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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709.0035 | On The Limitations of The Naive Lattice Decoding | In this paper, the inherent drawbacks of the naive lattice decoding for MIMO
fading systems is investigated. We show that using the naive lattice decoding
for MIMO systems has considerable deficiencies in terms of the rate-diversity
trade-off. Unlike the case of maximum-likelihood decoding, in this case, even
the per... | cs.IT math.IT | in this paper the inherent drawbacks of the naive lattice decoding for mimo fading systems is investigated we show that using the naive lattice decoding for mimo systems has considerable deficiencies in terms of the ratediversity tradeoff unlike the case of maximumlikelihood decoding in this case even the perfect latti... | [['in', 'this', 'paper', 'the', 'inherent', 'drawbacks', 'of', 'the', 'naive', 'lattice', 'decoding', 'for', 'mimo', 'fading', 'systems', 'is', 'investigated', 'we', 'show', 'that', 'using', 'the', 'naive', 'lattice', 'decoding', 'for', 'mimo', 'systems', 'has', 'considerable', 'deficiencies', 'in', 'terms', 'of', 'the... | [-0.21928588478205105, 0.0649162922637576, -0.048835031166672704, 0.07641246919364979, -0.023207904224594435, -0.22762356438674033, 0.12098936359165237, 0.38426181068023046, -0.24076049850632747, -0.21787933026750883, 0.09171452125379195, -0.2509998864432176, -0.2205258254536117, 0.13509016554492215, -0.134304774931321... |
709.0036 | Circular law for non-central random matrices | Let $(X_{jk})_{j,k\geq 1}$ be an infinite array of i.i.d. complex random
variables, with mean 0 and variance 1. Let $\la_{n,1},...,\la_{n,n}$ be the
eigenvalues of $(\frac{1}{\sqrt{n}}X_{jk})_{1\leq j,k\leq n}$. The strong
circular law theorem states that with probability one, the empirical spectral
distribution $\fr... | math.PR | let x_jk_jkgeq 1 be an infinite array of iid complex random variables with mean 0 and variance 1 let la_n1la_nn be the eigenvalues of frac1sqrtnx_jk_1leq jkleq n the strong circular law theorem states that with probability one the empirical spectral distribution frac1nde_la_n1de_la_nn converges weakly as ntoinfty to th... | [['let', 'x_jk_jkgeq', '1', 'be', 'an', 'infinite', 'array', 'of', 'iid', 'complex', 'random', 'variables', 'with', 'mean', '0', 'and', 'variance', '1', 'let', 'la_n1la_nn', 'be', 'the', 'eigenvalues', 'of', 'frac1sqrtnx_jk_1leq', 'jkleq', 'n', 'the', 'strong', 'circular', 'law', 'theorem', 'states', 'that', 'with', 'p... | [-0.08665643765663689, 0.1508910922481934, -0.13824489372231627, 0.05351269805944094, -0.0300590135006895, -0.18562633091063108, 0.03841078600230356, 0.33816758094615834, -0.26483659235940826, -0.24424564599319892, 0.0751761124226495, -0.3057211278814144, -0.08704377477675657, 0.14263878610255498, -0.09175584141805929,... |
709.0037 | Steiner-Minkowski Polynomials of Convex Sets in High Dimension, and
Limit Entire Functions | For a convex set (K) of the (n)-dimensional Euclidean space, the
Steiner-Minkowski polynomial (M_K(t)) is defined as the (n)-dimensional
Euclidean volume of the neighborhood of the radius (t). Being defined for
positive (t), the Steiner-Minkowski polynomials are considered for all complex
(t). The renormalization pro... | math.CV math.MG | for a convex set k of the ndimensional euclidean space the steinerminkowski polynomial m_kt is defined as the ndimensional euclidean volume of the neighborhood of the radius t being defined for positive t the steinerminkowski polynomials are considered for all complex t the renormalization procedure for steiner polynom... | [['for', 'a', 'convex', 'set', 'k', 'of', 'the', 'ndimensional', 'euclidean', 'space', 'the', 'steinerminkowski', 'polynomial', 'm_kt', 'is', 'defined', 'as', 'the', 'ndimensional', 'euclidean', 'volume', 'of', 'the', 'neighborhood', 'of', 'the', 'radius', 't', 'being', 'defined', 'for', 'positive', 't', 'the', 'steine... | [-0.15957756988117816, 0.12231075035352088, 0.0005153279786032659, 0.06349733452252285, -0.037209277420684146, -0.1019432659053968, -0.0033962463515948642, 0.30515828670037015, -0.28441784563646827, -0.18216325013242937, 0.10371183357373984, -0.3088382000914188, -0.11599764731040017, 0.16873690848135287, -0.03651354492... |
709.0038 | Experimental Consequences of Regular Charge-Monopole Electrodynamics | This work points out an application of the regular theory of charge-monopole
electrodynamics to the new experiments of very high energy. Using this theory,
it is explained why the new regions of high energy interactions that will be
explored by CERN's Large Hadron Collider may show a significant increase of the
cross... | physics.gen-ph | this work points out an application of the regular theory of chargemonopole electrodynamics to the new experiments of very high energy using this theory it is explained why the new regions of high energy interactions that will be explored by cerns large hadron collider may show a significant increase of the cross secti... | [['this', 'work', 'points', 'out', 'an', 'application', 'of', 'the', 'regular', 'theory', 'of', 'chargemonopole', 'electrodynamics', 'to', 'the', 'new', 'experiments', 'of', 'very', 'high', 'energy', 'using', 'this', 'theory', 'it', 'is', 'explained', 'why', 'the', 'new', 'regions', 'of', 'high', 'energy', 'interaction... | [-0.12022573273457561, 0.1251152064346065, -0.12212034361841183, 0.11299671967733754, -0.03542174391461433, -0.08731161706641109, 0.020753877937547967, 0.2701634358511203, -0.23387265980838695, -0.2918698412573172, 0.029972924023038812, -0.28293410688638687, -0.13888815348036587, 0.19097919640545216, -0.025934336005270... |
709.0039 | Thermally Assisted Current-Driven Bistable Precessional Regimes in
Asymmetric Spin Valves | Spin-transfer torque in asymmetric spin valves can destabilize both parallel
and antiparallel configurations and can lead to precessional modes also in the
absence of an external magnetic field. We find a bistable precessional regime
in such systems and show that thermal fluctuations can excite transitions
(telegraph... | cond-mat.mes-hall | spintransfer torque in asymmetric spin valves can destabilize both parallel and antiparallel configurations and can lead to precessional modes also in the absence of an external magnetic field we find a bistable precessional regime in such systems and show that thermal fluctuations can excite transitions telegraph nois... | [['spintransfer', 'torque', 'in', 'asymmetric', 'spin', 'valves', 'can', 'destabilize', 'both', 'parallel', 'and', 'antiparallel', 'configurations', 'and', 'can', 'lead', 'to', 'precessional', 'modes', 'also', 'in', 'the', 'absence', 'of', 'an', 'external', 'magnetic', 'field', 'we', 'find', 'a', 'bistable', 'precessio... | [-0.22398804225411048, 0.29090746737775214, -0.041436746218880896, 0.020331879582383906, -0.025634570631618593, -0.12286189903833848, 0.017787674866507158, 0.385145877853182, -0.3069527120530313, -0.2825579249948336, 0.033488582116643004, -0.2502418484392704, -0.14012879273835935, 0.253178699325551, 0.01885935562113802... |
709.004 | Comments on 'Controversy on a Dispersion Relation for MHD Waves' by
Chandra and Kumthekar | We comment on the work by Chandra and Kumthekar (2007, henceforth CK) which
is questionable. In the derivation of dispersion relation, CK neither invoke
the concept of vector space nor do they follow the basic criterion for the
elimination of perturbation terms under which the damped magnetoacoustic waves
are derived... | astro-ph | we comment on the work by chandra and kumthekar 2007 henceforth ck which is questionable in the derivation of dispersion relation ck neither invoke the concept of vector space nor do they follow the basic criterion for the elimination of perturbation terms under which the damped magnetoacoustic waves are derived | [['we', 'comment', 'on', 'the', 'work', 'by', 'chandra', 'and', 'kumthekar', '2007', 'henceforth', 'ck', 'which', 'is', 'questionable', 'in', 'the', 'derivation', 'of', 'dispersion', 'relation', 'ck', 'neither', 'invoke', 'the', 'concept', 'of', 'vector', 'space', 'nor', 'do', 'they', 'follow', 'the', 'basic', 'criteri... | [-0.15246390532322077, 0.11455432920032466, -0.08659264653426957, 0.10091704070539576, -0.16831072332451538, -0.09267027394808068, 0.0548367732256765, 0.33940273933872883, -0.20297430112615836, -0.2560870400344839, 0.12229863477975358, -0.20769061047431767, -0.19623571147724073, 0.177718893855297, -0.05596747047895072,... |
709.0041 | Spectral Analysis of Central Stars of Planetary Nebulae | Spectral analysis by means of NLTE model atmospheres has presently arrived at
a high level of sophistication. High-resolution spectra of central stars of
planetary nebulae can be reproduced in detail from the infrared to the X-ray
wavelength range.
In the case of LSV +4621, the exciting star of Sh 2-216, we demonst... | astro-ph | spectral analysis by means of nlte model atmospheres has presently arrived at a high level of sophistication highresolution spectra of central stars of planetary nebulae can be reproduced in detail from the infrared to the xray wavelength range in the case of lsv 4621 the exciting star of sh 2216 we demonstrate the sta... | [['spectral', 'analysis', 'by', 'means', 'of', 'nlte', 'model', 'atmospheres', 'has', 'presently', 'arrived', 'at', 'a', 'high', 'level', 'of', 'sophistication', 'highresolution', 'spectra', 'of', 'central', 'stars', 'of', 'planetary', 'nebulae', 'can', 'be', 'reproduced', 'in', 'detail', 'from', 'the', 'infrared', 'to... | [0.004037868711322666, 0.08750255760595159, -0.0762351979065839, 0.1007460486014477, -0.0681580681903887, -0.06483530648928701, 0.03472590852291895, 0.422514316130277, -0.173120708240207, -0.3920277838992794, 0.06410313593577703, -0.2837123412540869, -0.01852136234785512, 0.2354689539608965, -0.045947932592274525, 0.01... |
709.0042 | Two Higgs Bi-doublet Left-Right Model With Spontaneous P and CP
Violation | A left-right symmetric model with two Higgs bi-doublet is shown to be a
consistent model for both spontaneous P and CP violation. The flavor changing
neutral currents can be suppressed by the mechanism of approximate global U(1)
family symmetry. We calculate the constraints from neural $K$ meson mass
difference $\Del... | hep-ph | a leftright symmetric model with two higgs bidoublet is shown to be a consistent model for both spontaneous p and cp violation the flavor changing neutral currents can be suppressed by the mechanism of approximate global u1 family symmetry we calculate the constraints from neural k meson mass difference delta m_k and d... | [['a', 'leftright', 'symmetric', 'model', 'with', 'two', 'higgs', 'bidoublet', 'is', 'shown', 'to', 'be', 'a', 'consistent', 'model', 'for', 'both', 'spontaneous', 'p', 'and', 'cp', 'violation', 'the', 'flavor', 'changing', 'neutral', 'currents', 'can', 'be', 'suppressed', 'by', 'the', 'mechanism', 'of', 'approximate',... | [-0.09233506568577372, 0.2873065835327743, -0.0032115584840963344, 0.1558961877281205, -0.11029051049317447, -0.23326285569841818, 0.05325212897819623, 0.3234629855369744, -0.2763561389686667, -0.3091896623257339, 0.041004804132205454, -0.2847345802985039, -0.016446647355737892, 0.11100530512023556, 0.0521270690069343,... |
709.0043 | SUSY-QCD Corrections to Dark Matter Annihilation in the Higgs Funnel | We compute the full O(alpha_s) SUSY-QCD corrections to dark matter
annihilation in the Higgs-funnel, resumming potentially large mu tan beta and
A_b contributions and keeping all finite O(m_b,s,1/tan^2 beta) terms. We
demonstrate numerically that these corrections strongly influence the
extraction of SUSY mass parame... | hep-ph astro-ph | we compute the full oalpha_s susyqcd corrections to dark matter annihilation in the higgsfunnel resumming potentially large mu tan beta and a_b contributions and keeping all finite om_bs1tan2 beta terms we demonstrate numerically that these corrections strongly influence the extraction of susy mass parameters from cosm... | [['we', 'compute', 'the', 'full', 'oalpha_s', 'susyqcd', 'corrections', 'to', 'dark', 'matter', 'annihilation', 'in', 'the', 'higgsfunnel', 'resumming', 'potentially', 'large', 'mu', 'tan', 'beta', 'and', 'a_b', 'contributions', 'and', 'keeping', 'all', 'finite', 'om_bs1tan2', 'beta', 'terms', 'we', 'demonstrate', 'num... | [-0.0656958488013469, 0.17512255196727938, -0.03762396178760771, 0.1565677024645068, -0.06173147539750247, -0.12786312990079998, -0.0030037091918668503, 0.28910158610886943, -0.22445973731829957, -0.303894638794206, 0.06916061245394334, -0.31879748928092294, -0.028047497861750297, 0.1819595259937884, 0.0441378988878075... |
709.0044 | Can the anomaly cancellation method derive a correct Hawking temperature
of a Schwarzschild black hole in the isotropic coordinates ? | This paper has been withdrawn by the authors due to an incorrect statement on
the viability of the Robinson-Wilczek method when applied to the case when the
metric determinant vanishes at the horizon. This paper has been replaced by
arXiv:0803.1338 [hep-th].
| hep-th gr-qc | this paper has been withdrawn by the authors due to an incorrect statement on the viability of the robinsonwilczek method when applied to the case when the metric determinant vanishes at the horizon this paper has been replaced by arxiv08031338 hepth | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'due', 'to', 'an', 'incorrect', 'statement', 'on', 'the', 'viability', 'of', 'the', 'robinsonwilczek', 'method', 'when', 'applied', 'to', 'the', 'case', 'when', 'the', 'metric', 'determinant', 'vanishes', 'at', 'the', 'horizon', 'this', 'paper', 'ha... | [-0.07426790352910757, 0.016203057309394354, -0.10010170690948143, 0.003425763692939654, -0.06867324753839057, -0.09167167190462351, 0.0045346546568907796, 0.3090854400768876, -0.21434993455186485, -0.2735180142801255, 0.13107085949741304, -0.29699443010613324, -0.160749080684036, 0.13959225662983954, -0.19337568129412... |
709.0045 | First robotic monitoring of a lensed quasar: intrinsic variability of
SBS 0909+532 | To go into the details about the variability of the double quasar SBS
0909+532, we designed a monitoring programme with the 2 m Liverpool Robotic
Telescope in the r Sloan filter, spanning 1.5 years from 2005 January to 2006
June. The r-band light curves of the A and B components, several
cross-correlation techniques ... | astro-ph | to go into the details about the variability of the double quasar sbs 0909532 we designed a monitoring programme with the 2 m liverpool robotic telescope in the r sloan filter spanning 15 years from 2005 january to 2006 june the rband light curves of the a and b components several crosscorrelation techniques and a larg... | [['to', 'go', 'into', 'the', 'details', 'about', 'the', 'variability', 'of', 'the', 'double', 'quasar', 'sbs', '0909532', 'we', 'designed', 'a', 'monitoring', 'programme', 'with', 'the', '2', 'm', 'liverpool', 'robotic', 'telescope', 'in', 'the', 'r', 'sloan', 'filter', 'spanning', '15', 'years', 'from', '2005', 'janua... | [-0.08832729904787373, 0.06696122266085122, -0.12354080228100496, 0.09655709440563374, -0.11171793752280926, -0.1366030756991542, 0.05513915216714075, 0.42345032734899885, -0.2329231337412407, -0.3439301150911315, 0.11770521633109267, -0.3036929356447352, -0.09676513180858348, 0.22187697139991172, -0.07767365946535763,... |
709.0046 | Dark matter as a geometric effect in f(R) gravity | We consider the behavior of the tangential velocity of test particles moving
in stable circular orbits in f(R) modified theories of gravity. A large number
of observations at the galactic scale have shown that the rotational velocities
of massive test particles (hydrogen clouds) tend towards constant values at
large ... | gr-qc astro-ph | we consider the behavior of the tangential velocity of test particles moving in stable circular orbits in fr modified theories of gravity a large number of observations at the galactic scale have shown that the rotational velocities of massive test particles hydrogen clouds tend towards constant values at large distanc... | [['we', 'consider', 'the', 'behavior', 'of', 'the', 'tangential', 'velocity', 'of', 'test', 'particles', 'moving', 'in', 'stable', 'circular', 'orbits', 'in', 'fr', 'modified', 'theories', 'of', 'gravity', 'a', 'large', 'number', 'of', 'observations', 'at', 'the', 'galactic', 'scale', 'have', 'shown', 'that', 'the', 'r... | [-0.14916480436659185, 0.14012698935079648, -0.09562512925670792, 0.07379564429639787, -0.08391280135967666, -0.10056905626455166, -0.03683988820739614, 0.2885233331439344, -0.21686413603472626, -0.3216925540732013, -0.0022480058259033184, -0.22790476891289776, -0.06973175527107539, 0.14774834265052858, -0.025027481471... |
709.0047 | Quantum Informational Dark Energy: Dark energy from forgetting | We suggest that dark energy has a quantum informational origin. Landauer's
principle associated with the erasure of quantum information at a cosmic
horizon implies the non-zero vacuum energy having effective negative pressure.
