id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
707.313 | Angular momentum projection of cranked Hartree-Fock states: Application
to terminating bands in A~44 nuclei | We present the first systematic calculations based on the angular-momentum
projection of cranked Slater determinants. We propose the Iy --> I scheme, by
which one projects the angular momentum I from the 1D cranked state constrained
to the average spin projection of <I_y>=I. Calculations performed for the
rotational ... | nucl-th | we present the first systematic calculations based on the angularmomentum projection of cranked slater determinants we propose the iy i scheme by which one projects the angular momentum i from the 1d cranked state constrained to the average spin projection of i_yi calculations performed for the rotational band in 46ti ... | [['we', 'present', 'the', 'first', 'systematic', 'calculations', 'based', 'on', 'the', 'angularmomentum', 'projection', 'of', 'cranked', 'slater', 'determinants', 'we', 'propose', 'the', 'iy', 'i', 'scheme', 'by', 'which', 'one', 'projects', 'the', 'angular', 'momentum', 'i', 'from', 'the', '1d', 'cranked', 'state', 'c... | [-0.08074038456962035, 0.08377373108248178, -0.07760929113883003, 0.05216500944388507, 0.0035022682019636, -0.11699655284010396, 0.11921660189992715, 0.39356236267638833, -0.21336783431960563, -0.27841003729733066, 0.028994744877420823, -0.26503432747140004, -0.06779684273428038, 0.14487709465493823, 0.0215153381587904... |
707.3131 | Dynamics of Bloch Oscillations in Disordered Lattice Potentials | We present a detailed analysis of the dynamics of Bloch oscillations of
Bose-Einstein condensates in disordered lattice potentials. Due to the disorder
and the interparticle interactions these oscillations undergo a dephasing,
reflected in a damping of the center of mass oscillations, which should be
observable under... | cond-mat.other cond-mat.dis-nn | we present a detailed analysis of the dynamics of bloch oscillations of boseeinstein condensates in disordered lattice potentials due to the disorder and the interparticle interactions these oscillations undergo a dephasing reflected in a damping of the center of mass oscillations which should be observable under reali... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'the', 'dynamics', 'of', 'bloch', 'oscillations', 'of', 'boseeinstein', 'condensates', 'in', 'disordered', 'lattice', 'potentials', 'due', 'to', 'the', 'disorder', 'and', 'the', 'interparticle', 'interactions', 'these', 'oscillations', 'undergo', 'a', 'dephasing', '... | [-0.21072919486112981, 0.2633426821182611, -0.09834118669849809, 0.09066613757539631, -0.028767038549083364, -0.1140576930988737, 0.03176189070084996, 0.30065190442557255, -0.2938280571925353, -0.23406429633677725, 0.0368977178818075, -0.3005633675773819, -0.1544043288891574, 0.15869462421074151, 0.049286940864410746, ... |
707.3132 | The Dark Side of ROTSE-III Prompt GRB Observations | We present several cases of optical observations during gamma-ray bursts
(GRBs) which resulted in prompt limits but no detection of optical emission.
These limits constrain the prompt optical flux densities and the optical
brightness relative to the gamma-ray emission. The derived constraints fall
within the range of... | astro-ph | we present several cases of optical observations during gammaray bursts grbs which resulted in prompt limits but no detection of optical emission these limits constrain the prompt optical flux densities and the optical brightness relative to the gammaray emission the derived constraints fall within the range of propert... | [['we', 'present', 'several', 'cases', 'of', 'optical', 'observations', 'during', 'gammaray', 'bursts', 'grbs', 'which', 'resulted', 'in', 'prompt', 'limits', 'but', 'no', 'detection', 'of', 'optical', 'emission', 'these', 'limits', 'constrain', 'the', 'prompt', 'optical', 'flux', 'densities', 'and', 'the', 'optical', ... | [-0.03981891447897959, 0.14644026357596845, -0.014989860601765052, 0.14924673507973718, -0.09854505034268238, -0.073739091222164, 0.08235768033871742, 0.5060676958704933, -0.14356704895499717, -0.3473635632544756, 0.050799509581031924, -0.32621459661867847, 0.06743485693757036, 0.2554607603874246, 0.0016214459993238194... |
707.3133 | Evidence for Three Subpopulations of Globular Clusters in the Early-Type
Post-Starburst Shell Galaxy AM 0139-655 | We present deep HST ACS images of the post-starburt shell galaxy AM 0139-655.
