id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
707.133 | Proving the triviality of rational points on Atkin-Lehner quotients of
Shimura curves | In this paper we give a method for studying global rational points on certain
quotients of Shimura curves by Atkin-Lehner involutions. We obtain explicit
conditions on such quotients for rational points to be ``trivial'' (coming from
CM points only) and exhibit an explicit infinite family of such quotients
satisfying... | math.NT | in this paper we give a method for studying global rational points on certain quotients of shimura curves by atkinlehner involutions we obtain explicit conditions on such quotients for rational points to be trivial coming from cm points only and exhibit an explicit infinite family of such quotients satisfying these con... | [['in', 'this', 'paper', 'we', 'give', 'a', 'method', 'for', 'studying', 'global', 'rational', 'points', 'on', 'certain', 'quotients', 'of', 'shimura', 'curves', 'by', 'atkinlehner', 'involutions', 'we', 'obtain', 'explicit', 'conditions', 'on', 'such', 'quotients', 'for', 'rational', 'points', 'to', 'be', 'trivial', '... | [-0.2026255310093071, 0.030711740303576887, -0.11697508102538538, 0.06601485678259575, -0.09317572472397895, -0.1304583341778055, 0.07559221599698432, 0.31903063520496966, -0.3085164624978514, -0.21251684197169893, 0.1491240027301269, -0.2635486399316612, -0.16430242891039917, 0.29984144048363554, -0.17003061883516757,... |
707.1331 | Quantum Chaos, Delocalization, and Entanglement in Disordered Heisenberg
Models | We investigate disordered one- and two-dimensional Heisenberg spin lattices
across a transition from integrability to quantum chaos from both a statistical
many-body and a quantum-information perspective. Special emphasis is devoted to
quantitatively exploring the interplay between eigenvector statistics,
delocalizat... | quant-ph cond-mat.other | we investigate disordered one and twodimensional heisenberg spin lattices across a transition from integrability to quantum chaos from both a statistical manybody and a quantuminformation perspective special emphasis is devoted to quantitatively exploring the interplay between eigenvector statistics delocalization and ... | [['we', 'investigate', 'disordered', 'one', 'and', 'twodimensional', 'heisenberg', 'spin', 'lattices', 'across', 'a', 'transition', 'from', 'integrability', 'to', 'quantum', 'chaos', 'from', 'both', 'a', 'statistical', 'manybody', 'and', 'a', 'quantuminformation', 'perspective', 'special', 'emphasis', 'is', 'devoted', ... | [-0.12845355381072568, 0.1838665689211539, -0.08974700513476085, 0.10898381321420593, -0.0032639645981372045, -0.14259221600318547, 0.038022772661255054, 0.3326258072779784, -0.2580564735076761, -0.2359064566409616, 0.07831804267311047, -0.2881040110100081, -0.1496919051979378, 0.16117515594207793, 0.009563972404907627... |
707.1332 | Suppression of Higgsino mediated proton decay by cancellations in GUTs
and strings | A mechanism for the enhancement for proton lifetime in
supersymmetric/supergravity (SUSY/SUGRA) grand unified theories (GUTs) and in
string theory models is discussed where Higgsino mediated proton decay arising
from color triplets (anti-triplets) with charges $Q=-1/3(1/3)$ and
$Q=-4/3(4/3)$ is suppressed by an inter... | hep-ph | a mechanism for the enhancement for proton lifetime in supersymmetricsupergravity susysugra grand unified theories guts and in string theory models is discussed where higgsino mediated proton decay arising from color triplets antitriplets with charges q1313 and q4343 is suppressed by an internal cancellation due to con... | [['a', 'mechanism', 'for', 'the', 'enhancement', 'for', 'proton', 'lifetime', 'in', 'supersymmetricsupergravity', 'susysugra', 'grand', 'unified', 'theories', 'guts', 'and', 'in', 'string', 'theory', 'models', 'is', 'discussed', 'where', 'higgsino', 'mediated', 'proton', 'decay', 'arising', 'from', 'color', 'triplets',... | [-0.07314468363415251, 0.24461050390337089, -0.04721574002234898, 0.17680105552002698, -0.07835360047818858, -0.1797550635650252, 0.019858243626480792, 0.3267391959716141, -0.22189417763531788, -0.2873318986921996, 0.009304787176129977, -0.2631122891405327, -0.06910954697116378, 0.1202368494484899, 0.002782052450641556... |
707.1333 | Disproof of Bell's Theorem: Further Consolidations | The failure of Bell's theorem for Clifford algebra valued local variables is
further consolidated by proving that the conditions of remote parameter
independence and remote outcome independence are duly respected within the
recently constructed exact, local realistic model for the EPR-Bohm
correlations. Since the con... | quant-ph gr-qc | the failure of bells theorem for clifford algebra valued local variables is further consolidated by proving that the conditions of remote parameter independence and remote outcome independence are duly respected within the recently constructed exact local realistic model for the eprbohm correlations since the conjuncti... | [['the', 'failure', 'of', 'bells', 'theorem', 'for', 'clifford', 'algebra', 'valued', 'local', 'variables', 'is', 'further', 'consolidated', 'by', 'proving', 'that', 'the', 'conditions', 'of', 'remote', 'parameter', 'independence', 'and', 'remote', 'outcome', 'independence', 'are', 'duly', 'respected', 'within', 'the',... | [-0.10122887853376723, 0.12227276090780433, -0.119579111278005, 0.10222674748156924, -0.032864622967122316, -0.1789390025009121, 0.04626454918733244, 0.27239802315622774, -0.2626295552270587, -0.3116162939980574, 0.0746501240719735, -0.24906327642526452, -0.07294893412447007, 0.16699756495817403, -0.06695351255504037, ... |
707.1334 | Gravitational Wave Recoil and the Retention of Intermediate Mass Black
Holes | During the inspiral and merger of a binary black hole, gravitational
radiation is emitted anisotropically due to asymmetries in the merger
configuration. This anisotropic radiation leads to a gravitational wave kick,
or recoil velocity, as large as ~ 4000 km/sec. We investigate the effect
gravitational recoil has on ... | astro-ph | during the inspiral and merger of a binary black hole gravitational radiation is emitted anisotropically due to asymmetries in the merger configuration this anisotropic radiation leads to a gravitational wave kick or recoil velocity as large as 4000 kmsec we investigate the effect gravitational recoil has on the retent... | [['during', 'the', 'inspiral', 'and', 'merger', 'of', 'a', 'binary', 'black', 'hole', 'gravitational', 'radiation', 'is', 'emitted', 'anisotropically', 'due', 'to', 'asymmetries', 'in', 'the', 'merger', 'configuration', 'this', 'anisotropic', 'radiation', 'leads', 'to', 'a', 'gravitational', 'wave', 'kick', 'or', 'reco... | [-0.11345199746670856, 0.14426589438224746, -0.05711806477706658, 0.17608181357510774, -0.10240698452894342, -0.02632839210622744, 0.06171477291989246, 0.3830724633107447, -0.10242451804096823, -0.3707137889240456, 0.012753136249229345, -0.3259785626206938, -0.009594010054155095, 0.22221427259554227, -0.034687645559032... |
707.1335 | Functoriality and special values of L-functions | This is a semi-expository article concerning Langlands functoriality and
Deligne's conjecture on the special values of $L$-functions. The emphasis is on
symmetric power $L$-functions associated to a holomorphic cusp form, while
appealing to a recent work of Mahnkopf on the special values of automorphic
$L$-functions.... | math.NT math.RT | this is a semiexpository article concerning langlands functoriality and delignes conjecture on the special values of lfunctions the emphasis is on symmetric power lfunctions associated to a holomorphic cusp form while appealing to a recent work of mahnkopf on the special values of automorphic lfunctions | [['this', 'is', 'a', 'semiexpository', 'article', 'concerning', 'langlands', 'functoriality', 'and', 'delignes', 'conjecture', 'on', 'the', 'special', 'values', 'of', 'lfunctions', 'the', 'emphasis', 'is', 'on', 'symmetric', 'power', 'lfunctions', 'associated', 'to', 'a', 'holomorphic', 'cusp', 'form', 'while', 'appeal... | [-0.2612654858165317, -0.053587665926251145, -0.18494643236303496, 0.10027972587332544, -0.19842877342469162, -0.13267629135193096, -0.006069897622283962, 0.21813740457097688, -0.19346762546855542, -0.18971308320760727, 0.12123879534709785, -0.21923044721802903, -0.15927433040406969, 0.26778629463579917, -0.17062320988... |
707.1336 | Aluminium Nanowires: Influence of Work Hardening on Conductance
Histograms | Conductance histograms of work-hardened Al show a series up to 11 equidistant
peaks with a period of 1.15 +/- 0.02 of the quantum conductance unit G_0 =
2e^2/h. Assuming the peaks originate from atomic discreteness, this agrees with
the value of 1.16 G_0 per atom obtained in numerical calculations by Hasmy et
al.
| cond-mat.mes-hall cond-mat.mtrl-sci | conductance histograms of workhardened al show a series up to 11 equidistant peaks with a period of 115 002 of the quantum conductance unit g_0 2e2h assuming the peaks originate from atomic discreteness this agrees with the value of 116 g_0 per atom obtained in numerical calculations by hasmy et al | [['conductance', 'histograms', 'of', 'workhardened', 'al', 'show', 'a', 'series', 'up', 'to', '11', 'equidistant', 'peaks', 'with', 'a', 'period', 'of', '115', '002', 'of', 'the', 'quantum', 'conductance', 'unit', 'g_0', '2e2h', 'assuming', 'the', 'peaks', 'originate', 'from', 'atomic', 'discreteness', 'this', 'agrees'... | [-0.13227354807361047, 0.14202287496656787, -0.009979064063150056, -0.07052349290877048, 0.05123671187962196, -0.10549376028760964, 0.1059745370876044, 0.3421364836394787, -0.2195237234462889, -0.4012815001971868, -0.06306660921569457, -0.37626961839138245, -0.11329980194568634, 0.21521486305365606, -0.0683932248122838... |
707.1337 | Root Systems and the Quantum Cohomology of ADE resolutions | We compute the C*-equivariant quantum cohomology ring of Y, the minimal
resolution of the DuVal singularity C^2/G where G is a finite subgroup of
SU(2). The quantum product is expressed in terms of an ADE root system
canonically associated to G. We generalize the resulting Frobenius manifold to
non-simply laced root ... | math.AG hep-th math.QA | we compute the cequivariant quantum cohomology ring of y the minimal resolution of the duval singularity c2g where g is a finite subgroup of su2 the quantum product is expressed in terms of an ade root system canonically associated to g we generalize the resulting frobenius manifold to nonsimply laced root systems to o... | [['we', 'compute', 'the', 'cequivariant', 'quantum', 'cohomology', 'ring', 'of', 'y', 'the', 'minimal', 'resolution', 'of', 'the', 'duval', 'singularity', 'c2g', 'where', 'g', 'is', 'a', 'finite', 'subgroup', 'of', 'su2', 'the', 'quantum', 'product', 'is', 'expressed', 'in', 'terms', 'of', 'an', 'ade', 'root', 'system'... | [-0.24208599636547787, 0.01579246024884078, -0.07221684491445939, 0.05117065824709053, -0.10010920370235867, -0.1642707831572828, -0.04406428986315637, 0.2911830261447142, -0.3344637570296263, -0.21031555490091788, 0.09378358639430168, -0.2648288624030863, -0.12996234921576066, 0.13976354202862049, -0.18119711214459913... |
707.1338 | l-Adic representations associated to modular forms over imaginary
quadratic fields | Let pi be a regular algebraic cuspidal automorphic representation of GL(2)
over an imaginary quadratic number field K such that the central character of
pi is invariant under the non-trivial automorphism of K. We show that pi is
associated with an l-adic Galois representation rho over K such that at each
prime of K o... | math.NT | let pi be a regular algebraic cuspidal automorphic representation of gl2 over an imaginary quadratic number field k such that the central character of pi is invariant under the nontrivial automorphism of k we show that pi is associated with an ladic galois representation rho over k such that at each prime of k outside ... | [['let', 'pi', 'be', 'a', 'regular', 'algebraic', 'cuspidal', 'automorphic', 'representation', 'of', 'gl2', 'over', 'an', 'imaginary', 'quadratic', 'number', 'field', 'k', 'such', 'that', 'the', 'central', 'character', 'of', 'pi', 'is', 'invariant', 'under', 'the', 'nontrivial', 'automorphism', 'of', 'k', 'we', 'show',... | [-0.28488151201794687, 0.12401191666160717, -0.18772013639559, -0.03095618867918744, -0.13149734035554067, -0.1318570398594397, -0.029548275979681755, 0.2676724344754303, -0.3882016701177812, -0.16928537626763884, -0.028310733506272376, -0.2695513614059859, -0.1339854732004952, 0.22103511169552803, -0.05890542578319428... |
707.1339 | Finding the Charge of the top quark in the Dilepton Channel | There is a question about the identity of the top quark. Is it the top quark
of the Standard Model (SM) with electric charge 2/3 or is it an exotic quark
with charge -4/3? An exotic quark has been proposed by D. Chang et
al.\cite{hep-ph/9810531, hep-ph/9805273}. This analysis will use the standard
CDF run II dilepton... | hep-ex | there is a question about the identity of the top quark is it the top quark of the standard model sm with electric charge 23 or is it an exotic quark with charge 43 an exotic quark has been proposed by d chang et alcitehepph9810531 hepph9805273 this analysis will use the standard cdf run ii dilepton sample the key ingr... | [['there', 'is', 'a', 'question', 'about', 'the', 'identity', 'of', 'the', 'top', 'quark', 'is', 'it', 'the', 'top', 'quark', 'of', 'the', 'standard', 'model', 'sm', 'with', 'electric', 'charge', '23', 'or', 'is', 'it', 'an', 'exotic', 'quark', 'with', 'charge', '43', 'an', 'exotic', 'quark', 'has', 'been', 'proposed',... | [-0.04524324474768946, 0.1627353834247333, -0.11427479352802038, 0.0991357333608903, -0.05598617561161518, -0.147054236412514, 0.07235504115000367, 0.2663009169884026, -0.19524091094965115, -0.3134268240071833, 0.027808670150116087, -0.3053727378509939, -0.0191559663717635, 0.11725443380884826, 0.01049081325531006, 0.0... |
707.134 | Plasma Suppression of Large Scale Structure Formation in the Universe | We point out that during the reionization epoch of the cosmic history, the
plasma collective effect among the ordinary matter would suppress the large
scale structure formation. The imperfect Debye shielding at finite temperature
would induce a residual long-range electrostatic potential which, working
together with ... | astro-ph | we point out that during the reionization epoch of the cosmic history the plasma collective effect among the ordinary matter would suppress the large scale structure formation the imperfect debye shielding at finite temperature would induce a residual longrange electrostatic potential which working together with the ba... | [['we', 'point', 'out', 'that', 'during', 'the', 'reionization', 'epoch', 'of', 'the', 'cosmic', 'history', 'the', 'plasma', 'collective', 'effect', 'among', 'the', 'ordinary', 'matter', 'would', 'suppress', 'the', 'large', 'scale', 'structure', 'formation', 'the', 'imperfect', 'debye', 'shielding', 'at', 'finite', 'te... | [-0.12285403589662534, 0.24758572936896853, -0.09417877327099547, 0.07665537719287915, -0.08935313521798034, -0.05506092155142533, 0.008238686245576238, 0.300709979833776, -0.2567343681137885, -0.3042614062699113, 0.0456537633613122, -0.2775792894369941, -0.011184863441636083, 0.16180840431286997, 0.07308050175794918, ... |
707.1341 | Coherence of an optically illuminated single nuclear spin qubit | We investigate the coherence properties of individual nuclear spin quantum
bits in diamond [Dutt et al., Science, 316, 1312 (2007)] when a proximal
electronic spin associated with a nitrogen-vacancy (NV) center is being
interrogated by optical radiation. The resulting nuclear spin dynamics are
governed by time-depend... | quant-ph | we investigate the coherence properties of individual nuclear spin quantum bits in diamond dutt et al science 316 1312 2007 when a proximal electronic spin associated with a nitrogenvacancy nv center is being interrogated by optical radiation the resulting nuclear spin dynamics are governed by timedependent hyperfine i... | [['we', 'investigate', 'the', 'coherence', 'properties', 'of', 'individual', 'nuclear', 'spin', 'quantum', 'bits', 'in', 'diamond', 'dutt', 'et', 'al', 'science', '316', '1312', '2007', 'when', 'a', 'proximal', 'electronic', 'spin', 'associated', 'with', 'a', 'nitrogenvacancy', 'nv', 'center', 'is', 'being', 'interroga... | [-0.08650896358186332, 0.21107748930319017, -0.049098918100959864, 0.03207771592984622, 0.005671835887958021, -0.1181951510297338, 0.026331591089216975, 0.4263824035077035, -0.2690054166087677, -0.3148752166224377, 0.05110303459771197, -0.26903493336143613, -0.09680046660076248, 0.2007822744419188, -0.01685341917166189... |
707.1342 | Top Quark Production and Decay Properties at the Tevatron | The latest results from the CDF and D0 collaborations on the top-quark
pair-production cross section and limits on electroweak production are
presented. Included are measurements of properties of the top quark such as
charge, lifetime, and the decay branching ratio t->Wb. In addition to