Assuming the holographic principle, the minimum free energy condition, and the
Gibbons-Hawk... | hep-th astro-ph quant-ph | we suggest that dark energy has a quantum informational origin landauers principle associated with the erasure of quantum information at a cosmic horizon implies the nonzero vacuum energy having effective negative pressure assuming the holographic principle the minimum free energy condition and the gibbonshawking tempe... | [['we', 'suggest', 'that', 'dark', 'energy', 'has', 'a', 'quantum', 'informational', 'origin', 'landauers', 'principle', 'associated', 'with', 'the', 'erasure', 'of', 'quantum', 'information', 'at', 'a', 'cosmic', 'horizon', 'implies', 'the', 'nonzero', 'vacuum', 'energy', 'having', 'effective', 'negative', 'pressure',... | [-0.15956587464924352, 0.20247055660001934, -0.14919375436676835, 0.14651004467635753, -0.1000314638314938, -0.13066654925403948, 0.01990344652652063, 0.2772129639131229, -0.25262871145440097, -0.3341650157235563, 0.08392080501124094, -0.2888227546248924, 0.00701749708969146, 0.16774706350935792, -0.04166802096138285, ... |
709.0048 | The Ramsey number for a triple of large cycles | We find the asymptotic value of the Ramsey number for a triple of long
cycles, where the lengths of the cycles are large but may have different
parity.
| math.CO | we find the asymptotic value of the ramsey number for a triple of long cycles where the lengths of the cycles are large but may have different parity | [['we', 'find', 'the', 'asymptotic', 'value', 'of', 'the', 'ramsey', 'number', 'for', 'a', 'triple', 'of', 'long', 'cycles', 'where', 'the', 'lengths', 'of', 'the', 'cycles', 'are', 'large', 'but', 'may', 'have', 'different', 'parity']] | [-0.2729884043718422, 0.23678053060679563, -0.06953478392512936, 0.05093354771711996, 0.013344023060718817, -0.08353095822634973, 0.05579722226996507, 0.322684752621821, -0.24782364336507662, -0.34676147372062716, 0.13800809477522438, -0.21728925433542048, -0.07877062320975321, 0.17898237420013174, -0.03654084550882024... |
709.0049 | On the possibility of P-violation at finite baryon-number densities | We show how the introduction of a finite baryon density may trigger
spontaneous parity violation in the hadronic phase of QCD. Since this involves
strong interaction physics in an intermediate energy range we approximate QCD
by a \sigma model that retains the two lowest scalar and pseudoscalar
multiplets. We propose ... | hep-ph astro-ph hep-lat hep-th nucl-th | we show how the introduction of a finite baryon density may trigger spontaneous parity violation in the hadronic phase of qcd since this involves strong interaction physics in an intermediate energy range we approximate qcd by a sigma model that retains the two lowest scalar and pseudoscalar multiplets we propose a nov... | [['we', 'show', 'how', 'the', 'introduction', 'of', 'a', 'finite', 'baryon', 'density', 'may', 'trigger', 'spontaneous', 'parity', 'violation', 'in', 'the', 'hadronic', 'phase', 'of', 'qcd', 'since', 'this', 'involves', 'strong', 'interaction', 'physics', 'in', 'an', 'intermediate', 'energy', 'range', 'we', 'approximat... | [-0.11399325917591341, 0.28922987757817153, -0.10821641373539544, 0.14189804942101805, -0.08454407725366764, -0.13030432349270477, 0.07689216457947623, 0.32304104076008244, -0.20883544757296996, -0.26946559796176317, 0.010071121022130163, -0.22803766083338164, -0.09135248576889612, 0.07383759523301185, 0.05342061381920... |
709.005 | Interchangeability of Combined Piezoelectrooptic Effect in LiTaO3 and
LiNbO3 Crystals | In the present paper the coefficients of piezooptic (PO), electrooptic (EO)
and combined piezoelectrooptic (PEO) effects for LiNbO3 and LiTaO3 crystals are
reported. It is shown that the combined PEO effect is interchangeable, i.e. its
coefficients determined independ-ently from the EO and PO experiments are the
same... | physics.optics | in the present paper the coefficients of piezooptic po electrooptic eo and combined piezoelectrooptic peo effects for linbo3 and litao3 crystals are reported it is shown that the combined peo effect is interchangeable ie its coefficients determined independently from the eo and po experiments are the same | [['in', 'the', 'present', 'paper', 'the', 'coefficients', 'of', 'piezooptic', 'po', 'electrooptic', 'eo', 'and', 'combined', 'piezoelectrooptic', 'peo', 'effects', 'for', 'linbo3', 'and', 'litao3', 'crystals', 'are', 'reported', 'it', 'is', 'shown', 'that', 'the', 'combined', 'peo', 'effect', 'is', 'interchangeable', '... | [-0.11015866143861786, 0.15180197520100552, -0.0317322316620013, -0.10134151800150942, -0.038927136454731226, -0.14010111616074067, 0.0041913474358253825, 0.4567618373295535, -0.27637695484673197, -0.21995860103355802, 0.12183573574546482, -0.3516100343802701, -0.16128407947152204, 0.19819739797031102, -0.0258644784410... |
709.0051 | Electrooptic Effect in Non-Centrosymmetric CsLiB6O10 Borate Crystals | Electrooptic coefficient of CsLiB6O10 crystals has been experimentally
determined as r63=3.3*10-12m/V. The half-wave voltage for CsLiB6O10 (Ul/2=26
kV) is three orders of magnitude larger than that of the known KDP crystals.
| physics.optics | electrooptic coefficient of cslib6o10 crystals has been experimentally determined as r63331012mv the halfwave voltage for cslib6o10 ul226 kv is three orders of magnitude larger than that of the known kdp crystals | [['electrooptic', 'coefficient', 'of', 'cslib6o10', 'crystals', 'has', 'been', 'experimentally', 'determined', 'as', 'r63331012mv', 'the', 'halfwave', 'voltage', 'for', 'cslib6o10', 'ul226', 'kv', 'is', 'three', 'orders', 'of', 'magnitude', 'larger', 'than', 'that', 'of', 'the', 'known', 'kdp', 'crystals']] | [-0.14786222925478662, 0.20206893994300454, 0.008839414765437445, -0.10580586087976203, -0.04002663051640546, -0.17690678485841663, -0.036238811910152435, 0.47024213522672653, -0.1837249071923671, -0.28480757207230284, 0.0854539662875511, -0.30840788160761196, -0.06106792493826813, 0.36302038585698165, 0.05669156813787... |
709.0052 | Combined Piezoelectrooptic Effect in Rochelle Salt at the Phase
Transition | The results of study of piezoelectrooptic (PEO) effect in the course of
ferroelectric-ferroelastic phase transition in Rochelle salt crystals are
presented. The coefficient of the combined effect is obtained from measurements
of the changes in the electrooptic coefficients under the action of mechanical
stress and th... | physics.optics | the results of study of piezoelectrooptic peo effect in the course of ferroelectricferroelastic phase transition in rochelle salt crystals are presented the coefficient of the combined effect is obtained from measurements of the changes in the electrooptic coefficients under the action of mechanical stress and the chan... | [['the', 'results', 'of', 'study', 'of', 'piezoelectrooptic', 'peo', 'effect', 'in', 'the', 'course', 'of', 'ferroelectricferroelastic', 'phase', 'transition', 'in', 'rochelle', 'salt', 'crystals', 'are', 'presented', 'the', 'coefficient', 'of', 'the', 'combined', 'effect', 'is', 'obtained', 'from', 'measurements', 'of... | [-0.14188346144384806, 0.19376563790368198, -0.07732219337410354, -0.03527201953672355, -0.03163328687760898, -0.08117662271712538, 0.025717711329909056, 0.3598644623680295, -0.28466068157296387, -0.2696283222477642, 0.09432340408809375, -0.29257053128785365, -0.18979941594762822, 0.17361145221172639, 0.002521537760232... |
709.0053 | Phase Coexistence in Cs3Bi2I9 Ferroelastics: Optical, Dilatation and
Ultrasonic Velocity Studies | The results for dilatometric, ultrasonic velocity and the domain struct-ure
studies of Cs3Bi2I9 crystals in the course of ferroelastic phase trans-ition
are presented. It is shown that the phase transition in Cs3Bi2I9 is of the
first order. Basing on the thermal expansion results and the data obtained for
the elastic... | cond-mat.mtrl-sci | the results for dilatometric ultrasonic velocity and the domain structure studies of cs3bi2i9 crystals in the course of ferroelastic phase transition are presented it is shown that the phase transition in cs3bi2i9 is of the first order basing on the thermal expansion results and the data obtained for the elastic stiffn... | [['the', 'results', 'for', 'dilatometric', 'ultrasonic', 'velocity', 'and', 'the', 'domain', 'structure', 'studies', 'of', 'cs3bi2i9', 'crystals', 'in', 'the', 'course', 'of', 'ferroelastic', 'phase', 'transition', 'are', 'presented', 'it', 'is', 'shown', 'that', 'the', 'phase', 'transition', 'in', 'cs3bi2i9', 'is', 'o... | [-0.1345572533436662, 0.20195450818849892, -0.06441328070668763, -0.05855920505297335, -0.052348985366193174, -0.06384134590272096, 0.07567518609988538, 0.4015403032019923, -0.2483184173986127, -0.24227845640499382, 0.0991026045234367, -0.3113307145577443, -0.11063257343123985, 0.20019365993293026, 0.06225335207116448,... |
709.0054 | Acoustooptic Interaction in Barium Beta-Borate Crystals | Basing on the measurements of photoelastic coefficients, acoustic waves
velocities and the refractive indices, the possible geometries for acoustooptic
interaction in b-BaB2O4 crystals have been analysed. It has been shown that the
acoustooptic figure of merit achieves its maximum value when the transverse
acoustic w... | physics.optics | basing on the measurements of photoelastic coefficients acoustic waves velocities and the refractive indices the possible geometries for acoustooptic interaction in bbab2o4 crystals have been analysed it has been shown that the acoustooptic figure of merit achieves its maximum value when the transverse acoustic wave v1... | [['basing', 'on', 'the', 'measurements', 'of', 'photoelastic', 'coefficients', 'acoustic', 'waves', 'velocities', 'and', 'the', 'refractive', 'indices', 'the', 'possible', 'geometries', 'for', 'acoustooptic', 'interaction', 'in', 'bbab2o4', 'crystals', 'have', 'been', 'analysed', 'it', 'has', 'been', 'shown', 'that', '... | [-0.15442228472833944, 0.16522658651863986, -0.08526463446800005, -0.05832792941311544, -0.10732557385821234, -0.09183110627769069, -0.06040968271819028, 0.4466085134582086, -0.18909118290651927, -0.25789422419938174, 0.05902594329831614, -0.3320251510901885, -0.12973818772218443, 0.2658055244807408, 0.0112041006288067... |
709.0055 | Once More About the "Forbidden" Domain Structure and the Isolated Point
in K2Cd2xMn2(1-x)(SO4)3 Langbeinites | The domain structure in K2Cd2xMn2(1-x)(SO4)3 (x=0.5, 0.7 and 0.9) langbeinite
crystals is studied with the aid of optical polarization microscopy. It is
shown that the domain walls in ferro-elastic langbeinites separate
enantiomorphous orientation states. These orientation states appear in the
phase with the symmetry... | cond-mat.mtrl-sci | the domain structure in k2cd2xmn21xso43 x05 07 and 09 langbeinite crystals is studied with the aid of optical polarization microscopy it is shown that the domain walls in ferroelastic langbeinites separate enantiomorphous orientation states these orientation states appear in the phase with the symmetry 23 in connection... | [['the', 'domain', 'structure', 'in', 'k2cd2xmn21xso43', 'x05', '07', 'and', '09', 'langbeinite', 'crystals', 'is', 'studied', 'with', 'the', 'aid', 'of', 'optical', 'polarization', 'microscopy', 'it', 'is', 'shown', 'that', 'the', 'domain', 'walls', 'in', 'ferroelastic', 'langbeinites', 'separate', 'enantiomorphous', ... | [-0.13693161990653846, 0.17924696801337184, -0.07971326158320928, -0.031275697521956976, -0.061084274431598966, -0.09279511678108915, 0.034985713828183315, 0.43078176854330985, -0.2906840681957203, -0.2775099305512353, 0.11847035006570371, -0.30850678260941977, -0.09705333620859463, 0.11440757662057877, 0.0169040093686... |
709.0056 | Piezooptic Properties of beta-BaB2O4 and Li2B4O7 Crystals | Photoelastic coefficients of beta-BaB2O4 and Li2B4O7 crystals are calculated
on the basis of piezooptic measurements performed with interferometric
technique and the elastic compliance and stiffness data. Using the experimental
results, the acoustooptic (AO) figure of merit (FM) has been estimated for the
possible ge... | physics.optics | photoelastic coefficients of betabab2o4 and li2b4o7 crystals are calculated on the basis of piezooptic measurements performed with interferometric technique and the elastic compliance and stiffness data using the experimental results the acoustooptic ao figure of merit fm has been estimated for the possible geometries ... | [['photoelastic', 'coefficients', 'of', 'betabab2o4', 'and', 'li2b4o7', 'crystals', 'are', 'calculated', 'on', 'the', 'basis', 'of', 'piezooptic', 'measurements', 'performed', 'with', 'interferometric', 'technique', 'and', 'the', 'elastic', 'compliance', 'and', 'stiffness', 'data', 'using', 'the', 'experimental', 'resu... | [-0.14503423120287054, 0.15530908281573713, -0.04412821678463185, -0.048494641593021186, -0.08118524625528567, -0.09787115718394813, -0.023707808069147095, 0.4067842544305443, -0.23012596931271623, -0.2594183765324109, 0.11664735605031953, -0.3300869307748162, -0.11392330920950759, 0.25663426317422106, 0.05366274702021... |
709.0057 | Crystal Optical Properties of Inhomogeneous Plates and the Problems of
Polarization Tomography of Photoelastic Materials | Using the Jones matrix formalism, crystal optical properties of inhomogeneous
material consisting of a pile of weakly birefringent plates are analysed in
relation to the cell model adopted in polarization tomography of 3D dielectric
tensor field in photoelastic media. It is shown that the material manifests in
genera... | physics.optics | using the jones matrix formalism crystal optical properties of inhomogeneous material consisting of a pile of weakly birefringent plates are analysed in relation to the cell model adopted in polarization tomography of 3d dielectric tensor field in photoelastic media it is shown that the material manifests in general an... | [['using', 'the', 'jones', 'matrix', 'formalism', 'crystal', 'optical', 'properties', 'of', 'inhomogeneous', 'material', 'consisting', 'of', 'a', 'pile', 'of', 'weakly', 'birefringent', 'plates', 'are', 'analysed', 'in', 'relation', 'to', 'the', 'cell', 'model', 'adopted', 'in', 'polarization', 'tomography', 'of', '3d'... | [-0.15398296399955422, 0.15972489125310974, -0.04169637284492357, -0.04588908040657257, -0.06128796987020625, -0.11610359006609099, -0.06186098802404908, 0.4674634883562342, -0.2926308782054828, -0.2656031263132508, 0.03550254146998318, -0.264475471029679, -0.16525594670421037, 0.16978806120833048, 0.019926837436520517... |
709.0058 | An intermediate baryon system formation and the angular distributions of
the slow particles emitted in hadron-nuclear and nuclear-nuclear interactions
at high energies | We have analyzed the angular distributions of the b- particles emitted in
Kr+Em -reaction at 0.95 A GeV and in Au+Em -reaction at 10.7 A GeV and compared
these with lighter projectile experiments for which some structure in the
angular distribution of slow particles was observed. The same structure for the
b-particle... | nucl-ex | we have analyzed the angular distributions of the b particles emitted in krem reaction at 095 a gev and in auem reaction at 107 a gev and compared these with lighter projectile experiments for which some structure in the angular distribution of slow particles was observed the same structure for the bparticles almost di... | [['we', 'have', 'analyzed', 'the', 'angular', 'distributions', 'of', 'the', 'b', 'particles', 'emitted', 'in', 'krem', 'reaction', 'at', '095', 'a', 'gev', 'and', 'in', 'auem', 'reaction', 'at', '107', 'a', 'gev', 'and', 'compared', 'these', 'with', 'lighter', 'projectile', 'experiments', 'for', 'which', 'some', 'struc... | [-0.09835914885709146, 0.24564931123005646, -0.08050838361760634, 0.11808879519073368, 0.01207019791409776, -0.10985054991098943, 0.025868592538392625, 0.35183678109299493, -0.2327633113726168, -0.3340725497686648, 0.013532995150911177, -0.330385264487484, 0.018224454715613042, 0.1384047401661519, 0.04898985925021472, ... |