We find evidence for the presence of three distinct globular cluster
subpopulations associated with this galaxy: a centrally concentrated young
population (~ 0.4 Gyr), an intermediate age population (~ 1 Gyr) and an old,
metal-poor populati... | astro-ph | we present deep hst acs images of the poststarburt shell galaxy am 0139655 we find evidence for the presence of three distinct globular cluster subpopulations associated with this galaxy a centrally concentrated young population 04 gyr an intermediate age population 1 gyr and an old metalpoor population similar to that... | [['we', 'present', 'deep', 'hst', 'acs', 'images', 'of', 'the', 'poststarburt', 'shell', 'galaxy', 'am', '0139655', 'we', 'find', 'evidence', 'for', 'the', 'presence', 'of', 'three', 'distinct', 'globular', 'cluster', 'subpopulations', 'associated', 'with', 'this', 'galaxy', 'a', 'centrally', 'concentrated', 'young', '... | [-0.019228572338099846, 0.12787489500609095, -0.11190899225095144, 0.1337219625520129, -0.06303426007594884, -0.06419544607576738, 0.038849792601964014, 0.4423170989066675, -0.15057538388707264, -0.35829224114768676, 0.013307457048139841, -0.2954731313727464, -0.029709588302384047, 0.17335239496209065, -0.0830291239756... |
707.3134 | Photon emission rate from atomic systems in the CSL model | We calculate the photon emission rate from a general atomic system in the
mass- proportional CSL model. For an isolated charged particle emitting
kilovolt gamma rays, our results agree with those obtained by Fu. For a neutral
atomic system, photon emission is strongly suppressed for photon wavelengths
much larger tha... | quant-ph astro-ph hep-ph hep-th | we calculate the photon emission rate from a general atomic system in the mass proportional csl model for an isolated charged particle emitting kilovolt gamma rays our results agree with those obtained by fu for a neutral atomic system photon emission is strongly suppressed for photon wavelengths much larger than the a... | [['we', 'calculate', 'the', 'photon', 'emission', 'rate', 'from', 'a', 'general', 'atomic', 'system', 'in', 'the', 'mass', 'proportional', 'csl', 'model', 'for', 'an', 'isolated', 'charged', 'particle', 'emitting', 'kilovolt', 'gamma', 'rays', 'our', 'results', 'agree', 'with', 'those', 'obtained', 'by', 'fu', 'for', '... | [-0.08007038821184523, 0.19781544838238121, -0.01599972294017422, 0.12003954588787771, -0.017918405385234027, -0.13808599580079317, 0.019849462841613954, 0.3690961778883924, -0.18760419147042165, -0.2885765798757745, 0.04068116027717048, -0.30716949012600075, -0.058284702145361474, 0.24801009976864644, 0.02256497378781... |
707.3135 | Stress Tensor of Static Dipoles in strongly coupled $\cal{N}$=4 Gauge
Theory | In the context of the AdS/CFT correspondence we calculate the induced stress
tensor of static dipoles (electric-electric and electric-magnetic) in a
strongly coupled ${\cal N}=4$ SYM gauge theory, by solving the linearized
Einstein equation with Maldecena string as a source. Analytic expressions are
given for the far... | hep-th | in the context of the adscft correspondence we calculate the induced stress tensor of static dipoles electricelectric and electricmagnetic in a strongly coupled cal n4 sym gauge theory by solving the linearized einstein equation with maldecena string as a source analytic expressions are given for the farfield and a nea... | [['in', 'the', 'context', 'of', 'the', 'adscft', 'correspondence', 'we', 'calculate', 'the', 'induced', 'stress', 'tensor', 'of', 'static', 'dipoles', 'electricelectric', 'and', 'electricmagnetic', 'in', 'a', 'strongly', 'coupled', 'cal', 'n4', 'sym', 'gauge', 'theory', 'by', 'solving', 'the', 'linearized', 'einstein',... | [-0.12764679352985694, 0.18488835034659132, -0.06438085618428886, 0.07216389088425786, -0.06428848640061915, -0.16938761787023396, -0.056046719635196494, 0.33954164244933055, -0.189421278637019, -0.22842143507441506, 0.044993655540747565, -0.3147445433132816, -0.15119271108414978, 0.12187320388620719, 0.010642193630337... |
707.3136 | Towards an analytical theory for charged hard spheres | Ion mixtures require an exclusion core to avoid collapse. The Debye Hueckel
theory, where ions are point charges, is accurate only in the limit of infinite
dilution. The MSA is the embedding of hard cores into DH, is valid for higher
densities. In the MSA the properties of any ionic mixture can be represented by
