id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.053 | Self-similar cosmological solutions with dark energy. II: black holes,
naked singularities and wormholes | We use a combination of numerical and analytical methods, exploiting the
equations derived in a preceding paper, to classify all spherically symmetric
self-similar solutions which are asymptotically Friedmann at large distances
and contain a perfect fluid with equation of state $p=(\gamma -1)\mu$ with
$0<\gamma<2/3$.... | gr-qc astro-ph hep-th | we use a combination of numerical and analytical methods exploiting the equations derived in a preceding paper to classify all spherically symmetric selfsimilar solutions which are asymptotically friedmann at large distances and contain a perfect fluid with equation of state pgamma 1mu with 0gamma23 the expansion of th... | [['we', 'use', 'a', 'combination', 'of', 'numerical', 'and', 'analytical', 'methods', 'exploiting', 'the', 'equations', 'derived', 'in', 'a', 'preceding', 'paper', 'to', 'classify', 'all', 'spherically', 'symmetric', 'selfsimilar', 'solutions', 'which', 'are', 'asymptotically', 'friedmann', 'at', 'large', 'distances', ... | [-0.15614615224448797, 0.08949196822655142, -0.10233590553655138, 0.11074900215260122, -0.11011399742861033, -0.16509801179805364, -0.05498552215142519, 0.3233787697354883, -0.19599906979492923, -0.2566792276172831, 0.11223355018372476, -0.32209241876180944, -0.057404287413085224, 0.15939779039706473, -0.03640350362535... |
707.0531 | Construction of equilibrium networks with an energy function | We construct equilibrium networks by introducing an energy function depending
on the degree of each node as well as the product of neighboring degrees. With
this topological energy function, networks constitute a canonical ensemble,
which follows the Boltzmann distribution for given temperature. It is observed
that t... | cond-mat.stat-mech | we construct equilibrium networks by introducing an energy function depending on the degree of each node as well as the product of neighboring degrees with this topological energy function networks constitute a canonical ensemble which follows the boltzmann distribution for given temperature it is observed that the sys... | [['we', 'construct', 'equilibrium', 'networks', 'by', 'introducing', 'an', 'energy', 'function', 'depending', 'on', 'the', 'degree', 'of', 'each', 'node', 'as', 'well', 'as', 'the', 'product', 'of', 'neighboring', 'degrees', 'with', 'this', 'topological', 'energy', 'function', 'networks', 'constitute', 'a', 'canonical'... | [-0.13213380624505658, 0.1434777269962608, -0.07492029663235708, 0.03755474526594669, 0.0015634887817281265, -0.13261619437468686, 0.08831579367526704, 0.34251514863636756, -0.2874826878930132, -0.3089257500617317, 0.05281367461537701, -0.29906277918187835, -0.15784308508995715, 0.11175613631968628, 0.03408778257047137... |
707.0532 | A generalization of MacMahon's formula | We generalize the generating formula for plane partitions known as MacMahon's
formula as well as its analog for strict plane partitions. We give a
2-parameter generalization of these formulas related to Macdonald's symmetric
functions. The formula is especially simple in the Hall-Littlewood case. We
also give a bijec... | math.CO math-ph math.MP | we generalize the generating formula for plane partitions known as macmahons formula as well as its analog for strict plane partitions we give a 2parameter generalization of these formulas related to macdonalds symmetric functions the formula is especially simple in the halllittlewood case we also give a bijective proo... | [['we', 'generalize', 'the', 'generating', 'formula', 'for', 'plane', 'partitions', 'known', 'as', 'macmahons', 'formula', 'as', 'well', 'as', 'its', 'analog', 'for', 'strict', 'plane', 'partitions', 'we', 'give', 'a', '2parameter', 'generalization', 'of', 'these', 'formulas', 'related', 'to', 'macdonalds', 'symmetric'... | [-0.16246949177298506, 0.006483599527786344, -0.10033095978452998, 0.2058646559056242, -0.1706779139881985, -0.11314677351580585, 0.0835387341488721, 0.27765983264988003, -0.24060432745491045, -0.23339884502465946, 0.08972768739489365, -0.21744582161181053, -0.2347924959987907, 0.2912311339277332, -0.13384197967129927,... |
707.0533 | Super-elastic collisions in a thermally activated system | Impact phenomena of small clusters subject to thermal fluctuations are
numerically investigated. From the molecular dynamics simulation for colliding
two identical clusters, it is found that the restitution coefficient for
head-on collisions can exceed unity when the colliding speed is smaller than
the thermal veloci... | cond-mat.stat-mech | impact phenomena of small clusters subject to thermal fluctuations are numerically investigated from the molecular dynamics simulation for colliding two identical clusters it is found that the restitution coefficient for headon collisions can exceed unity when the colliding speed is smaller than the thermal velocity of... | [['impact', 'phenomena', 'of', 'small', 'clusters', 'subject', 'to', 'thermal', 'fluctuations', 'are', 'numerically', 'investigated', 'from', 'the', 'molecular', 'dynamics', 'simulation', 'for', 'colliding', 'two', 'identical', 'clusters', 'it', 'is', 'found', 'that', 'the', 'restitution', 'coefficient', 'for', 'headon... | [-0.1421259605664421, 0.23550458958783707, -0.12524828032965396, 0.08385906689618895, 0.01223205338087078, -0.0846704782845525, -0.02951717740317879, 0.32236639678768525, -0.2695195819553617, -0.2943365046536768, 0.020831682395746374, -0.30647095742744285, -0.09161217866296117, 0.2497422065058203, 0.04150838673405059, ... |
707.0534 | Anti-Hyperon polarization in high energy pp collisions with polarized
beams | We study the longitudinal polarization of the Sigma_bar and Xi_bar
anti-hyperons in polarized high energy pp collisions at large transverse
momenta, extending a recent study for the Lambda_bar anti-hyperon. We make
predictions by using different parametrizations of the polarized parton
densities and models for the po... | hep-ph | we study the longitudinal polarization of the sigma_bar and xi_bar antihyperons in polarized high energy pp collisions at large transverse momenta extending a recent study for the lambda_bar antihyperon we make predictions by using different parametrizations of the polarized parton densities and models for the polarize... | [['we', 'study', 'the', 'longitudinal', 'polarization', 'of', 'the', 'sigma_bar', 'and', 'xi_bar', 'antihyperons', 'in', 'polarized', 'high', 'energy', 'pp', 'collisions', 'at', 'large', 'transverse', 'momenta', 'extending', 'a', 'recent', 'study', 'for', 'the', 'lambda_bar', 'antihyperon', 'we', 'make', 'predictions',... | [-0.07997458828403876, 0.23878528725936632, -0.11968446776187153, 0.13633547936764995, -0.00044901058956813277, -0.03675050066072452, -0.013186756565936663, 0.4021290045393777, -0.23454798207607833, -0.22981179216444975, -0.06256110880659956, -0.3323722338157423, 0.03471560523520862, 0.12693143060451814, 0.092686381368... |
707.0535 | Measuring a Parity Violation Signature in the Early Universe via
Ground-based Laser Interferometers | We show that pairs of widely separated interferometers are advantageous for
measuring the Stokes parameter V of a stochastic background of gravitational
waves. This parameter characterizes asymmetry of amplitudes of right- and
left-handed waves and generation of the asymmetry is closely related to parity
violation in... | astro-ph gr-qc | we show that pairs of widely separated interferometers are advantageous for measuring the stokes parameter v of a stochastic background of gravitational waves this parameter characterizes asymmetry of amplitudes of right and lefthanded waves and generation of the asymmetry is closely related to parity violation in the ... | [['we', 'show', 'that', 'pairs', 'of', 'widely', 'separated', 'interferometers', 'are', 'advantageous', 'for', 'measuring', 'the', 'stokes', 'parameter', 'v', 'of', 'a', 'stochastic', 'background', 'of', 'gravitational', 'waves', 'this', 'parameter', 'characterizes', 'asymmetry', 'of', 'amplitudes', 'of', 'right', 'and... | [-0.17119304794644893, 0.2094200202047305, -0.04146954771195576, 0.10119622276532789, -0.04796306400148328, -0.12227786429291375, -0.033302585096206774, 0.3367575150156437, -0.2622008505602216, -0.28891815329620313, 0.05435984934609773, -0.2950633070539943, -0.06982203968800604, 0.19007962263665748, 0.02697157201378844... |
707.0536 | Adaptive FDR control under independence and dependence | In the context of multiple hypotheses testing, the proportion $\pi_0$ of true
null hypotheses in the pool of hypotheses to test often plays a crucial role,
although it is generally unknown a priori. A testing procedure using an
implicit or explicit estimate of this quantity in order to improve its
efficency is called... | math.ST stat.TH | in the context of multiple hypotheses testing the proportion pi_0 of true null hypotheses in the pool of hypotheses to test often plays a crucial role although it is generally unknown a priori a testing procedure using an implicit or explicit estimate of this quantity in order to improve its efficency is called adaptiv... | [['in', 'the', 'context', 'of', 'multiple', 'hypotheses', 'testing', 'the', 'proportion', 'pi_0', 'of', 'true', 'null', 'hypotheses', 'in', 'the', 'pool', 'of', 'hypotheses', 'to', 'test', 'often', 'plays', 'a', 'crucial', 'role', 'although', 'it', 'is', 'generally', 'unknown', 'a', 'priori', 'a', 'testing', 'procedure... | [-0.09368407998348854, 0.041074250551651884, -0.10258414539972056, 0.08785629674014062, -0.09024858308773165, -0.2034134641704341, 0.11714228701359937, 0.4036260833028177, -0.21038417640188922, -0.31317174018330907, 0.13963263709689214, -0.1720901140475382, -0.14223008926508132, 0.23009189958131307, -0.1269328978155063... |
707.0537 | Filtering the Wright-Fisher diffusion | We consider a Wright-Fisher diffusion (x(t)) whose current state cannot be
observed directly. Instead, at times t1 < t2 < . . ., the observations y(ti)
are such that, given the process (x(t)), the random variables (y(ti)) are
independent and the conditional distribution of y(ti) only depends on x(ti).
When this condi... | math.PR | we consider a wrightfisher diffusion xt whose current state cannot be observed directly instead at times t1 t2 the observations yti are such that given the process xt the random variables yti are independent and the conditional distribution of yti only depends on xti when this conditional distribution has a specific fo... | [['we', 'consider', 'a', 'wrightfisher', 'diffusion', 'xt', 'whose', 'current', 'state', 'can', 'not', 'be', 'observed', 'directly', 'instead', 'at', 'times', 't1', 't2', 'the', 'observations', 'yti', 'are', 'such', 'that', 'given', 'the', 'process', 'xt', 'the', 'random', 'variables', 'yti', 'are', 'independent', 'and... | [-0.08795791851906952, 0.1808977639387277, -0.08804181206505746, 0.08233756325268834, -0.04071165326220745, -0.16560498079369693, 0.014178513757757505, 0.39485051791098985, -0.30163850972259587, -0.23892645635218782, 0.10579082856420427, -0.28798237502236257, -0.07735337732910094, 0.1536559916397726, -0.066169234174727... |
707.0538 | Transformations of infinitely divisible distributions via improper
stochastic integrals | Let $X^{(\mu)}(ds)$ be an $\mathbb{R}^d$-valued homogeneous independently
scattered random measure over $\mathbb{R}$ having $\mu$ as the distribution of
$X^{(\mu)}((t,t+1])$. Let $f(s)$ be a nonrandom measurable function on an open
interval $(a,b)$ where $-\infty\leqslant a<b\leqslant\infty$. The improper
stochastic ... | math.PR | let xmuds be an mathbbrdvalued homogeneous independently scattered random measure over mathbbr having mu as the distribution of xmutt1 let fs be a nonrandom measurable function on an open interval ab where inftyleqslant ableqslantinfty the improper stochastic integral int_ab fsxmuds is studied its distribution phi_fmu ... | [['let', 'xmuds', 'be', 'an', 'mathbbrdvalued', 'homogeneous', 'independently', 'scattered', 'random', 'measure', 'over', 'mathbbr', 'having', 'mu', 'as', 'the', 'distribution', 'of', 'xmutt1', 'let', 'fs', 'be', 'a', 'nonrandom', 'measurable', 'function', 'on', 'an', 'open', 'interval', 'ab', 'where', 'inftyleqslant',... | [-0.13192919460407487, 0.17068282328490927, -0.07932784823545565, 0.08616760058088624, -0.03849840160656833, -0.14294135441058176, -0.021153862591635323, 0.402932829816233, -0.3170144222112316, -0.20195286338584442, 0.10464227932706391, -0.2623958101312658, -0.09582004360466574, 0.1953053619328068, -0.09325950148261407... |
707.0539 | Synchrotron Radiation Interferometer Calibration Check by Use of A Size
Control Bump in KEKB | In KEKB, synchrotron radiation interferometers (SRMs) are used for measuring
the transverse beam sizes. There is also a tool for enlarging the vertical beam
size intentionally by making an asymmetric bump, called an ``iSize'' bump, at
one of the strongest non-interleaved sextupole magnets in each KEKB ring. The
calib... | physics.acc-ph | in kekb synchrotron radiation interferometers srms are used for measuring the transverse beam sizes there is also a tool for enlarging the vertical beam size intentionally by making an asymmetric bump called an isize bump at one of the strongest noninterleaved sextupole magnets in each kekb ring the calibrations of the... | [['in', 'kekb', 'synchrotron', 'radiation', 'interferometers', 'srms', 'are', 'used', 'for', 'measuring', 'the', 'transverse', 'beam', 'sizes', 'there', 'is', 'also', 'a', 'tool', 'for', 'enlarging', 'the', 'vertical', 'beam', 'size', 'intentionally', 'by', 'making', 'an', 'asymmetric', 'bump', 'called', 'an', 'isize',... | [-0.07709663926689612, 0.12814489446581587, -0.05762614364820448, 0.07436094261503619, -0.012106723509578391, -0.1801272075943122, -0.028092974785132088, 0.44464774167216903, -0.19500551650281808, -0.295762196446609, 0.05565647550181232, -0.2914622764366519, 0.027422981336712837, 0.26014122209803325, -0.019289709564129... |
707.054 | How to project a bipartite network? | The one-mode projecting is extensively used to compress the bipartite
networks. Since the one-mode projection is always less informative than the
bipartite representation, a proper weighting method is required to better
retain the original information. In this article, inspired by the network-based
resource-allocatio... | physics.soc-ph physics.data-an | the onemode projecting is extensively used to compress the bipartite networks since the onemode projection is always less informative than the bipartite representation a proper weighting method is required to better retain the original information in this article inspired by the networkbased resourceallocation dynamics... | [['the', 'onemode', 'projecting', 'is', 'extensively', 'used', 'to', 'compress', 'the', 'bipartite', 'networks', 'since', 'the', 'onemode', 'projection', 'is', 'always', 'less', 'informative', 'than', 'the', 'bipartite', 'representation', 'a', 'proper', 'weighting', 'method', 'is', 'required', 'to', 'better', 'retain',... | [-0.008443500782180178, 0.018178010209729627, -0.1165128835730554, 0.10463982205692446, -0.1337763032310509, -0.18048707204122497, 0.018149659418018667, 0.402072527013453, -0.2904305316582655, -0.32100525038549677, 0.08882485806056398, -0.2534333881298413, -0.22072056403184043, 0.18362404079380212, -0.10291467930489619... |
707.0541 | The 3.3 $\mu$m PAH emission band of the Red Rectangle | A new analysis of long-slit CGS4 (UKIRT) spectra of the 3.3 $\mu$m feature of
the Red Rectangle and its evolution with offset along the NW whisker of the
nebula is presented. The results support a proposed two-component
interpretation for the 3.3 $\mu$m feature with peak wavelengths near 3.28
$\mu$m and 3.30 $\mu$m. ... | astro-ph | a new analysis of longslit cgs4 ukirt spectra of the 33 mum feature of the red rectangle and its evolution with offset along the nw whisker of the nebula is presented the results support a proposed twocomponent interpretation for the 33 mum feature with peak wavelengths near 328 mum and 330 mum both components exhibit ... | [['a', 'new', 'analysis', 'of', 'longslit', 'cgs4', 'ukirt', 'spectra', 'of', 'the', '33', 'mum', 'feature', 'of', 'the', 'red', 'rectangle', 'and', 'its', 'evolution', 'with', 'offset', 'along', 'the', 'nw', 'whisker', 'of', 'the', 'nebula', 'is', 'presented', 'the', 'results', 'support', 'a', 'proposed', 'twocomponen... | [-0.04099061827183561, 0.07783799087659629, -0.06757057564893523, -0.0279761250635642, -0.051682136005070885, -0.12728931292875018, 0.052853684118264806, 0.43145528577465925, -0.1795516263495768, -0.30371450527315647, 0.0716723072799994, -0.3161214383368471, -0.03498297507371918, 0.16488330696701212, -0.027599635904869... |
707.0542 | Elemental abundances of Galactic bulge planetary nebulae from optical
recombination lines | (abridged) Deep long-slit optical spectrophotometric observations are
presented for 25 Galactic bulge planetary nebulae (GBPNe) and 6 Galactic disk
planetary nebulae (GDPNe). The spectra, combined with archival ultraviolet
spectra obtained with the International Ultraviolet Explorer (IUE) and infrared
spectra obtaine... | astro-ph | abridged deep longslit optical spectrophotometric observations are presented for 25 galactic bulge planetary nebulae gbpne and 6 galactic disk planetary nebulae gdpne the spectra combined with archival ultraviolet spectra obtained with the international ultraviolet explorer iue and infrared spectra obtained with the in... | [['abridged', 'deep', 'longslit', 'optical', 'spectrophotometric', 'observations', 'are', 'presented', 'for', '25', 'galactic', 'bulge', 'planetary', 'nebulae', 'gbpne', 'and', '6', 'galactic', 'disk', 'planetary', 'nebulae', 'gdpne', 'the', 'spectra', 'combined', 'with', 'archival', 'ultraviolet', 'spectra', 'obtained... | [0.0353467360506823, 0.15644375087670337, -0.024519893716361544, 0.08111888181788027, -0.029568688447660012, -0.14052385269422774, 0.04455856988091528, 0.4500943658252557, -0.18701732590403639, -0.34270956873924396, 0.037747595075004324, -0.3382773103600621, 0.00818753014749214, 0.22403109107557453, -0.0133622288905728... |
707.0543 | Cosmological perturbations from inhomogeneous preheating and multi-field
trapping | We consider inhomogeneous preheating in a multi-field trapping model. The