measurements about the top qua... | hep-ex | the latest results from the cdf and d0 collaborations on the topquark pairproduction cross section and limits on electroweak production are presented included are measurements of properties of the top quark such as charge lifetime and the decay branching ratio twb in addition to measurements about the top quark the sel... | [['the', 'latest', 'results', 'from', 'the', 'cdf', 'and', 'd0', 'collaborations', 'on', 'the', 'topquark', 'pairproduction', 'cross', 'section', 'and', 'limits', 'on', 'electroweak', 'production', 'are', 'presented', 'included', 'are', 'measurements', 'of', 'properties', 'of', 'the', 'top', 'quark', 'such', 'as', 'cha... | [-0.04633760171179082, 0.25512849021396494, -0.04611067371325025, 0.14696634834325767, -0.05741635629836517, -0.07910084500437296, 0.10382455761862706, 0.32056967140753057, -0.16803145638513792, -0.3057027253310514, 0.013715317642280855, -0.3803994059562683, 0.07862517675620657, 0.1521849906089704, 0.10386099422990074,... |
707.1343 | Albus 1: A very bright white dwarf candidate | We have serendipitously discovered a previously-unknown, bright source (B_T =
11.75+/-0.07 mag) with a very blue V_T-K_s color, to which we have named Albus
1. A photometric and astrometric study using Virtual Observatory tools has
shown that it possesses an appreciable proper motion and magnitudes and colors
very si... | astro-ph | we have serendipitously discovered a previouslyunknown bright source b_t 1175007 mag with a very blue v_tk_s color to which we have named albus 1 a photometric and astrometric study using virtual observatory tools has shown that it possesses an appreciable proper motion and magnitudes and colors very similar to those o... | [['we', 'have', 'serendipitously', 'discovered', 'a', 'previouslyunknown', 'bright', 'source', 'b_t', '1175007', 'mag', 'with', 'a', 'very', 'blue', 'v_tk_s', 'color', 'to', 'which', 'we', 'have', 'named', 'albus', '1', 'a', 'photometric', 'and', 'astrometric', 'study', 'using', 'virtual', 'observatory', 'tools', 'has'... | [-0.04705140658188611, 0.08151853354433307, -0.14131361865193437, 0.10084953992382477, -0.14079401969517533, -0.13056783148847323, 0.05820094178381719, 0.44179837154714685, -0.15718505792319776, -0.3689090191435657, 0.08565938080366897, -0.3494892932474613, -0.0882667842223064, 0.19225304987355085, -0.13216155848318809... |
707.1344 | Piecewise principal comodule algebras | A comodule algebra P over a Hopf algebra H with bijective antipode is called
principal if the coaction of H is Galois and P is H-equivariantly projective
(faithfully flat) over the coaction-invariant subalgebra B. We prove that
principality is a piecewise property: given N comodule-algebra surjections
P->Pi whose ker... | math.QA math.RA | a comodule algebra p over a hopf algebra h with bijective antipode is called principal if the coaction of h is galois and p is hequivariantly projective faithfully flat over the coactioninvariant subalgebra b we prove that principality is a piecewise property given n comodulealgebra surjections ppi whose kernels inters... | [['a', 'comodule', 'algebra', 'p', 'over', 'a', 'hopf', 'algebra', 'h', 'with', 'bijective', 'antipode', 'is', 'called', 'principal', 'if', 'the', 'coaction', 'of', 'h', 'is', 'galois', 'and', 'p', 'is', 'hequivariantly', 'projective', 'faithfully', 'flat', 'over', 'the', 'coactioninvariant', 'subalgebra', 'b', 'we', '... | [-0.19092932838793786, 0.11793322412631824, -0.07355458266101778, 0.028433862852580205, -0.1080393807424116, -0.18628201015599188, -0.03523881145792984, 0.39850360923446715, -0.43562490682234056, -0.11730847247508791, 0.08627055680835838, -0.25768468639580533, -0.13618908150237985, 0.16397878454154124, -0.0770090175665... |
707.1345 | Loss of star forming gas in SDSS galaxies | Using the star formation rates from the SDSS galaxy sample, extracted using
the MOPED algorithm, and the empirical Kennicutt law relating star formation
rate to gas density, we calculate the time evolution of the gas fraction as a
function of the present stellar mass. We show how the gas-to-stars ratio varies
with st... | astro-ph | using the star formation rates from the sdss galaxy sample extracted using the moped algorithm and the empirical kennicutt law relating star formation rate to gas density we calculate the time evolution of the gas fraction as a function of the present stellar mass we show how the gastostars ratio varies with stellar ma... | [['using', 'the', 'star', 'formation', 'rates', 'from', 'the', 'sdss', 'galaxy', 'sample', 'extracted', 'using', 'the', 'moped', 'algorithm', 'and', 'the', 'empirical', 'kennicutt', 'law', 'relating', 'star', 'formation', 'rate', 'to', 'gas', 'density', 'we', 'calculate', 'the', 'time', 'evolution', 'of', 'the', 'gas',... | [-0.05725383228975637, 0.10435872247597154, -0.08426639221865555, 0.09433924992857821, -0.03488810097895049, -0.02125259777531028, 0.03997935324160639, 0.4122176664913523, -0.12948588359647367, -0.35108861551973325, 0.04153262166515121, -0.27693599536693814, -0.04507524510845542, 0.21084067063598796, 0.0209741576510513... |
707.1346 | Role of Charged Gauge Fields in Generating Magnetic Seed Fields in
Bubble Collisions during the Cosmological Electroweak Phase Transition | We calculate the magnetic field generated during bubble collisions in a
first-order electroweak phase transition that may occur for some choices of
parameters in the minimal supersymmetric Standard Model. We show that for
sufficiently gentle collisions, where the Higgs field is relatively unperturbed
in the bubble ov... | astro-ph | we calculate the magnetic field generated during bubble collisions in a firstorder electroweak phase transition that may occur for some choices of parameters in the minimal supersymmetric standard model we show that for sufficiently gentle collisions where the higgs field is relatively unperturbed in the bubble overlap... | [['we', 'calculate', 'the', 'magnetic', 'field', 'generated', 'during', 'bubble', 'collisions', 'in', 'a', 'firstorder', 'electroweak', 'phase', 'transition', 'that', 'may', 'occur', 'for', 'some', 'choices', 'of', 'parameters', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'we', 'show', 'that', 'for',... | [-0.15914532452951252, 0.25066312055862106, -0.03603918641645289, 0.0873235050837096, -0.0522405350201498, -0.05749154688839782, -0.06355035880469526, 0.3535897906604439, -0.23278607490367645, -0.3117038185109958, 0.03706909830077545, -0.24640226948833624, -0.04907858986191649, 0.18474913603589185, 0.03573048145441641,... |
707.1347 | Spitzer IRAC observations of newly-discovered planetary nebulae from the
Macquarie-AAO-Strasbourg H-alpha Planetary Nebula Project | We compare H-alpha, radio continuum, and Spitzer Space Telescope (SST) images
of 58 planetary nebulae (PNe) recently discovered by the Macquarie-AAO-Strasbo-
urg H-alpha PN Project (MASH) of the SuperCOSMOS H-alpha Survey. Using InfraRed
Array Camera (IRAC) data we define the IR colors of PNe and demonstrate good
iso... | astro-ph | we compare halpha radio continuum and spitzer space telescope sst images of 58 planetary nebulae pne recently discovered by the macquarieaaostrasbo urg halpha pn project mash of the supercosmos halpha survey using infrared array camera irac data we define the ir colors of pne and demonstrate good isolation between thes... | [['we', 'compare', 'halpha', 'radio', 'continuum', 'and', 'spitzer', 'space', 'telescope', 'sst', 'images', 'of', '58', 'planetary', 'nebulae', 'pne', 'recently', 'discovered', 'by', 'the', 'macquarieaaostrasbo', 'urg', 'halpha', 'pn', 'project', 'mash', 'of', 'the', 'supercosmos', 'halpha', 'survey', 'using', 'infrare... | [0.013425164128729395, 0.023828316873182993, -0.07870380074944176, 0.09156786508811232, -0.10194934663517473, -0.044528439868070424, 0.06256535842063649, 0.5089121980743989, -0.15268243473457574, -0.3743915873425009, 0.05030528513295905, -0.28743223572814636, -0.05723628249346828, 0.16883129132158772, -0.07130745484069... |
707.1348 | Engineering Quantum States of a Nano-Resonator via a Simple Auxiliary
System | We show how to engineer an extensive range of non-linear Hamiltonians for a
nano-mechanical resonator. The technique requires only a time dependent drive
applied to a Cooper-pair box or second oscillator to which the nano-resonator
is coupled. This method allows one to generate a large number of non-classical
states,... | cond-mat.mes-hall quant-ph | we show how to engineer an extensive range of nonlinear hamiltonians for a nanomechanical resonator the technique requires only a time dependent drive applied to a cooperpair box or second oscillator to which the nanoresonator is coupled this method allows one to generate a large number of nonclassical states as well a... | [['we', 'show', 'how', 'to', 'engineer', 'an', 'extensive', 'range', 'of', 'nonlinear', 'hamiltonians', 'for', 'a', 'nanomechanical', 'resonator', 'the', 'technique', 'requires', 'only', 'a', 'time', 'dependent', 'drive', 'applied', 'to', 'a', 'cooperpair', 'box', 'or', 'second', 'oscillator', 'to', 'which', 'the', 'na... | [-0.11650842500465183, 0.17207252244883547, -0.057406895751824026, 0.030331504551276308, -0.0981004196379719, -0.21725036441509066, 0.0319068747399985, 0.3697211344180436, -0.2557640326819543, -0.31486755821468504, 0.04406300396859196, -0.26441043928884783, -0.14336663494609167, 0.2802349883894404, -0.01364942850617306... |
707.1349 | Exploring improved holographic theories for QCD: Part II | This paper is a continuation of ArXiv:0707.1324 where improved holographic
theories for QCD were set up and explored. Here, the IR confining geometries
are classified and analyzed. They all end in a "good" (repulsive) singularity
in the IR. The glueball spectra are gaped and discrete, and they favorably
compare to th... | hep-th hep-lat hep-ph | this paper is a continuation of arxiv07071324 where improved holographic theories for qcd were set up and explored here the ir confining geometries are classified and analyzed they all end in a good repulsive singularity in the ir the glueball spectra are gaped and discrete and they favorably compare to the lattice dat... | [['this', 'paper', 'is', 'a', 'continuation', 'of', 'arxiv07071324', 'where', 'improved', 'holographic', 'theories', 'for', 'qcd', 'were', 'set', 'up', 'and', 'explored', 'here', 'the', 'ir', 'confining', 'geometries', 'are', 'classified', 'and', 'analyzed', 'they', 'all', 'end', 'in', 'a', 'good', 'repulsive', 'singul... | [-0.11576228462350131, 0.19963302435423952, -0.132782423833498, 0.1358176683142753, -0.05389619380179228, -0.16850664240491547, -0.007221370927502655, 0.4100588348087375, -0.1917550176890059, -0.22460334752262992, 0.08713881365750267, -0.2714237577765192, -0.09789244133174758, 0.12703771321949633, 0.0020179314588224797... |
707.135 | Cosmological expansion and local physics | The interplay between cosmological expansion and local attraction in a
gravitationally bound system is revisited in various regimes. First, weakly
gravitating Newtonian systems are considered, followed by various exact
solutions describing a relativistic central object embedded in a Friedmann
universe. It is shown th... | gr-qc astro-ph | the interplay between cosmological expansion and local attraction in a gravitationally bound system is revisited in various regimes first weakly gravitating newtonian systems are considered followed by various exact solutions describing a relativistic central object embedded in a friedmann universe it is shown that the... | [['the', 'interplay', 'between', 'cosmological', 'expansion', 'and', 'local', 'attraction', 'in', 'a', 'gravitationally', 'bound', 'system', 'is', 'revisited', 'in', 'various', 'regimes', 'first', 'weakly', 'gravitating', 'newtonian', 'systems', 'are', 'considered', 'followed', 'by', 'various', 'exact', 'solutions', 'd... | [-0.19695843079770428, 0.14465268605521747, -0.09291136651521638, 0.15049267677102415, -0.07499310388008044, -0.17942395641335418, -0.07953518120838063, 0.2514071868909966, -0.1929769067537217, -0.256581122250784, 0.07447685197638791, -0.30865371747918074, -0.08277869392408146, 0.1638599018544136, -0.002764568521109010... |
707.1351 | Inverse approach to Einstein's equations for fluids with vanishing
anisotropic stress tensor | We expand previous work on an inverse approach to Einstein Field Equations
where we include fluids with energy flux and consider the vanishing of the
anisotropic stress tensor. We consider the approach using warped product
spacetimes of class $B_1$. Although restricted, these spacetimes include many
exact solutions o... | gr-qc astro-ph.CO | we expand previous work on an inverse approach to einstein field equations where we include fluids with energy flux and consider the vanishing of the anisotropic stress tensor we consider the approach using warped product spacetimes of class b_1 although restricted these spacetimes include many exact solutions of inter... | [['we', 'expand', 'previous', 'work', 'on', 'an', 'inverse', 'approach', 'to', 'einstein', 'field', 'equations', 'where', 'we', 'include', 'fluids', 'with', 'energy', 'flux', 'and', 'consider', 'the', 'vanishing', 'of', 'the', 'anisotropic', 'stress', 'tensor', 'we', 'consider', 'the', 'approach', 'using', 'warped', 'p... | [-0.13506583813805043, 0.07246664234391972, -0.07890435018457427, 0.06339020940202583, -0.0935386969770373, -0.13140155969857714, -0.07023601311190826, 0.33823233084162563, -0.22217690032373025, -0.26509114977812803, 0.10104381524895249, -0.25338715188795835, -0.1381397569174424, 0.1872976215154489, -0.0488969646479434... |
707.1352 | Mixed Lefschetz Theorems and Hodge-Riemann Bilinear Relations | Statements analogous to the Hard Lefschetz Theorem (HLT) and the
Hodge-Riemann bilinear relations (HRR) hold in a variety of contexts: they
impose restrictions on the cohomology algebra of a smooth compact K\"ahler
manifold or on the intersection cohomology of a projective toric variety; they
restrict the local monod... | math.AG | statements analogous to the hard lefschetz theorem hlt and the hodgeriemann bilinear relations hrr hold in a variety of contexts they impose restrictions on the cohomology algebra of a smooth compact kahler manifold or on the intersection cohomology of a projective toric variety they restrict the local monodromy of a p... | [['statements', 'analogous', 'to', 'the', 'hard', 'lefschetz', 'theorem', 'hlt', 'and', 'the', 'hodgeriemann', 'bilinear', 'relations', 'hrr', 'hold', 'in', 'a', 'variety', 'of', 'contexts', 'they', 'impose', 'restrictions', 'on', 'the', 'cohomology', 'algebra', 'of', 'a', 'smooth', 'compact', 'kahler', 'manifold', 'or... | [-0.14665361083256948, 0.019278433852710983, -0.12155367860990302, 0.14929811653277744, -0.13040524280243093, -0.15441035044143422, 0.029077495456489563, 0.3290836741921531, -0.3203946280155436, -0.24439394146099058, 0.17006297007983576, -0.18464160621376105, -0.14154185497359387, 0.19253271711583603, -0.19523811319672... |
707.1353 | Poincare duality and Periodicity | We construct periodic families of Poincare complexes, partially solving a
question of Hodgson that was posed in the proceedings of the 1982 Northwestern
homotopy theory conference. We also construct infinite families of Poincare
complexes whose top cell falls off after one suspension but which fail to embed
in a sphe... | math.AT math.GT | we construct periodic families of poincare complexes partially solving a question of hodgson that was posed in the proceedings of the 1982 northwestern homotopy theory conference we also construct infinite families of poincare complexes whose top cell falls off after one suspension but which fail to embed in a sphere o... | [['we', 'construct', 'periodic', 'families', 'of', 'poincare', 'complexes', 'partially', 'solving', 'a', 'question', 'of', 'hodgson', 'that', 'was', 'posed', 'in', 'the', 'proceedings', 'of', 'the', '1982', 'northwestern', 'homotopy', 'theory', 'conference', 'we', 'also', 'construct', 'infinite', 'families', 'of', 'poi... | [-0.1669785134303807, 0.08758820467769649, -0.14381909455088052, 0.0803186540195549, -0.0787704995353565, -0.16620615575547246, 0.010730751356194642, 0.28668399606690265, -0.2924524564366562, -0.23327606366100637, 0.1000213391856629, -0.24876063966164083, -0.15320864119425867, 0.15184043181326354, -0.18537013056321125,... |
707.1354 | Microscopic surface structure of C/SiC composite mirrors for space
cryogenic telescopes | We report on the microscopic surface structure of carbon-fiber-reinforced
silicon carbide (C/SiC) composite mirrors that have been improved for the Space
Infrared Telescope for Cosmology and Astrophysics (SPICA) and other cooled
telescopes. The C/SiC composite consists of carbon fiber, silicon carbide, and
residual s... | astro-ph | we report on the microscopic surface structure of carbonfiberreinforced silicon carbide csic composite mirrors that have been improved for the space infrared telescope for cosmology and astrophysics spica and other cooled telescopes the csic composite consists of carbon fiber silicon carbide and residual silicon specif... | [['we', 'report', 'on', 'the', 'microscopic', 'surface', 'structure', 'of', 'carbonfiberreinforced', 'silicon', 'carbide', 'csic', 'composite', 'mirrors', 'that', 'have', 'been', 'improved', 'for', 'the', 'space', 'infrared', 'telescope', 'for', 'cosmology', 'and', 'astrophysics', 'spica', 'and', 'other', 'cooled', 'te... | [-0.05426512276753783, 0.22306964846519645, -0.0701565863304388, -0.00016870789181934123, -0.009678211994469166, -0.15609748651657035, 0.002056313433465274, 0.45696658579742205, -0.19039181677953285, -0.3654393480179886, 0.093904713696718, -0.31963707637589645, -0.08090622623396271, 0.23328961160116116, -0.050132859603... |
707.1355 | Graphs of functions and vanishing free entropy | Suppose X is an n-tuple of selfadjoint elements in a tracial von Neumann
algebra M. If z is a selfadjoint element in M and for some selfadjoint element
y in the von Neumann algebra generated by X $\delta_0(y, z) < \delta_0(y) +
