeter energy calibration and the systematic error on the measurement is dominated by the uniformity of the detector respo... | [['an', 'integrated', 'luminosity', 'of', '410', 'pb1', 'corresponding', 'to', '17', 'million', 'of', 'eta', 'events', 'has', 'been', 'analyzed', 'to', 'measure', 'the', 'eta', 'mass', 'using', 'the', 'decay', 'eta', 'to', 'gamma', 'gamma', 'the', 'measurement', 'is', 'insensitive', 'to', 'the', 'calorimeter', 'energy'... | [-0.05437115482359289, 0.1653530831389166, -0.1115082817752715, 0.06714753388910268, -0.02231122058012227, -0.07564452841059766, 0.05029979458940433, 0.3384834415862493, -0.18613909724251168, -0.356828432826099, -0.011095338719722894, -0.40168968469740074, 0.07828230069619473, 0.22704789895677469, 0.009189010680452964,... |
707.4617 | Integrality of instanton numbers | We prove the results announced in a joint paper (arXiv:hep-th/0603106) with
Maxim Kontsevich and Albert Schwarz.
| math.AG | we prove the results announced in a joint paper arxivhepth0603106 with maxim kontsevich and albert schwarz | [['we', 'prove', 'the', 'results', 'announced', 'in', 'a', 'joint', 'paper', 'arxivhepth0603106', 'with', 'maxim', 'kontsevich', 'and', 'albert', 'schwarz']] | [-0.14331840413312116, -0.06007334079282979, -0.12835742235183717, 0.010730973025783897, -0.14987114568551382, -0.1081592601723969, 0.030058476771228016, 0.2658939426143964, -0.20866709984838963, -0.2755207632978757, 0.049559939024038616, -0.2451831955462694, -0.31603370408217113, 0.1552078555027644, -0.326532089896500... |
707.4618 | Nonlinear Matroid Optimization and Experimental Design | We study the problem of optimizing nonlinear objective functions over
matroids presented by oracles or explicitly. Such functions can be interpreted
as the balancing of multi-criteria optimization. We provide a combinatorial
polynomial time algorithm for arbitrary oracle-presented matroids, that makes
repeated use of... | math.CO cs.CC cs.DM math.OC | we study the problem of optimizing nonlinear objective functions over matroids presented by oracles or explicitly such functions can be interpreted as the balancing of multicriteria optimization we provide a combinatorial polynomial time algorithm for arbitrary oraclepresented matroids that makes repeated use of matroi... | [['we', 'study', 'the', 'problem', 'of', 'optimizing', 'nonlinear', 'objective', 'functions', 'over', 'matroids', 'presented', 'by', 'oracles', 'or', 'explicitly', 'such', 'functions', 'can', 'be', 'interpreted', 'as', 'the', 'balancing', 'of', 'multicriteria', 'optimization', 'we', 'provide', 'a', 'combinatorial', 'po... | [-0.1197899909521867, 0.0012549362745630788, -0.058625473472703665, 0.08546571668800122, -0.11824192487013836, -0.12195306297831444, 0.03609900563929437, 0.42910255543473697, -0.3522345428290363, -0.30509109639226356, 0.10100116763149142, -0.15369304407957113, -0.23691185690242694, 0.21533963246878962, -0.1383013082215... |
707.4619 | Control of sub-excitable waves in neural networks by nonlocal coupling | Transient wave forms in neural networks with diffusive and nonlocal coupling
have attracted particular interest because they may mediate recruitment of
healthy cortical tissue into a pathological state during migraine. To
investigate this process, we use a reaction-diffusion system of