709.0059 | Anomalous Hall effect in (In,Mn)Sb dilute magnetic semiconductor | High magnetic field study of Hall resistivity in the ferromagnetic phase of
(In,Mn)Sb allows one to separate its normal and anomalous components. We show
that the anomalous Hall term is not proportional to the magnetization, and that
it even changes sign as a function of magnetic field. We also show that the
applicat... | cond-mat.other | high magnetic field study of hall resistivity in the ferromagnetic phase of inmnsb allows one to separate its normal and anomalous components we show that the anomalous hall term is not proportional to the magnetization and that it even changes sign as a function of magnetic field we also show that the application of p... | [['high', 'magnetic', 'field', 'study', 'of', 'hall', 'resistivity', 'in', 'the', 'ferromagnetic', 'phase', 'of', 'inmnsb', 'allows', 'one', 'to', 'separate', 'its', 'normal', 'and', 'anomalous', 'components', 'we', 'show', 'that', 'the', 'anomalous', 'hall', 'term', 'is', 'not', 'proportional', 'to', 'the', 'magnetiza... | [-0.1663900844443652, 0.21116816099283595, -0.09299343571012073, 0.03279505829684676, -0.10998234193099021, -0.1127289794150646, 0.06893346267028422, 0.36530422823143605, -0.2843014107696211, -0.2834514006815788, 0.029621925942615427, -0.28267942926420403, -0.20565133042508313, 0.1831415496891787, -0.002352415419676724... |
709.006 | Estimates for parameters and characteristics of the confining
SU(3)-gluonic field in $\eta$-meson from two-photon decay | On the basis of the confinement mechanism earlier proposed by author, the
electric form factor of $\eta$-meson is nonperturbatively calculated. The
latter is then applied to describe electromagnetic decay $\eta\to2\gamma$ which
entails estimates for parameters of the confining SU(3)-gluonic field in
$\eta$-meson. The... | hep-ph | on the basis of the confinement mechanism earlier proposed by author the electric form factor of etameson is nonperturbatively calculated the latter is then applied to describe electromagnetic decay etato2gamma which entails estimates for parameters of the confining su3gluonic field in etameson the corresponding estima... | [['on', 'the', 'basis', 'of', 'the', 'confinement', 'mechanism', 'earlier', 'proposed', 'by', 'author', 'the', 'electric', 'form', 'factor', 'of', 'etameson', 'is', 'nonperturbatively', 'calculated', 'the', 'latter', 'is', 'then', 'applied', 'to', 'describe', 'electromagnetic', 'decay', 'etato2gamma', 'which', 'entails... | [-0.0913461580353438, 0.21261507487039036, -0.06413623046313154, 0.09046093646635409, -0.04002549364155189, -0.0695966430939734, 0.005406340599426481, 0.3837853740351122, -0.1703984709456563, -0.29259443128115087, -0.008234594786371731, -0.2021500640319752, -0.05187026875429466, 0.1707017579894574, 0.04854002117072461,... |
709.0061 | GRB060602B = Swift J1749.4-2807: an unusual transiently accreting
neutron-star X-ray binary | We present an analysis of the Swift BAT and XRT data of GRB060602B, which is
most likely an accreting neutron star in a binary system and not a gamma-ray
burst. Our analysis shows that the BAT burst spectrum is consistent with a
thermonuclear flash (type-I X-ray burst) from the surface of an accreting
neutron star in... | astro-ph | we present an analysis of the swift bat and xrt data of grb060602b which is most likely an accreting neutron star in a binary system and not a gammaray burst our analysis shows that the bat burst spectrum is consistent with a thermonuclear flash typei xray burst from the surface of an accreting neutron star in a binary... | [['we', 'present', 'an', 'analysis', 'of', 'the', 'swift', 'bat', 'and', 'xrt', 'data', 'of', 'grb060602b', 'which', 'is', 'most', 'likely', 'an', 'accreting', 'neutron', 'star', 'in', 'a', 'binary', 'system', 'and', 'not', 'a', 'gammaray', 'burst', 'our', 'analysis', 'shows', 'that', 'the', 'bat', 'burst', 'spectrum',... | [-0.06897611978518996, 0.13988959950145374, -0.0846486477904133, 0.12920912401446613, -0.12549110121656654, -0.09908674295414795, 0.10095090374225445, 0.442384779884188, -0.20372066451992438, -0.34085772487894395, 0.14078956792120642, -0.37867940544435724, -0.043895866147610846, 0.29256967680073526, -0.0454264485082630... |
709.0062 | Anisotropy of Laser-Induced Bulk Damage of Single Crystals | The regularities of laser-induced damage of anisotropic materials, such as
LiNbO3 and KDP dielectric single crystals, are experimentally studied. It is
revealed that the shape of laser-induced damage in the dielectric crystals
depends on the elastic symmetry of crystal and the propagation direction of the
laser beam.... | physics.optics | the regularities of laserinduced damage of anisotropic materials such as linbo3 and kdp dielectric single crystals are experimentally studied it is revealed that the shape of laserinduced damage in the dielectric crystals depends on the elastic symmetry of crystal and the propagation direction of the laser beam when th... | [['the', 'regularities', 'of', 'laserinduced', 'damage', 'of', 'anisotropic', 'materials', 'such', 'as', 'linbo3', 'and', 'kdp', 'dielectric', 'single', 'crystals', 'are', 'experimentally', 'studied', 'it', 'is', 'revealed', 'that', 'the', 'shape', 'of', 'laserinduced', 'damage', 'in', 'the', 'dielectric', 'crystals', ... | [-0.1129510779946781, 0.21186122250040634, -0.06115200183060216, -0.07566251870483891, -0.048632758481656775, -0.09658096485419951, 0.0023804706727612044, 0.5083783322357034, -0.28104172691523116, -0.21943800304934644, 0.024204278047188398, -0.3214015501588093, -0.08456644487746975, 0.1716324782097026, 0.02606151273817... |
709.0063 | Hypergraph-theoretic charaterizations for LOCC incomparable ensembles of
multipartite CAT states | Using graphs and hypergraphs to systematically model collections of arbitrary
subsets of parties representing {\it ensembles (or collections)} of shared
multipartite CAT states, we study transformations between such {\it ensembles}
under {\it local operations and classical communication (LOCC)}. We show using
partial... | quant-ph | using graphs and hypergraphs to systematically model collections of arbitrary subsets of parties representing it ensembles or collections of shared multipartite cat states we study transformations between such it ensembles under it local operations and classical communication locc we show using partial entropic criteri... | [['using', 'graphs', 'and', 'hypergraphs', 'to', 'systematically', 'model', 'collections', 'of', 'arbitrary', 'subsets', 'of', 'parties', 'representing', 'it', 'ensembles', 'or', 'collections', 'of', 'shared', 'multipartite', 'cat', 'states', 'we', 'study', 'transformations', 'between', 'such', 'it', 'ensembles', 'unde... | [-0.1614125077612698, 0.18836290309131568, -0.03021044784955765, 0.07656078277266881, 0.032896995365841904, -0.2609990424521543, 0.0814911922531213, 0.40279576520763594, -0.27588765155748907, -0.284143662908305, 0.034174339671153575, -0.3033312961766073, -0.12711106237971267, 0.12419170223835284, -0.10605650918891611, ... |
709.0064 | On the distribution of conjugacy classes between the cosets of a finite
group in a cyclic extension | Let G be a finite group and H a normal subgroup such that G/H is cyclic.
Given a conjugacy class g^G of G we define its centralizing subgroup to be
HC_G(g). Let K be such that H\le K\le G. We show that the G-conjugacy classes
contained in K whose centralizing subgroup is K, are equally distributed
between the cosets ... | math.GR | let g be a finite group and h a normal subgroup such that gh is cyclic given a conjugacy class gg of g we define its centralizing subgroup to be hc_gg let k be such that hle kle g we show that the gconjugacy classes contained in k whose centralizing subgroup is k are equally distributed between the cosets of h in k the... | [['let', 'g', 'be', 'a', 'finite', 'group', 'and', 'h', 'a', 'normal', 'subgroup', 'such', 'that', 'gh', 'is', 'cyclic', 'given', 'a', 'conjugacy', 'class', 'gg', 'of', 'g', 'we', 'define', 'its', 'centralizing', 'subgroup', 'to', 'be', 'hc_gg', 'let', 'k', 'be', 'such', 'that', 'hle', 'kle', 'g', 'we', 'show', 'that',... | [-0.2125334417861369, 0.16886286311821114, -0.08295719073426844, -0.05150172929749871, -0.10633829625492747, -0.1279920311221345, 0.04893397882338519, 0.3825921660872421, -0.33879819911236714, -0.28272883065345916, 0.07145455206222268, -0.2699436054311015, -0.09032792302950654, 0.20167419108834983, -0.10688942683521997... |
709.0065 | Renormalized Wick expansion for a modified PQCD | The renormalization scheme for the Wick expansion of a modified version of
the perturbative QCD introduced in previous works is discussed. Massless QCD is
considered, by implementing the usual multiplicative scaling of the gluon and
quark wave functions and vertices. However, also massive quark and gluon
counter-term... | hep-ph | the renormalization scheme for the wick expansion of a modified version of the perturbative qcd introduced in previous works is discussed massless qcd is considered by implementing the usual multiplicative scaling of the gluon and quark wave functions and vertices however also massive quark and gluon counterterms are a... | [['the', 'renormalization', 'scheme', 'for', 'the', 'wick', 'expansion', 'of', 'a', 'modified', 'version', 'of', 'the', 'perturbative', 'qcd', 'introduced', 'in', 'previous', 'works', 'is', 'discussed', 'massless', 'qcd', 'is', 'considered', 'by', 'implementing', 'the', 'usual', 'multiplicative', 'scaling', 'of', 'the'... | [-0.11064415881315484, 0.24950407931667773, -0.08362807983229327, 0.1184944346821921, -0.05839543957479818, -0.06596898704802423, 0.05202510083557193, 0.31373963715118725, -0.17619819313201102, -0.2349448086921299, 0.035568344287660925, -0.23296833306499878, -0.06212994481503238, 0.14919473504685515, -0.006625722503549... |
709.0066 | Modelling of the influence of nanostructures' sizes on lattice
parameters | Computer modeling of formation of the one-dimensional and three-dimensional
monatomic nanostructures by the method of atom-atom potentials was done. The
arrangement of atoms was defined on the basis of the energy minimum. Our
calculations have shown that the distance between the nearest atoms depends on
number of ato... | cond-mat.soft cond-mat.dis-nn cond-mat.other | computer modeling of formation of the onedimensional and threedimensional monatomic nanostructures by the method of atomatom potentials was done the arrangement of atoms was defined on the basis of the energy minimum our calculations have shown that the distance between the nearest atoms depends on number of atoms thus... | [['computer', 'modeling', 'of', 'formation', 'of', 'the', 'onedimensional', 'and', 'threedimensional', 'monatomic', 'nanostructures', 'by', 'the', 'method', 'of', 'atomatom', 'potentials', 'was', 'done', 'the', 'arrangement', 'of', 'atoms', 'was', 'defined', 'on', 'the', 'basis', 'of', 'the', 'energy', 'minimum', 'our'... | [-0.11984572290810783, 0.1741526627151594, -0.021434537657325604, -0.01338422491192015, 0.042474021795540225, -0.09911771590605337, 0.06398283136051498, 0.436162705830355, -0.18966782318417869, -0.2986641198149702, 0.01669928878069809, -0.3140351181523103, -0.08015777005232583, 0.16703901318730324, 0.025727741162997583... |
709.0067 | Dimensional asymptotics of effective actions on S^n, and proof of
B\"ar-Schopka's conjecture | We study the dimensional asymptotics of the effective actions, or functional
determinants, for the Dirac operator D and Laplacians \Delta +\beta R on round
S^n. For Laplacians the behavior depends on ``the coupling strength'' \beta,
and one cannot in general expect a finite limit of \zeta'(0), and for the
ordinary La... | math-ph math.MP | we study the dimensional asymptotics of the effective actions or functional determinants for the dirac operator d and laplacians delta beta r on round sn for laplacians the behavior depends on the coupling strength beta and one cannot in general expect a finite limit of zeta0 and for the ordinary laplacian beta0 we pro... | [['we', 'study', 'the', 'dimensional', 'asymptotics', 'of', 'the', 'effective', 'actions', 'or', 'functional', 'determinants', 'for', 'the', 'dirac', 'operator', 'd', 'and', 'laplacians', 'delta', 'beta', 'r', 'on', 'round', 'sn', 'for', 'laplacians', 'the', 'behavior', 'depends', 'on', 'the', 'coupling', 'strength', '... | [-0.14996449443777757, 0.12299381672803844, -0.06086316747990038, 0.11371314049132966, -0.07624961114488542, -0.176203787419945, 0.018797087511380334, 0.29275088868370014, -0.2353817891263004, -0.22816427134509598, 0.11189911660289259, -0.31968526815762743, -0.15541306893407766, 0.13343924205983057, -0.0127824655260025... |
709.0068 | Off-Shell and Interference Effects for SUSY Particle Production | We show that the narrow-width approximation is insufficient for describing
production of supersymmetric particles at the ILC. Especially when cuts are
taken into account to extract signals using the narrow-width approximation can
be wrong by an order of magnitude.
| hep-ph | we show that the narrowwidth approximation is insufficient for describing production of supersymmetric particles at the ilc especially when cuts are taken into account to extract signals using the narrowwidth approximation can be wrong by an order of magnitude | [['we', 'show', 'that', 'the', 'narrowwidth', 'approximation', 'is', 'insufficient', 'for', 'describing', 'production', 'of', 'supersymmetric', 'particles', 'at', 'the', 'ilc', 'especially', 'when', 'cuts', 'are', 'taken', 'into', 'account', 'to', 'extract', 'signals', 'using', 'the', 'narrowwidth', 'approximation', 'c... | [-0.03147015705680809, 0.1506084284707098, -0.11130128245657453, 0.1633028762612062, -0.04711832417151294, -0.11176420270632474, -0.00835894358654817, 0.33939152325575167, -0.2336100650091584, -0.30077864850560826, 0.06272648579966372, -0.314297738747719, -0.015237413669148317, 0.16316295419939053, 0.06055836026103069,... |
709.0069 | On the statistical physics of metastable and non-equilibrium stationary
states | The optimization problems defining meta-stable or stationary equilibrium are
explored. The Gibbs scheme is modified aiming to describe the statistical
properties of a class of non-equilibrium and metastable states. The system is
assumed to maximize the usual definition of the Entropy, subject to the
standard constant... | cond-mat.stat-mech | the optimization problems defining metastable or stationary equilibrium are explored the gibbs scheme is modified aiming to describe the statistical properties of a class of nonequilibrium and metastable states the system is assumed to maximize the usual definition of the entropy subject to the standard constant energy... | [['the', 'optimization', 'problems', 'defining', 'metastable', 'or', 'stationary', 'equilibrium', 'are', 'explored', 'the', 'gibbs', 'scheme', 'is', 'modified', 'aiming', 'to', 'describe', 'the', 'statistical', 'properties', 'of', 'a', 'class', 'of', 'nonequilibrium', 'and', 'metastable', 'states', 'the', 'system', 'is... | [-0.12454682471515197, 0.13387019300561978, -0.11196449598962015, 0.0504327163001074, -0.025107375147786958, -0.10737759369927787, 0.048842002625827226, 0.27807922805098956, -0.28643245538437945, -0.3034378833534127, 0.100539687787575, -0.2634067966977859, -0.06283084144686452, 0.11771637351571203, -0.01139016748897524... |
709.007 | Origin of supermassive black holes | The origin of supermassive black holes in the galactic nuclei is quite
uncertain in spite of extensive set of observational data. We review the known
scenarios of galactic and cosmological formation of supermassive black holes.
