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 |
|---|---|---|---|---|---|---|
708.2949 | Can Extra Mixing in RGB and AGB Stars Be Attributed to Magnetic
Mechanisms? | It is known that there must be some weak form of transport (called cool
bottom processing, or CBP) acting in low mass RGB and AGB stars, adding nuclei,
newly produced near the hydrogen-burning shell, to the convective envelope. We
assume that this extra-mixing originates in a stellar dynamo operated by the
differenti... | astro-ph | it is known that there must be some weak form of transport called cool bottom processing or cbp acting in low mass rgb and agb stars adding nuclei newly produced near the hydrogenburning shell to the convective envelope we assume that this extramixing originates in a stellar dynamo operated by the differential rotation... | [['it', 'is', 'known', 'that', 'there', 'must', 'be', 'some', 'weak', 'form', 'of', 'transport', 'called', 'cool', 'bottom', 'processing', 'or', 'cbp', 'acting', 'in', 'low', 'mass', 'rgb', 'and', 'agb', 'stars', 'adding', 'nuclei', 'newly', 'produced', 'near', 'the', 'hydrogenburning', 'shell', 'to', 'the', 'convectiv... | [-0.10382432237709699, 0.21770138428517166, -0.0168598569154656, 0.09022027524509606, -0.08549138391651075, -0.04026846161438847, 0.06941393261980404, 0.39476173645608237, -0.19964783074014555, -0.34569511494821686, 0.07906660742131617, -0.23603446091309802, -0.03414129178168308, 0.18400164308207137, -0.056469390211790... |
708.295 | The D^4 R^4 term in type IIB string theory on T^2 and U-duality | We propose a manifestly U-duality invariant modular form for the D^4 R^4
interaction in type IIB string theory compactified on T^2. It receives
perturbative contributions upto two loops, and non-perturbative contributions
from D-instantons and (p,q) string instantons wrapping T^2. We provide evidence
for this modular... | hep-th | we propose a manifestly uduality invariant modular form for the d4 r4 interaction in type iib string theory compactified on t2 it receives perturbative contributions upto two loops and nonperturbative contributions from dinstantons and pq string instantons wrapping t2 we provide evidence for this modular form by showin... | [['we', 'propose', 'a', 'manifestly', 'uduality', 'invariant', 'modular', 'form', 'for', 'the', 'd4', 'r4', 'interaction', 'in', 'type', 'iib', 'string', 'theory', 'compactified', 'on', 't2', 'it', 'receives', 'perturbative', 'contributions', 'upto', 'two', 'loops', 'and', 'nonperturbative', 'contributions', 'from', 'd... | [-0.14644930697488404, 0.15309004789265265, -0.09404968727426995, 0.14764543595633806, -0.05466948089604618, -0.20675526104648323, 0.014818930641372352, 0.2877228416799873, -0.17948636911934665, -0.24540700281367583, 0.08686837086066634, -0.3235727698941316, -0.18447837540136353, 0.14071461617821404, -0.023040327313943... |
708.2951 | QCD corrections to t\bar t b \bar b productions via photon-photon
collisions at linear colliders | We calculated the complete next-to-leading order(NLO) QCD corrections to the
$t\bar t b \bar b$ production process at a $\gamma \gamma$ collider in the
standard model(SM). The calculation of the one-loop QCD correction includes the
evaluations of the hexagon and pentagon amplitudes. We studied the NLO QCD
corrected t... | hep-ph | we calculated the complete nexttoleading ordernlo qcd corrections to the tbar t b bar b production process at a gamma gamma collider in the standard modelsm the calculation of the oneloop qcd correction includes the evaluations of the hexagon and pentagon amplitudes we studied the nlo qcd corrected total cross section ... | [['we', 'calculated', 'the', 'complete', 'nexttoleading', 'ordernlo', 'qcd', 'corrections', 'to', 'the', 'tbar', 't', 'b', 'bar', 'b', 'production', 'process', 'at', 'a', 'gamma', 'gamma', 'collider', 'in', 'the', 'standard', 'modelsm', 'the', 'calculation', 'of', 'the', 'oneloop', 'qcd', 'correction', 'includes', 'the... | [-0.06805781271838236, 0.2100842764990684, -0.10075527882459116, 0.13188701949712042, -0.003591278939221809, -0.06599239311089702, 0.0587520464449007, 0.32404302055734435, -0.1911914802637268, -0.25504698895307537, -0.08091308321922507, -0.3854217807050137, 0.07321234428463808, 0.10484868220473621, 0.09411285888499525,... |
708.2952 | QED of excitons with nonlocal susceptibility in arbitrary-structured
dielectrics | We have constructed a complete quantum theory for an optical process of
excitons with nonlocal susceptibility originating from their center-of-mass
motion. This theory provides a practical calculation method for
arbitrary-structured nano-to-macro scale dielectrics where excitons are weakly
confined. We obtain good co... | physics.optics | we have constructed a complete quantum theory for an optical process of excitons with nonlocal susceptibility originating from their centerofmass motion this theory provides a practical calculation method for arbitrarystructured nanotomacro scale dielectrics where excitons are weakly confined we obtain good corresponde... | [['we', 'have', 'constructed', 'a', 'complete', 'quantum', 'theory', 'for', 'an', 'optical', 'process', 'of', 'excitons', 'with', 'nonlocal', 'susceptibility', 'originating', 'from', 'their', 'centerofmass', 'motion', 'this', 'theory', 'provides', 'a', 'practical', 'calculation', 'method', 'for', 'arbitrarystructured',... | [-0.08457161756714099, 0.16642376861825048, -0.07518454580086059, 0.034052521411028686, -0.053404564744439616, -0.20790695185885474, -0.008103239512600904, 0.3957516412603958, -0.21935949128137194, -0.2479163450068505, -0.04415626748432887, -0.3342389186587313, -0.16100565056669816, 0.1685908511923305, 0.02859237719455... |
708.2953 | Equilibrium-like behavior in far-from-equilibrium chemical reaction
networks | In an equilibrium chemical reaction mixture, the number of molecules present
obeys a Poisson distribution. We ask when the same is true of the steady state
of a nonequilibrium reaction network and obtain an essentially complete answer.
In particular, we show that networks with certain topological features must
have a... | cond-mat.stat-mech cond-mat.soft q-bio.MN | in an equilibrium chemical reaction mixture the number of molecules present obeys a poisson distribution we ask when the same is true of the steady state of a nonequilibrium reaction network and obtain an essentially complete answer in particular we show that networks with certain topological features must have a poiss... | [['in', 'an', 'equilibrium', 'chemical', 'reaction', 'mixture', 'the', 'number', 'of', 'molecules', 'present', 'obeys', 'a', 'poisson', 'distribution', 'we', 'ask', 'when', 'the', 'same', 'is', 'true', 'of', 'the', 'steady', 'state', 'of', 'a', 'nonequilibrium', 'reaction', 'network', 'and', 'obtain', 'an', 'essentiall... | [-0.10909882707918962, 0.13529119131418882, -0.14225986658358747, 0.0797456284694562, -0.015161344969875357, -0.1343607798982621, 0.05411248738626332, 0.3115482480982005, -0.3094774969759282, -0.2508335776177099, 0.02826868022499041, -0.2500962754109812, -0.16916834463606054, 0.1752393777178747, -0.0659112826544331, 0.... |
708.2954 | Coronal Neutrino Emission in Hypercritical Accretion Flows | Hypercritical accretion flows onto stellar mass black holes (BHs) are
commonly considered as a promising model of central engines of gamma-ray bursts
(GRBs). In this model a certain fraction of gravitational binding energy of
accreting matter is deposited to the energy of relativistic jets via neutrino
annihilation a... | astro-ph | hypercritical accretion flows onto stellar mass black holes bhs are commonly considered as a promising model of central engines of gammaray bursts grbs in this model a certain fraction of gravitational binding energy of accreting matter is deposited to the energy of relativistic jets via neutrino annihilation andor mag... | [['hypercritical', 'accretion', 'flows', 'onto', 'stellar', 'mass', 'black', 'holes', 'bhs', 'are', 'commonly', 'considered', 'as', 'a', 'promising', 'model', 'of', 'central', 'engines', 'of', 'gammaray', 'bursts', 'grbs', 'in', 'this', 'model', 'a', 'certain', 'fraction', 'of', 'gravitational', 'binding', 'energy', 'o... | [-0.05730491208146403, 0.22303556176950728, -0.015021524078603753, 0.17434211098261426, -0.07370048069628964, -0.057036586237861675, 0.04355340693811221, 0.3709072091282059, -0.22416340308142946, -0.34211356650021946, 0.048810493028158264, -0.2828108896924691, 0.011209044299588349, 0.23480227184018274, 0.00907961350603... |
708.2955 | Gamma-ray emission from massive young stellar objects | Massive stars form in dense and massive molecular cores. The exact formation
mechanism is unclear, but it is possible that some massive stars are formed by
processes similar to those that produce the low-mass stars, with
accretion/ejection phenomena occurring at some point of the evolution of the
protostar. This pict... | astro-ph | massive stars form in dense and massive molecular cores the exact formation mechanism is unclear but it is possible that some massive stars are formed by processes similar to those that produce the lowmass stars with accretionejection phenomena occurring at some point of the evolution of the protostar this picture seem... | [['massive', 'stars', 'form', 'in', 'dense', 'and', 'massive', 'molecular', 'cores', 'the', 'exact', 'formation', 'mechanism', 'is', 'unclear', 'but', 'it', 'is', 'possible', 'that', 'some', 'massive', 'stars', 'are', 'formed', 'by', 'processes', 'similar', 'to', 'those', 'that', 'produce', 'the', 'lowmass', 'stars', '... | [-0.09122931430499781, 0.187294735726227, -0.07230644781055733, 0.12894867631223272, -0.08542113910467984, -0.05950120897671463, -0.003622809796155814, 0.43953220013748195, -0.2153775910763572, -0.2963377965860726, 0.050433152958787246, -0.27671969742970726, -0.0006079992005491958, 0.18729448470140936, 0.01336475310883... |
708.2956 | At Least Half Of All Graphs Satisfy \chi \leq {1/4}\omega + {3/4}\Delta
+ 1 | We prove that for any graph G at least one of G or $\bar{G}$ satisfies $\chi
\leq {1/4}\omega + {3/4}\Delta + 1$. In particular, self-complementary graphs
satisfy this bound.
| math.CO | we prove that for any graph g at least one of g or barg satisfies chi leq 14omega 34delta 1 in particular selfcomplementary graphs satisfy this bound | [['we', 'prove', 'that', 'for', 'any', 'graph', 'g', 'at', 'least', 'one', 'of', 'g', 'or', 'barg', 'satisfies', 'chi', 'leq', '14omega', '34delta', '1', 'in', 'particular', 'selfcomplementary', 'graphs', 'satisfy', 'this', 'bound']] | [-0.24999261159449815, 0.15988053295761348, -0.043452028054744005, 0.00647602868732065, -0.11494257528334856, -0.2671924978494644, 0.010092854741960764, 0.36559963467530904, -0.24402286060154438, -0.33180230267345906, 0.06444756663870066, -0.3381089086830616, -0.09969456140883266, 0.13208859770558776, -0.06847566820681... |
708.2957 | A quantization of the Hitchin hamiltonian system and the
Beilinson-Drinfeld isomorphism | We will study the Hitchin's hamiltonian system for a modular stack of
principal SL_2(C) bundle on a smooth projective curve which has a parabolic
reduction at certain points. As an application we will obtain a generalization
of the Beilinson-Drinfeld isomorphism, which is a quantization of the Hitchin's
hamiltonian s... | math.AG math.QA | we will study the hitchins hamiltonian system for a modular stack of principal sl_2c bundle on a smooth projective curve which has a parabolic reduction at certain points as an application we will obtain a generalization of the beilinsondrinfeld isomorphism which is a quantization of the hitchins hamiltonian system | [['we', 'will', 'study', 'the', 'hitchins', 'hamiltonian', 'system', 'for', 'a', 'modular', 'stack', 'of', 'principal', 'sl_2c', 'bundle', 'on', 'a', 'smooth', 'projective', 'curve', 'which', 'has', 'a', 'parabolic', 'reduction', 'at', 'certain', 'points', 'as', 'an', 'application', 'we', 'will', 'obtain', 'a', 'genera... | [-0.26004038568662136, -0.01604171488546928, -0.15824716090585808, 0.029437964413866247, -0.10774829831658578, -0.15334286326922628, -0.010005687686557673, 0.29699365551374396, -0.32105250306883637, -0.1863793625439308, 0.1374863695201217, -0.23600894779118956, -0.19435200676778142, 0.2314678615681371, -0.1700452897051... |
708.2958 | Quantum critical phenomena of unconventional superconductors: U(1) gauge
model of link Cooper pair | In this paper we shall study quantum critical behavior of lattice model of
unconventional superconductors (SC) that was proposed in the previous papers.
In this model, the Cooper-pair (CP) field is defined on lattice links in order
to describe d-wave SC. The CP field can be regarded as a U(1) lattice gauge
field, and... | cond-mat.supr-con cond-mat.str-el hep-lat | in this paper we shall study quantum critical behavior of lattice model of unconventional superconductors sc that was proposed in the previous papers in this model the cooperpair cp field is defined on lattice links in order to describe dwave sc the cp field can be regarded as a u1 lattice gauge field and the sc phase ... | [['in', 'this', 'paper', 'we', 'shall', 'study', 'quantum', 'critical', 'behavior', 'of', 'lattice', 'model', 'of', 'unconventional', 'superconductors', 'sc', 'that', 'was', 'proposed', 'in', 'the', 'previous', 'papers', 'in', 'this', 'model', 'the', 'cooperpair', 'cp', 'field', 'is', 'defined', 'on', 'lattice', 'links... | [-0.20162056446541718, 0.20993895539964633, -0.06476124364386249, 0.05792102045884662, -0.04452319529459432, -0.10899968273080295, 0.08522866114360532, 0.3463485965446111, -0.24005619697666988, -0.2843954918497099, 0.04960936982130445, -0.2649158327322867, -0.1588204482979284, 0.09742799990012177, 0.05912361575029396, ... |
708.2959 | Molecular Line Observations of the Small Protostellar Group L1251B | We present molecular line observations of L1251B, a small group of pre- and
protostellar objects, and its immediate environment in the dense C18O core
L1251E. These data are complementary to near-infrared, submillimeter and
millimeter continuum observations reported by Lee et al. (2006, ApJ, 648, 491;
Paper I). The s... | astro-ph | we present molecular line observations of l1251b a small group of pre and protostellar objects and its immediate environment in the dense c18o core l1251e these data are complementary to nearinfrared submillimeter and millimeter continuum observations reported by lee et al 2006 apj 648 491 paper i the singledish data o... | [['we', 'present', 'molecular', 'line', 'observations', 'of', 'l1251b', 'a', 'small', 'group', 'of', 'pre', 'and', 'protostellar', 'objects', 'and', 'its', 'immediate', 'environment', 'in', 'the', 'dense', 'c18o', 'core', 'l1251e', 'these', 'data', 'are', 'complementary', 'to', 'nearinfrared', 'submillimeter', 'and', '... | [-0.07057906937371526, 0.09475782660903254, -0.029602793699337375, 0.03893997822577755, -0.06729055382725266, -0.09118195646545953, 0.026250505946162673, 0.48467751518719726, -0.15091960329200244, -0.32352604808906715, 0.08277301281897557, -0.24546048795597422, -0.057986364406016136, 0.14905358366254304, -0.02029325405... |
708.296 | Rational Solutions of the Noumi and Yamada System of type $A_5^{(1)}$ | We completely classify all of rational solutions of the Noumi and Yamada
system of type $A_5^{(1)}$, which is a generalization of the fifth Painlev\'e
equation. The rational solutions are classified to five classes by the
B\"acklund transformation group.
| math.CA math.AC math.AG | we completely classify all of rational solutions of the noumi and yamada system of type a_51 which is a generalization of the fifth painleve equation the rational solutions are classified to five classes by the backlund transformation group | [['we', 'completely', 'classify', 'all', 'of', 'rational', 'solutions', 'of', 'the', 'noumi', 'and', 'yamada', 'system', 'of', 'type', 'a_51', 'which', 'is', 'a', 'generalization', 'of', 'the', 'fifth', 'painleve', 'equation', 'the', 'rational', 'solutions', 'are', 'classified', 'to', 'five', 'classes', 'by', 'the', 'b... | [-0.21112568014742514, -0.03279472597090429, -0.05787239738396908, 0.040693839218491984, -0.13376565663585147, -0.2064311029757128, 0.0011607836380502896, 0.22745748599501034, -0.31751336872969804, -0.2347812360446704, 0.13067733960863398, -0.33653349429368973, -0.20120706977812866, 0.18332889024168253, -0.051286122688... |
708.2961 | Cancellation problem for projective modules over affine algebras | Let A be a ring of dimension d and let P be a projective A-module of rank d.
