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706.3714 | No phase transition for Gaussian fields with bounded spins | Let a<b, \Omega=[a,b]^{\Z^d} and H be the (formal) Hamiltonian defined on
\Omega by
H(\eta) = \frac12 \sum_{x,y\in\Z^d} J(x-y) (\eta(x)-\eta(y))^2 where
J:\Z^d\to\R is any summable non-negative symmetric function (J(x)\ge 0 for all
x\in\Z^d, \sum_x J(x)<\infty and J(x)=J(-x)). We prove that there is a unique
Gibbs ... | math.PR math-ph math.MP | let ab omegaabzd and h be the formal hamiltonian defined on omega by heta frac12 sum_xyinzd jxy etaxetay2 where jzdtor is any summable nonnegative symmetric function jxge 0 for all xinzd sum_x jxinfty and jxjx we prove that there is a unique gibbs measure on omega associated to h the result is a consequence of the fact... | [['let', 'ab', 'omegaabzd', 'and', 'h', 'be', 'the', 'formal', 'hamiltonian', 'defined', 'on', 'omega', 'by', 'heta', 'frac12', 'sum_xyinzd', 'jxy', 'etaxetay2', 'where', 'jzdtor', 'is', 'any', 'summable', 'nonnegative', 'symmetric', 'function', 'jxge', '0', 'for', 'all', 'xinzd', 'sum_x', 'jxinfty', 'and', 'jxjx', 'we... | [-0.1674355005638467, 0.1513280921656313, -0.11093467763728565, 0.05112749776832523, -0.06540542229684809, -0.192796126621524, -0.006212821838239001, 0.3772593734874612, -0.3087043979515632, -0.15879539617647728, 0.07177381875873026, -0.3181513726474747, -0.09188442508734408, 0.13073003291714166, -0.04932437534074462, ... |
706.3715 | Faraday Rotation in Global Accretion Disk Simulations: Implications for
Sgr A* | These Faraday rotation calculations of hot, thick accretion flows are
motivated by the measured steady rotation measure (RM) of $\approx -6 \times
10^5$ rad m$^{-2}$ from Sgr A*. In our numerical simulations, the quasi-steady
state structure of the accretion flow, and the RM it produces, depends on the
initial magnet... | astro-ph | these faraday rotation calculations of hot thick accretion flows are motivated by the measured steady rotation measure rm of approx 6 times 105 rad m2 from sgr a in our numerical simulations the quasisteady state structure of the accretion flow and the rm it produces depends on the initial magnetic field in spite of th... | [['these', 'faraday', 'rotation', 'calculations', 'of', 'hot', 'thick', 'accretion', 'flows', 'are', 'motivated', 'by', 'the', 'measured', 'steady', 'rotation', 'measure', 'rm', 'of', 'approx', '6', 'times', '105', 'rad', 'm2', 'from', 'sgr', 'a', 'in', 'our', 'numerical', 'simulations', 'the', 'quasisteady', 'state', ... | [-0.15543635659129687, 0.19089585307106896, 0.004127397282298287, 0.05971371417358504, -0.014124355159214579, -0.06961514698472661, -0.022680508419641778, 0.40382961136564405, -0.20512230534140927, -0.34293186793785907, 0.09852968469634324, -0.26586980652064085, 0.04300057112311446, 0.23828558725367208, -0.031673392376... |
706.3716 | Lieb--Thirring bounds for complex Jacobi matrices | We obtain various versions of classical Lieb--Thirring bounds for one- and
multi-dimensional complex Jacobi matrices. Our method is based on Fan-Mirski
Lemma and seems to be fairly general.
| math-ph math.MP math.SP | we obtain various versions of classical liebthirring bounds for one and multidimensional complex jacobi matrices our method is based on fanmirski lemma and seems to be fairly general | [['we', 'obtain', 'various', 'versions', 'of', 'classical', 'liebthirring', 'bounds', 'for', 'one', 'and', 'multidimensional', 'complex', 'jacobi', 'matrices', 'our', 'method', 'is', 'based', 'on', 'fanmirski', 'lemma', 'and', 'seems', 'to', 'be', 'fairly', 'general']] | [-0.05277927523409879, 0.005024351903961765, -0.1356273286251558, 0.17411962070899015, -0.12628888131843674, -0.19419252389559039, 0.01975653831053663, 0.325734986682181, -0.2496814726403466, -0.277115678983844, 0.1896018728794944, -0.20812901305207224, -0.18096190451264935, 0.3462046597290922, -0.11391246387803997, 0.... |
706.3717 | Corrections to the generalized vector dominance due to diffractive rho_3
production | The idea of the vector dominance is still in use in various analyses of
experimental data of photon-hadron reactions. It makes sense, therefore, to
recast results of microscopic calculations of such reactions in this language.
Here we present the diffractive DIS $\rho_3$ production as a specific
correction to the gen... | hep-ph hep-ex | the idea of the vector dominance is still in use in various analyses of experimental data of photonhadron reactions it makes sense therefore to recast results of microscopic calculations of such reactions in this language here we present the diffractive dis rho_3 production as a specific correction to the generalized v... | [['the', 'idea', 'of', 'the', 'vector', 'dominance', 'is', 'still', 'in', 'use', 'in', 'various', 'analyses', 'of', 'experimental', 'data', 'of', 'photonhadron', 'reactions', 'it', 'makes', 'sense', 'therefore', 'to', 'recast', 'results', 'of', 'microscopic', 'calculations', 'of', 'such', 'reactions', 'in', 'this', 'la... | [-0.07853038565017192, 0.15532353929408668, -0.14673906088829403, 0.13801799555558983, -0.07983913236842831, -0.07834097634569355, 0.06671712090965451, 0.3578998529261387, -0.2630518899049337, -0.2069503573882507, -0.005696453473519352, -0.3124397383525786, -0.12780056532654094, 0.1307696720170675, 0.01761238867553269,... |
706.3718 | Four Generations and Higgs Physics | In the light of the LHC, we revisit the implications of a fourth generation
of chiral matter. We identify a specific ensemble of particle masses and
mixings that are in agreement with all current experimental bounds as well as
minimize the contributions to electroweak precision observables. Higgs masses
between 115-3... | hep-ph | in the light of the lhc we revisit the implications of a fourth generation of chiral matter we identify a specific ensemble of particle masses and mixings that are in agreement with all current experimental bounds as well as minimize the contributions to electroweak precision observables higgs masses between 115315 115... | [['in', 'the', 'light', 'of', 'the', 'lhc', 'we', 'revisit', 'the', 'implications', 'of', 'a', 'fourth', 'generation', 'of', 'chiral', 'matter', 'we', 'identify', 'a', 'specific', 'ensemble', 'of', 'particle', 'masses', 'and', 'mixings', 'that', 'are', 'in', 'agreement', 'with', 'all', 'current', 'experimental', 'bound... | [-0.10273059203383364, 0.28083013396655376, -0.034545069107464944, 0.1946561079532957, -0.06663059104750511, -0.14034662259734793, 0.057795211985832505, 0.34443611621821474, -0.1841381921612916, -0.33922183391552013, 0.05813151251274247, -0.32552859745919704, 0.0008677471382152132, 0.17920100885862092, 0.02840828006507... |
706.3719 | Spectrum and thermal fluctuations of a microcavity polariton
Bose-Einstein condensate | The Hartree-Fock-Popov theory of interacting Bose particles is developed, for
modeling exciton-polaritons in semiconductor microcavities undergoing
Bose-Einstein condensation. A self-consistent treatment of the linear
exciton-photon coupling and of the exciton non-linearity provides a thermal
equilibrium description ... | cond-mat.mes-hall cond-mat.other | the hartreefockpopov theory of interacting bose particles is developed for modeling excitonpolaritons in semiconductor microcavities undergoing boseeinstein condensation a selfconsistent treatment of the linear excitonphoton coupling and of the exciton nonlinearity provides a thermal equilibrium description of the coll... | [['the', 'hartreefockpopov', 'theory', 'of', 'interacting', 'bose', 'particles', 'is', 'developed', 'for', 'modeling', 'excitonpolaritons', 'in', 'semiconductor', 'microcavities', 'undergoing', 'boseeinstein', 'condensation', 'a', 'selfconsistent', 'treatment', 'of', 'the', 'linear', 'excitonphoton', 'coupling', 'and',... | [-0.1758769113129299, 0.23902389603225807, -0.12876399138354158, 0.03039253379112077, -0.002712465561272805, -0.15163123364184508, 0.05521613470352206, 0.3573593461003743, -0.14299781237353096, -0.23087547260352917, -0.08192305651844659, -0.2937549697725396, -0.09991473042847294, 0.1599521535742832, 0.09873093154869582... |
706.372 | How Can We Avert Dangerous Climate Change? | Recent analyses indicate that the amount of atmospheric CO2 required to cause
dangerous climate change is at most 450 ppm, and likely less than that.
Reductions of non-CO2 climate forcings can provide only moderate, albeit
important, adjustments to the CO2 limit. Realization of how close the planet is
to "tipping poi... | physics.ao-ph | recent analyses indicate that the amount of atmospheric co2 required to cause dangerous climate change is at most 450 ppm and likely less than that reductions of nonco2 climate forcings can provide only moderate albeit important adjustments to the co2 limit realization of how close the planet is to tipping points with ... | [['recent', 'analyses', 'indicate', 'that', 'the', 'amount', 'of', 'atmospheric', 'co2', 'required', 'to', 'cause', 'dangerous', 'climate', 'change', 'is', 'at', 'most', '450', 'ppm', 'and', 'likely', 'less', 'than', 'that', 'reductions', 'of', 'nonco2', 'climate', 'forcings', 'can', 'provide', 'only', 'moderate', 'alb... | [-0.06987912983985971, 0.16457099034458814, -0.04235848396311741, 0.09385156549160947, -0.09711986532359308, -0.1292314231672601, 0.1269962962666476, 0.3404982861773287, -0.22379835761605282, -0.3536573605184015, 0.17113222027814168, -0.28980085097026786, -0.14544235502520728, 0.1784518546670222, -0.1386878681117417, 0... |
706.3721 | Stability Limits in Resonant Planetary Systems | The relationship between the boundaries for Hill and Lagrange stability in
orbital element space is modified in the case of resonantly interacting
planets. Hill stability requires the ordering of the planets to remain constant
while Lagrange stability also requires all planets to remain bound to the
central star. The... | astro-ph | the relationship between the boundaries for hill and lagrange stability in orbital element space is modified in the case of resonantly interacting planets hill stability requires the ordering of the planets to remain constant while lagrange stability also requires all planets to remain bound to the central star the hil... | [['the', 'relationship', 'between', 'the', 'boundaries', 'for', 'hill', 'and', 'lagrange', 'stability', 'in', 'orbital', 'element', 'space', 'is', 'modified', 'in', 'the', 'case', 'of', 'resonantly', 'interacting', 'planets', 'hill', 'stability', 'requires', 'the', 'ordering', 'of', 'the', 'planets', 'to', 'remain', 'c... | [-0.20133053470332093, 0.10184981516744618, -0.08241844179726246, 0.07941439328715205, -0.0715875255520982, -0.11799156479031334, 0.05688387211007268, 0.29946603864917287, -0.21858377871306045, -0.2912746520915433, 0.13564411592264863, -0.2538857591718071, -0.14324014509304264, 0.17412132986254342, -0.06281222755711971... |
706.3722 | Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at
High Q^2 and Determination of the Strong Coupling | Inclusive jet production is studied in neutral current deep-inelastic
positron-proton scattering at large four momentum transfer squared Q^2>150
GeV^2 with the H1 detector at HERA. Single and double differential inclusive
jet cross sections are measured as a function of Q^2 and of the transverse
energy E_T of the jet... | hep-ex | inclusive jet production is studied in neutral current deepinelastic positronproton scattering at large four momentum transfer squared q2150 gev2 with the h1 detector at hera single and double differential inclusive jet cross sections are measured as a function of q2 and of the transverse energy e_t of the jets in the ... | [['inclusive', 'jet', 'production', 'is', 'studied', 'in', 'neutral', 'current', 'deepinelastic', 'positronproton', 'scattering', 'at', 'large', 'four', 'momentum', 'transfer', 'squared', 'q2150', 'gev2', 'with', 'the', 'h1', 'detector', 'at', 'hera', 'single', 'and', 'double', 'differential', 'inclusive', 'jet', 'cros... | [-0.06255835107284162, 0.1470380803066041, -0.05534392682602629, 0.13148243537753684, 0.00335990439314361, -0.061938956712581934, -0.05372154945080433, 0.3657917306339795, -0.19648452147140827, -0.27876799878314, -0.04810291566189652, -0.37203923253974786, 0.10459756378699607, 0.16628048390389308, 0.12098924336322678, ... |
706.3723 | Order-Invariant MSO is Stronger than Counting MSO in the Finite | We compare the expressiveness of two extensions of monadic second-order logic
(MSO) over the class of finite structures. The first, counting monadic
second-order logic (CMSO), extends MSO with first-order modulo-counting
quantifiers, allowing the expression of queries like ``the number of elements
in the structure is... | cs.LO | we compare the expressiveness of two extensions of monadic secondorder logic mso over the class of finite structures the first counting monadic secondorder logic cmso extends mso with firstorder modulocounting quantifiers allowing the expression of queries like the number of elements in the structure is even the second... | [['we', 'compare', 'the', 'expressiveness', 'of', 'two', 'extensions', 'of', 'monadic', 'secondorder', 'logic', 'mso', 'over', 'the', 'class', 'of', 'finite', 'structures', 'the', 'first', 'counting', 'monadic', 'secondorder', 'logic', 'cmso', 'extends', 'mso', 'with', 'firstorder', 'modulocounting', 'quantifiers', 'al... | [-0.13538461173218247, 0.05217401975393219, -0.07728361090534906, 0.15321187347734322, -0.1640532911313992, -0.15887361421788992, 0.01769370382872263, 0.3558223938606189, -0.3182226156717853, -0.27074871456409855, 0.06739219811846085, -0.23672277466587394, -0.09078806656103361, 0.19740265885086142, -0.09804387535979531... |
706.3724 | Some Musings on Galaxy Morphology | Careful inspection of large-scale photographs of Shapley-Ames galaxies seems
to show a smooth transition between the morphological characteristics of
galaxies located on the narrow red, and on the broad blue, sequences in the
galaxian color-magnitude diagram. In other words there does not appear to be a
dichotomy bet... | astro-ph | careful inspection of largescale photographs of shapleyames galaxies seems to show a smooth transition between the morphological characteristics of galaxies located on the narrow red and on the broad blue sequences in the galaxian colormagnitude diagram in other words there does not appear to be a dichotomy between blu... | [['careful', 'inspection', 'of', 'largescale', 'photographs', 'of', 'shapleyames', 'galaxies', 'seems', 'to', 'show', 'a', 'smooth', 'transition', 'between', 'the', 'morphological', 'characteristics', 'of', 'galaxies', 'located', 'on', 'the', 'narrow', 'red', 'and', 'on', 'the', 'broad', 'blue', 'sequences', 'in', 'the... | [-0.05779801328622683, 0.10727563999095109, -0.11633401590344959, 0.11103707815988834, -0.10317527993614677, -0.04654177171069869, 0.04124786682443173, 0.4885306777432561, -0.10645452609047466, -0.3423497887344511, 0.005505781891474197, -0.2875151078356836, -0.09271822455826453, 0.17515375486305687, -0.0890710907934103... |
706.3725 | Weyl modules and opers without monodromy | We prove that the algebra of endomorphisms of a Weyl module of critical level
is isomorphic to the algebra of functions on the space of monodromy-free opers
on the disc with regular singularity and residue determined by the highest
weight of the Weyl module. This result may be used to test the local geometric
Langlan... | math.QA math.AG math.RT | we prove that the algebra of endomorphisms of a weyl module of critical level is isomorphic to the algebra of functions on the space of monodromyfree opers on the disc with regular singularity and residue determined by the highest weight of the weyl module this result may be used to test the local geometric langlands c... | [['we', 'prove', 'that', 'the', 'algebra', 'of', 'endomorphisms', 'of', 'a', 'weyl', 'module', 'of', 'critical', 'level', 'is', 'isomorphic', 'to', 'the', 'algebra', 'of', 'functions', 'on', 'the', 'space', 'of', 'monodromyfree', 'opers', 'on', 'the', 'disc', 'with', 'regular', 'singularity', 'and', 'residue', 'determi... | [-0.16541780630547193, 0.02182842678420486, -0.13498514100548722, 0.022213322978894858, -0.11060690723599927, -0.10992018646380354, -0.010141108322122524, 0.29144784189280004, -0.336223631428795, -0.20978741741348658, 0.08020600666584927, -0.20075963180692447, -0.1681431214956026, 0.18394254202083235, -0.12745495283255... |
706.3726 | Reversible stochastic pump currents in interacting nanoscale conductors | I argue that the geometric phase, responsible for reversible pump currents in
classical stochastic kinetics, can be observed experimentally with an
electronic setup, similar to the ones reported recently in [Phys. Rev. Lett.
