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708.2549 | The scalar curvature flow in Lorentzian manifolds | We prove the existence of closed hypersurfaces of prescribed scalar curvature
in globally hyperbolic Lorentzian manifolds provided there are barriers.
| math.DG | we prove the existence of closed hypersurfaces of prescribed scalar curvature in globally hyperbolic lorentzian manifolds provided there are barriers | [['we', 'prove', 'the', 'existence', 'of', 'closed', 'hypersurfaces', 'of', 'prescribed', 'scalar', 'curvature', 'in', 'globally', 'hyperbolic', 'lorentzian', 'manifolds', 'provided', 'there', 'are', 'barriers']] | [-0.3587132885120809, 0.12753073538187892, -0.033495814679190515, 0.14359138547442854, -0.07131309062242508, -0.22119614901021123, -0.15153923407196998, 0.3885337717831135, -0.17038326784968377, -0.15198301849886775, 0.06923348036943935, -0.29298628205433486, -0.17150032005738466, 0.1786063749343157, -0.16217147747520358, 0.08128891191445291, 0.07135619721375405, 0.1132015323266387, -0.04302988448180258, -0.2741910688579082, 0.5343094058334827, -0.1510410443879664, 0.16491197803989052, 0.18209897875785827, 0.16976422993466259, -0.11296008846256882, 0.04618680877611041, 0.07053443908225746, -0.2713142601773143, 0.1119281564373523, 0.2802471827948466, 0.07863100481918081, 0.1990195894963108, -0.4303485207259655, -0.2517313601449132, 0.2396139096468687, 0.15932798485737293, 0.018154537747614087, -0.1124560801894404, -0.3227469280362129, 0.09215192971751093, 0.05584177495911717, -0.33581415973603723, -0.10094934874214231, -0.038268675841391084, 0.019810154708102344, -0.15442938469350337, 0.10023549515753985, 0.09967253776267171, 0.1499156201723963, -0.1750510812504217, -0.050546898320317266, -0.1462045732885599, 0.07426751339808106, 0.10368236384820192, -0.027820983971469104, 0.06649746533948928, 0.03547272835858166, -0.09117775182821788, 0.27312953118234873, -0.12725293952971697, -0.3948746182024479, 0.01535294745117426, -0.17914852374233306, -0.09147258854936809, 0.18055266598239542, 0.1366864669136703, 0.21975933872163295, -0.035629544965922834, 0.25180644921492784, -0.010687706992030144, -0.014218198088929056, 0.20202651366125793, -0.04474477814510465, 0.14533777380129323, 0.046143556199967864, 0.22589261489920318, 0.09244608711451292, 0.06378982607275248, -0.16578937801532448, -0.45370734483003616, -0.22662329766899347, -0.11153881219215692, 0.241708005592227, -0.19906690809875727, -0.3197364263236523, 0.34637373872101307, -0.1201711737550795, 0.14010885674506426, 0.17812684285454453, 0.18496720446273685, 0.01339309249597136, -0.0131345359608531, 0.23063918855041265, 0.2463931443169713, 0.22140211635269225, 0.03515976807102561, -0.07368161007761956, -0.12261121715418995, 0.08333261073566973] |
708.255 | Triplet Dimerization Crossover Driven by Magnetic Frustration in In2VO5 | In2VO5, containing magnetically frustrated zig-zag chains, shows a remarkable
magnetic crossover at 120 K between paramagnetic states with positive (17 K)
and negative (-70 K) Weiss temperatures. Magnetic moment and entropy data show
that the V4+ S = 1/2 spins condense into S = 1 triplet dimers below the
crossover. A further freezing of the antiferromagnetically coupled triplet
dimers into a global singlet state is observed at 2.5 K, with no long range
magnetic order down to 0.42 K and in fields up to 9 T. No structural V-V
dimerization is observed by high-resolution X-ray diffraction down to 10 K, but
a subtle lattice anomaly evidences a spin-lattice coupling in the triplet dimer
state. This is assigned to longitudinal oxygen displacement modes that reduce
frustration within the chains and so couple to the spin dimer fluctuations.
| cond-mat.str-el | in2vo5 containing magnetically frustrated zigzag chains shows a remarkable magnetic crossover at 120 k between paramagnetic states with positive 17 k and negative 70 k weiss temperatures magnetic moment and entropy data show that the v4 s 12 spins condense into s 1 triplet dimers below the crossover a further freezing of the antiferromagnetically coupled triplet dimers into a global singlet state is observed at 25 k with no long range magnetic order down to 042 k and in fields up to 9 t no structural vv dimerization is observed by highresolution xray diffraction down to 10 k but a subtle lattice anomaly evidences a spinlattice coupling in the triplet dimer state this is assigned to longitudinal oxygen displacement modes that reduce frustration within the chains and so couple to the spin dimer fluctuations | [['in2vo5', 'containing', 'magnetically', 'frustrated', 'zigzag', 'chains', 'shows', 'a', 'remarkable', 'magnetic', 'crossover', 'at', '120', 'k', 'between', 'paramagnetic', 'states', 'with', 'positive', '17', 'k', 'and', 'negative', '70', 'k', 'weiss', 'temperatures', 'magnetic', 'moment', 'and', 'entropy', 'data', 'show', 'that', 'the', 'v4', 's', '12', 'spins', 'condense', 'into', 's', '1', 'triplet', 'dimers', 'below', 'the', 'crossover', 'a', 'further', 'freezing', 'of', 'the', 'antiferromagnetically', 'coupled', 'triplet', 'dimers', 'into', 'a', 'global', 'singlet', 'state', 'is', 'observed', 'at', '25', 'k', 'with', 'no', 'long', 'range', 'magnetic', 'order', 'down', 'to', '042', 'k', 'and', 'in', 'fields', 'up', 'to', '9', 't', 'no', 'structural', 'vv', 'dimerization', 'is', 'observed', 'by', 'highresolution', 'xray', 'diffraction', 'down', 'to', '10', 'k', 'but', 'a', 'subtle', 'lattice', 'anomaly', 'evidences', 'a', 'spinlattice', 'coupling', 'in', 'the', 'triplet', 'dimer', 'state', 'this', 'is', 'assigned', 'to', 'longitudinal', 'oxygen', 'displacement', 'modes', 'that', 'reduce', 'frustration', 'within', 'the', 'chains', 'and', 'so', 'couple', 'to', 'the', 'spin', 'dimer', 'fluctuations']] | [-0.17098418573515295, 0.3175404895680831, 0.025498921712321827, 0.03469062414465111, -0.016394043677927815, -0.19688963057097994, 0.10520023569932083, 0.4066422952047146, -0.25801615209193596, -0.3211793857001102, -0.010508309811728992, -0.38211091254045493, 0.008769169797314636, 0.05051685271979268, 0.15421840698465206, -0.0680832323277675, -0.03803881291654517, 0.05963380152920831, -0.09670740299173561, -0.24013964212221553, 0.18417584567681328, -0.033148558454157144, 0.25537949202776844, 0.1039329650389954, 0.05419164310546536, -0.027905485542393776, 0.16831474710228062, -0.01066958656145343, -0.17289233826430525, 0.021661197305778597, 0.26010335717044436, -0.07327805505370472, 0.18285114411959674, -0.36664925813118915, -0.17541316150228925, 0.04735031607213305, 0.143909836028865, 0.11277399419236984, 0.008014335727958536, -0.270913603114409, 0.06569823976467128, -0.09223020550231936, -0.08845888668803303, -0.11354602158153013, 0.03850475822074978, -0.07667300223247774, -0.2827825974673033, 0.15144141679959816, 0.12154677452662015, 0.16736738665251813, -0.0702499163132022, -0.17757676196729402, -0.10085874596965123, 0.014959648619892437, 0.05747561620152208, 0.12838583858944336, 0.13326957106326165, -0.06886828553675216, -0.10083412617417191, 0.3026336438488215, -0.12205899024900022, -0.008106320651609506, 0.1683039529659132, -0.2112408012513127, -0.10391184384587096, 0.2781368717863989, 0.05985116616322367, 0.07997323247715275, -0.12518040783731127, 0.050108151345291355, -0.0031233600257381576, 0.24644892059488974, 0.055513118341592935, 0.02015601430929252, 0.2691605609925047, 0.12461051177806846, 0.05796411951809232, 0.16887953454183777, -0.14153356141273502, -0.0924438285509319, -0.20626620726604292, -0.13728116817925293, -0.17585469967053174, 0.09880179377383928, -0.0830328222672601, -0.10447559888655347, 0.3333682604724847, 0.11851586045337009, 0.23957152560408881, -0.04313415032463955, 0.1749602413185483, 0.022274077393865183, 0.0987586585048229, 0.058689665428098683, 0.20175464813416796, 0.25943439075924846, 0.11885643975614611, -0.3168813006139235, -0.024100068695982222, -0.02025314048801396] |
708.2551 | Comments on Possible Variation of the Universal Constants | Discussion of the constancy, or otherwise, of the various so-called universal
constants which abound in physics has continued for many years. However,
relatively recent observations, which appear to indicate a variation in the
value of the fine structure constant, have reignited the subject. These
observations relate to quasars and that in itself raises questions. Also, since
many of the arguments utilise the Bekenstein-Hawking expression for the entropy
of a black hole, further controversy is introduced into the discussion
immediately. In what follows these two points will be examined and some less
well-known theoretical considerations introduced which, hopefully, will
instigate wider examination of this topic.
| physics.gen-ph | discussion of the constancy or otherwise of the various socalled universal constants which abound in physics has continued for many years however relatively recent observations which appear to indicate a variation in the value of the fine structure constant have reignited the subject these observations relate to quasars and that in itself raises questions also since many of the arguments utilise the bekensteinhawking expression for the entropy of a black hole further controversy is introduced into the discussion immediately in what follows these two points will be examined and some less wellknown theoretical considerations introduced which hopefully will instigate wider examination of this topic | [['discussion', 'of', 'the', 'constancy', 'or', 'otherwise', 'of', 'the', 'various', 'socalled', 'universal', 'constants', 'which', 'abound', 'in', 'physics', 'has', 'continued', 'for', 'many', 'years', 'however', 'relatively', 'recent', 'observations', 'which', 'appear', 'to', 'indicate', 'a', 'variation', 'in', 'the', 'value', 'of', 'the', 'fine', 'structure', 'constant', 'have', 'reignited', 'the', 'subject', 'these', 'observations', 'relate', 'to', 'quasars', 'and', 'that', 'in', 'itself', 'raises', 'questions', 'also', 'since', 'many', 'of', 'the', 'arguments', 'utilise', 'the', 'bekensteinhawking', 'expression', 'for', 'the', 'entropy', 'of', 'a', 'black', 'hole', 'further', 'controversy', 'is', 'introduced', 'into', 'the', 'discussion', 'immediately', 'in', 'what', 'follows', 'these', 'two', 'points', 'will', 'be', 'examined', 'and', 'some', 'less', 'wellknown', 'theoretical', 'considerations', 'introduced', 'which', 'hopefully', 'will', 'instigate', 'wider', 'examination', 'of', 'this', 'topic']] | [-0.0905014024151919, 0.13594188412221578, -0.1109917713329196, 0.10093420924833761, -0.1148109425110026, -0.1352601455649934, 0.060221456546479694, 0.313126600239999, -0.24027046328410506, -0.3123597298802521, 0.15518826321036053, -0.2567852672117834, -0.13895683383004956, 0.22867008130057143, -0.1063289951103238, 0.02875496179331094, 0.03501451212035205, 0.03234347653387186, -0.06982458678360742, -0.2827014449352506, 0.3095707150373178, 0.08166557321629415, 0.23996909326300597, 0.10400890247267223, 0.029397046986000184, -0.03828951195688345, -0.09613098873971747, 0.04601232833766307, -0.18370112694628915, 0.13109373164255744, 0.2568162741103711, 0.17029107288600734, 0.3137082216674641, -0.41287355416884214, -0.2588131578388409, 0.06731383467446833, 0.15028758690235777, 0.0947482097152925, -0.06932144631551077, -0.24055093544302508, 0.0609004699385528, -0.15590058149581848, -0.15068976381399596, -0.05944775652628428, 0.07368555778744988, -0.015848872543966327, -0.14991259290847944, 0.04948184909853108, 0.10903015237552328, 0.03268260184603815, -0.06948919587067884, -0.12422755436273292, 0.03403650087980518, 0.10243105750235443, 0.14652857055233864, 0.026492508663348138, 0.10188742574358073, -0.14835642908516233, -0.10410080536698493, 0.38173726285234666, 0.015742950801862977, -0.1303683005613633, 0.18373303400137678, -0.19645960740924168, -0.19092929481009308, 0.08565787882924689, 0.11803532157388802, 0.07806005055765407, -0.1405715381283349, 0.04824607071910018, -0.06071804134766213, 0.160699417671332, 0.08000207529403269, 0.06325738753926438, 0.2769271719824666, 0.08710335378642552, 0.005598409523372538, 0.08637533240051617, -0.01958492538632037, -0.13107962546368632, -0.2710802029816058, -0.15088764673027283, -0.13436627892392258, 0.08910347306832242, -0.05270966712207435, -0.17255886788748634, 0.3709586731767139, 0.16136836839947277, 0.24935571166973275, -0.009805914190320227, 0.21035284472208543, 0.0858122967944767, 0.07610567301834145, 0.02794555880021877, 0.2881829460263991, 0.12513923978146452, 0.12517823127116293, -0.15387265441957146, 0.05356296759530848, 0.024175086148226492] |
708.2552 | Quantum Hamilton-Jacobi Approach to Two Dimensional Singular Oscillator | We have obtained the solutions of two dimensional singular oscillator which
is known as the quantum Calogero-Sutherland model both in cartesian and
parabolic coordinates within the framework of quantum Hamilton Jacobi
formalism. Solvability conditions and eigenfunctions are obtained by using the
singularity structures of quantum momentum functions under some conditions. New
potentials are generated by using the first two states of singular oscillator
for parabolic coordinates.
| quant-ph | we have obtained the solutions of two dimensional singular oscillator which is known as the quantum calogerosutherland model both in cartesian and parabolic coordinates within the framework of quantum hamilton jacobi formalism solvability conditions and eigenfunctions are obtained by using the singularity structures of quantum momentum functions under some conditions new potentials are generated by using the first two states of singular oscillator for parabolic coordinates | [['we', 'have', 'obtained', 'the', 'solutions', 'of', 'two', 'dimensional', 'singular', 'oscillator', 'which', 'is', 'known', 'as', 'the', 'quantum', 'calogerosutherland', 'model', 'both', 'in', 'cartesian', 'and', 'parabolic', 'coordinates', 'within', 'the', 'framework', 'of', 'quantum', 'hamilton', 'jacobi', 'formalism', 'solvability', 'conditions', 'and', 'eigenfunctions', 'are', 'obtained', 'by', 'using', 'the', 'singularity', 'structures', 'of', 'quantum', 'momentum', 'functions', 'under', 'some', 'conditions', 'new', 'potentials', 'are', 'generated', 'by', 'using', 'the', 'first', 'two', 'states', 'of', 'singular', 'oscillator', 'for', 'parabolic', 'coordinates']] | [-0.14878836779318977, 0.11226046622984788, -0.07131332572493138, 0.03526286375320827, -0.023494480706920676, -0.17603926134831976, -0.08121714277799721, 0.33766998311109614, -0.2565122882299351, -0.19107245930442304, 0.09786118851854664, -0.2595845700777841, -0.16776603027458556, 0.22714386139220247, -0.007901304785980645, 0.14548307232502283, 0.09565858773633161, 0.052247196111376536, -0.12041364587617642, -0.2166078078814528, 0.41304275109855965, -0.02594746673077514, 0.20106860560675463, -0.02303545076530568, 0.12479668792873395, -0.0048467755868014965, 0.06701882468945713, 0.024818761217774765, -0.1407584729039985, 0.10921246005455032, 0.22253520828389534, 0.05683035311768904, 0.2333395549124389, -0.44978405639642116, -0.19129948653845172, 0.05219326079576135, 0.12059580070446387, 0.11511789793395578, -0.013678032044095524, -0.34567397533718386, 0.03205722858282653, -0.14889211156828838, -0.2053792931732129, -0.12219411066987297, -0.03246314156179627, 0.08035397896486701, -0.23206604873253542, 0.09125132083356606, 0.06520628742873669, 0.0781202448362654, -0.1396941011912669, -0.10801554213023999, -0.04319480101747269, 0.07999897480829421, -0.03360735662246236, -0.07742805311025938, 0.05641992761273727, -0.09858189012547056, -0.13863013180988756, 0.40661743186611793, -0.041617159858684645, -0.30241137505932286, 0.10990752866773894, -0.12604019999729865, -0.09760720367458733, 0.07541270396023085, 0.1059828031257811, 0.148248906190874, -0.17543028055154014, 0.17915209995011205, -0.02736381081525575, 0.032083985254620064, 0.14943965229869002, 0.03630600090731274, 0.11966420158348752, 0.029735120704792666, 0.07329209667108388, 0.14005099102205626, -0.030214655410611267, -0.20405003541346753, -0.36330024062684085, -0.1243527350505963, -0.20000517119963965, 0.08244885020240238, -0.11449404802326833, -0.19590720754455437, 0.4405347175444617, 0.06128379743754384, 0.1815298095938157, 0.023353657108435236, 0.21548047905900714, 0.2046611629352397, 0.03950355024161664, 0.06048694843070045, 0.24066287861426122, 0.21851610212417488, 0.06366123500717522, -0.19304533268212143, -0.061220694283926576, 0.18713523274654467] |
708.2553 | Band structure renormalization and weak pseudogap behavior in
Na_{0.33}CoO_2: Fluctuation exchange study based on a single band model | Based on a single band Hubbard model and the fluctuation exchange
approximation, the effective mass and the energy band renormalization in
Na$_{0.33}$CoO$_2$ is elaborated. The renormalization is observed to exhibit
certain kind of anisotropy, which agrees qualitatively with the angle-resolved
photoemission spectroscopy (ARPES) measurements. Moreover, the spectral
function and density of states (DOS) in the normal state are calculated, with a
weak pseudogap behavior being seen, which is explained as a result of the
strong Coulomb correlations. Our results suggest that the large Fermi surface
(FS) associated with the $a_{1g}$ band plays likely a central role in the
charge dynamics.
| cond-mat.str-el | based on a single band hubbard model and the fluctuation exchange approximation the effective mass and the energy band renormalization in na_033coo_2 is elaborated the renormalization is observed to exhibit certain kind of anisotropy which agrees qualitatively with the angleresolved photoemission spectroscopy arpes measurements moreover the spectral function and density of states dos in the normal state are calculated with a weak pseudogap behavior being seen which is explained as a result of the strong coulomb correlations our results suggest that the large fermi surface fs associated with the a_1g band plays likely a central role in the charge dynamics | [['based', 'on', 'a', 'single', 'band', 'hubbard', 'model', 'and', 'the', 'fluctuation', 'exchange', 'approximation', 'the', 'effective', 'mass', 'and', 'the', 'energy', 'band', 'renormalization', 'in', 'na_033coo_2', 'is', 'elaborated', 'the', 'renormalization', 'is', 'observed', 'to', 'exhibit', 'certain', 'kind', 'of', 'anisotropy', 'which', 'agrees', 'qualitatively', 'with', 'the', 'angleresolved', 'photoemission', 'spectroscopy', 'arpes', 'measurements', 'moreover', 'the', 'spectral', 'function', 'and', 'density', 'of', 'states', 'dos', 'in', 'the', 'normal', 'state', 'are', 'calculated', 'with', 'a', 'weak', 'pseudogap', 'behavior', 'being', 'seen', 'which', 'is', 'explained', 'as', 'a', 'result', 'of', 'the', 'strong', 'coulomb', 'correlations', 'our', 'results', 'suggest', 'that', 'the', 'large', 'fermi', 'surface', 'fs', 'associated', 'with', 'the', 'a_1g', 'band', 'plays', 'likely', 'a', 'central', 'role', 'in', 'the', 'charge', 'dynamics']] | [-0.15882618276571686, 0.15748309899554258, -0.1227420609387936, 0.1156925077096211, -0.012738519555164708, -0.12470443270667786, 0.06397620794560874, 0.37140437132782406, -0.2551827775878888, -0.3060453054071827, -0.018078639758797834, -0.34017530924668815, -0.12030295325875884, 0.16595490496709114, 0.04998662033014827, 0.007484448208200811, 0.026004691791692465, -0.02060131709834542, -0.13826166152380256, -0.14950629473532165, 0.3511039735278999, 0.07882257973342532, 0.3204057077604412, 0.13555274876493095, 0.012037295956315116, 0.049238406947221265, 0.05413949442027852, 0.030810236436963984, -0.12060411017885811, 0.0740398710677071, 0.26941574901116616, -0.11150699812975345, 0.22172113121816456, -0.3790847079433275, -0.24737986795265565, -0.024070713203400373, 0.10594593407586217, 0.10657905023121698, -0.07170489133274502, -0.2903301203999706, 0.014157525076168694, -0.1701652241842539, -0.17043946226917658, -0.0874025776436684, -0.04839720361574431, 0.0008631064485984318, -0.22376077605242078, 0.15963777082100877, 0.0007482509180489513, 0.049719775961053495, -0.1078716360427665, -0.0925178355725501, -0.11847293203122763, 0.050531432554690225, 0.08215771780250537, 0.07906114762517238, 0.12868221500750884, -0.11210653409738132, -0.08041035453318571, 0.35654739710041367, -0.10163895232659398, -0.07622667187542627, 0.16011016689137453, -0.2161493922461464, -0.0981074301572987, 0.1556332315779244, 0.03583347883470582, 0.06397966773371504, -0.09692502463579818, 0.0948403881577013, -0.057830761383155904, 0.19710232052984977, -0.003291647970638793, 0.10873705945024738, 0.20214298392900013, 0.17647867770677414, 0.033530052055162615, 0.07170048742696192, -0.17341488061973712, -0.07094052089660456, -0.275947389021196, -0.11177306205758618, -0.24995514398647678, 0.062137675328142565, -0.053934905936293576, -0.18699274973642796, 0.43612361994643717, 0.08029566509084719, 0.2493425759162302, -0.02157674262281319, 0.22225287052417042, 0.18636509289640482, 0.09011494186283513, 0.06604089402132715, 0.26521010239928433, 0.1514086365967876, 0.08494841491314348, -0.3258927294542317, 0.07864407438201586, 0.022227386650017868] |
708.2554 | On the Entropy of Four-Dimensional Near-Extremal N=2 Black Holes with
R^2-Terms | We consider the entropy of four-dimensional near-extremal N=2 black holes.
Without R^2-terms, the Bekenstein-Hawking entropy formula has the structure of
the extremal black holes entropy with a shift of the charges depending on the
non-extremality parameter and the moduli at infinity. We derive a generalized
Wald entropy formula for non-extremal N=2 black holes with R^2-terms. We
construct a class of small near-extremal horizon solutions with R^2-terms. In
this case the entropy is the same as in the extremal case to order O(mu^2), and
does not exhibit the charge shift behavior.
| hep-th | we consider the entropy of fourdimensional nearextremal n2 black holes without r2terms the bekensteinhawking entropy formula has the structure of the extremal black holes entropy with a shift of the charges depending on the nonextremality parameter and the moduli at infinity we derive a generalized wald entropy formula for nonextremal n2 black holes with r2terms we construct a class of small nearextremal horizon solutions with r2terms in this case the entropy is the same as in the extremal case to order omu2 and does not exhibit the charge shift behavior | [['we', 'consider', 'the', 'entropy', 'of', 'fourdimensional', 'nearextremal', 'n2', 'black', 'holes', 'without', 'r2terms', 'the', 'bekensteinhawking', 'entropy', 'formula', 'has', 'the', 'structure', 'of', 'the', 'extremal', 'black', 'holes', 'entropy', 'with', 'a', 'shift', 'of', 'the', 'charges', 'depending', 'on', 'the', 'nonextremality', 'parameter', 'and', 'the', 'moduli', 'at', 'infinity', 'we', 'derive', 'a', 'generalized', 'wald', 'entropy', 'formula', 'for', 'nonextremal', 'n2', 'black', 'holes', 'with', 'r2terms', 'we', 'construct', 'a', 'class', 'of', 'small', 'nearextremal', 'horizon', 'solutions', 'with', 'r2terms', 'in', 'this', 'case', 'the', 'entropy', 'is', 'the', 'same', 'as', 'in', 'the', 'extremal', 'case', 'to', 'order', 'omu2', 'and', 'does', 'not', 'exhibit', 'the', 'charge', 'shift', 'behavior']] | [-0.1479651372983224, 0.12162337489426137, -0.06122626188832025, 0.13541118456826856, -0.03428239414675368, -0.16791405173329016, 0.028661685090305075, 0.2151839081197977, -0.12401773910710795, -0.2592018522736099, 0.09202182892089089, -0.38954681590613394, -0.08386675505381491, 0.1375683646183461, -0.11955812246435218, 0.06509047591437896, -0.056049784096992676, 0.11603766945190727, -0.14070664174440833, -0.22510497865215356, 0.3653842272443904, 0.05610891308816564, 0.27279242941488824, 0.055667933149056305, 0.09557465582167626, 0.020768655800364084, 0.08544919488227201, 0.07621261213595669, -0.23350693741813303, 0.08192111897321107, 0.23878753301170136, 0.11888949758787122, 0.15332873484068033, -0.3709056216188603, -0.20533809883313048, 0.14663868490606546, 0.11780911257956177, 0.2019018207780189, -0.07417588147412364, -0.1770892090215865, 0.0751927932129345, -0.23176844080703127, -0.1862306734547019, -0.04954692656691703, 0.08077373746782542, -0.05688877347080658, -0.21276820235070773, 0.1463009176775813, 0.11135311594439877, -0.07564134103659954, -0.12841153047564957, -0.024669299667908085, -0.09786548261116776, 0.08192040200552178, 0.17409191597382434, -0.012058105004123515, 0.15478932085033092, -0.07743660823907703, -0.1221530442022615, 0.27229269270578194, -0.07248619073199936, -0.24634604242940744, 0.10922782019608551, -0.2820073652702073, -0.11776742611287369, 0.08834319454617798, 0.1076829410623759, 0.2987687135218746, -0.07818885951678062, 0.20761700897451696, -0.004558972890178362, 0.15175549825653434, 0.15824789159620803, 0.07466813925032814, 0.3210524165770039, 0.042117802690093714, 0.05480067533337408, 0.27123208621309863, -0.056272453863898085, -0.11130914234866698, -0.35128865755266614, -0.19397813740005304, -0.1717979564745393, 0.15787353111291952, -0.22230919647101674, -0.21844488179518118, 0.3082728727513717, 0.052769227801925604, 0.2197273323415882, 0.09270800098569856, 0.1682063693555392, 0.1406244590710331, 0.036326506697676245, 0.12372416263549692, 0.28269876698290725, 0.11393248937610123, 0.13771002958528697, -0.27237775305079087, -0.05302523301086492, 0.20792189410163298] |
708.2555 | A supermassive binary black hole with triple disks | Hierarchical structure formation inevitably leads to the formation of
supermassive binary black holes (BBHs) with a sub-parsec separation in galactic
nuclei. However, to date there has been no unambiguous detection of such
systems. In an effort to search for potential observational signatures of
supermassive BBHs, we performed high-resolution smoothed particle hydrodynamics
(SPH) simulations of two black holes in a binary of moderate eccentricity
surrounded by a circumbinary disk. Building on our previous work, which has
shown that gas can periodically transfer from the circumbinary disk to the
black holes when the binary is on an eccentric orbit, the current set of
simulations focuses on the formation of the individual accretion disks, their
evolution and mutual interaction, and the predicted radiative signature. The
variation in mass transfer with orbital phase from the circumbinary disk
induces periodic variations in the light curve of the two accretion disks at
ultraviolet wavelengths, but not in the optical or near-infrared. Searches for
this signal offer a promising method to detect supermassive BBHs.
| astro-ph gr-qc | hierarchical structure formation inevitably leads to the formation of supermassive binary black holes bbhs with a subparsec separation in galactic nuclei however to date there has been no unambiguous detection of such systems in an effort to search for potential observational signatures of supermassive bbhs we performed highresolution smoothed particle hydrodynamics sph simulations of two black holes in a binary of moderate eccentricity surrounded by a circumbinary disk building on our previous work which has shown that gas can periodically transfer from the circumbinary disk to the black holes when the binary is on an eccentric orbit the current set of simulations focuses on the formation of the individual accretion disks their evolution and mutual interaction and the predicted radiative signature the variation in mass transfer with orbital phase from the circumbinary disk induces periodic variations in the light curve of the two accretion disks at ultraviolet wavelengths but not in the optical or nearinfrared searches for this signal offer a promising method to detect supermassive bbhs | [['hierarchical', 'structure', 'formation', 'inevitably', 'leads', 'to', 'the', 'formation', 'of', 'supermassive', 'binary', 'black', 'holes', 'bbhs', 'with', 'a', 'subparsec', 'separation', 'in', 'galactic', 'nuclei', 'however', 'to', 'date', 'there', 'has', 'been', 'no', 'unambiguous', 'detection', 'of', 'such', 'systems', 'in', 'an', 'effort', 'to', 'search', 'for', 'potential', 'observational', 'signatures', 'of', 'supermassive', 'bbhs', 'we', 'performed', 'highresolution', 'smoothed', 'particle', 'hydrodynamics', 'sph', 'simulations', 'of', 'two', 'black', 'holes', 'in', 'a', 'binary', 'of', 'moderate', 'eccentricity', 'surrounded', 'by', 'a', 'circumbinary', 'disk', 'building', 'on', 'our', 'previous', 'work', 'which', 'has', 'shown', 'that', 'gas', 'can', 'periodically', 'transfer', 'from', 'the', 'circumbinary', 'disk', 'to', 'the', 'black', 'holes', 'when', 'the', 'binary', 'is', 'on', 'an', 'eccentric', 'orbit', 'the', 'current', 'set', 'of', 'simulations', 'focuses', 'on', 'the', 'formation', 'of', 'the', 'individual', 'accretion', 'disks', 'their', 'evolution', 'and', 'mutual', 'interaction', 'and', 'the', 'predicted', 'radiative', 'signature', 'the', 'variation', 'in', 'mass', 'transfer', 'with', 'orbital', 'phase', 'from', 'the', 'circumbinary', 'disk', 'induces', 'periodic', 'variations', 'in', 'the', 'light', 'curve', 'of', 'the', 'two', 'accretion', 'disks', 'at', 'ultraviolet', 'wavelengths', 'but', 'not', 'in', 'the', 'optical', 'or', 'nearinfrared', 'searches', 'for', 'this', 'signal', 'offer', 'a', 'promising', 'method', 'to', 'detect', 'supermassive', 'bbhs']] | [-0.14638388262832297, 0.08235625769056988, -0.07538555814845566, 0.07592860890467355, -0.09012420769379346, -0.07112721774816334, 0.012629446009603402, 0.3860781071261464, -0.19856314563532612, -0.33232832583738214, 0.06449109769961657, -0.2971218753673002, -0.062179688791588264, 0.21156822606254772, -0.013550451438048642, 0.06453644248941344, 0.09138189265950622, -0.07769808358049946, -0.07118418621328731, -0.22518099747280296, 0.33573654260692704, 0.1218304788724458, 0.08118865973334258, -0.0326936061070217, 0.05465698711473695, -0.03938108552414589, -0.03993983558395844, -0.047104097651819624, -0.17034887065812088, 0.04801980965135725, 0.22477237970050992, 0.11621322313987253, 0.22583501882053644, -0.41950665875533205, -0.2576808899607576, 0.0763141719602093, 0.19936221933918086, 0.13291919376620254, -0.17252692583220602, -0.231395434089769, 0.06337869002673396, -0.24996948664349888, -0.1045998676141869, 0.033525255307956726, 0.09464638023832422, -0.008610350915654647, -0.23646998140733677, 0.09063872662902682, 0.1035040162244399, -0.002934741943762331, -0.11894347383584938, -0.01765907423648827, -0.08584069121562078, 0.06911189044901717, 0.07108039999921656, 0.06581847805775211, 0.20618336300315435, -0.10840154120079548, -0.12032126921680784, 0.39216042269846635, -0.05961277967173896, -0.09947838534706992, 0.28687878771166425, -0.2537828708028499, -0.12081868856766088, 0.1805281031787574, 0.21728214038212498, 0.1771296444934553, -0.13021730347949534, 0.017125473246898525, -0.00459442332297742, 0.24151377198370005, 0.07579580599352896, 0.06324354937219223, 0.495364463012554, 0.16205805104398754, 0.0018889885967385447, 0.11179207446622456, -0.19251509713326875, -0.09438410912456359, -0.15663580262955434, -0.09042207890017304, -0.17751755004380634, 0.08504609293787124, -0.12117628704928682, -0.16776728829766993, 0.31768203764863895, 0.10492361913167475, 0.21728691884489384, -0.004709200114485791, 0.31121925225348157, 0.041803230436795534, 0.08500161755852356, 0.11978056357091593, 0.3802240826496241, 0.11934990698226287, 0.09391327899836092, -0.28643310977380254, 0.05773576363393288, 0.038848436353895476] |
708.2556 | Pursuit-Evasion Games with Incomplete Information in Discrete Time | Pursuit-Evasion Games (in discrete time) are stochastic games with
nonnegative daily payoffs, with the final payoff being the cumulative sum of
payoffs during the game. We show that such games admit a value even in the
presence of incomplete information and that this value is uniform, i.e. there
are epsilon-optimal strategies for both players that are epsilon-optimal in any
long enough prefix of the game. We give an example to demonstrate that
nonnegativity is essential and expand the results to leavable games.
| math.PR | pursuitevasion games in discrete time are stochastic games with nonnegative daily payoffs with the final payoff being the cumulative sum of payoffs during the game we show that such games admit a value even in the presence of incomplete information and that this value is uniform ie there are epsilonoptimal strategies for both players that are epsilonoptimal in any long enough prefix of the game we give an example to demonstrate that nonnegativity is essential and expand the results to leavable games | [['pursuitevasion', 'games', 'in', 'discrete', 'time', 'are', 'stochastic', 'games', 'with', 'nonnegative', 'daily', 'payoffs', 'with', 'the', 'final', 'payoff', 'being', 'the', 'cumulative', 'sum', 'of', 'payoffs', 'during', 'the', 'game', 'we', 'show', 'that', 'such', 'games', 'admit', 'a', 'value', 'even', 'in', 'the', 'presence', 'of', 'incomplete', 'information', 'and', 'that', 'this', 'value', 'is', 'uniform', 'ie', 'there', 'are', 'epsilonoptimal', 'strategies', 'for', 'both', 'players', 'that', 'are', 'epsilonoptimal', 'in', 'any', 'long', 'enough', 'prefix', 'of', 'the', 'game', 'we', 'give', 'an', 'example', 'to', 'demonstrate', 'that', 'nonnegativity', 'is', 'essential', 'and', 'expand', 'the', 'results', 'to', 'leavable', 'games']] | [-0.11118288781999806, 0.08364608171155222, -0.12061757770263487, 0.10986568183885359, -0.051452266339810544, -0.17486914264521114, 0.07044941439856718, 0.45408802631276624, -0.2588929219148409, -0.2695979818523528, 0.15617119171512944, -0.2785152283347683, -0.16433080430659983, 0.07936644513608405, -0.15689466261724586, -0.00019234068185826879, 0.1024653725311689, 0.08608580645127797, 0.041941432750864344, -0.3354140650883409, 0.31943340298150563, -0.03000039799299873, 0.16484910997067703, 0.054027025392394006, 0.14068449911213032, 0.01839538577967036, 0.005602866146040874, 0.08341696227751212, -0.10534900989287165, 0.034656071871588076, 0.33000604241488524, 0.22085560195975834, 0.4005441818340325, -0.43050282543962015, -0.11411120345453835, 0.23132801708983786, 0.07339644640142294, 0.11440607843299706, -0.0319977568945399, -0.2535282682489466, 0.0965798653167799, -0.14823741235275878, -0.05094200600568136, -0.0728010541966392, 0.0278284922702077, 0.07570899353811035, -0.3747577365993718, -0.007675058750240247, 0.037206647239257526, 0.012837100498102329, -0.08649225759946591, -0.1695451734840502, -0.008834400478704476, 0.18157299344117442, 0.049021505319547874, -0.028941908260565943, 0.07844867046784472, -0.16857556844946503, -0.23789631602940736, 0.37088984933992225, -0.09133417920186472, -0.18124481956302016, 0.11516049570967386, -0.12706406057645556, -0.09681740869411531, 0.13124804874813115, 0.14689100153146334, 0.15255819468322085, -0.08624820680254036, 0.061326678001528814, -0.1398526202933288, 0.19111423855101298, 0.05692016066017526, 0.08133333150791809, 0.15221114816535034, 0.1180943331255773, 0.21970114426940313, 0.10908134586614683, 0.045809376322273394, -0.23433358236618432, -0.3012546910042012, -0.12350498004184093, -0.14291550167318848, 0.04829493199509603, -0.12793948480041617, -0.1775784076501926, 0.3262021455131931, 0.13743625543321725, 0.09584185492713004, 0.18638454049963643, 0.2837589417503756, 0.1383638339991003, -0.011730784400837658, 0.10649544355907926, 0.17336279921015196, 0.05112390876690179, 0.13605451160742912, -0.2147661116503087, 0.16641365386039755, 0.035228896410388434] |
708.2557 | Secure Identification and QKD in the Bounded-Quantum-Storage Model | We consider the problem of secure identification: user U proves to server S
that he knows an agreed (possibly low-entropy) password w, while giving away as
little information on w as possible, namely the adversary can exclude at most
one possible password for each execution of the scheme. We propose a solution
in the bounded-quantum-storage model, where U and S may exchange qubits, and a
dishonest party is assumed to have limited quantum memory. No other restriction
is posed upon the adversary.
An improved version of the proposed identification scheme is also secure
against a man-in-the-middle attack, but requires U and S to additionally share
a high-entropy key k. However, security is still guaranteed if one party loses
k to the attacker but notices the loss. In both versions of the scheme, the
honest participants need no quantum memory, and noise and imperfect quantum
sources can be tolerated. The schemes compose sequentially, and w and k can
securely be re-used.
A small modification to the identification scheme results in a
quantum-key-distribution (QKD) scheme, secure in the bounded-quantum-storage
model, with the same re-usability properties of the keys, and without assuming
authenticated channels. This is in sharp contrast to known QKD schemes (with
unbounded adversary) without authenticated channels, where authentication keys
must be updated, and unsuccessful executions can cause the parties to run out
of keys.
| quant-ph | we consider the problem of secure identification user u proves to server s that he knows an agreed possibly lowentropy password w while giving away as little information on w as possible namely the adversary can exclude at most one possible password for each execution of the scheme we propose a solution in the boundedquantumstorage model where u and s may exchange qubits and a dishonest party is assumed to have limited quantum memory no other restriction is posed upon the adversary an improved version of the proposed identification scheme is also secure against a maninthemiddle attack but requires u and s to additionally share a highentropy key k however security is still guaranteed if one party loses k to the attacker but notices the loss in both versions of the scheme the honest participants need no quantum memory and noise and imperfect quantum sources can be tolerated the schemes compose sequentially and w and k can securely be reused a small modification to the identification scheme results in a quantumkeydistribution qkd scheme secure in the boundedquantumstorage model with the same reusability properties of the keys and without assuming authenticated channels this is in sharp contrast to known qkd schemes with unbounded adversary without authenticated channels where authentication keys must be updated and unsuccessful executions can cause the parties to run out of keys | [['we', 'consider', 'the', 'problem', 'of', 'secure', 'identification', 'user', 'u', 'proves', 'to', 'server', 's', 'that', 'he', 'knows', 'an', 'agreed', 'possibly', 'lowentropy', 'password', 'w', 'while', 'giving', 'away', 'as', 'little', 'information', 'on', 'w', 'as', 'possible', 'namely', 'the', 'adversary', 'can', 'exclude', 'at', 'most', 'one', 'possible', 'password', 'for', 'each', 'execution', 'of', 'the', 'scheme', 'we', 'propose', 'a', 'solution', 'in', 'the', 'boundedquantumstorage', 'model', 'where', 'u', 'and', 's', 'may', 'exchange', 'qubits', 'and', 'a', 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'secure', 'in', 'the', 'boundedquantumstorage', 'model', 'with', 'the', 'same', 'reusability', 'properties', 'of', 'the', 'keys', 'and', 'without', 'assuming', 'authenticated', 'channels', 'this', 'is', 'in', 'sharp', 'contrast', 'to', 'known', 'qkd', 'schemes', 'with', 'unbounded', 'adversary', 'without', 'authenticated', 'channels', 'where', 'authentication', 'keys', 'must', 'be', 'updated', 'and', 'unsuccessful', 'executions', 'can', 'cause', 'the', 'parties', 'to', 'run', 'out', 'of', 'keys']] | [-0.20442964815343398, 0.052135229003787184, -0.08009215988671972, 0.04869104036021911, -0.06965126203223397, -0.35354325176532647, 0.15710644496617274, 0.3723124013881066, -0.2875873444494833, -0.30749741150066257, 0.10511602139065092, -0.2798814158616421, -0.022661124886716216, 0.15443829557001923, -0.15944612259045243, 0.0761573419918672, 0.04200516724709554, 0.05584806481160091, 0.00427958844738896, -0.3359130946617889, 0.2852877607978631, 0.040730224405186685, 0.2461917353253479, 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708.2558 | 1+1+2 gravitational perturbations on LRS class II space-times: GEM
vector harmonic amplitudes | This is the second in a series of papers which considers first-order
gauge-invariant and covariant gravitational perturbations to locally
rotationally symmetric (LRS) class II space-times. This paper shows how to
decouple a complex combination of the gravito-electromagnetic (GEM) 2-vectors
with the 2-tensors describing the shear of the 2/3-sheets. An arbitrary
harmonic expansion is then used along with an eigen-vector/value analysis of
the first-order GEM system, analogous to the first paper in this series. This
results in four real decoupled equations governing four real combinations of
the harmonic amplitudes of the GEM 2-vectors and the (2/3-sheet) shear
2-tensors. Finally, these are categorized into polar and axial perturbations.
| gr-qc | this is the second in a series of papers which considers firstorder gaugeinvariant and covariant gravitational perturbations to locally rotationally symmetric lrs class ii spacetimes this paper shows how to decouple a complex combination of the gravitoelectromagnetic gem 2vectors with the 2tensors describing the shear of the 23sheets an arbitrary harmonic expansion is then used along with an eigenvectorvalue analysis of the firstorder gem system analogous to the first paper in this series this results in four real decoupled equations governing four real combinations of the harmonic amplitudes of the gem 2vectors and the 23sheet shear 2tensors finally these are categorized into polar and axial perturbations | [['this', 'is', 'the', 'second', 'in', 'a', 'series', 'of', 'papers', 'which', 'considers', 'firstorder', 'gaugeinvariant', 'and', 'covariant', 'gravitational', 'perturbations', 'to', 'locally', 'rotationally', 'symmetric', 'lrs', 'class', 'ii', 'spacetimes', 'this', 'paper', 'shows', 'how', 'to', 'decouple', 'a', 'complex', 'combination', 'of', 'the', 'gravitoelectromagnetic', 'gem', '2vectors', 'with', 'the', '2tensors', 'describing', 'the', 'shear', 'of', 'the', '23sheets', 'an', 'arbitrary', 'harmonic', 'expansion', 'is', 'then', 'used', 'along', 'with', 'an', 'eigenvectorvalue', 'analysis', 'of', 'the', 'firstorder', 'gem', 'system', 'analogous', 'to', 'the', 'first', 'paper', 'in', 'this', 'series', 'this', 'results', 'in', 'four', 'real', 'decoupled', 'equations', 'governing', 'four', 'real', 'combinations', 'of', 'the', 'harmonic', 'amplitudes', 'of', 'the', 'gem', '2vectors', 'and', 'the', '23sheet', 'shear', '2tensors', 'finally', 'these', 'are', 'categorized', 'into', 'polar', 'and', 'axial', 'perturbations']] | [-0.1723799501659882, 0.11101595983073088, -0.0674251236781044, -0.00010665044758143355, -0.05838923769306789, -0.08401827698627722, -0.09051768873022525, 0.30945010726493827, -0.27272450079399985, -0.19543699232309839, 0.08848017237479211, -0.24025125067355563, -0.16870768119137988, 0.1578209999659397, -0.02375764350262154, 0.0479001918473073, -0.008822309903832135, 0.038511333537278966, -0.12441600602373336, -0.2563693475145485, 0.3884865207579529, 0.01453946730194306, 0.24078991788538914, -0.048380798217162346, 0.10032753591895899, -0.023198513040608427, -0.09047802888507982, 0.03794909936366874, -0.10492322487232175, 0.1269528256747329, 0.22087143526217015, 0.0709555501489023, 0.20715951152796885, -0.41762352340574405, -0.162547007501487, 0.05021570669487119, 0.12828667266113522, 0.1106159653259188, 0.0009133872820191013, -0.2753103982150844, 0.0772264407296638, -0.1827920685020429, -0.1363291457494341, -0.09499662737949814, 0.035965975636200416, 0.043181597399841815, -0.28887247482260453, 0.07839796452520831, 0.09189882269581255, 0.021257074231912552, -0.1251432047704759, -0.05824145864699832, -0.0025258920860739007, 0.0734796182171089, 0.08495130593599119, 0.03272283355732566, 0.08680565075189309, -0.06707651350755715, -0.07516813039942419, 0.37539561651421044, -0.130564022045786, -0.250281924689279, 0.17107739860137688, -0.17421157161244055, -0.170579845384125, 0.11975559878877355, 0.18647095661393356, 0.16703885870090532, -0.19611263494414177, 0.09679417202567898, 0.0017800379580664404, 0.1379217721230251, 0.10856178002793668, -0.030186542296257703, 0.21477929979237248, 0.07474730344199874, 0.025313359233143838, 0.1720494859811208, -0.06215148294362628, -0.09559425379509034, -0.38765837396811514, -0.1819990642868362, -0.11612926717413571, 0.028804420286708158, -0.0904374180122299, -0.22130250631497034, 0.43253025723603167, 0.060367455597496726, 0.1404340339924019, 0.03988712083082646, 0.2954079124859525, 0.13898564470836947, 0.03296833536904124, 0.053861643847765275, 0.25924511562164837, 0.19150838431296419, 0.1275575589512936, -0.20522609168411576, -0.0524154967736923, 0.09025919744835316] |
708.2559 | 1+1+2 gravitational perturbations on LRS class II space-times: GEM
scalar harmonic amplitudes | This is the third in a series of papers which considers first-order
gauge-invariant and covariant gravitational perturbations to locally
rotationally symmetric (LRS) class II space-times. In this paper we complete
our analysis of the first-order gravito-electromagnetic (GEM) system by showing
how to derive three decoupled equations governing the GEM scalar fields. One of
these is for the gravito-magnetic scalar, whereas another two arise from the
2-gradient of the gravito-electric scalar.
| gr-qc | this is the third in a series of papers which considers firstorder gaugeinvariant and covariant gravitational perturbations to locally rotationally symmetric lrs class ii spacetimes in this paper we complete our analysis of the firstorder gravitoelectromagnetic gem system by showing how to derive three decoupled equations governing the gem scalar fields one of these is for the gravitomagnetic scalar whereas another two arise from the 2gradient of the gravitoelectric scalar | [['this', 'is', 'the', 'third', 'in', 'a', 'series', 'of', 'papers', 'which', 'considers', 'firstorder', 'gaugeinvariant', 'and', 'covariant', 'gravitational', 'perturbations', 'to', 'locally', 'rotationally', 'symmetric', 'lrs', 'class', 'ii', 'spacetimes', 'in', 'this', 'paper', 'we', 'complete', 'our', 'analysis', 'of', 'the', 'firstorder', 'gravitoelectromagnetic', 'gem', 'system', 'by', 'showing', 'how', 'to', 'derive', 'three', 'decoupled', 'equations', 'governing', 'the', 'gem', 'scalar', 'fields', 'one', 'of', 'these', 'is', 'for', 'the', 'gravitomagnetic', 'scalar', 'whereas', 'another', 'two', 'arise', 'from', 'the', '2gradient', 'of', 'the', 'gravitoelectric', 'scalar']] | [-0.19282592753407315, 0.11758898729053528, -0.05582647379217805, 0.045737904084819384, -0.09401719458401203, -0.13613615118210082, -0.09682118896550189, 0.2592999456261379, -0.23417447390966117, -0.23759784236334372, 0.05973954929335826, -0.24230162270259167, -0.15426377676751302, 0.12706268954333727, -0.020061169454045055, 0.010516113601624966, -0.032142373226225325, 0.05185439306365299, -0.11951452159606245, -0.2531820291120127, 0.44231764011193014, -0.01290677636321904, 0.1829144127558971, -0.04933223352376102, 0.11080479712657415, -0.02940249351946556, -0.08660293772033807, 0.02713813899975756, -0.0927425370403174, 0.10206842531814524, 0.2060504587090058, 0.09803643464313253, 0.22763548248811907, -0.39316440562623134, -0.19060149813151878, 0.06846090817851001, 0.10724654606125061, 0.15619005756688883, -0.032303558001159756, -0.30768982423604396, 0.09595166901261479, -0.20065618095163634, -0.13406325881436898, -0.06980779296313615, 0.023863697930684557, -0.0038581489571842594, -0.2907733044222645, 0.09883976586001075, 0.11543409183007274, -0.005350427729064139, -0.1084907675580378, -0.057930244394389076, -0.007986436358423553, 0.04369497057590364, 0.11496902906767809, 0.01765410934129487, 0.10980648084449163, -0.08360974570952248, -0.07909408120431707, 0.3836930371496988, -0.16232184787361842, -0.2488235804265824, 0.14610335886802361, -0.18184803638175345, -0.1687825977721292, 0.10765951396087589, 0.1653298755864734, 0.2169371669592363, -0.2367577788055591, 0.1386409688705538, 0.014822409461265888, 0.13185392726934853, 0.09700854948681334, 0.003021813071994246, 0.25917509138800093, 0.04728761355163179, 0.04044514624536901, 0.16053603162341143, -0.036581843038615974, -0.15726913326416517, -0.4157570386710374, -0.17800941658577463, -0.11046935497459186, 0.057609176561843764, -0.0836421114970859, -0.20410836959068757, 0.4268776162702968, 0.09602764200257219, 0.06979638120442953, 0.022723211463122374, 0.2812249192401119, 0.13131048998026096, 0.03902062021897755, 0.07124797867584055, 0.3227448217921715, 0.19838583507183669, 0.1523142381608351, -0.2052700506300544, -0.06861681176646464, 0.10679657379354256] |
708.256 | Application of quantum algorithms to the study of permutations and group
automorphisms | We discuss three applications of efficient quantum algorithms to determining
properties of permutations and group automorphisms. The first uses the
Bernstein-Vazirani algorithm to determine an unknown homomorphism from
$Z_{p-1}^{m}$ to $Aut(Z_{p})$ where $p$ is prime. The remaining two make use of
modifications of the Grover search algorithm. The first finds the fixed point
of a permutation or an automorphism (assuming it has only one besides the
identity). It can be generalized to find cycles of a specified size for
permutations or orbits of a specified size for automorphisms. The second finds
which of a set of permutations or automorphisms maps one particular element of
a set or group onto another. This has relevance to the conjugacy problem for
groups. We show how two of these algorithms can be implemented via programmable
quantum processors. This approach opens new perspectives in quantum information
processing, wherein both the data and the programs are represented by states of
quantum registers. In particular, quantum programs that specify control over
data can be treated using methods of quantum information theory.
| quant-ph | we discuss three applications of efficient quantum algorithms to determining properties of permutations and group automorphisms the first uses the bernsteinvazirani algorithm to determine an unknown homomorphism from z_p1m to autz_p where p is prime the remaining two make use of modifications of the grover search algorithm the first finds the fixed point of a permutation or an automorphism assuming it has only one besides the identity it can be generalized to find cycles of a specified size for permutations or orbits of a specified size for automorphisms the second finds which of a set of permutations or automorphisms maps one particular element of a set or group onto another this has relevance to the conjugacy problem for groups we show how two of these algorithms can be implemented via programmable quantum processors this approach opens new perspectives in quantum information processing wherein both the data and the programs are represented by states of quantum registers in particular quantum programs that specify control over data can be treated using methods of quantum information theory | [['we', 'discuss', 'three', 'applications', 'of', 'efficient', 'quantum', 'algorithms', 'to', 'determining', 'properties', 'of', 'permutations', 'and', 'group', 'automorphisms', 'the', 'first', 'uses', 'the', 'bernsteinvazirani', 'algorithm', 'to', 'determine', 'an', 'unknown', 'homomorphism', 'from', 'z_p1m', 'to', 'autz_p', 'where', 'p', 'is', 'prime', 'the', 'remaining', 'two', 'make', 'use', 'of', 'modifications', 'of', 'the', 'grover', 'search', 'algorithm', 'the', 'first', 'finds', 'the', 'fixed', 'point', 'of', 'a', 'permutation', 'or', 'an', 'automorphism', 'assuming', 'it', 'has', 'only', 'one', 'besides', 'the', 'identity', 'it', 'can', 'be', 'generalized', 'to', 'find', 'cycles', 'of', 'a', 'specified', 'size', 'for', 'permutations', 'or', 'orbits', 'of', 'a', 'specified', 'size', 'for', 'automorphisms', 'the', 'second', 'finds', 'which', 'of', 'a', 'set', 'of', 'permutations', 'or', 'automorphisms', 'maps', 'one', 'particular', 'element', 'of', 'a', 'set', 'or', 'group', 'onto', 'another', 'this', 'has', 'relevance', 'to', 'the', 'conjugacy', 'problem', 'for', 'groups', 'we', 'show', 'how', 'two', 'of', 'these', 'algorithms', 'can', 'be', 'implemented', 'via', 'programmable', 'quantum', 'processors', 'this', 'approach', 'opens', 'new', 'perspectives', 'in', 'quantum', 'information', 'processing', 'wherein', 'both', 'the', 'data', 'and', 'the', 'programs', 'are', 'represented', 'by', 'states', 'of', 'quantum', 'registers', 'in', 'particular', 'quantum', 'programs', 'that', 'specify', 'control', 'over', 'data', 'can', 'be', 'treated', 'using', 'methods', 'of', 'quantum', 'information', 'theory']] | [-0.1512723804727673, 0.10248101978758377, -0.10922071121654711, 0.028929427785252027, -0.0766662887478962, -0.15792860204711295, 0.06422794158611078, 0.3500320708195051, -0.3510218957374089, -0.3170402985997498, 0.11140094822283488, -0.257481180762244, -0.12268752910651613, 0.22078943973120171, -0.07992792490945566, 0.0647227696771192, 0.04471842611025729, 0.09773770771273628, -0.09086280812520864, -0.2719887491528129, 0.3131045533728591, -0.009159655807686016, 0.2010981569954649, -0.003640094263002623, 0.10605130126282876, 0.020933620512572138, -0.02523891119351394, 0.0014815245278526185, -0.08873825512582276, 0.10525471537047726, 0.28867931566593713, 0.1859126935823317, 0.26262680133317357, -0.4073218876647568, -0.1569954974408976, 0.1561928529503517, 0.14251409015390848, 0.13242466486367765, -0.06120291478975221, -0.269115214583973, 0.10616359735827563, -0.14632411408346407, -0.09689505129976761, -0.08017504722053229, 0.015041028460769285, -0.012927769075505175, -0.2606830680201393, -0.041409371439692415, 0.06671493308791934, 0.05724379218854876, 0.013105192677886767, -0.08739655641135001, 0.017001766938889443, 0.16127583006840893, -0.03306861402504796, 0.014324848488687949, 0.1326855225678057, -0.08674246175918555, -0.21719542719142207, 0.42012058148637066, 0.0017491236848886623, -0.20365639173068367, 0.13595081311731794, -0.10230432535646224, -0.1961873107871344, 0.09352436179544257, 0.17193077944035015, 0.13824835812759606, -0.12129107142018891, 0.11816723325200444, -0.0716821936793019, 0.16743996585424864, 0.06707253862378122, 0.006893089401189151, 0.1744566904489211, 0.12233439514814161, 0.09830514715204752, 0.17694725367568195, -0.022593806616875323, -0.07435982540076555, -0.29351655372721686, -0.18527962926363703, -0.18236334934873982, 0.035730023459574684, -0.08366830651577276, -0.17332469936877185, 0.4088650964211326, 0.15675022891725326, 0.16687971653638753, 0.04910376559209274, 0.2728508112107425, 0.08428545012886685, 0.10089095026731144, 0.10464094561080686, 0.1338668933793426, 0.14853827147013615, -0.03456557760905843, -0.19064793169385413, 0.04439291272713088, 0.10012293219306441] |
708.2561 | Mean free paths and in-medium scattering cross sections of energetic
nucleons in neutron-rich nucleonic matter within the relativistic impulse
approximation | The mean free paths and in-medium scattering cross sections of energetic
nucleons in neutron-rich nucleonic matter are investigated using the nucleon
optical potential obtained within the relativistic impulse approximation with
the empirical nucleon-nucleon scattering amplitudes and the nuclear densities
obtained in the relativistic mean field model. It is found that the
isospin-splitting of nucleon mean free paths, sensitive to the imaginary part
of the symmetry potential, changes its sign at certain high kinetic energy. The
in-medium nucleon-nucleon cross sections are analytically and numerically
demonstrated to be essentially independent of the isospin asymmetry of the
medium and increase linearly with density in the high energy region where the
relativistic impulse approximation is applicable.
| nucl-th nucl-ex | the mean free paths and inmedium scattering cross sections of energetic nucleons in neutronrich nucleonic matter are investigated using the nucleon optical potential obtained within the relativistic impulse approximation with the empirical nucleonnucleon scattering amplitudes and the nuclear densities obtained in the relativistic mean field model it is found that the isospinsplitting of nucleon mean free paths sensitive to the imaginary part of the symmetry potential changes its sign at certain high kinetic energy the inmedium nucleonnucleon cross sections are analytically and numerically demonstrated to be essentially independent of the isospin asymmetry of the medium and increase linearly with density in the high energy region where the relativistic impulse approximation is applicable | [['the', 'mean', 'free', 'paths', 'and', 'inmedium', 'scattering', 'cross', 'sections', 'of', 'energetic', 'nucleons', 'in', 'neutronrich', 'nucleonic', 'matter', 'are', 'investigated', 'using', 'the', 'nucleon', 'optical', 'potential', 'obtained', 'within', 'the', 'relativistic', 'impulse', 'approximation', 'with', 'the', 'empirical', 'nucleonnucleon', 'scattering', 'amplitudes', 'and', 'the', 'nuclear', 'densities', 'obtained', 'in', 'the', 'relativistic', 'mean', 'field', 'model', 'it', 'is', 'found', 'that', 'the', 'isospinsplitting', 'of', 'nucleon', 'mean', 'free', 'paths', 'sensitive', 'to', 'the', 'imaginary', 'part', 'of', 'the', 'symmetry', 'potential', 'changes', 'its', 'sign', 'at', 'certain', 'high', 'kinetic', 'energy', 'the', 'inmedium', 'nucleonnucleon', 'cross', 'sections', 'are', 'analytically', 'and', 'numerically', 'demonstrated', 'to', 'be', 'essentially', 'independent', 'of', 'the', 'isospin', 'asymmetry', 'of', 'the', 'medium', 'and', 'increase', 'linearly', 'with', 'density', 'in', 'the', 'high', 'energy', 'region', 'where', 'the', 'relativistic', 'impulse', 'approximation', 'is', 'applicable']] | [-0.08650379251672088, 0.2343151039177818, -0.1269268736484394, 0.14389398058951233, 0.004058826918480918, -0.044066772426179214, -0.00805181563815235, 0.3775214075576514, -0.2247658490752136, -0.2779102147282434, -0.06573523535189452, -0.3205268477187409, -0.02112010889686644, 0.09261509473227696, 0.1102362911039693, 0.08987157404304266, 0.032093714417507205, 0.09505929190865052, -0.06440099965506565, -0.18483942382902438, 0.32468556682384325, 0.08898414775155418, 0.22144698407958327, 0.1884753699133788, 0.1023722337808327, 0.10021750450999077, -0.03146630612484712, -0.005606316329379167, -0.10185892467760434, 0.07382738384389345, 0.25250487490432405, -0.021575299030895882, 0.14172091532132722, -0.4297517150740272, -0.21266040796347493, 0.09905106647472296, 0.13473665519684022, 0.12275435170574513, -0.043741848264679514, -0.27482875825704206, 0.020608903915022632, -0.22476578361654123, -0.19407575277312258, -0.06614287771351103, 0.0382550357764038, 0.0954169359818999, -0.2598158549517393, 0.1295404550453116, -0.08860250303821106, 0.015694688199021454, -0.11741790372616379, -0.20953562438704207, -0.04723785443223148, 0.007156477230767321, 0.10864178845502336, 0.05574773885018658, 0.21222479997439742, -0.1823812408090037, -0.020484617628556277, 0.43201131351816, -0.0324095666500008, -0.16976732253013843, 0.08517950927489437, -0.18253622539175143, -0.038395746964462366, 0.23859671447384503, 0.17272827355191112, 0.0977297823077866, -0.17601563463020803, 0.10179120461647731, -0.0005206299548652689, 0.14277001488621213, 0.07667871711185269, 0.04374702612819549, 0.13718419416233832, 0.13696119815410515, -0.008135725344930376, 0.04010181438206928, -0.13204974675733996, -0.14106363084283657, -0.36519507255538236, -0.03883809865718441, -0.16650075707418313, 0.023830381928876574, -0.10907032837141221, -0.11353722477049034, 0.36236341235261144, 0.0753705302985119, 0.1631215611268999, 0.006893254375816988, 0.33230475831909906, 0.19537231428798155, 0.05301354635490237, 0.0976886481096569, 0.3306821851708394, 0.25057536038470324, 0.09382197275200659, -0.3173156225051831, 0.02852927685931458, 0.04053176070738118] |
708.2562 | R-diagonal dilation semigroups | This paper addresses extensions of the complex Ornstein-Uhlenbeck semigroup
to operator algebras in free probability theory. If $a_1,...,a_k$ are
$\ast$-free $\mathscr{R}$-diagonal operators in a $\mathrm{II}_1$ factor, then
$D_t(a_{i_1}... a_{i_n}) = e^{-nt} a_{i_1}... a_{i_n}$ defines a dilation
semigroup on the non-self-adjoint operator algebra generated by $a_1,...,a_k$.