a si... | cond-mat.soft cond-mat.stat-mech | ion mixtures require an exclusion core to avoid collapse the debye hueckel theory where ions are point charges is accurate only in the limit of infinite dilution the msa is the embedding of hard cores into dh is valid for higher densities in the msa the properties of any ionic mixture can be represented by a single scr... | [['ion', 'mixtures', 'require', 'an', 'exclusion', 'core', 'to', 'avoid', 'collapse', 'the', 'debye', 'hueckel', 'theory', 'where', 'ions', 'are', 'point', 'charges', 'is', 'accurate', 'only', 'in', 'the', 'limit', 'of', 'infinite', 'dilution', 'the', 'msa', 'is', 'the', 'embedding', 'of', 'hard', 'cores', 'into', 'dh'... | [-0.08897432475674173, 0.1881798054909167, -0.04365279197938637, 0.06056774190397442, -0.02721564606084333, -0.14326306085826623, 0.06593976959185158, 0.3142304538745925, -0.21505140910287285, -0.28006867063878516, 0.012731670494152544, -0.28689727251831854, -0.04275680863712397, 0.15067845611257427, -0.011312591409983... |
707.3137 | Accurate theoretical fits to laser ARPES EDCs in the normal phase of
cuprate superconductors | Anderson has recently proposed a theory of the strange metal state above Tc
in the high Tc superconductors. [arXiv:cond-mat/0512471] It is based on the
idea that the unusual transport properties and spectral functions are caused by
the strong Mott- Hubbard interactions and can be computed by using the formal
apparatu... | cond-mat.str-el cond-mat.supr-con | anderson has recently proposed a theory of the strange metal state above tc in the high tc superconductors arxivcondmat0512471 it is based on the idea that the unusual transport properties and spectral functions are caused by the strong mott hubbard interactions and can be computed by using the formal apparatus of gutz... | [['anderson', 'has', 'recently', 'proposed', 'a', 'theory', 'of', 'the', 'strange', 'metal', 'state', 'above', 'tc', 'in', 'the', 'high', 'tc', 'superconductors', 'arxivcondmat0512471', 'it', 'is', 'based', 'on', 'the', 'idea', 'that', 'the', 'unusual', 'transport', 'properties', 'and', 'spectral', 'functions', 'are', ... | [-0.06409731977974945, 0.14066334483989826, -0.12082346015288042, 0.08554554664927612, -0.031717748950743245, -0.16539034131953181, 0.08709473591281697, 0.4033720100479614, -0.24761483256265315, -0.31688882345204344, 0.020563537800626364, -0.3276642164694042, -0.10115094588011037, 0.17962243489980917, -0.02445255130846... |
707.3138 | ACM sets of points in multiprojective space | If X is a finite set of points in a multiprojective space P^n1 x ... x P^nr
with r >= 2, then X may or may not be arithmetically Cohen-Macaulay (ACM). For
sets of points in P^1 x P^1 there are several classifications of the ACM sets
of points. In this paper we investigate the natural generalizations of these
classifi... | math.AC math.AG | if x is a finite set of points in a multiprojective space pn1 x x pnr with r 2 then x may or may not be arithmetically cohenmacaulay acm for sets of points in p1 x p1 there are several classifications of the acm sets of points in this paper we investigate the natural generalizations of these classifications to an arbit... | [['if', 'x', 'is', 'a', 'finite', 'set', 'of', 'points', 'in', 'a', 'multiprojective', 'space', 'pn1', 'x', 'x', 'pnr', 'with', 'r', '2', 'then', 'x', 'may', 'or', 'may', 'not', 'be', 'arithmetically', 'cohenmacaulay', 'acm', 'for', 'sets', 'of', 'points', 'in', 'p1', 'x', 'p1', 'there', 'are', 'several', 'classificati... | [-0.19142779459555945, 0.02656091262972702, -0.06980809615454589, 0.05449742427791911, -0.01553708934601434, -0.15205742716507026, 0.07373685340251247, 0.39821513036661077, -0.2954887499788193, -0.1656688427307991, 0.13799821868576487, -0.2694232890928032, -0.11909507905165995, 0.19341446893675385, -0.17962886181406, 0... |
707.3139 | Separators of points in a multiprojective space | In this note we develop some of the properties of separators of points in a
multiprojective space. In particular, we prove multigraded analogs of results
of Geramita, Maroscia, and Roberts relating the Hilbert function of X and X
\{P} via the degree of a separator, and Abrescia, Bazzotti, and Marino relating
the degr... | math.AC math.AG | in this note we develop some of the properties of separators of points in a multiprojective space in particular we prove multigraded analogs of results of geramita maroscia and roberts relating the hilbert function of x and x p via the degree of a separator and abrescia bazzotti and marino relating the degree of a sepa... | [['in', 'this', 'note', 'we', 'develop', 'some', 'of', 'the', 'properties', 'of', 'separators', 'of', 'points', 'in', 'a', 'multiprojective', 'space', 'in', 'particular', 'we', 'prove', 'multigraded', 'analogs', 'of', 'results', 'of', 'geramita', 'maroscia', 'and', 'roberts', 'relating', 'the', 'hilbert', 'function', '... | [-0.17328451139231524, 0.07313688819748208, -0.09027760998684574, 0.032569099547496684, -0.0007347810209136118, -0.048592212250117554, 0.061643239362941436, 0.3008157450381215, -0.317826291151119, -0.23934622950654363, 0.06617683525705202, -0.25233046214491356, -0.12256906791166826, 0.170064607748028, -0.13182040098631... |