96,076605 (2006)] and [Nature Physics 3, 243 - 247 (2007)].
| cond-mat.mes-hall cond-mat.stat-mech | i argue that the geometric phase responsible for reversible pump currents in classical stochastic kinetics can be observed experimentally with an electronic setup similar to the ones reported recently in phys rev lett 96076605 2006 and nature physics 3 243 247 2007 | [['i', 'argue', 'that', 'the', 'geometric', 'phase', 'responsible', 'for', 'reversible', 'pump', 'currents', 'in', 'classical', 'stochastic', 'kinetics', 'can', 'be', 'observed', 'experimentally', 'with', 'an', 'electronic', 'setup', 'similar', 'to', 'the', 'ones', 'reported', 'recently', 'in', 'phys', 'rev', 'lett', '... | [-0.05050302554694254, 0.17691433264216602, -0.04492229055158976, -0.0663902141471825, -0.04870831939141925, -0.13978643111157707, 0.0775210167133681, 0.3566728576154607, -0.1634511938687732, -0.3728713594013598, -0.06642507723952848, -0.21952199834830513, -0.23770338601273736, 0.22352171055518272, -0.13367798863115107... |
706.3727 | Bipairing and the Stripe Phase in 4-Leg Ladders | Density Matrix Renormalization Group (DMRG) calculations on 4-leg t-J and
Hubbard ladders have found a phase exhibiting "stripes" at intermediate doping.
Such behavior can be viewed as generalized Friedel oscillations, with
wavelength equal to the inverse hole density, induced by the open boundary
conditions. So far,... | cond-mat.supr-con cond-mat.str-el | density matrix renormalization group dmrg calculations on 4leg tj and hubbard ladders have found a phase exhibiting stripes at intermediate doping such behavior can be viewed as generalized friedel oscillations with wavelength equal to the inverse hole density induced by the open boundary conditions so far this phase h... | [['density', 'matrix', 'renormalization', 'group', 'dmrg', 'calculations', 'on', '4leg', 'tj', 'and', 'hubbard', 'ladders', 'have', 'found', 'a', 'phase', 'exhibiting', 'stripes', 'at', 'intermediate', 'doping', 'such', 'behavior', 'can', 'be', 'viewed', 'as', 'generalized', 'friedel', 'oscillations', 'with', 'waveleng... | [-0.15708462061630862, 0.22631602081744331, -0.07968123742349205, 0.11517467739195714, -0.022765126878455763, -0.20922396978243224, 0.05956604153278374, 0.3889210852824392, -0.2484130246925258, -0.25556264734496514, 0.07811327829446284, -0.31659170108576934, -0.12738384811447995, 0.12880114595144762, 0.069670369623289,... |
706.3728 | Superconductivity in hcp Sc under pressure - linear response results and
comparison with hcp Fe | This paper has been withdrawn due to some errors in the reported discussion,
and needs a thorough revision
| cond-mat.supr-con | this paper has been withdrawn due to some errors in the reported discussion and needs a thorough revision | [['this', 'paper', 'has', 'been', 'withdrawn', 'due', 'to', 'some', 'errors', 'in', 'the', 'reported', 'discussion', 'and', 'needs', 'a', 'thorough', 'revision']] | [-0.11407952196896076, -0.020469801034778357, -0.08719641767028305, 0.006913102354802605, -0.19375418695724672, -0.0699002492086341, 0.0986712752492167, 0.36670032640298206, -0.1801710766222742, -0.3624929469078779, 0.14966751223093727, -0.3135738737053341, -0.12407112111234003, 0.09956101100477907, -0.2964917900972068... |
706.3729 | Combinatorial and hybrid principles for sigma-directed families of
countable sets modulo finite | We consider strong combinatorial principles for sigma-directed families of
countable sets in the ordering by inclusion modulo finite, e.g. P-ideals of
countable sets. We try for principles as strong as possible while remaining
compatible with CH, and we also consider principles compatible with the
existence of nonspe... | math.LO | we consider strong combinatorial principles for sigmadirected families of countable sets in the ordering by inclusion modulo finite eg pideals of countable sets we try for principles as strong as possible while remaining compatible with ch and we also consider principles compatible with the existence of nonspecial aron... | [['we', 'consider', 'strong', 'combinatorial', 'principles', 'for', 'sigmadirected', 'families', 'of', 'countable', 'sets', 'in', 'the', 'ordering', 'by', 'inclusion', 'modulo', 'finite', 'eg', 'pideals', 'of', 'countable', 'sets', 'we', 'try', 'for', 'principles', 'as', 'strong', 'as', 'possible', 'while', 'remaining'... | [-0.11947842697428976, 0.12742500647005658, -0.04677797120961326, 0.11189782146485178, -0.14520167382319032, -0.12075180255658464, 0.09317844560194508, 0.36690372969081375, -0.3366242324312528, -0.2783321808034807, 0.11436317415396327, -0.26815430332481127, -0.11840302945024127, 0.1604572138361012, -0.11085230034961883... |
706.373 | Narrowing Constraints with Type Ia Supernovae: Converging on a
Cosmological Constant | We apply a parameterization-independent approach to fitting the dark energy
equation-of-state (EOS). Utilizing the latest type Ia supernova data, combined
with results from the cosmic microwave background and baryon acoustic
oscillations, we find that the dark energy is consistent with a cosmological
constant. We est... | astro-ph gr-qc hep-th | we apply a parameterizationindependent approach to fitting the dark energy equationofstate eos utilizing the latest type ia supernova data combined with results from the cosmic microwave background and baryon acoustic oscillations we find that the dark energy is consistent with a cosmological constant we establish inde... | [['we', 'apply', 'a', 'parameterizationindependent', 'approach', 'to', 'fitting', 'the', 'dark', 'energy', 'equationofstate', 'eos', 'utilizing', 'the', 'latest', 'type', 'ia', 'supernova', 'data', 'combined', 'with', 'results', 'from', 'the', 'cosmic', 'microwave', 'background', 'and', 'baryon', 'acoustic', 'oscillati... | [-0.0788547862876757, 0.13737564191476187, -0.10472207366785204, 0.11347930837285028, -0.10915222582724791, -0.12796067702636885, 0.04090636003847149, 0.3272541932322466, -0.18728291347030213, -0.39218865771598016, 0.054363188552881844, -0.29934348784895104, 0.02947636532904157, 0.1766629972706803, 0.027083396627197297... |
706.3731 | Calculation of the axial charge in the epsilon and epsilon' regimes of
HBChPT | The axial charge g_A is calculated in the epsilon regime of Heavy Baryon
Chiral Perturbation Theory to order epsilon^3. To perform this calculation, we
develop a technique to compute baryon properties in the epsilon regime of
Chiral Perturbation Theory. This technique includes contributions from pion
zero momentum mo... | hep-lat | the axial charge g_a is calculated in the epsilon regime of heavy baryon chiral perturbation theory to order epsilon3 to perform this calculation we develop a technique to compute baryon properties in the epsilon regime of chiral perturbation theory this technique includes contributions from pion zero momentum modes an... | [['the', 'axial', 'charge', 'g_a', 'is', 'calculated', 'in', 'the', 'epsilon', 'regime', 'of', 'heavy', 'baryon', 'chiral', 'perturbation', 'theory', 'to', 'order', 'epsilon3', 'to', 'perform', 'this', 'calculation', 'we', 'develop', 'a', 'technique', 'to', 'compute', 'baryon', 'properties', 'in', 'the', 'epsilon', 're... | [-0.15932654038698849, 0.17424106348438986, -0.08355667092837393, 0.05910172622902699, -0.030287619509106994, -0.0873602081745939, 0.11543569930268413, 0.3112391069987599, -0.21501705402090232, -0.25647863725257314, 0.025379568861075202, -0.2947193743394954, -0.0885171260143041, 0.10325173782754918, 0.04988376362895479... |
706.3732 | Toward faithful templates for non-spinning binary black holes using the
effective-one-body approach | We present an accurate approximation of the full gravitational radiation
waveforms generated in the merger of non-eccentric systems of two non-spinning
black holes. Utilizing information from recent numerical relativity simulations
and the natural flexibility of the effective-one-body (EOB) model, we extend
the latte... | gr-qc | we present an accurate approximation of the full gravitational radiation waveforms generated in the merger of noneccentric systems of two nonspinning black holes utilizing information from recent numerical relativity simulations and the natural flexibility of the effectiveonebody eob model we extend the latter so that ... | [['we', 'present', 'an', 'accurate', 'approximation', 'of', 'the', 'full', 'gravitational', 'radiation', 'waveforms', 'generated', 'in', 'the', 'merger', 'of', 'noneccentric', 'systems', 'of', 'two', 'nonspinning', 'black', 'holes', 'utilizing', 'information', 'from', 'recent', 'numerical', 'relativity', 'simulations',... | [-0.14071682961657644, 0.13674862376389105, -0.041031876993788914, 0.06846396765415028, -0.05100173763930797, -0.08892199550755323, -0.008211297324900939, 0.34195170121860097, -0.11762963156639175, -0.33430216301613574, 0.08696848048712127, -0.2901502187871797, -0.11874093241693283, 0.24988788989457217, 0.0009954430120... |
706.3733 | Interplay between lattice-scale physics and the quantum Hall effect in
graphene | Graphene's honeycomb lattice structure underlies much of the remarkable
physics inherent in this material, most strikingly through the formation of two
``flavors'' of Dirac cones for each spin. In the quantum Hall regime, the
resulting flavor degree of freedom leads to an interesting problem when a
Landau level is pa... | cond-mat.mes-hall | graphenes honeycomb lattice structure underlies much of the remarkable physics inherent in this material most strikingly through the formation of two flavors of dirac cones for each spin in the quantum hall regime the resulting flavor degree of freedom leads to an interesting problem when a landau level is partially oc... | [['graphenes', 'honeycomb', 'lattice', 'structure', 'underlies', 'much', 'of', 'the', 'remarkable', 'physics', 'inherent', 'in', 'this', 'material', 'most', 'strikingly', 'through', 'the', 'formation', 'of', 'two', 'flavors', 'of', 'dirac', 'cones', 'for', 'each', 'spin', 'in', 'the', 'quantum', 'hall', 'regime', 'the'... | [-0.17374831903725863, 0.277151888129239, -0.04193916804631174, 0.07907422047075151, -0.06227079413032958, -0.18380933906384078, 0.040169159895906754, 0.32500772045126985, -0.302058638762849, -0.25374001910510874, 0.007549701596976125, -0.29031305382959544, -0.1455585541070572, 0.14118845445336775, 0.007047351473011077... |
706.3734 | Higher Rank TQFT Representations of SL(2,Z) are Reducible | In this article we give examples which show that the TQFT representations of
the mapping class groups derived from quantum SU(N) for N>2 are generically
decomposable. One general decomposition of the representations is induced by
the symmetry which exchanges SU(N) representation labels by their conjugates.
The respec... | math.GT math.QA | in this article we give examples which show that the tqft representations of the mapping class groups derived from quantum sun for n2 are generically decomposable one general decomposition of the representations is induced by the symmetry which exchanges sun representation labels by their conjugates the respective summ... | [['in', 'this', 'article', 'we', 'give', 'examples', 'which', 'show', 'that', 'the', 'tqft', 'representations', 'of', 'the', 'mapping', 'class', 'groups', 'derived', 'from', 'quantum', 'sun', 'for', 'n2', 'are', 'generically', 'decomposable', 'one', 'general', 'decomposition', 'of', 'the', 'representations', 'is', 'ind... | [-0.1347409223492902, 0.13791572593422294, -0.07799305160929529, 0.0415486709898687, -0.08778103315629639, -0.11519460938870907, -0.02571296708013576, 0.341395740934576, -0.3345085632127638, -0.23159870765028664, 0.0945755503534411, -0.26432085211406675, -0.18757247681228015, 0.1456891422679361, -0.06638454852733187, -... |
706.3735 | Multi-bit information storage by multisite phosphorylation | Cells store information in DNA and in stable programs of gene expression,
which thereby implement forms of long-term cellular memory. Cells must also
possess short-term forms of information storage, implemented
post-translationally, to transduce and interpret external signals. CaMKII, for
instance, is thought to impl... | q-bio.MN | cells store information in dna and in stable programs of gene expression which thereby implement forms of longterm cellular memory cells must also possess shortterm forms of information storage implemented posttranslationally to transduce and interpret external signals camkii for instance is thought to implement a oneb... | [['cells', 'store', 'information', 'in', 'dna', 'and', 'in', 'stable', 'programs', 'of', 'gene', 'expression', 'which', 'thereby', 'implement', 'forms', 'of', 'longterm', 'cellular', 'memory', 'cells', 'must', 'also', 'possess', 'shortterm', 'forms', 'of', 'information', 'storage', 'implemented', 'posttranslationally',... | [-0.16109756742814743, 0.20105976965946262, 0.04200967389153521, 0.07508733527831776, -0.022386127590629773, -0.23344761992648588, 0.09602103025970087, 0.38311183337940474, -0.25861510040098534, -0.28074050398618844, 0.07122553127139505, -0.2805766416518448, -0.18748332115059793, 0.17839362812524587, -0.078254241922956... |
706.3736 | World-line Quantisation of a Reciprocally Invariant System | We present the world-line quantisation of a system invariant under the
symmetries of reciprocal relativity (pseudo-unitary transformations on ``phase
space coordinates" $(x^\mu(\tau),p^\mu(\tau))$ which preserve the Minkowski
metric and the symplectic form, and global shifts in these coordinates,
together with coordi... | hep-th math-ph math.MP | we present the worldline quantisation of a system invariant under the symmetries of reciprocal relativity pseudounitary transformations on phase space coordinates xmutaupmutau which preserve the minkowski metric and the symplectic form and global shifts in these coordinates together with coordinate dependent transforma... | [['we', 'present', 'the', 'worldline', 'quantisation', 'of', 'a', 'system', 'invariant', 'under', 'the', 'symmetries', 'of', 'reciprocal', 'relativity', 'pseudounitary', 'transformations', 'on', 'phase', 'space', 'coordinates', 'xmutaupmutau', 'which', 'preserve', 'the', 'minkowski', 'metric', 'and', 'the', 'symplectic... | [-0.1949616955676475, 0.1347487688855744, -0.0931348312418848, 0.01523026762277866, -0.10595153373283693, -0.09488230396072542, 0.012941737293770444, 0.3409039079009714, -0.2786425588214796, -0.24849438029419443, 0.11228101018506659, -0.2323308468135542, -0.0900780744434402, 0.13274951951380548, -0.03247746432137639, 0... |
706.3737 | Quantum Hall plateau transition in the lowest Landau level of disordered
graphene | We investigate, analytically and numerically, the effects of disorder on the
density of states and on the localization properties of the relativistic two
dimensional fermions in the lowest Landau level. Employing a supersymmetric
technique, we calculate the exact density of states for the Cauchy (Lorentzian)
distribu... | cond-mat.mes-hall cond-mat.str-el | we investigate analytically and numerically the effects of disorder on the density of states and on the localization properties of the relativistic two dimensional fermions in the lowest landau level employing a supersymmetric technique we calculate the exact density of states for the cauchy lorentzian distribution for... | [['we', 'investigate', 'analytically', 'and', 'numerically', 'the', 'effects', 'of', 'disorder', 'on', 'the', 'density', 'of', 'states', 'and', 'on', 'the', 'localization', 'properties', 'of', 'the', 'relativistic', 'two', 'dimensional', 'fermions', 'in', 'the', 'lowest', 'landau', 'level', 'employing', 'a', 'supersymm... | [-0.11865098666111451, 0.16745587208507848, -0.054645635490305725, 0.12672601114803303, 0.033877113838458345, -0.13208282604547483, 0.05282113520827677, 0.3357789548557429, -0.21305702550425415, -0.25280253377166534, 0.03736420729796269, -0.2849820452819889, -0.15572263713305196, 0.13161926734305562, 0.0312633617381964... |
706.3738 | Equivariant Littlewood-Richardson Skew Tableaux | We give a positive equivariant Littlewood-Richardson rule also discovered
independently by Molev. Our proof generalizes a proof by Stembridge of the
ordinary Littlewood-Richardson rule. We describe a weight-preserving bijection
between our indexing tableaux and the Knutson-Tao puzzles.