inhibitor-activator type as a ge... | nlin.PS nlin.AO | transient wave forms in neural networks with diffusive and nonlocal coupling have attracted particular interest because they may mediate recruitment of healthy cortical tissue into a pathological state during migraine to investigate this process we use a reactiondiffusion system of inhibitoractivator type as a generic ... | [['transient', 'wave', 'forms', 'in', 'neural', 'networks', 'with', 'diffusive', 'and', 'nonlocal', 'coupling', 'have', 'attracted', 'particular', 'interest', 'because', 'they', 'may', 'mediate', 'recruitment', 'of', 'healthy', 'cortical', 'tissue', 'into', 'a', 'pathological', 'state', 'during', 'migraine', 'to', 'inv... | [-0.19466619452111467, 0.15229658727207085, -0.0031640776326410645, 0.027296111813748282, -0.10528472058460799, -0.18025978921933938, 0.04164614536415587, 0.3746819542436541, -0.2682518820172373, -0.2158113253669003, 0.06301945698614594, -0.24781740761809903, -0.2620181347286144, 0.17428897643099248, 0.0015358390386095... |
707.462 | Nuclear equation of state at high baryonic density and compact star
constraints | A mean field calculation is carried out to obtain the equation of state (EoS)
of nuclear matter from a density dependent M3Y interaction (DDM3Y). The energy
per nucleon is minimized to obtain ground state of the symmetric nuclear matter
(SNM). The constants of density dependence of the effective interaction are
obtai... | nucl-th astro-ph hep-ph nucl-ex | a mean field calculation is carried out to obtain the equation of state eos of nuclear matter from a density dependent m3y interaction ddm3y the energy per nucleon is minimized to obtain ground state of the symmetric nuclear matter snm the constants of density dependence of the effective interaction are obtained by rep... | [['a', 'mean', 'field', 'calculation', 'is', 'carried', 'out', 'to', 'obtain', 'the', 'equation', 'of', 'state', 'eos', 'of', 'nuclear', 'matter', 'from', 'a', 'density', 'dependent', 'm3y', 'interaction', 'ddm3y', 'the', 'energy', 'per', 'nucleon', 'is', 'minimized', 'to', 'obtain', 'ground', 'state', 'of', 'the', 'sy... | [-0.06148009817624882, 0.1990045543818587, -0.15360461078492588, 0.11884642610468907, -0.047330379618403036, -0.06619444133330879, 0.007095192584509406, 0.31656496574888465, -0.212699529875192, -0.3375916632268924, 0.003428417007321787, -0.30242382208791263, 0.03643639999552493, 0.11065204139249246, 0.10679427040689955... |
707.4621 | Semiparametrically efficient rank-based inference for shape I. optimal
rank-based tests for sphericity | We propose a class of rank-based procedures for testing that the shape matrix
$\mathbf{V}$ of an elliptical distribution (with unspecified center of
symmetry, scale and radial density) has some fixed value ${\mathbf{V}}_0$; this
includes, for ${\mathbf{V}}_0={\mathbf{I}}_k$, the problem of testing for
sphericity as a... | math.ST stat.TH | we propose a class of rankbased procedures for testing that the shape matrix mathbfv of an elliptical distribution with unspecified center of symmetry scale and radial density has some fixed value mathbfv_0 this includes for mathbfv_0mathbfi_k the problem of testing for sphericity as an important particular case the pr... | [['we', 'propose', 'a', 'class', 'of', 'rankbased', 'procedures', 'for', 'testing', 'that', 'the', 'shape', 'matrix', 'mathbfv', 'of', 'an', 'elliptical', 'distribution', 'with', 'unspecified', 'center', 'of', 'symmetry', 'scale', 'and', 'radial', 'density', 'has', 'some', 'fixed', 'value', 'mathbfv_0', 'this', 'includ... | [-0.05884297052197608, 0.10487570925403722, -0.07773457368703335, 0.09426624762950112, -0.03608025657715565, -0.149851391213376, 0.006296888351338064, 0.4037357839747685, -0.20999246970188387, -0.3047283883826257, 0.13033996657357985, -0.24800351373289295, -0.0475692127977803, 0.1617229702784118, -0.08530485025779665, ... |