\delta_0(z)$, then $\chi(X \cup \{z\}) = -\infty$ (here $\chi$ and $\delta_0$
denote the m... | math.OA | suppose x is an ntuple of selfadjoint elements in a tracial von neumann algebra m if z is a selfadjoint element in m and for some selfadjoint element y in the von neumann algebra generated by x delta_0y z delta_0y delta_0z then chix cup z infty here chi and delta_0 denote the microstates free entropy and free entropy d... | [['suppose', 'x', 'is', 'an', 'ntuple', 'of', 'selfadjoint', 'elements', 'in', 'a', 'tracial', 'von', 'neumann', 'algebra', 'm', 'if', 'z', 'is', 'a', 'selfadjoint', 'element', 'in', 'm', 'and', 'for', 'some', 'selfadjoint', 'element', 'y', 'in', 'the', 'von', 'neumann', 'algebra', 'generated', 'by', 'x', 'delta_0y', '... | [-0.12788920083507296, 0.19374420546345, -0.06560815010535796, 0.014085170545773249, -0.013480813864069725, -0.20269717996208264, 0.0006281248393601605, 0.3193501219357131, -0.33680010164555696, -0.10331338742980734, 0.087691094740876, -0.35948121520673987, -0.016532487059261518, 0.17765986225484603, -0.123462610300131... |
707.1356 | Mirror symmetry aspects for compact G_2 manifolds | The present paper deals with mirror symmetry aspects of compact ``barely''
$G_2$ manifolds, that is, $G_2$ manifolds of the form (CY$\times
S^1)/\mathbb{Z}_2$. We propose that the mirror of any barely $G_2$ manifold is
another barely one and which is constructed as a fibration of the \emph{mirror}
of the CY base. Als... | hep-th math.AG math.GT | the present paper deals with mirror symmetry aspects of compact barely g_2 manifolds that is g_2 manifolds of the form cytimes s1mathbbz_2 we propose that the mirror of any barely g_2 manifold is another barely one and which is constructed as a fibration of the emphmirror of the cy base also we describe the joyce manif... | [['the', 'present', 'paper', 'deals', 'with', 'mirror', 'symmetry', 'aspects', 'of', 'compact', 'barely', 'g_2', 'manifolds', 'that', 'is', 'g_2', 'manifolds', 'of', 'the', 'form', 'cytimes', 's1mathbbz_2', 'we', 'propose', 'that', 'the', 'mirror', 'of', 'any', 'barely', 'g_2', 'manifold', 'is', 'another', 'barely', 'o... | [-0.17395565814850544, 0.07043042124421736, -0.07290297649517063, 0.08569321980844838, -0.10765062087209315, -0.11453954890271686, -0.03430712402455928, 0.34565185996956677, -0.21160143248687516, -0.23499026244493904, 0.15652821605426834, -0.24224637538219326, -0.234976695307734, 0.16792864257944687, -0.159600559939685... |
707.1357 | Calculations of canonical averages from the grand canonical ensemble | Grand canonical and canonical ensembles become equivalent in the
thermodynamic limit, but when the system size is finite the results obtained in
the two ensembles deviate from each other. In many important cases, the
canonical ensemble provides an appropriate physical description but it is often
much easier to perfor... | cond-mat.stat-mech | grand canonical and canonical ensembles become equivalent in the thermodynamic limit but when the system size is finite the results obtained in the two ensembles deviate from each other in many important cases the canonical ensemble provides an appropriate physical description but it is often much easier to perform the... | [['grand', 'canonical', 'and', 'canonical', 'ensembles', 'become', 'equivalent', 'in', 'the', 'thermodynamic', 'limit', 'but', 'when', 'the', 'system', 'size', 'is', 'finite', 'the', 'results', 'obtained', 'in', 'the', 'two', 'ensembles', 'deviate', 'from', 'each', 'other', 'in', 'many', 'important', 'cases', 'the', 'c... | [-0.05376254210603379, 0.16767092617242485, -0.12026340854575947, 0.13082327499010024, 0.07182707110907705, -0.07925639846583916, 0.00938715128272417, 0.358329166613874, -0.20281368032918268, -0.30161398458072824, 0.0271195531246208, -0.25144492309717903, -0.12072595101337702, 0.1621816380880773, -0.03445469630172565, ... |
707.1358 | Self-dual Vortices in the Abelian Chern-Simons Model with Two Complex
Scalar Fields | Making use of $\phi$-mapping topological current method, we discuss the
self-dual vortices in the Abelian Chern-Simons model with two complex scalar
fields. For each scalar field, an exact nontrivial equation with a topological
term which is missing in many references is derived analytically. The general
angular mome... | hep-th | making use of phimapping topological current method we discuss the selfdual vortices in the abelian chernsimons model with two complex scalar fields for each scalar field an exact nontrivial equation with a topological term which is missing in many references is derived analytically the general angular momentum is obta... | [['making', 'use', 'of', 'phimapping', 'topological', 'current', 'method', 'we', 'discuss', 'the', 'selfdual', 'vortices', 'in', 'the', 'abelian', 'chernsimons', 'model', 'with', 'two', 'complex', 'scalar', 'fields', 'for', 'each', 'scalar', 'field', 'an', 'exact', 'nontrivial', 'equation', 'with', 'a', 'topological', ... | [-0.19700044790685448, 0.17186962338761683, -0.05855666824694102, 0.12357253594018403, -0.09631622808228713, -0.11738196180764741, -0.06339731381012825, 0.3296145120402798, -0.23476437578210607, -0.2771604757484359, 0.04663014011384803, -0.22323902878148752, -0.15315965118740374, 0.16222108409177358, 0.0505755421375700... |
707.1359 | NMR Evidence for Spin Canting in a Bilayer nu = 2 Quantum Hall System | We investigate the electron spin states in the bilayer quantum Hall system at
total Landau level filling factor nu =2 exploiting current-pumped and
resistively detected NMR. The measured Knight shift, KS, of 75As nuclei reveals
continuous variation of the out-of-plane electronic spin polarization between
nearly full ... | cond-mat.mes-hall cond-mat.str-el | we investigate the electron spin states in the bilayer quantum hall system at total landau level filling factor nu 2 exploiting currentpumped and resistively detected nmr the measured knight shift ks of 75as nuclei reveals continuous variation of the outofplane electronic spin polarization between nearly full and zero ... | [['we', 'investigate', 'the', 'electron', 'spin', 'states', 'in', 'the', 'bilayer', 'quantum', 'hall', 'system', 'at', 'total', 'landau', 'level', 'filling', 'factor', 'nu', '2', 'exploiting', 'currentpumped', 'and', 'resistively', 'detected', 'nmr', 'the', 'measured', 'knight', 'shift', 'ks', 'of', '75as', 'nuclei', '... | [-0.19899237833710182, 0.2131529405287842, -0.021718282252550125, 0.02400153410465767, -0.008993698718647162, -0.11307236249558628, 0.07379959169775248, 0.3739757601585653, -0.24512586750917964, -0.31230968431466155, -0.02559556713482986, -0.297801805101335, -0.06385314349188573, 0.20083086655164759, 0.1201823657585514... |
707.136 | On the Distance and Molecular Environment of Westerlund 2 and HESS
J1023-575 | The extended TeV gamma-ray source HESS J1023-575 is coincident with the
massive, young stellar cluster Westerlund 2 (Wd2) and its surrounding HII
region RCW 49. On the basis of an analysis of the CO emission and 21 cm
absorption along the line of sight to Wd2, it is argued that this cluster, and
by assumption the TeV... | astro-ph | the extended tev gammaray source hess j1023575 is coincident with the massive young stellar cluster westerlund 2 wd2 and its surrounding hii region rcw 49 on the basis of an analysis of the co emission and 21 cm absorption along the line of sight to wd2 it is argued that this cluster and by assumption the tev source as... | [['the', 'extended', 'tev', 'gammaray', 'source', 'hess', 'j1023575', 'is', 'coincident', 'with', 'the', 'massive', 'young', 'stellar', 'cluster', 'westerlund', '2', 'wd2', 'and', 'its', 'surrounding', 'hii', 'region', 'rcw', '49', 'on', 'the', 'basis', 'of', 'an', 'analysis', 'of', 'the', 'co', 'emission', 'and', '21'... | [-0.07421248363302069, 0.054726242370853356, -0.04212358979215968, 0.058209210058103186, -0.05670237248206008, -0.046192043508491376, 0.07162622303912675, 0.43998752489522863, -0.1942463062453359, -0.3624307034115722, 0.04186292682828749, -0.2934881201707316, 0.009630900025911574, 0.14931854888810403, 0.043377336600912... |
707.1361 | A generalization of the Shestakov-Umirbaev inequality | We give a generalization of the Shestakov-Umirbaev inequality which plays an
important role in their solution of the tame generators conjecture.
| math.AC | we give a generalization of the shestakovumirbaev inequality which plays an important role in their solution of the tame generators conjecture | [['we', 'give', 'a', 'generalization', 'of', 'the', 'shestakovumirbaev', 'inequality', 'which', 'plays', 'an', 'important', 'role', 'in', 'their', 'solution', 'of', 'the', 'tame', 'generators', 'conjecture']] | [-0.19294126464852265, 0.018282003906538842, -0.13285707595891186, 0.11177680233404749, -0.03628963409435181, -0.12766750662454537, -0.049196503879058925, 0.2442918166163422, -0.2702634988263959, -0.2923042821210055, 0.08235299471388793, -0.22418483008541876, -0.22536910147893996, 0.22367163924943834, -0.12731225083449... |
707.1362 | Pareto Optima of Multicriteria Integer Linear Programs | We settle the computational complexity of fundamental questions related to
multicriteria integer linear programs, when the dimensions of the strategy
space and of the outcome space are considered fixed constants. In particular we
construct:
1. polynomial-time algorithms to exactly determine the number of Pareto
opt... | math.OC | we settle the computational complexity of fundamental questions related to multicriteria integer linear programs when the dimensions of the strategy space and of the outcome space are considered fixed constants in particular we construct 1 polynomialtime algorithms to exactly determine the number of pareto optima and p... | [['we', 'settle', 'the', 'computational', 'complexity', 'of', 'fundamental', 'questions', 'related', 'to', 'multicriteria', 'integer', 'linear', 'programs', 'when', 'the', 'dimensions', 'of', 'the', 'strategy', 'space', 'and', 'of', 'the', 'outcome', 'space', 'are', 'considered', 'fixed', 'constants', 'in', 'particular... | [-0.09074930871862012, 0.00865680890208685, -0.09642976678741114, 0.10386823478515621, -0.05713909999719141, -0.1725716596838456, 0.12734152921601324, 0.3748509329114411, -0.3499997490513566, -0.31332133621132624, 0.0995248969516356, -0.24567536432463843, -0.12267833114979235, 0.1339843095645208, -0.09387764166872781, ... |
707.1363 | A Compact Approximate Solution to the Kondo Problem | A compact approximate groundstate of the Kondo problem is introduced. It
consists of four Slater states. The spin up and down states of the localized
d-impurity are paired with two localized s-electron states of opposite spin.
All the remaining s-electron states are rearranged forming two new optimal
orthonormal base... | cond-mat.mes-hall cond-mat.str-el | a compact approximate groundstate of the kondo problem is introduced it consists of four slater states the spin up and down states of the localized dimpurity are paired with two localized selectron states of opposite spin all the remaining selectron states are rearranged forming two new optimal orthonormal bases throug... | [['a', 'compact', 'approximate', 'groundstate', 'of', 'the', 'kondo', 'problem', 'is', 'introduced', 'it', 'consists', 'of', 'four', 'slater', 'states', 'the', 'spin', 'up', 'and', 'down', 'states', 'of', 'the', 'localized', 'dimpurity', 'are', 'paired', 'with', 'two', 'localized', 'selectron', 'states', 'of', 'opposit... | [-0.18001293492125114, 0.2748708565632114, 0.0012656273211177904, 0.11502781325725664, 0.024340229767403798, -0.14781641408626456, 0.03428198586698272, 0.36628956436834414, -0.23307786865279922, -0.28454464094829746, 0.022177201680278813, -0.31315007609373424, -0.005393792147515342, 0.13837656995747238, 0.0935015064169... |
707.1364 | Report on Generic Case Complexity | This article is a short introduction to generic case complexity, which is a
recently developed way of measuring the difficulty of a computational problem
while ignoring atypical behavior on a small set of inputs. Generic case
complexity applies to both recursively solvable and recursively unsolvable
problems.
| cs.CC | this article is a short introduction to generic case complexity which is a recently developed way of measuring the difficulty of a computational problem while ignoring atypical behavior on a small set of inputs generic case complexity applies to both recursively solvable and recursively unsolvable problems | [['this', 'article', 'is', 'a', 'short', 'introduction', 'to', 'generic', 'case', 'complexity', 'which', 'is', 'a', 'recently', 'developed', 'way', 'of', 'measuring', 'the', 'difficulty', 'of', 'a', 'computational', 'problem', 'while', 'ignoring', 'atypical', 'behavior', 'on', 'a', 'small', 'set', 'of', 'inputs', 'gene... | [-0.10312069381546715, 0.08402444090208282, -0.03752436505569874, 0.10624274965021355, -0.15641004162962022, -0.1664257025670098, 0.054489903789742486, 0.2970260510869, -0.3231475879843144, -0.3012727306264898, 0.10385640173057176, -0.21458531391766408, -0.18966492504367363, 0.222939763015703, -0.11320551326903312, 0.0... |
707.1365 | Conditions for Generic Initial Ideals to be Almost Reverse Lexicographic | Let $I$ be a homogeneous Artinian ideal in a polynomial ring
$R=k[x_1,...,x_n]$ over a field $k$ of characteristic 0. We study an equivalent
condition for the generic initial ideal $\gin(I)$ with respect to reverse
lexicographic order to be almost reverse lexicographic. As a result, we show
that Moreno-Socias conject... | math.AC | let i be a homogeneous artinian ideal in a polynomial ring rkx_1x_n over a field k of characteristic 0 we study an equivalent condition for the generic initial ideal gini with respect to reverse lexicographic order to be almost reverse lexicographic as a result we show that morenosocias conjecture implies froberg conje... | [['let', 'i', 'be', 'a', 'homogeneous', 'artinian', 'ideal', 'in', 'a', 'polynomial', 'ring', 'rkx_1x_n', 'over', 'a', 'field', 'k', 'of', 'characteristic', '0', 'we', 'study', 'an', 'equivalent', 'condition', 'for', 'the', 'generic', 'initial', 'ideal', 'gini', 'with', 'respect', 'to', 'reverse', 'lexicographic', 'ord... | [-0.1536398012423888, 0.06011958596172917, -0.05071911904378794, 0.07778284466379166, -0.05943950425523023, -0.23678502563852816, -0.04813403732453783, 0.39224600621964784, -0.3754223323504751, -0.1458444207116069, 0.08914297025864168, -0.2580541632836685, -0.09193221378372982, 0.14413640879793094, -0.06959962557108762... |
707.1366 | Neutron Scattering Study of the Localized Mode in the beta-Pyrochlore
Superconductors AOs2O6 | Inelastic neutron scattering and neutron powder diffraction experiments were
carried out to investigate a localized mode, proposed from various bulk
measurements, in the beta-pyrochlore AOs2O6 (A=K, Rb, Cs). The localized mode
was identified in all the three compounds as well as another beta-pyrochlore
CsW2O6. The an... | cond-mat.mtrl-sci cond-mat.supr-con | inelastic neutron scattering and neutron powder diffraction experiments were carried out to investigate a localized mode proposed from various bulk measurements in the betapyrochlore aos2o6 ak rb cs the localized mode was identified in all the three compounds as well as another betapyrochlore csw2o6 the anharmonicity o... | [['inelastic', 'neutron', 'scattering', 'and', 'neutron', 'powder', 'diffraction', 'experiments', 'were', 'carried', 'out', 'to', 'investigate', 'a', 'localized', 'mode', 'proposed', 'from', 'various', 'bulk', 'measurements', 'in', 'the', 'betapyrochlore', 'aos2o6', 'ak', 'rb', 'cs', 'the', 'localized', 'mode', 'was', ... | [-0.11940930546577072, 0.20744340744469378, -0.02777960726012618, 0.020663715435302484, -0.018307163182772316, -0.12318114098950715, 0.12340694089751628, 0.3497493352930425, -0.2338171379494686, -0.232332976329756, 0.0603360490384117, -0.3874303774624053, -0.0748654310552056, 0.18262100174738946, 0.07076985883414035, 0... |
707.1367 | Generation and Measurement of Non Equilibrium Spin Currents in Two
Terminal Systems | Generation and measurement of non-equilibrium spin current in two probe
configuration is discussed. It is argued and shown that spin current can be
generated in two terminal non-magnetic system. Further it is shown that these
spin currents can be measured via conductance in two probe configuration when
the detector p... | cond-mat.mes-hall | generation and measurement of nonequilibrium spin current in two probe configuration is discussed it is argued and shown that spin current can be generated in two terminal nonmagnetic system further it is shown that these spin currents can be measured via conductance in two probe configuration when the detector probe i... | [['generation', 'and', 'measurement', 'of', 'nonequilibrium', 'spin', 'current', 'in', 'two', 'probe', 'configuration', 'is', 'discussed', 'it', 'is', 'argued', 'and', 'shown', 'that', 'spin', 'current', 'can', 'be', 'generated', 'in', 'two', 'terminal', 'nonmagnetic', 'system', 'further', 'it', 'is', 'shown', 'that', ... | [-0.15495076227055576, 0.25704350695014, -0.05435133686002631, 0.05155505726221376, 0.0113259288482368, -0.1956298909544085, -0.08994867151621012, 0.40830736700445414, -0.2944040023542654, -0.2929447224506965, 0.06051601380190382, -0.2657557923096017, -0.10547110924604707, 0.25702414040614924, 0.05068340455181897, -0.0... |
707.1368 | Generalized Bounded Variation and Inserting point masses | Let $d\mu$ be a probability measure on the unit circle and $d\nu$ be the
measure formed by adding a pure point to $d\mu$. We give a simple formula for
the Verblunsky coefficients of $d\nu$ based on a result of Simon.