curvature perturbation is generated by inhomogeneous preheating which induces
multi-field trapping at the enhanced symmetric point (ESP), and results in
fluctuation in the number of e-foldings. Instead of considering simple
reheating after preh... | hep-th astro-ph hep-ph | we consider inhomogeneous preheating in a multifield trapping model the curvature perturbation is generated by inhomogeneous preheating which induces multifield trapping at the enhanced symmetric point esp and results in fluctuation in the number of efoldings instead of considering simple reheating after preheating we ... | [['we', 'consider', 'inhomogeneous', 'preheating', 'in', 'a', 'multifield', 'trapping', 'model', 'the', 'curvature', 'perturbation', 'is', 'generated', 'by', 'inhomogeneous', 'preheating', 'which', 'induces', 'multifield', 'trapping', 'at', 'the', 'enhanced', 'symmetric', 'point', 'esp', 'and', 'results', 'in', 'fluctu... | [-0.17999211412977303, 0.2423915950905891, -0.10417260547363005, 0.12917144087627452, -0.06640360352537175, -0.1710923062215283, -0.023177622573112476, 0.34139954537194184, -0.2404029798044076, -0.26954025010435056, 0.08649900571793666, -0.2204799836611498, -0.12872237333219375, 0.14519092004303566, -0.0509988480454802... |
707.0544 | A catalogue of low-mass X-ray binaries in the Galaxy, LMC, and SMC
(Fourth edition) | We present a new edition of the catalogue of the low-mass X-ray binaries in
the Galaxy and the Magellanic Clouds. The catalogue contains source name(s),
coordinates, finding chart, X-ray luminosity, system parameters, and stellar
parameters of the components and other characteristic properties of 187
low-mass X-ray b... | astro-ph | we present a new edition of the catalogue of the lowmass xray binaries in the galaxy and the magellanic clouds the catalogue contains source names coordinates finding chart xray luminosity system parameters and stellar parameters of the components and other characteristic properties of 187 lowmass xray binaries togethe... | [['we', 'present', 'a', 'new', 'edition', 'of', 'the', 'catalogue', 'of', 'the', 'lowmass', 'xray', 'binaries', 'in', 'the', 'galaxy', 'and', 'the', 'magellanic', 'clouds', 'the', 'catalogue', 'contains', 'source', 'names', 'coordinates', 'finding', 'chart', 'xray', 'luminosity', 'system', 'parameters', 'and', 'stellar... | [-0.07570651058043984, 0.07689501921196544, -0.05983576824113449, 0.1294465914024445, -0.1661229242428975, -0.051060553611204124, 0.10174072737319638, 0.45258289596401385, -0.16913726331842543, -0.36757683568859695, 0.09304880598554191, -0.35510690466020695, -0.03409788262110597, 0.24424834092442663, -0.046422232325645... |
707.0545 | Relativistic Collisionless Shocks in Unmagnetized Electron-Positron
Plasmas | It is shown that collisionless shock waves can be driven in unmagnetized
electron-positron plasmas by performing a two-dimensional particle-in-cell
simulation. At the shock transition region, strong magnetic fields are
generated by a Weibel-like instability. The generated magnetic fields are
strong enough to deflect ... | astro-ph | it is shown that collisionless shock waves can be driven in unmagnetized electronpositron plasmas by performing a twodimensional particleincell simulation at the shock transition region strong magnetic fields are generated by a weibellike instability the generated magnetic fields are strong enough to deflect the incomi... | [['it', 'is', 'shown', 'that', 'collisionless', 'shock', 'waves', 'can', 'be', 'driven', 'in', 'unmagnetized', 'electronpositron', 'plasmas', 'by', 'performing', 'a', 'twodimensional', 'particleincell', 'simulation', 'at', 'the', 'shock', 'transition', 'region', 'strong', 'magnetic', 'fields', 'are', 'generated', 'by',... | [-0.1800451950427832, 0.26872871679027893, -0.02470523620243458, 0.09345122579271023, -0.06115523402773362, -0.050978571081902575, -0.03542728549277878, 0.37900462718730304, -0.3005541717175414, -0.28118167983437764, 0.03593035786410166, -0.2635779393398586, -0.030397801523042077, 0.22019165224410633, 0.134211488703563... |
707.0546 | Weighted Popular Matchings | We study the problem of assigning jobs to applicants. Each applicant has a
weight and provides a preference list ranking a subset of the jobs. A matching
M is popular if there is no other matching M' such that the weight of the
applicants who prefer M' over M exceeds the weight of those who prefer M over
M'. This pap... | cs.DS | we study the problem of assigning jobs to applicants each applicant has a weight and provides a preference list ranking a subset of the jobs a matching m is popular if there is no other matching m such that the weight of the applicants who prefer m over m exceeds the weight of those who prefer m over m this paper gives... | [['we', 'study', 'the', 'problem', 'of', 'assigning', 'jobs', 'to', 'applicants', 'each', 'applicant', 'has', 'a', 'weight', 'and', 'provides', 'a', 'preference', 'list', 'ranking', 'a', 'subset', 'of', 'the', 'jobs', 'a', 'matching', 'm', 'is', 'popular', 'if', 'there', 'is', 'no', 'other', 'matching', 'm', 'such', 't... | [-0.17456466515755487, 0.05573118346122404, -0.07334325845456785, 0.014412674970420388, -0.16375279035936627, -0.21802768753776844, 0.1446948771820947, 0.418638229318377, -0.19485621982150608, -0.3662861409700579, 0.0270344301372663, -0.34836978607604074, -0.07524300784441745, 0.099395124170567, -0.08476197288190532, -... |
707.0547 | A local ring such that the map between Grothendieck groups with rational
coefficient induced by completion is not injective | In this paper, we construct a local ring $A$ such that the kernel of the map
$G_0(A)\subq \to G_0(\hat{A})\subq$ is not zero, where $\hat{A}$ is the
comletion of $A$ with respect to the maximal ideal, and $G_0()\subq$ is the
Grothendieck group of finitely generated modules with rational coefficient. In
our example, $... | math.AC math.KT | in this paper we construct a local ring a such that the kernel of the map g_0asubq to g_0hatasubq is not zero where hata is the comletion of a with respect to the maximal ideal and g_0subq is the grothendieck group of finitely generated modules with rational coefficient in our example a is a twodimensional local ring w... | [['in', 'this', 'paper', 'we', 'construct', 'a', 'local', 'ring', 'a', 'such', 'that', 'the', 'kernel', 'of', 'the', 'map', 'g_0asubq', 'to', 'g_0hatasubq', 'is', 'not', 'zero', 'where', 'hata', 'is', 'the', 'comletion', 'of', 'a', 'with', 'respect', 'to', 'the', 'maximal', 'ideal', 'and', 'g_0subq', 'is', 'the', 'grot... | [-0.14836727143543313, 0.07540108688842895, -0.10057116864221309, -0.03313960647731742, -0.07166374005627499, -0.12916295774586833, -0.04921414629632691, 0.3492483641785472, -0.35828946024846675, -0.1412979509488596, 0.12873705754876694, -0.2536617108245394, -0.13881102553221272, 0.2137904304510622, -0.0811878874300242... |
707.0548 | From Royal Road to Epistatic Road for Variable Length Evolution
Algorithm | Although there are some real world applications where the use of variable
length representation (VLR) in Evolutionary Algorithm is natural and suitable,
an academic framework is lacking for such representations. In this work we
propose a family of tunable fitness landscapes based on VLR of genotypes. The
fitness land... | cs.NE | although there are some real world applications where the use of variable length representation vlr in evolutionary algorithm is natural and suitable an academic framework is lacking for such representations in this work we propose a family of tunable fitness landscapes based on vlr of genotypes the fitness landscapes ... | [['although', 'there', 'are', 'some', 'real', 'world', 'applications', 'where', 'the', 'use', 'of', 'variable', 'length', 'representation', 'vlr', 'in', 'evolutionary', 'algorithm', 'is', 'natural', 'and', 'suitable', 'an', 'academic', 'framework', 'is', 'lacking', 'for', 'such', 'representations', 'in', 'this', 'work'... | [-0.07151305320089212, 0.1172198358403711, -0.11289722319265985, 0.11570912231873519, -0.06493709486886769, -0.1560963064906221, 0.08049234626983034, 0.4202166012241449, -0.24915377066066735, -0.31745492021766414, 0.037011502832398714, -0.27237931074552146, -0.2437458276203048, 0.1559138100324984, -0.07541123967819724,... |
707.0549 | Catalogue of high-mass X-ray binaries in the Galaxy ($4^{th}$ edition) | We present a new edition of the catalogue of high-mass X-ray binaries in the
Galaxy. The catalogue contains source name(s), coordinates, finding chart,
X-ray luminosity, system parameters, and stellar parameters of the components
and other characteristic properties of 114 high-mass X-ray binaries, together
with a com... | astro-ph | we present a new edition of the catalogue of highmass xray binaries in the galaxy the catalogue contains source names coordinates finding chart xray luminosity system parameters and stellar parameters of the components and other characteristic properties of 114 highmass xray binaries together with a comprehensive selec... | [['we', 'present', 'a', 'new', 'edition', 'of', 'the', 'catalogue', 'of', 'highmass', 'xray', 'binaries', 'in', 'the', 'galaxy', 'the', 'catalogue', 'contains', 'source', 'names', 'coordinates', 'finding', 'chart', 'xray', 'luminosity', 'system', 'parameters', 'and', 'stellar', 'parameters', 'of', 'the', 'components', ... | [-0.08641763140361304, 0.08380818039594713, -0.0443163234848163, 0.13912871848883354, -0.17135085975832032, -0.07597332525287749, 0.10139415323642766, 0.4613199047313605, -0.14992534164931473, -0.3762146866735006, 0.09427872663256147, -0.3627602816747792, -0.025216905135026127, 0.2452221305198386, -0.03541624845500842,... |
707.055 | Blending in Gravitational Microlensing Experiments: Source Confusion And
Related Systematics | Gravitational microlensing surveys target very dense stellar fields in the
local group. As a consequence the microlensed source stars are often blended
with nearby unresolved stars. The presence of `blending' is a cause of major
uncertainty when determining the lensing properties of events towards the
Galactic centre... | astro-ph | gravitational microlensing surveys target very dense stellar fields in the local group as a consequence the microlensed source stars are often blended with nearby unresolved stars the presence of blending is a cause of major uncertainty when determining the lensing properties of events towards the galactic centre after... | [['gravitational', 'microlensing', 'surveys', 'target', 'very', 'dense', 'stellar', 'fields', 'in', 'the', 'local', 'group', 'as', 'a', 'consequence', 'the', 'microlensed', 'source', 'stars', 'are', 'often', 'blended', 'with', 'nearby', 'unresolved', 'stars', 'the', 'presence', 'of', 'blending', 'is', 'a', 'cause', 'of... | [-0.05765302240278275, 0.08419567752602945, -0.10097385350230109, 0.12996032071110886, -0.11320782293383357, -0.0468329924168875, 0.04803933097940424, 0.43041580191314005, -0.20155964795486542, -0.3584429634654004, 0.04680884846754413, -0.30158708977809956, -0.04848216631638723, 0.20116746161585214, -0.0657334651199944... |
707.0551 | Scanning tunneling spectroscopy characterization of the pseudogap and
the x = 1/8 anomaly in La2-xSrxCuO4 thin films | Using scanning tunneling spectroscopy we examined the local density of states
of thin c-axis La2-xSrxCuO4 films, over wide doping and temperature ranges. We
found that the pseudogap exists only at doping levels lower than optimal. For x
= 0.12, close to the 'anomalous' x = 1/8 doping level, a zero bias conductance
pe... | cond-mat.supr-con cond-mat.str-el | using scanning tunneling spectroscopy we examined the local density of states of thin caxis la2xsrxcuo4 films over wide doping and temperature ranges we found that the pseudogap exists only at doping levels lower than optimal for x 012 close to the anomalous x 18 doping level a zero bias conductance peak was the domina... | [['using', 'scanning', 'tunneling', 'spectroscopy', 'we', 'examined', 'the', 'local', 'density', 'of', 'states', 'of', 'thin', 'caxis', 'la2xsrxcuo4', 'films', 'over', 'wide', 'doping', 'and', 'temperature', 'ranges', 'we', 'found', 'that', 'the', 'pseudogap', 'exists', 'only', 'at', 'doping', 'levels', 'lower', 'than'... | [-0.17853912490730484, 0.1689714072213974, -0.06529772346321908, 0.06803192667818318, -0.02022416903119948, -0.18292170210948422, 0.15016881243532731, 0.4481946211722162, -0.2888142462302413, -0.274919453346067, -0.0433000613476098, -0.31827607660864793, -0.08329184904901518, 0.18227793303214843, 0.005372578842151496, ... |
707.0552 | AdS$_5$ rotating non-Abelian black holes | We present arguments for the existence of charged, rotating black holes with
equal magnitude angular momenta in $d=5$ Einstein-Yang-Mills theory with
negative cosmological constant. These solutions posses a regular horizon of
spherical topology and approach asymptotically the Anti-de Sitter spacetime
background. The ... | hep-th | we present arguments for the existence of charged rotating black holes with equal magnitude angular momenta in d5 einsteinyangmills theory with negative cosmological constant these solutions posses a regular horizon of spherical topology and approach asymptotically the antide sitter spacetime background the black hole ... | [['we', 'present', 'arguments', 'for', 'the', 'existence', 'of', 'charged', 'rotating', 'black', 'holes', 'with', 'equal', 'magnitude', 'angular', 'momenta', 'in', 'd5', 'einsteinyangmills', 'theory', 'with', 'negative', 'cosmological', 'constant', 'these', 'solutions', 'posses', 'a', 'regular', 'horizon', 'of', 'spher... | [-0.20360727469367837, 0.15349170341559565, -0.06508973832414658, 0.12221655181902288, -0.08834661152443768, -0.1608070622968637, -0.04379125685505799, 0.3006798713985417, -0.0955365961647512, -0.27543562209164657, 0.09424635244067758, -0.3437716280696569, -0.03818938809297519, 0.12578957927999673, 0.001776880509202817... |
707.0553 | Relativistic five-quark equations and a narrow N(1688) resonance | The relativistic five-quark equations are found in the framework of the
dispersion relation technique. The five-quark amplitude for the N(1688)
resonance including u-, d- quarks is calculated. The pole of this amplitude
determines the mass of non-strange pentaquark M=1686 MeV and the width about
7MeV. The results are... | hep-ph | the relativistic fivequark equations are found in the framework of the dispersion relation technique the fivequark amplitude for the n1688 resonance including u d quarks is calculated the pole of this amplitude determines the mass of nonstrange pentaquark m1686 mev and the width about 7mev the results are in good agree... | [['the', 'relativistic', 'fivequark', 'equations', 'are', 'found', 'in', 'the', 'framework', 'of', 'the', 'dispersion', 'relation', 'technique', 'the', 'fivequark', 'amplitude', 'for', 'the', 'n1688', 'resonance', 'including', 'u', 'd', 'quarks', 'is', 'calculated', 'the', 'pole', 'of', 'this', 'amplitude', 'determines... | [-0.13791303596060192, 0.18251135074699829, -0.08058457153882566, 0.15857744341649646, -0.04327256244817233, -0.07912122630347897, 0.03463812460125025, 0.33838776332725373, -0.14898624098194496, -0.28829539753496647, -0.05298939984641038, -0.31699309863948394, -0.02975260010654373, 0.14754099947666482, 0.10779157605221... |
707.0554 | Natural octonionic generalization of general relativity | An intriguingly natural generalization, using complex octonions, of general
relativity is pointed out. The starting point is the vierbein-based double dual
formulation of the Einstein-Hilbert action. In terms of two natural structures
on the (complex) quaternions and (complex) octonions, the inner product and the
cro... | math-ph math.MP | an intriguingly natural generalization using complex octonions of general relativity is pointed out the starting point is the vierbeinbased double dual formulation of the einsteinhilbert action in terms of two natural structures on the complex quaternions and complex octonions the inner product and the cross products r... | [['an', 'intriguingly', 'natural', 'generalization', 'using', 'complex', 'octonions', 'of', 'general', 'relativity', 'is', 'pointed', 'out', 'the', 'starting', 'point', 'is', 'the', 'vierbeinbased', 'double', 'dual', 'formulation', 'of', 'the', 'einsteinhilbert', 'action', 'in', 'terms', 'of', 'two', 'natural', 'struct... | [-0.13744095648625787, 0.07479828812262293, -0.037386744899649015, 0.07678916362035547, -0.12159663719505491, -0.04547260683292235, -0.0378263545498042, 0.3335587869162186, -0.33215807569803485, -0.2169339104972019, 0.05969003844730766, -0.22357162566934252, -0.26186078702899773, 0.1836899796264692, -0.0602247415267875... |
707.0555 | Multiplicative renormalization and Hopf algebras | We derive the existence of Hopf subalgebras generated by Green's functions in
the Hopf algebra of Feynman graphs of a quantum field theory. This means that
the coproduct closes on these Green's functions. It allows us for example to
derive Dyson's formulas in quantum electrodynamics relating the renormalized
and bare... | hep-th | we derive the existence of hopf subalgebras generated by greens functions in the hopf algebra of feynman graphs of a quantum field theory this means that the coproduct closes on these greens functions it allows us for example to derive dysons formulas in quantum electrodynamics relating the renormalized and bare proper... | [['we', 'derive', 'the', 'existence', 'of', 'hopf', 'subalgebras', 'generated', 'by', 'greens', 'functions', 'in', 'the', 'hopf', 'algebra', 'of', 'feynman', 'graphs', 'of', 'a', 'quantum', 'field', 'theory', 'this', 'means', 'that', 'the', 'coproduct', 'closes', 'on', 'these', 'greens', 'functions', 'it', 'allows', 'u... | [-0.16360730830732698, 0.14804489441917507, -0.1066267333271635, 0.12248684061757688, -0.12462583714007557, -0.09512778918875696, 0.0414871061651653, 0.32074881184168835, -0.24531998654053389, -0.21025587446600585, 0.030722128059533605, -0.23221376197516175, -0.21762388036283967, 0.20095789756069515, 0.0010861642193805... |
707.0556 | Determinacy in a synchronous pi-calculus | The S-pi-calculus is a synchronous pi-calculus which is based on the SL
model. The latter is a relaxation of the Esterel model where the reaction to
the absence of a signal within an instant can only happen at the next instant.