We show that $D_t$ extends (in two different ways) to a semigroup of completely
positive maps on the von Neumann algebra generated by $a_1,...,a_k$. Moreover,
we show that $D_t$ satisfies an optimal ultracontractive property: $\|D_t\colon
L^2\to L^\infty\| \sim t^{-1}$ for small $t>0$.
| math.FA math.OA | this paper addresses extensions of the complex ornsteinuhlenbeck semigroup to operator algebras in free probability theory if a_1a_k are astfree mathscrrdiagonal operators in a mathrmii_1 factor then d_ta_i_1 a_i_n ent a_i_1 a_i_n defines a dilation semigroup on the nonselfadjoint operator algebra generated by a_1a_k we show that d_t extends in two different ways to a semigroup of completely positive maps on the von neumann algebra generated by a_1a_k moreover we show that d_t satisfies an optimal ultracontractive property d_tcolon l2to linfty sim t1 for small t0 | [['this', 'paper', 'addresses', 'extensions', 'of', 'the', 'complex', 'ornsteinuhlenbeck', 'semigroup', 'to', 'operator', 'algebras', 'in', 'free', 'probability', 'theory', 'if', 'a_1a_k', 'are', 'astfree', 'mathscrrdiagonal', 'operators', 'in', 'a', 'mathrmii_1', 'factor', 'then', 'd_ta_i_1', 'a_i_n', 'ent', 'a_i_1', 'a_i_n', 'defines', 'a', 'dilation', 'semigroup', 'on', 'the', 'nonselfadjoint', 'operator', 'algebra', 'generated', 'by', 'a_1a_k', 'we', 'show', 'that', 'd_t', 'extends', 'in', 'two', 'different', 'ways', 'to', 'a', 'semigroup', 'of', 'completely', 'positive', 'maps', 'on', 'the', 'von', 'neumann', 'algebra', 'generated', 'by', 'a_1a_k', 'moreover', 'we', 'show', 'that', 'd_t', 'satisfies', 'an', 'optimal', 'ultracontractive', 'property', 'd_tcolon', 'l2to', 'linfty', 'sim', 't1', 'for', 'small', 't0']] | [-0.1255878993815938, 0.18921451592105756, -0.025092208039383463, 0.07271282471871625, -0.06957943744692997, -0.16361013734368263, -0.04854341977373639, 0.34965045086142643, -0.39879265078056003, -0.07580417782114243, 0.13037681951112814, -0.35122911788431216, -0.12416376547175056, 0.1970213170013862, -0.15107728473060292, 0.0315277926037433, 0.08025206225337805, 0.10563262699194896, -0.10822471051281433, -0.1814269205270749, 0.435643540310133, -0.05320771287747279, 0.16568379413428497, 0.060777107569860454, 0.131997678992281, -0.015616644952837148, -0.009166517214458665, 0.0034042194048747604, -0.20119613925958724, 0.03833164213754145, 0.2679607400233731, 0.12188543638007508, 0.28266435121128586, -0.3756355955782864, -0.1180204008648425, 0.19683135916007521, 0.13672723405833506, -0.047741711191419095, -0.01594609219615382, -0.28385532012692205, 0.13402831281914754, -0.19951130638335957, -0.0966291370295724, -0.06972907814714643, 0.08667017662765482, -0.046705351550316, -0.35708055422169926, 0.07551503837407555, 0.15381091738832586, 0.07625453797295506, -0.08893796665892925, -0.08435378761755095, -0.0390493327429817, 0.04438616235935946, -0.044906262032411715, 0.009199450958094754, 0.11844005396612632, 0.005690445723931914, -0.1216846310812405, 0.2649878166776932, -0.08402952308088173, -0.2497131459782889, 0.0773403909040132, -0.24404830732785257, -0.14493157480624907, 0.037273205138374996, 0.024991171756460342, 0.11800700297326218, -0.09971417419980337, 0.2426676778582695, -0.11906484184487734, 0.10693923774876712, 0.09155407052970042, 0.00831806458486819, 0.01121401632014938, 0.047509679978966345, 0.17307771600920846, 0.13155785509396667, 0.12638440837991644, -0.0187173161805136, -0.3572054019335795, -0.13980463116119304, -0.16723450719390387, 0.1587689476587844, -0.13523598767840017, -0.16588444573183855, 0.37040401354754043, 0.1398200270558857, 0.19709282360373087, 0.12013713093359529, 0.1739616597324242, 0.14580954984980232, 0.07041717414100321, 0.11955978689186367, 0.0637550373636416, 0.19517592837125708, 0.031284349568096205, -0.20229027405047767, -0.02852374860258014, 0.2438944488545351] |
708.2563 | Dynamics of the Langevin model subjected to colored noise:
Functional-integral method | We have discussed the dynamics of Langevin model subjected to colored noise,
by using the functional-integral method (FIM) combined with equations of motion
for mean and variance of the state variable. Two sets of colored noise have
been investigated: (a) one additive and one multiplicative colored noise, and
(b) one additive and two multiplicative colored noise. The case (b) is examined
with the relevance to a recent controversy on the stationary subthreshold
voltage distribution of an integrate-and-fire model including stochastic
excitatory and inhibitory synapses and a noisy input. We have studied the
stationary probability distribution and dynamical responses to time-dependent
(pulse and sinusoidal) inputs of the linear Langevin model. Model calculations
have shown that results of the FIM are in good agreement with those of direct
simulations (DSs). A comparison is made among various approximate analytic
solutions such as the universal colored noise approximation (UCNA). It has been
pointed out that dynamical responses to pulse and sinusoidal inputs calculated
by the UCNA are rather different from those of DS and the FIM, although they
yield the same stationary distribution.
| cond-mat.stat-mech cond-mat.dis-nn | we have discussed the dynamics of langevin model subjected to colored noise by using the functionalintegral method fim combined with equations of motion for mean and variance of the state variable two sets of colored noise have been investigated a one additive and one multiplicative colored noise and b one additive and two multiplicative colored noise the case b is examined with the relevance to a recent controversy on the stationary subthreshold voltage distribution of an integrateandfire model including stochastic excitatory and inhibitory synapses and a noisy input we have studied the stationary probability distribution and dynamical responses to timedependent pulse and sinusoidal inputs of the linear langevin model model calculations have shown that results of the fim are in good agreement with those of direct simulations dss a comparison is made among various approximate analytic solutions such as the universal colored noise approximation ucna it has been pointed out that dynamical responses to pulse and sinusoidal inputs calculated by the ucna are rather different from those of ds and the fim although they yield the same stationary distribution | [['we', 'have', 'discussed', 'the', 'dynamics', 'of', 'langevin', 'model', 'subjected', 'to', 'colored', 'noise', 'by', 'using', 'the', 'functionalintegral', 'method', 'fim', 'combined', 'with', 'equations', 'of', 'motion', 'for', 'mean', 'and', 'variance', 'of', 'the', 'state', 'variable', 'two', 'sets', 'of', 'colored', 'noise', 'have', 'been', 'investigated', 'a', 'one', 'additive', 'and', 'one', 'multiplicative', 'colored', 'noise', 'and', 'b', 'one', 'additive', 'and', 'two', 'multiplicative', 'colored', 'noise', 'the', 'case', 'b', 'is', 'examined', 'with', 'the', 'relevance', 'to', 'a', 'recent', 'controversy', 'on', 'the', 'stationary', 'subthreshold', 'voltage', 'distribution', 'of', 'an', 'integrateandfire', 'model', 'including', 'stochastic', 'excitatory', 'and', 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708.2564 | On the sum of the series formed from the prime numbers where the prime
numbers of the form $4n-1$ have a positive sign and those of the form $4n+1$
a negative sign | This is an English translation of the Latin original "De summa seriei ex
numeris primis formatae
${1/3}-{1/5}+{1/7}+{1/11}-{1/13}-{1/17}+{1/19}+{1/23}-{1/29}+{1/31}-$ etc. ubi
numeri primi formae $4n-1$ habent signum positivum formae autem $4n+1$ signum
negativum" (1775). E596 in the Enestrom index.
Let $\chi$ be the nontrivial character modulo 4. Euler wants to know what
$\sum_p \chi(p)/p$ is, either an exact expression or an approximation. He looks
for analogies to the harmonic series and the series of reciprocals of the
primes.
Another reason he is interested in this is that if this series has a finite
value (which is does, the best approximation Euler gets is 0.3349816 in section
27) then there are infinitely many primes congruent to 1 mod 4 and infinitely
many primes congruent to 3 mod 4.
In section 15 Euler gives the Euler product for the L(chi,1).
As a modern mathematical appendix appendix, I have written a proof following
Davenport that the series $\sum_p \frac{\chi(p)}{p}$ converges. This involves
applications of summation by parts, and uses Chebyshev's estimate for the
second Chebyshev function (summing the von Mangoldt function).
| math.HO math.NT | this is an english translation of the latin original de summa seriei ex numeris primis formatae 131517111113117119123129131 etc ubi numeri primi formae 4n1 habent signum positivum formae autem 4n1 signum negativum 1775 e596 in the enestrom index let chi be the nontrivial character modulo 4 euler wants to know what sum_p chipp is either an exact expression or an approximation he looks for analogies to the harmonic series and the series of reciprocals of the primes another reason he is interested in this is that if this series has a finite value which is does the best approximation euler gets is 03349816 in section 27 then there are infinitely many primes congruent to 1 mod 4 and infinitely many primes congruent to 3 mod 4 in section 15 euler gives the euler product for the lchi1 as a modern mathematical appendix appendix i have written a proof following davenport that the series sum_p fracchipp converges this involves applications of summation by parts and uses chebyshevs estimate for the second chebyshev function summing the von mangoldt function | [['this', 'is', 'an', 'english', 'translation', 'of', 'the', 'latin', 'original', 'de', 'summa', 'seriei', 'ex', 'numeris', 'primis', 'formatae', '131517111113117119123129131', 'etc', 'ubi', 'numeri', 'primi', 'formae', '4n1', 'habent', 'signum', 'positivum', 'formae', 'autem', '4n1', 'signum', 'negativum', '1775', 'e596', 'in', 'the', 'enestrom', 'index', 'let', 'chi', 'be', 'the', 'nontrivial', 'character', 'modulo', '4', 'euler', 'wants', 'to', 'know', 'what', 'sum_p', 'chipp', 'is', 'either', 'an', 'exact', 'expression', 'or', 'an', 'approximation', 'he', 'looks', 'for', 'analogies', 'to', 'the', 'harmonic', 'series', 'and', 'the', 'series', 'of', 'reciprocals', 'of', 'the', 'primes', 'another', 'reason', 'he', 'is', 'interested', 'in', 'this', 'is', 'that', 'if', 'this', 'series', 'has', 'a', 'finite', 'value', 'which', 'is', 'does', 'the', 'best', 'approximation', 'euler', 'gets', 'is', '03349816', 'in', 'section', '27', 'then', 'there', 'are', 'infinitely', 'many', 'primes', 'congruent', 'to', '1', 'mod', '4', 'and', 'infinitely', 'many', 'primes', 'congruent', 'to', '3', 'mod', '4', 'in', 'section', '15', 'euler', 'gives', 'the', 'euler', 'product', 'for', 'the', 'lchi1', 'as', 'a', 'modern', 'mathematical', 'appendix', 'appendix', 'i', 'have', 'written', 'a', 'proof', 'following', 'davenport', 'that', 'the', 'series', 'sum_p', 'fracchipp', 'converges', 'this', 'involves', 'applications', 'of', 'summation', 'by', 'parts', 'and', 'uses', 'chebyshevs', 'estimate', 'for', 'the', 'second', 'chebyshev', 'function', 'summing', 'the', 'von', 'mangoldt', 'function']] | [-0.15660946234711445, 0.077404230529919, -0.13197980672266568, 0.08470867166543031, -0.07329962003277615, -0.15780215782870072, -0.02320813258411363, 0.27028331776964476, -0.28597084228531455, -0.24731098808988464, 0.08577532107301522, -0.34059628829418215, -0.13292103855528695, 0.17700774889381138, -0.13568646865314804, 0.014988046950020362, 0.021675585336924996, 0.09234482553802081, -0.0323136603430612, -0.3249923375900835, 0.2832185821591338, -0.03266873491811566, 0.1801410913503787, 0.030785446593654342, 0.0920426012342432, 0.017083284273394384, -0.004410864847886842, -0.08272617948387051, -0.13223652948445305, 0.08474403643922415, 0.3030704525735928, 0.10817903804709203, 0.3057381132210139, -0.37397377686575056, -0.0689633146423148, 0.13677432351978497, 0.1694886496203253, -0.01750512823709869, 0.03815693520882633, -0.19066113120352385, 0.10761024690689283, -0.19144347431865755, -0.12323219550016802, -0.05178437929789652, 0.12810352145170328, 0.035534590101451616, -0.2779394503115327, 0.03300854060216807, 0.11548678348772227, 0.10910963820642791, -0.008779786189552396, -0.20265541421249508, 0.07725521951797418, 0.08889178909448674, 0.056259347387822345, 0.08097950537630823, 0.038249865212128496, -0.09444028448197059, -0.08846750446391524, 0.3629610585339833, -0.04514252428634791, -0.2172021877762745, 0.08122989502153359, -0.14602323004874052, -0.14012634196842555, 0.14653603642291274, 0.04052368017437402, 0.09399552314498578, -0.049265388216008434, 0.15964433810040646, -0.10578462430567015, 0.199679643206764, 0.1835983065451728, -0.10810817071178462, 0.09034587703936267, 0.030939843017767997, 0.04177445852183155, 0.11010930533302599, -0.031095842641661875, -0.039247192040784286, -0.32078499081544576, -0.2573011604625208, -0.20557016103848583, 0.15081755691207946, -0.07934121903936102, -0.19111259775818326, 0.3615873569215182, 0.060564016678836194, 0.14092975275416392, 0.09848489899377455, 0.255332425062079, 0.14904759363344056, 0.011924199038548976, 0.0767438221781049, 0.11819960510765667, 0.1314366136379249, 0.06760984683642164, -0.0918452091233121, 0.015222798290778883, 0.1896722130710259] |
708.2565 | Coupling of electron rotation with spin in semiconductors | Account of an intrinsic spin-orbit coupling in the valence bands of common
semiconductors yields the scalar spin-orbit-rotation term in the effective-mass
Hamiltonian of the conduction-band electron. This result is obtained within the
multiband envelope function approximation. Fundamentally, the
spin-orbit-rotation coupling can be described in purely geometric terms as a
consequence of the difference in the Berry phase acquired by the components of
the spin-orbitally mixed Kramers-doublet during its cyclic evolution in the
reciprocal momentum space.
| cond-mat.mes-hall | account of an intrinsic spinorbit coupling in the valence bands of common semiconductors yields the scalar spinorbitrotation term in the effectivemass hamiltonian of the conductionband electron this result is obtained within the multiband envelope function approximation fundamentally the spinorbitrotation coupling can be described in purely geometric terms as a consequence of the difference in the berry phase acquired by the components of the spinorbitally mixed kramersdoublet during its cyclic evolution in the reciprocal momentum space | [['account', 'of', 'an', 'intrinsic', 'spinorbit', 'coupling', 'in', 'the', 'valence', 'bands', 'of', 'common', 'semiconductors', 'yields', 'the', 'scalar', 'spinorbitrotation', 'term', 'in', 'the', 'effectivemass', 'hamiltonian', 'of', 'the', 'conductionband', 'electron', 'this', 'result', 'is', 'obtained', 'within', 'the', 'multiband', 'envelope', 'function', 'approximation', 'fundamentally', 'the', 'spinorbitrotation', 'coupling', 'can', 'be', 'described', 'in', 'purely', 'geometric', 'terms', 'as', 'a', 'consequence', 'of', 'the', 'difference', 'in', 'the', 'berry', 'phase', 'acquired', 'by', 'the', 'components', 'of', 'the', 'spinorbitally', 'mixed', 'kramersdoublet', 'during', 'its', 'cyclic', 'evolution', 'in', 'the', 'reciprocal', 'momentum', 'space']] | [-0.19255719721938172, 0.18841192130498208, -0.08545780364592145, 0.06634851682206823, -0.024539401470166113, -0.055177117503869035, 0.036878153655884996, 0.32339494791813195, -0.3111755988664097, -0.294600349980303, -0.005197621611942951, -0.22530754305060124, -0.14962180249858648, 0.11919297574301406, -0.01903651552210148, -0.04610437268679056, 0.020631452375609014, -0.02993852857293354, -0.13210876751691103, -0.18429505124933915, 0.3233665218576789, 0.01178762448641161, 0.22631559753467123, 0.06398038466674431, 0.0622154740202758, 0.063404152661355, 0.028154668365863875, -0.012926282671590647, -0.09139200993296173, 0.06245010557015323, 0.23965739522181037, -0.03425562782730493, 0.19987802327765772, -0.41893407811100286, -0.2366203736099932, 0.03415376043671535, 0.14518167915391839, 0.09274435551035115, -0.011830715760071244, -0.2768203502702009, -0.04099321039393544, -0.16935658674790627, -0.13972380853697863, -0.05223735714389477, -0.013286605063411925, -0.025614946770171326, -0.24546137565953863, 0.11974795487993914, 0.07279375253064144, 0.04199582657828513, -0.12083685690595303, -0.13652958822462502, -0.09104748136855455, 0.09224246827135277, 0.07406313260435127, 0.05369014834286645, 0.053645279003022656, -0.11096929898808917, -0.08309803673020927, 0.42873627345802057, -0.12876547608175315, -0.18796270285060424, 0.10304299242691034, -0.14108777855936852, -0.03187567075817949, 0.16007478401297703, 0.12399830559216854, 0.08463830674170619, -0.1452658978394336, 0.1362357933282207, -0.0005399884539656341, 0.12718864519976908, 0.011503370973514393, 0.12010352025067227, 0.22302492682097685, 0.1291633927741916, 0.025960987073934422, 0.1227720923537466, -0.09984535176772624, -0.12641664632570204, -0.29349389628946987, -0.1575540401196728, -0.2865214103561205, 0.05115898099676189, -0.13207590990027207, -0.17330640469056866, 0.4616889221813633, 0.05986998712695721, 0.17510730005516154, -0.0452363395500773, 0.2872526787945794, 0.1911119024201374, 0.09024941035830933, 0.017963881888944242, 0.3279515136835269, 0.17112830002184232, 0.08897144610010502, -0.30307264326580075, 0.059457749574600406, 0.07083213589309405] |
708.2566 | Discrete Denoising with Shifts | We introduce S-DUDE, a new algorithm for denoising DMC-corrupted data. The
algorithm, which generalizes the recently introduced DUDE (Discrete Universal
DEnoiser) of Weissman et al., aims to compete with a genie that has access, in
addition to the noisy data, also to the underlying clean data, and can choose
to switch, up to $m$ times, between sliding window denoisers in a way that
minimizes the overall loss. When the underlying data form an individual
sequence, we show that the S-DUDE performs essentially as well as this genie,
provided that $m$ is sub-linear in the size of the data. When the clean data is
emitted by a piecewise stationary process, we show that the S-DUDE achieves the
optimum distribution-dependent performance, provided that the same
sub-linearity condition is imposed on the number of switches. To further
substantiate the universal optimality of the S-DUDE, we show that when the
number of switches is allowed to grow linearly with the size of the data,
\emph{any} (sequence of) scheme(s) fails to compete in the above senses. Using
dynamic programming, we derive an efficient implementation of the S-DUDE, which
has complexity (time and memory) growing only linearly with the data size and
the number of switches $m$. Preliminary experimental results are presented,
suggesting that S-DUDE has the capacity to significantly improve on the
performance attained by the original DUDE in applications where the nature of
the data abruptly changes in time (or space), as is often the case in practice.
| cs.IT math.IT | we introduce sdude a new algorithm for denoising dmccorrupted data the algorithm which generalizes the recently introduced dude discrete universal denoiser of weissman et al aims to compete with a genie that has access in addition to the noisy data also to the underlying clean data and can choose to switch up to m times between sliding window denoisers in a way that minimizes the overall loss when the underlying data form an individual sequence we show that the sdude performs essentially as well as this genie provided that m is sublinear in the size of the data when the clean data is emitted by a piecewise stationary process we show that the sdude achieves the optimum distributiondependent performance provided that the same sublinearity condition is imposed on the number of switches to further substantiate the universal optimality of the sdude we show that when the number of switches is allowed to grow linearly with the size of the data emphany sequence of schemes fails to compete in the above senses using dynamic programming we derive an efficient implementation of the sdude which has complexity time and memory growing only linearly with the data size and the number of switches m preliminary experimental results are presented suggesting that sdude has the capacity to significantly improve on the performance attained by the original dude in applications where the nature of the data abruptly changes in time or space as is often the case in practice | [['we', 'introduce', 'sdude', 'a', 'new', 'algorithm', 'for', 'denoising', 'dmccorrupted', 'data', 'the', 'algorithm', 'which', 'generalizes', 'the', 'recently', 'introduced', 'dude', 'discrete', 'universal', 'denoiser', 'of', 'weissman', 'et', 'al', 'aims', 'to', 'compete', 'with', 'a', 'genie', 'that', 'has', 'access', 'in', 'addition', 'to', 'the', 'noisy', 'data', 'also', 'to', 'the', 'underlying', 'clean', 'data', 'and', 'can', 'choose', 'to', 'switch', 'up', 'to', 'm', 'times', 'between', 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708.2567 | Is there quantum chaos in the prime numbers? | A statistical analysis of the prime numbers indicates possible traces of
quantum chaos. We have computed the nearest neighbor spacing distribution,
number variance, skewness, and excess for sequences of the first N primes for
various values of N. All four statistical measures clearly show a transition
from random matrix statistics at small N toward Poisson statistics at large N.
In addition, the number variance saturates at large lengths as is common for
eigenvalue sequences. This data can be given a physical interpretation if the
primes are thought of as eigenvalues of a quantum system whose classical
dynamics is chaotic at low energy but regular at high energy. We discuss some
difficulties with this interpretation in an attempt to clarify what kind of
physical system might have the primes as its quantum eigenvalues.
| quant-ph | a statistical analysis of the prime numbers indicates possible traces of quantum chaos we have computed the nearest neighbor spacing distribution number variance skewness and excess for sequences of the first n primes for various values of n all four statistical measures clearly show a transition from random matrix statistics at small n toward poisson statistics at large n in addition the number variance saturates at large lengths as is common for eigenvalue sequences this data can be given a physical interpretation if the primes are thought of as eigenvalues of a quantum system whose classical dynamics is chaotic at low energy but regular at high energy we discuss some difficulties with this interpretation in an attempt to clarify what kind of physical system might have the primes as its quantum eigenvalues | [['a', 'statistical', 'analysis', 'of', 'the', 'prime', 'numbers', 'indicates', 'possible', 'traces', 'of', 'quantum', 'chaos', 'we', 'have', 'computed', 'the', 'nearest', 'neighbor', 'spacing', 'distribution', 'number', 'variance', 'skewness', 'and', 'excess', 'for', 'sequences', 'of', 'the', 'first', 'n', 'primes', 'for', 'various', 'values', 'of', 'n', 'all', 'four', 'statistical', 'measures', 'clearly', 'show', 'a', 'transition', 'from', 'random', 'matrix', 'statistics', 'at', 'small', 'n', 'toward', 'poisson', 'statistics', 'at', 'large', 'n', 'in', 'addition', 'the', 'number', 'variance', 'saturates', 'at', 'large', 'lengths', 'as', 'is', 'common', 'for', 'eigenvalue', 'sequences', 'this', 'data', 'can', 'be', 'given', 'a', 'physical', 'interpretation', 'if', 'the', 'primes', 'are', 'thought', 'of', 'as', 'eigenvalues', 'of', 'a', 'quantum', 'system', 'whose', 'classical', 'dynamics', 'is', 'chaotic', 'at', 'low', 'energy', 'but', 'regular', 'at', 'high', 'energy', 'we', 'discuss', 'some', 'difficulties', 'with', 'this', 'interpretation', 'in', 'an', 'attempt', 'to', 'clarify', 'what', 'kind', 'of', 'physical', 'system', 'might', 'have', 'the', 'primes', 'as', 'its', 'quantum', 'eigenvalues']] | [-0.1615292184128934, 0.15959067227749707, -0.09618456464500702, 0.12374719633777259, 0.00212155428060655, -0.12659949611759547, 0.03721058543041264, 0.3084899054868429, -0.28806244968577766, -0.3209237313377812, 0.07400104666576778, -0.317602139636592, -0.11223451063657801, 0.17446863283332664, -0.03749713377218348, 0.0706827981600575, 0.05225678499008416, 0.11832944771881695, -0.02597931851888654, -0.23336742234162308, 0.30558626462394994, 0.05868288209030376, 0.23736609923864968, 0.0077857740971287994, 0.05949437954889921, -0.03317823066291484, 0.019475367195396262, -0.008333492651934537, -0.09540996312121437, 0.06112986803936744, 0.27296751974658534, 0.09814635433157849, 0.30506462164956966, -0.3871938041199676, -0.16462677677698206, 0.17131760104552307, 0.16581750734864423, 0.09440002162150588, -0.0013562222456764148, -0.2132206327056117, 0.11557839843303416, -0.12431422682041585, -0.17944987080144612, -0.07025029283690717, 0.0675591431332357, 0.040453837239042376, -0.25549596255631046, 0.08310624509062053, 0.03859979957059929, 0.11404270156653541, 0.029476161034835968, -0.19284636321809198, 0.032607046159682795, 0.12509734696482844, 0.029683953480950247, -0.04309303545442438, 0.08518740981393917, -0.0975012949237487, -0.11198199428018239, 0.34920001186599786, -0.02080742567142641, -0.17802038592653294, 0.15886775639162146, -0.2093201833812407, -0.18245082423725928, 0.15135898852763188, 0.1349017576836614, 0.05701352263603247, -0.08984431108657384, 0.08058685456048945, -0.04325553344449762, 0.15355541816891424, 0.08561010935668353, 0.08475116803928165, 0.2457676999567246, 0.10550439382275341, 0.039441404356197876, 0.1306927641386265, -0.10903210630358169, -0.09390263447836111, -0.3260037069999133, -0.1417142222529616, -0.2754266341948868, 0.10117141103149731, -0.15337611028603118, -0.17268210377149057, 0.3500368599921013, 0.13961798272750015, 0.25162283819747355, 0.09524434828904993, 0.25566127184058796, 0.13145767156763186, 0.030973323520315302, 0.0600961318423012, 0.14466391521912583, 0.1354407098595843, 0.06761613653295419, -0.18217280892845752, 0.06335481738620508, 0.061068592818849014] |
708.2568 | Spacetime singularity resolution by M-theory fivebranes: calibrated
geometry, Anti-de Sitter solutions and special holonomy metrics | The supergravity description of various configurations of supersymmetric
M-fivebranes wrapped on calibrated cycles of special holonomy manifolds is
studied. The description is provided by solutions of eleven-dimensional
supergravity which interpolate smoothly between a special holonomy manifold and
an event horizon with Anti-de Sitter geometry. For known examples of Anti-de
Sitter solutions, the associated special holonomy metric is derived. One
explicit Anti-de Sitter solution of M-theory is so treated for fivebranes
wrapping each of the following cycles: K\"{a}hler cycles in Calabi-Yau two-,
three- and four-folds; special lagrangian cycles in three- and four-folds;
associative three- and co-associative four-cycles in $G_2$ manifolds; complex
lagrangian four-cycles in $Sp(2)$ manifolds; and Cayley four-cycles in
$Spin(7)$ manifolds. In each case, the associated special holonomy metric is
singular, and is a hyperbolic analogue of a known metric. The analogous known
metrics are respectively: Eguchi-Hanson, the resolved conifold and the
four-fold resolved conifold; the deformed conifold, and the Stenzel four-fold
metric; the Bryant-Salamon-Gibbons-Page-Pope $G_2$ metrics on an $\mathbb{R}^4$
bundle over $S^3$, and an $\mathbb{R}^3$ bundle over $S^4$ or $\mathbb{CP}^2$;
the Calabi hyper-K\"{a}hler metric on $T^*\mathbb{CP}^2$; and the
Bryant-Salamon-Gibbons-Page-Pope $Spin(7)$ metric on an $\mathbb{R}^4$ bundle
over $S^4$. By the AdS/CFT correspondence, a conformal field theory is
associated to each of the new singular special holonomy metrics, and defines
the quantum gravitational physics of the resolution of their singularities.
| hep-th | the supergravity description of various configurations of supersymmetric mfivebranes wrapped on calibrated cycles of special holonomy manifolds is studied the description is provided by solutions of elevendimensional supergravity which interpolate smoothly between a special holonomy manifold and an event horizon with antide sitter geometry for known examples of antide sitter solutions the associated special holonomy metric is derived one explicit antide sitter solution of mtheory is so treated for fivebranes wrapping each of the following cycles kahler cycles in calabiyau two three and fourfolds special lagrangian cycles in three and fourfolds associative three and coassociative fourcycles in g_2 manifolds complex lagrangian fourcycles in sp2 manifolds and cayley fourcycles in spin7 manifolds in each case the associated special holonomy metric is singular and is a hyperbolic analogue of a known metric the analogous known metrics are respectively eguchihanson the resolved conifold and the fourfold resolved conifold the deformed conifold and the stenzel fourfold metric the bryantsalamongibbonspagepope g_2 metrics on an mathbbr4 bundle over s3 and an mathbbr3 bundle over s4 or mathbbcp2 the calabi hyperkahler metric on tmathbbcp2 and the bryantsalamongibbonspagepope spin7 metric on an mathbbr4 bundle over s4 by the adscft correspondence a conformal field theory is associated to each of the new singular special holonomy metrics and defines the quantum gravitational physics of the resolution of their singularities | [['the', 'supergravity', 'description', 'of', 'various', 'configurations', 'of', 'supersymmetric', 'mfivebranes', 'wrapped', 'on', 'calibrated', 'cycles', 'of', 'special', 'holonomy', 'manifolds', 'is', 'studied', 'the', 'description', 'is', 'provided', 'by', 'solutions', 'of', 'elevendimensional', 'supergravity', 'which', 'interpolate', 'smoothly', 'between', 'a', 'special', 'holonomy', 'manifold', 'and', 'an', 'event', 'horizon', 'with', 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708.2569 | Algebraic Compactness OF $\prod M_\alpha / \oplus M_\alpha$ | In this note, we are working within the category $\rmod$ of (unitary, left)
$R$-modules, where $R$ is a {\bf countable} ring. It is well known (see e.g.
Kie{\l}pi\'nski & Simson [5], Theorem 2.2) that the latter condition implies
that the (left) pure global dimension of $R$ is at most 1. Given an infinite
index set $A$, and a family $M_\al\in\rmod$, $\al\in A$ we are concerned with
the conditions as to when the $R$-module $$\prod/\coprod=\prod_{\al\in
A}M_\al/\bigoplus_{\al\in A}M_\al$$ is or is not algebraically compact. There
are a number of special results regarding this question and this note is meant
to be an addition to and a generalization of the set of these results. Whether
the module in the title is algebraically compact or not depends on the numbers
of algebraically compact and non-compact modules among the components $M_\al$.
| math.AC math.GR math.LO math.RA | in this note we are working within the category rmod of unitary left rmodules where r is a bf countable ring it is well known see eg kielpinski simson 5 theorem 22 that the latter condition implies that the left pure global dimension of r is at most 1 given an infinite index set a and a family m_alinrmod alin a we are concerned with the conditions as to when the rmodule prodcoprodprod_alin am_albigoplus_alin am_al is or is not algebraically compact there are a number of special results regarding this question and this note is meant to be an addition to and a generalization of the set of these results whether the module in the title is algebraically compact or not depends on the numbers of algebraically compact and noncompact modules among the components m_al | [['in', 'this', 'note', 'we', 'are', 'working', 'within', 'the', 'category', 'rmod', 'of', 'unitary', 'left', 'rmodules', 'where', 'r', 'is', 'a', 'bf', 'countable', 'ring', 'it', 'is', 'well', 'known', 'see', 'eg', 'kielpinski', 'simson', '5', 'theorem', '22', 'that', 'the', 'latter', 'condition', 'implies', 'that', 'the', 'left', 'pure', 'global', 'dimension', 'of', 'r', 'is', 'at', 'most', '1', 'given', 'an', 'infinite', 'index', 'set', 'a', 'and', 'a', 'family', 'm_alinrmod', 'alin', 'a', 'we', 'are', 'concerned', 'with', 'the', 'conditions', 'as', 'to', 'when', 'the', 'rmodule', 'prodcoprodprod_alin', 'am_albigoplus_alin', 'am_al', 'is', 'or', 'is', 'not', 'algebraically', 'compact', 'there', 'are', 'a', 'number', 'of', 'special', 'results', 'regarding', 'this', 'question', 'and', 'this', 'note', 'is', 'meant', 'to', 'be', 'an', 'addition', 'to', 'and', 'a', 'generalization', 'of', 'the', 'set', 'of', 'these', 'results', 'whether', 'the', 'module', 'in', 'the', 'title', 'is', 'algebraically', 'compact', 'or', 'not', 'depends', 'on', 'the', 'numbers', 'of', 'algebraically', 'compact', 'and', 'noncompact', 'modules', 'among', 'the', 'components', 'm_al']] | [-0.1648649932859942, 0.11744082381234995, -0.04705817728324129, 0.049574521063401024, -0.07798485288057158, -0.14829623736007963, -0.028389913069676292, 0.3655918478503708, -0.29151564503409866, -0.2269205210528286, 0.15806960454391128, -0.2588348711927443, -0.11524004681584563, 0.2083143070777842, -0.12705866724808607, -0.06270816920292673, 0.017742953425663156, 0.15379667004151631, -0.025381920685948328, -0.2947182081813036, 0.38725521419803766, 0.0044345975088229935, 0.20009163043699985, 0.06995998467715789, 0.08262123971773211, -0.024628263815168954, -0.022657515445016613, 0.03180659733452769, -0.1300685820599536, 0.07904445447114318, 0.28850298442755096, 0.12560765402817506, 0.24998185717294988, -0.3322984056706114, -0.09814461794602432, 0.18078778758229933, 0.12477247602369027, 0.042825277143901636, 0.003605974501525882, -0.24519609370045076, 0.1714902197465647, -0.17683497448848892, -0.13737193593401606, -0.011681370711149901, 0.09802461671823448, -0.008107421609262625, -0.29166186899813107, 0.00859763734620209, 0.15163365532961076, 0.10479318361439248, -0.049116626674266056, -0.06989547683922358, -0.014348354968495031, 0.07956031915147846, 0.008342479270803489, 0.06148352765283266, 0.07539445264517626, -0.09125986629772152, -0.06818601713053767, 0.37089205480337706, -0.05375805601131085, -0.2535988583639305, 0.19994398419088286, -0.15960856049877498, -0.1271972726604562, 0.0941756487284361, 0.05260737781059141, 0.1569431046576261, -0.0842939905752112, 0.16873585310215924, -0.15482617278633884, 0.15732959787137518, 0.06375885409548475, 0.039011869954970455, 0.16289122334443207, 0.13222318209884615, 0.06704162355563595, 0.10966274221229201, -0.006465257743333805, -0.00883685602524946, -0.3723092340366092, -0.1856725498485242, -0.16889327790681996, 0.12640663482228026, -0.038880762742929766, -0.17103537538110516, 0.39258394354246845, 0.08001659024694516, 0.1815168883456567, 0.07764064412055963, 0.21235354660555375, 0.06737910510630116, 0.03484322916167651, 0.11803256919203226, 0.14476921673626783, 0.16275552350507919, 0.011224930503138508, -0.0913577098444523, 0.011576948589970206, 0.10155152957778164] |
708.257 | A Note on Surjective Inverse Systems | Given an upward directed set $I$ we consider surjective $I$-inverse systems
$\{X_\al,f_{\al\be}:X_\be\lra X_\al| \al\leq\be\in I\}$, namely those inverse
systems that have all $f_{\al\be}$ surjective. A number of properties of
$I$-inverse systems have been investigated; such are the Mittag-Leffler
condition, investigated by Grothendieck and flabby and semi-flabby $I$-inverse
systems studied by Jensen. We note that flabby implies semi-flabby implies
surjective implies Mittag-Leffler. Some of the results about surjective inverse
systems have been known for some time. The aim of this note is to give a series
of equivalent statements and implications involving surjective inverse systems
and the systems satisfying the Mittag-Leffler condition, together with
improvements of established results, as well as their relationships with the
already known, but scattered facts. The most prominent results relate
cardinalities of the index sets with right exactness of the inverse limit
functor and the non-vanishing of the inverse limit -- connections related to
cohomological dimensions.
| math.CT math.AC math.GR math.LO math.RA | given an upward directed set i we consider surjective iinverse systems x_alf_albex_belra x_al alleqbein i namely those inverse systems that have all f_albe surjective a number of properties of iinverse systems have been investigated such are the mittagleffler condition investigated by grothendieck and flabby and semiflabby iinverse systems studied by jensen we note that flabby implies semiflabby implies surjective implies mittagleffler some of the results about surjective inverse systems have been known for some time the aim of this note is to give a series of equivalent statements and implications involving surjective inverse systems and the systems satisfying the mittagleffler condition together with improvements of established results as well as their relationships with the already known but scattered facts the most prominent results relate cardinalities of the index sets with right exactness of the inverse limit functor and the nonvanishing of the inverse limit connections related to cohomological dimensions | [['given', 'an', 'upward', 'directed', 'set', 'i', 'we', 'consider', 'surjective', 'iinverse', 'systems', 'x_alf_albex_belra', 'x_al', 'alleqbein', 'i', 'namely', 'those', 'inverse', 'systems', 'that', 'have', 'all', 'f_albe', 'surjective', 'a', 'number', 'of', 'properties', 'of', 'iinverse', 'systems', 'have', 'been', 'investigated', 'such', 'are', 'the', 'mittagleffler', 'condition', 'investigated', 'by', 'grothendieck', 'and', 'flabby', 'and', 'semiflabby', 'iinverse', 'systems', 'studied', 'by', 'jensen', 'we', 'note', 'that', 'flabby', 'implies', 'semiflabby', 'implies', 'surjective', 'implies', 'mittagleffler', 'some', 'of', 'the', 'results', 'about', 'surjective', 'inverse', 'systems', 'have', 'been', 'known', 'for', 'some', 'time', 'the', 'aim', 'of', 'this', 'note', 'is', 'to', 'give', 'a', 'series', 'of', 'equivalent', 'statements', 'and', 'implications', 'involving', 'surjective', 'inverse', 'systems', 'and', 'the', 'systems', 'satisfying', 'the', 'mittagleffler', 'condition', 'together', 'with', 'improvements', 'of', 'established', 'results', 'as', 'well', 'as', 'their', 'relationships', 'with', 'the', 'already', 'known', 'but', 'scattered', 'facts', 'the', 'most', 'prominent', 'results', 'relate', 'cardinalities', 'of', 'the', 'index', 'sets', 'with', 'right', 'exactness', 'of', 'the', 'inverse', 'limit', 'functor', 'and', 'the', 'nonvanishing', 'of', 'the', 'inverse', 'limit', 'connections', 'related', 'to', 'cohomological', 'dimensions']] | [-0.13783708868639452, 0.06472529749106372, -0.0371556941979936, 0.12230142232004579, -0.06107438948669738, -0.1478037161205511, -0.01264980144251685, 0.3677582718770612, -0.32086571205449715, -0.23388036604241266, 0.14288914269748162, -0.2820773431221251, -0.16802242441246143, 0.2202873648391789, -0.10790993516834882, 0.07533004732519206, 0.03776543324982578, 0.0663086665546769, -0.08002126629796479, -0.25696809375105045, 0.3910425750968548, 0.007981010921091049, 0.21153447185349944, 0.06528010372054345, 0.11258983720823393, -0.01423325298933664, -0.05319895731428495, 0.031792296734931585, -0.17071647150492886, 0.098378980955617, 0.25816966628108723, 0.12717779168517815, 0.22161055820622852, -0.37433501912632605, -0.16326215461717097, 0.17625728134437094, 0.12750894965122003, -0.01672618606915841, -0.02042597244246179, -0.2684253163805062, 0.1087942883792379, -0.15613285628622853, -0.13133896507568643, -0.0701346502059719, 0.09315659766821387, 0.08066768638490067, -0.21952206240250513, 0.04101259622175794, 0.17148040150458294, 0.10331972400898805, -0.07924041934628887, -0.16268196735869755, -0.011649899152140101, 0.10155425394526633, 0.06973736857347372, -0.028921007846280204, 0.06341761556108827, -0.1154816935825572, -0.13774942170984886, 0.36162907068155237, -0.01683262400198858, -0.1637042678853536, 0.20560748021971512, -0.13639287838803513, -0.17462281881785996, 0.09061248314573422, 0.054067899095272265, 0.11294201843544736, -0.12186598239818236, 0.1528303012739496, -0.11439011892681564, 0.11327223825574546, 0.09712652168790256, 0.07117025473096467, 0.13457750294591997, 0.09056801870595534, 0.07105237346670062, 0.1591121259070542, 0.025635171342979778, -0.05393323972186243, -0.31345110807333376, -0.15217821565749762, -0.12089061644660973, 0.09673030123408066, -0.03825496226315911, -0.1291396730983226, 0.3340585913274672, 0.12746204459739335, 0.2035596896210438, 0.13470738316834024, 0.18644100740239336, 0.15012042781012866, 0.03124288917141413, 0.027745401991492176, 0.18344859211824482, 0.24663909493743644, 0.07052529684326553, -0.1420018286509374, 0.04145549207932309, 0.12388426714114376] |
708.2571 | On the Security of the Cha-Ko-Lee-Han-Cheon Braid Group Public Key
Cryptosystem | We show that a number of cryptographic protocols using non-commutative
semigroups including the Cha-Ko-Lee-Han-Cheon braid group public-key
cryptosystem and related public-key cryptosystems such as the Shpilrain-Ushakov
public-key cryptosystems are based on the MSCSP.
| cs.CR | we show that a number of cryptographic protocols using noncommutative semigroups including the chakoleehancheon braid group publickey cryptosystem and related publickey cryptosystems such as the shpilrainushakov publickey cryptosystems are based on the mscsp | [['we', 'show', 'that', 'a', 'number', 'of', 'cryptographic', 'protocols', 'using', 'noncommutative', 'semigroups', 'including', 'the', 'chakoleehancheon', 'braid', 'group', 'publickey', 'cryptosystem', 'and', 'related', 'publickey', 'cryptosystems', 'such', 'as', 'the', 'shpilrainushakov', 'publickey', 'cryptosystems', 'are', 'based', 'on', 'the', 'mscsp']] | [-0.274821787327528, -0.010197097901254892, -0.16532532715549073, 0.12077397331595421, -0.041243046956757706, -0.3378208871775617, 0.021462201947967212, 0.3031879544878999, -0.34308363075057663, -0.24454838068534931, 0.21372756813652813, -0.2911330180242658, -0.17416026579837005, 0.37750223005811373, -0.26516459858976305, 0.1937746923106412, -0.10569665820027391, 0.021791022457182407, -0.06316619957021127, -0.3631143314531073, 0.4735040741662184, -0.010603276741070053, 0.31403035814873875, 0.02074970578153928, 0.01055438257753849, 0.03145067013489703, -0.08259499177026251, -0.14680984144409498, -0.06445487600406825, 0.10109641049057246, 0.26861456951592116, 0.14819590779952704, 0.1767668318313857, -0.376159688582023, -0.1605107245966792, 0.12989237752432625, 0.10660123199534913, 0.13731482215225696, -0.18637162660015746, -0.3103683509553472, 0.08753848468574385, -0.3617662539705634, 0.009477889817208051, -0.07483240316311518, -0.07431887462735176, 0.11576432989289363, -0.13751744454105694, -0.08114529764279724, 0.01574470945633948, 0.15731085119768978, 0.14560780564012626, -0.09408280101294318, 0.041846498769397535, 0.05452412120066583, -0.02024088818579912, -0.05244532665237785, 0.19570208013368148, -0.06258027680839101, -0.3072344704841574, 0.5070805417994658, 0.05010716980323195, -0.1136780240262548, 0.05895783096396675, 0.08233701928208272, -0.25160235475438336, -0.00869622454047203, 0.14336719438433648, 0.13841042728163302, 0.027388057888795933, 0.10306793649797327, -0.2664522437378764, 0.23042419034366807, 0.06065810917255779, 0.2017116110927115, 0.061167896787325544, 0.027121670233706634, 0.041335005406290294, 0.08614393995764355, 0.024176970426924526, -0.17250957575937112, -0.25869277864694595, -0.22420637054989737, -0.17405030243098735, 0.04815969911093513, -0.0338521315556136, -0.19076568157567333, 0.39787335904935994, 0.2268520023363332, 0.013513275484244028, 0.06356996794541676, 0.34824291119972867, -0.02154738996565963, 0.1579794008905689, 0.17304314896464348, 0.06354113432268302, 0.13144526047011215, -0.040311201770479484, -0.12719795654217403, 0.1608750462376823, 0.264482088573277] |
708.2572 | The Ratio Monotonicity of the $q$-Derangement Numbers | We show that the $q$-derangement numbers satisfy a ratio monotone property,
which is analogous to the log-concavity and is stronger than the spiral
property and the unimodality.
| math.CO | we show that the qderangement numbers satisfy a ratio monotone property which is analogous to the logconcavity and is stronger than the spiral property and the unimodality | [['we', 'show', 'that', 'the', 'qderangement', 'numbers', 'satisfy', 'a', 'ratio', 'monotone', 'property', 'which', 'is', 'analogous', 'to', 'the', 'logconcavity', 'and', 'is', 'stronger', 'than', 'the', 'spiral', 'property', 'and', 'the', 'unimodality']] | [-0.1872449612451924, 0.10586824726865247, -0.12388886000823092, 0.1851551405550843, -0.11387516673723305, -0.11460316400216133, -0.02892176032980421, 0.3327583756159853, -0.2762521872365916, -0.2072199537522263, 0.06539794504297552, -0.2642634888697002, -0.18120653870412046, 0.16711061392669324, -0.06787889088607496, 0.04106123372912407, -0.017931886827918114, 0.017917164359931594, -0.08927815151400864, -0.25108168508719514, 0.3069828107125229, -0.019838551611260132, 0.3071639763398303, 0.06499131058377249, 0.06115325650683156, 0.003418615777735357, 0.07096256722730619, 0.05262194746346385, -0.16708117748607443, 0.08214254339260084, 0.09951899783616816, 0.15876107759497785, 0.2551243034777818, -0.35856005977149363, -0.08505213457263178, 0.20314415075160838, 0.09519585233216209, -0.005220639333991265, -0.031192909857189213, -0.21114117893631812, 0.19815190926332166, -0.08317447210127418, -0.20067481341323368, -0.03719958393938012, 0.02613548444652999, 0.12190576801421465, -0.3729873558989278, 0.09255070349684467, 0.23248912090504611, 0.04340218286961317, 0.03167582717206743, -0.12247500613469768, -0.04367805305109532, -0.01649655030902337, 0.06605402256482867, 0.04938028830414017, 0.055400242718557514, -0.12606829342742762, -0.023876107877758505, 0.3702846564076565, 0.002582345025816553, -0.18976707804810117, 0.1696090101160937, -0.1943924706429243, -0.1877321680938756, 0.09195925861045166, 0.030863348567099484, 0.10947591162942073, -0.008337963036158018, 0.00979022874445137, -0.19712114692838104, 0.15430796577560682, 0.1480890978127718, 0.11147133980153336, 0.09753865481319803, 0.01457275229471701, 0.16850683948508016, 0.19837076734337541, -0.012462541736938336, -0.0834483213170811, -0.2485753200739122, -0.22549732457156535, -0.15658175300686034, 0.10613783704185928, -0.11409059353064988, -0.10885915587897654, 0.3159036699820448, 0.1465630670664487, 0.18021458562321235, 0.1948394357373386, 0.25749523420300746, 0.1682047982596689, 0.1008486890544494, 0.054646319778705085, 0.21220438354821117, 0.24670009232229656, 0.037980827761607036, -0.16822073534475984, 0.1637685395501278, 0.14804875257390518] |
708.2573 | Exploring Neutron-Rich Oxygen Isotopes with MoNA | The Modular Neutron Array (MoNA) was used in conjunction with a large-gap
dipole magnet (Sweeper) to measure neutron-unbound states in oxygen isotopes
close to the neutron dripline. While no excited states were observed in 24O, a
resonance at 45(2) keV above the neutron separation energy was observed in 23O.
| nucl-ex | the modular neutron array mona was used in conjunction with a largegap dipole magnet sweeper to measure neutronunbound states in oxygen isotopes close to the neutron dripline while no excited states were observed in 24o a resonance at 452 kev above the neutron separation energy was observed in 23o | [['the', 'modular', 'neutron', 'array', 'mona', 'was', 'used', 'in', 'conjunction', 'with', 'a', 'largegap', 'dipole', 'magnet', 'sweeper', 'to', 'measure', 'neutronunbound', 'states', 'in', 'oxygen', 'isotopes', 'close', 'to', 'the', 'neutron', 'dripline', 'while', 'no', 'excited', 'states', 'were', 'observed', 'in', '24o', 'a', 'resonance', 'at', '452', 'kev', 'above', 'the', 'neutron', 'separation', 'energy', 'was', 'observed', 'in', '23o']] | [-0.03738728218844959, 0.2383093142178746, -0.040103493590972254, 0.17892195724844173, 0.026297030913434466, -0.10854884455626716, 0.09672358331783694, 0.37763976199286325, -0.13108548723465327, -0.3565899031379317, -0.045984231401234865, -0.40354415168035396, 0.09531876133108626, 0.1510015004409515, 0.0625359239436838, 0.06980700918226218, 0.051377748044169676, 0.07699660783899683, -0.08076379444374114, -0.0918973188880565, 0.21615593294061872, 0.12177492380237245, 0.25019702195589033, 0.05119240949196475, 0.021146492947193517, -0.048633091622127256, 0.15233904408405022, -0.11256789269724063, -0.0945599600482656, 0.01583510191341368, 0.36600019372239406, -0.014436123741800156, 0.09859164358278243, -0.4212490503809282, -0.1310657810001653, 0.06569675809456682, 0.11476229893385756, 0.10554129352355945, -0.055354385168709774, -0.34889496330704006, 0.0590836155627455, -0.20194418591504193, -0.19076566770672798, -0.03976743826072435, 0.031651186471690934, 0.029580922872160693, -0.2118891716069941, 0.03955974726348507, -0.00957746902594761, 0.06422727393005423, -0.18308384642385098, -0.24012101829356078, -0.018813761578378628, -0.02942415615733789, 0.02480033763247181, 0.11163693991470702, 0.1832601692603559, -0.029704272328894967, -0.08063327125748809, 0.28610536919868723, -0.03962194846410837, 0.00384112764435003, 0.1281982084774241, -0.24168541062889354, -0.17002510630088497, 0.25390736059266694, 0.0908933465834707, 0.1017897470797203, -0.1459208855106096, 0.022270149684378078, -0.009409312505693155, 0.268767454338317, 0.1552538660411932, -0.013329749026487828, 0.25604681492479026, 0.20092749513913782, -0.05362568620820435, 0.13433574355321423, -0.26236423583967344, -0.022993679310442234, -0.18390286707186274, -0.08847589384080196, -0.14863871589150965, 0.02760045873761481, 0.07810757851836328, -0.10491033992314312, 0.3326488749257156, -0.043865333197220246, 0.12516154058049528, -0.12281419459388268, 0.2142275865284764, 0.07210989692723568, 0.10560665780687895, 0.04341897529987048, 0.3866724942867853, 0.2740192581015658, 0.11814650159082091, -0.307748676600809, 0.07047406442425384, -0.04588052215130658] |
708.2574 | The Limiting Distribution of the Coefficients of the $q$-Catalan Numbers | We show that the limiting distributions of the coefficients of the
$q$-Catalan numbers and the generalized $q$-Catalan numbers are normal. Despite
the fact that these coefficients are not unimodal for small $n$, we conjecture
that for sufficiently large $n$, the coefficients are unimodal and even
log-concave except for a few terms of the head and tail.
| math.CO | we show that the limiting distributions of the coefficients of the qcatalan numbers and the generalized qcatalan numbers are normal despite the fact that these coefficients are not unimodal for small n we conjecture that for sufficiently large n the coefficients are unimodal and even logconcave except for a few terms of the head and tail | [['we', 'show', 'that', 'the', 'limiting', 'distributions', 'of', 'the', 'coefficients', 'of', 'the', 'qcatalan', 'numbers', 'and', 'the', 'generalized', 'qcatalan', 'numbers', 'are', 'normal', 'despite', 'the', 'fact', 'that', 'these', 'coefficients', 'are', 'not', 'unimodal', 'for', 'small', 'n', 'we', 'conjecture', 'that', 'for', 'sufficiently', 'large', 'n', 'the', 'coefficients', 'are', 'unimodal', 'and', 'even', 'logconcave', 'except', 'for', 'a', 'few', 'terms', 'of', 'the', 'head', 'and', 'tail']] | [-0.15279091730189975, 0.17827063080455577, -0.04312984993988981, 0.09202895256956774, -0.01395962480455637, -0.13159128954534285, -0.019677748462917016, 0.3583767841170941, -0.2582233681543065, -0.23664604699505226, 0.10313046547318143, -0.27457044181729934, -0.15981010893925227, 0.2322982479152935, -0.047172584787144194, 0.06412906372653586, 0.05453108041547239, 0.047518688653196604, -0.039132541220169514, -0.30053478236576275, 0.3261017892177084, -0.057899538404724026, 0.2216498926780852, 0.07402375859341451, 0.10374224561798785, -0.01452883196595524, -0.0005783220819596734, 0.02500636513702505, -0.09447288004061452, 0.1355542859029291, 0.23458903019283234, 0.09326610346657357, 0.23475336705762725, -0.37959898116865326, -0.11422325538088833, 0.1744532986444288, 0.1431873255600554, 0.05169111430378897, -0.03089941028572087, -0.1924794362359015, 0.1582922583412645, -0.17991369630077056, -0.1970115750529138, -0.10918397546213653, 0.08773802520175066, 0.136467969045043, -0.31853608841109754, 0.12024964503611305, 0.12802261686218636, 0.025256671344063113, -0.013910998590290546, -0.2181154487022598, 0.004008188324015853, 0.12133132332902667, 0.06663799535350076, -0.07145016620467816, 0.026767810201168425, -0.20580284711572208, -0.00520776751052056, 0.33658230883468476, -0.05323780334687659, -0.2324806613947398, 0.17189044456297, -0.27191597329718725, -0.19397302260456076, 0.13475923403166234, 0.0978275311811428, 0.14853513302244079, -0.029517866022485708, 0.0946694073468929, -0.14369883088095645, 0.0993835872172245, 0.14375030746616954, 0.026153605007233897, 0.1342262829920011, -0.022740485828502903, 0.03891414189378598, 0.12151915516837367, -0.09038037420915705, -0.07760756723083821, -0.3230564281776814, -0.15160250985458593, -0.24384664980295515, 0.038032691953048925, -0.16288279357753968, -0.17701244868138538, 0.33908132528553586, 0.0714338667582654, 0.26415469058390173, 0.19797288152455753, 0.20111775611128127, 0.15274059198730225, 0.02781122932875795, 0.06745952802676973, 0.14010839651538326, 0.13113736397852854, 0.011929767422511109, -0.1217390412597784, 0.12687305943940633, 0.04696967036163967] |
708.2575 | Rateless Coding for Gaussian Channels | A rateless code-i.e., a rate-compatible family of codes-has the property that
codewords of the higher rate codes are prefixes of those of the lower rate
ones. A perfect family of such codes is one in which each of the codes in the
family is capacity-achieving. We show by construction that perfect rateless
codes with low-complexity decoding algorithms exist for additive white Gaussian
noise channels. Our construction involves the use of layered encoding and
successive decoding, together with repetition using time-varying layer weights.