We prove that if for every finite extension R of A, R^d is cancellative, then P
is cancellative. This gives an alternate proof of Bhatwadekar's result: every
projective module of rank d over an affine algebra of dimension d over a
C_1-field ... | math.AC math.KT | let a be a ring of dimension d and let p be a projective amodule of rank d we prove that if for every finite extension r of a rd is cancellative then p is cancellative this gives an alternate proof of bhatwadekars result every projective module of rank d over an affine algebra of dimension d over a c_1field of characte... | [['let', 'a', 'be', 'a', 'ring', 'of', 'dimension', 'd', 'and', 'let', 'p', 'be', 'a', 'projective', 'amodule', 'of', 'rank', 'd', 'we', 'prove', 'that', 'if', 'for', 'every', 'finite', 'extension', 'r', 'of', 'a', 'rd', 'is', 'cancellative', 'then', 'p', 'is', 'cancellative', 'this', 'gives', 'an', 'alternate', 'proof... | [-0.22016437185526477, 0.1231053079867635, -0.11361258814805279, -0.06101177260850319, -0.04720709915729422, -0.2589813973115501, -0.06205975596665168, 0.34234032611928733, -0.39191066944862113, -0.07886213674118706, 0.07088152550539806, -0.23447171910483317, -0.09636819482707948, 0.20550965475986765, -0.13850355064998... |
708.2962 | A Procedure to Solve the Eigen Solution to Dirac Equation | In this paper, we provide a procedure to solve the eigen solutions of Dirac
equation with complicated potential approximately. At first, we solve the eigen
solutions of a linear Dirac equation with complete eigen system, which
approximately equals to the original equation. Take the eigen functions as base
of Hilbert ... | physics.gen-ph | in this paper we provide a procedure to solve the eigen solutions of dirac equation with complicated potential approximately at first we solve the eigen solutions of a linear dirac equation with complete eigen system which approximately equals to the original equation take the eigen functions as base of hilbert space a... | [['in', 'this', 'paper', 'we', 'provide', 'a', 'procedure', 'to', 'solve', 'the', 'eigen', 'solutions', 'of', 'dirac', 'equation', 'with', 'complicated', 'potential', 'approximately', 'at', 'first', 'we', 'solve', 'the', 'eigen', 'solutions', 'of', 'a', 'linear', 'dirac', 'equation', 'with', 'complete', 'eigen', 'syste... | [-0.08976364902554626, 0.01987912158397699, -0.10504339919942948, 0.030218258955177258, -0.11856469375579948, -0.11108423564865282, 0.02030748428513456, 0.29338994221479603, -0.32328775856229996, -0.251416095410182, 0.11369658244957188, -0.27284969993152025, -0.15052665417280162, 0.16931919528717043, -0.004283376884731... |
708.2963 | Tripartite entanglement and threshold properties of coupled intracavity
downconversion and sum-frequency generation | The process of cascaded downconversion and sum-frequency generation inside an
optical cavity has been predicted to be a potential source of three-mode
continuous-variable entanglement. When the cavity is pumped by two fields, the
threshold properties have been analysed, showing that these are more
complicated than in... | quant-ph | the process of cascaded downconversion and sumfrequency generation inside an optical cavity has been predicted to be a potential source of threemode continuousvariable entanglement when the cavity is pumped by two fields the threshold properties have been analysed showing that these are more complicated than in wellkno... | [['the', 'process', 'of', 'cascaded', 'downconversion', 'and', 'sumfrequency', 'generation', 'inside', 'an', 'optical', 'cavity', 'has', 'been', 'predicted', 'to', 'be', 'a', 'potential', 'source', 'of', 'threemode', 'continuousvariable', 'entanglement', 'when', 'the', 'cavity', 'is', 'pumped', 'by', 'two', 'fields', '... | [-0.1333856592951413, 0.1509899188118156, -0.08874666094638858, 0.018686875745557205, -0.023120804647491736, -0.15640984309456227, 0.025502260359864908, 0.4177846667993105, -0.23361304108490885, -0.2629687745109991, 0.10202640117407127, -0.2525626411500553, -0.09305192593478062, 0.2516674745923162, 0.002627073469656435... |
708.2964 | General multipartite entangled states and complex projective variety | We discuss and investigate the geometrical structure of general multipartite
states. In particular, we show that a geometrical measure of entanglement for
general multipartite states can be constructed by the complex projective
varieties defined by quadratic polynomials.
| quant-ph | we discuss and investigate the geometrical structure of general multipartite states in particular we show that a geometrical measure of entanglement for general multipartite states can be constructed by the complex projective varieties defined by quadratic polynomials | [['we', 'discuss', 'and', 'investigate', 'the', 'geometrical', 'structure', 'of', 'general', 'multipartite', 'states', 'in', 'particular', 'we', 'show', 'that', 'a', 'geometrical', 'measure', 'of', 'entanglement', 'for', 'general', 'multipartite', 'states', 'can', 'be', 'constructed', 'by', 'the', 'complex', 'projectiv... | [-0.17659841470319676, 0.1564274238221146, -0.06736490477782649, 0.12654361077206763, -0.018294642905931215, -0.1619884334127041, -0.0366478989253173, 0.32502595921726646, -0.2937596855131355, -0.20888076068179026, 0.044667653912502166, -0.1685374693794025, -0.20743573759053205, 0.16242617049027938, -0.1130850840158559... |
708.2965 | Constraining crystalline color superconducting quark matter with
gravitational-wave data | We estimate the maximum equatorial ellipticity sustainable by compact stars
composed of crystalline color-superconducting quark matter. For the
theoretically allowed range of the gap parameter $\Delta$, the maximum
ellipticity could be as large as $10^{-2}$, which is about 4 orders of
magnitude larger than the tighte... | astro-ph gr-qc hep-ph | we estimate the maximum equatorial ellipticity sustainable by compact stars composed of crystalline colorsuperconducting quark matter for the theoretically allowed range of the gap parameter delta the maximum ellipticity could be as large as 102 which is about 4 orders of magnitude larger than the tightest upper limit ... | [['we', 'estimate', 'the', 'maximum', 'equatorial', 'ellipticity', 'sustainable', 'by', 'compact', 'stars', 'composed', 'of', 'crystalline', 'colorsuperconducting', 'quark', 'matter', 'for', 'the', 'theoretically', 'allowed', 'range', 'of', 'the', 'gap', 'parameter', 'delta', 'the', 'maximum', 'ellipticity', 'could', '... | [-0.12301132748123361, 0.21470255270994837, -0.0224148522037366, 0.09008759615082657, -0.11000904538802085, -0.03661782650225279, 0.08270289773483658, 0.32380281553681317, -0.14503683477717763, -0.3653278954378847, 0.10001867485536625, -0.279459591586298, -0.027762709354040755, 0.27120987624867765, 0.02423678723991745,... |
708.2966 | Quantum fluctuations in the transverse Ising spin glass model: A field
theory of random quantum spin systems | We develop a mean-field theory for random quantum spin systems using the spin
coherent state path integral representation. After the model is reduced to the
mean field one-body Hamiltonian, the integral is analyzed with the aid of
several methods such as the semiclassical method and the gauge transformation.
As an ap... | cond-mat.dis-nn | we develop a meanfield theory for random quantum spin systems using the spin coherent state path integral representation after the model is reduced to the mean field onebody hamiltonian the integral is analyzed with the aid of several methods such as the semiclassical method and the gauge transformation as an applicati... | [['we', 'develop', 'a', 'meanfield', 'theory', 'for', 'random', 'quantum', 'spin', 'systems', 'using', 'the', 'spin', 'coherent', 'state', 'path', 'integral', 'representation', 'after', 'the', 'model', 'is', 'reduced', 'to', 'the', 'mean', 'field', 'onebody', 'hamiltonian', 'the', 'integral', 'is', 'analyzed', 'with', ... | [-0.1200354736763984, 0.13281989781450346, -0.12137281411560252, 0.08143283839841994, -0.034176310460316016, -0.05763300663481156, 0.03114600100767954, 0.33286548148219786, -0.25444342593352, -0.28636292621182896, 0.06677626258266779, -0.2592948459575079, -0.1314910172407205, 0.16960205981740728, 0.03855775299016386, 0... |
708.2967 | The Second Born Corrections to the Electrical and Thermal Conductivities
of Dense Matter in the Liquid Metal Phase | The second Born corrections to the electrical and thermal conductivities are
calculated for the dense matter in the liquid metal phase for various elemental
compositions of astrophysical importance. Inclusion up to the second Born
corrections is sufficiently accurate for the Coulomb scattering of the
electrons by the... | astro-ph | the second born corrections to the electrical and thermal conductivities are calculated for the dense matter in the liquid metal phase for various elemental compositions of astrophysical importance inclusion up to the second born corrections is sufficiently accurate for the coulomb scattering of the electrons by the at... | [['the', 'second', 'born', 'corrections', 'to', 'the', 'electrical', 'and', 'thermal', 'conductivities', 'are', 'calculated', 'for', 'the', 'dense', 'matter', 'in', 'the', 'liquid', 'metal', 'phase', 'for', 'various', 'elemental', 'compositions', 'of', 'astrophysical', 'importance', 'inclusion', 'up', 'to', 'the', 'sec... | [-0.040144860089101175, 0.11065876204535435, -0.07197509683216366, 0.06028704869478496, -0.011729996649494754, -0.058087320868002536, 0.07037431772782969, 0.35037890015698875, -0.17533081868009973, -0.32577409261048085, 0.03551184058279458, -0.3207966723697789, -0.06323748311112201, 0.23148107935229906, 0.0334127041676... |
708.2968 | Search for strange tribaryon states in the inclusive
^4He(K^{-}_{stopped}, p) reaction | A search for tribaryon states was performed at KEK-PS. We adopted the
$^4$He($K^-_{stopped}, p)$ reaction to populate the states with strangeness -1,
charge 0 and isospin 1. No significant narrow structure was observed in the
mass region from 3000 to 3200 MeV/c^2 in an inclusive missing mass spectrum.
The upper limit... | nucl-ex | a search for tribaryon states was performed at kekps we adopted the 4hek_stopped p reaction to populate the states with strangeness 1 charge 0 and isospin 1 no significant narrow structure was observed in the mass region from 3000 to 3200 mevc2 in an inclusive missing mass spectrum the upper limit of the formation bran... | [['a', 'search', 'for', 'tribaryon', 'states', 'was', 'performed', 'at', 'kekps', 'we', 'adopted', 'the', '4hek_stopped', 'p', 'reaction', 'to', 'populate', 'the', 'states', 'with', 'strangeness', '1', 'charge', '0', 'and', 'isospin', '1', 'no', 'significant', 'narrow', 'structure', 'was', 'observed', 'in', 'the', 'mas... | [-0.0985046325133625, 0.21443491603181095, -0.006668177680694498, 0.08692136012790043, 0.047699155257560494, -0.11546238933309413, 0.11883692696645129, 0.33666774790688625, -0.13207870958054937, -0.38245485638972465, -0.0012789437882375063, -0.3297293733169393, 0.1015392311042311, 0.09664915102000189, 0.060008044296055... |
708.2969 | Inequivalent quantization in the field of a ferromagnetic wire | We argue that it is possible to bind neutral atom (NA) to the ferromagnetic
wire (FW) by inequivalent quantization of the Hamiltonian. We follow the well
known von Neumann's method of self-adjoint extensions (SAE) to get this
inequivalent quantization, which is characterized by a parameter
\Sigma\in\mathbb{R}({mod}2\... | cond-mat.mtrl-sci hep-th | we argue that it is possible to bind neutral atom na to the ferromagnetic wire fw by inequivalent quantization of the hamiltonian we follow the well known von neumanns method of selfadjoint extensions sae to get this inequivalent quantization which is characterized by a parameter sigmainmathbbrmod2pi there exists a sin... | [['we', 'argue', 'that', 'it', 'is', 'possible', 'to', 'bind', 'neutral', 'atom', 'na', 'to', 'the', 'ferromagnetic', 'wire', 'fw', 'by', 'inequivalent', 'quantization', 'of', 'the', 'hamiltonian', 'we', 'follow', 'the', 'well', 'known', 'von', 'neumanns', 'method', 'of', 'selfadjoint', 'extensions', 'sae', 'to', 'get'... | [-0.16444613751497986, 0.17562896537544606, -0.06055385033947199, 0.08223899252126492, -0.08078758519176128, -0.2192117638935867, 0.0976055068624971, 0.31096612006825, -0.29678190184391234, -0.28748761400181266, 0.049588634308228005, -0.2466780842431555, -0.11027569974040878, 0.10153608812418367, -0.02950396723281301, ... |
708.297 | Wightman function and scalar Casimir densities for a wedge with two
cylindrical boundaries | Wightman function, the vacuum expectation values of the field square and the
energy-momentum tensor are investigated for a massive scalar field with general
curvature coupling parameter inside a wedge with two coaxial cylindrical
boundaries. It is assumed that the field obeys Dirichlet boundary condition on
bounding ... | hep-th quant-ph | wightman function the vacuum expectation values of the field square and the energymomentum tensor are investigated for a massive scalar field with general curvature coupling parameter inside a wedge with two coaxial cylindrical boundaries it is assumed that the field obeys dirichlet boundary condition on bounding surfa... | [['wightman', 'function', 'the', 'vacuum', 'expectation', 'values', 'of', 'the', 'field', 'square', 'and', 'the', 'energymomentum', 'tensor', 'are', 'investigated', 'for', 'a', 'massive', 'scalar', 'field', 'with', 'general', 'curvature', 'coupling', 'parameter', 'inside', 'a', 'wedge', 'with', 'two', 'coaxial', 'cylin... | [-0.1749686301781741, 0.1395530433301187, -0.07484779869711478, 0.04992055279899729, -0.07942098414744525, -0.09554919145782204, -0.045972065355825036, 0.31822017551509335, -0.22990592877575336, -0.2548868723238021, 0.09782073501150544, -0.2563029074785756, -0.12156204897240779, 0.14738713170164355, -0.0032760158449021... |
708.2971 | Indo-European languages tree by Levenshtein distance | The evolution of languages closely resembles the evolution of haploid
organisms. This similarity has been recently exploited \cite{GA,GJ} to
construct language trees. The key point is the definition of a distance among
all pairs of languages which is the analogous of a genetic distance. Many
methods have been propose... | physics.soc-ph physics.data-an q-bio.PE | the evolution of languages closely resembles the evolution of haploid organisms this similarity has been recently exploited citegagj to construct language trees the key point is the definition of a distance among all pairs of languages which is the analogous of a genetic distance many methods have been proposed to defi... | [['the', 'evolution', 'of', 'languages', 'closely', 'resembles', 'the', 'evolution', 'of', 'haploid', 'organisms', 'this', 'similarity', 'has', 'been', 'recently', 'exploited', 'citegagj', 'to', 'construct', 'language', 'trees', 'the', 'key', 'point', 'is', 'the', 'definition', 'of', 'a', 'distance', 'among', 'all', 'p... | [-0.09074164441496622, 0.07680386834767713, -0.08322009205664864, 0.12739237128128186, -0.09279152627810429, -0.10828500952256101, 0.07936424628164762, 0.37231677277980607, -0.2959485680456184, -0.3048953715294518, 0.04702012859287422, -0.31352317057387097, -0.1456736390316055, 0.18063956267414155, -0.08652131452830762... |
708.2972 | The inverse fallacy and quantum formalism | In the present article we consider the inverse fallacy, a well known
cognitive heuristic experimentally tested in cognitive science, which occurs
for intuitive judgments in situations of bounded rationality. We show that the
quantum formalism can be used to describe in a very simple and general way this
fallacy withi... | physics.gen-ph | in the present article we consider the inverse fallacy a well known cognitive heuristic experimentally tested in cognitive science which occurs for intuitive judgments in situations of bounded rationality we show that the quantum formalism can be used to describe in a very simple and general way this fallacy within the... | [['in', 'the', 'present', 'article', 'we', 'consider', 'the', 'inverse', 'fallacy', 'a', 'well', 'known', 'cognitive', 'heuristic', 'experimentally', 'tested', 'in', 'cognitive', 'science', 'which', 'occurs', 'for', 'intuitive', 'judgments', 'in', 'situations', 'of', 'bounded', 'rationality', 'we', 'show', 'that', 'the... | [-0.06435866077947316, 0.11627522754914514, -0.12249922878733586, 0.13739104937938065, -0.09285781293448697, -0.1830993491940473, 0.04512134562076137, 0.3683152672403106, -0.2735809198149094, -0.28185298384689705, -0.003919109233609605, -0.15106922473826603, -0.2767442407131922, 0.20723335525850062, -0.1261558530926023... |
708.2973 | Detecting q-Gaussian distributions and the normalization effect | We show that whenever data are gathered using a device that performs a
normalization-preprocessing, the ensuing normalized input, as recorded by the
measurement device, will always be q-Gaussian distributed if the incoming data
exhibit elliptical symmetry. As a consequence, great care should be exercised
when detecti... | cond-mat.stat-mech | we show that whenever data are gathered using a device that performs a normalizationpreprocessing the ensuing normalized input as recorded by the measurement device will always be qgaussian distributed if the incoming data exhibit elliptical symmetry as a consequence great care should be exercised when detecting qgauss... | [['we', 'show', 'that', 'whenever', 'data', 'are', 'gathered', 'using', 'a', 'device', 'that', 'performs', 'a', 'normalizationpreprocessing', 'the', 'ensuing', 'normalized', 'input', 'as', 'recorded', 'by', 'the', 'measurement', 'device', 'will', 'always', 'be', 'qgaussian', 'distributed', 'if', 'the', 'incoming', 'dat... | [-0.09063878632992146, 0.1376946314298674, -0.1638323013973703, 0.0686384053530553, -0.050358530150793765, -0.1653735561195357, 0.021956792336899834, 0.3949239171861884, -0.2901760280491358, -0.3062737114188901, 0.12842699453088802, -0.2727679096397955, -0.14712566078965922, 0.25564800839624313, -0.09559941727174334, 0... |
