id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
707.043 | Assisted Problem Solving and Decompositions of Finite Automata | A study of assisted problem solving formalized via decompositions of
deterministic finite automata is initiated. The landscape of new types of
decompositions of finite automata this study uncovered is presented. Languages
with various degrees of decomposability between undecomposable and perfectly
decomposable are sh... | cs.CC | a study of assisted problem solving formalized via decompositions of deterministic finite automata is initiated the landscape of new types of decompositions of finite automata this study uncovered is presented languages with various degrees of decomposability between undecomposable and perfectly decomposable are shown ... | [['a', 'study', 'of', 'assisted', 'problem', 'solving', 'formalized', 'via', 'decompositions', 'of', 'deterministic', 'finite', 'automata', 'is', 'initiated', 'the', 'landscape', 'of', 'new', 'types', 'of', 'decompositions', 'of', 'finite', 'automata', 'this', 'study', 'uncovered', 'is', 'presented', 'languages', 'with... | [-0.16479050299514914, 0.1565463391857015, -0.0779632845479581, 0.08168413909669552, -0.062254070843725154, -0.159256634188609, 0.06670829546120431, 0.34473098278459574, -0.34278321363445785, -0.25365349360638195, 0.09188266698684958, -0.18722990478078524, -0.14909668352661862, 0.15880806268089348, -0.06834772686577506... |
707.0431 | Wick ordering for coherent state quantization in 1+1 de Sitter space | We show that the coherent state quantization of massive particles in 1+1 de
Sitter space exhibits an ordering property: There exist some classical
observables $A$ and $A^*$ such that $O_{A^{*p}}O_{A^q}=O_{A^{*p} A^q}$ $p, q
\in \Z$, where $O_A$ is the quantum observable corresponding to the classical
observable $A$.
| math-ph math.MP | we show that the coherent state quantization of massive particles in 11 de sitter space exhibits an ordering property there exist some classical observables a and a such that o_apo_aqo_ap aq p q in z where o_a is the quantum observable corresponding to the classical observable a | [['we', 'show', 'that', 'the', 'coherent', 'state', 'quantization', 'of', 'massive', 'particles', 'in', '11', 'de', 'sitter', 'space', 'exhibits', 'an', 'ordering', 'property', 'there', 'exist', 'some', 'classical', 'observables', 'a', 'and', 'a', 'such', 'that', 'o_apo_aqo_ap', 'aq', 'p', 'q', 'in', 'z', 'where', 'o_a... | [-0.20091737304692683, 0.2464854840354351, -0.14257752761730683, 0.10276167703357161, -0.0162934937271411, -0.13473256619687637, 0.0019939559380240416, 0.3302698849659899, -0.268085483967772, -0.2066223767950483, 0.030446196005315236, -0.25949060833891446, -0.13440718861175296, 0.14872149674667287, -0.03275235944791981... |
707.0432 | An algebraic proof of the commutativity of the intersection with
divisors | We present a purely algebraic proof of the commutativity of the operation
defined by intersection with divisors on the Chow group of a local Noetherian
domain.
| math.AC math.AG | we present a purely algebraic proof of the commutativity of the operation defined by intersection with divisors on the chow group of a local noetherian domain | [['we', 'present', 'a', 'purely', 'algebraic', 'proof', 'of', 'the', 'commutativity', 'of', 'the', 'operation', 'defined', 'by', 'intersection', 'with', 'divisors', 'on', 'the', 'chow', 'group', 'of', 'a', 'local', 'noetherian', 'domain']] | [-0.31574029188889724, -0.026331508782907173, -0.19313994504941198, -0.01011970338339989, -0.12310715521184298, -0.11179061703240642, 0.04919031475527355, 0.23489439161494374, -0.361688647705775, -0.17468179407744452, 0.14625358959445015, -0.17537928458589774, -0.06500011548185004, 0.1500717755407095, -0.19912019830483... |
707.0433 | Unstable Semiclassical Trajectories in Tunneling | Some tunneling phenomena are described, in the semiclassical approximation,
by unstable complex trajectories. We develop a systematic procedure to
stabilize the trajectories and to calculate the tunneling probability,
including both the suppression exponent and prefactor. We find that the
instability of tunneling sol... | quant-ph cond-mat.stat-mech hep-th math-ph math.MP nlin.CD physics.chem-ph | some tunneling phenomena are described in the semiclassical approximation by unstable complex trajectories we develop a systematic procedure to stabilize the trajectories and to calculate the tunneling probability including both the suppression exponent and prefactor we find that the instability of tunneling solutions ... | [['some', 'tunneling', 'phenomena', 'are', 'described', 'in', 'the', 'semiclassical', 'approximation', 'by', 'unstable', 'complex', 'trajectories', 'we', 'develop', 'a', 'systematic', 'procedure', 'to', 'stabilize', 'the', 'trajectories', 'and', 'to', 'calculate', 'the', 'tunneling', 'probability', 'including', 'both',... | [-0.15334631521254777, 0.1337895107145111, -0.12380781793035567, 0.12667779360587397, -0.0013843311317032203, -0.15865100514298927, 0.06456505665555597, 0.2961772567437341, -0.2616474930352221, -0.27663775634331006, 0.004790798603789881, -0.3202728632449483, -0.1632962641461442, 0.20229784110561014, 0.00745812841341830... |
707.0434 | Another generalization of Mason's ABC-theorem | We show a generalization of Mason's ABC-theorem, with the only conditions
that the greatest common divisor has been divided out and no proper subsum of
the (possibly multivariate) polynomial sum f_1 + f_2 + ... + f_n = 0 vanishes.
As a result, we show that the generalized Fermat-Catalan equation for
polynomials: g_... | math.NT | we show a generalization of masons abctheorem with the only conditions that the greatest common divisor has been divided out and no proper subsum of the possibly multivariate polynomial sum f_1 f_2 f_n 0 vanishes as a result we show that the generalized fermatcatalan equation for polynomials g_1d_1 g_1d_2 g_nd_n 0 has ... | [['we', 'show', 'a', 'generalization', 'of', 'masons', 'abctheorem', 'with', 'the', 'only', 'conditions', 'that', 'the', 'greatest', 'common', 'divisor', 'has', 'been', 'divided', 'out', 'and', 'no', 'proper', 'subsum', 'of', 'the', 'possibly', 'multivariate', 'polynomial', 'sum', 'f_1', 'f_2', 'f_n', '0', 'vanishes', ... | [-0.20602702286015165, 0.08642017783874527, -0.08752145951593969, 0.06330226077029402, -0.07228138885074394, -0.1702303358234782, 0.001224161014258069, 0.31506587385616086, -0.2755035571716825, -0.12108569812683508, 0.08075282562702418, -0.3282608000086026, -0.1487706811250896, 0.17502786707089088, -0.03389033203587887... |
707.0435 | Spectrally resolved optical frequency comb from a self-referenced 5 GHz
femtosecond laser | We report a mode-locked Ti:sapphire femtosecond laser with 5GHz repetition
rate. Spectral broadening of the 24 fs pulses in a microstructured fiber yields
an octave-spanning spectrum and permits self-referencing and active
stabilization of the emitted femtosecond laser frequency comb (FLFC). The
individual modes of t... | physics.optics physics.atom-ph | we report a modelocked tisapphire femtosecond laser with 5ghz repetition rate spectral broadening of the 24 fs pulses in a microstructured fiber yields an octavespanning spectrum and permits selfreferencing and active stabilization of the emitted femtosecond laser frequency comb flfc the individual modes of the 5ghz fl... | [['we', 'report', 'a', 'modelocked', 'tisapphire', 'femtosecond', 'laser', 'with', '5ghz', 'repetition', 'rate', 'spectral', 'broadening', 'of', 'the', '24', 'fs', 'pulses', 'in', 'a', 'microstructured', 'fiber', 'yields', 'an', 'octavespanning', 'spectrum', 'and', 'permits', 'selfreferencing', 'and', 'active', 'stabil... | [-0.14967708168308794, 0.16699758734624387, -0.07786487064440735, -0.04648791304389306, -0.06686715205044796, -0.17668256861312936, 0.05581144392490387, 0.5520047328124443, -0.20512758328889807, -0.2556047351642822, 0.10889661684826327, -0.2202315627054001, -0.018732950964476913, 0.33259334803879026, -0.012726263614119... |
707.0436 | Multiparticle correlations and momentum conservation in nucleus-nucleus
collisions | Particle correlations are very actively studied in heavy-ion collisions at
ultra-relativistic energies. Here, an attempt is made at determining a proper
reference for such studies, by taking properly into account the multiparticle
correlations induced by the conservation of total momentum in the collisions.
| nucl-th | particle correlations are very actively studied in heavyion collisions at ultrarelativistic energies here an attempt is made at determining a proper reference for such studies by taking properly into account the multiparticle correlations induced by the conservation of total momentum in the collisions | [['particle', 'correlations', 'are', 'very', 'actively', 'studied', 'in', 'heavyion', 'collisions', 'at', 'ultrarelativistic', 'energies', 'here', 'an', 'attempt', 'is', 'made', 'at', 'determining', 'a', 'proper', 'reference', 'for', 'such', 'studies', 'by', 'taking', 'properly', 'into', 'account', 'the', 'multiparticl... | [-0.10084414785338003, 0.2670708503063124, -0.15423507148096727, 0.1486259538079287, 0.07082398380910934, -0.042845937239309385, -0.08992644639815701, 0.3805961599356906, -0.22856501519116898, -0.32026932873698166, -0.04047318918868726, -0.32632191002715466, 0.08586394245368104, 0.11051215712291725, 0.05968436841354813... |
707.0437 | Modular Abelian Variety of Odd Modular Degree | We will study modular Abelian varieties with odd congruence numbers, by
studying the cuspidal subgroup of $J_0(N)$. We show the conductor of such
Abelian varieties must be of a special type, for example if $N$ is odd then
$N=p^\alpha$ or $N=pq$ for some prime $p$ and $q$. We then focus our attention
to modular ellipt... | math.NT | we will study modular abelian varieties with odd congruence numbers by studying the cuspidal subgroup of j_0n we show the conductor of such abelian varieties must be of a special type for example if n is odd then npalpha or npq for some prime p and q we then focus our attention to modular elliptic curves and using resu... | [['we', 'will', 'study', 'modular', 'abelian', 'varieties', 'with', 'odd', 'congruence', 'numbers', 'by', 'studying', 'the', 'cuspidal', 'subgroup', 'of', 'j_0n', 'we', 'show', 'the', 'conductor', 'of', 'such', 'abelian', 'varieties', 'must', 'be', 'of', 'a', 'special', 'type', 'for', 'example', 'if', 'n', 'is', 'odd',... | [-0.24258878311830695, 0.09183385458005511, -0.13405508760605817, 0.09652142343744029, -0.13262049013080643, -0.21786948826427208, -0.03202764019775002, 0.31651254988315963, -0.2928867007696839, -0.261306137504542, 0.06692758879786276, -0.2740787052063514, -0.16382763420899762, 0.2657279030738763, -0.1398372106436316, ... |
707.0438 | High Performance Direct Gravitational N-body Simulations on Graphics
Processing Units -- II: An implementation in CUDA | We present the results of gravitational direct $N$-body simulations using the
Graphics Processing Unit (GPU) on a commercial NVIDIA GeForce 8800GTX designed
for gaming computers. The force evaluation of the $N$-body problem is
implemented in ``Compute Unified Device Architecture'' (CUDA) using the GPU to
speed-up the... | astro-ph physics.comp-ph | we present the results of gravitational direct nbody simulations using the graphics processing unit gpu on a commercial nvidia geforce 8800gtx designed for gaming computers the force evaluation of the nbody problem is implemented in compute unified device architecture cuda using the gpu to speedup the calculations we t... | [['we', 'present', 'the', 'results', 'of', 'gravitational', 'direct', 'nbody', 'simulations', 'using', 'the', 'graphics', 'processing', 'unit', 'gpu', 'on', 'a', 'commercial', 'nvidia', 'geforce', '8800gtx', 'designed', 'for', 'gaming', 'computers', 'the', 'force', 'evaluation', 'of', 'the', 'nbody', 'problem', 'is', '... | [-0.16341922072590226, 0.010419889910125223, -0.07096943484871211, 0.034726176336115216, -0.06654850673717828, -0.14970578032811194, -0.0014157162873515328, 0.39842787336396135, -0.2116094154265264, -0.38035571558068054, 0.08817165038618147, -0.2488660916701805, -0.05237139507415052, 0.2766101115241485, 0.0238333322211... |
707.0439 | Work and heat probability distribution of an optically driven Brownian
particle: Theory and experiments | We analyze the equations governing the evolution of distributions of the work
and the heat exchanged with the environment by a manipulated stochastic system,
by means of a compact and general derivation. We obtain explicit solutions for
these equations for the case of a dragged Brownian particle in a harmonic
potenti... | cond-mat.stat-mech cond-mat.soft | we analyze the equations governing the evolution of distributions of the work and the heat exchanged with the environment by a manipulated stochastic system by means of a compact and general derivation we obtain explicit solutions for these equations for the case of a dragged brownian particle in a harmonic potential w... | [['we', 'analyze', 'the', 'equations', 'governing', 'the', 'evolution', 'of', 'distributions', 'of', 'the', 'work', 'and', 'the', 'heat', 'exchanged', 'with', 'the', 'environment', 'by', 'a', 'manipulated', 'stochastic', 'system', 'by', 'means', 'of', 'a', 'compact', 'and', 'general', 'derivation', 'we', 'obtain', 'exp... | [-0.09632997124029014, 0.152313476515313, -0.08730587770541509, -0.008542100195772945, -0.0037130085937678815, -0.10267195612192154, 0.02857075083224724, 0.330130727365613, -0.2380267049682637, -0.30113761936624844, 0.06818951839270691, -0.2936545614215235, -0.11959062905982137, 0.21428852668963372, 0.00547967700908581... |
707.044 | Lagrangian Particle Statistics in Turbulent Flows from a Simple Vortex
Model | The statistics of Lagrangian particles in turbulent flows is considered in
the framework of a simple vortex model. Here, the turbulent velocity field is
represented by a temporal sequence of Burgers vortices of different
circulation, strain, and orientation. Based on suitable assumptions about the
vortices' statistic... | physics.flu-dyn | the statistics of lagrangian particles in turbulent flows is considered in the framework of a simple vortex model here the turbulent velocity field is represented by a temporal sequence of burgers vortices of different circulation strain and orientation based on suitable assumptions about the vortices statistical prope... | [['the', 'statistics', 'of', 'lagrangian', 'particles', 'in', 'turbulent', 'flows', 'is', 'considered', 'in', 'the', 'framework', 'of', 'a', 'simple', 'vortex', 'model', 'here', 'the', 'turbulent', 'velocity', 'field', 'is', 'represented', 'by', 'a', 'temporal', 'sequence', 'of', 'burgers', 'vortices', 'of', 'different... | [-0.1924497616694194, 0.1686857619437657, -0.1118815610797642, 0.08911404075987688, -0.029145538041444673, -0.04623451176392909, -0.03610570195341508, 0.342216316508512, -0.2901517307794053, -0.25725544263187744, 0.05955438330539898, -0.1720847437997055, -0.13494714099454552, 0.17997007497445974, -0.009327567016629323,... |
707.0441 | Kelvon-roton instability of vortex lines in dipolar Bose-Einstein
condensates | The physics of vortex lines in dipolar condensates is studied. Due to the
nonlocality of the dipolar interaction, the 3D character of the vortex plays a
more important role in dipolar gases than in typical short-range interacting
ones. In particular, the dipolar interaction significantly affects the
stability of the ... | cond-mat.other | the physics of vortex lines in dipolar condensates is studied due to the nonlocality of the dipolar interaction the 3d character of the vortex plays a more important role in dipolar gases than in typical shortrange interacting ones in particular the dipolar interaction significantly affects the stability of the transve... | [['the', 'physics', 'of', 'vortex', 'lines', 'in', 'dipolar', 'condensates', 'is', 'studied', 'due', 'to', 'the', 'nonlocality', 'of', 'the', 'dipolar', 'interaction', 'the', '3d', 'character', 'of', 'the', 'vortex', 'plays', 'a', 'more', 'important', 'role', 'in', 'dipolar', 'gases', 'than', 'in', 'typical', 'shortran... | [-0.2491247805442539, 0.20488331880038016, -0.048321904423080875, 0.07116190234860667, -0.0256655696696802, -0.11710456431469071, -0.016743339304420575, 0.32197691308264836, -0.21463173339752672, -0.24041990500713795, -0.00874544833199269, -0.2380760381146221, -0.08157877620118105, 0.17417692682035615, 0.04794546494382... |
707.0442 | Dyson's non-intersecting Brownian motions with a few outliers | Consider n non-intersecting particles on the real line (Dyson Brownian
motions), all starting from the origin at time=0, and forced to return to x=0
at time=1. For large n, the average mean density of particles has its support,
for each 0<t<1, within the interior of an ellipse. The Airy process is defined
as the moti... | math.PR math-ph math.MP | consider n nonintersecting particles on the real line dyson brownian motions all starting from the origin at time0 and forced to return to x0 at time1 for large n the average mean density of particles has its support for each 0t1 within the interior of an ellipse the airy process is defined as the motion of these nonin... | [['consider', 'n', 'nonintersecting', 'particles', 'on', 'the', 'real', 'line', 'dyson', 'brownian', 'motions', 'all', 'starting', 'from', 'the', 'origin', 'at', 'time0', 'and', 'forced', 'to', 'return', 'to', 'x0', 'at', 'time1', 'for', 'large', 'n', 'the', 'average', 'mean', 'density', 'of', 'particles', 'has', 'its'... | [-0.12743448995667078, 0.12319167953448813, -0.09817417929766745, 0.026779044296235066, -0.0395403520476709, -0.11092528735809937, 0.035631529758002885, 0.34739181734962254, -0.29629646194871606, -0.22169938105181222, 0.09333526588204066, -0.311184386045831, -0.09930954464007079, 0.16184570504034437, -0.055848932249198... |
707.0443 | On a possible interpretation of fusion in Stochastic Loewner Evolution | We suggest how to give a physical interpretation of Stochastic Loewner
Evolution traces approaching a marked point in the upper half plane. We show
that this may be related to the fusion of boundary with bulk fields in
Conformal Field Theory by taking a look at the probability of such an event.
