id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.3453 | Inefficient quantum walks on networks: the role of the density of states | We show by general arguments that networks whose density of states contains
few highly degenerate eigenvalues result in inefficient performances of
continuous-time quantum walks (CTQW) over these networks, while systems whose
eigenvalues all have the same degeneracy lead to very efficient transport. We
exemplify our ... | quant-ph cond-mat.stat-mech | we show by general arguments that networks whose density of states contains few highly degenerate eigenvalues result in inefficient performances of continuoustime quantum walks ctqw over these networks while systems whose eigenvalues all have the same degeneracy lead to very efficient transport we exemplify our results... | [['we', 'show', 'by', 'general', 'arguments', 'that', 'networks', 'whose', 'density', 'of', 'states', 'contains', 'few', 'highly', 'degenerate', 'eigenvalues', 'result', 'in', 'inefficient', 'performances', 'of', 'continuoustime', 'quantum', 'walks', 'ctqw', 'over', 'these', 'networks', 'while', 'systems', 'whose', 'ei... | [-0.1303640162714382, 0.14374023902928457, -0.05326048004767531, 0.09388105747858425, -0.005718570922247388, -0.19955182134161714, 0.03309121158415476, 0.440412294796922, -0.2505373016314267, -0.233844204944885, 0.11376538998507835, -0.26670299505954004, -0.21196946559788346, 0.2239215046457656, -0.041161261644069254, ... |
710.3454 | Measurement of Mass and Spin of Black Holes with QPOs | There are now four low mass X-ray binaries with black holes which show twin
resonant-like HFQPOs. Similar QPOs might have been found in Sgr A*. I review
the power spectral density distributions of the three X-ray flares and the six
NIR flares published for Sgr A* so far, in order to look for more similarities
than ju... | astro-ph | there are now four low mass xray binaries with black holes which show twin resonantlike hfqpos similar qpos might have been found in sgr a i review the power spectral density distributions of the three xray flares and the six nir flares published for sgr a so far in order to look for more similarities than just the fre... | [['there', 'are', 'now', 'four', 'low', 'mass', 'xray', 'binaries', 'with', 'black', 'holes', 'which', 'show', 'twin', 'resonantlike', 'hfqpos', 'similar', 'qpos', 'might', 'have', 'been', 'found', 'in', 'sgr', 'a', 'i', 'review', 'the', 'power', 'spectral', 'density', 'distributions', 'of', 'the', 'three', 'xray', 'fl... | [-0.10102144069864775, 0.15654508313617715, -0.0615127730258816, 0.17390236522486383, -0.08381269474803293, -0.10865865730856722, 0.04368632818207245, 0.42373156764015957, -0.12686009350996297, -0.345767682188674, 0.05215464570236535, -0.3719446511180371, -0.06355554951136713, 0.2549169435635679, -0.03932103505442003, ... |
710.3455 | Study of e+e- annihilation at low energies | The recent results of the CMD-2, SND, KLOE, and BABAR experiments on e+e-
annihilation into hadrons at low energies are reviewed.
| hep-ex | the recent results of the cmd2 snd kloe and babar experiments on ee annihilation into hadrons at low energies are reviewed | [['the', 'recent', 'results', 'of', 'the', 'cmd2', 'snd', 'kloe', 'and', 'babar', 'experiments', 'on', 'ee', 'annihilation', 'into', 'hadrons', 'at', 'low', 'energies', 'are', 'reviewed']] | [0.006781971026655464, 0.22256670717061275, -0.10599486629611679, 0.08148400272641863, -0.0425640773139007, -0.0867666279276212, -0.01523139403157291, 0.3115503371116661, -0.07786718638436425, -0.20096843686631127, -0.08645324870234444, -0.5741794584762483, 0.14997794297302053, 0.27812465000897646, 0.17051699252000876,... |
710.3456 | On an extreme two-point distribution | A bound for functional $\Delta(F)=\sup_{x\in\mathbb R}|F(x)-\Phi(x)|$ is
obtained, which is uniform for all distribution functions $F$ of random
variables with zero mean-value and unity variance. Moreover, a two-point
distribution is found, for which this bound is reached.
| math.PR | a bound for functional deltafsup_xinmathbb rfxphix is obtained which is uniform for all distribution functions f of random variables with zero meanvalue and unity variance moreover a twopoint distribution is found for which this bound is reached | [['a', 'bound', 'for', 'functional', 'deltafsup_xinmathbb', 'rfxphix', 'is', 'obtained', 'which', 'is', 'uniform', 'for', 'all', 'distribution', 'functions', 'f', 'of', 'random', 'variables', 'with', 'zero', 'meanvalue', 'and', 'unity', 'variance', 'moreover', 'a', 'twopoint', 'distribution', 'is', 'found', 'for', 'whi... | [-0.16007963908570153, 0.17443561669705168, -0.17835785674729518, 0.08880872611688184, -0.01494466650432774, -0.13382947506116968, 0.04380636985214161, 0.2958590626716614, -0.2181783384510449, -0.25401225559014295, 0.08542950523218938, -0.2601485743054322, -0.0957235153232302, 0.20052336816276822, 0.013925330766609737,... |
710.3457 | Disordered ground states in a quantum frustrated spin chain with side
chains | We study a frustrated mixed spin chain with side chains, where the spin
species and the exchange interactions are spatially varied. A nonlinear sigma
model method is formulated for this model, and a phase diagram with two
disordered spin-gap phases is obtained for typical cases. Among them we examine
the case with a ... | cond-mat.str-el cond-mat.stat-mech | we study a frustrated mixed spin chain with side chains where the spin species and the exchange interactions are spatially varied a nonlinear sigma model method is formulated for this model and a phase diagram with two disordered spingap phases is obtained for typical cases among them we examine the case with a main ch... | [['we', 'study', 'a', 'frustrated', 'mixed', 'spin', 'chain', 'with', 'side', 'chains', 'where', 'the', 'spin', 'species', 'and', 'the', 'exchange', 'interactions', 'are', 'spatially', 'varied', 'a', 'nonlinear', 'sigma', 'model', 'method', 'is', 'formulated', 'for', 'this', 'model', 'and', 'a', 'phase', 'diagram', 'wi... | [-0.17471109213807653, 0.20251658939688005, 0.009469546211120259, 0.040348747663234395, -0.0121867083599446, -0.20424934205409415, 0.045160063801126346, 0.3864234479627124, -0.24753203649608488, -0.22440650493027298, 0.08389372910864444, -0.30746467816815887, -0.10040208702493045, 0.10886851445926975, 0.101494383610164... |
710.3458 | Bayesian variable selection for high dimensional generalized linear
models: convergence rates of the fitted densities | Bayesian variable selection has gained much empirical success recently in a
variety of applications when the number $K$ of explanatory variables
$(x_1,...,x_K)$ is possibly much larger than the sample size $n$. For
generalized linear models, if most of the $x_j$'s have very small effects on
the response $y$, we show ... | math.ST stat.TH | bayesian variable selection has gained much empirical success recently in a variety of applications when the number k of explanatory variables x_1x_k is possibly much larger than the sample size n for generalized linear models if most of the x_js have very small effects on the response y we show that it is possible to ... | [['bayesian', 'variable', 'selection', 'has', 'gained', 'much', 'empirical', 'success', 'recently', 'in', 'a', 'variety', 'of', 'applications', 'when', 'the', 'number', 'k', 'of', 'explanatory', 'variables', 'x_1x_k', 'is', 'possibly', 'much', 'larger', 'than', 'the', 'sample', 'size', 'n', 'for', 'generalized', 'linea... | [-0.07499572716256571, 0.09039795213205376, -0.09781930372174058, 0.07903022140942338, -0.10362895546734509, -0.15979635280408186, 0.08982297446931431, 0.36470812066188135, -0.2787706170833157, -0.3088383788722374, 0.07817531481575353, -0.25285456118521077, -0.12225909425584963, 0.17791336379013956, -0.1189920263442062... |
710.3459 | Bounded step functions and factorial ratio sequences | We study certain step functions whose nonnegativity is related to the
integrality of sequences of ratios of factorial products. In particular, we
obtain a lower bound for the mean square of such step functions which allows us
to give a restriction on when such a factorial ratio sequence can be integral.
Additionally,... | math.NT | we study certain step functions whose nonnegativity is related to the integrality of sequences of ratios of factorial products in particular we obtain a lower bound for the mean square of such step functions which allows us to give a restriction on when such a factorial ratio sequence can be integral additionally we no... | [['we', 'study', 'certain', 'step', 'functions', 'whose', 'nonnegativity', 'is', 'related', 'to', 'the', 'integrality', 'of', 'sequences', 'of', 'ratios', 'of', 'factorial', 'products', 'in', 'particular', 'we', 'obtain', 'a', 'lower', 'bound', 'for', 'the', 'mean', 'square', 'of', 'such', 'step', 'functions', 'which',... | [-0.1226562939894696, 0.048019532142489246, -0.1250817324740417, 0.0725356824131626, -0.08815856478318121, -0.08420888096037688, 0.03609721809555071, 0.3577793227565108, -0.3104043741160157, -0.2674633373478145, 0.14235995990527567, -0.2117815839559295, -0.18532119850825632, 0.2107693221645825, -0.11606257281858813, 0.... |
710.346 | Boundary $C^*$-algebras for acylindrical groups | Let $\Delta$ be an infinite, locally finite tree with more than two ends. Let
$\Gamma<\aut(\Delta)$ be an acylindrical uniform lattice. Then the boundary
algebra $\cl A_\Gamma = C(\partial\Delta)\rtimes \Gamma$ is a simple
Cuntz-Krieger algebra whose K-theory is determined explicitly.
| math.OA math.GR | let delta be an infinite locally finite tree with more than two ends let gammaautdelta be an acylindrical uniform lattice then the boundary algebra cl a_gamma cpartialdeltartimes gamma is a simple cuntzkrieger algebra whose ktheory is determined explicitly | [['let', 'delta', 'be', 'an', 'infinite', 'locally', 'finite', 'tree', 'with', 'more', 'than', 'two', 'ends', 'let', 'gammaautdelta', 'be', 'an', 'acylindrical', 'uniform', 'lattice', 'then', 'the', 'boundary', 'algebra', 'cl', 'a_gamma', 'cpartialdeltartimes', 'gamma', 'is', 'a', 'simple', 'cuntzkrieger', 'algebra', '... | [-0.1778122410533898, 0.2835579387036786, -0.11059833695698115, 0.01453568396391347, -0.1887002423302167, -0.22649990181283405, -0.03958833891859589, 0.39161122631695533, -0.40341992903914714, -0.11981444930683614, 0.1306143596044017, -0.2575908498596012, -0.00830410596811109, 0.1852470313768006, -0.12547512484403947, ... |
710.3461 | The Frequency of Large Radius Hot and Very Hot Jupiters in omega
Centauri | We present the results of a deep, wide-field search for transiting `Hot
Jupiter (HJ)' planets in the globular cluster omega Centauri. As a result of a
25-night observing run with the ANU 40-inch telescope at Siding Spring
Observatory, a total of 109,726 stellar time series composed of 787 independent
data points were... | astro-ph | we present the results of a deep widefield search for transiting hot jupiter hj planets in the globular cluster omega centauri as a result of a 25night observing run with the anu 40inch telescope at siding spring observatory a total of 109726 stellar time series composed of 787 independent data points were produced wit... | [['we', 'present', 'the', 'results', 'of', 'a', 'deep', 'widefield', 'search', 'for', 'transiting', 'hot', 'jupiter', 'hj', 'planets', 'in', 'the', 'globular', 'cluster', 'omega', 'centauri', 'as', 'a', 'result', 'of', 'a', '25night', 'observing', 'run', 'with', 'the', 'anu', '40inch', 'telescope', 'at', 'siding', 'spr... | [-0.09763793414719653, 0.1265018123615483, -0.08136938430860664, 0.0521137644458487, -0.1292168513178458, -0.06516625776452602, 0.12045275813100166, 0.38238215342899073, -0.14244417590611183, -0.3854944232116232, 0.09750808922223111, -0.32953185334794105, -0.01146005607388116, 0.2665315932456421, -0.03876654043033585, ... |
710.3462 | Light hadron spectrum with 2+1 flavor dynamical $O(a)$-improved Wilson
quarks | We present preliminary results for the light harden spectrum in $N_f=2+1$
lattice QCD obtained with the nonperturbatively $O(a)$-improved Wilson quark
action and the Iwasaki gauge action. Simulations are carried out at
$\beta=1.90$ on a $32^3 \times 64$ lattice using the PACS-CS computer. We
employ L\"uscher's domain... | hep-lat | we present preliminary results for the light harden spectrum in n_f21 lattice qcd obtained with the nonperturbatively oaimproved wilson quark action and the iwasaki gauge action simulations are carried out at beta190 on a 323 times 64 lattice using the pacscs computer we employ luschers domaindecomposed hmc algorithm t... | [['we', 'present', 'preliminary', 'results', 'for', 'the', 'light', 'harden', 'spectrum', 'in', 'n_f21', 'lattice', 'qcd', 'obtained', 'with', 'the', 'nonperturbatively', 'oaimproved', 'wilson', 'quark', 'action', 'and', 'the', 'iwasaki', 'gauge', 'action', 'simulations', 'are', 'carried', 'out', 'at', 'beta190', 'on',... | [-0.04814948772989391, 0.29306779067320304, -0.10455697192256116, 0.05220311795849176, -0.028846587107788462, -0.07511839873179615, 0.17570428954648032, 0.46005938441625666, -0.11113625025332328, -0.29898009009637116, 0.059457049443153664, -0.3230860161794616, 0.036700393161958174, 0.14592759705348207, 0.08084514070790... |
710.3463 | Supersolid phases in the extended boson hubbard model | We present a comprehensive numerical study on the ground state phase diagram
of the two-dimensional hardcore boson extended Hubbard model with nearest
($V_1$) and next nearest neighbor ($V_2$) repulsions. In addition to the
quantum solid and superfluid phases, we report the existence of striped
supersolid and three-q... | cond-mat.str-el | we present a comprehensive numerical study on the ground state phase diagram of the twodimensional hardcore boson extended hubbard model with nearest v_1 and next nearest neighbor v_2 repulsions in addition to the quantum solid and superfluid phases we report the existence of striped supersolid and threequarter quarter... | [['we', 'present', 'a', 'comprehensive', 'numerical', 'study', 'on', 'the', 'ground', 'state', 'phase', 'diagram', 'of', 'the', 'twodimensional', 'hardcore', 'boson', 'extended', 'hubbard', 'model', 'with', 'nearest', 'v_1', 'and', 'next', 'nearest', 'neighbor', 'v_2', 'repulsions', 'in', 'addition', 'to', 'the', 'quan... | [-0.19584494567427196, 0.30167327663174975, -0.04623349863655963, 0.04727541684957319, -0.015183665564185695, -0.15162355628746904, 0.07815733911763681, 0.37774340606441625, -0.25727793283172345, -0.21125100143253803, 0.019577136286534368, -0.37605886591696425, -0.10305006772671875, 0.051256297609621755, 0.113108097220... |
710.3464 | Mathematical remarks on transcritical bifurcation in Hamiltonian systems | This article is meant as a mathematical appendix or comment on [BT]. We first
consider the notion of transcritical bifurcations of fixed points of general
area-preserving maps, and then adress some questions related to [BT] on
bifurcation in Poincar\'e maps of 2-dimensional Hamiltonian systems.