Then we consider $d\mu_0$, a probability measure on the unit circle with
$\ell^2$ Verblunsky coeffi... | math.CA | let dmu be a probability measure on the unit circle and dnu be the measure formed by adding a pure point to dmu we give a simple formula for the verblunsky coefficients of dnu based on a result of simon then we consider dmu_0 a probability measure on the unit circle with ell2 verblunsky coefficients alpha_n dmu_0_n0inf... | [['let', 'dmu', 'be', 'a', 'probability', 'measure', 'on', 'the', 'unit', 'circle', 'and', 'dnu', 'be', 'the', 'measure', 'formed', 'by', 'adding', 'a', 'pure', 'point', 'to', 'dmu', 'we', 'give', 'a', 'simple', 'formula', 'for', 'the', 'verblunsky', 'coefficients', 'of', 'dnu', 'based', 'on', 'a', 'result', 'of', 'sim... | [-0.13871264495983995, 0.12824673379308607, -0.07012535074023685, 0.029909968809681758, -0.02673035575808283, -0.11926953564826513, 0.09090700133295124, 0.3475295541796582, -0.3014862560238575, -0.16398281995435618, 0.10349071655276751, -0.33324641240703545, -0.13807179117032492, 0.1405032975977698, -0.1116190400328829... |
707.1369 | Impact of Locally Suppressed Wave sources on helioseismic travel times | Wave travel-time shifts in the vicinity of sunspots are typically interpreted
as arising predominantly from magnetic fields, flows, and local changes in
sound speed. We show here that the suppression of granulation related wave
sources in a sunspot can also contribute significantly to these travel-time
shifts, and in... | astro-ph | wave traveltime shifts in the vicinity of sunspots are typically interpreted as arising predominantly from magnetic fields flows and local changes in sound speed we show here that the suppression of granulation related wave sources in a sunspot can also contribute significantly to these traveltime shifts and in some ca... | [['wave', 'traveltime', 'shifts', 'in', 'the', 'vicinity', 'of', 'sunspots', 'are', 'typically', 'interpreted', 'as', 'arising', 'predominantly', 'from', 'magnetic', 'fields', 'flows', 'and', 'local', 'changes', 'in', 'sound', 'speed', 'we', 'show', 'here', 'that', 'the', 'suppression', 'of', 'granulation', 'related', ... | [-0.149337926510374, 0.2325924751886385, -0.025969518633279468, 0.10672164324506962, -0.040476377708403094, -0.03842910977051511, 0.04856426343611331, 0.4103038873417313, -0.27454839940448267, -0.34494848280102786, 0.08567171722832691, -0.3053526440249283, -0.09559663821996787, 0.23171392475843544, -0.02569982625750361... |
707.137 | Neutral-current Neutrino-nucleus Scattering in Quasielastic Region | The neutral-current neutrino-nucleus scattering is calculated through the
neutrino-induced knocked-out nucleon process in the quasielastic region by
using a relativistic single particle model for the bound and continuum states.
The incident energy range between 500 MeV and 1.0 GeV is used for the neutrino
(antineutri... | nucl-th | the neutralcurrent neutrinonucleus scattering is calculated through the neutrinoinduced knockedout nucleon process in the quasielastic region by using a relativistic single particle model for the bound and continuum states the incident energy range between 500 mev and 10 gev is used for the neutrino antineutrino scatte... | [['the', 'neutralcurrent', 'neutrinonucleus', 'scattering', 'is', 'calculated', 'through', 'the', 'neutrinoinduced', 'knockedout', 'nucleon', 'process', 'in', 'the', 'quasielastic', 'region', 'by', 'using', 'a', 'relativistic', 'single', 'particle', 'model', 'for', 'the', 'bound', 'and', 'continuum', 'states', 'the', '... | [-0.018230437683122394, 0.2613403837748089, -0.05370881104190807, 0.19262757327346353, 0.022271734758142328, -0.028798227883350937, 0.08202554807247757, 0.3561689409142523, -0.19588658092453062, -0.29354439856647285, -0.08462196157440471, -0.3665380867342781, 0.04436620899919167, 0.14481183705575656, 0.1305158170506932... |
707.1371 | Accesing the Gluon Polarization through the Double Longitudinal Spin
Asymmetrie in Charged Pion Production at PHENIX | With proton-proton collisions at PHENIX a variety of direct channels are used
to probe the proton substructure. Of the many channels available at PHENIX,
charged pion measurements are expected to have sensitivity of Delta g and thus
help in the global analysis that will constrain it. We present a measurement of
mid-r... | hep-ex | with protonproton collisions at phenix a variety of direct channels are used to probe the proton substructure of the many channels available at phenix charged pion measurements are expected to have sensitivity of delta g and thus help in the global analysis that will constrain it we present a measurement of midrapidity... | [['with', 'protonproton', 'collisions', 'at', 'phenix', 'a', 'variety', 'of', 'direct', 'channels', 'are', 'used', 'to', 'probe', 'the', 'proton', 'substructure', 'of', 'the', 'many', 'channels', 'available', 'at', 'phenix', 'charged', 'pion', 'measurements', 'are', 'expected', 'to', 'have', 'sensitivity', 'of', 'delta... | [-0.06777745790188075, 0.26284512241899566, -0.13566717336180847, 0.10356310098683713, 0.0010507901111063925, -0.11927232237114269, -0.04183122114517499, 0.3637266402208322, -0.19726749463636126, -0.3165175992039007, -0.06168563747180726, -0.403238939763223, 0.1781795825683386, 0.18503348491582516, 0.12051911644536902,... |
707.1372 | Computability Closure: Ten Years Later | The notion of computability closure has been introduced for proving the
termination of higher-order rewriting with first-order matching by Jean-Pierre
Jouannaud and Mitsuhiro Okada in a 1997 draft which later served as a basis for
the author's PhD. In this paper, we show how this notion can also be used for
dealing w... | cs.LO | the notion of computability closure has been introduced for proving the termination of higherorder rewriting with firstorder matching by jeanpierre jouannaud and mitsuhiro okada in a 1997 draft which later served as a basis for the authors phd in this paper we show how this notion can also be used for dealing with beta... | [['the', 'notion', 'of', 'computability', 'closure', 'has', 'been', 'introduced', 'for', 'proving', 'the', 'termination', 'of', 'higherorder', 'rewriting', 'with', 'firstorder', 'matching', 'by', 'jeanpierre', 'jouannaud', 'and', 'mitsuhiro', 'okada', 'in', 'a', '1997', 'draft', 'which', 'later', 'served', 'as', 'a', '... | [-0.11067434650853522, 0.09479011742019071, -0.12295713135587776, 0.09013886089448256, -0.15984177443175768, -0.10824325001290576, 0.051524676240149364, 0.3047396469830482, -0.3144915289330212, -0.3025352074841638, 0.07343752865779622, -0.25773083644896005, -0.15191088676979872, 0.11508639101400849, -0.1061215335214587... |
707.1373 | Polarized Parton Densities and Higher Twist in the Light of the Recent
CLAS and COMPASS data | The impact of the recent very precise CLAS and COMPASS g_1/F_1 data on
polarized parton densities and higher twist effects is discussed. We
demonstrate that the low Q^2 CLAS data improve essentially our knowledge of
higher twist corrections to the spin structure function g1, while the large Q^2
COMPASS data influence... | hep-ph hep-ex | the impact of the recent very precise clas and compass g_1f_1 data on polarized parton densities and higher twist effects is discussed we demonstrate that the low q2 clas data improve essentially our knowledge of higher twist corrections to the spin structure function g1 while the large q2 compass data influence mainly... | [['the', 'impact', 'of', 'the', 'recent', 'very', 'precise', 'clas', 'and', 'compass', 'g_1f_1', 'data', 'on', 'polarized', 'parton', 'densities', 'and', 'higher', 'twist', 'effects', 'is', 'discussed', 'we', 'demonstrate', 'that', 'the', 'low', 'q2', 'clas', 'data', 'improve', 'essentially', 'our', 'knowledge', 'of', ... | [-0.06165121575110558, 0.24078358921323376, -0.13882144872121602, 0.15428922632400574, -0.10667772427571556, -0.0742057717337935, 0.053279461521453346, 0.36982067589120693, -0.1878485509912562, -0.2500492338405316, -0.012480239104760071, -0.29553536519812174, -0.014549670348235642, 0.1470274034809007, 0.049521245092156... |
707.1374 | The quantummechanical wave equations from a relativistic viewpoint | A derivation is presented of the quantummechanical wave equations based upon
the Equity Principle of Einstein's General Relativity Theory. This is believed
to be more generic than the common derivations based upon Einstein's energy
relationship for moving particles. It is shown that Schrodinger's Equation, if
properl... | physics.gen-ph | a derivation is presented of the quantummechanical wave equations based upon the equity principle of einsteins general relativity theory this is believed to be more generic than the common derivations based upon einsteins energy relationship for moving particles it is shown that schrodingers equation if properly formul... | [['a', 'derivation', 'is', 'presented', 'of', 'the', 'quantummechanical', 'wave', 'equations', 'based', 'upon', 'the', 'equity', 'principle', 'of', 'einsteins', 'general', 'relativity', 'theory', 'this', 'is', 'believed', 'to', 'be', 'more', 'generic', 'than', 'the', 'common', 'derivations', 'based', 'upon', 'einsteins... | [-0.12158598885759263, 0.13800088803480934, -0.14019963318812012, 0.10888927551589525, -0.12652050189853434, -0.1253232892956136, -0.05112425646241838, 0.30279861109230266, -0.22410842269681483, -0.2557408066988216, -0.0030924393956728996, -0.27634440641289193, -0.15447564618325377, 0.1792218483190602, -0.0372353878912... |
707.1375 | Szego kernels, Toeplitz operators, and equivariant fixed point formulae | Let $\gamma$ be an automorphism of a polarized complex projective manifold
$(M,L)$. Then $\gamma$ induces an automorphism $\gamma_k$ of the space of
global holomorphic sections of the $k$-th tensor power of $L$, for every
$k=1,2,...$; for $k\gg 0$, the Lefschetz fixed point formula expresses the
trace of $\gamma_k$ i... | math.AG math.CV math.SG | let gamma be an automorphism of a polarized complex projective manifold ml then gamma induces an automorphism gamma_k of the space of global holomorphic sections of the kth tensor power of l for every k12 for kgg 0 the lefschetz fixed point formula expresses the trace of gamma_k in terms of fixed point data more genera... | [['let', 'gamma', 'be', 'an', 'automorphism', 'of', 'a', 'polarized', 'complex', 'projective', 'manifold', 'ml', 'then', 'gamma', 'induces', 'an', 'automorphism', 'gamma_k', 'of', 'the', 'space', 'of', 'global', 'holomorphic', 'sections', 'of', 'the', 'kth', 'tensor', 'power', 'of', 'l', 'for', 'every', 'k12', 'for', '... | [-0.19984042442383917, 0.09181713994461564, -0.08481517530554998, 0.045586910457944774, -0.07209756185386515, -0.10433087670013097, -0.007837046053366247, 0.334889176212489, -0.3297455807526906, -0.18514812102950845, 0.10110239356967575, -0.28925996659495307, -0.14549886640029172, 0.1713711421140833, -0.087602740609423... |
707.1376 | Can Phantom-Dominated Universe Decelerate Also in Future ? | Here Randall-Sundrum brane-gravity models of the homogeneous and flat
universe, dominated by phantom fluid, is considered. It is noted that
brane-gravity corrections effect the behaviour of phantom fluid in RS-II model
(where brane-tension $\lambda$ is negative) drastically. It is interesting to
see that, phantom flu... | gr-qc | here randallsundrum branegravity models of the homogeneous and flat universe dominated by phantom fluid is considered it is noted that branegravity corrections effect the behaviour of phantom fluid in rsii model where branetension lambda is negative drastically it is interesting to see that phantom fluid violates the w... | [['here', 'randallsundrum', 'branegravity', 'models', 'of', 'the', 'homogeneous', 'and', 'flat', 'universe', 'dominated', 'by', 'phantom', 'fluid', 'is', 'considered', 'it', 'is', 'noted', 'that', 'branegravity', 'corrections', 'effect', 'the', 'behaviour', 'of', 'phantom', 'fluid', 'in', 'rsii', 'model', 'where', 'bra... | [-0.12747964396692602, 0.19099846797040368, -0.10328313874823478, 0.11668810426387229, -0.10998948111163476, -0.24894637287641533, -0.07738543577238775, 0.28059058517359103, -0.21374343000234494, -0.2799228644492164, 0.024373303550660988, -0.25808532497715914, -0.03353027506183267, 0.09880054158842357, -0.0041168608048... |
707.1377 | On the Potential of Large Ring Lasers | We describe a new ring laser with area A = 833 m^2 and update performance
statistics for several such machines. Anandan & Chaio 1982 judged ring lasers
inferior to matter interferometers as possible detectors of gravitational
waves. However, we note that geophysically interesting results have been
obtained from large... | physics.optics physics.gen-ph | we describe a new ring laser with area a 833 m2 and update performance statistics for several such machines anandan chaio 1982 judged ring lasers inferior to matter interferometers as possible detectors of gravitational waves however we note that geophysically interesting results have been obtained from large ring lase... | [['we', 'describe', 'a', 'new', 'ring', 'laser', 'with', 'area', 'a', '833', 'm2', 'and', 'update', 'performance', 'statistics', 'for', 'several', 'such', 'machines', 'anandan', 'chaio', '1982', 'judged', 'ring', 'lasers', 'inferior', 'to', 'matter', 'interferometers', 'as', 'possible', 'detectors', 'of', 'gravitationa... | [-0.14187174587573667, 0.11117282355898771, -0.08885805412211407, 0.0566785594515534, -0.04992269719871929, -0.19087553302899507, 0.0010831065720610193, 0.4408867728533381, -0.20629877932231588, -0.2850320750247624, 0.11790990954170287, -0.28287403238148, -0.1292894963309232, 0.31169594972694326, -0.10226834861372235, ... |
707.1378 | Pileup subtraction using jet areas | One of the major challenges for the LHC will be to extract precise
information from hadronic final states in the presence of the large number of
additional soft pp collisions, pileup, that occur simultaneously with any hard
interaction in high luminosity runs. We propose a novel technique, based on jet
areas, that pr... | hep-ph hep-ex | one of the major challenges for the lhc will be to extract precise information from hadronic final states in the presence of the large number of additional soft pp collisions pileup that occur simultaneously with any hard interaction in high luminosity runs we propose a novel technique based on jet areas that provides ... | [['one', 'of', 'the', 'major', 'challenges', 'for', 'the', 'lhc', 'will', 'be', 'to', 'extract', 'precise', 'information', 'from', 'hadronic', 'final', 'states', 'in', 'the', 'presence', 'of', 'the', 'large', 'number', 'of', 'additional', 'soft', 'pp', 'collisions', 'pileup', 'that', 'occur', 'simultaneously', 'with', ... | [-0.026803642784341657, 0.15736141844636536, -0.15125847349328728, 0.13445724182910734, -0.08737941591293905, -0.13302130663590828, -0.03409135446819509, 0.38010388574811854, -0.2285454675177883, -0.3311893446852678, 0.08038899941261504, -0.2732333372636088, -0.02577105498118005, 0.2151837225136315, -0.0303061496514570... |
707.1379 | Streamwise evolution of the entrainment in a steady two-dimensional
bluff-body wake | This paper has been withdrawn by the authors, as it has been rejected in
October 2007.
| physics.flu-dyn | this paper has been withdrawn by the authors as it has been rejected in october 2007 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'as', 'it', 'has', 'been', 'rejected', 'in', 'october', '2007']] | [-0.02752448093087878, 0.013390174368396401, -0.2249844924081117, -0.04644613868003944, -0.13103044359013438, -0.0784574857680127, -0.05168490501091583, 0.4146173456683755, -0.12409932841546834, -0.45763926114887, 0.18716220664646244, -0.33418914396315813, -0.14523998624645174, 0.07401023164857179, -0.2967749878298491,... |
707.138 | Low-mass lithium-rich AGB stars in the Galactic bulge: evidence for Cool
Bottom Processing? | Context: The stellar production of the light element lithium is still a
matter of debate.