| hep-th math-ph math.MP | we suggest how to give a physical interpretation of stochastic loewner evolution traces approaching a marked point in the upper half plane we show that this may be related to the fusion of boundary with bulk fields in conformal field theory by taking a look at the probability of such an event | [['we', 'suggest', 'how', 'to', 'give', 'a', 'physical', 'interpretation', 'of', 'stochastic', 'loewner', 'evolution', 'traces', 'approaching', 'a', 'marked', 'point', 'in', 'the', 'upper', 'half', 'plane', 'we', 'show', 'that', 'this', 'may', 'be', 'related', 'to', 'the', 'fusion', 'of', 'boundary', 'with', 'bulk', 'f... | [-0.14823647336855245, 0.12862817025457984, -0.13988822852619565, 0.059776907918813564, -0.060499151989531055, -0.05515571978265563, 0.045780426918869264, 0.3493524616978203, -0.2827067863321505, -0.2490635811118409, 0.11633483220626098, -0.24108155266954923, -0.17017264197168586, 0.18328746144946378, -0.06113059345023... |
707.0444 | Necessary and Sufficient Conditions for the Trumping Relation | Entanglement catalysis allows one to convert certain entangled states into
others by the temporary involvement of another entangled state (so-called
catalyst), where after the conversion the catalyst is returned to the same
state. For bipartite pure entangled states that can be transformed in this way
with unit proba... | quant-ph | entanglement catalysis allows one to convert certain entangled states into others by the temporary involvement of another entangled state socalled catalyst where after the conversion the catalyst is returned to the same state for bipartite pure entangled states that can be transformed in this way with unit probability ... | [['entanglement', 'catalysis', 'allows', 'one', 'to', 'convert', 'certain', 'entangled', 'states', 'into', 'others', 'by', 'the', 'temporary', 'involvement', 'of', 'another', 'entangled', 'state', 'socalled', 'catalyst', 'where', 'after', 'the', 'conversion', 'the', 'catalyst', 'is', 'returned', 'to', 'the', 'same', 's... | [-0.10310420959555174, 0.1876564161579558, -0.08949098435308163, 0.06107180736338099, -0.05081399033251391, -0.17150115334273627, 0.0642941886649674, 0.27820374931346764, -0.28479880846484945, -0.25445367088023985, 0.08570050509189497, -0.2676061673643104, -0.06892209751876416, 0.16259437997790951, -0.0656704379189587,... |
707.0445 | Rubinstein distance on configurations spaces | By a method inspired of the Stein's method, we derive an upper-bound of the
Rubinstein distance between two absolutely continuous probability measures on
configurations space. As an application, we show that the best way to
approximate a Modulated Poisson Process (see below for the definition) by a
Poisson process is... | math.PR | by a method inspired of the steins method we derive an upperbound of the rubinstein distance between two absolutely continuous probability measures on configurations space as an application we show that the best way to approximate a modulated poisson process see below for the definition by a poisson process is to equat... | [['by', 'a', 'method', 'inspired', 'of', 'the', 'steins', 'method', 'we', 'derive', 'an', 'upperbound', 'of', 'the', 'rubinstein', 'distance', 'between', 'two', 'absolutely', 'continuous', 'probability', 'measures', 'on', 'configurations', 'space', 'as', 'an', 'application', 'we', 'show', 'that', 'the', 'best', 'way', ... | [-0.07320737712844103, 0.07179143185419014, -0.14207860313925064, 0.1023090687557905, -0.03515829356318271, -0.07315885093649505, 0.12901341744388142, 0.4108690274534402, -0.3053128099784738, -0.28014371663125026, 0.05086696691190203, -0.2231164946289802, -0.20558427388055456, 0.2341154313309946, -0.11232403165626305, ... |
707.0446 | $B \to K_1(1270) (\to \rho K) \ell^+ \ell^-$ in LEET | Flavour Changing Neutral Current decays of the $B$-meson are a very useful
tool for studying possible physics scenarios beyond the Standard Model (SM),
where of the many FCNC modes radiative, purely leptonic and semi-leptonic
decays of the $B$-meson are relatively clean tests. Within this context the
BELLE collaborat... | hep-ph | flavour changing neutral current decays of the bmeson are a very useful tool for studying possible physics scenarios beyond the standard model sm where of the many fcnc modes radiative purely leptonic and semileptonic decays of the bmeson are relatively clean tests within this context the belle collaboration has search... | [['flavour', 'changing', 'neutral', 'current', 'decays', 'of', 'the', 'bmeson', 'are', 'a', 'very', 'useful', 'tool', 'for', 'studying', 'possible', 'physics', 'scenarios', 'beyond', 'the', 'standard', 'model', 'sm', 'where', 'of', 'the', 'many', 'fcnc', 'modes', 'radiative', 'purely', 'leptonic', 'and', 'semileptonic'... | [-0.06265603422454392, 0.23713411404239104, -0.04420947839773094, 0.12417880288204153, -0.07179764692144569, -0.1774429934597466, 0.0988351099649733, 0.28752452571147175, -0.21777401330642576, -0.25105844585354936, 0.008088777593495829, -0.2901222879363065, -0.032549018431960265, 0.16996697675573907, 0.1053422747970407... |
707.0447 | Subrings which are closed with respect to taking the inverse | Let S be a subring of the ring R. We investigate the question of whether S
intersected by U(R) is equal to U(S) holds for the units. In many situations
our answer is positive. There is a special emphasis on the case when R is a
full matrix ring and S is a structural subring of R defined by a reflexive and
transitive ... | math.RA | let s be a subring of the ring r we investigate the question of whether s intersected by ur is equal to us holds for the units in many situations our answer is positive there is a special emphasis on the case when r is a full matrix ring and s is a structural subring of r defined by a reflexive and transitive relation | [['let', 's', 'be', 'a', 'subring', 'of', 'the', 'ring', 'r', 'we', 'investigate', 'the', 'question', 'of', 'whether', 's', 'intersected', 'by', 'ur', 'is', 'equal', 'to', 'us', 'holds', 'for', 'the', 'units', 'in', 'many', 'situations', 'our', 'answer', 'is', 'positive', 'there', 'is', 'a', 'special', 'emphasis', 'on'... | [-0.20242316238000058, 0.06447125542035792, -0.04886567304492928, 0.04009560709710058, -0.052395972423255444, -0.22242482897854643, 0.0019036101584788412, 0.3336726072593592, -0.3186344426940195, -0.17827020370168611, 0.10831769040487416, -0.2928615148739482, -0.0937792357581202, 0.18690330960816937, -0.119139535556314... |
707.0448 | Precision measurement of the $3d \to 2p$ x-ray energy in kaonic $^4$He | We have measured the Balmer-series x-rays of kaonic $^4$He atoms using novel
large-area silicon drift x-ray detectors in order to study the low-energy
$\bar{K}$-nucleus strong interaction. The energy of the $3d \to 2p$ transition
was determined to be 6467 $\pm$ 3 (stat) $\pm$ 2 (syst) eV. The resulting
strong-interac... | nucl-ex | we have measured the balmerseries xrays of kaonic 4he atoms using novel largearea silicon drift xray detectors in order to study the lowenergy barknucleus strong interaction the energy of the 3d to 2p transition was determined to be 6467 pm 3 stat pm 2 syst ev the resulting stronginteraction energylevel shift is in agr... | [['we', 'have', 'measured', 'the', 'balmerseries', 'xrays', 'of', 'kaonic', '4he', 'atoms', 'using', 'novel', 'largearea', 'silicon', 'drift', 'xray', 'detectors', 'in', 'order', 'to', 'study', 'the', 'lowenergy', 'barknucleus', 'strong', 'interaction', 'the', 'energy', 'of', 'the', '3d', 'to', '2p', 'transition', 'was... | [-0.05012127116972965, 0.1903206097730805, -0.0256957662410088, 0.06131449391296695, 0.02602778250233285, -0.12352771688223121, 0.06069455137069795, 0.40568958527393756, -0.20601787137251998, -0.4146915663565908, -0.06571429268279601, -0.40985885289098534, -0.01415096955846936, 0.13187791048253458, 0.000761477794084284... |
707.0449 | Optical spectroscopy of the low mass X-ray binary GX9+9 | Phase-resolved medium resolution VLT spectroscopy of the low mass X-ray
binary GX9+9 has revealed narrow CIII emission lines that move in phase
relative to our new estimate of the ephemeris, and show a velocity amplitude of
230+/-35 km/s. We identify the origin of these lines as coming from the surface
of the donor s... | astro-ph | phaseresolved medium resolution vlt spectroscopy of the low mass xray binary gx99 has revealed narrow ciii emission lines that move in phase relative to our new estimate of the ephemeris and show a velocity amplitude of 23035 kms we identify the origin of these lines as coming from the surface of the donor star thereby... | [['phaseresolved', 'medium', 'resolution', 'vlt', 'spectroscopy', 'of', 'the', 'low', 'mass', 'xray', 'binary', 'gx99', 'has', 'revealed', 'narrow', 'ciii', 'emission', 'lines', 'that', 'move', 'in', 'phase', 'relative', 'to', 'our', 'new', 'estimate', 'of', 'the', 'ephemeris', 'and', 'show', 'a', 'velocity', 'amplitud... | [-0.10369815352160115, 0.10369381598300403, -0.04042115815581731, 0.05916610325220972, -0.07503155515713181, -0.1130718084908792, 0.08546818064433741, 0.43298275791752483, -0.1988971019055936, -0.3109614728995955, 0.07542022972591911, -0.29479359881377515, -0.03880978328747859, 0.20972127890369544, -0.06358401355190622... |
707.045 | Large Negative Thermal Expansion in Pentacene due to Steric Hindrance | The uniaxial negative thermal expansion in pentacene crystals along $a$ is a
particularity in the series of the oligoacenes, and exeptionally large for a
crystalline solid. Full x-ray structure analysis from 120 K to 413 K reveals
that the dominant thermal motion is a libration of the rigid molecules about
their long... | cond-mat.mtrl-sci | the uniaxial negative thermal expansion in pentacene crystals along a is a particularity in the series of the oligoacenes and exeptionally large for a crystalline solid full xray structure analysis from 120 k to 413 k reveals that the dominant thermal motion is a libration of the rigid molecules about their long axes m... | [['the', 'uniaxial', 'negative', 'thermal', 'expansion', 'in', 'pentacene', 'crystals', 'along', 'a', 'is', 'a', 'particularity', 'in', 'the', 'series', 'of', 'the', 'oligoacenes', 'and', 'exeptionally', 'large', 'for', 'a', 'crystalline', 'solid', 'full', 'xray', 'structure', 'analysis', 'from', '120', 'k', 'to', '413... | [-0.19111737060803372, 0.20808833662910028, -0.032967368156084274, -0.033864576164365855, -0.028098691155614912, -0.09152057942873264, 0.06958274157778895, 0.38787775371437433, -0.31114590152731686, -0.28992060924590124, -0.0209016765030788, -0.3070745770132444, -0.08131053794335696, 0.12700826870124848, 0.046788259307... |
707.0451 | Robust and efficient generator of almost maximal multipartite
entanglement | Quantum chaotic maps can efficiently generate pseudo-random states carrying
almost maximal multipartite entanglement, as characterized by the probability
distribution of bipartite entanglement between all possible bipartitions of the
system. We show that such multipartite entanglement is robust, in the sense
that, wh... | quant-ph | quantum chaotic maps can efficiently generate pseudorandom states carrying almost maximal multipartite entanglement as characterized by the probability distribution of bipartite entanglement between all possible bipartitions of the system we show that such multipartite entanglement is robust in the sense that when real... | [['quantum', 'chaotic', 'maps', 'can', 'efficiently', 'generate', 'pseudorandom', 'states', 'carrying', 'almost', 'maximal', 'multipartite', 'entanglement', 'as', 'characterized', 'by', 'the', 'probability', 'distribution', 'of', 'bipartite', 'entanglement', 'between', 'all', 'possible', 'bipartitions', 'of', 'the', 's... | [-0.20432396818286003, 0.29542525353104765, -0.023125973599615383, 0.06367050781637541, 0.09968234538170162, -0.24215802499579628, 0.04494567250888517, 0.3400914603149268, -0.2575918806355391, -0.26789041529340085, 0.0343661350111213, -0.3100545241900567, -0.12573579245650057, 0.19519315298591086, -0.07565327389721772,... |
707.0452 | Instanton representation of Plebanski gravity: IX. Hamiltonian
minisuperspace dynamics in undensitized momentum space variables | In this paper we illustrate the dynamics of the instanton representation in
the description of vacuum GR in minisuperspace for undensitized variables. We
uncover a new class of general solutions in both the degenerate and the
nondegenerate sectors of the theory. Additionally, the individual sectors are
preserved unde... | gr-qc | in this paper we illustrate the dynamics of the instanton representation in the description of vacuum gr in minisuperspace for undensitized variables we uncover a new class of general solutions in both the degenerate and the nondegenerate sectors of the theory additionally the individual sectors are preserved under ham... | [['in', 'this', 'paper', 'we', 'illustrate', 'the', 'dynamics', 'of', 'the', 'instanton', 'representation', 'in', 'the', 'description', 'of', 'vacuum', 'gr', 'in', 'minisuperspace', 'for', 'undensitized', 'variables', 'we', 'uncover', 'a', 'new', 'class', 'of', 'general', 'solutions', 'in', 'both', 'the', 'degenerate',... | [-0.1424371946413885, 0.10268579214812235, -0.09126792450842913, 0.09816561065053975, -0.02799203761969693, -0.07324414492904907, -0.0006243733623705339, 0.3261406126257498, -0.25263739177171374, -0.2535941788373748, 0.09400179951262544, -0.242289399893707, -0.19087727676378563, 0.1271664175146725, -0.0322419799376803,... |
707.0453 | Bose-Einstein condensates under a spatially-modulated transverse
confinement | We derive an effective nonpolynomial Schrodinger equation (NPSE) for
self-repulsive or attractive BEC in the nearly-1D cigar-shaped trap, with the
transverse confining frequency periodically modulated along the axial
direction. Besides the usual linear cigar-shaped trap, where the periodic
modulation emulates the act... | cond-mat.other | we derive an effective nonpolynomial schrodinger equation npse for selfrepulsive or attractive bec in the nearly1d cigarshaped trap with the transverse confining frequency periodically modulated along the axial direction besides the usual linear cigarshaped trap where the periodic modulation emulates the action of an o... | [['we', 'derive', 'an', 'effective', 'nonpolynomial', 'schrodinger', 'equation', 'npse', 'for', 'selfrepulsive', 'or', 'attractive', 'bec', 'in', 'the', 'nearly1d', 'cigarshaped', 'trap', 'with', 'the', 'transverse', 'confining', 'frequency', 'periodically', 'modulated', 'along', 'the', 'axial', 'direction', 'besides',... | [-0.12426224139492485, 0.13801527657566187, -0.0500700075467994, 0.07562073581506176, -0.04451336852160462, -0.19805173557088301, -0.01007592317386808, 0.375384031658807, -0.24766511523317306, -0.21064199596828623, 0.06274783668960636, -0.2708971454266306, -0.12552680604143493, 0.16247755419925858, 0.050380423088416414... |
707.0454 | Optimal Strategies for Gaussian Jamming in Block-Fading Channels under
Delay and Power Constraints | Without assuming any knowledge on source's codebook and its output signals,
we formulate a Gaussian jamming problem in block fading channels as a
two-player zero sum game. The outage probability is adopted as an objective
function, over which transmitter aims at minimization and jammer aims at
maximization by selecti... | cs.IT math.IT | without assuming any knowledge on sources codebook and its output signals we formulate a gaussian jamming problem in block fading channels as a twoplayer zero sum game the outage probability is adopted as an objective function over which transmitter aims at minimization and jammer aims at maximization by selecting thei... | [['without', 'assuming', 'any', 'knowledge', 'on', 'sources', 'codebook', 'and', 'its', 'output', 'signals', 'we', 'formulate', 'a', 'gaussian', 'jamming', 'problem', 'in', 'block', 'fading', 'channels', 'as', 'a', 'twoplayer', 'zero', 'sum', 'game', 'the', 'outage', 'probability', 'is', 'adopted', 'as', 'an', 'objecti... | [-0.15979013905267825, -0.03876887412453388, -0.09758037669922817, 0.08782713949701494, -0.04433979468462481, -0.2442185140638189, 0.16258549719879573, 0.39198375716805456, -0.2882924735292115, -0.23719224286350338, 0.1288437884502028, -0.2702840208710933, -0.1632763971489939, 0.10947277350351214, -0.13618473274294626,... |
707.0455 | Strings and D-branes in a supersymmetric magnetic flux background | We investigate how the presence of RR magnetic $F_{p+2}$ fluxes affects the
energy of classical Dp branes, for specific string theory supersymmetric
backgrounds which are solutions to the leading order in $\alpha'$ including
back-reaction effects. The Dp brane dynamics is found to be similar to the well
known dynamic... | hep-th | we investigate how the presence of rr magnetic f_p2 fluxes affects the energy of classical dp branes for specific string theory supersymmetric backgrounds which are solutions to the leading order in alpha including backreaction effects the dp brane dynamics is found to be similar to the well known dynamics of particles... | [['we', 'investigate', 'how', 'the', 'presence', 'of', 'rr', 'magnetic', 'f_p2', 'fluxes', 'affects', 'the', 'energy', 'of', 'classical', 'dp', 'branes', 'for', 'specific', 'string', 'theory', 'supersymmetric', 'backgrounds', 'which', 'are', 'solutions', 'to', 'the', 'leading', 'order', 'in', 'alpha', 'including', 'bac... | [-0.16749445712796862, 0.21241402264228829, -0.044160495435135616, 0.15729732852070694, -0.08433928184559662, -0.14434403633002005, -0.004196445575099532, 0.2773306645225171, -0.21647617807812827, -0.32534833637689303, 0.04922582539847027, -0.2594791649063553, -0.09042274393308773, 0.13375073318744896, -0.0308248919481... |
707.0456 | Blocking: New examples and properties of products | We say that a pair of points x and y is secure if there exist a finite set of
blocking points such that any geodesic between x and y passes through one of
the blocking points. The main point of this paper is to exhibit new examples of
blocking phenomena both in the manifold and the billiard table setting. As an
appro... | math.DG math.DS | we say that a pair of points x and y is secure if there exist a finite set of blocking points such that any geodesic between x and y passes through one of the blocking points the main point of this paper is to exhibit new examples of blocking phenomena both in the manifold and the billiard table setting as an approach ... | [['we', 'say', 'that', 'a', 'pair', 'of', 'points', 'x', 'and', 'y', 'is', 'secure', 'if', 'there', 'exist', 'a', 'finite', 'set', 'of', 'blocking', 'points', 'such', 'that', 'any', 'geodesic', 'between', 'x', 'and', 'y', 'passes', 'through', 'one', 'of', 'the', 'blocking', 'points', 'the', 'main', 'point', 'of', 'this... | [-0.23574911207335708, 0.06425241762903072, -0.09560047466645405, 0.0505820805888198, -0.02898895935680492, -0.1828687548881159, 0.12487575321242639, 0.3860695953262132, -0.2852184621667202, -0.20067402846144744, 0.13261147828119488, -0.30701939881022944, -0.1565227931124727, 0.19666423844079794, -0.11851091278816929, ... |
707.0457 | Density of critical points for a Gaussian random function | Critical points of a scalar quantitiy are either extremal points or saddle
points. The character of the critical points is determined by the sign
distribution of the eigenvalues of the Hessian matrix. For a two-dimensional
homogeneous and isotropic random function topological arguments are sufficient
to show that all... | physics.flu-dyn | critical points of a scalar quantitiy are either extremal points or saddle points the character of the critical points is determined by the sign distribution of the eigenvalues of the hessian matrix for a twodimensional homogeneous and isotropic random function topological arguments are sufficient to show that all poss... | [['critical', 'points', 'of', 'a', 'scalar', 'quantitiy', 'are', 'either', 'extremal', 'points', 'or', 'saddle', 'points', 'the', 'character', 'of', 'the', 'critical', 'points', 'is', 'determined', 'by', 'the', 'sign', 'distribution', 'of', 'the', 'eigenvalues', 'of', 'the', 'hessian', 'matrix', 'for', 'a', 'twodimensi... | [-0.21719029581894306, 0.1533304157687612, -0.08558800933813607, 0.0959723256830195, -0.034889846971189534, -0.15905655512189562, 0.08438903825029868, 0.3217758070849986, -0.2232165228213287, -0.22707122969182414, 0.09775182332615023, -0.35450016651992444, -0.1417854950392481, 0.15704353800080112, 0.0032922547845238887... |
707.0458 | Number fluctuations in cold quantum gases | In ultracold gases many experiments use atom imaging as a basic observable.