[BT] M. Brack and K.... | math.SG math.DS nlin.CD | this article is meant as a mathematical appendix or comment on bt we first consider the notion of transcritical bifurcations of fixed points of general areapreserving maps and then adress some questions related to bt on bifurcation in poincare maps of 2dimensional hamiltonian systems bt m brack and k tanaka arxiv070507... | [['this', 'article', 'is', 'meant', 'as', 'a', 'mathematical', 'appendix', 'or', 'comment', 'on', 'bt', 'we', 'first', 'consider', 'the', 'notion', 'of', 'transcritical', 'bifurcations', 'of', 'fixed', 'points', 'of', 'general', 'areapreserving', 'maps', 'and', 'then', 'adress', 'some', 'questions', 'related', 'to', 'b... | [-0.2058272512629628, 0.05811725366860628, -0.06601039597706404, 0.07525218775495887, -0.08582483075093478, -0.1772787334304303, 0.07611632317304612, 0.24927947336807846, -0.26872656950727103, -0.19000444564968347, 0.1442860517068766, -0.2815384075697511, -0.2533317711064592, 0.16477481096051633, -0.1518918607197702, 0... |
710.3465 | Critical Behavior of Disordered Systems with a Free Surface | The behavior of homogeneous and disordered systems with a free boundary is
described on the basis of group theory in the two-loop approximation directly
in three-dimensional space. The effect of the free boundary on the regime of
the bulk critical behavior is revealed. It is shown that the boundedness of the
system s... | cond-mat.stat-mech cond-mat.dis-nn | the behavior of homogeneous and disordered systems with a free boundary is described on the basis of group theory in the twoloop approximation directly in threedimensional space the effect of the free boundary on the regime of the bulk critical behavior is revealed it is shown that the boundedness of the system slightl... | [['the', 'behavior', 'of', 'homogeneous', 'and', 'disordered', 'systems', 'with', 'a', 'free', 'boundary', 'is', 'described', 'on', 'the', 'basis', 'of', 'group', 'theory', 'in', 'the', 'twoloop', 'approximation', 'directly', 'in', 'threedimensional', 'space', 'the', 'effect', 'of', 'the', 'free', 'boundary', 'on', 'th... | [-0.16384556069148376, 0.19006758170572163, -0.08853015426190242, 0.05003260346369215, 0.006344082710497519, -0.11152791220571517, 0.020654887244317625, 0.3014164295763133, -0.23213266962043502, -0.2421548399142921, 0.0898221480935771, -0.33513376387589444, -0.19637429970658987, 0.2019830189528875, 0.01971984825863996,... |
710.3466 | Bifurcation of straight-line librations | We study a class of 2-dimensional Hamiltonian systems
$H(x,y,p_x,p_y)=\frac12(p_x^2+p_y^2) +V(x,y)$ in which the plane $x$=$p_x$=0 is
invariant under the Hamiltonian flow, so that straight-line librations along
the y axis exist, and we also consider perturbations $\delta H=\delta\cdot
F(x,y,p_x,p_y)$ that preserve th... | math.SG math.DS nlin.CD | we study a class of 2dimensional hamiltonian systems hxyp_xp_yfrac12p_x2p_y2 vxy in which the plane xp_x0 is invariant under the hamiltonian flow so that straightline librations along the y axis exist and we also consider perturbations delta hdeltacdot fxyp_xp_y that preserve these librations we describe a procedure fo... | [['we', 'study', 'a', 'class', 'of', '2dimensional', 'hamiltonian', 'systems', 'hxyp_xp_yfrac12p_x2p_y2', 'vxy', 'in', 'which', 'the', 'plane', 'xp_x0', 'is', 'invariant', 'under', 'the', 'hamiltonian', 'flow', 'so', 'that', 'straightline', 'librations', 'along', 'the', 'y', 'axis', 'exist', 'and', 'we', 'also', 'consi... | [-0.20521570282289758, 0.11048163201000231, -0.07038878470969696, 0.07678961598746052, -0.044329191126356214, -0.12939076950472858, -0.00280946108008114, 0.3449557617229099, -0.28312860702862963, -0.25041763778426684, 0.10864085916788706, -0.2756674982762585, -0.19258890473671877, 0.14669236448874776, -0.03648455443423... |
710.3467 | Application of chiral perturbation theory to 2+1 flavor lattice QCD with
O(a)-improved Wilson quarks | We apply chiral perturbation theory to the pseudoscalar meson mass and decay
constant data obtained in the PACS-CS Project toward 2+1 flavor lattice QCD
simulations with the O(a)-improved Wilson quarks. We examine the existence of
chiral logarithms in the quark mass range from m_{ud}=47 MeV down to 6 MeV on a
(2.8 fm... | hep-lat | we apply chiral perturbation theory to the pseudoscalar meson mass and decay constant data obtained in the pacscs project toward 21 flavor lattice qcd simulations with the oaimproved wilson quarks we examine the existence of chiral logarithms in the quark mass range from m_ud47 mev down to 6 mev on a 28 fm3 box with th... | [['we', 'apply', 'chiral', 'perturbation', 'theory', 'to', 'the', 'pseudoscalar', 'meson', 'mass', 'and', 'decay', 'constant', 'data', 'obtained', 'in', 'the', 'pacscs', 'project', 'toward', '21', 'flavor', 'lattice', 'qcd', 'simulations', 'with', 'the', 'oaimproved', 'wilson', 'quarks', 'we', 'examine', 'the', 'existe... | [-0.09304972278850177, 0.3203413055066161, -0.04163354428343569, 0.09079758751005688, -0.029361162241106218, -0.05025709101553016, 0.1093177589664495, 0.3805535554037064, -0.13306184221483483, -0.2583814984794612, 0.05512139841890599, -0.32974738720804453, 0.035238845072704354, 0.05821836328346141, 0.09396720103495106,... |
710.3468 | Meson correlators in the epsilon-regime of two-flavor lattice QCD | We calculate the meson correlators in the $\epsilon$-regime of two-flavor
QCD. On a $16^3\times 32$ lattice with $a\sim 0.11$ fm, the lattice simulations
are performed with the dynamical overlap fermions. We reduce the sea quark mass
down to $\sim$ 3 MeV and the valence quark masses are taken in the range 1-4
MeV. Th... | hep-lat | we calculate the meson correlators in the epsilonregime of twoflavor qcd on a 163times 32 lattice with asim 011 fm the lattice simulations are performed with the dynamical overlap fermions we reduce the sea quark mass down to sim 3 mev and the valence quark masses are taken in the range 14 mev the meson correlators in ... | [['we', 'calculate', 'the', 'meson', 'correlators', 'in', 'the', 'epsilonregime', 'of', 'twoflavor', 'qcd', 'on', 'a', '163times', '32', 'lattice', 'with', 'asim', '011', 'fm', 'the', 'lattice', 'simulations', 'are', 'performed', 'with', 'the', 'dynamical', 'overlap', 'fermions', 'we', 'reduce', 'the', 'sea', 'quark', ... | [-0.10458878052886575, 0.34161387986503544, -0.05441627193009481, 0.12465491166338324, 0.026996549731411506, -0.047173271413194016, 0.10287435051403009, 0.3570658074133098, -0.11034372352063655, -0.2421686525386758, 0.015081992232007907, -0.38036135855130854, 0.03848838798934594, 0.012144801877439023, 0.143698859019204... |
710.3469 | The physics case of DAFNE-2 | We present the physics case of DAFNE-2, an $e^+e^-$ collider expected to
deliver 20-50 fb$^{-1}$ at the $\phi(1020)$ peak, and $\sim$ 5 fb$^{-1}$ in the
energy region between 1 and 2.5 GeV.
| hep-ex | we present the physics case of dafne2 an ee collider expected to deliver 2050 fb1 at the phi1020 peak and sim 5 fb1 in the energy region between 1 and 25 gev | [['we', 'present', 'the', 'physics', 'case', 'of', 'dafne2', 'an', 'ee', 'collider', 'expected', 'to', 'deliver', '2050', 'fb1', 'at', 'the', 'phi1020', 'peak', 'and', 'sim', '5', 'fb1', 'in', 'the', 'energy', 'region', 'between', '1', 'and', '25', 'gev']] | [-0.009415979504645351, 0.16216766559603368, -0.01038531712707012, 0.1724417525073213, 0.014186811002512132, -0.06057365521067573, 0.023146554549795487, 0.3725588170270766, -0.21298521925364772, -0.4322411787485884, -0.030068544013756176, -0.4593515130541017, 0.1619492813554262, 0.17300878921824117, 0.1303049927613052,... |
710.347 | Wahl's conjecture holds in odd characteristics for symplectic and
orthogonal Grassmannians | It is shown that the proof by Mehta and Parameswaran of Wahl's conjecture for
Grassmannians in positive odd characteristics also works for symplectic and
orthogonal Grassmannians.
| math.AG math.RT | it is shown that the proof by mehta and parameswaran of wahls conjecture for grassmannians in positive odd characteristics also works for symplectic and orthogonal grassmannians | [['it', 'is', 'shown', 'that', 'the', 'proof', 'by', 'mehta', 'and', 'parameswaran', 'of', 'wahls', 'conjecture', 'for', 'grassmannians', 'in', 'positive', 'odd', 'characteristics', 'also', 'works', 'for', 'symplectic', 'and', 'orthogonal', 'grassmannians']] | [-0.17700195483988723, 0.06852325768424915, -0.09301039307879713, 0.10232278105104342, -0.0919932470871852, -0.2585704094515397, -0.06574668086921939, 0.31122112240140826, -0.19841213803738356, -0.1781050359400419, 0.07214015078856252, -0.1889211211550551, -0.27752969757868695, 0.24030234127377087, -0.17747451801999256... |
710.3471 | Dual Actions for Born-Infeld and Dp-Brane Theories | Dual actions with respect to U(1) gauge fields for Born-Infeld and $Dp$-brane
theories are reexamined. Taking into account an additional condition, i.e. a
corollary to the field equation of the auxiliary metric, one obtains an
alternative dual action that does not involve the infinite power series in the
auxiliary me... | hep-th | dual actions with respect to u1 gauge fields for borninfeld and dpbrane theories are reexamined taking into account an additional condition ie a corollary to the field equation of the auxiliary metric one obtains an alternative dual action that does not involve the infinite power series in the auxiliary metric given by... | [['dual', 'actions', 'with', 'respect', 'to', 'u1', 'gauge', 'fields', 'for', 'borninfeld', 'and', 'dpbrane', 'theories', 'are', 'reexamined', 'taking', 'into', 'account', 'an', 'additional', 'condition', 'ie', 'a', 'corollary', 'to', 'the', 'field', 'equation', 'of', 'the', 'auxiliary', 'metric', 'one', 'obtains', 'an... | [-0.16301246011180096, 0.14694432719271422, -0.0802938828991469, 0.08283642026322798, -0.14344644348683028, -0.15303832679858495, -0.024586853481315334, 0.31143292011371976, -0.24853739083969387, -0.26358964138961366, 0.07458896730175435, -0.27021360106701997, -0.14891812016480954, 0.1567250669901741, -0.07434898589111... |
710.3472 | Memory effects in quantum information transmission across a Hamiltonian
dephasing channel | We study a dephasing channel with memory, modelled by a multimode environment
of oscillators. Focusing on the case of two channel uses, we show that memory
effects can enhance the amount of coherent quantum information transmitted down
the channel. We also show the Kraus representation for two channel uses.
Finally, ... | quant-ph cond-mat.mes-hall | we study a dephasing channel with memory modelled by a multimode environment of oscillators focusing on the case of two channel uses we show that memory effects can enhance the amount of coherent quantum information transmitted down the channel we also show the kraus representation for two channel uses finally we propo... | [['we', 'study', 'a', 'dephasing', 'channel', 'with', 'memory', 'modelled', 'by', 'a', 'multimode', 'environment', 'of', 'oscillators', 'focusing', 'on', 'the', 'case', 'of', 'two', 'channel', 'uses', 'we', 'show', 'that', 'memory', 'effects', 'can', 'enhance', 'the', 'amount', 'of', 'coherent', 'quantum', 'information... | [-0.21711913338213257, 0.11436139871225212, -0.08714308087347132, 0.023846652222952496, -0.03076700083064762, -0.19384672484981516, 0.10547839406750757, 0.41619744140541914, -0.27905742987764603, -0.2428725604532343, 0.08171385374964413, -0.22321169620210474, -0.16511818612431825, 0.19420587325073552, -0.09340252568169... |
710.3473 | Modelling the effects of air pollution on health using Bayesian Dynamic
Generalised Linear Models | The relationship between short-term exposure to air pollution and mortality
or morbidity has been the subject of much recent research, in which the
standard method of analysis uses Poisson linear or additive models. In this
paper we use a Bayesian dynamic generalised linear model (DGLM) to estimate
this relationship,... | stat.AP stat.ME | the relationship between shortterm exposure to air pollution and mortality or morbidity has been the subject of much recent research in which the standard method of analysis uses poisson linear or additive models in this paper we use a bayesian dynamic generalised linear model dglm to estimate this relationship which a... | [['the', 'relationship', 'between', 'shortterm', 'exposure', 'to', 'air', 'pollution', 'and', 'mortality', 'or', 'morbidity', 'has', 'been', 'the', 'subject', 'of', 'much', 'recent', 'research', 'in', 'which', 'the', 'standard', 'method', 'of', 'analysis', 'uses', 'poisson', 'linear', 'or', 'additive', 'models', 'in', ... | [-0.04201344283825228, 0.07272923532540296, -0.11115075792912717, 0.09734473408392176, -0.07783415107691737, -0.10561848066564154, 0.06861341416208623, 0.4132019326607616, -0.26732678594056924, -0.32360606718097806, 0.15936525185885866, -0.28644807056553806, -0.13949121946416462, 0.19251178829887655, -0.070065379121227... |
710.3474 | Numerical study of transport through a single impurity in a spinful
Tomonaga-Luttinger liquid | The single impurity problem in a spinful Tomonaga-Luttinger liquid is studied
numerically using path-integral Monte Carlo methods. The advantage of our
approach is that the system allows for extensive analyses of charge and spin
conductance in the non-perturbative regime. By closely examining the behavior
of conducta... | cond-mat.mes-hall | the single impurity problem in a spinful tomonagaluttinger liquid is studied numerically using pathintegral monte carlo methods the advantage of our approach is that the system allows for extensive analyses of charge and spin conductance in the nonperturbative regime by closely examining the behavior of conductances at... | [['the', 'single', 'impurity', 'problem', 'in', 'a', 'spinful', 'tomonagaluttinger', 'liquid', 'is', 'studied', 'numerically', 'using', 'pathintegral', 'monte', 'carlo', 'methods', 'the', 'advantage', 'of', 'our', 'approach', 'is', 'that', 'the', 'system', 'allows', 'for', 'extensive', 'analyses', 'of', 'charge', 'and'... | [-0.13986228994598102, 0.15120101936465827, -0.11902784533523339, 0.07378215779709615, -0.029589108379625285, -0.1413605997309938, 0.08369577783907865, 0.3571557931486189, -0.2649756734659944, -0.2597081268162809, 0.07219212493193311, -0.3009644102105669, -0.1325827452216606, 0.17922938192128132, 0.006745481646470147, ... |
710.3475 | Can distributed delays perfectly stabilize dynamical networks? | Signal transmission delays tend to destabilize dynamical networks leading to
oscillation, but their dispersion contributes oppositely toward stabilization.
We analyze an integro-differential equation that describes the collective
dynamics of a neural network with distributed signal delays. With the gamma
distributed ... | cond-mat.dis-nn nlin.AO | signal transmission delays tend to destabilize dynamical networks leading to oscillation but their dispersion contributes oppositely toward stabilization we analyze an integrodifferential equation that describes the collective dynamics of a neural network with distributed signal delays with the gamma distributed delays... | [['signal', 'transmission', 'delays', 'tend', 'to', 'destabilize', 'dynamical', 'networks', 'leading', 'to', 'oscillation', 'but', 'their', 'dispersion', 'contributes', 'oppositely', 'toward', 'stabilization', 'we', 'analyze', 'an', 'integrodifferential', 'equation', 'that', 'describes', 'the', 'collective', 'dynamics'... | [-0.22974224305466917, 0.18752659287304432, -0.10237067608306041, 0.04543758630274962, -0.03912004834423081, -0.2150401804037989, 0.019416343587904405, 0.38230344975510466, -0.312062216982341, -0.2761827318642575, 0.08345489053933236, -0.29871009156489986, -0.169179947509502, 0.15344700257843122, -0.0561041172940093, 0... |
710.3476 | Multi-particle entanglement and generalized N-particle teleportation
using quantum statistical correlations | Construction of multi-particle entangled states and direct teleportation of
N-(spin 1/2) particles are important areas of quantum information processing. A
number of different schemes which have been presented already, address the
problem through controlled teleportation. In this article, a criterion based on
standar... | quant-ph | construction of multiparticle entangled states and direct teleportation of nspin 12 particles are important areas of quantum information processing a number of different schemes which have been presented already address the problem through controlled teleportation in this article a criterion based on standard quantum s... | [['construction', 'of', 'multiparticle', 'entangled', 'states', 'and', 'direct', 'teleportation', 'of', 'nspin', '12', 'particles', 'are', 'important', 'areas', 'of', 'quantum', 'information', 'processing', 'a', 'number', 'of', 'different', 'schemes', 'which', 'have', 'been', 'presented', 'already', 'address', 'the', '... | [-0.11729861496158106, 0.2240641412234096, -0.12040575112054205, 0.09307492701842895, 0.02474840428153782, -0.19291180987518441, 0.030948308083917134, 0.3505277202181194, -0.240599164577282, -0.27744466599238954, 0.07004978260045629, -0.24880389114436896, -0.09740656802592718, 0.24906456932101562, -0.03843483898140814,... |
710.3477 | The poorly constrained cluster disruption time-scale in the Large
Magellanic Cloud | We use Monte-Carlo simulations, combined with homogeneously determined age
and mass distributions based on multi-wavelength photometry, to constrain the
cluster formation history and the rate of bound cluster disruption in the Large
Magellanic Cloud (LMC) cluster system. We evolve synthetic star cluster systems
forme... | astro-ph | we use montecarlo simulations combined with homogeneously determined age and mass distributions based on multiwavelength photometry to constrain the cluster formation history and the rate of bound cluster disruption in the large magellanic cloud lmc cluster system we evolve synthetic star cluster systems formed with a ... | [['we', 'use', 'montecarlo', 'simulations', 'combined', 'with', 'homogeneously', 'determined', 'age', 'and', 'mass', 'distributions', 'based', 'on', 'multiwavelength', 'photometry', 'to', 'constrain', 'the', 'cluster', 'formation', 'history', 'and', 'the', 'rate', 'of', 'bound', 'cluster', 'disruption', 'in', 'the', 'l... | [-0.06042551878118545, 0.1311421140562743, -0.1170252048635741, 0.12608777647140346, -0.04194705002388113, -0.06518451537136728, 0.09816558787679898, 0.40287646096088797, -0.19643057189421184, -0.3686851735902607, 0.03545077671700356, -0.2417616071885566, -0.00042146093301691066, 0.17477533369264583, -0.036174915894859... |
710.3478 | Nonparametric estimation of a point-spread function in multivariate
problems | The removal of blur from a signal, in the presence of noise, is readily
accomplished if the blur can be described in precise mathematical terms.