707.314 | Interaction-controlled transport of an ultracold Fermi gas | We explore the transport properties of an interacting Fermi gas in a
three-dimensional optical lattice. The center of mass dynamics of the atoms
after a sudden displacement of the trap minimum is monitored for different
interaction strengths and lattice fillings. With increasingly strong attractive
interactions the w... | cond-mat.str-el quant-ph | we explore the transport properties of an interacting fermi gas in a threedimensional optical lattice the center of mass dynamics of the atoms after a sudden displacement of the trap minimum is monitored for different interaction strengths and lattice fillings with increasingly strong attractive interactions the weakly... | [['we', 'explore', 'the', 'transport', 'properties', 'of', 'an', 'interacting', 'fermi', 'gas', 'in', 'a', 'threedimensional', 'optical', 'lattice', 'the', 'center', 'of', 'mass', 'dynamics', 'of', 'the', 'atoms', 'after', 'a', 'sudden', 'displacement', 'of', 'the', 'trap', 'minimum', 'is', 'monitored', 'for', 'differe... | [-0.17773347977552237, 0.2195390906622744, -0.04376276111592246, 0.028747062393409763, -0.006676283865541655, -0.12872380489673818, 0.07877203197826896, 0.3325979006561675, -0.2921595621351017, -0.2820827913246233, 0.0033596603745377086, -0.28339381783161427, -0.055328097221625114, 0.14930425048635823, 0.06573909248504... |
707.3141 | The Nature of CO Emission From z~6 Quasars | We investigate the nature of CO emission from z~6 quasars by combining
non-LTE radiative transfer calculations with merger-driven models of z~6 quasar
formation that arise naturally in LCDM cosmological simulations. We consider
four model quasars formed in 10^12-10^13 M_sun halos from different merging
histories. Our... | astro-ph | we investigate the nature of co emission from z6 quasars by combining nonlte radiative transfer calculations with mergerdriven models of z6 quasar formation that arise naturally in lcdm cosmological simulations we consider four model quasars formed in 10121013 m_sun halos from different merging histories our main resul... | [['we', 'investigate', 'the', 'nature', 'of', 'co', 'emission', 'from', 'z6', 'quasars', 'by', 'combining', 'nonlte', 'radiative', 'transfer', 'calculations', 'with', 'mergerdriven', 'models', 'of', 'z6', 'quasar', 'formation', 'that', 'arise', 'naturally', 'in', 'lcdm', 'cosmological', 'simulations', 'we', 'consider',... | [-0.038422181729914316, 0.08398107359264519, 0.025947767439786946, 0.11170730574636943, -0.07352369114786098, -0.09730373796331368, 0.01759900131695707, 0.4985058822408384, -0.10517402949704441, -0.3148280791971098, 0.004128834154394547, -0.29676869748457224, 0.04629200122308504, 0.16234458254118989, 0.0785760377893125... |
707.3142 | The Accretion Geometry in Radio-Loud Active Galaxies | We review the latest attempts to determine the accretion geometry in
radio-loud active galactic nuclei (AGN). These objects, which comprise ~10-20%
of the AGN population, produce powerful collimated radio jets that can extend
thousands of parsecs from the center of the host galaxy. Recent multiwavelength
surveys have... | astro-ph | we review the latest attempts to determine the accretion geometry in radioloud active galactic nuclei agn these objects which comprise 1020 of the agn population produce powerful collimated radio jets that can extend thousands of parsecs from the center of the host galaxy recent multiwavelength surveys have shown that ... | [['we', 'review', 'the', 'latest', 'attempts', 'to', 'determine', 'the', 'accretion', 'geometry', 'in', 'radioloud', 'active', 'galactic', 'nuclei', 'agn', 'these', 'objects', 'which', 'comprise', '1020', 'of', 'the', 'agn', 'population', 'produce', 'powerful', 'collimated', 'radio', 'jets', 'that', 'can', 'extend', 't... | [-0.053073465809657494, 0.09863066627913007, -0.021016999463534962, 0.17544076402045491, -0.16497186605955375, -0.12480298772791011, 0.0048764852489907775, 0.48782922378030874, -0.08205287561075772, -0.32249381697321006, 0.08681487434446328, -0.303941099588775, 0.02865928100911364, 0.24508799601867162, -0.0440825996904... |
707.3143 | A parameterization of the Fermat curves satisfying x^(2N)+y^(2N)=1 | Note that the family of closed curves C_N={(x,y)\in R^2;x^(2N)+y^(2N)=1} for
N=1,2,3,... approaches the boundary of [-1,1]^2 as N \to \infty. In this paper
we exhibit a natural parameterization of these curves and generalize to a
larger class of equations.