The resulting image is averaged over a number of realizations and mostly only
this average is used. Only recently the noise has been measured to extract
physical information. In the present paper we investigate the quantum noise
arising in th... | cond-mat.stat-mech | in ultracold gases many experiments use atom imaging as a basic observable the resulting image is averaged over a number of realizations and mostly only this average is used only recently the noise has been measured to extract physical information in the present paper we investigate the quantum noise arising in these g... | [['in', 'ultracold', 'gases', 'many', 'experiments', 'use', 'atom', 'imaging', 'as', 'a', 'basic', 'observable', 'the', 'resulting', 'image', 'is', 'averaged', 'over', 'a', 'number', 'of', 'realizations', 'and', 'mostly', 'only', 'this', 'average', 'is', 'used', 'only', 'recently', 'the', 'noise', 'has', 'been', 'measu... | [-0.1307028551686675, 0.1642414970534848, -0.05222349048397887, 0.05333538306019972, 0.02450633932910631, -0.12871244321777228, 0.017591407046184813, 0.3295117634651394, -0.24302739150925007, -0.24105462173651332, 0.0967951435145802, -0.3127181252201825, -0.10204531371102817, 0.1548299381253738, 0.00014245581378920312,... |
707.0459 | Physical Network Coding in Two-Way Wireless Relay Channels | It has recently been recognized that the wireless networks represent a
fertile ground for devising communication modes based on network coding. A
particularly suitable application of the network coding arises for the two--way
relay channels, where two nodes communicate with each other assisted by using a
third, relay... | cs.IT cs.NI math.IT | it has recently been recognized that the wireless networks represent a fertile ground for devising communication modes based on network coding a particularly suitable application of the network coding arises for the twoway relay channels where two nodes communicate with each other assisted by using a third relay node s... | [['it', 'has', 'recently', 'been', 'recognized', 'that', 'the', 'wireless', 'networks', 'represent', 'a', 'fertile', 'ground', 'for', 'devising', 'communication', 'modes', 'based', 'on', 'network', 'coding', 'a', 'particularly', 'suitable', 'application', 'of', 'the', 'network', 'coding', 'arises', 'for', 'the', 'twowa... | [-0.26115800772783576, 0.014326231028403967, -0.03794572664980566, 0.007367511523664699, -0.034181153335701174, -0.3120659622714244, 0.1463708732795391, 0.3879833420117696, -0.2786138484095504, -0.20305812944688142, 0.10195602631754673, -0.19721922623644514, -0.16539622399698123, 0.19476847795854693, -0.055388510207174... |
707.046 | Gaussian potentials facilitate access to quantum Hall states in rotating
Bose gases | Through exact numerical diagonalization for small numbers of atoms, we show
that it is possible to access quantum Hall states in harmonically confined Bose
gases at rotation frequencies well below the centrifugal limit by applying a
repulsive Gaussian potential at the trap center. The main idea is to reduce or
elimin... | cond-mat.mes-hall | through exact numerical diagonalization for small numbers of atoms we show that it is possible to access quantum hall states in harmonically confined bose gases at rotation frequencies well below the centrifugal limit by applying a repulsive gaussian potential at the trap center the main idea is to reduce or eliminate ... | [['through', 'exact', 'numerical', 'diagonalization', 'for', 'small', 'numbers', 'of', 'atoms', 'we', 'show', 'that', 'it', 'is', 'possible', 'to', 'access', 'quantum', 'hall', 'states', 'in', 'harmonically', 'confined', 'bose', 'gases', 'at', 'rotation', 'frequencies', 'well', 'below', 'the', 'centrifugal', 'limit', '... | [-0.12144457024092284, 0.2746270230387521, -0.016011698184928928, 0.017856746346716627, -0.007270056416298478, -0.17601440801249388, 0.08238534730424782, 0.33895014382254046, -0.2656737855510213, -0.26832038062499264, 0.0498823601262232, -0.27024073984760505, -0.06337652289836954, 0.18023647963799214, 0.011688126685420... |
707.0461 | High charge-carrier mobility and low trap density in a rubrene
derivative | We have synthesized, crystallized and studied the structural and electric
transport properties of organic molecular crystals based on a rubrene
derivative with {\em t}-butyl sidegroups at the 5,11 positions. Two crystalline
modifications are observed: one (A) distinct from that of rubrene with larger
spacings between... | cond-mat.mtrl-sci | we have synthesized crystallized and studied the structural and electric transport properties of organic molecular crystals based on a rubrene derivative with em tbutyl sidegroups at the 511 positions two crystalline modifications are observed one a distinct from that of rubrene with larger spacings between the naphtac... | [['we', 'have', 'synthesized', 'crystallized', 'and', 'studied', 'the', 'structural', 'and', 'electric', 'transport', 'properties', 'of', 'organic', 'molecular', 'crystals', 'based', 'on', 'a', 'rubrene', 'derivative', 'with', 'em', 'tbutyl', 'sidegroups', 'at', 'the', '511', 'positions', 'two', 'crystalline', 'modific... | [-0.1514969285145947, 0.17958461903697576, -0.034511380115518256, -0.0037008569832811724, 0.020828307102819077, -0.12474024193304614, 0.05357646082936809, 0.43279541040793423, -0.21972940215931797, -0.357205177941246, 0.011183833461340017, -0.30779018743735986, -0.045604647655414825, 0.1683980269050907, 0.0149694024017... |
707.0462 | M-estimation of Boolean models for particle flow experiments | Probability models are proposed for passage time data collected in
experiments with a device designed to measure particle flow during aerial
application of fertilizer. Maximum likelihood estimation of flow intensity is
reviewed for the simple linear Boolean model, which arises with the assumption
that each particle r... | stat.AP | probability models are proposed for passage time data collected in experiments with a device designed to measure particle flow during aerial application of fertilizer maximum likelihood estimation of flow intensity is reviewed for the simple linear boolean model which arises with the assumption that each particle requi... | [['probability', 'models', 'are', 'proposed', 'for', 'passage', 'time', 'data', 'collected', 'in', 'experiments', 'with', 'a', 'device', 'designed', 'to', 'measure', 'particle', 'flow', 'during', 'aerial', 'application', 'of', 'fertilizer', 'maximum', 'likelihood', 'estimation', 'of', 'flow', 'intensity', 'is', 'review... | [-0.05656698404578492, 0.11672697955407785, -0.1048119998909533, 0.04291977320564911, -0.015893158204853534, -0.13793936606962234, 0.005486436933279037, 0.372245386056602, -0.2532313649170101, -0.32572288560681045, 0.1016611284215469, -0.2736656721588224, -0.10198618484660983, 0.20104596886900253, -0.06755615940317511,... |
707.0463 | Blind Estimation of Multiple Carrier Frequency Offsets | Multiple carrier-frequency offsets (CFO) arise in a distributed antenna
system, where data are transmitted simultaneously from multiple antennas. In
such systems the received signal contains multiple CFOs due to mismatch between
the local oscillators of transmitters and receiver. This results in a
time-varying rotati... | cs.IT math.IT | multiple carrierfrequency offsets cfo arise in a distributed antenna system where data are transmitted simultaneously from multiple antennas in such systems the received signal contains multiple cfos due to mismatch between the local oscillators of transmitters and receiver this results in a timevarying rotation of the... | [['multiple', 'carrierfrequency', 'offsets', 'cfo', 'arise', 'in', 'a', 'distributed', 'antenna', 'system', 'where', 'data', 'are', 'transmitted', 'simultaneously', 'from', 'multiple', 'antennas', 'in', 'such', 'systems', 'the', 'received', 'signal', 'contains', 'multiple', 'cfos', 'due', 'to', 'mismatch', 'between', '... | [-0.22482730255578645, 0.03674912031829081, -0.047442408907227215, -0.004937841953142197, -0.053651805108529516, -0.22311692784132903, 0.05833350258253631, 0.35811164149199615, -0.2928430967498571, -0.29479896414559337, 0.16313315922379842, -0.24419584242859854, -0.20075955748216073, 0.1766761518883868, -0.137815394479... |
707.0464 | Far Infrared Prperties of M Dwarfs | We report the mid- and far-infrared properties of nearby M dwarfs.
Spitzer/MIPS measurements were obtained for a sample of 62 stars at 24 um, with
subsamples of 41 and 20 stars observed at 70 um and 160 um respectively. We
compare the results with current models of M star photospheres and look for
indications of circ... | astro-ph | we report the mid and farinfrared properties of nearby m dwarfs spitzermips measurements were obtained for a sample of 62 stars at 24 um with subsamples of 41 and 20 stars observed at 70 um and 160 um respectively we compare the results with current models of m star photospheres and look for indications of circumstella... | [['we', 'report', 'the', 'mid', 'and', 'farinfrared', 'properties', 'of', 'nearby', 'm', 'dwarfs', 'spitzermips', 'measurements', 'were', 'obtained', 'for', 'a', 'sample', 'of', '62', 'stars', 'at', '24', 'um', 'with', 'subsamples', 'of', '41', 'and', '20', 'stars', 'observed', 'at', '70', 'um', 'and', '160', 'um', 're... | [-0.010166356573497294, 0.11058789557437339, -0.0153075929671999, 0.06581874880397683, -0.025725024627896134, -0.040916773461041944, 0.10500157208775697, 0.456577264639751, -0.06291416441272112, -0.4366833958799443, 0.04579732230945771, -0.3904938554729578, 0.03950156193739666, 0.17045726530037072, -0.03257260807431376... |
707.0465 | The game chromatic number of random graphs | Given a graph G and an integer k, two players take turns coloring the
vertices of G one by one using k colors so that neighboring vertices get
different colors. The first player wins iff at the end of the game all the
vertices of G are colored. The game chromatic number \chi_g(G) is the minimum k
for which the first ... | math.CO | given a graph g and an integer k two players take turns coloring the vertices of g one by one using k colors so that neighboring vertices get different colors the first player wins iff at the end of the game all the vertices of g are colored the game chromatic number chi_gg is the minimum k for which the first player h... | [['given', 'a', 'graph', 'g', 'and', 'an', 'integer', 'k', 'two', 'players', 'take', 'turns', 'coloring', 'the', 'vertices', 'of', 'g', 'one', 'by', 'one', 'using', 'k', 'colors', 'so', 'that', 'neighboring', 'vertices', 'get', 'different', 'colors', 'the', 'first', 'player', 'wins', 'iff', 'at', 'the', 'end', 'of', 't... | [-0.18985031738749616, 0.15634904310378084, -0.11443578373760946, 0.006521087087270233, -0.10479811164775803, -0.1837578196746988, 0.10821600090956406, 0.3811604711133236, -0.25067590426413283, -0.36160519094987503, 0.03693717466423198, -0.34121856660274186, -0.15210043724566216, -0.0038355038230938297, -0.114540553869... |
707.0466 | Lattice-Induced Double-Valley Degeneracy Lifting in Magnetic Field in
Graphene | We show that the recently discovered double-valley splitting of the low-lying
Landau level(s) in the Quantum Hall Effect in graphene can be explained as
perturbative orbital interaction of intra- and inter-valley microscopic orbital
currents with a magnetic field. This effect is provided by the
translational-non-inva... | cond-mat.mes-hall | we show that the recently discovered doublevalley splitting of the lowlying landau levels in the quantum hall effect in graphene can be explained as perturbative orbital interaction of intra and intervalley microscopic orbital currents with a magnetic field this effect is provided by the translationalnoninvariant terms... | [['we', 'show', 'that', 'the', 'recently', 'discovered', 'doublevalley', 'splitting', 'of', 'the', 'lowlying', 'landau', 'levels', 'in', 'the', 'quantum', 'hall', 'effect', 'in', 'graphene', 'can', 'be', 'explained', 'as', 'perturbative', 'orbital', 'interaction', 'of', 'intra', 'and', 'intervalley', 'microscopic', 'or... | [-0.20174433077685536, 0.24678447512133667, -0.05685087228814761, 0.07072053437431654, -0.05045354457572102, -0.11971309047813217, 0.03467175429221243, 0.3762998160471519, -0.24143190664549669, -0.29944561706855893, -0.06199309000279754, -0.26941498203823966, -0.17703812916452685, 0.13655273617710917, 0.010780966468155... |
707.0467 | Star Formation Rate Determinations | I review determinations of star formation rates (SFR) from the ultraviolet to
the infrared, in the context of their use for galaxies and galaxy surveys. The
mid-infrared SFR indicators have garnered interest in recent years thanks to
the Spitzer capabilities and the opportunities offered by the upcoming Herschel
Spac... | astro-ph | i review determinations of star formation rates sfr from the ultraviolet to the infrared in the context of their use for galaxies and galaxy surveys the midinfrared sfr indicators have garnered interest in recent years thanks to the spitzer capabilities and the opportunities offered by the upcoming herschel space teles... | [['i', 'review', 'determinations', 'of', 'star', 'formation', 'rates', 'sfr', 'from', 'the', 'ultraviolet', 'to', 'the', 'infrared', 'in', 'the', 'context', 'of', 'their', 'use', 'for', 'galaxies', 'and', 'galaxy', 'surveys', 'the', 'midinfrared', 'sfr', 'indicators', 'have', 'garnered', 'interest', 'in', 'recent', 'ye... | [0.03437359300507626, 0.049896989398124356, -0.08968924927774449, 0.05065027827029707, -0.14107020865653602, -0.005666561831366009, 0.062463236959572406, 0.5043237480059476, -0.1600437840630471, -0.2984789317526238, 0.09719583285401877, -0.3256152139871683, -0.09287658118328053, 0.23357052674425216, -0.0858349092239120... |
707.0468 | A Spitzer Study of the Mass Loss Histories of Three Bipolar
Pre-Planetary Nebulae | We present the results of far-infrared imaging of extended regions around
three bipolar pre-planetary nebulae, AFGL 2688, OH 231.8+4.2, and IRAS
16342$-$3814, at 70 and 160 $\mu$m with the MIPS instrument on the Spitzer
Space Telescope. After a careful subtraction of the point spread function of
the central star from... | astro-ph | we present the results of farinfrared imaging of extended regions around three bipolar preplanetary nebulae afgl 2688 oh 231842 and iras 163423814 at 70 and 160 mum with the mips instrument on the spitzer space telescope after a careful subtraction of the point spread function of the central star from these images we p... | [['we', 'present', 'the', 'results', 'of', 'farinfrared', 'imaging', 'of', 'extended', 'regions', 'around', 'three', 'bipolar', 'preplanetary', 'nebulae', 'afgl', '2688', 'oh', '231842', 'and', 'iras', '163423814', 'at', '70', 'and', '160', 'mum', 'with', 'the', 'mips', 'instrument', 'on', 'the', 'spitzer', 'space', 't... | [-0.06195297021102825, 0.07091296309306085, -0.02037456252162351, 0.06958226239994536, -0.03758225087900044, -0.05639996678967561, 0.04804839647919903, 0.45865388544035607, -0.15161847345274398, -0.32967415254849775, 0.1005948139200158, -0.26856016121221843, 0.04254591110840338, 0.17580261105294562, -0.0308654332417855... |
707.0469 | WMAP 3yr data with the CCA: anomalous emission and impact of component
separation on the CMB power spectrum | The Correlated Component Analysis (CCA) allows us to estimate how the
different diffuse emissions mix in CMB experiments, exploiting also
complementary information from other surveys. It is especially useful to deal
with possible additional components. An application of CCA to WMAP maps
assuming that only the canonic... | astro-ph | the correlated component analysis cca allows us to estimate how the different diffuse emissions mix in cmb experiments exploiting also complementary information from other surveys it is especially useful to deal with possible additional components an application of cca to wmap maps assuming that only the canonical gala... | [['the', 'correlated', 'component', 'analysis', 'cca', 'allows', 'us', 'to', 'estimate', 'how', 'the', 'different', 'diffuse', 'emissions', 'mix', 'in', 'cmb', 'experiments', 'exploiting', 'also', 'complementary', 'information', 'from', 'other', 'surveys', 'it', 'is', 'especially', 'useful', 'to', 'deal', 'with', 'poss... | [-0.05161397894257753, 0.0938466268090401, -0.09503911614718694, 0.13123316457036766, -0.08109565471082662, -0.1200574567517647, -0.015015775573166733, 0.404075180627699, -0.24414163045117662, -0.3080719238445969, 0.06184458721055114, -0.35495468682347564, -0.0602002847276529, 0.2111771152754439, 0.011286346793658739, ... |
707.047 | Search for Extra Dimensions with Atlas and CMS Detectors at the LHC | A brief review of the discovery potential of the ATLAS and CMS experiments to
search for signals from extra dimensions in different luminosity scenarios is
given.