| math.AG math.CO | we give a positive equivariant littlewoodrichardson rule also discovered independently by molev our proof generalizes a proof by stembridge of the ordinary littlewoodrichardson rule we describe a weightpreserving bijection between our indexing tableaux and the knutsontao puzzles | [['we', 'give', 'a', 'positive', 'equivariant', 'littlewoodrichardson', 'rule', 'also', 'discovered', 'independently', 'by', 'molev', 'our', 'proof', 'generalizes', 'a', 'proof', 'by', 'stembridge', 'of', 'the', 'ordinary', 'littlewoodrichardson', 'rule', 'we', 'describe', 'a', 'weightpreserving', 'bijection', 'between... | [-0.10667352825151505, 0.05604311242397573, -0.1673242928510582, 0.11178243734143875, -0.2077717335038894, -0.2068547706774159, 0.18732139853936797, 0.2578510964616529, -0.3574980922622254, -0.26984169332285385, 0.03428830215204004, -0.2172014832093909, -0.21420654830699032, 0.13985827298381845, -0.1931310040070801, -0... |
706.3739 | Gorenstein cohomology in abelian categories | We investigate relative cohomology functors on subcategories of abelian
categories via Auslander-Buchweitz approximations and the resulting strict
resolutions. We verify that certain comparison maps between these functors are
isomorphisms and introduce a notion of perfection for this context. Our main
theorem is a ba... | math.KT math.AC | we investigate relative cohomology functors on subcategories of abelian categories via auslanderbuchweitz approximations and the resulting strict resolutions we verify that certain comparison maps between these functors are isomorphisms and introduce a notion of perfection for this context our main theorem is a balance... | [['we', 'investigate', 'relative', 'cohomology', 'functors', 'on', 'subcategories', 'of', 'abelian', 'categories', 'via', 'auslanderbuchweitz', 'approximations', 'and', 'the', 'resulting', 'strict', 'resolutions', 'we', 'verify', 'that', 'certain', 'comparison', 'maps', 'between', 'these', 'functors', 'are', 'isomorphi... | [-0.13745145939412665, -0.028908630161256086, -0.07932062420352805, 0.1427632127506811, -0.03825975450702378, -0.08896304842573209, 0.027934061424409757, 0.3577345798982949, -0.35872545704764663, -0.2607006029393829, 0.09882777346084352, -0.1902723577461343, -0.13268896399951371, 0.1810241599842051, -0.2312849218056338... |
706.374 | Randomized series and Geometry of Banach spaces | We study some properties of the randomized series and their applications to
the geometric structure of Banach spaces. For $n\ge 2$ and $1<p<\infty$, it is
shown that $\ell_\infty^n$ is representable in a Banach space $X$ if and only
if it is representable in the Lebesgue-Bochner $L_p(X)$. New criteria for
various con... | math.FA | we study some properties of the randomized series and their applications to the geometric structure of banach spaces for nge 2 and 1pinfty it is shown that ell_inftyn is representable in a banach space x if and only if it is representable in the lebesguebochner l_px new criteria for various convexity properties in bana... | [['we', 'study', 'some', 'properties', 'of', 'the', 'randomized', 'series', 'and', 'their', 'applications', 'to', 'the', 'geometric', 'structure', 'of', 'banach', 'spaces', 'for', 'nge', '2', 'and', '1pinfty', 'it', 'is', 'shown', 'that', 'ell_inftyn', 'is', 'representable', 'in', 'a', 'banach', 'space', 'x', 'if', 'an... | [-0.10225169017500622, 0.15662278341000327, -0.09237585977955472, 0.10946681146685144, -0.08604381145854102, -0.14677324145571283, -0.007647455019857919, 0.48472356671780936, -0.3899061086006684, -0.072049103506684, 0.16489117247822446, -0.2820476593016324, -0.14730641508640924, 0.20894118480495003, -0.1159349503825501... |
706.3741 | Observational Signatures of High-Energy Emission during the Shallow
Decay Phase of GRB X-Ray Afterglows | The widely existing shallow decay phase of the X-ray afterglows of gamma-ray
bursts (GRBs) is generally accepted to be due to long-lasting energy injection.
The outflows carrying the injecting energy, based on the component that is
dominative in energy, fall into two possible types: baryon-dominated and
lepton-domina... | astro-ph | the widely existing shallow decay phase of the xray afterglows of gammaray bursts grbs is generally accepted to be due to longlasting energy injection the outflows carrying the injecting energy based on the component that is dominative in energy fall into two possible types baryondominated and leptondominated ones the ... | [['the', 'widely', 'existing', 'shallow', 'decay', 'phase', 'of', 'the', 'xray', 'afterglows', 'of', 'gammaray', 'bursts', 'grbs', 'is', 'generally', 'accepted', 'to', 'be', 'due', 'to', 'longlasting', 'energy', 'injection', 'the', 'outflows', 'carrying', 'the', 'injecting', 'energy', 'based', 'on', 'the', 'component',... | [-0.057673884581308815, 0.21330086293729256, -0.08456739141047001, 0.18218810137314723, -0.08930556801892817, -0.10581080572493375, 0.019803313363343476, 0.4198063223361969, -0.2425862345714122, -0.2939523715823889, 0.03872495466563851, -0.2946747909137048, -0.0024295058995485305, 0.25712737647164613, 0.025693972317501... |
706.3742 | The Bloch-Okounkov correlation functions of negative levels | Bloch and Okounkov introduced an $n$-point correlation function on the
fermionic Fock space and found a closed formula in terms of theta functions.
This function affords several distinguished interpretations and in particular
can be formulated as correlation functions on irreducible
$\hat{gl}_\infty$-modules of level... | math.RT | bloch and okounkov introduced an npoint correlation function on the fermionic fock space and found a closed formula in terms of theta functions this function affords several distinguished interpretations and in particular can be formulated as correlation functions on irreducible hatgl_inftymodules of level one these co... | [['bloch', 'and', 'okounkov', 'introduced', 'an', 'npoint', 'correlation', 'function', 'on', 'the', 'fermionic', 'fock', 'space', 'and', 'found', 'a', 'closed', 'formula', 'in', 'terms', 'of', 'theta', 'functions', 'this', 'function', 'affords', 'several', 'distinguished', 'interpretations', 'and', 'in', 'particular', ... | [-0.11207105893321255, 0.08954760345260447, -0.0811391295815107, 0.13146413271615823, -0.013606991899269883, -0.08518580201592657, -0.008488650712865574, 0.342380051170626, -0.2841671894014042, -0.2311502524003166, 0.08497363592182557, -0.2579943663490716, -0.20232474498991523, 0.19381270803991826, -0.03296673537221967... |
706.3743 | Dynamical Response of Nanomechanical Resonators to Biomolecular
Interactions | We studied the dynamical response of a nanomechanical resonator to
biomolecular (e.g. DNA) adsorptions on a resonator's surface by using a
theoretical model, which considers the Hamiltonian H such that the potential
energy consists of elastic bending energy of a resonator and the potential
energy for biomolecular int... | cond-mat.soft q-bio.QM | we studied the dynamical response of a nanomechanical resonator to biomolecular eg dna adsorptions on a resonators surface by using a theoretical model which considers the hamiltonian h such that the potential energy consists of elastic bending energy of a resonator and the potential energy for biomolecular interaction... | [['we', 'studied', 'the', 'dynamical', 'response', 'of', 'a', 'nanomechanical', 'resonator', 'to', 'biomolecular', 'eg', 'dna', 'adsorptions', 'on', 'a', 'resonators', 'surface', 'by', 'using', 'a', 'theoretical', 'model', 'which', 'considers', 'the', 'hamiltonian', 'h', 'such', 'that', 'the', 'potential', 'energy', 'c... | [-0.15237953547249264, 0.17136370695273703, -0.04161174446441388, 0.014756351316464134, -0.03050910989339981, -0.1552256667063274, 0.06108448749485736, 0.38128650343666476, -0.23602595215197653, -0.28095747822792166, -0.03028593292563326, -0.269872268791207, -0.1760497010093079, 0.21908141081318414, 0.02999103730932499... |
706.3744 | The Imprint of Cosmic Reionization on Galaxy Clustering | We consider the effect of reionization on the clustering properties of galaxy
samples at intermediate redshifts (z~0.3-5.5). Current models for the
reionization of intergalactic hydrogen predict that overdense regions will be
reionized early, thus delaying the build up of stellar mass in the progenitors
of massive lo... | astro-ph | we consider the effect of reionization on the clustering properties of galaxy samples at intermediate redshifts z0355 current models for the reionization of intergalactic hydrogen predict that overdense regions will be reionized early thus delaying the build up of stellar mass in the progenitors of massive lowerredshif... | [['we', 'consider', 'the', 'effect', 'of', 'reionization', 'on', 'the', 'clustering', 'properties', 'of', 'galaxy', 'samples', 'at', 'intermediate', 'redshifts', 'z0355', 'current', 'models', 'for', 'the', 'reionization', 'of', 'intergalactic', 'hydrogen', 'predict', 'that', 'overdense', 'regions', 'will', 'be', 'reion... | [-0.042135162266442254, 0.14297835973124937, -0.0801755626435448, 0.1560196950350735, -0.09658218066165732, -0.018399384393970566, 0.02478087905513927, 0.41690932794925617, -0.10725891779205113, -0.36854180958383065, 0.0187261793996158, -0.28899482300392154, 0.0023041001528106403, 0.19613323187413148, 0.001689325139688... |
706.3745 | Gale duality for complete intersections | We show that every complete intersection of Laurent polynomials in an
algebraic torus is isomorphic to a complete intersection of master functions in
the complement of a hyperplane arrangement, and vice versa. We call this
association Gale duality because the exponents of the monomials in the
polynomials annihilate t... | math.AG math.AC | we show that every complete intersection of laurent polynomials in an algebraic torus is isomorphic to a complete intersection of master functions in the complement of a hyperplane arrangement and vice versa we call this association gale duality because the exponents of the monomials in the polynomials annihilate the w... | [['we', 'show', 'that', 'every', 'complete', 'intersection', 'of', 'laurent', 'polynomials', 'in', 'an', 'algebraic', 'torus', 'is', 'isomorphic', 'to', 'a', 'complete', 'intersection', 'of', 'master', 'functions', 'in', 'the', 'complement', 'of', 'a', 'hyperplane', 'arrangement', 'and', 'vice', 'versa', 'we', 'call', ... | [-0.2089789160960462, 0.031925364729283694, -0.15223474144870633, 0.09666241853847168, -0.1068384105686185, -0.11539499435660451, 0.08363444138274984, 0.2682798860424068, -0.3294628453982431, -0.1548005327863922, 0.07633087101939329, -0.2622265686595076, -0.1946456666905866, 0.16119238461346128, -0.13665926494354078, -... |
706.3746 | Nonrelativistic conformal field theories | We study representations of the Schr\"odinger algebra in terms of operators
in nonrelativistic conformal field theories. We prove a correspondence between
primary operators and eigenstates of few-body systems in a harmonic potential.
Using the correspondence we compute analytically the energy of fermions at
unitarity... | hep-th cond-mat.other hep-ph | we study representations of the schrodinger algebra in terms of operators in nonrelativistic conformal field theories we prove a correspondence between primary operators and eigenstates of fewbody systems in a harmonic potential using the correspondence we compute analytically the energy of fermions at unitarity in a h... | [['we', 'study', 'representations', 'of', 'the', 'schrodinger', 'algebra', 'in', 'terms', 'of', 'operators', 'in', 'nonrelativistic', 'conformal', 'field', 'theories', 'we', 'prove', 'a', 'correspondence', 'between', 'primary', 'operators', 'and', 'eigenstates', 'of', 'fewbody', 'systems', 'in', 'a', 'harmonic', 'poten... | [-0.16472333697208635, 0.16513547007466706, -0.07119635065597757, 0.0900473114706471, 0.033048207091141334, -0.12442823850982626, 0.016590297930467297, 0.3279373529301563, -0.20552862383110423, -0.2032575897947667, 0.018220300928846946, -0.3232080326530374, -0.16099818582764605, 0.14723033133999142, 0.02619364527119717... |
706.3747 | Superconductors described with CSM.(a new paper, 2008-10-16) | The properties of the known superconductors can be explained with the
correlations dominated superconducting mechanism (CSM). The correlations have
the spin correlation, the charge correlation and the spin-charge correlation,
and their strengths can be described by the related correlation lengths in
their correlation... | physics.gen-ph | the properties of the known superconductors can be explained with the correlations dominated superconducting mechanism csm the correlations have the spin correlation the charge correlation and the spincharge correlation and their strengths can be described by the related correlation lengths in their correlation functio... | [['the', 'properties', 'of', 'the', 'known', 'superconductors', 'can', 'be', 'explained', 'with', 'the', 'correlations', 'dominated', 'superconducting', 'mechanism', 'csm', 'the', 'correlations', 'have', 'the', 'spin', 'correlation', 'the', 'charge', 'correlation', 'and', 'the', 'spincharge', 'correlation', 'and', 'the... | [-0.1602350632903956, 0.1813313871670638, -0.10881275140296368, 0.1269114870226046, -0.043848390050973934, -0.11595453983349328, 0.058964803285225874, 0.37974205916809245, -0.24133292938719428, -0.28881038270308085, 0.009213538999863463, -0.30891672375069057, -0.1686196092006384, 0.1619620910954388, 0.05593443818178505... |
706.3748 | On Monge-Ampere equations with homogeneous right hand side | We study the regularity and behavior at the origin of solutions to the
two-dimensional degenerate Monge-Ampere equation with homogeneous right hand
side of degree alpha, alpha>-2. We show that when alpha > 0, solutions admit
only two possible behaviors near the origin, radial and non-radial. We also
show that the rad... | math.AP | we study the regularity and behavior at the origin of solutions to the twodimensional degenerate mongeampere equation with homogeneous right hand side of degree alpha alpha2 we show that when alpha 0 solutions admit only two possible behaviors near the origin radial and nonradial we also show that the radial behavior i... | [['we', 'study', 'the', 'regularity', 'and', 'behavior', 'at', 'the', 'origin', 'of', 'solutions', 'to', 'the', 'twodimensional', 'degenerate', 'mongeampere', 'equation', 'with', 'homogeneous', 'right', 'hand', 'side', 'of', 'degree', 'alpha', 'alpha2', 'we', 'show', 'that', 'when', 'alpha', '0', 'solutions', 'admit', ... | [-0.17331233364877416, 0.08882364810013504, -0.08812427374103399, 0.06444757504896052, -0.11642210422876055, -0.19452178717326762, -0.014455005512642326, 0.3579074848832479, -0.2813753292047933, -0.15635037021850473, 0.12532923773709517, -0.34991346724998595, -0.16543394507868076, 0.1696185295803667, 0.0316518266727008... |
706.3749 | Quantum Operation Time Reversal | The dynamics of an open quantum system can be described by a quantum
operation, a linear, complete positive map of operators. Here, I exhibit a
compact expression for the time reversal of a quantum operation, which is
closely analogous to the time reversal of a classical Markov transition matrix.