However, there is growing interest in problems where the extent of blur is
known only approximately, for example in terms of a blur function which depends
on unknown paramet... | math.ST stat.TH | the removal of blur from a signal in the presence of noise is readily accomplished if the blur can be described in precise mathematical terms however there is growing interest in problems where the extent of blur is known only approximately for example in terms of a blur function which depends on unknown parameters tha... | [['the', 'removal', 'of', 'blur', 'from', 'a', 'signal', 'in', 'the', 'presence', 'of', 'noise', 'is', 'readily', 'accomplished', 'if', 'the', 'blur', 'can', 'be', 'described', 'in', 'precise', 'mathematical', 'terms', 'however', 'there', 'is', 'growing', 'interest', 'in', 'problems', 'where', 'the', 'extent', 'of', 'b... | [-0.0558817164335374, 0.03359415457242802, -0.11011307296446628, 0.06297008858786689, -0.10151534303505387, -0.13918713032423208, 0.025727684726654036, 0.4358018897692091, -0.2793475203849893, -0.29506396057808565, 0.16605904922536058, -0.21316308954264968, -0.1983714369073924, 0.24113035703388352, -0.1699136602666436,... |
710.3479 | Constrained Gauge Fields from Spontaneous Lorentz Violation | Spontaneous Lorentz violation realized through a nonlinear vector field
constraint of the type $A_{\mu}A^{\mu}=M^{2}$ ($M$ is the proposed scale for
Lorentz violation) is shown to generate massless vector Goldstone bosons,
gauging the starting global internal symmetries in arbitrary relativistically
invariant theorie... | hep-th hep-ph | spontaneous lorentz violation realized through a nonlinear vector field constraint of the type a_muamum2 m is the proposed scale for lorentz violation is shown to generate massless vector goldstone bosons gauging the starting global internal symmetries in arbitrary relativistically invariant theories the gauge invarian... | [['spontaneous', 'lorentz', 'violation', 'realized', 'through', 'a', 'nonlinear', 'vector', 'field', 'constraint', 'of', 'the', 'type', 'a_muamum2', 'm', 'is', 'the', 'proposed', 'scale', 'for', 'lorentz', 'violation', 'is', 'shown', 'to', 'generate', 'massless', 'vector', 'goldstone', 'bosons', 'gauging', 'the', 'star... | [-0.14926094972636877, 0.2968108188507364, -0.04420228123828863, 0.10813599630660208, -0.13993570605093766, -0.18314759028964214, 0.006967886303457777, 0.2826621432938033, -0.2243703754571905, -0.26315101724756446, 0.047683839918313396, -0.2086498707696889, -0.10710599000782431, 0.08522683777919614, -0.0224294417930192... |
710.348 | Penrose Limits vs String Expansions | We analyse the relation between two a priori quite different expansions of
the string equations of motion and constraints in a general curved background,
namely one based on the covariant Penrose-Fermi expansion of the metric
G_{\mu\nu} around a Penrose limit plane wave associated to a null geodesic
\gamma, and the o... | hep-th gr-qc | we analyse the relation between two a priori quite different expansions of the string equations of motion and constraints in a general curved background namely one based on the covariant penrosefermi expansion of the metric g_munu around a penrose limit plane wave associated to a null geodesic gamma and the other on th... | [['we', 'analyse', 'the', 'relation', 'between', 'two', 'a', 'priori', 'quite', 'different', 'expansions', 'of', 'the', 'string', 'equations', 'of', 'motion', 'and', 'constraints', 'in', 'a', 'general', 'curved', 'background', 'namely', 'one', 'based', 'on', 'the', 'covariant', 'penrosefermi', 'expansion', 'of', 'the',... | [-0.17863287973006703, 0.12824217692398318, -0.10505045557302006, 0.12424372964492325, -0.15101724654405238, -0.09968996562001949, 0.014823156327925087, 0.3215821286591377, -0.2241558183257298, -0.2219658382700046, 0.05388392741375124, -0.30061408656633853, -0.13171006064059326, 0.1518723739527207, 0.000346838344835280... |
710.3481 | Holomorphic Sobolev spaces, Hermite ans special Hermite semigroups and a
Paley-Wiener theorem for the windowed Fourier transform | The images of Hermite and Laguerre Sobolev spaces under the Hermite and
special Hermite semigroups (respectively) are characterised. These are used to
characterise the Schwartz class of rapidly decreasing functions. The image of
the space of all tempered distributions is also considered and a Paley-Wiener
theorem for... | math.FA | the images of hermite and laguerre sobolev spaces under the hermite and special hermite semigroups respectively are characterised these are used to characterise the schwartz class of rapidly decreasing functions the image of the space of all tempered distributions is also considered and a paleywiener theorem for the wi... | [['the', 'images', 'of', 'hermite', 'and', 'laguerre', 'sobolev', 'spaces', 'under', 'the', 'hermite', 'and', 'special', 'hermite', 'semigroups', 'respectively', 'are', 'characterised', 'these', 'are', 'used', 'to', 'characterise', 'the', 'schwartz', 'class', 'of', 'rapidly', 'decreasing', 'functions', 'the', 'image', ... | [-0.05757952333902413, 0.111960505223218, -0.09783259749342248, 0.1822070760239478, -0.06587679916114178, -0.06798427721995087, -0.06656713052740637, 0.4193746166409187, -0.33494887922732336, -0.11181332627838513, 0.14190632896058542, -0.24765522551793112, -0.11545076418035435, 0.2666581761583967, -0.12083700631376144,... |
710.3482 | A generalization of the Ginzburg-Landau theory to p-wave superconductors | We succeed to build up a straightforward theoretical model for spin-triplet
p-wave superconductors by introducing in Ginzburg-Landau theory a second order
parameter and a suitable interaction between the two mean fields.
| cond-mat.supr-con hep-ph | we succeed to build up a straightforward theoretical model for spintriplet pwave superconductors by introducing in ginzburglandau theory a second order parameter and a suitable interaction between the two mean fields | [['we', 'succeed', 'to', 'build', 'up', 'a', 'straightforward', 'theoretical', 'model', 'for', 'spintriplet', 'pwave', 'superconductors', 'by', 'introducing', 'in', 'ginzburglandau', 'theory', 'a', 'second', 'order', 'parameter', 'and', 'a', 'suitable', 'interaction', 'between', 'the', 'two', 'mean', 'fields']] | [-0.18727901062717842, 0.18695171444766945, -0.0779408140768928, 0.11748230301084057, -0.12975565049677126, -0.18711205609443207, 0.12742856036375969, 0.3437226201077142, -0.20536030792901594, -0.29813254991125676, -0.06353767166635202, -0.2567289882609921, -0.11667016109511737, 0.13100795302870533, 0.06747408100073377... |
710.3483 | On Dimensional Analysis, Redundancy in set of fundamental quantities and
Proposal of a New Set | Inclusion of redundant fundamental quantities in SI system has resulted in
lot of ambiguities and confusion in modern theories. The incompatibilities
between the existing theories can possibly be due to incorrect assumption of
fundamental quantities and existence of newer fundamental quantities. This
paper is an atte... | physics.gen-ph | inclusion of redundant fundamental quantities in si system has resulted in lot of ambiguities and confusion in modern theories the incompatibilities between the existing theories can possibly be due to incorrect assumption of fundamental quantities and existence of newer fundamental quantities this paper is an attempt ... | [['inclusion', 'of', 'redundant', 'fundamental', 'quantities', 'in', 'si', 'system', 'has', 'resulted', 'in', 'lot', 'of', 'ambiguities', 'and', 'confusion', 'in', 'modern', 'theories', 'the', 'incompatibilities', 'between', 'the', 'existing', 'theories', 'can', 'possibly', 'be', 'due', 'to', 'incorrect', 'assumption',... | [-0.13230273368006404, 0.07105923351826443, -0.06857723404625149, 0.049936087854263005, -0.08147759351202033, -0.12119887105443261, 0.06978505355602299, 0.3218215716325424, -0.30773965358508354, -0.31721846442105195, 0.07562288161028516, -0.25038411753026374, -0.162565467460081, 0.21218905091095208, -0.1052466354191754... |
710.3484 | Hidden multiferroic order in graphene zigzag ribbons | The insulating magnetic phase in graphene zigzag ribbons, predicted both by
density functional and mean field Hubbard model calculations, is described
without additional approximations with a BCS wave function of two phase-locked
condensates of spin-polarized electron-hole pairs. The associated order
parameter is the... | cond-mat.str-el cond-mat.mes-hall | the insulating magnetic phase in graphene zigzag ribbons predicted both by density functional and mean field hubbard model calculations is described without additional approximations with a bcs wave function of two phaselocked condensates of spinpolarized electronhole pairs the associated order parameter is the spin di... | [['the', 'insulating', 'magnetic', 'phase', 'in', 'graphene', 'zigzag', 'ribbons', 'predicted', 'both', 'by', 'density', 'functional', 'and', 'mean', 'field', 'hubbard', 'model', 'calculations', 'is', 'described', 'without', 'additional', 'approximations', 'with', 'a', 'bcs', 'wave', 'function', 'of', 'two', 'phaselock... | [-0.2334413130789302, 0.21635851682012164, -0.008308064175612662, 0.08106437251702774, -0.02807627042936876, -0.11336549923776887, 0.059856481568584606, 0.41432813308093436, -0.22369444739550007, -0.28998054156274816, -0.0504130614924158, -0.3127992270232806, -0.10104928878244272, 0.11017345258597891, 0.094087700687110... |
710.3485 | Symmetry of $osp(m|n)$ spin Calogero-Sutherland models | We introduce osp(m|n) spin Calogero-Sutherland models and find that the
models have the symmetry of osp(m|n) half-loop algebra or Yangian of osp(m|n)
if and only if the coupling constant of the model equals to 2/(m-n-4).
| nlin.SI | we introduce ospmn spin calogerosutherland models and find that the models have the symmetry of ospmn halfloop algebra or yangian of ospmn if and only if the coupling constant of the model equals to 2mn4 | [['we', 'introduce', 'ospmn', 'spin', 'calogerosutherland', 'models', 'and', 'find', 'that', 'the', 'models', 'have', 'the', 'symmetry', 'of', 'ospmn', 'halfloop', 'algebra', 'or', 'yangian', 'of', 'ospmn', 'if', 'and', 'only', 'if', 'the', 'coupling', 'constant', 'of', 'the', 'model', 'equals', 'to', '2mn4']] | [-0.13491101595847046, 0.1718399108058828, -0.015567477518583046, 0.016201926148770487, -0.08514589147970957, -0.23042838028906024, -0.02425514588899472, 0.34771809989915176, -0.288345273145858, -0.22254061271600864, 0.1136431938776856, -0.24932948757401285, -0.1602642814806827, 0.10253908376976409, -0.0078221058527774... |
710.3486 | Smooth crossing of $w_{\Lambda} = -1$ line in a single scalar field
model | Smooth double crossing of the phantom divide line $w_{\Lambda}=-1$ has been
found possible with a single minimally coupled scalar field for the most simple
form of generalized k-essence cosmological model, in the presence of background
cold dark matter. Such crossing is a sufficiently late time transient phenomena
an... | astro-ph | smooth double crossing of the phantom divide line w_lambda1 has been found possible with a single minimally coupled scalar field for the most simple form of generalized kessence cosmological model in the presence of background cold dark matter such crossing is a sufficiently late time transient phenomena and does not h... | [['smooth', 'double', 'crossing', 'of', 'the', 'phantom', 'divide', 'line', 'w_lambda1', 'has', 'been', 'found', 'possible', 'with', 'a', 'single', 'minimally', 'coupled', 'scalar', 'field', 'for', 'the', 'most', 'simple', 'form', 'of', 'generalized', 'kessence', 'cosmological', 'model', 'in', 'the', 'presence', 'of', ... | [-0.15443329448990645, 0.14005815574071473, -0.11938473854765848, 0.0754417609531191, -0.15744864869931782, -0.22882840604762789, -0.08964049869596406, 0.300719012816747, -0.1663716103885909, -0.3028025202220306, 0.024318844293399405, -0.2300932902187385, -0.12027064217599454, 0.15583104412157642, 0.0032894456569381334... |
710.3487 | Decoherence of nuclear spins due to direct dipole-dipole interactions
probed by resistively detected nuclear magnetic resonance | We study decoherence of nuclear spins in a GaAs quantum well structure using
resistively detected nuclear magnetic resonance. The transverse decoherence
time T2 of 75As nuclei is estimated from Rabi-type coherent oscillations as
well as by using spin-echo techniques. By analyzing T2 obtained by decoupling
techniques,... | cond-mat.mes-hall | we study decoherence of nuclear spins in a gaas quantum well structure using resistively detected nuclear magnetic resonance the transverse decoherence time t2 of 75as nuclei is estimated from rabitype coherent oscillations as well as by using spinecho techniques by analyzing t2 obtained by decoupling techniques we ext... | [['we', 'study', 'decoherence', 'of', 'nuclear', 'spins', 'in', 'a', 'gaas', 'quantum', 'well', 'structure', 'using', 'resistively', 'detected', 'nuclear', 'magnetic', 'resonance', 'the', 'transverse', 'decoherence', 'time', 't2', 'of', '75as', 'nuclei', 'is', 'estimated', 'from', 'rabitype', 'coherent', 'oscillations'... | [-0.14813507902859288, 0.2331083795219493, -0.02430785621041338, 0.0882260841811358, 0.024545414843643556, -0.13151150160572594, 0.012387343609442164, 0.4177091925621334, -0.24582615708744135, -0.29587504935610776, -0.009705083322419662, -0.28315209751628867, -0.09658764342241215, 0.2432642817906471, 0.0783547392594769... |
710.3488 | Microwave vortex dynamics in Tl-2212 thin films | We present measurements of the effective surface impedance changes due to a
static magnetic field, $\Delta Z(H,T)=\Delta R(H,T)+\rmi \Delta X(H,T)$, in a
Tl-2212 thin film with $T_c>$ 103 K, grown on a CeO$_2$ buffered sapphire
substrate. Measurements were performed through a dielectric resonator operating
at 47.7 GH... | cond-mat.supr-con | we present measurements of the effective surface impedance changes due to a static magnetic field delta zhtdelta rhtrmi delta xht in a tl2212 thin film with t_c 103 k grown on a ceo_2 buffered sapphire substrate measurements were performed through a dielectric resonator operating at 477 ghz for temperatures 60 kleq tt_... | [['we', 'present', 'measurements', 'of', 'the', 'effective', 'surface', 'impedance', 'changes', 'due', 'to', 'a', 'static', 'magnetic', 'field', 'delta', 'zhtdelta', 'rhtrmi', 'delta', 'xht', 'in', 'a', 'tl2212', 'thin', 'film', 'with', 't_c', '103', 'k', 'grown', 'on', 'a', 'ceo_2', 'buffered', 'sapphire', 'substrate'... | [-0.1717339725792408, 0.20065013690943098, -0.023384329531607885, -0.00014973618622337069, -0.045660902905677044, -0.1265877249517611, 0.07369662724036191, 0.3980923992927585, -0.22857306198882205, -0.35133249741313716, 0.05800715371775108, -0.280223465744223, -0.05026230106928519, 0.20527545290999114, 0.01663321244330... |
710.3489 | Misssing experiments in relativity and gravity | The proposal is submitted for the measurement of the relativistic length
contraction using the nanoscopic dumbbell moving in LHC or ILC. Some paradoxes
concerning the length contraction and simultaneity are discussed. The dynamical
states of rods and strings accelerated by the gravitational field and
non-gravitationa... | physics.gen-ph | the proposal is submitted for the measurement of the relativistic length contraction using the nanoscopic dumbbell moving in lhc or ilc some paradoxes concerning the length contraction and simultaneity are discussed the dynamical states of rods and strings accelerated by the gravitational field and nongravitational fie... | [['the', 'proposal', 'is', 'submitted', 'for', 'the', 'measurement', 'of', 'the', 'relativistic', 'length', 'contraction', 'using', 'the', 'nanoscopic', 'dumbbell', 'moving', 'in', 'lhc', 'or', 'ilc', 'some', 'paradoxes', 'concerning', 'the', 'length', 'contraction', 'and', 'simultaneity', 'are', 'discussed', 'the', 'd... | [-0.13921175105807682, 0.23532532140612603, -0.04842413788195699, 0.07424967814857761, -0.047140292649467785, -0.15946633830200882, -0.08688342672966731, 0.3586734485129515, -0.2708825417732199, -0.2590337944527467, 0.05528920932207257, -0.29261529316194357, 0.0003629196776698033, 0.19718590785749257, 0.023330189709862... |
710.349 | Minkowski space structure of the Higgs potential in 2HDM: II. Minima,
symmetries, and topology | We continue to explore the consequences of the recently discovered Minkowski
space structure of the Higgs potential in the two-Higgs-doublet model. Here, we
focus on the vacuum properties. The search for extrema of the Higgs potential
is reformulated in terms of 3-quadrics in the 3+1-dimensional Minkowski space.