The common drawback of galactic scenarios is a lack of time and shortage of
matter supply ... | astro-ph | the origin of supermassive black holes in the galactic nuclei is quite uncertain in spite of extensive set of observational data we review the known scenarios of galactic and cosmological formation of supermassive black holes the common drawback of galactic scenarios is a lack of time and shortage of matter supply for ... | [['the', 'origin', 'of', 'supermassive', 'black', 'holes', 'in', 'the', 'galactic', 'nuclei', 'is', 'quite', 'uncertain', 'in', 'spite', 'of', 'extensive', 'set', 'of', 'observational', 'data', 'we', 'review', 'the', 'known', 'scenarios', 'of', 'galactic', 'and', 'cosmological', 'formation', 'of', 'supermassive', 'blac... | [-0.14410628679074444, 0.05556684658408495, -0.006365114400639783, 0.17740565656446095, -0.12382513754134782, -0.06643385537033684, 0.04391762623455116, 0.3283862714157548, -0.14016533161372727, -0.3482133019498961, 0.08792267724747098, -0.3113980411097061, -0.030091725484749605, 0.22671328064833962, -0.064373475412816... |
709.0071 | Theta Series Associated with the Weil-Schroedinger Representation | The Weil representation discovered by Andre Weil plays an important role in
the study of the tranformation properties of theta series. In this paper, we
define the Weil-Schroedinger representation of the Jacobi group and prove that
the theta series associated with the Weil-Schroedinger representation is a
Jacobi form... | math.NT math.RT | the weil representation discovered by andre weil plays an important role in the study of the tranformation properties of theta series in this paper we define the weilschroedinger representation of the jacobi group and prove that the theta series associated with the weilschroedinger representation is a jacobi form with ... | [['the', 'weil', 'representation', 'discovered', 'by', 'andre', 'weil', 'plays', 'an', 'important', 'role', 'in', 'the', 'study', 'of', 'the', 'tranformation', 'properties', 'of', 'theta', 'series', 'in', 'this', 'paper', 'we', 'define', 'the', 'weilschroedinger', 'representation', 'of', 'the', 'jacobi', 'group', 'and'... | [-0.21511051118181185, 0.04970530059478639, -0.16072531244396393, 0.04194433311128925, -0.11179019419219473, -0.02736574473212762, -0.018158911042927026, 0.3134996319382355, -0.3719107723505846, -0.22679329274627702, 0.0778425034047265, -0.22669299635715012, -0.23813655086118599, 0.1758561465760757, -0.1026002673817605... |
709.0072 | Quasi-Anosov diffeomorphisms of 3-manifolds | In 1969, Hirsch posed the following problem: given a diffeomorphism, and a
compact invariant hyperbolic set, describe its topology and restricted
dynamics. We solve the problem where the hyperbolic invariant set is a closed
3-manifold: if the manifold is orientable, then it is a connected sum of tori
and handles; oth... | math.DS | in 1969 hirsch posed the following problem given a diffeomorphism and a compact invariant hyperbolic set describe its topology and restricted dynamics we solve the problem where the hyperbolic invariant set is a closed 3manifold if the manifold is orientable then it is a connected sum of tori and handles otherwise it i... | [['in', '1969', 'hirsch', 'posed', 'the', 'following', 'problem', 'given', 'a', 'diffeomorphism', 'and', 'a', 'compact', 'invariant', 'hyperbolic', 'set', 'describe', 'its', 'topology', 'and', 'restricted', 'dynamics', 'we', 'solve', 'the', 'problem', 'where', 'the', 'hyperbolic', 'invariant', 'set', 'is', 'a', 'closed... | [-0.24258065509440546, 0.13765631200195375, -0.05869584892537783, 0.0941989980452821, -0.12975130721778524, -0.16260442762127655, 0.003285160902040926, 0.31351226521655917, -0.3225826743397523, -0.22573064755521377, 0.13017422584049532, -0.3036197765772654, -0.1652733592094261, 0.16406543108380653, -0.17524552496615797... |
709.0073 | Static Universe model existing due to the Matter-Dark Energy coupling | The work investigate a static, isotropic and almost homogeneous Universe
containing a real scalar field modeling the Dark-Energy (quintaessence)
interacting with pressureless matter. It is argued that the interaction between
matter and the Dark Energy, is essential for the very existence of the
considered solution. A... | gr-qc | the work investigate a static isotropic and almost homogeneous universe containing a real scalar field modeling the darkenergy quintaessence interacting with pressureless matter it is argued that the interaction between matter and the dark energy is essential for the very existence of the considered solution assuming t... | [['the', 'work', 'investigate', 'a', 'static', 'isotropic', 'and', 'almost', 'homogeneous', 'universe', 'containing', 'a', 'real', 'scalar', 'field', 'modeling', 'the', 'darkenergy', 'quintaessence', 'interacting', 'with', 'pressureless', 'matter', 'it', 'is', 'argued', 'that', 'the', 'interaction', 'between', 'matter'... | [-0.14875266131579498, 0.18792094149379224, -0.0867137663962343, 0.09131775896176932, -0.0904218067394428, -0.09778723927786503, -0.02096816322389, 0.2887362508999207, -0.2211209247566618, -0.3564859255676783, 0.06069444708638129, -0.24394305106959766, -0.020968933409975864, 0.14095801011883194, 0.05386087680353394, 0.... |
709.0074 | Submerged turbulence detection with optical satellites | During fall periods in 2002, 2003 and 2004 three major oceanographic
expeditions were carried out in Mamala Bay, Hawaii. These were part of the RASP
Remote Anthropogenic Sensing Program. Ikonos and Quickbird optical satellite
images of sea surface glint revealed ~100 m spectral anomalies in km^2
averaging patches in ... | astro-ph | during fall periods in 2002 2003 and 2004 three major oceanographic expeditions were carried out in mamala bay hawaii these were part of the rasp remote anthropogenic sensing program ikonos and quickbird optical satellite images of sea surface glint revealed 100 m spectral anomalies in km2 averaging patches in regions ... | [['during', 'fall', 'periods', 'in', '2002', '2003', 'and', '2004', 'three', 'major', 'oceanographic', 'expeditions', 'were', 'carried', 'out', 'in', 'mamala', 'bay', 'hawaii', 'these', 'were', 'part', 'of', 'the', 'rasp', 'remote', 'anthropogenic', 'sensing', 'program', 'ikonos', 'and', 'quickbird', 'optical', 'satell... | [-0.12704298042459414, 0.23187406181838013, -0.041832035833213016, 0.09300641665351578, -0.05144228137505706, -0.07096298017539084, -0.008288946435786784, 0.3437648081080988, -0.2586126123619033, -0.332332125781104, 0.09355824240250513, -0.27455028156822664, -0.07425983751891181, 0.17004150877939536, -0.063417243354488... |
709.0075 | Final state hadronic interactions and non-resonant $B^\pm\to
K^\pm\pi^+\pi^-$ decays | We evaluate the non-resonant decay amplitude of the process $B^\pm\to
K^\pm\pi^+ \pi^-$ using an approach based on final state hadronic interactions
described in terms of meson exchanges. We conclude that this mechanism
generates inhomogeneities in the Dalitz plot of the B decay.
| hep-ph hep-ex | we evaluate the nonresonant decay amplitude of the process bpmto kpmpi pi using an approach based on final state hadronic interactions described in terms of meson exchanges we conclude that this mechanism generates inhomogeneities in the dalitz plot of the b decay | [['we', 'evaluate', 'the', 'nonresonant', 'decay', 'amplitude', 'of', 'the', 'process', 'bpmto', 'kpmpi', 'pi', 'using', 'an', 'approach', 'based', 'on', 'final', 'state', 'hadronic', 'interactions', 'described', 'in', 'terms', 'of', 'meson', 'exchanges', 'we', 'conclude', 'that', 'this', 'mechanism', 'generates', 'inh... | [-0.14136157003117772, 0.2361681719751398, -0.13989873683199333, 0.12307864441643732, -0.017419636726561116, -0.07153998696949423, 0.09799416592662655, 0.27960790284886594, -0.23387835140726188, -0.18005242998280177, -0.0806460701008668, -0.32576333944935626, -0.10472495790298392, 0.13291145624910913, 0.103374330145193... |
709.0076 | Entropy calculation for a toy black hole | In this note we carry out the counting of states for a black hole in loop
quantum gravity, however assuming an equidistant area spectrum. We find that
this toy-model is exactly solvable, and we show that its behavior is very
similar to that of the correct model. Thus this toy-model can be used as a nice
and simplifyi... | gr-qc hep-th math-ph math.MP | in this note we carry out the counting of states for a black hole in loop quantum gravity however assuming an equidistant area spectrum we find that this toymodel is exactly solvable and we show that its behavior is very similar to that of the correct model thus this toymodel can be used as a nice and simplifying labor... | [['in', 'this', 'note', 'we', 'carry', 'out', 'the', 'counting', 'of', 'states', 'for', 'a', 'black', 'hole', 'in', 'loop', 'quantum', 'gravity', 'however', 'assuming', 'an', 'equidistant', 'area', 'spectrum', 'we', 'find', 'that', 'this', 'toymodel', 'is', 'exactly', 'solvable', 'and', 'we', 'show', 'that', 'its', 'be... | [-0.09460485202905078, 0.08198453081400098, -0.16200195677005327, 0.1426335745688098, -0.051836403688559164, -0.1531744350679219, 0.03493256106292113, 0.36220752791716504, -0.2127101541711734, -0.2879352967326458, 0.07825204794868254, -0.26065913854310147, -0.17141044042431391, 0.2253444733778731, -0.07536964711661522,... |
709.0077 | Dependence of nuclear binding on hadronic mass variation | We examine how the binding of light ($A\leq 8$) nuclei depends on possible
variations of hadronic masses, including meson, nucleon, and nucleon-resonance
masses. Small variations in hadronic masses may have occurred over time; the
present results can help evaluate the consequences for big bang
nucleosynthesis. Larger... | nucl-th astro-ph hep-ph | we examine how the binding of light aleq 8 nuclei depends on possible variations of hadronic masses including meson nucleon and nucleonresonance masses small variations in hadronic masses may have occurred over time the present results can help evaluate the consequences for big bang nucleosynthesis larger variations ma... | [['we', 'examine', 'how', 'the', 'binding', 'of', 'light', 'aleq', '8', 'nuclei', 'depends', 'on', 'possible', 'variations', 'of', 'hadronic', 'masses', 'including', 'meson', 'nucleon', 'and', 'nucleonresonance', 'masses', 'small', 'variations', 'in', 'hadronic', 'masses', 'may', 'have', 'occurred', 'over', 'time', 'th... | [-0.0652724537774449, 0.23291242660487704, -0.06674977379309736, 0.1171031030118937, -0.03236651317833408, -0.06623785268468192, 0.055035598588840176, 0.33795378799648473, -0.19853350574559364, -0.32470160214361077, 0.021677818353177846, -0.34368606128647355, -0.005328607786975345, 0.15964013893542348, 0.01039219443992... |
709.0078 | Holding strategies in a bus-route model | A major source of delays in public transportation is the clustering
instability, which causes late buses to become progressively later while the
buses trailing it become progressively earlier. In this paper, we study this
instability and how to neutralize it using the common practices of holding and
schedule slack. S... | physics.soc-ph | a major source of delays in public transportation is the clustering instability which causes late buses to become progressively later while the buses trailing it become progressively earlier in this paper we study this instability and how to neutralize it using the common practices of holding and schedule slack startin... | [['a', 'major', 'source', 'of', 'delays', 'in', 'public', 'transportation', 'is', 'the', 'clustering', 'instability', 'which', 'causes', 'late', 'buses', 'to', 'become', 'progressively', 'later', 'while', 'the', 'buses', 'trailing', 'it', 'become', 'progressively', 'earlier', 'in', 'this', 'paper', 'we', 'study', 'this... | [-0.1403089055919554, 0.1334443355923577, -0.08623666231054812, 0.041308155964361506, -0.04236360481358133, -0.14630238382145763, 0.08467254393850453, 0.3811274018697441, -0.28813643094152214, -0.3108783174864948, 0.15812463774345814, -0.290370748732239, -0.1398806387768127, 0.19112708956003188, -0.06426213323138655, 0... |
709.0079 | Non-Abelian spin-orbit gauge: Persistent spin helix and quantum square
ring | We re-express the Rashba and Dresselhaus interactions as non-Abelian
spin-orbit gauges and provide a new perspective in understanding the persistent
spin helix [Phys. Rev. Lett. 97, 236601 (2006)]. A spin-orbit interacting
system can be transformed into a free electron gas in the equal-strength
Rashba-Dresselhaus [00... | cond-mat.mes-hall | we reexpress the rashba and dresselhaus interactions as nonabelian spinorbit gauges and provide a new perspective in understanding the persistent spin helix phys rev lett 97 236601 2006 a spinorbit interacting system can be transformed into a free electron gas in the equalstrength rashbadresselhaus 001 linear model the... | [['we', 'reexpress', 'the', 'rashba', 'and', 'dresselhaus', 'interactions', 'as', 'nonabelian', 'spinorbit', 'gauges', 'and', 'provide', 'a', 'new', 'perspective', 'in', 'understanding', 'the', 'persistent', 'spin', 'helix', 'phys', 'rev', 'lett', '97', '236601', '2006', 'a', 'spinorbit', 'interacting', 'system', 'can'... | [-0.23392753483879133, 0.16911751578931525, -0.01728306919498861, 0.0033704511006362736, -0.03823032478784334, -0.23322293537510735, 0.014405623037710716, 0.36823140530196846, -0.22529258779887074, -0.2828763477715119, -0.07916043827393672, -0.26499815124420906, -0.149557622760218, 0.1773299625327916, 0.018171018417836... |
709.008 | Magneto-Acoustic Spectroscopy in Superfluid 3He-B | We have used the recently discovered acoustic Faraday effect in superfluid
3He to perform high resolution spectroscopy of an excited state of the
superfluid condensate. With acoustic cavity interferometry we measure the
rotation of the plane of polarization of a transverse sound wave propagating in
the direction of m... | cond-mat.supr-con | we have used the recently discovered acoustic faraday effect in superfluid 3he to perform high resolution spectroscopy of an excited state of the superfluid condensate with acoustic cavity interferometry we measure the rotation of the plane of polarization of a transverse sound wave propagating in the direction of magn... | [['we', 'have', 'used', 'the', 'recently', 'discovered', 'acoustic', 'faraday', 'effect', 'in', 'superfluid', '3he', 'to', 'perform', 'high', 'resolution', 'spectroscopy', 'of', 'an', 'excited', 'state', 'of', 'the', 'superfluid', 'condensate', 'with', 'acoustic', 'cavity', 'interferometry', 'we', 'measure', 'the', 'ro... | [-0.17098652283343804, 0.22801505789243243, -0.07455119309284222, 0.019507546888684835, -0.04694279643532994, -0.04508119437249971, 0.025597567173683052, 0.3697535199430454, -0.23905615551540485, -0.2935671505037245, -0.025675347063352692, -0.27779082648947345, -0.010738862176927237, 0.18584057945594357, 0.102378133561... |
709.0081 | Photospheric processes and magnetic flux tubes | In the first part of these lecture notes, new high-resolution observations of
small-scale magnetic flux concentrations are presented and compared to results
from new three-dimensional magnetohydrodynamic simulations. Special attention
is paid to the physics of faculae and to new three-dimensional radiation
magnetohyd... | astro-ph | in the first part of these lecture notes new highresolution observations of smallscale magnetic flux concentrations are presented and compared to results from new threedimensional magnetohydrodynamic simulations special attention is paid to the physics of faculae and to new threedimensional radiation magnetohydrodynami... | [['in', 'the', 'first', 'part', 'of', 'these', 'lecture', 'notes', 'new', 'highresolution', 'observations', 'of', 'smallscale', 'magnetic', 'flux', 'concentrations', 'are', 'presented', 'and', 'compared', 'to', 'results', 'from', 'new', 'threedimensional', 'magnetohydrodynamic', 'simulations', 'special', 'attention', '... | [-0.12578910350111983, 0.12815433419848432, -0.0063649128533143084, 0.0774932646745583, -0.07337848705356009, -0.0564427925455675, -0.004418669363076333, 0.32832616075029364, -0.24878716556122527, -0.34079936768102925, 0.10675430022274668, -0.2410960813449492, -0.07609646435594186, 0.20295709680431173, -0.0073371030521... |
709.0082 | Observational signatures of Jordan-Brans-Dicke theories of gravity | We analyze the Jordan-Brans-Dicke model (JBD) of gravity, where deviations
from General Relativity (GR) are described by a scalar field non-minimally
coupled to gravity. The theory is characterized by a constant coupling
parameter, $\omega_{\rm JBD}$; GR is recovered in the limit $\omega_{\rm JBD}
\to \infty$. In suc... | astro-ph | we analyze the jordanbransdicke model jbd of gravity where deviations from general relativity gr are described by a scalar field nonminimally coupled to gravity the theory is characterized by a constant coupling parameter omega_rm jbd gr is recovered in the limit omega_rm jbd to infty in such theories gravity modificat... | [['we', 'analyze', 'the', 'jordanbransdicke', 'model', 'jbd', 'of', 'gravity', 'where', 'deviations', 'from', 'general', 'relativity', 'gr', 'are', 'described', 'by', 'a', 'scalar', 'field', 'nonminimally', 'coupled', 'to', 'gravity', 'the', 'theory', 'is', 'characterized', 'by', 'a', 'constant', 'coupling', 'parameter... | [-0.08779665766837629, 0.14531811841738385, -0.10933100581924254, 0.1425726259832044, -0.1035538185337508, -0.14168577021793335, -0.05369631682170203, 0.29433981185225216, -0.20671051891419936, -0.3272693657140071, 0.08821076411703552, -0.27620411211675083, -0.10557120017002564, 0.19683634830965988, -0.0297458563528945... |
709.0083 | Embedding of the Lie superalgebra $D(2, 1 ; \alpha)$ into the Lie
superalgebra of pseudodifferential symbols on $S^{1|2}$ | We obtain an embedding of a one-parameter family of exceptional simple Lie
superalgebras $D(2, 1 ; \alpha)$ into the Lie superalgebra of
pseudodifferential symbols on the supercircle $S^{1|2}$. Correspondingly, there
is an embedding of $D(2, 1 ; \alpha)$ into a nontrivial central extension of
the derived contact supe... | math-ph math.MP | we obtain an embedding of a oneparameter family of exceptional simple lie superalgebras d2 1 alpha into the lie superalgebra of pseudodifferential symbols on the supercircle s12 correspondingly there is an embedding of d2 1 alpha into a nontrivial central extension of the derived contact superconformal algebra k4 reali... | [['we', 'obtain', 'an', 'embedding', 'of', 'a', 'oneparameter', 'family', 'of', 'exceptional', 'simple', 'lie', 'superalgebras', 'd2', '1', 'alpha', 'into', 'the', 'lie', 'superalgebra', 'of', 'pseudodifferential', 'symbols', 'on', 'the', 'supercircle', 's12', 'correspondingly', 'there', 'is', 'an', 'embedding', 'of', ... | [-0.2092382321449912, 0.07445676928293354, 0.022321560964682848, 0.02952914472503619, -0.0855463874542107, -0.22084938691360717, -0.05123202983779296, 0.33663016444040555, -0.25549522990960694, -0.19208952573806806, 0.11042891906661187, -0.2782823654302096, -0.15042410557300356, 0.1664788504880932, -0.06649824984419017... |
709.0084 | A Fixed Point Conjecture | Inverse limits, unlike direct limits, can in general be void, [1]. The
existence of fixed points for arbitrary mappings $T : X \longrightarrow X$ is
conjectured to be equivalent with the fact that related direct limits of all
finite partitions of X are not void.