| math.GM | note that the family of closed curves c_nxyin r2x2ny2n1 for n123 approaches the boundary of 112 as n to infty in this paper we exhibit a natural parameterization of these curves and generalize to a larger class of equations | [['note', 'that', 'the', 'family', 'of', 'closed', 'curves', 'c_nxyin', 'r2x2ny2n1', 'for', 'n123', 'approaches', 'the', 'boundary', 'of', '112', 'as', 'n', 'to', 'infty', 'in', 'this', 'paper', 'we', 'exhibit', 'a', 'natural', 'parameterization', 'of', 'these', 'curves', 'and', 'generalize', 'to', 'a', 'larger', 'clas... | [-0.13164463875865615, 0.1084938292215402, -0.0830072382011929, 0.048564730573923805, -0.05347780047638996, -0.12442851212580462, 0.017991747282369918, 0.3158857407602104, -0.23527302250668808, -0.2873679140481997, 0.04399707804220049, -0.2817398864977263, -0.1748973042011966, 0.23613355418264464, -0.10917240929966038,... |
707.3144 | The Distances to Open Clusters from Main-Sequence Fitting. IV. Galactic
Cepheids, the LMC, and the Local Distance Scale | We derive the basic properties of seven Galactic open clusters containing
Cepheids and construct their period-luminosity (P-L) relations. For our cluster
main-sequence fitting we extend previous Hyades-based empirical
color-temperature corrections to hotter stars using the Pleiades as a template.
We use BVI_{C}JHK_{s... | astro-ph | we derive the basic properties of seven galactic open clusters containing cepheids and construct their periodluminosity pl relations for our cluster mainsequence fitting we extend previous hyadesbased empirical colortemperature corrections to hotter stars using the pleiades as a template we use bvi_cjhk_s data to test ... | [['we', 'derive', 'the', 'basic', 'properties', 'of', 'seven', 'galactic', 'open', 'clusters', 'containing', 'cepheids', 'and', 'construct', 'their', 'periodluminosity', 'pl', 'relations', 'for', 'our', 'cluster', 'mainsequence', 'fitting', 'we', 'extend', 'previous', 'hyadesbased', 'empirical', 'colortemperature', 'co... | [-0.04103905138658756, 0.07348049969671165, -0.10828673994041471, 0.08839927788264676, -0.09435135796834457, -0.09260709340315701, 0.12512710767360516, 0.4468471050228789, -0.17836574713295572, -0.3737818210340857, 0.01483651555711815, -0.33936934512721967, -0.005807265831109877, 0.25021320033863365, -0.128369996993686... |
707.3145 | Muon production in low-energy electron-nucleon and electron-nucleus
scattering | Recently, muon production in electron-proton scattering has been suggested as
a possible candidate reaction for the identification of lepton-flavor violation
due to physics beyond the Standard Model. Here we point out that the
Standard-Model processes $e^- p \to \mu^- p \bar{\nu}_\mu \nu_e$ and $e^- p \to
e^- n \mu^+... | hep-ph nucl-ex nucl-th | recently muon production in electronproton scattering has been suggested as a possible candidate reaction for the identification of leptonflavor violation due to physics beyond the standard model here we point out that the standardmodel processes e p to mu p barnu_mu nu_e and e p to e n mu nu_mu can cloud potential bey... | [['recently', 'muon', 'production', 'in', 'electronproton', 'scattering', 'has', 'been', 'suggested', 'as', 'a', 'possible', 'candidate', 'reaction', 'for', 'the', 'identification', 'of', 'leptonflavor', 'violation', 'due', 'to', 'physics', 'beyond', 'the', 'standard', 'model', 'here', 'we', 'point', 'out', 'that', 'th... | [-0.0918023535383067, 0.19594336671716706, -0.05149956412253455, 0.11052439128029712, -0.03331680702549234, -0.13742054171137968, 0.1139088156823145, 0.28521140261401173, -0.263411325602127, -0.26884250624143347, -0.10862916567106257, -0.3653942739533983, -0.013326473878601528, 0.147540449228955, 0.060524079934408774, ... |
707.3146 | Detecting Early Galaxies Through Their 21-cm Signature | New observations over the next few years of the emission of distant objects
will help unfold the chapter in cosmic history around the era of the first
galaxies. These observations will use the neutral hydrogen emission or
absorption at a wavelength of 21-cm as a detector of the hydrogen abundance. We
predict the sign... | astro-ph | new observations over the next few years of the emission of distant objects will help unfold the chapter in cosmic history around the era of the first galaxies these observations will use the neutral hydrogen emission or absorption at a wavelength of 21cm as a detector of the hydrogen abundance we predict the signature... | [['new', 'observations', 'over', 'the', 'next', 'few', 'years', 'of', 'the', 'emission', 'of', 'distant', 'objects', 'will', 'help', 'unfold', 'the', 'chapter', 'in', 'cosmic', 'history', 'around', 'the', 'era', 'of', 'the', 'first', 'galaxies', 'these', 'observations', 'will', 'use', 'the', 'neutral', 'hydrogen', 'emi... | [-0.06475017841769774, 0.10683668278056202, -0.0547577434719154, 0.05897009341619772, -0.02756448163687842, -0.026554141440655946, 0.00792074168992524, 0.38236145736513344, -0.22174969294641547, -0.299192087804308, 0.06887693087877024, -0.3442777169345901, -0.052997838338076066, 0.16348678252813065, 0.05452771755162536... |