| hep-ex | a brief review of the discovery potential of the atlas and cms experiments to search for signals from extra dimensions in different luminosity scenarios is given | [['a', 'brief', 'review', 'of', 'the', 'discovery', 'potential', 'of', 'the', 'atlas', 'and', 'cms', 'experiments', 'to', 'search', 'for', 'signals', 'from', 'extra', 'dimensions', 'in', 'different', 'luminosity', 'scenarios', 'is', 'given']] | [-0.07705349607679707, 0.1149900139381106, -0.04489269974426581, 0.053294054684766494, -0.10521630742228948, -0.14281030491782495, 0.011506380656590829, 0.31578961931742155, -0.16310361586511135, -0.3869063786875743, 0.13658032316911536, -0.36147398272385967, -0.08856401621149136, 0.19539111332358935, -0.01224023744893... |
707.0471 | Method to extract the primary cosmic ray spectrum from very high energy
gamma-ray data and its application to SNR RX J1713.7-3946 | Supernova remnants are likely to be the accelerators of the galactic cosmic
rays. Assuming the correctness of this hypothesis, we develop a method to
extract the parent cosmic ray spectrum from the VHE gamma ray flux emitted by
supernova remnants (and other gamma transparent sources). Namely, we calculate
semi-analyt... | astro-ph | supernova remnants are likely to be the accelerators of the galactic cosmic rays assuming the correctness of this hypothesis we develop a method to extract the parent cosmic ray spectrum from the vhe gamma ray flux emitted by supernova remnants and other gamma transparent sources namely we calculate semianalytically th... | [['supernova', 'remnants', 'are', 'likely', 'to', 'be', 'the', 'accelerators', 'of', 'the', 'galactic', 'cosmic', 'rays', 'assuming', 'the', 'correctness', 'of', 'this', 'hypothesis', 'we', 'develop', 'a', 'method', 'to', 'extract', 'the', 'parent', 'cosmic', 'ray', 'spectrum', 'from', 'the', 'vhe', 'gamma', 'ray', 'fl... | [-0.04328675245866921, 0.14243202763746765, -0.07654379310596521, 0.15889318689617185, -0.12105150587239842, -0.032343696538880945, 0.01790438544384803, 0.4161487325290396, -0.28970612246679606, -0.34696526298667213, 0.01786781516323566, -0.3117267953492938, -0.00791099718119356, 0.24760898089208372, 0.0110050765208004... |
707.0472 | Dark Matter | The nature of the main constituents of the mass of the universe is one of the
outstanding riddles of cosmology and astro-particle physics. Current models
explaining the evolution of the universe, and measurements of the various
components of its mass, all have in common that an appreciable contribution to
that mass i... | astro-ph hep-ex | the nature of the main constituents of the mass of the universe is one of the outstanding riddles of cosmology and astroparticle physics current models explaining the evolution of the universe and measurements of the various components of its mass all have in common that an appreciable contribution to that mass is nonl... | [['the', 'nature', 'of', 'the', 'main', 'constituents', 'of', 'the', 'mass', 'of', 'the', 'universe', 'is', 'one', 'of', 'the', 'outstanding', 'riddles', 'of', 'cosmology', 'and', 'astroparticle', 'physics', 'current', 'models', 'explaining', 'the', 'evolution', 'of', 'the', 'universe', 'and', 'measurements', 'of', 'th... | [-0.11841277288990694, 0.1875760962711615, -0.1345773945442922, 0.09781179453754678, -0.09660138875468198, -0.04212135374289724, -0.039849011517992805, 0.22951226891232057, -0.1860996133331722, -0.38442314442230063, 0.09099473820149112, -0.28384814083943605, -0.028069534744862297, 0.15054368394333015, 0.015032344566628... |
707.0473 | Entanglement generation resonances in XY chains | We examine the maximum entanglement reached by an initially fully aligned
state evolving in an XY Heisenberg spin chain placed in a uniform transverse
magnetic field. Both the global entanglement between one qubit and the rest of
the chain and the pairwise entanglement between adjacent qubits is analyzed. It
is shown... | quant-ph | we examine the maximum entanglement reached by an initially fully aligned state evolving in an xy heisenberg spin chain placed in a uniform transverse magnetic field both the global entanglement between one qubit and the rest of the chain and the pairwise entanglement between adjacent qubits is analyzed it is shown tha... | [['we', 'examine', 'the', 'maximum', 'entanglement', 'reached', 'by', 'an', 'initially', 'fully', 'aligned', 'state', 'evolving', 'in', 'an', 'xy', 'heisenberg', 'spin', 'chain', 'placed', 'in', 'a', 'uniform', 'transverse', 'magnetic', 'field', 'both', 'the', 'global', 'entanglement', 'between', 'one', 'qubit', 'and',... | [-0.18200104575578488, 0.2254989886697649, -0.017730499349214546, 0.08455663760466947, 0.004794659054455307, -0.1779386560101222, 0.0007612593000629014, 0.4013343775884871, -0.2612994557355125, -0.25653147751299743, 0.06971523008006482, -0.2906083896773313, -0.05753279608771479, 0.17209604707049445, 0.03488418576736117... |
707.0474 | Parsec-Scale Jet-Environment Interactions in AGN | Observations made with the VLBA have led to fundamental advances in our
understanding of how radio jets in AGN evolve from parsec-scales out to
distances exceeding several hundred kiloparsecs. In this review I discuss
current models of young radio source evolution, as well as the observational
evidence for a rapid ch... | astro-ph | observations made with the vlba have led to fundamental advances in our understanding of how radio jets in agn evolve from parsecscales out to distances exceeding several hundred kiloparsecs in this review i discuss current models of young radio source evolution as well as the observational evidence for a rapid change ... | [['observations', 'made', 'with', 'the', 'vlba', 'have', 'led', 'to', 'fundamental', 'advances', 'in', 'our', 'understanding', 'of', 'how', 'radio', 'jets', 'in', 'agn', 'evolve', 'from', 'parsecscales', 'out', 'to', 'distances', 'exceeding', 'several', 'hundred', 'kiloparsecs', 'in', 'this', 'review', 'i', 'discuss', ... | [-0.10683066760455924, 0.14284027036371993, -0.06110727677471728, 0.12899940732435572, -0.09222710881706166, -0.08432321430484747, 0.02090956190722468, 0.4517524543432345, -0.19812879016657609, -0.306258065897902, 0.0648254356484409, -0.2430153600379871, -0.01484861307754326, 0.19648549043405686, 0.008538332143046471, ... |
707.0475 | Nonlocal Interferometry: Beyond Bell's Inequality | This paper presents a tutorial review of nonlocal interferometry. The role of
the Feynman propagator in optical coherence is also discussed, including the
possibility of generating optical coherence and entanglement outside of the
light cone.
| quant-ph | this paper presents a tutorial review of nonlocal interferometry the role of the feynman propagator in optical coherence is also discussed including the possibility of generating optical coherence and entanglement outside of the light cone | [['this', 'paper', 'presents', 'a', 'tutorial', 'review', 'of', 'nonlocal', 'interferometry', 'the', 'role', 'of', 'the', 'feynman', 'propagator', 'in', 'optical', 'coherence', 'is', 'also', 'discussed', 'including', 'the', 'possibility', 'of', 'generating', 'optical', 'coherence', 'and', 'entanglement', 'outside', 'of... | [-0.16628780174734337, 0.17433866622325564, -0.12119992833052362, 0.05383524099098785, -0.06232547775975295, -0.09851208444950836, 0.024971323277402136, 0.39211456584078924, -0.23668571806379726, -0.2200630813038775, 0.08539750502511327, -0.2641909719311765, -0.18755129958902086, 0.20029648137944087, -0.041238015943339... |
707.0476 | Fractional Power Control for Decentralized Wireless Networks | We consider a new approach to power control in decentralized wireless
networks, termed fractional power control (FPC). Transmission power is chosen
as the current channel quality raised to an exponent -s, where s is a constant
between 0 and 1. The choices s = 1 and s = 0 correspond to the familiar cases
of channel in... | cs.IT math.IT | we consider a new approach to power control in decentralized wireless networks termed fractional power control fpc transmission power is chosen as the current channel quality raised to an exponent s where s is a constant between 0 and 1 the choices s 1 and s 0 correspond to the familiar cases of channel inversion and c... | [['we', 'consider', 'a', 'new', 'approach', 'to', 'power', 'control', 'in', 'decentralized', 'wireless', 'networks', 'termed', 'fractional', 'power', 'control', 'fpc', 'transmission', 'power', 'is', 'chosen', 'as', 'the', 'current', 'channel', 'quality', 'raised', 'to', 'an', 'exponent', 's', 'where', 's', 'is', 'a', '... | [-0.19031334897949242, 0.06761948704654504, -0.01906904094183529, 0.04749267078288984, -0.05840009944721129, -0.22112800998333404, 0.1137920261662401, 0.4037754433972875, -0.2678439389278089, -0.29274909847149266, 0.07997827736459708, -0.2539515504581409, -0.1420917878246608, 0.15311412565779606, -0.09792018621862635, ... |
707.0477 | Alternative Approach to 3D Displaying | A method for displaying volumetric images, which exploits our binocular
vision and does not require eyewear, is discussed. The display can be rendered
as a matrix of pivoting micromirrors irradiated by a light beam; each
micromirror focuses its pixel beams to the same point of displayed volumetric
image. 3D perceptio... | physics.optics physics.ins-det | a method for displaying volumetric images which exploits our binocular vision and does not require eyewear is discussed the display can be rendered as a matrix of pivoting micromirrors irradiated by a light beam each micromirror focuses its pixel beams to the same point of displayed volumetric image 3d perception of im... | [['a', 'method', 'for', 'displaying', 'volumetric', 'images', 'which', 'exploits', 'our', 'binocular', 'vision', 'and', 'does', 'not', 'require', 'eyewear', 'is', 'discussed', 'the', 'display', 'can', 'be', 'rendered', 'as', 'a', 'matrix', 'of', 'pivoting', 'micromirrors', 'irradiated', 'by', 'a', 'light', 'beam', 'eac... | [-0.07363464168443436, 0.07219199731316366, -0.14526892528200233, -0.018017447610962873, -0.052180910915870904, -0.19868793713033828, -0.0190586950236433, 0.4798618698309005, -0.261214513122596, -0.3243800393292602, 0.0973134916784032, -0.25683283351991376, -0.13244085488709764, 0.23387398631115194, -0.1822438803060770... |
707.0478 | Particle-Hole Symmetry and the $\nu={5/2}$ Quantum Hall State | We discuss the implications of approximate particle-hole symmetry in a
half-filled Landau level in which a paired quantum Hall state forms. We note
that the Pfaffian state is not particle-hole symmetric. Therefore, in the limit
of vanishing Landau level mixing, in which particle-hole transformation is an
exact symmet... | cond-mat.mes-hall | we discuss the implications of approximate particlehole symmetry in a halffilled landau level in which a paired quantum hall state forms we note that the pfaffian state is not particlehole symmetric therefore in the limit of vanishing landau level mixing in which particlehole transformation is an exact symmetry the pfa... | [['we', 'discuss', 'the', 'implications', 'of', 'approximate', 'particlehole', 'symmetry', 'in', 'a', 'halffilled', 'landau', 'level', 'in', 'which', 'a', 'paired', 'quantum', 'hall', 'state', 'forms', 'we', 'note', 'that', 'the', 'pfaffian', 'state', 'is', 'not', 'particlehole', 'symmetric', 'therefore', 'in', 'the', ... | [-0.18142872412988384, 0.22043868947928005, -0.08624273597794985, 0.1301560284079252, -0.04005617813340255, -0.1359774680142956, 0.08937347281690954, 0.3261440561552133, -0.2403141876682639, -0.22474694295919367, 0.05749400625604072, -0.22950033200239497, -0.16731660478648597, 0.06727676603643756, 0.015603956982626446,... |
707.0479 | Precoding for the AWGN Channel with Discrete Interference | For a state-dependent DMC with input alphabet $\mathcal{X}$ and state
alphabet $\mathcal{S}$ where the i.i.d. state sequence is known causally at the
transmitter, it is shown that by using at most
$|\mathcal{X}||\mathcal{S}|-|\mathcal{S}|+1$ out of
$|\mathcal{X}|^{|\mathcal{S}|}$ input symbols of the Shannon's
\emph{... | cs.IT math.IT | for a statedependent dmc with input alphabet mathcalx and state alphabet mathcals where the iid state sequence is known causally at the transmitter it is shown that by using at most mathcalxmathcalsmathcals1 out of mathcalxmathcals input symbols of the shannons emphassociated channel the capacity is achievable as an ex... | [['for', 'a', 'statedependent', 'dmc', 'with', 'input', 'alphabet', 'mathcalx', 'and', 'state', 'alphabet', 'mathcals', 'where', 'the', 'iid', 'state', 'sequence', 'is', 'known', 'causally', 'at', 'the', 'transmitter', 'it', 'is', 'shown', 'that', 'by', 'using', 'at', 'most', 'mathcalxmathcalsmathcals1', 'out', 'of', '... | [-0.24748809603735497, 0.10477473912843506, -0.02468152373109626, 0.014860869833648416, -0.041701420192618535, -0.2860367755564755, 0.10500760318245739, 0.35088779081154287, -0.3300287021844223, -0.20299266656872497, 0.12855547278731932, -0.2737857712376745, -0.1202719119359751, 0.12798034386632703, -0.1185873361669858... |
707.048 | Entropic Effects in the Very Low Temperature Regime of Diluted Ising
Spin Glasses with Discrete Couplings | We study link-diluted $\pm J$ Ising spin glass models on the hierarchical
lattice and on a three-dimensional lattice close to the percolation threshold.