Since open quantum d... | quant-ph cond-mat.stat-mech | the dynamics of an open quantum system can be described by a quantum operation a linear complete positive map of operators here i exhibit a compact expression for the time reversal of a quantum operation which is closely analogous to the time reversal of a classical markov transition matrix since open quantum dynamics ... | [['the', 'dynamics', 'of', 'an', 'open', 'quantum', 'system', 'can', 'be', 'described', 'by', 'a', 'quantum', 'operation', 'a', 'linear', 'complete', 'positive', 'map', 'of', 'operators', 'here', 'i', 'exhibit', 'a', 'compact', 'expression', 'for', 'the', 'time', 'reversal', 'of', 'a', 'quantum', 'operation', 'which', ... | [-0.15847754735221095, 0.2005992908594873, -0.10325429393683025, 0.04775198821139426, -0.02491882262603493, -0.16370781799169065, 0.04848020579274222, 0.35071442141763376, -0.33722274875807984, -0.2200397431554499, 0.13591858606010884, -0.21519161760807037, -0.12718577353527474, 0.20575142124337015, -0.0278384789305002... |
706.375 | Pruning Processes and a New Characterization of Convex Geometries | We provide a new characterization of convex geometries via a multivariate
version of an identity that was originally proved by Maneva, Mossel and
Wainwright for certain combinatorial objects arising in the context of the
k-SAT problem. We thus highlight the connection between various
characterizations of convex geome... | math.CO cs.DM math.PR | we provide a new characterization of convex geometries via a multivariate version of an identity that was originally proved by maneva mossel and wainwright for certain combinatorial objects arising in the context of the ksat problem we thus highlight the connection between various characterizations of convex geometries... | [['we', 'provide', 'a', 'new', 'characterization', 'of', 'convex', 'geometries', 'via', 'a', 'multivariate', 'version', 'of', 'an', 'identity', 'that', 'was', 'originally', 'proved', 'by', 'maneva', 'mossel', 'and', 'wainwright', 'for', 'certain', 'combinatorial', 'objects', 'arising', 'in', 'the', 'context', 'of', 'th... | [-0.0991236952599138, 0.037385925427709785, -0.07783497381024063, 0.09195961127212891, -0.06313119384770592, -0.09867388131873062, 0.047301279458527766, 0.34261501729488375, -0.29060626834010084, -0.2771137789512674, 0.13441693516991413, -0.22755391085520388, -0.2183070029442509, 0.22719836101556817, -0.144399681485568... |
706.3751 | The AdS/CFT Correspondence: Classical, Quantum, and Thermodynamical
Aspects | Certain aspects of the AdS/CFT correspondence are studied in detail. We
investigate the one-loop mass shift to certain two-impurity string states in
light-cone string field theory on a plane wave background. We find that there
exist logarithmic divergences in the sums over intermediate mode numbers which
cancel betwe... | hep-th | certain aspects of the adscft correspondence are studied in detail we investigate the oneloop mass shift to certain twoimpurity string states in lightcone string field theory on a plane wave background we find that there exist logarithmic divergences in the sums over intermediate mode numbers which cancel between the c... | [['certain', 'aspects', 'of', 'the', 'adscft', 'correspondence', 'are', 'studied', 'in', 'detail', 'we', 'investigate', 'the', 'oneloop', 'mass', 'shift', 'to', 'certain', 'twoimpurity', 'string', 'states', 'in', 'lightcone', 'string', 'field', 'theory', 'on', 'a', 'plane', 'wave', 'background', 'we', 'find', 'that', '... | [-0.1517911458870263, 0.1989746623643961, -0.05599180429812155, 0.11308237756560889, -0.020510093467808993, -0.11034155028340008, 0.03755646137007196, 0.3466762316945408, -0.19613896398139852, -0.2736226513965188, 0.05710158168970208, -0.3216586201451719, -0.1473427570208774, 0.11458825048092487, 0.01026601187435777, 0... |
706.3752 | Secure Nested Codes for Type II Wiretap Channels | This paper considers the problem of secure coding design for a type II
wiretap channel, where the main channel is noiseless and the eavesdropper
channel is a general binary-input symmetric-output memoryless channel. The
proposed secure error-correcting code has a nested code structure. Two secure
nested coding scheme... | cs.IT cs.CR math.IT | this paper considers the problem of secure coding design for a type ii wiretap channel where the main channel is noiseless and the eavesdropper channel is a general binaryinput symmetricoutput memoryless channel the proposed secure errorcorrecting code has a nested code structure two secure nested coding schemes are st... | [['this', 'paper', 'considers', 'the', 'problem', 'of', 'secure', 'coding', 'design', 'for', 'a', 'type', 'ii', 'wiretap', 'channel', 'where', 'the', 'main', 'channel', 'is', 'noiseless', 'and', 'the', 'eavesdropper', 'channel', 'is', 'a', 'general', 'binaryinput', 'symmetricoutput', 'memoryless', 'channel', 'the', 'pr... | [-0.2578062230344016, -0.025164426410012947, -0.02548449159674118, 0.06286359982539334, -0.008398963925514393, -0.32556519326839617, 0.14235614294091958, 0.3631413118582379, -0.2775332965356715, -0.1910259063738438, 0.11598336899315972, -0.17925236664392466, -0.1042794322786407, 0.18089502390496937, -0.1507259568265936... |
706.3753 | Multiple Access Channels with Generalized Feedback and Confidential
Messages | This paper considers the problem of secret communication over a multiple
access channel with generalized feedback. Two trusted users send independent
confidential messages to an intended receiver, in the presence of a passive
eavesdropper. In this setting, an active cooperation between two trusted users
is enabled th... | cs.IT math.IT | this paper considers the problem of secret communication over a multiple access channel with generalized feedback two trusted users send independent confidential messages to an intended receiver in the presence of a passive eavesdropper in this setting an active cooperation between two trusted users is enabled through ... | [['this', 'paper', 'considers', 'the', 'problem', 'of', 'secret', 'communication', 'over', 'a', 'multiple', 'access', 'channel', 'with', 'generalized', 'feedback', 'two', 'trusted', 'users', 'send', 'independent', 'confidential', 'messages', 'to', 'an', 'intended', 'receiver', 'in', 'the', 'presence', 'of', 'a', 'passi... | [-0.3077637311937504, -0.01074751308099854, -0.008980624843388796, 0.0020546752534438533, -0.07697945441725816, -0.354797073239244, 0.2118625500263798, 0.39405625590751336, -0.2931676998864426, -0.2296128980598824, 0.064429450099259, -0.2494917576266236, -0.10015341343877968, 0.14762312233404712, -0.16260534769660512, ... |
706.3754 | Binary Stars as the Source of the Far-UV Excess in Elliptical Galaxies | The discovery of an excess of light in the far-ultraviolet (UV) spectrum in
elliptical galaxies was a major surprise in 1969. While it is now clear that
this UV excess is caused by an old population of hot helium-burning stars
without large hydrogen-rich envelopes rather than young stars, their origin has
remained a ... | astro-ph | the discovery of an excess of light in the farultraviolet uv spectrum in elliptical galaxies was a major surprise in 1969 while it is now clear that this uv excess is caused by an old population of hot heliumburning stars without large hydrogenrich envelopes rather than young stars their origin has remained a mystery h... | [['the', 'discovery', 'of', 'an', 'excess', 'of', 'light', 'in', 'the', 'farultraviolet', 'uv', 'spectrum', 'in', 'elliptical', 'galaxies', 'was', 'a', 'major', 'surprise', 'in', '1969', 'while', 'it', 'is', 'now', 'clear', 'that', 'this', 'uv', 'excess', 'is', 'caused', 'by', 'an', 'old', 'population', 'of', 'hot', 'h... | [-0.029350888016029395, 0.15172172696636244, -0.1126820886572503, 0.1250406639581148, -0.12565952746325548, -0.04533591886399357, 0.06563360435276769, 0.4377249906706901, -0.15541966565780677, -0.333589208106162, 0.06487119584059954, -0.2863915286192187, -0.09895865302817285, 0.17659250752047728, -0.13826516260506713, ... |
706.3755 | Two-Pulse Propagation in Media with Quantum-Mixed Ground States | We examine fully coherent two-pulse propagation in a lambda-type medium,
under two-photon resonance conditions and including inhomogeneous broadening.
We examine both the effects of short pulse preparation and the effects of
medium preparation. We contrast cases in which the two pulses have matched
envelopes or not, ... | quant-ph nlin.PS | we examine fully coherent twopulse propagation in a lambdatype medium under twophoton resonance conditions and including inhomogeneous broadening we examine both the effects of short pulse preparation and the effects of medium preparation we contrast cases in which the two pulses have matched envelopes or not and contr... | [['we', 'examine', 'fully', 'coherent', 'twopulse', 'propagation', 'in', 'a', 'lambdatype', 'medium', 'under', 'twophoton', 'resonance', 'conditions', 'and', 'including', 'inhomogeneous', 'broadening', 'we', 'examine', 'both', 'the', 'effects', 'of', 'short', 'pulse', 'preparation', 'and', 'the', 'effects', 'of', 'medi... | [-0.11401020375206687, 0.15089896226659916, -0.06822168849156064, 0.07163756757337958, -0.01993034342136155, -0.1186540078271133, 0.022863236200695827, 0.44679768802335035, -0.23216561581623757, -0.2564299131143775, 0.06933686226714234, -0.24200073330760816, -0.127230289542132, 0.21596900998229307, -0.02630553891787589... |
706.3756 | Choice of Measurement Sets in Qubit Tomography | Optimal generalized measurements for state estimation are well understood.
However, practical quantum state tomography is typically performed using a
fixed set of projective measurements and the question of how to choose these
measurements has been largely unexplored in the literature. In this work we
develop theoret... | quant-ph | optimal generalized measurements for state estimation are well understood however practical quantum state tomography is typically performed using a fixed set of projective measurements and the question of how to choose these measurements has been largely unexplored in the literature in this work we develop theoretical ... | [['optimal', 'generalized', 'measurements', 'for', 'state', 'estimation', 'are', 'well', 'understood', 'however', 'practical', 'quantum', 'state', 'tomography', 'is', 'typically', 'performed', 'using', 'a', 'fixed', 'set', 'of', 'projective', 'measurements', 'and', 'the', 'question', 'of', 'how', 'to', 'choose', 'these... | [-0.04926826026161561, 0.11293312927505167, -0.08276072219429113, 0.01798686609916979, -0.025197146988317074, -0.13860618692389368, 0.08169975365157064, 0.4018003466253233, -0.2449762781685458, -0.30983940568190105, 0.13650460470015977, -0.28660593045377497, -0.08260594228153477, 0.20218014401224635, -0.082191404821996... |
706.3757 | Instability of holographic dark energy models | We investigate the difference between holographic dark energy, Chaplygin gas,
and tachyon model with constant potential. For this purpose, we examine their
squared speeds of sound which are evaluated to zeroth order in perturbation
theory and hence depends only on time. We find that the squared speed for
holographic ... | gr-qc astro-ph hep-th | we investigate the difference between holographic dark energy chaplygin gas and tachyon model with constant potential for this purpose we examine their squared speeds of sound which are evaluated to zeroth order in perturbation theory and hence depends only on time we find that the squared speed for holographic dark en... | [['we', 'investigate', 'the', 'difference', 'between', 'holographic', 'dark', 'energy', 'chaplygin', 'gas', 'and', 'tachyon', 'model', 'with', 'constant', 'potential', 'for', 'this', 'purpose', 'we', 'examine', 'their', 'squared', 'speeds', 'of', 'sound', 'which', 'are', 'evaluated', 'to', 'zeroth', 'order', 'in', 'per... | [-0.13227644999428728, 0.17207451668788784, -0.12192918333829832, 0.1447089994866305, -0.11292174610203688, -0.1901709321771086, -0.05207354929322166, 0.3377219465820445, -0.21153671584408923, -0.29070347694910526, 0.05078652876875719, -0.26815489973373635, -0.044480011282373486, 0.12643485983651245, -0.013764748877855... |
706.3758 | Diffusion of Macromolecules across the Nuclear Pore Complex | Nuclear pore complexes (NPCs) are very selective filters that monitor the
transport between the cytoplasm and the nucleoplasm. Two models have been
suggested for the plug of the NPC. They are (i) it is a reversible hydrogel or
(ii) it is a polymer brush. We propose a mesoscopic model for the transport of
a protein th... | cond-mat.soft cond-mat.stat-mech physics.bio-ph q-bio.CB | nuclear pore complexes npcs are very selective filters that monitor the transport between the cytoplasm and the nucleoplasm two models have been suggested for the plug of the npc they are i it is a reversible hydrogel or ii it is a polymer brush we propose a mesoscopic model for the transport of a protein through the p... | [['nuclear', 'pore', 'complexes', 'npcs', 'are', 'very', 'selective', 'filters', 'that', 'monitor', 'the', 'transport', 'between', 'the', 'cytoplasm', 'and', 'the', 'nucleoplasm', 'two', 'models', 'have', 'been', 'suggested', 'for', 'the', 'plug', 'of', 'the', 'npc', 'they', 'are', 'i', 'it', 'is', 'a', 'reversible', '... | [-0.0827556611620821, 0.17068529153831735, -0.12123186807773674, 0.04770098910614876, -0.044834691906042064, -0.16601463951128745, 0.0022450121529678357, 0.4142617930922268, -0.284801286617433, -0.21125187355079758, 0.09246650021158354, -0.24501202832351424, -0.16203069394635064, 0.168102201722465, -0.02697316514077916... |
706.3759 | Sharp linear and bilinear restriction estimates for paraboloids in the
cylindrically symmetric case | For cylindrically symmetric functions dyadically supported on the paraboloid,
we obtain a family of sharp linear and bilinear adjoint restriction estimates.
As corollaries, we first extend the ranges of exponents for the classical
\textit{linear or bilinear adjoint restriction conjectures} for such functions
and veri... | math.CA math.AP | for cylindrically symmetric functions dyadically supported on the paraboloid we obtain a family of sharp linear and bilinear adjoint restriction estimates as corollaries we first extend the ranges of exponents for the classical textitlinear or bilinear adjoint restriction conjectures for such functions and verify the t... | [['for', 'cylindrically', 'symmetric', 'functions', 'dyadically', 'supported', 'on', 'the', 'paraboloid', 'we', 'obtain', 'a', 'family', 'of', 'sharp', 'linear', 'and', 'bilinear', 'adjoint', 'restriction', 'estimates', 'as', 'corollaries', 'we', 'first', 'extend', 'the', 'ranges', 'of', 'exponents', 'for', 'the', 'cla... | [-0.09362066709660892, 0.041572678469525406, -0.06271763320967376, 0.10268028294078511, -0.13233320707881666, -0.11266605875241649, 0.006266524501885456, 0.28284731509124705, -0.2716458205986454, -0.19340156559153537, 0.16566138921574836, -0.2611876606284809, -0.1134963475801724, 0.24337008770229857, -0.066217607947582... |
706.376 | Correlation between transport properties and lattice effects in the
NdCoO3 based catalysts and sensor materials | This study presents correlations between the structural and transport
properties of pure and doped neodymium cobaltate, a compound of great interest
for its foreseen applications as catalyst, sensor and thermoelectric material.
Neutron and x-ray powder diffraction data have been combined to carefully
determine lattic... | cond-mat.mtrl-sci | this study presents correlations between the structural and transport properties of pure and doped neodymium cobaltate a compound of great interest for its foreseen applications as catalyst sensor and thermoelectric material neutron and xray powder diffraction data have been combined to carefully determine lattice cons... | [['this', 'study', 'presents', 'correlations', 'between', 'the', 'structural', 'and', 'transport', 'properties', 'of', 'pure', 'and', 'doped', 'neodymium', 'cobaltate', 'a', 'compound', 'of', 'great', 'interest', 'for', 'its', 'foreseen', 'applications', 'as', 'catalyst', 'sensor', 'and', 'thermoelectric', 'material', ... | [-0.10216523362656257, 0.1606121284378149, -0.029374493421951992, -0.004118896197955709, -0.027214668715742896, -0.10274033783501164, 0.10846943332472388, 0.4115011758454468, -0.2731329509120735, -0.28360848709462233, 0.06124919387569755, -0.33994020872766745, -0.06991175365466509, 0.17856544418757933, 0.03698492645262... |
706.3761 | Uppers to zero and semistar operations in polynomial rings | Given a stable semistar operation of finite type $\star$ on an integral
domain $D$, we show that it is possible to define in a canonical way a stable
semistar operation of finite type $[\star]$ on the polynomial ring $D[X]$, such
that $D$ is a $\star$-quasi-Pr\"ufer domain if and only if each upper to zero
in $D[X]$ ... | math.AC math.AG | given a stable semistar operation of finite type star on an integral domain d we show that it is possible to define in a canonical way a stable semistar operation of finite type star on the polynomial ring dx such that d is a starquasiprufer domain if and only if each upper to zero in dx is a quasistarmaximal ideal thi... | [['given', 'a', 'stable', 'semistar', 'operation', 'of', 'finite', 'type', 'star', 'on', 'an', 'integral', 'domain', 'd', 'we', 'show', 'that', 'it', 'is', 'possible', 'to', 'define', 'in', 'a', 'canonical', 'way', 'a', 'stable', 'semistar', 'operation', 'of', 'finite', 'type', 'star', 'on', 'the', 'polynomial', 'ring'... | [-0.18667428285947868, 0.07669916053782799, -0.08942199363040605, 0.020436390173355384, -0.08513646761088499, -0.1356512631555753, 0.04111999305896461, 0.3462637710983732, -0.3346084740079407, -0.1296415747575728, 0.13500630096532404, -0.21963333619226302, -0.11111360138747842, 0.20586904288419255, -0.11537685447505543... |
706.3762 | Dynamics and neutrino signal of black hole formation in non-rotating
failed supernovae. I. EOS dependence | We study the black hole formation and the neutrino signal from the
gravitational collapse of a non-rotating massive star of 40 Msun. Adopting two
different sets of realistic equation of state (EOS) of dense matter, we perform
the numerical simulations of general relativistic neutrino-radiation
hydrodynamics under the... | astro-ph hep-ph nucl-th | we study the black hole formation and the neutrino signal from the gravitational collapse of a nonrotating massive star of 40 msun adopting two different sets of realistic equation of state eos of dense matter we perform the numerical simulations of general relativistic neutrinoradiation hydrodynamics under the spheric... | [['we', 'study', 'the', 'black', 'hole', 'formation', 'and', 'the', 'neutrino', 'signal', 'from', 'the', 'gravitational', 'collapse', 'of', 'a', 'nonrotating', 'massive', 'star', 'of', '40', 'msun', 'adopting', 'two', 'different', 'sets', 'of', 'realistic', 'equation', 'of', 'state', 'eos', 'of', 'dense', 'matter', 'we... | [-0.098578813851811, 0.1935986549607478, -0.07303513107262552, 0.12373859859397635, -0.08944920916110277, -0.060836999085266144, 0.03922542511904612, 0.32313694326579573, -0.17980158075131475, -0.33418099221587183, 0.06930073501868174, -0.2801464807279408, 0.013303832110017538, 0.18696796375513078, 0.03715241015024367,... |
706.3763 | Suppression of Heating Rates in Cryogenic Surface-Electrode Ion Traps | Dense arrays of trapped ions provide one way of scaling up ion trap quantum