707.3147 | A Model of Turbulence in Magnetized Plasmas: Implications for the
Dissipation Range in the Solar Wind | This paper studies the turbulent cascade of magnetic energy in weakly
collisional magnetized plasmas. A cascade model is presented, based on the
assumptions of local nonlinear energy transfer in wavenumber space, critical
balance between linear propagation and nonlinear interaction times, and the
applicability of lin... | astro-ph | this paper studies the turbulent cascade of magnetic energy in weakly collisional magnetized plasmas a cascade model is presented based on the assumptions of local nonlinear energy transfer in wavenumber space critical balance between linear propagation and nonlinear interaction times and the applicability of linear di... | [['this', 'paper', 'studies', 'the', 'turbulent', 'cascade', 'of', 'magnetic', 'energy', 'in', 'weakly', 'collisional', 'magnetized', 'plasmas', 'a', 'cascade', 'model', 'is', 'presented', 'based', 'on', 'the', 'assumptions', 'of', 'local', 'nonlinear', 'energy', 'transfer', 'in', 'wavenumber', 'space', 'critical', 'ba... | [-0.16126200186236422, 0.25584212919600385, -0.039009352134219015, 0.10578907664676372, -0.025963456581260664, -0.0690055276317724, -0.05304158946646968, 0.29625488567843017, -0.2813201209073924, -0.2970428764820099, 0.03757490888359511, -0.2290979125293862, -0.026646613738084413, 0.24494916385990645, 0.056463070193223... |
707.3148 | Decaying Dark Energy in Higher-Dimensional Gravity | We use data from observational cosmology to put constraints on
higher-dimensional extensions of general relativity in which the effective
four-dimensional dark-energy density (or cosmological "constant") decays with
time. In particular we study the implications of this decaying dark energy for
the age of the universe... | astro-ph | we use data from observational cosmology to put constraints on higherdimensional extensions of general relativity in which the effective fourdimensional darkenergy density or cosmological constant decays with time in particular we study the implications of this decaying dark energy for the age of the universe largescal... | [['we', 'use', 'data', 'from', 'observational', 'cosmology', 'to', 'put', 'constraints', 'on', 'higherdimensional', 'extensions', 'of', 'general', 'relativity', 'in', 'which', 'the', 'effective', 'fourdimensional', 'darkenergy', 'density', 'or', 'cosmological', 'constant', 'decays', 'with', 'time', 'in', 'particular', ... | [-0.0843582793425482, 0.14306761709471735, -0.0947866657605538, 0.17941860734964182, -0.1628560421343606, -0.09257181583178373, 0.028011496975803032, 0.29006214445689693, -0.21716059453319758, -0.3098762846874216, 0.07986228161406381, -0.25493059050495503, -0.0048890722660312, 0.22200852456780223, -0.004056807215699966... |
707.3149 | Dissipation-Scale Turbulence in the Solar Wind | We present a cascade model for turbulence in weakly collisional plasmas that
follows the nonlinear cascade of energy from the large scales of driving in the
MHD regime to the small scales of the kinetic Alfven wave regime where the
turbulence is dissipated by kinetic processes. Steady-state solutions of the
model for... | astro-ph | we present a cascade model for turbulence in weakly collisional plasmas that follows the nonlinear cascade of energy from the large scales of driving in the mhd regime to the small scales of the kinetic alfven wave regime where the turbulence is dissipated by kinetic processes steadystate solutions of the model for the... | [['we', 'present', 'a', 'cascade', 'model', 'for', 'turbulence', 'in', 'weakly', 'collisional', 'plasmas', 'that', 'follows', 'the', 'nonlinear', 'cascade', 'of', 'energy', 'from', 'the', 'large', 'scales', 'of', 'driving', 'in', 'the', 'mhd', 'regime', 'to', 'the', 'small', 'scales', 'of', 'the', 'kinetic', 'alfven', ... | [-0.13236110831743905, 0.21229475610172294, -0.038546298559023334, 0.10588497170579753, -0.012378892849665136, -0.08615922025804008, -0.027346094390044786, 0.2793263976470501, -0.29402184454125485, -0.35455155105197006, 0.04516134560731838, -0.2423903416443084, -0.06370984751598112, 0.2396477239867506, 0.01365446971862... |
707.315 | Angular distribution of leptons from the decay of massive vector bosons | We examine the transverse momentum $Q_\perp$ dependence of the helicity
structure functions for massive vector bosons of mass $Q$ in hadron reactions.