Aims: We report the detection of low-mass, Li-rich Asymptotic Giant Branch
(AGB) stars located in the Galactic bulge.
Methods: A homogeneous and well-selected sample of low mass, oxygen-rich AGB
stars in the Galactic bulge h... | astro-ph | context the stellar production of the light element lithium is still a matter of debate aims we report the detection of lowmass lirich asymptotic giant branch agb stars located in the galactic bulge methods a homogeneous and wellselected sample of low mass oxygenrich agb stars in the galactic bulge has been searched fo... | [['context', 'the', 'stellar', 'production', 'of', 'the', 'light', 'element', 'lithium', 'is', 'still', 'a', 'matter', 'of', 'debate', 'aims', 'we', 'report', 'the', 'detection', 'of', 'lowmass', 'lirich', 'asymptotic', 'giant', 'branch', 'agb', 'stars', 'located', 'in', 'the', 'galactic', 'bulge', 'methods', 'a', 'hom... | [-0.048802600764430104, 0.16806929990619768, -0.048936145187516406, 0.11493683182802725, -0.09650862358377715, -0.06442926340478372, 0.11899179344375928, 0.39229519224920156, -0.13242636158072155, -0.3658902996507694, 0.03958315914403273, -0.2942761310776434, -0.006382374907376237, 0.1602068829582069, -0.13193539407171... |
707.1381 | The characteristic quasi-polynomials of the arrangements of root systems
and mid-hyperplane arrangements | Let $q$ be a positive integer. In our recent paper, we proved that the
cardinality of the complement of an integral arrangement, after the modulo $q$
reduction, is a quasi-polynomial of $q$, which we call the characteristic
quasi-polynomial. In this paper, we study general properties of the
characteristic quasi-polyn... | math.CO math.RT | let q be a positive integer in our recent paper we proved that the cardinality of the complement of an integral arrangement after the modulo q reduction is a quasipolynomial of q which we call the characteristic quasipolynomial in this paper we study general properties of the characteristic quasipolynomial as well as d... | [['let', 'q', 'be', 'a', 'positive', 'integer', 'in', 'our', 'recent', 'paper', 'we', 'proved', 'that', 'the', 'cardinality', 'of', 'the', 'complement', 'of', 'an', 'integral', 'arrangement', 'after', 'the', 'modulo', 'q', 'reduction', 'is', 'a', 'quasipolynomial', 'of', 'q', 'which', 'we', 'call', 'the', 'characterist... | [-0.16833021614088942, 0.0732099206662266, -0.08034701763527162, 0.039932511790321944, -0.06243665064963053, -0.12731714969250693, -0.010922106399909775, 0.30437042344180837, -0.3020371041649869, -0.26576900950619087, 0.09456467107911386, -0.2536872331150321, -0.19882849330575997, 0.21240653921224512, -0.06557130575207... |
707.1382 | Thermal Phase in Bubbling Geometries | This paper has been withdrawn by the author due to a crucial sign error in
equation 1.
| hep-th | this paper has been withdrawn by the author due to a crucial sign error in equation 1 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'a', 'crucial', 'sign', 'error', 'in', 'equation', '1']] | [-0.13030415652867625, -0.017005475895369753, -0.09216447875780218, -0.006315592601073577, -0.10587231431375532, -0.12000912271768731, -0.009933547000400722, 0.2967071235179901, -0.28005319965236325, -0.3795580270097536, 0.1219479086849948, -0.2789364844998893, -0.17245428954415462, 0.06643538264667287, -0.252092899809... |
707.1383 | Vortex rings in ferromagnets | Vortex ring solutions are presented for the Landau-Lifshitz equation, which
models the dynamics of a three-dimensional ferromagnet. The vortex rings
propagate at constant speed along their symmetry axis and are characterized by
the integer-valued Hopf charge. They are stable to axial perturbations, but it
is demonstr... | cond-mat.mes-hall hep-ph hep-th | vortex ring solutions are presented for the landaulifshitz equation which models the dynamics of a threedimensional ferromagnet the vortex rings propagate at constant speed along their symmetry axis and are characterized by the integervalued hopf charge they are stable to axial perturbations but it is demonstrated that... | [['vortex', 'ring', 'solutions', 'are', 'presented', 'for', 'the', 'landaulifshitz', 'equation', 'which', 'models', 'the', 'dynamics', 'of', 'a', 'threedimensional', 'ferromagnet', 'the', 'vortex', 'rings', 'propagate', 'at', 'constant', 'speed', 'along', 'their', 'symmetry', 'axis', 'and', 'are', 'characterized', 'by'... | [-0.2660728018062756, 0.17051304558269254, -0.08794842120664922, 0.0661305480322841, -0.09151392375807399, -0.13798116168498223, -0.08252645687746775, 0.37841411678363446, -0.29844453696809387, -0.197401701974804, 0.10949345777803303, -0.23638347456960573, -0.077879458244728, 0.16396037562213758, 0.028818794752916564, ... |
707.1384 | Asymptotically Optimal Estimator of the Parameter of Semi-Linear
Autoregression | The difference equations $\xi_{k}=af(\xi_{k-1})+\epsilon_{k}$, where
$(\epsilon_k)$ is a square integrable difference martingale, and the
differential equation ${\rm d}\xi=-af(\xi){\rm d}t+{\rm d}\eta$, where $\eta$
is a square integrable martingale, are considered. A family of estimators
depending, besides the sampl... | math.ST math.DS stat.AP stat.TH | the difference equations xi_kafxi_k1epsilon_k where epsilon_k is a square integrable difference martingale and the differential equation rm dxiafxirm dtrm deta where eta is a square integrable martingale are considered a family of estimators depending besides the sample size n or the observation period if time is conti... | [['the', 'difference', 'equations', 'xi_kafxi_k1epsilon_k', 'where', 'epsilon_k', 'is', 'a', 'square', 'integrable', 'difference', 'martingale', 'and', 'the', 'differential', 'equation', 'rm', 'dxiafxirm', 'dtrm', 'deta', 'where', 'eta', 'is', 'a', 'square', 'integrable', 'martingale', 'are', 'considered', 'a', 'family... | [-0.16522597939835798, 0.13840474963894692, -0.07430419498444374, 0.12055630053008168, -0.07891851957437807, -0.15574089571801497, -0.020270229228932797, 0.3502849060399779, -0.31040626253675796, -0.16438374453192128, 0.19691692226855406, -0.3165829174605937, -0.09859016576203807, 0.15590659080571012, -0.05520298397810... |
707.1385 | Measurement of eta photoproduction on the proton from threshold to 1500
MeV | Beam asymmetry and differential cross section for the reaction gamma+p->eta+p
were measured from production threshold to 1500 MeV photon laboratory energy.
The two dominant neutral decay modes of the eta meson, eta->2g and eta->3pi0,
were analyzed. The full set of measurements is in good agreement with
previously pub... | nucl-ex | beam asymmetry and differential cross section for the reaction gammapetap were measured from production threshold to 1500 mev photon laboratory energy the two dominant neutral decay modes of the eta meson eta2g and eta3pi0 were analyzed the full set of measurements is in good agreement with previously published results... | [['beam', 'asymmetry', 'and', 'differential', 'cross', 'section', 'for', 'the', 'reaction', 'gammapetap', 'were', 'measured', 'from', 'production', 'threshold', 'to', '1500', 'mev', 'photon', 'laboratory', 'energy', 'the', 'two', 'dominant', 'neutral', 'decay', 'modes', 'of', 'the', 'eta', 'meson', 'eta2g', 'and', 'eta... | [-0.06641474597315054, 0.16521705325874614, -0.06056045436210896, 0.12489840955751744, -0.012907111652766173, -0.14777224600065228, 0.02455151480304577, 0.40041722548080655, -0.1567366325932487, -0.35324808905219157, 0.01698355350739936, -0.3862096720670418, 0.02064068127060082, 0.20794591694933975, 0.08948859718923526... |
707.1386 | Optical far-infrared properties of graphene monolayer and multilayers | We analyze the features of the graphene mono- and multilayer reflectance in
the far-infrared region as a function of frequency, temperature, and carrier
density taking the intraband conductance and the interband electron absorbtion
into account. The dispersion of plasmon mode of the multilayers is calculated
using Ma... | cond-mat.soft cond-mat.mes-hall | we analyze the features of the graphene mono and multilayer reflectance in the farinfrared region as a function of frequency temperature and carrier density taking the intraband conductance and the interband electron absorbtion into account the dispersion of plasmon mode of the multilayers is calculated using maxwells ... | [['we', 'analyze', 'the', 'features', 'of', 'the', 'graphene', 'mono', 'and', 'multilayer', 'reflectance', 'in', 'the', 'farinfrared', 'region', 'as', 'a', 'function', 'of', 'frequency', 'temperature', 'and', 'carrier', 'density', 'taking', 'the', 'intraband', 'conductance', 'and', 'the', 'interband', 'electron', 'abso... | [-0.09880075084805574, 0.16230601405767703, -0.059389943658406365, 0.04222319909537361, -0.006116517937217636, -0.083962835767574, 0.08509926911143736, 0.40890177193729355, -0.24041085385171504, -0.2704226848583711, -0.02279932779961148, -0.31725421363766165, -0.12195983744258511, 0.17822402582942753, 0.048920315152085... |
707.1387 | Equisingularity classes of birational projections of normal
singularities to a plane | Given a birational normal extension S of a two-dimensional local regular ring
R, we describe all the equisingularity types of the complete ideals J in R
whose blowing-up has some point at which the local ring is analytically
isomorphic to S.
The problem of classifying the germs of such normal surface singularities ... | math.AG math.AC | given a birational normal extension s of a twodimensional local regular ring r we describe all the equisingularity types of the complete ideals j in r whose blowingup has some point at which the local ring is analytically isomorphic to s the problem of classifying the germs of such normal surface singularities was alre... | [['given', 'a', 'birational', 'normal', 'extension', 's', 'of', 'a', 'twodimensional', 'local', 'regular', 'ring', 'r', 'we', 'describe', 'all', 'the', 'equisingularity', 'types', 'of', 'the', 'complete', 'ideals', 'j', 'in', 'r', 'whose', 'blowingup', 'has', 'some', 'point', 'at', 'which', 'the', 'local', 'ring', 'is'... | [-0.16786886293516315, 0.0013814764849916852, -0.0842005639675666, 0.01793885918985582, -0.08524472672360564, -0.12109519951421806, -0.017055068459041943, 0.29787595099722497, -0.3475674979078273, -0.1971305543227554, 0.1249252010320285, -0.2553726403510687, -0.13961030504750935, 0.14775679368676262, -0.123535883634097... |
707.1388 | Three-Loop Chromomagnetic Interaction in HQET | We compute the three-loop QCD corrections to the quark chromomagnetic moment
and thus obtain the matching coefficient and the anomalous dimension of the
chromomagnetic interaction in HQET. As a byproduct we obtain the three-loop
corrections to the quark anomalous magnetic moment.
| hep-ph | we compute the threeloop qcd corrections to the quark chromomagnetic moment and thus obtain the matching coefficient and the anomalous dimension of the chromomagnetic interaction in hqet as a byproduct we obtain the threeloop corrections to the quark anomalous magnetic moment | [['we', 'compute', 'the', 'threeloop', 'qcd', 'corrections', 'to', 'the', 'quark', 'chromomagnetic', 'moment', 'and', 'thus', 'obtain', 'the', 'matching', 'coefficient', 'and', 'the', 'anomalous', 'dimension', 'of', 'the', 'chromomagnetic', 'interaction', 'in', 'hqet', 'as', 'a', 'byproduct', 'we', 'obtain', 'the', 'th... | [-0.09632424633132249, 0.24282832066642074, -0.06804855572196042, 0.19923758130838595, -0.10358414761494936, 0.01001305498250919, 0.0801543413644384, 0.2642013376987562, -0.15146802443011506, -0.26669931202763464, 0.008167373547444075, -0.33607065236968237, -0.06016950466011355, 0.05952597024180449, 0.1045372425010655,... |
707.1389 | The AS-Cohen-Macaulay property for quantum flag manifolds of minuscule
weight | It is shown that quantum homogeneous coordinate rings of generalised flag
manifolds corresponding to minuscule weights, their Schubert varieties, big
cells, and determinantal varieties are AS-Cohen-Macaulay. The main ingredient
in the proof is the notion of a quantum graded algebra with a straightening
law, introduce... | math.QA | it is shown that quantum homogeneous coordinate rings of generalised flag manifolds corresponding to minuscule weights their schubert varieties big cells and determinantal varieties are ascohenmacaulay the main ingredient in the proof is the notion of a quantum graded algebra with a straightening law introduced by th l... | [['it', 'is', 'shown', 'that', 'quantum', 'homogeneous', 'coordinate', 'rings', 'of', 'generalised', 'flag', 'manifolds', 'corresponding', 'to', 'minuscule', 'weights', 'their', 'schubert', 'varieties', 'big', 'cells', 'and', 'determinantal', 'varieties', 'are', 'ascohenmacaulay', 'the', 'main', 'ingredient', 'in', 'th... | [-0.15176902437815443, 0.08276688777320822, -0.06320763874789823, 0.05402980725078745, -0.1051745206166647, -0.20025084999782083, -0.0377059986686187, 0.2865486278100626, -0.3629330171740883, -0.1755479310001982, 0.09015493163927826, -0.21029078147349586, -0.19529676025635317, 0.18623620038852096, -0.20994931824603363,... |
707.139 | Probability Measures and Effective Randomness | We study the question, ``For which reals $x$ does there exist a measure $\mu$
such that $x$ is random relative to $\mu$?'' We show that for every
nonrecursive $x$, there is a measure which makes $x$ random without
concentrating on $x$. We give several conditions on $x$ equivalent to there
being continuous measure whi... | math.LO | we study the question for which reals x does there exist a measure mu such that x is random relative to mu we show that for every nonrecursive x there is a measure which makes x random without concentrating on x we give several conditions on x equivalent to there being continuous measure which makes x random we show th... | [['we', 'study', 'the', 'question', 'for', 'which', 'reals', 'x', 'does', 'there', 'exist', 'a', 'measure', 'mu', 'such', 'that', 'x', 'is', 'random', 'relative', 'to', 'mu', 'we', 'show', 'that', 'for', 'every', 'nonrecursive', 'x', 'there', 'is', 'a', 'measure', 'which', 'makes', 'x', 'random', 'without', 'concentrat... | [-0.15892924353004254, 0.13366539881967787, -0.08144549009000966, 0.053306230034595774, -0.04242581290318005, -0.16194080709785558, 0.0924709358377688, 0.4414949444567423, -0.2904326279800552, -0.16746294034867368, 0.08709678539585795, -0.27259596102217687, -0.1231799256543059, 0.21046016126203893, -0.10102357143021898... |
707.1391 | Tc oscillations in multilayered cuprates superconductors | When combining the BCS expression of Tc with a shear modulus constant model,
we can demonstrate that Tc oscillates depending on the number of the cuprate
planes and that it reaches its first maximum for three planes. This is in good
agreement with experimental data and suggests that the electron- phonon
coupling is e... | cond-mat.supr-con | when combining the bcs expression of tc with a shear modulus constant model we can demonstrate that tc oscillates depending on the number of the cuprate planes and that it reaches its first maximum for three planes this is in good agreement with experimental data and suggests that the electron phonon coupling is essent... | [['when', 'combining', 'the', 'bcs', 'expression', 'of', 'tc', 'with', 'a', 'shear', 'modulus', 'constant', 'model', 'we', 'can', 'demonstrate', 'that', 'tc', 'oscillates', 'depending', 'on', 'the', 'number', 'of', 'the', 'cuprate', 'planes', 'and', 'that', 'it', 'reaches', 'its', 'first', 'maximum', 'for', 'three', 'p... | [-0.18447656130883844, 0.16540520924221103, -0.05399264981970191, 0.0067242306210876755, -0.06194245840112368, -0.14613561790126064, 0.11560447349523505, 0.3525815381978949, -0.22414011353005966, -0.2643088056395451, 0.010358181066112592, -0.3537566738203168, -0.12028408051313212, 0.232924033945892, -0.0019415725449410... |
707.1392 | Doped Valence Bond Solid and Superconductivity on the Shastry-Sutherland
Lattice | Motivated by recent experiments on SrCu$_2$(BO$_3$)$_2$, we investigate the
ground states of the doped Mott insulator on the Shastry-Sutherland lattice. To
provide a unified theoretical framework for both the valence-bond solid state
found in undoped SrCu$_2$(BO$_3$)$_2$ and the doped counterpart being pursued
in on-... | cond-mat.str-el cond-mat.supr-con | motivated by recent experiments on srcu_2bo_3_2 we investigate the ground states of the doped mott insulator on the shastrysutherland lattice to provide a unified theoretical framework for both the valencebond solid state found in undoped srcu_2bo_3_2 and the doped counterpart being pursued in ongoing experiments we an... | [['motivated', 'by', 'recent', 'experiments', 'on', 'srcu_2bo_3_2', 'we', 'investigate', 'the', 'ground', 'states', 'of', 'the', 'doped', 'mott', 'insulator', 'on', 'the', 'shastrysutherland', 'lattice', 'to', 'provide', 'a', 'unified', 'theoretical', 'framework', 'for', 'both', 'the', 'valencebond', 'solid', 'state', ... | [-0.11338801643947458, 0.20740458891704316, -0.03196021182485288, 0.04798842173370692, -0.03176431397612139, -0.15952946714171004, 0.12871974898593092, 0.401906606673104, -0.21081420699157183, -0.23085851603323912, 0.06991035024147117, -0.3523935287986405, -0.14629631386729094, 0.14716489004573172, 0.05984670001013977,... |
707.1393 | Hidden nonlinear su(2|2) superunitary symmetry of N=2 superextended 1D
Dirac delta potential problem | We show that the N=2 superextended 1D quantum Dirac delta potential problem
is characterized by the hidden nonlinear $su(2|2)$ superunitary symmetry. The
unexpected feature of this simple supersymmetric system is that it admits three
different $\mathbb Z_2$-gradings, which produce a separation of 16 integrals of
moti... | hep-th | we show that the n2 superextended 1d quantum dirac delta potential problem is characterized by the hidden nonlinear su22 superunitary symmetry the unexpected feature of this simple supersymmetric system is that it admits three different mathbb z_2gradings which produce a separation of 16 integrals of motion into three ... | [['we', 'show', 'that', 'the', 'n2', 'superextended', '1d', 'quantum', 'dirac', 'delta', 'potential', 'problem', 'is', 'characterized', 'by', 'the', 'hidden', 'nonlinear', 'su22', 'superunitary', 'symmetry', 'the', 'unexpected', 'feature', 'of', 'this', 'simple', 'supersymmetric', 'system', 'is', 'that', 'it', 'admits'... | [-0.16682987924665213, 0.16213984044268728, -0.05580230864075323, 0.08166813150048256, -0.06676209021514902, -0.1672792783162246, -0.06355539545261611, 0.31708149845401445, -0.2740385208216806, -0.2607021501706913, 0.08238892305021485, -0.2808354455046356, -0.16372597333975136, 0.15956568640191107, -0.00538088650753100... |
707.1394 | Running anti-de Sitter radius from QCD-like strings | We consider renormalization effects for a bosonic QCD-like string, whose
partons have $1/p^{2}$ propagators instead of Gaussian. Classically this model
resembles (the bosonic part of) the projective light-cone (zero-radius) limit
of a string on an AdS${}_5$ background, where Schwinger parameters give rise to
the fift... | hep-th | we consider renormalization effects for a bosonic qcdlike string whose partons have 1p2 propagators instead of gaussian classically this model resembles the bosonic part of the projective lightcone zeroradius limit of a string on an ads_5 background where schwinger parameters give rise to the fifth dimension quantum ef... | [['we', 'consider', 'renormalization', 'effects', 'for', 'a', 'bosonic', 'qcdlike', 'string', 'whose', 'partons', 'have', '1p2', 'propagators', 'instead', 'of', 'gaussian', 'classically', 'this', 'model', 'resembles', 'the', 'bosonic', 'part', 'of', 'the', 'projective', 'lightcone', 'zeroradius', 'limit', 'of', 'a', 's... | [-0.1497566446260963, 0.24942107768058325, -0.12681980384513736, 0.12550750405838093, -0.07982117495784122, -0.12965521110971975, -0.035656328256461874, 0.29179508875434595, -0.17226459522640247, -0.13782971090525584, 0.028602124088340335, -0.28302340204310084, -0.06573598552495241, 0.12252288220851268, -0.020949527065... |
707.1395 | Continuous first-passage percolation and continuous greedy paths model:
linear growth | We study a random growth model on $\R^d$ introduced by Deijfen. This is a
continuous first-passage percolation model. The growth occurs by means of
spherical outbursts with random radii in the infected region. We aim at finding
conditions on the distribution of the random radii to determine whether the
growth of the ... | math.PR | we study a random growth model on rd introduced by deijfen this is a continuous firstpassage percolation model the growth occurs by means of spherical outbursts with random radii in the infected region we aim at finding conditions on the distribution of the random radii to determine whether the growth of the process is... | [['we', 'study', 'a', 'random', 'growth', 'model', 'on', 'rd', 'introduced', 'by', 'deijfen', 'this', 'is', 'a', 'continuous', 'firstpassage', 'percolation', 'model', 'the', 'growth', 'occurs', 'by', 'means', 'of', 'spherical', 'outbursts', 'with', 'random', 'radii', 'in', 'the', 'infected', 'region', 'we', 'aim', 'at'... | [-0.07506137451547308, 0.15001420109697125, -0.07174180832636708, 0.034555269858002946, -0.03405837356112897, -0.09794644356760032, 0.08335079412688227, 0.40538265716613214, -0.26664145251407345, -0.2040371947647894, 0.12887143909328563, -0.2792433286414427, -0.16446480943054398, 0.11844455634709447, -0.061329935346935... |
707.1396 | Induced cosmology on a regularized brane in six-dimensional flux
compactification | We consider a six-dimensional Einstein-Maxwell system compactified in an
axisymmetric two-dimensional space with one capped regularized conical brane of
codimension one. We study the cosmological evolution which is induced on the
regularized brane as it moves in between known static bulk and cap solutions.