In the present work, we present and characterise a compositional semantics of
the S-pi-cal... | cs.LO | the spicalculus is a synchronous picalculus which is based on the sl model the latter is a relaxation of the esterel model where the reaction to the absence of a signal within an instant can only happen at the next instant in the present work we present and characterise a compositional semantics of the spicalculus base... | [['the', 'spicalculus', 'is', 'a', 'synchronous', 'picalculus', 'which', 'is', 'based', 'on', 'the', 'sl', 'model', 'the', 'latter', 'is', 'a', 'relaxation', 'of', 'the', 'esterel', 'model', 'where', 'the', 'reaction', 'to', 'the', 'absence', 'of', 'a', 'signal', 'within', 'an', 'instant', 'can', 'only', 'happen', 'at'... | [-0.13470598238419337, 0.07020577451327104, -0.09917715079388133, 0.05528760258478662, -0.0809548143016915, -0.10170930864132312, 0.0779401361044631, 0.3236115799251809, -0.30511935896251396, -0.24827230988766055, 0.08072341015107974, -0.2120145214609353, -0.1272479670111045, 0.12393216286640031, -0.050760645467047415,... |
707.0557 | Hyperfine-mediated gate-driven electron spin resonance | An all-electrical spin resonance effect in a GaAs few-electron double quantum
dot is investigated experimentally and theoretically. The magnetic field
dependence and absence of associated Rabi oscillations are consistent with a
novel hyperfine mechanism. The resonant frequency is sensitive to the
instantaneous hyperf... | cond-mat.mes-hall | an allelectrical spin resonance effect in a gaas fewelectron double quantum dot is investigated experimentally and theoretically the magnetic field dependence and absence of associated rabi oscillations are consistent with a novel hyperfine mechanism the resonant frequency is sensitive to the instantaneous hyperfine ef... | [['an', 'allelectrical', 'spin', 'resonance', 'effect', 'in', 'a', 'gaas', 'fewelectron', 'double', 'quantum', 'dot', 'is', 'investigated', 'experimentally', 'and', 'theoretically', 'the', 'magnetic', 'field', 'dependence', 'and', 'absence', 'of', 'associated', 'rabi', 'oscillations', 'are', 'consistent', 'with', 'a', ... | [-0.1828393628205544, 0.2389244759955246, -0.006870171573909023, 0.07798689295231259, -0.05900314741449643, -0.21712524966702243, 0.04076442624666268, 0.4390104951077624, -0.2603506982750908, -0.3217481477068195, -0.04137294062507586, -0.22990750691181497, -0.06470039819921308, 0.2275644484200055, 0.04601422775112375, ... |
707.0558 | Verification of the Effectiveness of VSOP-2 Phase Referencing with a
Newly Developed Simulation Tool, ARIS | The next-generation space VLBI mission, VSOP-2, is expected to provide
unprecedented spatial resolutions at 8.4, 22, and 43GHz. In this report, phase
referencing with VSOP-2 is examined in detail based on a simulation tool called
ARIS. The criterion for successful phase referencing was to keep the phase
errors below ... | astro-ph | the nextgeneration space vlbi mission vsop2 is expected to provide unprecedented spatial resolutions at 84 22 and 43ghz in this report phase referencing with vsop2 is examined in detail based on a simulation tool called aris the criterion for successful phase referencing was to keep the phase errors below one radian si... | [['the', 'nextgeneration', 'space', 'vlbi', 'mission', 'vsop2', 'is', 'expected', 'to', 'provide', 'unprecedented', 'spatial', 'resolutions', 'at', '84', '22', 'and', '43ghz', 'in', 'this', 'report', 'phase', 'referencing', 'with', 'vsop2', 'is', 'examined', 'in', 'detail', 'based', 'on', 'a', 'simulation', 'tool', 'ca... | [-0.09761703205193677, 0.11437159307309269, -0.06710783704740765, 0.05407632007130735, -0.06266819922324351, -0.1397228188503979, 0.08825166577615005, 0.4428301175610851, -0.15811886146421666, -0.38412050600669795, 0.1712639009144724, -0.2598018370968614, -0.046123315456181604, 0.23761374997759602, -0.07034265884178002... |
707.0559 | Diffusive transport in graphene: the role of interband correlation | We present a kinetic equation approach to investigate dc transport properties
of graphene in the diffusive regime considering long-range electron-impurity
scattering. In our study, the effects of interband correlation (or
polarization) on conductivity are taken into account. We find that the
conductivity contains not... | cond-mat.mtrl-sci | we present a kinetic equation approach to investigate dc transport properties of graphene in the diffusive regime considering longrange electronimpurity scattering in our study the effects of interband correlation or polarization on conductivity are taken into account we find that the conductivity contains not only the... | [['we', 'present', 'a', 'kinetic', 'equation', 'approach', 'to', 'investigate', 'dc', 'transport', 'properties', 'of', 'graphene', 'in', 'the', 'diffusive', 'regime', 'considering', 'longrange', 'electronimpurity', 'scattering', 'in', 'our', 'study', 'the', 'effects', 'of', 'interband', 'correlation', 'or', 'polarizati... | [-0.15618065331520312, 0.23002382824496262, -0.026923423908000826, 0.037699462804512036, 0.008267087208719662, -0.15292098322858247, 0.03248859901565608, 0.3269582961845343, -0.24937853509647734, -0.2820732052025429, -0.006827315269506868, -0.39801950851492834, -0.0983632161616404, 0.13536957166182664, 0.03222041077061... |
707.056 | Percolation and Loop Statistics in Complex Networks | Complex networks display various types of percolation transitions. We show
that the degree distribution and the degree-degree correlation alone are not
sufficient to describe diverse percolation critical phenomena. This suggests
that a genuine structural correlation is an essential ingredient in
characterizing networ... | cond-mat.stat-mech | complex networks display various types of percolation transitions we show that the degree distribution and the degreedegree correlation alone are not sufficient to describe diverse percolation critical phenomena this suggests that a genuine structural correlation is an essential ingredient in characterizing networks as... | [['complex', 'networks', 'display', 'various', 'types', 'of', 'percolation', 'transitions', 'we', 'show', 'that', 'the', 'degree', 'distribution', 'and', 'the', 'degreedegree', 'correlation', 'alone', 'are', 'not', 'sufficient', 'to', 'describe', 'diverse', 'percolation', 'critical', 'phenomena', 'this', 'suggests', 't... | [-0.16039729170678627, 0.15749345211481255, -0.06152594280207441, 0.09814169822327261, -0.010039518010758218, -0.1526036556455351, 0.012249384653044953, 0.38916648605040144, -0.242755111209893, -0.28664737448284755, 0.04205266919120082, -0.2945307710873229, -0.19754476299110268, 0.13617499571825778, -0.0020136016344795... |
707.0561 | Stellar Population Gradients in Bulges along the Hubble Sequence: II.
Relations with Galaxy Properties | We present the analysis of the radial gradients of stellar absorption lines
in a sample of 32 bulges of edge-on spiral galaxies, spanning nearly the full
Hubble sequence (from S0 to Sc types), and a large range of velocity dispersion
(from about 60 to 300 km/s). Different diagnostics such as index-index,
gradient-gra... | astro-ph | we present the analysis of the radial gradients of stellar absorption lines in a sample of 32 bulges of edgeon spiral galaxies spanning nearly the full hubble sequence from s0 to sc types and a large range of velocity dispersion from about 60 to 300 kms different diagnostics such as indexindex gradientgradient diagrams... | [['we', 'present', 'the', 'analysis', 'of', 'the', 'radial', 'gradients', 'of', 'stellar', 'absorption', 'lines', 'in', 'a', 'sample', 'of', '32', 'bulges', 'of', 'edgeon', 'spiral', 'galaxies', 'spanning', 'nearly', 'the', 'full', 'hubble', 'sequence', 'from', 's0', 'to', 'sc', 'types', 'and', 'a', 'large', 'range', '... | [-0.06309810347221274, 0.10220315773557458, -0.09794467678034885, 0.13048196271281792, -0.0805998909765751, -0.03531208539174663, 0.02640794271331591, 0.43577295791926896, -0.18434578609756297, -0.38677882626652715, 0.014502557337335829, -0.26455727586936617, -0.016070098652400906, 0.20008546579629183, -0.0423877024790... |
707.0562 | On a Non-Context-Free Extension of PDL | Over the last 25 years, a lot of work has been done on seeking for decidable
non-regular extensions of Propositional Dynamic Logic (PDL). Only recently, an
expressive extension of PDL, allowing visibly pushdown automata (VPAs) as a
formalism to describe programs, was introduced and proven to have a
satisfiability pro... | cs.LO | over the last 25 years a lot of work has been done on seeking for decidable nonregular extensions of propositional dynamic logic pdl only recently an expressive extension of pdl allowing visibly pushdown automata vpas as a formalism to describe programs was introduced and proven to have a satisfiability problem complet... | [['over', 'the', 'last', '25', 'years', 'a', 'lot', 'of', 'work', 'has', 'been', 'done', 'on', 'seeking', 'for', 'decidable', 'nonregular', 'extensions', 'of', 'propositional', 'dynamic', 'logic', 'pdl', 'only', 'recently', 'an', 'expressive', 'extension', 'of', 'pdl', 'allowing', 'visibly', 'pushdown', 'automata', 'vp... | [-0.07020911833367159, 0.06851476573326265, -0.09023002336620756, 0.1467030837129577, -0.17193421665314876, -0.20528998298583723, 0.056322791531899986, 0.38937058257507096, -0.2961349022006682, -0.28572135501217544, 0.0918414564605089, -0.21817039444725564, -0.08994993573163655, 0.17893119391172807, -0.1380031769484255... |
707.0563 | Role of oxygen vacancies in Cr-doped SrTiO3 for resistance-change memory | Transition-metal oxides exhibiting a bistable resistance state are attractive
for non-volatile memory applications. The relevance of oxygen vacancies (VO)
for the resistance-change memory was investigated with x-ray fluorescence,
infrared microscopy, and x-ray absorption spectroscopy using Cr-doped SrTiO3 as
example.... | cond-mat.mtrl-sci cond-mat.str-el | transitionmetal oxides exhibiting a bistable resistance state are attractive for nonvolatile memory applications the relevance of oxygen vacancies vo for the resistancechange memory was investigated with xray fluorescence infrared microscopy and xray absorption spectroscopy using crdoped srtio3 as example we propose th... | [['transitionmetal', 'oxides', 'exhibiting', 'a', 'bistable', 'resistance', 'state', 'are', 'attractive', 'for', 'nonvolatile', 'memory', 'applications', 'the', 'relevance', 'of', 'oxygen', 'vacancies', 'vo', 'for', 'the', 'resistancechange', 'memory', 'was', 'investigated', 'with', 'xray', 'fluorescence', 'infrared', ... | [-0.11839419280124061, 0.14951772440883146, 0.034167313153910285, 0.023891887391287395, -0.019759575233739966, -0.18786330050651862, 0.12004173975626198, 0.48801410274908824, -0.27614955547923115, -0.26245075613534186, 0.021618427256779635, -0.3556429984267144, -0.1815106658374562, 0.1951805811806801, -0.04082234881763... |
707.0564 | Predictions for the LHC heavy ion programme | Apparently universal trends have been observed in relativistic
nucleus-nucleus collisions up to RHIC energies. Here, we review these trends
and we discuss their agnostic extrapolation to heavy ion collisions at the LHC.
| hep-ph nucl-ex nucl-th | apparently universal trends have been observed in relativistic nucleusnucleus collisions up to rhic energies here we review these trends and we discuss their agnostic extrapolation to heavy ion collisions at the lhc | [['apparently', 'universal', 'trends', 'have', 'been', 'observed', 'in', 'relativistic', 'nucleusnucleus', 'collisions', 'up', 'to', 'rhic', 'energies', 'here', 'we', 'review', 'these', 'trends', 'and', 'we', 'discuss', 'their', 'agnostic', 'extrapolation', 'to', 'heavy', 'ion', 'collisions', 'at', 'the', 'lhc']] | [0.0010135502670891583, 0.269624462001957, -0.2030391388834687, 0.2047403242904693, -0.00026818783953785896, -0.13658805846353061, -0.07110783559619449, 0.46305985655635595, -0.21747262605640572, -0.29800096567487344, -0.07473142059825477, -0.37402792923967354, 0.1008938369632233, 0.1135572497951216, 0.0364644958899589... |
707.0565 | Uninformative memories will prevail: the storage of correlated
representations and its consequences | Autoassociative networks were proposed in the 80's as simplified models of
memory function in the brain, using recurrent connectivity with hebbian
plasticity to store patterns of neural activity that can be later recalled.