We p... | hep-ph hep-th | we continue to explore the consequences of the recently discovered minkowski space structure of the higgs potential in the twohiggsdoublet model here we focus on the vacuum properties the search for extrema of the higgs potential is reformulated in terms of 3quadrics in the 31dimensional minkowski space we prove that 2... | [['we', 'continue', 'to', 'explore', 'the', 'consequences', 'of', 'the', 'recently', 'discovered', 'minkowski', 'space', 'structure', 'of', 'the', 'higgs', 'potential', 'in', 'the', 'twohiggsdoublet', 'model', 'here', 'we', 'focus', 'on', 'the', 'vacuum', 'properties', 'the', 'search', 'for', 'extrema', 'of', 'the', 'h... | [-0.1552460437698258, 0.14683081044489119, -0.0866065597655172, 0.15162517351365018, -0.113227484588567, -0.10500457405677846, 0.05321422206540393, 0.3261388234065798, -0.22589122731254524, -0.23557521959241384, 0.0685103129919889, -0.21715333368868017, -0.1535363998900876, 0.15485735396400857, -0.030379179713881422, 0... |
710.3491 | A ridge-parameter approach to deconvolution | Kernel methods for deconvolution have attractive features, and prevail in the
literature. However, they have disadvantages, which include the fact that they
are usually suitable only for cases where the error distribution is infinitely
supported and its characteristic function does not ever vanish. Even in these
sett... | math.ST stat.TH | kernel methods for deconvolution have attractive features and prevail in the literature however they have disadvantages which include the fact that they are usually suitable only for cases where the error distribution is infinitely supported and its characteristic function does not ever vanish even in these settings op... | [['kernel', 'methods', 'for', 'deconvolution', 'have', 'attractive', 'features', 'and', 'prevail', 'in', 'the', 'literature', 'however', 'they', 'have', 'disadvantages', 'which', 'include', 'the', 'fact', 'that', 'they', 'are', 'usually', 'suitable', 'only', 'for', 'cases', 'where', 'the', 'error', 'distribution', 'is'... | [-0.062206177539621474, 0.053164731123293126, -0.11275876232204919, 0.10964166317036018, -0.0869660170596912, -0.16513351774741467, 0.020045272783865056, 0.46300578521604235, -0.2716480060414484, -0.2672338357182048, 0.1373105266631799, -0.20572399526028662, -0.1349513512335929, 0.20041220775947424, -0.0978227584153836... |
710.3492 | Global Mixed Periods and local Klyachko models for the general linear
group | We show that every irreducible representation in the discrete automorphic
spectrum of GL(n) admits a non vanishing mixed (Whittaker-symplectic) period
integral. The analog local problem is a study of models first considered by
Klyachko over a finite field. Locally, we show that for a p-adic field F every
irreducible,... | math.RT math.NT | we show that every irreducible representation in the discrete automorphic spectrum of gln admits a non vanishing mixed whittakersymplectic period integral the analog local problem is a study of models first considered by klyachko over a finite field locally we show that for a padic field f every irreducible unitary rep... | [['we', 'show', 'that', 'every', 'irreducible', 'representation', 'in', 'the', 'discrete', 'automorphic', 'spectrum', 'of', 'gln', 'admits', 'a', 'non', 'vanishing', 'mixed', 'whittakersymplectic', 'period', 'integral', 'the', 'analog', 'local', 'problem', 'is', 'a', 'study', 'of', 'models', 'first', 'considered', 'by'... | [-0.24135927262250334, 0.09858484263116095, -0.2152782556866961, 0.05365690899322674, -0.07486935003128435, -0.12529845235569934, -0.042852915416006, 0.3212140837463916, -0.29605172561215504, -0.12508158798196486, 0.0778423220680062, -0.1854942203831992, -0.194572159854163, 0.19810448729549535, -0.08409727961822812, -0... |
710.3493 | Small value probabilities via the branching tree heuristic | In the first part of this paper we give easy and intuitive proofs for the
small value probabilities of the martingale limit of a supercritical
Galton-Watson process in both the Schr\"oder and the B\"ottcher case. These
results are well-known, but the most cited proofs rely on generating function
arguments which are h... | math.PR | in the first part of this paper we give easy and intuitive proofs for the small value probabilities of the martingale limit of a supercritical galtonwatson process in both the schroder and the bottcher case these results are wellknown but the most cited proofs rely on generating function arguments which are hard to tra... | [['in', 'the', 'first', 'part', 'of', 'this', 'paper', 'we', 'give', 'easy', 'and', 'intuitive', 'proofs', 'for', 'the', 'small', 'value', 'probabilities', 'of', 'the', 'martingale', 'limit', 'of', 'a', 'supercritical', 'galtonwatson', 'process', 'in', 'both', 'the', 'schroder', 'and', 'the', 'bottcher', 'case', 'these... | [-0.08585805793981101, 0.07538188323010936, -0.07449299927081979, 0.10267495453976344, -0.06876920710170739, -0.10074430515299339, 0.07326388545027983, 0.3533157032032154, -0.2799405929062663, -0.2947303923010303, 0.13292264294598186, -0.24116017772374967, -0.13256163251782327, 0.2191686277061276, -0.10733431744748693,... |
710.3494 | Vector bundles on Hirzebruch surfaces whose twists by a non-ample line
bundle have natural cohomology | Here we study vector bundles $E$ on the Hirzebruch surface $F_e$ such that
their twists by a spanned, but not ample, line bundle $M = \mathcal
{O}_{F_e}(h+ef)$ have natural cohomology, i.e. $h^0(F_e,E(tM)) >0$ implies
$h^1(F_e,E(tM)) = 0$.
| math.AG | here we study vector bundles e on the hirzebruch surface f_e such that their twists by a spanned but not ample line bundle m mathcal o_f_ehef have natural cohomology ie h0f_eetm 0 implies h1f_eetm 0 | [['here', 'we', 'study', 'vector', 'bundles', 'e', 'on', 'the', 'hirzebruch', 'surface', 'f_e', 'such', 'that', 'their', 'twists', 'by', 'a', 'spanned', 'but', 'not', 'ample', 'line', 'bundle', 'm', 'mathcal', 'o_f_ehef', 'have', 'natural', 'cohomology', 'ie', 'h0f_eetm', '0', 'implies', 'h1f_eetm', '0']] | [-0.2797969098537578, 0.11499654337785614, -0.005160424625501037, 0.03890138253336772, -0.11682833128725179, -0.2123573543940438, 0.0029517113871406764, 0.4073237937409431, -0.28820949036162347, -0.18091166636440903, 0.06772207350877579, -0.2420199466869235, -0.15189457952510566, 0.16714537986990763, -0.095057065362198... |
710.3495 | Novel features of the energy momentum tensor of a Casimir apparatus in a
weak gravitational field | The influence of the gravity acceleration on the regularized energy-momentum
tensor of the quantized electromagnetic field between two plane parallel
conducting plates is derived. A perturbative expansion, to first order in the
constant acceleration parameter, of the Green functions involved and of the
energy-momentu... | hep-th | the influence of the gravity acceleration on the regularized energymomentum tensor of the quantized electromagnetic field between two plane parallel conducting plates is derived a perturbative expansion to first order in the constant acceleration parameter of the green functions involved and of the energymomentum tenso... | [['the', 'influence', 'of', 'the', 'gravity', 'acceleration', 'on', 'the', 'regularized', 'energymomentum', 'tensor', 'of', 'the', 'quantized', 'electromagnetic', 'field', 'between', 'two', 'plane', 'parallel', 'conducting', 'plates', 'is', 'derived', 'a', 'perturbative', 'expansion', 'to', 'first', 'order', 'in', 'the... | [-0.23300119547517775, 0.15724239801056683, -0.08867953254634307, 0.062220605114513695, -0.1422888820751622, -0.052342772606708526, -0.07158840111353332, 0.3238287667789134, -0.2498160027898848, -0.2319833526853472, 0.002214725075949294, -0.24109059877486694, -0.12917882033313313, 0.10479209357355204, 0.066544543680114... |
710.3496 | Use and misuse of ChPT in the heavy-light systems | We discuss the range of validity of ChPT when applied to the systems of
heavy-light mesons. Having in mind the recent experimental evidence according
to which the heavy-light scalar and axial states are closer to the ground
states than anticipated, we revisited the prediction for the chiral behavior of
the B-Bbar mix... | hep-lat hep-ph | we discuss the range of validity of chpt when applied to the systems of heavylight mesons having in mind the recent experimental evidence according to which the heavylight scalar and axial states are closer to the ground states than anticipated we revisited the prediction for the chiral behavior of the bbbar mixing amp... | [['we', 'discuss', 'the', 'range', 'of', 'validity', 'of', 'chpt', 'when', 'applied', 'to', 'the', 'systems', 'of', 'heavylight', 'mesons', 'having', 'in', 'mind', 'the', 'recent', 'experimental', 'evidence', 'according', 'to', 'which', 'the', 'heavylight', 'scalar', 'and', 'axial', 'states', 'are', 'closer', 'to', 'th... | [-0.07175225407357917, 0.26760301987093144, -0.06738473712786577, 0.1542032374369464, -0.025848569330014642, -0.11013854575478507, 0.07180477077326247, 0.3411648702089682, -0.14663377951631565, -0.24850670113192716, 0.03910443144548286, -0.3165338484584603, -0.006856440577144159, 0.13870068356032192, 0.0602609565959646... |
710.3497 | Applicability of Boussinesq approximation in a turbulent fluid with
constant properties | The equations of motion describing buoyant fluids are often simplified using
a set of approximations proposed by J. Boussinesq one century ago. To resume,
they consist in assuming constant fluid properties, incompressibility and
conservation of calories during heat transport. Assuming fulfilment of the
first requirem... | physics.class-ph physics.flu-dyn | the equations of motion describing buoyant fluids are often simplified using a set of approximations proposed by j boussinesq one century ago to resume they consist in assuming constant fluid properties incompressibility and conservation of calories during heat transport assuming fulfilment of the first requirement con... | [['the', 'equations', 'of', 'motion', 'describing', 'buoyant', 'fluids', 'are', 'often', 'simplified', 'using', 'a', 'set', 'of', 'approximations', 'proposed', 'by', 'j', 'boussinesq', 'one', 'century', 'ago', 'to', 'resume', 'they', 'consist', 'in', 'assuming', 'constant', 'fluid', 'properties', 'incompressibility', '... | [-0.1454851624341551, 0.18673430607984903, -0.06472215080572832, 0.04059615044062522, -0.04382241643077441, -0.12143128513898178, 0.042398064114397095, 0.28758046190715697, -0.2722266223907218, -0.32754572925688785, 0.10542678404610308, -0.26708020794066106, -0.06875561407297223, 0.1846945249229652, -0.0049577664494705... |
710.3498 | B_s Mixing and B Hadron Lifetimes at CDF | We present the CDF results using 1.0 fb^{-1} of data on the mixing frequency
measurement in the B_s system and the lifetime measurements of several B
hadrons. We obtain \Delta m_s=17.77 +- 0.1 +- 0.07 ps^{-1} and
c\tau(\Lambda_b)=473.8 +- 23.1 +- 3.5 \mu m. The later one is more than 3 sigma
above the world average, ... | hep-ex | we present the cdf results using 10 fb1 of data on the mixing frequency measurement in the b_s system and the lifetime measurements of several b hadrons we obtain delta m_s1777 01 007 ps1 and ctaulambda_b4738 231 35 mu m the later one is more than 3 sigma above the world average but in reasonable agreement with hqe cal... | [['we', 'present', 'the', 'cdf', 'results', 'using', '10', 'fb1', 'of', 'data', 'on', 'the', 'mixing', 'frequency', 'measurement', 'in', 'the', 'b_s', 'system', 'and', 'the', 'lifetime', 'measurements', 'of', 'several', 'b', 'hadrons', 'we', 'obtain', 'delta', 'm_s1777', '01', '007', 'ps1', 'and', 'ctaulambda_b4738', '... | [-0.10780058706612244, 0.16886610920916786, -0.03840771188403953, 0.06710538004418802, 0.007488087113750608, -0.10794154414090149, 0.118042450328766, 0.34914291871450187, -0.15161904855222816, -0.36777897546754074, 0.06783135578019969, -0.38842691673913543, 0.043342037878015584, 0.1814445460035482, 0.03356816015091904,... |
710.3499 | Ultraviolet observations of the X-ray photoionized wind of Cygnus X-1
during X-ray soft/high state | (Shortened) Ultraviolet observations of the black hole X-ray binary Cygnus
X-1 were obtained using the STIS on HSTubble. We detect P Cygni line features
show strong, broad absorption components when the X-ray source is behind the
companion star and noticeably weaker absorption when the X-ray source is
between us and ... | astro-ph | shortened ultraviolet observations of the black hole xray binary cygnus x1 were obtained using the stis on hstubble we detect p cygni line features show strong broad absorption components when the xray source is behind the companion star and noticeably weaker absorption when the xray source is between us and the compan... | [['shortened', 'ultraviolet', 'observations', 'of', 'the', 'black', 'hole', 'xray', 'binary', 'cygnus', 'x1', 'were', 'obtained', 'using', 'the', 'stis', 'on', 'hstubble', 'we', 'detect', 'p', 'cygni', 'line', 'features', 'show', 'strong', 'broad', 'absorption', 'components', 'when', 'the', 'xray', 'source', 'is', 'beh... | [-0.04640795663484217, 0.07471691778475287, -0.05615060899942888, 0.10644591577536887, -0.09647474838702967, -0.1604667795031811, 0.052884057333523575, 0.44091404738337403, -0.1746169626674582, -0.3301028483218015, 0.0831127364465948, -0.3228105273064828, 0.018835661155254008, 0.25271141680070397, -0.04869069906470196,... |
710.35 | Heat Flow in Classical and Quantum Systems and Thermal Rectification | The understanding of the underlying dynamical mechanisms which determine the
macroscopic laws of heat conduction is a long standing task of non-equilibrium
statistical mechanics. A better understanding of the mechanism of heat
conduction may lead to potentially interesting applications based on the
possibility to con... | cond-mat.stat-mech nlin.CD quant-ph | the understanding of the underlying dynamical mechanisms which determine the macroscopic laws of heat conduction is a long standing task of nonequilibrium statistical mechanics a better understanding of the mechanism of heat conduction may lead to potentially interesting applications based on the possibility to control... | [['the', 'understanding', 'of', 'the', 'underlying', 'dynamical', 'mechanisms', 'which', 'determine', 'the', 'macroscopic', 'laws', 'of', 'heat', 'conduction', 'is', 'a', 'long', 'standing', 'task', 'of', 'nonequilibrium', 'statistical', 'mechanics', 'a', 'better', 'understanding', 'of', 'the', 'mechanism', 'of', 'heat... | [-0.11759765066640222, 0.13646883739490215, -0.09826627769507468, 0.06278230995976379, -0.0941676846801061, -0.1314973878420647, 0.039132853534570196, 0.3492325777379311, -0.34369479599472597, -0.2893658726012066, 0.11133588623249112, -0.26020699077005155, -0.16974859757425442, 0.27459361594272397, -0.03695764778858076... |
710.3501 | Boundary-value problems in cosmological dynamics | The dynamics of cosmological gravitating system is governed by the Euler and
the Poisson equations. Tiny fluctuations near the big bang singularity are
amplified by gravitational instability into the observed structure today. Given
the current distribution of galaxies and assuming initial homogeneity,
dynamical recon... | astro-ph | the dynamics of cosmological gravitating system is governed by the euler and the poisson equations tiny fluctuations near the big bang singularity are amplified by gravitational instability into the observed structure today given the current distribution of galaxies and assuming initial homogeneity dynamical reconstruc... | [['the', 'dynamics', 'of', 'cosmological', 'gravitating', 'system', 'is', 'governed', 'by', 'the', 'euler', 'and', 'the', 'poisson', 'equations', 'tiny', 'fluctuations', 'near', 'the', 'big', 'bang', 'singularity', 'are', 'amplified', 'by', 'gravitational', 'instability', 'into', 'the', 'observed', 'structure', 'today'... | [-0.11804287014196493, 0.12090815497096974, -0.14548664749322815, 0.08080359804721195, -0.06782289639869261, -0.052514254756499124, -0.05847654365269201, 0.2888603374040464, -0.26221080955777626, -0.3379223701970962, 0.07369731557888112, -0.26741337100836626, -0.04122457797971687, 0.16803953591443133, 0.003124709576479... |
710.3502 | Using Synchronic and Diachronic Relations for Summarizing Multiple
Documents Describing Evolving Events | In this paper we present a fresh look at the problem of summarizing evolving
events from multiple sources. After a discussion concerning the nature of
evolving events we introduce a distinction between linearly and non-linearly
evolving events. We present then a general methodology for the automatic
creation of summa... | cs.CL cs.IR | in this paper we present a fresh look at the problem of summarizing evolving events from multiple sources after a discussion concerning the nature of evolving events we introduce a distinction between linearly and nonlinearly evolving events we present then a general methodology for the automatic creation of summaries ... | [['in', 'this', 'paper', 'we', 'present', 'a', 'fresh', 'look', 'at', 'the', 'problem', 'of', 'summarizing', 'evolving', 'events', 'from', 'multiple', 'sources', 'after', 'a', 'discussion', 'concerning', 'the', 'nature', 'of', 'evolving', 'events', 'we', 'introduce', 'a', 'distinction', 'between', 'linearly', 'and', 'n... | [-0.13065515366906766, 0.12199326343463988, -0.10079624982658557, 0.1130384767609278, -0.08907985605235974, -0.1048604933576743, 0.08637629889629105, 0.3711993650490926, -0.2621412003328177, -0.30987946547049267, 0.10230455046389993, -0.3433340132151815, -0.1746753557275621, 0.2006708166895392, -0.07851781609563412, -0... |
710.3503 | Enhanced van der Waals interaction at interfaces | Using a recently obtained (general) formula for the interaction energy