| math.GM | inverse limits unlike direct limits can in general be void 1 the existence of fixed points for arbitrary mappings t x longrightarrow x is conjectured to be equivalent with the fact that related direct limits of all finite partitions of x are not void | [['inverse', 'limits', 'unlike', 'direct', 'limits', 'can', 'in', 'general', 'be', 'void', '1', 'the', 'existence', 'of', 'fixed', 'points', 'for', 'arbitrary', 'mappings', 't', 'x', 'longrightarrow', 'x', 'is', 'conjectured', 'to', 'be', 'equivalent', 'with', 'the', 'fact', 'that', 'related', 'direct', 'limits', 'of',... | [-0.13250514505092392, 0.13284395545170727, -0.04330088511448015, 0.051935324395096606, -0.08790854694300586, -0.11470888339152391, 0.0746894350106066, 0.3677324265326289, -0.28106254775246436, -0.20764365962664175, 0.11543001015194353, -0.27261121524497867, -0.04967236407736147, 0.19835768747990104, -0.036150843370705... |
709.0085 | Sodium vacancy ordering and the co-existence of localized spins and
itinerant charges in NaxCoO2 | The sodium cobaltate family (NaxCoO2) is unique among transition metal oxides
because the Co sits on a triangular lattice and its valence can be tuned over a
wide range by varying the Na concentration x. Up to now detailed modeling of
the rich phenomenology (which ranges from unconventional superconductivity to
enhan... | cond-mat.str-el | the sodium cobaltate family naxcoo2 is unique among transition metal oxides because the co sits on a triangular lattice and its valence can be tuned over a wide range by varying the na concentration x up to now detailed modeling of the rich phenomenology which ranges from unconventional superconductivity to enhanced th... | [['the', 'sodium', 'cobaltate', 'family', 'naxcoo2', 'is', 'unique', 'among', 'transition', 'metal', 'oxides', 'because', 'the', 'co', 'sits', 'on', 'a', 'triangular', 'lattice', 'and', 'its', 'valence', 'can', 'be', 'tuned', 'over', 'a', 'wide', 'range', 'by', 'varying', 'the', 'na', 'concentration', 'x', 'up', 'to', ... | [-0.12190620971462095, 0.19806209126913762, -0.05379721556133759, 0.014670482644858962, -0.03144754273452269, -0.1601161476286375, 0.13091200408006806, 0.3852246320197718, -0.2606234236238861, -0.31675713763611546, -0.007753155800494287, -0.326791407777479, -0.07474725898663816, 0.1693571685330875, 0.016663281160442446... |
709.0086 | A wildland fire model with data assimilation | A wildfire model is formulated based on balance equations for energy and
fuel, where the fuel loss due to combustion corresponds to the fuel reaction
rate. The resulting coupled partial differential equations have coefficients
that can be approximated from prior measurements of wildfires. An ensemble
Kalman filter te... | math.NA | a wildfire model is formulated based on balance equations for energy and fuel where the fuel loss due to combustion corresponds to the fuel reaction rate the resulting coupled partial differential equations have coefficients that can be approximated from prior measurements of wildfires an ensemble kalman filter techniq... | [['a', 'wildfire', 'model', 'is', 'formulated', 'based', 'on', 'balance', 'equations', 'for', 'energy', 'and', 'fuel', 'where', 'the', 'fuel', 'loss', 'due', 'to', 'combustion', 'corresponds', 'to', 'the', 'fuel', 'reaction', 'rate', 'the', 'resulting', 'coupled', 'partial', 'differential', 'equations', 'have', 'coeffi... | [0.004170817859965015, 0.09054923324865925, -0.11923935719348766, 0.035258721209805916, -0.05698908875430269, -0.15738439656394934, 0.026887929575441748, 0.35425338898880443, -0.28606072896426277, -0.32274824890251064, 0.13535763384128102, -0.3141495269837276, -0.07329676414326745, 0.1913559337084809, -0.06772502921331... |
709.0087 | Research News -- Quantum Mechanical Entanglement and Tests of CPT
Theorem with Neutral Mesons at e+ e- Colliders | We review the recent confirmation of quantum entanglement in e+ e- collisions
at the BELLE experiment at KEK-B in Japan with neutral B- mesons, and at the
KLOE experiment at the DAFNE in Italy with neutral K- mesons. Such effects in
the latter system seen already in proton-antiproton collisions by the CPLEAR
experime... | physics.pop-ph hep-ph physics.ed-ph quant-ph | we review the recent confirmation of quantum entanglement in e e collisions at the belle experiment at kekb in japan with neutral b mesons and at the kloe experiment at the dafne in italy with neutral k mesons such effects in the latter system seen already in protonantiproton collisions by the cplear experiment are als... | [['we', 'review', 'the', 'recent', 'confirmation', 'of', 'quantum', 'entanglement', 'in', 'e', 'e', 'collisions', 'at', 'the', 'belle', 'experiment', 'at', 'kekb', 'in', 'japan', 'with', 'neutral', 'b', 'mesons', 'and', 'at', 'the', 'kloe', 'experiment', 'at', 'the', 'dafne', 'in', 'italy', 'with', 'neutral', 'k', 'mes... | [-0.053790917840639225, 0.19924149754163073, -0.09484618730034287, 0.05675761391237182, 0.033787377920050765, -0.17601485817546123, 0.0143670560516368, 0.2910735190012737, -0.10667931952660806, -0.2616101319573844, -0.013337597002789966, -0.43588546782388893, 0.015244161416041223, 0.1817823611261127, 0.0531525614634646... |
709.0088 | Revisiting Quaternionic Dual Electrodynamics | Dual electrodynamics and corresponding Maxwell's equations (in the presence
of monopole only) are revisited from dual symmetry and accordingly the
quaternionic reformulation of field equations and equation of motion is
developed in simple, compact and consistent manner.
| hep-th | dual electrodynamics and corresponding maxwells equations in the presence of monopole only are revisited from dual symmetry and accordingly the quaternionic reformulation of field equations and equation of motion is developed in simple compact and consistent manner | [['dual', 'electrodynamics', 'and', 'corresponding', 'maxwells', 'equations', 'in', 'the', 'presence', 'of', 'monopole', 'only', 'are', 'revisited', 'from', 'dual', 'symmetry', 'and', 'accordingly', 'the', 'quaternionic', 'reformulation', 'of', 'field', 'equations', 'and', 'equation', 'of', 'motion', 'is', 'developed',... | [-0.12586288264877088, 0.08725283669647635, -0.07361045197860615, 0.033141884062363694, -0.16434207003613985, -0.13938004480725205, -0.05752032079003953, 0.2951728944238779, -0.21333920301215067, -0.26823856872884005, 0.0730175294070127, -0.2573876423207489, -0.18410296300174417, 0.14714188717708393, -0.075132529553328... |
709.0089 | New q-Euler numbers and polynomials associated with p-adic q-integrals | In this paper we study q-Euler numbers and polynomials by using p-adic
q-fermionic integrals on Z_p. The methods to study q-Euler numbers and
polynomials in this paper are new.
| math.NT | in this paper we study qeuler numbers and polynomials by using padic qfermionic integrals on z_p the methods to study qeuler numbers and polynomials in this paper are new | [['in', 'this', 'paper', 'we', 'study', 'qeuler', 'numbers', 'and', 'polynomials', 'by', 'using', 'padic', 'qfermionic', 'integrals', 'on', 'z_p', 'the', 'methods', 'to', 'study', 'qeuler', 'numbers', 'and', 'polynomials', 'in', 'this', 'paper', 'are', 'new']] | [-0.25052422870482716, 0.0985391229457621, -0.13152809321348155, 0.08563933992991224, -0.09766898264310189, -0.02464537914576275, 0.03769607267375769, 0.29331405547314454, -0.31984350324741434, -0.2481004489319665, 0.051628912740852684, -0.25744946726730894, -0.2766217428392598, 0.25418480911425184, -0.1627163799213511... |
709.009 | Accretion onto the Companion of Eta Carinae During the Spectroscopic
Event. V. the Infrared Decline | We propose that the decline in the near-IR flux from the massive binary
system Eta Carinae during the spectroscopic event might be explained by
accreted mass that absorbs the radiation from the secondary star, and by that
reduces the heating of the dust that is responsible for the near-IR emission.
This binary system... | astro-ph | we propose that the decline in the nearir flux from the massive binary system eta carinae during the spectroscopic event might be explained by accreted mass that absorbs the radiation from the secondary star and by that reduces the heating of the dust that is responsible for the nearir emission this binary system has a... | [['we', 'propose', 'that', 'the', 'decline', 'in', 'the', 'nearir', 'flux', 'from', 'the', 'massive', 'binary', 'system', 'eta', 'carinae', 'during', 'the', 'spectroscopic', 'event', 'might', 'be', 'explained', 'by', 'accreted', 'mass', 'that', 'absorbs', 'the', 'radiation', 'from', 'the', 'secondary', 'star', 'and', '... | [-0.10370962388937387, 0.17372525358310134, -0.0690347240968616, 0.05795812681146444, -0.07375170525970844, -0.04187173685037591, 0.03072774830838204, 0.39399106739037626, -0.22891758528266767, -0.30285542236145485, 0.08891020374321336, -0.3062506796142787, -0.03629697137058353, 0.1881302095610016, -0.07448005559333544... |
709.0091 | Gaseous Flows in Galaxies | The gas component plays a major role in the dynamics of spiral galaxies,
because of its dissipative character, and its ability to exchange angular
momentum with stars in the disk. Due to its small velocity dispersion, it
triggers gravitational instabilities, and the corresponding non-axisymmetric
patterns produce gra... | astro-ph | the gas component plays a major role in the dynamics of spiral galaxies because of its dissipative character and its ability to exchange angular momentum with stars in the disk due to its small velocity dispersion it triggers gravitational instabilities and the corresponding nonaxisymmetric patterns produce gravity tor... | [['the', 'gas', 'component', 'plays', 'a', 'major', 'role', 'in', 'the', 'dynamics', 'of', 'spiral', 'galaxies', 'because', 'of', 'its', 'dissipative', 'character', 'and', 'its', 'ability', 'to', 'exchange', 'angular', 'momentum', 'with', 'stars', 'in', 'the', 'disk', 'due', 'to', 'its', 'small', 'velocity', 'dispersio... | [-0.16090325915009837, 0.1753873174364023, -0.08153692162629929, 0.07095133422562332, -0.09181307341136477, -0.03893177762545426, -0.03470004628830151, 0.38062232760164666, -0.2937435899203753, -0.28253737309098464, 0.041049018513363345, -0.2705403074676938, -0.03793665431165958, 0.16223654726876274, 0.0243672469964220... |
709.0092 | Theorie ergodique des fractions rationnelles sur un corps ultrametrique | We make the first steps towards an understanding of the ergodic properties of
a rational map defined over a complete algebraically closed non-archimedean
field. For such a rational map R, we construct a natural invariant probability
measure m_R which reprensents the asymptotic distribution of preimages of
non-excepti... | math.DS | we make the first steps towards an understanding of the ergodic properties of a rational map defined over a complete algebraically closed nonarchimedean field for such a rational map r we construct a natural invariant probability measure m_r which reprensents the asymptotic distribution of preimages of nonexceptional p... | [['we', 'make', 'the', 'first', 'steps', 'towards', 'an', 'understanding', 'of', 'the', 'ergodic', 'properties', 'of', 'a', 'rational', 'map', 'defined', 'over', 'a', 'complete', 'algebraically', 'closed', 'nonarchimedean', 'field', 'for', 'such', 'a', 'rational', 'map', 'r', 'we', 'construct', 'a', 'natural', 'invaria... | [-0.19944705083085004, 0.07413190696779663, -0.14998938776152107, 0.10617504440127842, -0.01965417326377925, -0.12884427393756567, 0.07707535116983358, 0.31885209558181143, -0.29378763542220154, -0.1711387564077653, 0.08788323538097483, -0.2816127485205089, -0.1537546462226679, 0.19911403277067727, -0.10168997014764217... |
709.0093 | Data formats for numerical relativity waves | This document proposes data formats to exchange numerical relativity results,
in particular gravitational waveforms. The primary goal is to further the
interaction between gravitational-wave source modeling groups and the
gravitational-wave data-analysis community. We present a simple and extendable
format which is a... | gr-qc | this document proposes data formats to exchange numerical relativity results in particular gravitational waveforms the primary goal is to further the interaction between gravitationalwave source modeling groups and the gravitationalwave dataanalysis community we present a simple and extendable format which is applicabl... | [['this', 'document', 'proposes', 'data', 'formats', 'to', 'exchange', 'numerical', 'relativity', 'results', 'in', 'particular', 'gravitational', 'waveforms', 'the', 'primary', 'goal', 'is', 'to', 'further', 'the', 'interaction', 'between', 'gravitationalwave', 'source', 'modeling', 'groups', 'and', 'the', 'gravitation... | [-0.15424022270433072, 0.08159076147712767, -0.06346549361145921, 0.14287987362393842, -0.17322890012791115, -0.11952710381842085, -0.024893332502272512, 0.3899627126154623, -0.21234403449509826, -0.29275055055040866, 0.08224733681916925, -0.254010042840881, -0.1516599116979965, 0.29508065884666784, -0.0245192390600485... |
709.0094 | Nonresonant microwave absorption in epitaxial La-Sr-Mn-O films and its
relation to colossal magnetoresistance | We study magnetic-field-dependent nonresonant microwave absorption and
dispersion in thin La$_{0.7}$Sr$_{0.3}$MnO$_{3}$ films and show that it
originates from the colossal magnetoresistance. We develop the model for
magnetoresistance of a thin ferromagnetic film in oblique magnetic field. The
model accounts fairly we... | cond-mat.str-el cond-mat.mtrl-sci | we study magneticfielddependent nonresonant microwave absorption and dispersion in thin la_07sr_03mno_3 films and show that it originates from the colossal magnetoresistance we develop the model for magnetoresistance of a thin ferromagnetic film in oblique magnetic field the model accounts fairly well for our experimen... | [['we', 'study', 'magneticfielddependent', 'nonresonant', 'microwave', 'absorption', 'and', 'dispersion', 'in', 'thin', 'la_07sr_03mno_3', 'films', 'and', 'show', 'that', 'it', 'originates', 'from', 'the', 'colossal', 'magnetoresistance', 'we', 'develop', 'the', 'model', 'for', 'magnetoresistance', 'of', 'a', 'thin', '... | [-0.15922053153044544, 0.13727342590573244, -0.01722790829371661, -0.012323152301541995, -0.11066492816898972, -0.1362371803028509, 0.015545994957210495, 0.4637290719896555, -0.24346727449446917, -0.32443817970342936, -0.015629255733801983, -0.29235730873497234, -0.15008456294890493, 0.3321046512981411, 0.0655116097186... |
709.0095 | 8D-spectral triple on 4D-Moyal space and the vacuum of noncommutative
gauge theory | Observing that the Hamiltonian of the renormalisable scalar field theory on
4-dimensional Moyal space A is the square of a Dirac operator D of spectral
dimension 8, we complete (A,D) to a compact 8-dimensional spectral triple. We
add another Connes-Lott copy and compute the spectral action of the
corresponding U(1)-Y... | hep-th | observing that the hamiltonian of the renormalisable scalar field theory on 4dimensional moyal space a is the square of a dirac operator d of spectral dimension 8 we complete ad to a compact 8dimensional spectral triple we add another conneslott copy and compute the spectral action of the corresponding u1yangmillshiggs... | [['observing', 'that', 'the', 'hamiltonian', 'of', 'the', 'renormalisable', 'scalar', 'field', 'theory', 'on', '4dimensional', 'moyal', 'space', 'a', 'is', 'the', 'square', 'of', 'a', 'dirac', 'operator', 'd', 'of', 'spectral', 'dimension', '8', 'we', 'complete', 'ad', 'to', 'a', 'compact', '8dimensional', 'spectral', ... | [-0.19086112033956767, 0.19884164784929123, -0.08210984069261361, 0.08549695761281659, -0.1172045692674477, -0.18550800670107656, -0.01779404065508226, 0.3242433302104473, -0.18573348597644573, -0.22222060177644545, 0.037506956188008186, -0.24568495334718715, -0.13585133988579565, 0.10489115706560287, -0.02174186871641... |
709.0096 | The magic functions and automorphisms of a domain | We introduce the notion of magic functions of a general domain in
d-dimensional complex space and show that the set of magic functions of a given
domain is an intrinsic complex-geometric object. We determine the set of magic
functions of the symmetrised bidisc G, and thereby find all automorphisms of G
and a formula ... | math.CV math.FA | we introduce the notion of magic functions of a general domain in ddimensional complex space and show that the set of magic functions of a given domain is an intrinsic complexgeometric object we determine the set of magic functions of the symmetrised bidisc g and thereby find all automorphisms of g and a formula for th... | [['we', 'introduce', 'the', 'notion', 'of', 'magic', 'functions', 'of', 'a', 'general', 'domain', 'in', 'ddimensional', 'complex', 'space', 'and', 'show', 'that', 'the', 'set', 'of', 'magic', 'functions', 'of', 'a', 'given', 'domain', 'is', 'an', 'intrinsic', 'complexgeometric', 'object', 'we', 'determine', 'the', 'set... | [-0.14449420295034845, 0.0776575792680281, -0.06299110784505804, 0.0775075530904966, -0.08781259189515064, -0.04277028979267925, 0.06306479321792721, 0.38051645160497477, -0.27441764312485856, -0.25908026909455656, 0.0793484513706062, -0.2475658073866119, -0.147697291377699, 0.19210158546144765, -0.08811649272684008, 0... |
709.0097 | Identification of NeVIII lines in H-deficient (pre-) white dwarfs: a new
tool to constrain the temperature of the hottest stars | For the first time, we have identified NeVIII absorption lines in far-UV
spectra of the hottest known (Teff>150,000 K) hydrogen-deficient (pre-) white
dwarfs of spectral type PG1159. They are of photospheric origin and can be
matched by synthetic non-LTE line profiles. We also show that a number of UV
and optical emi... | astro-ph | for the first time we have identified neviii absorption lines in faruv spectra of the hottest known teff150000 k hydrogendeficient pre white dwarfs of spectral type pg1159 they are of photospheric origin and can be matched by synthetic nonlte line profiles we also show that a number of uv and optical emission lines in ... | [['for', 'the', 'first', 'time', 'we', 'have', 'identified', 'neviii', 'absorption', 'lines', 'in', 'faruv', 'spectra', 'of', 'the', 'hottest', 'known', 'teff150000', 'k', 'hydrogendeficient', 'pre', 'white', 'dwarfs', 'of', 'spectral', 'type', 'pg1159', 'they', 'are', 'of', 'photospheric', 'origin', 'and', 'can', 'be'... | [-0.02400924485427728, 0.17039207042161125, -0.01919614209991354, 0.1110979805572605, -0.10710891079485725, -0.14781704408308452, 0.05287062730688428, 0.48152460765884947, -0.1653402258806085, -0.32725567451721643, 0.05378612273293089, -0.2977785260291104, -0.023938541569616743, 0.15870231099986504, -0.0730702629978792... |
709.0098 | WMAP-Compliant Benchmark Surfaces for MSSM Higgs Bosons | We explore `benchmark surfaces' suitable for studying the phenomenology of
Higgs bosons in the minimal supersymmetric extension of the Standard Model
(MSSM), which are chosen so that the supersymmetric relic density is generally
compatible with the range of cold dark matter density preferred by WMAP and
other observa... | hep-ph | we explore benchmark surfaces suitable for studying the phenomenology of higgs bosons in the minimal supersymmetric extension of the standard model mssm which are chosen so that the supersymmetric relic density is generally compatible with the range of cold dark matter density preferred by wmap and other observations t... | [['we', 'explore', 'benchmark', 'surfaces', 'suitable', 'for', 'studying', 'the', 'phenomenology', 'of', 'higgs', 'bosons', 'in', 'the', 'minimal', 'supersymmetric', 'extension', 'of', 'the', 'standard', 'model', 'mssm', 'which', 'are', 'chosen', 'so', 'that', 'the', 'supersymmetric', 'relic', 'density', 'is', 'general... | [-0.09736346813605917, 0.23653033787816571, -0.012964307104106766, 0.1613590568907434, -0.10739235157039152, -0.20257044185475423, -0.003950143298247784, 0.3573537454514469, -0.21174834067819687, -0.33150059724135733, 0.06597069010320233, -0.261099939129497, -0.02057584027174815, 0.1986902494738787, 0.02952725976980972... |
709.0099 | The road coloring problem | The synchronizing word of deterministic automaton is a word in the alphabet
of colors (considered as letters) of its edges that maps the automaton to a
single state. A coloring of edges of a directed graph is synchronizing if the
coloring turns the graph into deterministic finite automaton possessing a
synchronizing ... | cs.DM | the synchronizing word of deterministic automaton is a word in the alphabet of colors considered as letters of its edges that maps the automaton to a single state a coloring of edges of a directed graph is synchronizing if the coloring turns the graph into deterministic finite automaton possessing a synchronizing word ... | [['the', 'synchronizing', 'word', 'of', 'deterministic', 'automaton', 'is', 'a', 'word', 'in', 'the', 'alphabet', 'of', 'colors', 'considered', 'as', 'letters', 'of', 'its', 'edges', 'that', 'maps', 'the', 'automaton', 'to', 'a', 'single', 'state', 'a', 'coloring', 'of', 'edges', 'of', 'a', 'directed', 'graph', 'is', '... | [-0.20214565462273362, 0.16215266059220268, -0.02354632199242495, 0.03633791566117788, -0.12270748063051344, -0.1855405857651562, 0.11616935501587104, 0.3854847837212509, -0.3499191771328881, -0.25498050429345365, 0.06357665010517044, -0.3392952869416795, -0.14160074695836808, 0.10689077469641747, -0.12742317612350418,... |
709.01 | Saturation effects in elastic scattering at the LHC | The problems linked to the extraction of the basic parameters of the hadron
elastic scattering amplitude at the LHC are explored. The impact of the Black
Disk Limit (BDL)$-$ which constitutes a new regime of the scattering processes
- on the determination of these values is examined.