As an illustration of our framework, we design a practical three-rate code
family. We further construct rich sets of near-perfect rateless codes within
our architecture that require either significantly fewer layers or lower
complexity than their perfect counterparts. Variations of the basic
construction are also developed, including one for time-varying channels in
which there is no a priori stochastic model.
| cs.IT math.IT | a rateless codeie a ratecompatible family of codeshas the property that codewords of the higher rate codes are prefixes of those of the lower rate ones a perfect family of such codes is one in which each of the codes in the family is capacityachieving we show by construction that perfect rateless codes with lowcomplexity decoding algorithms exist for additive white gaussian noise channels our construction involves the use of layered encoding and successive decoding together with repetition using timevarying layer weights as an illustration of our framework we design a practical threerate code family we further construct rich sets of nearperfect rateless codes within our architecture that require either significantly fewer layers or lower complexity than their perfect counterparts variations of the basic construction are also developed including one for timevarying channels in which there is no a priori stochastic model | [['a', 'rateless', 'codeie', 'a', 'ratecompatible', 'family', 'of', 'codeshas', 'the', 'property', 'that', 'codewords', 'of', 'the', 'higher', 'rate', 'codes', 'are', 'prefixes', 'of', 'those', 'of', 'the', 'lower', 'rate', 'ones', 'a', 'perfect', 'family', 'of', 'such', 'codes', 'is', 'one', 'in', 'which', 'each', 'of', 'the', 'codes', 'in', 'the', 'family', 'is', 'capacityachieving', 'we', 'show', 'by', 'construction', 'that', 'perfect', 'rateless', 'codes', 'with', 'lowcomplexity', 'decoding', 'algorithms', 'exist', 'for', 'additive', 'white', 'gaussian', 'noise', 'channels', 'our', 'construction', 'involves', 'the', 'use', 'of', 'layered', 'encoding', 'and', 'successive', 'decoding', 'together', 'with', 'repetition', 'using', 'timevarying', 'layer', 'weights', 'as', 'an', 'illustration', 'of', 'our', 'framework', 'we', 'design', 'a', 'practical', 'threerate', 'code', 'family', 'we', 'further', 'construct', 'rich', 'sets', 'of', 'nearperfect', 'rateless', 'codes', 'within', 'our', 'architecture', 'that', 'require', 'either', 'significantly', 'fewer', 'layers', 'or', 'lower', 'complexity', 'than', 'their', 'perfect', 'counterparts', 'variations', 'of', 'the', 'basic', 'construction', 'are', 'also', 'developed', 'including', 'one', 'for', 'timevarying', 'channels', 'in', 'which', 'there', 'is', 'no', 'a', 'priori', 'stochastic', 'model']] | [-0.1851171582582132, 0.06103361957204417, -0.040050662732381614, 0.05341308036226136, -0.03228253106713938, -0.24499759460270082, 0.07683365761215309, 0.4093731202774768, -0.2967457761452031, -0.2639632730865382, 0.10266699399145843, -0.23893797097446248, -0.19580847883208408, 0.21430738052862475, -0.1213018211599761, 0.0885457259656446, 0.07446039528351464, 0.02929524796229298, -0.12929624420081487, -0.31431741324812845, 0.3120685159429747, 0.14490227059715782, 0.28062252655437736, -0.07826388461461706, 0.09952201309472343, -0.014898846613531328, -0.0054291508080129575, -0.048476384229046834, -0.14058664142527483, 0.12142774483135385, 0.26263625628696824, 0.17863889910253905, 0.22607728852990935, -0.3719280714959764, -0.29668208796689255, 0.08182065676656558, 0.11195018908436906, 0.1984749859148258, -0.09839846424778535, -0.18749047989166415, 0.16351272387885682, -0.23260497687746295, -0.009870970099092387, -0.004983448430145387, -0.0626625037222779, 0.05744990726544274, -0.31613728998852025, -0.01652045409457269, 0.12113006281827261, 0.04233994334936142, -0.025324934256001772, -0.17728423655515524, 0.030873329913002446, 0.1014060294573872, -0.027406620401922585, 0.010668868057449892, 0.030938438062803993, -0.0724615747872874, -0.1635631032852563, 0.3197516094873954, -0.048581688094188176, -0.2309919669328043, 0.17184035003305875, -0.04261065193907552, -0.10973778788482758, 0.19180716351076638, 0.21003334804793164, 0.12094376909231647, -0.11899152747606657, 0.040811691288719046, -0.08332601473030211, 0.19734999320382696, 0.10352114145811513, 0.15712028880613663, 0.15526527847438085, 0.11099722330867172, 0.07804656030757608, 0.18419566428248615, -0.043644405040461166, -0.1149247334064018, -0.28305793567661114, -0.12848970198081705, -0.1618296202362629, -0.011859524355223068, -0.13375449407309303, -0.21425824024356072, 0.38661157621888165, 0.10975307330703564, 0.14130453130886925, 0.13829498541903207, 0.29940042674889883, 0.030594168286167567, 0.10554678212656982, 0.18622663103566645, 0.14843102686757073, 0.14094265209169213, -0.030595504339590077, -0.13603411675573213, 0.09255832308407524, 0.07020976121048275] |
708.2576 | The Nature of the Hard-X-Ray Emitting Symbiotic Star RT Cru | We describe Chandra High-Energy Transmission Grating Spectrometer
observations of RT Cru, the first of a new sub-class of symbiotic stars that
appear to contain white dwarfs (WDs) capable of producing hard X-ray emission
out to greater than 50 keV. The production of such hard X-ray emission from the
objects in this sub-class (which also includes CD -57 3057, T CrB, and CH Cyg)
challenges our understanding of accreting WDs. We find that the 0.3 -- 8.0 keV
X-ray spectrum of RT Cru emanates from an isobaric cooling flow, as in the
optically thin accretion-disk boundary layers of some dwarf novae. The
parameters of the spectral fit confirm that the compact accretor is a WD, and
they are consistent with the WD being massive. We detect rapid, stochastic
variability from the X-ray emission below 4 keV. The combination of flickering
variability and a cooling-flow spectrum indicates that RT Cru is likely powered
by accretion through a disk. Whereas the cataclysmic variable stars with the
hardest X-ray emission are typically magnetic accretors with X-ray flux
modulated at the WD spin period, we find that the X-ray emission from RT Cru is
not pulsed. RT Cru therefore shows no evidence for magnetically channeled
accretion, consistent with our interpretation that the Chandra spectrum arises
from an accretion-disk boundary layer.
| astro-ph | we describe chandra highenergy transmission grating spectrometer observations of rt cru the first of a new subclass of symbiotic stars that appear to contain white dwarfs wds capable of producing hard xray emission out to greater than 50 kev the production of such hard xray emission from the objects in this subclass which also includes cd 57 3057 t crb and ch cyg challenges our understanding of accreting wds we find that the 03 80 kev xray spectrum of rt cru emanates from an isobaric cooling flow as in the optically thin accretiondisk boundary layers of some dwarf novae the parameters of the spectral fit confirm that the compact accretor is a wd and they are consistent with the wd being massive we detect rapid stochastic variability from the xray emission below 4 kev the combination of flickering variability and a coolingflow spectrum indicates that rt cru is likely powered by accretion through a disk whereas the cataclysmic variable stars with the hardest xray emission are typically magnetic accretors with xray flux modulated at the wd spin period we find that the xray emission from rt cru is not pulsed rt cru therefore shows no evidence for magnetically channeled accretion consistent with our interpretation that the chandra spectrum arises from an accretiondisk boundary layer | [['we', 'describe', 'chandra', 'highenergy', 'transmission', 'grating', 'spectrometer', 'observations', 'of', 'rt', 'cru', 'the', 'first', 'of', 'a', 'new', 'subclass', 'of', 'symbiotic', 'stars', 'that', 'appear', 'to', 'contain', 'white', 'dwarfs', 'wds', 'capable', 'of', 'producing', 'hard', 'xray', 'emission', 'out', 'to', 'greater', 'than', '50', 'kev', 'the', 'production', 'of', 'such', 'hard', 'xray', 'emission', 'from', 'the', 'objects', 'in', 'this', 'subclass', 'which', 'also', 'includes', 'cd', '57', '3057', 't', 'crb', 'and', 'ch', 'cyg', 'challenges', 'our', 'understanding', 'of', 'accreting', 'wds', 'we', 'find', 'that', 'the', '03', '80', 'kev', 'xray', 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708.2577 | The Transfer of Knowledge from Physics and Mathematics to Engineering
Applications | The objective of this paper is to describe a development of an innovative
approach to enable students studying science, technology, engineering, and
mathematics (STEM) to apply the concepts learned in physics and mathematics to
engineering problem-solving challenges. Our goal is to facilitate students
transfer of knowledge from theory to engineering applications, thereby
increasing student academic performance, retention, persistence, and
graduation. To achieve the goal we are creating a virtual community of students
and faculty as a vehicle for promoting the transfer of knowledge using
e-learning and e-teaching mechanisms.
| physics.ed-ph physics.gen-ph | the objective of this paper is to describe a development of an innovative approach to enable students studying science technology engineering and mathematics stem to apply the concepts learned in physics and mathematics to engineering problemsolving challenges our goal is to facilitate students transfer of knowledge from theory to engineering applications thereby increasing student academic performance retention persistence and graduation to achieve the goal we are creating a virtual community of students and faculty as a vehicle for promoting the transfer of knowledge using elearning and eteaching mechanisms | [['the', 'objective', 'of', 'this', 'paper', 'is', 'to', 'describe', 'a', 'development', 'of', 'an', 'innovative', 'approach', 'to', 'enable', 'students', 'studying', 'science', 'technology', 'engineering', 'and', 'mathematics', 'stem', 'to', 'apply', 'the', 'concepts', 'learned', 'in', 'physics', 'and', 'mathematics', 'to', 'engineering', 'problemsolving', 'challenges', 'our', 'goal', 'is', 'to', 'facilitate', 'students', 'transfer', 'of', 'knowledge', 'from', 'theory', 'to', 'engineering', 'applications', 'thereby', 'increasing', 'student', 'academic', 'performance', 'retention', 'persistence', 'and', 'graduation', 'to', 'achieve', 'the', 'goal', 'we', 'are', 'creating', 'a', 'virtual', 'community', 'of', 'students', 'and', 'faculty', 'as', 'a', 'vehicle', 'for', 'promoting', 'the', 'transfer', 'of', 'knowledge', 'using', 'elearning', 'and', 'eteaching', 'mechanisms']] | [0.026734086176888508, 0.06699997454829414, -0.10616979390298101, 0.04964024321816396, -0.20372952787015078, -0.12738553516630252, 0.06148773627038198, 0.38692155448635196, -0.2879000767239962, -0.4198636517658914, 0.05349541135762014, -0.2597400996812873, -0.2047491325488822, 0.20848771726543253, -0.14363479665586387, 0.025622685433270155, 0.07299426505447958, -0.020024178570813754, -0.0408769032874261, -0.2839567342995327, 0.28612546632278035, 0.09125791786407883, 0.36493770547465165, 0.09504336742049252, 0.08400972818146163, 0.009535966779698025, -0.06004510767822715, -0.07382250227965415, -0.09591973554977978, 0.2721774572591213, 0.4858018627088644, 0.26809188736264, 0.4635961392725056, -0.40191379976882174, -0.1592251812002029, 0.008264124721542677, 0.09231729235299016, 0.10261296432211318, -0.05921225912276317, -0.2969074008499526, 0.056742426293732766, -0.20920578899941492, -0.13641390491234648, -0.09685421042112549, -0.027446688340701672, -0.01836665211753412, -0.23505499200969512, -0.08016584734220734, 0.06516117410633755, 0.1657057345834222, -0.049250343576369975, -0.12807338393229822, 0.052420031461885876, 0.2813590260021473, 0.04176258586283604, 0.03864915949154899, 0.1766261619208804, -0.2374270312165291, -0.2040572713065723, 0.391408323331482, 0.049517191539052874, -0.12843635193580252, 0.23630547446241093, -0.06572523315183142, -0.09538989288690077, 0.04245297599118203, 0.28459811150308023, 0.023812163626478814, -0.17077313660411164, 0.03174032385934631, 0.10593492780621587, 0.13350144992794163, 0.03774964857306755, -0.050770771560068664, 0.20224648407417012, 0.2488044932251796, 0.052625361078588125, 0.09400464883021248, 0.03197831506787969, -0.11081131223777034, -0.22982161414322697, -0.24214548704383726, -0.17456900870522737, 0.03501406621018594, 0.03835533017544632, -0.10602968646509742, 0.4062929950755047, 0.21594113409942525, 0.029342283079379493, 0.009818685886619443, 0.27239495420574467, 0.020559933470477434, 0.060002365996214474, 0.057666229412213645, 0.18072070664890239, 0.11041587173663588, 0.23884658963652328, -0.16521772725073705, 0.09695079781390219, -0.012121144131841984] |
708.2578 | A Survey of z~6 Quasars in the SDSS Deep Stripe: I. a Flux-Limited
Sample at z_{AB}<21 | We present the discovery of five quasars at z~6 selected from 260 deg^2 of
the Sloan Digital Sky Survey (SDSS) southern survey, a deep imaging survey
obtained by repeatedly scanning a stripe along the Celestial Equator. The five
quasars with 20<z_{AB}<21 are 1-2 magnitudes fainter than the luminous z~6
quasars discovered in the SDSS main survey. One of them was independently
discovered by the UKIRT Infrared Deep Sky Survey. These quasars, combined with
another z~6 quasar known in this region, make a complete flux- limited quasar
sample at z_{AB}<21. The sample spans the redshift range 5.85<z<6.12 and the
luminosity range -26.5<M_{1450}<-25.4 (H_0=70 km s^{-1} Mpc^{-1},
Omega_{m}=0.3, and Omega_{Lambda}=0.7). We use the 1/V_{a} method to determine
that the comoving quasar spatial density at <z>=6.0 and <M_{1450}>=-25.8 is
(5.0+/-2.1) x 10^{-9} Mpc^{-3} mag^{-1}. We model the bright-end quasar
luminosity function (QLF) at z~6 as a power law Phi(L_{1450}) \propto
L_{1450}^{beta}. The slope beta calculated from a combination of our sample and
the luminous SDSS quasar sample is -3.1+/-0.4, significantly steeper than the
slope of the QLF at z~4. Based on the derived QLF, we find that the quasar/AGN
population cannot provide enough photons to ionize the intergalactic medium
(IGM) at z~6 unless the IGM is very homogeneous and the luminosity (L*_{1450})
at which the QLF power law breaks is very low.
| astro-ph | we present the discovery of five quasars at z6 selected from 260 deg2 of the sloan digital sky survey sdss southern survey a deep imaging survey obtained by repeatedly scanning a stripe along the celestial equator the five quasars with 20z_ab21 are 12 magnitudes fainter than the luminous z6 quasars discovered in the sdss main survey one of them was independently discovered by the ukirt infrared deep sky survey these quasars combined with another z6 quasar known in this region make a complete flux limited quasar sample at z_ab21 the sample spans the redshift range 585z612 and the luminosity range 265m_1450254 h_070 km s1 mpc1 omega_m03 and omega_lambda07 we use the 1v_a method to determine that the comoving quasar spatial density at z60 and m_1450258 is 5021 x 109 mpc3 mag1 we model the brightend quasar luminosity function qlf at z6 as a power law phil_1450 propto l_1450beta the slope beta calculated from a combination of our sample and the luminous sdss quasar sample is 3104 significantly steeper than the slope of the qlf at z4 based on the derived qlf we find that the quasaragn population cannot provide enough photons to ionize the intergalactic medium igm at z6 unless the igm is very homogeneous and the luminosity l_1450 at which the qlf power law breaks is very low | [['we', 'present', 'the', 'discovery', 'of', 'five', 'quasars', 'at', 'z6', 'selected', 'from', '260', 'deg2', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'southern', 'survey', 'a', 'deep', 'imaging', 'survey', 'obtained', 'by', 'repeatedly', 'scanning', 'a', 'stripe', 'along', 'the', 'celestial', 'equator', 'the', 'five', 'quasars', 'with', '20z_ab21', 'are', '12', 'magnitudes', 'fainter', 'than', 'the', 'luminous', 'z6', 'quasars', 'discovered', 'in', 'the', 'sdss', 'main', 'survey', 'one', 'of', 'them', 'was', 'independently', 'discovered', 'by', 'the', 'ukirt', 'infrared', 'deep', 'sky', 'survey', 'these', 'quasars', 'combined', 'with', 'another', 'z6', 'quasar', 'known', 'in', 'this', 'region', 'make', 'a', 'complete', 'flux', 'limited', 'quasar', 'sample', 'at', 'z_ab21', 'the', 'sample', 'spans', 'the', 'redshift', 'range', '585z612', 'and', 'the', 'luminosity', 'range', '265m_1450254', 'h_070', 'km', 's1', 'mpc1', 'omega_m03', 'and', 'omega_lambda07', 'we', 'use', 'the', '1v_a', 'method', 'to', 'determine', 'that', 'the', 'comoving', 'quasar', 'spatial', 'density', 'at', 'z60', 'and', 'm_1450258', 'is', '5021', 'x', '109', 'mpc3', 'mag1', 'we', 'model', 'the', 'brightend', 'quasar', 'luminosity', 'function', 'qlf', 'at', 'z6', 'as', 'a', 'power', 'law', 'phil_1450', 'propto', 'l_1450beta', 'the', 'slope', 'beta', 'calculated', 'from', 'a', 'combination', 'of', 'our', 'sample', 'and', 'the', 'luminous', 'sdss', 'quasar', 'sample', 'is', '3104', 'significantly', 'steeper', 'than', 'the', 'slope', 'of', 'the', 'qlf', 'at', 'z4', 'based', 'on', 'the', 'derived', 'qlf', 'we', 'find', 'that', 'the', 'quasaragn', 'population', 'can', 'not', 'provide', 'enough', 'photons', 'to', 'ionize', 'the', 'intergalactic', 'medium', 'igm', 'at', 'z6', 'unless', 'the', 'igm', 'is', 'very', 'homogeneous', 'and', 'the', 'luminosity', 'l_1450', 'at', 'which', 'the', 'qlf', 'power', 'law', 'breaks', 'is', 'very', 'low']] | [-0.0064382036580699735, 0.06912676624344635, -0.04374883245093024, 0.10546070877495729, -0.15212495487858652, -0.05771477719971919, 0.07517107502751547, 0.4440430637042952, -0.07372221256323794, -0.3473780619783848, 0.0420682705895781, -0.3921680834356219, 0.05177681716114848, 0.2075946477704372, 0.021568696651143193, -0.050923922327314, -0.04174752623368037, -0.17312527954745574, -0.0053806068409224354, -0.3556524712715951, 0.25182097134460646, 0.0868741021978766, 0.23272674949398325, -0.10782993377144426, 0.14572335670424086, -0.09770359497482037, -0.1459496894816016, -0.019544440456246738, -0.20686621331231575, -0.007850759664894704, 0.2967209185018994, 0.1382866012637605, 0.2603522264635879, -0.22751849058999513, 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708.2579 | Direction-sensitive dark matter search results in a surface laboratory | We developed a three-dimensional gaseous tracking device and performed a
direction-sensitive dark matter search in a surface laboratory. By using 150
Torr carbon-tetrafluoride (CF_4 gas), we obtained a sky map drawn with the
recoil directions of the carbon and fluorine nuclei, and set the first limit on
the spin-dependent WIMP (Weakly Interacting Massive Particles)-proton cross
section by a direction-sensitive method. Thus, we showed that a WIMP-search
experiment with a gaseous tracking device can actually set limits. Furthermore,
we demonstrated that this method will potentially play a certain role in
revealing the nature of dark matter when a low-background large-volume detector
is developed.
| astro-ph | we developed a threedimensional gaseous tracking device and performed a directionsensitive dark matter search in a surface laboratory by using 150 torr carbontetrafluoride cf_4 gas we obtained a sky map drawn with the recoil directions of the carbon and fluorine nuclei and set the first limit on the spindependent wimp weakly interacting massive particlesproton cross section by a directionsensitive method thus we showed that a wimpsearch experiment with a gaseous tracking device can actually set limits furthermore we demonstrated that this method will potentially play a certain role in revealing the nature of dark matter when a lowbackground largevolume detector is developed | [['we', 'developed', 'a', 'threedimensional', 'gaseous', 'tracking', 'device', 'and', 'performed', 'a', 'directionsensitive', 'dark', 'matter', 'search', 'in', 'a', 'surface', 'laboratory', 'by', 'using', '150', 'torr', 'carbontetrafluoride', 'cf_4', 'gas', 'we', 'obtained', 'a', 'sky', 'map', 'drawn', 'with', 'the', 'recoil', 'directions', 'of', 'the', 'carbon', 'and', 'fluorine', 'nuclei', 'and', 'set', 'the', 'first', 'limit', 'on', 'the', 'spindependent', 'wimp', 'weakly', 'interacting', 'massive', 'particlesproton', 'cross', 'section', 'by', 'a', 'directionsensitive', 'method', 'thus', 'we', 'showed', 'that', 'a', 'wimpsearch', 'experiment', 'with', 'a', 'gaseous', 'tracking', 'device', 'can', 'actually', 'set', 'limits', 'furthermore', 'we', 'demonstrated', 'that', 'this', 'method', 'will', 'potentially', 'play', 'a', 'certain', 'role', 'in', 'revealing', 'the', 'nature', 'of', 'dark', 'matter', 'when', 'a', 'lowbackground', 'largevolume', 'detector', 'is', 'developed']] | [-0.08550096857004182, 0.14202255250351264, -0.11796839096316017, 0.03054516084289344, -0.012233110767152935, -0.1019202643489041, 0.04809359851118067, 0.3589934410324486, -0.1548795386558712, -0.3495050107709842, 0.019516091483142595, -0.2967138841268745, -0.06120603499786541, 0.23039150198386743, 0.048037250069809134, 0.052726591096618695, 0.07587761996028078, -0.01970656820121083, -0.03623380688581579, -0.24506501239346395, 0.25549394312535995, 0.11744296434104885, 0.23395199318517848, 0.05846034372017931, 0.16498312214850494, 0.003699269791198249, -0.04877832358112872, 0.009332864300928789, -0.13594020058537515, 0.08044097738082309, 0.2652052979395347, 0.062161076689452525, 0.184007717513175, -0.41626209955625604, -0.19458023267844232, 0.13612405903231684, 0.12722325430477574, 0.08877540328124962, -0.17256916011222592, -0.3600355802601812, 0.059948960143962116, -0.23578396015616115, -0.13607946675879382, -0.024355396121223963, -0.03591866062028076, -0.002634670875855897, -0.23397627957902922, 0.025637057363193962, 0.0009278803738179884, -0.007889454663353095, -0.052606528800091534, -0.10767801335118342, 0.019556091107096118, -0.00439633846387848, -0.022291618296738234, 0.01111989485856035, 0.27957146834250135, -0.14627130709745284, -0.03582158269323778, 0.379895543698037, -0.11946180419959497, -0.14886846213998034, 0.19683898671871364, -0.1753169221268727, -0.11667162619097766, 0.18403885930333988, 0.171668724073927, 0.10467752108193638, -0.1995678172387139, 0.06772154779231065, -0.0748905137752985, 0.20322596762642856, 0.0782865849554096, -0.02104407714652174, 0.3016099671252293, 0.27361985152854706, 0.06884964767585297, 0.07474019166340332, -0.2081921145776379, 0.011066567514663433, -0.2843143620555944, -0.18225415865199104, -0.11787964793678263, 0.021653958361441416, -0.00310945135064649, -0.0962144055975472, 0.3232863158319551, 0.09348825761808617, 0.17309705108994305, -0.023489073947035144, 0.3154095929890576, 0.013753818648021282, 0.029023913101818743, 0.02177692057638623, 0.2825804972412563, 0.14277490834004736, 0.10976630925560499, -0.19843468656947855, -0.003257361826219476, 0.02731665976271771] |
708.258 | Flavor Dependence of T-odd PDFs | The flavor dependence of the naive time reversal odd (``T-odd'') parton
distributions for $u$- and $d$-quarks are explored in the spectator model. The
flavor dependence of $h_{1}^{\perp}$ is of significance for the analysis of the
azimuthal $\cos(2\phi)$ asymmetries in unpolarized SIDIS and DY-processes, as
well as for the overall physical understanding of the distribution of
transversely polarized quarks in unpolarized nucleons. As a by-product of the
formalism, we calculate the chiral-odd but ``T-even'' function $h_{1L}^{\perp}$
which enables us to present a prediction for the single spin asymmetry
$A_{UL}^{\sin(2\phi)}$ for a longitudinally polarized target in SIDIS.
| hep-ph | the flavor dependence of the naive time reversal odd todd parton distributions for u and dquarks are explored in the spectator model the flavor dependence of h_1perp is of significance for the analysis of the azimuthal cos2phi asymmetries in unpolarized sidis and dyprocesses as well as for the overall physical understanding of the distribution of transversely polarized quarks in unpolarized nucleons as a byproduct of the formalism we calculate the chiralodd but teven function h_1lperp which enables us to present a prediction for the single spin asymmetry a_ulsin2phi for a longitudinally polarized target in sidis | [['the', 'flavor', 'dependence', 'of', 'the', 'naive', 'time', 'reversal', 'odd', 'todd', 'parton', 'distributions', 'for', 'u', 'and', 'dquarks', 'are', 'explored', 'in', 'the', 'spectator', 'model', 'the', 'flavor', 'dependence', 'of', 'h_1perp', 'is', 'of', 'significance', 'for', 'the', 'analysis', 'of', 'the', 'azimuthal', 'cos2phi', 'asymmetries', 'in', 'unpolarized', 'sidis', 'and', 'dyprocesses', 'as', 'well', 'as', 'for', 'the', 'overall', 'physical', 'understanding', 'of', 'the', 'distribution', 'of', 'transversely', 'polarized', 'quarks', 'in', 'unpolarized', 'nucleons', 'as', 'a', 'byproduct', 'of', 'the', 'formalism', 'we', 'calculate', 'the', 'chiralodd', 'but', 'teven', 'function', 'h_1lperp', 'which', 'enables', 'us', 'to', 'present', 'a', 'prediction', 'for', 'the', 'single', 'spin', 'asymmetry', 'a_ulsin2phi', 'for', 'a', 'longitudinally', 'polarized', 'target', 'in', 'sidis']] | [-0.07562980274870111, 0.2368733007160406, -0.1739573615518028, 0.19117067146530595, -0.0451022655232459, -0.06181143423271997, 0.023341094241327336, 0.38509400921963877, -0.20194761320868487, -0.22548519535571016, -0.0982569926919075, -0.2855496583155967, 0.01383804065746165, 0.12890179381926134, 0.11723274803690371, 0.07479982397028355, 0.0012662175151529492, -0.04161187808119481, -0.08606142322382619, -0.16863301500517835, 0.33686939102687663, 0.010904835774913751, 0.2771942249088678, 0.1767372417273701, 0.07781464514643034, 0.16155995958815178, -0.09351239495620292, -0.09525090580185254, -0.041615930886598686, 0.03772459892175531, 0.22892074284434158, 0.057072381817570496, 0.051479260882823376, -0.38324705321061353, -0.11439671173130952, 0.09679532380554304, 0.16052757914087945, 0.11217422047204348, -0.013064700081163356, -0.24196081258036117, -0.00854595723031189, -0.22451835350003294, -0.206372367476003, -0.13230696955059845, 0.04893592821173771, 0.015303140661368767, -0.3509980279511662, 0.10584539081901312, 0.028963018376480347, 0.027028321919421994, -0.005945143072054752, -0.23911616860097776, -0.10212253126245673, 0.05741475050848338, 0.13577906430012956, 0.1500049708210813, 0.11064531898090957, -0.2035350077535196, -0.1575262727396142, 0.38174577434960333, -0.07709332719014617, -0.24363263493143422, 0.03867002119941096, -0.2838984165761259, -0.16767170249925106, 0.08002482057468946, 0.27368546930712556, 0.11553099001407303, -0.16614783166216746, 0.08473128763713464, -0.10377448364110883, 0.12704166812541826, 0.08687382159874804, 0.05197449149664051, 0.1991801187696476, 0.20876623105297806, 0.004944000122768264, 0.10572209095542309, -0.1508457112696863, -0.09159919168920286, -0.37277765423860604, -0.12053338918614769, -0.08418883703729158, 0.09990275607279112, -0.07048971051198771, -0.10860991882540846, 0.43870594173855076, 0.05942818700456091, 0.25743399760986285, 0.0016241634717731866, 0.3292162432385388, 0.08747942171495167, 0.053676556931027485, 0.01573913850413475, 0.2058881911479177, 0.20256277002764725, 0.15635419078171253, -0.2705766219340305, 0.11055803817186144, 0.00369815392199383] |
708.2581 | Non-equilibrium theory of charge qubit decoherence in the quantum point
contact measurement | A non-equilibrium theory describing the charge qubit dynamics measured by a
quantum point contact is developed based on Schwinger-Keldysh's approach. Using
the real-time diagram technique, we derive the master equation to all orders in
perturbation expansions. The non-Markovian processes in the qubit dynamics is
naturally taken into account. The qubit decoherence, in particular, the
influence of the tunneling-electron fluctuation in the quantum point contact
with a longer time correlation, is studied in the framework. We consider the
Lorentzian-type spectral density to characterize the channel mixture of the
electron tunneling processes induced by the measurement and determine the
correlation time scale of the tunneling-electron fluctuation. The result shows
that as the quantum point contact is casted with a narrower profile of the
spectral density, tunneling electrons can propagate with a longer time
correlation and lead to the non-Markovian processes of the qubit dynamics. The
qubit electron in the charge qubit will be driven coherently. The quantum point
contact measurement with the minimum deviation of the electron tunneling
processes prevents the qubit state from the decoherence.
| cond-mat.mes-hall | a nonequilibrium theory describing the charge qubit dynamics measured by a quantum point contact is developed based on schwingerkeldyshs approach using the realtime diagram technique we derive the master equation to all orders in perturbation expansions the nonmarkovian processes in the qubit dynamics is naturally taken into account the qubit decoherence in particular the influence of the tunnelingelectron fluctuation in the quantum point contact with a longer time correlation is studied in the framework we consider the lorentziantype spectral density to characterize the channel mixture of the electron tunneling processes induced by the measurement and determine the correlation time scale of the tunnelingelectron fluctuation the result shows that as the quantum point contact is casted with a narrower profile of the spectral density tunneling electrons can propagate with a longer time correlation and lead to the nonmarkovian processes of the qubit dynamics the qubit electron in the charge qubit will be driven coherently the quantum point contact measurement with the minimum deviation of the electron tunneling processes prevents the qubit state from the decoherence | [['a', 'nonequilibrium', 'theory', 'describing', 'the', 'charge', 'qubit', 'dynamics', 'measured', 'by', 'a', 'quantum', 'point', 'contact', 'is', 'developed', 'based', 'on', 'schwingerkeldyshs', 'approach', 'using', 'the', 'realtime', 'diagram', 'technique', 'we', 'derive', 'the', 'master', 'equation', 'to', 'all', 'orders', 'in', 'perturbation', 'expansions', 'the', 'nonmarkovian', 'processes', 'in', 'the', 'qubit', 'dynamics', 'is', 'naturally', 'taken', 'into', 'account', 'the', 'qubit', 'decoherence', 'in', 'particular', 'the', 'influence', 'of', 'the', 'tunnelingelectron', 'fluctuation', 'in', 'the', 'quantum', 'point', 'contact', 'with', 'a', 'longer', 'time', 'correlation', 'is', 'studied', 'in', 'the', 'framework', 'we', 'consider', 'the', 'lorentziantype', 'spectral', 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708.2582 | Density Functional Theory Characterization of the Multiferroicity in
Spin Spiral Chain Cuprates | The ferroelectricity of the spiral magnets LiCu2O2 and LiCuVO4 was examined
by calculating the electric polarizations of their spin spiral states on the
basis of density functional theory with spin-orbit coupling. Our work
unambiguously reveals that spin-orbit coupling is responsible for the
ferroelectricity with the primary contribution from the spin-orbit coupling on
the Cu sites, but the asymmetric density distribution responsible for the
electric polarization occurs mainly around the O atoms. The electric
polarization is calculated to be much greater for the ab- than for the bc-plane
spin spiral. The observed spin-spiral plane is found to be consistent with the
observed direction of the electric polarization for LiCuVO4, but inconsistent
for LiCu2O2.
| cond-mat.mtrl-sci cond-mat.str-el | the ferroelectricity of the spiral magnets licu2o2 and licuvo4 was examined by calculating the electric polarizations of their spin spiral states on the basis of density functional theory with spinorbit coupling our work unambiguously reveals that spinorbit coupling is responsible for the ferroelectricity with the primary contribution from the spinorbit coupling on the cu sites but the asymmetric density distribution responsible for the electric polarization occurs mainly around the o atoms the electric polarization is calculated to be much greater for the ab than for the bcplane spin spiral the observed spinspiral plane is found to be consistent with the observed direction of the electric polarization for licuvo4 but inconsistent for licu2o2 | [['the', 'ferroelectricity', 'of', 'the', 'spiral', 'magnets', 'licu2o2', 'and', 'licuvo4', 'was', 'examined', 'by', 'calculating', 'the', 'electric', 'polarizations', 'of', 'their', 'spin', 'spiral', 'states', 'on', 'the', 'basis', 'of', 'density', 'functional', 'theory', 'with', 'spinorbit', 'coupling', 'our', 'work', 'unambiguously', 'reveals', 'that', 'spinorbit', 'coupling', 'is', 'responsible', 'for', 'the', 'ferroelectricity', 'with', 'the', 'primary', 'contribution', 'from', 'the', 'spinorbit', 'coupling', 'on', 'the', 'cu', 'sites', 'but', 'the', 'asymmetric', 'density', 'distribution', 'responsible', 'for', 'the', 'electric', 'polarization', 'occurs', 'mainly', 'around', 'the', 'o', 'atoms', 'the', 'electric', 'polarization', 'is', 'calculated', 'to', 'be', 'much', 'greater', 'for', 'the', 'ab', 'than', 'for', 'the', 'bcplane', 'spin', 'spiral', 'the', 'observed', 'spinspiral', 'plane', 'is', 'found', 'to', 'be', 'consistent', 'with', 'the', 'observed', 'direction', 'of', 'the', 'electric', 'polarization', 'for', 'licuvo4', 'but', 'inconsistent', 'for', 'licu2o2']] | [-0.19643019072412113, 0.17721919003607972, -0.008626768623279142, 0.04609176382551335, -0.03662145451276696, -0.09792814276547038, 0.021095841816401974, 0.4095339152928708, -0.2230131693275845, -0.29092040430155713, -0.032813539379276335, -0.2932927807393883, -0.08012190174901791, 0.1640770017568554, 0.12818288869623626, -0.05539084674923548, -0.06657404236362449, -0.028804829236053462, -0.06766578798955639, -0.17099560309933232, 0.26695743265944266, 0.049483163764567246, 0.30713357462497826, 0.054990035664169615, 0.031669070170859674, 0.01686295511483747, 0.09000630183644327, 0.012141642742790282, -0.09921251595194137, 0.11020157417013772, 0.2027725814716957, -0.07416633072508765, 0.1214554553319301, -0.44587084722505615, -0.16250171281613543, 0.004891024885832199, 0.11479716502695478, 0.17987699460770404, -0.06411820216245749, -0.29382075131746077, 0.028933524237280444, -0.11005094447942351, -0.18672616500823228, -0.0654944133628825, 0.05535621989526719, 0.027043325098929927, -0.2914021304376157, 0.1142366493919066, 0.07005411368611801, 0.10212022352165409, -0.12322538133594207, -0.18195358560270897, -0.14413189586775843, 0.007196948938404343, 0.10860133594854103, 0.14591417621912633, 0.15498251541950075, -0.08748806179210078, -0.10106509652437776, 0.38247843633871526, -0.05187409326195588, -0.11532071949581482, 0.10614726178547633, -0.24894436802631909, -0.07604119123425335, 0.15821439450207567, 0.08506607149112304, 0.10517129613851596, -0.11298414518907, 0.06517919538756749, 0.01766412768795687, 0.15871010160481092, 0.0363253857275205, 0.05310915326117538, 0.3115434750631851, 0.13259053447732835, 0.038314428988607166, 0.10278275374314814, -0.1408414696301666, -0.07328285271900573, -0.21955511127037294, -0.12499722800151046, -0.23131720772965178, 0.042214447447414774, -0.06269315347045838, -0.13133935002510302, 0.4079603178376731, 0.13906420400183248, 0.131028035557912, -0.06767944804076771, 0.24832146889197507, 0.11765929669542986, 0.12035252720358715, 0.03959794554560046, 0.355419389654084, 0.23331834080870198, 0.09090939050903606, -0.3487101590934409, 0.16378965026732267, -0.04705873386202646] |
708.2583 | Boundary Harnack Principle for Subordinate Brownian Motions | We establish a boundary Harnack principle for a large class of subordinate
Brownian motion, including mixtures of symmetric stable processes, in bounded
$\kappa$-fat open set (disconnected analogue of John domains). As an
application of the boundary Harnack principle, we identify the Martin boundary
and the minimal Martin boundary of bounded $\kappa$-fat open sets with respect
to these processes with their Euclidean boundary.
| math.PR | we establish a boundary harnack principle for a large class of subordinate brownian motion including mixtures of symmetric stable processes in bounded kappafat open set disconnected analogue of john domains as an application of the boundary harnack principle we identify the martin boundary and the minimal martin boundary of bounded kappafat open sets with respect to these processes with their euclidean boundary | [['we', 'establish', 'a', 'boundary', 'harnack', 'principle', 'for', 'a', 'large', 'class', 'of', 'subordinate', 'brownian', 'motion', 'including', 'mixtures', 'of', 'symmetric', 'stable', 'processes', 'in', 'bounded', 'kappafat', 'open', 'set', 'disconnected', 'analogue', 'of', 'john', 'domains', 'as', 'an', 'application', 'of', 'the', 'boundary', 'harnack', 'principle', 'we', 'identify', 'the', 'martin', 'boundary', 'and', 'the', 'minimal', 'martin', 'boundary', 'of', 'bounded', 'kappafat', 'open', 'sets', 'with', 'respect', 'to', 'these', 'processes', 'with', 'their', 'euclidean', 'boundary']] | [-0.12871472325716768, 0.14512027410490835, -0.056736170644721674, 0.040450544366913456, -0.11193632816655501, -0.151279472565699, 0.0442062497679745, 0.3267735073778538, -0.3464310526427242, -0.18449623334961343, 0.2117907763702885, -0.27629702057569255, -0.06304619389195595, 0.19260224282381036, -0.17253284088726487, 0.1481934397841894, 0.08032427480324142, 0.007116659615759647, 0.006703986140388635, -0.16528022349549218, 0.4143975504463719, -0.14644411745511235, 0.17182897695250088, 0.12351808390550074, 0.10192178590824047, -0.043159042762952946, -0.03763516067767576, 0.027814970231584964, -0.23673811810271395, 0.17550419761438765, 0.2155596293028324, 0.04567878170599861, 0.2577948566045492, -0.3865485446107003, -0.20604569796893385, 0.16344153248674928, 0.03790182588742145, 0.02689020146781038, -0.015184529065605133, -0.37423386328643365, 0.03649220508973925, -0.048009443532435164, -0.2959302443289949, -0.013127188438609723, 0.05768087410157727, 0.0011418782955696506, -0.2848601230690556, 0.09151797985748178, 0.11940060056475622, 0.09291041299941079, -0.1520300067871088, -0.09543529552437606, -0.03817871596378785, 0.10732888681213221, -0.013430462744567663, 0.034064446575939655, 0.08428997125837111, -0.04915410724859084, -0.15468477854324925, 0.3001074861254423, -0.08769987837501592, -0.28132401656119094, 0.2529464785249964, -0.16998440138394794, -0.11935425023998945, 0.07566024133214547, 0.16426485012315453, 0.15913671658434456, -0.19043709381273197, 0.20827392906217174, -0.08437241301984497, -0.0019956326070842485, 0.19069092019250797, -0.013265183856410364, 0.11562652725561132, 0.11581861623562872, 0.1738826265228131, 0.22343541660736646, -0.0020718159446973475, -0.13685693591833115, -0.4334940377382501, -0.18030850611807359, -0.15565171788236307, 0.09625671309749445, -0.1514880319213731, -0.32057967006919846, 0.24725324668050294, 0.0923204945114952, 0.1857015648143246, 0.06886061090194891, 0.14276861460624082, 0.09427563413144878, 0.014531553523885387, 0.13764592748315585, 0.0976784189697355, 0.2056274578020337, 0.08104838400838836, -0.17981395217019222, 0.015208075236108514, 0.1461493240893751] |
708.2584 | Claw Finding Algorithms Using Quantum Walk | The claw finding problem has been studied in terms of query complexity as one
of the problems closely connected to cryptography. For given two functions, f
and g, as an oracle which have domains of size N and M (N<=M), respectively,
and the same range, the goal of the problem is to find x and y such that
f(x)=g(y). This paper describes an optimal algorithm using quantum walk that
solves this problem. Our algorithm can be generalized to find a claw of k
functions for any constant integer k>1, where the domains of the functions may
have different size.
| quant-ph cs.CC | the claw finding problem has been studied in terms of query complexity as one of the problems closely connected to cryptography for given two functions f and g as an oracle which have domains of size n and m nm respectively and the same range the goal of the problem is to find x and y such that fxgy this paper describes an optimal algorithm using quantum walk that solves this problem our algorithm can be generalized to find a claw of k functions for any constant integer k1 where the domains of the functions may have different size | [['the', 'claw', 'finding', 'problem', 'has', 'been', 'studied', 'in', 'terms', 'of', 'query', 'complexity', 'as', 'one', 'of', 'the', 'problems', 'closely', 'connected', 'to', 'cryptography', 'for', 'given', 'two', 'functions', 'f', 'and', 'g', 'as', 'an', 'oracle', 'which', 'have', 'domains', 'of', 'size', 'n', 'and', 'm', 'nm', 'respectively', 'and', 'the', 'same', 'range', 'the', 'goal', 'of', 'the', 'problem', 'is', 'to', 'find', 'x', 'and', 'y', 'such', 'that', 'fxgy', 'this', 'paper', 'describes', 'an', 'optimal', 'algorithm', 'using', 'quantum', 'walk', 'that', 'solves', 'this', 'problem', 'our', 'algorithm', 'can', 'be', 'generalized', 'to', 'find', 'a', 'claw', 'of', 'k', 'functions', 'for', 'any', 'constant', 'integer', 'k1', 'where', 'the', 'domains', 'of', 'the', 'functions', 'may', 'have', 'different', 'size']] | [-0.13738507602476713, 0.08005294444849667, -0.05125968392589717, 0.009848601423495572, -0.051506701711038445, -0.15558971260965923, 0.011900631530972367, 0.3813103809200152, -0.31508993827784904, -0.33107698654210327, 0.09139525253123444, -0.2719754824283147, -0.14524402089576904, 0.1862955173510456, -0.0771687646452902, 0.07226525926303984, 0.013637767808342522, 0.06484182917447102, -0.045639415765463404, -0.2976924701772555, 0.301648519326453, -0.03527880704848829, 0.197480085555163, 0.07609804609621112, 0.12435818607025224, 0.002008829486904421, 0.052322407441232545, 0.049798388956020574, -0.13772602096000672, 0.0800841445999333, 0.29313355699567256, 0.1645787899415338, 0.2997516729643173, -0.36278759962832086, -0.18871222255807935, 0.17066257444182129, 0.1622850846468631, 0.05116594459913257, 0.008083442235459584, -0.2037403218570457, 0.15284756698052993, -0.09135116638634543, -0.08484511649367785, 0.016052772968330166, 0.10194457350110617, 0.019827682393217326, -0.3069197134199468, -0.0032906996772972623, 0.0722937393096285, 0.010572760713973431, -0.0025824481160426982, -0.16887992714541128, 0.028269935246425296, 0.13460459348962012, 0.005610644927888055, 0.12151904498236347, 0.05141575921402134, -0.09337211372989296, -0.17584511864403582, 0.37715719683998916, -0.029966548630836035, -0.19553011208020074, 0.12426982636121336, -0.11075788607463391, -0.14139558464721447, 0.1029979921477574, 0.15822033567890298, 0.18215648118745198, -0.11113491890519256, 0.15778100224108332, -0.11599795072518214, 0.17273131398615812, 0.08031817991756882, 0.020699994102346176, 0.12009822149441172, 0.11636937644586644, 0.13431780387393452, 0.17713804265385438, -0.009686779381349833, -0.019068754447454758, -0.27266984495847024, -0.15294003917487584, -0.2359111020106333, 0.04307052795069687, -0.1314523868125186, -0.1918975141068751, 0.36287562359086795, 0.10870756408448962, 0.21292949167804587, 0.08173885415755024, 0.22366297694929696, 0.12717108485274808, 0.032389167499198755, 0.13056092887100848, 0.13576831280093904, 0.09849582116749853, 0.03578322412765989, -0.2076275925377779, 0.07884436011352021, 0.07472502620834293] |
708.2585 | Robustness of Attractor States in Complex Networks with Scale-free
Topology | We study the intrinsic properties of attractors in the Boolean dynamics in
complex network with scale-free topology, comparing with those of the so-called
random Kauffman networks. We have numerically investigated the frozen and
relevant nodes for each attractor, and the robustness of the attractors to the
perturbation that flips the state of a single node of attractors in the
relatively small network ($N=30 \sim 200$). It is shown that the rate of frozen
nodes in the complex networks with scale-free topology is larger than that in
the random Kauffman model. Furthermore, we have found that in the complex
scale-free networks with fluctuations of in-degree number the attractors are
more sensitive to the state flip of a highly connected node than to the state
flip of a less connected node.
| cond-mat.dis-nn | we study the intrinsic properties of attractors in the boolean dynamics in complex network with scalefree topology comparing with those of the socalled random kauffman networks we have numerically investigated the frozen and relevant nodes for each attractor and the robustness of the attractors to the perturbation that flips the state of a single node of attractors in the relatively small network n30 sim 200 it is shown that the rate of frozen nodes in the complex networks with scalefree topology is larger than that in the random kauffman model furthermore we have found that in the complex scalefree networks with fluctuations of indegree number the attractors are more sensitive to the state flip of a highly connected node than to the state flip of a less connected node | [['we', 'study', 'the', 'intrinsic', 'properties', 'of', 'attractors', 'in', 'the', 'boolean', 'dynamics', 'in', 'complex', 'network', 'with', 'scalefree', 'topology', 'comparing', 'with', 'those', 'of', 'the', 'socalled', 'random', 'kauffman', 'networks', 'we', 'have', 'numerically', 'investigated', 'the', 'frozen', 'and', 'relevant', 'nodes', 'for', 'each', 'attractor', 'and', 'the', 'robustness', 'of', 'the', 'attractors', 'to', 'the', 'perturbation', 'that', 'flips', 'the', 'state', 'of', 'a', 'single', 'node', 'of', 'attractors', 'in', 'the', 'relatively', 'small', 'network', 'n30', 'sim', '200', 'it', 'is', 'shown', 'that', 'the', 'rate', 'of', 'frozen', 'nodes', 'in', 'the', 'complex', 'networks', 'with', 'scalefree', 'topology', 'is', 'larger', 'than', 'that', 'in', 'the', 'random', 'kauffman', 'model', 'furthermore', 'we', 'have', 'found', 'that', 'in', 'the', 'complex', 'scalefree', 'networks', 'with', 'fluctuations', 'of', 'indegree', 'number', 'the', 'attractors', 'are', 'more', 'sensitive', 'to', 'the', 'state', 'flip', 'of', 'a', 'highly', 'connected', 'node', 'than', 'to', 'the', 'state', 'flip', 'of', 'a', 'less', 'connected', 'node']] | [-0.20675901293415258, 0.17132016006395107, -0.04247303675253724, 0.07305276137054717, 0.004421137424922267, -0.1537619858669738, 0.052604032236389646, 0.3485044718741678, -0.2681955085496974, -0.25051042229630227, 0.059426582589846594, -0.2975187297015227, -0.2161508128768945, 0.11416208965508917, -0.02163952885758738, 0.0393462996458808, 0.054990158320671716, 0.10939065931191624, 0.016744657030668426, -0.2549914990790015, 0.3501443543666324, 0.06603472274114457, 0.26738762932057064, -0.025187451969976574, 0.05521943157379942, -0.05077083438432725, 0.03198754030113765, 0.06848358997331513, -0.08971817178634545, 0.08840484313609064, 0.19020723322381142, 0.08398983193662508, 0.22554241279645484, -0.4532970342525216, -0.23221148323274918, 0.1794175687534807, 0.12997215002046017, 0.10716588624803595, 0.020732738400151586, -0.29231780319828393, 0.16206868508895642, -0.16742178475278494, -0.13496901778966303, -0.07509653296956952, 0.06427520371670294, 0.06891736590534506, -0.19903767191220162, 0.042992339572822315, 0.047349774507921216, 0.02704915961308419, -0.0034402702942259553, -0.06356326535401881, -0.12670694608349614, 0.13107079910764166, -0.011889974352932542, 0.059067048181151584, 0.11371637754820922, -0.17613996179095764, -0.13550157767771057, 0.3407005071206841, -0.008746081433672271, -0.21674177946582393, 0.1934738239533333, -0.16613807131413572, -0.18091930716493448, 0.14265027664991659, 0.1564872294678822, 0.10512103634171707, -0.117070986463349, 0.02034154705533599, -0.03538374792307962, 0.15152497141975765, 0.04155339882889575, 0.05834679352661032, 0.12026183619055637, 0.2113477460292796, 0.10872399027625373, 0.17129892626075188, -0.09001310846891052, -0.18616587233318146, -0.19084258171072763, -0.0725833771537354, -0.22733273260410905, 0.07280278692469579, -0.18864928403586806, -0.17881424794070128, 0.4801482433568715, 0.1281580817380328, 0.2653005145627341, 0.07893001879096147, 0.24598003762174947, 0.07830862158389632, 0.08041905366288599, 0.14277792528863678, 0.21310953827675924, 0.1561177137791533, 0.09210438494996508, -0.16905155296206417, 0.13812771914959993, 0.021312599084809307] |
708.2586 | The ALTCRISS project on board the International Space Station | The Altcriss project aims to perform a long term survey of the radiation
environment on board the International Space Station. Measurements are being
performed with active and passive devices in different locations and
orientations of the Russian segment of the station. The goal is to perform a
detailed evaluation of the differences in particle fluence and nuclear
composition due to different shielding material and attitude of the station.