between an excited and a ground-state atom (Sherkunov Y 2007 Phys. Rev. A 75
012705), we consider the interaction energy between two such atoms near the
interface between two media. We demonstrate that under the circumstances of the
resonant coupl... | quant-ph | using a recently obtained general formula for the interaction energy between an excited and a groundstate atom sherkunov y 2007 phys rev a 75 012705 we consider the interaction energy between two such atoms near the interface between two media we demonstrate that under the circumstances of the resonant coupling of the ... | [['using', 'a', 'recently', 'obtained', 'general', 'formula', 'for', 'the', 'interaction', 'energy', 'between', 'an', 'excited', 'and', 'a', 'groundstate', 'atom', 'sherkunov', 'y', '2007', 'phys', 'rev', 'a', '75', '012705', 'we', 'consider', 'the', 'interaction', 'energy', 'between', 'two', 'such', 'atoms', 'near', '... | [-0.16764617630873213, 0.1697877495172923, -0.02215638740348037, 0.0258751916275783, 0.03953011707000604, -0.12477527491071007, 0.06516036934176968, 0.36095205597071484, -0.21844863857735286, -0.33982626868369564, -0.09747383587554478, -0.3365439999086613, -0.10490516111762686, 0.19666378014847974, 0.08501273166885684,... |
710.3504 | High-Mass X-ray Binaries and the Spiral Structure of the Host Galaxy | We investigate the manifestation of the spiral structure in the distribution
of high-mass X-ray binaries (HMXBs) over the host galaxy. We construct the
simple kinematic model. It shows that the HMXBs should be displaced relative to
the spiral structure observed in such traditional star formation rate
indicators as th... | astro-ph | we investigate the manifestation of the spiral structure in the distribution of highmass xray binaries hmxbs over the host galaxy we construct the simple kinematic model it shows that the hmxbs should be displaced relative to the spiral structure observed in such traditional star formation rate indicators as the halpha... | [['we', 'investigate', 'the', 'manifestation', 'of', 'the', 'spiral', 'structure', 'in', 'the', 'distribution', 'of', 'highmass', 'xray', 'binaries', 'hmxbs', 'over', 'the', 'host', 'galaxy', 'we', 'construct', 'the', 'simple', 'kinematic', 'model', 'it', 'shows', 'that', 'the', 'hmxbs', 'should', 'be', 'displaced', 'r... | [-0.04665536880637183, 0.07290172772049981, -0.0921738556989459, 0.14495576837774576, -0.09527021048460924, 0.00811064644169408, 0.06259512976676072, 0.45304931047343716, -0.15819349973318503, -0.34932125052533197, 0.012664292368332174, -0.3109476570347228, -0.034003505975334455, 0.1880978415792174, -0.0293515855171921... |
710.3505 | Recent Studies in Superconductivity at Extreme Pressures | Studies of the effect of high pressure on superconductivity began in 1925
with the seminal work of Sizoo and Onnes on Sn to 0.03 GPa and have continued
up to the present day to pressures in the 200 - 300 GPa range. Such enormous
pressures cause profound changes in all condensed matter properties, including
supercondu... | cond-mat.supr-con | studies of the effect of high pressure on superconductivity began in 1925 with the seminal work of sizoo and onnes on sn to 003 gpa and have continued up to the present day to pressures in the 200 300 gpa range such enormous pressures cause profound changes in all condensed matter properties including superconductivity... | [['studies', 'of', 'the', 'effect', 'of', 'high', 'pressure', 'on', 'superconductivity', 'began', 'in', '1925', 'with', 'the', 'seminal', 'work', 'of', 'sizoo', 'and', 'onnes', 'on', 'sn', 'to', '003', 'gpa', 'and', 'have', 'continued', 'up', 'to', 'the', 'present', 'day', 'to', 'pressures', 'in', 'the', '200', '300', ... | [-0.08518476794290888, 0.22558256077380584, -0.03433768502436578, -0.025486647510635, -0.020151092645911767, -0.10925847067098532, 0.12078241062782971, 0.4041848262505872, -0.2324008842630844, -0.35717424577368156, 0.0833036416359911, -0.3189039227669127, -0.03742769751198856, 0.17912868625052006, -0.007067876811405378... |
710.3506 | Dynamics in One-Dimensional Spin Systems - Density-Matrix
Renormalization Group Study | We study the one-dimensional $S=1/2$ Heisenberg model with a uniform and a
staggered magnetic fields, using the dynamical density-matrix renormalization
group (DDMRG) technique. The DDMRG enables us to investigate the dynamical
properties of chain with lengths up to a few hundreds, and the results are
numerically exa... | cond-mat.str-el | we study the onedimensional s12 heisenberg model with a uniform and a staggered magnetic fields using the dynamical densitymatrix renormalization group ddmrg technique the ddmrg enables us to investigate the dynamical properties of chain with lengths up to a few hundreds and the results are numerically exact in the sam... | [['we', 'study', 'the', 'onedimensional', 's12', 'heisenberg', 'model', 'with', 'a', 'uniform', 'and', 'a', 'staggered', 'magnetic', 'fields', 'using', 'the', 'dynamical', 'densitymatrix', 'renormalization', 'group', 'ddmrg', 'technique', 'the', 'ddmrg', 'enables', 'us', 'to', 'investigate', 'the', 'dynamical', 'proper... | [-0.14630740994055355, 0.13278903013893537, -0.0894288363277304, 0.05389409211858613, -0.04064471918224756, -0.07218337206203225, 0.053771736663386076, 0.3981470686896723, -0.26367357932981483, -0.28781957812464737, 0.11510462886820148, -0.2544223831168243, -0.13990529551056727, 0.19303547609739993, 0.05479566131870509... |
710.3507 | Attractors in coherent systems of differential equations | Attractors of cooperative dynamical systems are particularly simple; for
example, a nontrivial periodic orbit cannot be an attractor. This paper
provides characterizations of attractors for the wider class of coherent
systems, defined by the property that no directed feedback loops are negative.
Several new results f... | math.DS | attractors of cooperative dynamical systems are particularly simple for example a nontrivial periodic orbit cannot be an attractor this paper provides characterizations of attractors for the wider class of coherent systems defined by the property that no directed feedback loops are negative several new results for coop... | [['attractors', 'of', 'cooperative', 'dynamical', 'systems', 'are', 'particularly', 'simple', 'for', 'example', 'a', 'nontrivial', 'periodic', 'orbit', 'can', 'not', 'be', 'an', 'attractor', 'this', 'paper', 'provides', 'characterizations', 'of', 'attractors', 'for', 'the', 'wider', 'class', 'of', 'coherent', 'systems'... | [-0.25326294276035494, 0.1654683690783848, -0.05700929278369855, 0.09667286060711275, -0.05948659418909638, -0.17150397183313207, 0.016216840411760605, 0.37678393445633074, -0.28000600097907913, -0.2064117300151675, 0.12660444567747484, -0.2313459163479921, -0.2216969014369641, 0.2899325452744961, -0.0764961631330489, ... |
710.3508 | Wavelet sets without groups | Most of the examples of wavelet sets are for dilation sets which are groups.
We find a necessary and sufficient condition under which subspace wavelet sets
exist for dilation sets of the form $A B$, which are not necessarily groups. We
explain the construction by a few examples.
| math.FA | most of the examples of wavelet sets are for dilation sets which are groups we find a necessary and sufficient condition under which subspace wavelet sets exist for dilation sets of the form a b which are not necessarily groups we explain the construction by a few examples | [['most', 'of', 'the', 'examples', 'of', 'wavelet', 'sets', 'are', 'for', 'dilation', 'sets', 'which', 'are', 'groups', 'we', 'find', 'a', 'necessary', 'and', 'sufficient', 'condition', 'under', 'which', 'subspace', 'wavelet', 'sets', 'exist', 'for', 'dilation', 'sets', 'of', 'the', 'form', 'a', 'b', 'which', 'are', 'n... | [-0.12707777981025478, 0.1302196421311237, -0.07759943895507604, 0.10520049040981878, -0.027120673020059865, -0.10656038595091862, 0.010704004889703356, 0.4112165066568802, -0.2605283411612618, -0.21831515109321722, 0.20489803451346233, -0.24263796644906202, -0.1746857076844511, 0.2738427298415142, -0.08904977296090995... |
710.3509 | Integral curves of noisy vector fields and statistical problems in
diffusion tensor imaging: nonparametric kernel estimation and hypotheses
testing | Let $v$ be a vector field in a bounded open set $G\subset {\mathbb {R}}^d$.
Suppose that $v$ is observed with a random noise at random points $X_i,
i=1,...,n,$ that are independent and uniformly distributed in $G.$ The problem
is to estimate the integral curve of the differential equation
\[\frac{dx(t)}{dt}=v(x(t)),\... | math.ST stat.TH | let v be a vector field in a bounded open set gsubset mathbb rd suppose that v is observed with a random noise at random points x_i i1n that are independent and uniformly distributed in g the problem is to estimate the integral curve of the differential equation fracdxtdtvxtqquad tgeq 0x0x_0in g starting at a given poi... | [['let', 'v', 'be', 'a', 'vector', 'field', 'in', 'a', 'bounded', 'open', 'set', 'gsubset', 'mathbb', 'rd', 'suppose', 'that', 'v', 'is', 'observed', 'with', 'a', 'random', 'noise', 'at', 'random', 'points', 'x_i', 'i1n', 'that', 'are', 'independent', 'and', 'uniformly', 'distributed', 'in', 'g', 'the', 'problem', 'is'... | [-0.11995122810498018, 0.06348911012502396, -0.14667264645815722, 0.046034333209704695, -0.08005222497956345, -0.13139723421729826, 0.030132460720940595, 0.36303685031037913, -0.29205365593769345, -0.24511703409392524, 0.1252047295121614, -0.2733878931651513, -0.14203632860767862, 0.18867733759538236, -0.07527994464013... |
710.351 | EPR Paradox,Locality and Completeness of Quantum Theory | The quantum theory (QT) and new stochastic approaches have no deterministic
prediction for a single measurement or for a single time -series of events
observed for a trapped ion, electron or any other individual physical system.
The predictions of QT being of probabilistic character apply to the statistical
distribut... | quant-ph | the quantum theory qt and new stochastic approaches have no deterministic prediction for a single measurement or for a single time series of events observed for a trapped ion electron or any other individual physical system the predictions of qt being of probabilistic character apply to the statistical distribution of ... | [['the', 'quantum', 'theory', 'qt', 'and', 'new', 'stochastic', 'approaches', 'have', 'no', 'deterministic', 'prediction', 'for', 'a', 'single', 'measurement', 'or', 'for', 'a', 'single', 'time', 'series', 'of', 'events', 'observed', 'for', 'a', 'trapped', 'ion', 'electron', 'or', 'any', 'other', 'individual', 'physica... | [-0.08205019977872477, 0.11733377494659607, -0.1242601032045797, 0.12151352819862923, -0.0632320544905823, -0.1872948031748793, 0.06834056408907462, 0.3575054500904965, -0.26292657956031107, -0.29103046593795845, 0.09792447944448374, -0.27495295777951273, -0.1192691667465926, 0.21649121845096378, -0.06141392284243048, ... |
710.3511 | Deformations of metabelian representations of knot groups into
$SL(3,\mathbb{C})$ | Let K be a knot in $S^3$ and $X$ its complement. We study deformations of
reducible metabelian representations of the knot group $\pi_1(X)$ into
$SL(3,\mathbb{C})$ which are associated to a double root of the Alexander
polynomial. We prove that these reducible metabelian representations are smooth
points of the repre... | math.GT | let k be a knot in s3 and x its complement we study deformations of reducible metabelian representations of the knot group pi_1x into sl3mathbbc which are associated to a double root of the alexander polynomial we prove that these reducible metabelian representations are smooth points of the representation variety and ... | [['let', 'k', 'be', 'a', 'knot', 'in', 's3', 'and', 'x', 'its', 'complement', 'we', 'study', 'deformations', 'of', 'reducible', 'metabelian', 'representations', 'of', 'the', 'knot', 'group', 'pi_1x', 'into', 'sl3mathbbc', 'which', 'are', 'associated', 'to', 'a', 'double', 'root', 'of', 'the', 'alexander', 'polynomial',... | [-0.2438475821359918, 0.1051592080299903, -0.1561917339387382, 0.01865569238775763, -0.14872681424985157, -0.17733202019610025, -0.049689405822548376, 0.3993259627082995, -0.38504450241553373, -0.16643741864165099, 0.11661227563484411, -0.24972723925421977, -0.18818231257770596, 0.17590760240523978, -0.1419129039096678... |
710.3512 | Radiation Hydrodynamics in Kerr Spacetime: Equations without Coordinate
Singularity at the Event Horizon | Equations of fully general relativistic radiation hydrodynamics around a
rotating black hole are derived by using the Kerr-Schild coordinate where there
is no coordinate singularity at the event horizon. Since the radiation
interacts with matter moving with relativistic velocities near the event
horizon, the interpla... | astro-ph | equations of fully general relativistic radiation hydrodynamics around a rotating black hole are derived by using the kerrschild coordinate where there is no coordinate singularity at the event horizon since the radiation interacts with matter moving with relativistic velocities near the event horizon the interplay bet... | [['equations', 'of', 'fully', 'general', 'relativistic', 'radiation', 'hydrodynamics', 'around', 'a', 'rotating', 'black', 'hole', 'are', 'derived', 'by', 'using', 'the', 'kerrschild', 'coordinate', 'where', 'there', 'is', 'no', 'coordinate', 'singularity', 'at', 'the', 'event', 'horizon', 'since', 'the', 'radiation', ... | [-0.13412985559843946, 0.1089001343701966, -0.10138350851448194, 0.08967529304936761, -0.07033559334813617, -0.09938477071700617, -0.07664543876253446, 0.3261560330633074, -0.21614761525124776, -0.286747809802182, 0.0470557669075788, -0.3074453291366808, -0.011597527039702982, 0.1435435437684646, -0.02279218263720395, ... |
710.3513 | Circumventing the No-Go Theorem in Noncommutative Gauge Field Theory | Stringent restrictions for model building are imposed by a no-go theorem in
noncommutative gauge field theory. Circumventing this theorem is crucial for
the construction of realistic models of particle interactions. To this end, the
noncommutative construction of tensor representations of gauge groups using
half-infi... | hep-th | stringent restrictions for model building are imposed by a nogo theorem in noncommutative gauge field theory circumventing this theorem is crucial for the construction of realistic models of particle interactions to this end the noncommutative construction of tensor representations of gauge groups using halfinfinite wi... | [['stringent', 'restrictions', 'for', 'model', 'building', 'are', 'imposed', 'by', 'a', 'nogo', 'theorem', 'in', 'noncommutative', 'gauge', 'field', 'theory', 'circumventing', 'this', 'theorem', 'is', 'crucial', 'for', 'the', 'construction', 'of', 'realistic', 'models', 'of', 'particle', 'interactions', 'to', 'this', '... | [-0.14302737734590967, 0.1721349500323413, -0.08536674689889576, 0.08131949140845487, -0.10581792923932275, -0.1692158085294068, 0.025297931077269218, 0.2948512081056833, -0.18971661346654098, -0.3156897961348295, 0.08885407013663402, -0.20321759706072043, -0.09702126092587908, 0.19644774506955098, -0.08025592780361573... |
710.3514 | Coxeter Groups, Wavelets, Multiresolution and Sampling | In this short note we discuss the interplay between finite Coxeter groups and
construction of wavelet sets, generalized multiresolution analysis and
sampling.
| math.FA | in this short note we discuss the interplay between finite coxeter groups and construction of wavelet sets generalized multiresolution analysis and sampling | [['in', 'this', 'short', 'note', 'we', 'discuss', 'the', 'interplay', 'between', 'finite', 'coxeter', 'groups', 'and', 'construction', 'of', 'wavelet', 'sets', 'generalized', 'multiresolution', 'analysis', 'and', 'sampling']] | [-0.15223441954532807, 0.15355382607826454, -0.18212628686292606, 0.14228198268260298, -0.07199517121030526, -0.054925831204110924, 0.055352390659126366, 0.391723191534931, -0.39589285088533704, -0.20986599286764182, 0.09546054467368363, -0.22238918918777595, -0.24128616385331209, 0.1803537191272798, -0.140649167228151... |
710.3515 | Remarks Concerning Lubotzky's Filtration | A discrete group which admits a faithful, finite dimensional, linear
representation over a field $\mathbb F$ of characteristic zero is called
linear. This note combines the natural structure of semi-direct products with
work of A. Lubotzky on the existence of linear representations to develop a
technique to give suff... | math.GR | a discrete group which admits a faithful finite dimensional linear representation over a field mathbb f of characteristic zero is called linear this note combines the natural structure of semidirect products with work of a lubotzky on the existence of linear representations to develop a technique to give sufficient con... | [['a', 'discrete', 'group', 'which', 'admits', 'a', 'faithful', 'finite', 'dimensional', 'linear', 'representation', 'over', 'a', 'field', 'mathbb', 'f', 'of', 'characteristic', 'zero', 'is', 'called', 'linear', 'this', 'note', 'combines', 'the', 'natural', 'structure', 'of', 'semidirect', 'products', 'with', 'work', '... | [-0.14920536210411228, 0.12050515893366764, -0.1276433595121489, 0.020433386326658365, -0.1503022987571967, -0.10566607990404009, 0.011192710874638578, 0.3471542482220684, -0.3442541871318099, -0.21991603665173898, 0.12574870717412523, -0.21842603119876003, -0.1491920020462203, 0.20762965038375114, -0.0967940439859376,... |
710.3516 | Realization of two Fourier-limited solid-state single-photon sources | We demonstrate two solid-state sources of indistinguishable single photons.