We demonstrate that large logarithmic terms of the form $\ln(Q/Q_\perp)$ in the
helicity structure functions have the same origin as the logarithmic terms in
the angul... | hep-ph nucl-th | we examine the transverse momentum q_perp dependence of the helicity structure functions for massive vector bosons of mass q in hadron reactions we demonstrate that large logarithmic terms of the form lnqq_perp in the helicity structure functions have the same origin as the logarithmic terms in the angularintegrated cr... | [['we', 'examine', 'the', 'transverse', 'momentum', 'q_perp', 'dependence', 'of', 'the', 'helicity', 'structure', 'functions', 'for', 'massive', 'vector', 'bosons', 'of', 'mass', 'q', 'in', 'hadron', 'reactions', 'we', 'demonstrate', 'that', 'large', 'logarithmic', 'terms', 'of', 'the', 'form', 'lnqq_perp', 'in', 'the'... | [-0.1525296027585864, 0.16292728948406876, -0.08242812251672149, 0.14484299620613456, -0.02034436403773725, 0.025361789476592095, -0.029005357005517, 0.3137289352528751, -0.2518127750232816, -0.25764587910845876, -0.040453113957773894, -0.2904100201278925, -0.0572147704847157, 0.1426059485692531, 0.07793797778896988, 0... |
707.3151 | Stable Tameness of Two-Dimensional Polynomial Automorphisms Over a
Regular Ring | In this paper it is established that all two-dimensional polynomial
automorphisms over a regular ring R are stably tame. In the case R is a
Dedekind Q-algebra, some stronger results are obtained. A key element in the
proof is a theorem which yields the following corollary: Over an Artinian ring
A all two-dimensional ... | math.AC math.AG | in this paper it is established that all twodimensional polynomial automorphisms over a regular ring r are stably tame in the case r is a dedekind qalgebra some stronger results are obtained a key element in the proof is a theorem which yields the following corollary over an artinian ring a all twodimensional polynomia... | [['in', 'this', 'paper', 'it', 'is', 'established', 'that', 'all', 'twodimensional', 'polynomial', 'automorphisms', 'over', 'a', 'regular', 'ring', 'r', 'are', 'stably', 'tame', 'in', 'the', 'case', 'r', 'is', 'a', 'dedekind', 'qalgebra', 'some', 'stronger', 'results', 'are', 'obtained', 'a', 'key', 'element', 'in', 't... | [-0.2117098992554626, 0.08303210208911575, -0.14432260857817406, 0.06096026537488797, -0.09265431691892445, -0.18943198722748397, -0.11487729179862072, 0.3507384618666644, -0.39442427235189825, -0.10161004706363504, 0.12938335734846382, -0.21714439483669898, -0.15043281677693207, 0.227475955694293, -0.15698590130584003... |
707.3152 | New Physics Effects in Higgs Decay to Tau Leptons | We study the possible effects of TeV scale new physics (NP) on the rate for
Higgs boson decays to charged leptons, focusing on the tau tau channel which
can be readily studied at the Large Hadron collider. Using an SU(3)_C X SU(2)_L
X U(1)_Y invariant effective theory valid below a NP scale Lambda, we determine
all e... | hep-ph | we study the possible effects of tev scale new physics np on the rate for higgs boson decays to charged leptons focusing on the tau tau channel which can be readily studied at the large hadron collider using an su3_c x su2_l x u1_y invariant effective theory valid below a np scale lambda we determine all effective oper... | [['we', 'study', 'the', 'possible', 'effects', 'of', 'tev', 'scale', 'new', 'physics', 'np', 'on', 'the', 'rate', 'for', 'higgs', 'boson', 'decays', 'to', 'charged', 'leptons', 'focusing', 'on', 'the', 'tau', 'tau', 'channel', 'which', 'can', 'be', 'readily', 'studied', 'at', 'the', 'large', 'hadron', 'collider', 'usin... | [-0.10703892954708343, 0.23614833103723262, -0.05908553684102593, 0.17248120356608915, -0.08161175105072159, -0.18301364911686896, 0.04230331982537228, 0.30642436709465637, -0.2786660590597118, -0.28559704279039233, 0.06362926313886419, -0.26720490814685555, -0.006600681819864327, 0.16966163385569372, 0.076810813253922... |
707.3153 | Consequences of the H-Theorem from Nonlinear Fokker-Planck Equations | A general type of nonlinear Fokker-Planck equation is derived directly from a
master equation, by introducing generalized transition rates. The H-theorem is
demonstrated for systems that follow those classes of nonlinear Fokker-Planck
equations, in the presence of an external potential. For that, a relation
involving... | cond-mat.stat-mech | a general type of nonlinear fokkerplanck equation is derived directly from a master equation by introducing generalized transition rates the htheorem is demonstrated for systems that follow those classes of nonlinear fokkerplanck equations in the presence of an external potential for that a relation involving terms of ... | [['a', 'general', 'type', 'of', 'nonlinear', 'fokkerplanck', 'equation', 'is', 'derived', 'directly', 'from', 'a', 'master', 'equation', 'by', 'introducing', 'generalized', 'transition', 'rates', 'the', 'htheorem', 'is', 'demonstrated', 'for', 'systems', 'that', 'follow', 'those', 'classes', 'of', 'nonlinear', 'fokkerp... | [-0.08022936066798866, 0.09419528561562765, -0.13954797435179353, 0.09989057553187013, -0.11676400823146105, -0.16426677400618792, -0.0324490464925766, 0.25223439711332324, -0.3494031662940979, -0.23571754885092377, 0.03404669242631644, -0.30531954868137834, -0.17179808031022548, 0.22540945374965668, -0.037586470060050... |