707.4622 | Theory of spin qubits in nanostructures | We review recent advances on the theory of spin qubits in nanostructures. We
focus on four selected topics. First, we show how to form spin qubits in the
new and promising material graphene. Afterwards, we discuss spin relaxation and
decoherence in quantum dots. In particular, we demonstrate how charge
fluctations in... | cond-mat.mes-hall | we review recent advances on the theory of spin qubits in nanostructures we focus on four selected topics first we show how to form spin qubits in the new and promising material graphene afterwards we discuss spin relaxation and decoherence in quantum dots in particular we demonstrate how charge fluctations in the surr... | [['we', 'review', 'recent', 'advances', 'on', 'the', 'theory', 'of', 'spin', 'qubits', 'in', 'nanostructures', 'we', 'focus', 'on', 'four', 'selected', 'topics', 'first', 'we', 'show', 'how', 'to', 'form', 'spin', 'qubits', 'in', 'the', 'new', 'and', 'promising', 'material', 'graphene', 'afterwards', 'we', 'discuss', '... | [-0.1698736706258435, 0.20636492155787428, -0.01269766805987609, 0.03293924333513388, -0.06800068652649459, -0.13828568124588123, -0.006723077454105869, 0.43662498925665494, -0.2695847321955258, -0.25659189660821047, -0.001305146884222172, -0.2896981743397191, -0.15555024650274663, 0.1973592683574871, 0.038685147450387... |
707.4623 | Preliminary measurement of Gamma(Ke2)/Gamma(Km2) at KLOE | A preliminary measurement of RK = Gamma(Ke2)/Gamma(Km2) at the KLOE
experiment is discussed. The result, RK = (2.55+-0.05+-0.05)x 10^-5, is based
on 1.7 fb^-1 of luminosity integrated on the phi-meson peak at the Frascati
e^+e^- collider DAFNE, corresponding to ~8000 observed Ke2 events. Perspectives
on the methods p... | hep-ex | a preliminary measurement of rk gammake2gammakm2 at the kloe experiment is discussed the result rk 255005005x 105 is based on 17 fb1 of luminosity integrated on the phimeson peak at the frascati ee collider dafne corresponding to 8000 observed ke2 events perspectives on the methods planned to improve both the statistic... | [['a', 'preliminary', 'measurement', 'of', 'rk', 'gammake2gammakm2', 'at', 'the', 'kloe', 'experiment', 'is', 'discussed', 'the', 'result', 'rk', '255005005x', '105', 'is', 'based', 'on', '17', 'fb1', 'of', 'luminosity', 'integrated', 'on', 'the', 'phimeson', 'peak', 'at', 'the', 'frascati', 'ee', 'collider', 'dafne', ... | [-0.029415154821305935, 0.10311913256321402, -0.09335366404515558, 0.13118925080717808, -0.02435521442436896, -0.09737990564566903, 0.04327320686674544, 0.3484451298468879, -0.1435678227405463, -0.3075892148824226, 0.09474008882950459, -0.4366705144722281, 0.07959042369787182, 0.24829777696036867, 0.030037890521011183,... |
707.4624 | Conceptual Design of a Micron-Scale Atomic Clock | A theoretical proposal for reducing an entire atomic clock to micron
dimensions. A phosphorus or nitrogen atom is introduced into a fullerene cage.