High resolution laser spectroscopy and optical microscopy were combined at T =
1.4 K to identify individual molecules in two independent microscopes. The
Stark effect was exploited to shift the transition frequency of a given
molecule and thu... | quant-ph | we demonstrate two solidstate sources of indistinguishable single photons high resolution laser spectroscopy and optical microscopy were combined at t 14 k to identify individual molecules in two independent microscopes the stark effect was exploited to shift the transition frequency of a given molecule and thus obtain... | [['we', 'demonstrate', 'two', 'solidstate', 'sources', 'of', 'indistinguishable', 'single', 'photons', 'high', 'resolution', 'laser', 'spectroscopy', 'and', 'optical', 'microscopy', 'were', 'combined', 'at', 't', '14', 'k', 'to', 'identify', 'individual', 'molecules', 'in', 'two', 'independent', 'microscopes', 'the', '... | [-0.1319522504878401, 0.16722571853758164, -0.04352356658094156, 0.004138098909965598, -0.013863450637690618, -0.18026848200997206, 0.0977472099237813, 0.4646860564678488, -0.2518604280243457, -0.3541507904785095, -0.0011155349153264518, -0.35117659565638487, -0.03488898298926127, 0.2067480959575361, 0.0091465657025995... |
710.3517 | Pulsar High-Energy Emission From the Polar Cap and Slot Gap | Forty years after the discovery of rotation-powered pulsars, we still do not
understand many aspects of their pulsed emission. In the last few years there
have been some fundamental developments in acceleration and emission models. I
will review both the basic physics of the models as well as the latest
developments ... | astro-ph | forty years after the discovery of rotationpowered pulsars we still do not understand many aspects of their pulsed emission in the last few years there have been some fundamental developments in acceleration and emission models i will review both the basic physics of the models as well as the latest developments in und... | [['forty', 'years', 'after', 'the', 'discovery', 'of', 'rotationpowered', 'pulsars', 'we', 'still', 'do', 'not', 'understand', 'many', 'aspects', 'of', 'their', 'pulsed', 'emission', 'in', 'the', 'last', 'few', 'years', 'there', 'have', 'been', 'some', 'fundamental', 'developments', 'in', 'acceleration', 'and', 'emissi... | [-0.054444788448098635, 0.18433288397888342, -0.05137248849151311, 0.14316857958436702, -0.11962538487364159, -0.12128217053703136, -0.024094841196374207, 0.4172756131600451, -0.22586884889061803, -0.32713784320555905, 0.09679243377996263, -0.2928499281147702, -0.08761255189396992, 0.2707755442165459, -0.02262055517165... |
710.3518 | HESS J1023-575: Non-thermal particle acceleration associated with the
young stellar cluster Westerlund 2 | The results from H.E.S.S. observations towards Westerlund 2 are presented.
The detection of very-high-energy gamma-ray emission towards the young stellar
cluster Westerlund 2 in the HII complex RCW49 by H.E.S.S. provides ample
evidence that particle acceleration to extreme energies is associated with this
region. A v... | astro-ph | the results from hess observations towards westerlund 2 are presented the detection of veryhighenergy gammaray emission towards the young stellar cluster westerlund 2 in the hii complex rcw49 by hess provides ample evidence that particle acceleration to extreme energies is associated with this region a variety of possi... | [['the', 'results', 'from', 'hess', 'observations', 'towards', 'westerlund', '2', 'are', 'presented', 'the', 'detection', 'of', 'veryhighenergy', 'gammaray', 'emission', 'towards', 'the', 'young', 'stellar', 'cluster', 'westerlund', '2', 'in', 'the', 'hii', 'complex', 'rcw49', 'by', 'hess', 'provides', 'ample', 'eviden... | [-0.05221889889361407, 0.1684249256863574, -0.03106170206827889, 0.1609381841385345, -0.10431405258385983, -0.08313729953987145, 0.018877849031827952, 0.4350313451106107, -0.1763597820269266, -0.3253898687408607, 0.0021637798097908943, -0.3212185428106695, 0.024304306232615522, 0.25428092246262457, -0.00014451944722318... |
710.3519 | P-matrix recognition is co-NP-complete | This is a summary of the proof by G.E. Coxson that P-matrix recognition is
co-NP-complete. The result follows by a reduction from the MAX CUT problem
using results of S. Poljak and J. Rohn.
| cs.CC | this is a summary of the proof by ge coxson that pmatrix recognition is conpcomplete the result follows by a reduction from the max cut problem using results of s poljak and j rohn | [['this', 'is', 'a', 'summary', 'of', 'the', 'proof', 'by', 'ge', 'coxson', 'that', 'pmatrix', 'recognition', 'is', 'conpcomplete', 'the', 'result', 'follows', 'by', 'a', 'reduction', 'from', 'the', 'max', 'cut', 'problem', 'using', 'results', 'of', 's', 'poljak', 'and', 'j', 'rohn']] | [-0.07468807522320386, 0.07121080297017188, -0.07862177818562045, 0.006764043704606593, -0.04021553359361309, -0.16027157942792683, 0.07376705533401533, 0.2618797194551338, -0.29166627020546887, -0.3226661628930632, 0.12451444958534205, -0.31181076552831766, -0.14623414523278674, 0.18432178550089398, -0.121691940369959... |
710.352 | Three-way tiling sets in two dimensions | In this article we show that there exist measurable sets W in the plane with
finite measure that tile the plane in a measurable way under the action of a
expansive matrix A, an affine Weyl group W, and a full rank lattice G. This
note is follow-up research to the earlier article "Coxeter groups and wavelet
sets" by t... | math.FA | in this article we show that there exist measurable sets w in the plane with finite measure that tile the plane in a measurable way under the action of a expansive matrix a an affine weyl group w and a full rank lattice g this note is followup research to the earlier article coxeter groups and wavelet sets by the first... | [['in', 'this', 'article', 'we', 'show', 'that', 'there', 'exist', 'measurable', 'sets', 'w', 'in', 'the', 'plane', 'with', 'finite', 'measure', 'that', 'tile', 'the', 'plane', 'in', 'a', 'measurable', 'way', 'under', 'the', 'action', 'of', 'a', 'expansive', 'matrix', 'a', 'an', 'affine', 'weyl', 'group', 'w', 'and', '... | [-0.1331738399944323, 0.10403195941514294, -0.08549646085867768, 0.028488684675026247, -0.0716374402947943, -0.09166234022430966, 0.06504303076551021, 0.36259130008847396, -0.2638354535851463, -0.2745804534951115, 0.11299718944698244, -0.3081787204821868, -0.1901782445335651, 0.17042976291165413, -0.09789484602344387, ... |
710.3521 | $C^*-$crossed product of groupoid actions on categories | Suppose that $G$ is a groupoid acting on a small category $H$ in the sense of
\cite[Definition 4]{NOT} and $H\times_\alpha G$ is the resulting semi-direct
product category (as in \cite[Proposition 8]{NOT}). We show that there exists a
subcategory $H_r \subseteq H$ satisfying some nice property called
``regularity'' s... | math.OA math.CT | suppose that g is a groupoid acting on a small category h in the sense of citedefinition 4not and htimes_alpha g is the resulting semidirect product category as in citeproposition 8not we show that there exists a subcategory h_r subseteq h satisfying some nice property called regularity such that h_r times_alpha g htim... | [['suppose', 'that', 'g', 'is', 'a', 'groupoid', 'acting', 'on', 'a', 'small', 'category', 'h', 'in', 'the', 'sense', 'of', 'citedefinition', '4not', 'and', 'htimes_alpha', 'g', 'is', 'the', 'resulting', 'semidirect', 'product', 'category', 'as', 'in', 'citeproposition', '8not', 'we', 'show', 'that', 'there', 'exists',... | [-0.18408132412561984, 0.14245017992494546, -0.054235030689438725, 0.01840844829870469, -0.1078797050792238, -0.12764218861601598, -0.03174160840495935, 0.4267872292548418, -0.32597907002934295, -0.1872028480587608, 0.06150334094063905, -0.2398687685313432, -0.15464167036217355, 0.18062914112258865, -0.1492707703323306... |
710.3522 | K-string tensions at finite temperature and integrable models | It has recently been pointed out that simple scaling properties of Polyakov
correlation functions of gauge systems in the confining phase suggest that the
ratios of k-string tensions in the low temperature region is constant up to
terms of order T^3. Here we argue that, at least in a three-dimensional Z_4
gauge model... | hep-lat hep-th | it has recently been pointed out that simple scaling properties of polyakov correlation functions of gauge systems in the confining phase suggest that the ratios of kstring tensions in the low temperature region is constant up to terms of order t3 here we argue that at least in a threedimensional z_4 gauge model the ab... | [['it', 'has', 'recently', 'been', 'pointed', 'out', 'that', 'simple', 'scaling', 'properties', 'of', 'polyakov', 'correlation', 'functions', 'of', 'gauge', 'systems', 'in', 'the', 'confining', 'phase', 'suggest', 'that', 'the', 'ratios', 'of', 'kstring', 'tensions', 'in', 'the', 'low', 'temperature', 'region', 'is', '... | [-0.14105374270992488, 0.1935426354536981, -0.07800653821443082, 0.03468297491661398, 0.008052730450368266, -0.1183505906992275, 0.032257604278316816, 0.382334905359702, -0.19255984599519635, -0.2637086816074461, 0.0811179709553565, -0.2879321515060884, -0.1537688314463444, 0.13577390411513446, 0.028152532916043204, 0.... |
710.3523 | A combinatorial framework for RNA tertiary interaction | In this paper we show how to express RNA tertiary interactions via the
concepts of tangled diagrams. Tangled diagrams allow to formulate RNA base
triples and pseudoknot-interactions and to control the maximum number of
mutually crossing arcs. In particular we study two subsets of tangled diagrams:
3-noncrossing tangl... | math.CO math.AP | in this paper we show how to express rna tertiary interactions via the concepts of tangled diagrams tangled diagrams allow to formulate rna base triples and pseudoknotinteractions and to control the maximum number of mutually crossing arcs in particular we study two subsets of tangled diagrams 3noncrossing tangleddiagr... | [['in', 'this', 'paper', 'we', 'show', 'how', 'to', 'express', 'rna', 'tertiary', 'interactions', 'via', 'the', 'concepts', 'of', 'tangled', 'diagrams', 'tangled', 'diagrams', 'allow', 'to', 'formulate', 'rna', 'base', 'triples', 'and', 'pseudoknotinteractions', 'and', 'to', 'control', 'the', 'maximum', 'number', 'of',... | [-0.24436456327745265, 0.16777194033010004, -0.03785286363002784, 0.0936851680904644, -0.10147742162791824, -0.08683701994222238, 0.07863326438002015, 0.3155791627396958, -0.2843509323279792, -0.3049520231407443, -0.020664765958785327, -0.2769261175433362, -0.18840626354004605, 0.11899969951941743, -0.06007490229233245... |
710.3524 | Construction of potentials using mixed scattering data | The long-standing problem of constructing a potential from mixed scattering
data is discussed. We first consider the fixed-$\ell$ inverse scattering
problem. We show that the zeros of the regular solution of the Schr\"odinger
equation, $r_{n}(E)$ which are monotonic functions of the energy, determine a
unique potenti... | math-ph hep-th math.MP | the longstanding problem of constructing a potential from mixed scattering data is discussed we first consider the fixedell inverse scattering problem we show that the zeros of the regular solution of the schrodinger equation r_ne which are monotonic functions of the energy determine a unique potential when the domain ... | [['the', 'longstanding', 'problem', 'of', 'constructing', 'a', 'potential', 'from', 'mixed', 'scattering', 'data', 'is', 'discussed', 'we', 'first', 'consider', 'the', 'fixedell', 'inverse', 'scattering', 'problem', 'we', 'show', 'that', 'the', 'zeros', 'of', 'the', 'regular', 'solution', 'of', 'the', 'schrodinger', 'e... | [-0.13557251914005194, 0.07437903733558154, -0.08345839432440698, 0.06142068045280342, -0.06557201667622264, -0.12735254561328993, 0.0060005305368187175, 0.325238852349243, -0.3351491623558104, -0.2310923703547035, 0.11504001020803116, -0.31124956269216325, -0.10347207912044333, 0.1694101701490581, 0.011062961613892445... |
710.3525 | Radiative B-L symmetry breaking in supersymmetric models | We propose a scheme where the three relevant physics scales related to the
supersymmetry, electroweak, and baryon minus lepton (B-L) breakings are linked
together and occur at the TeV scale. The phenomenological implications in the
Higgs and leptonic sectors are discussed.
| hep-ph | we propose a scheme where the three relevant physics scales related to the supersymmetry electroweak and baryon minus lepton bl breakings are linked together and occur at the tev scale the phenomenological implications in the higgs and leptonic sectors are discussed | [['we', 'propose', 'a', 'scheme', 'where', 'the', 'three', 'relevant', 'physics', 'scales', 'related', 'to', 'the', 'supersymmetry', 'electroweak', 'and', 'baryon', 'minus', 'lepton', 'bl', 'breakings', 'are', 'linked', 'together', 'and', 'occur', 'at', 'the', 'tev', 'scale', 'the', 'phenomenological', 'implications', ... | [-0.08735432103276253, 0.3202261786862481, 0.00513830018888523, 0.2505587843224043, -0.11821140197855307, -0.19688728924772544, 0.00794547755362057, 0.29734837745384474, -0.22082779028384789, -0.2898835731079666, 0.07999893646721341, -0.27465098925934334, -0.0017882116684099522, 0.08689003576320119, 0.06889735191787888... |
710.3526 | Clumping effects on non-thermal particle spectra in massive star systems | Observational evidence exists that winds of massive stars are clumped. Many
massive star systems are known as non-thermal particle production sites, as
indicated by their synchrotron emission in the radio band. As a consequence
they are also considered as candidate sites for non-thermal high-energy photon
production ... | astro-ph | observational evidence exists that winds of massive stars are clumped many massive star systems are known as nonthermal particle production sites as indicated by their synchrotron emission in the radio band as a consequence they are also considered as candidate sites for nonthermal highenergy photon production up to ga... | [['observational', 'evidence', 'exists', 'that', 'winds', 'of', 'massive', 'stars', 'are', 'clumped', 'many', 'massive', 'star', 'systems', 'are', 'known', 'as', 'nonthermal', 'particle', 'production', 'sites', 'as', 'indicated', 'by', 'their', 'synchrotron', 'emission', 'in', 'the', 'radio', 'band', 'as', 'a', 'conseq... | [-0.07633609492953589, 0.2245406764834217, -0.03766755495359254, 0.14215352812923654, -0.06062976575329298, -0.0997419333192433, 0.03398293475273372, 0.4279937515069979, -0.22752431862241362, -0.33583435919482885, 0.01791383377030515, -0.3121348499256817, 0.030572569602232726, 0.20978372482227173, 0.023793523293675463,... |
710.3527 | Toward theory of quantum Hall effect in graphene | We analyze a gap equation for the propagator of Dirac quasiparticles and
conclude that in graphene in a magnetic field, the order parameters connected
with the quantum Hall ferromagnetism dynamics and those connected with the
magnetic catalysis dynamics necessarily coexist (the latter have the form of
Dirac masses an... | cond-mat.mes-hall hep-th | we analyze a gap equation for the propagator of dirac quasiparticles and conclude that in graphene in a magnetic field the order parameters connected with the quantum hall ferromagnetism dynamics and those connected with the magnetic catalysis dynamics necessarily coexist the latter have the form of dirac masses and co... | [['we', 'analyze', 'a', 'gap', 'equation', 'for', 'the', 'propagator', 'of', 'dirac', 'quasiparticles', 'and', 'conclude', 'that', 'in', 'graphene', 'in', 'a', 'magnetic', 'field', 'the', 'order', 'parameters', 'connected', 'with', 'the', 'quantum', 'hall', 'ferromagnetism', 'dynamics', 'and', 'those', 'connected', 'wi... | [-0.21302357963849228, 0.2201486005368489, -0.056584967515216425, 0.05269552873073985, -0.049421333467362674, -0.1412819462859041, 0.028939941204613545, 0.35363639461306423, -0.2452950672154407, -0.29609785994494353, -0.00056036814131293, -0.28419378844018167, -0.17128219621276464, 0.1438145744153759, 0.033961343801590... |
710.3528 | The H.E.S.S. survey of the inner Galactic plane | The High Energy Stereoscopic System (H.E.S.S.), located in the Khomas
Highlands of Namibia, is an array of four imaging atmospheric-Cherenkov
telescopes designed to detect gamma-rays in the very high energy (VHE; > 100
GeV) domain. Its high sensitivity and large field-of-view (5 deg) make it an
ideal instrument to pe... | astro-ph | the high energy stereoscopic system hess located in the khomas highlands of namibia is an array of four imaging atmosphericcherenkov telescopes designed to detect gammarays in the very high energy vhe 100 gev domain its high sensitivity and large fieldofview 5 deg make it an ideal instrument to perform a survey within ... | [['the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'located', 'in', 'the', 'khomas', 'highlands', 'of', 'namibia', 'is', 'an', 'array', 'of', 'four', 'imaging', 'atmosphericcherenkov', 'telescopes', 'designed', 'to', 'detect', 'gammarays', 'in', 'the', 'very', 'high', 'energy', 'vhe', '100', 'gev', 'domain', ... | [-0.11061158298431766, 0.11937028572147476, 0.03364376948963179, 0.08425352838917131, -0.15734469770743956, -0.07566717995681846, 0.05596159008469005, 0.41303640677303566, -0.18806746689083634, -0.468736092056163, 0.08197744345563449, -0.35120562361705987, 0.040378054916919745, 0.21881596708181697, -0.03010760087373887... |
710.3529 | Scalable experimental estimation of multipartite entanglement | We present an efficient experimental estimation of the multipartite
entanglement of mixed quantum states in terms of simple parity measurements.
| quant-ph | we present an efficient experimental estimation of the multipartite entanglement of mixed quantum states in terms of simple parity measurements | [['we', 'present', 'an', 'efficient', 'experimental', 'estimation', 'of', 'the', 'multipartite', 'entanglement', 'of', 'mixed', 'quantum', 'states', 'in', 'terms', 'of', 'simple', 'parity', 'measurements']] | [-0.1816218686988577, 0.22782129387560418, -0.08678212739760056, 0.022130299935815854, 0.04203873281367123, -0.18042515385895969, 0.030778478807769717, 0.31227066926658154, -0.19003036841750146, -0.2596150994300842, 0.039595784147968514, -0.24548792708665132, -0.10301880110055209, 0.1400747274979949, -0.063295552926138... |
710.353 | Clustering Properties of restframe UV selected galaxies I: the
correlation length derived from GALEX data in the local Universe | We present the first measurements of the angular correlation function of
galaxies selected in the far (1530 A) and near (2310 A) Ultraviolet from the
GALEX survey fields overlapping SDSS DR5 in low galactic extinction regions.