The Sileye-3/Alteino detector is used to identify nuclei up to Iron in the
energy range above 60 MeV/n. Several passive dosimeters (TLDs, CR39) are also
placed in the same location of Sileye-3 detector. Polyethylene shielding is
periodically interposed in front of the detectors to evaluate the effectiveness
of shielding on the nuclear component of the cosmic radiation. The project was
submitted to ESA in reply to the AO in the Life and Physical Science of 2004
and data taking began in December 2005. Dosimeters and data cards are rotated
every six months: up to now three launches of dosimeters and data cards have
been performed and have been returned with the end of expedition 12 and 13.
| astro-ph | the altcriss project aims to perform a long term survey of the radiation environment on board the international space station measurements are being performed with active and passive devices in different locations and orientations of the russian segment of the station the goal is to perform a detailed evaluation of the differences in particle fluence and nuclear composition due to different shielding material and attitude of the station the sileye3alteino detector is used to identify nuclei up to iron in the energy range above 60 mevn several passive dosimeters tlds cr39 are also placed in the same location of sileye3 detector polyethylene shielding is periodically interposed in front of the detectors to evaluate the effectiveness of shielding on the nuclear component of the cosmic radiation the project was submitted to esa in reply to the ao in the life and physical science of 2004 and data taking began in december 2005 dosimeters and data cards are rotated every six months up to now three launches of dosimeters and data cards have been performed and have been returned with the end of expedition 12 and 13 | [['the', 'altcriss', 'project', 'aims', 'to', 'perform', 'a', 'long', 'term', 'survey', 'of', 'the', 'radiation', 'environment', 'on', 'board', 'the', 'international', 'space', 'station', 'measurements', 'are', 'being', 'performed', 'with', 'active', 'and', 'passive', 'devices', 'in', 'different', 'locations', 'and', 'orientations', 'of', 'the', 'russian', 'segment', 'of', 'the', 'station', 'the', 'goal', 'is', 'to', 'perform', 'a', 'detailed', 'evaluation', 'of', 'the', 'differences', 'in', 'particle', 'fluence', 'and', 'nuclear', 'composition', 'due', 'to', 'different', 'shielding', 'material', 'and', 'attitude', 'of', 'the', 'station', 'the', 'sileye3alteino', 'detector', 'is', 'used', 'to', 'identify', 'nuclei', 'up', 'to', 'iron', 'in', 'the', 'energy', 'range', 'above', '60', 'mevn', 'several', 'passive', 'dosimeters', 'tlds', 'cr39', 'are', 'also', 'placed', 'in', 'the', 'same', 'location', 'of', 'sileye3', 'detector', 'polyethylene', 'shielding', 'is', 'periodically', 'interposed', 'in', 'front', 'of', 'the', 'detectors', 'to', 'evaluate', 'the', 'effectiveness', 'of', 'shielding', 'on', 'the', 'nuclear', 'component', 'of', 'the', 'cosmic', 'radiation', 'the', 'project', 'was', 'submitted', 'to', 'esa', 'in', 'reply', 'to', 'the', 'ao', 'in', 'the', 'life', 'and', 'physical', 'science', 'of', '2004', 'and', 'data', 'taking', 'began', 'in', 'december', '2005', 'dosimeters', 'and', 'data', 'cards', 'are', 'rotated', 'every', 'six', 'months', 'up', 'to', 'now', 'three', 'launches', 'of', 'dosimeters', 'and', 'data', 'cards', 'have', 'been', 'performed', 'and', 'have', 'been', 'returned', 'with', 'the', 'end', 'of', 'expedition', '12', 'and', '13']] | [-0.08786043283212316, 0.12675615352358424, -0.05681293722047665, 0.0006816592617574465, -0.05049723555630708, -0.08865758137659753, 0.03310810067885361, 0.3962586114571972, -0.18054214116712972, -0.41996451186855416, 0.13416604111326097, -0.3633512518481239, -0.021255376923363656, 0.18784611084521494, -0.046394446396504294, 0.049088631894766956, 0.03753826192037745, 0.0111876277554944, -0.020292343741527805, -0.263979418213469, 0.2417338836585059, 0.17424192162650218, 0.2803116459552977, 0.004824794222508649, 0.1099103098481914, -0.033350677064435744, -0.08874388008888882, -0.035219622691639106, -0.07566117522931033, 0.0417090413598139, 0.27705499358925517, 0.1287376767582168, 0.23931279251669216, -0.47852220206318685, -0.1503671260478978, 0.058535921021177856, 0.05480861871766827, 0.014073869098325843, -0.03555071455679813, -0.2931632859540264, 0.05115895370881145, -0.19486549834958738, -0.11564518381183607, 0.037877931111174955, 0.03350724125854098, 0.058011309461857466, -0.20153984360417332, -0.04254454314650502, -0.02037677980171373, 0.07556612713705073, -0.09545380436499656, -0.12564204997833367, -0.006738255414497721, 0.19032962232321862, 0.03751252156739561, 0.04975684776973839, 0.18420558452835195, -0.09012927361702448, -0.07741727809176095, 0.3884027797887409, -0.02367618542092924, -0.07948749272951058, 0.18594019990388796, -0.16960282014186526, -0.10242215460511743, 0.16204775706545071, 0.22414641755704695, 0.08944200557544009, -0.19417009576848085, 0.030500545173468948, 0.006177162981827508, 0.18367547560342495, 0.08782513014675415, -0.023880919195957237, 0.19659263943577862, 0.19809137187273865, 0.024727087421854445, 0.1344223350438719, -0.20308234578684217, -0.05325897182286768, -0.2520803993946494, -0.1540396419906436, -0.14109266762990136, -0.004047047670490548, 0.002152063500853818, -0.0768895939473513, 0.3834422505383922, 0.13345393399416294, 0.13116741101231918, -0.05947026518649411, 0.2953899828026296, -0.018010225408623546, 0.08940066759516792, 0.046421617382093446, 0.31749258501260735, 0.10210921410675887, 0.16790249124988094, -0.1884807493169229, 0.037662237882614136, -0.009630209745859706] |
708.2587 | Detection of the high energy component of Jovian electrons in Low Earth
Orbit with the PAMELA experiment | The PAMELA experiment is devoted to the study of cosmic rays in Low Earth
Orbit with an apparatus optimized to perform a precise determination of the
galactic antimatter component of c.r. It is constituted by a number of
detectors built around a permanent magnet spectrometer. PAMELA was launched in
space on June 15th 2006 on board the Russian Resurs-DK1 satellite for a mission
duration of three years. The characteristics of the detectors, the long
lifetime and the orbit of the satellite, will allow to address several aspects
of cosmic-ray physics. In this work we discuss the observational capabilities
of PAMELA to detect the electron component above 50 MeV. The magnetic
spectrometer allows a detailed measurement of the energy spectrum of electrons
of galactic and Jovian origin. Long term measurements and correlations with
Earth-Jupiter 13 months synodic period will allow to separate these two
contributions and to measure the primary electron Jovian component, dominant in
the 50-70 MeV energy range. With this technique it will also be possible to
study the contribution to the electron spectrum of Jovian e- reaccelerated up
to 2 GeV at the Solar Wind Termination Shock.
| astro-ph | the pamela experiment is devoted to the study of cosmic rays in low earth orbit with an apparatus optimized to perform a precise determination of the galactic antimatter component of cr it is constituted by a number of detectors built around a permanent magnet spectrometer pamela was launched in space on june 15th 2006 on board the russian resursdk1 satellite for a mission duration of three years the characteristics of the detectors the long lifetime and the orbit of the satellite will allow to address several aspects of cosmicray physics in this work we discuss the observational capabilities of pamela to detect the electron component above 50 mev the magnetic spectrometer allows a detailed measurement of the energy spectrum of electrons of galactic and jovian origin long term measurements and correlations with earthjupiter 13 months synodic period will allow to separate these two contributions and to measure the primary electron jovian component dominant in the 5070 mev energy range with this technique it will also be possible to study the contribution to the electron spectrum of jovian e reaccelerated up to 2 gev at the solar wind termination shock | [['the', 'pamela', 'experiment', 'is', 'devoted', 'to', 'the', 'study', 'of', 'cosmic', 'rays', 'in', 'low', 'earth', 'orbit', 'with', 'an', 'apparatus', 'optimized', 'to', 'perform', 'a', 'precise', 'determination', 'of', 'the', 'galactic', 'antimatter', 'component', 'of', 'cr', 'it', 'is', 'constituted', 'by', 'a', 'number', 'of', 'detectors', 'built', 'around', 'a', 'permanent', 'magnet', 'spectrometer', 'pamela', 'was', 'launched', 'in', 'space', 'on', 'june', '15th', '2006', 'on', 'board', 'the', 'russian', 'resursdk1', 'satellite', 'for', 'a', 'mission', 'duration', 'of', 'three', 'years', 'the', 'characteristics', 'of', 'the', 'detectors', 'the', 'long', 'lifetime', 'and', 'the', 'orbit', 'of', 'the', 'satellite', 'will', 'allow', 'to', 'address', 'several', 'aspects', 'of', 'cosmicray', 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708.2588 | LHC Signatures of New Gauge Bosons in the Minimal Higgsless Model | We study the LHC signatures of new gauge bosons in the gauge-invariant
minimal Higgsless model. It predicts an extra pair of W_1 and Z_1 bosons which
can be as light as ~400GeV and play a key role in the delay of unitarity
violation. We analyze the W_1 signals in pp --> W_0Z_0Z_0 --> jj4\ell and pp
--> jj W_0Z_0 --> jj3\ell\nu processes at the LHC, including the complete
electroweak and QCD backgrounds. We reveal the complementarity between these
two channels for discovering the W_1 boson, and demonstrate the LHC discovery
potential over the full range of allowed W_1 mass.
| hep-ph hep-ex | we study the lhc signatures of new gauge bosons in the gaugeinvariant minimal higgsless model it predicts an extra pair of w_1 and z_1 bosons which can be as light as 400gev and play a key role in the delay of unitarity violation we analyze the w_1 signals in pp w_0z_0z_0 jj4ell and pp jj w_0z_0 jj3ellnu processes at the lhc including the complete electroweak and qcd backgrounds we reveal the complementarity between these two channels for discovering the w_1 boson and demonstrate the lhc discovery potential over the full range of allowed w_1 mass | [['we', 'study', 'the', 'lhc', 'signatures', 'of', 'new', 'gauge', 'bosons', 'in', 'the', 'gaugeinvariant', 'minimal', 'higgsless', 'model', 'it', 'predicts', 'an', 'extra', 'pair', 'of', 'w_1', 'and', 'z_1', 'bosons', 'which', 'can', 'be', 'as', 'light', 'as', '400gev', 'and', 'play', 'a', 'key', 'role', 'in', 'the', 'delay', 'of', 'unitarity', 'violation', 'we', 'analyze', 'the', 'w_1', 'signals', 'in', 'pp', 'w_0z_0z_0', 'jj4ell', 'and', 'pp', 'jj', 'w_0z_0', 'jj3ellnu', 'processes', 'at', 'the', 'lhc', 'including', 'the', 'complete', 'electroweak', 'and', 'qcd', 'backgrounds', 'we', 'reveal', 'the', 'complementarity', 'between', 'these', 'two', 'channels', 'for', 'discovering', 'the', 'w_1', 'boson', 'and', 'demonstrate', 'the', 'lhc', 'discovery', 'potential', 'over', 'the', 'full', 'range', 'of', 'allowed', 'w_1', 'mass']] | [-0.11805434453884488, 0.22575920974406552, -0.05584846019417375, 0.14605068024452572, -0.0314866140162429, -0.1820413678485368, 0.03537982339960533, 0.3178038175862569, -0.2590305686488256, -0.26117735929214037, 0.01521450948036675, -0.32115570235751817, -0.04264887669993626, 0.11943683731062645, 0.08078823636726036, 0.07475255717201015, 0.062799647626989, -0.00669232490063123, -0.06091256281053954, -0.24606078697116163, 0.28244408559831946, 0.031490062189462424, 0.20279581534706956, 0.12098849942181054, 0.10419408017053054, 0.10166968087471284, -0.057226307157959254, -0.11249561243751956, -0.14281378402809644, 0.045339839021255685, 0.2102678728857267, 0.09239284104186592, 0.13298435083457402, -0.3412537938444415, -0.13335547898128464, 0.20183282643351907, 0.1633845115244225, 0.10664907181354055, -0.06458248100806396, -0.3293913509492036, 0.10339079025600638, -0.21672294330322645, -0.07257153596575526, -0.03853614650574605, -0.026637112752503748, -0.0771285396422372, -0.3270892528202999, 0.08236507032127989, -0.033286109019152736, 0.025818234115102135, 0.0350764925018526, -0.14035696265093245, -0.09997789884129396, 0.04542948332727774, 0.11453329167804671, 0.032961829767593154, 0.08343436026556807, -0.2037236916290207, -0.21250752963197345, 0.4083347350338494, -0.08424207632133103, -0.14451515787168517, 0.2047617827563874, -0.1539978278892954, -0.142736189630251, 0.06453212809104186, 0.23701351932198791, 0.031736327949297295, -0.17671125423633954, 0.1712193451994508, -0.030039129717336906, 0.1317646628562975, 0.05883034797651427, 0.1662848930074168, 0.2550656990209533, 0.18746066985877005, 0.03177479734378202, 0.0652826498300963, -0.07593617679367026, -0.06727342028170824, -0.49487168521167463, -0.17370638659653756, -0.07941488149975028, 0.02700630229530641, -0.10465415515780198, -0.042447310944016166, 0.3801619218877302, 0.13345491236771692, 0.28368132646390043, 0.012467864073127263, 0.21366367491146365, 0.07324659682881947, 0.06186031302498592, 0.042817681633795686, 0.3178729980846273, 0.1367881044868257, 0.10281797508059254, -0.22935128069718133, -0.015395255534203497, 0.08808709938427085] |
708.2589 | On manifolds satisfying stable systolic inequalities | We show that for closed orientable manifolds the $k$-dimensional stable
systole admits a metric-independent volume bound if and only if there are
cohomology classes of degree $k$ that generate cohomology in top-degree.
Moreover, it turns out that in the nonorientable case such a bound does not
exist for stable systoles of dimension at least two.
Additionally, we prove that the stable systolic constant depends only on the
image of the fundamental class in a suitable Eilenberg-Mac Lane space.
Consequently, the stable $k$-systolic constant is completely determined by the
multilinear intersection form on $k$-dimensional cohomology.
| math.GT math.DG | we show that for closed orientable manifolds the kdimensional stable systole admits a metricindependent volume bound if and only if there are cohomology classes of degree k that generate cohomology in topdegree moreover it turns out that in the nonorientable case such a bound does not exist for stable systoles of dimension at least two additionally we prove that the stable systolic constant depends only on the image of the fundamental class in a suitable eilenbergmac lane space consequently the stable ksystolic constant is completely determined by the multilinear intersection form on kdimensional cohomology | [['we', 'show', 'that', 'for', 'closed', 'orientable', 'manifolds', 'the', 'kdimensional', 'stable', 'systole', 'admits', 'a', 'metricindependent', 'volume', 'bound', 'if', 'and', 'only', 'if', 'there', 'are', 'cohomology', 'classes', 'of', 'degree', 'k', 'that', 'generate', 'cohomology', 'in', 'topdegree', 'moreover', 'it', 'turns', 'out', 'that', 'in', 'the', 'nonorientable', 'case', 'such', 'a', 'bound', 'does', 'not', 'exist', 'for', 'stable', 'systoles', 'of', 'dimension', 'at', 'least', 'two', 'additionally', 'we', 'prove', 'that', 'the', 'stable', 'systolic', 'constant', 'depends', 'only', 'on', 'the', 'image', 'of', 'the', 'fundamental', 'class', 'in', 'a', 'suitable', 'eilenbergmac', 'lane', 'space', 'consequently', 'the', 'stable', 'ksystolic', 'constant', 'is', 'completely', 'determined', 'by', 'the', 'multilinear', 'intersection', 'form', 'on', 'kdimensional', 'cohomology']] | [-0.21198021223213762, 0.14803948471362285, -0.06882168830649808, 0.0677825326280807, -0.06292594157337666, -0.19123841321313792, 0.012698898255389104, 0.3536588582111166, -0.30027032251212193, -0.18893677981055162, 0.11554445574887375, -0.2085290337922646, -0.17450199269768882, 0.21526142612020385, -0.1276004304465382, -0.0387200416620583, 0.07022246719149754, 0.14832766379348616, -0.04885697647671592, -0.3306333660940699, 0.4144397552343125, -0.08450165462303669, 0.2227682036922333, 0.1008323641701978, 0.1510406751964338, -0.0492888278590436, 0.02698216536280481, 0.05103703494093312, -0.18729149528557404, 0.1087167173267362, 0.2991876072805137, 0.0680196228080449, 0.1727307157917939, -0.3512572565096173, -0.14103045361116529, 0.23337375909644872, 0.13825682109281262, -0.0065934978266979785, -0.022227691431985573, -0.21760523261532108, 0.15941464092998586, -0.06749177615525463, -0.15600455318518142, -0.10278486128199221, 0.0963590794163657, -0.04284508449602575, -0.21306803691240542, 0.013477803876702773, 0.12128499234739215, 0.042520657023216814, -0.07441986323968369, -0.09766647097793349, -0.0942516239072652, 0.09834876719322254, -0.04315817207742007, 0.04569902853852019, 0.10210130475659637, -0.08712401985317132, -0.06304608288399399, 0.34968539822272005, -0.09227589250324254, -0.25891180274645215, 0.1252292576072579, -0.16783902890970337, -0.1990351273153136, 0.17559492451317132, 0.08119493030368331, 0.204886726232523, 0.01794352664790572, 0.19759203668899258, -0.14448136977970283, 0.14078243850282038, 0.1563279531113407, -0.016222511269548472, 0.15289016792976715, 0.07707260921102096, 0.2046036517960911, 0.10326354413112487, -0.027179593334291527, -0.08396221335699901, -0.34713614815251626, -0.2067687883143353, -0.1700509364835601, 0.13953405934242913, -0.12661994116345515, -0.20883635685164878, 0.349550125617633, 0.014860124465949993, 0.17947035798049987, 0.1400197700082146, 0.2630448423504354, 0.036403547908040755, 0.061300080918528614, 0.16464458098337847, 0.18445026033379613, 0.12367923897839686, -0.08046085369262963, -0.13235859368479455, 0.04433156556370569, 0.2020673092003872] |
708.259 | Hierarchy Problem, Dilatonic Fifth Force, and Origin of Mass | Based on the fact that the scalar curvature of the internal space determines
the mass of the dilaton in higher-dimensional unified theories, we show how the
dilaton mass can explain the origin of mass and resolve the hierarchy problem.
Moreover, we show that cosmology puts a strong constraint on dilaton mass, and
requires the scale of the internal space to be larger than $10^{-9} m$.
| hep-ph gr-qc hep-th | based on the fact that the scalar curvature of the internal space determines the mass of the dilaton in higherdimensional unified theories we show how the dilaton mass can explain the origin of mass and resolve the hierarchy problem moreover we show that cosmology puts a strong constraint on dilaton mass and requires the scale of the internal space to be larger than 109 m | [['based', 'on', 'the', 'fact', 'that', 'the', 'scalar', 'curvature', 'of', 'the', 'internal', 'space', 'determines', 'the', 'mass', 'of', 'the', 'dilaton', 'in', 'higherdimensional', 'unified', 'theories', 'we', 'show', 'how', 'the', 'dilaton', 'mass', 'can', 'explain', 'the', 'origin', 'of', 'mass', 'and', 'resolve', 'the', 'hierarchy', 'problem', 'moreover', 'we', 'show', 'that', 'cosmology', 'puts', 'a', 'strong', 'constraint', 'on', 'dilaton', 'mass', 'and', 'requires', 'the', 'scale', 'of', 'the', 'internal', 'space', 'to', 'be', 'larger', 'than', '109', 'm']] | [-0.14668594984194408, 0.15828994279010938, -0.06294977386983541, 0.15015452429652215, -0.12804213852549975, -0.09704629910321763, 0.007247831371541206, 0.284253731656533, -0.2047057919204235, -0.36570322823065976, 0.0680836763429957, -0.20129397646165811, -0.10482429151351635, 0.1742235763392483, -0.05507798886929567, -0.020356470410926985, -0.012673832762699861, 0.07614158540964126, -0.12790984176815703, -0.2381415508938237, 0.4337641506240918, 0.048910289687606, 0.2053051022382883, 0.11150238843491445, 0.14240001392765686, -0.055063753578668606, -0.009832887781354098, 0.009959943554041764, -0.13526518120399067, 0.09985193704577307, 0.08536154162138701, 0.1540113314269827, 0.2097298766557987, -0.3929617823316501, -0.21636106512294365, 0.12721167403058364, 0.15452003057759542, 0.0794879523679041, -0.03891620084715004, -0.2520036931794423, 0.07627852348467479, -0.11929535574924488, -0.13174858379106108, -0.04912772751771487, -0.014447582656374344, -0.08537697238990893, -0.24580821859148833, 0.11319518042370104, 0.015777880560535078, -0.06184688674715849, -0.11057925011532811, -0.07081830970799693, -0.08902655707385677, 0.045715665344435434, 0.13848414143117574, 0.05173065947512021, 0.1535420215330445, -0.13984023897120587, -0.0586005493443316, 0.4124047206571469, -0.1262209118534184, -0.20848205126821995, 0.1400467413298499, -0.18829755268704432, -0.16780586640995282, 0.07432962704736452, 0.18269826284108254, 0.10926255878920739, -0.09493469039981182, 0.19372784359058223, -0.06912060844210478, 0.22908762254967138, 0.05785531904906607, 0.06327812029765202, 0.2963618371349115, 0.1623840822909887, 0.08412984649722392, 0.08097646853779085, -0.05461254585534334, -0.08863969130011705, -0.33554157494352416, -0.1550248150857022, -0.1450874172294369, 0.08179200699266333, -0.16400625770150398, -0.1107822574961644, 0.34553219244027367, 0.16257419559674768, 0.24804817541287497, 0.09474221837635223, 0.23771043953557427, 0.105629604567702, 0.10721262648271826, 0.07072493877405157, 0.32298289491580084, 0.1362183750821994, 0.08328614995743219, -0.3055543689093051, -0.05326375959870907, 0.06898583537684037] |
708.2591 | The off-shell Veneziano amplitude in Schnabl gauge | We give a careful definition of the open string propagator in Schnabl gauge
and present its worldsheet interpretation. The propagator requires two
Schwinger parameters and contains the BRST operator. It builds surfaces by
gluing strips of variable width to the left and to the right of off-shell
states with contracted or expanded local frames. We evaluate explicitly the
four-point amplitude of off-shell tachyons. The computation involves a subtle
boundary term, crucial to enforce the correct exchange symmetries.
Interestingly, the familiar on-shell physics emerges even though string
diagrams produce Riemann surfaces more than once. Off-shell, the amplitudes do
not factorize over intermediate on-shell states.
| hep-th | we give a careful definition of the open string propagator in schnabl gauge and present its worldsheet interpretation the propagator requires two schwinger parameters and contains the brst operator it builds surfaces by gluing strips of variable width to the left and to the right of offshell states with contracted or expanded local frames we evaluate explicitly the fourpoint amplitude of offshell tachyons the computation involves a subtle boundary term crucial to enforce the correct exchange symmetries interestingly the familiar onshell physics emerges even though string diagrams produce riemann surfaces more than once offshell the amplitudes do not factorize over intermediate onshell states | [['we', 'give', 'a', 'careful', 'definition', 'of', 'the', 'open', 'string', 'propagator', 'in', 'schnabl', 'gauge', 'and', 'present', 'its', 'worldsheet', 'interpretation', 'the', 'propagator', 'requires', 'two', 'schwinger', 'parameters', 'and', 'contains', 'the', 'brst', 'operator', 'it', 'builds', 'surfaces', 'by', 'gluing', 'strips', 'of', 'variable', 'width', 'to', 'the', 'left', 'and', 'to', 'the', 'right', 'of', 'offshell', 'states', 'with', 'contracted', 'or', 'expanded', 'local', 'frames', 'we', 'evaluate', 'explicitly', 'the', 'fourpoint', 'amplitude', 'of', 'offshell', 'tachyons', 'the', 'computation', 'involves', 'a', 'subtle', 'boundary', 'term', 'crucial', 'to', 'enforce', 'the', 'correct', 'exchange', 'symmetries', 'interestingly', 'the', 'familiar', 'onshell', 'physics', 'emerges', 'even', 'though', 'string', 'diagrams', 'produce', 'riemann', 'surfaces', 'more', 'than', 'once', 'offshell', 'the', 'amplitudes', 'do', 'not', 'factorize', 'over', 'intermediate', 'onshell', 'states']] | [-0.18890433138557394, 0.2218445747456676, -0.11925121994454016, 0.16753765980450852, -0.14288721711022181, -0.1685096242281979, 0.04399106872846707, 0.3381843204492504, -0.18973299694582096, -0.2364646846844444, 0.024384923210340435, -0.2535169435466088, -0.10794785408782366, 0.07852416368341525, -0.039463639322349586, 0.02988245363010419, 0.07154665442038942, 0.05678610796181178, -0.12748797906752568, -0.25396975968937274, 0.34233088037270365, -0.014913150678994586, 0.21891869458333743, 0.08312362998054879, 0.1298176036103294, 0.11027271692184461, -0.08249717797785636, -0.06579188159802585, -0.07735399591049306, 0.08407218906422625, 0.22411357372709848, 0.07096960295434789, 0.10771423709596896, -0.46369782733296955, -0.1581190997097207, 0.05144499482822071, 0.2009973412298245, 0.12859032359607156, 0.05628575771542388, -0.2794434482828506, 0.011911686862484344, -0.14236973818771323, -0.1700692016968178, -0.13273487442164023, 0.022470279081353864, -0.16390873217792476, -0.20625880302339158, 0.09408404478278842, 0.02539450391331344, 0.010114999126317432, -0.009496546161668465, -0.1280415079384608, -0.11624160348844614, 0.09759586302843849, 0.10348902239568206, 0.0762908447102092, 0.13728514874709466, -0.20640073563287303, -0.09480786840804373, 0.3251429177906581, -0.02039950851701964, -0.25930370904224953, 0.13731482155729555, -0.1175131792184508, -0.12987350520578403, 0.1297588207684367, 0.03597171361404426, 0.12917200291022948, -0.1759747219027825, 0.20159462579238924, 0.011030003486101706, 0.1405192313984814, 0.15240378317974726, 0.05740538422126793, 0.19932721284878196, 0.04178988495705993, 0.030138376763416002, 0.14767480434542432, 0.004392528703020325, -0.13137847414800843, -0.4430753723673016, -0.13825772423749266, -0.0660416069621383, 0.07718102500612341, -0.09002771384144333, -0.2493570806295837, 0.38750222390427175, 0.13771047374432527, 0.1788747992998925, 0.07114234433319529, 0.24778957345785158, 0.13615620457250804, 0.15129415856818984, 0.06883509626083112, 0.2046900157719507, 0.17230744107662546, 0.06132988929545091, -0.22874496259740146, -0.055787577499517974, 0.19491802507477984] |
708.2592 | Triplet-singlet relaxation in semiconductor single and double quantum
dots | We study the triplet-singlet relaxation in two-electron semiconductor quantum
dots. Both single dots and vertically coupled double dots are discussed. In our
work, the electron-electron Coulomb interaction, which plays an important role
in the electronic structure, is included. The spin mixing is caused by
spin-orbit coupling which is the key to the triplet-singlet relaxation. We show
that the selection rule widely used in the literature is incorrect unless near
the crossing/anticrossing point in single quantum dots. The triplet/singlet
relaxation in double quantum dots can be markedly changed by varying barrier
height, inter-dot distance, external magnetic field and dot size.
| cond-mat.mtrl-sci cond-mat.mes-hall | we study the tripletsinglet relaxation in twoelectron semiconductor quantum dots both single dots and vertically coupled double dots are discussed in our work the electronelectron coulomb interaction which plays an important role in the electronic structure is included the spin mixing is caused by spinorbit coupling which is the key to the tripletsinglet relaxation we show that the selection rule widely used in the literature is incorrect unless near the crossinganticrossing point in single quantum dots the tripletsinglet relaxation in double quantum dots can be markedly changed by varying barrier height interdot distance external magnetic field and dot size | [['we', 'study', 'the', 'tripletsinglet', 'relaxation', 'in', 'twoelectron', 'semiconductor', 'quantum', 'dots', 'both', 'single', 'dots', 'and', 'vertically', 'coupled', 'double', 'dots', 'are', 'discussed', 'in', 'our', 'work', 'the', 'electronelectron', 'coulomb', 'interaction', 'which', 'plays', 'an', 'important', 'role', 'in', 'the', 'electronic', 'structure', 'is', 'included', 'the', 'spin', 'mixing', 'is', 'caused', 'by', 'spinorbit', 'coupling', 'which', 'is', 'the', 'key', 'to', 'the', 'tripletsinglet', 'relaxation', 'we', 'show', 'that', 'the', 'selection', 'rule', 'widely', 'used', 'in', 'the', 'literature', 'is', 'incorrect', 'unless', 'near', 'the', 'crossinganticrossing', 'point', 'in', 'single', 'quantum', 'dots', 'the', 'tripletsinglet', 'relaxation', 'in', 'double', 'quantum', 'dots', 'can', 'be', 'markedly', 'changed', 'by', 'varying', 'barrier', 'height', 'interdot', 'distance', 'external', 'magnetic', 'field', 'and', 'dot', 'size']] | [-0.1588495752907225, 0.2114587021691366, 0.008103380580812844, 0.04915341614669531, 0.05125024425322, -0.2137663800944099, -0.001945931918215843, 0.41048747834236343, -0.32454096648975145, -0.2672210639076574, -0.03935164930916638, -0.25862834941861884, -0.1347505766708328, 0.20245963337888218, 0.03677001088021361, 0.004499571901575035, 0.009501895940938622, -0.0445790764714154, -0.025047366357674555, -0.20979442464292278, 0.30047223630256725, 0.03741841591367194, 0.2807390665854042, 0.11683462754994327, -0.007732834080139137, 0.07548253159323821, 0.13373695524903584, 0.000758501187879212, -0.1444846058805023, 0.0442806518902736, 0.2289230193169455, -0.08325832432649118, 0.26435520948737634, -0.46444695024770133, -0.12570607224099187, 0.018916604992914563, 0.21692202822305262, 0.16348369539316213, -0.06541378346476134, -0.2746394342785625, 0.009104983800337935, -0.11917390094206393, -0.06230568894356185, -0.020704239502321094, -0.001529459681181351, 0.0066842918678623985, -0.2849175743075629, 0.07431674589003835, 0.07357184014910338, 0.005469401357505395, 0.019744425886120572, -0.10881187684111754, -0.0008743219624026393, 0.10970018666275606, 0.029222440558998863, 0.08165892163928294, 0.22674230564081546, -0.09844962069443997, -0.15576164188262606, 0.33823855307751466, -0.06046000510758283, -0.15383184062583105, 0.11402533908982818, -0.16214551013533254, -0.06679000231266326, 0.10337581957823463, 0.08620633448626162, 0.10280814745382653, -0.14745127244636283, 0.16074973274359708, 0.02721743535592544, 0.17869887728278516, 0.04313758803930666, 0.10690299857274763, 0.25241346472912296, 0.1563509968869692, 0.0337751394099727, 0.12107099487080372, -0.1470270929810572, -0.19663985339658602, -0.252353896862086, -0.17372993440177215, -0.24250508643382665, 0.14074655309110423, -0.07548160124445401, -0.16392265699271644, 0.3704364925794593, 0.11653082650059796, 0.1483119330772826, -0.13668486361667437, 0.24352849766193907, 0.18784941226476803, 0.09380910536559413, -0.00278704373489077, 0.2774590781737803, 0.21212256346753208, 0.01710654572317643, -0.37264386480864214, 0.0660735031599369, -0.0123392051176111] |
708.2593 | Derivation of Relativistic law of Addition of Velocities from
Superposition of Eigenfunctions and Discreteness | We have defined a slowness, s, as the reciprocal conjugate of velocity, v. s
= -ih/v. We have shown that Einstein's postulate (v has an upper limit) implies
that s is discrete. A velocity operator is defined as the derivative with
respect to s. Superposition of corresponding Eigenfunctions give Galilean law
of addition of velocities. We have replaced the differential operator by the
corresponding finite difference symmetric operator. We have shown that
superposition of corresponding discrete Eigenfunctions give relativistic law of
addition of velocities. A reciprocal symmetric number system is developed and
with the help of this number system we have shown the relation between
superposition and relativistic law of addition of velocities.
| physics.gen-ph | we have defined a slowness s as the reciprocal conjugate of velocity v s ihv we have shown that einsteins postulate v has an upper limit implies that s is discrete a velocity operator is defined as the derivative with respect to s superposition of corresponding eigenfunctions give galilean law of addition of velocities we have replaced the differential operator by the corresponding finite difference symmetric operator we have shown that superposition of corresponding discrete eigenfunctions give relativistic law of addition of velocities a reciprocal symmetric number system is developed and with the help of this number system we have shown the relation between superposition and relativistic law of addition of velocities | [['we', 'have', 'defined', 'a', 'slowness', 's', 'as', 'the', 'reciprocal', 'conjugate', 'of', 'velocity', 'v', 's', 'ihv', 'we', 'have', 'shown', 'that', 'einsteins', 'postulate', 'v', 'has', 'an', 'upper', 'limit', 'implies', 'that', 's', 'is', 'discrete', 'a', 'velocity', 'operator', 'is', 'defined', 'as', 'the', 'derivative', 'with', 'respect', 'to', 's', 'superposition', 'of', 'corresponding', 'eigenfunctions', 'give', 'galilean', 'law', 'of', 'addition', 'of', 'velocities', 'we', 'have', 'replaced', 'the', 'differential', 'operator', 'by', 'the', 'corresponding', 'finite', 'difference', 'symmetric', 'operator', 'we', 'have', 'shown', 'that', 'superposition', 'of', 'corresponding', 'discrete', 'eigenfunctions', 'give', 'relativistic', 'law', 'of', 'addition', 'of', 'velocities', 'a', 'reciprocal', 'symmetric', 'number', 'system', 'is', 'developed', 'and', 'with', 'the', 'help', 'of', 'this', 'number', 'system', 'we', 'have', 'shown', 'the', 'relation', 'between', 'superposition', 'and', 'relativistic', 'law', 'of', 'addition', 'of', 'velocities']] | [-0.16134586970233736, 0.1451991589149714, -0.12679221143690148, 0.0009541970295915464, -0.07698781402815166, -0.12810839255768303, -0.01148067363370042, 0.3466558704857488, -0.258362209038423, -0.26376919664687953, 0.03275280445394618, -0.2715133641519257, -0.1029510077567318, 0.1675316604569571, -0.03711817735336251, 0.05920719176212007, 0.004794838011835341, 0.11784544473446838, -0.1001051854864518, -0.1844963174950969, 0.34008162960342997, -0.003498187439667212, 0.23156746340965903, -0.004924984548140217, 0.15500549688465423, -0.043753806723969745, -0.038120813793628604, 0.06055120782777751, -0.10924363032350189, 0.1003701732921842, 0.17520017016611927, 0.09085077998807302, 0.25619990559848577, -0.38409459100918725, -0.1923456634206043, 0.13344860821123328, 0.1455849439392353, 0.0417966152130215, -0.02500045805464725, -0.2746899689270838, 0.0817050712585852, -0.22195394263342694, -0.21019788109487644, -0.060828146432434116, 0.11239787765048645, 0.06601384884535193, -0.23516769972336185, 0.13646037812000728, 0.10484221792698058, 0.06660554562417396, -0.05567329628225248, -0.10049883796212573, -0.08492523901634388, 0.06776592977395332, 0.04551966428161003, 0.015484642917038622, 0.024599817019325117, -0.019814294970569177, -0.09271041224165275, 0.40502803410227234, -0.09837863128212793, -0.23120234436816997, 0.12608001830039528, -0.16980614436387614, -0.046011296981895294, 0.09818404093300512, 0.14533404637597971, 0.11710654064872132, -0.1081135897301473, 0.14351843376455173, -0.10538413156629414, 0.10686436395983102, 0.11235189285162869, 0.06138520953371315, 0.15673644943917925, 0.029550617627866635, 0.10540676884025939, 0.12030733869251636, -0.08431567436478495, -0.0772400119316739, -0.3631186990050582, -0.17078697635332826, -0.20341911213892, 0.08471881792888986, -0.0749827248066861, -0.13460270136092403, 0.3339123933970391, 0.09450281700035473, 0.20088725817297493, 0.0792923707447879, 0.17951663373759738, 0.259316736617522, 0.0541689723293792, 0.09316190832655306, 0.2223236258015842, 0.2220445967463961, 0.07999601307417359, -0.2418218311887268, 0.035342842734813154, 0.141349342274102] |
708.2594 | Molecular Aspect of Annelid Neuroendocrine system | Hormonal processes along with enzymatic processing similar to that found in
vertebrates occur in annelids. Amino acid sequence determination of annelids
precursor gene products reveals the presence of the respective peptides that
exhibit high sequence identity to their mammalian counterparts. Furthermore,
these neuropeptides exert similar physiological function in annelids than the
ones found in vertebrates. In this respect, the high conservation in course of
evolution of these molecules families reflects their importance. Nevertheless,
some specific neuropeptides to annelids or invertebrates have also been in
these animals.
| q-bio.NC | hormonal processes along with enzymatic processing similar to that found in vertebrates occur in annelids amino acid sequence determination of annelids precursor gene products reveals the presence of the respective peptides that exhibit high sequence identity to their mammalian counterparts furthermore these neuropeptides exert similar physiological function in annelids than the ones found in vertebrates in this respect the high conservation in course of evolution of these molecules families reflects their importance nevertheless some specific neuropeptides to annelids or invertebrates have also been in these animals | [['hormonal', 'processes', 'along', 'with', 'enzymatic', 'processing', 'similar', 'to', 'that', 'found', 'in', 'vertebrates', 'occur', 'in', 'annelids', 'amino', 'acid', 'sequence', 'determination', 'of', 'annelids', 'precursor', 'gene', 'products', 'reveals', 'the', 'presence', 'of', 'the', 'respective', 'peptides', 'that', 'exhibit', 'high', 'sequence', 'identity', 'to', 'their', 'mammalian', 'counterparts', 'furthermore', 'these', 'neuropeptides', 'exert', 'similar', 'physiological', 'function', 'in', 'annelids', 'than', 'the', 'ones', 'found', 'in', 'vertebrates', 'in', 'this', 'respect', 'the', 'high', 'conservation', 'in', 'course', 'of', 'evolution', 'of', 'these', 'molecules', 'families', 'reflects', 'their', 'importance', 'nevertheless', 'some', 'specific', 'neuropeptides', 'to', 'annelids', 'or', 'invertebrates', 'have', 'also', 'been', 'in', 'these', 'animals']] | [-0.10943679505049489, 0.1551837491109794, -0.023110549312171547, 0.08070389265167462, -0.0035897712250305123, -0.10851021619990121, 0.022496362744700595, 0.43735938891768456, -0.22653048879705195, -0.2866022798407357, 0.0573813391072394, -0.2865080026649805, -0.21063072218418902, 0.1565054029112595, -0.095073735839579, -0.024306518193550928, 0.07136294684307866, 0.06309923706549155, 0.030705077882293007, -0.22025876847463985, 0.21380007314647353, 0.052122878576737156, 0.25702514448528024, -0.006788564255721, 0.05981929303515096, -0.08700514231743507, -0.027446420860563425, -0.07792444178986169, -0.10827291671401242, 0.11738960539142407, 0.307866606179105, 0.11469591653981615, 0.23617622100336608, -0.454310727587273, -0.21714110834372424, 0.15130257340646242, 0.1862913691898981, 0.10790194852580857, -0.06683263580076569, -0.21003927205970815, 0.1057686070413437, -0.11620736969797331, -0.08372200356774726, -0.06135807886752192, 0.048570417127636975, 0.12298382563668109, -0.1506036466751031, 0.14669382487400706, 0.0370996473736108, 0.14795601204427522, -0.11574998807681855, -0.18381634762857196, -0.11099660686260565, 0.1954538821822119, 0.11790150332502848, -0.008964765145508357, 0.21340291303864053, -0.12944865884898274, -0.09583491447779653, 0.3368780313622813, -0.02117074498731432, -0.16889230105592762, 0.26667809571940887, -0.1836160546802201, -0.22861121128161632, 0.17893944220444144, 0.1268935438805953, 0.09157727798447013, -0.17278883539595055, -0.057439597588855515, 0.03000315956684739, 0.14531424095810846, 0.1707220216346688, 0.06477522284745477, 0.20205459046870644, 0.12178154532299486, -0.02133720654853468, 0.110514257617598, -0.0034354338205830996, -0.10216913957738989, -0.15559371549982665, -0.1663830512593132, -0.07500197696174647, 0.052297208122475895, -0.08856652334852275, -0.17993501710656726, 0.3505045523986134, 0.11255607195756924, 0.17181202856997072, 0.060755767263905254, 0.16628646148845208, 0.019391119639865707, 0.14894216735630708, -0.03644466309180094, 0.18277646821204757, 0.08911097486405958, 0.11320474502890436, -0.2581820579592225, 0.20430880185246447, -0.004332390862928573] |
708.2595 | Manipulating the spin texture in spin-orbit superlattice by terahertz
radiation | The spin texture in a gate-controlled superlattice with Rashba spin-orbit
coupling is studied in the presence of external terahertz radiation causing the
superlattice miniband transitions. It is shown that the local distribution of
spin density can be flipped by tuning the radiation intensity, allowing the
controlled coupling of spins and photons with different polarizations.
| cond-mat.mes-hall | the spin texture in a gatecontrolled superlattice with rashba spinorbit coupling is studied in the presence of external terahertz radiation causing the superlattice miniband transitions it is shown that the local distribution of spin density can be flipped by tuning the radiation intensity allowing the controlled coupling of spins and photons with different polarizations | [['the', 'spin', 'texture', 'in', 'a', 'gatecontrolled', 'superlattice', 'with', 'rashba', 'spinorbit', 'coupling', 'is', 'studied', 'in', 'the', 'presence', 'of', 'external', 'terahertz', 'radiation', 'causing', 'the', 'superlattice', 'miniband', 'transitions', 'it', 'is', 'shown', 'that', 'the', 'local', 'distribution', 'of', 'spin', 'density', 'can', 'be', 'flipped', 'by', 'tuning', 'the', 'radiation', 'intensity', 'allowing', 'the', 'controlled', 'coupling', 'of', 'spins', 'and', 'photons', 'with', 'different', 'polarizations']] | [-0.24012655097154761, 0.292703028526847, 0.01712708451129772, -0.018095530513501552, -0.02454755917467453, -0.17823310116202468, -0.00507280342625799, 0.4529783391152267, -0.2686997948869787, -0.3594120463563336, -0.06612455519347417, -0.24997890409496096, -0.07253072626405845, 0.14629729657813353, 0.07428204606252688, -0.026030016614607087, -0.06164299688060527, -0.10988750677831748, -0.06811641547742679, -0.17547684904463864, 0.29612935650894306, 0.03738001840947955, 0.3161884028447309, 0.0784547308942786, 0.06614243668607539, 0.04792579902439482, 0.13199506318024187, -0.033246661312188265, -0.04320546756652119, 0.0348000544278572, 0.21649091651111288, -0.13276738921801248, 0.16648539452365152, -0.4537173548230418, -0.21604953526898665, 0.026143256730089586, 0.13299676427548682, 0.1863241539578195, -0.07602583444935994, -0.3239583018822251, -0.03263458419867136, -0.15654595427353074, -0.1121691712954392, -0.05595700577315357, -0.0074950602871400335, 0.0014396524401726547, -0.3111487475603267, 0.04721571137714717, 0.05398801064843105, 0.03842653320343406, -0.07007601959372146, -0.031659983193363855, -0.14504578490569084, 0.06077663994532217, 0.08946045845988448, 0.07153078739496845, 0.21890396586860772, -0.12876187894424354, -0.1413645384212335, 0.341425648511008, -0.11485735113146128, -0.18560271137997647, 0.11382221786684736, -0.23458751181519968, 0.006498961450739039, 0.1647625591054007, 0.09598903025121049, 0.09311951446795354, -0.1311277276750102, 0.11816637668029957, 0.02510677178657648, 0.17634259992175633, 0.09369830615577046, 0.1074624875370689, 0.33736399443889103, 0.14433678043833761, 0.04856498070337154, 0.1541607772254523, -0.15847411175706871, -0.03878289970776273, -0.1979719773624782, -0.08014821697509399, -0.2670768951928174, 0.10173335281649122, -0.09706598139961932, -0.13047299091865877, 0.47856624109705015, 0.16234399555078535, 0.12953371966809588, -0.0851762746633203, 0.2800066268019792, 0.18024628534826828, 0.11759444792685961, -0.0104777661272911, 0.3152842482517439, 0.20481941432053982, 0.056815023848752456, -0.3543577941858934, 0.06764160349309721, -0.08861599236088633] |
708.2596 | Soliton transverse instabilities in nonlocal nonlinear media | We analyze the transverse instabilities of spatial bright solitons in
nonlocal nonlinear media, both analytically and numerically. We demonstrate
that the nonlocal nonlinear response leads to a dramatic suppression of the
transverse instability of the soliton stripes, and we derive the asymptotic
expressions for the instability growth rate in both short- and long-wave
approximations.
| physics.optics | we analyze the transverse instabilities of spatial bright solitons in nonlocal nonlinear media both analytically and numerically we demonstrate that the nonlocal nonlinear response leads to a dramatic suppression of the transverse instability of the soliton stripes and we derive the asymptotic expressions for the instability growth rate in both short and longwave approximations | [['we', 'analyze', 'the', 'transverse', 'instabilities', 'of', 'spatial', 'bright', 'solitons', 'in', 'nonlocal', 'nonlinear', 'media', 'both', 'analytically', 'and', 'numerically', 'we', 'demonstrate', 'that', 'the', 'nonlocal', 'nonlinear', 'response', 'leads', 'to', 'a', 'dramatic', 'suppression', 'of', 'the', 'transverse', 'instability', 'of', 'the', 'soliton', 'stripes', 'and', 'we', 'derive', 'the', 'asymptotic', 'expressions', 'for', 'the', 'instability', 'growth', 'rate', 'in', 'both', 'short', 'and', 'longwave', 'approximations']] | [-0.2051783581264317, 0.10150302029042332, -0.1044117477722466, 0.13739451935894234, -0.059393128776853835, -0.07378480223835343, -0.0447614075577197, 0.35696811102227205, -0.23572332018348216, -0.18615013305787687, 0.09030122089596396, -0.27050672158279837, -0.18770471827506466, 0.16737824498192855, 0.04420760154931082, 0.07309142145418769, -0.0051420318799231335, -0.058028711661420485, -0.04503249342087656, -0.1795582700934675, 0.2950083274670221, 0.0019983520550239417, 0.3458788311281414, 0.10006905554069413, 0.0859176069325595, 0.003982900314171005, -0.0022540300981038148, 0.010788681951385957, -0.2376277247252195, 0.013073133252975013, 0.18881820307837593, -0.028805739886593074, 0.2653217067493609, -0.492276886685027, -0.2221682935228778, 0.04921360453698543, 0.22427348668376604, 0.22602077635625997, -0.048549095565384184, -0.2507294220591171, 0.03917991530357136, -0.1415826911796574, -0.1850566633425101, -0.09262835033479389, 0.013842264431770201, 0.10864764817718726, -0.27809693703979804, 0.2073910122487211, 0.10427163699986758, -0.002445571503981396, -0.09661121543979755, 0.0213416235142008, -0.06643552507308347, 0.023811957264250075, 0.09475465349364472, -0.07144018255726055, 0.044587125475690874, -0.2109272933944508, -0.06958408565777871, 0.32651240152686284, -0.1601192961981589, -0.19274965709903175, 0.18528520496544876, -0.18403615276501686, 0.025142204775302497, 0.1751791201531887, 0.2629971834227305, 0.133609925603701, -0.10579862009251008, 0.004681972680070127, 0.018365158664959448, 0.14249570299526332, 0.13459930070503442, 0.10245954461775168, 0.17095976490182457, 0.17696140271921953, 0.018505473138281592, 0.19777561412020414, -0.11140969027420161, -0.11408679084679871, -0.3165610443662714, -0.07466245678908846, -0.08487029523692197, 0.01666141789475525, -0.140472582644078, -0.18450145604502824, 0.4595587430176912, 0.13340461643895618, 0.1597064343039636, 0.028383705799502355, 0.26479482202342264, 0.19767003999678073, 0.022622058107690128, 0.1008806053928479, 0.29963868072566885, 0.15970291733672773, 0.1469363106276702, -0.3537789615198832, -0.014774473034776747, 0.051739415981703334] |
708.2597 | Mechanisms of dissipation in wet granular matter | The impact dynamics between wet surfaces, which dominates the mechanical
properties of wet granular matter, is studied both experimentally and
theoretically. It is shown that the hysteretic formation and rupture of liquid
capillary bridges between adjacent grains accounts reasonably well for most
relevant cases of wet granular matter. The various dissipation mechanisms are
discussed with particular emphasis on their relevance. Variations of the
rupture energy loss with the impact energy are quantified and discussed.
| cond-mat.soft | the impact dynamics between wet surfaces which dominates the mechanical properties of wet granular matter is studied both experimentally and theoretically it is shown that the hysteretic formation and rupture of liquid capillary bridges between adjacent grains accounts reasonably well for most relevant cases of wet granular matter the various dissipation mechanisms are discussed with particular emphasis on their relevance variations of the rupture energy loss with the impact energy are quantified and discussed | [['the', 'impact', 'dynamics', 'between', 'wet', 'surfaces', 'which', 'dominates', 'the', 'mechanical', 'properties', 'of', 'wet', 'granular', 'matter', 'is', 'studied', 'both', 'experimentally', 'and', 'theoretically', 'it', 'is', 'shown', 'that', 'the', 'hysteretic', 'formation', 'and', 'rupture', 'of', 'liquid', 'capillary', 'bridges', 'between', 'adjacent', 'grains', 'accounts', 'reasonably', 'well', 'for', 'most', 'relevant', 'cases', 'of', 'wet', 'granular', 'matter', 'the', 'various', 'dissipation', 'mechanisms', 'are', 'discussed', 'with', 'particular', 'emphasis', 'on', 'their', 'relevance', 'variations', 'of', 'the', 'rupture', 'energy', 'loss', 'with', 'the', 'impact', 'energy', 'are', 'quantified', 'and', 'discussed']] | [-0.15132011116224317, 0.23074308090616721, -0.06947950935746366, 0.10725653480197228, -0.017151220802318404, -0.11378005388620738, -0.01316321242248287, 0.3978402471622905, -0.24377321942891875, -0.3155619558702047, 0.06245671746925124, -0.2579372363366388, -0.2012160064249828, 0.199241379275918, 0.008400920602316791, 0.07863422976083097, -0.0010396490200749926, -0.0682696454176629, -0.020169579952552513, -0.21920893988194498, 0.2760732757380685, 0.08746727926002161, 0.32827125962924314, 0.17127661435547084, 0.09090855174597252, -0.02972782856591653, -0.017230782909570513, 0.03953057298346992, -0.22917333886869382, 0.030167035909520613, 0.23490717133658157, -0.04131753175720774, 0.20945140374572696, -0.4921410442707506, -0.29915600658922986, 0.08121475416260797, 0.04847330551254689, 0.043227909590633634, -0.0797845598458111, -0.1968659485841321, 0.02044077974593116, -0.1572647702225761, -0.08062186493613832, -0.020187913496802386, 0.06643499768767003, 0.10816003392234985, -0.17011979109028708, 0.13813120258871364, 0.043742176209815554, 0.033424700358630835, -0.08510178317177437, -0.09764729023634179, -0.11888826900079998, 0.10498169530183077, 0.09922293009160943, -0.10057769335705687, 0.266993661694279, -0.15650475479511394, -0.019167949370033032, 0.45543849886067816, 0.002822122728527599, -0.1683357683690013, 0.2628168603531211, -0.13280902898278893, -0.02905482253865213, 0.16084267105907202, 0.14111208392156138, 0.0666370132585635, -0.15706756929992824, -0.014329854992841295, 0.023259978149891704, 0.09741104288479767, 0.11554371876440742, 0.046333820087130405, 0.26183084907589127, 0.2767020309236958, -0.039380508168235524, 0.1612115296963099, -0.1041995585688415, -0.14949535719446233, -0.2872891455410501, -0.13968295085785054, -0.1848467600129142, -0.0468249823268805, -0.058255131028606744, -0.1349691796077988, 0.3258908201210402, 0.07688330979766073, 0.19381637387984507, -0.009226413247037074, 0.2718541360258855, 0.02213160915778497, 0.005504522463180931, 0.06985920388251543, 0.31877785776364237, 0.16218290355912335, 0.09416153574538594, -0.2781186718651018, 0.17998791942247064, -0.034905484682452435] |
708.2598 | Mechanism for linear preferential attachment in growing networks | The network properties of a graph ensemble subject to the constraints imposed
by the expected degree sequence are studied. It is found that the linear
preferential attachment is a fundamental rule, as it keeps the maximal entropy
in sparse growing networks. This provides theoretical evidence in support of
the linear preferential attachment widely exists in real networks and adopted
as a crucial assumption in growing network models. Besides, in the sparse
limit, we develop a method to calculate the degree correlation and clustering
coefficient in our ensemble model, which is suitable for all kinds of sparse
networks including the BA model, proposed by Barabasi and Albert.
| physics.data-an physics.soc-ph | the network properties of a graph ensemble subject to the constraints imposed by the expected degree sequence are studied it is found that the linear preferential attachment is a fundamental rule as it keeps the maximal entropy in sparse growing networks this provides theoretical evidence in support of the linear preferential attachment widely exists in real networks and adopted as a crucial assumption in growing network models besides in the sparse limit we develop a method to calculate the degree correlation and clustering coefficient in our ensemble model which is suitable for all kinds of sparse networks including the ba model proposed by barabasi and albert | [['the', 'network', 'properties', 'of', 'a', 'graph', 'ensemble', 'subject', 'to', 'the', 'constraints', 'imposed', 'by', 'the', 'expected', 'degree', 'sequence', 'are', 'studied', 'it', 'is', 'found', 'that', 'the', 'linear', 'preferential', 'attachment', 'is', 'a', 'fundamental', 'rule', 'as', 'it', 'keeps', 'the', 'maximal', 'entropy', 'in', 'sparse', 'growing', 'networks', 'this', 'provides', 'theoretical', 'evidence', 'in', 'support', 'of', 'the', 'linear', 'preferential', 'attachment', 'widely', 'exists', 'in', 'real', 'networks', 'and', 'adopted', 'as', 'a', 'crucial', 'assumption', 'in', 'growing', 'network', 'models', 'besides', 'in', 'the', 'sparse', 'limit', 'we', 'develop', 'a', 'method', 'to', 'calculate', 'the', 'degree', 'correlation', 'and', 'clustering', 'coefficient', 'in', 'our', 'ensemble', 'model', 'which', 'is', 'suitable', 'for', 'all', 'kinds', 'of', 'sparse', 'networks', 'including', 'the', 'ba', 'model', 'proposed', 'by', 'barabasi', 'and', 'albert']] | [-0.10209680034752654, 0.06635058537687895, -0.048462241369668604, 0.06657804050131368, -0.04185716782801978, -0.14570825423975037, 0.03312507112409463, 0.38027465060948534, -0.281105681322515, -0.272430019751894, 0.05797490356094643, -0.2533040949371907, -0.23350547852416365, 0.13389120078294203, -0.023463664264506044, 0.08209914848195249, 0.03571108345904405, 0.07187718511471208, 0.022705347975715995, -0.24714935058535664, 0.30238898344478515, 0.09964712073516874, 0.35447545172119477, 0.029637391459337383, 0.09942293345471317, 0.03481313433357567, -0.045965139754116535, 0.058032260891401545, -0.09318420262206928, 0.14180279394308598, 0.21824101242830538, 0.16676943772911745, 0.29985018260776997, -0.4007066836721211, -0.28049934879472516, 0.1391669710535767, 0.10982531219070672, 0.10770943710352031, -0.039078719764596447, -0.20388519691900825, 0.09914222972485114, -0.17617239749618094, -0.10432804954888404, -0.06810059472215625, 0.040286591638951506, 0.0497407914789499, -0.3154488732419987, 0.08492686283194793, 0.11523992099957366, 0.039866570769897046, -0.015427491592489323, -0.11814697887221316, -0.027899900552342243, 0.10344341839663684, 0.024515055796518078, 0.021615238765799353, 0.07941318057336898, -0.12418486432497443, -0.13709818955701952, 0.39339619335490017, -0.07499698021906023, -0.20040319732583636, 0.1854495744589927, -0.07352023868698557, -0.18362430992694395, 0.07640565162577298, 0.18273754384509236, 0.08788928280162783, -0.15878457023393153, 0.078682522634857, -0.07662773683649611, 0.1400622449780129, 0.023699573702442477, -0.009384485892951488, 0.17674585426542558, 0.20585413040804132, 0.07677886249796259, 0.13596949801134509, -0.06457427220050034, -0.12352657158648209, -0.22238146431111502, -0.09225438060326818, -0.223114494832874, 0.011784790523069084, -0.15563994366634432, -0.17440264766820585, 0.3971314232726142, 0.13653899426352373, 0.22763036069776513, 0.07973633697014829, 0.2532157791143652, 0.09784374626261129, 0.08766635921168721, 0.08403921771776986, 0.23099987967080385, 0.17794976577180316, 0.08970288435910952, -0.16124619744313917, 0.14202930508752548, 0.0556029974689426] |
708.2599 | Extragalactic jets on subpc and large scales | Jets can be probed in their innermost regions (d~0.1 pc) through the study of
the relativistically-boosted emission of blazars. On the other extreme of
spatial scales, the study of structure and dynamics of extragalactic
relativistic jets received renewed impulse after the discovery, made by
Chandra, of bright X-ray emission from regions at distances larger than
hundreds of kpc from the central engine. At both scales it is thus possible to
infer some of the basic parameters of the flow (speed, density, magnetic field
intensity, power). After a brief review of the available observational
evidence, I discuss how the comparison between the physical quantities
independently derived at the two scales can be used to shed light on the global
dynamics of the jet, from the innermost regions to the hundreds of kpc scale.
| astro-ph | jets can be probed in their innermost regions d01 pc through the study of the relativisticallyboosted emission of blazars on the other extreme of spatial scales the study of structure and dynamics of extragalactic relativistic jets received renewed impulse after the discovery made by chandra of bright xray emission from regions at distances larger than hundreds of kpc from the central engine at both scales it is thus possible to infer some of the basic parameters of the flow speed density magnetic field intensity power after a brief review of the available observational evidence i discuss how the comparison between the physical quantities independently derived at the two scales can be used to shed light on the global dynamics of the jet from the innermost regions to the hundreds of kpc scale | [['jets', 'can', 'be', 'probed', 'in', 'their', 'innermost', 'regions', 'd01', 'pc', 'through', 'the', 'study', 'of', 'the', 'relativisticallyboosted', 'emission', 'of', 'blazars', 'on', 'the', 'other', 'extreme', 'of', 'spatial', 'scales', 'the', 'study', 'of', 'structure', 'and', 'dynamics', 'of', 'extragalactic', 'relativistic', 'jets', 'received', 'renewed', 'impulse', 'after', 'the', 'discovery', 'made', 'by', 'chandra', 'of', 'bright', 'xray', 'emission', 'from', 'regions', 'at', 'distances', 'larger', 'than', 'hundreds', 'of', 'kpc', 'from', 'the', 'central', 'engine', 'at', 'both', 'scales', 'it', 'is', 'thus', 'possible', 'to', 'infer', 'some', 'of', 'the', 'basic', 'parameters', 'of', 'the', 'flow', 'speed', 'density', 'magnetic', 'field', 'intensity', 'power', 'after', 'a', 'brief', 'review', 'of', 'the', 'available', 'observational', 'evidence', 'i', 'discuss', 'how', 'the', 'comparison', 'between', 'the', 'physical', 'quantities', 'independently', 'derived', 'at', 'the', 'two', 'scales', 'can', 'be', 'used', 'to', 'shed', 'light', 'on', 'the', 'global', 'dynamics', 'of', 'the', 'jet', 'from', 'the', 'innermost', 'regions', 'to', 'the', 'hundreds', 'of', 'kpc', 'scale']] | [-0.07246810229932607, 0.1293670116980193, -0.08798005160431123, 0.09361790026146495, -0.08068095395962398, -0.06000952214658768, 0.014149597836270308, 0.3845369600775567, -0.27835883643957926, -0.33170052843563486, 0.09474483227875846, -0.2830514114166638, 0.004175462821766621, 0.22889648524208248, 0.04025339223726681, -0.01744013198318002, 0.02388420550921706, -0.009545013566049889, -0.06414917234206134, -0.1814591207869605, 0.3095295427774545, 0.11849075279755969, 0.20020595362990262, 0.03521394825215931, 0.08623553302745815, -0.07004467793872622, -0.08254163101303151, 0.011552436822305688, -0.11039644001037673, 0.0946999659486623, 0.1841598074675086, 0.1313441093758835, 0.2547616036562514, -0.44495752511658904, -0.2472891056430385, 0.03454367339321779, 0.16268497129732912, 0.03676016545906543, -0.0071166306892833245, -0.2955412580913892, 0.06583671178051384, -0.13854322372759326, -0.1632238790414042, 0.03772750770969486, 0.048035271547798235, 0.04653405630255513, -0.17472163467909646, 0.11032506554417496, -0.020934254812097854, 0.07757232719891224, -0.045969573301122044, -0.07676140077510905, -0.040574123610206174, 0.11580465144167344, 0.10314141601415802, 0.044926700870167806, 0.2067699872387686, -0.15757008716746262, -0.0807788960113557, 0.3797297600064088, -0.022486889807734053, -0.03941192962035226, 0.21820963969521195, -0.24202176808577144, -0.1479609697972509, 0.17072623104887139, 0.2109889625465836, 0.14213130561719564, -0.1395399476278919, 0.016234412111578313, -0.02595492568533783, 0.20224801556270738, 0.045766968160133925, 0.1052080300657756, 0.31581494945919875, 0.13935040554938358, 0.026280677690396482, 0.13017595153007389, -0.21859529190458654, -0.07817443166586048, -0.3120509866046522, -0.04715337827237266, -0.14057782354454199, 0.0646004003514959, -0.1403649703626632, -0.06454620752695271, 0.420824854221957, 0.1684103027536449, 0.2348629223027577, 0.0014842619350405805, 0.30611804876278975, 0.03525934939159814, 0.08370384984035892, 0.1237541020699692, 0.3333292262406868, 0.1470104259541117, 0.10018142319467822, -0.21451552198127363, 0.06663417364258996, 0.014163126440535329] |
708.26 | Growing small-world networks based on a modified BA model | We propose a simple growing model for the evolution of small-world networks.