This type of computation has been suggested to take place in the CA3 region of
the hippocampus ... | cond-mat.dis-nn cond-mat.other | autoassociative networks were proposed in the 80s as simplified models of memory function in the brain using recurrent connectivity with hebbian plasticity to store patterns of neural activity that can be later recalled this type of computation has been suggested to take place in the ca3 region of the hippocampus and a... | [['autoassociative', 'networks', 'were', 'proposed', 'in', 'the', '80s', 'as', 'simplified', 'models', 'of', 'memory', 'function', 'in', 'the', 'brain', 'using', 'recurrent', 'connectivity', 'with', 'hebbian', 'plasticity', 'to', 'store', 'patterns', 'of', 'neural', 'activity', 'that', 'can', 'be', 'later', 'recalled',... | [-0.07639742570997014, 0.11363814601660421, -0.056838180625107974, 0.10088670564986461, -0.10033273979622338, -0.14898659443074114, 0.034890021128005023, 0.41298428390707287, -0.28154666445869003, -0.288103125286936, 0.07199285183356105, -0.289254529186648, -0.26332341499296397, 0.14775952901477374, -0.1422782240932028... |
707.0566 | Coma cluster object populations down to M_R~-9.5 | This study follows a recent analysis of the galaxy luminosity functions and
colour-magnitude red sequences in the Coma cluster (Adami et al. 2007). We
analyze here the distribution of very faint galaxies and globular clusters in
an east-west strip of $\sim 42 \times 7$ arcmin$^2$ crossing the Coma cluster
center (her... | astro-ph | this study follows a recent analysis of the galaxy luminosity functions and colourmagnitude red sequences in the coma cluster adami et al 2007 we analyze here the distribution of very faint galaxies and globular clusters in an eastwest strip of sim 42 times 7 arcmin2 crossing the coma cluster center hereafter the cs st... | [['this', 'study', 'follows', 'a', 'recent', 'analysis', 'of', 'the', 'galaxy', 'luminosity', 'functions', 'and', 'colourmagnitude', 'red', 'sequences', 'in', 'the', 'coma', 'cluster', 'adami', 'et', 'al', '2007', 'we', 'analyze', 'here', 'the', 'distribution', 'of', 'very', 'faint', 'galaxies', 'and', 'globular', 'clu... | [-0.037455468138139096, 0.04633184836218847, -0.09797035002710439, 0.07812617854052474, -0.06539280695204813, -0.04006358618367343, 0.01923214349775545, 0.43913488582237276, -0.12232768336080656, -0.3553355316811752, 0.05154429606953135, -0.2998410062814352, -0.04140600592013128, 0.17815960520848392, -0.077202311826034... |
707.0567 | Exploring nervous system transcriptomes during embryogenesis and
metamorphosis in Xenopus tropicalis using EST analysis | Xenopus tropicalis is an anuran amphibian species used as model in vertebrate
comparative genomics. It provides the same advantages as Xenopus laevis but is
diploid and has a smaller genome of 1.7 Gbp. Therefore X. tropicalis is more
amenable to systematic transcriptome surveys. We initiated a large-scale
partial cDN... | q-bio.GN q-bio.QM | xenopus tropicalis is an anuran amphibian species used as model in vertebrate comparative genomics it provides the same advantages as xenopus laevis but is diploid and has a smaller genome of 17 gbp therefore x tropicalis is more amenable to systematic transcriptome surveys we initiated a largescale partial cdna sequen... | [['xenopus', 'tropicalis', 'is', 'an', 'anuran', 'amphibian', 'species', 'used', 'as', 'model', 'in', 'vertebrate', 'comparative', 'genomics', 'it', 'provides', 'the', 'same', 'advantages', 'as', 'xenopus', 'laevis', 'but', 'is', 'diploid', 'and', 'has', 'a', 'smaller', 'genome', 'of', '17', 'gbp', 'therefore', 'x', 't... | [-0.06606659375210391, 0.06653459070750731, -0.0355091228665031, 0.09938460584417817, -0.047835438273985814, -0.11832758728414774, 0.05725912067325825, 0.3772200500037759, -0.24846318323153413, -0.28452263105155384, 0.05226479167604145, -0.2546209946589326, -0.21794380071260866, 0.21164605345978263, -0.1304766979306302... |
707.0568 | Optimal Linear Precoding Strategies for Wideband Non-Cooperative Systems
based on Game Theory-Part I: Nash Equilibria | In this two-parts paper we propose a decentralized strategy, based on a
game-theoretic formulation, to find out the optimal precoding/multiplexing
matrices for a multipoint-to-multipoint communication system composed of a set
of wideband links sharing the same physical resources, i.e., time and
bandwidth. We assume, ... | cs.IT cs.GT math.IT | in this twoparts paper we propose a decentralized strategy based on a gametheoretic formulation to find out the optimal precodingmultiplexing matrices for a multipointtomultipoint communication system composed of a set of wideband links sharing the same physical resources ie time and bandwidth we assume as optimality c... | [['in', 'this', 'twoparts', 'paper', 'we', 'propose', 'a', 'decentralized', 'strategy', 'based', 'on', 'a', 'gametheoretic', 'formulation', 'to', 'find', 'out', 'the', 'optimal', 'precodingmultiplexing', 'matrices', 'for', 'a', 'multipointtomultipoint', 'communication', 'system', 'composed', 'of', 'a', 'set', 'of', 'wi... | [-0.15704524803901265, -0.030081805830159, -0.08422762084059245, 0.0675319095729677, -0.055618992903767976, -0.19145003044544612, 0.12157767431408008, 0.3761043712503977, -0.26445749150715453, -0.28631168136611407, 0.12994722068912617, -0.20562704080759092, -0.14950705667445074, 0.12303914170253791, -0.1105461317812121... |
707.0569 | Spontaneous Fluxon Production in Annular Josephson Tunnel Junctions in
the Presence of a Magnetic Field | We report on the spontaneous production of fluxons in the presence of a
symmetry-breaking magnetic field for annular Josephson tunnel junctions during
a thermal quench. The dependence on field intensity $B$ of the probability
$\bar{f_1}$ to trap a single defect during the N-S phase transition drastically
depends on t... | cond-mat.supr-con | we report on the spontaneous production of fluxons in the presence of a symmetrybreaking magnetic field for annular josephson tunnel junctions during a thermal quench the dependence on field intensity b of the probability barf_1 to trap a single defect during the ns phase transition drastically depends on the sample ci... | [['we', 'report', 'on', 'the', 'spontaneous', 'production', 'of', 'fluxons', 'in', 'the', 'presence', 'of', 'a', 'symmetrybreaking', 'magnetic', 'field', 'for', 'annular', 'josephson', 'tunnel', 'junctions', 'during', 'a', 'thermal', 'quench', 'the', 'dependence', 'on', 'field', 'intensity', 'b', 'of', 'the', 'probabil... | [-0.19410927069209818, 0.20564786181155895, -0.05185426596703159, 0.031323252019245885, 0.0035546148523084215, -0.10953722330993293, 0.11519079738472765, 0.3688974994410937, -0.22684586990618374, -0.29616716643166097, 0.03315663290040165, -0.21823720216146997, -0.07589317801584666, 0.18828642720001046, 0.00833158186208... |
707.057 | Gauss--Berezin integral operators and spinors over supergroups
$\mathrm{OSp}(2p|2q)$, and Lagrangian super-Grasmannians | We obtain explicit formulas for the spinor representation $\rho$ of the real
orthosymplectic supergroup $\mathrm{OSp}(2p|2q,\mathbb{R})$ by integral
'Gauss--Berezin' operators. Next, we extend $\rho$ to a complex domain and get
a representation of a larger semigroup, which is a counterpart of Olshanski
subsemigroups ... | math.RT math-ph math.MP | we obtain explicit formulas for the spinor representation rho of the real orthosymplectic supergroup mathrmosp2p2qmathbbr by integral gaussberezin operators next we extend rho to a complex domain and get a representation of a larger semigroup which is a counterpart of olshanski subsemigroups in semisimple lie groups fu... | [['we', 'obtain', 'explicit', 'formulas', 'for', 'the', 'spinor', 'representation', 'rho', 'of', 'the', 'real', 'orthosymplectic', 'supergroup', 'mathrmosp2p2qmathbbr', 'by', 'integral', 'gaussberezin', 'operators', 'next', 'we', 'extend', 'rho', 'to', 'a', 'complex', 'domain', 'and', 'get', 'a', 'representation', 'of'... | [-0.15772348449714832, 0.0896078410860698, -0.11735950599266391, 0.09624191317904987, -0.13306342948772856, -0.06554214723566372, 0.0019054990668148505, 0.374435226134253, -0.29330318730394794, -0.1961922434264056, 0.0963941711695197, -0.2510737130848937, -0.1910448018615222, 0.16305772589414186, -0.08978680724578465, ... |
707.0571 | Linear automorphism groups of relatively free groups | Let G be a free group in a variety of groups, but G is not absolutely free.
We prove that the group of automorphisms Aut(G) is linear iff G is a virtually
nilpotent group.
| math.GR math.RT | let g be a free group in a variety of groups but g is not absolutely free we prove that the group of automorphisms autg is linear iff g is a virtually nilpotent group | [['let', 'g', 'be', 'a', 'free', 'group', 'in', 'a', 'variety', 'of', 'groups', 'but', 'g', 'is', 'not', 'absolutely', 'free', 'we', 'prove', 'that', 'the', 'group', 'of', 'automorphisms', 'autg', 'is', 'linear', 'iff', 'g', 'is', 'a', 'virtually', 'nilpotent', 'group']] | [-0.26207511726191596, 0.20060344755320864, -0.22392561431864605, -0.06570410471313688, -0.19865033419474082, -0.13844246078994782, -0.030067348524051553, 0.44156913985224333, -0.36290156183873906, -0.19432692169485724, 0.11231841371216647, -0.2623943836592576, -0.06974926781635184, 0.19238034882308805, -0.192710826748... |
707.0572 | On the deprojection of clusters of galaxies combining X-ray,
Sunyaev-Zeldovich temperature decrement and gravitational lensing maps | Knowledge of the intrinsic shape of galaxy clusters is very important in
investigating cosmic structure formation and astrophysical processes. The
reconstruction of the 3-dimensional structure usually relies on deprojecting
2-dimensional X-ray, Sunyaev-Zeldovich (SZ) and/or gravitational lensing
observations. As know... | astro-ph | knowledge of the intrinsic shape of galaxy clusters is very important in investigating cosmic structure formation and astrophysical processes the reconstruction of the 3dimensional structure usually relies on deprojecting 2dimensional xray sunyaevzeldovich sz andor gravitational lensing observations as known a joint an... | [['knowledge', 'of', 'the', 'intrinsic', 'shape', 'of', 'galaxy', 'clusters', 'is', 'very', 'important', 'in', 'investigating', 'cosmic', 'structure', 'formation', 'and', 'astrophysical', 'processes', 'the', 'reconstruction', 'of', 'the', '3dimensional', 'structure', 'usually', 'relies', 'on', 'deprojecting', '2dimensi... | [-0.1183928081790563, 0.09118006314565719, -0.08772878587155396, 0.09670298364545926, -0.1122400617190309, -0.08711860838768727, -0.027685861098924996, 0.415883859878199, -0.2365626304289671, -0.3213058039934064, 0.09585233258069449, -0.23091620007714178, -0.05489786093649282, 0.17906466442380203, -0.007873376348504314... |
707.0573 | Ibis/Picsit Status | We report about the status of the PICsIT layer of the imager IBIS. The
instrument has been tested in both Spectral Imaging and Spectral Timing Mode.
PICsIT Single Events, Multiple and ISGRI data of the Crab are simultaneously
fitted to a power law model and fit parameters are compared with the standard
values. We pre... | astro-ph | we report about the status of the picsit layer of the imager ibis the instrument has been tested in both spectral imaging and spectral timing mode picsit single events multiple and isgri data of the crab are simultaneously fitted to a power law model and fit parameters are compared with the standard values we present a... | [['we', 'report', 'about', 'the', 'status', 'of', 'the', 'picsit', 'layer', 'of', 'the', 'imager', 'ibis', 'the', 'instrument', 'has', 'been', 'tested', 'in', 'both', 'spectral', 'imaging', 'and', 'spectral', 'timing', 'mode', 'picsit', 'single', 'events', 'multiple', 'and', 'isgri', 'data', 'of', 'the', 'crab', 'are',... | [-0.0626592824493747, 0.050292049290261945, -0.11799260032464667, 0.0792448521709291, -0.09853865361154669, -0.14285360251341273, 0.03409793790162421, 0.4274682676659362, -0.2069626748377439, -0.39599730202116734, 0.1604153204623997, -0.29532410542821824, -0.04217821877855476, 0.2330398840603815, -0.05950483213188035, ... |
707.0574 | Detecting spatial patterns with the cumulant function. Part I: The
theory | In climate studies, detecting spatial patterns that largely deviate from the
sample mean still remains a statistical challenge. Although a Principal
Component Analysis (PCA), or equivalently a Empirical Orthogonal Functions
(EOF) decomposition, is often applied on this purpose, it can only provide
meaningful results ... | math.ST stat.TH | in climate studies detecting spatial patterns that largely deviate from the sample mean still remains a statistical challenge although a principal component analysis pca or equivalently a empirical orthogonal functions eof decomposition is often applied on this purpose it can only provide meaningful results if the unde... | [['in', 'climate', 'studies', 'detecting', 'spatial', 'patterns', 'that', 'largely', 'deviate', 'from', 'the', 'sample', 'mean', 'still', 'remains', 'a', 'statistical', 'challenge', 'although', 'a', 'principal', 'component', 'analysis', 'pca', 'or', 'equivalently', 'a', 'empirical', 'orthogonal', 'functions', 'eof', 'd... | [-0.061638217897185286, 0.02989123109838444, -0.1469781740670097, 0.11335169536313175, -0.08587339820154893, -0.09714164041364522, 0.03145825255538615, 0.3790994856012235, -0.27012917587464075, -0.2748817956092728, 0.11760860029718358, -0.27099477009130785, -0.14718229793038626, 0.1888184979109985, -0.03768930374155035... |
707.0575 | The Manakov system as two moving interacting curves | The two time-dependent Schrodinger equations in a potential V(s,u), $u$
denoting time, can be interpreted geometrically as a moving interacting curves
whose Fermi-Walker phase density is given by -dV/ds. The Manakov model appears
as two moving interacting curves using extended da Rios system and two Hasimoto
transfor... | nlin.SI | the two timedependent schrodinger equations in a potential vsu u denoting time can be interpreted geometrically as a moving interacting curves whose fermiwalker phase density is given by dvds the manakov model appears as two moving interacting curves using extended da rios system and two hasimoto transformations | [['the', 'two', 'timedependent', 'schrodinger', 'equations', 'in', 'a', 'potential', 'vsu', 'u', 'denoting', 'time', 'can', 'be', 'interpreted', 'geometrically', 'as', 'a', 'moving', 'interacting', 'curves', 'whose', 'fermiwalker', 'phase', 'density', 'is', 'given', 'by', 'dvds', 'the', 'manakov', 'model', 'appears', '... | [-0.2073826586989605, 0.17230146854063091, -0.12380394588589021, 0.0448596394018513, -0.04429348104673883, -0.2175427001050633, -0.030173195833492133, 0.3349522938546927, -0.29754202300682664, -0.2556817783852634, 0.08868857440488088, -0.3076895041310269, -0.12351059146306437, 0.17630458780584615, -0.006768360197463114... |
707.0576 | Magnetically-dominated jets inside collapsing stars as a model for
gamma-ray bursts and supernova explosions | It has been suggested that magnetic fields play a dynamically-important role
in core-collapse explosions of massive stars. In particular, they may be
important in the collapsar scenario for gamma-ray bursts (GRB), where the
central engine is a hyper-accreting black hole or a millisecond magnetar. The
present paper is... | astro-ph physics.plasm-ph | it has been suggested that magnetic fields play a dynamicallyimportant role in corecollapse explosions of massive stars in particular they may be important in the collapsar scenario for gammaray bursts grb where the central engine is a hyperaccreting black hole or a millisecond magnetar the present paper is focussed on... | [['it', 'has', 'been', 'suggested', 'that', 'magnetic', 'fields', 'play', 'a', 'dynamicallyimportant', 'role', 'in', 'corecollapse', 'explosions', 'of', 'massive', 'stars', 'in', 'particular', 'they', 'may', 'be', 'important', 'in', 'the', 'collapsar', 'scenario', 'for', 'gammaray', 'bursts', 'grb', 'where', 'the', 'ce... | [-0.11778857804744561, 0.1773048926943115, -0.05550242230148834, 0.1148473456378418, -0.12153493124155365, -0.055229741975437015, 0.01843021608537481, 0.36006141195955155, -0.2153964743626361, -0.2999753090267887, 0.07264358543135149, -0.22339899614548347, -0.034725210429834466, 0.23237730368914805, -0.0069451433045751... |
707.0577 | Pulsar kicks by anisotropic neutrino emission from quark matter | We discuss an acceleration mechanism for pulsars out of their supernova
remnants based on asymmetric neutrino emission from quark matter in the
presence of a strong magnetic field. The polarized electron spin fixes the
neutrino emission from the direct quark Urca process in one direction along the
magnetic field. We ... | astro-ph | we discuss an acceleration mechanism for pulsars out of their supernova remnants based on asymmetric neutrino emission from quark matter in the presence of a strong magnetic field the polarized electron spin fixes the neutrino emission from the direct quark urca process in one direction along the magnetic field we calc... | [['we', 'discuss', 'an', 'acceleration', 'mechanism', 'for', 'pulsars', 'out', 'of', 'their', 'supernova', 'remnants', 'based', 'on', 'asymmetric', 'neutrino', 'emission', 'from', 'quark', 'matter', 'in', 'the', 'presence', 'of', 'a', 'strong', 'magnetic', 'field', 'the', 'polarized', 'electron', 'spin', 'fixes', 'the'... | [-0.08124607064976141, 0.2445761660088185, -0.050732369683324716, 0.18032905524827444, -0.10438256308149833, -0.07616086227890964, 0.07732646109607931, 0.38523312936035486, -0.2510575623323138, -0.2898410631630283, 0.011911334494988506, -0.2425398414918723, 0.002803472336381674, 0.1906187251335583, 0.0651469629472838, ... |
707.0578 | Charge transport in disordered organic solids: A Monte Carlo simulation
study on the effects of film morphology | The influence of ordered regions (micro crystallites and aggregates) in the
other wise disordered polymer host matrix on field and temperature dependence
of mobility (\mu) has been simulated. Increase in concentration of ordered
regions leads to increase in magnitude of mobility and in high field regime the
saturatio... | cond-mat.dis-nn cond-mat.mtrl-sci | the influence of ordered regions micro crystallites and aggregates in the other wise disordered polymer host matrix on field and temperature dependence of mobility mu has been simulated increase in concentration of ordered regions leads to increase in magnitude of mobility and in high field regime the saturation of the... | [['the', 'influence', 'of', 'ordered', 'regions', 'micro', 'crystallites', 'and', 'aggregates', 'in', 'the', 'other', 'wise', 'disordered', 'polymer', 'host', 'matrix', 'on', 'field', 'and', 'temperature', 'dependence', 'of', 'mobility', 'mu', 'has', 'been', 'simulated', 'increase', 'in', 'concentration', 'of', 'ordere... | [-0.13019389626928246, 0.2098337107230551, -0.0477783298985555, 0.03929812946201613, 0.023099380806506347, -0.07405435515997502, 0.07180698493324691, 0.36196504330310303, -0.23151658637186465, -0.3569498653941525, 0.03683051026578491, -0.3120462198813374, -0.06846470145645957, 0.12856164935212105, 0.00968984254909745, ... |
707.0579 | Perspectives on Beam-Shaping Optimization for Thermal-Noise Reduction in
Advanced Gravitational-Wave Interferometric Detectors: Bounds, Profiles, and
Critical Parameters | Suitable shaping (in particular, flattening and broadening) of the laser beam
has recently been proposed as an effective device to reduce internal (mirror)
thermal noise in advanced gravitational wave interferometric detectors. Based
on some recently published analytic approximations (valid in the
infinite-test-mass ... | gr-qc | suitable shaping in particular flattening and broadening of the laser beam has recently been proposed as an effective device to reduce internal mirror thermal noise in advanced gravitational wave interferometric detectors based on some recently published analytic approximations valid in the infinitetestmass limit for t... | [['suitable', 'shaping', 'in', 'particular', 'flattening', 'and', 'broadening', 'of', 'the', 'laser', 'beam', 'has', 'recently', 'been', 'proposed', 'as', 'an', 'effective', 'device', 'to', 'reduce', 'internal', 'mirror', 'thermal', 'noise', 'in', 'advanced', 'gravitational', 'wave', 'interferometric', 'detectors', 'ba... | [-0.10977009010170341, 0.10844838735274127, -0.05681709613571385, 0.09082632229438116, -0.08187583785069077, -0.14231254906994045, 0.018270874513147742, 0.4118018209395048, -0.2384032140161205, -0.34443110468993454, 0.12387980616461534, -0.2578460883447214, -0.13399510529186381, 0.22900155707152167, -0.0920583520323577... |
707.058 | Force unfolding kinetics of RNA using optical tweezers. I. Effects of
experimental variables on measured results | Experimental variables of optical tweezers instrumentation that affect RNA
folding/unfolding kinetics were investigated. A model RNA hairpin, P5ab, was
attached to two micron-sized beads through hybrid RNA/DNA handles; one bead was
trapped by dual-beam lasers and the other was held by a micropipette. Several
experime... | physics.bio-ph cond-mat.soft cond-mat.stat-mech q-bio.BM | experimental variables of optical tweezers instrumentation that affect rna foldingunfolding kinetics were investigated a model rna hairpin p5ab was attached to two micronsized beads through hybrid rnadna handles one bead was trapped by dualbeam lasers and the other was held by a micropipette several experimental variab... | [['experimental', 'variables', 'of', 'optical', 'tweezers', 'instrumentation', 'that', 'affect', 'rna', 'foldingunfolding', 'kinetics', 'were', 'investigated', 'a', 'model', 'rna', 'hairpin', 'p5ab', 'was', 'attached', 'to', 'two', 'micronsized', 'beads', 'through', 'hybrid', 'rnadna', 'handles', 'one', 'bead', 'was', ... | [-0.10738149869017476, 0.19365636174415432, -0.020650768119755178, 0.017711089054517837, 0.002637863147267422, -0.17913633517671895, 0.07553573466978188, 0.38706706928652385, -0.27902773126396674, -0.32554225751380217, 0.04188748790265256, -0.24027393450310758, -0.091953585284957, 0.2060868338335219, -0.045115575005386... |
707.0581 | Compact Manifolds Covered by a Torus | Let $X$ be a connected compact complex manifold admitting a finite surjective
map $A \to X$ from a complex torus $A.$ We prove that up to finite \'etale
cover, $X$ is a product of projective spaces and a torus.