708.2974 | The Fuzzy Vault for fingerprints is Vulnerable to Brute Force Attack | The \textit{fuzzy vault} approach is one of the best studied and well
accepted ideas for binding cryptographic security into biometric
authentication. The vault has been implemented in connection with fingerprint
data by Uludag and Jain. We show that this instance of the vault is vulnerable
to brute force attack. An ... | cs.CV cs.CR | the textitfuzzy vault approach is one of the best studied and well accepted ideas for binding cryptographic security into biometric authentication the vault has been implemented in connection with fingerprint data by uludag and jain we show that this instance of the vault is vulnerable to brute force attack an intercep... | [['the', 'textitfuzzy', 'vault', 'approach', 'is', 'one', 'of', 'the', 'best', 'studied', 'and', 'well', 'accepted', 'ideas', 'for', 'binding', 'cryptographic', 'security', 'into', 'biometric', 'authentication', 'the', 'vault', 'has', 'been', 'implemented', 'in', 'connection', 'with', 'fingerprint', 'data', 'by', 'ulud... | [-0.10824065793888991, -0.028747891783196183, -0.1328126637387898, 0.12271904835098801, -0.1063743097666692, -0.2885844237938687, 0.059673178961480056, 0.3744338323863653, -0.27773537101981405, -0.32803823750793604, 0.14263143030553033, -0.2889257472284793, -0.1330388059320215, 0.22804825169617657, -0.16396032823863757... |
708.2975 | Neutrino flavor oscillations in background matter | We study the evolution of two mixed Dirac neutrinos in an external
axial-vector field. The dynamics of this system is described in the framework
of relativistic wave equations approach on the basis of the known solutions of
the Dirac equation in an external field with a given initial condition. The
general solution o... | hep-ph hep-th | we study the evolution of two mixed dirac neutrinos in an external axialvector field the dynamics of this system is described in the framework of relativistic wave equations approach on the basis of the known solutions of the dirac equation in an external field with a given initial condition the general solution of the... | [['we', 'study', 'the', 'evolution', 'of', 'two', 'mixed', 'dirac', 'neutrinos', 'in', 'an', 'external', 'axialvector', 'field', 'the', 'dynamics', 'of', 'this', 'system', 'is', 'described', 'in', 'the', 'framework', 'of', 'relativistic', 'wave', 'equations', 'approach', 'on', 'the', 'basis', 'of', 'the', 'known', 'sol... | [-0.16048786405693083, 0.12347526943074841, -0.06080734126518626, 0.08138003269228719, -0.032500596607432646, -0.09281113690367955, -0.008057976789845555, 0.3064921896393393, -0.23869025425793713, -0.3116992706177281, 0.05828422661322881, -0.2429085311082685, -0.1344606904815152, 0.1410837733670704, 0.03695752410053769... |
708.2976 | Voltage and temperature dependencies of conductivity in gated graphene | The resistivity of gated graphene is studied taking into account electron and
hole scattering by short- and long-range structural imperfections the
characteristics of disorder were taken from the scanning tunneling microscopy
data and by acoustic phonons. The calculations are based on the quasiclassical
kinetic equat... | cond-mat.mtrl-sci cond-mat.mes-hall | the resistivity of gated graphene is studied taking into account electron and hole scattering by short and longrange structural imperfections the characteristics of disorder were taken from the scanning tunneling microscopy data and by acoustic phonons the calculations are based on the quasiclassical kinetic equation w... | [['the', 'resistivity', 'of', 'gated', 'graphene', 'is', 'studied', 'taking', 'into', 'account', 'electron', 'and', 'hole', 'scattering', 'by', 'short', 'and', 'longrange', 'structural', 'imperfections', 'the', 'characteristics', 'of', 'disorder', 'were', 'taken', 'from', 'the', 'scanning', 'tunneling', 'microscopy', '... | [-0.13116012419355505, 0.1743170713975646, -0.08867740231554633, 0.019966096620155888, -0.007705072047372843, -0.154585421729235, 0.049072790775235374, 0.38974014646661137, -0.2596071674316018, -0.2828135285526514, 0.02775828627564795, -0.3855012070249628, -0.08925447741776336, 0.20790033952769948, 0.03477271251886347,... |
708.2977 | Two Component Model of Dark Energy | We consider the possibility that the dark energy is made up of two or more
independent components, each having a different equation of state. We fit the
model with supernova and gamma-ray burst (GRB) data from resent observations,
and use the Markov Chain Monte Carlo (MCMC) technique to estimate the allowed
parameter... | astro-ph | we consider the possibility that the dark energy is made up of two or more independent components each having a different equation of state we fit the model with supernova and gammaray burst grb data from resent observations and use the markov chain monte carlo mcmc technique to estimate the allowed parameter regions w... | [['we', 'consider', 'the', 'possibility', 'that', 'the', 'dark', 'energy', 'is', 'made', 'up', 'of', 'two', 'or', 'more', 'independent', 'components', 'each', 'having', 'a', 'different', 'equation', 'of', 'state', 'we', 'fit', 'the', 'model', 'with', 'supernova', 'and', 'gammaray', 'burst', 'grb', 'data', 'from', 'rese... | [-0.03899991168102989, 0.0820835647515624, -0.09849656998481163, 0.10508802980064716, -0.12336212607538875, -0.21194878058261513, 0.049121833180406076, 0.4207569949383683, -0.2466026597574134, -0.36870028954752554, 0.07752524186542038, -0.2973085738828077, 0.0095131016239654, 0.19113657145541818, 0.05407080698676188, 0... |
708.2978 | Entanglement Entropy in Extended Quantum Systems | After a brief introduction to the concept of entanglement in quantum systems,
I apply these ideas to many-body systems and show that the von Neumann entropy
is an effective way of characterising the entanglement between the degrees of
freedom in different regions of space. Close to a quantum phase transition it
has u... | cond-mat.stat-mech quant-ph | after a brief introduction to the concept of entanglement in quantum systems i apply these ideas to manybody systems and show that the von neumann entropy is an effective way of characterising the entanglement between the degrees of freedom in different regions of space close to a quantum phase transition it has univer... | [['after', 'a', 'brief', 'introduction', 'to', 'the', 'concept', 'of', 'entanglement', 'in', 'quantum', 'systems', 'i', 'apply', 'these', 'ideas', 'to', 'manybody', 'systems', 'and', 'show', 'that', 'the', 'von', 'neumann', 'entropy', 'is', 'an', 'effective', 'way', 'of', 'characterising', 'the', 'entanglement', 'betwe... | [-0.1177326888562395, 0.21509345026830629, -0.13726594526983368, 0.05370405799252554, 0.013383554411120713, -0.15897235844302207, 0.024649179979370765, 0.29255306393651365, -0.2779936914403851, -0.24227081252432142, 0.08958585887963776, -0.2694161896271488, -0.15540401272189158, 0.1727156043679525, -0.04935063760226162... |
708.2979 | Phase coexistence of cluster crystals: beyond the Gibbs phase rule | We report a study of the phase behavior of multiple-occupancy crystals
through simulation. We argue that in order to reproduce the equilibrium
behavior of such crystals it is essential to treat the number of lattice sites
as a constraining thermodynamic variable. The resulting free-energy
calculations thus differ con... | cond-mat.soft | we report a study of the phase behavior of multipleoccupancy crystals through simulation we argue that in order to reproduce the equilibrium behavior of such crystals it is essential to treat the number of lattice sites as a constraining thermodynamic variable the resulting freeenergy calculations thus differ considera... | [['we', 'report', 'a', 'study', 'of', 'the', 'phase', 'behavior', 'of', 'multipleoccupancy', 'crystals', 'through', 'simulation', 'we', 'argue', 'that', 'in', 'order', 'to', 'reproduce', 'the', 'equilibrium', 'behavior', 'of', 'such', 'crystals', 'it', 'is', 'essential', 'to', 'treat', 'the', 'number', 'of', 'lattice',... | [-0.09309450263662317, 0.1375094060209432, -0.13278242339441013, 0.04755042047374751, -0.029175543065278607, -0.09048868829349631, 0.0879987160605596, 0.3754634521205292, -0.24259378422469458, -0.2820714064395038, 0.06555002069461952, -0.30148340266406815, -0.1457755744790307, 0.18485027916781674, 0.045354809383557085,... |
708.298 | Astrophysical Configurations with Background Cosmology: Probing Dark
Energy at Astrophysical Scales | We explore the effects of a positive cosmological constant on astrophysical
and cosmological configurations described by a polytropic equation of state. We
derive the conditions for equilibrium and stability of such configurations and
consider some astrophysical examples where our analysis may be relevant. We
show th... | astro-ph gr-qc | we explore the effects of a positive cosmological constant on astrophysical and cosmological configurations described by a polytropic equation of state we derive the conditions for equilibrium and stability of such configurations and consider some astrophysical examples where our analysis may be relevant we show that i... | [['we', 'explore', 'the', 'effects', 'of', 'a', 'positive', 'cosmological', 'constant', 'on', 'astrophysical', 'and', 'cosmological', 'configurations', 'described', 'by', 'a', 'polytropic', 'equation', 'of', 'state', 'we', 'derive', 'the', 'conditions', 'for', 'equilibrium', 'and', 'stability', 'of', 'such', 'configura... | [-0.11916353975244787, 0.13747437233362003, -0.08666467477876191, 0.08278312281119439, -0.0756165963150247, -0.10413844084754335, 0.00527686130757747, 0.3110408313661353, -0.21795900684933106, -0.3236194367028689, 0.10192273601724798, -0.24755151082206978, -0.06600158403658968, 0.18206355465298749, 0.005863041318743751... |
708.2981 | A stabilization theorem for dynamics of continuous opinions | A stabilization theorem for processes of opinion dynamics is presented. The
theorem is applicable to a wide class of models of continuous opinion dynamics
based on averaging (like the models of Hegselmann-Krause and
Weisbuch-Deffuant). The analysis detects self-confidence as a driving force of
stabilization.
| physics.soc-ph | a stabilization theorem for processes of opinion dynamics is presented the theorem is applicable to a wide class of models of continuous opinion dynamics based on averaging like the models of hegselmannkrause and weisbuchdeffuant the analysis detects selfconfidence as a driving force of stabilization | [['a', 'stabilization', 'theorem', 'for', 'processes', 'of', 'opinion', 'dynamics', 'is', 'presented', 'the', 'theorem', 'is', 'applicable', 'to', 'a', 'wide', 'class', 'of', 'models', 'of', 'continuous', 'opinion', 'dynamics', 'based', 'on', 'averaging', 'like', 'the', 'models', 'of', 'hegselmannkrause', 'and', 'weisb... | [-0.1365946295078505, 0.08184878206388517, -0.14577842354562812, 0.07471861117201942, -0.04909757503562353, -0.1405488362810998, 0.04398309786550023, 0.32011509009382944, -0.24449492220512845, -0.23141300055960362, 0.14217430018206043, -0.19584310837936672, -0.14431975383988835, 0.23818884377198463, -0.0470230628270655... |
708.2982 | ILC Positron Production Target Simulation | A photon-positron conversion target of the undulator or laser based polarized
positron source is optimized using a modified GEANT-3 program adapted to count
the spin transfer. High intensity positron beam with around 0.75 polarisation
could be achieved choosing tungsten conversion target of 0.3 and 0.7 radiation
leng... | physics.ins-det | a photonpositron conversion target of the undulator or laser based polarized positron source is optimized using a modified geant3 program adapted to count the spin transfer high intensity positron beam with around 075 polarisation could be achieved choosing tungsten conversion target of 03 and 07 radiation lengths for ... | [['a', 'photonpositron', 'conversion', 'target', 'of', 'the', 'undulator', 'or', 'laser', 'based', 'polarized', 'positron', 'source', 'is', 'optimized', 'using', 'a', 'modified', 'geant3', 'program', 'adapted', 'to', 'count', 'the', 'spin', 'transfer', 'high', 'intensity', 'positron', 'beam', 'with', 'around', '075', '... | [-0.033089604426421365, 0.20581990933783775, -0.045806663954314195, 0.0630412675233839, -0.01694608360247792, -0.19992139297625366, 0.035166661202345254, 0.5128651906929489, -0.2463707266867442, -0.3649315905739676, 0.0017145716339209169, -0.27640227340864687, 0.1333686458605851, 0.26405584351335354, 0.0318948329197910... |
708.2983 | Velocity fluctuations in a one dimensional Inelastic Maxwell model | We consider the velocity fluctuations of a system of particles described by
the Inelastic Maxwell Model. The present work extends the methods, previously
employed to obtain the one-particle velocity distribution function, to the
study of the two particle correlations. Results regarding both the homogeneous
cooling pr... | cond-mat.stat-mech cond-mat.soft | we consider the velocity fluctuations of a system of particles described by the inelastic maxwell model the present work extends the methods previously employed to obtain the oneparticle velocity distribution function to the study of the two particle correlations results regarding both the homogeneous cooling process a... | [['we', 'consider', 'the', 'velocity', 'fluctuations', 'of', 'a', 'system', 'of', 'particles', 'described', 'by', 'the', 'inelastic', 'maxwell', 'model', 'the', 'present', 'work', 'extends', 'the', 'methods', 'previously', 'employed', 'to', 'obtain', 'the', 'oneparticle', 'velocity', 'distribution', 'function', 'to', '... | [-0.12800171733639823, 0.13312634521571454, -0.11800253488278638, 0.06120063091433773, 0.017400380175483104, -0.0447179372907461, 0.009380917421367485, 0.31451221151898306, -0.26408257011886843, -0.27197953894695576, 0.056952938376828875, -0.2877041285391897, -0.10562376963207498, 0.16582799487150623, 0.052639051454207... |
708.2984 | Are neutron stars with crystalline colour superconducting cores
interesting for the LIGO experiment? | We estimate the maximal deformation that can be sustained by a rotating
neutron star with a crystalline colour superconducting quark core. Our results
suggest that current gravitational-wave data from LIGO have already reached the
level where a detection would have been possible over a wide range of the
poorly constr... | gr-qc astro-ph | we estimate the maximal deformation that can be sustained by a rotating neutron star with a crystalline colour superconducting quark core our results suggest that current gravitationalwave data from ligo have already reached the level where a detection would have been possible over a wide range of the poorly constraine... | [['we', 'estimate', 'the', 'maximal', 'deformation', 'that', 'can', 'be', 'sustained', 'by', 'a', 'rotating', 'neutron', 'star', 'with', 'a', 'crystalline', 'colour', 'superconducting', 'quark', 'core', 'our', 'results', 'suggest', 'that', 'current', 'gravitationalwave', 'data', 'from', 'ligo', 'have', 'already', 'reac... | [-0.05811925702715946, 0.18830125325141436, -0.09805598349726581, 0.03863798518060766, -0.10649988736382666, -0.054403462932702706, 0.06886615832658247, 0.4091801235174879, -0.20430216182796088, -0.31746336091012556, 0.10518619739524822, -0.2299996289880352, -0.0896415017189785, 0.22141564581691822, -0.0607328765698649... |
708.2985 | Suppression of vortex channeling in meandered YBa2Cu3O7-d grain
boundaries | We report on the in-plane magnetic field (H) dependence of the critical
current density (Jc) in meandered and planar single grain boundaries (GBs)
isolated in YBa2Cu3O7-d (YBCO) coated conductors. The Jc(H)properties of the
planar GB are consistent with those previously seen in single GBs of YBCO films
grown on SrTiO... | cond-mat.supr-con | we report on the inplane magnetic field h dependence of the critical current density jc in meandered and planar single grain boundaries gbs isolated in yba2cu3o7d ybco coated conductors the jchproperties of the planar gb are consistent with those previously seen in single gbs of ybco films grown on srtio3 bicrystals in... | [['we', 'report', 'on', 'the', 'inplane', 'magnetic', 'field', 'h', 'dependence', 'of', 'the', 'critical', 'current', 'density', 'jc', 'in', 'meandered', 'and', 'planar', 'single', 'grain', 'boundaries', 'gbs', 'isolated', 'in', 'yba2cu3o7d', 'ybco', 'coated', 'conductors', 'the', 'jchproperties', 'of', 'the', 'planar'... | [-0.193936877142714, 0.16436646393101131, 0.02050318426157975, -0.05090320793726501, -0.052437848772625535, -0.13699052119342497, 0.04025536824530941, 0.45992277110261576, -0.20669197256923938, -0.28151263161657414, 0.031654957045173765, -0.23922873333058492, -0.04986773085381303, 0.2620064670467103, -0.032614150429049... |
708.2986 | On the Security of the Ping-Pong Protocol | We briefly review the security of the ping-pong protocol in light of several
attack scenarios suggested by various authors since the proposal of the
protocol. We refute one recent attack on an ideal quantum channel, and show
that a recent claim of falseness of our original security proof is erroneous.