It is introduced as a modified BA model in which all the edges connected to the
new nodes are made locally to the creator and its nearest neighbors. It is
found that this model can produce small-world networks with power-law degree
distributions. Properties of our model, including the degree distribution,
clustering, and the average path length are compared with that of the BA model.
Since most real networks are both scale-free and small-world networks, our
model may provide a satisfactory description for empirical characteristics of
real networks.
| math-ph math.MP | we propose a simple growing model for the evolution of smallworld networks it is introduced as a modified ba model in which all the edges connected to the new nodes are made locally to the creator and its nearest neighbors it is found that this model can produce smallworld networks with powerlaw degree distributions properties of our model including the degree distribution clustering and the average path length are compared with that of the ba model since most real networks are both scalefree and smallworld networks our model may provide a satisfactory description for empirical characteristics of real networks | [['we', 'propose', 'a', 'simple', 'growing', 'model', 'for', 'the', 'evolution', 'of', 'smallworld', 'networks', 'it', 'is', 'introduced', 'as', 'a', 'modified', 'ba', 'model', 'in', 'which', 'all', 'the', 'edges', 'connected', 'to', 'the', 'new', 'nodes', 'are', 'made', 'locally', 'to', 'the', 'creator', 'and', 'its', 'nearest', 'neighbors', 'it', 'is', 'found', 'that', 'this', 'model', 'can', 'produce', 'smallworld', 'networks', 'with', 'powerlaw', 'degree', 'distributions', 'properties', 'of', 'our', 'model', 'including', 'the', 'degree', 'distribution', 'clustering', 'and', 'the', 'average', 'path', 'length', 'are', 'compared', 'with', 'that', 'of', 'the', 'ba', 'model', 'since', 'most', 'real', 'networks', 'are', 'both', 'scalefree', 'and', 'smallworld', 'networks', 'our', 'model', 'may', 'provide', 'a', 'satisfactory', 'description', 'for', 'empirical', 'characteristics', 'of', 'real', 'networks']] | [-0.12431218202291715, 0.06891693335703829, -0.06983846249152915, 0.07249062279394518, -0.049334317772658634, -0.18140749495965663, 0.008752030461575046, 0.43992214225852305, -0.2604633987178048, -0.290395110883195, 0.019461620108676, -0.3128688663168989, -0.24973121471703053, 0.13015339048014898, -0.009171675025212645, 0.015138783412773839, 0.0734517449898777, 0.07176282022232448, 0.03974919058288438, -0.2810467066386752, 0.29066508760995635, 0.08798250975087285, 0.30327846301070444, 0.01927574219727757, 0.05433852663687007, -0.0362091647470464, 0.019344103823632303, 0.07313389015017134, -0.0735935557974947, 0.1425910848898418, 0.16232687816719968, 0.13519773350069017, 0.22837820067305606, -0.3970970864774603, -0.2984071819939547, 0.16590171425151778, 0.1438897120615825, 0.09779969523919539, -0.008508405902168968, -0.274829315788329, 0.13986190479022986, -0.18971046034718225, -0.11445239862671705, -0.09800826578114107, 0.030339704426663994, 0.09866495496320604, -0.2625602850210712, 0.04873416209687488, 0.04470789734499924, 0.03226658806317684, -0.011601130919051215, -0.11994794424096442, -0.0737472825890614, 0.15049617034336082, -0.020730497440172718, 0.01001921061642769, 0.0537334220258124, -0.1457076041907486, -0.1396663376327717, 0.3905855762452414, -0.01703864757460777, -0.17344381619771623, 0.21322524562628584, -0.08668878858890196, -0.13366136349493055, 0.06394298240598856, 0.19300138983273446, 0.0886301993618183, -0.17603692035143725, 0.025545923564361993, -0.0650065236941281, 0.1498001820285513, -0.02609783522032126, 0.008292597937256549, 0.1630832833786068, 0.2220857006525903, 0.04197411714215772, 0.10931923041811609, -0.07678850216207782, -0.1295071903926631, -0.22709562381108603, -0.08632515985142401, -0.21788426845997685, 0.02236286293000284, -0.18896304690376078, -0.2116356058742362, 0.45587656269734256, 0.15248046054697661, 0.2691515444617982, 0.14993446566884153, 0.26047435881936865, 0.07632300125627844, 0.09148783323289168, 0.12414882016942055, 0.1926280895643162, 0.11895960771285863, 0.09206657012868108, -0.11354236090743933, 0.14982205003293025, 0.010780383597570236] |
708.2601 | A novel configuration model for random graphs with given degree sequence | Recently, random graphs in which vertices are characterized by hidden
variables controlling the establishment of edges between pairs of vertices have
attracted much attention. Here, we present a specific realization of a class of
random network models in which the connection probability between two vertices
(i,j) is a specific function of degrees ki and kj. In the framework of the
configuration model of random graphs, we find analytical expressions for the
degree correlation and clustering as a function of the variance of the desired
degree distribution. The expressions obtained are checked by means of numerical
simulations. Possible applications of our model are discussed.
| math-ph math.MP | recently random graphs in which vertices are characterized by hidden variables controlling the establishment of edges between pairs of vertices have attracted much attention here we present a specific realization of a class of random network models in which the connection probability between two vertices ij is a specific function of degrees ki and kj in the framework of the configuration model of random graphs we find analytical expressions for the degree correlation and clustering as a function of the variance of the desired degree distribution the expressions obtained are checked by means of numerical simulations possible applications of our model are discussed | [['recently', 'random', 'graphs', 'in', 'which', 'vertices', 'are', 'characterized', 'by', 'hidden', 'variables', 'controlling', 'the', 'establishment', 'of', 'edges', 'between', 'pairs', 'of', 'vertices', 'have', 'attracted', 'much', 'attention', 'here', 'we', 'present', 'a', 'specific', 'realization', 'of', 'a', 'class', 'of', 'random', 'network', 'models', 'in', 'which', 'the', 'connection', 'probability', 'between', 'two', 'vertices', 'ij', 'is', 'a', 'specific', 'function', 'of', 'degrees', 'ki', 'and', 'kj', 'in', 'the', 'framework', 'of', 'the', 'configuration', 'model', 'of', 'random', 'graphs', 'we', 'find', 'analytical', 'expressions', 'for', 'the', 'degree', 'correlation', 'and', 'clustering', 'as', 'a', 'function', 'of', 'the', 'variance', 'of', 'the', 'desired', 'degree', 'distribution', 'the', 'expressions', 'obtained', 'are', 'checked', 'by', 'means', 'of', 'numerical', 'simulations', 'possible', 'applications', 'of', 'our', 'model', 'are', 'discussed']] | [-0.158914947872405, 0.1161395749325855, -0.03984548005013211, 0.030287582387704657, -0.03706830975066111, -0.13923836761669625, 0.06708642949228112, 0.4000327213875298, -0.22342355121198354, -0.334342749563308, 0.03875220793828332, -0.28273752896856624, -0.1975111520636682, 0.1252470084791551, 0.0016262434576683252, 0.0574842635903833, 0.0374048062175223, 0.05103980252537334, -0.03773175753727646, -0.22841564205687637, 0.29834064861162773, 0.030903073778213226, 0.25438472030467346, 0.03584550519121214, 0.11157623863354035, 0.015774712058488342, -0.04230343038216233, 0.05483555261981538, -0.15108483876056464, 0.12938064534795804, 0.1919108126690067, 0.13356616220536452, 0.27481534888117926, -0.3937041544382578, -0.23221819321579726, 0.14023389070050665, 0.10838712887494888, 0.09533850334865014, -0.0453974889383371, -0.2622264129769744, 0.08496355962514587, -0.16140562989234752, -0.1214053837030909, -0.04657090174992686, 0.06101292048499567, 0.08973143893990268, -0.2995011139010052, 0.05234443174914719, 0.04842809346748642, 0.07286005886723694, 0.029798375899243414, -0.16357584148803636, -0.06410969575659091, 0.13546862159019282, 0.012064426542865565, 0.0057129073047160524, 0.0471352504801403, -0.1763059685495004, -0.1566162899139934, 0.33561853889050414, -0.004784949915031496, -0.2099968306403788, 0.14318681142103035, -0.13156071775457234, -0.13327909336036559, 0.08770639792952722, 0.17183396420938876, 0.16030362922951436, -0.1637440887686697, 0.0679774711087111, -0.06605956466977024, 0.10448709858617591, 0.0664500171924462, 0.06258892851149284, 0.20083142771810583, 0.14011638814547253, 0.030724298672352747, 0.1960656545814398, -0.05513511394891996, -0.11865672389626304, -0.30264539113358674, -0.11884555358041837, -0.24859961637666503, 0.01827571863869151, -0.1653400204464843, -0.15175731351725685, 0.4451258677302055, 0.1336591076786806, 0.24904654148821403, 0.07807373149022098, 0.22327292246689784, 0.11778270247057804, 0.04402529203685597, 0.06594306392170199, 0.1769132751754476, 0.16749824996748305, 0.01255038643744096, -0.14338369891318736, 0.11926948781762706, 0.07444879268657742] |
708.2602 | Negative magnetoresistance of ultra-narrow superconducting nanowires in
the resistive state | We present a phenomenological model qualitatively explaining negative
magnetoresistance in quasi-one-dimensional superconducting channels in the
resistive state. The model is based on the assumption that fluctuations of the
order parameter (phase slips) are responsible for the finite effective
resistance of a narrow superconducting wire sufficiently close to the critical
temperature. Each fluctuation is accompanied by an instant formation of a
quasi-normal region of the order of the non-equilibrium quasiparticle
relaxation length 'pinned' to the core of the phase slip. The effective
time-averaged voltage measured in experiment is a sum of two terms. First one
is the conventional contribution linked to the rate of the fluctuations via the
Josephson relation. Second term is the Ohmic contribution of this quasi-normal
region. Depending on material properties of the wire, there might be a range of
magnetic fields where the first term is not much affected, while the second
term is effectively suppressed contributing to the experimentally observed
negative magnetoresistance.
| cond-mat.supr-con | we present a phenomenological model qualitatively explaining negative magnetoresistance in quasionedimensional superconducting channels in the resistive state the model is based on the assumption that fluctuations of the order parameter phase slips are responsible for the finite effective resistance of a narrow superconducting wire sufficiently close to the critical temperature each fluctuation is accompanied by an instant formation of a quasinormal region of the order of the nonequilibrium quasiparticle relaxation length pinned to the core of the phase slip the effective timeaveraged voltage measured in experiment is a sum of two terms first one is the conventional contribution linked to the rate of the fluctuations via the josephson relation second term is the ohmic contribution of this quasinormal region depending on material properties of the wire there might be a range of magnetic fields where the first term is not much affected while the second term is effectively suppressed contributing to the experimentally observed negative magnetoresistance | [['we', 'present', 'a', 'phenomenological', 'model', 'qualitatively', 'explaining', 'negative', 'magnetoresistance', 'in', 'quasionedimensional', 'superconducting', 'channels', 'in', 'the', 'resistive', 'state', 'the', 'model', 'is', 'based', 'on', 'the', 'assumption', 'that', 'fluctuations', 'of', 'the', 'order', 'parameter', 'phase', 'slips', 'are', 'responsible', 'for', 'the', 'finite', 'effective', 'resistance', 'of', 'a', 'narrow', 'superconducting', 'wire', 'sufficiently', 'close', 'to', 'the', 'critical', 'temperature', 'each', 'fluctuation', 'is', 'accompanied', 'by', 'an', 'instant', 'formation', 'of', 'a', 'quasinormal', 'region', 'of', 'the', 'order', 'of', 'the', 'nonequilibrium', 'quasiparticle', 'relaxation', 'length', 'pinned', 'to', 'the', 'core', 'of', 'the', 'phase', 'slip', 'the', 'effective', 'timeaveraged', 'voltage', 'measured', 'in', 'experiment', 'is', 'a', 'sum', 'of', 'two', 'terms', 'first', 'one', 'is', 'the', 'conventional', 'contribution', 'linked', 'to', 'the', 'rate', 'of', 'the', 'fluctuations', 'via', 'the', 'josephson', 'relation', 'second', 'term', 'is', 'the', 'ohmic', 'contribution', 'of', 'this', 'quasinormal', 'region', 'depending', 'on', 'material', 'properties', 'of', 'the', 'wire', 'there', 'might', 'be', 'a', 'range', 'of', 'magnetic', 'fields', 'where', 'the', 'first', 'term', 'is', 'not', 'much', 'affected', 'while', 'the', 'second', 'term', 'is', 'effectively', 'suppressed', 'contributing', 'to', 'the', 'experimentally', 'observed', 'negative', 'magnetoresistance']] | [-0.22048573089668003, 0.21508123594694786, -0.058413259410418764, 0.043286913592451945, -0.062151316072767936, -0.1273523997813941, 0.05628920765444397, 0.29698240913402957, -0.2541680962133866, -0.25853914128711974, 0.03726697486649172, -0.2952572004332279, -0.11195272394270898, 0.1790613304877367, 0.028162062302073583, 0.008866054447702108, -0.02762068526368612, 0.051062911960821696, -0.06006089136159668, -0.20359833722408766, 0.33382065204354244, 0.06333928315255505, 0.3099018884434675, 0.1101909276868145, 0.0665364874055227, -0.07238099332122754, 0.05069514584297744, 0.04045962319912341, -0.12879231318784617, 0.014251604616546478, 0.22744083020967457, -0.07361932789894919, 0.2254523007103648, -0.4183587206539531, -0.20256103541797552, 0.09063200556482069, 0.1592412856571639, 0.13236499189261872, -0.007994943923758676, -0.24106513208542496, 0.07371473841619892, -0.15255514009951207, -0.10878217309110393, -0.018198413989291742, 0.02015178116524998, -0.021247371219662733, -0.26443259232641697, 0.1379934830172435, 0.06647865941900258, 0.02483962917810855, -0.0674235576014512, -0.07608362333252071, -0.014305900316685438, 0.08490058570187568, 0.0726870696600646, 0.058597853902775124, 0.17183768428945675, -0.13616917925797586, -0.061715276032769814, 0.330768868955485, -0.08374600334672067, -0.1317214613104275, 0.12120525940554217, -0.19448597110413873, -0.024993554984505933, 0.17775324443564153, 0.1081206131225022, 0.09761670953594148, -0.15368183326716414, 0.0360047544624346, 0.02801001653409539, 0.18670862951712947, 0.021479093357741546, 0.05266362936116564, 0.2570637340705173, 0.21775157682714052, 0.022529308940880954, 0.1709519370760506, -0.11782964038698432, -0.0882485698377236, -0.3314586575978842, -0.1248311886134056, -0.2171513568609953, 0.02294794034269916, -0.07704956472540896, -0.19953329177895704, 0.4309514566587332, 0.147578973048486, 0.21228582571105412, -0.008504254213617876, 0.29491115893977576, 0.17051598245131735, 0.09683225322544622, 0.0467135034298572, 0.2780974766650709, 0.17104301156807475, 0.13959055917653948, -0.3213499184486677, 0.12019152980811225, 0.039252069778740406] |
708.2603 | Double parton scattering, diffraction and effective cross section | The rates of multiparton collisions in high energy hadronic interactions
provide information on the typical transverse distances between partons in the
hadron structure. The different configurations of the hadron in transverse
space are, on the other hand, at the origin of hadron diffraction. The relation
between the two phenomena is exploted in an eikonal model of hadronic
interactions.
| hep-ph | the rates of multiparton collisions in high energy hadronic interactions provide information on the typical transverse distances between partons in the hadron structure the different configurations of the hadron in transverse space are on the other hand at the origin of hadron diffraction the relation between the two phenomena is exploted in an eikonal model of hadronic interactions | [['the', 'rates', 'of', 'multiparton', 'collisions', 'in', 'high', 'energy', 'hadronic', 'interactions', 'provide', 'information', 'on', 'the', 'typical', 'transverse', 'distances', 'between', 'partons', 'in', 'the', 'hadron', 'structure', 'the', 'different', 'configurations', 'of', 'the', 'hadron', 'in', 'transverse', 'space', 'are', 'on', 'the', 'other', 'hand', 'at', 'the', 'origin', 'of', 'hadron', 'diffraction', 'the', 'relation', 'between', 'the', 'two', 'phenomena', 'is', 'exploted', 'in', 'an', 'eikonal', 'model', 'of', 'hadronic', 'interactions']] | [-0.12189291760717567, 0.26776734658893764, -0.15885106443729774, 0.17089435769645334, -0.0176553503005651, -0.02571974890796762, -0.06415188825574883, 0.36299987248422805, -0.23939354131161644, -0.2535587583521479, -0.04831079453262582, -0.36081339830630704, 0.02797937396456275, 0.14342044067993892, 0.12658761036500596, 0.03661521110814391, 0.086444625124466, 0.03340059034005543, -0.06888559274375439, -0.16494489415025895, 0.3759934981108496, 0.09147826644281547, 0.25429039716459156, 0.18130771877864996, 0.10676790667665109, 0.07729802788398638, -0.010309251940302681, -0.036543210127427686, -0.10309940132132747, 0.08184558950954836, 0.2481129430561212, 0.025190483443765788, 0.13665075577681132, -0.4336201052197762, -0.14226437375161863, 0.07452308695371214, 0.12439259330398943, 0.10424336379295901, -0.01578202228094533, -0.21532661174097212, 0.024947447963712507, -0.18818603991939312, -0.1279534259320874, -0.01993544786972435, -0.043297224302302324, 0.05400119434323227, -0.23167614966912783, 0.10237824416866428, -0.003119358008629397, 0.06006548292281335, -0.022838509118739973, -0.13033369286475996, -0.055399040683385053, 0.08561051585466455, 0.08966436447257078, 0.04783498881213171, 0.11050466676814515, -0.24579304715071135, -0.18316041823607265, 0.42259096342808844, 0.04132705540069493, -0.1951976401584321, 0.247761375025699, -0.24311268532223868, -0.13178715104106486, 0.17220768131511777, 0.2786765347904803, 0.05584360253915452, -0.21142212273818523, 0.09584085347555708, 0.009003554838464448, 0.13611285308408633, 0.06899794591018897, 0.1356160180528828, 0.2209754511387202, 0.2189944905081862, -0.04654140337452031, 0.085379025883556, -0.1450589363577596, -0.11521104657859133, -0.37047897973669724, -0.07876029581223663, -0.15691371809429766, -0.0056842131470738536, -0.15961703064181565, -0.1141982864621177, 0.36714104810533554, 0.10734861082675164, 0.30018058433115746, -0.05649174650183372, 0.3326691449211355, 0.034845672645851186, 0.03177932503616862, 0.05776857644760687, 0.32703283940556277, 0.14542342454456447, 0.165101507596933, -0.29307386338743463, 0.055792786548600384, 0.1046945414456882] |
708.2604 | Measurements of time-dependent CP violation in B^0 -> psi(2S) K_S decays | We report improved measurements of time-dependent CP violation parameters for
B^0(\bar{B}^0) -> psi(2S) K_S. This analysis is based on a data sample of
657x10^6 BBbar pairs collected at the Y(4S) resonance with the Belle detector
at the KEKB energy-asymmetric e+e- collider. We fully reconstruct one neutral B
meson in the psi(2S) K_S CP-eigenstate decay channel, and the flavor of the
accompanying B meson is identified to be either B^0 or \bar{B}^0 from its decay
products. CP violation parameters are obtained from the asymmetries in the
distributions of the proper-time intervals between the two B decays:
S (psi(2S) K_S) = +0.72 +/- 0.09(stat) +/- 0.03(syst),
A (psi(2S) K_S) = +0.04 +/- 0.07(stat) +/- 0.05(syst).
These results are in agreement with results from measurements of B^0 -> J/psi
K^0.
| hep-ex | we report improved measurements of timedependent cp violation parameters for b0barb0 psi2s k_s this analysis is based on a data sample of 657x106 bbbar pairs collected at the y4s resonance with the belle detector at the kekb energyasymmetric ee collider we fully reconstruct one neutral b meson in the psi2s k_s cpeigenstate decay channel and the flavor of the accompanying b meson is identified to be either b0 or barb0 from its decay products cp violation parameters are obtained from the asymmetries in the distributions of the propertime intervals between the two b decays s psi2s k_s 072 009stat 003syst a psi2s k_s 004 007stat 005syst these results are in agreement with results from measurements of b0 jpsi k0 | [['we', 'report', 'improved', 'measurements', 'of', 'timedependent', 'cp', 'violation', 'parameters', 'for', 'b0barb0', 'psi2s', 'k_s', 'this', 'analysis', 'is', 'based', 'on', 'a', 'data', 'sample', 'of', '657x106', 'bbbar', 'pairs', 'collected', 'at', 'the', 'y4s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'energyasymmetric', 'ee', 'collider', 'we', 'fully', 'reconstruct', 'one', 'neutral', 'b', 'meson', 'in', 'the', 'psi2s', 'k_s', 'cpeigenstate', 'decay', 'channel', 'and', 'the', 'flavor', 'of', 'the', 'accompanying', 'b', 'meson', 'is', 'identified', 'to', 'be', 'either', 'b0', 'or', 'barb0', 'from', 'its', 'decay', 'products', 'cp', 'violation', 'parameters', 'are', 'obtained', 'from', 'the', 'asymmetries', 'in', 'the', 'distributions', 'of', 'the', 'propertime', 'intervals', 'between', 'the', 'two', 'b', 'decays', 's', 'psi2s', 'k_s', '072', '009stat', '003syst', 'a', 'psi2s', 'k_s', '004', '007stat', '005syst', 'these', 'results', 'are', 'in', 'agreement', 'with', 'results', 'from', 'measurements', 'of', 'b0', 'jpsi', 'k0']] | [-0.09009241088520453, 0.19828364170085983, -0.10975810172458907, 0.09554904652465948, -0.04433611716156505, -0.16402905775202797, 0.10753431253060855, 0.280654006121101, -0.16863161558285356, -0.22085892457217604, -0.031972775363926814, -0.46442848266329334, 0.1040634418732072, 0.13104825879705428, 0.11189298046862378, 0.11769187257736687, 0.1753933310993955, -0.011437578326357263, -0.06997715750270907, -0.1362811853353936, 0.18811621406788648, -0.06731333017756208, 0.2022361710272385, 0.053266363797568474, -0.06945774188370858, 0.005981819281558029, -0.10994518342420083, -0.08121780705239091, -0.21965038324041025, 0.006136298716702193, 0.2269055754095003, 0.15459848800918652, 0.07434234693411644, -0.2689279551779095, 0.05578392109356257, 0.1983710419926636, 0.13341773688761877, 0.00016976118150378476, -0.0032011286997306746, -0.46909939328662487, 0.15823832214536035, -0.14920222051363408, 0.01031861366594539, -0.024315753791230816, 0.04925338413660266, -0.1287144319537808, -0.40448846661744, 0.15986428409619177, -0.12816433954451764, 0.09916631646841734, -0.015431885530256486, -0.2987217932798657, -0.032348371388688055, -0.03224215288098682, 0.08900329185172352, 0.14665412447736167, 0.1852417367455714, -0.0847465435391245, -0.19079328292370343, 0.3474218527465558, -0.1014771240851656, -0.1422080570409278, 0.10230365724883926, -0.294698685161112, -0.12185385856511337, 0.21032179700320258, 0.2238946669870017, 0.05071292951812639, -0.23750815128109284, 0.13087930736090878, -0.03308874578019526, 0.1563970740540188, 0.09229958277320911, 0.1288857248297109, 0.13724806468088588, 0.1653309017028503, -0.03440847105010092, 0.04181896667720108, -0.16609257065002345, 0.03746195618031906, -0.4370615852668005, -0.12568169528571496, -0.0500960177389764, 0.13151883691678434, -0.026138348207381524, -0.0047773390601412585, 0.36024613009311823, -0.03201157462532718, 0.34932914640003143, -0.02505539030525364, 0.3054153468272015, 0.049733534328122976, 0.00671966844546499, 0.08487813768968545, 0.34626555269067527, 0.2447259895926138, 0.19298357232141175, -0.344423463538743, 0.025729873878959596, -0.03479604655094132] |
708.2605 | The properties of the young stellar populations in powerful radio
galaxies at low and intermediate redshifts | Abridged. We present high-quality optical spectra for 12 powerful radio
sources at low and intermediate redshifts (z < 0.7) that show evidence for a
substantial UV excess. These data were taken using the WHT and VLT to determine
the detailed properties of the young stellar populations (YSPs) in the host
galaxies as part of a larger project to investigate evolutionary scenarios for
the AGN host galaxies. The results of our spectral synthesis model fits to the
spectra highlight the importance of taking into account AGN-related components
(emission lines, nebular continuum, scattered light) and reddening of the
stellar populations in studies of this type. It is also clear that careful
examination of the fits to the spectra, as well consideration of auxilary
polarimetric and imaging data, are required to avoid degeneracies in the model
solutions. In 3/12 sources in our sample we find broad permitted line
components, and a combination of AGN-related continuum components and an old
(12.5 Gyr) stellar population provides an adequate fit to the data. In the
remaining 9 sources we find strong evidence for YSPs. In contrast to some
recent studies that suggest relatively old post-starburst ages for the YSPs in
radio galaxies (0.3-2.5 Gyr), we deduce a wide range of ages for the YSPs in
our sample objects (0.02-1.5 Gyr), with ~50% of the sample showing evidence for
young YSP ages (<~0.1 Gyr) in their nuclear regions. The nuclear YSPs are often
significantly reddened (0.2 < E(B-V) < 1.4) and make up a substantial fraction
(~1-35%) of the total stellar mass in the regions sampled by the spectroscopic
slits. Moreover, in all the cases in which we have sufficient spatial
resolution we find that the UV excess is extended across the full measureable
extent of the galaxy (typically 5-30 kpc), suggesting galaxy-wide starbursts.
| astro-ph | abridged we present highquality optical spectra for 12 powerful radio sources at low and intermediate redshifts z 07 that show evidence for a substantial uv excess these data were taken using the wht and vlt to determine the detailed properties of the young stellar populations ysps in the host galaxies as part of a larger project to investigate evolutionary scenarios for the agn host galaxies the results of our spectral synthesis model fits to the spectra highlight the importance of taking into account agnrelated components emission lines nebular continuum scattered light and reddening of the stellar populations in studies of this type it is also clear that careful examination of the fits to the spectra as well consideration of auxilary polarimetric and imaging data are required to avoid degeneracies in the model solutions in 312 sources in our sample we find broad permitted line components and a combination of agnrelated continuum components and an old 125 gyr stellar population provides an adequate fit to the data in the remaining 9 sources we find strong evidence for ysps in contrast to some recent studies that suggest relatively old poststarburst ages for the ysps in radio galaxies 0325 gyr we deduce a wide range of ages for the ysps in our sample objects 00215 gyr with 50 of the sample showing evidence for young ysp ages 01 gyr in their nuclear regions the nuclear ysps are often significantly reddened 02 ebv 14 and make up a substantial fraction 135 of the total stellar mass in the regions sampled by the spectroscopic slits moreover in all the cases in which we have sufficient spatial resolution we find that the uv excess is extended across the full measureable extent of the galaxy typically 530 kpc suggesting galaxywide starbursts | [['abridged', 'we', 'present', 'highquality', 'optical', 'spectra', 'for', '12', 'powerful', 'radio', 'sources', 'at', 'low', 'and', 'intermediate', 'redshifts', 'z', '07', 'that', 'show', 'evidence', 'for', 'a', 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708.2606 | Scaling and correlations in three bus-transport networks of China | We report the statistical properties of three bus-transport networks (BTN) in
three different cities of China. These networks are composed of a set of bus
lines and stations serviced by these. Network properties, including the degree
distribution, clustering and average path length are studied in different
definitions of network topology. We explore scaling laws and correlations that
may govern intrinsic features of such networks. Besides, we create a weighted
network representation for BTN with lines mapped to nodes and number of common
stations to weights between lines. In such a representation, the distributions
of degree, strength and weight are investigated. A linear behavior between
strength and degree s(k) ~ k is also observed.
| physics.soc-ph | we report the statistical properties of three bustransport networks btn in three different cities of china these networks are composed of a set of bus lines and stations serviced by these network properties including the degree distribution clustering and average path length are studied in different definitions of network topology we explore scaling laws and correlations that may govern intrinsic features of such networks besides we create a weighted network representation for btn with lines mapped to nodes and number of common stations to weights between lines in such a representation the distributions of degree strength and weight are investigated a linear behavior between strength and degree sk k is also observed | [['we', 'report', 'the', 'statistical', 'properties', 'of', 'three', 'bustransport', 'networks', 'btn', 'in', 'three', 'different', 'cities', 'of', 'china', 'these', 'networks', 'are', 'composed', 'of', 'a', 'set', 'of', 'bus', 'lines', 'and', 'stations', 'serviced', 'by', 'these', 'network', 'properties', 'including', 'the', 'degree', 'distribution', 'clustering', 'and', 'average', 'path', 'length', 'are', 'studied', 'in', 'different', 'definitions', 'of', 'network', 'topology', 'we', 'explore', 'scaling', 'laws', 'and', 'correlations', 'that', 'may', 'govern', 'intrinsic', 'features', 'of', 'such', 'networks', 'besides', 'we', 'create', 'a', 'weighted', 'network', 'representation', 'for', 'btn', 'with', 'lines', 'mapped', 'to', 'nodes', 'and', 'number', 'of', 'common', 'stations', 'to', 'weights', 'between', 'lines', 'in', 'such', 'a', 'representation', 'the', 'distributions', 'of', 'degree', 'strength', 'and', 'weight', 'are', 'investigated', 'a', 'linear', 'behavior', 'between', 'strength', 'and', 'degree', 'sk', 'k', 'is', 'also', 'observed']] | [-0.20289400890301745, 0.10651256629844776, -0.029837719953476307, 0.045711805487076776, -0.019342845540728654, -0.12966076227592993, 0.0646177975603522, 0.43479987270794473, -0.2907135817935472, -0.3231746356699381, 0.017650254944398126, -0.31348546027197494, -0.17513270897639766, 0.14812535128077944, -0.0034359815438185725, 0.02045104967279209, 0.028928037997133827, 0.03755404368076507, -0.03999167660393895, -0.20863438860056, 0.3396468870090069, 0.013884911435312248, 0.32639630068395586, 0.0212844446037166, 0.09685221999261721, -0.03629690826844806, -0.027815676493536647, 0.07904562885822677, -0.0954016577980092, 0.14119477385785095, 0.25708121404802714, 0.1512685001152358, 0.2300147926476826, -0.40852243968428253, -0.2342085951419027, 0.1453173460338164, 0.11021650312489385, 0.02083812533198176, 0.06599453940719098, -0.2531124190511266, 0.10379500723515243, -0.14335097488671905, -0.11913385723826585, -0.04799263358225224, 0.04203970048593374, 0.12292460373053243, -0.24659994457688955, 0.02703834718343936, 0.022396704681775625, 0.11540833577043838, -6.718570702113547e-05, -0.14839538425072893, -0.0554229937690973, 0.19146072469769163, 0.001460570474952325, -0.05622020536647723, 0.10062936584356132, -0.14883870875613914, -0.12477865766079442, 0.3255069627518858, -0.016751920644965796, -0.163912093073868, 0.1981371869039428, -0.09891061825879119, -0.15627871062984136, 0.06794779291292569, 0.22498955147609384, 0.06719905265967722, -0.15100178057076158, -0.010716118198517408, -0.04212343281655161, 0.1513022867845254, 0.06754961887139592, 0.09370246383692934, 0.19336219952287842, 0.16001097258885164, 0.05131643185777976, 0.13600196935255332, -0.13560877820090936, -0.10807596428135226, -0.24381412672264888, -0.11742604137104642, -0.18571433893967051, 0.037987824383628056, -0.1358994712860655, -0.12448176812498016, 0.4454830201963584, 0.10741693490323283, 0.24407290874535706, 0.07537440839643078, 0.21111346307202233, 0.06469304966942202, 0.07965884720151489, 0.12346478736002904, 0.16347503471649713, 0.1263476508566774, 0.07632856343784747, -0.16284820651593576, 0.0779136152519018, 0.062080806817624484] |
708.2607 | Gamma-ray emission associated with the Cluster-scale AGN Outbursts in
the Hydra A system | Recent observations have revealed the existence of an enormously energetic >
10^61 erg AGN outburst in the Hydra A cluster of galaxies. This outburst has
produced cavities in the intra-cluster medium, apparently supported by pressure
from cosmic rays. Here we argue that if these cavities are filled with > GeV
particles, these particles are very likely protons and nuclei. For a plausible
spatial distribution of the target gas, based on observations and
hydrodynamical simulations, we show that the pi^0-decay gamma-rays from these
cosmic-rays may be detectable with the H.E.S.S.experiment.
| astro-ph | recent observations have revealed the existence of an enormously energetic 1061 erg agn outburst in the hydra a cluster of galaxies this outburst has produced cavities in the intracluster medium apparently supported by pressure from cosmic rays here we argue that if these cavities are filled with gev particles these particles are very likely protons and nuclei for a plausible spatial distribution of the target gas based on observations and hydrodynamical simulations we show that the pi0decay gammarays from these cosmicrays may be detectable with the hessexperiment | [['recent', 'observations', 'have', 'revealed', 'the', 'existence', 'of', 'an', 'enormously', 'energetic', '1061', 'erg', 'agn', 'outburst', 'in', 'the', 'hydra', 'a', 'cluster', 'of', 'galaxies', 'this', 'outburst', 'has', 'produced', 'cavities', 'in', 'the', 'intracluster', 'medium', 'apparently', 'supported', 'by', 'pressure', 'from', 'cosmic', 'rays', 'here', 'we', 'argue', 'that', 'if', 'these', 'cavities', 'are', 'filled', 'with', 'gev', 'particles', 'these', 'particles', 'are', 'very', 'likely', 'protons', 'and', 'nuclei', 'for', 'a', 'plausible', 'spatial', 'distribution', 'of', 'the', 'target', 'gas', 'based', 'on', 'observations', 'and', 'hydrodynamical', 'simulations', 'we', 'show', 'that', 'the', 'pi0decay', 'gammarays', 'from', 'these', 'cosmicrays', 'may', 'be', 'detectable', 'with', 'the', 'hessexperiment']] | [-0.06400135957681964, 0.23594079788406733, -0.10291205223129932, 0.10368193488237773, -0.04701546466974325, -0.04114336823113263, 0.00686500082875407, 0.4812411677395535, -0.1805310803682132, -0.3286698744957184, 0.015546038608759815, -0.33637851289321863, 0.007694342585150586, 0.189411795435495, 0.025149613775876024, -0.05365784695510059, 0.12560012699429726, -0.09188279613505962, 0.016375710998206984, -0.25198345016254936, 0.3135657199810064, 0.15856837825633066, 0.1373673055678346, 0.023938044461659914, 0.11370793192885643, -0.13576335119906552, -0.04471919976911226, -0.01908871563974508, -0.11960140258959781, 0.06219143833326132, 0.21057486098779496, 0.10301483936234225, 0.20506510487216156, -0.4749311883608962, -0.28462791390890296, 0.09443882732045684, 0.20016782931160443, 0.010982219552144755, -0.11745584484996534, -0.2970542136016627, 0.04464013555065491, -0.2101161819557811, -0.18514311169599032, 0.051526995884731065, -0.012330427018622326, 0.08530658417446323, -0.18790427589556202, 0.12413850914670674, 0.0025057013093786273, 0.012053647782480302, -0.1257196392019301, -0.06715967352393755, -0.02002489528358849, -0.018308978243514375, 0.10327114037043134, 0.04185164046235556, 0.20087424980823038, -0.13212988406235657, -0.06063615089434004, 0.39591974366542904, -0.0030311701364468696, 0.006011404514009523, 0.25653500727995104, -0.22683073340395335, -0.19808940547464285, 0.20762478550462876, 0.1555448757961046, 0.05667072295503647, -0.1442093102797476, 0.0009896314667732736, -0.08440704973479517, 0.20290133665954738, 0.046147023934091244, 0.05295043633617921, 0.33315365391155316, 0.11401309459578506, -0.020180124375254436, 0.09244774708518931, -0.19257799203258527, 0.038893618122782816, -0.26426786847066047, -0.07364471033648697, -0.1701413916456405, 0.13053936678997435, -0.11871367363160379, -0.07544921563808309, 0.30929445455847093, 0.09276303573820177, 0.19850469001590512, -0.03151033592388727, 0.27033323723129754, 0.04908004570968969, 0.04396329559439923, 0.1832728607493431, 0.3747864871090928, 0.1339408738760624, 0.08299073863363024, -0.19442171923448007, 0.05859607274151342, -0.011830004581878351] |
708.2608 | Empirical analysis of the ship-transport network of China | Structural properties of the ship-transport network of China (STNC) are
studied in the light of recent investigations of complex networks. STNC is
composed of a set of routes and ports located along the sea or river. Network
properties including the degree distribution, degree correlations, clustering,
shortest path length, centrality and betweenness are studied in different
definition of network topology. It is found that geographical constraint plays
an important role in the network topology of STNC. We also study the traffic
flow of STNC based on the weighted network representation, and demonstrate the
weight distribution can be described by power law or exponential function
depending on the assumed definition of network topology. Other features related
to STNC are also investigated.
| physics.soc-ph | structural properties of the shiptransport network of china stnc are studied in the light of recent investigations of complex networks stnc is composed of a set of routes and ports located along the sea or river network properties including the degree distribution degree correlations clustering shortest path length centrality and betweenness are studied in different definition of network topology it is found that geographical constraint plays an important role in the network topology of stnc we also study the traffic flow of stnc based on the weighted network representation and demonstrate the weight distribution can be described by power law or exponential function depending on the assumed definition of network topology other features related to stnc are also investigated | [['structural', 'properties', 'of', 'the', 'shiptransport', 'network', 'of', 'china', 'stnc', 'are', 'studied', 'in', 'the', 'light', 'of', 'recent', 'investigations', 'of', 'complex', 'networks', 'stnc', 'is', 'composed', 'of', 'a', 'set', 'of', 'routes', 'and', 'ports', 'located', 'along', 'the', 'sea', 'or', 'river', 'network', 'properties', 'including', 'the', 'degree', 'distribution', 'degree', 'correlations', 'clustering', 'shortest', 'path', 'length', 'centrality', 'and', 'betweenness', 'are', 'studied', 'in', 'different', 'definition', 'of', 'network', 'topology', 'it', 'is', 'found', 'that', 'geographical', 'constraint', 'plays', 'an', 'important', 'role', 'in', 'the', 'network', 'topology', 'of', 'stnc', 'we', 'also', 'study', 'the', 'traffic', 'flow', 'of', 'stnc', 'based', 'on', 'the', 'weighted', 'network', 'representation', 'and', 'demonstrate', 'the', 'weight', 'distribution', 'can', 'be', 'described', 'by', 'power', 'law', 'or', 'exponential', 'function', 'depending', 'on', 'the', 'assumed', 'definition', 'of', 'network', 'topology', 'other', 'features', 'related', 'to', 'stnc', 'are', 'also', 'investigated']] | [-0.19751683270984913, 0.09726259831876309, -0.08855063223153732, 0.052600839863910134, -0.036406397866874426, -0.11460205895226386, 0.009957381267637268, 0.39690938702452994, -0.2937110081725454, -0.2929095228565699, 0.05872468494956176, -0.30052251090942805, -0.218573529573189, 0.1578894942422729, -0.04093126760858853, 0.0450768224595083, 0.04797899871877142, 0.0780374468264754, -0.010625980168944067, -0.2150736395555738, 0.3544060345423424, 0.07890504993640392, 0.3584959748027436, 0.09771742913783212, 0.06414089832155002, 0.015622036799914757, -0.06772364260849811, 0.05445920074776888, -0.09904311972472203, 0.12373899872900283, 0.2175832465330486, 0.15091326021218388, 0.2259790729810247, -0.423228501957857, -0.26857082538653987, 0.10511326144638834, 0.11524599161930382, -0.007457355589811075, 0.02842335094958228, -0.2608529781070301, 0.09318567451653939, -0.1449628377363374, -0.12649706963812773, -0.023040104351574713, 0.019828882695854467, 0.0925352441332445, -0.2127031838221444, 0.04984078469037047, 0.033830268959656865, 0.07827744096659629, -0.013022426902553287, -0.12578856038182215, -0.08442911292007982, 0.1573230618397879, 0.02182355992322377, 0.015808904888818705, 0.14140727061983513, -0.14630497392203848, -0.11298310318251409, 0.3476522903952558, 0.002969799405437405, -0.17862024642842805, 0.14511110902945432, -0.0773571550064736, -0.14020001061529047, 0.05866448749527651, 0.2464432974653792, 0.09501372552527385, -0.15426857081455006, 0.024499246778158505, -0.06937194195718079, 0.14305618215131305, 0.0739840152318258, 0.08594854572645814, 0.1594582384043907, 0.23081383618952359, 0.09625252362309118, 0.14527615340144406, -0.10232310497075699, -0.15498679091017378, -0.21909967275588946, -0.08550837632047675, -0.21087009778593557, 0.023218015082559343, -0.13990914672812924, -0.14393094951934102, 0.4588042183668684, 0.07928080280248265, 0.21338049082038135, 0.03611868515736976, 0.2406775783737569, 0.07090161660584025, 0.05773788492463655, 0.11556265192120918, 0.17868151387862735, 0.12251590876701936, 0.10376266263409566, -0.18145937810186297, 0.1580338752022017, 0.07101095574355479] |
708.2609 | Incomplete normalization of probability on multifractals | This work is an extension of the incomplete probability theory from the
simple case of monofractals previously studied to the more general case of
multifractals which can occur in the phase space without equiprobable
partition.
| cond-mat.stat-mech | this work is an extension of the incomplete probability theory from the simple case of monofractals previously studied to the more general case of multifractals which can occur in the phase space without equiprobable partition | [['this', 'work', 'is', 'an', 'extension', 'of', 'the', 'incomplete', 'probability', 'theory', 'from', 'the', 'simple', 'case', 'of', 'monofractals', 'previously', 'studied', 'to', 'the', 'more', 'general', 'case', 'of', 'multifractals', 'which', 'can', 'occur', 'in', 'the', 'phase', 'space', 'without', 'equiprobable', 'partition']] | [-0.0760895812052435, 0.12312589109185085, -0.08537549493568285, 0.08768425339034626, -0.04381239930433886, -0.0900165546286319, 0.05541766552986311, 0.3256333727389574, -0.24401962899469903, -0.2391124628218157, 0.06080839347559959, -0.22463061570056847, -0.20756921395659447, 0.17206249620233263, -0.09612831770708519, 0.026016484733138764, -0.024365635881466525, 0.10381153968295881, -0.0795384210867009, -0.2660867732084755, 0.3378765842877328, 0.060733100239719666, 0.25902917885354587, -0.036047028164778436, -0.0011609648221305438, 0.04872544551534312, 5.929557207439627e-05, 0.050213007588172334, -0.11356715010479093, 0.08299850978489433, 0.2525999172723719, 0.1131196279078722, 0.21759201203073775, -0.4103247705580933, -0.26716223752924373, 0.1844593383105738, 0.13720302573804344, 0.1449837089749053, -0.008865471645341521, -0.2548227864317596, 0.04261172283440828, -0.2165436904877424, -0.15917871791337218, -0.0140392512748284, 0.000815013430214354, -0.0601243936589786, -0.27463320781077655, 0.07726090137979814, 0.11880333349108696, 0.02630445095045226, -0.049664192517021935, -0.08390752337540366, -0.0007349280374390738, 0.11868437850581748, 0.03649941203849656, 0.057567510421254804, 0.03567733627610973, -0.1028840234436627, -0.12256572315735477, 0.3833123269890036, -6.155576556921005e-05, -0.22635138545717512, 0.17811169419770262, -0.16477750271026578, -0.1654509569252176, 0.1402330479451588, 0.12544966925467763, 0.18403283213930471, -0.150733436484422, 0.1256725100800395, -0.09194230855043445, 0.1359669697470963, 0.08834871993001019, 0.021649904730397143, 0.1361942595137017, 0.12792387596730675, 0.05555151678355677, 0.19586622382381133, -0.047881833064768994, -0.18308673383934157, -0.3018465946827616, -0.13887520363288267, -0.2097489045666797, 0.05331949988113982, -0.07950428170817239, -0.17720017204327243, 0.36703577431450995, 0.1213363011367619, 0.20014871353549615, 0.06178567973963384, 0.26643299162387846, 0.1394258392176458, 0.006774555000343493, 0.009158340123082911, 0.18262909689385975, 0.09979337483112301, 0.0481801748541849, -0.1206019197524126, 0.08071886086836458, 0.07297809344849417] |
708.261 | Connection probability for random graphs with given degree sequence | Recently, the classical configuration model for random graphs with given
degree distribution has been extensively used as a null model in contraposition
to real networks with the same degree distribution. In this paper, we briefly
review the applications of this model and derive analytical expression for
connection probability by the expanding coefficient method. We also use our
expanding coefficient method to obtain the connection probability for the
directed configuration model.
| math-ph math.MP | recently the classical configuration model for random graphs with given degree distribution has been extensively used as a null model in contraposition to real networks with the same degree distribution in this paper we briefly review the applications of this model and derive analytical expression for connection probability by the expanding coefficient method we also use our expanding coefficient method to obtain the connection probability for the directed configuration model | [['recently', 'the', 'classical', 'configuration', 'model', 'for', 'random', 'graphs', 'with', 'given', 'degree', 'distribution', 'has', 'been', 'extensively', 'used', 'as', 'a', 'null', 'model', 'in', 'contraposition', 'to', 'real', 'networks', 'with', 'the', 'same', 'degree', 'distribution', 'in', 'this', 'paper', 'we', 'briefly', 'review', 'the', 'applications', 'of', 'this', 'model', 'and', 'derive', 'analytical', 'expression', 'for', 'connection', 'probability', 'by', 'the', 'expanding', 'coefficient', 'method', 'we', 'also', 'use', 'our', 'expanding', 'coefficient', 'method', 'to', 'obtain', 'the', 'connection', 'probability', 'for', 'the', 'directed', 'configuration', 'model']] | [-0.05936230820204531, 0.03814787967130542, -0.08070668881492955, 0.04518653256486037, -0.05069502804960523, -0.12657481487175185, 0.02823810801741534, 0.4065736323595047, -0.22974643937112496, -0.29203319094542945, 0.06336824649645548, -0.23053064298416887, -0.23836655438478505, 0.14802432250164982, -0.02015420420627509, 0.09417095008705344, 0.05069044052091028, 0.08633244037628174, -0.023494750248002155, -0.23859109441151044, 0.3143372344651392, 0.10203433771218573, 0.31525515454954334, 0.05403447904224907, 0.11836324771200972, 0.02307153475869979, -0.019873700982757977, 0.05093059153961284, -0.17337701046573264, 0.14076129937810558, 0.17734789908198373, 0.15401954735030554, 0.208335887560887, -0.3870793825813702, -0.2801939741575292, 0.1522537506185472, 0.12961122642404266, 0.126863513486543, -0.049778115030910286, -0.2609091533081872, 0.07651299356615969, -0.23541978264069519, -0.2130875294163291, -0.05584339432950531, 0.05909671759498971, 0.05518816809302994, -0.2728292143238442, 0.06919272717246454, 0.038422055409422944, 0.04021801474903311, -0.027337719551620208, -0.11464959649103028, 0.046215272159315646, 0.12469995832735939, 0.030358430137857793, 0.04833311646112374, 0.017124352896852154, -0.11222734732021178, -0.13608289816017663, 0.32893641599054846, -0.0732903691141733, -0.25790319533220357, 0.1443684645870235, -0.1361542236259473, -0.16154563925894244, 0.047388203904431846, 0.20201340684933322, 0.13619291218263763, -0.17118220660569414, 0.10924458204286307, -0.059931744156139236, 0.09418771831052644, 0.05100798469835094, -0.016870868485420944, 0.15332569370844534, 0.14018736125768294, 0.04049946724969362, 0.19641329393988208, -0.09000139680158879, -0.14296818471380643, -0.2792774775996804, -0.15373620336343136, -0.19884594336950354, 0.040714501842324224, -0.11884223229364059, -0.15671445040497928, 0.4186627327863659, 0.18801792523091926, 0.22493763148252452, 0.10625667082411902, 0.29478715104716163, 0.1416285335285855, -0.005980364186689258, 0.08295536034607462, 0.18009768500924112, 0.17874423579778523, 0.10066492983273097, -0.11735431304467576, 0.11433268622495234, 0.102309200912714] |
708.2611 | Boundedness and Compactness of Toeplitz operators with L^1 symbols on
the Bergman space | We characterise the boundedness of a Toeplitz operator on the Bergman space
with an L^1 symbol.We also prove that the compactness of a Toeplitz operator on
the Bergman space with an L^1 symbol is completely determined by the boundary
behaviour of itss Berezin transform. This result extends known results in the
cases when the symbol is either a positive L^1 function, an L^\infty function
or a general BMO^1 function.
| math.CV math.CA | we characterise the boundedness of a toeplitz operator on the bergman space with an l1 symbolwe also prove that the compactness of a toeplitz operator on the bergman space with an l1 symbol is completely determined by the boundary behaviour of itss berezin transform this result extends known results in the cases when the symbol is either a positive l1 function an linfty function or a general bmo1 function | [['we', 'characterise', 'the', 'boundedness', 'of', 'a', 'toeplitz', 'operator', 'on', 'the', 'bergman', 'space', 'with', 'an', 'l1', 'symbolwe', 'also', 'prove', 'that', 'the', 'compactness', 'of', 'a', 'toeplitz', 'operator', 'on', 'the', 'bergman', 'space', 'with', 'an', 'l1', 'symbol', 'is', 'completely', 'determined', 'by', 'the', 'boundary', 'behaviour', 'of', 'itss', 'berezin', 'transform', 'this', 'result', 'extends', 'known', 'results', 'in', 'the', 'cases', 'when', 'the', 'symbol', 'is', 'either', 'a', 'positive', 'l1', 'function', 'an', 'linfty', 'function', 'or', 'a', 'general', 'bmo1', 'function']] | [-0.12933787861017182, 0.07593078381850159, -0.051336905234219396, 0.1317285260216415, -0.08656648899812032, -0.05958341223680798, -0.001736391897258513, 0.32613934740862427, -0.32261474650380584, -0.12446667731958716, 0.21741973526385502, -0.27975782505168084, -0.18754844930748837, 0.1545783403391183, -0.1662164394853308, 0.04865731466013719, 0.0639673157060957, 0.120570929001962, -0.1862705537932925, -0.22533150230917862, 0.44585346742807064, 0.023137480636839482, 0.15690766909050152, 0.03874882141484276, 0.05831191093688283, 0.03136733100537265, -0.010592568912269437, -0.1060696480381279, -0.1370588316457382, 0.08985606692594421, 0.20562170330873308, 0.12481064105753938, 0.30897004097042713, -0.3590055906268604, -0.18128301548388073, 0.1698260709098951, 0.13963875401874676, -0.0653605348951019, -0.022984682376879978, -0.3338429023073438, 0.06157505115055863, -0.114200027043219, -0.16105586093823043, -0.07187938031411785, 0.007435476318385233, 0.040839020573698426, -0.3706468945944353, 0.0316610277920571, 0.173466224278159, 0.03516640983905424, -0.1724293152185376, -0.10760510032688377, 0.006876716088941868, 0.07615441380638753, 0.03208410222877694, 0.1198072777085198, 0.045315371805747205, -0.0309214905856232, -0.06420948644004323, 0.2521175199927872, -0.11226236221024438, -0.31571624586350105, 0.10996184988385614, -0.22437116948490524, -0.08496387634316788, 0.05838254996684983, 0.0700623528305989, 0.19940196809714988, -0.10386339077654959, 0.18848048738779172, -0.09618953805629109, 0.16194751790231643, 0.08793759724358097, 0.06502868020513286, 0.0432887792806415, 0.08344993770793628, 0.2168741799695828, 0.17587626881568746, -0.026395785899641103, -0.027507038581568527, -0.33731830454267125, -0.18946413341087892, -0.24982583329684155, 0.0569003839388161, -0.14774166207815356, -0.22719988443286104, 0.35670890528982613, 0.011391152600374292, 0.24401251323904624, 0.12697050580754876, 0.25398889649659395, 0.20961663609041886, 0.076973980785731, 0.08186127806958907, 0.1565021817188929, 0.18468228116741076, 0.12192916735897169, -0.21354032321216757, 0.015601557138485505, 0.2265234816723558] |
708.2612 | First Results From the Large Binocular Telescope: Deep Photometry of New
dSphs | This contribution describes photometry for two Galactic dSphs obtained with
the Large Binocular Telescope to a magnitude of ~25.5. Using the Large
Binocular Camera, a purpose-built wide-field imager for the LBT, we have
examined the structure and star formation histories of two newly-discovered
Local Group members, the Hercules dSph and the Leo T dSph/dIrr system. We have
constructed a structural map for the Hercules system using three-filter
photometry to V ~ 25.5. This is the first deep photometry for this system, and
it indicates that Hercules is unusually elongated, possibly indicating
distortion due to the Galactic tidal field. We have also derived the first star
formation history for the Leo T system, and find that its oldest population of
stars (age ~ 13 Gyr) were relatively metal-rich, with [Fe/H] ~ -1.5.
| astro-ph | this contribution describes photometry for two galactic dsphs obtained with the large binocular telescope to a magnitude of 255 using the large binocular camera a purposebuilt widefield imager for the lbt we have examined the structure and star formation histories of two newlydiscovered local group members the hercules dsph and the leo t dsphdirr system we have constructed a structural map for the hercules system using threefilter photometry to v 255 this is the first deep photometry for this system and it indicates that hercules is unusually elongated possibly indicating distortion due to the galactic tidal field we have also derived the first star formation history for the leo t system and find that its oldest population of stars age 13 gyr were relatively metalrich with feh 15 | [['this', 'contribution', 'describes', 'photometry', 'for', 'two', 'galactic', 'dsphs', 'obtained', 'with', 'the', 'large', 'binocular', 'telescope', 'to', 'a', 'magnitude', 'of', '255', 'using', 'the', 'large', 'binocular', 'camera', 'a', 'purposebuilt', 'widefield', 'imager', 'for', 'the', 'lbt', 'we', 'have', 'examined', 'the', 'structure', 'and', 'star', 'formation', 'histories', 'of', 'two', 'newlydiscovered', 'local', 'group', 'members', 'the', 'hercules', 'dsph', 'and', 'the', 'leo', 't', 'dsphdirr', 'system', 'we', 'have', 'constructed', 'a', 'structural', 'map', 'for', 'the', 'hercules', 'system', 'using', 'threefilter', 'photometry', 'to', 'v', '255', 'this', 'is', 'the', 'first', 'deep', 'photometry', 'for', 'this', 'system', 'and', 'it', 'indicates', 'that', 'hercules', 'is', 'unusually', 'elongated', 'possibly', 'indicating', 'distortion', 'due', 'to', 'the', 'galactic', 'tidal', 'field', 'we', 'have', 'also', 'derived', 'the', 'first', 'star', 'formation', 'history', 'for', 'the', 'leo', 't', 'system', 'and', 'find', 'that', 'its', 'oldest', 'population', 'of', 'stars', 'age', '13', 'gyr', 'were', 'relatively', 'metalrich', 'with', 'feh', '15']] | [-0.09097804073462612, 0.06626083195442334, -0.13498593986878404, 0.0502624970567922, -0.12950332976470236, -0.0820558176819759, 0.04299221060500713, 0.42261801147833467, -0.19957723791594617, -0.3856806817348115, 0.0420370603678748, -0.289338163449429, -0.08773036774800858, 0.1843355822202284, -0.07268815161660314, -0.06885144475427296, 0.12487332694945508, -0.0665340566119994, -0.0220183830242604, -0.3220923593999032, 0.28085575435397914, 0.027148617454940904, 0.12480976993902004, -0.12221467998506341, 0.10690337412961526, -0.07419955758814467, -0.04953750042113825, -0.013456554501317441, -0.16125524602523456, 0.014836287184152752, 0.21413504441079567, 0.10774799024511594, 0.22660659401481098, -0.292534595442703, -0.16259761033870745, 0.007013392892986303, 0.18031138885999098, 0.017473926061938982, -0.12071090475365054, -0.3127909133763751, 0.10720811422652332, -0.20341137290233746, -0.18821527312684339, 0.08352789919217685, 0.09862134770537523, 0.022024625326594105, -0.23797214588421411, 0.08443596786014496, -0.008875841362169012, 0.18079797289465205, -0.17025940807161533, -0.13042406921158545, -0.03334944456901212, 0.10342630585000734, -0.03327960973183508, 0.12164916742403875, 0.12253257627162384, -0.12933260343561415, 0.02421885596413631, 0.3983977488896926, -0.11391411466320278, 0.07203352484611969, 0.21620220177464944, -0.22691918689088197, -0.21683527778805, 0.07675515090727458, 0.12740828717505792, 0.11141720112573239, -0.22271878353831198, 0.06079089207742072, -0.001337926911219256, 0.18992039341901545, 0.031595283006026875, 0.0475848831483745, 0.2766455374912766, 0.15451712463095646, 0.06898725330211164, 0.049659517431791755, -0.33114560386093217, -0.02603830622001624, -0.18542275622166926, -0.10142997071670834, -0.1077390026403009, 0.049950796164921485, -0.13668224431921772, -0.10945985665239277, 0.34023167578561697, 0.10630447971561807, 0.21031440762453713, 0.05084658320356539, 0.28978594276941294, 0.03867496836801365, 0.18036688447318738, 0.11544451495137764, 0.30726608927943744, 0.1733166050635191, 0.10676005916320719, -0.2590506357742015, 0.06985086555141606, 0.012639085318369325] |
708.2613 | Pion freeze-out through HBT correlation in HICs from AGS/FAIR to RHIC
energies | In this talk we present the results of two-pion HBT correlation at freeze-out
in heavy ion collisions (HICs) from AGS to RHIC energies. The UrQMD
hadron-string transport model as well as the CRAB analyzing program are
adopted. Based on the cascade mode, in general, the calculations are satisfying
and well in line with the experimental data although discrepancies are not
negligible. Such as: I), the HBT time-related puzzle exists at all energies.