| math.AG | let x be a connected compact complex manifold admitting a finite surjective map a to x from a complex torus a we prove that up to finite etale cover x is a product of projective spaces and a torus | [['let', 'x', 'be', 'a', 'connected', 'compact', 'complex', 'manifold', 'admitting', 'a', 'finite', 'surjective', 'map', 'a', 'to', 'x', 'from', 'a', 'complex', 'torus', 'a', 'we', 'prove', 'that', 'up', 'to', 'finite', 'etale', 'cover', 'x', 'is', 'a', 'product', 'of', 'projective', 'spaces', 'and', 'a', 'torus']] | [-0.2170970428448457, 0.08305753860622644, -0.13180559443739745, 0.03897993898508736, -0.13115373296806446, -0.1696275553952616, 0.044639244580116026, 0.4004227327994811, -0.3557009215538318, -0.09433437229540104, 0.13526274274604824, -0.24255293836960426, -0.08013835406074157, 0.2299365151960116, -0.1698739956586789, ... |
707.0582 | Quenched lattice calculation of the B --> D l nu decay rate | We calculate, in the continuum limit of quenched lattice QCD, the form factor
that enters in the decay rate of the semileptonic decay B --> D l nu. Making
use of the step scaling method (SSM), previously introduced to handle two scale
problems in lattice QCD, and of flavour twisted boundary conditions we extract
G(w)... | hep-lat hep-ph | we calculate in the continuum limit of quenched lattice qcd the form factor that enters in the decay rate of the semileptonic decay b d l nu making use of the step scaling method ssm previously introduced to handle two scale problems in lattice qcd and of flavour twisted boundary conditions we extract gw at finite mome... | [['we', 'calculate', 'in', 'the', 'continuum', 'limit', 'of', 'quenched', 'lattice', 'qcd', 'the', 'form', 'factor', 'that', 'enters', 'in', 'the', 'decay', 'rate', 'of', 'the', 'semileptonic', 'decay', 'b', 'd', 'l', 'nu', 'making', 'use', 'of', 'the', 'step', 'scaling', 'method', 'ssm', 'previously', 'introduced', 't... | [-0.06090201632692837, 0.22776374670646185, -0.07117057703230735, 0.08091475722472091, -0.053132388983842926, -0.11793822640358664, 0.10103565155641063, 0.33491354472525825, -0.2585729663516139, -0.2265368451743008, 0.06340597798423535, -0.27193675121640437, -0.0012574625933276756, 0.1265854416594196, 0.083874712232500... |
707.0583 | Low-loss grating for coupling to a high-finesse cavity | A concept for a low loss all-reflective cavity coupler is experimentally
demonstrated at a wavelength of 1064 nm. A 1450 nm period dielectric reflection
grating with a diffraction efficiency of 0.58 % in the -1st order is used in
2nd order Littrow configuration as a coupler to form a cavity with a finesse of
400. The... | physics.optics | a concept for a low loss allreflective cavity coupler is experimentally demonstrated at a wavelength of 1064 nm a 1450 nm period dielectric reflection grating with a diffraction efficiency of 058 in the 1st order is used in 2nd order littrow configuration as a coupler to form a cavity with a finesse of 400 the applicat... | [['a', 'concept', 'for', 'a', 'low', 'loss', 'allreflective', 'cavity', 'coupler', 'is', 'experimentally', 'demonstrated', 'at', 'a', 'wavelength', 'of', '1064', 'nm', 'a', '1450', 'nm', 'period', 'dielectric', 'reflection', 'grating', 'with', 'a', 'diffraction', 'efficiency', 'of', '058', 'in', 'the', '1st', 'order', ... | [-0.17211007848872165, 0.14577603171040354, -0.01820408222633169, -0.04417709181220025, -0.07264712898023917, -0.17241629490653346, 0.0145864052112876, 0.5040179371441665, -0.1505223241892006, -0.33433946602561165, 0.11591804080403802, -0.3069061467203459, -0.07168728536558583, 0.2615798882478358, -0.023804395689359426... |
707.0584 | Magnetic susceptibility of the two-dimensional Hubbard model using a
power series for the hopping constant | The magnetic susceptibility of the two-dimensional repulsive Hubbard model
with nearest-neighbor hopping is investigated using the diagram technique
developed for the case of strong correlations. In this technique a power series
in the hopping constant is used. At half-filling the calculated zero-frequency
susceptibi... | cond-mat.str-el | the magnetic susceptibility of the twodimensional repulsive hubbard model with nearestneighbor hopping is investigated using the diagram technique developed for the case of strong correlations in this technique a power series in the hopping constant is used at halffilling the calculated zerofrequency susceptibility and... | [['the', 'magnetic', 'susceptibility', 'of', 'the', 'twodimensional', 'repulsive', 'hubbard', 'model', 'with', 'nearestneighbor', 'hopping', 'is', 'investigated', 'using', 'the', 'diagram', 'technique', 'developed', 'for', 'the', 'case', 'of', 'strong', 'correlations', 'in', 'this', 'technique', 'a', 'power', 'series',... | [-0.17033213474364442, 0.19856573556308876, 0.010395457512223637, 0.08807599090586801, -0.00146127671941177, -0.15109365292453578, 0.06152607839215885, 0.3648548537305185, -0.22896920441539137, -0.2716170592767584, 0.018356927474341974, -0.3964627908699058, -0.10997714478363994, 0.16282685660965532, 0.1396594899185523,... |
707.0585 | Wave function of the Universe in the early stage of its evolution | In quantum cosmological models, constructed in the framework of
Friedmann-Robertson-Walker metrics, a nucleation of the Universe with its
further expansion is described as a tunneling transition through an effective
barrier between regions with small and large values of the scale factor $a$ at
non-zero (or zero) ener... | gr-qc astro-ph hep-th | in quantum cosmological models constructed in the framework of friedmannrobertsonwalker metrics a nucleation of the universe with its further expansion is described as a tunneling transition through an effective barrier between regions with small and large values of the scale factor a at nonzero or zero energy the appr... | [['in', 'quantum', 'cosmological', 'models', 'constructed', 'in', 'the', 'framework', 'of', 'friedmannrobertsonwalker', 'metrics', 'a', 'nucleation', 'of', 'the', 'universe', 'with', 'its', 'further', 'expansion', 'is', 'described', 'as', 'a', 'tunneling', 'transition', 'through', 'an', 'effective', 'barrier', 'between... | [-0.14117933575856595, 0.1375578585645652, -0.09730384601382813, 0.058649488384510146, -0.023016407354803318, -0.06882434964106376, 0.05442522975200143, 0.3019583137938753, -0.2752271156812854, -0.28516627067480893, 0.07429337846534668, -0.2729698901530355, -0.12907325253528304, 0.1778302713869112, 0.04002892617983675,... |
707.0586 | Numerical studies of the Pfaffian model of the nu=5/2 fractional quantum
Hall effect | The Pfaffian model has been proposed for the fractional quantum Hall effect
(FQHE) at nu=5/2. We examine it for the quasihole excitations by comparison
with exact diagonalization results. Specifically, we consider the structure of
the low-energy spectrum, accuracy of the microscopic wave functions,
particle-hole symm... | cond-mat.mes-hall cond-mat.str-el | the pfaffian model has been proposed for the fractional quantum hall effect fqhe at nu52 we examine it for the quasihole excitations by comparison with exact diagonalization results specifically we consider the structure of the lowenergy spectrum accuracy of the microscopic wave functions particlehole symmetry splittin... | [['the', 'pfaffian', 'model', 'has', 'been', 'proposed', 'for', 'the', 'fractional', 'quantum', 'hall', 'effect', 'fqhe', 'at', 'nu52', 'we', 'examine', 'it', 'for', 'the', 'quasihole', 'excitations', 'by', 'comparison', 'with', 'exact', 'diagonalization', 'results', 'specifically', 'we', 'consider', 'the', 'structure'... | [-0.1448304612366393, 0.17760521061837864, -0.0756343675729556, 0.16634423763324052, -0.06851571592956017, -0.1317725846878229, 0.021715874100127854, 0.33736621404592043, -0.21986520670067805, -0.31690956296351475, 0.051698473073207796, -0.24342502801655194, -0.1783940521104691, 0.14399925892715915, 0.0460891215226207,... |
707.0587 | Quenched lattice calculation of semileptonic heavy-light meson form
factors | We calculate, in the continuum limit of quenched lattice QCD, the matrix
elements of the heavy-heavy vector current between heavy-light pseudoscalar
meson states. We present the form factors for different values of the initial
and final meson masses at finite momentum transfer. In particular, we calculate
the non-per... | hep-lat hep-ph | we calculate in the continuum limit of quenched lattice qcd the matrix elements of the heavyheavy vector current between heavylight pseudoscalar meson states we present the form factors for different values of the initial and final meson masses at finite momentum transfer in particular we calculate the nonperturbative ... | [['we', 'calculate', 'in', 'the', 'continuum', 'limit', 'of', 'quenched', 'lattice', 'qcd', 'the', 'matrix', 'elements', 'of', 'the', 'heavyheavy', 'vector', 'current', 'between', 'heavylight', 'pseudoscalar', 'meson', 'states', 'we', 'present', 'the', 'form', 'factors', 'for', 'different', 'values', 'of', 'the', 'init... | [-0.13194742187709158, 0.26599381432153174, -0.035633516707120165, 0.10959437739646988, 0.011798440337019123, -0.08484764104924988, 0.09695459930968565, 0.3005537248715974, -0.2050908378770818, -0.18051482912530933, -0.023346799351544916, -0.28259693890594056, 0.00133645240271437, 0.06383872692189786, 0.108254933399080... |
707.0588 | Lattice Refining LQC and the Matter Hamiltonian | In the context of loop quantum cosmology, we parametrise the lattice
refinement by a parameter, $A$, and the matter Hamiltonian by a parameter,
$\delta$. We then solve the Hamiltonian constraint for both a self-adjoint, and
a non-self-adjoint Hamiltonian operator. Demanding that the solutions for the
wave-functions o... | gr-qc astro-ph hep-ex hep-ph hep-th | in the context of loop quantum cosmology we parametrise the lattice refinement by a parameter a and the matter hamiltonian by a parameter delta we then solve the hamiltonian constraint for both a selfadjoint and a nonselfadjoint hamiltonian operator demanding that the solutions for the wavefunctions obey certain physic... | [['in', 'the', 'context', 'of', 'loop', 'quantum', 'cosmology', 'we', 'parametrise', 'the', 'lattice', 'refinement', 'by', 'a', 'parameter', 'a', 'and', 'the', 'matter', 'hamiltonian', 'by', 'a', 'parameter', 'delta', 'we', 'then', 'solve', 'the', 'hamiltonian', 'constraint', 'for', 'both', 'a', 'selfadjoint', 'and', '... | [-0.14476452049750246, 0.16330061740192928, -0.09135604427980357, 0.07947404995119493, -0.1355637154100757, -0.1501659503280136, 0.057415378782408016, 0.2930918846181349, -0.2629262516275048, -0.27569522910849437, 0.10974384053138476, -0.23550325013255993, -0.11532187358917374, 0.15083741362047332, -0.01185261779832408... |
707.0589 | Observation and Mass Measurement of the Baryon $\Xi^-_b$ | We report the observation and measurement of the mass of the bottom, strange
baryon $\Xi^-_b$ through the decay chain $\Xi^-_b \to J/\psi \Xi^-$, where
$J/\psi \to \mu^+ \mu^-$, $\Xi^- \to \Lambda \pi^-$, and $\Lambda \to p \pi^-$.
Evidence for observation is based on a signal whose probability of arising from
the es... | hep-ex | we report the observation and measurement of the mass of the bottom strange baryon xi_b through the decay chain xi_b to jpsi xi where jpsi to mu mu xi to lambda pi and lambda to p pi evidence for observation is based on a signal whose probability of arising from the estimated background is 66 x 1015 or 77 gaussian stan... | [['we', 'report', 'the', 'observation', 'and', 'measurement', 'of', 'the', 'mass', 'of', 'the', 'bottom', 'strange', 'baryon', 'xi_b', 'through', 'the', 'decay', 'chain', 'xi_b', 'to', 'jpsi', 'xi', 'where', 'jpsi', 'to', 'mu', 'mu', 'xi', 'to', 'lambda', 'pi', 'and', 'lambda', 'to', 'p', 'pi', 'evidence', 'for', 'obse... | [-0.105550547381863, 0.24720495972782375, -0.08446786182622115, 0.06844284338100502, -0.023972210120409728, -0.13274503061547877, 0.1222645318120097, 0.27724285279711086, -0.2070377866923809, -0.2976599308475852, -0.04241412072229044, -0.39943897277116774, 0.0931089412762473, 0.11152245393954217, 0.051345918911198773, ... |
707.059 | Dispersal of planets hosted in binaries, transitional members of
multiple star systems | This paper explains why planets in binary star systems might have a lower
frequency. A transient triple state of the binary causes the dispersal of
planets.
| astro-ph | this paper explains why planets in binary star systems might have a lower frequency a transient triple state of the binary causes the dispersal of planets | [['this', 'paper', 'explains', 'why', 'planets', 'in', 'binary', 'star', 'systems', 'might', 'have', 'a', 'lower', 'frequency', 'a', 'transient', 'triple', 'state', 'of', 'the', 'binary', 'causes', 'the', 'dispersal', 'of', 'planets']] | [-0.25998959955401146, 0.1937535016152721, -0.09684659044544858, 0.09414833734403007, -0.10920928081927392, -0.06425816748434535, 0.1405961443714869, 0.28607373512708223, -0.18653149243730766, -0.24497032653576192, 0.08754938505500412, -0.23710291632092917, -0.20752457106629243, 0.17143006192950103, -0.1419328332950289... |
707.0591 | Arbiter as the Third Man in classical and quantum games | We study possible influence of not necessarily sincere arbiter on the course
of classical and quantum 2x2 games and we show that this influence in the
quantum case is much bigger than in the classical case. Extreme sensitivity of
quantum games on initial states of quantum objects used as carriers of
information in a ... | quant-ph | we study possible influence of not necessarily sincere arbiter on the course of classical and quantum 2x2 games and we show that this influence in the quantum case is much bigger than in the classical case extreme sensitivity of quantum games on initial states of quantum objects used as carriers of information in a gam... | [['we', 'study', 'possible', 'influence', 'of', 'not', 'necessarily', 'sincere', 'arbiter', 'on', 'the', 'course', 'of', 'classical', 'and', 'quantum', '2x2', 'games', 'and', 'we', 'show', 'that', 'this', 'influence', 'in', 'the', 'quantum', 'case', 'is', 'much', 'bigger', 'than', 'in', 'the', 'classical', 'case', 'ext... | [-0.08384129368372399, 0.14337031065210962, -0.14924005062008897, 0.12878035908000096, -0.00662298928256388, -0.19205319765455056, 0.07020859534559012, 0.37081474900521616, -0.22218014225708665, -0.2800908069755813, 0.09542648902128416, -0.23701773411421864, -0.18054767606426375, 0.15022439857151498, -0.129648677220016... |
707.0592 | Triangles with two given integral sides | We study some Diophantine problems related to triangles with two given
integral sides. We solve two problems posed by Zolt\'an Bertalan and we also
provide some generalization.