| quant-ph | we briefly review the security of the pingpong protocol in light of several attack scenarios suggested by various authors since the proposal of the protocol we refute one recent attack on an ideal quantum channel and show that a recent claim of falseness of our original security proof is erroneous | [['we', 'briefly', 'review', 'the', 'security', 'of', 'the', 'pingpong', 'protocol', 'in', 'light', 'of', 'several', 'attack', 'scenarios', 'suggested', 'by', 'various', 'authors', 'since', 'the', 'proposal', 'of', 'the', 'protocol', 'we', 'refute', 'one', 'recent', 'attack', 'on', 'an', 'ideal', 'quantum', 'channel', ... | [-0.18809219679795205, 0.009927808738138992, -0.128373978510499, 0.03719506402732804, -0.02652311881072819, -0.22664263769052923, 0.11067095569800585, 0.30123675033450126, -0.1953995544370264, -0.28220829196274283, 0.13025875537423418, -0.23917173802852632, -0.20096758849918842, 0.21977787708863616, -0.1961926392279565... |
708.2987 | On the Low-lying zeros of Hasse-Weil L-functions for Elliptic Curves | In this paper, we obtain an unconditional density theorem concerning the
low-lying zeros of Hasse-Weil L-functions for a family of elliptic curves. From
this together with the Riemann hypothesis for these L-functions, we infer the
majorant of 27/14 (which is strictly less than 2) for the average rank of the
elliptic ... | math.NT | in this paper we obtain an unconditional density theorem concerning the lowlying zeros of hasseweil lfunctions for a family of elliptic curves from this together with the riemann hypothesis for these lfunctions we infer the majorant of 2714 which is strictly less than 2 for the average rank of the elliptic curves in th... | [['in', 'this', 'paper', 'we', 'obtain', 'an', 'unconditional', 'density', 'theorem', 'concerning', 'the', 'lowlying', 'zeros', 'of', 'hasseweil', 'lfunctions', 'for', 'a', 'family', 'of', 'elliptic', 'curves', 'from', 'this', 'together', 'with', 'the', 'riemann', 'hypothesis', 'for', 'these', 'lfunctions', 'we', 'infe... | [-0.18085937275840291, 0.043134396595821176, -0.16820433006445268, 0.10653598060739099, -0.07226301547428914, -0.12131608286591504, 0.050809329198994516, 0.2907380714595061, -0.21082120233793453, -0.27023496907525535, 0.12876766966354777, -0.25834271967474265, -0.08128171385233772, 0.2320175981630796, -0.09395688301723... |
708.2988 | The in-flight spectroscopic performance of the Swift XRT CCD camera
during 2006-2007 | The Swift X-ray Telescope focal plane camera is a front-illuminated MOS CCD,
providing a spectral response kernel of 135 eV FWHM at 5.9 keV as measured
before launch. We describe the CCD calibration program based on celestial and
on-board calibration sources, relevant in-flight experiences, and developments
in the CC... | astro-ph | the swift xray telescope focal plane camera is a frontilluminated mos ccd providing a spectral response kernel of 135 ev fwhm at 59 kev as measured before launch we describe the ccd calibration program based on celestial and onboard calibration sources relevant inflight experiences and developments in the ccd response ... | [['the', 'swift', 'xray', 'telescope', 'focal', 'plane', 'camera', 'is', 'a', 'frontilluminated', 'mos', 'ccd', 'providing', 'a', 'spectral', 'response', 'kernel', 'of', '135', 'ev', 'fwhm', 'at', '59', 'kev', 'as', 'measured', 'before', 'launch', 'we', 'describe', 'the', 'ccd', 'calibration', 'program', 'based', 'on',... | [-0.04920212397883006, 0.09133059710802627, -0.061182490335340844, 0.05697255514405697, -0.04518776618351694, -0.11119891769840251, 0.054091630821858416, 0.4550010101229418, -0.195716569049182, -0.40376444306457415, 0.10257917851686216, -0.36446959667955525, -0.07946635481494013, 0.2273394749936415, -0.0997047404434852... |
708.2989 | Fast optimal CMB power spectrum estimation with Hamiltonian sampling | We present a method for fast optimal estimation of the temperature angular
power spectrum from observations of the cosmic microwave background. We employ
a Hamiltonian Monte Carlo (HMC) sampler to obtain samples from the posterior
probability distribution of all the power spectrum coefficients given a set of
observat... | astro-ph | we present a method for fast optimal estimation of the temperature angular power spectrum from observations of the cosmic microwave background we employ a hamiltonian monte carlo hmc sampler to obtain samples from the posterior probability distribution of all the power spectrum coefficients given a set of observations ... | [['we', 'present', 'a', 'method', 'for', 'fast', 'optimal', 'estimation', 'of', 'the', 'temperature', 'angular', 'power', 'spectrum', 'from', 'observations', 'of', 'the', 'cosmic', 'microwave', 'background', 'we', 'employ', 'a', 'hamiltonian', 'monte', 'carlo', 'hmc', 'sampler', 'to', 'obtain', 'samples', 'from', 'the'... | [-0.055276584748957136, 0.042092221765713804, -0.14097600760730677, 0.055951694078715655, -0.06683846055391009, -0.09849662832053963, 0.08810887722569559, 0.4360641409823699, -0.23225795750770328, -0.37413078896117524, 0.11157881688681055, -0.27440467096670573, -0.07085364145824491, 0.2693402696515559, -0.0250319636308... |
708.299 | Quantum gravity and charge renormalization | We study the question of the gauge dependence of the quantum gravity
contribution to the running gauge coupling constant for electromagnetism. The
calculations are performed using dimensional regularization in a manifestly
gauge invariant and gauge condition independent formulation of the effective
action. It is show... | hep-th | we study the question of the gauge dependence of the quantum gravity contribution to the running gauge coupling constant for electromagnetism the calculations are performed using dimensional regularization in a manifestly gauge invariant and gauge condition independent formulation of the effective action it is shown th... | [['we', 'study', 'the', 'question', 'of', 'the', 'gauge', 'dependence', 'of', 'the', 'quantum', 'gravity', 'contribution', 'to', 'the', 'running', 'gauge', 'coupling', 'constant', 'for', 'electromagnetism', 'the', 'calculations', 'are', 'performed', 'using', 'dimensional', 'regularization', 'in', 'a', 'manifestly', 'ga... | [-0.15956862295845625, 0.20553324778086027, -0.1160257778168228, 0.09234418363681667, -0.07712397110220548, -0.16004987280639643, 0.005772524554206914, 0.32633746657017115, -0.16995179715465653, -0.33601126059688424, 0.03197459825408972, -0.27186656725668423, -0.1552633276662311, 0.09939489495072111, -0.018041996801322... |
708.2991 | Shape resonances in modified effective range theory for
electron-molecule collisions | We develop a simple model of shape resonances in electron-molecule collisions
that is based on the modified effective-range expansion and analytical
solutions of the Schrodinger equation for the long-range part of the
interaction potential. We apply our model to electron scattering on N$_2$ and
CO$_2$. The parameters... | physics.atom-ph | we develop a simple model of shape resonances in electronmolecule collisions that is based on the modified effectiverange expansion and analytical solutions of the schrodinger equation for the longrange part of the interaction potential we apply our model to electron scattering on n_2 and co_2 the parameters of the eff... | [['we', 'develop', 'a', 'simple', 'model', 'of', 'shape', 'resonances', 'in', 'electronmolecule', 'collisions', 'that', 'is', 'based', 'on', 'the', 'modified', 'effectiverange', 'expansion', 'and', 'analytical', 'solutions', 'of', 'the', 'schrodinger', 'equation', 'for', 'the', 'longrange', 'part', 'of', 'the', 'intera... | [-0.07915649252875785, 0.1243419431210939, -0.050338762876067665, 0.10294272695873155, -0.006452956785713988, -0.07665701833043602, 0.002238066345896749, 0.36027156386435744, -0.20101736859760422, -0.33166478433746044, 0.014703648864746182, -0.3148610025112118, -0.10554592940302211, 0.19493035574781797, 0.0596428618238... |
708.2992 | Quantum private queries | We propose a cheat sensitive quantum protocol to perform a private search on
a classical database which is efficient in terms of communication complexity.
It allows a user to retrieve an item from the server in possession of the
database without revealing which item she retrieved: if the server tries to
obtain inform... | quant-ph | we propose a cheat sensitive quantum protocol to perform a private search on a classical database which is efficient in terms of communication complexity it allows a user to retrieve an item from the server in possession of the database without revealing which item she retrieved if the server tries to obtain informatio... | [['we', 'propose', 'a', 'cheat', 'sensitive', 'quantum', 'protocol', 'to', 'perform', 'a', 'private', 'search', 'on', 'a', 'classical', 'database', 'which', 'is', 'efficient', 'in', 'terms', 'of', 'communication', 'complexity', 'it', 'allows', 'a', 'user', 'to', 'retrieve', 'an', 'item', 'from', 'the', 'server', 'in', ... | [-0.12051649874178913, -0.019149113415078606, -0.10061283251747313, 0.05236318475185475, -0.12220056814519234, -0.23422819881619314, 0.17364713497364556, 0.33991731627015614, -0.3184091089601357, -0.35599120323386735, 0.0855587825436795, -0.32351034408351353, -0.07768935690575286, 0.18424470459228368, -0.16267073171957... |
708.2993 | Quantum-like Description of Probabilistic Data from Shafir-Tversky
Experiments: evidence of trigonometric and hyperbolic (!) interference | In this paper we present quantum-like (QL) representation of the
Shafir-Tversky statistical effect. We apply so called contextual approach. The
Shafir-Tversky effect is considered as a consequence of combination of a number
of incompatible contexts which are involved e.g. in Prisoner's Dilemma or in
more general game... | physics.gen-ph | in this paper we present quantumlike ql representation of the shafirtversky statistical effect we apply so called contextual approach the shafirtversky effect is considered as a consequence of combination of a number of incompatible contexts which are involved eg in prisoners dilemma or in more general games inducing t... | [['in', 'this', 'paper', 'we', 'present', 'quantumlike', 'ql', 'representation', 'of', 'the', 'shafirtversky', 'statistical', 'effect', 'we', 'apply', 'so', 'called', 'contextual', 'approach', 'the', 'shafirtversky', 'effect', 'is', 'considered', 'as', 'a', 'consequence', 'of', 'combination', 'of', 'a', 'number', 'of',... | [-0.09521303120834221, 0.07096742688012975, -0.0891607355366328, 0.13161205471027643, -0.07848450298021947, -0.15810699907563894, 0.08713221769713397, 0.3308827640062996, -0.27426756556544984, -0.3243012299734567, 0.07243464917144073, -0.27250513411526167, -0.25855266134254634, 0.14963783906506642, -0.11782066722001348... |
708.2994 | Surface electric potential dynamic on graphite | We observe variations on the surface potential of graphite samples that we
attribute to the adsorption physisorption of tetracene isomers.
| cond-mat.mtrl-sci | we observe variations on the surface potential of graphite samples that we attribute to the adsorption physisorption of tetracene isomers | [['we', 'observe', 'variations', 'on', 'the', 'surface', 'potential', 'of', 'graphite', 'samples', 'that', 'we', 'attribute', 'to', 'the', 'adsorption', 'physisorption', 'of', 'tetracene', 'isomers']] | [-0.05729361418634653, 0.07956918841227889, -0.09327916130423546, 0.027450141590088607, 0.06184369260445237, -0.08726393850520253, 0.15256910879397764, 0.540305270254612, -0.24183782786130906, -0.2803830146789551, -0.09141344171948732, -0.34861104637384416, -0.15640957280993462, 0.07789633511565626, -0.0187113188672810... |
708.2995 | On the conjecture of Kevin Walker | In 1985 Kevin Walker in his study of topology of polygon spaces raised an
interesting conjecture in the spirit of the well-known question "Can you hear
the shape of a drum?" of Marc Kac. Roughly, Walker's conjecture asks if one can
recover relative lengths of the bars of a linkage from intrinsic algebraic
properties ... | math.AT math.GT | in 1985 kevin walker in his study of topology of polygon spaces raised an interesting conjecture in the spirit of the wellknown question can you hear the shape of a drum of marc kac roughly walkers conjecture asks if one can recover relative lengths of the bars of a linkage from intrinsic algebraic properties of the co... | [['in', '1985', 'kevin', 'walker', 'in', 'his', 'study', 'of', 'topology', 'of', 'polygon', 'spaces', 'raised', 'an', 'interesting', 'conjecture', 'in', 'the', 'spirit', 'of', 'the', 'wellknown', 'question', 'can', 'you', 'hear', 'the', 'shape', 'of', 'a', 'drum', 'of', 'marc', 'kac', 'roughly', 'walkers', 'conjecture'... | [-0.17463906260018938, 0.06724570850389447, -0.11960715772531759, 0.08312051285782912, -0.10397520714983595, -0.1485722333459665, 0.0007476954468463161, 0.3132724039507716, -0.3307445201881523, -0.22360140622038854, 0.0932882623289178, -0.23646809140303998, -0.17239120549370607, 0.18316748037311678, -0.1799124484630615... |
708.2996 | Structure and Nuclear Composition of General Relativistic,
Magnetohydrodynamic Outflows from Neutrino-Cooled Disks | We compute the structure and degree of neutronization of general relativistic
magnetohydrodynamic (GRMHD) outflows originating from the inner region of
neutrino-cooled disks. We consider both, outflows expelled from a hydrostatic
disk corona and outflows driven by disk turbulence. We show that in outflows
driven ther... | astro-ph | we compute the structure and degree of neutronization of general relativistic magnetohydrodynamic grmhd outflows originating from the inner region of neutrinocooled disks we consider both outflows expelled from a hydrostatic disk corona and outflows driven by disk turbulence we show that in outflows driven thermally fr... | [['we', 'compute', 'the', 'structure', 'and', 'degree', 'of', 'neutronization', 'of', 'general', 'relativistic', 'magnetohydrodynamic', 'grmhd', 'outflows', 'originating', 'from', 'the', 'inner', 'region', 'of', 'neutrinocooled', 'disks', 'we', 'consider', 'both', 'outflows', 'expelled', 'from', 'a', 'hydrostatic', 'di... | [-0.10749847261375556, 0.24600326633154754, -0.00468038768684935, 0.1554861168112857, -0.07912225930929362, -0.07904305986991698, -0.02889798880214729, 0.3999665409385685, -0.2734401876860786, -0.2929842704167915, 0.05278849151513968, -0.2681702157807729, 0.015414938600438218, 0.22885693101182816, 0.017655673593657814,... |
708.2997 | Topology of randon linkages | Betti numbers of configuration spaces of mechanical linkages (known also as
polygon spaces) depend on a large number of parameters -- the lengths of the
bars of the linkage. Motivated by applications in topological robotics,
statistical shape theory and molecular biology, we view these lengths as random
variables and... | math.AT math.PR | betti numbers of configuration spaces of mechanical linkages known also as polygon spaces depend on a large number of parameters the lengths of the bars of the linkage motivated by applications in topological robotics statistical shape theory and molecular biology we view these lengths as random variables and study asy... | [['betti', 'numbers', 'of', 'configuration', 'spaces', 'of', 'mechanical', 'linkages', 'known', 'also', 'as', 'polygon', 'spaces', 'depend', 'on', 'a', 'large', 'number', 'of', 'parameters', 'the', 'lengths', 'of', 'the', 'bars', 'of', 'the', 'linkage', 'motivated', 'by', 'applications', 'in', 'topological', 'robotics'... | [-0.17731773363231051, 0.1336912764686971, -0.04554824881826437, 0.1027260938464033, -0.041817209841082656, -0.05439127528018529, 0.06856537936818635, 0.31582532294334903, -0.25664111315798493, -0.31363766893909706, 0.09178802429420513, -0.2577707696736099, -0.1839372766853851, 0.2128581335062101, -0.11672736050170515,... |
708.2998 | Relative non-relativistic mechanics | Dynamic equations of non-relativistic mechanics are written in
covariant-coordinate form in terms of relative velocities and accelerations
with respect to an arbitrary reference frame. The notions of the
non-relativistic reference frame, inertial force, free motion equation, and
inertial frame are discussed.