We show that previously computed zero temperature fixed points are unstable
with respect to temperature perturbations and do not belong to any critical
line in the d... | cond-mat.dis-nn cond-mat.stat-mech | we study linkdiluted pm j ising spin glass models on the hierarchical lattice and on a threedimensional lattice close to the percolation threshold we show that previously computed zero temperature fixed points are unstable with respect to temperature perturbations and do not belong to any critical line in the dilutiont... | [['we', 'study', 'linkdiluted', 'pm', 'j', 'ising', 'spin', 'glass', 'models', 'on', 'the', 'hierarchical', 'lattice', 'and', 'on', 'a', 'threedimensional', 'lattice', 'close', 'to', 'the', 'percolation', 'threshold', 'we', 'show', 'that', 'previously', 'computed', 'zero', 'temperature', 'fixed', 'points', 'are', 'unst... | [-0.13085883105409213, 0.14347053083708916, -0.07819703421501935, 0.06084047189389152, -0.060207905381618215, -0.1441238389949946, 0.08990994153608536, 0.3941713251259135, -0.21968191959520525, -0.2348572876840969, 0.1149556223857056, -0.29296462881196844, -0.14223509960561648, 0.15056448017284488, -0.01919614118470371... |
707.0481 | Treelets--An adaptive multi-scale basis for sparse unordered data | In many modern applications, including analysis of gene expression and text
documents, the data are noisy, high-dimensional, and unordered--with no
particular meaning to the given order of the variables. Yet, successful
learning is often possible due to sparsity: the fact that the data are
typically redundant with un... | stat.ME | in many modern applications including analysis of gene expression and text documents the data are noisy highdimensional and unorderedwith no particular meaning to the given order of the variables yet successful learning is often possible due to sparsity the fact that the data are typically redundant with underlying str... | [['in', 'many', 'modern', 'applications', 'including', 'analysis', 'of', 'gene', 'expression', 'and', 'text', 'documents', 'the', 'data', 'are', 'noisy', 'highdimensional', 'and', 'unorderedwith', 'no', 'particular', 'meaning', 'to', 'the', 'given', 'order', 'of', 'the', 'variables', 'yet', 'successful', 'learning', 'i... | [-0.06255723688883161, 0.04208112796752377, -0.07549724747624362, 0.10204550157879677, -0.1373726319947346, -0.1380122583665217, 0.0331610013287505, 0.4249533052283405, -0.3040373496560737, -0.3032408995918972, 0.16234076006933013, -0.263703251295168, -0.1974062675979421, 0.1948295525784341, -0.08867625896395608, 0.065... |
707.0482 | Comparison of two formulas for metric connections in the bundle of Dirac
spinors | Two explicit formulas for metric connections in the bundle of Dirac spinors
are studied. Their equivalence is proved. The explicit formula relating the
spinor curvature tensor with the Riemann curvature tensor is rederived.
| math.DG gr-qc hep-ph hep-th math-ph math.MP | two explicit formulas for metric connections in the bundle of dirac spinors are studied their equivalence is proved the explicit formula relating the spinor curvature tensor with the riemann curvature tensor is rederived | [['two', 'explicit', 'formulas', 'for', 'metric', 'connections', 'in', 'the', 'bundle', 'of', 'dirac', 'spinors', 'are', 'studied', 'their', 'equivalence', 'is', 'proved', 'the', 'explicit', 'formula', 'relating', 'the', 'spinor', 'curvature', 'tensor', 'with', 'the', 'riemann', 'curvature', 'tensor', 'is', 'rederived'... | [-0.26828651090688777, 0.13681017716810334, -0.07092188614787477, 0.15740301361956605, -0.19749179115575372, -0.18662792692581812, -0.12353097344219516, 0.34766711339806067, -0.18587594998605322, -0.20141194557601755, 0.05434487864135228, -0.25598036782872496, -0.23010436761559863, 0.12616570993806375, 0.00288728677013... |
707.0483 | Particle-hole symmetry and the Pfaffian state | We consider the properties of the Moore-Read Pfaffian state under
particle-hole conjugation. We show that the particle-hole conjugate of the
Pfaffian state - or "anti-Pfaffian" state - is in a different universality
class from the Pfaffian state, with different topological order. The two states
can be distinguished b... | cond-mat.mes-hall cond-mat.str-el | we consider the properties of the mooreread pfaffian state under particlehole conjugation we show that the particlehole conjugate of the pfaffian state or antipfaffian state is in a different universality class from the pfaffian state with different topological order the two states can be distinguished by both their bu... | [['we', 'consider', 'the', 'properties', 'of', 'the', 'mooreread', 'pfaffian', 'state', 'under', 'particlehole', 'conjugation', 'we', 'show', 'that', 'the', 'particlehole', 'conjugate', 'of', 'the', 'pfaffian', 'state', 'or', 'antipfaffian', 'state', 'is', 'in', 'a', 'different', 'universality', 'class', 'from', 'the',... | [-0.17704647139225926, 0.2417241400835337, -0.0954838092193313, 0.06997963937647, -0.0032502445901627652, -0.18402217149559874, 0.05795724803556368, 0.28788601491851296, -0.25726668095467176, -0.2887638015090488, 0.03838110888227675, -0.29104669878142886, -0.10162897489863099, 0.12723115770313598, 0.05629049421804666, ... |
707.0484 | $\mu$--PhotoZ: Photometric Redshifts by Inverting the Tolman Surface
Brightness Test | Surface brightness is a fundamental observational parameter of galaxies. We
show, for the first time in detail, how it can be used to obtain photometric
redshifts for galaxies, the $\mu$-PhotoZ method.
We demonstrate that the Tolman surface brightness relation, $\mu \propto
(1+z)^{-4}$, is a powerful tool for deter... | astro-ph | surface brightness is a fundamental observational parameter of galaxies we show for the first time in detail how it can be used to obtain photometric redshifts for galaxies the muphotoz method we demonstrate that the tolman surface brightness relation mu propto 1z4 is a powerful tool for determining galaxy redshifts fr... | [['surface', 'brightness', 'is', 'a', 'fundamental', 'observational', 'parameter', 'of', 'galaxies', 'we', 'show', 'for', 'the', 'first', 'time', 'in', 'detail', 'how', 'it', 'can', 'be', 'used', 'to', 'obtain', 'photometric', 'redshifts', 'for', 'galaxies', 'the', 'muphotoz', 'method', 'we', 'demonstrate', 'that', 'th... | [-0.004832770468922155, 0.023448411671173137, -0.14744585484177583, 0.13308354832753094, -0.10010815115224216, -0.08011621488202807, 0.07679715372034393, 0.4667564251327089, -0.14753243038319938, -0.3160509734935615, 0.036996312048618814, -0.2807051268589151, -0.09475918443924802, 0.2485754701095478, -0.070198106135995... |
707.0485 | Linking the X-ray timing and spectral properties of the glitching AXP
1RXS J170849-400910 | Previous studies of the X-ray flux and spectral properties of 1RXS
J170849-400910 showed hints of a possible correlation with the spin glitches
that occurred in 1999 and 2001. However, due to the sparseness of spectral
measurements and the paucity of detected glitches no firm conclusion could be
drawn. We retrieved a... | astro-ph | previous studies of the xray flux and spectral properties of 1rxs j170849400910 showed hints of a possible correlation with the spin glitches that occurred in 1999 and 2001 however due to the sparseness of spectral measurements and the paucity of detected glitches no firm conclusion could be drawn we retrieved and anal... | [['previous', 'studies', 'of', 'the', 'xray', 'flux', 'and', 'spectral', 'properties', 'of', '1rxs', 'j170849400910', 'showed', 'hints', 'of', 'a', 'possible', 'correlation', 'with', 'the', 'spin', 'glitches', 'that', 'occurred', 'in', '1999', 'and', '2001', 'however', 'due', 'to', 'the', 'sparseness', 'of', 'spectral'... | [-0.12995924397125944, 0.09607308568536407, -0.09199585722138484, 0.07144945623887772, -0.0772401115719091, -0.08266511704703725, 0.13196202808370192, 0.40721241143290643, -0.12871653419764092, -0.4067027792196583, 0.1359991476819333, -0.324921729957202, -0.08831177923345455, 0.2247552103742405, -0.057105981775869924, ... |
707.0486 | Blazar Demographics with MOJAVE and GLAST | MOJAVE is a long term VLBA program to investigate the kinematics and
polarization evolution of a complete sample of 133 active galactic nuclei
selected on the basis of compact, relativistically beamed jet emission at 15
GHz. By fitting to the apparent distributions of superluminal speed and jet
luminosity, we can con... | astro-ph | mojave is a long term vlba program to investigate the kinematics and polarization evolution of a complete sample of 133 active galactic nuclei selected on the basis of compact relativistically beamed jet emission at 15 ghz by fitting to the apparent distributions of superluminal speed and jet luminosity we can constrai... | [['mojave', 'is', 'a', 'long', 'term', 'vlba', 'program', 'to', 'investigate', 'the', 'kinematics', 'and', 'polarization', 'evolution', 'of', 'a', 'complete', 'sample', 'of', '133', 'active', 'galactic', 'nuclei', 'selected', 'on', 'the', 'basis', 'of', 'compact', 'relativistically', 'beamed', 'jet', 'emission', 'at', ... | [-0.08554101303422776, 0.14401085368584832, -0.0656204611236134, 0.17446363024795666, -0.16022125657540387, -0.06666519837334561, 0.04827923561918933, 0.4864471605620705, -0.16494565760382476, -0.36117077674731635, 0.01884598518163563, -0.3000214549127775, 0.04253904999066622, 0.2149510451962646, 0.0028364574312805557,... |
707.0487 | $z$-Classes of Isometries of The Hyperbolic Space | Let $G$ be a group. Two elements $x, y$ are said to be {\it $z$-equivalent}
if their centralizers are conjugate in $G$. The class equation of $G$ is the
partition of $G$ into conjugacy classes. Further decomposition of conjugacy
classes into $z$-classes provides an important information about the internal
structure o... | math.GT math.GR | let g be a group two elements x y are said to be it zequivalent if their centralizers are conjugate in g the class equation of g is the partition of g into conjugacy classes further decomposition of conjugacy classes into zclasses provides an important information about the internal structure of the group let ihn denot... | [['let', 'g', 'be', 'a', 'group', 'two', 'elements', 'x', 'y', 'are', 'said', 'to', 'be', 'it', 'zequivalent', 'if', 'their', 'centralizers', 'are', 'conjugate', 'in', 'g', 'the', 'class', 'equation', 'of', 'g', 'is', 'the', 'partition', 'of', 'g', 'into', 'conjugacy', 'classes', 'further', 'decomposition', 'of', 'conj... | [-0.18708381532476498, 0.13170814313489246, -0.10504556646427284, 0.03845425259250288, -0.11356011000103676, -0.07392401030519977, 0.0021187040865278013, 0.3435414130871113, -0.3459631498222454, -0.2720253400146388, 0.060325043765792195, -0.27029875504712647, -0.09720090213231743, 0.20204734613295072, -0.11093381525088... |
707.0488 | Theoretical Interpretation of Experimental Data from Direct Dark Matter
Detection | Weakly Interacting Massive Particles (WIMPs) are one of the leading
candidates for Dark Matter. Currently, the most promising method to detect
WIMPs is the direct detection of the recoil energy deposited in a
low-background laboratory detector due to elastic WIMP-nucleus scattering. So
far the usual procedure has bee... | astro-ph hep-ph | weakly interacting massive particles wimps are one of the leading candidates for dark matter currently the most promising method to detect wimps is the direct detection of the recoil energy deposited in a lowbackground laboratory detector due to elastic wimpnucleus scattering so far the usual procedure has been to pred... | [['weakly', 'interacting', 'massive', 'particles', 'wimps', 'are', 'one', 'of', 'the', 'leading', 'candidates', 'for', 'dark', 'matter', 'currently', 'the', 'most', 'promising', 'method', 'to', 'detect', 'wimps', 'is', 'the', 'direct', 'detection', 'of', 'the', 'recoil', 'energy', 'deposited', 'in', 'a', 'lowbackground... | [-0.05234948340989831, 0.14784727880325477, -0.12474562446004711, 0.09355294456648977, -0.09258163914455508, -0.077917068176248, 0.007764470042275207, 0.3414174309655209, -0.21250878913497218, -0.35880552815797273, 0.0615112566638345, -0.30031241118467733, -0.06165100541988977, 0.2074964133012145, 0.027111119254186633,... |
707.0489 | An Unbiased Survey of 500 Nearby Stars for Debris Disks: A JCMT Legacy
Program | We present the scientific motivation and observing plan for an upcoming
detection survey for debris disks using the James Clerk Maxwell Telescope. The
SCUBA-2 Unbiased Nearby Stars (SUNS) Survey will observe 500 nearby main
sequence and sub-giant stars (100 of each of the A, F, G, K and M spectral
classes) to the 850... | astro-ph | we present the scientific motivation and observing plan for an upcoming detection survey for debris disks using the james clerk maxwell telescope the scuba2 unbiased nearby stars suns survey will observe 500 nearby main sequence and subgiant stars 100 of each of the a f g k and m spectral classes to the 850 micron extr... | [['we', 'present', 'the', 'scientific', 'motivation', 'and', 'observing', 'plan', 'for', 'an', 'upcoming', 'detection', 'survey', 'for', 'debris', 'disks', 'using', 'the', 'james', 'clerk', 'maxwell', 'telescope', 'the', 'scuba2', 'unbiased', 'nearby', 'stars', 'suns', 'survey', 'will', 'observe', '500', 'nearby', 'mai... | [-0.10679488221868515, 0.11776256753052751, -0.030362996633075887, 0.0782750645039847, -0.1412528293486315, -0.025364793796879462, 0.0629010508358959, 0.38776207801383283, -0.17655941307182527, -0.40451725745122763, 0.1223829427067863, -0.29756693553090807, 0.005965682141120649, 0.20054385798848381, -0.0584770296506273... |
707.049 | The Galactic Deuterium Abundance and Dust Depletion: Insights From an
Expanded Ti/H Sample | The primordial abundance of deuterium (D/H) yields a measure of the density
of baryons in the universe and is an important complement to determinations
from cosmic microwave background (CMB) experiments. Indeed, the current small
sample of high redshift D/H measurements from quasar absorption line studies
are in exce... | astro-ph | the primordial abundance of deuterium dh yields a measure of the density of baryons in the universe and is an important complement to determinations from cosmic microwave background cmb experiments indeed the current small sample of high redshift dh measurements from quasar absorption line studies are in excellent agre... | [['the', 'primordial', 'abundance', 'of', 'deuterium', 'dh', 'yields', 'a', 'measure', 'of', 'the', 'density', 'of', 'baryons', 'in', 'the', 'universe', 'and', 'is', 'an', 'important', 'complement', 'to', 'determinations', 'from', 'cosmic', 'microwave', 'background', 'cmb', 'experiments', 'indeed', 'the', 'current', 's... | [-0.06337911043304008, 0.1332802100710897, -0.02591983297992096, 0.08234140090254866, 0.010392865602300957, -0.09375502978759682, 0.05381574734983114, 0.3885197863363588, -0.17845230880340554, -0.3426559405110527, 0.008878088386583948, -0.29477459778766874, -0.046101637725583296, 0.15856889464401686, -0.020809534487927... |
707.0491 | L.V.Kantorovich and Linear Programming | I want to write about what I know and remember about the activities of Leonid
Vital'evich Kantorovich, an outstanding scientist of the 20th century; about
his dramatic struggle for recognition of his mathematical economic theories;
about the initial stage of the history of linear programming; about beautuful
Kantorov... | math.HO math.OC | i want to write about what i know and remember about the activities of leonid vitalevich kantorovich an outstanding scientist of the 20th century about his dramatic struggle for recognition of his mathematical economic theories about the initial stage of the history of linear programming about beautuful kantorovich met... | [['i', 'want', 'to', 'write', 'about', 'what', 'i', 'know', 'and', 'remember', 'about', 'the', 'activities', 'of', 'leonid', 'vitalevich', 'kantorovich', 'an', 'outstanding', 'scientist', 'of', 'the', '20th', 'century', 'about', 'his', 'dramatic', 'struggle', 'for', 'recognition', 'of', 'his', 'mathematical', 'economic... | [-0.034310026381547766, 0.028426038931590663, -0.11613097413667156, 0.13657136594171626, -0.21612066184562223, -0.1676966898212923, 0.07229031103654443, 0.31733395770588174, -0.3165985656049207, -0.3454812415744935, 0.16110807992996665, -0.2979493938281993, -0.19379757836713482, 0.17796366950105352, -0.2224316236837201... |
707.0492 | Low Surface Brightness Galaxies around the HDF-S: II. Distances and
volume densities | With this study we aim at the spectroscopic verification of a photometrically
selected sample of Low Surface Brightness (LSB) galaxy candidates in a field
around the Hubble Deep Field-South (HDF-S). The sample helps to extend the
parameter space for LSB galaxies to lower central surface brightnesses and to
provide be... | astro-ph | with this study we aim at the spectroscopic verification of a photometrically selected sample of low surface brightness lsb galaxy candidates in a field around the hubble deep fieldsouth hdfs the sample helps to extend the parameter space for lsb galaxies to lower central surface brightnesses and to provide better esti... | [['with', 'this', 'study', 'we', 'aim', 'at', 'the', 'spectroscopic', 'verification', 'of', 'a', 'photometrically', 'selected', 'sample', 'of', 'low', 'surface', 'brightness', 'lsb', 'galaxy', 'candidates', 'in', 'a', 'field', 'around', 'the', 'hubble', 'deep', 'fieldsouth', 'hdfs', 'the', 'sample', 'helps', 'to', 'ext... | [-0.022588036284889913, 0.04300239927818911, -0.15613296786483075, 0.11396324990193316, -0.11520983450926137, -0.05760715802723758, 0.06474930132215127, 0.45086643104581364, -0.12100112955325759, -0.3919492100936045, 0.07351763402721385, -0.28526318790750826, -0.005220383063934008, 0.22711323798722047, -0.1096758301221... |
707.0493 | A comment on `Wave-breaking Limits for relativistic electrostatic waves
in a one-dimensional warm plasma' Phys. Plasmas 13 123102 by R. M. G. M.