information processing. However, miniaturization of ion traps is currently
limited by sharply increasing motional state decoherence at sub-100 um
ion-electrode distances. We characterize heating rates in cryogenically cooled
surface-electrode... | quant-ph | dense arrays of trapped ions provide one way of scaling up ion trap quantum information processing however miniaturization of ion traps is currently limited by sharply increasing motional state decoherence at sub100 um ionelectrode distances we characterize heating rates in cryogenically cooled surfaceelectrode traps w... | [['dense', 'arrays', 'of', 'trapped', 'ions', 'provide', 'one', 'way', 'of', 'scaling', 'up', 'ion', 'trap', 'quantum', 'information', 'processing', 'however', 'miniaturization', 'of', 'ion', 'traps', 'is', 'currently', 'limited', 'by', 'sharply', 'increasing', 'motional', 'state', 'decoherence', 'at', 'sub100', 'um', ... | [-0.09186843981627714, 0.2994505606069596, 0.0698699385299338, -0.040087414633113314, 0.061098571283498194, -0.18860291243728364, 0.05386097961801546, 0.43771945489476427, -0.22909081172235687, -0.36268500936678566, 0.068538482303289, -0.3234978081432707, 0.08343657446705331, 0.25648219659548216, 0.0018671694496232602,... |
706.3764 | Scanning tunneling spectroscopy of inhomogeneous electronic structure in
monolayer and bilayer graphene on SiC | We present a scanning tunneling spectroscopy (STS) study of the local
electronic structure of single and bilayer graphene grown epitaxially on a
SiC(0001) surface. Low voltage topographic images reveal fine, atomic-scale
carbon networks, whereas higher bias images are dominated by emergent spatially
inhomogeneous lar... | cond-mat.str-el | we present a scanning tunneling spectroscopy sts study of the local electronic structure of single and bilayer graphene grown epitaxially on a sic0001 surface low voltage topographic images reveal fine atomicscale carbon networks whereas higher bias images are dominated by emergent spatially inhomogeneous largescale st... | [['we', 'present', 'a', 'scanning', 'tunneling', 'spectroscopy', 'sts', 'study', 'of', 'the', 'local', 'electronic', 'structure', 'of', 'single', 'and', 'bilayer', 'graphene', 'grown', 'epitaxially', 'on', 'a', 'sic0001', 'surface', 'low', 'voltage', 'topographic', 'images', 'reveal', 'fine', 'atomicscale', 'carbon', '... | [-0.1707677847282453, 0.1067252008381977, -0.06368861291980879, 0.040555302245246075, -0.02030659105036069, -0.20070219936526634, 0.053134838248264385, 0.48266755982556125, -0.3046452951871536, -0.3667044962333007, -0.025068599972027268, -0.3221024653212887, -0.18001382144549014, 0.15236138659529389, 0.0469578575829721... |
706.3765 | A surprising method for polarising antiprotons | We propose a method for polarising antiprotons in a storage ring by means of
a polarised positron beam moving parallel to the antiprotons. If the relative
velocity is adjusted to $v/c \approx 0.002$ the cross section for spin-flip is
as large as about $2 \cdot 10^{13}$ barn as shown by new QED-calculations of
the tri... | physics.acc-ph | we propose a method for polarising antiprotons in a storage ring by means of a polarised positron beam moving parallel to the antiprotons if the relative velocity is adjusted to vc approx 0002 the cross section for spinflip is as large as about 2 cdot 1013 barn as shown by new qedcalculations of the triple spincross se... | [['we', 'propose', 'a', 'method', 'for', 'polarising', 'antiprotons', 'in', 'a', 'storage', 'ring', 'by', 'means', 'of', 'a', 'polarised', 'positron', 'beam', 'moving', 'parallel', 'to', 'the', 'antiprotons', 'if', 'the', 'relative', 'velocity', 'is', 'adjusted', 'to', 'vc', 'approx', '0002', 'the', 'cross', 'section',... | [-0.09309057898353786, 0.19992974494659418, -0.041343797048604164, 0.07004644534915586, 0.019505111806918992, -0.13615461394341813, 0.026409245798886576, 0.39880668725314977, -0.23337272852659224, -0.36355128940572407, 0.01977237914563031, -0.3091170802309706, 0.09361583170657223, 0.253454038649294, 0.02506811756741356... |
706.3766 | Photoproduction of Hadron Pairs at Fixed-Target Experiments | We consider the photoproduction of two hadrons in polarized lepton-nucleon
collisions in the framework of perturbative QCD at the next-to-leading order
accuracy. After illustrating how to obtain the experimentally relevant
observables, a phenomenological study of the photoproduction of hadron pairs at
high transverse... | hep-ph | we consider the photoproduction of two hadrons in polarized leptonnucleon collisions in the framework of perturbative qcd at the nexttoleading order accuracy after illustrating how to obtain the experimentally relevant observables a phenomenological study of the photoproduction of hadron pairs at high transverse moment... | [['we', 'consider', 'the', 'photoproduction', 'of', 'two', 'hadrons', 'in', 'polarized', 'leptonnucleon', 'collisions', 'in', 'the', 'framework', 'of', 'perturbative', 'qcd', 'at', 'the', 'nexttoleading', 'order', 'accuracy', 'after', 'illustrating', 'how', 'to', 'obtain', 'the', 'experimentally', 'relevant', 'observab... | [-0.04225985240370322, 0.16648471521643493, -0.13608307731696045, 0.17028342322983708, 0.0011807427920687656, -0.027681224012317564, -0.029125249701050612, 0.3867152382261478, -0.16454650355646244, -0.2193912712713847, -0.08919523052083185, -0.3723653852366484, 0.05747816629277972, 0.16247045532442056, 0.11982619586185... |
706.3767 | Evolutionary stage of the spectral variable BD+48 1220=IRAS 05040+4820 | Based on high-resolution observations (R=60000 and 75000), we have studied
the optical spectral variability of the star BD+48 1220 (IRAS05040+4820). We
have measured the equivalent widths of numerous absorption lines of neutral
atoms and ions at wavelengths from 4500 to 6760 AA, as well as the
corresponding radial ve... | astro-ph | based on highresolution observations r60000 and 75000 we have studied the optical spectral variability of the star bd48 1220 iras050404820 we have measured the equivalent widths of numerous absorption lines of neutral atoms and ions at wavelengths from 4500 to 6760 aa as well as the corresponding radial velocities we u... | [['based', 'on', 'highresolution', 'observations', 'r60000', 'and', '75000', 'we', 'have', 'studied', 'the', 'optical', 'spectral', 'variability', 'of', 'the', 'star', 'bd48', '1220', 'iras050404820', 'we', 'have', 'measured', 'the', 'equivalent', 'widths', 'of', 'numerous', 'absorption', 'lines', 'of', 'neutral', 'ato... | [-0.02784768942910887, 0.12046364935364788, -0.008423914743616479, 0.035023532057797034, -0.04885565905412174, -0.0678487173524142, 0.06542762076484603, 0.4435893456296374, -0.18203298700973392, -0.35762586733471835, 0.032528920704862685, -0.32213394428739167, 0.04350598320949454, 0.1779430760058555, -0.038757162107989... |
706.3768 | Dynamic Exploration of Networks: from general principles to the
traceroute process | Dynamical processes taking place on real networks define on them evolving
subnetworks whose topology is not necessarily the same of the underlying one.
We investigate the problem of determining the emerging degree distribution,
focusing on a class of tree-like processes, such as those used to explore the
Internet's t... | physics.soc-ph cond-mat.dis-nn cs.NI physics.data-an | dynamical processes taking place on real networks define on them evolving subnetworks whose topology is not necessarily the same of the underlying one we investigate the problem of determining the emerging degree distribution focusing on a class of treelike processes such as those used to explore the internets topology... | [['dynamical', 'processes', 'taking', 'place', 'on', 'real', 'networks', 'define', 'on', 'them', 'evolving', 'subnetworks', 'whose', 'topology', 'is', 'not', 'necessarily', 'the', 'same', 'of', 'the', 'underlying', 'one', 'we', 'investigate', 'the', 'problem', 'of', 'determining', 'the', 'emerging', 'degree', 'distribu... | [-0.14119196623362892, 0.054591750776322154, -0.07338553026099415, 0.1169281916113059, -0.06065526509694025, -0.0970188263214796, 0.06652361256819145, 0.34149826321677834, -0.2791350777580531, -0.3024194493122837, 0.10782602326214022, -0.24070909195214363, -0.22421295999311933, 0.20121880797851904, -0.02083306992540647... |
706.3769 | Molecular gas and star formation in M81 | We present IRAM 30m observations of the central 1.6 kpc of the spiral M81
galaxy. The molecular gas appears weak and with an unusual excitation physics.
We discuss a possible link between low CO emission and weak FUV surface
brightness.
| astro-ph | we present iram 30m observations of the central 16 kpc of the spiral m81 galaxy the molecular gas appears weak and with an unusual excitation physics we discuss a possible link between low co emission and weak fuv surface brightness | [['we', 'present', 'iram', '30m', 'observations', 'of', 'the', 'central', '16', 'kpc', 'of', 'the', 'spiral', 'm81', 'galaxy', 'the', 'molecular', 'gas', 'appears', 'weak', 'and', 'with', 'an', 'unusual', 'excitation', 'physics', 'we', 'discuss', 'a', 'possible', 'link', 'between', 'low', 'co', 'emission', 'and', 'weak... | [-0.11950855072500417, 0.027738935072920867, -0.041629669908434155, 0.11436366809066385, -0.1018642779730726, -0.09902478758012875, 0.025726327573647723, 0.4767689922824502, -0.1630769688170403, -0.3132245915941894, 0.009106118360068648, -0.25705047852825375, -0.047127797198481855, 0.10273082182975486, 0.05870350104523... |
706.377 | Motion of a Vector Particle in a Curved Space-time. IV. Asymptotical
shape of caustic | The studies of influence of spin on a photon motion in a Schwartzschild
spacetime is continued. In the previous paper [2] the first order correction to
the geodesic motion is reduced to a non-uniform linear ordinary differential
equation and the equation obtained has been solved by the standard method of
integration ... | gr-qc | the studies of influence of spin on a photon motion in a schwartzschild spacetime is continued in the previous paper 2 the first order correction to the geodesic motion is reduced to a nonuniform linear ordinary differential equation and the equation obtained has been solved by the standard method of integration of the... | [['the', 'studies', 'of', 'influence', 'of', 'spin', 'on', 'a', 'photon', 'motion', 'in', 'a', 'schwartzschild', 'spacetime', 'is', 'continued', 'in', 'the', 'previous', 'paper', '2', 'the', 'first', 'order', 'correction', 'to', 'the', 'geodesic', 'motion', 'is', 'reduced', 'to', 'a', 'nonuniform', 'linear', 'ordinary'... | [-0.13298175637082188, 0.07071108085861832, -0.11480807042056598, 0.04844926122201549, -0.12002096902915113, -0.08519284734886486, 0.015125049036908318, 0.32487280182924466, -0.24811215916187646, -0.2983022697135499, 0.07303141699575809, -0.2821356308089627, -0.113658537970587, 0.19155649181224943, -0.03701037985570345... |
706.3771 | Embedded Stellar Populations towards Young Massive Star Formation
Regions I. G305.2+0.2 | We present deep, wide-field J, H and Ks images taken with IRIS2 on the Anglo
Australian Telescope, towards the massive star formation region G305.2+0.2.
Combined with 3.6, 4.5, 5.8 and 8.0 micron data from the GLIMPSE survey on the
Spitzer Space Telescope, we investigate the properties of the embedded stellar
populat... | astro-ph | we present deep widefield j h and ks images taken with iris2 on the anglo australian telescope towards the massive star formation region g305202 combined with 36 45 58 and 80 micron data from the glimpse survey on the spitzer space telescope we investigate the properties of the embedded stellar populations after removi... | [['we', 'present', 'deep', 'widefield', 'j', 'h', 'and', 'ks', 'images', 'taken', 'with', 'iris2', 'on', 'the', 'anglo', 'australian', 'telescope', 'towards', 'the', 'massive', 'star', 'formation', 'region', 'g305202', 'combined', 'with', '36', '45', '58', 'and', '80', 'micron', 'data', 'from', 'the', 'glimpse', 'surve... | [-0.056988819654482846, 0.0408130452997284, -0.050866590114310384, 0.09360910394085901, -0.0666708266750599, 0.008998208055951787, 0.09679588615714844, 0.44570770176748437, -0.16090765254254316, -0.3529537346912548, 0.09519105230841281, -0.3229242270075095, -0.06069966684844985, 0.1413394376049837, -0.04229323264799708... |
706.3772 | Valdivia compact Abelian groups | Let R denote the smallest class of compact spaces containing all metric
compacta and closed under limits of continuous inverse sequences of
retractions. Class R is striclty larger than the class of Valdivia compact
spaces. We show that every compact connected Abelian group which is a
topological retract of a space fr... | math.GN | let r denote the smallest class of compact spaces containing all metric compacta and closed under limits of continuous inverse sequences of retractions class r is striclty larger than the class of valdivia compact spaces we show that every compact connected abelian group which is a topological retract of a space from c... | [['let', 'r', 'denote', 'the', 'smallest', 'class', 'of', 'compact', 'spaces', 'containing', 'all', 'metric', 'compacta', 'and', 'closed', 'under', 'limits', 'of', 'continuous', 'inverse', 'sequences', 'of', 'retractions', 'class', 'r', 'is', 'striclty', 'larger', 'than', 'the', 'class', 'of', 'valdivia', 'compact', 's... | [-0.19695320623438983, 0.13408997840625012, -0.043068076722279545, 0.01584930630425723, -0.13843181440218663, -0.1251284150528677, -0.019926169088908603, 0.37694485512162956, -0.2731783757695839, -0.1646378596889831, 0.1292738275563655, -0.2622235198394351, -0.09360098814968729, 0.23739563877738656, -0.1379806457109572... |
706.3773 | Two Component Baryonic-Dark Matter Structure Formation in Top-Hat Model | In this work we extend simple top-hat model of structure formation to the
two-component system made of baryonic and dark matter. We use
Harrison-Zeldovich spectrum as the initial condition for the structures and
calculate their evolution up to the present time. While we do not take into
account some complications dur... | astro-ph | in this work we extend simple tophat model of structure formation to the twocomponent system made of baryonic and dark matter we use harrisonzeldovich spectrum as the initial condition for the structures and calculate their evolution up to the present time while we do not take into account some complications during the... | [['in', 'this', 'work', 'we', 'extend', 'simple', 'tophat', 'model', 'of', 'structure', 'formation', 'to', 'the', 'twocomponent', 'system', 'made', 'of', 'baryonic', 'and', 'dark', 'matter', 'we', 'use', 'harrisonzeldovich', 'spectrum', 'as', 'the', 'initial', 'condition', 'for', 'the', 'structures', 'and', 'calculate'... | [-0.10636079044121763, 0.09241678851373893, -0.1290654702927709, 0.10590397710955314, -0.07175561388873536, -0.03483943458825859, -0.005068252873982979, 0.363372843105184, -0.24713630901840486, -0.3452968590701959, 0.06500070973918397, -0.2221116780098065, -0.13042987809047935, 0.17847157611659156, 0.021517790133792975... |
706.3774 | Superfluid equation of state of dilute composite bosons | We present an exact theory of the BEC-BCS crossover in the BEC regime, which
treats explicitely dimers as made of two fermions. We apply our framework, at
zero temperature, to the calculation of the equation of state. We find that,
when expanding the chemical potential in powers of the density n up to the
Lee-Huang-Y... | cond-mat.stat-mech | we present an exact theory of the becbcs crossover in the bec regime which treats explicitely dimers as made of two fermions we apply our framework at zero temperature to the calculation of the equation of state we find that when expanding the chemical potential in powers of the density n up to the leehuangyang order p... | [['we', 'present', 'an', 'exact', 'theory', 'of', 'the', 'becbcs', 'crossover', 'in', 'the', 'bec', 'regime', 'which', 'treats', 'explicitely', 'dimers', 'as', 'made', 'of', 'two', 'fermions', 'we', 'apply', 'our', 'framework', 'at', 'zero', 'temperature', 'to', 'the', 'calculation', 'of', 'the', 'equation', 'of', 'sta... | [-0.14505765497464165, 0.19563664310322, -0.050520803073361036, 0.03709106807852344, 0.016979515492435423, -0.11016635833087787, 0.03459544729326241, 0.28569298499934775, -0.24392761715677796, -0.2525580385449513, -0.0005510697762171427, -0.3237788538518612, -0.12352664174664746, 0.09232250108353553, 0.0811649656163588... |
706.3775 | How particles emerge from decaying classical fields in heavy ion
collisions: towards a kinetic description of the Glasma | We develop the formalism discussed previously in hep-ph/0601209 and
hep-ph/0605246 to construct a kinetic theory that provides insight into the
earliest ``Glasma'' stage of a high energy heavy ion collision. Particles
produced from the decay of classical fields in the Glasma obey a Boltzmann
equation whose novel feat... | hep-ph hep-th nucl-th | we develop the formalism discussed previously in hepph0601209 and hepph0605246 to construct a kinetic theory that provides insight into the earliest glasma stage of a high energy heavy ion collision particles produced from the decay of classical fields in the glasma obey a boltzmann equation whose novel features includ... | [['we', 'develop', 'the', 'formalism', 'discussed', 'previously', 'in', 'hepph0601209', 'and', 'hepph0605246', 'to', 'construct', 'a', 'kinetic', 'theory', 'that', 'provides', 'insight', 'into', 'the', 'earliest', 'glasma', 'stage', 'of', 'a', 'high', 'energy', 'heavy', 'ion', 'collision', 'particles', 'produced', 'fro... | [-0.06099719710081168, 0.22403500672146986, -0.14109334872995058, 0.11022545685789184, -0.0287982069624021, -0.10864469657067473, -0.057271400031269244, 0.26255141662271775, -0.28467245467776514, -0.28411808757759305, -0.011088230208058478, -0.29286731263298704, -0.0259842156716015, 0.13562775602306076, 0.0372986925421... |
706.3776 | On an explicit construction of Parisi landscapes in finite dimensional
Euclidean spaces | We construct a N-dimensional Gaussian landscape with multiscale, translation
invariant, logarithmic correlations and investigate the statistical mechanics
of a single particle in this environment. In the limit of high dimension N>>1
the free energy of the system in the thermodynamic limit coincides with the
most gene... | cond-mat.dis-nn cond-mat.mes-hall | we construct a ndimensional gaussian landscape with multiscale translation invariant logarithmic correlations and investigate the statistical mechanics of a single particle in this environment in the limit of high dimension n1 the free energy of the system in the thermodynamic limit coincides with the most general vers... | [['we', 'construct', 'a', 'ndimensional', 'gaussian', 'landscape', 'with', 'multiscale', 'translation', 'invariant', 'logarithmic', 'correlations', 'and', 'investigate', 'the', 'statistical', 'mechanics', 'of', 'a', 'single', 'particle', 'in', 'this', 'environment', 'in', 'the', 'limit', 'of', 'high', 'dimension', 'n1'... | [-0.1213269390123473, 0.17056242645379494, -0.11161541152978316, 0.08385985283133447, 0.0301499616259455, -0.10481517292580313, -0.002981426139740506, 0.2771615276578814, -0.25638353900417726, -0.25597778956448153, 0.046925095817476344, -0.2606427993265573, -0.13481925664977593, 0.1496014983581104, -0.05779749346600676... |
706.3777 | Using VO tools to investigate distant radio starbursts hosting obscured
AGN in the HDF(N) region | A 10-arcmin field around the HDF(N) contains 92 radio sources >40 uJy,