II), at low AGS energies, the calculated volume as well as the mean free path
of pion source at freeze-out are lower than data. It implies that a better
description of interactions of particles at early stage of HICs is required.
| nucl-th | in this talk we present the results of twopion hbt correlation at freezeout in heavy ion collisions hics from ags to rhic energies the urqmd hadronstring transport model as well as the crab analyzing program are adopted based on the cascade mode in general the calculations are satisfying and well in line with the experimental data although discrepancies are not negligible such as i the hbt timerelated puzzle exists at all energies ii at low ags energies the calculated volume as well as the mean free path of pion source at freezeout are lower than data it implies that a better description of interactions of particles at early stage of hics is required | [['in', 'this', 'talk', 'we', 'present', 'the', 'results', 'of', 'twopion', 'hbt', 'correlation', 'at', 'freezeout', 'in', 'heavy', 'ion', 'collisions', 'hics', 'from', 'ags', 'to', 'rhic', 'energies', 'the', 'urqmd', 'hadronstring', 'transport', 'model', 'as', 'well', 'as', 'the', 'crab', 'analyzing', 'program', 'are', 'adopted', 'based', 'on', 'the', 'cascade', 'mode', 'in', 'general', 'the', 'calculations', 'are', 'satisfying', 'and', 'well', 'in', 'line', 'with', 'the', 'experimental', 'data', 'although', 'discrepancies', 'are', 'not', 'negligible', 'such', 'as', 'i', 'the', 'hbt', 'timerelated', 'puzzle', 'exists', 'at', 'all', 'energies', 'ii', 'at', 'low', 'ags', 'energies', 'the', 'calculated', 'volume', 'as', 'well', 'as', 'the', 'mean', 'free', 'path', 'of', 'pion', 'source', 'at', 'freezeout', 'are', 'lower', 'than', 'data', 'it', 'implies', 'that', 'a', 'better', 'description', 'of', 'interactions', 'of', 'particles', 'at', 'early', 'stage', 'of', 'hics', 'is', 'required']] | [-0.03151462319620217, 0.19880896791469602, -0.13428671313789714, 0.15692235863215365, 0.0175853206557675, -0.14330045315560647, -0.06093432778797516, 0.3621251197218631, -0.19947000828662279, -0.33133821987209067, 0.014956243578303375, -0.3565901769737227, 0.04313801595759866, 0.1722219271427721, 0.0654347255883689, 0.06531523539379766, 0.12227875555956126, 0.03901880410442178, -0.06380219396978484, -0.14736130682800988, 0.32458404148516734, 0.16802077924222808, 0.22565769845108807, 0.18601937122556456, 0.0659158025946534, 0.006915411582233104, 0.0050959930079371, 0.013149890043171106, -0.12023318789939785, 0.031768177873176824, 0.28626597282039906, 0.06620266286870546, 0.1557515597514874, -0.4152691772916412, -0.18154575361713635, 0.0835500750196191, 0.1482778761651268, 0.1602011996082368, -0.04531937287564068, -0.1808572641071097, 0.06872881748260254, -0.18020130122756273, -0.12712990600549806, -0.0180252382894401, -0.021128551362791157, 0.064916966271801, -0.2565896144318106, 0.14280245196799526, -0.02988762281365297, 0.10108513313089858, -0.04395937903545204, -0.24268707327144962, -0.052639070702551874, 0.05244020131968819, 0.06069497470393678, 0.06634690566503533, 0.1544122468573, -0.12433195782442108, -0.10029060975390906, 0.4427243539882181, -0.04867160137996708, -0.0892781026381175, 0.1826831501006124, -0.16865265403824767, -0.15778592610484468, 0.16048678079109013, 0.1692905087637987, 0.08933302912056504, -0.1785930275373095, -0.011065007665707623, -0.012954475044940425, 0.13061284050268798, 0.08160057551004982, 0.060874068246746384, 0.18600594036187615, 0.20365578747370933, -0.03551007980332438, 0.05961501645890118, -0.09666038255734716, -0.11834222935881894, -0.3991044138484033, -0.07698184528709513, -0.1701494906923375, 0.006380266998405156, -0.039835286198829846, -0.07691802380326311, 0.33896094073533223, 0.12871987534381976, 0.25266388294377684, 0.036900771299657305, 0.2964210098277596, 0.09766866843137824, 0.0723539597923513, 0.12072633878672774, 0.2690906502570199, 0.08375256667449345, 0.20846942236515142, -0.2548146695166464, 0.06753948484588645, 0.04469124228998491] |
708.2614 | On the blow up phenomenon for the $L^2$-critical focusing Hartree
equation in $\Bbb R^4$ | We characterize the dynamics of the finite time blow up solutions with
minimal mass for the focusing mass critical Hartree equation with
$H^1(\mathbb{R}^4)$ data and $L^2(\mathbb{R}^4)$ data, where we make use of the
refined Gagliardo-Nirenberg inequality of convolution type and the profile
decomposition. Moreover, we also analyze the mass concentration phenomenon of
such blow up solutions.
| math.AP math-ph math.MP | we characterize the dynamics of the finite time blow up solutions with minimal mass for the focusing mass critical hartree equation with h1mathbbr4 data and l2mathbbr4 data where we make use of the refined gagliardonirenberg inequality of convolution type and the profile decomposition moreover we also analyze the mass concentration phenomenon of such blow up solutions | [['we', 'characterize', 'the', 'dynamics', 'of', 'the', 'finite', 'time', 'blow', 'up', 'solutions', 'with', 'minimal', 'mass', 'for', 'the', 'focusing', 'mass', 'critical', 'hartree', 'equation', 'with', 'h1mathbbr4', 'data', 'and', 'l2mathbbr4', 'data', 'where', 'we', 'make', 'use', 'of', 'the', 'refined', 'gagliardonirenberg', 'inequality', 'of', 'convolution', 'type', 'and', 'the', 'profile', 'decomposition', 'moreover', 'we', 'also', 'analyze', 'the', 'mass', 'concentration', 'phenomenon', 'of', 'such', 'blow', 'up', 'solutions']] | [-0.09078715067695488, 0.07147460617548362, -0.07261698350140994, 0.09598704840649258, -0.06663180399178104, -0.13434423746710475, 0.06508830325169997, 0.2936769585802474, -0.3107750932601365, -0.27975854131985795, 0.16697213315320286, -0.3009173156185584, -0.06319688309661367, 0.17559963060034947, -0.009512646902691234, 0.09407506632533941, 0.028134008937261323, 0.02850365008820187, -0.12335688242561776, -0.2496956389566714, 0.4224748132242398, -0.043863806257087905, 0.23274773359298706, 0.09812704805623401, 0.10891313356855377, -0.04379815975712104, -0.0024391320534050465, -0.03289535583250902, -0.256590015466579, 0.06978969488038936, 0.13747007738460193, 0.11298565742644397, 0.2526759379289367, -0.40977983691475606, -0.16834575278176503, 0.14804306517947805, 0.16218962208791213, 0.09554015277800235, -0.09428207158026371, -0.24717828062447636, 0.051851558634503324, -0.1434327668087049, -0.2602538320828568, -0.10339944962073457, -0.00700846929949793, 0.09482985247265209, -0.28442342575978147, 0.15162751975585706, 0.0005307895046743479, 0.0037184413099153476, -0.13552178359505804, -0.030043947493488137, -0.017888169651004402, 0.08115825393999165, 0.0677136967805299, -0.019719569300386038, 0.06585998471656984, -0.11707753328691152, -0.0327992322770032, 0.340269870954481, -0.10680958190086214, -0.200198049039781, 0.13878934846513652, -0.19056327244774862, -0.12976846418936144, 0.10627429953522304, 0.19107981103218413, 0.14420306227931923, -0.12989786804061043, 0.10696302567481655, -0.025446279719471932, 0.17568176354874265, 0.12048731409013272, 0.015750208327716047, 0.057693563858893786, 0.19276219191960992, 0.11340331455523317, 0.0915700339288874, -0.09950871423140846, -0.08006028167226098, -0.3069680530747229, -0.19181062164293095, -0.11911418353292075, 0.09230436473153532, -0.16178592242755588, -0.15933673209087415, 0.37667865257032895, 0.13140371380035173, 0.2049530958079479, 0.1002437929368832, 0.2038773480125449, 0.16431651165370237, 0.07746331341225993, 0.1082523650913076, 0.20055231137878515, 0.14016588228670032, 0.13945853304625913, -0.23334721072830938, -0.05057543670250611, 0.11918583698570728] |
708.2615 | Aging dynamics of non-linear elastic interfaces: the Kardar-Parisi-Zhang
equation | In this work, the out-of-equilibrium dynamics of the Kardar-Parisi-Zhang
equation in (1+1) dimensions is studied by means of numerical simulations,
focussing on the two-times evolution of an interface in the absence of any
disordered environment. This work shows that even in this simple case, a rich
aging behavior develops. A multiplicative aging scenario for the two-times
roughness of the system is observed, characterized by the same growth exponent
as in the stationary regime. The analysis permits the identification of the
relevant growing correlation length, accounting for the important scaling
variables in the system. The distribution function of the two-times roughness
is also computed and described in terms of a generalized scaling relation.
These results give good insight into the glassy dynamics of the important case
of a non-linear elastic line in a disordered medium.
| cond-mat.stat-mech | in this work the outofequilibrium dynamics of the kardarparisizhang equation in 11 dimensions is studied by means of numerical simulations focussing on the twotimes evolution of an interface in the absence of any disordered environment this work shows that even in this simple case a rich aging behavior develops a multiplicative aging scenario for the twotimes roughness of the system is observed characterized by the same growth exponent as in the stationary regime the analysis permits the identification of the relevant growing correlation length accounting for the important scaling variables in the system the distribution function of the twotimes roughness is also computed and described in terms of a generalized scaling relation these results give good insight into the glassy dynamics of the important case of a nonlinear elastic line in a disordered medium | [['in', 'this', 'work', 'the', 'outofequilibrium', 'dynamics', 'of', 'the', 'kardarparisizhang', 'equation', 'in', '11', 'dimensions', 'is', 'studied', 'by', 'means', 'of', 'numerical', 'simulations', 'focussing', 'on', 'the', 'twotimes', 'evolution', 'of', 'an', 'interface', 'in', 'the', 'absence', 'of', 'any', 'disordered', 'environment', 'this', 'work', 'shows', 'that', 'even', 'in', 'this', 'simple', 'case', 'a', 'rich', 'aging', 'behavior', 'develops', 'a', 'multiplicative', 'aging', 'scenario', 'for', 'the', 'twotimes', 'roughness', 'of', 'the', 'system', 'is', 'observed', 'characterized', 'by', 'the', 'same', 'growth', 'exponent', 'as', 'in', 'the', 'stationary', 'regime', 'the', 'analysis', 'permits', 'the', 'identification', 'of', 'the', 'relevant', 'growing', 'correlation', 'length', 'accounting', 'for', 'the', 'important', 'scaling', 'variables', 'in', 'the', 'system', 'the', 'distribution', 'function', 'of', 'the', 'twotimes', 'roughness', 'is', 'also', 'computed', 'and', 'described', 'in', 'terms', 'of', 'a', 'generalized', 'scaling', 'relation', 'these', 'results', 'give', 'good', 'insight', 'into', 'the', 'glassy', 'dynamics', 'of', 'the', 'important', 'case', 'of', 'a', 'nonlinear', 'elastic', 'line', 'in', 'a', 'disordered', 'medium']] | [-0.14816351725529608, 0.1351582547329382, -0.12266807354736461, 0.06281142224255365, 0.0254001096216788, -0.09905428726073187, -0.003480383926488237, 0.2957919884606442, -0.258636140730232, -0.2484287580391809, 0.06813682846502582, -0.25044323370180355, -0.2032699138308361, 0.18790226351511455, 0.015401097685237652, 0.06635916377626248, -0.004211422959481602, -0.001583327125730132, -0.05726409549807518, -0.19612369021929021, 0.3159590655131571, 0.052332488051094396, 0.2919236364246193, 0.04812502659120555, 0.07018723989725668, 0.042172855409574626, -0.020270479216636505, 0.05602077171102222, -0.16421280755973533, 0.05979892388055685, 0.20663237219516523, 0.02087949301679132, 0.25905434322307136, -0.40309812334963857, -0.2568077528605988, 0.0503712544641666, 0.18114996927011925, 0.09103058457961861, -0.057211684943142056, -0.24394505007762407, 0.031342638315938746, -0.13864584279997247, -0.19819372569891944, -0.014991405447805995, 0.046435196098607426, 0.020231111448192136, -0.24223119620261574, 0.1419202930364782, 0.11022469671026094, 0.07948318925866885, -0.08649099692215782, -0.04633135424836525, 0.0037315367293585815, 0.13878622415228817, 0.041469010116129336, -0.00993391082955719, 0.12823896216395408, -0.16920905618115203, -0.0647777323450358, 0.3774574235595985, -0.05520176692559982, -0.19469082711000385, 0.19349623261603402, -0.182785930204094, -0.12198512171353422, 0.14778536614273854, 0.16981796719439662, 0.08128374783711424, -0.16727252865432582, 0.09977533951982266, -0.046015559550576304, 0.1745127584288286, 0.011609819147791436, 0.020693097044644292, 0.15671406949022368, 0.24486668542055273, -0.002486050045534746, 0.204461459746348, -0.029858951948569225, -0.142287319553877, -0.30538853522695936, -0.1663285271028307, -0.19128675569967826, 0.07421192203721365, -0.13904897814324219, -0.18419684089525645, 0.4041884781709358, 0.1258672576175252, 0.20278807906711946, 0.05182243018140043, 0.24331572264738716, 0.15644125924914826, 0.027299883181173632, 0.05150184123568348, 0.22270435866302074, 0.12260151000731666, 0.12596532150950115, -0.2714409989186688, 0.12566142456272422, 0.041701502922519264] |
708.2616 | An Experimental Investigation of Secure Communication With Chaos Masking | The most exciting recent development in nonlinear dynamics is realization
that chaos can be useful. One application involves "Secure Communication". Two
piecewise linear systems with switching nonlinearities have been taken as chaos
generators. In the present work the phenomenon of secure communication with
chaos masking has been investigated experimentally. In this investigation chaos
which is generated from two chaos generators is masked with the massage signal
to be transmitted, thus makes communication is more secure.
| cs.CR | the most exciting recent development in nonlinear dynamics is realization that chaos can be useful one application involves secure communication two piecewise linear systems with switching nonlinearities have been taken as chaos generators in the present work the phenomenon of secure communication with chaos masking has been investigated experimentally in this investigation chaos which is generated from two chaos generators is masked with the massage signal to be transmitted thus makes communication is more secure | [['the', 'most', 'exciting', 'recent', 'development', 'in', 'nonlinear', 'dynamics', 'is', 'realization', 'that', 'chaos', 'can', 'be', 'useful', 'one', 'application', 'involves', 'secure', 'communication', 'two', 'piecewise', 'linear', 'systems', 'with', 'switching', 'nonlinearities', 'have', 'been', 'taken', 'as', 'chaos', 'generators', 'in', 'the', 'present', 'work', 'the', 'phenomenon', 'of', 'secure', 'communication', 'with', 'chaos', 'masking', 'has', 'been', 'investigated', 'experimentally', 'in', 'this', 'investigation', 'chaos', 'which', 'is', 'generated', 'from', 'two', 'chaos', 'generators', 'is', 'masked', 'with', 'the', 'massage', 'signal', 'to', 'be', 'transmitted', 'thus', 'makes', 'communication', 'is', 'more', 'secure']] | [-0.24346033640671522, 0.12055259643743435, -0.11804581058522065, 0.01414779827153931, -0.08220944815625747, -0.21775515442093213, -0.04456233487464487, 0.3790201458831628, -0.3100464748855059, -0.21136757085720698, 0.16878804955786714, -0.24181753121316432, -0.22976252398143213, 0.2610025321692228, -0.07253175883088261, 0.11562629106299331, 0.0012040941541393599, -0.0317805979338785, 0.02498813814483583, -0.24688590951574346, 0.25827621389801303, 0.07300830054290904, 0.26980877907636264, -0.029887706246227025, 0.04261489029973745, -0.011739279391864936, -0.030070992627491553, -0.04219572661444545, -0.0769229526356988, 0.10669412203133107, 0.31884928164382775, 0.12183955465753873, 0.30464236286779245, -0.3929067664965987, -0.2846774354701241, 0.10948562080661456, 0.1674817013864716, 0.16330916206507634, -0.10388347371578371, -0.2786233961333831, 0.06493734247982502, -0.173376506799832, -0.09139212371471027, -0.07522220592945814, 0.030828112264474232, 0.024163019706805546, -0.2784973335514466, 0.049386123820828895, 0.03805880730894084, 0.12799115762114524, 0.0861549722434332, 0.013343612824877104, -0.012878255645434062, 0.13496847349529464, -0.025697560533881187, 0.029706205539405346, 0.09492825378974279, -0.07430172649212181, -0.19002473248479268, 0.3663936463991801, -0.020405310764908792, -0.1729201056037952, 0.21003609834238887, -0.11080029870073001, -0.14383834895056982, 0.14859465730686983, 0.17642448846871653, 0.02957164972399672, -0.1988705531756083, 0.06634627694264054, 0.011015726632128159, 0.17706052691365282, 0.08800983598455786, 0.1283793277790149, 0.18087992074899376, 0.21317200899124145, 0.079001493928954, 0.15762234235492845, -0.03546543808033069, -0.16474723579051595, -0.21182263344526292, -0.12993181073417268, -0.22967250941942136, 0.056896836571395396, -0.03547796970854203, -0.08657613355045517, 0.3664145369827747, 0.21299821208541592, 0.13464208966121077, -0.011037432857168218, 0.36281836917002996, 0.15558401946444064, 0.09676921972384056, 0.08622886231789986, 0.3003454647461573, 0.1486931606630484, 0.08649531679538389, -0.13099333765450866, 0.14787981823086738, 0.005958297836283843] |
708.2617 | Sensitivity to SUSY Seesaw Parameters and Lepton Flavour Violation | We address the constraints on the SUSY seesaw parameters arising from Lepton
Flavour Violation observables. Working in the Constrained Minimal
Supersymmetric Standard Model extended by three right-handed (s)neutrinos, we
study the predictions for the branching ratios of $l_j \to l_i \gamma$ and $l_j
\to 3 l_i$ channels. We impose compatibility with neutrino data, electric
dipole moment bounds, and further require a successful baryon asymmetry of the
Universe (via thermal leptogenesis). We emphasise the interesting interplay
between $\theta_{13}$ and the LFV muon decays, pointing out the hints on the
SUSY seesaw parameters that can arise from measurements of $\theta_{13}$ and
LFV branching ratios. This is a brief summary of the work of Ref.
\cite{Antusch:2006vw}.
| hep-ph | we address the constraints on the susy seesaw parameters arising from lepton flavour violation observables working in the constrained minimal supersymmetric standard model extended by three righthanded sneutrinos we study the predictions for the branching ratios of l_j to l_i gamma and l_j to 3 l_i channels we impose compatibility with neutrino data electric dipole moment bounds and further require a successful baryon asymmetry of the universe via thermal leptogenesis we emphasise the interesting interplay between theta_13 and the lfv muon decays pointing out the hints on the susy seesaw parameters that can arise from measurements of theta_13 and lfv branching ratios this is a brief summary of the work of ref citeantusch2006vw | [['we', 'address', 'the', 'constraints', 'on', 'the', 'susy', 'seesaw', 'parameters', 'arising', 'from', 'lepton', 'flavour', 'violation', 'observables', 'working', 'in', 'the', 'constrained', 'minimal', 'supersymmetric', 'standard', 'model', 'extended', 'by', 'three', 'righthanded', 'sneutrinos', 'we', 'study', 'the', 'predictions', 'for', 'the', 'branching', 'ratios', 'of', 'l_j', 'to', 'l_i', 'gamma', 'and', 'l_j', 'to', '3', 'l_i', 'channels', 'we', 'impose', 'compatibility', 'with', 'neutrino', 'data', 'electric', 'dipole', 'moment', 'bounds', 'and', 'further', 'require', 'a', 'successful', 'baryon', 'asymmetry', 'of', 'the', 'universe', 'via', 'thermal', 'leptogenesis', 'we', 'emphasise', 'the', 'interesting', 'interplay', 'between', 'theta_13', 'and', 'the', 'lfv', 'muon', 'decays', 'pointing', 'out', 'the', 'hints', 'on', 'the', 'susy', 'seesaw', 'parameters', 'that', 'can', 'arise', 'from', 'measurements', 'of', 'theta_13', 'and', 'lfv', 'branching', 'ratios', 'this', 'is', 'a', 'brief', 'summary', 'of', 'the', 'work', 'of', 'ref', 'citeantusch2006vw']] | [-0.11224476070180701, 0.2793155620404702, 0.0324200635410047, 0.19119954330381006, -0.12655034559845393, -0.1919100748657781, 0.10082503104318416, 0.28357764358848464, -0.22255755988797837, -0.2789805350174512, 0.0332692696299221, -0.28208357925385436, -0.0010982004335216647, 0.12485106034312464, 0.04056913567806727, 0.05519421482209249, 0.04831631900118997, -0.06700795692657786, -0.09711988312067531, -0.1822269371062118, 0.27921271035614026, 0.0733822595565081, 0.19289542941260152, 0.08361799697325166, 0.04471389074647699, -0.0872976089885924, -0.07553775430382562, -0.09288302775738495, -0.17094459494683178, 0.054788718528080996, 0.16661526439877758, 0.14318580445251428, 0.01676702825592916, -0.4156742402452177, -0.09478452121506312, 0.2444444514528316, 0.1409254841938881, 0.06554926077868524, -0.04907689800061884, -0.31672720559540074, 0.04488214572276255, -0.19691494619889585, -0.0648057200555091, -0.06537056307219505, -0.041957231205222864, -0.1016383182161787, -0.4024487922807956, 0.09691735573453895, -0.03478056988043526, 0.0026704699266701937, 0.06088259479396844, -0.2352249670470233, -0.009142157397166426, -0.0007860212686604687, 0.24411182321377314, -0.06526289482592672, 0.18735160644739932, -0.16661307065390116, -0.19153873348529618, 0.42103234671854545, -0.06846667546155263, -0.16016252483573876, 0.09775171819221994, -0.18013665171539678, -0.22839051134568372, 0.08174073962228638, 0.19508115073715868, 0.036804888823618445, -0.18088407479185012, 0.22439883921054257, -0.07905230131499204, 0.10922206526031784, 0.03304606215429625, 0.04638239473985907, 0.2938921396021864, 0.21475659392308444, 0.05842494051570871, 0.0060375154633740226, -0.0934106764907483, -0.020057281662177826, -0.47834395266337587, -0.09151276210468495, -0.05170436935648987, 0.11877168475101436, -0.10132573602719017, -0.017315790363811954, 0.442288463344864, 0.15200761321882186, 0.26508095339938464, 0.05815904256892931, 0.2997260571241246, 0.07926837577023045, 0.0645922883413732, -0.012551521603849583, 0.311032122013525, 0.1912766759653875, 0.14051819226837584, -0.30941384007538936, 0.011631325614871457, 0.07548003563091957] |
708.2618 | Using Local Volume data to constrain Dark Matter dynamics | The peculiar velocity reconstruction methods allow one to have a deeper
insight into the distribution of dark matter: both to measure mean matter
density and to obtain the primordial density fluctuations. We present here the
Monge-Ampere-Kantorovitch method applied to mock catalogues mimicking in both
redshift and distance catalogues. After having discussed the results obtained
for a class of biases that may be corrected for, we focus on the systematics
coming from the unknown distribution of unobserved mass and from the
statistical relationship between mass and luminosity. We then show how to use
these systematics to put constraints on the dark matter distribution. Finally a
preliminary application to an extended version (c z < 3000 km/s) of the
Neighbour Galaxy Catalogue is presented. We recover the peculiar velocities in
our neighbourhood and present a preliminary measurement of the local Omega_M.
| astro-ph | the peculiar velocity reconstruction methods allow one to have a deeper insight into the distribution of dark matter both to measure mean matter density and to obtain the primordial density fluctuations we present here the mongeamperekantorovitch method applied to mock catalogues mimicking in both redshift and distance catalogues after having discussed the results obtained for a class of biases that may be corrected for we focus on the systematics coming from the unknown distribution of unobserved mass and from the statistical relationship between mass and luminosity we then show how to use these systematics to put constraints on the dark matter distribution finally a preliminary application to an extended version c z 3000 kms of the neighbour galaxy catalogue is presented we recover the peculiar velocities in our neighbourhood and present a preliminary measurement of the local omega_m | [['the', 'peculiar', 'velocity', 'reconstruction', 'methods', 'allow', 'one', 'to', 'have', 'a', 'deeper', 'insight', 'into', 'the', 'distribution', 'of', 'dark', 'matter', 'both', 'to', 'measure', 'mean', 'matter', 'density', 'and', 'to', 'obtain', 'the', 'primordial', 'density', 'fluctuations', 'we', 'present', 'here', 'the', 'mongeamperekantorovitch', 'method', 'applied', 'to', 'mock', 'catalogues', 'mimicking', 'in', 'both', 'redshift', 'and', 'distance', 'catalogues', 'after', 'having', 'discussed', 'the', 'results', 'obtained', 'for', 'a', 'class', 'of', 'biases', 'that', 'may', 'be', 'corrected', 'for', 'we', 'focus', 'on', 'the', 'systematics', 'coming', 'from', 'the', 'unknown', 'distribution', 'of', 'unobserved', 'mass', 'and', 'from', 'the', 'statistical', 'relationship', 'between', 'mass', 'and', 'luminosity', 'we', 'then', 'show', 'how', 'to', 'use', 'these', 'systematics', 'to', 'put', 'constraints', 'on', 'the', 'dark', 'matter', 'distribution', 'finally', 'a', 'preliminary', 'application', 'to', 'an', 'extended', 'version', 'c', 'z', '3000', 'kms', 'of', 'the', 'neighbour', 'galaxy', 'catalogue', 'is', 'presented', 'we', 'recover', 'the', 'peculiar', 'velocities', 'in', 'our', 'neighbourhood', 'and', 'present', 'a', 'preliminary', 'measurement', 'of', 'the', 'local', 'omega_m']] | [-0.03900564533665123, 0.07182635284586807, -0.16550949368163617, 0.11801179825841537, -0.10332296529689627, -0.04883765931628699, 0.04725048515986461, 0.3918497128697642, -0.2288600432322816, -0.3597667714866408, 0.05288297448130529, -0.2840060290071542, -0.03831132086687279, 0.20070458556369056, -0.012316977431875294, 0.01512816388255162, 0.04672415889323737, -0.006481765169500761, -0.08806314372725658, -0.2595819840734539, 0.32956208337615006, 0.06384435480963575, 0.21170986888685475, -0.0005538279987722092, 0.09374106386493736, -0.030504036409250142, -0.10902014218209596, 0.023287503164343155, -0.2083692387051572, 0.08698030919462008, 0.16341019814738827, 0.13887398328333006, 0.22124886730631446, -0.356529049527743, -0.20321925407289154, 0.1202894372212952, 0.1474402895278848, 0.13184633623319167, -0.09798288246766276, -0.3291668955263865, 0.06630824201733526, -0.18261849301031036, -0.1564734128242644, -0.044507598803535, 0.011611610202349885, 0.037017671095656, -0.23126688878388435, 0.14939183879127033, -0.02072528813265427, 0.0007705500444574078, -0.07698185913040419, -0.15084808591980978, -0.04204537430064358, 0.09050552037129872, 0.030604090716649036, 0.03510601943984193, 0.1508752933676171, -0.14685953633832563, -0.021367239463313, 0.39731205583815155, -0.09620155096708383, -0.13484321457986467, 0.15370840159156463, -0.15963482503255788, -0.19428257844716745, 0.070191215445036, 0.2263248187360646, 0.03510131264091843, -0.15008349674515917, 0.027615448536035217, -0.0013318586887207126, 0.19464613818121654, 0.004170642462117176, 0.02978989258793057, 0.26589935010700166, 0.0993226995168213, 0.06721031243817704, 0.1004141193719404, -0.20581864722644108, -0.014406932976749474, -0.323942079541892, -0.10713983170372046, -0.16723703411339788, 0.038380544408340087, -0.09711117155620078, -0.1316138033710087, 0.3926090591716288, 0.20947496680437458, 0.2401612808836121, 0.08562291835359957, 0.2968320392418897, 0.07318286568922311, 0.03267894848249853, 0.056318136003466635, 0.2748681383384188, 0.19330606067784295, 0.055003799961193256, -0.18974237448542658, 0.026406704030088046, -0.0032694668213354193] |
708.2619 | Factors influencing the Martensitic interactions in Ni50Mn35Sn15: An
EXAFS study | Extended x-ray absorption fine-structure (EXAFS) measurements have been
carried out on Ni$_{50}$Mn$_{35}$Sn$_{15}$ in the austenitic and martensitic
phase. The temperatures associated with structural and magnetic phase
transformations are obtained from magnetization measurements. The system orders
ferromagnetically below 319 K while the structural phase transition occurs at
T$_M$ $\sim$ 200 K. EXAFS measurements have been carried out at Mn and Ni
K-edges and changes associated with respect to the local structure of these
absorbing atoms are compared. Significant changes in the nearest neighbour
interactions are seen as the system transits to the low temperature martensitic
phase. EXAFS provides evidence for local structural distortion even in the
cubic phase that is not seen from the x-ray diffraction studies. The results
obtained are understood in terms of changing hybridization between the
constituent atoms that influence the electronic structure at the Fermi level,
associated with the austenitic-to-martensitic transition.
| cond-mat.mtrl-sci | extended xray absorption finestructure exafs measurements have been carried out on ni_50mn_35sn_15 in the austenitic and martensitic phase the temperatures associated with structural and magnetic phase transformations are obtained from magnetization measurements the system orders ferromagnetically below 319 k while the structural phase transition occurs at t_m sim 200 k exafs measurements have been carried out at mn and ni kedges and changes associated with respect to the local structure of these absorbing atoms are compared significant changes in the nearest neighbour interactions are seen as the system transits to the low temperature martensitic phase exafs provides evidence for local structural distortion even in the cubic phase that is not seen from the xray diffraction studies the results obtained are understood in terms of changing hybridization between the constituent atoms that influence the electronic structure at the fermi level associated with the austenitictomartensitic transition | [['extended', 'xray', 'absorption', 'finestructure', 'exafs', 'measurements', 'have', 'been', 'carried', 'out', 'on', 'ni_50mn_35sn_15', 'in', 'the', 'austenitic', 'and', 'martensitic', 'phase', 'the', 'temperatures', 'associated', 'with', 'structural', 'and', 'magnetic', 'phase', 'transformations', 'are', 'obtained', 'from', 'magnetization', 'measurements', 'the', 'system', 'orders', 'ferromagnetically', 'below', '319', 'k', 'while', 'the', 'structural', 'phase', 'transition', 'occurs', 'at', 't_m', 'sim', '200', 'k', 'exafs', 'measurements', 'have', 'been', 'carried', 'out', 'at', 'mn', 'and', 'ni', 'kedges', 'and', 'changes', 'associated', 'with', 'respect', 'to', 'the', 'local', 'structure', 'of', 'these', 'absorbing', 'atoms', 'are', 'compared', 'significant', 'changes', 'in', 'the', 'nearest', 'neighbour', 'interactions', 'are', 'seen', 'as', 'the', 'system', 'transits', 'to', 'the', 'low', 'temperature', 'martensitic', 'phase', 'exafs', 'provides', 'evidence', 'for', 'local', 'structural', 'distortion', 'even', 'in', 'the', 'cubic', 'phase', 'that', 'is', 'not', 'seen', 'from', 'the', 'xray', 'diffraction', 'studies', 'the', 'results', 'obtained', 'are', 'understood', 'in', 'terms', 'of', 'changing', 'hybridization', 'between', 'the', 'constituent', 'atoms', 'that', 'influence', 'the', 'electronic', 'structure', 'at', 'the', 'fermi', 'level', 'associated', 'with', 'the', 'austenitictomartensitic', 'transition']] | [-0.12139149627346597, 0.18869361514553532, -0.010447685271058835, 0.02060452909258024, -0.006281089111441143, -0.10179732082096833, 0.11657681643084006, 0.47011360745798325, -0.2755531647150785, -0.3263026779557703, 0.05079305898332575, -0.3971597468808398, -0.08021734793290076, 0.12198596186960496, 0.11648515371841864, 0.010012404514397954, -0.025742694978195597, 0.004726356296704977, -0.1734364983842144, -0.21146791818892766, 0.25336904540448124, 0.07970529567109237, 0.25077084459784166, 0.049519106207913915, 0.016776351969767834, -0.027833854166371092, 0.04305568596013677, 0.06867199867937557, -0.12265898310630599, 0.0028186350870052757, 0.26199383268946075, -0.03617309863534822, 0.15317990715799093, -0.428730867278408, -0.22552812784011672, 0.034167332587842374, 0.09841606439366726, 0.07640100448739938, -0.04569628901294315, -0.28868784928615665, 0.06080446944368715, -0.07231371817638127, -0.10265704494258257, -0.10560842191318418, -0.040372661278832336, 0.010207505706077914, -0.20929532836627504, 0.11510174708362196, 0.057434868615146885, 0.16759257740013198, -0.12525417845250225, -0.13829020100717865, -0.10667734167499232, 0.08011177848552314, 0.021975958862499347, 0.0839366729096198, 0.16436538050397181, -0.041852995061354946, -0.07842736099649902, 0.4052556640612827, -0.04783217734526056, 0.006651950747587941, 0.19903999806749045, -0.22682614437579898, -0.1474557497774736, 0.25879385562049567, 0.089019756285395, 0.07201576319155874, -0.12193217267639751, 0.06987546276793861, 0.04547004293466748, 0.22911233278516102, 0.08384865043606136, 0.06198467706776106, 0.2324561905181429, 0.1275674334192701, 0.017813170463187804, 0.13825977406862952, -0.15046827550805306, -0.06659926451426196, -0.21694678662371047, -0.10202014755087079, -0.17630662389335708, 0.010588425823301242, -0.10642145109046447, -0.11929368827177185, 0.3390455147658121, 0.11345881449294762, 0.22575832166853296, -0.06518212279213041, 0.20846136663400922, 0.09580241559847245, 0.07834385805697718, 0.015371268995525971, 0.2849417196252239, 0.1771420099654458, 0.14573673321373604, -0.294813506431471, 0.14615504192778658, 0.014589587278978926] |
708.262 | On the (circular) polarization-independence of microwave-induced
resistance oscillations and zero resistance state | The immunity of microwave-induced magneto-resistance oscillations and
corresponding zero resistance regions to the direction of (circular)
polarization of microwave is studied in this paper. We propose that a
spontaneous circular motion of the whole electron fluid would stabilize the
system and minimize the polarization sensitivity of the oscillatory DC
resistance. Results of a self-consistent calculation capture the qualitative
features of the experimental observation.
| cond-mat.mes-hall cond-mat.other | the immunity of microwaveinduced magnetoresistance oscillations and corresponding zero resistance regions to the direction of circular polarization of microwave is studied in this paper we propose that a spontaneous circular motion of the whole electron fluid would stabilize the system and minimize the polarization sensitivity of the oscillatory dc resistance results of a selfconsistent calculation capture the qualitative features of the experimental observation | [['the', 'immunity', 'of', 'microwaveinduced', 'magnetoresistance', 'oscillations', 'and', 'corresponding', 'zero', 'resistance', 'regions', 'to', 'the', 'direction', 'of', 'circular', 'polarization', 'of', 'microwave', 'is', 'studied', 'in', 'this', 'paper', 'we', 'propose', 'that', 'a', 'spontaneous', 'circular', 'motion', 'of', 'the', 'whole', 'electron', 'fluid', 'would', 'stabilize', 'the', 'system', 'and', 'minimize', 'the', 'polarization', 'sensitivity', 'of', 'the', 'oscillatory', 'dc', 'resistance', 'results', 'of', 'a', 'selfconsistent', 'calculation', 'capture', 'the', 'qualitative', 'features', 'of', 'the', 'experimental', 'observation']] | [-0.20562598557906256, 0.14670701735349934, -0.07433809426110534, -0.019434921864774964, -0.06392135922723109, -0.09302196483172122, 0.04384882465219273, 0.3156746855330846, -0.2714318569513067, -0.27845031292074257, 0.015520240488787375, -0.3096723778483768, -0.1477744768831938, 0.18002426967261329, -0.014636686042187706, 0.05470880258473612, 0.022441585171258167, 0.0072938011153527195, -0.051984523478451936, -0.15536580206308928, 0.24320003286647124, 0.08773154480057577, 0.34881570870204576, 0.0593250770240076, 0.10726272060151493, -0.012208749270362277, 0.00926362591544314, 0.08002429845048085, -0.11876614924992845, 0.07489148487469979, 0.21179081676971345, -0.002121164701834676, 0.19895117138586346, -0.44952019377951585, -0.18567708208565675, 0.06257392607614516, 0.12185474604900394, 0.18379099820814435, -0.028379740940022564, -0.25189335276150987, 0.04054505942714593, -0.11174554957283868, -0.1540697759519967, -0.07600968588320982, 0.00974087777458841, 0.0071737973078612296, -0.2593942136755065, 0.13777923704464995, 0.08481909843191268, 0.07330989117719351, -0.10979819046481261, -0.060684645413568924, -0.035155265399860955, 0.08622189985203838, 0.06807895286733077, 0.023868517809739663, 0.18499278014762296, -0.1257156583532277, -0.15154948256288966, 0.30644930252391434, -0.08265704852491913, -0.12121356779798156, 0.11144471863314273, -0.24132693465799093, -0.02723225172875183, 0.16654553234813704, 0.19143849460127216, 0.11262393218006879, -0.1491639519272934, 0.02376793955992316, -0.026900208717773832, 0.14323784848527302, 0.09042326504335044, 0.04348455884656499, 0.2541875314736177, 0.18420312147114484, 0.04297404480536306, 0.14625709241862217, -0.18719856367106474, -0.03555649252135366, -0.30396598346886183, -0.12420056763729671, -0.12386544022916092, 0.06861304921940678, -0.029524052448640946, -0.2076945293192116, 0.49734462188586354, 0.17325744390605935, 0.20029703421252115, 0.0032656165061607247, 0.3499570847119367, 0.11364850537881019, 0.039772680332322445, -0.019464754477320684, 0.3062864419605051, 0.1873144671793968, 0.15617285742764436, -0.37739818585326984, 0.08937802981023514, -0.05954284798206082] |
708.2621 | Luminescence quenching of the triplet excimer state by air traces in
gaseous argon | While developing a liquid argon detector for dark matter searches we
investigate the influence of air contamination on the VUV scintillation yield
in gaseous argon at atmospheric pressure. We determine with a radioactive
alpha-source the photon yield for various partial air pressures and different
reflectors and wavelength shifters. We find for the fast scintillation
component a time constant tau1= 11.3 +- 2.8 ns, independent of gas purity.
However, the decay time of the slow component depends on gas purity and is a
good indicator for the total VUV light yield. This dependence is attributed to
impurities destroying the long-lived argon excimer states. The population ratio
between the slowly and the fast decaying excimer states is determined for
alpha-particles to be 5.5 +-0.6 in argon gas at 1100 mbar and room temperature.
The measured mean life of the slow component is tau2 = 3.140 +- 0.067 microsec
at a partial air pressure of 2 x 10-6 mbar.
| physics.ins-det physics.atm-clus | while developing a liquid argon detector for dark matter searches we investigate the influence of air contamination on the vuv scintillation yield in gaseous argon at atmospheric pressure we determine with a radioactive alphasource the photon yield for various partial air pressures and different reflectors and wavelength shifters we find for the fast scintillation component a time constant tau1 113 28 ns independent of gas purity however the decay time of the slow component depends on gas purity and is a good indicator for the total vuv light yield this dependence is attributed to impurities destroying the longlived argon excimer states the population ratio between the slowly and the fast decaying excimer states is determined for alphaparticles to be 55 06 in argon gas at 1100 mbar and room temperature the measured mean life of the slow component is tau2 3140 0067 microsec at a partial air pressure of 2 x 106 mbar | [['while', 'developing', 'a', 'liquid', 'argon', 'detector', 'for', 'dark', 'matter', 'searches', 'we', 'investigate', 'the', 'influence', 'of', 'air', 'contamination', 'on', 'the', 'vuv', 'scintillation', 'yield', 'in', 'gaseous', 'argon', 'at', 'atmospheric', 'pressure', 'we', 'determine', 'with', 'a', 'radioactive', 'alphasource', 'the', 'photon', 'yield', 'for', 'various', 'partial', 'air', 'pressures', 'and', 'different', 'reflectors', 'and', 'wavelength', 'shifters', 'we', 'find', 'for', 'the', 'fast', 'scintillation', 'component', 'a', 'time', 'constant', 'tau1', '113', '28', 'ns', 'independent', 'of', 'gas', 'purity', 'however', 'the', 'decay', 'time', 'of', 'the', 'slow', 'component', 'depends', 'on', 'gas', 'purity', 'and', 'is', 'a', 'good', 'indicator', 'for', 'the', 'total', 'vuv', 'light', 'yield', 'this', 'dependence', 'is', 'attributed', 'to', 'impurities', 'destroying', 'the', 'longlived', 'argon', 'excimer', 'states', 'the', 'population', 'ratio', 'between', 'the', 'slowly', 'and', 'the', 'fast', 'decaying', 'excimer', 'states', 'is', 'determined', 'for', 'alphaparticles', 'to', 'be', '55', '06', 'in', 'argon', 'gas', 'at', '1100', 'mbar', 'and', 'room', 'temperature', 'the', 'measured', 'mean', 'life', 'of', 'the', 'slow', 'component', 'is', 'tau2', '3140', '0067', 'microsec', 'at', 'a', 'partial', 'air', 'pressure', 'of', '2', 'x', '106', 'mbar']] | [-0.07126570137307425, 0.29182983715896754, -0.07135588843131961, 0.036194034863500764, 0.08088633624435056, -0.11495307916044897, 0.06043291152751658, 0.3879099491727995, -0.20290970163772892, -0.3465597104217273, 0.06194296056173401, -0.329919114428895, 0.07561081404694253, 0.18080425151209864, 0.020587103100481376, 0.04963884899222286, 0.015229976477308406, -0.04272525886901551, -0.06888631578942675, -0.19932087708654161, 0.18509534543100137, 0.1074375053806827, 0.2597047874058773, 0.10620457762654481, 0.1404165205746597, -0.07101885718445665, -0.031967346736053434, -0.09721127970393723, -0.11402853840682046, -0.042266465118611415, 0.24620246314413213, 0.044045748492256585, 0.17892531897063105, -0.4105247244774516, -0.19635027138138908, 0.11026427853590766, 0.0893981957616394, 0.03204271362278781, -0.08169446257551755, -0.2472526819621718, 0.06045919908758472, -0.16154047458438703, -0.15987037483745808, 0.03429987170471767, 0.03779703961743127, -0.0007791103092493988, -0.2720644748800136, 0.10614434744724456, -0.015676079649672985, 0.0676250589092329, -0.07090743839378572, -0.15741810936775985, 0.006071790046168163, 0.022794430652402, 0.03214796392164905, 0.0377229872369664, 0.2917700974161134, -0.10412931186147034, 0.059094138638256424, 0.35832916909305296, -0.15881815944262628, -0.07055759087590702, 0.20109751849782234, -0.18562011173591506, -0.04842940534410231, 0.3006681632524466, 0.16608102780346776, 0.10904028265755258, -0.12637241940117544, -0.0018583565506798039, 0.01777908688006326, 0.26798969112774906, 0.14325923469295007, 0.06310708785362638, 0.2198973409831524, 0.1990411766908235, 0.06694908635203842, 0.092007261985499, -0.20129992370341532, 0.03156993997258931, -0.254450647772162, -0.22395374259631473, -0.0967020589875033, 0.0720870698789999, -0.07871734235712306, -0.1219055023945235, 0.37247769024490923, 0.05068349859257247, 0.15473227634465966, -0.008722374504858178, 0.3010182437255638, 0.08236393442048746, -0.006480012155971886, 0.04612692051987145, 0.30653871805863636, 0.1752881034386947, 0.11462420816350655, -0.29065373514434995, 0.08498059262466781, -0.022039097190524142] |
708.2622 | The LCFIVertex Package: vertex detector-based Reconstruction at the ILC | The contribution gives an overview of the LCFIVertex package, providing
software tools for high-level event reconstruction at the International Linear
Collider using vertex-detector information. The package was validated using a
fast Monte Carlo simulation. Performance obtained with a more realistic
GEANT4-based detector simulation and realistic tracking code is presented. The
influence of hadronic interactions on flavour tagging is discussed.
| physics.ins-det physics.data-an | the contribution gives an overview of the lcfivertex package providing software tools for highlevel event reconstruction at the international linear collider using vertexdetector information the package was validated using a fast monte carlo simulation performance obtained with a more realistic geant4based detector simulation and realistic tracking code is presented the influence of hadronic interactions on flavour tagging is discussed | [['the', 'contribution', 'gives', 'an', 'overview', 'of', 'the', 'lcfivertex', 'package', 'providing', 'software', 'tools', 'for', 'highlevel', 'event', 'reconstruction', 'at', 'the', 'international', 'linear', 'collider', 'using', 'vertexdetector', 'information', 'the', 'package', 'was', 'validated', 'using', 'a', 'fast', 'monte', 'carlo', 'simulation', 'performance', 'obtained', 'with', 'a', 'more', 'realistic', 'geant4based', 'detector', 'simulation', 'and', 'realistic', 'tracking', 'code', 'is', 'presented', 'the', 'influence', 'of', 'hadronic', 'interactions', 'on', 'flavour', 'tagging', 'is', 'discussed']] | [-0.06482535414999865, 0.010416426898857401, -0.11494234282170133, 0.12191198281702939, -0.06969999579776978, -0.16425423030259795, -0.0908567364295495, 0.39183042635177745, -0.19760200765048122, -0.36678586816736336, 0.07848283282384791, -0.31930245703150484, -0.02585079474374652, 0.27021111103561546, 0.06769972500905137, 0.12836496120896831, 0.22592915151396703, -0.0283479989377846, -0.09005620564205637, -0.1996472186633739, 0.18489552254724348, 0.28703887824868335, 0.26228709046825255, 0.05733055155724287, 0.12770641106180847, 0.07305478881883981, -0.1734001580304627, -0.02473103697411716, -0.14677010584173017, 0.08775833978092876, 0.2970931400175624, 0.20621427562457093, 0.18243808952834586, -0.41285796347877074, -0.16430043385781604, -0.026729959705523377, 0.09587029152517688, 0.09978491934728889, -0.17422772279929505, -0.34134741705553284, 0.05335297352024194, -0.2831326990131417, -0.08881711604972851, -0.07841983201496046, -0.0782942540686706, -0.014188061223429596, -0.3129285756370117, -0.02706048742402345, -0.07866327172337935, 0.14126794562064882, 0.054331025767043746, -0.1628183729320379, 0.002802537681920261, 0.10401274695799782, -0.024985023880586158, 0.05660536718065048, 0.17943665899882286, -0.09119395422749221, -0.17519659468711452, 0.35871384023078556, -0.00710993431556713, -0.1948655092574913, 0.21051199018056022, -0.07023531368708816, -0.15144029350806798, 0.18259490577600382, 0.24863876534047827, 0.07151353558332756, -0.256860565667137, 0.12073824117823247, 0.040330725243307074, 0.18562981972856255, -0.07160121925849595, -0.04516377729556427, 0.16238368058914382, 0.3438206781344167, -0.03837470124186627, 0.15815951036698794, -0.10559633517525448, -0.11073724768156636, -0.3517587315612312, -0.10785592850779407, -0.13665404845960438, -0.0332795628386646, -0.04147448021379613, -0.14016193413207756, 0.43008333695088996, 0.17819100094493479, 0.06405525457852616, 0.02403161064561071, 0.39033400819733227, 0.017371329863290784, 0.027043344571901454, 0.09309791371799356, 0.2079641088072596, 0.0859842228879831, 0.12242698230266828, -0.2398070070475083, 0.08874248927619693, 0.08375764448308097] |
708.2623 | Reversed propagation dynamics of Laguerre-Gaussian beams in left-handed
materials | On the basis of angular spectrum representation, the reversed propagation
dynamics of Laguerre-Gaussian beam in left-handed materials (LHMs) is
presented. We show that negative phase velocity gives rise to a reversed screw
of wave-front, and ultimately leads to a reversed rotation of optical vortex.