| math-ph gr-qc math.MP | dynamic equations of nonrelativistic mechanics are written in covariantcoordinate form in terms of relative velocities and accelerations with respect to an arbitrary reference frame the notions of the nonrelativistic reference frame inertial force free motion equation and inertial frame are discussed | [['dynamic', 'equations', 'of', 'nonrelativistic', 'mechanics', 'are', 'written', 'in', 'covariantcoordinate', 'form', 'in', 'terms', 'of', 'relative', 'velocities', 'and', 'accelerations', 'with', 'respect', 'to', 'an', 'arbitrary', 'reference', 'frame', 'the', 'notions', 'of', 'the', 'nonrelativistic', 'reference', '... | [-0.15500057672616094, 0.18155324078725243, -0.07008422746002907, -0.004397075902670622, -0.030030329804867507, -0.09724474193062634, -0.15474639711901544, 0.3871298442129046, -0.2825318745337427, -0.28135136966157004, -0.06969095676322468, -0.22817932826001197, 0.009715818299446255, 0.1517357293283567, -0.120493867760... |
708.2999 | On the estimation of a parameter with incomplete knowledge on a nuisance
parameter | In this paper we consider the problem of estimating a parameter of a
probability distribution when we have some prior information on a nuisance
parameter. We start by the very simple case where we know perfectly the value
of the nuisance parameter. The complete likelihood is the classical tool in
this case. Then, pro... | physics.data-an | in this paper we consider the problem of estimating a parameter of a probability distribution when we have some prior information on a nuisance parameter we start by the very simple case where we know perfectly the value of the nuisance parameter the complete likelihood is the classical tool in this case then progressi... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'estimating', 'a', 'parameter', 'of', 'a', 'probability', 'distribution', 'when', 'we', 'have', 'some', 'prior', 'information', 'on', 'a', 'nuisance', 'parameter', 'we', 'start', 'by', 'the', 'very', 'simple', 'case', 'where', 'we', 'know', 'perfectly',... | [-0.04804937895875745, 0.050015221986473166, -0.10457934203735564, 0.08570514635221287, -0.08747225219980301, -0.09182676625671737, 0.10126956730508961, 0.3698814691564117, -0.271730084476246, -0.2960038483892794, 0.11971080270404003, -0.2336288546368982, -0.15414399543449228, 0.1604733794287967, -0.09788289340910561, ... |
708.3 | The Physical Properties of LBGs at z>5: Outflows and the "pre-enrichment
problem" | We discuss the properties of Lyman Break galaxies (LBGs) at z>5 as determined
from disparate fields covering approximately 500 sq. arcmin. While the broad
characteristics of the LBG population has been discussed extensively in the
literature, such as luminosity functions and clustering amplitude, we focus on
the deta... | astro-ph | we discuss the properties of lyman break galaxies lbgs at z5 as determined from disparate fields covering approximately 500 sq arcmin while the broad characteristics of the lbg population has been discussed extensively in the literature such as luminosity functions and clustering amplitude we focus on the detailed phys... | [['we', 'discuss', 'the', 'properties', 'of', 'lyman', 'break', 'galaxies', 'lbgs', 'at', 'z5', 'as', 'determined', 'from', 'disparate', 'fields', 'covering', 'approximately', '500', 'sq', 'arcmin', 'while', 'the', 'broad', 'characteristics', 'of', 'the', 'lbg', 'population', 'has', 'been', 'discussed', 'extensively', ... | [-0.031016878399742678, 0.11178400273805103, -0.0663378296997847, 0.15641428835070076, -0.07531955481102937, -0.017443655220039905, 0.03976438092123941, 0.46953102044693856, -0.13306507365834191, -0.34590652011649076, 0.06927637802436948, -0.28654271564572625, -0.04281935009387243, 0.19024853209168258, -0.0146531706299... |
708.3001 | Anomaly induced effects in a magnetic field | We consider a modification of electrodynamics by an additional light massive
vector field, interacting with the photon via Chern-Simons-like coupling. This
theory predicts observable effects for the experiments studying the propagation
of light in an external magnetic field, very similar to those, predicted by
theori... | hep-ph hep-th | we consider a modification of electrodynamics by an additional light massive vector field interacting with the photon via chernsimonslike coupling this theory predicts observable effects for the experiments studying the propagation of light in an external magnetic field very similar to those predicted by theories of ax... | [['we', 'consider', 'a', 'modification', 'of', 'electrodynamics', 'by', 'an', 'additional', 'light', 'massive', 'vector', 'field', 'interacting', 'with', 'the', 'photon', 'via', 'chernsimonslike', 'coupling', 'this', 'theory', 'predicts', 'observable', 'effects', 'for', 'the', 'experiments', 'studying', 'the', 'propaga... | [-0.13971344489926615, 0.2690762521396839, -0.054818949163801825, 0.13029399334202305, -0.08380086274387745, -0.14006215527008933, 0.024537722762817373, 0.29424786392885904, -0.20093112088954793, -0.36563864283693526, 0.02587374881662142, -0.27859302590816065, -0.1296613464776713, 0.18759110342138088, 0.027353521049595... |
708.3002 | Twisting all the way: from Classical Mechanics to Quantum Fields | We discuss the effects that a noncommutative geometry induced by a Drinfeld
twist has on physical theories. We systematically deform all products and
symmetries of the theory. We discuss noncommutative classical mechanics, in
particular its deformed Poisson bracket and hence time evolution and
symmetries. The twistin... | hep-th math-ph math.MP math.QA | we discuss the effects that a noncommutative geometry induced by a drinfeld twist has on physical theories we systematically deform all products and symmetries of the theory we discuss noncommutative classical mechanics in particular its deformed poisson bracket and hence time evolution and symmetries the twisting is t... | [['we', 'discuss', 'the', 'effects', 'that', 'a', 'noncommutative', 'geometry', 'induced', 'by', 'a', 'drinfeld', 'twist', 'has', 'on', 'physical', 'theories', 'we', 'systematically', 'deform', 'all', 'products', 'and', 'symmetries', 'of', 'the', 'theory', 'we', 'discuss', 'noncommutative', 'classical', 'mechanics', 'i... | [-0.13401223811052126, 0.16352076404583976, -0.1142209107344298, 0.12520991957424804, -0.12368922691897864, -0.08939894509127307, -0.007415088971347078, 0.323874933126661, -0.34152421554473716, -0.2423917747741162, 0.04809847600114791, -0.21524190046277242, -0.21075551432663017, 0.15810229516943397, -0.1407892982355143... |
708.3003 | The dynamics of vortex generation in superfluid 3He-B | A profound change occurs in the stability of quantized vortices in externally
applied flow of superfluid 3He-B at temperatures ~ 0.6 Tc, owing to the rapidly
decreasing damping in vortex motion with decreasing temperature. At low damping
an evolving vortex may become unstable and generate a new independent vortex
loo... | cond-mat.stat-mech cond-mat.supr-con | a profound change occurs in the stability of quantized vortices in externally applied flow of superfluid 3heb at temperatures 06 tc owing to the rapidly decreasing damping in vortex motion with decreasing temperature at low damping an evolving vortex may become unstable and generate a new independent vortex loop this s... | [['a', 'profound', 'change', 'occurs', 'in', 'the', 'stability', 'of', 'quantized', 'vortices', 'in', 'externally', 'applied', 'flow', 'of', 'superfluid', '3heb', 'at', 'temperatures', '06', 'tc', 'owing', 'to', 'the', 'rapidly', 'decreasing', 'damping', 'in', 'vortex', 'motion', 'with', 'decreasing', 'temperature', 'a... | [-0.19341400417366197, 0.2858245415847272, -0.08143933977310856, 0.011990688133630014, -0.04964310217515699, -0.13862845734914853, 0.04932376431256887, 0.33140560192543833, -0.2653140191698358, -0.24178532273508607, 0.08832235530107505, -0.26059850644142857, -0.022461089367667834, 0.18402624981965693, -0.01037539072512... |
708.3004 | The Far-Infrared Surveyor (FIS) for AKARI | The Far-Infrared Surveyor (FIS) is one of two focal plane instruments on the
AKARI satellite. FIS has four photometric bands at 65, 90, 140, and 160 um, and
uses two kinds of array detectors. The FIS arrays and optics are designed to
sweep the sky with high spatial resolution and redundancy. The actual scan
width is ... | astro-ph | the farinfrared surveyor fis is one of two focal plane instruments on the akari satellite fis has four photometric bands at 65 90 140 and 160 um and uses two kinds of array detectors the fis arrays and optics are designed to sweep the sky with high spatial resolution and redundancy the actual scan width is more than ei... | [['the', 'farinfrared', 'surveyor', 'fis', 'is', 'one', 'of', 'two', 'focal', 'plane', 'instruments', 'on', 'the', 'akari', 'satellite', 'fis', 'has', 'four', 'photometric', 'bands', 'at', '65', '90', '140', 'and', '160', 'um', 'and', 'uses', 'two', 'kinds', 'of', 'array', 'detectors', 'the', 'fis', 'arrays', 'and', 'o... | [-0.1079628061008087, 0.07513239620775394, -0.09815652340722199, 0.05770377663941542, -0.05032970915563855, -0.09188229052073599, 0.018024227707288586, 0.4476488215418962, -0.19341586062500438, -0.36619807673352106, 0.1285472007968545, -0.346163064558673, -0.07144294023657075, 0.25177954230329613, -0.03713913290866313,... |
708.3005 | The Struve-Sahade effect in the optical spectra of O-type binaries I.
Main-sequence systems | We present a spectroscopic analysis of four massive binary systems that are
known or are good candidates to display the Struve-Sahade effect (defined as
the apparent strengthening of the secondary spectrum of the binary when the
star is approaching, and the corresponding weakening of the lines when it is
receding).
... | astro-ph | we present a spectroscopic analysis of four massive binary systems that are known or are good candidates to display the struvesahade effect defined as the apparent strengthening of the secondary spectrum of the binary when the star is approaching and the corresponding weakening of the lines when it is receding we use h... | [['we', 'present', 'a', 'spectroscopic', 'analysis', 'of', 'four', 'massive', 'binary', 'systems', 'that', 'are', 'known', 'or', 'are', 'good', 'candidates', 'to', 'display', 'the', 'struvesahade', 'effect', 'defined', 'as', 'the', 'apparent', 'strengthening', 'of', 'the', 'secondary', 'spectrum', 'of', 'the', 'binary'... | [-0.15439054361342291, 0.10077859597184197, -0.04721949583700284, 0.06830613184579168, -0.05655431526600185, -0.13836541344091824, 0.04177107116104, 0.38067106991027944, -0.22873396254182826, -0.3184975507960777, 0.1142068924194183, -0.2578520678193073, -0.1116723799654706, 0.19967912600700263, -0.0563866020059901, -0.... |
708.3006 | Ihara's lemma for imaginary quadratic fields | An analogue over imaginary quadratic fields of a result in algebraic number
theory known as Ihara's lemma is established. More precisely, we show that for
a prime ideal P of the ring of integers of an imaginary quadratic field F, the
kernel of the sum of the two standard P-degeneracy maps between the cuspidal
sheaf c... | math.NT | an analogue over imaginary quadratic fields of a result in algebraic number theory known as iharas lemma is established more precisely we show that for a prime ideal p of the ring of integers of an imaginary quadratic field f the kernel of the sum of the two standard pdegeneracy maps between the cuspidal sheaf cohomolo... | [['an', 'analogue', 'over', 'imaginary', 'quadratic', 'fields', 'of', 'a', 'result', 'in', 'algebraic', 'number', 'theory', 'known', 'as', 'iharas', 'lemma', 'is', 'established', 'more', 'precisely', 'we', 'show', 'that', 'for', 'a', 'prime', 'ideal', 'p', 'of', 'the', 'ring', 'of', 'integers', 'of', 'an', 'imaginary',... | [-0.25518706135423574, 0.04637693995027803, -0.14783122514684996, 0.05974769744565805, -0.09611581854352896, -0.11831078532556391, -0.01885603232699625, 0.2899671305121497, -0.3698839278458947, -0.2009240196773199, 0.06084754703110178, -0.25240253868531626, -0.16573945068838922, 0.27086158261888404, -0.1000924795781346... |
708.3007 | On the measurement of B(E2, 0+ -> 2+) using intermediate-energy Coulomb
excitation | Coulomb excitation is a standard method used to extract quadrupole excitation
strengths of even-even nuclei. In typical analyses the reaction is assumed to
be one-step, Coulomb only, and is treated within a semi-classical model. In
this work, fully-quantal coupled-channel calculations are performed for three
test cas... | nucl-th nucl-ex | coulomb excitation is a standard method used to extract quadrupole excitation strengths of eveneven nuclei in typical analyses the reaction is assumed to be onestep coulomb only and is treated within a semiclassical model in this work fullyquantal coupledchannel calculations are performed for three test cases in order ... | [['coulomb', 'excitation', 'is', 'a', 'standard', 'method', 'used', 'to', 'extract', 'quadrupole', 'excitation', 'strengths', 'of', 'eveneven', 'nuclei', 'in', 'typical', 'analyses', 'the', 'reaction', 'is', 'assumed', 'to', 'be', 'onestep', 'coulomb', 'only', 'and', 'is', 'treated', 'within', 'a', 'semiclassical', 'mo... | [-0.0052201602957211435, 0.1435730410653066, -0.08139753828246994, 0.14613108811437547, -0.009050350725548724, -0.12758655010161232, 0.04495873578109664, 0.36199616067979024, -0.18754604654003904, -0.30824843552346304, -0.00435332187103771, -0.3344275204413762, -0.04012340541342146, 0.19605401086490218, 0.0187816119111... |
708.3008 | Exciting Maser Science with New Instruments - the Promise of the EVLA | In the near future, the Expanded Very Large Array (EVLA) will allow surveys
for maser sources with unprecedented sensitivity, spectral coverage and
spectroscopic capabilities. In particular, comprehensive surveys for many maser
species with simultaneous sensitive continuum imaging and absorption studies
will give a c... | astro-ph | in the near future the expanded very large array evla will allow surveys for maser sources with unprecedented sensitivity spectral coverage and spectroscopic capabilities in particular comprehensive surveys for many maser species with simultaneous sensitive continuum imaging and absorption studies will give a comprehen... | [['in', 'the', 'near', 'future', 'the', 'expanded', 'very', 'large', 'array', 'evla', 'will', 'allow', 'surveys', 'for', 'maser', 'sources', 'with', 'unprecedented', 'sensitivity', 'spectral', 'coverage', 'and', 'spectroscopic', 'capabilities', 'in', 'particular', 'comprehensive', 'surveys', 'for', 'many', 'maser', 'sp... | [-0.07629451132737673, 0.07910864499684137, 0.048528584841495526, 0.037965086446358605, -0.12814039155984155, -0.08987083008709865, 0.042281045203708345, 0.4852331238583876, -0.1067872112007955, -0.29888035704453403, 0.12296173158612804, -0.2850672569090071, 0.005720118594427522, 0.18058916453558665, 0.0417157205788848... |
708.3009 | BMW algebra, quantized coordinate algebra and type C Schur--Weyl duality | We prove an integral version of the Schur--Weyl duality between the
specialized Birman--Murakami--Wenzl algebra $B_n(-q^{2m+1},q)$ and the quantum
algebra associated to the symplectic Lie algebra sp_{2m}. In particular, we
deduce that this Schur--Weyl duality holds over arbitrary (commutative) ground
rings, which ans... | math.QA math.RT | we prove an integral version of the schurweyl duality between the specialized birmanmurakamiwenzl algebra b_nq2m1q and the quantum algebra associated to the symplectic lie algebra sp_2m in particular we deduce that this schurweyl duality holds over arbitrary commutative ground rings which answers a question of lehrer a... | [['we', 'prove', 'an', 'integral', 'version', 'of', 'the', 'schurweyl', 'duality', 'between', 'the', 'specialized', 'birmanmurakamiwenzl', 'algebra', 'b_nq2m1q', 'and', 'the', 'quantum', 'algebra', 'associated', 'to', 'the', 'symplectic', 'lie', 'algebra', 'sp_2m', 'in', 'particular', 'we', 'deduce', 'that', 'this', 's... | [-0.18873784227964832, 0.06130567963033252, -0.08330747997894397, 0.06762453854785037, -0.1425926850339317, -0.16812778467251716, -0.04444976826451476, 0.3147933201196239, -0.41340884378650633, -0.20369085639148302, 0.08716902316993345, -0.17915551632177085, -0.1690541783641295, 0.18429664666157053, -0.1905635211151093... |
708.301 | Prospects of Open Charm Production at GSI-FAIR and J-PARC | We present a detailed phenomenological study of the prospects of open charm
physics at the future $\bar{p}p$ and $pp$ facilities GSI-FAIR and J-PARC,
respectively. In particular, we concentrate on differential cross sections and
the charge and longitudinal double-spin asymmetries at next-to-leading order
accuracy. Th... | hep-ph | we present a detailed phenomenological study of the prospects of open charm physics at the future barpp and pp facilities gsifair and jparc respectively in particular we concentrate on differential cross sections and the charge and longitudinal doublespin asymmetries at nexttoleading order accuracy theoretical uncertai... | [['we', 'present', 'a', 'detailed', 'phenomenological', 'study', 'of', 'the', 'prospects', 'of', 'open', 'charm', 'physics', 'at', 'the', 'future', 'barpp', 'and', 'pp', 'facilities', 'gsifair', 'and', 'jparc', 'respectively', 'in', 'particular', 'we', 'concentrate', 'on', 'differential', 'cross', 'sections', 'and', 't... | [-0.0717873327796244, 0.1845488657967912, -0.08880530726460237, 0.14969112187446582, -0.025621044937343823, -0.06255947922666867, 0.03421201844078799, 0.33631643024273217, -0.17686816318965856, -0.2666950787654117, 0.006843898502651543, -0.3842283659392879, 0.06896739466381925, 0.15581861629136026, 0.11221792035928321,... |
708.3011 | The design and performance of the ZEUS Micro Vertex detector | In order to extend the tracking acceptance, to improve the primary and
secondary vertex reconstruction and thus enhancing the tagging capabilities for
short lived particles, the ZEUS experiment at the HERA Collider at DESY
installed a silicon strip vertex detector. The barrel part of the detector is a
63 cm long cyli... | physics.ins-det | in order to extend the tracking acceptance to improve the primary and secondary vertex reconstruction and thus enhancing the tagging capabilities for short lived particles the zeus experiment at the hera collider at desy installed a silicon strip vertex detector the barrel part of the detector is a 63 cm long cylinder ... | [['in', 'order', 'to', 'extend', 'the', 'tracking', 'acceptance', 'to', 'improve', 'the', 'primary', 'and', 'secondary', 'vertex', 'reconstruction', 'and', 'thus', 'enhancing', 'the', 'tagging', 'capabilities', 'for', 'short', 'lived', 'particles', 'the', 'zeus', 'experiment', 'at', 'the', 'hera', 'collider', 'at', 'de... | [-0.11181437799604524, 0.11208035324931405, -0.03713494819512061, -0.025662632327988197, -0.01222181098467303, -0.1387322740832241, -0.04462763188628975, 0.3661115850373214, -0.17093855066549615, -0.3393178445654451, 0.09300848222316302, -0.3752798948847099, 0.01768646119247883, 0.16569124323469714, -0.0071246453449813... |
708.3012 | Perturbation Expansion for Option Pricing with Stochastic Volatility | We fit the volatility fluctuations of the S&P 500 index well by a Chi
distribution, and the distribution of log-returns by a corresponding
superposition of Gaussian distributions. The Fourier transform of this is,
remarkably, of the Tsallis type. An option pricing formula is derived from the
same superposition of Bla... | q-fin.PR cond-mat.stat-mech math-ph math.MP physics.data-an physics.soc-ph | we fit the volatility fluctuations of the sp 500 index well by a chi distribution and the distribution of logreturns by a corresponding superposition of gaussian distributions the fourier transform of this is remarkably of the tsallis type an option pricing formula is derived from the same superposition of blackscholes... | [['we', 'fit', 'the', 'volatility', 'fluctuations', 'of', 'the', 'sp', '500', 'index', 'well', 'by', 'a', 'chi', 'distribution', 'and', 'the', 'distribution', 'of', 'logreturns', 'by', 'a', 'corresponding', 'superposition', 'of', 'gaussian', 'distributions', 'the', 'fourier', 'transform', 'of', 'this', 'is', 'remarkabl... | [-0.08215159886855293, 0.07357220516198802, -0.18459752906170307, 0.12255377008202203, -0.0655316814998955, -0.07968608305126315, 0.04521785593224746, 0.32736970867368986, -0.2794197455796441, -0.26829010136795906, 0.12602896338582717, -0.3006517758776406, -0.10143293743727333, 0.18933588202873414, -0.04922164445319636... |
708.3013 | Bayesian segmentation of hyperspectral images | In this paper we consider the problem of joint segmentation of hyperspectral
images in the Bayesian framework. The proposed approach is based on a Hidden
Markov Modeling (HMM) of the images with common segmentation, or equivalently
with common hidden classification label variables which is modeled by a Potts
Markov R... | physics.data-an | in this paper we consider the problem of joint segmentation of hyperspectral images in the bayesian framework the proposed approach is based on a hidden markov modeling hmm of the images with common segmentation or equivalently with common hidden classification label variables which is modeled by a potts markov random ... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'joint', 'segmentation', 'of', 'hyperspectral', 'images', 'in', 'the', 'bayesian', 'framework', 'the', 'proposed', 'approach', 'is', 'based', 'on', 'a', 'hidden', 'markov', 'modeling', 'hmm', 'of', 'the', 'images', 'with', 'common', 'segmentation', 'or'... | [-0.01873044805335147, 0.05110258146243203, -0.06625625743929829, 0.08144899880945948, -0.08737992005688804, -0.1603634910524956, 0.03391917876267273, 0.48693303726613524, -0.2995687452011875, -0.31663719232061077, 0.12433073859595295, -0.20865129136613436, -0.1660080267282735, 0.11493056360299565, -0.07886024968964712... |
708.3014 | Explicit formulas for efficient multiplication in F_{3^{6m}} | Efficient computation of the Tate pairing is an important part of
pairing-based cryptography. Recently with the introduction of the Duursma-Lee
method special attention has been given to the fields of characteristic 3.