resolved by MERLIN+VLA at 0".2-2".0 resolution. 55 have Chandra X-ray
counterparts including 18 with a hard X-ray photon index and high luminosity
characteristic of a type-II (obscured) AGN. >70% of the radio sources have been
classified as starbu... | astro-ph | a 10arcmin field around the hdfn contains 92 radio sources 40 ujy resolved by merlinvla at 0220 resolution 55 have chandra xray counterparts including 18 with a hard xray photon index and high luminosity characteristic of a typeii obscured agn 70 of the radio sources have been classified as starbursts or agn using radi... | [['a', '10arcmin', 'field', 'around', 'the', 'hdfn', 'contains', '92', 'radio', 'sources', '40', 'ujy', 'resolved', 'by', 'merlinvla', 'at', '0220', 'resolution', '55', 'have', 'chandra', 'xray', 'counterparts', 'including', '18', 'with', 'a', 'hard', 'xray', 'photon', 'index', 'and', 'high', 'luminosity', 'characteris... | [0.004316293158940313, 0.10500695906460611, -0.017432218965679033, 0.18282905266893362, -0.1122068509874148, -0.07951214964717113, 0.07261521171189371, 0.5458152668859955, -0.05867958517478575, -0.3814744395746886, 0.07339867714269238, -0.3792234679631389, 0.022460932842564403, 0.19371927470798872, 0.021158494094761858... |
706.3778 | Photon spectra from final stages of a primordial black hole evaporation
in different theoretical models | Possibilities of an experimental search for gamma-ray bursts from primordial
black hole (PBH) evaporations in space are reconsidered. It is argued that the
corresponding constraints which can be obtained in experiments with cosmic ray
detectors strongly depend on theoretical approach used for a description of the
PBH... | astro-ph | possibilities of an experimental search for gammaray bursts from primordial black hole pbh evaporations in space are reconsidered it is argued that the corresponding constraints which can be obtained in experiments with cosmic ray detectors strongly depend on theoretical approach used for a description of the pbh evapo... | [['possibilities', 'of', 'an', 'experimental', 'search', 'for', 'gammaray', 'bursts', 'from', 'primordial', 'black', 'hole', 'pbh', 'evaporations', 'in', 'space', 'are', 'reconsidered', 'it', 'is', 'argued', 'that', 'the', 'corresponding', 'constraints', 'which', 'can', 'be', 'obtained', 'in', 'experiments', 'with', 'c... | [-0.02596595711485647, 0.1767696763788134, -0.11266709213583347, 0.1613803853424275, -0.06000548671342104, -0.06874025430229, -0.005154006772071999, 0.37181525050169406, -0.16903456951053264, -0.34611707824446697, 0.04018747332327835, -0.3098275489310789, -0.03531159316052628, 0.3557749385911259, 0.022414697758743867, ... |
706.3779 | Analogy between the wave of the falling dominoes and the growth of
martensitic crystal (a simple enunciating for experimenters) | A number of laws being characteristic for switching waves are illustrated by
the examples of waves of a falling dominoes. The specificity of a switching
wave at the martensite crystal growth caused by dynamic structure of interphase
area is noted. For the first time the influence of finite deformation on the
conditio... | cond-mat.mtrl-sci | a number of laws being characteristic for switching waves are illustrated by the examples of waves of a falling dominoes the specificity of a switching wave at the martensite crystal growth caused by dynamic structure of interphase area is noted for the first time the influence of finite deformation on the condition of... | [['a', 'number', 'of', 'laws', 'being', 'characteristic', 'for', 'switching', 'waves', 'are', 'illustrated', 'by', 'the', 'examples', 'of', 'waves', 'of', 'a', 'falling', 'dominoes', 'the', 'specificity', 'of', 'a', 'switching', 'wave', 'at', 'the', 'martensite', 'crystal', 'growth', 'caused', 'by', 'dynamic', 'structu... | [-0.19681235783112547, 0.23646721015829825, -0.05166462297137413, 0.023970871257026575, -0.04369556652382016, -0.04944392814714876, 0.030392510630190373, 0.3301933449123883, -0.28392507756976154, -0.25161481843226485, 0.09764230981883075, -0.273605285719451, -0.12213191595704605, 0.18429098080636727, 0.0251410028690265... |
706.378 | The Magellanic Squall: Gas Replenishment from the Small to Large
Magellanic Cloud | We first show that a large amount of metal-poor gas is stripped from the
Small Magellanic Cloud (SMC) and fallen into the Large Magellanic Cloud (LMC)
during the tidal interaction between the SMC, the LMC, and the Galaxy over the
last 2 Gyrs. We propose that this metal-poor gas can closely be associated with
the orig... | astro-ph | we first show that a large amount of metalpoor gas is stripped from the small magellanic cloud smc and fallen into the large magellanic cloud lmc during the tidal interaction between the smc the lmc and the galaxy over the last 2 gyrs we propose that this metalpoor gas can closely be associated with the origin of lmcs ... | [['we', 'first', 'show', 'that', 'a', 'large', 'amount', 'of', 'metalpoor', 'gas', 'is', 'stripped', 'from', 'the', 'small', 'magellanic', 'cloud', 'smc', 'and', 'fallen', 'into', 'the', 'large', 'magellanic', 'cloud', 'lmc', 'during', 'the', 'tidal', 'interaction', 'between', 'the', 'smc', 'the', 'lmc', 'and', 'the', ... | [-0.05247949822718253, 0.14553795481075954, -0.10474840497264001, 0.08068120187669746, -0.04258862990717016, -0.012221924451682551, 0.1081314294463007, 0.39172869861776016, -0.23972838506333333, -0.35968793481505945, 0.021349270689503118, -0.2749784698244184, 0.00988365557102437, 0.18043924780949885, -0.058678581219926... |
706.3781 | Numerical simulation of spray coalescence in an eulerian framework :
direct quadrature method of moments and multi-fluid method | The scope of the present study is Eulerian modeling and simulation of
polydisperse liquid sprays undergoing droplet coalescence and evaporation. The
fundamental mathematical description is the Williams spray equation governing
the joint number density function f(v, u; x, t) of droplet volume and velocity.
Eulerian mu... | math.NA physics.class-ph | the scope of the present study is eulerian modeling and simulation of polydisperse liquid sprays undergoing droplet coalescence and evaporation the fundamental mathematical description is the williams spray equation governing the joint number density function fv u x t of droplet volume and velocity eulerian multifluid ... | [['the', 'scope', 'of', 'the', 'present', 'study', 'is', 'eulerian', 'modeling', 'and', 'simulation', 'of', 'polydisperse', 'liquid', 'sprays', 'undergoing', 'droplet', 'coalescence', 'and', 'evaporation', 'the', 'fundamental', 'mathematical', 'description', 'is', 'the', 'williams', 'spray', 'equation', 'governing', 't... | [-0.0888520198236422, 0.07686511950526873, -0.12157387682995961, 0.03048919677562283, -0.07382949060031577, -0.10360969369977956, -0.04009511683556332, 0.30807240246845735, -0.2659687986572111, -0.31368592761092534, 0.041152363153979306, -0.2520746018626201, -0.12605097517624256, 0.17553646176921853, -0.020099127528500... |
706.3782 | The Virgo - MiniGRAIL cross correlation for the detection of scalar
gravitational waves | After a review of the frequency - dependent angular pattern of
interferometers in the TT gauge for scalar gravitational waves (SGWs), which
has been recently analysed by Capozziello and Corda, in this letter the result
is used to study the cross correlation between the Virgo interferometer and the
MiniGRAIL resonant ... | astro-ph | after a review of the frequency dependent angular pattern of interferometers in the tt gauge for scalar gravitational waves sgws which has been recently analysed by capozziello and corda in this letter the result is used to study the cross correlation between the virgo interferometer and the minigrail resonant sphere i... | [['after', 'a', 'review', 'of', 'the', 'frequency', 'dependent', 'angular', 'pattern', 'of', 'interferometers', 'in', 'the', 'tt', 'gauge', 'for', 'scalar', 'gravitational', 'waves', 'sgws', 'which', 'has', 'been', 'recently', 'analysed', 'by', 'capozziello', 'and', 'corda', 'in', 'this', 'letter', 'the', 'result', 'is... | [-0.13644760109837278, 0.12907511174901398, -0.102687361946964, 0.09207392652176198, -0.03186570525496871, -0.04981577472126746, -0.019633233122486663, 0.3561651355658586, -0.1730055458188712, -0.30664064526394175, 0.05605561075384145, -0.2891686383000278, -0.1553064188996719, 0.18345032511586015, 0.04630489194008348, ... |
706.3783 | S-Matrix Poles Close to Thresholds in Confined Geometries | We have studied the behavior of the S-matrix poles near threshold for quantum
waveguides coupled to a cavity with a defect. We emphasize the occurrence of
both dominant and shadow poles on the various sheets of the energy Riemann
surface, and show that the changes of the total conductivity near threshold as
the cavit... | cond-mat.mes-hall | we have studied the behavior of the smatrix poles near threshold for quantum waveguides coupled to a cavity with a defect we emphasize the occurrence of both dominant and shadow poles on the various sheets of the energy riemann surface and show that the changes of the total conductivity near threshold as the cavitys wi... | [['we', 'have', 'studied', 'the', 'behavior', 'of', 'the', 'smatrix', 'poles', 'near', 'threshold', 'for', 'quantum', 'waveguides', 'coupled', 'to', 'a', 'cavity', 'with', 'a', 'defect', 'we', 'emphasize', 'the', 'occurrence', 'of', 'both', 'dominant', 'and', 'shadow', 'poles', 'on', 'the', 'various', 'sheets', 'of', '... | [-0.18200463144136453, 0.13196222253366194, -0.05365940521874312, 0.07472105133486216, -0.013776421310630307, -0.05904235405875231, 0.05591109538721894, 0.3520582577547253, -0.23249187626278223, -0.2646982915588279, 0.09097336123957223, -0.29831000245106754, -0.1775311339201767, 0.16814547499169163, -0.0001122799993895... |
706.3784 | Status of QGSJET | Basic physics concepts of the QGSJET model are discussed, starting from the
general picture of high energy hadronic interactions and addressing in some
detail the treatment of multiple scattering processes, contributions of
``soft'' and ``semihard'' parton dynamics, implementation of non-linear
interaction effects. T... | hep-ph | basic physics concepts of the qgsjet model are discussed starting from the general picture of high energy hadronic interactions and addressing in some detail the treatment of multiple scattering processes contributions of soft and semihard parton dynamics implementation of nonlinear interaction effects the predictions ... | [['basic', 'physics', 'concepts', 'of', 'the', 'qgsjet', 'model', 'are', 'discussed', 'starting', 'from', 'the', 'general', 'picture', 'of', 'high', 'energy', 'hadronic', 'interactions', 'and', 'addressing', 'in', 'some', 'detail', 'the', 'treatment', 'of', 'multiple', 'scattering', 'processes', 'contributions', 'of', ... | [-0.03195000950247049, 0.18080163694297274, -0.07207034850881125, 0.1971898752031848, -0.05398554382224878, -0.1494469713171323, -0.06236369974911213, 0.3317244958877563, -0.23772580136855442, -0.3030742877535522, 0.04338965980801732, -0.3479892627646526, -0.05366465870290995, 0.17302568219291667, 0.07577950209379196, ... |
706.3785 | Order from Randomness | We consider an elementary discrete process which starts from purely random
configuration and leads to well-ordered and stable state. Complete analytical
solution to this problem is presented.
| math.HO | we consider an elementary discrete process which starts from purely random configuration and leads to wellordered and stable state complete analytical solution to this problem is presented | [['we', 'consider', 'an', 'elementary', 'discrete', 'process', 'which', 'starts', 'from', 'purely', 'random', 'configuration', 'and', 'leads', 'to', 'wellordered', 'and', 'stable', 'state', 'complete', 'analytical', 'solution', 'to', 'this', 'problem', 'is', 'presented']] | [-0.1034826264820165, 0.13185738250063472, -0.11135231337889477, 0.035379196390311805, -0.1141497080248815, -0.12385047599673271, 0.07529155078292307, 0.3958346709884979, -0.32942097504726714, -0.19990460512538752, 0.09261470234573439, -0.23583539244201449, -0.11206360834141917, 0.10650317163930999, -0.0631766273743576... |
706.3786 | Plumbing the Abyss: Black Ring Microstates | We construct the first smooth, horizonless ``microstate geometries'' that
have the same charges, dipole charges and angular momenta as a BPS black ring
whose horizon is macroscopic. These solutions have exactly the same geometry as
black rings, except that the usual infinite throat is smoothly capped off at a
very la... | hep-th | we construct the first smooth horizonless microstate geometries that have the same charges dipole charges and angular momenta as a bps black ring whose horizon is macroscopic these solutions have exactly the same geometry as black rings except that the usual infinite throat is smoothly capped off at a very large depth ... | [['we', 'construct', 'the', 'first', 'smooth', 'horizonless', 'microstate', 'geometries', 'that', 'have', 'the', 'same', 'charges', 'dipole', 'charges', 'and', 'angular', 'momenta', 'as', 'a', 'bps', 'black', 'ring', 'whose', 'horizon', 'is', 'macroscopic', 'these', 'solutions', 'have', 'exactly', 'the', 'same', 'geome... | [-0.14731632201662173, 0.13276491954457015, -0.11966381328076953, 0.10984376165584696, -0.09716810866397012, -0.21227241806789404, -0.00740158248025878, 0.30843171001021047, -0.2189621199209841, -0.2526001769957351, 0.11520688396800931, -0.279866935895112, -0.10164760123078861, 0.1473370599258622, -0.10198045630089904,... |
706.3787 | The formation of black holes in spherically symmetric gravitational
collapse | We consider the spherically symmetric, asymptotically flat Einstein-Vlasov
system. We find explicit conditions on the initial data, with ADM mass M, such
that the resulting spacetime has the following properties: there is a family of
radially outgoing null geodesics where the area radius r along each geodesic is
boun... | gr-qc | we consider the spherically symmetric asymptotically flat einsteinvlasov system we find explicit conditions on the initial data with adm mass m such that the resulting spacetime has the following properties there is a family of radially outgoing null geodesics where the area radius r along each geodesic is bounded by 2... | [['we', 'consider', 'the', 'spherically', 'symmetric', 'asymptotically', 'flat', 'einsteinvlasov', 'system', 'we', 'find', 'explicit', 'conditions', 'on', 'the', 'initial', 'data', 'with', 'adm', 'mass', 'm', 'such', 'that', 'the', 'resulting', 'spacetime', 'has', 'the', 'following', 'properties', 'there', 'is', 'a', '... | [-0.18303964353521893, 0.09710570925074678, -0.06987893536049676, 0.08182274444353473, -0.058797326534802685, -0.14226975544404827, -0.05456371571543921, 0.3488147121449736, -0.18506246627504497, -0.265049397310481, 0.13809866852840824, -0.31003805203669654, -0.07563903780292573, 0.15816332325860122, -0.046010379439777... |
706.3788 | Measurement of the Neutrino Asymmetry Parameter B in Neutron Decay | A new measurement of the neutrino asymmetry parameter B in neutron decay, the
angular correlation between neutron spin and anti-neutrino momentum, is
presented. The result, B=0.9802(50), agrees with the Standard Model expectation
and earlier measurements, and permits improved tests on ``new physics'' in
neutron decay... | hep-ph | a new measurement of the neutrino asymmetry parameter b in neutron decay the angular correlation between neutron spin and antineutrino momentum is presented the result b0980250 agrees with the standard model expectation and earlier measurements and permits improved tests on new physics in neutron decay | [['a', 'new', 'measurement', 'of', 'the', 'neutrino', 'asymmetry', 'parameter', 'b', 'in', 'neutron', 'decay', 'the', 'angular', 'correlation', 'between', 'neutron', 'spin', 'and', 'antineutrino', 'momentum', 'is', 'presented', 'the', 'result', 'b0980250', 'agrees', 'with', 'the', 'standard', 'model', 'expectation', 'a... | [-0.0653645505239679, 0.24232151130193166, -0.09547894497783008, 0.12666384333120237, -0.07092289736663754, -0.11528966121841222, 0.07715548342093825, 0.2745288625698198, -0.1930098690076689, -0.330806117547168, -0.03163834021490237, -0.3262238221941516, 0.041580163619735024, 0.25899469284658233, 0.05951867841014808, 0... |
706.3789 | Symbolic Computations for Nonlinear Resonances | Nonlinear dynamics and pattern formation in the systems with quadratic
nonlinearity is computed symbolically by specially developed MATHEMATICA
package. A Web interface for the presented methods is developed, which turns
the implementations from only locally available software to Web-based services
that can be access... | nlin.PS | nonlinear dynamics and pattern formation in the systems with quadratic nonlinearity is computed symbolically by specially developed mathematica package a web interface for the presented methods is developed which turns the implementations from only locally available software to webbased services that can be accessed fr... | [['nonlinear', 'dynamics', 'and', 'pattern', 'formation', 'in', 'the', 'systems', 'with', 'quadratic', 'nonlinearity', 'is', 'computed', 'symbolically', 'by', 'specially', 'developed', 'mathematica', 'package', 'a', 'web', 'interface', 'for', 'the', 'presented', 'methods', 'is', 'developed', 'which', 'turns', 'the', 'i... | [-0.13062173625474074, 0.02987366335308355, -0.0933946617088228, 0.03560751769472054, -0.15006011058268892, -0.24326186057812763, -0.07595911913744684, 0.3694093679780808, -0.30136310033289326, -0.30588206044345534, 0.15212094668795373, -0.24589459817715972, -0.13298367609858583, 0.27806582070562, -0.04180778221011421,... |
706.379 | Measurement of the p anti-p to t anti-t Production Cross Section and the
Top Quark Mass at sqrt{s}=1.96 TeV in the All-Hadronic Decay Mode | We report the measurements of the t anti-t production cross section and of
the top quark mass using 1.02 fb^-1 of p anti-p data collected with the CDFII
detector at the Fermilab Tevatron. We select events with six or more jets on
which a number of kinematical requirements are imposed by means of a neural
network algo... | hep-ex | we report the measurements of the t antit production cross section and of the top quark mass using 102 fb1 of p antip data collected with the cdfii detector at the fermilab tevatron we select events with six or more jets on which a number of kinematical requirements are imposed by means of a neural network algorithm at... | [['we', 'report', 'the', 'measurements', 'of', 'the', 't', 'antit', 'production', 'cross', 'section', 'and', 'of', 'the', 'top', 'quark', 'mass', 'using', '102', 'fb1', 'of', 'p', 'antip', 'data', 'collected', 'with', 'the', 'cdfii', 'detector', 'at', 'the', 'fermilab', 'tevatron', 'we', 'select', 'events', 'with', 'si... | [-0.05686458362821401, 0.1584845793850977, -0.08438567018160469, 0.08085897113577913, -0.0355318625746616, -0.1272494081801189, 0.04892078925983916, 0.3265094114306929, -0.1802057186864188, -0.3842972840889004, 0.022193667896348853, -0.3596705178698075, 0.0564213394215491, 0.15591930816198923, 0.050251188334719886, 0.1... |
706.3791 | Secure Reusable Base-String in Quantum Key Distribution | Protecting secure random key from eavesdropping in quantum key distribution
protocols has been well developed. In this letter, we further study how to
detect and eliminate eavesdropping on the random base string in such protocols.