Furthermore, negative Gouy-phase shift causes an inverse spiral of Poynting
vector. It is found that the Laguerre-Gaussian beam in LHMs will present the
same propagation characteristics as the counterpart with opposite topological
charges in regular right-handed materials (RHMs). The momentum conservation
theorem insures that the tangential component of the wave momentum at the
RHM-LHM boundary is conserved. It is shown that although the linear momentum
reverses its direction, the angular momentum remains unchanged.
| physics.optics | on the basis of angular spectrum representation the reversed propagation dynamics of laguerregaussian beam in lefthanded materials lhms is presented we show that negative phase velocity gives rise to a reversed screw of wavefront and ultimately leads to a reversed rotation of optical vortex furthermore negative gouyphase shift causes an inverse spiral of poynting vector it is found that the laguerregaussian beam in lhms will present the same propagation characteristics as the counterpart with opposite topological charges in regular righthanded materials rhms the momentum conservation theorem insures that the tangential component of the wave momentum at the rhmlhm boundary is conserved it is shown that although the linear momentum reverses its direction the angular momentum remains unchanged | [['on', 'the', 'basis', 'of', 'angular', 'spectrum', 'representation', 'the', 'reversed', 'propagation', 'dynamics', 'of', 'laguerregaussian', 'beam', 'in', 'lefthanded', 'materials', 'lhms', 'is', 'presented', 'we', 'show', 'that', 'negative', 'phase', 'velocity', 'gives', 'rise', 'to', 'a', 'reversed', 'screw', 'of', 'wavefront', 'and', 'ultimately', 'leads', 'to', 'a', 'reversed', 'rotation', 'of', 'optical', 'vortex', 'furthermore', 'negative', 'gouyphase', 'shift', 'causes', 'an', 'inverse', 'spiral', 'of', 'poynting', 'vector', 'it', 'is', 'found', 'that', 'the', 'laguerregaussian', 'beam', 'in', 'lhms', 'will', 'present', 'the', 'same', 'propagation', 'characteristics', 'as', 'the', 'counterpart', 'with', 'opposite', 'topological', 'charges', 'in', 'regular', 'righthanded', 'materials', 'rhms', 'the', 'momentum', 'conservation', 'theorem', 'insures', 'that', 'the', 'tangential', 'component', 'of', 'the', 'wave', 'momentum', 'at', 'the', 'rhmlhm', 'boundary', 'is', 'conserved', 'it', 'is', 'shown', 'that', 'although', 'the', 'linear', 'momentum', 'reverses', 'its', 'direction', 'the', 'angular', 'momentum', 'remains', 'unchanged']] | [-0.21064546621586802, 0.2524984775466652, -0.09520078935134021, 0.04368747671681416, -0.14155321884900332, -0.09473193160627726, -0.04794547489107809, 0.41899674823102745, -0.30438221722193387, -0.20452061044457165, 0.005192221106920877, -0.24890268924443618, -0.0927430662933899, 0.1798967252040039, -0.013436048291623592, 0.014929747921110981, 0.026659213018644115, 0.008810944960493108, -0.09269193552596414, -0.14241921193087878, 0.2849429570735716, 0.05795336519570454, 0.33864681460975626, 0.02850751386874396, 0.15494117365907067, 0.028668260624956178, -0.003821719786071259, -0.014557801207284565, -0.08009284087228993, 0.049425426704566115, 0.15758606313687304, -0.0001418455665850121, 0.18790811982167804, -0.39893817017259803, -0.17089221970704588, 0.04847594001532897, 0.18539753306414122, 0.1299354557838777, -0.08069142367407356, -0.22658518911946726, 0.037593881304011395, -0.12178115649452514, -0.23389425175264478, -0.052566179463072966, 0.056697682244703174, 0.01240849560936508, -0.221932198787513, 0.13139589543899763, 0.1298431470828212, 0.02323790189364682, -0.08355369243224192, -0.1067968596400612, -0.15019155431376852, 0.02213353341769265, 0.11263868830308481, 0.07763375982075282, 0.12662254154034283, -0.13907595451759255, -0.10083846885548986, 0.3890251460566145, -0.0371779482761074, -0.22647829927180124, 0.08914383489476597, -0.2149586407563892, -0.009044437343254686, 0.1731410871523068, 0.15102223581027077, 0.06760094344777906, -0.058579708133702696, 0.024685875682220998, -0.06389611611109855, 0.14650353154410486, 0.12674082140235798, 0.04064753711142618, 0.2644726945492237, 0.0758186442149884, 0.13367351183222365, 0.1266612470149994, -0.12325733633226027, -0.06868864786203789, -0.31103914822249307, -0.1833056251356459, -0.18021744765017345, 0.054678117690744564, -0.039010134165089215, -0.1447159328708, 0.43276043152841537, 0.10893699404095178, 0.17202079191819117, -0.028024472334705616, 0.3131554802474768, 0.16167986130078688, 0.09326642593444812, 0.0740048974590457, 0.3047313546275963, 0.2124375730186053, 0.190263362115492, -0.28962748429697494, 0.03244510975504375, 0.036776417254915705] |
708.2624 | Josephson junctions with negative second harmonic in the current-phase
relation: properties of novel varphi-junctions | Several recent experiments revealed a change of the sign of the first
harmonic in the current-phase relation of Josephson junctions (JJ) based on
novel superconductors, e.g., d-wave based or JJ with ferromagnetic barrier. In
this situation the role of the second harmonic becomes dominant and it
determines the scenario of a 0-pi transition. We discuss different mechanisms
of the second harmonic generation and its sign. If the second harmonic is
negative the 0-pi transition becomes continuous and the realization of the
so-called varphi junction is possible. We study the unusual properties of such
a novel JJ and analyze the possible experimental techniques for their
observation.
| cond-mat.supr-con | several recent experiments revealed a change of the sign of the first harmonic in the currentphase relation of josephson junctions jj based on novel superconductors eg dwave based or jj with ferromagnetic barrier in this situation the role of the second harmonic becomes dominant and it determines the scenario of a 0pi transition we discuss different mechanisms of the second harmonic generation and its sign if the second harmonic is negative the 0pi transition becomes continuous and the realization of the socalled varphi junction is possible we study the unusual properties of such a novel jj and analyze the possible experimental techniques for their observation | [['several', 'recent', 'experiments', 'revealed', 'a', 'change', 'of', 'the', 'sign', 'of', 'the', 'first', 'harmonic', 'in', 'the', 'currentphase', 'relation', 'of', 'josephson', 'junctions', 'jj', 'based', 'on', 'novel', 'superconductors', 'eg', 'dwave', 'based', 'or', 'jj', 'with', 'ferromagnetic', 'barrier', 'in', 'this', 'situation', 'the', 'role', 'of', 'the', 'second', 'harmonic', 'becomes', 'dominant', 'and', 'it', 'determines', 'the', 'scenario', 'of', 'a', '0pi', 'transition', 'we', 'discuss', 'different', 'mechanisms', 'of', 'the', 'second', 'harmonic', 'generation', 'and', 'its', 'sign', 'if', 'the', 'second', 'harmonic', 'is', 'negative', 'the', '0pi', 'transition', 'becomes', 'continuous', 'and', 'the', 'realization', 'of', 'the', 'socalled', 'varphi', 'junction', 'is', 'possible', 'we', 'study', 'the', 'unusual', 'properties', 'of', 'such', 'a', 'novel', 'jj', 'and', 'analyze', 'the', 'possible', 'experimental', 'techniques', 'for', 'their', 'observation']] | [-0.23605216688786942, 0.15006501749157905, -0.02209132525271603, 0.04050627411675772, -0.10305222334074123, -0.15185396289896397, 0.08353873498383023, 0.35029267274907655, -0.25993982741520516, -0.22907026206098852, 0.03868798719763401, -0.2838248766160437, -0.1714796069632506, 0.20602857225485854, 0.0366352856469651, 0.04870855182442548, -0.02085177188827878, 0.03551220361675535, -0.09673621473678698, -0.15078209603116627, 0.36269096336438367, -0.01801752739896377, 0.306591601326086, 0.09975508930427687, 0.0542264288734822, -0.025474913914998374, 0.03603335463308862, -0.04693639996860709, -0.16049646061673273, 0.08133027339354157, 0.17323366370983423, -0.012252178829207662, 0.2203590107106027, -0.4355457591513793, -0.1459016607276031, 0.12511992564957056, 0.09925638083188373, 0.11474563767690034, -0.047013195259274825, -0.2783782281513725, 0.04712959743504013, -0.14889342703723482, -0.09025099355106553, -0.043678904484425275, 0.027636584972164462, 0.03090548811347357, -0.26342571673116516, 0.08279179610711124, 0.13525510042395797, 0.04813477320685273, -0.0036773993822169448, -0.08813774489875262, -0.03158430988856015, 0.09298012389446653, 0.04875814521995683, 0.033078620048417225, 0.09599661039842647, -0.14759107990733658, -0.1506848025069173, 0.35794009003078653, -0.07886127522880478, -0.11876823255969655, 0.1510532105740692, -0.16235820991652353, -0.11674367626685472, 0.047028892536071086, 0.1006610352634674, 0.11057882051294049, -0.10802934116550854, 0.08883582846527653, 0.01450312499489103, 0.1382511173951484, 0.058746444183357414, 0.03614160566635075, 0.23450395192596174, 0.24020747255888722, 0.06584627583977722, 0.1843254579231143, -0.1433153893687718, -0.07634314335106561, -0.32766462704610255, -0.18571898722854843, -0.20851811315154745, 0.030608385393307323, -0.025531983366125218, -0.20385163473408846, 0.4327083150900546, 0.1459635545765715, 0.247752041050366, -0.054820317225087255, 0.29124433895839114, 0.18325743014436394, 0.024890829314522092, -0.0370409234382567, 0.24777598561652536, 0.14391048729774497, 0.13062983978805798, -0.29261255522142166, 0.06970838005876258, 0.005294028829251017] |
708.2625 | Search for a signal on intermediate baryon systems formation in
hadron-nuclear and nuclear-nuclear interactions at high energies | We have analyzed the behavior of different characteristics of hadron-nuclear
and nuclear-nuclear interactions as a function of centrality to get a signal on
the formation of intermediate baryon systems. We observed that the data
demonstrate the regime change and saturation. The angular distributions of slow
particles exhibit some structure in the above mentioned reactions at low
energy. We believe that the structure could be connected with the formation and
decay of the percolation cluster. With increasing the mass of colliding nuclei,
the structure starts to become weak and almost disappears ultimately. This
shows that the number of secondary internuclear interactions increases with
increasing the mass of the colliding nuclei. The latter could be a reason of
the disintegration of any intermediate formations as well as clusters, which
decrease their influence on the angular distribution of the emitted particles.
| nucl-ex | we have analyzed the behavior of different characteristics of hadronnuclear and nuclearnuclear interactions as a function of centrality to get a signal on the formation of intermediate baryon systems we observed that the data demonstrate the regime change and saturation the angular distributions of slow particles exhibit some structure in the above mentioned reactions at low energy we believe that the structure could be connected with the formation and decay of the percolation cluster with increasing the mass of colliding nuclei the structure starts to become weak and almost disappears ultimately this shows that the number of secondary internuclear interactions increases with increasing the mass of the colliding nuclei the latter could be a reason of the disintegration of any intermediate formations as well as clusters which decrease their influence on the angular distribution of the emitted particles | [['we', 'have', 'analyzed', 'the', 'behavior', 'of', 'different', 'characteristics', 'of', 'hadronnuclear', 'and', 'nuclearnuclear', 'interactions', 'as', 'a', 'function', 'of', 'centrality', 'to', 'get', 'a', 'signal', 'on', 'the', 'formation', 'of', 'intermediate', 'baryon', 'systems', 'we', 'observed', 'that', 'the', 'data', 'demonstrate', 'the', 'regime', 'change', 'and', 'saturation', 'the', 'angular', 'distributions', 'of', 'slow', 'particles', 'exhibit', 'some', 'structure', 'in', 'the', 'above', 'mentioned', 'reactions', 'at', 'low', 'energy', 'we', 'believe', 'that', 'the', 'structure', 'could', 'be', 'connected', 'with', 'the', 'formation', 'and', 'decay', 'of', 'the', 'percolation', 'cluster', 'with', 'increasing', 'the', 'mass', 'of', 'colliding', 'nuclei', 'the', 'structure', 'starts', 'to', 'become', 'weak', 'and', 'almost', 'disappears', 'ultimately', 'this', 'shows', 'that', 'the', 'number', 'of', 'secondary', 'internuclear', 'interactions', 'increases', 'with', 'increasing', 'the', 'mass', 'of', 'the', 'colliding', 'nuclei', 'the', 'latter', 'could', 'be', 'a', 'reason', 'of', 'the', 'disintegration', 'of', 'any', 'intermediate', 'formations', 'as', 'well', 'as', 'clusters', 'which', 'decrease', 'their', 'influence', 'on', 'the', 'angular', 'distribution', 'of', 'the', 'emitted', 'particles']] | [-0.13691797219149338, 0.2174742042451449, -0.10901870908286504, 0.1013388629896023, -0.0014391528186050878, -0.05522663698913833, 0.027466192186904558, 0.343428872525692, -0.2690076605632793, -0.33520575208535447, 0.029052724374248984, -0.3081939658150077, -0.055523135922039335, 0.13368585819472978, 0.05523296732765933, -0.02376466200929945, 0.05119698328316968, 0.06367441693968746, -0.054591900289423116, -0.20054516538579448, 0.34088034473656526, 0.10716411976845584, 0.25085739345303265, 0.11019547385555031, 0.07463881527360501, 0.012814300170208773, 0.02425479565821318, 0.025553330418019406, -0.10525508408102104, 0.061231293936978785, 0.18745531187311787, 0.09247065977314892, 0.21960040411500234, -0.3811564720404483, -0.21128213176152844, 0.11204583838959967, 0.20183646986665932, 0.11844414773825691, -0.0837518153121641, -0.24915537575556748, 0.07334575109669696, -0.1797507311001528, -0.1794623464912824, -0.005775921370672143, 0.03648631627657923, 0.12628556316063833, -0.22551128180128982, 0.10256866753384795, 0.05985385546059199, 0.020509532333918563, -0.08901530630090207, -0.11492025242119595, -0.08938269066266662, 0.13988820446884612, 0.08891822662933366, 0.009130437113091593, 0.18818684320464946, -0.14529630321287212, -0.057198752153097936, 0.3668349412357624, -0.020244551896779, -0.10628447498775263, 0.22069122644303285, -0.20554234738718125, -0.1352328476101663, 0.1635817873563307, 0.1997914043646576, 0.09676178832929852, -0.08689888589129702, 0.0038876806495903547, 0.003829126509473376, 0.16513032277209172, 0.0708500317979496, 0.07286114642814989, 0.21760758636789262, 0.1979446934816171, 0.034962338910006205, 0.12167503225002978, -0.11154975157663011, -0.08592817026521146, -0.2686471718268982, -0.11291280444593345, -0.15879720791776164, 0.045378925405321235, -0.09733432352473703, -0.15021178006545466, 0.3617946446630294, 0.09597325589730525, 0.2950762087627705, 0.030089466779432056, 0.2457598297573302, 0.1085556302113337, 0.09203293130132437, 0.04912226876594882, 0.2965613475613097, 0.14506151867470285, 0.11538733592243407, -0.2636791635169715, 0.09275203948651535, -0.027392530002280313] |
708.2626 | A cohomological construction of modules over Fedosov deformation
quantization algebra | In certain neighborhood $U$ of an arbitrary point of a symplectic manifold
$M$ we construct a Fedosov-type star-product $\ast_L$ such that for an
arbitrary leaf $\wp$ of a given polarization $\mathcal{D}\subset TM$ the
algebra $C^\infty (\wp \cap U)[[h]]$ has a natural structure of left module
over the deformed algebra $(C^\infty (U)[[h]], \ast_L)$. With certain
additional assumptions on $M$, $\ast_L$ becomes a so-called star-product with
separation of variables.
| math.QA math-ph math.MP | in certain neighborhood u of an arbitrary point of a symplectic manifold m we construct a fedosovtype starproduct ast_l such that for an arbitrary leaf wp of a given polarization mathcaldsubset tm the algebra cinfty wp cap uh has a natural structure of left module over the deformed algebra cinfty uh ast_l with certain additional assumptions on m ast_l becomes a socalled starproduct with separation of variables | [['in', 'certain', 'neighborhood', 'u', 'of', 'an', 'arbitrary', 'point', 'of', 'a', 'symplectic', 'manifold', 'm', 'we', 'construct', 'a', 'fedosovtype', 'starproduct', 'ast_l', 'such', 'that', 'for', 'an', 'arbitrary', 'leaf', 'wp', 'of', 'a', 'given', 'polarization', 'mathcaldsubset', 'tm', 'the', 'algebra', 'cinfty', 'wp', 'cap', 'uh', 'has', 'a', 'natural', 'structure', 'of', 'left', 'module', 'over', 'the', 'deformed', 'algebra', 'cinfty', 'uh', 'ast_l', 'with', 'certain', 'additional', 'assumptions', 'on', 'm', 'ast_l', 'becomes', 'a', 'socalled', 'starproduct', 'with', 'separation', 'of', 'variables']] | [-0.25163028360024764, 0.0610642728031745, -0.0640896373331102, 0.046928582629605906, -0.11909775463725204, -0.1281533413566649, -0.0514587923439581, 0.3447790116961323, -0.3335659183673005, -0.1625929122491837, 0.08897435467572076, -0.2233860277529083, -0.11736663135894533, 0.14899949332587978, -0.10453236014790722, -0.03309250664688758, 0.05490678137362893, 0.15375619580441002, -0.1514765650777619, -0.18236721887725837, 0.42621943665974177, 0.011337694538228991, 0.16860835380685418, -0.04359521060737211, 0.2167230193301646, 0.03811795265177515, 0.053360111114860914, -0.012576002502508128, -0.13924874646518356, 0.07713424151679918, 0.23546791882879697, 0.11367189130092513, 0.20809403568186532, -0.33922240510582924, -0.13592122862143302, 0.16364203820199663, 0.1187663647943913, -0.05409021550483668, -0.01002467549649248, -0.308459873491926, 0.10799668078074481, -0.16102738339982148, -0.156121200576091, -0.05132512337052083, 0.11375403262452403, -0.013172734542680321, -0.29511104864433213, -0.05267228666387165, 0.12381768146175336, 0.12017071798944207, -0.0937461318281382, -0.12123758154017712, -0.14744513465870004, 0.04138013216625176, -0.07356663439561849, 0.17796324793972187, 0.10858240635342785, -0.048830904855406775, -0.030713437208488806, 0.31645624867793337, -0.06605318672746531, -0.3093576548315251, 0.07766651389981384, -0.16697607138680656, -0.17103354648144833, 0.10321824235230018, 0.06994231921662368, 0.12728562481256564, -0.05562883716358094, 0.2780191192208831, -0.12526547725993528, 0.10323336928493844, 0.12910876727277246, 0.0014468425287128385, 0.11399250853556528, 0.12102738413751236, 0.14821217729668343, 0.08411777255111444, -0.013722052822000723, -0.001189323614782362, -0.38612753530936456, -0.18143441128447207, -0.10148167357182325, 0.18590898372219014, -0.14586544565078038, -0.21428835517101325, 0.3342683581468552, 0.003648552904600528, 0.23615710515487218, 0.06538534887246232, 0.1576322835327974, 0.08513805542641611, 0.08107059264082962, 0.07756593338311163, 0.06253977172743919, 0.19422993250191212, 0.014426944469824544, -0.14709230788997305, -0.07716317773004298, 0.15514740420143996] |
708.2627 | The holomorphic anomaly for open string moduli | We complete the holomorphic anomaly equations for topological strings with
their dependence on open moduli. We obtain the complete system by standard path
integral arguments generalizing the analysis of BCOV (Commun. Math. Phys. 165
(1994) 311) to strings with boundaries. We study both the anti-holomorphic
dependence on open moduli and on closed moduli in presence of Wilson lines. By
providing the compactification a' la Deligne-Mumford of the moduli space of
Riemann surfaces with boundaries, we show that the open holomorphic anomaly
equations are structured on the (real codimension one) boundary components of
this space.
| hep-th math.AG | we complete the holomorphic anomaly equations for topological strings with their dependence on open moduli we obtain the complete system by standard path integral arguments generalizing the analysis of bcov commun math phys 165 1994 311 to strings with boundaries we study both the antiholomorphic dependence on open moduli and on closed moduli in presence of wilson lines by providing the compactification a la delignemumford of the moduli space of riemann surfaces with boundaries we show that the open holomorphic anomaly equations are structured on the real codimension one boundary components of this space | [['we', 'complete', 'the', 'holomorphic', 'anomaly', 'equations', 'for', 'topological', 'strings', 'with', 'their', 'dependence', 'on', 'open', 'moduli', 'we', 'obtain', 'the', 'complete', 'system', 'by', 'standard', 'path', 'integral', 'arguments', 'generalizing', 'the', 'analysis', 'of', 'bcov', 'commun', 'math', 'phys', '165', '1994', '311', 'to', 'strings', 'with', 'boundaries', 'we', 'study', 'both', 'the', 'antiholomorphic', 'dependence', 'on', 'open', 'moduli', 'and', 'on', 'closed', 'moduli', 'in', 'presence', 'of', 'wilson', 'lines', 'by', 'providing', 'the', 'compactification', 'a', 'la', 'delignemumford', 'of', 'the', 'moduli', 'space', 'of', 'riemann', 'surfaces', 'with', 'boundaries', 'we', 'show', 'that', 'the', 'open', 'holomorphic', 'anomaly', 'equations', 'are', 'structured', 'on', 'the', 'real', 'codimension', 'one', 'boundary', 'components', 'of', 'this', 'space']] | [-0.2127808622144004, 0.08986616284745012, -0.07709295796899204, 0.03949551678019913, -0.12878584031491203, -0.06681160135888198, 0.04237427876548881, 0.3198110788882254, -0.2300048562836774, -0.25866510262068837, 0.12335004666919246, -0.26784428363626306, -0.1596794390823058, 0.19859156969617656, -0.12091320234925505, 0.03434435981623036, 0.04344676386446078, -0.0197336015544158, -0.09739936570924251, -0.3301017249022868, 0.4304244310119526, -0.039149167521440605, 0.2595537044900529, 0.10079774873806759, 0.09575806002806317, 0.04409362749503727, -0.04630604147059011, -0.027417288395264087, -0.18982268377751213, 0.18134939452098248, 0.2442939499729967, 0.013199015302543944, 0.08810851134439097, -0.4143163989040446, -0.2238169165744268, 0.10729147726669908, 0.08540094078907327, 0.022765926828489026, 0.06725562249429207, -0.3176387692900731, 0.0691096542131879, -0.03775587839884386, -0.18619749488735057, -0.09763535058641053, 0.07417516644172212, -0.028583927310388932, -0.1513288438003114, 0.04574009362964871, 0.04339644976673608, 0.14466345818475523, -0.12208569330408515, -0.10691042262639731, -0.08260338408674331, 0.04019462857692641, 0.027023243207603374, 0.09269432186277861, 0.07207417354344371, -0.09408876706816335, -0.12222626005755143, 0.31669302629505064, -0.12341134838432946, -0.24105051973279804, 0.17831895374098516, -0.12862156622825152, -0.1391403830283262, 0.12220573888995939, 0.11837047821980842, 0.17071994430722393, -0.07190401234881992, 0.23854144964741167, -0.08006942678277598, 0.09196761526548838, 0.1408441358374709, -0.027908393831433172, 0.19940051455968716, 0.11714083195089343, 0.032522451020377825, 0.12775500530954154, -0.038689997153693534, -0.11566086521649614, -0.41660049638928887, -0.22048540089398305, -0.06313119736064146, 0.1517050474909372, -0.12205129294105721, -0.23341549193843247, 0.3693404252680534, 0.07823567068524116, 0.23396040829136333, 0.06469979744523446, 0.18984944593319866, 0.0477350531344084, 0.023769756657705504, 0.11959810296390602, 0.16668214382692934, 0.17259899568942158, 0.05014852130230754, -0.1965197281282831, -0.09780938036373242, 0.2111669447808031] |
708.2628 | Twisted conjugacy classes in Symplectic groups, Mapping class groups and
Braid groups(including an Appendix written with Francois Dahmani) | We prove that the symplectic group $Sp(2n,\mathbb Z)$ and the mapping class
group $Mod_{S}$ of a compact surface $S$ satisfy the $R_{\infty}$ property. We
also show that $B_n(S)$, the full braid group on $n$-strings of a surface $S$,
satisfies the $R_{\infty}$ property in the cases where $S$ is either the
compact disk $D$, or the sphere $S^2$. This means that for any automorphism
$\phi$ of $G$, where $G$ is one of the above groups, the number of twisted
$\phi$-conjugacy classes is infinite.
| math.GR math.GT | we prove that the symplectic group sp2nmathbb z and the mapping class group mod_s of a compact surface s satisfy the r_infty property we also show that b_ns the full braid group on nstrings of a surface s satisfies the r_infty property in the cases where s is either the compact disk d or the sphere s2 this means that for any automorphism phi of g where g is one of the above groups the number of twisted phiconjugacy classes is infinite | [['we', 'prove', 'that', 'the', 'symplectic', 'group', 'sp2nmathbb', 'z', 'and', 'the', 'mapping', 'class', 'group', 'mod_s', 'of', 'a', 'compact', 'surface', 's', 'satisfy', 'the', 'r_infty', 'property', 'we', 'also', 'show', 'that', 'b_ns', 'the', 'full', 'braid', 'group', 'on', 'nstrings', 'of', 'a', 'surface', 's', 'satisfies', 'the', 'r_infty', 'property', 'in', 'the', 'cases', 'where', 's', 'is', 'either', 'the', 'compact', 'disk', 'd', 'or', 'the', 'sphere', 's2', 'this', 'means', 'that', 'for', 'any', 'automorphism', 'phi', 'of', 'g', 'where', 'g', 'is', 'one', 'of', 'the', 'above', 'groups', 'the', 'number', 'of', 'twisted', 'phiconjugacy', 'classes', 'is', 'infinite']] | [-0.21593575703769197, 0.13633805016676584, -0.08904856066276998, 0.030928740752171033, -0.09434080476884121, -0.13720513741129342, 0.023004545462260276, 0.358697825913421, -0.29385892146002546, -0.21268448332485593, 0.1024466709357422, -0.26505453955888014, -0.10057151934166474, 0.19422510749499464, -0.05923562456658225, -0.044832111370784265, 0.03498229522396017, 0.15513971401953403, -0.12077008042036107, -0.249704091930417, 0.3833363760193741, -0.09544806708409279, 0.18405907168800448, 0.03005938261264452, 0.09750214150106465, 0.00264693212258503, 0.036487157077149106, 0.013209628296402869, -0.15799239087973097, 0.06235778167337915, 0.18816291966854973, 0.056841382138822, 0.1864024027262205, -0.3348992407597877, -0.19216783238965787, 0.20522899749792284, 0.0763699396478909, -0.05444311604685621, -0.03137437678890786, -0.2599146835919883, 0.17545994764400852, -0.1670362267781187, -0.16235909162572137, 0.0251093657894267, 0.13289818593105415, -0.006302881709955356, -0.24052622644115745, -0.010170921778527698, 0.13868132739523312, 0.0652270366633196, 0.007416249350587159, -0.09056919269309735, -0.10029849293354301, 0.1157184102497765, -0.0050799645063823754, 0.09152455481896062, 0.1066347982297525, -0.08761287313587043, -0.03460859200905687, 0.3967321195444207, -0.08390888344944904, -0.20744035524074678, 0.140195190343132, -0.22869093225762985, -0.22990495279247378, 0.13719430201353483, 0.07407179085629774, 0.1574674678210422, 0.007269484795813943, 0.2369880574966643, -0.18325574976610548, 0.14092202996260222, 0.06556517239889981, -0.013904231123304293, 0.10788891413306564, 0.07304641357508063, 0.1407389003247379, 0.1076535336719251, -0.035405615261284475, 0.08330074651741687, -0.3793865702356453, -0.2418609048228389, -0.1518227433682316, 0.1252789630635101, -0.09527437524984297, -0.14495396531577923, 0.35055496481557685, 0.010256397802336717, 0.1487343530688021, 0.09010737965941246, 0.16387347038835287, 0.04898947221514435, 0.07244461316638338, 0.13340559486805656, 0.10980636244754732, 0.18714817049970597, -0.11299556597814332, -0.2179900635562745, -0.034428597847574655, 0.18104819503877265] |
708.2629 | Dynamics of the spontaneous breakdown of superhydrophobicity | Drops deposited on rough and hydrophobic surfaces can stay suspended with gas
pockets underneath the liquid, then showing very low hydrodynamic resistance.
When this superhydrophobic state breaks down, the subsequent wetting process
can show different dynamical properties. A suitable choice of the geometry can
make the wetting front propagate in a stepwise manner leading to {\it
square-shaped} wetted area: the front propagation is slow and the patterned
surface fills by rows through a {\it zipping} mechanism. The multiple time
scale scenario of this wetting process is experimentally characterized and
compared to numerical simulations.
| physics.flu-dyn cond-mat.dis-nn nlin.PS | drops deposited on rough and hydrophobic surfaces can stay suspended with gas pockets underneath the liquid then showing very low hydrodynamic resistance when this superhydrophobic state breaks down the subsequent wetting process can show different dynamical properties a suitable choice of the geometry can make the wetting front propagate in a stepwise manner leading to it squareshaped wetted area the front propagation is slow and the patterned surface fills by rows through a it zipping mechanism the multiple time scale scenario of this wetting process is experimentally characterized and compared to numerical simulations | [['drops', 'deposited', 'on', 'rough', 'and', 'hydrophobic', 'surfaces', 'can', 'stay', 'suspended', 'with', 'gas', 'pockets', 'underneath', 'the', 'liquid', 'then', 'showing', 'very', 'low', 'hydrodynamic', 'resistance', 'when', 'this', 'superhydrophobic', 'state', 'breaks', 'down', 'the', 'subsequent', 'wetting', 'process', 'can', 'show', 'different', 'dynamical', 'properties', 'a', 'suitable', 'choice', 'of', 'the', 'geometry', 'can', 'make', 'the', 'wetting', 'front', 'propagate', 'in', 'a', 'stepwise', 'manner', 'leading', 'to', 'it', 'squareshaped', 'wetted', 'area', 'the', 'front', 'propagation', 'is', 'slow', 'and', 'the', 'patterned', 'surface', 'fills', 'by', 'rows', 'through', 'a', 'it', 'zipping', 'mechanism', 'the', 'multiple', 'time', 'scale', 'scenario', 'of', 'this', 'wetting', 'process', 'is', 'experimentally', 'characterized', 'and', 'compared', 'to', 'numerical', 'simulations']] | [-0.1363866476308284, 0.2464638860916258, -0.10913928765403007, -0.003657324313270917, -0.03886739150070215, -0.17892659930587415, 0.07846184743578316, 0.4231587844770602, -0.3268883521918968, -0.2822583189574621, 0.07578542446892869, -0.2673039642433005, -0.13049340787874433, 0.16010528223173473, -0.0427969526599652, 0.0616724435089817, 0.04914975110241162, -0.08221790901515433, -0.06413296317701699, -0.22169674988034913, 0.25852679667033013, 0.06784205137681897, 0.3128762352530674, 0.11365140443767911, 0.09342052535684679, -0.049358172474869635, 0.06437582894502539, 0.0444481518139602, -0.1682260755564697, -0.013232147836837398, 0.21132837776445174, -0.06638512440446404, 0.23407158556003724, -0.5344469909786537, -0.24292909991877373, -0.02577362389814469, 0.15916130769877665, 0.12893338158967033, -0.05237916119581949, -0.2568659887258564, 0.029475458737422702, -0.10513843995549026, -0.16101371867942713, -0.013914132931379861, -0.038533808553331, -0.009608940101511556, -0.18257423397153616, 0.0880250535731364, 0.04812417976071267, -0.009955404569790448, -0.010554104928247711, -0.012769116148833306, -0.10386173304931451, 0.09229843175290303, 0.07103719331652067, 0.019108871811680417, 0.28920917657594525, -0.12006154623363287, 0.00056830993653225, 0.34574179932154636, -0.027882221355153027, -0.18457683128485036, 0.2585656979792221, -0.1592221743416577, 0.01867480715236036, 0.24608330898768, 0.16371169441970446, 0.12080092692524896, -0.12113518767157114, 0.0021261972414645097, -0.03155391801446576, 0.1976345172877954, 0.14731371552953798, -0.09902293583558451, 0.26843957292536896, 0.2644052887710953, 0.02775294792347698, 0.16557587956589076, -0.1214838054316539, -0.10842200771464856, -0.26359672196802775, -0.1772327668456641, -0.1227046605500002, 0.03254974587389859, -0.10099974317148813, -0.22499377571887547, 0.33169342110544364, 0.07851966792437177, 0.22564599240419045, 0.03164770942737138, 0.2743066928441128, 0.029300362392458864, 0.03501691924588334, 0.07821100486457468, 0.23249006155197338, 0.1092368462561099, 0.09778170199233598, -0.20268266408839414, 0.15336609736425422, 0.03604159212761348] |
708.263 | Suppression of High-p_T Neutral Pion Production in Central Pb+Pb
Collisions at sqrt{s_NN} = 17.3 GeV Relative to p+C and p+Pb Collisions | Neutral pion transverse momentum spectra were measured in p+C and p+Pb
collisions at sqrt{s_NN} = 17.4 GeV at mid-rapidity 2.3 < eta_lab < 3.0 over
the range 0.7< p_T < 3.5 GeV/c. The spectra are compared to pi0 spectra
measured in Pb+Pb collisions at sqrt{s_NN} = 17.3 GeV in the same experiment.
For a wide range of Pb+Pb centralities (N_part < 300) the yield of pi0's with
p_T > 2 GeV/c is larger than or consistent with the p+C or p+Pb yields scaled
with the number of nucleon-nucleon collisions (N_coll), while for central Pb+Pb
collisions with N_part > 350 the pi0 yield is suppressed.
| nucl-ex | neutral pion transverse momentum spectra were measured in pc and ppb collisions at sqrts_nn 174 gev at midrapidity 23 eta_lab 30 over the range 07 p_t 35 gevc the spectra are compared to pi0 spectra measured in pbpb collisions at sqrts_nn 173 gev in the same experiment for a wide range of pbpb centralities n_part 300 the yield of pi0s with p_t 2 gevc is larger than or consistent with the pc or ppb yields scaled with the number of nucleonnucleon collisions n_coll while for central pbpb collisions with n_part 350 the pi0 yield is suppressed | [['neutral', 'pion', 'transverse', 'momentum', 'spectra', 'were', 'measured', 'in', 'pc', 'and', 'ppb', 'collisions', 'at', 'sqrts_nn', '174', 'gev', 'at', 'midrapidity', '23', 'eta_lab', '30', 'over', 'the', 'range', '07', 'p_t', '35', 'gevc', 'the', 'spectra', 'are', 'compared', 'to', 'pi0', 'spectra', 'measured', 'in', 'pbpb', 'collisions', 'at', 'sqrts_nn', '173', 'gev', 'in', 'the', 'same', 'experiment', 'for', 'a', 'wide', 'range', 'of', 'pbpb', 'centralities', 'n_part', '300', 'the', 'yield', 'of', 'pi0s', 'with', 'p_t', '2', 'gevc', 'is', 'larger', 'than', 'or', 'consistent', 'with', 'the', 'pc', 'or', 'ppb', 'yields', 'scaled', 'with', 'the', 'number', 'of', 'nucleonnucleon', 'collisions', 'n_coll', 'while', 'for', 'central', 'pbpb', 'collisions', 'with', 'n_part', '350', 'the', 'pi0', 'yield', 'is', 'suppressed']] | [-0.010755416603856965, 0.3353718228883257, -0.15890794982153333, 0.09953930557607428, 0.11856991948412829, -0.10796809162160284, -0.16264415549506483, 0.36800988892975606, -0.11911858862609064, -0.38659831893287205, -0.2050195212904854, -0.5065564596143208, 0.3236901616138455, 0.1851492951354502, 0.118724188257597, 0.1045483014105182, 0.1733841169380436, 0.01962492252258878, -0.051659478325592846, -0.1636341606732458, 0.19049495088034554, 0.1748229150317217, 0.1761251889953488, 0.2150530873846851, 0.03470060939067288, 0.0926125173309916, 0.01629532657182273, 0.002072106046896232, -0.16109237224843942, -0.008674609326561424, 0.3882040625707687, -0.06335893741955882, 0.11664080402176631, -0.19273050545077575, -0.04418995177471324, 0.14626685210846757, 0.16807243166687458, -0.009674054729801259, -0.06548988066221538, -0.2555599233723785, 0.2548056807467028, -0.2946746211057823, -0.13517239391803743, 0.038878342273988224, 0.03248509452923348, 0.04793307963011198, -0.30672702405013536, 0.2683326647224787, -0.0898505280725658, 0.24064622507062985, -0.03743866844788978, -0.33257346098360263, -0.10986719940740027, -0.09932012736895367, 0.08322952452949003, 0.21059598327050671, 0.2636136183319123, -0.07675240435392448, -0.1582815654379757, 0.45647051334381106, 0.0749613319932618, -0.021098100541061475, 0.18429890390681594, -0.30069745767273404, -0.08388563624926304, 0.2771208485318838, 0.2897924040493212, 0.06871194131672383, -0.21959064256792005, -0.0449900172951043, -0.01667143929945795, 0.27784337228850314, 0.2124749876215662, 0.10211398203514124, 0.08678437539523369, 0.17619672238973802, -0.05237191555727469, 0.03005011258401761, -0.20576308636288893, -0.08095381518727855, -0.3949086168793177, -0.010122239162324388, -0.039991794722644906, 0.09018511904256517, -0.18582920679611178, 0.11627194226572388, 0.3202971895372397, 0.05092997345767033, 0.4278387433212054, 0.04113821784818643, 0.24290566828690077, 0.06429416104955109, 0.09749042616274796, 0.17776134877318614, 0.30968662112167006, 0.1711654488021802, 0.3619508568944998, -0.17779905210053057, -0.028344423809137785, -0.018955982809788302] |
708.2631 | Intrinsic Axis Ratio Distribution of Early-type Galaxies From Sloan
Digital Sky Survey | Using Sloan Digital Sky Survey Data Release 5, we have investigated the
intrinsic axis ratio distribution (ARD) for early-type galaxies. We have
constructed a volume-limited sample of 3,922 visually-inspected early-type
galaxies at $0.05 \leq z \leq 0.06$ carefully considering sampling biases
caused by the galaxy isophotal size and luminosity. We attempt to de-project
the observed ARD into three-dimensional types (oblate, prolate, and triaxial),
which are classified in terms of triaxiality. We confirm that no linear
combination of $randomly$-distributed axis ratios of the three types can
reproduce the observed ARD. However, using Gaussian intrinsic distributions, we
have found reasonable fits to the data with preferred mean axis ratios for
oblate, prolate, and triaxial (triaxials in two axis ratios), $\mu_o=0.44,
\mu_p=0.72, \mu_{t,\beta}=0.92, \mu_{t,\gamma}=0.78$ where the fractions of
oblate, prolate and triaxial types are
\textrm{O:P:T}=0.29^{\pm0.09}:0.26^{\pm0.11}:0.45^{\pm0.13}$. We have also
found that the luminous sample ($-23.3 < M_r \leq -21.2$) tends to have more
triaxials than the less luminous ($-21.2 < M_r <-19.3$) sample does. Oblate is
relatively more abundant among the less luminous galaxies. Interestingly, the
preferences of axis ratios for triaxial types in the two luminosity classes are
remarkably similar. We have not found any significant influence of the local
galaxy number density on ARD. We show that the results can be seriously
affected by the details in the data selection and type classification scheme.
Caveats and implications on galaxy formation are discussed.
| astro-ph | using sloan digital sky survey data release 5 we have investigated the intrinsic axis ratio distribution ard for earlytype galaxies we have constructed a volumelimited sample of 3922 visuallyinspected earlytype galaxies at 005 leq z leq 006 carefully considering sampling biases caused by the galaxy isophotal size and luminosity we attempt to deproject the observed ard into threedimensional types oblate prolate and triaxial which are classified in terms of triaxiality we confirm that no linear combination of randomlydistributed axis ratios of the three types can reproduce the observed ard however using gaussian intrinsic distributions we have found reasonable fits to the data with preferred mean axis ratios for oblate prolate and triaxial triaxials in two axis ratios mu_o044 mu_p072 mu_tbeta092 mu_tgamma078 where the fractions of oblate prolate and triaxial types are textrmopt029pm009026pm011045pm013 we have also found that the luminous sample 233 m_r leq 212 tends to have more triaxials than the less luminous 212 m_r 193 sample does oblate is relatively more abundant among the less luminous galaxies interestingly the preferences of axis ratios for triaxial types in the two luminosity classes are remarkably similar we have not found any significant influence of the local galaxy number density on ard we show that the results can be seriously affected by the details in the data selection and type classification scheme caveats and implications on galaxy formation are discussed | [['using', 'sloan', 'digital', 'sky', 'survey', 'data', 'release', '5', 'we', 'have', 'investigated', 'the', 'intrinsic', 'axis', 'ratio', 'distribution', 'ard', 'for', 'earlytype', 'galaxies', 'we', 'have', 'constructed', 'a', 'volumelimited', 'sample', 'of', '3922', 'visuallyinspected', 'earlytype', 'galaxies', 'at', '005', 'leq', 'z', 'leq', '006', 'carefully', 'considering', 'sampling', 'biases', 'caused', 'by', 'the', 'galaxy', 'isophotal', 'size', 'and', 'luminosity', 'we', 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708.2632 | Zonotopal algebra | A wealth of geometric and combinatorial properties of a given linear
endomorphism $X$ of $\R^N$ is captured in the study of its associated zonotope
$Z(X)$, and, by duality, its associated hyperplane arrangement ${\cal H}(X)$.
This well-known line of study is particularly interesting in case $n\eqbd\rank
X \ll N$. We enhance this study to an algebraic level, and associate $X$ with
three algebraic structures, referred herein as {\it external, central, and
internal.} Each algebraic structure is given in terms of a pair of homogeneous
polynomial ideals in $n$ variables that are dual to each other: one encodes
properties of the arrangement ${\cal H}(X)$, while the other encodes by duality
properties of the zonotope $Z(X)$. The algebraic structures are defined purely
in terms of the combinatorial structure of $X$, but are subsequently proved to
be equally obtainable by applying suitable algebro-analytic operations to
either of $Z(X)$ or ${\cal H}(X)$. The theory is universal in the sense that it
requires no assumptions on the map $X$ (the only exception being that the
algebro-analytic operations on $Z(X)$ yield sought-for results only in case $X$
is unimodular), and provides new tools that can be used in enumerative
combinatorics, graph theory, representation theory, polytope geometry, and
approximation theory.
| math.AC math.CA math.CO | a wealth of geometric and combinatorial properties of a given linear endomorphism x of rn is captured in the study of its associated zonotope zx and by duality its associated hyperplane arrangement cal hx this wellknown line of study is particularly interesting in case neqbdrank x ll n we enhance this study to an algebraic level and associate x with three algebraic structures referred herein as it external central and internal each algebraic structure is given in terms of a pair of homogeneous polynomial ideals in n variables that are dual to each other one encodes properties of the arrangement cal hx while the other encodes by duality properties of the zonotope zx the algebraic structures are defined purely in terms of the combinatorial structure of x but are subsequently proved to be equally obtainable by applying suitable algebroanalytic operations to either of zx or cal hx the theory is universal in the sense that it requires no assumptions on the map x the only exception being that the algebroanalytic operations on zx yield soughtfor results only in case x is unimodular and provides new tools that can be used in enumerative combinatorics graph theory representation theory polytope geometry and approximation theory | [['a', 'wealth', 'of', 'geometric', 'and', 'combinatorial', 'properties', 'of', 'a', 'given', 'linear', 'endomorphism', 'x', 'of', 'rn', 'is', 'captured', 'in', 'the', 'study', 'of', 'its', 'associated', 'zonotope', 'zx', 'and', 'by', 'duality', 'its', 'associated', 'hyperplane', 'arrangement', 'cal', 'hx', 'this', 'wellknown', 'line', 'of', 'study', 'is', 'particularly', 'interesting', 'in', 'case', 'neqbdrank', 'x', 'll', 'n', 'we', 'enhance', 'this', 'study', 'to', 'an', 'algebraic', 'level', 'and', 'associate', 'x', 'with', 'three', 'algebraic', 'structures', 'referred', 'herein', 'as', 'it', 'external', 'central', 'and', 'internal', 'each', 'algebraic', 'structure', 'is', 'given', 'in', 'terms', 'of', 'a', 'pair', 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708.2633 | Bouncing and Colliding Branes | In a braneworld description of our universe, we must allow for the
possibility of having dynamical branes around the time of the big bang. Some
properties of such domain walls in motion are discussed here, for example the
ability of negative-tension domain walls to bounce off spacetime singularities
and the consequences for cosmological perturbations. In this context, we will
also review a colliding branes solution of heterotic M-theory that has been
proposed as a model for early universe cosmology.
| hep-th | in a braneworld description of our universe we must allow for the possibility of having dynamical branes around the time of the big bang some properties of such domain walls in motion are discussed here for example the ability of negativetension domain walls to bounce off spacetime singularities and the consequences for cosmological perturbations in this context we will also review a colliding branes solution of heterotic mtheory that has been proposed as a model for early universe cosmology | [['in', 'a', 'braneworld', 'description', 'of', 'our', 'universe', 'we', 'must', 'allow', 'for', 'the', 'possibility', 'of', 'having', 'dynamical', 'branes', 'around', 'the', 'time', 'of', 'the', 'big', 'bang', 'some', 'properties', 'of', 'such', 'domain', 'walls', 'in', 'motion', 'are', 'discussed', 'here', 'for', 'example', 'the', 'ability', 'of', 'negativetension', 'domain', 'walls', 'to', 'bounce', 'off', 'spacetime', 'singularities', 'and', 'the', 'consequences', 'for', 'cosmological', 'perturbations', 'in', 'this', 'context', 'we', 'will', 'also', 'review', 'a', 'colliding', 'branes', 'solution', 'of', 'heterotic', 'mtheory', 'that', 'has', 'been', 'proposed', 'as', 'a', 'model', 'for', 'early', 'universe', 'cosmology']] | [-0.130124055986776, 0.09397884919249182, -0.1398354699080692, 0.10592904237034154, -0.12703588746393782, -0.10210737944551142, -0.029304079242828716, 0.33740397843331854, -0.1916075461143274, -0.24409811409732587, 0.14153250528033823, -0.2555477820171774, -0.09146825872550282, 0.1561137332162478, -0.08202572798804392, 0.021462635054618498, 0.006769434808270086, 0.02268460631971778, -0.0399012106435397, -0.26448710821568966, 0.3827025861703331, 0.05388223006142468, 0.21530507391177212, 0.04961111169614935, 0.08960767922027013, -0.1025340989809719, 0.022968581574084827, 0.04052866026287592, -0.17189183737833974, 0.05001458727837175, 0.21890198893876764, 0.14398818164238636, 0.2102553150321864, -0.49595162121555475, -0.2833172323512314, 0.13957040326646233, 0.23277317668323086, 0.215099911488404, -0.10572671887016843, -0.29260848759661745, 0.08768396174735567, -0.16480531772787246, -0.18303007519320597, -0.06309275330586618, 0.06034678317417827, -0.05219719874307136, -0.1699269189664363, 0.06680228227205705, 0.03198956232923201, -0.039934957170080915, -0.09745458614882789, -0.03145538107786752, 0.0027829167592233117, 0.062454967582716216, 0.13280983797209692, -0.0016524950337089316, 0.1262635600788495, -0.1698962877279065, -0.12305567769593076, 0.39465881396037866, -0.08122546380957518, -0.18163704461877858, 0.15958676402327382, -0.1712997010024854, -0.14636878688418883, 0.04887820539194383, 0.13548912631223992, 0.13987183518990687, -0.13865015642788214, 0.17846624570371158, 0.05171274945222407, 0.09991539030960656, 0.1394935537518674, 0.057518839582659395, 0.334635292462816, 0.22390406425523607, -0.0007076362925994245, 0.09510132785933682, -0.06326713407695105, -0.11972837501995359, -0.41885599008278, -0.15855837638690312, -0.11733042435791297, 0.08785806562091354, -0.1579681366644844, -0.16721330693321704, 0.3849763577403147, 0.1352864155970231, 0.17977283822514023, -0.011725169167370547, 0.2353976618357097, -0.03845952878576479, -0.005293471573651592, 0.04389773562986734, 0.2503498183888283, 0.0800960835016368, 0.16303175586405433, -0.20767455295765702, -0.05330337957726627, 0.07385583835819005] |
708.2634 | Bremsstrahlung in weak charged current polarized lepton-nucleon deep
inelastic scattering | The processes of lepton-nucleon scattering, including ones with both
polarized beams, at high energy provide relevant information about interaction
and particles structure, allowing to analyze nucleon spin structure. As energy
and experimental accuracy rise, necessity to improve Born cross sections and
polarized asymmetries with higher order radiative corrections becomes
substantial. In this report we stress on lowest order bremsstrahlung
corrections treatment using helicity amplitudes method as applied to actual
nowadays charged current lepton-nucleon deep inelastic processes, that allows
to simplify matrix element calculation procedure. Real photon emission
contribution is calculated by means of Lorentz-invariant formalism. Kinematical
peculiarities on bremsstrahlung correction are discussed.
| hep-ph | the processes of leptonnucleon scattering including ones with both polarized beams at high energy provide relevant information about interaction and particles structure allowing to analyze nucleon spin structure as energy and experimental accuracy rise necessity to improve born cross sections and polarized asymmetries with higher order radiative corrections becomes substantial in this report we stress on lowest order bremsstrahlung corrections treatment using helicity amplitudes method as applied to actual nowadays charged current leptonnucleon deep inelastic processes that allows to simplify matrix element calculation procedure real photon emission contribution is calculated by means of lorentzinvariant formalism kinematical peculiarities on bremsstrahlung correction are discussed | [['the', 'processes', 'of', 'leptonnucleon', 'scattering', 'including', 'ones', 'with', 'both', 'polarized', 'beams', 'at', 'high', 'energy', 'provide', 'relevant', 'information', 'about', 'interaction', 'and', 'particles', 'structure', 'allowing', 'to', 'analyze', 'nucleon', 'spin', 'structure', 'as', 'energy', 'and', 'experimental', 'accuracy', 'rise', 'necessity', 'to', 'improve', 'born', 'cross', 'sections', 'and', 'polarized', 'asymmetries', 'with', 'higher', 'order', 'radiative', 'corrections', 'becomes', 'substantial', 'in', 'this', 'report', 'we', 'stress', 'on', 'lowest', 'order', 'bremsstrahlung', 'corrections', 'treatment', 'using', 'helicity', 'amplitudes', 'method', 'as', 'applied', 'to', 'actual', 'nowadays', 'charged', 'current', 'leptonnucleon', 'deep', 'inelastic', 'processes', 'that', 'allows', 'to', 'simplify', 'matrix', 'element', 'calculation', 'procedure', 'real', 'photon', 'emission', 'contribution', 'is', 'calculated', 'by', 'means', 'of', 'lorentzinvariant', 'formalism', 'kinematical', 'peculiarities', 'on', 'bremsstrahlung', 'correction', 'are', 'discussed']] | [-0.03637983913758231, 0.16149755669118582, -0.06700930481904424, 0.16162411752156913, -0.07361437515446953, -0.0799994542007791, 0.02460644655751393, 0.41443340399978207, -0.19532222917084308, -0.30586269364564445, -0.03927692017339937, -0.3340507031661771, -0.0334054257574619, 0.17275867680105947, 0.09647226887846402, 0.06347459251079343, 0.07589807653543997, -0.04080931277341876, -0.04604941179437161, -0.17874357391573378, 0.3389799580635393, 0.11513451901098996, 0.29004197043604124, 0.1703676079107704, 0.07512442775837638, 0.10335122472058762, -0.09373818087738518, -0.049942123498219776, -0.0879230217637372, 0.07309784983312163, 0.26390429416628025, 0.008440173580881902, 0.08846415625428598, -0.46773106291634486, -0.1665923146384896, 0.05392512218917117, 0.1559965692177488, 0.1537129425845456, -0.018913053042328386, -0.25067454119048577, -0.011801546174740675, -0.21860570437731405, -0.15922211417837032, -0.1893087861050541, 0.006051822821153146, -0.05113129405414357, -0.2855254948725833, 0.0965362115735736, -0.030742605350336388, -0.0038913164068670836, -0.05661162952538671, -0.1857555305913967, -0.02666685389190474, 0.06423554632484037, 0.07697849671639428, 0.04022804827899581, 0.20752117586979532, -0.15155312986633576, -0.15309230917060346, 0.378187854078087, -0.05842796154091975, -0.17904570203858847, 0.11373400509896159, -0.20746804503997898, -0.09804914718009897, 0.25544360563085944, 0.2303831954874719, 0.10912741472323735, -0.17134854866890237, 0.06659768893687036, 0.09333397937007248, 0.1348770452896133, 0.08505415477716893, 0.06943963412035659, 0.18104059134573475, 0.16565729683155522, -0.06309157326890558, 0.0865454279552853, -0.11747343956456319, -0.11403466791243237, -0.3408599937626836, -0.09656208842584331, -0.07626004308900412, 0.07720465157363637, -0.03663126155166252, -0.100082763067821, 0.31464638496183006, 0.14961150078577737, 0.17761358982591213, -0.016003483203331045, 0.38159128428235944, 0.15422100456164436, 0.08702688156535812, 0.02627818144894406, 0.2715704899883884, 0.2512455393090004, 0.132882772191592, -0.2540866996243815, 0.05396692431988377, 0.03204725413610611] |
708.2635 | Boundedness and Compactness of products of Toeplitz operators on the
Bergman Space | In a celebrated conjecture D.Sarason stated a necessary and sufficient
condition on the symbols f, g in the Bergman space, L^2_a(\Delta) of the unit
disk, \Delta, for the products T_{f}T_{\bar g} of associated Toeplitz operators
to be bounded (respectively compact) on L^2_a(\Delta) . K. Stroethoff and D.