Trines and P. A. Norreys | Trines and Norreys state that a principle aim of their work on warm
wave-breaking was ``to create some order in the diverse landscape of warm fluid
models and establish which model is most suitable for the study of wave
breaking in thermal plasma.'' Unfortunately, we must conclude that they have
obfuscated more than ... | physics.plasm-ph | trines and norreys state that a principle aim of their work on warm wavebreaking was to create some order in the diverse landscape of warm fluid models and establish which model is most suitable for the study of wave breaking in thermal plasma unfortunately we must conclude that they have obfuscated more than they have... | [['trines', 'and', 'norreys', 'state', 'that', 'a', 'principle', 'aim', 'of', 'their', 'work', 'on', 'warm', 'wavebreaking', 'was', 'to', 'create', 'some', 'order', 'in', 'the', 'diverse', 'landscape', 'of', 'warm', 'fluid', 'models', 'and', 'establish', 'which', 'model', 'is', 'most', 'suitable', 'for', 'the', 'study'... | [-0.09054578453887606, 0.1507269055582583, -0.11927116846325933, 0.0791110005748861, -0.07286381323796672, -0.15457783192647873, -0.0008219705353415495, 0.37530843918589324, -0.20155235041543287, -0.32379280266075117, 0.12414904908163825, -0.2500256537585645, -0.1239515360652444, 0.16540065050641126, -0.033399888918407... |
707.0494 | Additional Symmetry of CKP hierarchy | Based on the Orlov and Shulman's M operator, the additional symmetries and
the string equation of the CKP hierarchy are established, and then the higher
order constraints on $L^l$ are obtained. In addition, the generating function
and some properties are also given. In particular, the additional symmetry
flows form a... | nlin.SI | based on the orlov and shulmans m operator the additional symmetries and the string equation of the ckp hierarchy are established and then the higher order constraints on ll are obtained in addition the generating function and some properties are also given in particular the additional symmetry flows form a new infinit... | [['based', 'on', 'the', 'orlov', 'and', 'shulmans', 'm', 'operator', 'the', 'additional', 'symmetries', 'and', 'the', 'string', 'equation', 'of', 'the', 'ckp', 'hierarchy', 'are', 'established', 'and', 'then', 'the', 'higher', 'order', 'constraints', 'on', 'll', 'are', 'obtained', 'in', 'addition', 'the', 'generating',... | [-0.15765493459431296, 0.11157650617345916, -0.06720544568310349, 0.0954320968495745, -0.1358355918457195, -0.11037761545976844, -0.01011151154288801, 0.29280914511468453, -0.28693430289878685, -0.2688678009751237, 0.1763530594683489, -0.2859698475606866, -0.1498687374326637, 0.16121602754929434, -0.018960077915403804,... |
707.0495 | Vibrating Superconducting Island in a Josephson Junction | We consider a combined nanomechanical-supercondcuting device that allows the
Cooper pair tunneling to interfere with the mechanical motion of the middle
superconducting island. Coupling of mechanical oscillations of a
superconducting island between two superconducting leads to the electronic
tunneling generate a supe... | cond-mat.mes-hall | we consider a combined nanomechanicalsupercondcuting device that allows the cooper pair tunneling to interfere with the mechanical motion of the middle superconducting island coupling of mechanical oscillations of a superconducting island between two superconducting leads to the electronic tunneling generate a supercur... | [['we', 'consider', 'a', 'combined', 'nanomechanicalsupercondcuting', 'device', 'that', 'allows', 'the', 'cooper', 'pair', 'tunneling', 'to', 'interfere', 'with', 'the', 'mechanical', 'motion', 'of', 'the', 'middle', 'superconducting', 'island', 'coupling', 'of', 'mechanical', 'oscillations', 'of', 'a', 'superconductin... | [-0.2663673144131106, 0.2334082314169946, -0.03748123205088554, 0.004078766440061179, -0.0700513117357177, -0.198065191522201, 0.08230373511113168, 0.32800663333941016, -0.2330038828894179, -0.2854705346361833, -0.029154857463312357, -0.3012563117825924, -0.09477502688210696, 0.21114295534789562, 0.0034149386127419927,... |
707.0496 | Controlled spontaneous emission | The problem of spontaneous emission is studied by a direct computer
simulation of the dynamics of a combined system: atom + radiation field. The
parameters of the discrete finite model, including up to 20k field oscillators,
have been optimized by a comparison with the exact solution for the case when
the oscillators... | quant-ph | the problem of spontaneous emission is studied by a direct computer simulation of the dynamics of a combined system atom radiation field the parameters of the discrete finite model including up to 20k field oscillators have been optimized by a comparison with the exact solution for the case when the oscillators have eq... | [['the', 'problem', 'of', 'spontaneous', 'emission', 'is', 'studied', 'by', 'a', 'direct', 'computer', 'simulation', 'of', 'the', 'dynamics', 'of', 'a', 'combined', 'system', 'atom', 'radiation', 'field', 'the', 'parameters', 'of', 'the', 'discrete', 'finite', 'model', 'including', 'up', 'to', '20k', 'field', 'oscillat... | [-0.15035488336450523, 0.16791712825910912, -0.04291589384795063, 0.0034546900330395956, 0.0011041115736588835, -0.11253025867044926, 0.05185162520372412, 0.3937943638612827, -0.23797112678229396, -0.2987074217034711, 0.08153065082927545, -0.2763758771535423, -0.07371646683249208, 0.22717270677029672, 0.067667969481812... |
707.0497 | Moduli Stabilization in Meta-Stable Heterotic Supergravity Vacua | We revisit the issue of moduli stabilization in a class of N=1 four
dimensional supergravity theories which are low energy descriptions of standard
perturbative heterotic string vacua compactified on Calabi-Yau spaces. In
particular, we show how it is possible to stabilize the universal dilaton and
Kahler moduli in a... | hep-th hep-ph | we revisit the issue of moduli stabilization in a class of n1 four dimensional supergravity theories which are low energy descriptions of standard perturbative heterotic string vacua compactified on calabiyau spaces in particular we show how it is possible to stabilize the universal dilaton and kahler moduli in a de si... | [['we', 'revisit', 'the', 'issue', 'of', 'moduli', 'stabilization', 'in', 'a', 'class', 'of', 'n1', 'four', 'dimensional', 'supergravity', 'theories', 'which', 'are', 'low', 'energy', 'descriptions', 'of', 'standard', 'perturbative', 'heterotic', 'string', 'vacua', 'compactified', 'on', 'calabiyau', 'spaces', 'in', 'pa... | [-0.1582638855910866, 0.255904786918575, -0.05594079262123276, 0.1857992006922499, -0.08983689699417506, -0.20455140148838744, -0.02203049312512844, 0.29949432069387955, -0.1488424920811294, -0.26431553290249443, 0.11039042347319758, -0.20729266671248928, -0.1521412946570378, 0.09211983710813981, -0.12832021438636076, ... |
707.0498 | The Role of Time in the Creation of Knowledge | This paper I assume that in humans the creation of knowledge depends on a
discrete time, or stage, sequential decision-making process subjected to a
stochastic, information transmitting environment. For each time-stage, this
environment randomly transmits Shannon type information-packets to the
decision-maker, who ex... | cs.LG cs.AI cs.IT math.IT | this paper i assume that in humans the creation of knowledge depends on a discrete time or stage sequential decisionmaking process subjected to a stochastic information transmitting environment for each timestage this environment randomly transmits shannon type informationpackets to the decisionmaker who examines each ... | [['this', 'paper', 'i', 'assume', 'that', 'in', 'humans', 'the', 'creation', 'of', 'knowledge', 'depends', 'on', 'a', 'discrete', 'time', 'or', 'stage', 'sequential', 'decisionmaking', 'process', 'subjected', 'to', 'a', 'stochastic', 'information', 'transmitting', 'environment', 'for', 'each', 'timestage', 'this', 'env... | [-0.07365252636708051, 0.07090945880886891, -0.10441593591646432, 0.03242123568167091, -0.1125802398665989, -0.17915325823889897, 0.12302672610389531, 0.37084760983213244, -0.29477939253552354, -0.3011330166134796, 0.08029577711499933, -0.25250412515706294, -0.1762559077377505, 0.1382528079921554, -0.14126775097503935,... |
707.0499 | Lovelock inflation and the number of large dimensions | We discuss an inflationary scenario based on Lovelock terms. These higher
order curvature terms can lead to inflation when there are more than three
spatial dimensions. Inflation will end if the extra dimensions are stabilised,
so that at most three dimensions are free to expand. This relates graceful exit
to the num... | hep-th astro-ph gr-qc hep-ph | we discuss an inflationary scenario based on lovelock terms these higher order curvature terms can lead to inflation when there are more than three spatial dimensions inflation will end if the extra dimensions are stabilised so that at most three dimensions are free to expand this relates graceful exit to the number of... | [['we', 'discuss', 'an', 'inflationary', 'scenario', 'based', 'on', 'lovelock', 'terms', 'these', 'higher', 'order', 'curvature', 'terms', 'can', 'lead', 'to', 'inflation', 'when', 'there', 'are', 'more', 'than', 'three', 'spatial', 'dimensions', 'inflation', 'will', 'end', 'if', 'the', 'extra', 'dimensions', 'are', 's... | [-0.14803127594588494, 0.25789713264596437, -0.03141641823405569, 0.07802858483681285, -0.09556367256763307, -0.1800528570162979, -0.11779483737085353, 0.3449434012851932, -0.17205784316809677, -0.2933538341556083, 0.14140819205309857, -0.2497185731306672, -0.16013562814755875, 0.14949748632498086, -0.10557433827356859... |
707.05 | Location-Aided Fast Distributed Consensus in Wireless Networks | Existing works on distributed consensus explore linear iterations based on
reversible Markov chains, which contribute to the slow convergence of the
algorithms. It has been observed that by overcoming the diffusive behavior of
reversible chains, certain nonreversible chains lifted from reversible ones mix
substantial... | cs.IT math.IT | existing works on distributed consensus explore linear iterations based on reversible markov chains which contribute to the slow convergence of the algorithms it has been observed that by overcoming the diffusive behavior of reversible chains certain nonreversible chains lifted from reversible ones mix substantially fa... | [['existing', 'works', 'on', 'distributed', 'consensus', 'explore', 'linear', 'iterations', 'based', 'on', 'reversible', 'markov', 'chains', 'which', 'contribute', 'to', 'the', 'slow', 'convergence', 'of', 'the', 'algorithms', 'it', 'has', 'been', 'observed', 'that', 'by', 'overcoming', 'the', 'diffusive', 'behavior', ... | [-0.16466054310249406, 0.03506310842391846, -0.05475758856306944, 0.005827292367908301, -0.048270204158676465, -0.22039834682123158, 0.08727215847616678, 0.4448893449494037, -0.31006162251839575, -0.2797775930639232, 0.09758213928505248, -0.19437989713583975, -0.1473802051502922, 0.1683611792792237, -0.0813945480973604... |
707.0501 | K-band spectroscopy of pre-cataclysmic variables | We have taken K-band spectroscopy of a sample of 13 pre-CVs in order to
examine them for anomalous chemical abundances. In particular, we study the
strength of the 12CO and 13CO absorption bands that have been found diminished
and enhanced, respectively, in similar studies of CVs.
All our systems show CO abundances... | astro-ph | we have taken kband spectroscopy of a sample of 13 precvs in order to examine them for anomalous chemical abundances in particular we study the strength of the 12co and 13co absorption bands that have been found diminished and enhanced respectively in similar studies of cvs all our systems show co abundances that are w... | [['we', 'have', 'taken', 'kband', 'spectroscopy', 'of', 'a', 'sample', 'of', '13', 'precvs', 'in', 'order', 'to', 'examine', 'them', 'for', 'anomalous', 'chemical', 'abundances', 'in', 'particular', 'we', 'study', 'the', 'strength', 'of', 'the', '12co', 'and', '13co', 'absorption', 'bands', 'that', 'have', 'been', 'fou... | [-0.06650837028670746, 0.11881905856838178, -0.01642819502740167, 0.07927552231922164, -0.06806998191314051, -0.08657090627699897, 0.08207141259602697, 0.41604384064946015, -0.17849980671113977, -0.33227071694182087, 0.07840692290301376, -0.2925401481964703, -0.0730208579285924, 0.19447236395596215, -0.0432459572512016... |
707.0502 | Deflated GMRES for Systems with Multiple Shifts and Multiple Right-Hand
Sides | We consider solution of multiply shifted systems of nonsymmetric linear
equations, possibly also with multiple right-hand sides. First, for a single
right-hand side, the matrix is shifted by several multiples of the identity.
Such problems arise in a number of applications, including lattice quantum
chromodynamics wh... | math-ph hep-lat math.MP | we consider solution of multiply shifted systems of nonsymmetric linear equations possibly also with multiple righthand sides first for a single righthand side the matrix is shifted by several multiples of the identity such problems arise in a number of applications including lattice quantum chromodynamics where the ma... | [['we', 'consider', 'solution', 'of', 'multiply', 'shifted', 'systems', 'of', 'nonsymmetric', 'linear', 'equations', 'possibly', 'also', 'with', 'multiple', 'righthand', 'sides', 'first', 'for', 'a', 'single', 'righthand', 'side', 'the', 'matrix', 'is', 'shifted', 'by', 'several', 'multiples', 'of', 'the', 'identity', ... | [-0.1267114607327865, 0.08719245536000624, -0.0722040489926345, 0.028132192041372385, -0.0859875493067301, -0.2412811947307723, -0.01183074074639481, 0.3772036988803812, -0.33578461320218395, -0.23379865095103528, 0.19133782805480315, -0.2905023871621085, -0.1494233352395227, 0.21678927102873344, -0.04849362209712887, ... |
707.0503 | Spin-Orbit Alignment for the Eccentric Exoplanet HD 147506b | The short-period exoplanet HD 147506b (also known as HAT-P-2b) has an
eccentric orbit, raising the possibility that it migrated through planet-planet
scattering or Kozai oscillations accompanied by tidal dissipation. Either of
these scenarios could have significantly tilted the orbit relative to the host
star's equat... | astro-ph | the shortperiod exoplanet hd 147506b also known as hatp2b has an eccentric orbit raising the possibility that it migrated through planetplanet scattering or kozai oscillations accompanied by tidal dissipation either of these scenarios could have significantly tilted the orbit relative to the host stars equatorial plane... | [['the', 'shortperiod', 'exoplanet', 'hd', '147506b', 'also', 'known', 'as', 'hatp2b', 'has', 'an', 'eccentric', 'orbit', 'raising', 'the', 'possibility', 'that', 'it', 'migrated', 'through', 'planetplanet', 'scattering', 'or', 'kozai', 'oscillations', 'accompanied', 'by', 'tidal', 'dissipation', 'either', 'of', 'these... | [-0.2075379503211964, 0.14263443659382294, -0.0577225554647429, 0.055266726579273416, -0.1451804717637111, -0.08539621675578511, 0.08131646100762431, 0.3827185761009421, -0.23698841562825385, -0.30618052969677984, 0.08783510877863965, -0.26569192528846525, -0.1387024431001987, 0.22495166337222, -0.03629173073595581, -0... |
707.0504 | Experimental Free Energy Surface Reconstruction From Single-Molecule
Force Spectroscopy Using Jarzynski's Equality | We used the atomic force microscope to manipulate and unfold individual
molecules of the titin I27 domain and reconstructed its free energy surface
using Jarzynski's equality. The free energy surface for both stretching and
unfolding was reconstructed using an exact formula that relates the
nonequilibrium work fluctu... | physics.bio-ph physics.gen-ph | we used the atomic force microscope to manipulate and unfold individual molecules of the titin i27 domain and reconstructed its free energy surface using jarzynskis equality the free energy surface for both stretching and unfolding was reconstructed using an exact formula that relates the nonequilibrium work fluctuatio... | [['we', 'used', 'the', 'atomic', 'force', 'microscope', 'to', 'manipulate', 'and', 'unfold', 'individual', 'molecules', 'of', 'the', 'titin', 'i27', 'domain', 'and', 'reconstructed', 'its', 'free', 'energy', 'surface', 'using', 'jarzynskis', 'equality', 'the', 'free', 'energy', 'surface', 'for', 'both', 'stretching', '... | [-0.057113876883985004, 0.1431461616744838, -0.14014607535242146, 0.10716027508285245, -0.014386330983627623, -0.11293463650481583, 0.03809683989933648, 0.3554646543044353, -0.32543609572017446, -0.3435052563828007, -0.00035736115462207626, -0.25363979065599285, -0.08749590264024021, 0.23514006644700627, 0.012868337012... |
707.0505 | Deflated Iterative Methods for Linear Equations with Multiple Right-Hand
Sides | A new approach is discussed for solving large nonsymmetric systems of linear
equations with multiple right-hand sides. The first system is solved with a
deflated GMRES method that generates eigenvector information at the same time
that the linear equations are solved. Subsequent systems are solved by
combining restar... | math-ph hep-lat math.MP | a new approach is discussed for solving large nonsymmetric systems of linear equations with multiple righthand sides the first system is solved with a deflated gmres method that generates eigenvector information at the same time that the linear equations are solved subsequent systems are solved by combining restarted g... | [['a', 'new', 'approach', 'is', 'discussed', 'for', 'solving', 'large', 'nonsymmetric', 'systems', 'of', 'linear', 'equations', 'with', 'multiple', 'righthand', 'sides', 'the', 'first', 'system', 'is', 'solved', 'with', 'a', 'deflated', 'gmres', 'method', 'that', 'generates', 'eigenvector', 'information', 'at', 'the', ... | [-0.09626562236980707, 0.05590887353432158, -0.1004856521298212, 0.04888115394860506, -0.09519357056253486, -0.2300135627871862, -0.016215634447763916, 0.37687059269735107, -0.32005205303430556, -0.26602730429386373, 0.1646491864627158, -0.2581481666476638, -0.13647623964309416, 0.252512853399471, -0.03970866251426439,... |
707.0506 | The Distance to SS433/W50 and its Interaction with the ISM | [ABRIDGED] The distance to the relativistic jet source SS433 and the related
supernova remnant W50 is re-examined using new observations of HI in absorption
from the VLA, HI in emission from the GBT, and 12CO emission from the FCRAO.