The correlation between the base string and the key enables Alice and Bob to
use specif... | quant-ph | protecting secure random key from eavesdropping in quantum key distribution protocols has been well developed in this letter we further study how to detect and eliminate eavesdropping on the random base string in such protocols the correlation between the base string and the key enables alice and bob to use specific pr... | [['protecting', 'secure', 'random', 'key', 'from', 'eavesdropping', 'in', 'quantum', 'key', 'distribution', 'protocols', 'has', 'been', 'well', 'developed', 'in', 'this', 'letter', 'we', 'further', 'study', 'how', 'to', 'detect', 'and', 'eliminate', 'eavesdropping', 'on', 'the', 'random', 'base', 'string', 'in', 'such'... | [-0.18190598574172542, 0.047544612461591466, -0.09883884547606987, 0.06617189456626554, -0.05736811202676857, -0.2907102644333945, 0.14678686890915474, 0.337494575539056, -0.2742159899762448, -0.3004428357543314, 0.04595655866569894, -0.2263602489934248, -0.11871907076634028, 0.15858427429681315, -0.1657588916063747, 0... |
706.3792 | Renormalized Fermi hypernetted chain approach in medium-heavy nuclei | The application of the Correlated basis function theory and of the Fermi
hypernetted chain technique, to the description of the ground state of
medium-heavy nuclei is reviewed. We discuss how the formalism, originally
developed for symmetric nuclear matter, should be changed in order to describe
finite nuclear system... | nucl-th | the application of the correlated basis function theory and of the fermi hypernetted chain technique to the description of the ground state of mediumheavy nuclei is reviewed we discuss how the formalism originally developed for symmetric nuclear matter should be changed in order to describe finite nuclear systems with ... | [['the', 'application', 'of', 'the', 'correlated', 'basis', 'function', 'theory', 'and', 'of', 'the', 'fermi', 'hypernetted', 'chain', 'technique', 'to', 'the', 'description', 'of', 'the', 'ground', 'state', 'of', 'mediumheavy', 'nuclei', 'is', 'reviewed', 'we', 'discuss', 'how', 'the', 'formalism', 'originally', 'deve... | [-0.05216136182545973, 0.21649420850685444, -0.11285582059243662, 0.14915374607441884, 0.005720088760175839, -0.0905269153480386, 0.030592202523056868, 0.350047057093089, -0.17001521234111538, -0.28026476795070393, -0.12693835529077252, -0.32179181709103305, -0.02298367080471382, 0.13023299929196144, 0.1032146358910691... |
706.3793 | Critical tests of unintegrated gluon distributions | We use the unintegrated Parton Density Functions of the gluon obtained from a
fit to measurements of the structure functions F2 and F2c at HERA to describe
the experimental data for F2b, FL and FL at fixed W.
| hep-ph | we use the unintegrated parton density functions of the gluon obtained from a fit to measurements of the structure functions f2 and f2c at hera to describe the experimental data for f2b fl and fl at fixed w | [['we', 'use', 'the', 'unintegrated', 'parton', 'density', 'functions', 'of', 'the', 'gluon', 'obtained', 'from', 'a', 'fit', 'to', 'measurements', 'of', 'the', 'structure', 'functions', 'f2', 'and', 'f2c', 'at', 'hera', 'to', 'describe', 'the', 'experimental', 'data', 'for', 'f2b', 'fl', 'and', 'fl', 'at', 'fixed', 'w... | [0.010422759173387612, 0.12350708621277197, -0.17668850294540864, 0.11128047629687432, -0.026204214764859627, -0.06141911178663675, 0.041713001508567785, 0.3747208762813259, -0.22978345986858412, -0.2083256473211018, 0.008519269135856145, -0.3216799644098894, 0.015297305996756296, 0.13413813674973474, 0.129561567729389... |
706.3794 | On systematic scan for sampling H-colourings of the path | This paper is concerned with sampling from the uniform distribution on
H-colourings of the n-vertex path using systematic scan Markov chains. An
H-colouring of the n-vertex path is a homomorphism from the n-vertex path to
some fixed graph H. We show that systematic scan for H-colourings of the
n-vertex path mixes in ... | math.PR | this paper is concerned with sampling from the uniform distribution on hcolourings of the nvertex path using systematic scan markov chains an hcolouring of the nvertex path is a homomorphism from the nvertex path to some fixed graph h we show that systematic scan for hcolourings of the nvertex path mixes in olog n scan... | [['this', 'paper', 'is', 'concerned', 'with', 'sampling', 'from', 'the', 'uniform', 'distribution', 'on', 'hcolourings', 'of', 'the', 'nvertex', 'path', 'using', 'systematic', 'scan', 'markov', 'chains', 'an', 'hcolouring', 'of', 'the', 'nvertex', 'path', 'is', 'a', 'homomorphism', 'from', 'the', 'nvertex', 'path', 'to... | [-0.15833254788369333, 0.19126138314500232, -0.04490254898752335, 0.010593163594767504, -0.05331377460929552, -0.15697012861705267, 0.11078871330853, 0.43231511862397615, -0.25439509600532095, -0.33427526005773317, 0.07771348427000627, -0.31870787450387866, -0.06772899829854691, 0.1454489646269612, -0.058113326398905, ... |
706.3795 | Scaling theory put into practice: first-principles modeling of transport
in doped silicon nanowires | We combine the ideas of scaling theory and universal conductance fluctuations
with density-functional theory to analyze the conductance properties of doped
silicon nanowires. Specifically, we study the cross-over from ballistic to
diffusive transport in boron (B) or phosphorus (P) doped Si-nanowires by
computing the ... | cond-mat.mes-hall | we combine the ideas of scaling theory and universal conductance fluctuations with densityfunctional theory to analyze the conductance properties of doped silicon nanowires specifically we study the crossover from ballistic to diffusive transport in boron b or phosphorus p doped sinanowires by computing the mean free p... | [['we', 'combine', 'the', 'ideas', 'of', 'scaling', 'theory', 'and', 'universal', 'conductance', 'fluctuations', 'with', 'densityfunctional', 'theory', 'to', 'analyze', 'the', 'conductance', 'properties', 'of', 'doped', 'silicon', 'nanowires', 'specifically', 'we', 'study', 'the', 'crossover', 'from', 'ballistic', 'to'... | [-0.11026610408572289, 0.1599616552758082, -0.09205762057576153, 0.03371957085630673, 0.03556287553762709, -0.1709603403262266, 0.09163013794074407, 0.391824443905255, -0.25518718416120595, -0.29057335573446563, -0.047471174456025146, -0.37228353449150803, -0.14073834747193367, 0.1529112065496935, 0.0017231792710193498... |
706.3796 | Selection and reconstruction of very inclined air showers with the
Surface Detector of the Pierre Auger Observatory | The water-Cherenkov tanks of the Pierre Auger Observatory can detect
particles at all zenith angles and are therefore well-suited for the study of
inclined and horizontal air showers (60 - 90 degrees). Such showers are
characterised by a dominance of the muonic component at ground, and by a very
elongated and asymmet... | astro-ph | the watercherenkov tanks of the pierre auger observatory can detect particles at all zenith angles and are therefore wellsuited for the study of inclined and horizontal air showers 60 90 degrees such showers are characterised by a dominance of the muonic component at ground and by a very elongated and asymmetrical foot... | [['the', 'watercherenkov', 'tanks', 'of', 'the', 'pierre', 'auger', 'observatory', 'can', 'detect', 'particles', 'at', 'all', 'zenith', 'angles', 'and', 'are', 'therefore', 'wellsuited', 'for', 'the', 'study', 'of', 'inclined', 'and', 'horizontal', 'air', 'showers', '60', '90', 'degrees', 'such', 'showers', 'are', 'cha... | [-0.09662836508579524, 0.22832442933280134, -0.034541309915711076, 0.10118034130855634, -0.016531566319493006, -0.026431176529921666, -0.03506414158440822, 0.4128215729962198, -0.1974582596187841, -0.4145922161714763, 0.09762894218919409, -0.31564058924131855, -0.07381036463288629, 0.19542111862184747, 0.04639290236126... |
706.3797 | On solutions of the standard-model Lagrangian with a Majorana mass term | It is demonstrated that the standard-model Lagrangian with a Majorana mass
term for the neutrino admits no non-trivial solution. Because the standard
model is generally believed to describe the gauge interactions of neutrinos
correctly, the Majorana mass term must vanish and thus cannot enable
neutrino-less double be... | hep-ph | it is demonstrated that the standardmodel lagrangian with a majorana mass term for the neutrino admits no nontrivial solution because the standard model is generally believed to describe the gauge interactions of neutrinos correctly the majorana mass term must vanish and thus cannot enable neutrinoless double beta deca... | [['it', 'is', 'demonstrated', 'that', 'the', 'standardmodel', 'lagrangian', 'with', 'a', 'majorana', 'mass', 'term', 'for', 'the', 'neutrino', 'admits', 'no', 'nontrivial', 'solution', 'because', 'the', 'standard', 'model', 'is', 'generally', 'believed', 'to', 'describe', 'the', 'gauge', 'interactions', 'of', 'neutrino... | [-0.12780873966164097, 0.3056301573316937, -0.08274711600396374, 0.21937816192823373, -0.14337594471616696, -0.22530929381282974, -0.013586573570660532, 0.34531286358833313, -0.17904324640762315, -0.28834519887419596, 0.009651959111454757, -0.27971645896259234, -0.11380258298874514, 0.15007570371022194, -0.001792127789... |
706.3798 | Earthshine observation of vegetation and implication for life detection
on other planets - A review of 2001 - 2006 works | The detection of exolife is one of the goals of very ambitious future space
missions that aim to take direct images of Earth-like planets. While
associations of simple molecules present in the planet's atmosphere ($O_2$,
$O_3$, $CO_2$ etc.) have been identified as possible global biomarkers, we
review here the detect... | astro-ph | the detection of exolife is one of the goals of very ambitious future space missions that aim to take direct images of earthlike planets while associations of simple molecules present in the planets atmosphere o_2 o_3 co_2 etc have been identified as possible global biomarkers we review here the detectability of a sign... | [['the', 'detection', 'of', 'exolife', 'is', 'one', 'of', 'the', 'goals', 'of', 'very', 'ambitious', 'future', 'space', 'missions', 'that', 'aim', 'to', 'take', 'direct', 'images', 'of', 'earthlike', 'planets', 'while', 'associations', 'of', 'simple', 'molecules', 'present', 'in', 'the', 'planets', 'atmosphere', 'o_2',... | [-0.08016406707886725, 0.14886471339101418, -0.062017626145438466, 0.0813809586124138, -0.06264623658473979, -0.0786732951139516, 0.06923951469064552, 0.3583446643235994, -0.20568187491264828, -0.33828143164753277, 0.1321661716614394, -0.3015093099405776, -0.14472190507172428, 0.16815441060672573, -0.08511147871811656,... |
706.3799 | Mott insulators and correlated superfluids in ultracold Bose-Fermi
mixtures | We study the effects of interaction between bosons and fermions in a
Bose-Fermi mixtures loaded in an optical lattice. We concentrate on the
destruction of a bosonic Mott phase driven by repulsive interaction between
bosons and fermions. Once the Mott phase is destroyed, the system enters a
superfluid phase where the... | cond-mat.stat-mech | we study the effects of interaction between bosons and fermions in a bosefermi mixtures loaded in an optical lattice we concentrate on the destruction of a bosonic mott phase driven by repulsive interaction between bosons and fermions once the mott phase is destroyed the system enters a superfluid phase where the movem... | [['we', 'study', 'the', 'effects', 'of', 'interaction', 'between', 'bosons', 'and', 'fermions', 'in', 'a', 'bosefermi', 'mixtures', 'loaded', 'in', 'an', 'optical', 'lattice', 'we', 'concentrate', 'on', 'the', 'destruction', 'of', 'a', 'bosonic', 'mott', 'phase', 'driven', 'by', 'repulsive', 'interaction', 'between', '... | [-0.21965945112065244, 0.36542439823302303, -0.08495712221170273, 0.04871533021856195, 0.029801556130107015, -0.17486905508961242, 0.09730728684912603, 0.35083310692929304, -0.21021827044060978, -0.17658569385560277, 0.0032397488651510617, -0.34907934255898, -0.1324721410846672, 0.04648058707467639, 0.08314145660887544... |
706.38 | Finding gaps in a spectrum | We propose a method for finding gaps in the spectrum of a differential
operator. When applied to the one-dimensional Hamiltonian of the quartic
oscillator, a simple algebraic algorithm is proposed that, step by step,
separates with a remarkable precision all the energies even for a double-well
configuration in a tunn... | quant-ph math-ph math.MP | we propose a method for finding gaps in the spectrum of a differential operator when applied to the onedimensional hamiltonian of the quartic oscillator a simple algebraic algorithm is proposed that step by step separates with a remarkable precision all the energies even for a doublewell configuration in a tunnelling r... | [['we', 'propose', 'a', 'method', 'for', 'finding', 'gaps', 'in', 'the', 'spectrum', 'of', 'a', 'differential', 'operator', 'when', 'applied', 'to', 'the', 'onedimensional', 'hamiltonian', 'of', 'the', 'quartic', 'oscillator', 'a', 'simple', 'algebraic', 'algorithm', 'is', 'proposed', 'that', 'step', 'by', 'step', 'sep... | [-0.12510328661532155, 0.0859385042466105, -0.10714873131216755, 0.04423007985673076, -0.04526992558339049, -0.18966917404609304, 0.058875765891686554, 0.35246731840547113, -0.26484293390124564, -0.2813348148668569, 0.04737182903207011, -0.22632289364460914, -0.16898242457370674, 0.22602764126800357, -0.038773411071844... |
706.3801 | Inverted Mass Hierarchy from Scaling in the Neutrino Mass Matrix: Low
and High Energy Phenomenology | Best-fit values of recent global analyzes of neutrino data imply large solar
neutrino mixing, vanishing U_{e3} and a non-maximal atmospheric neutrino mixing
angle theta_{23}. We show that these values emerge naturally by the hypothesis
of "scaling" in the Majorana neutrino mass matrix, which states that the ratios
of... | hep-ph | bestfit values of recent global analyzes of neutrino data imply large solar neutrino mixing vanishing u_e3 and a nonmaximal atmospheric neutrino mixing angle theta_23 we show that these values emerge naturally by the hypothesis of scaling in the majorana neutrino mass matrix which states that the ratios of its elements... | [['bestfit', 'values', 'of', 'recent', 'global', 'analyzes', 'of', 'neutrino', 'data', 'imply', 'large', 'solar', 'neutrino', 'mixing', 'vanishing', 'u_e3', 'and', 'a', 'nonmaximal', 'atmospheric', 'neutrino', 'mixing', 'angle', 'theta_23', 'we', 'show', 'that', 'these', 'values', 'emerge', 'naturally', 'by', 'the', 'h... | [-0.12013421508841714, 0.3108490447671487, 0.0076641485300230775, 0.18996463837674266, -0.052692023096053656, -0.18563207370323775, 0.0806369820443945, 0.30008681963485967, -0.2340225200721268, -0.30888261842853154, 0.059985634154577, -0.26472003518019693, -0.03730174201793211, 0.16595787314749402, 0.041825219436343444... |
706.3802 | Cosmic Microwave Background Quadrupole and Ellipsoidal Universe | Recent Wilkinson Microwave Anisotropy Probe (WMAP) data confirm the Cosmic
Microwave Background (CMB) quadrupole anomaly. We further elaborate our
previous proposal that the quadrupole power can be naturally suppressed in
axis-symmetric universes. In particular, we discuss in greater detail the CMB