Zheng proved that these conditions are necessary. We prove the sufficiency of
these conditions, thus solvind Sarason's conjecture.
| math.CV math.CA | in a celebrated conjecture dsarason stated a necessary and sufficient condition on the symbols f g in the bergman space l2_adelta of the unit disk delta for the products t_ft_bar g of associated toeplitz operators to be bounded respectively compact on l2_adelta k stroethoff and d zheng proved that these conditions are necessary we prove the sufficiency of these conditions thus solvind sarasons conjecture | [['in', 'a', 'celebrated', 'conjecture', 'dsarason', 'stated', 'a', 'necessary', 'and', 'sufficient', 'condition', 'on', 'the', 'symbols', 'f', 'g', 'in', 'the', 'bergman', 'space', 'l2_adelta', 'of', 'the', 'unit', 'disk', 'delta', 'for', 'the', 'products', 't_ft_bar', 'g', 'of', 'associated', 'toeplitz', 'operators', 'to', 'be', 'bounded', 'respectively', 'compact', 'on', 'l2_adelta', 'k', 'stroethoff', 'and', 'd', 'zheng', 'proved', 'that', 'these', 'conditions', 'are', 'necessary', 'we', 'prove', 'the', 'sufficiency', 'of', 'these', 'conditions', 'thus', 'solvind', 'sarasons', 'conjecture']] | [-0.21683719145754973, 0.0965305565080295, -0.0353138519761463, 0.08511474679689854, -0.06437591743888334, -0.13525221787082653, 0.0338519107705603, 0.33303997792924445, -0.25228010714054105, -0.2097775237945219, 0.16403479929625367, -0.18455813760713985, -0.13531739683821797, 0.2025240909929077, -0.1466994540145, 0.06111636273562908, 0.08247677113977261, 0.0825484824211647, -0.08793898120444889, -0.3309075276988248, 0.36453673100719847, -0.03563679317012429, 0.16106327081409594, 0.14292688661953434, 0.04295302371804913, -0.03013272563305994, -0.03153223854412014, -0.06348392438036778, -0.22036967456479034, 0.0945598334694902, 0.22668990117187302, 0.14457018928369508, 0.25662642400711777, -0.38763049493233365, -0.14913354293288042, 0.17985066357068719, 0.05210109631686161, -0.09552281196229159, 0.03314563435318026, -0.31238773033643763, 0.14999620948607723, -0.06437775659918164, -0.16983245783485473, -0.053387039752366645, 0.07887477131250004, -0.0038282790260079007, -0.3647999604853491, 0.061194842820987104, 0.19442793133979042, 0.04653479678866764, -0.1087315620156005, -0.12953016029205172, -0.07415095681208186, 0.06056858508770044, -0.06663043998802702, 0.05091062205998848, 0.0029099593016629417, -0.035846251691691575, -0.04436826073409369, 0.30466772032280764, -0.06044104856749376, -0.21289069140329958, 0.13251814637333154, -0.19869333604971567, -0.1656973933723445, 0.06514437585913886, 0.10391541112524767, 0.1785452029046913, -0.07949378901782135, 0.17043228815115677, -0.12983282927113274, 0.05174903497099877, 0.1767429535665239, 0.0416015324764885, 0.09251690442906693, 0.004014651624796291, 0.155727516564851, 0.1316714995133225, 0.03508638141114109, 0.030487459040402124, -0.37534984623392426, -0.1678073072185119, -0.19391931196053822, 0.11377979250003895, -0.11259668384785376, -0.13488479588801663, 0.2947297224076465, 0.06727519650012255, 0.1756430460140109, 0.10148958147037775, 0.1639851391936342, 0.09355959026822044, 0.04456487516872585, 0.10674526471023758, 0.11599942153940598, 0.2896551138100525, 0.05142655242234469, -0.16571208954167863, 0.0232224769036596, 0.179998939329865] |
708.2636 | Genericity of supercuspidal representations of p-adic Sp(4) | We describe the supercuspidal representations of Sp(4,F), for F a
non-archimedean local field of residual characteristic different from 2, and
determine which are generic.
| math.RT math.NT | we describe the supercuspidal representations of sp4f for f a nonarchimedean local field of residual characteristic different from 2 and determine which are generic | [['we', 'describe', 'the', 'supercuspidal', 'representations', 'of', 'sp4f', 'for', 'f', 'a', 'nonarchimedean', 'local', 'field', 'of', 'residual', 'characteristic', 'different', 'from', '2', 'and', 'determine', 'which', 'are', 'generic']] | [-0.17036412154202876, 0.07792414765319099, -0.16527472476920355, 0.07494001422563325, -0.06267315076421136, -0.11922207513176229, -0.08286951858874249, 0.2951454418589887, -0.3721457344034444, -0.2341359309528185, 0.026635206243752138, -0.16076865468336188, -0.14943462658835494, 0.22598461041469936, -0.031149856381766174, -0.0702001323275592, -0.06912779462847697, 0.15544348963252877, -0.12546525470426548, -0.24440090123402036, 0.4455601365669914, -0.10921665054300557, 0.24973550795213037, -0.015645788820541424, 0.11778550987820262, 0.030539352952948084, -0.04838932159802188, -0.026946387324563188, -0.10779711502887633, 0.14049725710292874, 0.3271282942479719, 0.1179448828789527, 0.20104779480227633, -0.4451674640826557, -0.1643011820624056, 0.22351240686586368, 0.102715526505009, 0.08860131910414962, 0.018190274683191725, -0.2883545725160967, 0.2042670249129119, -0.1457766245888627, -0.08665805893099826, -0.1443841784544613, 0.06262137346556815, 0.07718934758525828, -0.318070282511737, 0.024944511606641438, 0.0917482117757849, 0.24423743683196927, -0.1432703891971513, -0.1284255507685568, 0.016105013535074566, 0.13222898945779257, -0.004103349359787028, 0.11238781239270516, 0.13691417026616956, -0.1712817149034337, -0.003292340501818968, 0.337920637720305, -0.10787154568116301, -0.13148544592094485, 0.20995327668345493, -0.14856447927329852, -0.10638313752639553, 0.11931528887994912, 0.18296906481618466, 0.13055445021018386, -0.07832252805161735, 0.1519894546439426, -0.09612967916156935, 0.058749786998226264, 0.03217819601337871, -0.018228647906495178, 0.20853818437772925, 0.0016871813036825347, 0.05671418899589259, 0.09634522534906864, -0.06704339741364769, 0.05661034656931525, -0.3794234777274339, -0.15807877497180647, -0.12560362678588086, 0.08970669735951917, -0.1137157781853128, -0.14610760671127102, 0.5548359401848005, 0.13643315766492617, 0.20677741811327313, 0.15812634442345766, 0.18006625411141178, 0.09706773811384388, 0.06205078165816224, 0.07583546519036526, 0.1345931103695994, 0.1543368193037484, -0.10101925213213848, -0.1680871516607864, -0.030812759559763515, 0.1094287961680928] |
708.2637 | On the orientation of the Sagittarius A* system | The near-infrared emission from the black hole at the Galactic center (Sgr
A*) has unique properties. The most striking feature is a suggestive periodic
sub-structure that has been observed in a couple of flares so far. Using
near-infrared polarimetric observations and modelling the quasi-periodicity in
terms of an orbiting blob, we try to constrain the three dimensional
orientation of the Sgr A* system. We report on so far unpublished polarimetric
data from 2003. They support the observations of a roughly constant mean
polarization angle of 60 degr \pm 20 degr from 2004-2006. Prior investigations
of the 2006 data are deepened. In particular, the blob model fits are evaluated
such that constraints on the position angle of Sgr A* can be derived.
Confidence contours in the position-inclination angle plane are derived. On a
3sigma level the position angle of the equatorial plane normal is in the range
60 degr - 108 degr (east of north) in combination with a large inclination
angle. This agrees well with recent independent work in which radio
spectral/morphological properties of Sgr A* and X-ray observations,
respectively, have been used. However, the quality of the presently available
data and the uncertainties in our model bring some ambiguity to our
conclusions.
| astro-ph | the nearinfrared emission from the black hole at the galactic center sgr a has unique properties the most striking feature is a suggestive periodic substructure that has been observed in a couple of flares so far using nearinfrared polarimetric observations and modelling the quasiperiodicity in terms of an orbiting blob we try to constrain the three dimensional orientation of the sgr a system we report on so far unpublished polarimetric data from 2003 they support the observations of a roughly constant mean polarization angle of 60 degr pm 20 degr from 20042006 prior investigations of the 2006 data are deepened in particular the blob model fits are evaluated such that constraints on the position angle of sgr a can be derived confidence contours in the positioninclination angle plane are derived on a 3sigma level the position angle of the equatorial plane normal is in the range 60 degr 108 degr east of north in combination with a large inclination angle this agrees well with recent independent work in which radio spectralmorphological properties of sgr a and xray observations respectively have been used however the quality of the presently available data and the uncertainties in our model bring some ambiguity to our conclusions | [['the', 'nearinfrared', 'emission', 'from', 'the', 'black', 'hole', 'at', 'the', 'galactic', 'center', 'sgr', 'a', 'has', 'unique', 'properties', 'the', 'most', 'striking', 'feature', 'is', 'a', 'suggestive', 'periodic', 'substructure', 'that', 'has', 'been', 'observed', 'in', 'a', 'couple', 'of', 'flares', 'so', 'far', 'using', 'nearinfrared', 'polarimetric', 'observations', 'and', 'modelling', 'the', 'quasiperiodicity', 'in', 'terms', 'of', 'an', 'orbiting', 'blob', 'we', 'try', 'to', 'constrain', 'the', 'three', 'dimensional', 'orientation', 'of', 'the', 'sgr', 'a', 'system', 'we', 'report', 'on', 'so', 'far', 'unpublished', 'polarimetric', 'data', 'from', '2003', 'they', 'support', 'the', 'observations', 'of', 'a', 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'available', 'data', 'and', 'the', 'uncertainties', 'in', 'our', 'model', 'bring', 'some', 'ambiguity', 'to', 'our', 'conclusions']] | [-0.0994728981029006, 0.06509945590336591, -0.07563088337117019, 0.03368407769003577, -0.11230065556073941, -0.06626226997758211, 0.0497708877476757, 0.4205324095372685, -0.19508738006263582, -0.3367986876832609, 0.11201116006412493, -0.317062452030067, -0.05300618683113091, 0.21213651833295896, -0.06120199178442804, 0.008008296226128989, 0.07141053452578128, -0.028289608738445375, -0.06103564779661058, -0.1749982031349519, 0.2179403696788373, 0.08879301955793702, 0.19794350864819774, 0.0005340282312960396, 0.09583851096043085, -0.051575700982951035, -0.04333384414620475, 0.007435170268704791, -0.1396815183701194, 0.07439732667427137, 0.21244986121547385, 0.12553708366403182, 0.18450357680398952, -0.35300379520773295, -0.20472226883006742, 0.006900478274890439, 0.12886575105008136, 0.03826641373797343, -0.015610537728623705, -0.28461092327772386, 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708.2638 | Three-State Feshbach Resonances Mediated By Second-Order Couplings | We present an analytical study of three-state Feshbach resonances induced by
second-order couplings. Such resonances arise when the scattering amplitude is
modified by the interaction with a bound state that is not directly coupled to
the scattering state containing incoming flux. Coupling occurs indirectly
through an intermediate state. We consider two problems: (i) the intermediate
state is a scattering state in a distinct open channel; (ii) the intermediate
state is an off-resonant bound state in a distinct closed channel. The first
problem is a model of electric-field-induced resonances in ultracold collisions
of alkali metal atoms [Phys. Rev. A 75, 032709 (2007)] and the second problem
is relevant for ultracold collisions of complex polyatomic molecules, chemical
reaction dynamics, photoassociation of ultracold atoms, and electron - molecule
scattering. Our analysis yields general expressions for the energy dependence
of the T-matrix elements modified by three-state resonances and the dependence
of the resonance positions and widths on coupling amplitudes for the
weak-coupling limit. We show that the second problem can be generalized to
describe resonances induced by indirect coupling through an arbitrary number of
sequentially coupled off-resonant bound states and analyze the dependence of
the resonance width on the number of the intermediate states.
| physics.atom-ph physics.chem-ph | we present an analytical study of threestate feshbach resonances induced by secondorder couplings such resonances arise when the scattering amplitude is modified by the interaction with a bound state that is not directly coupled to the scattering state containing incoming flux coupling occurs indirectly through an intermediate state we consider two problems i the intermediate state is a scattering state in a distinct open channel ii the intermediate state is an offresonant bound state in a distinct closed channel the first problem is a model of electricfieldinduced resonances in ultracold collisions of alkali metal atoms phys rev a 75 032709 2007 and the second problem is relevant for ultracold collisions of complex polyatomic molecules chemical reaction dynamics photoassociation of ultracold atoms and electron molecule scattering our analysis yields general expressions for the energy dependence of the tmatrix elements modified by threestate resonances and the dependence of the resonance positions and widths on coupling amplitudes for the weakcoupling limit we show that the second problem can be generalized to describe resonances induced by indirect coupling through an arbitrary number of sequentially coupled offresonant bound states and analyze the dependence of the resonance width on the number of the intermediate states | [['we', 'present', 'an', 'analytical', 'study', 'of', 'threestate', 'feshbach', 'resonances', 'induced', 'by', 'secondorder', 'couplings', 'such', 'resonances', 'arise', 'when', 'the', 'scattering', 'amplitude', 'is', 'modified', 'by', 'the', 'interaction', 'with', 'a', 'bound', 'state', 'that', 'is', 'not', 'directly', 'coupled', 'to', 'the', 'scattering', 'state', 'containing', 'incoming', 'flux', 'coupling', 'occurs', 'indirectly', 'through', 'an', 'intermediate', 'state', 'we', 'consider', 'two', 'problems', 'i', 'the', 'intermediate', 'state', 'is', 'a', 'scattering', 'state', 'in', 'a', 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708.2639 | Black holes in the TeVeS theory of gravity and their thermodynamics | TeVeS, a relativistic theory of gravity, was designed to provide a basis for
the modified Newtonian dynamics. Since TeVeS differs from general relativity
(e.g., it has two metrics, an Einstein metric and a physical metric), black
hole solutions of it would be valuable for a number of endeavors ranging from
astrophysical modeling to investigations into the interrelation between gravity
and thermodynamics. Giannios has recently found a TeVeS analogue of the
Schwarzschild black hole solution. We proceed further with the program by
analytically solving the TeVeS equations for a static spherically symmetric and
asymptotically flat system of electromagnetic and gravity fields. We show that
one solution is provided by the Reissner-Nordstrom metric as physical metric,
the TeVeS vector field pointing in the time direction, and a TeVeS scalar field
positive everywhere (the last feature protects from superluminal propagation of
disturbances in the fields). We work out black hole thermodynamics in TeVeS
using the physical metric; black hole entropy, temperature and electric
potential turn out to be identical to those in general relativity. We find it
inconsistent to base thermodynamics on the Einstein metric. In light of this we
reconsider the Dubovsky-Sibiryakov scenario for violating the second law of
thermodynamics in theories with Lorentz symmetry violation.
| gr-qc astro-ph hep-th | teves a relativistic theory of gravity was designed to provide a basis for the modified newtonian dynamics since teves differs from general relativity eg it has two metrics an einstein metric and a physical metric black hole solutions of it would be valuable for a number of endeavors ranging from astrophysical modeling to investigations into the interrelation between gravity and thermodynamics giannios has recently found a teves analogue of the schwarzschild black hole solution we proceed further with the program by analytically solving the teves equations for a static spherically symmetric and asymptotically flat system of electromagnetic and gravity fields we show that one solution is provided by the reissnernordstrom metric as physical metric the teves vector field pointing in the time direction and a teves scalar field positive everywhere the last feature protects from superluminal propagation of disturbances in the fields we work out black hole thermodynamics in teves using the physical metric black hole entropy temperature and electric potential turn out to be identical to those in general relativity we find it inconsistent to base thermodynamics on the einstein metric in light of this we reconsider the dubovskysibiryakov scenario for violating the second law of thermodynamics in theories with lorentz symmetry violation | [['teves', 'a', 'relativistic', 'theory', 'of', 'gravity', 'was', 'designed', 'to', 'provide', 'a', 'basis', 'for', 'the', 'modified', 'newtonian', 'dynamics', 'since', 'teves', 'differs', 'from', 'general', 'relativity', 'eg', 'it', 'has', 'two', 'metrics', 'an', 'einstein', 'metric', 'and', 'a', 'physical', 'metric', 'black', 'hole', 'solutions', 'of', 'it', 'would', 'be', 'valuable', 'for', 'a', 'number', 'of', 'endeavors', 'ranging', 'from', 'astrophysical', 'modeling', 'to', 'investigations', 'into', 'the', 'interrelation', 'between', 'gravity', 'and', 'thermodynamics', 'giannios', 'has', 'recently', 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708.264 | An investigation of Fe XVI emission lines in solar and stellar EUV and
soft X-ray spectra | New fully relativistic calculations of radiative rates and electron impact
excitation cross sections for Fe XVI are used to determine theoretical
emission-line ratios applicable to the 251 - 361 A and 32 - 77 A portions of
the extreme-ultraviolet (EUV) and soft X-ray spectral regions, respectively. A
comparison of the EUV results with observations from the Solar
Extreme-Ultraviolet Research Telescope and Spectrograph (SERTS) reveals
excellent agreement between theory and experiment. However, for emission lines
in the 32 - 49 A portion of the soft X-ray spectral region, there are large
discrepancies between theory and measurement for both a solar flare spectrum
obtained with the X-Ray Spectrometer/Spectrograph Telescope (XSST) and
observations of Capella from the Low Energy Transmission Grating Spectrometer
(LETGS) on the Chandra X-ray Observatory. These are probably due to blending in
the solar flare and Capella data from both first order lines and from shorter
wavelength transitions detected in second and third order. By contrast, there
is very good agreement between our theoretical results and the XSST and LETGS
observations in the 50 - 77 A wavelength range, contrary to previous results.
In particular, there is no evidence that the Fe XVI emission from the XSST
flare arises from plasma at a much higher temperature than that expected for Fe
XVI in ionization equilibrium, as suggested by earlier work.
| astro-ph | new fully relativistic calculations of radiative rates and electron impact excitation cross sections for fe xvi are used to determine theoretical emissionline ratios applicable to the 251 361 a and 32 77 a portions of the extremeultraviolet euv and soft xray spectral regions respectively a comparison of the euv results with observations from the solar extremeultraviolet research telescope and spectrograph serts reveals excellent agreement between theory and experiment however for emission lines in the 32 49 a portion of the soft xray spectral region there are large discrepancies between theory and measurement for both a solar flare spectrum obtained with the xray spectrometerspectrograph telescope xsst and observations of capella from the low energy transmission grating spectrometer letgs on the chandra xray observatory these are probably due to blending in the solar flare and capella data from both first order lines and from shorter wavelength transitions detected in second and third order by contrast there is very good agreement between our theoretical results and the xsst and letgs observations in the 50 77 a wavelength range contrary to previous results in particular there is no evidence that the fe xvi emission from the xsst flare arises from plasma at a much higher temperature than that expected for fe xvi in ionization equilibrium as suggested by earlier work | [['new', 'fully', 'relativistic', 'calculations', 'of', 'radiative', 'rates', 'and', 'electron', 'impact', 'excitation', 'cross', 'sections', 'for', 'fe', 'xvi', 'are', 'used', 'to', 'determine', 'theoretical', 'emissionline', 'ratios', 'applicable', 'to', 'the', '251', '361', 'a', 'and', '32', '77', 'a', 'portions', 'of', 'the', 'extremeultraviolet', 'euv', 'and', 'soft', 'xray', 'spectral', 'regions', 'respectively', 'a', 'comparison', 'of', 'the', 'euv', 'results', 'with', 'observations', 'from', 'the', 'solar', 'extremeultraviolet', 'research', 'telescope', 'and', 'spectrograph', 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'and', 'letgs', 'observations', 'in', 'the', '50', '77', 'a', 'wavelength', 'range', 'contrary', 'to', 'previous', 'results', 'in', 'particular', 'there', 'is', 'no', 'evidence', 'that', 'the', 'fe', 'xvi', 'emission', 'from', 'the', 'xsst', 'flare', 'arises', 'from', 'plasma', 'at', 'a', 'much', 'higher', 'temperature', 'than', 'that', 'expected', 'for', 'fe', 'xvi', 'in', 'ionization', 'equilibrium', 'as', 'suggested', 'by', 'earlier', 'work']] | [-0.02297668887605501, 0.1266947010277532, -0.014342632307129543, 0.10183898559121718, -0.03246537917077021, -0.09698447563230644, 0.062370511268936966, 0.4555591379097381, -0.1255934088512562, -0.3976948275728974, 0.057581631865265756, -0.3577805746433347, -0.04158603745122808, 0.2527664230389217, 0.007422629374398871, 0.013619602099061013, 0.09055978752087888, -0.09452621594158023, -0.042370765924800276, -0.14448864082480933, 0.24258501112060404, 0.1351600099798985, 0.22757514550155677, 0.045246391004861095, 0.03628757731003557, 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708.2641 | Quantum Treatment of Continuum Electrons in the Fields of Moving Charges | An ab initio, three-dimensional quantum mechanical calculation has been
performed for the time-evolution of continuum electrons in the fields of moving
charges. Here the essential singularity associated with the diverging phase
factor in the continuum wave function is identified and removed analytically.
As a result, the continuum components of the regularized wave function are
slowly varying with time. Therefore, one can propagate continuum electrons to
asymptotically large times and obtain numerically stable, well-converged
ejected electron momentum spectra with very low numerical noise. As a
consequence, our approach resolves outstanding controversies concerning
structures in electron momentum distributions. The main conclusions are general
and are illustrated here for ionization of atomic hydrogen by proton impact.
Our results show that in order to obtain correct long-time free-particle
propagation, the essential singularity identified here should be removed from
the continuum components of solutions to the time-dependent Schrodinger
equation.
| physics.atom-ph physics.comp-ph quant-ph | an ab initio threedimensional quantum mechanical calculation has been performed for the timeevolution of continuum electrons in the fields of moving charges here the essential singularity associated with the diverging phase factor in the continuum wave function is identified and removed analytically as a result the continuum components of the regularized wave function are slowly varying with time therefore one can propagate continuum electrons to asymptotically large times and obtain numerically stable wellconverged ejected electron momentum spectra with very low numerical noise as a consequence our approach resolves outstanding controversies concerning structures in electron momentum distributions the main conclusions are general and are illustrated here for ionization of atomic hydrogen by proton impact our results show that in order to obtain correct longtime freeparticle propagation the essential singularity identified here should be removed from the continuum components of solutions to the timedependent schrodinger equation | [['an', 'ab', 'initio', 'threedimensional', 'quantum', 'mechanical', 'calculation', 'has', 'been', 'performed', 'for', 'the', 'timeevolution', 'of', 'continuum', 'electrons', 'in', 'the', 'fields', 'of', 'moving', 'charges', 'here', 'the', 'essential', 'singularity', 'associated', 'with', 'the', 'diverging', 'phase', 'factor', 'in', 'the', 'continuum', 'wave', 'function', 'is', 'identified', 'and', 'removed', 'analytically', 'as', 'a', 'result', 'the', 'continuum', 'components', 'of', 'the', 'regularized', 'wave', 'function', 'are', 'slowly', 'varying', 'with', 'time', 'therefore', 'one', 'can', 'propagate', 'continuum', 'electrons', 'to', 'asymptotically', 'large', 'times', 'and', 'obtain', 'numerically', 'stable', 'wellconverged', 'ejected', 'electron', 'momentum', 'spectra', 'with', 'very', 'low', 'numerical', 'noise', 'as', 'a', 'consequence', 'our', 'approach', 'resolves', 'outstanding', 'controversies', 'concerning', 'structures', 'in', 'electron', 'momentum', 'distributions', 'the', 'main', 'conclusions', 'are', 'general', 'and', 'are', 'illustrated', 'here', 'for', 'ionization', 'of', 'atomic', 'hydrogen', 'by', 'proton', 'impact', 'our', 'results', 'show', 'that', 'in', 'order', 'to', 'obtain', 'correct', 'longtime', 'freeparticle', 'propagation', 'the', 'essential', 'singularity', 'identified', 'here', 'should', 'be', 'removed', 'from', 'the', 'continuum', 'components', 'of', 'solutions', 'to', 'the', 'timedependent', 'schrodinger', 'equation']] | [-0.08777982902150445, 0.1563341684968691, -0.09303218015379065, 0.08815230599025704, -0.005522469933364644, -0.10715909719187443, -0.003846607851098977, 0.3816214570090071, -0.23648778042600802, -0.2757715574892548, 0.04719306017149291, -0.28594205455010524, -0.08925410016996062, 0.15399738843229394, 0.026771329741071288, 0.08481815399136394, 0.06604711395630147, -0.03492631563373531, -0.0680595428356254, -0.16474779952032906, 0.3204928827269921, 0.08012250407531003, 0.21897809159903167, 0.08183393432086127, 0.08208991863001655, -0.009747248369320814, -0.029554066772107035, 0.029310605019822508, -0.12498180560078254, 0.047502662824829005, 0.2439537759006877, 0.018615214146039862, 0.24229779229547907, -0.4748492199384297, -0.2521231876857605, 0.019381174449032795, 0.20252998735910901, 0.14482898568611643, -0.04128567184347452, -0.2795329190945874, 0.04261234332645674, -0.13169120676724966, -0.246878141197764, -0.09393942257156596, 0.0436909621479976, 0.053855673806942325, -0.22598198080150825, 0.13027436786150146, 0.010736408974076362, -0.008089191545473618, -0.10501195224464431, -0.11321149680669704, -0.046911742159863934, 0.10491921501751575, 0.08604131195582138, 0.053419214911021605, 0.13461685401853174, -0.11293967577189, -0.08932219552742834, 0.3832286633842159, -0.06810280711457987, -0.18948951154015958, 0.1701475467707496, -0.17605435091435437, -0.0929611095537742, 0.20825956045236024, 0.11464733199843774, 0.10466061734283964, -0.13427832388939956, 0.06079062633277014, -0.024035654813107814, 0.16432419270535725, 0.07133144906321023, 0.05095512578918715, 0.1997600216095129, 0.11671238860516395, 0.010219541535863956, 0.11587162688778739, -0.10314705094505269, -0.09882072151392801, -0.30393091594386434, -0.12445898827475806, -0.20414135524252844, 0.11356001664595776, -0.06951362453370773, -0.17571248031648187, 0.3832531891983106, 0.12174212769766907, 0.16688733914149148, 0.0006667274477270743, 0.2969689384270977, 0.19092023334491792, 0.006089525318303559, 0.07612249999915043, 0.26759497847847846, 0.17950346607216894, 0.06591747767460118, -0.2480943717026902, 0.009650301359619739, 0.04229555683559738] |
708.2642 | On the metallicity dependence of the 24micron luminosity as a star
formation tracer | We investigate the use of the rest-frame 24microns luminosity as an indicator
of the star formation rate (SFR) in galaxies with different metallicities by
comparing it to the (extinction corrected) Halpha luminosity. We carry out this
analysis in 2 steps: First, we compare the emission from HII regions in
different galaxies with metallicities between 12+log(O/H) = 8.1 and 8.9. We
find that the 24microns and the extinction corrected Halpha luminosities from
individual HII regions follow the same correlation for all galaxies,
independent of their metallicity. Second, the role of metallicity is explored
further for the integrated luminosity in a sample of galaxies with
metallicities in the range of 12+log(O/H) = 7.2 - 9.1. For this sample we
compare the 24microns and Halpha luminosities integrated over the entire
galaxies and find a lack of the 24microns emission for a given Halpha
luminosity for low metallicity objects, likely reflecting a low dust content.
These results suggest that the 24microns luminosity is a good metallicity
independent tracer for the SFR in individual HII regions. On the other hand,
metallicity has to be taken into account when using the 24microns luminosity as
a tracer for the SFR of entire galaxies.
| astro-ph | we investigate the use of the restframe 24microns luminosity as an indicator of the star formation rate sfr in galaxies with different metallicities by comparing it to the extinction corrected halpha luminosity we carry out this analysis in 2 steps first we compare the emission from hii regions in different galaxies with metallicities between 12logoh 81 and 89 we find that the 24microns and the extinction corrected halpha luminosities from individual hii regions follow the same correlation for all galaxies independent of their metallicity second the role of metallicity is explored further for the integrated luminosity in a sample of galaxies with metallicities in the range of 12logoh 72 91 for this sample we compare the 24microns and halpha luminosities integrated over the entire galaxies and find a lack of the 24microns emission for a given halpha luminosity for low metallicity objects likely reflecting a low dust content these results suggest that the 24microns luminosity is a good metallicity independent tracer for the sfr in individual hii regions on the other hand metallicity has to be taken into account when using the 24microns luminosity as a tracer for the sfr of entire galaxies | [['we', 'investigate', 'the', 'use', 'of', 'the', 'restframe', '24microns', 'luminosity', 'as', 'an', 'indicator', 'of', 'the', 'star', 'formation', 'rate', 'sfr', 'in', 'galaxies', 'with', 'different', 'metallicities', 'by', 'comparing', 'it', 'to', 'the', 'extinction', 'corrected', 'halpha', 'luminosity', 'we', 'carry', 'out', 'this', 'analysis', 'in', '2', 'steps', 'first', 'we', 'compare', 'the', 'emission', 'from', 'hii', 'regions', 'in', 'different', 'galaxies', 'with', 'metallicities', 'between', '12logoh', '81', 'and', '89', 'we', 'find', 'that', 'the', '24microns', 'and', 'the', 'extinction', 'corrected', 'halpha', 'luminosities', 'from', 'individual', 'hii', 'regions', 'follow', 'the', 'same', 'correlation', 'for', 'all', 'galaxies', 'independent', 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708.2643 | On fixed points of permutations | The number of fixed points of a random permutation of 1,2,...,n has a
limiting Poisson distribution. We seek a generalization, looking at other
actions of the symmetric group. Restricting attention to primitive actions, a
complete classification of the limiting distributions is given. For most
examples, they are trivial -- almost every permutation has no fixed points. For
the usual action of the symmetric group on k-sets of 1,2,...,n, the limit is a
polynomial in independent Poisson variables. This exhausts all cases. We obtain
asymptotic estimates in some examples, and give a survey of related results.
| math.CO math.GR | the number of fixed points of a random permutation of 12n has a limiting poisson distribution we seek a generalization looking at other actions of the symmetric group restricting attention to primitive actions a complete classification of the limiting distributions is given for most examples they are trivial almost every permutation has no fixed points for the usual action of the symmetric group on ksets of 12n the limit is a polynomial in independent poisson variables this exhausts all cases we obtain asymptotic estimates in some examples and give a survey of related results | [['the', 'number', 'of', 'fixed', 'points', 'of', 'a', 'random', 'permutation', 'of', '12n', 'has', 'a', 'limiting', 'poisson', 'distribution', 'we', 'seek', 'a', 'generalization', 'looking', 'at', 'other', 'actions', 'of', 'the', 'symmetric', 'group', 'restricting', 'attention', 'to', 'primitive', 'actions', 'a', 'complete', 'classification', 'of', 'the', 'limiting', 'distributions', 'is', 'given', 'for', 'most', 'examples', 'they', 'are', 'trivial', 'almost', 'every', 'permutation', 'has', 'no', 'fixed', 'points', 'for', 'the', 'usual', 'action', 'of', 'the', 'symmetric', 'group', 'on', 'ksets', 'of', '12n', 'the', 'limit', 'is', 'a', 'polynomial', 'in', 'independent', 'poisson', 'variables', 'this', 'exhausts', 'all', 'cases', 'we', 'obtain', 'asymptotic', 'estimates', 'in', 'some', 'examples', 'and', 'give', 'a', 'survey', 'of', 'related', 'results']] | [-0.16645834783211033, 0.1014927281611698, -0.09898963796985434, 0.05234098747159612, -0.07401795762571249, -0.11835930595531109, 0.0997582343605129, 0.3461915596209942, -0.22647862251416997, -0.21155702968207288, 0.12124945385569826, -0.3295417670160532, -0.12881305733537105, 0.18435534956726304, -0.10772292992159566, 0.021443037282764674, 0.03848390871698552, 0.1579269196223864, -0.11312976208183557, -0.30724171508460285, 0.3223761424392541, -0.004136424910455467, 0.22838241810058343, -0.040955866043000146, 0.10413535885968582, 0.01286226938022895, -0.08777995107378414, -0.0023326630061227603, -0.11661067347604524, 0.07069314663556028, 0.25191212783845024, 0.1081217670982098, 0.26036871728076144, -0.32548301825343207, -0.16285975490934512, 0.22945833654004208, 0.1271508133752232, 0.09439428990578001, -0.039926492387399155, -0.23347280558912045, 0.1377419210930771, -0.15188210861301643, -0.16111936155667014, -0.04881381443602607, 0.060062592373566426, 0.045467515535494114, -0.2821204809253996, -0.018715069282482913, 0.12232097266539138, 0.09154288624391639, -0.02337071313175987, -0.14657099545001984, -0.01330625336181293, 0.16298382387476715, 0.04044329978902131, 0.0025673869828832276, 0.08164679477464389, -0.13011364281880966, -0.12588985470876574, 0.41833135715507447, 0.005966564088049246, -0.257890443416669, 0.15090068735856008, -0.15958748603279285, -0.2057981291696667, 0.1403520678757056, 0.12424140137204147, 0.1583725062416906, -0.09619290303399271, 0.13197122013847778, -0.157980525482228, 0.07393095210600803, 0.10256258578118967, 0.007539970001473309, 0.14932030525573708, 0.10827908569827993, 0.13485369383372328, 0.15976750691473346, -0.013972695225829933, -0.08810916370613144, -0.37036127517832085, -0.11977877971676594, -0.1800552720285734, 0.1049814194718257, -0.16590154871943363, -0.19274605566913144, 0.42014802663408696, 0.08120130172167767, 0.21242433093597202, 0.10512364736976142, 0.19509796637724688, 0.13351245871943204, 0.01866242407444627, 0.09314117981913558, 0.10416119394760748, 0.15856930907776065, -0.03695041948354783, -0.11230753528256406, 0.045328873605962765, 0.10525114494474962] |
708.2644 | Optimal Monotonicity of $L^p$ Integral of Conformal Invariant Green
Function | Both analytic and geometric forms of an optimal monotone principle for
$L^p$-integral of the Green function of a simply-connected planar domain
$\Omega$ with rectifiable simple curve as boundary are established through a
sharp one-dimensional power integral estimate of Riemann-Stieltjes type and the
Huber analytic and geometric isoperimetric inequalities under finiteness of the
positive part of total Gauss curvature of a conformal metric on $\Omega$.
Consequently, new analytic and geometric isoperimetric-type inequalities are
discovered. Furthermore, when applying the geometric principle to
two-dimensional Riemannian manifolds, we find fortunately that $\{0,1\}$-form
of the induced principle is midway between Moser-Trudinger's inequality and
Nash-Sobolev's inequality on complete noncompact boundary-free surfaces, and
yet equivalent to Nash-Sobolev's/Faber-Krahn's
eigenvalue/Heat-kernel-upper-bound/Log-Sobolev's inequality on the surfaces
with finite total Gauss curvature and quadratic area growth.
| math.DG math.FA | both analytic and geometric forms of an optimal monotone principle for lpintegral of the green function of a simplyconnected planar domain omega with rectifiable simple curve as boundary are established through a sharp onedimensional power integral estimate of riemannstieltjes type and the huber analytic and geometric isoperimetric inequalities under finiteness of the positive part of total gauss curvature of a conformal metric on omega consequently new analytic and geometric isoperimetrictype inequalities are discovered furthermore when applying the geometric principle to twodimensional riemannian manifolds we find fortunately that 01form of the induced principle is midway between mosertrudingers inequality and nashsobolevs inequality on complete noncompact boundaryfree surfaces and yet equivalent to nashsobolevsfaberkrahns eigenvalueheatkernelupperboundlogsobolevs inequality on the surfaces with finite total gauss curvature and quadratic area growth | [['both', 'analytic', 'and', 'geometric', 'forms', 'of', 'an', 'optimal', 'monotone', 'principle', 'for', 'lpintegral', 'of', 'the', 'green', 'function', 'of', 'a', 'simplyconnected', 'planar', 'domain', 'omega', 'with', 'rectifiable', 'simple', 'curve', 'as', 'boundary', 'are', 'established', 'through', 'a', 'sharp', 'onedimensional', 'power', 'integral', 'estimate', 'of', 'riemannstieltjes', 'type', 'and', 'the', 'huber', 'analytic', 'and', 'geometric', 'isoperimetric', 'inequalities', 'under', 'finiteness', 'of', 'the', 'positive', 'part', 'of', 'total', 'gauss', 'curvature', 'of', 'a', 'conformal', 'metric', 'on', 'omega', 'consequently', 'new', 'analytic', 'and', 'geometric', 'isoperimetrictype', 'inequalities', 'are', 'discovered', 'furthermore', 'when', 'applying', 'the', 'geometric', 'principle', 'to', 'twodimensional', 'riemannian', 'manifolds', 'we', 'find', 'fortunately', 'that', '01form', 'of', 'the', 'induced', 'principle', 'is', 'midway', 'between', 'mosertrudingers', 'inequality', 'and', 'nashsobolevs', 'inequality', 'on', 'complete', 'noncompact', 'boundaryfree', 'surfaces', 'and', 'yet', 'equivalent', 'to', 'nashsobolevsfaberkrahns', 'eigenvalueheatkernelupperboundlogsobolevs', 'inequality', 'on', 'the', 'surfaces', 'with', 'finite', 'total', 'gauss', 'curvature', 'and', 'quadratic', 'area', 'growth']] | [-0.15487274128215842, 0.06410903840811488, -0.100086102316923, 0.1015993034156008, -0.1408696818584185, -0.15727939145608233, 0.02161184454164585, 0.3359602005064425, -0.2577584822106512, -0.24182008219757625, 0.1501163247417064, -0.2686930181450766, -0.1636541347971241, 0.26107688256179395, -0.13982546485240469, 0.07437157159780755, 0.008969867740906462, 0.052241576686814555, -0.11249001247088324, -0.2400707091760485, 0.40035291341673424, -0.08061818320679814, 0.2351995897792405, 0.14514839957701042, 0.13772422476256357, 0.01398211796650616, -0.00022087416791615366, 0.06536042804931518, -0.2463921182576744, 0.20068519266259646, 0.19323356048117915, 0.06619461761599704, 0.21917942081805036, -0.40816364726912574, -0.20007660254022153, 0.15532783602419145, 0.07020942130157364, -0.02493339468638937, -0.04413614277884427, -0.29160855588417095, 0.029767897372337513, -0.02641580599759306, -0.19264783990812026, -0.07182979038251298, 0.03677737168936419, 0.030836905472610584, -0.24766117119926864, 0.1322925654122559, 0.11261115559697651, 0.0880993428784853, -0.09543860329416808, -0.08315190657808938, -0.05520348801441929, 0.04848714014676697, 0.027217679553344344, 0.06453373519891575, 0.07454798118986126, -0.04029086707629451, -0.07289884968058151, 0.28082582914904386, -0.08100058361027046, -0.24800094101233644, 0.09265817891994194, -0.16322837859204337, -0.10699501650861833, 0.10023968360003303, 0.14171985501595655, 0.15995948285964012, -0.14290727400908174, 0.17131801096364432, -0.042532881325650806, 0.062313641370381735, 0.1417272908519171, 0.0017585943985198224, 0.11470781175904915, 0.03084093886975418, 0.1982937432559473, 0.18254860783261911, -0.018543579780003604, -0.10469677342696726, -0.4084781449241172, -0.20586620854260793, -0.20682683647336328, 0.16266949196099578, -0.18100515584289703, -0.206990102685581, 0.3187607031299913, -0.07775196233754997, 0.13676953813483736, 0.1373288450809587, 0.24200155150865307, 0.10982438808350097, 0.04771621771031568, 0.059006250612124674, 0.19641081608456223, 0.24067676341466354, 0.027868437439891973, -0.1763685510039893, -0.029700879770636308, 0.15441768893878124] |
708.2645 | The Toomre Sequence Revisited with HST/NICMOS: Nuclear Brightness
Profiles and Colors of Interacting and Merging Galaxies | We discuss the near-infrared properties of the nuclei in the 11 merging
galaxies of the Toomre sequence, based on high spatial resolution J, H, and K
imaging data using NICMOS onboard the Hubble Space Telescope (HST). The
observations are less affected by dust extinction than our previous HST/WFPC2
observations and offer higher spatial resolution than existing ground-based
near-IR data. We see a marginal trend for the nuclei to become bluer with
advancing merger stage, which we attribute to a dispersal of dust at late times
in the merging process. Our data also indicate a statistically significant
trend for the nuclei in the sequence to become more luminous, within an
aperture of fixed physical size and after correcting for dust extinction, with
advancing merger stage. We derive K-band surface brightness profiles for those
nuclei for which the morphology allows a meaningful isophotal analysis, and fit
the profiles with a ``Nuker law'' for comparison with other samples of galaxies
observed with HST. The majority of the nuclei have steep profiles that can be
characterized as power-law type. In general, the Toomre sequence galaxies tend
to have steeper profiles and higher central luminosity surface densities than
E/S0's. We derive V-K color profiles for the nuclei to further address this
possibility, but find that the large amounts of dust extinction complicate
their interpretation. Overall, our results are consistent with the generic
predictions of N-body simulations of spiral galaxy mergers. If left to evolve
and fade for several Gyrs, it is possible that the properties of the Toomre
sequence nuclei would resemble theproperties of the nuclei of normal E/S0
galaxies. Our results therefore support the view that mergers of spiral
galaxies can lead to the formation of early-type galaxies (Abridged).
| astro-ph | we discuss the nearinfrared properties of the nuclei in the 11 merging galaxies of the toomre sequence based on high spatial resolution j h and k imaging data using nicmos onboard the hubble space telescope hst the observations are less affected by dust extinction than our previous hstwfpc2 observations and offer higher spatial resolution than existing groundbased nearir data we see a marginal trend for the nuclei to become bluer with advancing merger stage which we attribute to a dispersal of dust at late times in the merging process our data also indicate a statistically significant trend for the nuclei in the sequence to become more luminous within an aperture of fixed physical size and after correcting for dust extinction with advancing merger stage we derive kband surface brightness profiles for those nuclei for which the morphology allows a meaningful isophotal analysis and fit the profiles with a nuker law for comparison with other samples of galaxies observed with hst the majority of the nuclei have steep profiles that can be characterized as powerlaw type in general the toomre sequence galaxies tend to have steeper profiles and higher central luminosity surface densities than es0s we derive vk color profiles for the nuclei to further address this possibility but find that the large amounts of dust extinction complicate their interpretation overall our results are consistent with the generic predictions of nbody simulations of spiral galaxy mergers if left to evolve and fade for several gyrs it is possible that the properties of the toomre sequence nuclei would resemble theproperties of the nuclei of normal es0 galaxies our results therefore support the view that mergers of spiral galaxies can lead to the formation of earlytype galaxies abridged | [['we', 'discuss', 'the', 'nearinfrared', 'properties', 'of', 'the', 'nuclei', 'in', 'the', '11', 'merging', 'galaxies', 'of', 'the', 'toomre', 'sequence', 'based', 'on', 'high', 'spatial', 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708.2646 | Constraining axion by polarized prompt emission from gamma ray bursts | A polarized gamma ray emission spread over a sufficiently wide energy band
from a strongly magnetized astrophysical object like gamma ray bursts (GRBs)
offers an opportunity to test the hypothesis of invisible axion. The axionic
induced dichroism of gamma rays at different energies should cause a
misalignment of the polarization plane for higher energy events relative to
that one for lower energies events resulting in the loss of statistics needed
to form a pattern of the polarization signal to be recognized in a detector.
According to this, any evidence of polarized gamma rays coming from an object
with extended magnetic field could be interpreted as a constraint on the
existence of the invisible axion for a certain parameter range. Based on
reports of polarized MeV emission detected in several GRBs we derive a
constraint on the axion-photon coupling. This constraint $\g_{a\gamma\gamma}\le
2.2\cdot 10^{-11} {\rm GeV^{-1}}$ calculated for the axion mass $m_a=10^{-3}
{\rm eV}$ is competitive with the sensitivity of CAST and becomes even stronger
for lower masses.
| hep-ph astro-ph gr-qc hep-th | a polarized gamma ray emission spread over a sufficiently wide energy band from a strongly magnetized astrophysical object like gamma ray bursts grbs offers an opportunity to test the hypothesis of invisible axion the axionic induced dichroism of gamma rays at different energies should cause a misalignment of the polarization plane for higher energy events relative to that one for lower energies events resulting in the loss of statistics needed to form a pattern of the polarization signal to be recognized in a detector according to this any evidence of polarized gamma rays coming from an object with extended magnetic field could be interpreted as a constraint on the existence of the invisible axion for a certain parameter range based on reports of polarized mev emission detected in several grbs we derive a constraint on the axionphoton coupling this constraint g_agammagammale 22cdot 1011 rm gev1 calculated for the axion mass m_a103 rm ev is competitive with the sensitivity of cast and becomes even stronger for lower masses | [['a', 'polarized', 'gamma', 'ray', 'emission', 'spread', 'over', 'a', 'sufficiently', 'wide', 'energy', 'band', 'from', 'a', 'strongly', 'magnetized', 'astrophysical', 'object', 'like', 'gamma', 'ray', 'bursts', 'grbs', 'offers', 'an', 'opportunity', 'to', 'test', 'the', 'hypothesis', 'of', 'invisible', 'axion', 'the', 'axionic', 'induced', 'dichroism', 'of', 'gamma', 'rays', 'at', 'different', 'energies', 'should', 'cause', 'a', 'misalignment', 'of', 'the', 'polarization', 'plane', 'for', 'higher', 'energy', 'events', 'relative', 'to', 'that', 'one', 'for', 'lower', 'energies', 'events', 'resulting', 'in', 'the', 'loss', 'of', 'statistics', 'needed', 'to', 'form', 'a', 'pattern', 'of', 'the', 'polarization', 'signal', 'to', 'be', 'recognized', 'in', 'a', 'detector', 'according', 'to', 'this', 'any', 'evidence', 'of', 'polarized', 'gamma', 'rays', 'coming', 'from', 'an', 'object', 'with', 'extended', 'magnetic', 'field', 'could', 'be', 'interpreted', 'as', 'a', 'constraint', 'on', 'the', 'existence', 'of', 'the', 'invisible', 'axion', 'for', 'a', 'certain', 'parameter', 'range', 'based', 'on', 'reports', 'of', 'polarized', 'mev', 'emission', 'detected', 'in', 'several', 'grbs', 'we', 'derive', 'a', 'constraint', 'on', 'the', 'axionphoton', 'coupling', 'this', 'constraint', 'g_agammagammale', '22cdot', '1011', 'rm', 'gev1', 'calculated', 'for', 'the', 'axion', 'mass', 'm_a103', 'rm', 'ev', 'is', 'competitive', 'with', 'the', 'sensitivity', 'of', 'cast', 'and', 'becomes', 'even', 'stronger', 'for', 'lower', 'masses']] | [-0.13664408327682262, 0.20077974127663056, -0.057932846614432223, 0.150172700654721, -0.10310615019013157, -0.0710946050211333, 0.059034166752542486, 0.3916670137493894, -0.22944253468573683, -0.36329650038444417, 0.015092325562230743, -0.26626458253268515, 0.018720878958247783, 0.2653214272406952, 0.045027012028163525, -0.012645588980465219, 0.0341290791934958, 0.025123915987134707, -0.059858813819407324, -0.15136964789328375, 0.26490842986982543, 0.12071430258645971, 0.21878057733609726, 0.07854172812842923, 0.08324742187297245, -0.014750116127088847, 0.014299769238455266, -0.017836638267420688, -0.1048253987131519, 0.08555764493975425, 0.22941965308812698, 0.09331716001374511, 0.15688777452039465, -0.36246988714513617, -0.21790532797870293, 0.16062119065942923, 0.09517742067904825, 0.03212281826936084, -0.07935671477575741, -0.30236867653197474, 0.08291037289550664, -0.16291785327058922, -0.13392990522893009, 0.05207912653695974, 0.016346601287340293, -0.006721588862469283, -0.29127765145357243, 0.057757850798846384, 0.021799098640879425, -0.00966372898291433, -0.06738399353769903, -0.10958239925377888, -0.011943741738455506, 0.018957425016773548, 0.12140088165377654, 0.0932854102042833, 0.15737847931876142, -0.156404394593953, -0.10253371139022908, 0.4336392782832973, -0.11784181881854992, -0.11215968471497478, 0.15449462295083966, -0.17717073075246156, -0.15679709826845947, 0.250124549260363, 0.20852610132395766, 0.10942971376878233, -0.12454241399139325, 0.07949600092003338, -0.013991476042287015, 0.2062363258332991, 0.0882552968644787, 0.0569402214917695, 0.30698523222093993, 0.14986560486893102, 0.09004400704459219, 0.08758938080125783, -0.16497638168966217, 0.03788689870625825, -0.3182969331434678, -0.10608934261197248, -0.1356878865619542, 0.13414449810913606, -0.08744006883486091, -0.13028480562313302, 0.36206606457651613, 0.10830153752169458, 0.20447053844744492, 0.011733498234051938, 0.25964105693430345, 0.11020352602751766, 0.04918498531120216, 0.03300770358807158, 0.3357925775529044, 0.14261261737201272, 0.07402232079695706, -0.19625001168162448, 0.025834273356694457, -0.01988016854312907] |
708.2647 | Mirror symmetry breaking as a problem in dynamical critical phenomena | The critical properties of the Frank model of spontaneous chiral synthesis
are discussed by applying results from the field theoretic renormalization
group (RG). The long time and long wavelength features of this microscopic
reaction scheme belong to the same universality class as multi-colored directed
percolation processes. Thus, the following RG fixed points (FP) govern the
critical dynamics of the Frank model for d<4: one unstable FP that corresponds
to complete decoupling between the two enantiomers, a saddle-point that
corresponds to symmetric interspecies coupling, and two stable FPs that
individually correspond to unidirectional couplings between the two chiral
molecules. These latter two FPs are associated with the breakdown of mirror or
chiral symmetry. In this simplified model of molecular synthesis, homochirality
is a natural consequence of the intrinsic reaction noise in the critical
regime, which corresponds to extremely dilute chemical systems.
| q-bio.PE cond-mat.stat-mech | the critical properties of the frank model of spontaneous chiral synthesis are discussed by applying results from the field theoretic renormalization group rg the long time and long wavelength features of this microscopic reaction scheme belong to the same universality class as multicolored directed percolation processes thus the following rg fixed points fp govern the critical dynamics of the frank model for d4 one unstable fp that corresponds to complete decoupling between the two enantiomers a saddlepoint that corresponds to symmetric interspecies coupling and two stable fps that individually correspond to unidirectional couplings between the two chiral molecules these latter two fps are associated with the breakdown of mirror or chiral symmetry in this simplified model of molecular synthesis homochirality is a natural consequence of the intrinsic reaction noise in the critical regime which corresponds to extremely dilute chemical systems | [['the', 'critical', 'properties', 'of', 'the', 'frank', 'model', 'of', 'spontaneous', 'chiral', 'synthesis', 'are', 'discussed', 'by', 'applying', 'results', 'from', 'the', 'field', 'theoretic', 'renormalization', 'group', 'rg', 'the', 'long', 'time', 'and', 'long', 'wavelength', 'features', 'of', 'this', 'microscopic', 'reaction', 'scheme', 'belong', 'to', 'the', 'same', 'universality', 'class', 'as', 'multicolored', 'directed', 'percolation', 'processes', 'thus', 'the', 'following', 'rg', 'fixed', 'points', 'fp', 'govern', 'the', 'critical', 'dynamics', 'of', 'the', 'frank', 'model', 'for', 'd4', 'one', 'unstable', 'fp', 'that', 'corresponds', 'to', 'complete', 'decoupling', 'between', 'the', 'two', 'enantiomers', 'a', 'saddlepoint', 'that', 'corresponds', 'to', 'symmetric', 'interspecies', 'coupling', 'and', 'two', 'stable', 'fps', 'that', 'individually', 'correspond', 'to', 'unidirectional', 'couplings', 'between', 'the', 'two', 'chiral', 'molecules', 'these', 'latter', 'two', 'fps', 'are', 'associated', 'with', 'the', 'breakdown', 'of', 'mirror', 'or', 'chiral', 'symmetry', 'in', 'this', 'simplified', 'model', 'of', 'molecular', 'synthesis', 'homochirality', 'is', 'a', 'natural', 'consequence', 'of', 'the', 'intrinsic', 'reaction', 'noise', 'in', 'the', 'critical', 'regime', 'which', 'corresponds', 'to', 'extremely', 'dilute', 'chemical', 'systems']] | [-0.14988222585192748, 0.18491025244584308, -0.08130367375269998, 0.04620079436322807, -0.030584458536135832, -0.16899139819932835, 0.043417996793453185, 0.34843110559242113, -0.26945642147080173, -0.2509868235817911, 0.04823314422808055, -0.23961910836265554, -0.1378674117798385, 0.11147892382661147, 0.025121890893206, 0.049529288411473055, -0.03605569141052131, 0.030086060001381806, -0.0419490035972558, -0.17524557828104922, 0.3133096754817026, -0.002294440693887217, 0.29368085859210363, 0.03491246237702269, 0.07121686110206481, -0.016438094639618483, 0.04949380083375477, -0.020463088610475615, -0.11654704235339262, 0.07742426187032833, 0.22792444937263748, -0.0010385975374707153, 0.20390553091918784, -0.4156105365737208, -0.2176898983440229, 0.10392031121965764, 0.1287019339589668, 0.1611045372830371, -0.032756428304336234, -0.2640973649586418, 0.08141986037537988, -0.12861225461820142, -0.16956230012833007, -0.025126292175679868, 0.03049473840759934, 0.01542655916086265, -0.2493066708956446, 0.09350527939885589, 0.08069006457434236, 0.06605621720830511, -0.04808760252115982, -0.08129369288549891, -0.07549879187593303, 0.13877359590925542, 0.05998044988456448, 0.022301615948007177, 0.14130937291858053, -0.14962503885118558, -0.12782247767484348, 0.4139610874000937, -0.06391500571376778, -0.14442972730279768, 0.21945192280358503, -0.08872826237431063, -0.14972889724387123, 0.18504044454311952, 0.11691927375504747, 0.11479184433950909, -0.14433102928368108, 0.08359424001121495, -0.03872632244269231, 0.14671693040457154, 0.08413117694269334, 0.012563344676579748, 0.21184918735442418, 0.17292877400094378, 0.049385524873754805, 0.10690847290513505, -0.042975202984858435, -0.19907258523661378, -0.3242509992044818, -0.09772438144178262, -0.14305764240811447, 0.07414719065085852, -0.11640439045794275, -0.14435219654281226, 0.3861540557775827, 0.15900387426040002, 0.2044391137680837, 0.030326457540338327, 0.21458049822332603, 0.1040295851990647, 0.06955402768882257, 0.007522660077665932, 0.25564250078584466, 0.16442175166448578, 0.05551896440530462, -0.30203357813380927, -0.0009830821530028646, 0.11515724420314655] |
708.2648 | Noncommutative correspondences, duality and D-branes in bivariant
K-theory | We describe a categorical framework for the classification of D-branes on
noncommutative spaces using techniques from bivariant K-theory of C*-algebras.
We present a new description of bivariant K-theory in terms of noncommutative
correspondences which is nicely adapted to the study of T-duality in open
string theory. We systematically use the diagram calculus for bivariant
K-theory as detailed in our previous paper. We explicitly work out our theory
for a number of examples of noncommutative manifolds.
| hep-th math.KT | we describe a categorical framework for the classification of dbranes on noncommutative spaces using techniques from bivariant ktheory of calgebras we present a new description of bivariant ktheory in terms of noncommutative correspondences which is nicely adapted to the study of tduality in open string theory we systematically use the diagram calculus for bivariant ktheory as detailed in our previous paper we explicitly work out our theory for a number of examples of noncommutative manifolds | [['we', 'describe', 'a', 'categorical', 'framework', 'for', 'the', 'classification', 'of', 'dbranes', 'on', 'noncommutative', 'spaces', 'using', 'techniques', 'from', 'bivariant', 'ktheory', 'of', 'calgebras', 'we', 'present', 'a', 'new', 'description', 'of', 'bivariant', 'ktheory', 'in', 'terms', 'of', 'noncommutative', 'correspondences', 'which', 'is', 'nicely', 'adapted', 'to', 'the', 'study', 'of', 'tduality', 'in', 'open', 'string', 'theory', 'we', 'systematically', 'use', 'the', 'diagram', 'calculus', 'for', 'bivariant', 'ktheory', 'as', 'detailed', 'in', 'our', 'previous', 'paper', 'we', 'explicitly', 'work', 'out', 'our', 'theory', 'for', 'a', 'number', 'of', 'examples', 'of', 'noncommutative', 'manifolds']] | [-0.10014968814328312, 0.019988631730278334, -0.15558004441360632, 0.15421691530228904, -0.08203365786621968, -0.09938811210915446, 0.027928027034116287, 0.3640441564718882, -0.29983086287975313, -0.24707041719307501, 0.056440117397966484, -0.1956760282300335, -0.22479386049012343, 0.20677106149494648, -0.25435391658296186, -0.006615209579467774, 0.032599498803416886, 0.049202078205222884, -0.1447669764670233, -0.2540688650930921, 0.4687653270487984, 0.010925440850357215, 0.22170644379531343, 0.04488266673559944, 0.05069651044905186, 0.041718470755343635, -0.07725417687712859, 0.029967331718653442, -0.18546780857567985, 0.19946705769592274, 0.3599688217882067, 0.06812348938857515, 0.14151463679969312, -0.39841291688382624, -0.17260031604518494, 0.08896339738120636, 0.12163817496349415, 0.10974894891648243, -0.022294082661780217, -0.3225332332029939, 0.062312441281974315, -0.2539575765033563, -0.08029206683238348, -0.20245525370041528, 0.02205330381790797, -0.025191983695452412, -0.184791311606726, -0.04627617476508021, 0.06834842294454574, 0.16080091081559658, -0.11690189349154631, -0.0021505128716429074, -0.004457349398483833, 0.10027980726212263, 0.011316854267691573, 0.046780289780969424, 0.1217278514864544, -0.06625328704714775, -0.20997158737309898, 0.3435713122288386, -0.053968896865844725, -0.19495529549817245, 0.11248435995541513, -0.10511030413210393, -0.2957926145506402, 0.07005910744269689, 0.06601656533777714, 0.24074394142255187, -0.04855954986065626, 0.224520024775217, -0.11763250942031543, 0.08212878776869426, 0.04787156524447103, 0.04878918037128945, 0.16634141822655996, 0.12445049131910006, 0.010956695129474003, 0.18103645662466686, 0.028654596647247673, -0.12368136147890861, -0.39827716891964277, -0.18719264281292755, -0.05931184640464683, 0.13321660491482665, -0.09963441264505188, -0.19550797854860624, 0.44629443672796093, 0.16547235184659562, 0.16719506487250327, 0.1251003883111601, 0.2644924574966232, 0.030454353468182187, -0.0014022963990767796, -0.0243102786069115, 0.1253180144308135, 0.24641747088481983, 0.08129032931601007, -0.11716220423734436, -0.14281276389335593, 0.2793865850257377] |
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