| math.NT | we study some diophantine problems related to triangles with two given integral sides we solve two problems posed by zoltan bertalan and we also provide some generalization | [['we', 'study', 'some', 'diophantine', 'problems', 'related', 'to', 'triangles', 'with', 'two', 'given', 'integral', 'sides', 'we', 'solve', 'two', 'problems', 'posed', 'by', 'zoltan', 'bertalan', 'and', 'we', 'also', 'provide', 'some', 'generalization']] | [-0.14866584353148937, -0.02715019269201618, 0.009120680320148285, 0.11521252461422521, -0.184453004398025, -0.2048499539781075, 0.0018498841314934767, 0.3698969360154409, -0.3397536389529705, -0.29670527692024523, 0.19567277986341372, -0.3245927394869236, -0.21584547884189165, 0.25784712026898676, -0.1545657429199379,... |
707.0593 | Arithmetic progressions of squares, cubes and $n$-th powers | In this paper we continue the investigations about unlike powers in
arithmetic progression. We provide sharp upper bounds for the length of
primitive non-constant arithmetic progressions consisting of squares/cubes and
$n$-th powers.
| math.NT | in this paper we continue the investigations about unlike powers in arithmetic progression we provide sharp upper bounds for the length of primitive nonconstant arithmetic progressions consisting of squarescubes and nth powers | [['in', 'this', 'paper', 'we', 'continue', 'the', 'investigations', 'about', 'unlike', 'powers', 'in', 'arithmetic', 'progression', 'we', 'provide', 'sharp', 'upper', 'bounds', 'for', 'the', 'length', 'of', 'primitive', 'nonconstant', 'arithmetic', 'progressions', 'consisting', 'of', 'squarescubes', 'and', 'nth', 'powe... | [-0.2446228326824043, 0.10817195997843819, -0.075879275182923, 0.0749438109830202, -0.028212089091539383, -0.03217066713278332, 0.07126019652106709, 0.29281809087842703, -0.25091724698582, -0.22193798337191825, 0.11878526967108971, -0.3048482509630342, -0.17487189924765018, 0.2875530197315158, -0.1285788872609696, 0.06... |
707.0594 | Towards an understanding of the Of?p star HD 191612: optical
spectroscopy | We present extensive optical spectroscopy of the early-type magnetic star HD
191612 (O6.5f?pe-O8fp). The Balmer and HeI lines show strongly variable
emission which is highly reproducible on a well-determined 538-d period. Metal
lines and HeII absorptions (including many selective emission lines but
excluding He II 46... | astro-ph | we present extensive optical spectroscopy of the earlytype magnetic star hd 191612 o65fpeo8fp the balmer and hei lines show strongly variable emission which is highly reproducible on a welldetermined 538d period metal lines and heii absorptions including many selective emission lines but excluding he ii 4686a emission ... | [['we', 'present', 'extensive', 'optical', 'spectroscopy', 'of', 'the', 'earlytype', 'magnetic', 'star', 'hd', '191612', 'o65fpeo8fp', 'the', 'balmer', 'and', 'hei', 'lines', 'show', 'strongly', 'variable', 'emission', 'which', 'is', 'highly', 'reproducible', 'on', 'a', 'welldetermined', '538d', 'period', 'metal', 'lin... | [-0.16125382538131602, 0.13601929174407867, -0.018460500661817873, 0.03667570625240093, -0.11239859233747292, -0.18373104900135384, 0.06924502296640318, 0.45553936845595566, -0.1689397257501054, -0.2790288293669137, 0.08561858574188698, -0.2595769001910573, -0.04268350746047765, 0.1933575320187682, -0.03879270129961215... |
707.0595 | High resolution spectroscopy of the high velocity hot post-AGB star LS
III +52 24 (IRAS 22023+5249) | Aims: To investigate the first high resolution optical spectrum of the B-type
star, LS III +52 24, identified as the optical counterpart of the hot post-AGB
candidate IRAS 22023+5249 (I22023).
Methods: We carried out detailed identifications of the observed absorption
and emission features in the high resolution sp... | astro-ph | aims to investigate the first high resolution optical spectrum of the btype star ls iii 52 24 identified as the optical counterpart of the hot postagb candidate iras 220235249 i22023 methods we carried out detailed identifications of the observed absorption and emission features in the high resolution spectrum 4290 901... | [['aims', 'to', 'investigate', 'the', 'first', 'high', 'resolution', 'optical', 'spectrum', 'of', 'the', 'btype', 'star', 'ls', 'iii', '52', '24', 'identified', 'as', 'the', 'optical', 'counterpart', 'of', 'the', 'hot', 'postagb', 'candidate', 'iras', '220235249', 'i22023', 'methods', 'we', 'carried', 'out', 'detailed'... | [-0.026266588976971934, 0.09199738821623596, -0.04946426684863024, 0.05964359841703798, -0.06610223044821571, -0.11706795652524658, 0.03894127810687473, 0.43616711912721756, -0.14399611130507, -0.35151102093438946, 0.03054609596203532, -0.28319541633461465, 0.03431188903871976, 0.16455159012055506, -0.02838807406853095... |
707.0596 | Note on a paper "An Extension of a Theorem of Euler" by Hirata-Kohno et
al | In this paper we extend a result of Hirata-Kohno, Laishram, Shorey and
Tijdeman on the Diophantine equation $n(n+d)...(n+(k-1)d)=by^2,$ where
$n,d,k\geq 2$ and $y$ are positive integers such that $\gcd(n,d)=1.$
| math.NT | in this paper we extend a result of hiratakohno laishram shorey and tijdeman on the diophantine equation nndnk1dby2 where ndkgeq 2 and y are positive integers such that gcdnd1 | [['in', 'this', 'paper', 'we', 'extend', 'a', 'result', 'of', 'hiratakohno', 'laishram', 'shorey', 'and', 'tijdeman', 'on', 'the', 'diophantine', 'equation', 'nndnk1dby2', 'where', 'ndkgeq', '2', 'and', 'y', 'are', 'positive', 'integers', 'such', 'that', 'gcdnd1']] | [-0.15899484239829084, 0.0723743976498857, -0.04068490397185087, 0.013545874016320644, -0.05885040781383092, -0.1371977409774748, 0.030846986575246167, 0.2780961405175428, -0.26985679054632783, -0.22345048918699226, 0.08969504897928952, -0.32076912202561897, -0.2145586620705823, 0.1815447158102567, -0.10901607186921562... |
707.0597 | Approximately Einstein ACH metrics, volume renormalization, and an
invariant for contact manifolds | To any smooth compact manifold $M$ endowed with a contact structure $H$ and
partially integrable almost CR structure $J$, we prove the existence and
uniqueness, modulo high-order error terms and diffeomorphism action, of an
approximately Einstein ACH (asymptotically complex hyperbolic) metric $g$ on
$M\times (-1,0)$.... | math.DG | to any smooth compact manifold m endowed with a contact structure h and partially integrable almost cr structure j we prove the existence and uniqueness modulo highorder error terms and diffeomorphism action of an approximately einstein ach asymptotically complex hyperbolic metric g on mtimes 10 we consider the asympto... | [['to', 'any', 'smooth', 'compact', 'manifold', 'm', 'endowed', 'with', 'a', 'contact', 'structure', 'h', 'and', 'partially', 'integrable', 'almost', 'cr', 'structure', 'j', 'we', 'prove', 'the', 'existence', 'and', 'uniqueness', 'modulo', 'highorder', 'error', 'terms', 'and', 'diffeomorphism', 'action', 'of', 'an', 'a... | [-0.2248122661101265, 0.07009266359370245, -0.06306087316153812, 0.026500958869706628, -0.1067435572821396, -0.12719284336763034, -0.02421342523242564, 0.3506202055865156, -0.24398061480231997, -0.24592063986543092, 0.08809151754345397, -0.2745487007512735, -0.16695741173531378, 0.13393377277088095, -0.0958460498199474... |
707.0598 | Discriminant Analysis and Secondary-Beam Charge Recognition | The discriminant-analysis method has been applied to optimize the exotic-beam
charge recognition in a projectile fragmentation experiment. The experiment was
carried out at the GSI using the fragment separator (FRS) to produce and select
the relativistic secondary beams, and the ALADIN setup to measure their
fragment... | nucl-ex | the discriminantanalysis method has been applied to optimize the exoticbeam charge recognition in a projectile fragmentation experiment the experiment was carried out at the gsi using the fragment separator frs to produce and select the relativistic secondary beams and the aladin setup to measure their fragmentation pr... | [['the', 'discriminantanalysis', 'method', 'has', 'been', 'applied', 'to', 'optimize', 'the', 'exoticbeam', 'charge', 'recognition', 'in', 'a', 'projectile', 'fragmentation', 'experiment', 'the', 'experiment', 'was', 'carried', 'out', 'at', 'the', 'gsi', 'using', 'the', 'fragment', 'separator', 'frs', 'to', 'produce', ... | [0.008623330620211287, 0.11923533371187371, -0.14286662313082965, 0.09491939724108084, -0.020480178008459027, -0.12976002827179517, 0.050680103355000235, 0.3842602444129239, -0.16340355266877216, -0.31767986006130255, 0.00354497256209712, -0.31376961990185886, 0.04226783724675933, 0.1756676430763717, 0.0042662256658613... |
707.0599 | Origin of the excitonic recombinations in hexagonal boron nitride by
spatially resolved cathodoluminescence spectroscopy | The excitonic recombinations in hexagonal boron nitride (hBN) are
investigated with spatially resolved cathodoluminescence spectroscopy in the UV
range. Cathodoluminescence images of an individual hBN crystallite reveals that
the 215 nm free excitonic line is quite homogeneously emitted along the
crystallite whereas ... | cond-mat.mtrl-sci | the excitonic recombinations in hexagonal boron nitride hbn are investigated with spatially resolved cathodoluminescence spectroscopy in the uv range cathodoluminescence images of an individual hbn crystallite reveals that the 215 nm free excitonic line is quite homogeneously emitted along the crystallite whereas the 2... | [['the', 'excitonic', 'recombinations', 'in', 'hexagonal', 'boron', 'nitride', 'hbn', 'are', 'investigated', 'with', 'spatially', 'resolved', 'cathodoluminescence', 'spectroscopy', 'in', 'the', 'uv', 'range', 'cathodoluminescence', 'images', 'of', 'an', 'individual', 'hbn', 'crystallite', 'reveals', 'that', 'the', '215... | [-0.07050829443492387, 0.22055026978931366, -0.004150551925168226, -0.02434169342894548, 0.08462615485646223, -0.1437504731412781, 0.06443200495130824, 0.5764816390448495, -0.21255948234741626, -0.3522953391663338, -0.019130080829276457, -0.38035877828339215, -0.02466411965065881, 0.13997319197392483, 0.037589510187114... |
707.06 | Does heterosexual transmission drive the HIV/AIDS epidemic in
Sub-Saharan Africa (or elsewhere)? | A two-sex Basic Reproduction Number (BRN) is used to investigate the
conditions under which the Human Immunodeficiency Virus (HIV) may spread
through heterosexual contacts in Sub-Saharan Africa. (The BRN is the expected
number of new infections generated by one infected individual; the disease
spreads if the BRN is l... | stat.AP | a twosex basic reproduction number brn is used to investigate the conditions under which the human immunodeficiency virus hiv may spread through heterosexual contacts in subsaharan africa the brn is the expected number of new infections generated by one infected individual the disease spreads if the brn is larger than ... | [['a', 'twosex', 'basic', 'reproduction', 'number', 'brn', 'is', 'used', 'to', 'investigate', 'the', 'conditions', 'under', 'which', 'the', 'human', 'immunodeficiency', 'virus', 'hiv', 'may', 'spread', 'through', 'heterosexual', 'contacts', 'in', 'subsaharan', 'africa', 'the', 'brn', 'is', 'the', 'expected', 'number', ... | [-0.1225053929640357, 0.14090059607994954, -0.011136109846498753, 0.09613434754909592, -0.029195036543963875, -0.20862338049444934, 0.10950737402268357, 0.343344223486378, -0.17767551644689086, -0.26111332112061925, 0.11445298219890995, -0.3358069937245522, -0.13756051919314705, 0.1784659082223419, -0.11067137002643478... |
707.0601 | Diffusion in an Expanding Plasma using AdS/CFT | We consider the diffusion of a non-relativistic heavy quark of fixed mass M,
in a one-dimensionally expanding and strongly coupled plasma using the AdS/CFT
duality. The Green's function constructed around a static string embedded in a
background with a moving horizon, is identified with the noise correlation
function... | hep-th hep-ph | we consider the diffusion of a nonrelativistic heavy quark of fixed mass m in a onedimensionally expanding and strongly coupled plasma using the adscft duality the greens function constructed around a static string embedded in a background with a moving horizon is identified with the noise correlation function in a lan... | [['we', 'consider', 'the', 'diffusion', 'of', 'a', 'nonrelativistic', 'heavy', 'quark', 'of', 'fixed', 'mass', 'm', 'in', 'a', 'onedimensionally', 'expanding', 'and', 'strongly', 'coupled', 'plasma', 'using', 'the', 'adscft', 'duality', 'the', 'greens', 'function', 'constructed', 'around', 'a', 'static', 'string', 'emb... | [-0.15809911812963054, 0.2197077189689701, -0.1102672662242379, 0.0539266397335648, -0.010188719061049588, -0.12260625627597124, -0.014231748570681288, 0.3466103336710519, -0.26318821303763434, -0.22801836500468764, 0.06514173592508599, -0.2901136385801348, -0.030477519169702982, 0.11258942515643548, 0.0282710547721718... |
707.0602 | Limitation of the modulation method to smooth wire guide roughness | It was recently demonstrated that wire guide roughness can be suppressed by
modulating the wire currents so that the atoms experience a time-averaged
potential without roughness. We theoretically study the limitations of this
technique. At low modulation frequency, we show that the longitudinal potential
modulation p... | cond-mat.other | it was recently demonstrated that wire guide roughness can be suppressed by modulating the wire currents so that the atoms experience a timeaveraged potential without roughness we theoretically study the limitations of this technique at low modulation frequency we show that the longitudinal potential modulation produce... | [['it', 'was', 'recently', 'demonstrated', 'that', 'wire', 'guide', 'roughness', 'can', 'be', 'suppressed', 'by', 'modulating', 'the', 'wire', 'currents', 'so', 'that', 'the', 'atoms', 'experience', 'a', 'timeaveraged', 'potential', 'without', 'roughness', 'we', 'theoretically', 'study', 'the', 'limitations', 'of', 'th... | [-0.16884324120680297, 0.18928045976547686, -0.04694258017414139, 0.03584906354997542, -0.029964846470869902, -0.12947711571097725, 0.07968830855060956, 0.4341067611496514, -0.2804498649312286, -0.2772460984374125, 0.045769508307484365, -0.20703796115447218, -0.14119301615356225, 0.2610378094442834, -0.0386630991862456... |
707.0603 | Covariant Mappings for the Description of Measurement, Dissipation and
Decoherence in Quantum Mechanics | The general formalism of quantum mechanics for the description of statistical
experiments is briefly reviewed, introducing in particular position and
momentum observables as POVM characterized by their covariance properties with
respect to the isochronous Galilei group. Mappings describing state
transformations both ... | quant-ph | the general formalism of quantum mechanics for the description of statistical experiments is briefly reviewed introducing in particular position and momentum observables as povm characterized by their covariance properties with respect to the isochronous galilei group mappings describing state transformations both as a... | [['the', 'general', 'formalism', 'of', 'quantum', 'mechanics', 'for', 'the', 'description', 'of', 'statistical', 'experiments', 'is', 'briefly', 'reviewed', 'introducing', 'in', 'particular', 'position', 'and', 'momentum', 'observables', 'as', 'povm', 'characterized', 'by', 'their', 'covariance', 'properties', 'with', ... | [-0.11550454136109754, 0.12317961995918932, -0.09197747275714627, 0.07372910095760704, -0.06453359408011095, -0.1528075210955465, -0.01252980331963535, 0.3476033984484632, -0.281117815396152, -0.2561387038980009, 0.06695458913886439, -0.256983856410259, -0.14042340981737408, 0.1923280920862126, -0.051919717991756, 0.10... |
707.0604 | Not-so-normal mode decomposition | We provide a generalization of the normal mode decomposition for
non-symmetric or locality constrained situations. This allows for instance to
locally decouple a bipartitioned collection of arbitrarily correlated
oscillators up to elementary pairs into which all correlations are condensed.