The new measurements show HI in absorption against SS433 to a velocity of 75
km/s bu... | astro-ph | abridged the distance to the relativistic jet source ss433 and the related supernova remnant w50 is reexamined using new observations of hi in absorption from the vla hi in emission from the gbt and 12co emission from the fcrao the new measurements show hi in absorption against ss433 to a velocity of 75 kms but not to ... | [['abridged', 'the', 'distance', 'to', 'the', 'relativistic', 'jet', 'source', 'ss433', 'and', 'the', 'related', 'supernova', 'remnant', 'w50', 'is', 'reexamined', 'using', 'new', 'observations', 'of', 'hi', 'in', 'absorption', 'from', 'the', 'vla', 'hi', 'in', 'emission', 'from', 'the', 'gbt', 'and', '12co', 'emission... | [-0.09782126192674712, 0.06344543811937692, -0.03678486163255286, 0.04027474087532945, -0.08147015305677871, -0.05141585239862279, 0.061539858742197556, 0.41322544152784096, -0.19919502496119454, -0.29905253633026135, 0.052059235052323086, -0.3109979647653619, 0.028706214913690055, 0.1824294404006443, 0.014794773126773... |
707.0507 | Incommensurate magnetic structure in the orthorhombic perovskite ErMnO_3 | By combining dielectric, specific heat, and magnetization measurements and
high-resolution neutron powder diffraction, we have investigated the
thermodynamic and magnetic/structural properties of the metastable orthorhombic
perovskite ErMnO_3 prepared by high-pressure synthesis. The system becomes
antiferromagnetical... | cond-mat.str-el | by combining dielectric specific heat and magnetization measurements and highresolution neutron powder diffraction we have investigated the thermodynamic and magneticstructural properties of the metastable orthorhombic perovskite ermno_3 prepared by highpressure synthesis the system becomes antiferromagnetically correl... | [['by', 'combining', 'dielectric', 'specific', 'heat', 'and', 'magnetization', 'measurements', 'and', 'highresolution', 'neutron', 'powder', 'diffraction', 'we', 'have', 'investigated', 'the', 'thermodynamic', 'and', 'magneticstructural', 'properties', 'of', 'the', 'metastable', 'orthorhombic', 'perovskite', 'ermno_3',... | [-0.16667480647907054, 0.31793000721862835, 0.015200555349062932, -0.03985903605720714, -0.04550097985376947, -0.11294174879960912, 0.14597209465251867, 0.4268700709125321, -0.2699664077280383, -0.29814284069365576, 0.05941478876813658, -0.37762735949486104, -0.07004806287831773, 0.13833397064407013, 0.1446971239669150... |
707.0508 | X-ray Spectral Signatures of the Photon Bubble Model for Ultraluminous
X-ray Sources | The nature of ultraluminous X-ray sources in nearby galaxies is one of the
major open questions in modern X-ray astrophysics. One possible explanation for
these objects is an inhomogeneous, radiation dominated accretion disk around a
$\sim 10 M_{\odot}$ black hole -- the so-called ``photon bubble'' model. While
previ... | astro-ph | the nature of ultraluminous xray sources in nearby galaxies is one of the major open questions in modern xray astrophysics one possible explanation for these objects is an inhomogeneous radiation dominated accretion disk around a sim 10 m_odot black hole the socalled photon bubble model while previous studies of this m... | [['the', 'nature', 'of', 'ultraluminous', 'xray', 'sources', 'in', 'nearby', 'galaxies', 'is', 'one', 'of', 'the', 'major', 'open', 'questions', 'in', 'modern', 'xray', 'astrophysics', 'one', 'possible', 'explanation', 'for', 'these', 'objects', 'is', 'an', 'inhomogeneous', 'radiation', 'dominated', 'accretion', 'disk'... | [-0.056258596490927355, 0.12292168437914594, -0.07062615075709201, 0.13753020505352448, -0.05765047957745526, -0.12778811966470704, 0.017173651691086995, 0.42187462386926766, -0.2082480503918197, -0.35271492962156076, 0.07847912512417282, -0.3281205674562762, -0.0071247809012619095, 0.2385284895545216, -0.0183363620895... |
707.0509 | Order-Parameter Correlation Functions in Quantum Critical Phenomena | We investigate the functional form of the order-parameter (two-point)
correlation function in quantum critical phenomena. Contrary to the common
lore, when there is no particle-hole symmetry we find that the equal-time
correlation function at criticality does not display a diverging correlation
length. We illustrate ... | cond-mat.stat-mech cond-mat.str-el | we investigate the functional form of the orderparameter twopoint correlation function in quantum critical phenomena contrary to the common lore when there is no particlehole symmetry we find that the equaltime correlation function at criticality does not display a diverging correlation length we illustrate our conclus... | [['we', 'investigate', 'the', 'functional', 'form', 'of', 'the', 'orderparameter', 'twopoint', 'correlation', 'function', 'in', 'quantum', 'critical', 'phenomena', 'contrary', 'to', 'the', 'common', 'lore', 'when', 'there', 'is', 'no', 'particlehole', 'symmetry', 'we', 'find', 'that', 'the', 'equaltime', 'correlation',... | [-0.15725077606611332, 0.16873165020340328, -0.14221565998396127, 0.17462717031397051, 0.0040395354883650605, -0.13608930787955553, 0.019780768357785576, 0.38161614852941644, -0.19529381571278387, -0.2117722900426489, -0.02685538955206462, -0.3556179791467927, -0.22926612409873534, 0.10982711863372538, 0.08217699456958... |
707.051 | Computational coarse graining of a randomly forced 1-D Burgers equation | We explore a computational approach to coarse graining the evolution of the
large-scale features of a randomly forced Burgers equation in one spatial
dimension. The long term evolution of the solution energy spectrum appears
self-similar in time. We demonstrate coarse projective integration and coarse
dynamic renorma... | physics.comp-ph | we explore a computational approach to coarse graining the evolution of the largescale features of a randomly forced burgers equation in one spatial dimension the long term evolution of the solution energy spectrum appears selfsimilar in time we demonstrate coarse projective integration and coarse dynamic renormalizati... | [['we', 'explore', 'a', 'computational', 'approach', 'to', 'coarse', 'graining', 'the', 'evolution', 'of', 'the', 'largescale', 'features', 'of', 'a', 'randomly', 'forced', 'burgers', 'equation', 'in', 'one', 'spatial', 'dimension', 'the', 'long', 'term', 'evolution', 'of', 'the', 'solution', 'energy', 'spectrum', 'app... | [-0.1362074334376856, 0.1116712826429727, -0.12774121549749828, 0.11485541137011276, -0.07864894310478121, -0.1062326451520557, -0.01843207269785521, 0.3570566131776381, -0.3615197256895835, -0.2841308729459896, 0.08712537527975181, -0.218296992645027, -0.11164121683585741, 0.16254612491668566, 0.03612786511202221, 0.1... |
707.0511 | The S-matrix of the Faddeev-Reshetikhin Model, Diagonalizability and PT
Symmetry | We study the question of diagonalizability of the Hamiltonian for the
Faddeev-Reshetikhin (FR) model in the two particle sector. Although the two
particle S-matrix element for the FR model, which may be relevant for the
quantization of strings on $AdS_{5}\times S^{5}$, has been calculated recently
using field theoret... | hep-th | we study the question of diagonalizability of the hamiltonian for the faddeevreshetikhin fr model in the two particle sector although the two particle smatrix element for the fr model which may be relevant for the quantization of strings on ads_5times s5 has been calculated recently using field theoretic methods we fin... | [['we', 'study', 'the', 'question', 'of', 'diagonalizability', 'of', 'the', 'hamiltonian', 'for', 'the', 'faddeevreshetikhin', 'fr', 'model', 'in', 'the', 'two', 'particle', 'sector', 'although', 'the', 'two', 'particle', 'smatrix', 'element', 'for', 'the', 'fr', 'model', 'which', 'may', 'be', 'relevant', 'for', 'the',... | [-0.13427386711144612, 0.15563941090678177, -0.0858091030580302, 0.11045526258595702, -0.059256231016996834, -0.16417071351057125, -0.04713663982434405, 0.34012560087773536, -0.2270656352888586, -0.26792531855197416, 0.05489353567879233, -0.25238882180303335, -0.17698257617290236, 0.11194955553911212, -0.01037153206869... |
707.0512 | $(\alpha')^4$ Corrections in Holographic Large N_c QCD and $\pi - \pi$
Scattering | We calculate the ${\alpha'}^4$ corrections to the non-Abelian DBI action on
the D8-brane in the holographic dual of large N_c QCD proposed by Sakai and
Sugimoto. These give rise to higher derivative terms, in particular, four
derivative contact terms for the pion field with the coupling uniquely
determined. We calcul... | hep-th hep-ph | we calculate the alpha4 corrections to the nonabelian dbi action on the d8brane in the holographic dual of large n_c qcd proposed by sakai and sugimoto these give rise to higher derivative terms in particular four derivative contact terms for the pion field with the coupling uniquely determined we calculate the pionpio... | [['we', 'calculate', 'the', 'alpha4', 'corrections', 'to', 'the', 'nonabelian', 'dbi', 'action', 'on', 'the', 'd8brane', 'in', 'the', 'holographic', 'dual', 'of', 'large', 'n_c', 'qcd', 'proposed', 'by', 'sakai', 'and', 'sugimoto', 'these', 'give', 'rise', 'to', 'higher', 'derivative', 'terms', 'in', 'particular', 'fou... | [-0.14011855163912781, 0.17878456621239072, -0.06739706530660282, 0.10277349269017577, -0.07031850864672486, -0.09963148080415148, 0.019579525511824826, 0.2934304665883674, -0.12893064000630095, -0.2653273867224069, 0.02442074181025793, -0.3198761765516418, -0.12624419647652438, 0.13173818590311223, -0.0043081683243679... |
707.0513 | On the zero-temperature limit of one-dimensional Gibbs measures | This paper has been withdrawn by the authors due to an error in the main
theorem.
| math.DS math-ph math.MP | this paper has been withdrawn by the authors due to an error in the main theorem | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'due', 'to', 'an', 'error', 'in', 'the', 'main', 'theorem']] | [-0.07619959546718746, -0.050974507429600635, -0.13152720127254725, -0.02332609616132686, -0.034820380504243076, -0.008879365399479866, -0.0001076522094081156, 0.300877729896456, -0.2812039719428867, -0.3330938358558342, 0.12334491640649503, -0.26468220038805157, -0.14985200494993478, 0.13950609101448208, -0.3806827086... |
707.0514 | Phase space methods and psychoacoustic models in lossy transform coding | I present a method for lossy transform coding of digital audio that uses the
Weyl symbol calculus for constructing the encoding and decoding transformation.
The method establishes a direct connection between a time-frequency
representation of the signal dependent threshold of masked noise and the
encode/decode pair. ... | cs.IT cs.SD math.IT | i present a method for lossy transform coding of digital audio that uses the weyl symbol calculus for constructing the encoding and decoding transformation the method establishes a direct connection between a timefrequency representation of the signal dependent threshold of masked noise and the encodedecode pair the fo... | [['i', 'present', 'a', 'method', 'for', 'lossy', 'transform', 'coding', 'of', 'digital', 'audio', 'that', 'uses', 'the', 'weyl', 'symbol', 'calculus', 'for', 'constructing', 'the', 'encoding', 'and', 'decoding', 'transformation', 'the', 'method', 'establishes', 'a', 'direct', 'connection', 'between', 'a', 'timefrequenc... | [-0.14672507077921182, 0.03672088443168572, -0.16611226265584783, 0.061515203810163906, -0.1116625495113632, -0.19804883374932356, 0.1001896695857535, 0.37063372294817654, -0.32306375567402157, -0.20641070145315357, 0.03593388541568337, -0.23542867518595553, -0.24596027076976107, 0.18586096578344172, -0.077141499479434... |
707.0515 | High Energy neutrino signals from the Epoch of Reionization | We perform a new estimate of the high energy neutrinos expected from GRBs
associated with the first generation of stars in light of new models and
constraints on the epoch of reionization and a more detailed evaluation of the
neutrino emission yields. We also compare the diffuse high energy neutrino
background from P... | astro-ph | we perform a new estimate of the high energy neutrinos expected from grbs associated with the first generation of stars in light of new models and constraints on the epoch of reionization and a more detailed evaluation of the neutrino emission yields we also compare the diffuse high energy neutrino background from popu... | [['we', 'perform', 'a', 'new', 'estimate', 'of', 'the', 'high', 'energy', 'neutrinos', 'expected', 'from', 'grbs', 'associated', 'with', 'the', 'first', 'generation', 'of', 'stars', 'in', 'light', 'of', 'new', 'models', 'and', 'constraints', 'on', 'the', 'epoch', 'of', 'reionization', 'and', 'a', 'more', 'detailed', 'e... | [0.00341565738463859, 0.17530585573562843, -0.02991440802967797, 0.20298321309030254, -0.10434676562153707, -0.0902079877612943, 0.100627916808607, 0.3856141371652484, -0.16931153682614394, -0.3588719392287065, 0.060679244239123145, -0.3076925667207406, -0.0020305455179892087, 0.23991988270338907, 0.011654344597252819,... |
707.0516 | Deep VLT infrared observations of X-ray Dim Isolated Neutron Stars | X-ray observations have unveiled the existence of a family of radio-quiet
Isolated Neutron Stars whose X-ray emission is purely thermal, hence dubbed
X-ray Dim Isolated Neutron Stars (XDINSs). While optical observations have
allowed to relate the thermal emission to the neutron star cooling and to build
the neutron s... | astro-ph | xray observations have unveiled the existence of a family of radioquiet isolated neutron stars whose xray emission is purely thermal hence dubbed xray dim isolated neutron stars xdinss while optical observations have allowed to relate the thermal emission to the neutron star cooling and to build the neutron star surfac... | [['xray', 'observations', 'have', 'unveiled', 'the', 'existence', 'of', 'a', 'family', 'of', 'radioquiet', 'isolated', 'neutron', 'stars', 'whose', 'xray', 'emission', 'is', 'purely', 'thermal', 'hence', 'dubbed', 'xray', 'dim', 'isolated', 'neutron', 'stars', 'xdinss', 'while', 'optical', 'observations', 'have', 'allo... | [-0.059532272740497126, 0.0898288653814721, -0.08774717045640067, 0.11101808302079144, -0.14371470893854002, -0.06330604178082806, 0.1027197263541604, 0.4087947821712207, -0.19474180333928115, -0.34892600222985615, 0.12525169823998702, -0.2998642073554536, -0.03224700597157725, 0.20940836578038635, -0.00521392945324900... |
707.0517 | On the nature of Delta Scuti star HD 115520 | As a continuation of the study of the newly found Delta Scuti star HD 115520,
we present a period analysis of recently acquired photometric data covering
four nights, as well as some conclusions on the nature of this star.