The area used covers 120 sqdeg (GALEX - MIS) down to magnitude AB = 22,
yielding a total of... | astro-ph | we present the first measurements of the angular correlation function of galaxies selected in the far 1530 a and near 2310 a ultraviolet from the galex survey fields overlapping sdss dr5 in low galactic extinction regions the area used covers 120 sqdeg galex mis down to magnitude ab 22 yielding a total of 100000 galaxi... | [['we', 'present', 'the', 'first', 'measurements', 'of', 'the', 'angular', 'correlation', 'function', 'of', 'galaxies', 'selected', 'in', 'the', 'far', '1530', 'a', 'and', 'near', '2310', 'a', 'ultraviolet', 'from', 'the', 'galex', 'survey', 'fields', 'overlapping', 'sdss', 'dr5', 'in', 'low', 'galactic', 'extinction',... | [-0.043751943162673675, 0.061811569886029726, -0.06938901792191307, 0.10670787007266642, -0.050646626393642, -0.027625154888244883, 0.09543471266953087, 0.4277474113283741, -0.14677568126294838, -0.370896019897855, 0.02683814420621067, -0.34620029995555446, -0.025377594216198555, 0.1614938521579583, -0.0249236664741031... |
710.3531 | $n$-blocks collections on Fano manifolds and sheaves with regularity
$-\infty$ | Let $X$ be a smooth Fano manifold equipped with a `` nice '' $n$-blocks
collection in the sense of \cite{cm2} and $\mathcal {F}$ a coherent sheaf on
$X$. Assume that $X$ is Fano and that all blocks are coherent sheaves. Here we
prove that $\mathcal {F}$ has regularity $-\infty$ in the sense of \cite{cm2}
if ${Supp}(\... | math.AG | let x be a smooth fano manifold equipped with a nice nblocks collection in the sense of citecm2 and mathcal f a coherent sheaf on x assume that x is fano and that all blocks are coherent sheaves here we prove that mathcal f has regularity infty in the sense of citecm2 if suppmathcal f is finite the converse being true ... | [['let', 'x', 'be', 'a', 'smooth', 'fano', 'manifold', 'equipped', 'with', 'a', 'nice', 'nblocks', 'collection', 'in', 'the', 'sense', 'of', 'citecm2', 'and', 'mathcal', 'f', 'a', 'coherent', 'sheaf', 'on', 'x', 'assume', 'that', 'x', 'is', 'fano', 'and', 'that', 'all', 'blocks', 'are', 'coherent', 'sheaves', 'here', '... | [-0.1829695657331061, 0.08497337143499308, -0.10561517415592422, 0.03420878984124775, -0.04497866481300685, -0.18950102842328223, -0.005335892647408046, 0.3863139483448747, -0.31711439420650533, -0.12110936577589095, 0.06869378849991005, -0.24478977415468786, -0.14675514138751217, 0.19131343215462063, -0.20619366940280... |
710.3532 | Importance of Metastable States in the Free Energy Landscapes of
Polypeptide Chains | We show that the interplay between excluded volume effects, hydrophobicity,
and hydrogen bonding of a tube-like representation of a polypeptide chain gives
rise to free energy landscapes that exhibit a small number of metastable minima
corresponding to common structural motifs observed in proteins. The complexity
of ... | cond-mat.soft cond-mat.stat-mech | we show that the interplay between excluded volume effects hydrophobicity and hydrogen bonding of a tubelike representation of a polypeptide chain gives rise to free energy landscapes that exhibit a small number of metastable minima corresponding to common structural motifs observed in proteins the complexity of the la... | [['we', 'show', 'that', 'the', 'interplay', 'between', 'excluded', 'volume', 'effects', 'hydrophobicity', 'and', 'hydrogen', 'bonding', 'of', 'a', 'tubelike', 'representation', 'of', 'a', 'polypeptide', 'chain', 'gives', 'rise', 'to', 'free', 'energy', 'landscapes', 'that', 'exhibit', 'a', 'small', 'number', 'of', 'met... | [-0.14688644392816264, 0.2041501855754041, -0.08608934345489769, 0.09540171047920692, -0.020239379365763095, -0.12544314772169166, 0.1022996551130907, 0.34468895903675356, -0.29261836287713494, -0.2914059418210081, 0.011069742375201433, -0.286966224470846, -0.14781182089159003, 0.1185097214722327, -0.008380365314258037... |
710.3533 | Mechanism of Ambipolar Field-Effect Transistors on One-Dimensional
Organic Mott Insulators | The experimentally observed, ambipolar field-effect characteristics of Mott
insulators are reproduced in the one-dimensional Hubbard model attached to a
tight-binding model for source and drain electrodes. The formation of Schottky
barriers, originating from the work-function difference, is taken into account
by a po... | cond-mat.str-el | the experimentally observed ambipolar fieldeffect characteristics of mott insulators are reproduced in the onedimensional hubbard model attached to a tightbinding model for source and drain electrodes the formation of schottky barriers originating from the workfunction difference is taken into account by a potential sa... | [['the', 'experimentally', 'observed', 'ambipolar', 'fieldeffect', 'characteristics', 'of', 'mott', 'insulators', 'are', 'reproduced', 'in', 'the', 'onedimensional', 'hubbard', 'model', 'attached', 'to', 'a', 'tightbinding', 'model', 'for', 'source', 'and', 'drain', 'electrodes', 'the', 'formation', 'of', 'schottky', '... | [-0.1456126551510191, 0.08972393501715166, -0.045562268388868475, 0.05438540476846837, -0.036115145283367706, -0.2761580390746103, 0.0323093929738902, 0.4122132241506787, -0.2844138230498442, -0.2734490004505086, -0.03208114058446988, -0.3024080636746743, -0.13270757161080837, 0.22414459181976887, -0.01740204592865399,... |
710.3534 | Influence of stellar X-ray luminosity distribution and its evolution on
exoplanetary mass loss | Aims: We investigate the influence of high-energy stellar radiation at
close-in orbits on atmospheric mass loss during stellar evolution of a G-type
star. Methods: High-energy stellar luminosity varies over a wide range for G
field stars. The temporal evolution of the distribution of stellar X-ray
luminosity and its ... | astro-ph | aims we investigate the influence of highenergy stellar radiation at closein orbits on atmospheric mass loss during stellar evolution of a gtype star methods highenergy stellar luminosity varies over a wide range for g field stars the temporal evolution of the distribution of stellar xray luminosity and its influence o... | [['aims', 'we', 'investigate', 'the', 'influence', 'of', 'highenergy', 'stellar', 'radiation', 'at', 'closein', 'orbits', 'on', 'atmospheric', 'mass', 'loss', 'during', 'stellar', 'evolution', 'of', 'a', 'gtype', 'star', 'methods', 'highenergy', 'stellar', 'luminosity', 'varies', 'over', 'a', 'wide', 'range', 'for', 'g... | [-0.05408530072230151, 0.18546001116771813, -0.09159405729444013, 0.15612528632437064, -0.10738701011333088, 0.02496607058371107, 0.049566264635236085, 0.41978851414290863, -0.16166118428171586, -0.3951392130936775, 0.020449822306853986, -0.288216956138695, 0.005054817158770932, 0.24851628832945252, -0.0461640205552622... |
710.3535 | JANUS: an FPGA-based System for High Performance Scientific Computing | This paper describes JANUS, a modular massively parallel and reconfigurable
FPGA-based computing system. Each JANUS module has a computational core and a
host. The computational core is a 4x4 array of FPGA-based processing elements
with nearest-neighbor data links. Processors are also directly connected to an
I/O nod... | cs.AR | this paper describes janus a modular massively parallel and reconfigurable fpgabased computing system each janus module has a computational core and a host the computational core is a 4x4 array of fpgabased processing elements with nearestneighbor data links processors are also directly connected to an io node attached... | [['this', 'paper', 'describes', 'janus', 'a', 'modular', 'massively', 'parallel', 'and', 'reconfigurable', 'fpgabased', 'computing', 'system', 'each', 'janus', 'module', 'has', 'a', 'computational', 'core', 'and', 'a', 'host', 'the', 'computational', 'core', 'is', 'a', '4x4', 'array', 'of', 'fpgabased', 'processing', '... | [-0.16210474132990035, 0.04364620021801243, -0.016737300415777347, -0.006246459003622559, -0.0944153322883836, -0.19684860442758545, 0.016565073902679646, 0.4209453316236084, -0.25718021261590446, -0.35380695489319886, 0.11929925597334684, -0.25961568624015663, -0.1476524697447365, 0.25128107778060454, -0.0725626149214... |
710.3536 | Common Beliefs and Public Announcements in Strategic Games with
Arbitrary Strategy Sets | We provide an epistemic analysis of arbitrary strategic games based on
possibility correspondences. We first establish a generic result that links
true common beliefs (and, respectively, common knowledge) of players'
rationality defined by means of `monotonic' properties, with the iterated
elimination of strategies t... | cs.GT | we provide an epistemic analysis of arbitrary strategic games based on possibility correspondences we first establish a generic result that links true common beliefs and respectively common knowledge of players rationality defined by means of monotonic properties with the iterated elimination of strategies that do not ... | [['we', 'provide', 'an', 'epistemic', 'analysis', 'of', 'arbitrary', 'strategic', 'games', 'based', 'on', 'possibility', 'correspondences', 'we', 'first', 'establish', 'a', 'generic', 'result', 'that', 'links', 'true', 'common', 'beliefs', 'and', 'respectively', 'common', 'knowledge', 'of', 'players', 'rationality', 'd... | [-0.10417121836598481, 0.023417440637572798, -0.17383193242010372, 0.10816132427947917, -0.14694573275488, -0.12660646372442616, 0.12095135816469274, 0.3460358254996867, -0.29320608187338404, -0.2525968833344764, 0.06951076971639976, -0.20200300499624252, -0.18944156121077207, 0.1641661182375111, -0.15667717492304228, ... |
710.3537 | Two-pion-exchange effects in the $pp\to pp\pi^0$ reaction | We study the pp \to pp\pi^0 reaction near threshold based on heavy-baryon
chiral perturbation theory. We show that the two-pion-exchange diagrams give
much larger contribution than the one-pion-exchange diagram which is of lower
chiral order in Weinberg's counting scheme. We also discuss the relation of our
results t... | nucl-th | we study the pp to pppi0 reaction near threshold based on heavybaryon chiral perturbation theory we show that the twopionexchange diagrams give much larger contribution than the onepionexchange diagram which is of lower chiral order in weinbergs counting scheme we also discuss the relation of our results to the momentu... | [['we', 'study', 'the', 'pp', 'to', 'pppi0', 'reaction', 'near', 'threshold', 'based', 'on', 'heavybaryon', 'chiral', 'perturbation', 'theory', 'we', 'show', 'that', 'the', 'twopionexchange', 'diagrams', 'give', 'much', 'larger', 'contribution', 'than', 'the', 'onepionexchange', 'diagram', 'which', 'is', 'of', 'lower',... | [-0.12362683882327893, 0.14166788795353988, -0.1513271844602199, 0.1296486061608168, -0.07729590680593482, -0.04094502996080197, 0.08848456947732931, 0.3214489843902321, -0.152026980327299, -0.26617961531715434, -0.021506507722034048, -0.3061675648384083, -0.16599050307055363, 0.14682459892579713, 0.014023209241433786,... |
710.3538 | Classical and new loglog-theorems | We present integral variants of results due to Carleman, Wolf, Levinson,
Sjoberg, and Matsaev on majorants of analytic functions. Main ingredient is a
complete description for radial projections of harmonic measures of strictly
star-shaped domains in the plane.
| math.CV | we present integral variants of results due to carleman wolf levinson sjoberg and matsaev on majorants of analytic functions main ingredient is a complete description for radial projections of harmonic measures of strictly starshaped domains in the plane | [['we', 'present', 'integral', 'variants', 'of', 'results', 'due', 'to', 'carleman', 'wolf', 'levinson', 'sjoberg', 'and', 'matsaev', 'on', 'majorants', 'of', 'analytic', 'functions', 'main', 'ingredient', 'is', 'a', 'complete', 'description', 'for', 'radial', 'projections', 'of', 'harmonic', 'measures', 'of', 'strictl... | [-0.14500389250583554, -0.017672972618847302, -0.09815190761889282, 0.10772102592378169, -0.0814633162134621, -0.043796722887476026, 0.008744986831994825, 0.3266418206284901, -0.179501741548608, -0.1599498339193432, 0.12581917693483105, -0.2726422080672101, -0.14444040746648648, 0.2576185906747062, -0.13349185783514067... |
710.3539 | Dynamics, dephasing and clustering of impurity atoms in Bose-Einstein
condensates | We investigate the influence of a Bose-Einstein condensate (BEC) on the
properties of immersed impurity atoms, which are trapped in an optical lattice.
Assuming a weak coupling of the impurity atoms to the BEC, we derive a quantum
master equation for the lattice system. In the special case of fixed impurities
with tw... | quant-ph | we investigate the influence of a boseeinstein condensate bec on the properties of immersed impurity atoms which are trapped in an optical lattice assuming a weak coupling of the impurity atoms to the bec we derive a quantum master equation for the lattice system in the special case of fixed impurities with two interna... | [['we', 'investigate', 'the', 'influence', 'of', 'a', 'boseeinstein', 'condensate', 'bec', 'on', 'the', 'properties', 'of', 'immersed', 'impurity', 'atoms', 'which', 'are', 'trapped', 'in', 'an', 'optical', 'lattice', 'assuming', 'a', 'weak', 'coupling', 'of', 'the', 'impurity', 'atoms', 'to', 'the', 'bec', 'we', 'deri... | [-0.16430992769230876, 0.24106188567673764, -0.04032675723217174, 0.05151740103478501, 0.026436589106610467, -0.17396495516930538, 0.07837441737832375, 0.36837974205528473, -0.2570433147788704, -0.22317265988518062, -0.016014762364978775, -0.3212236939011332, -0.08063549089869908, 0.1497992879369783, 0.0676203735922833... |
710.354 | N=2 supersymmetric spin foams in three dimensions | We construct the spin foam model for N=2 supergravity in three dimensions.