This endohedral fullerene is then coated with an insulating shell and a number
of them are deposited as a thin layer on a silicon chip. Next to this layer a
GMR sensor is... | physics.atom-ph physics.ins-det | a theoretical proposal for reducing an entire atomic clock to micron dimensions a phosphorus or nitrogen atom is introduced into a fullerene cage this endohedral fullerene is then coated with an insulating shell and a number of them are deposited as a thin layer on a silicon chip next to this layer a gmr sensor is fabr... | [['a', 'theoretical', 'proposal', 'for', 'reducing', 'an', 'entire', 'atomic', 'clock', 'to', 'micron', 'dimensions', 'a', 'phosphorus', 'or', 'nitrogen', 'atom', 'is', 'introduced', 'into', 'a', 'fullerene', 'cage', 'this', 'endohedral', 'fullerene', 'is', 'then', 'coated', 'with', 'an', 'insulating', 'shell', 'and', ... | [-0.12017525721436748, 0.1536458902166531, 0.029631378716811627, -0.07262384461544746, -0.027172831230774432, -0.15125308145561356, 0.07915184831706784, 0.4238992517881365, -0.20112132423568563, -0.3240946358776685, 0.04790799382790721, -0.28536500374741675, -0.05980236734353365, 0.16941809345524847, -0.038050821797181... |
707.4625 | Holographic Dark Energy Model with Modified Generalized Chaplygin Gas | We present a holographic dark energy model of the universe considering
modified generalized Chaplygin gas (GCG). The modified GCG behaves as an
ordinary barotropic fluid in the early epoch when the universe was tiny but
behaves subsequently as a $\Lambda$CDM model at late epoch. An equivalent model
with scalar field ... | gr-qc | we present a holographic dark energy model of the universe considering modified generalized chaplygin gas gcg the modified gcg behaves as an ordinary barotropic fluid in the early epoch when the universe was tiny but behaves subsequently as a lambdacdm model at late epoch an equivalent model with scalar field is obtain... | [['we', 'present', 'a', 'holographic', 'dark', 'energy', 'model', 'of', 'the', 'universe', 'considering', 'modified', 'generalized', 'chaplygin', 'gas', 'gcg', 'the', 'modified', 'gcg', 'behaves', 'as', 'an', 'ordinary', 'barotropic', 'fluid', 'in', 'the', 'early', 'epoch', 'when', 'the', 'universe', 'was', 'tiny', 'bu... | [-0.09826771432586436, 0.15102116874780916, -0.15887552187828127, 0.1271473346303107, -0.09269811037767639, -0.17947827910964367, -0.11057608696051262, 0.25853577316288023, -0.22402240808612556, -0.3214413102926506, 0.013912645436482884, -0.23486772890613283, -0.036116234637716765, 0.09398853377519195, 0.02275751389422... |
707.4626 | The First Swift BAT Gamma-Ray Burst Catalog | We present the first Swift Burst Alert Telescope (BAT) catalog of gamma-ray
bursts (GRBs), which contains bursts detected by the BAT between 2004 December
19 and 2007 June 16. This catalog (hereafter BAT1 catalog) contains burst
trigger time, location, 90% error radius, duration, fluence, peak flux, and
time averaged... | astro-ph | we present the first swift burst alert telescope bat catalog of gammaray bursts grbs which contains bursts detected by the bat between 2004 december 19 and 2007 june 16 this catalog hereafter bat1 catalog contains burst trigger time location 90 error radius duration fluence peak flux and time averaged spectral paramete... | [['we', 'present', 'the', 'first', 'swift', 'burst', 'alert', 'telescope', 'bat', 'catalog', 'of', 'gammaray', 'bursts', 'grbs', 'which', 'contains', 'bursts', 'detected', 'by', 'the', 'bat', 'between', '2004', 'december', '19', 'and', '2007', 'june', '16', 'this', 'catalog', 'hereafter', 'bat1', 'catalog', 'contains',... | [-0.03875679223975866, 0.16219385706138598, -0.04330907363412267, 0.20547072845443845, -0.10331973434436657, -0.09441262515493254, 0.1300057614561321, 0.522232244383393, -0.10095283746277925, -0.448686535109502, 0.010552183493455021, -0.3990830818266538, -0.0035815934268380867, 0.293275301520998, -0.03708241113213919, ... |
707.4627 | GRI: focusing on the evolving violent Universe | The Gamma-Ray Imager (GRI) is a novel mission concept that will provide an