| hep-ph | the problems linked to the extraction of the basic parameters of the hadron elastic scattering amplitude at the lhc are explored the impact of the black disk limit bdl which constitutes a new regime of the scattering processes on the determination of these values is examined | [['the', 'problems', 'linked', 'to', 'the', 'extraction', 'of', 'the', 'basic', 'parameters', 'of', 'the', 'hadron', 'elastic', 'scattering', 'amplitude', 'at', 'the', 'lhc', 'are', 'explored', 'the', 'impact', 'of', 'the', 'black', 'disk', 'limit', 'bdl', 'which', 'constitutes', 'a', 'new', 'regime', 'of', 'the', 'sca... | [-0.12209932607315156, 0.1495255144191501, -0.08829052196613149, 0.08233136422780302, -0.03899580333381891, -0.04354644081879245, 0.035541275799598385, 0.2649430530550687, -0.27578998454239056, -0.23802639394188704, 0.10932222648483256, -0.2955309413778393, -0.04600125757734413, 0.22378238468714381, 0.06354774501296165... |
709.0101 | Heegaard genus and Property 'tau' for hyperbolic 3-manifolds | We show that any finitely generated non-elementary Kleinian group has a
co-final family of finite index normal subgroups with respect to which it has
Property $\tau$. As a consequence, any closed hyperbolic 3-manifold has a
co-final family of finite index normal subgroups for which the infimal Heegaard
gradient is po... | math.GT math.GR | we show that any finitely generated nonelementary kleinian group has a cofinal family of finite index normal subgroups with respect to which it has property tau as a consequence any closed hyperbolic 3manifold has a cofinal family of finite index normal subgroups for which the infimal heegaard gradient is positive | [['we', 'show', 'that', 'any', 'finitely', 'generated', 'nonelementary', 'kleinian', 'group', 'has', 'a', 'cofinal', 'family', 'of', 'finite', 'index', 'normal', 'subgroups', 'with', 'respect', 'to', 'which', 'it', 'has', 'property', 'tau', 'as', 'a', 'consequence', 'any', 'closed', 'hyperbolic', '3manifold', 'has', 'a... | [-0.1729092556424439, 0.1957325735501945, -0.1615990449860692, 0.06061048957752064, -0.16415607783943414, -0.18318748825229705, -0.014916852451860904, 0.4198967437446117, -0.36430693306028844, -0.1764302741701249, 0.08469566539861262, -0.2988183802738786, -0.07856832231394946, 0.22752052616328, -0.17338551634922625, -0... |
709.0102 | Towards the First Galaxies | The formation of the first galaxies at redshifts z~10-15 signaled the
transition from the simple initial state of the universe to one of ever
increasing complexity. We here review recent progress in understanding their
assembly process with numerical simulations, starting with cosmological initial
conditions and mode... | astro-ph | the formation of the first galaxies at redshifts z1015 signaled the transition from the simple initial state of the universe to one of ever increasing complexity we here review recent progress in understanding their assembly process with numerical simulations starting with cosmological initial conditions and modelling ... | [['the', 'formation', 'of', 'the', 'first', 'galaxies', 'at', 'redshifts', 'z1015', 'signaled', 'the', 'transition', 'from', 'the', 'simple', 'initial', 'state', 'of', 'the', 'universe', 'to', 'one', 'of', 'ever', 'increasing', 'complexity', 'we', 'here', 'review', 'recent', 'progress', 'in', 'understanding', 'their', ... | [-0.06165081083022487, 0.13623200297643917, -0.06784588469391954, 0.07056192581046436, -0.08988090532384665, -0.002624710641121344, 0.04595809393665857, 0.3820156979832857, -0.18180767532497172, -0.3203602758132749, 0.060036831812578295, -0.26752431716932545, -0.06395660701488691, 0.1742584982827779, 0.0339954773674161... |
709.0103 | On the low regularity of the fifth order Kadomtsev-Petviashvili I
equation | We consider the fifth order Kadomtsev-Petviashvili I (KP-I) equation as
$\partial_tu+\alpha\partial_x^3u+\partial^5_xu+\partial_x^{-1}\partial_y^2u+uu_x=0,$
while $\alpha\in \mathbb{R}$. We introduce an interpolated energy space $E_s$
to consider the well-posedeness of the initial value problem (IVP) of the fifth
ord... | math.AP math-ph math.MP | we consider the fifth order kadomtsevpetviashvili i kpi equation as partial_tualphapartial_x3upartial5_xupartial_x1partial_y2uuu_x0 while alphain mathbbr we introduce an interpolated energy space e_s to consider the wellposedeness of the initial value problem ivp of the fifth order kpi equation we obtain the local well... | [['we', 'consider', 'the', 'fifth', 'order', 'kadomtsevpetviashvili', 'i', 'kpi', 'equation', 'as', 'partial_tualphapartial_x3upartial5_xupartial_x1partial_y2uuu_x0', 'while', 'alphain', 'mathbbr', 'we', 'introduce', 'an', 'interpolated', 'energy', 'space', 'e_s', 'to', 'consider', 'the', 'wellposedeness', 'of', 'the',... | [-0.18069581734863194, 0.060555030080749105, -0.07486628273671324, 0.12481585884974762, -0.12575215732848102, -0.07337274151346222, -0.04755956612908366, 0.20217331471768293, -0.33331906937740063, -0.2048962884074585, 0.12542438247262247, -0.30041251798922364, -0.07898976393520239, 0.12537321649883365, 0.01488789591768... |
709.0104 | Symmetry classes connected with the magnetic Heisenberg ring | We define symmetry classes and commutation symmetries in the Hilbert space H
of the 1D spin-1/2 Heisenberg magnetic ring with N sites and investigate them
by means of tools from the representation theory of symmetric groups S_N such
as decompositions of ideals of the group ring C[S_N], idempotents of C[S_N],
discrete... | math.CO math.QA | we define symmetry classes and commutation symmetries in the hilbert space h of the 1d spin12 heisenberg magnetic ring with n sites and investigate them by means of tools from the representation theory of symmetric groups s_n such as decompositions of ideals of the group ring cs_n idempotents of cs_n discrete fourier t... | [['we', 'define', 'symmetry', 'classes', 'and', 'commutation', 'symmetries', 'in', 'the', 'hilbert', 'space', 'h', 'of', 'the', '1d', 'spin12', 'heisenberg', 'magnetic', 'ring', 'with', 'n', 'sites', 'and', 'investigate', 'them', 'by', 'means', 'of', 'tools', 'from', 'the', 'representation', 'theory', 'of', 'symmetric'... | [-0.17229984649906824, 0.12573313428282828, -0.026729051684114068, 0.011756972947411917, -0.06910761995029381, -0.1372473092114722, 0.006545828492909839, 0.33923502501354297, -0.3424454973121597, -0.214216947380919, 0.09076297805983234, -0.3127943095878105, -0.08251750487940047, 0.13771867138778113, -0.0048267731358381... |
709.0105 | Representations and characters of the Virasoro algebra and N=1
super-Virasoro algebras | We present the list of irreducible (generalized) highest weight modules over
the Virasoro algebra and N=1 super-Virasoro algebras obtained as factor-modules
of (generalized) Verma modules. We present also the character formulae of all
these modules and single out the unitary irreducible ones. Most formulas are
valid ... | hep-th math-ph math.MP math.QA math.RT | we present the list of irreducible generalized highest weight modules over the virasoro algebra and n1 supervirasoro algebras obtained as factormodules of generalized verma modules we present also the character formulae of all these modules and single out the unitary irreducible ones most formulas are valid for the thr... | [['we', 'present', 'the', 'list', 'of', 'irreducible', 'generalized', 'highest', 'weight', 'modules', 'over', 'the', 'virasoro', 'algebra', 'and', 'n1', 'supervirasoro', 'algebras', 'obtained', 'as', 'factormodules', 'of', 'generalized', 'verma', 'modules', 'we', 'present', 'also', 'the', 'character', 'formulae', 'of',... | [-0.17296961155058682, 0.09567244683358181, -0.03632432115736647, 0.045391044140779886, -0.06671549914998637, -0.18020098856852754, -0.055516081322254475, 0.33487931736137555, -0.3095543011769895, -0.1973461933919917, 0.1457801889628172, -0.24148142095815484, -0.13525653425334155, 0.20669508799640596, -0.06504361125521... |
709.0106 | Antiphase Stripe Order as the Origin of Electron Pockets Observed in
1/8-Hole-Doped Cuprates | Recent quantum oscillation measurements on underdoped cuprates are shown to
be consistent with the predictions of a mean field theory of the 1/8 magnetic
antiphase stripe order proposed to occur in high-$T_c$ cuprates. In particular,
for intermediate values of the stripe order parameter, the magneto-transport is
foun... | cond-mat.supr-con cond-mat.str-el | recent quantum oscillation measurements on underdoped cuprates are shown to be consistent with the predictions of a mean field theory of the 18 magnetic antiphase stripe order proposed to occur in hight_c cuprates in particular for intermediate values of the stripe order parameter the magnetotransport is found to be do... | [['recent', 'quantum', 'oscillation', 'measurements', 'on', 'underdoped', 'cuprates', 'are', 'shown', 'to', 'be', 'consistent', 'with', 'the', 'predictions', 'of', 'a', 'mean', 'field', 'theory', 'of', 'the', '18', 'magnetic', 'antiphase', 'stripe', 'order', 'proposed', 'to', 'occur', 'in', 'hight_c', 'cuprates', 'in',... | [-0.17513598633404062, 0.23864156062336406, -0.021215913437858776, 0.06707985465699393, -0.05777546939336591, -0.1021285199439498, 0.05696769139979518, 0.3305768269907545, -0.22081397801499675, -0.29303010861676065, 0.016640667713040277, -0.3625086982975955, -0.09338018638771717, 0.2274025705539518, -0.0071546492184063... |
709.0107 | Real-world ballistics: A dropped bucket | I discuss an apparently simple ballistics problem: the time it takes an
object to fall a small vertical distance near the surface of the Earth. It
turns out to be not so simple; I spend a great deal of time on the quantitative
assessment of the assumptions involved, especially with regards to the
influence of the air... | physics.ed-ph | i discuss an apparently simple ballistics problem the time it takes an object to fall a small vertical distance near the surface of the earth it turns out to be not so simple i spend a great deal of time on the quantitative assessment of the assumptions involved especially with regards to the influence of the air the p... | [['i', 'discuss', 'an', 'apparently', 'simple', 'ballistics', 'problem', 'the', 'time', 'it', 'takes', 'an', 'object', 'to', 'fall', 'a', 'small', 'vertical', 'distance', 'near', 'the', 'surface', 'of', 'the', 'earth', 'it', 'turns', 'out', 'to', 'be', 'not', 'so', 'simple', 'i', 'spend', 'a', 'great', 'deal', 'of', 't... | [-0.06960534046145582, 0.10015460242092081, -0.10887628169414604, 0.10095080742277047, -0.11606506475492112, -0.16838702130904895, 0.021670171683180636, 0.3459191129037763, -0.2894764271470071, -0.31161680068599723, 0.12418902945365377, -0.2864773808347093, -0.13723162390583715, 0.18648718467467637, -0.0819603235271396... |
709.0108 | X-ray Group and cluster mass profiles in MOND: Unexplained mass on the
group scale | Although very successful in explaining the observed conspiracy between the
baryonic distribution and the gravitational field in spiral galaxies without
resorting to dark matter (DM), the modified Newtonian dynamics (MOND) paradigm
still requires DM in X-ray bright systems. Here, to get a handle on the
distribution an... | astro-ph | although very successful in explaining the observed conspiracy between the baryonic distribution and the gravitational field in spiral galaxies without resorting to dark matter dm the modified newtonian dynamics mond paradigm still requires dm in xray bright systems here to get a handle on the distribution and importan... | [['although', 'very', 'successful', 'in', 'explaining', 'the', 'observed', 'conspiracy', 'between', 'the', 'baryonic', 'distribution', 'and', 'the', 'gravitational', 'field', 'in', 'spiral', 'galaxies', 'without', 'resorting', 'to', 'dark', 'matter', 'dm', 'the', 'modified', 'newtonian', 'dynamics', 'mond', 'paradigm',... | [-0.08356989542951414, 0.1765369813020211, -0.07774279500870396, 0.15598187437858577, -0.05947415966652478, -0.11382663320224776, 0.054145523827963386, 0.3425801453097586, -0.18856451172036906, -0.3946218553735593, 0.028818906193270617, -0.2665479439761952, -0.014971467411838645, 0.1754629222076935, 0.01379483997676965... |
709.0109 | Local convergence for alternating and averaged nonconvex projections | The idea of a finite collection of closed sets having "strongly regular
intersection" at a given point is crucial in variational analysis. We show that
this central theoretical tool also has striking algorithmic consequences.