Classically, it is a BF theory with gauge algebra osp(2|2). This algebra has
representations which are not completely reducible. This complicates the
procedure when building a state sum. Fortunately, one can and should excise
these representat... | gr-qc hep-th | we construct the spin foam model for n2 supergravity in three dimensions classically it is a bf theory with gauge algebra osp22 this algebra has representations which are not completely reducible this complicates the procedure when building a state sum fortunately one can and should excise these representations we show... | [['we', 'construct', 'the', 'spin', 'foam', 'model', 'for', 'n2', 'supergravity', 'in', 'three', 'dimensions', 'classically', 'it', 'is', 'a', 'bf', 'theory', 'with', 'gauge', 'algebra', 'osp22', 'this', 'algebra', 'has', 'representations', 'which', 'are', 'not', 'completely', 'reducible', 'this', 'complicates', 'the',... | [-0.11377677367711517, 0.21219154314930774, -0.0618979236619039, 0.0742632555073004, -0.07300751568934272, -0.1761334145264623, -0.027443663724159344, 0.35945291817573105, -0.2294254767119669, -0.2200722520755342, 0.09261748409629915, -0.24448187746050332, -0.18551270971613482, 0.1194763408169489, -0.08464243223174853,... |
710.3541 | Dynamical parallax of sigma Ori AB: mass, distance and age | The massive OB-type binary sigma Ori AB is in the centre of the very young
sigma Orionis cluster. I have computed the most probable distances and masses
of the binary for several ages using a dynamical parallax-like method. It
incorporates the BVRIH-band apparent magnitudes of both components, precise
orbital paramet... | astro-ph | the massive obtype binary sigma ori ab is in the centre of the very young sigma orionis cluster i have computed the most probable distances and masses of the binary for several ages using a dynamical parallaxlike method it incorporates the bvrihband apparent magnitudes of both components precise orbital parameters inte... | [['the', 'massive', 'obtype', 'binary', 'sigma', 'ori', 'ab', 'is', 'in', 'the', 'centre', 'of', 'the', 'very', 'young', 'sigma', 'orionis', 'cluster', 'i', 'have', 'computed', 'the', 'most', 'probable', 'distances', 'and', 'masses', 'of', 'the', 'binary', 'for', 'several', 'ages', 'using', 'a', 'dynamical', 'parallaxl... | [-0.07591868518255383, 0.11330508481195656, -0.07108500208906668, 0.11773061754496889, -0.09779808015676497, -0.07840530660502586, 0.08928465726617858, 0.3752424738657989, -0.2132308972445015, -0.351483388254486, 0.06670010900677671, -0.27356644267578134, -0.0372252067309811, 0.18741653414096401, -0.03849586465885099, ... |
710.3542 | Transport and percolation in a low-density high-mobility two-dimensional
hole system | We present a study of the temperature and density dependence of the
resistivity of an extremely high quality two-dimensional hole system grown on
the (100) surface of GaAs. For high densities in the metallic regime ($p\agt 4
\times 10^{9}$ cm$^{-2}$), the nonmonotonic temperature dependence ($\sim
50-300$ mK) of the ... | cond-mat.mes-hall | we present a study of the temperature and density dependence of the resistivity of an extremely high quality twodimensional hole system grown on the 100 surface of gaas for high densities in the metallic regime pagt 4 times 109 cm2 the nonmonotonic temperature dependence sim 50300 mk of the resistivity is consistent wi... | [['we', 'present', 'a', 'study', 'of', 'the', 'temperature', 'and', 'density', 'dependence', 'of', 'the', 'resistivity', 'of', 'an', 'extremely', 'high', 'quality', 'twodimensional', 'hole', 'system', 'grown', 'on', 'the', '100', 'surface', 'of', 'gaas', 'for', 'high', 'densities', 'in', 'the', 'metallic', 'regime', 'p... | [-0.14857334962321653, 0.23927348963835457, -0.01299694645115071, -0.03406521321869352, 0.07593203167327577, -0.10922868594320284, 0.09292425757222292, 0.34016382495562236, -0.15922025413148932, -0.3613347446338998, 0.035874455379477393, -0.3714048955589533, 0.01814926956883735, 0.17456010942502567, 0.02511484309410055... |
710.3543 | The significance of numerical coincidences in nature | This is the first part of a survey whose ultimate purpose is to clarify the
significance of the famous coincidence between the Hubble age of the universe
and a certain combination of microphysical parameters. In this part the way is
prepared by a discussion of the manner in which familiar local phenomena depend
quali... | hep-th astro-ph gr-qc hep-ph | this is the first part of a survey whose ultimate purpose is to clarify the significance of the famous coincidence between the hubble age of the universe and a certain combination of microphysical parameters in this part the way is prepared by a discussion of the manner in which familiar local phenomena depend qualitat... | [['this', 'is', 'the', 'first', 'part', 'of', 'a', 'survey', 'whose', 'ultimate', 'purpose', 'is', 'to', 'clarify', 'the', 'significance', 'of', 'the', 'famous', 'coincidence', 'between', 'the', 'hubble', 'age', 'of', 'the', 'universe', 'and', 'a', 'certain', 'combination', 'of', 'microphysical', 'parameters', 'in', 't... | [-0.12022213023457178, 0.15241751442577847, -0.05145231098867953, 0.08588121350591169, -0.11004578407339163, -0.051365581838150605, 0.04073205948991113, 0.317976486468851, -0.2554153841618947, -0.3304264080923116, 0.055177788847032117, -0.2307188567386842, -0.10409088698705952, 0.18512592876325934, -0.00076616658081643... |
710.3544 | Wigner functions, Fresnel optics, and symplectic connections on phase
space | We prove that Wigner functions contain a symplectic connection. The latter
covariantises the symplectic exterior derivative on phase space. We analyse the
role played by this connection and introduce the notion of local symplectic
covariance of quantum-mechanical states. This latter symmetry is at work in the
Schroed... | math-ph hep-th math.MP quant-ph | we prove that wigner functions contain a symplectic connection the latter covariantises the symplectic exterior derivative on phase space we analyse the role played by this connection and introduce the notion of local symplectic covariance of quantummechanical states this latter symmetry is at work in the schroedinger ... | [['we', 'prove', 'that', 'wigner', 'functions', 'contain', 'a', 'symplectic', 'connection', 'the', 'latter', 'covariantises', 'the', 'symplectic', 'exterior', 'derivative', 'on', 'phase', 'space', 'we', 'analyse', 'the', 'role', 'played', 'by', 'this', 'connection', 'and', 'introduce', 'the', 'notion', 'of', 'local', '... | [-0.18993242451921105, 0.11618081262335181, -0.12576122650643812, 0.09336725583998487, -0.11183098251698538, -0.041269821850582956, 0.005817690510302782, 0.3454914901405573, -0.2620375307369977, -0.2120777479559183, 0.04752608227310702, -0.23452413212507964, -0.2392721326649189, 0.05849712233990431, -0.0717381857894361... |
710.3545 | Search for Dark Matter Annihilation in Draco with STACEE | For some time, the Draco dwarf spheroidal galaxy has garnered interest as a
possible source for the indirect detection of dark matter. Its large
mass-to-light ratio and relative proximity to the Earth provide favorable
conditions for the production of detectable gamma rays from dark matter
self-annihilation in its co... | astro-ph | for some time the draco dwarf spheroidal galaxy has garnered interest as a possible source for the indirect detection of dark matter its large masstolight ratio and relative proximity to the earth provide favorable conditions for the production of detectable gamma rays from dark matter selfannihilation in its core the ... | [['for', 'some', 'time', 'the', 'draco', 'dwarf', 'spheroidal', 'galaxy', 'has', 'garnered', 'interest', 'as', 'a', 'possible', 'source', 'for', 'the', 'indirect', 'detection', 'of', 'dark', 'matter', 'its', 'large', 'masstolight', 'ratio', 'and', 'relative', 'proximity', 'to', 'the', 'earth', 'provide', 'favorable', '... | [-0.09734975873749246, 0.2042069305222997, -0.06155468239829096, 0.1377205324266581, -0.1027092083846694, -0.05296186363913727, 0.015933097499346703, 0.38454285340041533, -0.14967896063260885, -0.4447244306151964, 0.041042886995140235, -0.3131359040509073, 0.019488976548463866, 0.2485841516861502, 0.012423668004458353,... |
710.3546 | OCHA and the swiss-cheese operad | In this paper we show that the relation between Kajiura-Stasheff's OCHA and
A. Voronov's swiss-cheese operad is analogous to the relation between SH Lie
algebras and the little discs operad. More precisely, we show that the OCHA
operad is quasi-isomorphic to the operad of top-dimensional homology classes of
the swiss... | math.QA math.AT | in this paper we show that the relation between kajiurastasheffs ocha and a voronovs swisscheese operad is analogous to the relation between sh lie algebras and the little discs operad more precisely we show that the ocha operad is quasiisomorphic to the operad of topdimensional homology classes of the swisscheese oper... | [['in', 'this', 'paper', 'we', 'show', 'that', 'the', 'relation', 'between', 'kajiurastasheffs', 'ocha', 'and', 'a', 'voronovs', 'swisscheese', 'operad', 'is', 'analogous', 'to', 'the', 'relation', 'between', 'sh', 'lie', 'algebras', 'and', 'the', 'little', 'discs', 'operad', 'more', 'precisely', 'we', 'show', 'that', ... | [-0.16943713291781023, -0.004801378017291426, -0.07151483315974475, 0.19375646469416097, -0.1784108379110694, -0.08840823579579592, -0.07821206195047126, 0.442020815089345, -0.4411471888050437, -0.2371669030096382, 0.0486513861711137, -0.21969018336385487, -0.26972891099750995, 0.14658427257090806, -0.25230681350454687... |
710.3547 | Quantum Noise, Scaling and Domain Formation in a Spinor BEC | In this paper we discuss Bose-Einstein spinor condensates for F=1 atoms in
the context of 87Rb, as studied experimentally by the Stamper-Kurn group
[Sadler et al. Nature (2006)]. The dynamical quantum fluctuations of a sample
that starts as a condensate of N atoms in a pure F=1, m_F = 0 state are
described in analogy... | cond-mat.stat-mech quant-ph | in this paper we discuss boseeinstein spinor condensates for f1 atoms in the context of 87rb as studied experimentally by the stamperkurn group sadler et al nature 2006 the dynamical quantum fluctuations of a sample that starts as a condensate of n atoms in a pure f1 m_f 0 state are described in analogy to the twomode ... | [['in', 'this', 'paper', 'we', 'discuss', 'boseeinstein', 'spinor', 'condensates', 'for', 'f1', 'atoms', 'in', 'the', 'context', 'of', '87rb', 'as', 'studied', 'experimentally', 'by', 'the', 'stamperkurn', 'group', 'sadler', 'et', 'al', 'nature', '2006', 'the', 'dynamical', 'quantum', 'fluctuations', 'of', 'a', 'sample... | [-0.16048629292250646, 0.24417345872681434, -0.033828560191670784, -0.00017164092187394763, 0.07569812824828671, -0.09903767022270975, 0.03461121490705976, 0.3094273624675615, -0.22034681499285574, -0.2677396373436242, 0.032204832165054494, -0.27281946911742644, -0.05914313463696774, 0.13381653681530484, 0.016146576149... |
710.3548 | Single and binary evolution of Population III stars and their supernovae
light curves | We present stellar evolution calculations for Population III stars for both
single and binary star evolution. Our models include 10 Msun and 16.5 Msun
single stars and a 10 Msun model star that undergoes an episode of accretion
resulting in a final mass of 16.1 Msun. For comparison, we present the
evolution of a sola... | astro-ph | we present stellar evolution calculations for population iii stars for both single and binary star evolution our models include 10 msun and 165 msun single stars and a 10 msun model star that undergoes an episode of accretion resulting in a final mass of 161 msun for comparison we present the evolution of a solar heavy... | [['we', 'present', 'stellar', 'evolution', 'calculations', 'for', 'population', 'iii', 'stars', 'for', 'both', 'single', 'and', 'binary', 'star', 'evolution', 'our', 'models', 'include', '10', 'msun', 'and', '165', 'msun', 'single', 'stars', 'and', 'a', '10', 'msun', 'model', 'star', 'that', 'undergoes', 'an', 'episode... | [-0.010698677394325838, 0.13731728069484678, -0.048336271955525034, 0.11389453181613038, -0.07720280010502018, -0.07760546119343348, 0.06636880757420445, 0.4177534327280658, -0.1200113441930188, -0.38655154746850484, 0.060054604452856965, -0.31943612258511644, -0.016369170379533452, 0.19904127833611182, -0.016299624033... |
710.3549 | Two-Qubit Hilbert-Schmidt Separability Functions and Probabilities for
Full-Dimensional Even-Dyson-Index Scenarios | We extend the findings and analyses of our two recent studies (Phys. Rev. A,
75, 032326 [2007] and arXiv:0704.3723) by, first, obtaining numerical estimates
of the separability function based on the (Euclidean, flat) Hilbert-Schmidt
(HS) metric for the 27-dimensional convex set of quaternionic two-qubit
systems. The ... | quant-ph math-ph math.MP | we extend the findings and analyses of our two recent studies phys rev a 75 032326 2007 and arxiv07043723 by first obtaining numerical estimates of the separability function based on the euclidean flat hilbertschmidt hs metric for the 27dimensional convex set of quaternionic twoqubit systems the estimated function appe... | [['we', 'extend', 'the', 'findings', 'and', 'analyses', 'of', 'our', 'two', 'recent', 'studies', 'phys', 'rev', 'a', '75', '032326', '2007', 'and', 'arxiv07043723', 'by', 'first', 'obtaining', 'numerical', 'estimates', 'of', 'the', 'separability', 'function', 'based', 'on', 'the', 'euclidean', 'flat', 'hilbertschmidt',... | [-0.10968761388760279, 0.0893518286250422, -0.019547532654970008, 0.0592040632474784, -0.008726395526900887, -0.17121402944219025, 0.04157435918562388, 0.32845334242481516, -0.16677852180813824, -0.24829993215868906, 0.09870338924708502, -0.28881681646795615, -0.17783204430495114, 0.174494181566543, -0.0459012773065992... |
710.355 | Free frobenius algebra on the differential forms of a manifold | We construct an action of a free resolution of the Frobenius properad on the
differential forms of a closed oriented manifold. As a consequence, the forms
of a manifold with values in a semi-simple Lie algebra have an additional
structure given by an action of a free resolution of the properad describing
Lie di-algeb... | math.QA math.AT | we construct an action of a free resolution of the frobenius properad on the differential forms of a closed oriented manifold as a consequence the forms of a manifold with values in a semisimple lie algebra have an additional structure given by an action of a free resolution of the properad describing lie dialgebras wi... | [['we', 'construct', 'an', 'action', 'of', 'a', 'free', 'resolution', 'of', 'the', 'frobenius', 'properad', 'on', 'the', 'differential', 'forms', 'of', 'a', 'closed', 'oriented', 'manifold', 'as', 'a', 'consequence', 'the', 'forms', 'of', 'a', 'manifold', 'with', 'values', 'in', 'a', 'semisimple', 'lie', 'algebra', 'ha... | [-0.22417076611727998, 0.023030106075007974, -0.09933287240238044, 0.010374187442817186, -0.1404966512008717, -0.07675516397871993, -0.07080148487237461, 0.3682487837382053, -0.33974625111410495, -0.26216527469979045, 0.11257291944460585, -0.18918759604556518, -0.14123300971920816, 0.18945929914582194, -0.1306223653649... |
710.3551 | Rubber friction on (apparently) smooth lubricated surfaces | We study rubber sliding friction on hard lubricated surfaces. We show that
even if the hard surface appears smooth to the naked eye, it may exhibit short
wavelength roughness, which may give the dominant contribution to rubber
friction. That is, the observed sliding friction is mainly due to the
viscoelastic deformat... | cond-mat.soft | we study rubber sliding friction on hard lubricated surfaces we show that even if the hard surface appears smooth to the naked eye it may exhibit short wavelength roughness which may give the dominant contribution to rubber friction that is the observed sliding friction is mainly due to the viscoelastic deformations of... | [['we', 'study', 'rubber', 'sliding', 'friction', 'on', 'hard', 'lubricated', 'surfaces', 'we', 'show', 'that', 'even', 'if', 'the', 'hard', 'surface', 'appears', 'smooth', 'to', 'the', 'naked', 'eye', 'it', 'may', 'exhibit', 'short', 'wavelength', 'roughness', 'which', 'may', 'give', 'the', 'dominant', 'contribution',... | [-0.16837863285433163, 0.1809881244931225, -0.16046399843286385, 0.032923511958185145, -0.12100339857498546, -0.22148444331795364, -0.046500424739553944, 0.4149409950069793, -0.2853118557144295, -0.24777620239788062, 0.09063376803646565, -0.27059421572205306, -0.2426803162285163, 0.22444816647012802, -0.181315709268311... |
710.3552 | Testing Born-Infeld electrodynamics in waveguides | Waveguides can be employed to test non-linear effects in electrodynamics. We
solve Born-Infeld equations for TE waves in a rectangular waveguide. We show
that the energy velocity acquires a dependence on the amplitude, and harmonic
components appear as a consequence of the non-linear behavior.
| hep-th physics.optics | waveguides can be employed to test nonlinear effects in electrodynamics we solve borninfeld equations for te waves in a rectangular waveguide we show that the energy velocity acquires a dependence on the amplitude and harmonic components appear as a consequence of the nonlinear behavior | [['waveguides', 'can', 'be', 'employed', 'to', 'test', 'nonlinear', 'effects', 'in', 'electrodynamics', 'we', 'solve', 'borninfeld', 'equations', 'for', 'te', 'waves', 'in', 'a', 'rectangular', 'waveguide', 'we', 'show', 'that', 'the', 'energy', 'velocity', 'acquires', 'a', 'dependence', 'on', 'the', 'amplitude', 'and'... | [-0.1712253093296154, 0.13266857086934827, -0.08604373841080815, 0.058579487461512064, -0.11417817493202165, -0.12225780867844481, -0.05800082688008181, 0.37273536647923966, -0.22847889990820971, -0.23542406236414204, 0.020710576584943654, -0.3191034040329131, -0.20084039073183454, 0.23092290458523415, 0.02443687738427... |
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