| astro-ph | as a continuation of the study of the newly found delta scuti star hd 115520 we present a period analysis of recently acquired photometric data covering four nights as well as some conclusions on the nature of this star | [['as', 'a', 'continuation', 'of', 'the', 'study', 'of', 'the', 'newly', 'found', 'delta', 'scuti', 'star', 'hd', '115520', 'we', 'present', 'a', 'period', 'analysis', 'of', 'recently', 'acquired', 'photometric', 'data', 'covering', 'four', 'nights', 'as', 'well', 'as', 'some', 'conclusions', 'on', 'the', 'nature', 'of... | [-0.11945776592351888, 0.03775222322560454, -0.1251811906695366, 0.020276992272365055, -0.1208858402127302, -0.058706368197147786, 0.12429913745482306, 0.3356933852559642, -0.13625905211818845, -0.3761556859275228, 0.1622586019067584, -0.28450699542698105, -0.1356637035251448, 0.2283782908987058, -0.05630769948229978, ... |
707.0518 | Generalized handlebody sets and non-Haken 3-manifolds | In the curve complex for a surface, a handlebody set is the set of loops that
bound properly embedded disks in a given handlebody bounded by the surface. A
boundary set is the set of non-separating loops in the curve complex that bound
two-sided, properly embedded surfaces. For a Heegaard splitting, the distance
betw... | math.GT | in the curve complex for a surface a handlebody set is the set of loops that bound properly embedded disks in a given handlebody bounded by the surface a boundary set is the set of nonseparating loops in the curve complex that bound twosided properly embedded surfaces for a heegaard splitting the distance between the b... | [['in', 'the', 'curve', 'complex', 'for', 'a', 'surface', 'a', 'handlebody', 'set', 'is', 'the', 'set', 'of', 'loops', 'that', 'bound', 'properly', 'embedded', 'disks', 'in', 'a', 'given', 'handlebody', 'bounded', 'by', 'the', 'surface', 'a', 'boundary', 'set', 'is', 'the', 'set', 'of', 'nonseparating', 'loops', 'in', ... | [-0.22166855661382917, 0.12627217408885147, -0.09334150742333715, 0.04015419463567104, -0.06576384084834026, -0.13478554794933684, 0.042924909732571924, 0.3726960577734626, -0.26814310798550595, -0.2332962446311249, 0.11309899579120412, -0.29894511919874367, -0.1338024087997135, 0.20500801515645614, -0.1111907009738451... |
707.0519 | NaV2O4: a Quasi-1D Metallic Antiferromagnet with Half-Metallic Chains | NaV2O4 crystals were grown under high pressure using a NaCl flux, and the
crystals were characterized with X-ray diffraction, electrical resistivity,
heat capacity, and magnetization. The structure of NaV2O4 consists of double
chains of edge-sharing VO6 octahedra. The resistivity is highly anisotropic,
with the resis... | cond-mat.str-el cond-mat.supr-con | nav2o4 crystals were grown under high pressure using a nacl flux and the crystals were characterized with xray diffraction electrical resistivity heat capacity and magnetization the structure of nav2o4 consists of double chains of edgesharing vo6 octahedra the resistivity is highly anisotropic with the resistivity perp... | [['nav2o4', 'crystals', 'were', 'grown', 'under', 'high', 'pressure', 'using', 'a', 'nacl', 'flux', 'and', 'the', 'crystals', 'were', 'characterized', 'with', 'xray', 'diffraction', 'electrical', 'resistivity', 'heat', 'capacity', 'and', 'magnetization', 'the', 'structure', 'of', 'nav2o4', 'consists', 'of', 'double', '... | [-0.2019925582000393, 0.24294355993413114, 0.03572386293989521, 0.0006017338294027881, -0.06140734966717322, -0.16825143048031763, 0.04727064457256347, 0.44423389915715567, -0.24516474903899838, -0.265343584662134, 0.04744612423025749, -0.40571083467115054, -0.05629175842781974, 0.1928553934018551, 0.13265393892811103,... |
707.052 | The Real Scalar Field Equation for Nariai Black Hole in the 5D
Schwarzschild-de Sitter Black String Space | The Nariai black hole, whose two horizons are lying close to each other, is
an extreme and important case in the research of black hole. In this paper we
study the evolution of a massless scalar field scattered around in 5D
Schwarzschild-de Sitter black string space. Using the method shown by Brevik
and Simonsen (200... | gr-qc | the nariai black hole whose two horizons are lying close to each other is an extreme and important case in the research of black hole in this paper we study the evolution of a massless scalar field scattered around in 5d schwarzschildde sitter black string space using the method shown by brevik and simonsen 2001 we sol... | [['the', 'nariai', 'black', 'hole', 'whose', 'two', 'horizons', 'are', 'lying', 'close', 'to', 'each', 'other', 'is', 'an', 'extreme', 'and', 'important', 'case', 'in', 'the', 'research', 'of', 'black', 'hole', 'in', 'this', 'paper', 'we', 'study', 'the', 'evolution', 'of', 'a', 'massless', 'scalar', 'field', 'scattere... | [-0.12051727658455583, 0.0977227999169722, -0.04161920428920824, 0.0743859494429601, -0.08823406468050402, -0.17077125299972698, -0.0352772668545815, 0.34062212431588423, -0.20182770339306444, -0.26146800444425583, 0.11438640413577489, -0.3083536757263713, -0.14881437610781106, 0.1615303421869892, -0.048018134655789114... |
707.0521 | The distance to the Fornax Dwarf Spheroidal Galaxy | A large multicolour, wide-field photometric database of the Fornax dwarf
spheroidal galaxy has been analysed using three different methods to provide
revised distance estimates based on stellar populations in different age
intervals. The distance to Fornax was obtained from the Tip of the Red Giant
Branch measured by... | astro-ph | a large multicolour widefield photometric database of the fornax dwarf spheroidal galaxy has been analysed using three different methods to provide revised distance estimates based on stellar populations in different age intervals the distance to fornax was obtained from the tip of the red giant branch measured by a ne... | [['a', 'large', 'multicolour', 'widefield', 'photometric', 'database', 'of', 'the', 'fornax', 'dwarf', 'spheroidal', 'galaxy', 'has', 'been', 'analysed', 'using', 'three', 'different', 'methods', 'to', 'provide', 'revised', 'distance', 'estimates', 'based', 'on', 'stellar', 'populations', 'in', 'different', 'age', 'int... | [-0.028475404313990267, 0.08071853983505019, -0.1726201504195944, 0.05255355401173362, -0.1010573014263706, -0.02646321870129684, 0.11115413090487107, 0.4289638634385734, -0.13061278467066587, -0.3791584367863834, 0.02776889559042094, -0.33053692229220577, -0.010754950768474875, 0.21955818873669566, -0.1249130170583596... |
707.0522 | Superconductivity in spinel oxide LiTi2O4 epitaxial thin films | LiTi2O4 is a unique material in that it is the only known oxide spinel
superconductor. Although bulk studies have demonstrated that superconductivity
can be generally described by the Bardeen-Cooper-Schreiffer theory, the
microscopic mechanisms of superconductivity are not yet resolved fully. The
sensitivity of the s... | cond-mat.supr-con cond-mat.mtrl-sci | liti2o4 is a unique material in that it is the only known oxide spinel superconductor although bulk studies have demonstrated that superconductivity can be generally described by the bardeencooperschreiffer theory the microscopic mechanisms of superconductivity are not yet resolved fully the sensitivity of the supercon... | [['liti2o4', 'is', 'a', 'unique', 'material', 'in', 'that', 'it', 'is', 'the', 'only', 'known', 'oxide', 'spinel', 'superconductor', 'although', 'bulk', 'studies', 'have', 'demonstrated', 'that', 'superconductivity', 'can', 'be', 'generally', 'described', 'by', 'the', 'bardeencooperschreiffer', 'theory', 'the', 'micros... | [-0.12543162531721103, 0.21414160395030818, -0.046140649506451754, -0.008039957513127126, -0.058597035958169244, -0.18189244945044758, 0.10091390312091031, 0.4560197623374548, -0.27400787116043807, -0.28768338713774366, 0.011072095252318791, -0.30235413445908454, -0.13075312263671907, 0.1568136258975047, 0.008437190670... |
707.0523 | Upper critical field of electron-doped Pr$_{2-x}$Ce$_x$CuO$_{4-\delta}$
in parallel magnetic fields | We report a systematic study of the resistive superconducting transition in
the electron-doped cuprates Pr$_{2-x}$Ce$_{x}$CuO$_{4-\delta}$ down to 1.5 K
for magnetic field up to 58 T applied parallel to the conducting ab-planes. We
find that the zero temperature parallel critical field (H$_{c2\parallel
ab}$(0)) excee... | cond-mat.supr-con cond-mat.str-el | we report a systematic study of the resistive superconducting transition in the electrondoped cuprates pr_2xce_xcuo_4delta down to 15 k for magnetic field up to 58 t applied parallel to the conducting abplanes we find that the zero temperature parallel critical field h_c2parallel ab0 exceeds 58 t for the underdoped and... | [['we', 'report', 'a', 'systematic', 'study', 'of', 'the', 'resistive', 'superconducting', 'transition', 'in', 'the', 'electrondoped', 'cuprates', 'pr_2xce_xcuo_4delta', 'down', 'to', '15', 'k', 'for', 'magnetic', 'field', 'up', 'to', '58', 't', 'applied', 'parallel', 'to', 'the', 'conducting', 'abplanes', 'we', 'find'... | [-0.21037138183838783, 0.2588122395278259, 0.03674173508580698, 0.013499278900669697, -0.040293268293940594, -0.17498414784346764, 0.17674227047958696, 0.35410370881080017, -0.22074248654246972, -0.2569312904486243, -0.03482111342659942, -0.34908722641364653, -0.0058114610740686865, 0.1975751534123354, 0.06044044657444... |
707.0524 | Smart Electromechanical Pumping of Electrons in a Nanopillars Transistor | Analysis of room-temperature current-voltage (I-V) characteristics of a
silicon box in a nanopillar transistor suggests that a weak electromechanical
coupling of 0.17 is responsible for the stable tunnel of single-electron. The
dynamics involves a few electrons and the numbers (N) specified are periodical
at 3, 6, an... | quant-ph | analysis of roomtemperature currentvoltage iv characteristics of a silicon box in a nanopillar transistor suggests that a weak electromechanical coupling of 017 is responsible for the stable tunnel of singleelectron the dynamics involves a few electrons and the numbers n specified are periodical at 3 6 and 12 quantized... | [['analysis', 'of', 'roomtemperature', 'currentvoltage', 'iv', 'characteristics', 'of', 'a', 'silicon', 'box', 'in', 'a', 'nanopillar', 'transistor', 'suggests', 'that', 'a', 'weak', 'electromechanical', 'coupling', 'of', '017', 'is', 'responsible', 'for', 'the', 'stable', 'tunnel', 'of', 'singleelectron', 'the', 'dyna... | [-0.22093121378089894, 0.19490918623579837, 0.0031788276889446105, 0.04829311509913003, 0.011568407269872048, -0.22344121904620393, 0.0653168789322742, 0.32972037804059007, -0.2308885517868806, -0.3440032005733387, 0.013575164011721923, -0.31582588621650676, -0.0895174853800034, 0.21751359258355066, 0.03413594930686734... |
707.0525 | High-Resolution Submillimeter Imaging of the Ly-alpha Blob1 in SSA 22 | We present ~2" resolution submillimeter observations of the submillimeter
luminous giant Ly-alpha blob (LAB1) in the SSA 22 protocluster at redshift
z=3.1 with the Submillimeter Array (SMA). Although the expected submillimeter
flux density is 16 mJy at 880 micron, no emission is detected with the 2".4 x
1".9 (18 x 14... | astro-ph | we present 2 resolution submillimeter observations of the submillimeter luminous giant lyalpha blob lab1 in the ssa 22 protocluster at redshift z31 with the submillimeter array sma although the expected submillimeter flux density is 16 mjy at 880 micron no emission is detected with the 24 x 19 18 x 14 kpc beam at the 3... | [['we', 'present', '2', 'resolution', 'submillimeter', 'observations', 'of', 'the', 'submillimeter', 'luminous', 'giant', 'lyalpha', 'blob', 'lab1', 'in', 'the', 'ssa', '22', 'protocluster', 'at', 'redshift', 'z31', 'with', 'the', 'submillimeter', 'array', 'sma', 'although', 'the', 'expected', 'submillimeter', 'flux', ... | [-0.047368903467334654, 0.10470521140208196, -0.013267315206273148, 0.04860551250506736, -0.09181501370161034, -0.06264843281193559, -0.014610291971621336, 0.46077707286652486, -0.04525771411924021, -0.35725966116054525, 0.08348372446706283, -0.31759568809866323, 0.018231113960306782, 0.12648818212178034, 0.03030956891... |
707.0526 | Two generalizations of Cheeger-Gromoll splitting theorem via
Bakry-\'{E}mery Ricci curvature | In this paper, we prove two generalized versions of the Cheeger-Gromoll
splitting theorem via the non-negativity of the Bakry-\'Emery Ricci curavture
on complete Riemannian manifolds.
| math.DG math.GT | in this paper we prove two generalized versions of the cheegergromoll splitting theorem via the nonnegativity of the bakryemery ricci curavture on complete riemannian manifolds | [['in', 'this', 'paper', 'we', 'prove', 'two', 'generalized', 'versions', 'of', 'the', 'cheegergromoll', 'splitting', 'theorem', 'via', 'the', 'nonnegativity', 'of', 'the', 'bakryemery', 'ricci', 'curavture', 'on', 'complete', 'riemannian', 'manifolds']] | [-0.18989279435481876, 0.007630418869666755, -0.09576434036716819, 0.16786927494589085, -0.13483739054451385, -0.12429151963442564, -0.09257330073645183, 0.2733873873949051, -0.2795034336547057, -0.19032862464276454, 0.13844667599672297, -0.24580590384236226, -0.1527748724523311, 0.14556465455098078, -0.207621080024788... |
707.0527 | A general Schwarz Lemma for almost-Hermitian manifolds | We prove a version of Yau's Schwarz Lemma for general almost-complex
manifolds equipped with Hermitian metrics. This requires an extension to this
setting of the Laplacian comparison theorem. As an application we show that the
product of two almost-complex manifolds does not admit any complete Hermitian
metric with b... | math.DG | we prove a version of yaus schwarz lemma for general almostcomplex manifolds equipped with hermitian metrics this requires an extension to this setting of the laplacian comparison theorem as an application we show that the product of two almostcomplex manifolds does not admit any complete hermitian metric with bisectio... | [['we', 'prove', 'a', 'version', 'of', 'yaus', 'schwarz', 'lemma', 'for', 'general', 'almostcomplex', 'manifolds', 'equipped', 'with', 'hermitian', 'metrics', 'this', 'requires', 'an', 'extension', 'to', 'this', 'setting', 'of', 'the', 'laplacian', 'comparison', 'theorem', 'as', 'an', 'application', 'we', 'show', 'that... | [-0.2141581486269343, 0.001689016086633363, -0.08690080992480526, 0.10466143413691124, -0.1808769421987846, -0.22044445524663955, -0.06788062834043483, 0.4005325638238707, -0.23787211061867533, -0.21628480082469398, 0.13615088984675583, -0.24951274605605323, -0.21426233119468707, 0.19167889776777047, -0.187563592930645... |
707.0528 | Self-similar cosmological solutions with dark energy. I: formulation and
asymptotic analysis | Based on the asymptotic analysis of ordinary differential equations, we
classify all spherically symmetric self-similar solutions to the Einstein
equations which are asymptotically Friedmann at large distances and contain a
perfect fluid with equation of state $p=(\gamma -1)\mu$ with $0<\gamma<2/3$.
This corresponds ... | gr-qc astro-ph hep-th | based on the asymptotic analysis of ordinary differential equations we classify all spherically symmetric selfsimilar solutions to the einstein equations which are asymptotically friedmann at large distances and contain a perfect fluid with equation of state pgamma 1mu with 0gamma23 this corresponds to a dark energy fl... | [['based', 'on', 'the', 'asymptotic', 'analysis', 'of', 'ordinary', 'differential', 'equations', 'we', 'classify', 'all', 'spherically', 'symmetric', 'selfsimilar', 'solutions', 'to', 'the', 'einstein', 'equations', 'which', 'are', 'asymptotically', 'friedmann', 'at', 'large', 'distances', 'and', 'contain', 'a', 'perfe... | [-0.16314627530953388, 0.09964334937758046, -0.09206338959153403, 0.07282308731049869, -0.06014947560459875, -0.15383024850378982, -0.022294833505878214, 0.32476911441596784, -0.23083736331750188, -0.2559334688717455, 0.09960286220887667, -0.3260201208452743, -0.0903588673723728, 0.1515102880833109, -0.0148129906175595... |
707.0529 | Realization of universal quantum cloning with SQUID qubits in a cavity | We propose a scheme to realize $1\to 2$ universal quantum cloning machine
(UQCM) with superconducting quantum interference device (SQUID) qubits, embeded
in a high-Q cavity. CNOT operations are derived to present our scheme, and the
two-photon Raman resonance processes are used to increase the operation rate.
Compare... | quant-ph | we propose a scheme to realize 1to 2 universal quantum cloning machine uqcm with superconducting quantum interference device squid qubits embeded in a highq cavity cnot operations are derived to present our scheme and the twophoton raman resonance processes are used to increase the operation rate compared with previous... | [['we', 'propose', 'a', 'scheme', 'to', 'realize', '1to', '2', 'universal', 'quantum', 'cloning', 'machine', 'uqcm', 'with', 'superconducting', 'quantum', 'interference', 'device', 'squid', 'qubits', 'embeded', 'in', 'a', 'highq', 'cavity', 'cnot', 'operations', 'are', 'derived', 'to', 'present', 'our', 'scheme', 'and'... | [-0.17255460436562778, 0.12455632685698935, -0.041963877370123005, -0.06862856935495969, -0.0038534763162253335, -0.28390764721409706, 0.1312494980930885, 0.46412737178997915, -0.21216334894177366, -0.26347491218418373, 0.003386303778646178, -0.23931327739302985, -0.13995908841979307, 0.27829009596808035, -0.0869501572... |
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