Especially multiplication in F_{3^{6m}}, where m is prime, is an important
operation in the above m... | cs.CR cs.CC | efficient computation of the tate pairing is an important part of pairingbased cryptography recently with the introduction of the duursmalee method special attention has been given to the fields of characteristic 3 especially multiplication in f_36m where m is prime is an important operation in the above method in this... | [['efficient', 'computation', 'of', 'the', 'tate', 'pairing', 'is', 'an', 'important', 'part', 'of', 'pairingbased', 'cryptography', 'recently', 'with', 'the', 'introduction', 'of', 'the', 'duursmalee', 'method', 'special', 'attention', 'has', 'been', 'given', 'to', 'the', 'fields', 'of', 'characteristic', '3', 'especi... | [-0.13218447234015912, 0.040557845400471706, -0.08033586638979613, 0.015747243211371824, -0.04696667377604172, -0.10969050639774651, -8.876216015778482e-05, 0.3799444491788745, -0.23711610224097968, -0.32177366465330126, 0.12059531796141527, -0.19890600586979418, -0.16700942961499096, 0.28473584957188, -0.1250253692724... |
708.3015 | Decreasing elliptic flow at the LHC: Calculations in a parton
recombination approach | We apply the parton recombination approach to study the energy dependence of
the elliptic flow, v_2 in heavy ion collisions from AGS to LHC energies. The
relevant input quantities ($T, \mu_B, \eta_T$) at the various center of mass
energies are obtained from fits to the available data. The model yields a good
descript... | nucl-th | we apply the parton recombination approach to study the energy dependence of the elliptic flow v_2 in heavy ion collisions from ags to lhc energies the relevant input quantities t mu_b eta_t at the various center of mass energies are obtained from fits to the available data the model yields a good description of the in... | [['we', 'apply', 'the', 'parton', 'recombination', 'approach', 'to', 'study', 'the', 'energy', 'dependence', 'of', 'the', 'elliptic', 'flow', 'v_2', 'in', 'heavy', 'ion', 'collisions', 'from', 'ags', 'to', 'lhc', 'energies', 'the', 'relevant', 'input', 'quantities', 't', 'mu_b', 'eta_t', 'at', 'the', 'various', 'center... | [-0.035898322728462516, 0.23726769958622754, -0.1552831554443886, 0.13050417514905954, 0.004780183240460853, -0.10630320778116584, -0.0765888227429241, 0.378006184771657, -0.2433169646343837, -0.3015215555050721, -0.06479333096959938, -0.38516309260701137, 0.1284278710046783, 0.17953032398596405, 0.05783578022072713, 0... |
708.3016 | Star and Planet Formation with ALMA: an Overview | Submillimeter observations with ALMA will be the essential next step in our
understanding of how stars and planets form. Key projects range from detailed
imaging of the collapse of pre-stellar cores and measuring the accretion rate
of matter onto deeply embedded protostars, to unravelling the chemistry and
dynamics o... | astro-ph | submillimeter observations with alma will be the essential next step in our understanding of how stars and planets form key projects range from detailed imaging of the collapse of prestellar cores and measuring the accretion rate of matter onto deeply embedded protostars to unravelling the chemistry and dynamics of hig... | [['submillimeter', 'observations', 'with', 'alma', 'will', 'be', 'the', 'essential', 'next', 'step', 'in', 'our', 'understanding', 'of', 'how', 'stars', 'and', 'planets', 'form', 'key', 'projects', 'range', 'from', 'detailed', 'imaging', 'of', 'the', 'collapse', 'of', 'prestellar', 'cores', 'and', 'measuring', 'the', '... | [-0.03770111434591504, 0.1247528807976498, -0.06089492090619528, 0.04996129977875031, -0.07606251316789825, 0.008051588174958641, 0.011691956623242452, 0.3868522482422682, -0.1811816857411311, -0.35592085959819647, 0.0896719958113793, -0.21926358036267068, -0.024466241792274208, 0.13969944932569678, 0.03462794506205962... |
708.3017 | Black Holes and Quantum Gravity at the LHC | We argue that the highly studied black hole signatures based on thermal
multiparticle final states are very unlikely and only occur in a very limited
parameter regime if at all. However, we show that if the higher-dimensional
quantum gravity scale is low, it should be possible to study quantum gravity in
the context ... | hep-ph | we argue that the highly studied black hole signatures based on thermal multiparticle final states are very unlikely and only occur in a very limited parameter regime if at all however we show that if the higherdimensional quantum gravity scale is low it should be possible to study quantum gravity in the context of hig... | [['we', 'argue', 'that', 'the', 'highly', 'studied', 'black', 'hole', 'signatures', 'based', 'on', 'thermal', 'multiparticle', 'final', 'states', 'are', 'very', 'unlikely', 'and', 'only', 'occur', 'in', 'a', 'very', 'limited', 'parameter', 'regime', 'if', 'at', 'all', 'however', 'we', 'show', 'that', 'if', 'the', 'high... | [-0.1225861722319308, 0.2185117740941755, -0.0769823322435683, 0.14135007292103274, -0.0543376977152933, -0.1904269184056922, 0.007014720471796848, 0.33080295968990203, -0.1926857911808006, -0.27874837291695304, 0.11571381640052265, -0.2466186021407277, -0.15682339852959928, 0.2286652350735109, -0.029165390594783475, -... |
708.3018 | Multiphase Plasma in Sub-Damped Lyman Alpha Systems: A Hidden Metal
Reservoir | We present a VLT/UVES spectrum of a proximate sub-damped Lyman-alpha
(sub-DLA) system at z=2.65618 toward the quasar Q0331-4505
(z_qso=2.6785+/-0.0030). Absorption lines of O I, Si II, Si III, Si IV, C II, C
III, C IV, Fe II, Al II, and O VI are seen in the sub-DLA, which has a neutral
hydrogen column density log N(H... | astro-ph | we present a vltuves spectrum of a proximate subdamped lymanalpha subdla system at z265618 toward the quasar q03314505 z_qso2678500030 absorption lines of o i si ii si iii si iv c ii c iii c iv fe ii al ii and o vi are seen in the subdla which has a neutral hydrogen column density log nh i1982005 the absorber is at a v... | [['we', 'present', 'a', 'vltuves', 'spectrum', 'of', 'a', 'proximate', 'subdamped', 'lymanalpha', 'subdla', 'system', 'at', 'z265618', 'toward', 'the', 'quasar', 'q03314505', 'z_qso2678500030', 'absorption', 'lines', 'of', 'o', 'i', 'si', 'ii', 'si', 'iii', 'si', 'iv', 'c', 'ii', 'c', 'iii', 'c', 'iv', 'fe', 'ii', 'al'... | [-0.03704530173500915, 0.07505676887487456, 0.0899390757062846, -0.01768031401696515, 0.01818321955832258, -0.19102441142497342, 0.09735041624592818, 0.4471812596765615, -0.12616285213235093, -0.3202141838011432, -0.011463638137904979, -0.36025522966832346, 0.0249143938947006, 0.07450417235840932, 0.009681878151045849,... |
708.3019 | Single-Symbol ML Decodable Distributed STBCs for Partially-Coherent
Cooperative Networks | Space-time block codes (STBCs) that are single-symbol decodable (SSD) in a
co-located multiple antenna setting need not be SSD in a distributed
cooperative communication setting. A relay network with N relays and a single
source-destination pair is called a partially-coherent relay channel (PCRC) if
the destination h... | cs.IT math.IT | spacetime block codes stbcs that are singlesymbol decodable ssd in a colocated multiple antenna setting need not be ssd in a distributed cooperative communication setting a relay network with n relays and a single sourcedestination pair is called a partiallycoherent relay channel pcrc if the destination has perfect cha... | [['spacetime', 'block', 'codes', 'stbcs', 'that', 'are', 'singlesymbol', 'decodable', 'ssd', 'in', 'a', 'colocated', 'multiple', 'antenna', 'setting', 'need', 'not', 'be', 'ssd', 'in', 'a', 'distributed', 'cooperative', 'communication', 'setting', 'a', 'relay', 'network', 'with', 'n', 'relays', 'and', 'a', 'single', 's... | [-0.2449220026974498, 0.07942705582036245, -0.03924105823413976, 0.017137452322651694, -0.05033373209183971, -0.3051310916409673, 0.07426749847867098, 0.36774567492363763, -0.25918028453854003, -0.2209930041279917, 0.1390209607258583, -0.23793601708012024, -0.14700568755854884, 0.12631546609997246, -0.12480160585086807... |
708.302 | The short period end of the contact binary period distribution based on
the All Sky Automated Survey (ASAS) | The search-volume corrected period distribution of contact binaries of the W
UMa type appears to reflect primarily the constant number ratio of ~1/500 to
the number of stars along the Main Sequence; there exist no evidence for
angular momentum evolution. The maximum in contact binary numbers is located at
shorter per... | astro-ph | the searchvolume corrected period distribution of contact binaries of the w uma type appears to reflect primarily the constant number ratio of 1500 to the number of stars along the main sequence there exist no evidence for angular momentum evolution the maximum in contact binary numbers is located at shorter periods th... | [['the', 'searchvolume', 'corrected', 'period', 'distribution', 'of', 'contact', 'binaries', 'of', 'the', 'w', 'uma', 'type', 'appears', 'to', 'reflect', 'primarily', 'the', 'constant', 'number', 'ratio', 'of', '1500', 'to', 'the', 'number', 'of', 'stars', 'along', 'the', 'main', 'sequence', 'there', 'exist', 'no', 'ev... | [-0.19291626495531702, 0.1970069876632991, -0.058516026826872104, 0.06792802220226916, -0.030426815275795164, -0.16239871590736166, 0.1013165361487999, 0.3420729565277564, -0.23784354540923264, -0.377952441573143, 0.04949197552344078, -0.311405767959932, -0.0031042526377183673, 0.18481022336899378, -0.04605779855917282... |
708.3021 | Discovery of VHE gamma-rays from the distant BL Lac 1ES 0347-121 | Aims: Our aim is to study the production mechanism for very-high-energy (VHE;
>100GeV) gamma-rays in distant active galactic nuclei (AGN) and use the
observed VHE spectrum to derive limits on the Extragalactic Background Light
(EBL). We also want to determine physical quantities through the modeling of
the object's b... | astro-ph | aims our aim is to study the production mechanism for veryhighenergy vhe 100gev gammarays in distant active galactic nuclei agn and use the observed vhe spectrum to derive limits on the extragalactic background light ebl we also want to determine physical quantities through the modeling of the objects broadband spectra... | [['aims', 'our', 'aim', 'is', 'to', 'study', 'the', 'production', 'mechanism', 'for', 'veryhighenergy', 'vhe', '100gev', 'gammarays', 'in', 'distant', 'active', 'galactic', 'nuclei', 'agn', 'and', 'use', 'the', 'observed', 'vhe', 'spectrum', 'to', 'derive', 'limits', 'on', 'the', 'extragalactic', 'background', 'light',... | [-0.0034230570735109193, 0.12461318406077032, -0.09104554823922419, 0.17947414994476305, -0.12582284872288133, -0.08687182239487796, 0.055648123548461464, 0.4644321323808752, -0.1502764021471788, -0.40799471331892284, -0.005264498293858139, -0.32281825308849316, 0.04304321636317489, 0.2533454678496199, -0.0520104872194... |
708.3022 | Efficient FPGA-based multipliers for F_{3^97} and F_{3^{6*97}} | In this work we present a new structure for multiplication in finite fields.