quadrupole anisotr... | astro-ph | recent wilkinson microwave anisotropy probe wmap data confirm the cosmic microwave background cmb quadrupole anomaly we further elaborate our previous proposal that the quadrupole power can be naturally suppressed in axissymmetric universes in particular we discuss in greater detail the cmb quadrupole anisotropy and co... | [['recent', 'wilkinson', 'microwave', 'anisotropy', 'probe', 'wmap', 'data', 'confirm', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'quadrupole', 'anomaly', 'we', 'further', 'elaborate', 'our', 'previous', 'proposal', 'that', 'the', 'quadrupole', 'power', 'can', 'be', 'naturally', 'suppressed', 'in', 'axissymmet... | [-0.10881455805315281, 0.12146741860710131, -0.06742576800441398, 0.045084448365089375, -0.0950694911125052, -0.044712689143555764, -0.01123317728842829, 0.3593984948424978, -0.22114670458640762, -0.33764275841642427, 0.05288507918318919, -0.30560081960448554, -0.051340837259101504, 0.2508437980449837, -0.0041580459241... |
706.3803 | Magnetic confinement of the superconducting condensate in
superconductor/ferromagnet hybrid composites | The influence of an inhomogeneous magnetic field on the magnetoresistance of
thin Al films, used in different superconductor/ferromagnet hybrids, has been
investigated. Two contrasting magnetic textures with out-of-plane magnetization
are explored, namely (i) a plain film in a multidomain state and (ii) an array
of m... | cond-mat.supr-con | the influence of an inhomogeneous magnetic field on the magnetoresistance of thin al films used in different superconductorferromagnet hybrids has been investigated two contrasting magnetic textures with outofplane magnetization are explored namely i a plain film in a multidomain state and ii an array of microsized dot... | [['the', 'influence', 'of', 'an', 'inhomogeneous', 'magnetic', 'field', 'on', 'the', 'magnetoresistance', 'of', 'thin', 'al', 'films', 'used', 'in', 'different', 'superconductorferromagnet', 'hybrids', 'has', 'been', 'investigated', 'two', 'contrasting', 'magnetic', 'textures', 'with', 'outofplane', 'magnetization', 'a... | [-0.17689854085620027, 0.2550532731933117, -0.04015962999983458, -0.01893032175667031, -0.0636188241551281, -0.14683145139497356, 0.0325939071153698, 0.4275411129274289, -0.2540078281526803, -0.31090801948448643, 0.008326366624714865, -0.2599514856992755, -0.06983347013010643, 0.1739241980467341, 0.04382536185221397, 0... |
706.3804 | A Model for the Formation of Large Circumbinary Disks Around Post AGB
Stars | We propose that the large, radius of ~1000 AU, circumbinary rotating disks
observed around some post-asymptotic giant branch (post-AGB) binary stars are
formed from slow AGB wind material that is pushed back to the center of the
nebula by wide jets. We perform 2D-axisymmetrical numerical simulations of fast
and wide ... | astro-ph | we propose that the large radius of 1000 au circumbinary rotating disks observed around some postasymptotic giant branch postagb binary stars are formed from slow agb wind material that is pushed back to the center of the nebula by wide jets we perform 2daxisymmetrical numerical simulations of fast and wide jets that i... | [['we', 'propose', 'that', 'the', 'large', 'radius', 'of', '1000', 'au', 'circumbinary', 'rotating', 'disks', 'observed', 'around', 'some', 'postasymptotic', 'giant', 'branch', 'postagb', 'binary', 'stars', 'are', 'formed', 'from', 'slow', 'agb', 'wind', 'material', 'that', 'is', 'pushed', 'back', 'to', 'the', 'center'... | [-0.11593056953836979, 0.14974674562483392, -0.07807017792389913, 0.03586366787848403, -0.10356376846850722, -0.08516035775213453, 0.0019575273004656065, 0.40454636158388174, -0.2531961140339263, -0.3021526346819665, 0.05124981175971491, -0.2707807283686797, -0.004633924877828734, 0.19634273063536442, -0.02349740366345... |
706.3805 | Reachability and recoverability of sink nodes in growing acyclic
directed networks | We study the growth of networks from a set of isolated ground nodes by the
addition of one new node per time step and also of a fixed number of directed
edges leading from the new node to randomly selected nodes already in the
network. A fixed-width time window is used so that, in general, only nodes that
entered the... | cond-mat.stat-mech | we study the growth of networks from a set of isolated ground nodes by the addition of one new node per time step and also of a fixed number of directed edges leading from the new node to randomly selected nodes already in the network a fixedwidth time window is used so that in general only nodes that entered the netwo... | [['we', 'study', 'the', 'growth', 'of', 'networks', 'from', 'a', 'set', 'of', 'isolated', 'ground', 'nodes', 'by', 'the', 'addition', 'of', 'one', 'new', 'node', 'per', 'time', 'step', 'and', 'also', 'of', 'a', 'fixed', 'number', 'of', 'directed', 'edges', 'leading', 'from', 'the', 'new', 'node', 'to', 'randomly', 'sel... | [-0.14910837519859516, 0.15638021068590566, -0.04760522998495263, 0.0032749588113150678, -0.06989775079111345, -0.12904105568101312, 0.11980295766197861, 0.37254931992855267, -0.31118422905267845, -0.3128914802363671, 0.10378158680523246, -0.30040463060248634, -0.11719994517307582, 0.1526813557611445, -0.03124741313818... |
706.3806 | The Higgs mechanism as a cut-off effect | We compute the Coleman-Weinberg potential with a finite cut-off for pure
SU(2) and SU(3) five-dimensional gauge theories compactified on an interval. We
show that besides the expected Coulomb phase located at and in the vicinity of
the free infrared stable or "trivial" fixed point, the theory possesses also a
Higgs p... | hep-ph hep-lat | we compute the colemanweinberg potential with a finite cutoff for pure su2 and su3 fivedimensional gauge theories compactified on an interval we show that besides the expected coulomb phase located at and in the vicinity of the free infrared stable or trivial fixed point the theory possesses also a higgs phase we compa... | [['we', 'compute', 'the', 'colemanweinberg', 'potential', 'with', 'a', 'finite', 'cutoff', 'for', 'pure', 'su2', 'and', 'su3', 'fivedimensional', 'gauge', 'theories', 'compactified', 'on', 'an', 'interval', 'we', 'show', 'that', 'besides', 'the', 'expected', 'coulomb', 'phase', 'located', 'at', 'and', 'in', 'the', 'vic... | [-0.11208466596872313, 0.18138293874130795, -0.11550258248462342, 0.07302837418683339, -0.017314502070803428, -0.143530600485974, 0.07572081129728758, 0.3716479407994484, -0.1910285947160446, -0.21205211024789605, 0.0839996870035975, -0.3091976413561497, -0.13203283933762577, 0.1251223505314556, -0.0007065365566631954,... |
706.3807 | Twist two operators at finite volume | We calculate the volume corrections to the two-pion matrix element of twist
two operators.
| hep-lat | we calculate the volume corrections to the twopion matrix element of twist two operators | [['we', 'calculate', 'the', 'volume', 'corrections', 'to', 'the', 'twopion', 'matrix', 'element', 'of', 'twist', 'two', 'operators']] | [-0.14071385396112288, 0.2006620581793998, -0.08529218884983233, 0.15547683502414397, 0.024444205137634917, -0.025626621741269315, -0.010245565325021744, 0.32080342727048056, -0.26738088338502813, -0.13327783053474768, 0.03640083473042718, -0.4163629322179726, -0.06437391122536999, 0.06353954298953925, 0.03642567771540... |
706.3808 | Birefringence (rotation of polarization plane and spin dichroism) of
deuterons in carbon target | Birefringence phenomenon for deuteron with energy up 20 MeV in carbon target
is considered. The estimation for spin dichroism and for angle of rotation of
polarization plane of deuterons is presented. It is shown that magnitude of the
phenomenon strongly depends on behavior of the deuteron wave functions on small
dis... | nucl-th | birefringence phenomenon for deuteron with energy up 20 mev in carbon target is considered the estimation for spin dichroism and for angle of rotation of polarization plane of deuterons is presented it is shown that magnitude of the phenomenon strongly depends on behavior of the deuteron wave functions on small distanc... | [['birefringence', 'phenomenon', 'for', 'deuteron', 'with', 'energy', 'up', '20', 'mev', 'in', 'carbon', 'target', 'is', 'considered', 'the', 'estimation', 'for', 'spin', 'dichroism', 'and', 'for', 'angle', 'of', 'rotation', 'of', 'polarization', 'plane', 'of', 'deuterons', 'is', 'presented', 'it', 'is', 'shown', 'that... | [-0.11412229764656248, 0.24044226584109393, -0.035324262412772936, 0.0668343883219429, -0.04577337500734509, -0.05241247672926296, 0.012879827339202166, 0.41749569685621696, -0.21419459124180404, -0.2719892862845551, -0.05173496126874604, -0.3098362982273102, -0.055477848242629656, 0.2365719495002519, 0.077301208539442... |
706.3809 | High-E_T dijet photoproduction at HERA | The cross section for high-E_T dijet production in photoproduction has been
measured with the ZEUS detector at HERA using an integrated luminosity of 81.8
pb-1. The events were required to have a virtuality of the incoming photon,
Q^2, of less than 1 GeV^2 and a photon-proton centre-of-mass energy in the
range 142 < ... | hep-ex | the cross section for highe_t dijet production in photoproduction has been measured with the zeus detector at hera using an integrated luminosity of 818 pb1 the events were required to have a virtuality of the incoming photon q2 of less than 1 gev2 and a photonproton centreofmass energy in the range 142 w 293 gev event... | [['the', 'cross', 'section', 'for', 'highe_t', 'dijet', 'production', 'in', 'photoproduction', 'has', 'been', 'measured', 'with', 'the', 'zeus', 'detector', 'at', 'hera', 'using', 'an', 'integrated', 'luminosity', 'of', '818', 'pb1', 'the', 'events', 'were', 'required', 'to', 'have', 'a', 'virtuality', 'of', 'the', 'in... | [-0.012792168731441882, 0.23717781677431937, -0.09195751518627086, 0.14848236981816004, 0.008960210138887871, -0.06554442678768863, -0.023271180337338937, 0.38957534962165075, -0.12314579272129404, -0.38527168957406555, -0.028341579905483784, -0.40255701317136566, 0.18438653034840044, 0.16245389468307922, 0.08755902518... |
706.381 | The Camassa-Holm equation as a geodesic flow for the $H^1$
right-invariant metric | The fundamental role played by the Lie groups in mechanics, and especially by
the dual space of the Lie algebra of the group and the coadjoint action are
illustrated through the Camassa-Holm equation (CH). In 1996 Misio{\l}ek
observed that CH is a geodesic flow equation on the group of diffeomorphisms,
preserving the... | nlin.SI math-ph math.MP | the fundamental role played by the lie groups in mechanics and especially by the dual space of the lie algebra of the group and the coadjoint action are illustrated through the camassaholm equation ch in 1996 misiolek observed that ch is a geodesic flow equation on the group of diffeomorphisms preserving the h1 metric ... | [['the', 'fundamental', 'role', 'played', 'by', 'the', 'lie', 'groups', 'in', 'mechanics', 'and', 'especially', 'by', 'the', 'dual', 'space', 'of', 'the', 'lie', 'algebra', 'of', 'the', 'group', 'and', 'the', 'coadjoint', 'action', 'are', 'illustrated', 'through', 'the', 'camassaholm', 'equation', 'ch', 'in', '1996', '... | [-0.19699590254145172, 0.06119891498159492, -0.09919431245563408, 0.030061588988890154, -0.11424624249697304, -0.07032517403937304, -0.05938744181050704, 0.303786033563889, -0.29986211852385447, -0.21433043679079183, 0.12526493943027722, -0.2983776985381085, -0.12294993897040303, 0.1757182364280407, -0.0870714312777496... |
706.3811 | Criticality, Scaling and Chiral Symmetry Breaking in External Magnetic
Field | We consider a D7-brane probe of $AdS_{5}\times S^5$ in the presence of pure
gauge $B$-field. The dual gauge theory is flavored Yang-Mills theory in
external magnetic field. We explore the dependence of the fermionic condensate
on the bare quark mass $m_{q}$ and study the discrete self-similar behavior of
the theory n... | hep-th | we consider a d7brane probe of ads_5times s5 in the presence of pure gauge bfield the dual gauge theory is flavored yangmills theory in external magnetic field we explore the dependence of the fermionic condensate on the bare quark mass m_q and study the discrete selfsimilar behavior of the theory near the origin of th... | [['we', 'consider', 'a', 'd7brane', 'probe', 'of', 'ads_5times', 's5', 'in', 'the', 'presence', 'of', 'pure', 'gauge', 'bfield', 'the', 'dual', 'gauge', 'theory', 'is', 'flavored', 'yangmills', 'theory', 'in', 'external', 'magnetic', 'field', 'we', 'explore', 'the', 'dependence', 'of', 'the', 'fermionic', 'condensate',... | [-0.1701955754942358, 0.26002299649651345, -0.11609871451284236, 0.09848217355650363, -0.022288202605672432, -0.07636347202820454, 0.06618062086114938, 0.2876769502746261, -0.15958948297957792, -0.2059707763785524, 0.02525765656444953, -0.27784139779048844, -0.0964126400997056, 0.06732603135421428, 0.058838983094180695... |
706.3812 | Java Components Vulnerabilities - An Experimental Classification
Targeted at the OSGi Platform | The OSGi Platform finds a growing interest in two different applications
domains: embedded systems, and applications servers. However, the security
properties of this platform are hardly studied, which is likely to hinder its
use in production systems. This is all the more important that the dynamic
aspect of OSGi-ba... | cs.CR cs.OS | the osgi platform finds a growing interest in two different applications domains embedded systems and applications servers however the security properties of this platform are hardly studied which is likely to hinder its use in production systems this is all the more important that the dynamic aspect of osgibased appli... | [['the', 'osgi', 'platform', 'finds', 'a', 'growing', 'interest', 'in', 'two', 'different', 'applications', 'domains', 'embedded', 'systems', 'and', 'applications', 'servers', 'however', 'the', 'security', 'properties', 'of', 'this', 'platform', 'are', 'hardly', 'studied', 'which', 'is', 'likely', 'to', 'hinder', 'its'... | [-0.13227824494841375, 0.004896211058367044, -0.07428370749045696, 0.0706960947099807, -0.14265356074220367, -0.16749866639396974, 0.06733055211603642, 0.384665149765455, -0.25864327353292277, -0.3036665344238281, 0.13088038253132253, -0.28600415116974287, -0.14602414452603885, 0.2184658915469689, -0.10983265192913158,... |
706.3813 | Entanglement invariant for the double Jaynes-Cummings model | We study entanglement dynamics between four qubits interacting through two
isolated Jaynes-Cummings hamiltonians, via the entanglement measure based on
the wedge product. We compare the results with similar results obtained using
bipartite concurrence resulting in what is referred to as "entanglement sudden
death". W... | quant-ph | we study entanglement dynamics between four qubits interacting through two isolated jaynescummings hamiltonians via the entanglement measure based on the wedge product we compare the results with similar results obtained using bipartite concurrence resulting in what is referred to as entanglement sudden death we find a... | [['we', 'study', 'entanglement', 'dynamics', 'between', 'four', 'qubits', 'interacting', 'through', 'two', 'isolated', 'jaynescummings', 'hamiltonians', 'via', 'the', 'entanglement', 'measure', 'based', 'on', 'the', 'wedge', 'product', 'we', 'compare', 'the', 'results', 'with', 'similar', 'results', 'obtained', 'using'... | [-0.16303381433089575, 0.22113001734018325, -0.06288663717607657, 0.05584261346918841, 0.06274229033539692, -0.19766170342142383, 0.009284325319652757, 0.35892575144767763, -0.2187310116738081, -0.23977007164309422, 0.056033078368442756, -0.3025071446100871, -0.16011152300362785, 0.1905720837103824, -0.0096326315030455... |
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