Looking at... | hep-th gr-qc | we consider a sixdimensional einsteinmaxwell system compactified in an axisymmetric twodimensional space with one capped regularized conical brane of codimension one we study the cosmological evolution which is induced on the regularized brane as it moves in between known static bulk and cap solutions looking at the re... | [['we', 'consider', 'a', 'sixdimensional', 'einsteinmaxwell', 'system', 'compactified', 'in', 'an', 'axisymmetric', 'twodimensional', 'space', 'with', 'one', 'capped', 'regularized', 'conical', 'brane', 'of', 'codimension', 'one', 'we', 'study', 'the', 'cosmological', 'evolution', 'which', 'is', 'induced', 'on', 'the',... | [-0.14285497756448584, 0.10949731977326277, -0.05905069453015088, 0.08845548601233548, -0.0801095635016562, -0.16886595998690507, -0.04491350353721564, 0.2930004187689868, -0.2381362395500329, -0.2813444354562698, 0.06912618197901087, -0.3135830997271794, -0.09090305189602077, 0.10866868948981723, -0.024591811300499068... |
707.1397 | Mid-infrared diagnostics of starburst galaxies: clumpy, dense structures
in star-forming regions in the Antennae (NGC 4038/4039) | Recently, mid-infrared instruments have become available on several large
ground-based telescopes, resulting in data sets with unprecedented spatial
resolution at these long wavelengths. In this paper we examine
'ground-based-only' diagnostics, which can be used in the study of star-forming
regions in starburst galax... | astro-ph | recently midinfrared instruments have become available on several large groundbased telescopes resulting in data sets with unprecedented spatial resolution at these long wavelengths in this paper we examine groundbasedonly diagnostics which can be used in the study of starforming regions in starburst galaxies by combin... | [['recently', 'midinfrared', 'instruments', 'have', 'become', 'available', 'on', 'several', 'large', 'groundbased', 'telescopes', 'resulting', 'in', 'data', 'sets', 'with', 'unprecedented', 'spatial', 'resolution', 'at', 'these', 'long', 'wavelengths', 'in', 'this', 'paper', 'we', 'examine', 'groundbasedonly', 'diagnos... | [-0.021207382766597345, 0.13110117086449563, -0.046243215255793266, 0.10524572760585224, -0.0431280522512449, -0.05879284635531754, 0.008382073286983998, 0.500698805192477, -0.13502007176703457, -0.3768326414841737, 0.06681224615713455, -0.28587167729450835, -0.003038639218516951, 0.18351095325494715, -0.00409660371490... |
707.1398 | Experimental studies of liquid-liquid dispersion in a turbulent shear
flow | We study liquid-liquid dispersions in a turbulent Taylor - Couette flow,
produced between two counterrotating coaxial cylinders. In pure Water and in
counterrotation, Reynolds numbers up to 1.4 10^5 are reached. We first
characterize the single-phase flow, in terms of threshold for transition to
turbulence, scaling o... | physics.flu-dyn | we study liquidliquid dispersions in a turbulent taylor couette flow produced between two counterrotating coaxial cylinders in pure water and in counterrotation reynolds numbers up to 14 105 are reached we first characterize the singlephase flow in terms of threshold for transition to turbulence scaling of the torque a... | [['we', 'study', 'liquidliquid', 'dispersions', 'in', 'a', 'turbulent', 'taylor', 'couette', 'flow', 'produced', 'between', 'two', 'counterrotating', 'coaxial', 'cylinders', 'in', 'pure', 'water', 'and', 'in', 'counterrotation', 'reynolds', 'numbers', 'up', 'to', '14', '105', 'are', 'reached', 'we', 'first', 'character... | [-0.20265028636398105, 0.21067360900148438, -0.06824132078327239, -0.02907990600215271, 0.005452892558726792, -0.05257571326122464, -0.027870303058686357, 0.3210063365210469, -0.2769450989289908, -0.3391520449561843, 0.06150283841391987, -0.27769723658760387, -0.06285514661188547, 0.2228599456915011, -0.018787627933003... |
707.1399 | Detection of SiO emission from a massive dense cold core | We report the detection of the SiO (J = 2 - 1) transition from the massive
cold dense core G333.125-0.562. The core remains undetected at wavelengths
shorter than 70 micron and has compact 1.2 mm dust continuum. The SiO emission
is localised to the core. The observations are part of a continuing
multi-molecular line ... | astro-ph | we report the detection of the sio j 2 1 transition from the massive cold dense core g3331250562 the core remains undetected at wavelengths shorter than 70 micron and has compact 12 mm dust continuum the sio emission is localised to the core the observations are part of a continuing multimolecular line survey of the gi... | [['we', 'report', 'the', 'detection', 'of', 'the', 'sio', 'j', '2', '1', 'transition', 'from', 'the', 'massive', 'cold', 'dense', 'core', 'g3331250562', 'the', 'core', 'remains', 'undetected', 'at', 'wavelengths', 'shorter', 'than', '70', 'micron', 'and', 'has', 'compact', '12', 'mm', 'dust', 'continuum', 'the', 'sio',... | [-0.052315663515632466, 0.10698099601528763, 0.05160728848511071, 0.005551753422442937, -0.019189818259893042, -0.06655289798579885, 0.06161172145300291, 0.4743712951288079, -0.13866622337055476, -0.29564670617833283, 0.0747454683945486, -0.25973033832781245, 0.018982189509904747, 0.057168073523225206, 0.05707315837145... |
707.14 | Lower bounds for sup + inf and sup * inf and an Extension of Chen-Lin
result in dimension 3 | We give two results about Harnack type inequalities. First, on compact smooth
Riemannian surface without boundary, we have an estimate of the type $\sup
+\inf$. The second result concerns the solutions of prescribed scalar curvature
equation on the unit ball of ${\mathbb R}^n$ with Dirichlet condition. Next, we
give ... | math.AP | we give two results about harnack type inequalities first on compact smooth riemannian surface without boundary we have an estimate of the type sup inf the second result concerns the solutions of prescribed scalar curvature equation on the unit ball of mathbb rn with dirichlet condition next we give an inequality of th... | [['we', 'give', 'two', 'results', 'about', 'harnack', 'type', 'inequalities', 'first', 'on', 'compact', 'smooth', 'riemannian', 'surface', 'without', 'boundary', 'we', 'have', 'an', 'estimate', 'of', 'the', 'type', 'sup', 'inf', 'the', 'second', 'result', 'concerns', 'the', 'solutions', 'of', 'prescribed', 'scalar', 'c... | [-0.22132390703773125, 0.03858753998811153, -0.05484880946605699, 0.009319658952153986, -0.08640947355270327, -0.15679927715100347, -0.06917447731539142, 0.2212093098758487, -0.22021219327725702, -0.20645533756614895, 0.1317056971944112, -0.35890425702673384, -0.09007416128988552, 0.193502940156759, -0.1537655722582712... |
707.1401 | Complete Two-Loop Corrections to H -> gamma gamma | In this paper the complete two-loop corrections to the Higgs-boson decay, H
-> gamma gamma, are presented. The evaluations of both QCD and electroweak
corrections are based on a numerical approach. The results cover all
kinematical regions, including the WW normal-threshold, by introducing complex
masses in the relev... | hep-ph | in this paper the complete twoloop corrections to the higgsboson decay h gamma gamma are presented the evaluations of both qcd and electroweak corrections are based on a numerical approach the results cover all kinematical regions including the ww normalthreshold by introducing complex masses in the relevant gaugeinvar... | [['in', 'this', 'paper', 'the', 'complete', 'twoloop', 'corrections', 'to', 'the', 'higgsboson', 'decay', 'h', 'gamma', 'gamma', 'are', 'presented', 'the', 'evaluations', 'of', 'both', 'qcd', 'and', 'electroweak', 'corrections', 'are', 'based', 'on', 'a', 'numerical', 'approach', 'the', 'results', 'cover', 'all', 'kine... | [-0.07578355699122229, 0.190903708519828, -0.07235437557446184, 0.1193391686904727, -0.04423164066651629, -0.03352302032591844, 0.024829927411499537, 0.34504990583216705, -0.1350709646595297, -0.22455482291816561, 0.028079407651805215, -0.3140014248934609, -0.05978538668541997, 0.1773635191084058, 0.06908888818213234, ... |
707.1402 | Construction and test of a moving boundary model for negative streamer
discharges | Starting from the minimal model for the electrically interacting particle
densities in negative streamer discharges, we derive a moving boundary
approximation for the ionization fronts. The boundary condition on the moving
front is found to be of 'kinetic undercooling' type. The boundary
approximation, whose first re... | physics.plasm-ph physics.flu-dyn | starting from the minimal model for the electrically interacting particle densities in negative streamer discharges we derive a moving boundary approximation for the ionization fronts the boundary condition on the moving front is found to be of kinetic undercooling type the boundary approximation whose first results ha... | [['starting', 'from', 'the', 'minimal', 'model', 'for', 'the', 'electrically', 'interacting', 'particle', 'densities', 'in', 'negative', 'streamer', 'discharges', 'we', 'derive', 'a', 'moving', 'boundary', 'approximation', 'for', 'the', 'ionization', 'fronts', 'the', 'boundary', 'condition', 'on', 'the', 'moving', 'fro... | [-0.09364753293736679, 0.1342816637579079, -0.0973153895494051, 0.024398988944750916, -0.024746432130951887, -0.13624241646583668, 0.0082765747895947, 0.329811140332689, -0.1673684033264247, -0.31310078422198206, 0.06827732199386313, -0.2651556830671502, -0.12144003360441363, 0.15336614012826097, -0.010579023544290444,... |
707.1403 | Accretion of Low Angular Momentum Material onto Black Holes: Radiation
Properties of Axisymmetric MHD Flows | Numerical simulations of MHD accretion flows in the vicinity of a
supermasssive black hole provide important insights to the problem of why and
how systems -- such as the Galactic Center -- are underluminous and variable.