This structure is based on a digit-level LFSR (Linear Feedback Shift Register)
multiplier in which the area of digit-multipliers are reduced using the
Karatsuba method. We compare our results with the other works in the literature
for F_{3^9... | cs.CR | in this work we present a new structure for multiplication in finite fields this structure is based on a digitlevel lfsr linear feedback shift register multiplier in which the area of digitmultipliers are reduced using the karatsuba method we compare our results with the other works in the literature for f_397 we also ... | [['in', 'this', 'work', 'we', 'present', 'a', 'new', 'structure', 'for', 'multiplication', 'in', 'finite', 'fields', 'this', 'structure', 'is', 'based', 'on', 'a', 'digitlevel', 'lfsr', 'linear', 'feedback', 'shift', 'register', 'multiplier', 'in', 'which', 'the', 'area', 'of', 'digitmultipliers', 'are', 'reduced', 'us... | [-0.0846891851117245, 0.08149193714761847, -0.06073745708511789, 0.035283363338772064, -0.07470649624644202, -0.09810863080422712, 0.05156203654382519, 0.3690097347562072, -0.2697836551048993, -0.29933551019882854, 0.12377638686625168, -0.23125703608627501, -0.17891181429517986, 0.29206452371340386, -0.1148525798215112... |
708.3023 | Fine frequency shift of sigle vortex entrance and exit in
superconducting loops | The heat capacity $C_{p}$ of an array of independent aluminum rings has been
measured under an external magnetic field $\vec{H}$ using highly sensitive
ac-calorimetry based on a silicon membrane sensor. Each superconducting vortex
entrance induces a phase transition and a heat capacity jump and hence $C_{p}$
oscillat... | cond-mat.mes-hall | the heat capacity c_p of an array of independent aluminum rings has been measured under an external magnetic field vech using highly sensitive accalorimetry based on a silicon membrane sensor each superconducting vortex entrance induces a phase transition and a heat capacity jump and hence c_p oscillates with vech this... | [['the', 'heat', 'capacity', 'c_p', 'of', 'an', 'array', 'of', 'independent', 'aluminum', 'rings', 'has', 'been', 'measured', 'under', 'an', 'external', 'magnetic', 'field', 'vech', 'using', 'highly', 'sensitive', 'accalorimetry', 'based', 'on', 'a', 'silicon', 'membrane', 'sensor', 'each', 'superconducting', 'vortex',... | [-0.21715805158899643, 0.17808062044068954, -0.08390637032257822, -0.0027737995178307383, -0.07580500454283677, -0.10340686104982758, 0.03912140476929311, 0.3493707899051981, -0.271040600608103, -0.27233155762466293, 0.08395405976364437, -0.2698662002714208, -0.09251017176593916, 0.23095906236565683, -0.008843337158815... |
708.3024 | Pump-Probe Experiments on the Single-Molecule Magnet Fe8 : Measurement
of Excited Level Lifetimes | We present magnetization measurements on the single molecule magnet Fe8 in
the presence of pulsed microwave radiation. A pump-probe technique is used with
two microwave pulses with frequencies of 107 GHz and 118 GHz and pulse lengths
of several nanoseconds to study the spin dynamics via time-resolved
magnetization me... | cond-mat.mes-hall | we present magnetization measurements on the single molecule magnet fe8 in the presence of pulsed microwave radiation a pumpprobe technique is used with two microwave pulses with frequencies of 107 ghz and 118 ghz and pulse lengths of several nanoseconds to study the spin dynamics via timeresolved magnetization measure... | [['we', 'present', 'magnetization', 'measurements', 'on', 'the', 'single', 'molecule', 'magnet', 'fe8', 'in', 'the', 'presence', 'of', 'pulsed', 'microwave', 'radiation', 'a', 'pumpprobe', 'technique', 'is', 'used', 'with', 'two', 'microwave', 'pulses', 'with', 'frequencies', 'of', '107', 'ghz', 'and', '118', 'ghz', 'a... | [-0.1715321906764681, 0.18424241539280586, -0.03969536235780214, -0.01731299934046412, -0.02063356485666224, -0.11160069688964912, 0.07258748151232591, 0.43255181184590413, -0.1927493697601474, -0.32660029978594846, 0.06073723527865864, -0.2773166766618723, -0.030598794308456558, 0.3064267390269648, 0.08996327750867715... |
708.3025 | The Green's function and the Ahlfors map | The classical Green's function associated to a simply connected domain in the
complex plane is easily expressed in terms of a Riemann mapping function. The
purpose of this paper is to express the Green's function of a finitely
connected domain in the plane in terms of a single Ahlfors mapping of the
domain, which is ... | math.CV | the classical greens function associated to a simply connected domain in the complex plane is easily expressed in terms of a riemann mapping function the purpose of this paper is to express the greens function of a finitely connected domain in the plane in terms of a single ahlfors mapping of the domain which is a prop... | [['the', 'classical', 'greens', 'function', 'associated', 'to', 'a', 'simply', 'connected', 'domain', 'in', 'the', 'complex', 'plane', 'is', 'easily', 'expressed', 'in', 'terms', 'of', 'a', 'riemann', 'mapping', 'function', 'the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'express', 'the', 'greens', 'function', 'of... | [-0.18023119025121007, 0.017391347125927104, -0.07017528319943554, 0.035162309136041264, -0.12450888962779619, -0.0021913310666155966, 0.008114342060517756, 0.3427269909106478, -0.3328612436410747, -0.17710203986284853, 0.1296374757797752, -0.24470955166447012, -0.1714502152385591, 0.21696375069927565, -0.0720468277017... |
708.3026 | Controlling the Ratchet Effect for Cold Atoms | Low-order quantum resonances manifested by directed currents have been
realized with cold atoms. Here we show that by increasing the strength of an
experimentally achievable delta-kicking ratchet potential, quantum resonances
of a very high order may naturally emerge and can induce larger ratchet
currents than low-or... | quant-ph | loworder quantum resonances manifested by directed currents have been realized with cold atoms here we show that by increasing the strength of an experimentally achievable deltakicking ratchet potential quantum resonances of a very high order may naturally emerge and can induce larger ratchet currents than loworder res... | [['loworder', 'quantum', 'resonances', 'manifested', 'by', 'directed', 'currents', 'have', 'been', 'realized', 'with', 'cold', 'atoms', 'here', 'we', 'show', 'that', 'by', 'increasing', 'the', 'strength', 'of', 'an', 'experimentally', 'achievable', 'deltakicking', 'ratchet', 'potential', 'quantum', 'resonances', 'of', ... | [-0.17221086794630375, 0.31466087917367225, -0.030669872704615343, 0.03596134622817609, -0.018754923938592866, -0.1733953905111151, 0.02134226293150169, 0.3498126448430955, -0.26352047492096675, -0.2854040374617968, -0.006223725730122359, -0.24877713984851516, -0.16361378569767546, 0.2083893520340546, -0.00389846681214... |
708.3027 | Free 3-distributions: holonomy, Fefferman constructions and dual
distributions | This paper analyses the parabolic geometries generated by a free
3-distribution in the tangent space of a manifold. It shows the existence of
normal Fefferman constructions over CR and Lagrangian contact structures
corresponding to holonomy reductions to SO(4,2) and SO(3,3), respectively.
There is also a fascinating ... | math.DG | this paper analyses the parabolic geometries generated by a free 3distribution in the tangent space of a manifold it shows the existence of normal fefferman constructions over cr and lagrangian contact structures corresponding to holonomy reductions to so42 and so33 respectively there is also a fascinating construction... | [['this', 'paper', 'analyses', 'the', 'parabolic', 'geometries', 'generated', 'by', 'a', 'free', '3distribution', 'in', 'the', 'tangent', 'space', 'of', 'a', 'manifold', 'it', 'shows', 'the', 'existence', 'of', 'normal', 'fefferman', 'constructions', 'over', 'cr', 'and', 'lagrangian', 'contact', 'structures', 'correspo... | [-0.17616038585958235, 0.10783031753517743, -0.05330889220075572, 0.07583516660173807, -0.1122032747918959, -0.12775212935829425, -0.021028665993499625, 0.36354168666088404, -0.24197540686958852, -0.22521008833256714, 0.08940086303354132, -0.2671484544681495, -0.18189445073606775, 0.2014959777623196, -0.129357362576924... |
708.3028 | Boundary three-point function on AdS2 D-branes | Using the H3+-Liouville relation, I explicitly compute the boundary
three-point function on AdS2 D-branes in H3+, and check that it exhibits the
expected symmetry properties and has the correct geometrical limit. I then find
a simple relation between this boundary three-point function and certain fusing
matrix elemen... | hep-th | using the h3liouville relation i explicitly compute the boundary threepoint function on ads2 dbranes in h3 and check that it exhibits the expected symmetry properties and has the correct geometrical limit i then find a simple relation between this boundary threepoint function and certain fusing matrix elements which su... | [['using', 'the', 'h3liouville', 'relation', 'i', 'explicitly', 'compute', 'the', 'boundary', 'threepoint', 'function', 'on', 'ads2', 'dbranes', 'in', 'h3', 'and', 'check', 'that', 'it', 'exhibits', 'the', 'expected', 'symmetry', 'properties', 'and', 'has', 'the', 'correct', 'geometrical', 'limit', 'i', 'then', 'find',... | [-0.1493273147511794, 0.10161894775025525, -0.1173415532075735, 0.1407102910344229, -0.08251518998728243, -0.11766882833136721, 0.008267694910944895, 0.3312836460292686, -0.2061499447973315, -0.21629029067319838, 0.08440503347150678, -0.2797051456345375, -0.1648637454436962, 0.05212000925310476, -0.07649083682985673, 0... |
708.3029 | Interplay between field-induced and frustration-induced quantum
criticalities in the frustrated two-leg Heisenberg ladder | The antiferromagnetic Heisenberg two-leg ladder in the presence of
frustration and an external magnetic field is a system that is characterized by
two sorts of quantum criticalities, not only one. One criticality is the
consequence of intrinsic frustration, and the other one is a result of the
external magnetic field... | cond-mat.str-el | the antiferromagnetic heisenberg twoleg ladder in the presence of frustration and an external magnetic field is a system that is characterized by two sorts of quantum criticalities not only one one criticality is the consequence of intrinsic frustration and the other one is a result of the external magnetic field so th... | [['the', 'antiferromagnetic', 'heisenberg', 'twoleg', 'ladder', 'in', 'the', 'presence', 'of', 'frustration', 'and', 'an', 'external', 'magnetic', 'field', 'is', 'a', 'system', 'that', 'is', 'characterized', 'by', 'two', 'sorts', 'of', 'quantum', 'criticalities', 'not', 'only', 'one', 'one', 'criticality', 'is', 'the',... | [-0.2070573846299556, 0.1972207915203485, -0.04360859359924992, 0.061160315884210704, -0.05241153800919179, -0.1509790158024915, 0.00652314919242931, 0.336812978950403, -0.2607369002302192, -0.3052346156762233, 0.07529277799628853, -0.3010899935449873, -0.15422007931758547, 0.19477586102272784, 0.0464250555055009, -0.0... |
708.303 | QCD sum rules study of \Xi_c and \Xi_b baryons | We use QCD sum rules to study the masses of the baryons $\Xi_c$ and $\Xi_b$.
We work with a current where the strange and the light quarks are in a relative
spin zero, at leading order in $\alpha_s$. We consider the contributions of
condensates up to dimension six. For $\Xi_b$ we get $m_{\Xi_{b}}= (5.75\pm
0.25) {\rm... | hep-ph | we use qcd sum rules to study the masses of the baryons xi_c and xi_b we work with a current where the strange and the light quarks are in a relative spin zero at leading order in alpha_s we consider the contributions of condensates up to dimension six for xi_b we get m_xi_b 575pm 025 rm gev and for xi_c we get m_xi_c ... | [['we', 'use', 'qcd', 'sum', 'rules', 'to', 'study', 'the', 'masses', 'of', 'the', 'baryons', 'xi_c', 'and', 'xi_b', 'we', 'work', 'with', 'a', 'current', 'where', 'the', 'strange', 'and', 'the', 'light', 'quarks', 'are', 'in', 'a', 'relative', 'spin', 'zero', 'at', 'leading', 'order', 'in', 'alpha_s', 'we', 'consider'... | [-0.0760884004270249, 0.23357135393634076, -0.05487147786245659, 0.10889082687066459, -0.010959315056935317, -0.08647322388956459, 0.1008470368503434, 0.3726409344547769, -0.15229485676305868, -0.27645623847478773, 0.005531346688058409, -0.3883651129265384, 0.08214982772223288, 0.11811765316851074, 0.06766262130312077,... |
708.3031 | Bounds to binding energies from the concavity of thermodynamical
functions | Sequences of experimental ground-state energies are mapped onto concave
patterns cured from convexities due to pairing and/or shell effects. The same
patterns, completed by a list of excitation energies, can be used to give
numerical estimates of the grand potential $\Omega(\beta,\mu)$ for a mixture of
nuclei at low ... | nucl-th | sequences of experimental groundstate energies are mapped onto concave patterns cured from convexities due to pairing andor shell effects the same patterns completed by a list of excitation energies can be used to give numerical estimates of the grand potential omegabetamu for a mixture of nuclei at low or moderate tem... | [['sequences', 'of', 'experimental', 'groundstate', 'energies', 'are', 'mapped', 'onto', 'concave', 'patterns', 'cured', 'from', 'convexities', 'due', 'to', 'pairing', 'andor', 'shell', 'effects', 'the', 'same', 'patterns', 'completed', 'by', 'a', 'list', 'of', 'excitation', 'energies', 'can', 'be', 'used', 'to', 'give... | [-0.06572253984815013, 0.14266643931070758, -0.06083906835981838, 0.1449459097414049, -0.0038657297919147044, -0.13146221540200542, 0.1171652321899954, 0.3890887224437587, -0.22148498382899653, -0.3045751303610093, 0.03505966034439632, -0.2918918765159712, -0.020069041401411424, 0.17395021075107533, 0.03017545083530879... |
708.3032 | Charged Black Holes on DGP Brane | We consider charged black holes localized on a three-brane in the DGP model.
With a spherically symmetric metric ansatz on the brane and assuming a
Z_2-symmetry across the brane, we find two types of solutions which correspond
to the so-called regular and accelerated branches in the DGP model. When the
charge of the ... | hep-th | we consider charged black holes localized on a threebrane in the dgp model with a spherically symmetric metric ansatz on the brane and assuming a z_2symmetry across the brane we find two types of solutions which correspond to the socalled regular and accelerated branches in the dgp model when the charge of the black ho... | [['we', 'consider', 'charged', 'black', 'holes', 'localized', 'on', 'a', 'threebrane', 'in', 'the', 'dgp', 'model', 'with', 'a', 'spherically', 'symmetric', 'metric', 'ansatz', 'on', 'the', 'brane', 'and', 'assuming', 'a', 'z_2symmetry', 'across', 'the', 'brane', 'we', 'find', 'two', 'types', 'of', 'solutions', 'which'... | [-0.12153156748493477, 0.06286905101596323, -0.053534821251078564, 0.11947831712142729, -0.04822450274985064, -0.19144454456674045, -0.02267055503804894, 0.2659111955367467, -0.11792784282828078, -0.25252808118239045, 0.07000535221167785, -0.33974488665733266, -0.10033038425642778, 0.1306576806682107, -0.03484043062609... |
708.3033 | Osculating orbits in Schwarzschild spacetime, with an application to
extreme mass-ratio inspirals | We present a method to integrate the equations of motion that govern bound,
accelerated orbits in Schwarzschild spacetime. At each instant the true
worldline is assumed to lie tangent to a reference geodesic, called an
osculating orbit, such that the worldline evolves smoothly from one such
geodesic to the next. Beca... | gr-qc | we present a method to integrate the equations of motion that govern bound accelerated orbits in schwarzschild spacetime at each instant the true worldline is assumed to lie tangent to a reference geodesic called an osculating orbit such that the worldline evolves smoothly from one such geodesic to the next because a g... | [['we', 'present', 'a', 'method', 'to', 'integrate', 'the', 'equations', 'of', 'motion', 'that', 'govern', 'bound', 'accelerated', 'orbits', 'in', 'schwarzschild', 'spacetime', 'at', 'each', 'instant', 'the', 'true', 'worldline', 'is', 'assumed', 'to', 'lie', 'tangent', 'to', 'a', 'reference', 'geodesic', 'called', 'an... | [-0.1583991986276074, 0.11319362062041807, -0.09654421710855643, 0.03909721947335234, -0.09670937676290589, -0.05056371595248703, 0.003809321980561661, 0.3248661645449513, -0.27305845642166043, -0.27239217843152275, 0.06432856692767064, -0.2622368978721297, -0.13484472608143724, 0.18672907235984082, -0.0758458524605659... |
708.3034 | Dust formation in electric arc furnace : birth of the particles | The characterization of Electric Arc Furnace (EAF) dust shows that bubble
burst at the liquid steel surface is the principal source of dust emission. We
have therefore developed an experimental device for studying this phenomenon.