Similarly, it enables us to... | quant-ph math-ph math.MP | we provide a generalization of the normal mode decomposition for nonsymmetric or locality constrained situations this allows for instance to locally decouple a bipartitioned collection of arbitrarily correlated oscillators up to elementary pairs into which all correlations are condensed similarly it enables us to decou... | [['we', 'provide', 'a', 'generalization', 'of', 'the', 'normal', 'mode', 'decomposition', 'for', 'nonsymmetric', 'or', 'locality', 'constrained', 'situations', 'this', 'allows', 'for', 'instance', 'to', 'locally', 'decouple', 'a', 'bipartitioned', 'collection', 'of', 'arbitrarily', 'correlated', 'oscillators', 'up', 't... | [-0.1277696653917453, 0.16098795240660282, -0.10499478487525432, 0.05170755878762892, -0.07298114947215337, -0.18617996025237848, 0.020476787406633692, 0.344573588586751, -0.30263368687188963, -0.26205488084617007, 0.03440378281811718, -0.2584119020058014, -0.12239847954862687, 0.18108561393455602, -0.03556833436397772... |
707.0605 | Do O-stars form in isolation? | Around 4% of O-stars are observed in apparent isolation, with no associated
cluster, and no indication of having been ejected from a nearby cluster. We
define an isolated O-star as a star > 17.5 M_\odot in a cluster with total mass
<100 M_\odot which contains no other massive (>10 M_\odot) stars. We show that
the fra... | astro-ph | around 4 of ostars are observed in apparent isolation with no associated cluster and no indication of having been ejected from a nearby cluster we define an isolated ostar as a star 175 m_odot in a cluster with total mass 100 m_odot which contains no other massive 10 m_odot stars we show that the fraction of apparently... | [['around', '4', 'of', 'ostars', 'are', 'observed', 'in', 'apparent', 'isolation', 'with', 'no', 'associated', 'cluster', 'and', 'no', 'indication', 'of', 'having', 'been', 'ejected', 'from', 'a', 'nearby', 'cluster', 'we', 'define', 'an', 'isolated', 'ostar', 'as', 'a', 'star', '175', 'm_odot', 'in', 'a', 'cluster', '... | [-0.09414042068366595, 0.15320916925162967, -0.06383155743737205, 0.10206866942165534, -0.06401416281440934, -0.04429521724949179, 0.05604196493165428, 0.4023813358476373, -0.12761372914870403, -0.3923488584834905, 0.033502161391174456, -0.31069295139995967, -0.05167085419529352, 0.1796906816259939, -0.0301869367819507... |
707.0606 | Infinite Horizon and Ergodic Optimal Quadratic Control for an Affine
Equation with Stochastic Coefficients | We study quadratic optimal stochastic control problems with control dependent
noise state equation perturbed by an affine term and with stochastic
coefficients. Both infinite horizon case and ergodic case are treated. To this
purpose we introduce a Backward Stochastic Riccati Equation and a dual backward
stochastic e... | math.PR | we study quadratic optimal stochastic control problems with control dependent noise state equation perturbed by an affine term and with stochastic coefficients both infinite horizon case and ergodic case are treated to this purpose we introduce a backward stochastic riccati equation and a dual backward stochastic equat... | [['we', 'study', 'quadratic', 'optimal', 'stochastic', 'control', 'problems', 'with', 'control', 'dependent', 'noise', 'state', 'equation', 'perturbed', 'by', 'an', 'affine', 'term', 'and', 'with', 'stochastic', 'coefficients', 'both', 'infinite', 'horizon', 'case', 'and', 'ergodic', 'case', 'are', 'treated', 'to', 'th... | [-0.17619950214231556, 0.048248883486435676, -0.06248735662136989, 0.08575958102168939, -0.12274859783991071, -0.177294645992912, 0.017091684493193912, 0.31817047380503605, -0.3507976310158318, -0.20993942676366054, 0.1774727493691237, -0.24353266792885817, -0.1416699695824222, 0.1870297271102159, -0.07293138212249191,... |
707.0607 | A Magnus- and Fer-type formula in dendriform algebras | We provide a refined approach to the classical Magnus and Fer expansion,
unveiling a new structure by using the language of dendriform and pre-Lie
algebras. The recursive formula for the logarithm of the solutions of the
equations X=1+ta<X and Y=1-tY> a in A[[t]] is provided, where (A,<,>) is a
dendriform algebra. Th... | math.CO math-ph math.CA math.MP math.RA | we provide a refined approach to the classical magnus and fer expansion unveiling a new structure by using the language of dendriform and prelie algebras the recursive formula for the logarithm of the solutions of the equations x1tax and y1ty a in at is provided where a is a dendriform algebra then we present the solut... | [['we', 'provide', 'a', 'refined', 'approach', 'to', 'the', 'classical', 'magnus', 'and', 'fer', 'expansion', 'unveiling', 'a', 'new', 'structure', 'by', 'using', 'the', 'language', 'of', 'dendriform', 'and', 'prelie', 'algebras', 'the', 'recursive', 'formula', 'for', 'the', 'logarithm', 'of', 'the', 'solutions', 'of',... | [-0.1404607824748382, 0.03418182850355152, -0.09469448871095665, 0.08659714299428742, -0.13340782920713537, -0.06446391527715604, -0.01960126499470789, 0.3210633703187341, -0.37665308364667, -0.22044995670439677, 0.14756057790364138, -0.25029291277751325, -0.1962377476040274, 0.21473268928239123, -0.05102896098978817, ... |
707.0608 | Fluctuation-induced first order transition due to Griffiths anomalies of
the Cluster glass phase | In itinerant magnetic systems with disorder, the quantum Griffiths phase at
T=0 is unstable to formation of a cluster glass (CG) of frozen droplet degrees
of freedom. In the absence of the fluctuations associated with these degrees of
freedom, the transition from the paramagnetic Fermi liquid (PMFL) to the
ordered ph... | cond-mat.dis-nn | in itinerant magnetic systems with disorder the quantum griffiths phase at t0 is unstable to formation of a cluster glass cg of frozen droplet degrees of freedom in the absence of the fluctuations associated with these degrees of freedom the transition from the paramagnetic fermi liquid pmfl to the ordered phase procee... | [['in', 'itinerant', 'magnetic', 'systems', 'with', 'disorder', 'the', 'quantum', 'griffiths', 'phase', 'at', 't0', 'is', 'unstable', 'to', 'formation', 'of', 'a', 'cluster', 'glass', 'cg', 'of', 'frozen', 'droplet', 'degrees', 'of', 'freedom', 'in', 'the', 'absence', 'of', 'the', 'fluctuations', 'associated', 'with', ... | [-0.18039060503360815, 0.30501639356537324, -0.08236902422088731, 0.040438260003741434, -0.01379108869670225, -0.11982226575907719, 0.06788350163800974, 0.29702634776809383, -0.2891538234793448, -0.2236004046862945, 0.06486589379346697, -0.3008159979695587, -0.12406527451821603, 0.07437400699460081, 0.04487402022017964... |
707.0609 | Maps of random walks on complex networks reveal community structure | To comprehend the multipartite organization of large-scale biological and
social systems, we introduce a new information theoretic approach that reveals
community structure in weighted and directed networks. The method decomposes a
network into modules by optimally compressing a description of information
flows on th... | physics.soc-ph cond-mat.dis-nn physics.data-an | to comprehend the multipartite organization of largescale biological and social systems we introduce a new information theoretic approach that reveals community structure in weighted and directed networks the method decomposes a network into modules by optimally compressing a description of information flows on the net... | [['to', 'comprehend', 'the', 'multipartite', 'organization', 'of', 'largescale', 'biological', 'and', 'social', 'systems', 'we', 'introduce', 'a', 'new', 'information', 'theoretic', 'approach', 'that', 'reveals', 'community', 'structure', 'in', 'weighted', 'and', 'directed', 'networks', 'the', 'method', 'decomposes', '... | [-0.11124579761078474, 0.06980242642821918, -0.09732369745565618, 0.0635454674266453, -0.08351001048313199, -0.07716348502289155, 0.06075205811610941, 0.3696175857661493, -0.33286194846690664, -0.31179718812592594, 0.04532545735965744, -0.2596758045662335, -0.2512763178565626, 0.19366572300816398, -0.033554688871590244... |
707.061 | Unfolding Orthogonal Terrains | It is shown that every orthogonal terrain, i.e., an orthogonal (right-angled)
polyhedron based on a rectangle that meets every vertical line in a segment,
has a grid unfolding: its surface may be unfolded to a single non-overlapping
piece by cutting along grid edges defined by coordinate planes through every
vertex.
| cs.CG | it is shown that every orthogonal terrain ie an orthogonal rightangled polyhedron based on a rectangle that meets every vertical line in a segment has a grid unfolding its surface may be unfolded to a single nonoverlapping piece by cutting along grid edges defined by coordinate planes through every vertex | [['it', 'is', 'shown', 'that', 'every', 'orthogonal', 'terrain', 'ie', 'an', 'orthogonal', 'rightangled', 'polyhedron', 'based', 'on', 'a', 'rectangle', 'that', 'meets', 'every', 'vertical', 'line', 'in', 'a', 'segment', 'has', 'a', 'grid', 'unfolding', 'its', 'surface', 'may', 'be', 'unfolded', 'to', 'a', 'single', 'n... | [-0.20381899799918757, 0.09065186140389414, -0.09830905348062516, -0.07376791235757992, -0.10004108598455787, -0.18896235155873, 0.046577841751277445, 0.4482481499761343, -0.2947976794838905, -0.1591047877445817, 0.11518409282667562, -0.3047873843461275, -0.11882474716752768, 0.15183236846001819, -0.13770667733391748, ... |
707.0611 | Circumnuclear Gas in Seyfert 1 Galaxies: Morphology, Kinematics, and
Direct Measurement of Black Hole Masses | (Abridged) The two-dimensional distribution and kinematics of the molecular,
ionized, and highly ionized gas in the nuclear regions of Seyfert 1 galaxies
have been measured using high spatial resolution (~0''.09) near-infrared
spectroscopy from NIRSPEC with adaptive optics on the Keck telescope. Molecular
hydrogen, H... | astro-ph | abridged the twodimensional distribution and kinematics of the molecular ionized and highly ionized gas in the nuclear regions of seyfert 1 galaxies have been measured using high spatial resolution 009 nearinfrared spectroscopy from nirspec with adaptive optics on the keck telescope molecular hydrogen h2 is detected in... | [['abridged', 'the', 'twodimensional', 'distribution', 'and', 'kinematics', 'of', 'the', 'molecular', 'ionized', 'and', 'highly', 'ionized', 'gas', 'in', 'the', 'nuclear', 'regions', 'of', 'seyfert', '1', 'galaxies', 'have', 'been', 'measured', 'using', 'high', 'spatial', 'resolution', '009', 'nearinfrared', 'spectrosc... | [-0.038330576517246015, 0.05921172801054728, -0.01214205610277034, 0.07127620341403909, -0.011305853265308441, -0.10394382695075229, 0.0025949100367497744, 0.47923238644902094, -0.09629295910108276, -0.32602885471436255, 0.030707737714869947, -0.306260679585645, 0.050293981100072375, 0.18250619622133185, -0.00625050420... |
707.0612 | Spectral Analysis of a Family of Second-Order Elliptic Operators with
Nonlocal Boundary Condition Indexed by a Probabilty Measure | Let $D\subset R^d$ be a bounded domain and let \[ L=\frac12\nabla\cdot
a\nabla +b\cdot\nabla \] %\[
%L=\frac12\sum_{i,j=1}^da_{i,j}\frac{\partial^2}{\partial x_i\partial
x_j}+\sum_{i=1}^db_i\frac{\partial}{\partial x_i}, %\] be a second order
elliptic operator on $D$. Let $\nu$ be a probability measure on $D$.
Deno... | math.SP math.AP | let dsubset rd be a bounded domain and let lfrac12nablacdot anabla bcdotnabla lfrac12sum_ij1da_ijfracpartial2partial x_ipartial x_jsum_i1db_ifracpartialpartial x_i be a second order elliptic operator on d let nu be a probability measure on d denote by mathcal l the differential operator whose domain is specified by the... | [['let', 'dsubset', 'rd', 'be', 'a', 'bounded', 'domain', 'and', 'let', 'lfrac12nablacdot', 'anabla', 'bcdotnabla', 'lfrac12sum_ij1da_ijfracpartial2partial', 'x_ipartial', 'x_jsum_i1db_ifracpartialpartial', 'x_i', 'be', 'a', 'second', 'order', 'elliptic', 'operator', 'on', 'd', 'let', 'nu', 'be', 'a', 'probability', 'm... | [-0.17814567358865857, 0.12371650318192014, -0.05066686316441076, -0.020709096084572547, -0.06989080559474249, -0.16315355299052614, -0.005536365460825319, 0.30224090396092296, -0.31795388627916765, -0.17793250509585518, 0.11067251537595159, -0.32575800853709763, -0.07258308355290538, 0.1091418800314363, -0.08159205346... |
707.0613 | Ferromagnetic behaviour in the strongly interacting two-component Bose
gas | We investigate the low temperature behaviour of the integrable 1D
two-component spinor Bose gas using the thermodynamic Bethe ansatz. We find
that for strong coupling the characteristics of the thermodynamics at low
temperatures are quantitatively affected by the spin ferromagnetic states,
which are described by an e... | cond-mat.stat-mech cond-mat.str-el | we investigate the low temperature behaviour of the integrable 1d twocomponent spinor bose gas using the thermodynamic bethe ansatz we find that for strong coupling the characteristics of the thermodynamics at low temperatures are quantitatively affected by the spin ferromagnetic states which are described by an effect... | [['we', 'investigate', 'the', 'low', 'temperature', 'behaviour', 'of', 'the', 'integrable', '1d', 'twocomponent', 'spinor', 'bose', 'gas', 'using', 'the', 'thermodynamic', 'bethe', 'ansatz', 'we', 'find', 'that', 'for', 'strong', 'coupling', 'the', 'characteristics', 'of', 'the', 'thermodynamics', 'at', 'low', 'tempera... | [-0.16805723418080054, 0.2644725125041773, -0.01231476599225562, 0.08075278047347229, -0.02182868700443248, -0.1791660226225203, 0.02431515442838755, 0.32846320565280523, -0.20647330202112263, -0.2378932744477119, 0.0026288273839605034, -0.34695936563180996, -0.04382293923889231, 0.1852799859585478, 0.14222218760683034... |
707.0614 | The bitwisted Cartesian model for the free loop fibration | Using the notion of truncating twisting function from a simplicial set to a
cubical set a special, bitwisted, Cartesian product of these sets is defined.
For the universal truncating twisting function, the (co)chain complex of the
corresponding bitwisted Cartesian product agrees with the standard Cartier
(Hochschild)... | math.AT | using the notion of truncating twisting function from a simplicial set to a cubical set a special bitwisted cartesian product of these sets is defined for the universal truncating twisting function the cochain complex of the corresponding bitwisted cartesian product agrees with the standard cartier hochschild chain com... | [['using', 'the', 'notion', 'of', 'truncating', 'twisting', 'function', 'from', 'a', 'simplicial', 'set', 'to', 'a', 'cubical', 'set', 'a', 'special', 'bitwisted', 'cartesian', 'product', 'of', 'these', 'sets', 'is', 'defined', 'for', 'the', 'universal', 'truncating', 'twisting', 'function', 'the', 'cochain', 'complex'... | [-0.20167522388510406, 0.06025131856146496, -0.030219995465207223, 0.08574584291272913, -0.10166542382406381, -0.10151968281328057, -0.05488405319435211, 0.3474884694830204, -0.421086745414262, -0.15452857500834702, 0.07186124264262617, -0.22822574008750962, -0.1291301809833385, 0.1826845730893183, -0.13196462490789904... |
707.0615 | Gibbs' paradox and black-hole entropy | In statistical mechanics Gibbs' paradox is avoided if the particles of a gas
are assumed to be indistinguishable. The resulting entropy then agrees with the
empirically tested thermodynamic entropy up to a term proportional to the
logarithm of the particle number. We discuss here how analogous situations
arise in the... | gr-qc | in statistical mechanics gibbs paradox is avoided if the particles of a gas are assumed to be indistinguishable the resulting entropy then agrees with the empirically tested thermodynamic entropy up to a term proportional to the logarithm of the particle number we discuss here how analogous situations arise in the stat... | [['in', 'statistical', 'mechanics', 'gibbs', 'paradox', 'is', 'avoided', 'if', 'the', 'particles', 'of', 'a', 'gas', 'are', 'assumed', 'to', 'be', 'indistinguishable', 'the', 'resulting', 'entropy', 'then', 'agrees', 'with', 'the', 'empirically', 'tested', 'thermodynamic', 'entropy', 'up', 'to', 'a', 'term', 'proportio... | [-0.053331224490746024, 0.153645247998378, -0.14413979593356532, 0.13610861039805142, -0.0338128897446123, -0.14518431731122583, 0.03854233856925795, 0.29165576952548067, -0.28895374242801314, -0.29893426313103477, 0.054365975059730516, -0.31170264610728204, -0.10113132909548368, 0.17594314304667272, -0.139969347881861... |
707.0616 | Geometrical and Physical Properties of SXR Loop-Top Flare Kernels | We investigate how the geometrical and physical properties of soft X-ray
flare kernels change with their altitude above the photosphere. We analyze limb
flares well observed by {\em Yohkoh}/SXT showing clear geometry with well
separated loop-top kernels. Our analysis concerns relations between kernel
size, plasma pre... | astro-ph | we investigate how the geometrical and physical properties of soft xray flare kernels change with their altitude above the photosphere we analyze limb flares well observed by em yohkohsxt showing clear geometry with well separated looptop kernels our analysis concerns relations between kernel size plasma pressure energ... | [['we', 'investigate', 'how', 'the', 'geometrical', 'and', 'physical', 'properties', 'of', 'soft', 'xray', 'flare', 'kernels', 'change', 'with', 'their', 'altitude', 'above', 'the', 'photosphere', 'we', 'analyze', 'limb', 'flares', 'well', 'observed', 'by', 'em', 'yohkohsxt', 'showing', 'clear', 'geometry', 'with', 'we... | [-0.08838901428812691, 0.18212011295624755, -0.03624056176472963, 0.1772252679643729, -0.09412627248093486, -0.04029237349327146, 0.04467546383702112, 0.4633124481928958, -0.27419562169201195, -0.3854013413444839, 0.0553133823123062, -0.25563119328580797, -0.14024416511925997, 0.18873502556446262, -0.03248614449561997,... |
707.0617 | Dynamics of Jupiter Trojans during the 2:1 mean motion resonance
crossing of Jupiter and Saturn | We study the dynamics of Jupiter Trojans in the early phase of the Solar
system while the outer planets migrated due to their interaction with the
planetesimal disk.
| astro-ph | we study the dynamics of jupiter trojans in the early phase of the solar system while the outer planets migrated due to their interaction with the planetesimal disk | [['we', 'study', 'the', 'dynamics', 'of', 'jupiter', 'trojans', 'in', 'the', 'early', 'phase', 'of', 'the', 'solar', 'system', 'while', 'the', 'outer', 'planets', 'migrated', 'due', 'to', 'their', 'interaction', 'with', 'the', 'planetesimal', 'disk']] | [-0.15333544311579317, 0.16993372664520784, -0.08237583675820913, 0.0421014497987926, -0.029070254614842788, 0.014104297018742986, 0.036727856778140576, 0.2796994546162231, -0.20726907991671137, -0.35694359375962187, 0.10657704068996411, -0.263584335334599, -0.1480752389013235, 0.10778007982298732, -0.10110650051917348... |
707.0618 | Implications of Compressed Supersymmetry for Collider and Dark Matter
Searches | Martin has proposed a scenario dubbed ``compressed supersymmetry'' (SUSY)
where the MSSM is the effective field theory between energy scales M_{\rm weak}
and M_{\rm GUT}, but with the GUT scale SU(3) gaugino mass M_3<< M_1 or M_2. As
a result, squark and gluino masses are suppressed relative to slepton, chargino
and ... | hep-ph | martin has proposed a scenario dubbed compressed supersymmetry susy where the mssm is the effective field theory between energy scales m_rm weak and m_rm gut but with the gut scale su3 gaugino mass m_3 m_1 or m_2 as a result squark and gluino masses are suppressed relative to slepton chargino and neutralino masses lead... | [['martin', 'has', 'proposed', 'a', 'scenario', 'dubbed', 'compressed', 'supersymmetry', 'susy', 'where', 'the', 'mssm', 'is', 'the', 'effective', 'field', 'theory', 'between', 'energy', 'scales', 'm_rm', 'weak', 'and', 'm_rm', 'gut', 'but', 'with', 'the', 'gut', 'scale', 'su3', 'gaugino', 'mass', 'm_3', 'm_1', 'or', '... | [-0.09343799269366328, 0.2990801877373989, -0.0565158643899864, 0.20801474081330584, -0.09682889606584076, -0.16248105695599888, 0.024842513564262328, 0.3391267671779828, -0.2281915718458623, -0.329825317839206, 0.042432465988998795, -0.26243273356770414, 0.0558051615073232, 0.15550617196046315, 0.04682079347075773, 0.... |
707.0619 | Markov evolutions and hierarchical equations in the continuum I.