To access applicability of such flows to real objects, we examine the dynamical
MHD studies with... | astro-ph | numerical simulations of mhd accretion flows in the vicinity of a supermasssive black hole provide important insights to the problem of why and how systems such as the galactic center are underluminous and variable to access applicability of such flows to real objects we examine the dynamical mhd studies with computati... | [['numerical', 'simulations', 'of', 'mhd', 'accretion', 'flows', 'in', 'the', 'vicinity', 'of', 'a', 'supermasssive', 'black', 'hole', 'provide', 'important', 'insights', 'to', 'the', 'problem', 'of', 'why', 'and', 'how', 'systems', 'such', 'as', 'the', 'galactic', 'center', 'are', 'underluminous', 'and', 'variable', '... | [-0.09167128710466768, 0.07811076432253392, -0.08154765024946461, 0.11610238593270732, -0.03535043313017776, -0.08062518933776676, 0.005139768979842624, 0.37647091344960276, -0.23420505746898632, -0.31445878712956105, 0.1048924550151212, -0.30232728775140016, -0.09330775796796285, 0.2426965711225245, -0.008016936173061... |
707.1404 | Corings with exact rational functors and injective objects | We describe how some aspects of abstract localization on module categories
have applications to the study of injective comodules over some special types
of corings. We specialize the general results to the case of Doi-Koppinen
modules, generalizing previous results in this setting.
| math.RA | we describe how some aspects of abstract localization on module categories have applications to the study of injective comodules over some special types of corings we specialize the general results to the case of doikoppinen modules generalizing previous results in this setting | [['we', 'describe', 'how', 'some', 'aspects', 'of', 'abstract', 'localization', 'on', 'module', 'categories', 'have', 'applications', 'to', 'the', 'study', 'of', 'injective', 'comodules', 'over', 'some', 'special', 'types', 'of', 'corings', 'we', 'specialize', 'the', 'general', 'results', 'to', 'the', 'case', 'of', 'do... | [-0.09655496348604196, -0.030078760825279282, -0.03397129650977326, 0.08230145973800795, -0.0823809887486987, -0.11366395611406827, -0.05685155234504037, 0.4071646707087028, -0.31247755035576297, -0.18079637354466974, 0.11623753560423034, -0.20193750460535606, -0.21685009702994693, 0.25717364478765464, -0.2212320962784... |
707.1405 | Symmetries of Electrostatic Interaction between DNA Molecules | We study a model for pair interaction $U$ of DNA molecules generated by the
discrete dipole moments of base-pairs and the charges of phosphate groups, and
find noncommutative group of eighth order ${\cal S}$ of symmetries that leave
$U$ invariant. We classify the minima using group ${\cal S}$ and employ
numerical met... | cond-mat.soft | we study a model for pair interaction u of dna molecules generated by the discrete dipole moments of basepairs and the charges of phosphate groups and find noncommutative group of eighth order cal s of symmetries that leave u invariant we classify the minima using group cal s and employ numerical methods for finding th... | [['we', 'study', 'a', 'model', 'for', 'pair', 'interaction', 'u', 'of', 'dna', 'molecules', 'generated', 'by', 'the', 'discrete', 'dipole', 'moments', 'of', 'basepairs', 'and', 'the', 'charges', 'of', 'phosphate', 'groups', 'and', 'find', 'noncommutative', 'group', 'of', 'eighth', 'order', 'cal', 's', 'of', 'symmetries... | [-0.171896509119435, 0.22110293438447168, -0.04541196890096081, 0.021952665992186846, 0.007766160379157316, -0.15300643827488764, 0.08253023013842443, 0.3943029792834047, -0.2819033397513554, -0.2904028079822554, 0.03364040868370034, -0.3150549393282635, -0.11860282462361064, 0.11419040519836629, 0.015491744100466266, ... |
707.1406 | Uniqueness at infinity in time for the Maxwell-Schr"odinger system with
arbitrarily large asymptotic data | We prove the uniqueness of solutions of the Maxwell-Schr"odinger system with
given asymptotic behaviour at infinity in time. The assumptions include
suitable restrictions on the growth of solutions for large time and on the
accuracy of their asymptotics, but no restriction on their size. The result
applies to the sol... | math.AP | we prove the uniqueness of solutions of the maxwellschrodinger system with given asymptotic behaviour at infinity in time the assumptions include suitable restrictions on the growth of solutions for large time and on the accuracy of their asymptotics but no restriction on their size the result applies to the solutions ... | [['we', 'prove', 'the', 'uniqueness', 'of', 'solutions', 'of', 'the', 'maxwellschrodinger', 'system', 'with', 'given', 'asymptotic', 'behaviour', 'at', 'infinity', 'in', 'time', 'the', 'assumptions', 'include', 'suitable', 'restrictions', 'on', 'the', 'growth', 'of', 'solutions', 'for', 'large', 'time', 'and', 'on', 't... | [-0.14720963527336076, 0.015021725702260074, -0.10266471651768119, 0.037058121974355186, -0.0487832328111961, -0.08342138290052013, 0.05403800372331371, 0.28890082386225974, -0.21024669931623444, -0.2753864247351885, 0.19101670670628162, -0.2798566849067293, -0.07418799053492217, 0.18601815840871683, -0.064428448612833... |
707.1407 | Reliability of genetic networks is evolvable | Control of the living cell functions with remarkable reliability despite the
stochastic nature of the underlying molecular networks -- a property presumably
optimized by biological evolution. We here ask to what extent the property of a
stochastic dynamical network to produce reliable dynamics is an evolvable
trait. ... | q-bio.MN | control of the living cell functions with remarkable reliability despite the stochastic nature of the underlying molecular networks a property presumably optimized by biological evolution we here ask to what extent the property of a stochastic dynamical network to produce reliable dynamics is an evolvable trait using a... | [['control', 'of', 'the', 'living', 'cell', 'functions', 'with', 'remarkable', 'reliability', 'despite', 'the', 'stochastic', 'nature', 'of', 'the', 'underlying', 'molecular', 'networks', 'a', 'property', 'presumably', 'optimized', 'by', 'biological', 'evolution', 'we', 'here', 'ask', 'to', 'what', 'extent', 'the', 'pr... | [-0.14665225548649966, 0.08267037177648813, -0.09305169403363588, 0.08620095806160816, -0.04931444166449167, -0.13975691966519108, 0.09881336903554719, 0.3931411036558576, -0.3131475115857892, -0.28515729974260773, 0.09145623251748414, -0.1892373195683615, -0.2380463731972406, 0.14645372095944012, -0.07210657007196414,... |
707.1408 | Module Shifts and Measure Rigidity in Linear Cellular Automata | Suppose R is a finite commutative ring of prime characteristic, A is a finite
R-module, M:=Z^D x N^E, and F is an R-linear cellular automaton on A^M. If mu
is an F-invariant measure which is multiply shift-mixing in a certain way, then
we show that mu must be the Haar measure on a coset of some submodule shift of
A^M... | math.DS | suppose r is a finite commutative ring of prime characteristic a is a finite rmodule mzd x ne and f is an rlinear cellular automaton on am if mu is an finvariant measure which is multiply shiftmixing in a certain way then we show that mu must be the haar measure on a coset of some submodule shift of am under certain co... | [['suppose', 'r', 'is', 'a', 'finite', 'commutative', 'ring', 'of', 'prime', 'characteristic', 'a', 'is', 'a', 'finite', 'rmodule', 'mzd', 'x', 'ne', 'and', 'f', 'is', 'an', 'rlinear', 'cellular', 'automaton', 'on', 'am', 'if', 'mu', 'is', 'an', 'finvariant', 'measure', 'which', 'is', 'multiply', 'shiftmixing', 'in', '... | [-0.19899668270157497, 0.1827453649064609, -0.12252256927424915, 0.019664405256650117, -0.06703559606182963, -0.19526438843076155, 0.00980402516481811, 0.3897787193474296, -0.3560544972193159, -0.08927037331199095, 0.10059208650786225, -0.2350686132040334, -0.0934120991254506, 0.1501088102973283, -0.17176842925534264, ... |
707.1409 | Poisson-Vlasov : Stochastic representation and numerical codes | A stochastic representation for the solutions of the Poisson-Vlasov equation,
with several charged species, is obtained. The representation involves both an
exponential and a branching process and it provides an intuitive
characterization of the nature of the solutions and its fluctuations. Here, the
stochastic repre... | physics.plasm-ph | a stochastic representation for the solutions of the poissonvlasov equation with several charged species is obtained the representation involves both an exponential and a branching process and it provides an intuitive characterization of the nature of the solutions and its fluctuations here the stochastic representatio... | [['a', 'stochastic', 'representation', 'for', 'the', 'solutions', 'of', 'the', 'poissonvlasov', 'equation', 'with', 'several', 'charged', 'species', 'is', 'obtained', 'the', 'representation', 'involves', 'both', 'an', 'exponential', 'and', 'a', 'branching', 'process', 'and', 'it', 'provides', 'an', 'intuitive', 'charac... | [-0.09619371434934598, 0.04563621835078611, -0.14316831179091644, 0.05892101107762975, -0.05483246469420606, -0.07208044107618003, 0.016491873125577795, 0.2832846075681777, -0.2646742610196615, -0.2578991076684204, 0.13476910710270548, -0.2891826304398349, -0.1838396267066228, 0.21128314036217616, 0.014938006691377738,... |
707.141 | The quadratic speedup in Grover's search algorithm from the entanglement
perspective | We analyze the role played by entanglement in the dynamical evolution of
Grover's search algorithm in the space of qubits. We show that the algorithm
can be equivalently described as an iterative change of the entanglement
between the qubits, which governs the evolution of the initial state towards
the target state, ... | quant-ph | we analyze the role played by entanglement in the dynamical evolution of grovers search algorithm in the space of qubits we show that the algorithm can be equivalently described as an iterative change of the entanglement between the qubits which governs the evolution of the initial state towards the target state and wh... | [['we', 'analyze', 'the', 'role', 'played', 'by', 'entanglement', 'in', 'the', 'dynamical', 'evolution', 'of', 'grovers', 'search', 'algorithm', 'in', 'the', 'space', 'of', 'qubits', 'we', 'show', 'that', 'the', 'algorithm', 'can', 'be', 'equivalently', 'described', 'as', 'an', 'iterative', 'change', 'of', 'the', 'enta... | [-0.1156319705074683, 0.14020643264607754, -0.13248513022347563, 0.05891979915360289, 0.005373750084770783, -0.14752577452248172, 0.08723236169222923, 0.32989074021667963, -0.2863773649197913, -0.32403036071017627, 0.07713670105271551, -0.22042173317893157, -0.13505599243686564, 0.16005696458629362, -0.0224118041875895... |
707.1411 | Constructing Simplicial Branched Covers | Branched covers are applied frequently in topology - most prominently in the
construction of closed oriented PL d-manifolds. In particular, strong bounds
for the number of sheets and the topology of the branching set are known for
dimension d<=4. On the other hand, Izmestiev and Joswig described how to obtain
a simpl... | math.CO math.GT | branched covers are applied frequently in topology most prominently in the construction of closed oriented pl dmanifolds in particular strong bounds for the number of sheets and the topology of the branching set are known for dimension d4 on the other hand izmestiev and joswig described how to obtain a simplicial cover... | [['branched', 'covers', 'are', 'applied', 'frequently', 'in', 'topology', 'most', 'prominently', 'in', 'the', 'construction', 'of', 'closed', 'oriented', 'pl', 'dmanifolds', 'in', 'particular', 'strong', 'bounds', 'for', 'the', 'number', 'of', 'sheets', 'and', 'the', 'topology', 'of', 'the', 'branching', 'set', 'are', ... | [-0.14759485089294702, 0.09162887786198588, -0.018602501799904025, 0.07909288179486519, -0.09273811689243444, -0.11307856925193546, -0.002081719973097438, 0.33377983410236906, -0.2961807457551595, -0.2537295693911395, 0.11943885282323995, -0.24755705760122793, -0.18631229870636196, 0.22147623021878954, -0.1323927792096... |
707.1412 | On natural and conformally equivariant quantizations | The concept of conformally equivariant quantizations was introduced by Duval,
Lecomte and Ovsienko in \cite{DLO} for manifolds endowed with flat conformal
structures. They obtained results of existence and uniqueness (up to
normalization) of such a quantization procedure. A natural generalization of
this concept is t... | math.DG | the concept of conformally equivariant quantizations was introduced by duval lecomte and ovsienko in citedlo for manifolds endowed with flat conformal structures they obtained results of existence and uniqueness up to normalization of such a quantization procedure a natural generalization of this concept is to seek for... | [['the', 'concept', 'of', 'conformally', 'equivariant', 'quantizations', 'was', 'introduced', 'by', 'duval', 'lecomte', 'and', 'ovsienko', 'in', 'citedlo', 'for', 'manifolds', 'endowed', 'with', 'flat', 'conformal', 'structures', 'they', 'obtained', 'results', 'of', 'existence', 'and', 'uniqueness', 'up', 'to', 'normal... | [-0.13431880567700435, 0.09094702162994789, -0.08179392493688144, 0.055169717120364885, -0.08035196053007475, -0.14862000002072026, -0.017100642880168146, 0.35591065743221684, -0.26047543617896735, -0.27566345057133823, 0.08144222438239898, -0.24002517910721974, -0.2021071362762879, 0.17120154895700324, -0.162231724491... |
707.1413 | Minimizing the linewidth of the Flux-Flow Oscillator | For the first time the linewidth of Flux-Flow Oscillator has been calculated
by direct computer simulation of the sine-Gordon equation with noise. Nearly
perfect agreement of the numerical results with the formula derived in [Phys.
Rev. B, {\bf 65}, 054504 (2002)] has been achieved. It has been demonstrated
that for ... | cond-mat.supr-con cond-mat.stat-mech | for the first time the linewidth of fluxflow oscillator has been calculated by direct computer simulation of the sinegordon equation with noise nearly perfect agreement of the numerical results with the formula derived in phys rev b bf 65 054504 2002 has been achieved it has been demonstrated that for homogeneous bias ... | [['for', 'the', 'first', 'time', 'the', 'linewidth', 'of', 'fluxflow', 'oscillator', 'has', 'been', 'calculated', 'by', 'direct', 'computer', 'simulation', 'of', 'the', 'sinegordon', 'equation', 'with', 'noise', 'nearly', 'perfect', 'agreement', 'of', 'the', 'numerical', 'results', 'with', 'the', 'formula', 'derived', ... | [-0.12968395607955058, 0.10982126802658644, -0.038577441430746394, -0.04141982189144626, -0.061174198567310226, -0.1204275114561875, 0.038775681084996766, 0.4178116055832149, -0.19711289985897454, -0.32742043177240365, 0.05265939960508634, -0.22125507003375303, -0.06608138865982748, 0.28475012289029417, -0.042768870132... |
707.1414 | Experimental studies of turbulent Taylor-Couette flows: single phase and
liquid-liquid dispersions | We study liquid-liquid dispersions in a turbulent Taylor-Couette flow,
produced between two counterrotating coaxial cylinders. In pure Water and in
counterrotation, Reynolds numbers up to 1.4 10^5 are reached. The liquids we
use are a low-viscous Oil and pure Water or a Sodium Iodide solution with a
refractive index ... | physics.flu-dyn | we study liquidliquid dispersions in a turbulent taylorcouette flow produced between two counterrotating coaxial cylinders in pure water and in counterrotation reynolds numbers up to 14 105 are reached the liquids we use are a lowviscous oil and pure water or a sodium iodide solution with a refractive index matched to ... | [['we', 'study', 'liquidliquid', 'dispersions', 'in', 'a', 'turbulent', 'taylorcouette', 'flow', 'produced', 'between', 'two', 'counterrotating', 'coaxial', 'cylinders', 'in', 'pure', 'water', 'and', 'in', 'counterrotation', 'reynolds', 'numbers', 'up', 'to', '14', '105', 'are', 'reached', 'the', 'liquids', 'we', 'use'... | [-0.1596765223047918, 0.20729621680128196, -0.07248339182623321, -0.029380580521233025, -0.0008899083227983543, -0.07641063652154693, -0.011813030230797945, 0.3589955810457468, -0.2491225260420747, -0.3334130839267302, 0.08837856971547894, -0.3024923529712454, -0.07031603607844325, 0.19766521911942475, -0.0292610806849... |
707.1415 | Constructing Combinatorial 4-Manifolds | Every closed oriented PL 4-manifold is a branched cover of the 4-sphere
branched over a PL-surface with finitely many singularities by Piergallini
[Topology 34(3):497-508, 1995]. This generalizes a long standing result by
Hilden and Montesinos to dimension four. Izmestiev and Joswig [Adv. Geom.