unprecedented sensitivity leap in the soft gamma-ray domain by using for the
first time a focusing lens built of Laue diffracting crystals. The lens will
cover an energy band from 200 - 1300 keV with an effective area reaching 600
cm2. It will... | astro-ph | the gammaray imager gri is a novel mission concept that will provide an unprecedented sensitivity leap in the soft gammaray domain by using for the first time a focusing lens built of laue diffracting crystals the lens will cover an energy band from 200 1300 kev with an effective area reaching 600 cm2 it will be comple... | [['the', 'gammaray', 'imager', 'gri', 'is', 'a', 'novel', 'mission', 'concept', 'that', 'will', 'provide', 'an', 'unprecedented', 'sensitivity', 'leap', 'in', 'the', 'soft', 'gammaray', 'domain', 'by', 'using', 'for', 'the', 'first', 'time', 'a', 'focusing', 'lens', 'built', 'of', 'laue', 'diffracting', 'crystals', 'th... | [-0.06555283781265396, 0.1360619816368302, -0.07896696716885675, 0.07626679909519611, -0.10948513994596644, -0.08492487255857255, -0.009736183925821078, 0.4140836994646992, -0.1850265744309802, -0.41324966843239963, 0.11780911228825888, -0.31825073482468724, -0.02230988592892765, 0.2473341252061249, -0.0480856958831392... |
707.4628 | Forbidden patterns and shift systems | The scope of this paper is two-fold. First, to present to the researchers in
combinatorics an interesting implementation of permutations avoiding
generalized patterns in the framework of discrete-time dynamical systems.
Indeed, the orbits generated by piecewise monotone maps on one-dimensional
intervals have forbidde... | math.DS math.CO | the scope of this paper is twofold first to present to the researchers in combinatorics an interesting implementation of permutations avoiding generalized patterns in the framework of discretetime dynamical systems indeed the orbits generated by piecewise monotone maps on onedimensional intervals have forbidden order p... | [['the', 'scope', 'of', 'this', 'paper', 'is', 'twofold', 'first', 'to', 'present', 'to', 'the', 'researchers', 'in', 'combinatorics', 'an', 'interesting', 'implementation', 'of', 'permutations', 'avoiding', 'generalized', 'patterns', 'in', 'the', 'framework', 'of', 'discretetime', 'dynamical', 'systems', 'indeed', 'th... | [-0.16800577878448353, 0.15271060498913222, -0.07411826601201275, 0.0913621831178611, -0.07755232071757417, -0.103969224982065, 0.07009787582570598, 0.36122935876681084, -0.32847453581587394, -0.2491306425135608, 0.11898154178776835, -0.2602365687172733, -0.1827068008849917, 0.19762095391550766, -0.060745156065206085, ... |
707.4629 | On the role of stochastic Fermi acceleration in setting the dissipation
scale of turbulence in the interstellar medium | We consider the dissipation by Fermi acceleration of magnetosonic turbulence
in the Reynolds Layer of the interstellar medium. The scale in the cascade at
which electron acceleration via stochastic Fermi acceleration (STFA) becomes
comparable to further cascade of the turbulence defines the inner scale. For
any magne... | astro-ph | we consider the dissipation by fermi acceleration of magnetosonic turbulence in the reynolds layer of the interstellar medium the scale in the cascade at which electron acceleration via stochastic fermi acceleration stfa becomes comparable to further cascade of the turbulence defines the inner scale for any magnetic tu... | [['we', 'consider', 'the', 'dissipation', 'by', 'fermi', 'acceleration', 'of', 'magnetosonic', 'turbulence', 'in', 'the', 'reynolds', 'layer', 'of', 'the', 'interstellar', 'medium', 'the', 'scale', 'in', 'the', 'cascade', 'at', 'which', 'electron', 'acceleration', 'via', 'stochastic', 'fermi', 'acceleration', 'stfa', '... | [-0.1147247506830084, 0.2386568906969822, -0.06545011197462432, 0.07865741101712766, -0.049210617888033145, -0.06997188123628743, -0.016944961095290197, 0.3388826804808699, -0.2763662627094763, -0.30166542072074265, 0.012995503489746825, -0.2533238015373002, -0.015483022709684139, 0.2105035931396472, 0.0236512893480811... |
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