Specifically, we consider the case of two sets, one of which we assume to be
suitably "regul... | math.OC math.NA | the idea of a finite collection of closed sets having strongly regular intersection at a given point is crucial in variational analysis we show that this central theoretical tool also has striking algorithmic consequences specifically we consider the case of two sets one of which we assume to be suitably regular specia... | [['the', 'idea', 'of', 'a', 'finite', 'collection', 'of', 'closed', 'sets', 'having', 'strongly', 'regular', 'intersection', 'at', 'a', 'given', 'point', 'is', 'crucial', 'in', 'variational', 'analysis', 'we', 'show', 'that', 'this', 'central', 'theoretical', 'tool', 'also', 'has', 'striking', 'algorithmic', 'consequen... | [-0.13245963450031775, 0.058118708567680234, -0.09962070440655968, 0.06569044057442977, -0.023835499917095812, -0.15074939318817027, 0.05246163713643803, 0.3467818958698398, -0.3297117845372834, -0.1600454218352526, 0.1520526282978754, -0.2826411042440628, -0.11975197071195955, 0.20461214400732713, -0.09633910483306776... |
709.011 | New bounds on the neutrino magnetic moment from the plasma induced
neutrino chirality flip in a supernova | The neutrino chirality-flip process under the conditions of the supernova
core is investigated in detail with the plasma polarization effects in the
photon propagator taken into account, in a more consistent way than in earlier
publications. It is shown in part that the contribution of the proton fraction
of plasma i... | hep-ph | the neutrino chiralityflip process under the conditions of the supernova core is investigated in detail with the plasma polarization effects in the photon propagator taken into account in a more consistent way than in earlier publications it is shown in part that the contribution of the proton fraction of plasma is ess... | [['the', 'neutrino', 'chiralityflip', 'process', 'under', 'the', 'conditions', 'of', 'the', 'supernova', 'core', 'is', 'investigated', 'in', 'detail', 'with', 'the', 'plasma', 'polarization', 'effects', 'in', 'the', 'photon', 'propagator', 'taken', 'into', 'account', 'in', 'a', 'more', 'consistent', 'way', 'than', 'in'... | [-0.05941277853942112, 0.20829492232802768, -0.006191070746306492, 0.14774645452608123, -0.010002003770078654, -0.0037290603990423614, 0.08301810013312523, 0.34219103272518386, -0.14619665671463894, -0.34868953349473686, 0.056786249127522434, -0.31047499500538994, 0.02788927510542714, 0.2294210096416266, 0.054502234004... |
709.0111 | A new method for the estimation of variance matrix with prescribed zeros
in nonlinear mixed effects models | We propose a new method for the Maximum Likelihood Estimator (MLE) of
nonlinear mixed effects models when the variance matrix of Gaussian random
effects has a prescribed pattern of zeros (PPZ). The method consists in
coupling the recently developed Iterative Conditional Fitting (ICF) algorithm
with the Expectation Ma... | stat.ME | we propose a new method for the maximum likelihood estimator mle of nonlinear mixed effects models when the variance matrix of gaussian random effects has a prescribed pattern of zeros ppz the method consists in coupling the recently developed iterative conditional fitting icf algorithm with the expectation maximizatio... | [['we', 'propose', 'a', 'new', 'method', 'for', 'the', 'maximum', 'likelihood', 'estimator', 'mle', 'of', 'nonlinear', 'mixed', 'effects', 'models', 'when', 'the', 'variance', 'matrix', 'of', 'gaussian', 'random', 'effects', 'has', 'a', 'prescribed', 'pattern', 'of', 'zeros', 'ppz', 'the', 'method', 'consists', 'in', '... | [-0.05481321582919918, 0.04713236086536199, -0.1427440999483224, 0.08665242271672469, -0.11260471345158293, -0.18422396883252076, 0.034904642721812706, 0.3917011815938167, -0.22374176354060182, -0.3013449265621603, 0.109700044382771, -0.22496352951275184, -0.18201753906614612, 0.16930949029920156, -0.07228477349271997,... |
709.0112 | On the precision of the spectral profile | We examine the spectral profile bound of Goel, Montenegro and Tetali for the
uniform mixing time of continuous-time random walk in reversible settings. We
find that it is precise up to a log log factor, and that this log log factor
cannot be improved.
| math.PR | we examine the spectral profile bound of goel montenegro and tetali for the uniform mixing time of continuoustime random walk in reversible settings we find that it is precise up to a log log factor and that this log log factor cannot be improved | [['we', 'examine', 'the', 'spectral', 'profile', 'bound', 'of', 'goel', 'montenegro', 'and', 'tetali', 'for', 'the', 'uniform', 'mixing', 'time', 'of', 'continuoustime', 'random', 'walk', 'in', 'reversible', 'settings', 'we', 'find', 'that', 'it', 'is', 'precise', 'up', 'to', 'a', 'log', 'log', 'factor', 'and', 'that',... | [-0.10311546747883162, 0.12644592614637482, -0.09227646928694513, 0.08119978830218315, -0.013325955304834578, -0.18259548562475378, 0.15336562419931093, 0.4097968107296361, -0.23072163445047206, -0.34267728072591125, 0.08437600937516739, -0.22532634718550576, -0.11855507890383403, 0.20112975426018237, -0.11590837792803... |
709.0113 | A remark on utility streams | We consider arbitrarily long, but finite utility streams, and some
appropriate axioms.
| math.LO | we consider arbitrarily long but finite utility streams and some appropriate axioms | [['we', 'consider', 'arbitrarily', 'long', 'but', 'finite', 'utility', 'streams', 'and', 'some', 'appropriate', 'axioms']] | [-0.22926198619340235, 0.16640238968345025, -0.08036078186705709, 0.23829808738082647, -0.16340154269710183, -0.25184139236807823, 0.08666008089979489, 0.4569593171278636, -0.3371460270136595, -0.22608422177533308, 0.1857767936695988, -0.22941870180269083, -0.08172872895374894, 0.10004800891814132, -0.1451513921347214,... |
709.0114 | Unveiling the core of the Globular Cluster M15 in the Ultraviolet | We have obtained deep far- (FUV) and near-ultraviolet (NUV) images of the
inner region of the dense globular cluster M15 with the Advanced Camera for
Surveys on board the Hubble Space Telescope. The FUV-NUV colour-magnitude
diagram shows a well defined track of horizontal branch stars, as well as a
trail of blue stra... | astro-ph | we have obtained deep far fuv and nearultraviolet nuv images of the inner region of the dense globular cluster m15 with the advanced camera for surveys on board the hubble space telescope the fuvnuv colourmagnitude diagram shows a well defined track of horizontal branch stars as well as a trail of blue stragglers and w... | [['we', 'have', 'obtained', 'deep', 'far', 'fuv', 'and', 'nearultraviolet', 'nuv', 'images', 'of', 'the', 'inner', 'region', 'of', 'the', 'dense', 'globular', 'cluster', 'm15', 'with', 'the', 'advanced', 'camera', 'for', 'surveys', 'on', 'board', 'the', 'hubble', 'space', 'telescope', 'the', 'fuvnuv', 'colourmagnitude'... | [-0.03874444594814606, 0.1096507060100962, -0.10088352512872015, 0.13807696730394092, -0.14723599244053015, -0.06816901990448329, 0.12398311527108158, 0.4561665490301638, -0.15619774836104547, -0.35089744224568803, 0.040588545548038105, -0.3240481810484385, -0.12493338735345472, 0.19822603906904518, -0.1230175158184055... |
709.0115 | Distinguishing between $w < -1$ Dark Energy Models | Recent data and new data analysis methods show that most probably the
parameter $w$ in the equation of state of the dark energy is smaller than -1 at
low redshifts. We briefly review some of the models with such a property and
without violating null energy condition. We investigate the difference between
the observab... | astro-ph hep-ph | recent data and new data analysis methods show that most probably the parameter w in the equation of state of the dark energy is smaller than 1 at low redshifts we briefly review some of the models with such a property and without violating null energy condition we investigate the difference between the observables and... | [['recent', 'data', 'and', 'new', 'data', 'analysis', 'methods', 'show', 'that', 'most', 'probably', 'the', 'parameter', 'w', 'in', 'the', 'equation', 'of', 'state', 'of', 'the', 'dark', 'energy', 'is', 'smaller', 'than', '1', 'at', 'low', 'redshifts', 'we', 'briefly', 'review', 'some', 'of', 'the', 'models', 'with', '... | [-0.09164899145850004, 0.1349471424563, -0.09867889549917518, 0.1268684216372024, -0.06908936192317364, -0.12177918066915411, 0.0374751787346143, 0.34376052289437026, -0.25628978424281695, -0.3533726443942541, 0.10495433529379228, -0.2962435607989438, -0.05447631266911347, 0.1872182294505481, 0.021221738326578185, 0.02... |
709.0116 | On Ultrametric Algorithmic Information | How best to quantify the information of an object, whether natural or
artifact, is a problem of wide interest. A related problem is the computability
of an object. We present practical examples of a new way to address this
problem. By giving an appropriate representation to our objects, based on a
hierarchical coding... | cs.AI cs.CL | how best to quantify the information of an object whether natural or artifact is a problem of wide interest a related problem is the computability of an object we present practical examples of a new way to address this problem by giving an appropriate representation to our objects based on a hierarchical coding of info... | [['how', 'best', 'to', 'quantify', 'the', 'information', 'of', 'an', 'object', 'whether', 'natural', 'or', 'artifact', 'is', 'a', 'problem', 'of', 'wide', 'interest', 'a', 'related', 'problem', 'is', 'the', 'computability', 'of', 'an', 'object', 'we', 'present', 'practical', 'examples', 'of', 'a', 'new', 'way', 'to', '... | [-0.08749318422599771, 0.0254049951378885, -0.10609707094985864, 0.10431259866514854, -0.15547076302270094, -0.08809251826384971, 0.05950355816407707, 0.3744922201095641, -0.32542010295022833, -0.3246895898904266, 0.11590076237649324, -0.21269782674338283, -0.18301719925152246, 0.2177172460962601, -0.1799947001553815, ... |
709.0117 | On Zariski's multiplicity conjecture | We discuss some features of the so-called Zariski's multiplicity problem
especially the application of the work of A'Campo on the zeta function of a
monodromy of an isolated singularity of a complex hypersurface to the problem.
| math.AG math.AT | we discuss some features of the socalled zariskis multiplicity problem especially the application of the work of acampo on the zeta function of a monodromy of an isolated singularity of a complex hypersurface to the problem | [['we', 'discuss', 'some', 'features', 'of', 'the', 'socalled', 'zariskis', 'multiplicity', 'problem', 'especially', 'the', 'application', 'of', 'the', 'work', 'of', 'acampo', 'on', 'the', 'zeta', 'function', 'of', 'a', 'monodromy', 'of', 'an', 'isolated', 'singularity', 'of', 'a', 'complex', 'hypersurface', 'to', 'the... | [-0.23664479438836375, -0.049796482945465764, -0.15881719140128958, 0.11728867267568906, -0.07951317159070943, -0.05430372175760567, -0.013684640690270398, 0.24518804236625633, -0.30600975602606517, -0.23014500569034782, 0.12241959231646939, -0.2849051577504724, -0.1965579011787971, 0.19518669800729388, -0.097533638977... |
709.0118 | Scanning optical homodyne detection of high-frequency picoscale
resonances in cantilever and tuning fork sensors | Higher harmonic modes in nanoscale silicon cantilevers and microscale quartz
tuning forks are detected and characterized using a custom scanning optical
homodyne interferometer. Capable of both mass and force sensing, these
resonators exhibit high-frequency harmonic motion content with picometer-scale
amplitudes dete... | cond-mat.other | higher harmonic modes in nanoscale silicon cantilevers and microscale quartz tuning forks are detected and characterized using a custom scanning optical homodyne interferometer capable of both mass and force sensing these resonators exhibit highfrequency harmonic motion content with picometerscale amplitudes detected i... | [['higher', 'harmonic', 'modes', 'in', 'nanoscale', 'silicon', 'cantilevers', 'and', 'microscale', 'quartz', 'tuning', 'forks', 'are', 'detected', 'and', 'characterized', 'using', 'a', 'custom', 'scanning', 'optical', 'homodyne', 'interferometer', 'capable', 'of', 'both', 'mass', 'and', 'force', 'sensing', 'these', 're... | [-0.17536162436970146, 0.26798934177698003, 0.0386456991545856, -0.0826595918295662, -0.08248130595513983, -0.22856284874559724, 0.0502551895966146, 0.5343934431186189, -0.18661438650008716, -0.35521453631150984, 0.05654252944868463, -0.27170540327611176, -0.0842990102853788, 0.2638313906158462, 0.034036014130201096, 0... |
709.0119 | The surface density profile of NGC 6388: a good candidate for harboring
an intermediate-mass black hole | We have used a combination of high resolution (HST ACS-HRC, ACS-WFC, and
WFPC2) and wide-field (ESO-WFI) observations of the galactic globular cluster
NGC 6388 to derive its center of gravity, projected density profile, and
central surface brightness profile. While the overall projected profiles are
well fit by a Kin... | astro-ph | we have used a combination of high resolution hst acshrc acswfc and wfpc2 and widefield esowfi observations of the galactic globular cluster ngc 6388 to derive its center of gravity projected density profile and central surface brightness profile while the overall projected profiles are well fit by a king model with in... | [['we', 'have', 'used', 'a', 'combination', 'of', 'high', 'resolution', 'hst', 'acshrc', 'acswfc', 'and', 'wfpc2', 'and', 'widefield', 'esowfi', 'observations', 'of', 'the', 'galactic', 'globular', 'cluster', 'ngc', '6388', 'to', 'derive', 'its', 'center', 'of', 'gravity', 'projected', 'density', 'profile', 'and', 'cen... | [-0.05153594497044521, 0.035988672582399364, -0.11693458412940215, 0.09720971709716, -0.0629439946995782, -0.12026052732835524, 0.01459424156928435, 0.4044644040820588, -0.1356669762587574, -0.40536354387690415, 0.08985730141284876, -0.28433975509168313, -0.012870997857784719, 0.16277607887708914, -0.03405191796576089,... |
709.012 | Pointed and copointed Hopf algebras as cocycle deformations | We show that all finite dimensional pointed Hopf algebras with the same
diagram in the classification scheme of Andruskiewitsch and Schneider are
cocycle deformations of each other. This is done by giving first a suitable
characterization of such Hopf algebras, which allows for the application of a
result of Masuoka ... | math.RA math.QA | we show that all finite dimensional pointed hopf algebras with the same diagram in the classification scheme of andruskiewitsch and schneider are cocycle deformations of each other this is done by giving first a suitable characterization of such hopf algebras which allows for the application of a result of masuoka abou... | [['we', 'show', 'that', 'all', 'finite', 'dimensional', 'pointed', 'hopf', 'algebras', 'with', 'the', 'same', 'diagram', 'in', 'the', 'classification', 'scheme', 'of', 'andruskiewitsch', 'and', 'schneider', 'are', 'cocycle', 'deformations', 'of', 'each', 'other', 'this', 'is', 'done', 'by', 'giving', 'first', 'a', 'sui... | [-0.17424321512226015, 0.06440418392594438, -0.07267443329328671, 0.06448686067597009, -0.11899567433768728, -0.13612616244548312, -0.04142536172245551, 0.32247869406516355, -0.3670455641501273, -0.22044365212544412, 0.15433113259738698, -0.18461957181959102, -0.2006831144365909, 0.23026155235129409, -0.152579155144242... |
709.0121 | Introduction to shape stability for a storage model | We consider a new idea for a storage model on n nodes, namely stability of
shape. These nodes support K neighborhoods S_i \subset {1, ..., n} and items
arrive at the S_i as independent Poisson streams with rates lambda_i, i=1,
...,K. Upon arrival at S_i an item is stored at node j \in S_i where j is
determined by som... | math.PR | we consider a new idea for a storage model on n nodes namely stability of shape these nodes support k neighborhoods s_i subset 1 n and items arrive at the s_i as independent poisson streams with rates lambda_i i1 k upon arrival at s_i an item is stored at node j in s_i where j is determined by some policy under natural... | [['we', 'consider', 'a', 'new', 'idea', 'for', 'a', 'storage', 'model', 'on', 'n', 'nodes', 'namely', 'stability', 'of', 'shape', 'these', 'nodes', 'support', 'k', 'neighborhoods', 's_i', 'subset', '1', 'n', 'and', 'items', 'arrive', 'at', 'the', 's_i', 'as', 'independent', 'poisson', 'streams', 'with', 'rates', 'lambd... | [-0.18198798933336813, 0.16352260502957194, 0.024222525097029185, -0.02589518454990094, -0.038234631194212346, -0.22008498815158684, 0.12454916075152415, 0.3936607146495453, -0.3210958220385095, -0.2298297291040741, 0.03821176494195868, -0.3409838033239207, -0.06917562454398121, 0.08212550207521886, -0.0268650629297299... |
709.0122 | Towards Low Cost Coupling Structures for Short-Distance Optical
Interconnections | The performance of short distance optical interconnections in general relies
very strongly on coupling structures, since they will determine the overall
efficiency of the system to a large extent. Different configurations can be
considered and a variety of manufacturing technologies can be used. We present