As in the case of the air-water system, the bubble-burst gives birth to two
types of dr... | cond-mat.mtrl-sci | the characterization of electric arc furnace eaf dust shows that bubble burst at the liquid steel surface is the principal source of dust emission we have therefore developed an experimental device for studying this phenomenon as in the case of the airwater system the bubbleburst gives birth to two types of droplets fi... | [['the', 'characterization', 'of', 'electric', 'arc', 'furnace', 'eaf', 'dust', 'shows', 'that', 'bubble', 'burst', 'at', 'the', 'liquid', 'steel', 'surface', 'is', 'the', 'principal', 'source', 'of', 'dust', 'emission', 'we', 'have', 'therefore', 'developed', 'an', 'experimental', 'device', 'for', 'studying', 'this', ... | [-0.08444748030677529, 0.16082402887791672, -0.08190479233407562, -0.014844658939278145, -0.019086958558641766, -0.09689956986786503, 0.02362841696671431, 0.39802426010627595, -0.23387564765902139, -0.3302609157736266, 0.10267034991442128, -0.3239865780158557, -0.031240042838218966, 0.1980657149741953, -0.0570651207082... |
708.3035 | Topology effects on the heat capacity of mesoscopic superconducting
disks | Phase transitions in superconducting mesoscopic disks have been studied over
the H-T phase diagram through heat capacity measurement of an array of
independent aluminium disks. These disks exhibit non periodic modulations
versus H of the height of the heat capacity jump at the superconducting to
normal transition. Th... | cond-mat.mes-hall | phase transitions in superconducting mesoscopic disks have been studied over the ht phase diagram through heat capacity measurement of an array of independent aluminium disks these disks exhibit non periodic modulations versus h of the height of the heat capacity jump at the superconducting to normal transition this be... | [['phase', 'transitions', 'in', 'superconducting', 'mesoscopic', 'disks', 'have', 'been', 'studied', 'over', 'the', 'ht', 'phase', 'diagram', 'through', 'heat', 'capacity', 'measurement', 'of', 'an', 'array', 'of', 'independent', 'aluminium', 'disks', 'these', 'disks', 'exhibit', 'non', 'periodic', 'modulations', 'vers... | [-0.20726683233350293, 0.2945193337692936, -0.044396989690417894, 0.012586717908235906, -0.004839140887080289, -0.14961231126686309, 0.115038902140848, 0.3500364986109311, -0.24422942595417374, -0.27372381048026817, 0.0373891079251015, -0.3180373415225811, -0.06021471388130657, 0.17604112696535051, 0.04876677331027276,... |
708.3036 | On the algebraic classification of K-local spectra | In 1996, Jens Franke proved the equivalence of certain triangulated
categories possessing an Adams spectral sequence. One particular application of
this theorem is that the K_(p)-local stable homotopy category at an odd prime
can be described as the derived category of an abelian category. We explain
this proof from ... | math.AT | in 1996 jens franke proved the equivalence of certain triangulated categories possessing an adams spectral sequence one particular application of this theorem is that the k_plocal stable homotopy category at an odd prime can be described as the derived category of an abelian category we explain this proof from a topolo... | [['in', '1996', 'jens', 'franke', 'proved', 'the', 'equivalence', 'of', 'certain', 'triangulated', 'categories', 'possessing', 'an', 'adams', 'spectral', 'sequence', 'one', 'particular', 'application', 'of', 'this', 'theorem', 'is', 'that', 'the', 'k_plocal', 'stable', 'homotopy', 'category', 'at', 'an', 'odd', 'prime'... | [-0.1374348922356687, 0.01811140247796343, -0.13973424056786354, 0.1291906707639875, -0.05148740916478413, -0.13896967635352026, -0.04017781050384252, 0.3213533509729637, -0.39044045884576106, -0.25155060312331273, 0.08820273015536023, -0.1568955277196235, -0.1129539196069042, 0.1828854298564019, -0.2569825813105261, -... |
708.3037 | Multi-scale analysis of the electromagnetic self-force in a weak
gravitational field | We examine the motion of a charged particle in a weak gravitational field. In
addition to the Newtonian gravity exerted by a large central body, the particle
is subjected to an electromagnetic self-force that contains both a conservative
piece and a radiation-reaction piece. This toy problem shares many of the
featur... | gr-qc | we examine the motion of a charged particle in a weak gravitational field in addition to the newtonian gravity exerted by a large central body the particle is subjected to an electromagnetic selfforce that contains both a conservative piece and a radiationreaction piece this toy problem shares many of the features of t... | [['we', 'examine', 'the', 'motion', 'of', 'a', 'charged', 'particle', 'in', 'a', 'weak', 'gravitational', 'field', 'in', 'addition', 'to', 'the', 'newtonian', 'gravity', 'exerted', 'by', 'a', 'large', 'central', 'body', 'the', 'particle', 'is', 'subjected', 'to', 'an', 'electromagnetic', 'selfforce', 'that', 'contains'... | [-0.17756216075235098, 0.08037165573020945, -0.12934835369806344, 0.10837182891789131, -0.10426536636677426, -0.08541710915783392, -0.00870093327230919, 0.32114902476606955, -0.26450747683007814, -0.28823591496364853, 0.05139373094966663, -0.254493135612589, -0.13666981131063036, 0.19615289772364625, -0.071562902091641... |
708.3038 | f(R) Gravity with Torsion: The Metric-Affine Approach | The role of torsion in f(R) gravity is considered in the framework of
metric-affine formalism. We discuss the field equations in empty space and in
presence of perfect fluid matter taking into account the analogy with the
Palatini formalism. As a result, the extra curvature and torsion degrees of
freedom can be dealt... | gr-qc | the role of torsion in fr gravity is considered in the framework of metricaffine formalism we discuss the field equations in empty space and in presence of perfect fluid matter taking into account the analogy with the palatini formalism as a result the extra curvature and torsion degrees of freedom can be dealt as an e... | [['the', 'role', 'of', 'torsion', 'in', 'fr', 'gravity', 'is', 'considered', 'in', 'the', 'framework', 'of', 'metricaffine', 'formalism', 'we', 'discuss', 'the', 'field', 'equations', 'in', 'empty', 'space', 'and', 'in', 'presence', 'of', 'perfect', 'fluid', 'matter', 'taking', 'into', 'account', 'the', 'analogy', 'wit... | [-0.19007554055168863, 0.1129588867019842, -0.15190359083765254, 0.09814061176332804, -0.12247518209240786, -0.10721823859891695, -0.06810824893040174, 0.2678502123666609, -0.23507914529182017, -0.3242253975761009, 0.022807477751928495, -0.2009383115758438, -0.12717965526063357, 0.09353413348790349, -0.0597349343389817... |
708.3039 | Exact Solution of Strongly Interacting Quasi-One-Dimensional Spinor Bose
Gases | We present an exact analytical solution of the fundamental system of
quasi-one-dimensional spin-1 bosons with infinite delta-repulsion. The
eigenfunctions are constructed from the wave functions of non-interacting
spinless fermions, based on Girardeau's Fermi-Bose mapping, and from the wave
functions of distinguishab... | cond-mat.other | we present an exact analytical solution of the fundamental system of quasionedimensional spin1 bosons with infinite deltarepulsion the eigenfunctions are constructed from the wave functions of noninteracting spinless fermions based on girardeaus fermibose mapping and from the wave functions of distinguishable spins we ... | [['we', 'present', 'an', 'exact', 'analytical', 'solution', 'of', 'the', 'fundamental', 'system', 'of', 'quasionedimensional', 'spin1', 'bosons', 'with', 'infinite', 'deltarepulsion', 'the', 'eigenfunctions', 'are', 'constructed', 'from', 'the', 'wave', 'functions', 'of', 'noninteracting', 'spinless', 'fermions', 'base... | [-0.1837118825827351, 0.26140248504476554, -0.051894500947374606, 0.08726243513296837, -0.0008493064463173396, -0.1351725139620357, 0.008139662359728017, 0.32837826027491385, -0.19891903585989343, -0.21831703669974736, -0.012730007521181462, -0.34544034649522226, -0.09026256747865857, 0.1103020292123623, 0.111708536857... |
708.304 | The evolution of stars in the Taurus-Auriga T association | In a recent study, individual parallaxes were determined for many stars of
the Taurus-Auriga T association that are members of the same moving group. We
use these new parallaxes to re-address the issue of the relationship between
classical T Tauri stars (CTTSs) and weak-emission line T Tauri stars (WTTSs).
With the a... | astro-ph | in a recent study individual parallaxes were determined for many stars of the taurusauriga t association that are members of the same moving group we use these new parallaxes to readdress the issue of the relationship between classical t tauri stars cttss and weakemission line t tauri stars wttss with the available spe... | [['in', 'a', 'recent', 'study', 'individual', 'parallaxes', 'were', 'determined', 'for', 'many', 'stars', 'of', 'the', 'taurusauriga', 't', 'association', 'that', 'are', 'members', 'of', 'the', 'same', 'moving', 'group', 'we', 'use', 'these', 'new', 'parallaxes', 'to', 'readdress', 'the', 'issue', 'of', 'the', 'relatio... | [-0.026828666300107745, 0.1639598859087752, -0.07566141734462735, 0.14143897924883367, -0.09885558156785242, -0.07453027469076784, 0.10560698180828523, 0.4601358354024823, -0.20198152410994064, -0.3744397296824998, 0.04751085433190179, -0.2878874422055189, 0.012836720417525135, 0.17871242320564923, -0.06987326491766112... |
708.3041 | Convergence Rate of K-Step Maximum Likelihood Estimate in Semiparametric
Models | We suggest an iterative approach to computing K-step maximum likelihood
estimates (MLE) of the parametric components in semiparametric models based on
their profile likelihoods. The higher order convergence rate of K-step MLE
mainly depends on the precision of its initial estimate and the convergence
rate of the nuis... | math.ST stat.TH | we suggest an iterative approach to computing kstep maximum likelihood estimates mle of the parametric components in semiparametric models based on their profile likelihoods the higher order convergence rate of kstep mle mainly depends on the precision of its initial estimate and the convergence rate of the nuisance fu... | [['we', 'suggest', 'an', 'iterative', 'approach', 'to', 'computing', 'kstep', 'maximum', 'likelihood', 'estimates', 'mle', 'of', 'the', 'parametric', 'components', 'in', 'semiparametric', 'models', 'based', 'on', 'their', 'profile', 'likelihoods', 'the', 'higher', 'order', 'convergence', 'rate', 'of', 'kstep', 'mle', '... | [-0.06267517094966024, 0.019034059389772057, -0.11397095995683533, 0.11053436753233352, -0.06635391987704982, -0.13418765109963715, 0.05752679606060459, 0.4087171840365045, -0.21753652510233223, -0.2688478527707048, 0.17135515196666043, -0.23726562884015343, -0.13114850615177906, 0.23291656296108462, -0.101299228025406... |
708.3042 | Neutron channelling in a magnetic tube trap | Neutron channelling in a magnetic tube trap is discussed
| nucl-th | neutron channelling in a magnetic tube trap is discussed | [['neutron', 'channelling', 'in', 'a', 'magnetic', 'tube', 'trap', 'is', 'discussed']] | [-0.20840347868700823, 0.37940680152840084, 0.04872251467572318, 0.11931508785993275, -0.034032366135054164, -0.13874716761832437, -0.0338687544895543, 0.45055052306916976, -0.11711009353813198, -0.20104269310832024, 0.02143269470737626, -0.23057773926605782, 0.08374471755491363, 0.29559824036227333, -0.006053785793483... |
708.3043 | The dark nature of GRB 051022 and its host galaxy | We present multiwavelength (X-ray/optical/near-infrared/millimetre)
observations of GRB 051022 between 2.5 hours and ~1.15 yr after the event. It
is the most intense gamma-ray burst (~ 10^-4 erg cm^-2) detected by HETE-2,
with the exception of the nearby GRB 030329. Optical and near infrared
observations did not dete... | astro-ph | we present multiwavelength xrayopticalnearinfraredmillimetre observations of grb 051022 between 25 hours and 115 yr after the event it is the most intense gammaray burst 104 erg cm2 detected by hete2 with the exception of the nearby grb 030329 optical and near infrared observations did not detect the afterglow despite ... | [['we', 'present', 'multiwavelength', 'xrayopticalnearinfraredmillimetre', 'observations', 'of', 'grb', '051022', 'between', '25', 'hours', 'and', '115', 'yr', 'after', 'the', 'event', 'it', 'is', 'the', 'most', 'intense', 'gammaray', 'burst', '104', 'erg', 'cm2', 'detected', 'by', 'hete2', 'with', 'the', 'exception', ... | [-0.03972025096059271, 0.10661945218290914, -0.02515317450014526, 0.10192550657477846, -0.07816358783664248, -0.11171716418269713, 0.04791044343259561, 0.511475724710835, -0.09317805009254207, -0.3350057406384471, 0.04211117610755785, -0.31355681792973616, 0.04416064850788349, 0.17211772174782086, 0.0024581058929706153... |
708.3044 | Nondegenerate 3D complex Euclidean superintegrable systems and algebraic
varieties | A classical (or quantum) second order superintegrable system is an integrable
n-dimensional Hamiltonian system with potential that admits 2n-1 functionally
independent second order constants of the motion polynomial in the momenta, the
maximum possible. Such systems have remarkable properties: multi-integrability
and... | math-ph math.MP | a classical or quantum second order superintegrable system is an integrable ndimensional hamiltonian system with potential that admits 2n1 functionally independent second order constants of the motion polynomial in the momenta the maximum possible such systems have remarkable properties multiintegrability and multisepa... | [['a', 'classical', 'or', 'quantum', 'second', 'order', 'superintegrable', 'system', 'is', 'an', 'integrable', 'ndimensional', 'hamiltonian', 'system', 'with', 'potential', 'that', 'admits', '2n1', 'functionally', 'independent', 'second', 'order', 'constants', 'of', 'the', 'motion', 'polynomial', 'in', 'the', 'momenta'... | [-0.1948079841558135, 0.07971727971043217, -0.03139642432984645, 0.034395876069498815, -0.10508325089612146, -0.1842044959062316, -0.03295865330172118, 0.3371401214904159, -0.29474689254034175, -0.2351467082596445, 0.10364762837675665, -0.32138794716481583, -0.19389317362963554, 0.18750483334492757, -0.0660129758031413... |
708.3045 | From the BRST invariant Hamiltonian to the Field-Antifield Formalism | We study the relation between the lagrangian field-antifield formalism and
the BRST invariant phase space formulation of gauge theories. Starting from the
Batalin-Fradkin-Vilkovisky unitarized action, we demonstrate in a deductive way
the equivalence of the phase space, and the lagrangian field-antifield
partition fu... | hep-th | we study the relation between the lagrangian fieldantifield formalism and the brst invariant phase space formulation of gauge theories starting from the batalinfradkinvilkovisky unitarized action we demonstrate in a deductive way the equivalence of the phase space and the lagrangian fieldantifield partition functions f... | [['we', 'study', 'the', 'relation', 'between', 'the', 'lagrangian', 'fieldantifield', 'formalism', 'and', 'the', 'brst', 'invariant', 'phase', 'space', 'formulation', 'of', 'gauge', 'theories', 'starting', 'from', 'the', 'batalinfradkinvilkovisky', 'unitarized', 'action', 'we', 'demonstrate', 'in', 'a', 'deductive', 'w... | [-0.15177481930118566, 0.14258315325166812, -0.160630589752805, 0.10579496023117327, -0.08162872006605361, -0.061389735927257466, 0.019763669072120797, 0.31266391211572814, -0.26395518449591654, -0.24215082385960748, -0.016431957056435447, -0.22415967676423343, -0.24184387907678007, 0.04575626192358779, -0.043153013924... |
708.3046 | Metric fluctuations of an evaporating black hole from back reaction of
stress tensor fluctuations | This paper delineates the first steps in a systematic quantitative study of
the spacetime fluctuations induced by quantum fields in an evaporating black
hole under the stochastic gravity program. The central object of interest is
the noise kernel, which is the symmetrized two-point quantum correlation
function of the... | gr-qc | this paper delineates the first steps in a systematic quantitative study of the spacetime fluctuations induced by quantum fields in an evaporating black hole under the stochastic gravity program the central object of interest is the noise kernel which is the symmetrized twopoint quantum correlation function of the stre... | [['this', 'paper', 'delineates', 'the', 'first', 'steps', 'in', 'a', 'systematic', 'quantitative', 'study', 'of', 'the', 'spacetime', 'fluctuations', 'induced', 'by', 'quantum', 'fields', 'in', 'an', 'evaporating', 'black', 'hole', 'under', 'the', 'stochastic', 'gravity', 'program', 'the', 'central', 'object', 'of', 'i... | [-0.13216988177831868, 0.14252464078257676, -0.1223177191748367, 0.12289874481247375, -0.029212031345928043, -0.08558918416714939, -0.001075127591261625, 0.31331097707247013, -0.2222732922584727, -0.28103338798926386, 0.11476606358225055, -0.2862200582068938, -0.13416230623142764, 0.1756849120696628, -0.037368824586226... |
708.3047 | High energy neutrino yields from astrophysical sources II: Magnetized
sources | We calculate the yield of high energy neutrinos produced in astrophysical
sources for arbitrary interaction depths $\tau_0$ and magnetic field strengths
$B$. We take into account energy loss processes like synchrotron radiation and
diffusion of charged particles in turbulent magnetic fields as well as the
scattering ... | astro-ph hep-ph | we calculate the yield of high energy neutrinos produced in astrophysical sources for arbitrary interaction depths tau_0 and magnetic field strengths b we take into account energy loss processes like synchrotron radiation and diffusion of charged particles in turbulent magnetic fields as well as the scattering of secon... | [['we', 'calculate', 'the', 'yield', 'of', 'high', 'energy', 'neutrinos', 'produced', 'in', 'astrophysical', 'sources', 'for', 'arbitrary', 'interaction', 'depths', 'tau_0', 'and', 'magnetic', 'field', 'strengths', 'b', 'we', 'take', 'into', 'account', 'energy', 'loss', 'processes', 'like', 'synchrotron', 'radiation', ... | [-0.0658980060624139, 0.29600678259495555, 0.0019875196390785276, 0.16969526227368342, -0.001224241241992962, -0.11181936866093066, 0.0006095375602824554, 0.37226222511981766, -0.2401148047157368, -0.3588183196441781, -0.007270615453261041, -0.33950872775017016, 0.08106878797914233, 0.18480800245212572, 0.0754307975091... |
708.3048 | Identifying Small Mean Reverting Portfolios | Given multivariate time series, we study the problem of forming portfolios
with maximum mean reversion while constraining the number of assets in these
portfolios. We show that it can be formulated as a sparse canonical correlation
analysis and study various algorithms to solve the corresponding sparse
generalized ei... | cs.CE | given multivariate time series we study the problem of forming portfolios with maximum mean reversion while constraining the number of assets in these portfolios we show that it can be formulated as a sparse canonical correlation analysis and study various algorithms to solve the corresponding sparse generalized eigenv... | [['given', 'multivariate', 'time', 'series', 'we', 'study', 'the', 'problem', 'of', 'forming', 'portfolios', 'with', 'maximum', 'mean', 'reversion', 'while', 'constraining', 'the', 'number', 'of', 'assets', 'in', 'these', 'portfolios', 'we', 'show', 'that', 'it', 'can', 'be', 'formulated', 'as', 'a', 'sparse', 'canonic... | [-0.08271221513859928, 0.023240327600589288, -0.0845502544327506, 0.15899622060990493, -0.05963689744073365, -0.11440507731666523, 0.049219495350761075, 0.4082014654896089, -0.333358406914132, -0.3153843535908631, 0.17884837515718702, -0.25247398203771027, -0.19671235389209218, 0.15287015342286656, -0.10886816059106162... |
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