One-component systems | General birth-and-death as well as hopping stochastic dynamics of infinite
particle systems in the continuum are considered. We derive corresponding
evolution equations for correlation functions and generating functionals.
General considerations are illustrated in a number of concrete examples of
Markov evolutions ap... | math-ph math.MP | general birthanddeath as well as hopping stochastic dynamics of infinite particle systems in the continuum are considered we derive corresponding evolution equations for correlation functions and generating functionals general considerations are illustrated in a number of concrete examples of markov evolutions appearin... | [['general', 'birthanddeath', 'as', 'well', 'as', 'hopping', 'stochastic', 'dynamics', 'of', 'infinite', 'particle', 'systems', 'in', 'the', 'continuum', 'are', 'considered', 'we', 'derive', 'corresponding', 'evolution', 'equations', 'for', 'correlation', 'functions', 'and', 'generating', 'functionals', 'general', 'con... | [-0.11479716091840104, 0.16386108922465195, -0.021366204812445423, 0.20137589672495695, -0.005843732770617035, -0.11660193352409723, -0.058822966032576834, 0.35219853138551116, -0.25212690216721967, -0.274894919839095, 0.13205519726298834, -0.2690081302584572, -0.18884112829850477, 0.22402132715003312, -0.0058894603809... |
707.062 | A generalized no-broadcasting theorem | We prove a generalized version of the no-broadcasting theorem, applicable to
essentially \emph{any} nonclassical finite-dimensional probabilistic model
satisfying a no-signaling criterion, including ones with ``super-quantum''
correlations. A strengthened version of the quantum no-broadcasting theorem
follows, and it... | quant-ph | we prove a generalized version of the nobroadcasting theorem applicable to essentially emphany nonclassical finitedimensional probabilistic model satisfying a nosignaling criterion including ones with superquantum correlations a strengthened version of the quantum nobroadcasting theorem follows and its proof is signifi... | [['we', 'prove', 'a', 'generalized', 'version', 'of', 'the', 'nobroadcasting', 'theorem', 'applicable', 'to', 'essentially', 'emphany', 'nonclassical', 'finitedimensional', 'probabilistic', 'model', 'satisfying', 'a', 'nosignaling', 'criterion', 'including', 'ones', 'with', 'superquantum', 'correlations', 'a', 'strengt... | [-0.11254097769051441, 0.061109017638955265, -0.19870616068025507, 0.21242473368814294, -0.08935479555899899, -0.3138641508218522, 0.08451684278649434, 0.19693461060523987, -0.2608671902756517, -0.22415103511108705, 0.057405130695163585, -0.21045548369875178, -0.09980242922514056, 0.28687309061933775, -0.17227730742888... |
707.0621 | Diffractive Optics for Gravitational Wave Detectors | All-reflective interferometry based on nano-structured diffraction gratings
offers new possibilities for gravitational wave detection. We investigate an
all-reflective Fabry-Perot interferometer concept in 2nd order Littrow mount.
The input-output relations for such a resonator are derived treating the
grating couple... | physics.optics | allreflective interferometry based on nanostructured diffraction gratings offers new possibilities for gravitational wave detection we investigate an allreflective fabryperot interferometer concept in 2nd order littrow mount the inputoutput relations for such a resonator are derived treating the grating coupler by mean... | [['allreflective', 'interferometry', 'based', 'on', 'nanostructured', 'diffraction', 'gratings', 'offers', 'new', 'possibilities', 'for', 'gravitational', 'wave', 'detection', 'we', 'investigate', 'an', 'allreflective', 'fabryperot', 'interferometer', 'concept', 'in', '2nd', 'order', 'littrow', 'mount', 'the', 'inputou... | [-0.19251875724920398, 0.08774691465452744, -0.1158405915184906, -0.02484738543121652, -0.137553303181476, -0.19904350242436383, -0.010470432375741162, 0.49174918155326985, -0.17532415052339662, -0.2936886148245046, 0.06286141628956873, -0.29157239932453993, -0.16158968675176077, 0.2647492740952382, -0.0170320561526089... |
707.0622 | On prospects for dark matter indirect detection in the Constrained MSSM | In the framework of the Constrained MSSM we derive the most probable ranges
of the diffuse gamma radiation flux from the direction of the Galactic center
and of the positron flux from the Galactic halo due to neutralino dark matter
annihilation. We find that, for a given halo model, and assuming flat priors,
the 68% ... | astro-ph hep-ph | in the framework of the constrained mssm we derive the most probable ranges of the diffuse gamma radiation flux from the direction of the galactic center and of the positron flux from the galactic halo due to neutralino dark matter annihilation we find that for a given halo model and assuming flat priors the 68 probabi... | [['in', 'the', 'framework', 'of', 'the', 'constrained', 'mssm', 'we', 'derive', 'the', 'most', 'probable', 'ranges', 'of', 'the', 'diffuse', 'gamma', 'radiation', 'flux', 'from', 'the', 'direction', 'of', 'the', 'galactic', 'center', 'and', 'of', 'the', 'positron', 'flux', 'from', 'the', 'galactic', 'halo', 'due', 'to'... | [-0.06503425295019534, 0.15795187763108304, -0.029016919785513066, 0.136343462798311, -0.08984295299874162, -0.045314686009718934, 0.04728591960595639, 0.3629497649527372, -0.19604296593578333, -0.4088194357288369, 0.049494134185326125, -0.2829134601004328, 0.03278061511645199, 0.2323408984072483, 0.011835438200622599,... |
707.0623 | An analysis of the fluctuations of the geomagnetic dipole | The time evolution of the strength of the Earth's virtual axial dipole moment
(VADM) is analyzed by relating it to the Fokker-Planck equation, which
describes a random walk with VADM-dependent drift and diffusion coefficients.
We demonstrate first that our method is able to retrieve the correct shape of
the drift and... | physics.geo-ph | the time evolution of the strength of the earths virtual axial dipole moment vadm is analyzed by relating it to the fokkerplanck equation which describes a random walk with vadmdependent drift and diffusion coefficients we demonstrate first that our method is able to retrieve the correct shape of the drift and diffusio... | [['the', 'time', 'evolution', 'of', 'the', 'strength', 'of', 'the', 'earths', 'virtual', 'axial', 'dipole', 'moment', 'vadm', 'is', 'analyzed', 'by', 'relating', 'it', 'to', 'the', 'fokkerplanck', 'equation', 'which', 'describes', 'a', 'random', 'walk', 'with', 'vadmdependent', 'drift', 'and', 'diffusion', 'coefficient... | [-0.12403874388999409, 0.16030459993240068, -0.07952352297020915, 0.027659995535986474, -0.07430097808268059, -0.06315027679931833, -0.002065646075528621, 0.319400373652267, -0.28863358818408513, -0.2677613379847672, 0.07614658659045229, -0.2419878468894756, -0.13424489293592395, 0.20524778168642732, 0.0216771428714747... |
707.0624 | Kinematical Studies of the Low Mass X-Ray Binary GR Mus (XB1254-690) | We present simultaneous high-resolution optical spectroscopy and X-ray data
of the X-ray binary system GR Mus (XB1254-690), obtained over a full range of
orbital phases. The X-ray observations are used to re-establish the orbital
ephemeris for this source. The optical data includes the first spectroscopic
detection o... | astro-ph | we present simultaneous highresolution optical spectroscopy and xray data of the xray binary system gr mus xb1254690 obtained over a full range of orbital phases the xray observations are used to reestablish the orbital ephemeris for this source the optical data includes the first spectroscopic detection of the donor s... | [['we', 'present', 'simultaneous', 'highresolution', 'optical', 'spectroscopy', 'and', 'xray', 'data', 'of', 'the', 'xray', 'binary', 'system', 'gr', 'mus', 'xb1254690', 'obtained', 'over', 'a', 'full', 'range', 'of', 'orbital', 'phases', 'the', 'xray', 'observations', 'are', 'used', 'to', 'reestablish', 'the', 'orbita... | [-0.07210911825684413, 0.057768839443125324, -0.05033621398044454, 0.040173732622300284, -0.06930502459067399, -0.09613966298285245, 0.09473220913270576, 0.41501610923697735, -0.20783470420462785, -0.3409549235148686, 0.11192342954269985, -0.3000153871340172, -0.007909617063080214, 0.24771731273297257, -0.0189701450213... |
707.0625 | Input-output relations for a 3-port grating coupled Fabry-Perot cavity | We analyze an optical 3-port reflection grating by means of a scattering
matrix formalism. Amplitude and phase relations between the 3 ports, i.e. the 3
orders of diffraction are derived. Such a grating can be used as an
all-reflective, low-loss coupler to Fabry-Perot cavities. We derive the input
output relations of... | physics.optics | we analyze an optical 3port reflection grating by means of a scattering matrix formalism amplitude and phase relations between the 3 ports ie the 3 orders of diffraction are derived such a grating can be used as an allreflective lowloss coupler to fabryperot cavities we derive the input output relations of a 3port grat... | [['we', 'analyze', 'an', 'optical', '3port', 'reflection', 'grating', 'by', 'means', 'of', 'a', 'scattering', 'matrix', 'formalism', 'amplitude', 'and', 'phase', 'relations', 'between', 'the', '3', 'ports', 'ie', 'the', '3', 'orders', 'of', 'diffraction', 'are', 'derived', 'such', 'a', 'grating', 'can', 'be', 'used', '... | [-0.20303909606082016, 0.14800807989964737, -0.05445955753720437, -0.05104755088933206, -0.0876240549931446, -0.24861071749518698, -0.005904090634430759, 0.48228517349343747, -0.24249730649395274, -0.2734560182255406, 0.04220121290955621, -0.29556262854916543, -0.14776384313322175, 0.23307523179503803, -0.0116841586294... |
707.0626 | The importance of thermal disorder and electronic occupation for the
T-dependence of the optical conductivity in FeSi and MnSi | The spectral weight (SW) for optical transitions in FeSi and MnSi are
calculated as function of temperature by means of LMTO-LDA band calculations.
The main effects, caused by structural disorder and electronic Fermi-Dirac
distribution, act oppositely on the T-dependence of the SW, while the variation
of the magnetic... | cond-mat.mtrl-sci | the spectral weight sw for optical transitions in fesi and mnsi are calculated as function of temperature by means of lmtolda band calculations the main effects caused by structural disorder and electronic fermidirac distribution act oppositely on the tdependence of the sw while the variation of the magnetic moment in ... | [['the', 'spectral', 'weight', 'sw', 'for', 'optical', 'transitions', 'in', 'fesi', 'and', 'mnsi', 'are', 'calculated', 'as', 'function', 'of', 'temperature', 'by', 'means', 'of', 'lmtolda', 'band', 'calculations', 'the', 'main', 'effects', 'caused', 'by', 'structural', 'disorder', 'and', 'electronic', 'fermidirac', 'd... | [-0.13073527293982096, 0.1901857710386189, -0.06611646140751602, 0.01002004753880121, 0.003334035810369712, -0.0664028250561147, 0.07102024736673479, 0.40190206451730415, -0.2735223011164875, -0.3189207865436981, 0.025490423377889853, -0.3197066265639368, -0.14850548802168814, 0.1542222039194542, 0.0414677196294888, 0.... |
707.0627 | Dependence of Temporal Properties on Energy in Long-Lag, Wide-Pulse
Gamma-Ray Bursts | We employed a sample compiled by Norris et al. (2005, ApJ, 625, 324) to study
the dependence of the pulse temporal properties on energy in long-lag,
wide-pulse gamma-ray bursts. Our analysis shows that the pulse peak time, rise
time scale and decay time scale are power law functions of energy, which is a
preliminary ... | astro-ph | we employed a sample compiled by norris et al 2005 apj 625 324 to study the dependence of the pulse temporal properties on energy in longlag widepulse gammaray bursts our analysis shows that the pulse peak time rise time scale and decay time scale are power law functions of energy which is a preliminary report on the r... | [['we', 'employed', 'a', 'sample', 'compiled', 'by', 'norris', 'et', 'al', '2005', 'apj', '625', '324', 'to', 'study', 'the', 'dependence', 'of', 'the', 'pulse', 'temporal', 'properties', 'on', 'energy', 'in', 'longlag', 'widepulse', 'gammaray', 'bursts', 'our', 'analysis', 'shows', 'that', 'the', 'pulse', 'peak', 'tim... | [-0.1022212076262653, 0.17823795342746726, -0.11672232081930255, 0.10555794481295314, -0.07627944939605737, -0.10081765238422456, 0.024141207845263916, 0.4669712659097011, -0.2545852176072993, -0.3540242522414484, 0.0824596776043118, -0.2973655659905659, -0.0758115205144114, 0.22174135728744027, 0.015722221086872983, 0... |
707.0628 | Dark Matter in a Constrained NMSSM | We explore the parameter space of a Constrained Next-to-Minimal
Supersymmetric Standard Model with GUT scale boundary conditions (CNMSSM) and
find regions where the relic density of the lightest neutralino is compatible
with the WMAP measurement. We emphasize differences with the MSSM: cases where
annihilation of the... | hep-ph | we explore the parameter space of a constrained nexttominimal supersymmetric standard model with gut scale boundary conditions cnmssm and find regions where the relic density of the lightest neutralino is compatible with the wmap measurement we emphasize differences with the mssm cases where annihilation of the lsp occ... | [['we', 'explore', 'the', 'parameter', 'space', 'of', 'a', 'constrained', 'nexttominimal', 'supersymmetric', 'standard', 'model', 'with', 'gut', 'scale', 'boundary', 'conditions', 'cnmssm', 'and', 'find', 'regions', 'where', 'the', 'relic', 'density', 'of', 'the', 'lightest', 'neutralino', 'is', 'compatible', 'with', '... | [-0.05626622357921602, 0.2553521216751131, -0.01641073788735358, 0.17792724627732098, -0.09778194643520549, -0.18199130716304496, -0.0067716351089378195, 0.29802959311214805, -0.21045657108519591, -0.33001783454571576, 0.08198679240612204, -0.2709886314685219, 0.05043022141006647, 0.13965456877657048, 0.052533657627874... |
707.0629 | Penrose Quantum Antiferromagnet | The Penrose tiling is a perfectly ordered two dimensional structure with
fivefold symmetry and scale invariance under site decimation. Quantum spin
models on such a system can be expected to differ significantly from more
conventional structures as a result of its special symmetries. In one
dimension, for example, ap... | cond-mat.str-el | the penrose tiling is a perfectly ordered two dimensional structure with fivefold symmetry and scale invariance under site decimation quantum spin models on such a system can be expected to differ significantly from more conventional structures as a result of its special symmetries in one dimension for example aperiodi... | [['the', 'penrose', 'tiling', 'is', 'a', 'perfectly', 'ordered', 'two', 'dimensional', 'structure', 'with', 'fivefold', 'symmetry', 'and', 'scale', 'invariance', 'under', 'site', 'decimation', 'quantum', 'spin', 'models', 'on', 'such', 'a', 'system', 'can', 'be', 'expected', 'to', 'differ', 'significantly', 'from', 'mo... | [-0.13746104440207618, 0.1877080022945608, -0.05615554166050922, 0.08450242810757022, -0.07349218286904752, -0.11292303648415807, 0.02045622797250919, 0.40551746363359453, -0.2703876098262538, -0.25085216707176233, 0.08087104639210003, -0.27319936864353767, -0.1612424320529068, 0.17115710379010507, 0.017312652279782157... |
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