two differ... | physics.optics | the performance of short distance optical interconnections in general relies very strongly on coupling structures since they will determine the overall efficiency of the system to a large extent different configurations can be considered and a variety of manufacturing technologies can be used we present two different d... | [['the', 'performance', 'of', 'short', 'distance', 'optical', 'interconnections', 'in', 'general', 'relies', 'very', 'strongly', 'on', 'coupling', 'structures', 'since', 'they', 'will', 'determine', 'the', 'overall', 'efficiency', 'of', 'the', 'system', 'to', 'a', 'large', 'extent', 'different', 'configurations', 'can'... | [-0.1708298325933435, 0.147741973347476, -0.05003706783501674, 0.03794257214817069, -0.062260880620907184, -0.131920646685783, -0.038307002119962935, 0.429273433788963, -0.2772106059057557, -0.3224347842047396, 0.11573823896317702, -0.23213302975763445, -0.14284641694520478, 0.25704340214800575, -0.047551625051900095, ... |
709.0123 | Fluctuation of the initial condition from Glauber models | We analyze measures of the azimuthal asymmetry, in particular the participant
harmonic moments, epsilon*, in a variety of Glauber-like models for the early
stage of collisions at RHIC. Quantitative comparisons indicate substantial
model dependence for epsilon*, reflecting different effective number of
sources, while ... | nucl-th nucl-ex | we analyze measures of the azimuthal asymmetry in particular the participant harmonic moments epsilon in a variety of glauberlike models for the early stage of collisions at rhic quantitative comparisons indicate substantial model dependence for epsilon reflecting different effective number of sources while the depende... | [['we', 'analyze', 'measures', 'of', 'the', 'azimuthal', 'asymmetry', 'in', 'particular', 'the', 'participant', 'harmonic', 'moments', 'epsilon', 'in', 'a', 'variety', 'of', 'glauberlike', 'models', 'for', 'the', 'early', 'stage', 'of', 'collisions', 'at', 'rhic', 'quantitative', 'comparisons', 'indicate', 'substantial... | [-0.09546152493375504, 0.12526253188686992, -0.08897718760982423, 0.12512665059107975, 0.01880658191243956, -0.07544136547879456, 0.018207570005342098, 0.34206157863630865, -0.21690587513148785, -0.33543604457873605, 0.05454218909311705, -0.33027384246693936, -0.009459385129729074, 0.20811421464163876, 0.00140435871679... |
709.0124 | High Rate Single-Symbol ML Decodable Precoded DSTBCs for Cooperative
Networks | Distributed Orthogonal Space-Time Block Codes (DOSTBCs) achieving full
diversity order and single-symbol ML decodability have been introduced recently
by Yi and Kim for cooperative networks and an upperbound on the maximal rate of
such codes along with code constructions has been presented. In this paper, we
introduc... | cs.IT math.IT | distributed orthogonal spacetime block codes dostbcs achieving full diversity order and singlesymbol ml decodability have been introduced recently by yi and kim for cooperative networks and an upperbound on the maximal rate of such codes along with code constructions has been presented in this paper we introduce a new ... | [['distributed', 'orthogonal', 'spacetime', 'block', 'codes', 'dostbcs', 'achieving', 'full', 'diversity', 'order', 'and', 'singlesymbol', 'ml', 'decodability', 'have', 'been', 'introduced', 'recently', 'by', 'yi', 'and', 'kim', 'for', 'cooperative', 'networks', 'and', 'an', 'upperbound', 'on', 'the', 'maximal', 'rate'... | [-0.19795994800703567, 0.07083654338730333, -0.03351758454222736, 0.028670807202818383, -0.02694212689113246, -0.2363104491401057, 0.029376302607353435, 0.3759322311062219, -0.24830144952830663, -0.25827540930637105, 0.12045982398660081, -0.25787663759712504, -0.1428854343477295, 0.19622108100823993, -0.091397819637959... |
709.0125 | Differential and graphical approaches to multistability theory for
chemical reaction networks | The use of mathematical models has helped to shed light on countless
phenomena in chemistry and biology. Often, though, one finds that systems of
interest in these fields are dauntingly complex. In this paper, we attempt to
synthesize and expand upon the body of mathematical results pertaining to the
theory of multip... | q-bio.MN q-bio.QM | the use of mathematical models has helped to shed light on countless phenomena in chemistry and biology often though one finds that systems of interest in these fields are dauntingly complex in this paper we attempt to synthesize and expand upon the body of mathematical results pertaining to the theory of multiple equi... | [['the', 'use', 'of', 'mathematical', 'models', 'has', 'helped', 'to', 'shed', 'light', 'on', 'countless', 'phenomena', 'in', 'chemistry', 'and', 'biology', 'often', 'though', 'one', 'finds', 'that', 'systems', 'of', 'interest', 'in', 'these', 'fields', 'are', 'dauntingly', 'complex', 'in', 'this', 'paper', 'we', 'atte... | [-0.07056065424080563, 0.052585066894257286, -0.11892317175900419, 0.029200902137127834, -0.10640956365734065, -0.13612039432510598, 0.08101224373393787, 0.3229573801065872, -0.23725314046162257, -0.3156361039898811, 0.08523817907232757, -0.25788098649728464, -0.22556376429872776, 0.23043193391720773, -0.13285726761040... |
709.0126 | Rapidity-dependent chemical potentials in a statistical approach | We present a single-freeze-out model with thermal and geometric parameters
dependent on the position within the fireball and use it to describe the
rapidity and transverse-momentum spectra of pions, kaons, protons, and
antiprotons measured at RHIC at 200 GeV} by BRAHMS. THERMINATOR is used to
perform the necessary si... | nucl-th nucl-ex | we present a singlefreezeout model with thermal and geometric parameters dependent on the position within the fireball and use it to describe the rapidity and transversemomentum spectra of pions kaons protons and antiprotons measured at rhic at 200 gev by brahms therminator is used to perform the necessary simulation w... | [['we', 'present', 'a', 'singlefreezeout', 'model', 'with', 'thermal', 'and', 'geometric', 'parameters', 'dependent', 'on', 'the', 'position', 'within', 'the', 'fireball', 'and', 'use', 'it', 'to', 'describe', 'the', 'rapidity', 'and', 'transversemomentum', 'spectra', 'of', 'pions', 'kaons', 'protons', 'and', 'antiprot... | [-0.03446913007298175, 0.19890291584944503, -0.13993725970756005, 0.09195010016366023, -0.016769533531950726, -0.06057365808665832, 0.0021228847812293445, 0.3360021551597844, -0.21490138964627914, -0.3196353074661232, -0.017370411679198478, -0.32995781427458487, 0.061469571321286304, 0.157120686122789, 0.03655375676779... |
709.0127 | Effective Pruefer Angles and Relative Oscillation Criteria | We present a streamlined approach to relative oscillation criteria based on
effective Pruefer angles adapted to the use at the edges of the essential
spectrum.
Based on this we provided a new scale of oscillation criteria for general
Sturm-Liouville operators which answer the question whether a perturbation
inserts... | math.SP math-ph math.MP | we present a streamlined approach to relative oscillation criteria based on effective pruefer angles adapted to the use at the edges of the essential spectrum based on this we provided a new scale of oscillation criteria for general sturmliouville operators which answer the question whether a perturbation inserts a fin... | [['we', 'present', 'a', 'streamlined', 'approach', 'to', 'relative', 'oscillation', 'criteria', 'based', 'on', 'effective', 'pruefer', 'angles', 'adapted', 'to', 'the', 'use', 'at', 'the', 'edges', 'of', 'the', 'essential', 'spectrum', 'based', 'on', 'this', 'we', 'provided', 'a', 'new', 'scale', 'of', 'oscillation', '... | [-0.08598240478796527, 0.08320294544589954, -0.10285236902548585, 0.10847436696008601, -0.09039515851590624, -0.13475175030242176, 0.07633236702036192, 0.2806163016667074, -0.21760525855612248, -0.29477105648355917, 0.1317331072975921, -0.2475720897460594, -0.1536357318313713, 0.2036232376406762, -0.08882486904436286, ... |
709.0128 | A Universal Operator Theoretic Framework for Quantum Fault Tolerance | In this paper we introduce a universal operator theoretic framework for
quantum fault tolerance. This incorporates a top-down approach that implements
a system-level criterion based on specification of the full system dynamics,
applied at every level of error correction concatenation. This leads to more
accurate dete... | quant-ph | in this paper we introduce a universal operator theoretic framework for quantum fault tolerance this incorporates a topdown approach that implements a systemlevel criterion based on specification of the full system dynamics applied at every level of error correction concatenation this leads to more accurate determinati... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'universal', 'operator', 'theoretic', 'framework', 'for', 'quantum', 'fault', 'tolerance', 'this', 'incorporates', 'a', 'topdown', 'approach', 'that', 'implements', 'a', 'systemlevel', 'criterion', 'based', 'on', 'specification', 'of', 'the', 'full', 'system', 'dynamics'... | [-0.13543821980658946, 0.041314170451065065, -0.10753370762573305, 0.09046584879805737, -0.026467271789008363, -0.20631691925366646, 0.054470434338340895, 0.3263869586942801, -0.2435661615150522, -0.2552306264527698, 0.08414128907076987, -0.1962926612120928, -0.22598751580843063, 0.24792478340608415, -0.125507503129375... |
709.0129 | Numerical analysis of a nonlocal parabolic problem resulting from
thermistor problem | We analyze the spatially semidiscrete piecewise linear finite element method
for a nonlocal parabolic equation resulting from thermistor problem. Our
approach is based on the properties of the elliptic projection defined by the
bilinear form associated with the variational formulation of the finite element
method. We... | math.AP math.NA | we analyze the spatially semidiscrete piecewise linear finite element method for a nonlocal parabolic equation resulting from thermistor problem our approach is based on the properties of the elliptic projection defined by the bilinear form associated with the variational formulation of the finite element method we ass... | [['we', 'analyze', 'the', 'spatially', 'semidiscrete', 'piecewise', 'linear', 'finite', 'element', 'method', 'for', 'a', 'nonlocal', 'parabolic', 'equation', 'resulting', 'from', 'thermistor', 'problem', 'our', 'approach', 'is', 'based', 'on', 'the', 'properties', 'of', 'the', 'elliptic', 'projection', 'defined', 'by',... | [-0.07504834576199453, -0.006873598222487739, -0.11195229313203267, 0.06133439823974013, -0.10507428681566602, -0.14312473202257284, 0.00747535905490319, 0.35490537449784043, -0.35818569475252715, -0.2178666380766247, 0.1340389337634579, -0.23330790085795647, -0.15266122610011648, 0.2012037214423929, -0.038034704184004... |
709.013 | Magic wavelengths for the np-ns transitions in alkali-metal atoms | Extensive calculations of the electric-dipole matrix elements in alkali-metal
atoms are conducted using the relativistic all-order method. This approach is a
linearized version of the coupled-cluster method, which sums infinite sets of
many-body perturbation theory terms. All allowed transitions between the lowest
ns... | physics.atom-ph | extensive calculations of the electricdipole matrix elements in alkalimetal atoms are conducted using the relativistic allorder method this approach is a linearized version of the coupledcluster method which sums infinite sets of manybody perturbation theory terms all allowed transitions between the lowest ns np_12 np_... | [['extensive', 'calculations', 'of', 'the', 'electricdipole', 'matrix', 'elements', 'in', 'alkalimetal', 'atoms', 'are', 'conducted', 'using', 'the', 'relativistic', 'allorder', 'method', 'this', 'approach', 'is', 'a', 'linearized', 'version', 'of', 'the', 'coupledcluster', 'method', 'which', 'sums', 'infinite', 'sets'... | [-0.11577737469046392, 0.2370035464940756, -0.0006538260250205272, 0.02322579126727457, 0.08073980875493011, -0.10946481518055264, 0.1036852751889168, 0.40300660554254264, -0.17297965698270945, -0.2797367438273668, -0.03003885501713835, -0.32824300762200564, -0.05599629346755121, 0.13101304272238753, 0.1225927983157402... |
709.0131 | How cold is cold dark matter? Small scales constraints from the flux
power spectrum of the high-redshift Lyman-alpha forest | We present constraints on the mass of warm dark matter (WDM) particles
derived from the Lyman-alpha flux power spectrum of 55 high- resolution HIRES
spectra at 2.0 < z < 6.4. From the HIRES spectra, we obtain a lower limit of
mwdm > 1.2 keV 2 sigma if the WDM consists of early decoupled thermal relics
and mwdm > 5.6 ... | astro-ph hep-th | we present constraints on the mass of warm dark matter wdm particles derived from the lymanalpha flux power spectrum of 55 high resolution hires spectra at 20 z 64 from the hires spectra we obtain a lower limit of mwdm 12 kev 2 sigma if the wdm consists of early decoupled thermal relics and mwdm 56 kev 2 sigma for ster... | [['we', 'present', 'constraints', 'on', 'the', 'mass', 'of', 'warm', 'dark', 'matter', 'wdm', 'particles', 'derived', 'from', 'the', 'lymanalpha', 'flux', 'power', 'spectrum', 'of', '55', 'high', 'resolution', 'hires', 'spectra', 'at', '20', 'z', '64', 'from', 'the', 'hires', 'spectra', 'we', 'obtain', 'a', 'lower', 'l... | [-0.05002580326506678, 0.20832113357621948, 0.002903533467490758, 0.12088889125924633, -0.05783179301616489, -0.13324447039381734, 0.05085332781713152, 0.3395223688638332, -0.13373393411002696, -0.4483647231506754, 0.035960089134964714, -0.3989251337717382, 0.09781361420695879, 0.17343779861670444, 0.060863194678320874... |
709.0132 | On the index of the Heegner subgroup of elliptic curves | Let E be an elliptic curve of conductor N and rank one over Q. So there is a
non-constant morphism X+0(N) --> E defined over Q, where X+0(N) = X0(N)/wN and
wN is the Fricke involution of the modular curve X+0(N). Under this morphism
the traces of the Heegner points of X+0(N) map to rational points on E. In this
paper... | math.NT math.AG | let e be an elliptic curve of conductor n and rank one over q so there is a nonconstant morphism x0n e defined over q where x0n x0nwn and wn is the fricke involution of the modular curve x0n under this morphism the traces of the heegner points of x0n map to rational points on e in this paper we study the index i of the... | [['let', 'e', 'be', 'an', 'elliptic', 'curve', 'of', 'conductor', 'n', 'and', 'rank', 'one', 'over', 'q', 'so', 'there', 'is', 'a', 'nonconstant', 'morphism', 'x0n', 'e', 'defined', 'over', 'q', 'where', 'x0n', 'x0nwn', 'and', 'wn', 'is', 'the', 'fricke', 'involution', 'of', 'the', 'modular', 'curve', 'x0n', 'under', '... | [-0.20147962806030836, 0.09113311016779158, -0.09526428076007017, -0.010223780081482468, -0.042837725415621405, -0.13816449232399464, 0.04028224447747783, 0.31725190031745404, -0.27674003667766, -0.26606064364200505, 0.07509961455532281, -0.3021146728935447, -0.13501327182734157, 0.21337795991694736, -0.119832674762597... |
709.0133 | Temperature-dependent Raman scattering of natural and isotopically
substituted PbS | Lead sulfide is an important semiconductor that has found technological
applications for over a century. Raman spectroscopy, a standard tool for the
investigation and characterization of semiconductors, has limited application
to this material because of the forbidden nature of its first order scattering
and its opac... | cond-mat.mtrl-sci cond-mat.dis-nn | lead sulfide is an important semiconductor that has found technological applications for over a century raman spectroscopy a standard tool for the investigation and characterization of semiconductors has limited application to this material because of the forbidden nature of its first order scattering and its opacity t... | [['lead', 'sulfide', 'is', 'an', 'important', 'semiconductor', 'that', 'has', 'found', 'technological', 'applications', 'for', 'over', 'a', 'century', 'raman', 'spectroscopy', 'a', 'standard', 'tool', 'for', 'the', 'investigation', 'and', 'characterization', 'of', 'semiconductors', 'has', 'limited', 'application', 'to'... | [-0.08216718980469383, 0.16334187747885992, -0.05747008392085823, -0.011138191040999328, -0.011215503062479771, -0.10947978228975375, 0.08554549997564978, 0.4511434961396914, -0.225608240856001, -0.2846865092475827, 0.06070814260478633, -0.33252840175006826, -0.08198578413575888, 0.2214166601242211, 0.04975988883883334... |
709.0134 | Harder-Narasimhan Filtrations and K-Groups of an Elliptic Curve | Let $X$ be an elliptic curve over an algebraically closed field. We prove
that some exact sub-categories of the category of vector bundles over $X$,
defined using Harder-Narasimhan filtrations, have the same K-groups as the
whole category.
| math.KT math.AG | let x be an elliptic curve over an algebraically closed field we prove that some exact subcategories of the category of vector bundles over x defined using hardernarasimhan filtrations have the same kgroups as the whole category | [['let', 'x', 'be', 'an', 'elliptic', 'curve', 'over', 'an', 'algebraically', 'closed', 'field', 'we', 'prove', 'that', 'some', 'exact', 'subcategories', 'of', 'the', 'category', 'of', 'vector', 'bundles', 'over', 'x', 'defined', 'using', 'hardernarasimhan', 'filtrations', 'have', 'the', 'same', 'kgroups', 'as', 'the',... | [-0.23733999625452468, 0.017829904357141286, -0.13781934775839988, 0.04333081700511881, -0.07759472274699726, -0.13178334222804453, -0.08056877407471875, 0.43020798567984553, -0.45351975587372845, -0.11369203947283127, 0.06467457325827028, -0.18508070421631675, -0.041044684869514125, 0.24075656379195484, -0.22105095082... |
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