3(2):191-225, 2003] ga... | math.CO math.GT | every closed oriented pl 4manifold is a branched cover of the 4sphere branched over a plsurface with finitely many singularities by piergallini topology 343497508 1995 this generalizes a long standing result by hilden and montesinos to dimension four izmestiev and joswig adv geom 32191225 2003 gave a combinatorial equi... | [['every', 'closed', 'oriented', 'pl', '4manifold', 'is', 'a', 'branched', 'cover', 'of', 'the', '4sphere', 'branched', 'over', 'a', 'plsurface', 'with', 'finitely', 'many', 'singularities', 'by', 'piergallini', 'topology', '343497508', '1995', 'this', 'generalizes', 'a', 'long', 'standing', 'result', 'by', 'hilden', '... | [-0.21291235421917268, 0.06543994473887015, -0.08486180306299702, 0.09240808776595148, -0.13207583341767992, -0.1900554126804019, -0.008328362756951169, 0.31450179444400816, -0.3093815504286725, -0.30340334761294196, 0.07680460605975035, -0.22398752976045178, -0.18836805612682928, 0.20559973007702564, -0.27249222146449... |
707.1416 | The Impact of Ultraviolet Regularization on the Spectrum of Curvature
Perturbations During Inflation | Inflationary predictions based on the linear theory of cosmological
perturbations are related to the two point function of a (second quantized)
real scalar free field during the accelerated stage. Such a two point function
is finite, in contrast with its coincidence limit, which is divergent due to
the ultraviolet di... | hep-th astro-ph | inflationary predictions based on the linear theory of cosmological perturbations are related to the two point function of a second quantized real scalar free field during the accelerated stage such a two point function is finite in contrast with its coincidence limit which is divergent due to the ultraviolet divergenc... | [['inflationary', 'predictions', 'based', 'on', 'the', 'linear', 'theory', 'of', 'cosmological', 'perturbations', 'are', 'related', 'to', 'the', 'two', 'point', 'function', 'of', 'a', 'second', 'quantized', 'real', 'scalar', 'free', 'field', 'during', 'the', 'accelerated', 'stage', 'such', 'a', 'two', 'point', 'functio... | [-0.11187511304054748, 0.13360184231265024, -0.13405185574242337, 0.09532864653526552, -0.1052006053992293, -0.12385693449865688, -0.015152496643449096, 0.3393751666881144, -0.2570732817530039, -0.25736324343491684, 0.10738279140258039, -0.2694868017919362, -0.1582412283888764, 0.13545950613175095, -0.03935674099484458... |
707.1417 | Characteristic Functions of Liftings | We introduce characteristic functions for certain contractive liftings of row
contractions. These are multi-analytic operators which classify the liftings up
to unitary equivalence and provide a kind of functional model. The most
important cases are subisometric and coisometric liftings. We also identify the
most gen... | math.OA | we introduce characteristic functions for certain contractive liftings of row contractions these are multianalytic operators which classify the liftings up to unitary equivalence and provide a kind of functional model the most important cases are subisometric and coisometric liftings we also identify the most general s... | [['we', 'introduce', 'characteristic', 'functions', 'for', 'certain', 'contractive', 'liftings', 'of', 'row', 'contractions', 'these', 'are', 'multianalytic', 'operators', 'which', 'classify', 'the', 'liftings', 'up', 'to', 'unitary', 'equivalence', 'and', 'provide', 'a', 'kind', 'of', 'functional', 'model', 'the', 'mo... | [-0.11591205536844391, 0.09410736617043286, -0.04736999946865527, 0.11172220451465133, -0.05962186209473978, -0.17070028268476473, 0.044618915600985215, 0.3573647517455267, -0.3762639669071445, -0.1592285978589572, 0.11032138034865699, -0.2706908592771666, -0.2250320205565396, 0.16410713253871484, -0.09618647455228675,... |
707.1418 | On the transformation semitopological semigroup | In this paper we introduce the notion of weighted (weakly) almost periodic
compactifcation of a semitopological semigroup and generalize this notion to
corresponding notion for transformation semigroup.The inclusion relation and
equality of some well known function spaces on a weighted transformation
semigroup is als... | math.FA | in this paper we introduce the notion of weighted weakly almost periodic compactifcation of a semitopological semigroup and generalize this notion to corresponding notion for transformation semigroupthe inclusion relation and equality of some well known function spaces on a weighted transformation semigroup is also inv... | [['in', 'this', 'paper', 'we', 'introduce', 'the', 'notion', 'of', 'weighted', 'weakly', 'almost', 'periodic', 'compactifcation', 'of', 'a', 'semitopological', 'semigroup', 'and', 'generalize', 'this', 'notion', 'to', 'corresponding', 'notion', 'for', 'transformation', 'semigroupthe', 'inclusion', 'relation', 'and', 'e... | [-0.10429432875541754, 0.12996131399115765, -0.05460196153022522, 0.15874405507117423, -0.11411507790475044, -0.062266137840789416, 0.043094234473375216, 0.3766834980180097, -0.4181289894636287, -0.198318826944329, 0.11293237244569544, -0.2960433050297027, -0.2160654740278111, 0.17835315932021584, -0.14657524639610633,... |
707.1419 | Unparticle as a field with continuously distributed mass | We point out that the notion of an unparticle, recently introduced by Georgi,
can be interpreted as a particular case of a field with continuously
distributed mass considered in ref.\cite{14}. We also point out that the
simplest renormalizable extension of the $SU_c(3)\otimes SU_L(2)\otimes U(1)$
Standard Model is th... | hep-ph | we point out that the notion of an unparticle recently introduced by georgi can be interpreted as a particular case of a field with continuously distributed mass considered in refcite14 we also point out that the simplest renormalizable extension of the su_c3otimes su_l2otimes u1 standard model is the extension with th... | [['we', 'point', 'out', 'that', 'the', 'notion', 'of', 'an', 'unparticle', 'recently', 'introduced', 'by', 'georgi', 'can', 'be', 'interpreted', 'as', 'a', 'particular', 'case', 'of', 'a', 'field', 'with', 'continuously', 'distributed', 'mass', 'considered', 'in', 'refcite14', 'we', 'also', 'point', 'out', 'that', 'the... | [-0.10800929179750994, 0.16042864948084584, -0.08649824884124711, 0.07027191281906467, -0.06026101387945599, -0.1465276295594016, 0.022455866769200465, 0.31533926187968647, -0.21958727104070244, -0.22825149428404745, 0.06102917313415435, -0.25145853164254645, -0.156886133441671, 0.10196145818965724, -0.0496159638278186... |
707.142 | Parastrophic invariance of Smarandache quasigroups | Every quasigroup $(L,\cdot)$ belongs to a set of 6 quasigroups, called
parastrophes denoted by $(L,\pi_i)$, $i\in \{1,2,3,4,5,6\}$. It is shown that
$(L,\pi_i)$ is a Smarandache quasigroup with associative subquasigroup
$(S,\pi_i) \forall i\in \{1,2,3,4,5,6\}$ if and only if for any of some four
$j\in \{1,2,3,4,5,6\}... | math.GM | every quasigroup lcdot belongs to a set of 6 quasigroups called parastrophes denoted by lpi_i iin 123456 it is shown that lpi_i is a smarandache quasigroup with associative subquasigroup spi_i forall iin 123456 if and only if for any of some four jin 123456 spi_j is an isotope of spi_i or spi_k for one kin 123456 such ... | [['every', 'quasigroup', 'lcdot', 'belongs', 'to', 'a', 'set', 'of', '6', 'quasigroups', 'called', 'parastrophes', 'denoted', 'by', 'lpi_i', 'iin', '123456', 'it', 'is', 'shown', 'that', 'lpi_i', 'is', 'a', 'smarandache', 'quasigroup', 'with', 'associative', 'subquasigroup', 'spi_i', 'forall', 'iin', '123456', 'if', 'a... | [-0.168390021896145, 0.17176061930383893, 0.018636738115714657, 0.031749719662022675, -0.0968069789543127, -0.2952194595968144, -0.01752088296537598, 0.39400232169363236, -0.26512734598169724, -0.07651262891789277, 0.1178544244159841, -0.3727156903180811, -0.12093948612455278, 0.1566132522265737, -0.11439651054744092, ... |
707.1421 | Consequences of U dualities for Intersecting Branes in the Universe | We consider N -- charge, intersecting brane antibrane configurations in M
theory which are smeared uniformly in the common transverse space and may
describe our universe. We study the consequences of U dualities and find that
they imply relations among the scale factors. We find using Einstein's
equations that U dual... | hep-th astro-ph gr-qc | we consider n charge intersecting brane antibrane configurations in m theory which are smeared uniformly in the common transverse space and may describe our universe we study the consequences of u dualities and find that they imply relations among the scale factors we find using einsteins equations that u dualities als... | [['we', 'consider', 'n', 'charge', 'intersecting', 'brane', 'antibrane', 'configurations', 'in', 'm', 'theory', 'which', 'are', 'smeared', 'uniformly', 'in', 'the', 'common', 'transverse', 'space', 'and', 'may', 'describe', 'our', 'universe', 'we', 'study', 'the', 'consequences', 'of', 'u', 'dualities', 'and', 'find', ... | [-0.16442140253064663, 0.17275004312452943, -0.0617170197052419, 0.07939301632848897, -0.009080410819444665, -0.1448092876869618, 0.019214379458506136, 0.32419196353819135, -0.20847250565298295, -0.2673853597764794, 0.025239885516842843, -0.33127935504526795, -0.12443980008111637, 0.10797425247011076, 0.009901395694289... |
707.1422 | Alpha-prime corrections to space-like branes | Space-like branes or S-branes are certain class of time dependent solutions
of M/string theories having isometries ISO(p+1) $\times$ SO(d-p-2,1), where
$d=11,10$ respectively and have singularities at t=0. In \cite{Roy:2006du}, we
found that the asymptotically flat S-branes have the structure of generalized
Kasner ge... | hep-th | spacelike branes or sbranes are certain class of time dependent solutions of mstring theories having isometries isop1 times sodp21 where d1110 respectively and have singularities at t0 in citeroy2006du we found that the asymptotically flat sbranes have the structure of generalized kasner geometry near t0 in this work w... | [['spacelike', 'branes', 'or', 'sbranes', 'are', 'certain', 'class', 'of', 'time', 'dependent', 'solutions', 'of', 'mstring', 'theories', 'having', 'isometries', 'isop1', 'times', 'sodp21', 'where', 'd1110', 'respectively', 'and', 'have', 'singularities', 'at', 't0', 'in', 'citeroy2006du', 'we', 'found', 'that', 'the',... | [-0.13949624791910703, 0.12217302830381827, -0.10353651988658716, 0.14073702370726757, -0.062227474970065734, -0.19699907624586063, -0.017824953800829296, 0.3189807903317904, -0.17604994655544445, -0.18899219847517088, 0.07853307587581433, -0.35090779158371416, -0.09045969783963466, 0.10890988284954801, -0.048283331765... |
707.1423 | Smarandache Isotopy Theory Of Smarandache: Quasigroups And Loops | The concept of Smarandache isotopy is introduced and its study is explored
for Smarandache: groupoids, quasigroups and loops just like the study of
isotopy theory was carried out for groupoids, quasigroups and loops. The
exploration includes: Smarandache; isotopy and isomorphy classes, Smarandache
$f,g$ principal iso... | math.GM | the concept of smarandache isotopy is introduced and its study is explored for smarandache groupoids quasigroups and loops just like the study of isotopy theory was carried out for groupoids quasigroups and loops the exploration includes smarandache isotopy and isomorphy classes smarandache fg principal isotopes and gs... | [['the', 'concept', 'of', 'smarandache', 'isotopy', 'is', 'introduced', 'and', 'its', 'study', 'is', 'explored', 'for', 'smarandache', 'groupoids', 'quasigroups', 'and', 'loops', 'just', 'like', 'the', 'study', 'of', 'isotopy', 'theory', 'was', 'carried', 'out', 'for', 'groupoids', 'quasigroups', 'and', 'loops', 'the',... | [-0.25611160155583884, 0.12035996207293678, -0.01087100005292512, 0.185643052667419, -0.12407360511257294, -0.17206680458633505, 0.05564460384986423, 0.44199336863103067, -0.2736602936811904, -0.23852332744826663, 0.055010165048247954, -0.3083984795957804, -0.14217137149039735, 0.1704550157994666, -0.1452472076176646, ... |
707.1424 | Pion scattering poles and chiral symmetry restoration | Using unitarized Chiral Perturbation Theory methods, we perform a detailed
analysis of the $\pi\pi$ scattering poles $f_0(600)$ and $\rho(770)$ behaviour
when medium effects such as temperature or density drive the system towards
Chiral Symmetry Restoration. In the analysis of real poles below threshold, we
show that... | hep-ph | using unitarized chiral perturbation theory methods we perform a detailed analysis of the pipi scattering poles f_0600 and rho770 behaviour when medium effects such as temperature or density drive the system towards chiral symmetry restoration in the analysis of real poles below threshold we show that it is crucial to ... | [['using', 'unitarized', 'chiral', 'perturbation', 'theory', 'methods', 'we', 'perform', 'a', 'detailed', 'analysis', 'of', 'the', 'pipi', 'scattering', 'poles', 'f_0600', 'and', 'rho770', 'behaviour', 'when', 'medium', 'effects', 'such', 'as', 'temperature', 'or', 'density', 'drive', 'the', 'system', 'towards', 'chira... | [-0.11313984710939748, 0.19019367207155757, -0.13413870327315444, 0.11380415797222752, -0.05518548676018538, -0.10048242284087898, 0.0698923128596128, 0.35003870200950565, -0.18749175188104558, -0.22170496574971219, 0.028243421097761522, -0.31200364311658885, -0.12610301062814805, 0.08635499173312361, 0.066875496969302... |
707.1425 | How light can the lightest neutralino be? | We show that in the Minimal Supersymmetric Standard Model, the mass of the
lightest neutralino is experimentally unconstrained if the GUT relation between
the gaugino mass parameters M_1 and M_2 is dropped. We discuss what the impact
of light or massless neutralinos would be on their production at LEP, as well
as on ... | hep-ph | we show that in the minimal supersymmetric standard model the mass of the lightest neutralino is experimentally unconstrained if the gut relation between the gaugino mass parameters m_1 and m_2 is dropped we discuss what the impact of light or massless neutralinos would be on their production at lep as well as on elect... | [['we', 'show', 'that', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'the', 'mass', 'of', 'the', 'lightest', 'neutralino', 'is', 'experimentally', 'unconstrained', 'if', 'the', 'gut', 'relation', 'between', 'the', 'gaugino', 'mass', 'parameters', 'm_1', 'and', 'm_2', 'is', 'dropped', 'we', 'discuss', ... | [-0.06050170665030699, 0.314123237852828, -0.014400794967945855, 0.23529040925915085, -0.07333458686184327, -0.16588742642710774, 0.05708587978832361, 0.357715894290546, -0.21856483267778057, -0.3264048073630212, 0.07366738696701004, -0.3076019073852291, -0.003997832177585717, 0.15977216744203498, -0.020937555438002287... |
707.1426 | Cosmological evolution of regularized branes in 6D warped flux
compactifications | We study the cosmological evolution of extended branes in 6D warped flux
compactification models. The branes are endowed with the three ordinary spatial
dimensions, which are assumed to be homogeneous and isotropic, as well as an
internal extra dimension compactified on a circle. We embed these codimension 1
branes i... | hep-th astro-ph gr-qc | we study the cosmological evolution of extended branes in 6d warped flux compactification models the branes are endowed with the three ordinary spatial dimensions which are assumed to be homogeneous and isotropic as well as an internal extra dimension compactified on a circle we embed these codimension 1 branes in a st... | [['we', 'study', 'the', 'cosmological', 'evolution', 'of', 'extended', 'branes', 'in', '6d', 'warped', 'flux', 'compactification', 'models', 'the', 'branes', 'are', 'endowed', 'with', 'the', 'three', 'ordinary', 'spatial', 'dimensions', 'which', 'are', 'assumed', 'to', 'be', 'homogeneous', 'and', 'isotropic', 'as', 'we... | [-0.15023613644880243, 0.13960345594978207, -0.0595236760127591, 0.09692256678754348, -0.09485366462176899, -0.1752523061208194, -0.07481215757215978, 0.3071867832375574, -0.178298797539901, -0.2537885930185439, 0.12322110924433219, -0.2753391806152649, -0.11917687756358646, 0.09860175972862635, -0.0728536653536139, -0... |
707.1427 | Analytic perturbation theory versus 1/N expansion in the Gross-Neveu
model | The 1/N expansion can be successfully used to calculate the Green functions
of the two-dimensional O(2N) Gross - Neveu model. In parallel, the methods of
analytic perturbation theory are also applied. Comparing the results of these
two calculations at leading order, we report on the surprising agreement
between them.... | hep-ph hep-th | the 1n expansion can be successfully used to calculate the green functions of the twodimensional o2n gross neveu model in parallel the methods of analytic perturbation theory are also applied comparing the results of these two calculations at leading order we report on the surprising agreement between them | [['the', '1n', 'expansion', 'can', 'be', 'successfully', 'used', 'to', 'calculate', 'the', 'green', 'functions', 'of', 'the', 'twodimensional', 'o2n', 'gross', 'neveu', 'model', 'in', 'parallel', 'the', 'methods', 'of', 'analytic', 'perturbation', 'theory', 'are', 'also', 'applied', 'comparing', 'the', 'results', 'of',... | [-0.09255471485084854, 0.03842361771967262, -0.12043989992040831, 0.12107396498322487, 0.017786159747629426, -0.05721227803345149, 0.021219623587967362, 0.36132147213599336, -0.20169282017741352, -0.2886359498370439, 0.0710544370789042, -0.30107955836380523, -0.17916564926660308, 0.20205844834951373, 0.0348797087790444... |
707.1428 | Development of CaMoO4 crystal scintillators for double beta decay
experiment with 100-Mo | Energy resolution, alpha/beta ratio, pulse-shape discrimination for gamma
rays and alpha particles, temperature dependence of scintillation properties,
and radioactive contamination were studied with CaMoO4 crystal scintillators. A
high sensitivity experiment to search for neutrinoless double beta decay of
100-Mo by ... | nucl-ex | energy resolution alphabeta ratio pulseshape discrimination for gamma rays and alpha particles temperature dependence of scintillation properties and radioactive contamination were studied with camoo4 crystal scintillators a high sensitivity experiment to search for neutrinoless double beta decay of 100mo by using camo... | [['energy', 'resolution', 'alphabeta', 'ratio', 'pulseshape', 'discrimination', 'for', 'gamma', 'rays', 'and', 'alpha', 'particles', 'temperature', 'dependence', 'of', 'scintillation', 'properties', 'and', 'radioactive', 'contamination', 'were', 'studied', 'with', 'camoo4', 'crystal', 'scintillators', 'a', 'high', 'sen... | [0.026706075575202704, 0.33588953328629334, -0.03963624346587393, 0.10601428458725827, 0.015574997896328569, -0.22646811599325803, 0.04949254789907071, 0.45040574106905196, -0.19337482270525974, -0.3554813135984457, -0.010952608137288027, -0.40904767767836653, 0.07571716508310702, 0.2240105236104379, 0.0833317699738674... |
707.1429 | Tangential projections and secant defective varieties | Going one step further in Zak's classification of Scorza varieties with
secant defect equal to one, we characterize the Veronese embedding of $\P^n$
given by the complete linear system of quadrics and its smooth projections from
a point as the only smooth irreducible complex and non-degenerate projective
subvarieties... | math.AG | going one step further in zaks classification of scorza varieties with secant defect equal to one we characterize the veronese embedding of pn given by the complete linear system of quadrics and its smooth projections from a point as the only smooth irreducible complex and nondegenerate projective subvarieties of pn th... | [['going', 'one', 'step', 'further', 'in', 'zaks', 'classification', 'of', 'scorza', 'varieties', 'with', 'secant', 'defect', 'equal', 'to', 'one', 'we', 'characterize', 'the', 'veronese', 'embedding', 'of', 'pn', 'given', 'by', 'the', 'complete', 'linear', 'system', 'of', 'quadrics', 'and', 'its', 'smooth', 'projectio... | [-0.12445236258369324, -0.022868127899308657, -0.08131295261133847, 0.019177907355258178, -0.03524093814836494, -0.2065334653257039, -0.007465677424173416, 0.3065385178438035, -0.3427152881270339, -0.13407985723159951, 0.08264732059966452, -0.2704955150116363, -0.1326357789361721, 0.18949705037962775, -0.12584522873933... |
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