707.3154 | Hysteresis of spectral evolution in the soft state of black-hole binary
LMC X-3 | We report the discovery of hysteresis between the x-ray spectrum and
luminosity of black-hole binary LMC X-3. Our observations, with the
Proportional Counter Array on the Rossi X-ray Timing Explorer, took place
entirely within the soft spectral state, dominated by a spectral component that
was fitted well with a mult... | astro-ph | we report the discovery of hysteresis between the xray spectrum and luminosity of blackhole binary lmc x3 our observations with the proportional counter array on the rossi xray timing explorer took place entirely within the soft spectral state dominated by a spectral component that was fitted well with a multicolor dis... | [['we', 'report', 'the', 'discovery', 'of', 'hysteresis', 'between', 'the', 'xray', 'spectrum', 'and', 'luminosity', 'of', 'blackhole', 'binary', 'lmc', 'x3', 'our', 'observations', 'with', 'the', 'proportional', 'counter', 'array', 'on', 'the', 'rossi', 'xray', 'timing', 'explorer', 'took', 'place', 'entirely', 'withi... | [-0.06729767122700558, 0.12986169748692603, -0.0878242560935938, 0.09201422997942395, -0.09180829714389128, -0.09388266467505087, 0.07627003728070081, 0.45204594537699966, -0.18756535578003458, -0.34764908544987566, 0.13892821157166976, -0.34350975862267497, -0.07373021475149918, 0.20872722353028544, -0.067867644354806... |
707.3155 | A Random Change of Variables and Applications to the Stochastic Porous
Medium Equation with Multiplicative Time Noise | A change of variables is introduced to reduce certain nonlinear stochastic
evolution equations with multiplicative noise to the corresponding
deterministic equation. The result is then used to investigate a stochastic
porous medium equation.
| math.PR math.AP | a change of variables is introduced to reduce certain nonlinear stochastic evolution equations with multiplicative noise to the corresponding deterministic equation the result is then used to investigate a stochastic porous medium equation | [['a', 'change', 'of', 'variables', 'is', 'introduced', 'to', 'reduce', 'certain', 'nonlinear', 'stochastic', 'evolution', 'equations', 'with', 'multiplicative', 'noise', 'to', 'the', 'corresponding', 'deterministic', 'equation', 'the', 'result', 'is', 'then', 'used', 'to', 'investigate', 'a', 'stochastic', 'porous', '... | [-0.09575940620605693, 0.09229133727917956, -0.0866201227022843, 0.06859038622033867, -0.1559053959578953, -0.12250685542257446, -0.017914511771364647, 0.25690720388383576, -0.41001932819684345, -0.24985746020507632, 0.08686878865189625, -0.24821220242390127, -0.2019187237954501, 0.11841205817957719, -0.097913457024278... |
707.3156 | Gluelump spectrum from Coulomb gauge QCD | We compute the energy spectrum of gluelumps defined as gluonic excitations
bound to a localized, static octet source. We are able to reproduce the
nontrivial ordering of the spin-parity levels and show how this is related to
the non-abelian part of the Coulomb interaction between color charges.
| hep-ph | we compute the energy spectrum of gluelumps defined as gluonic excitations bound to a localized static octet source we are able to reproduce the nontrivial ordering of the spinparity levels and show how this is related to the nonabelian part of the coulomb interaction between color charges | [['we', 'compute', 'the', 'energy', 'spectrum', 'of', 'gluelumps', 'defined', 'as', 'gluonic', 'excitations', 'bound', 'to', 'a', 'localized', 'static', 'octet', 'source', 'we', 'are', 'able', 'to', 'reproduce', 'the', 'nontrivial', 'ordering', 'of', 'the', 'spinparity', 'levels', 'and', 'show', 'how', 'this', 'is', 'r... | [-0.12131509515754085, 0.21921507942866772, -0.07917969468782873, 0.1792162243831665, -0.06600347846904968, -0.07039085631952324, 0.02633916517283688, 0.3667655484156406, -0.20678703475030177, -0.32274704608828464, -0.04910442030968818, -0.3010785291962167, -0.08863861937069042, 0.042423070428219245, 0.0297354173034112... |
707.3157 | Accurate retrieval of structural information from laser-induced
photoelectron and high-harmonic spectra by few-cycle laser pulses | By analyzing ``exact'' theoretical results from solving the time-dependent
Schr\"odinger equation of atoms in few-cycle laser pulses, we established the
general conclusion that differential elastic scattering and photo-recombination
cross sections of the target ion with {\em free} electrons can be extracted
accuratel... | physics.atom-ph | by analyzing exact theoretical results from solving the timedependent schrodinger equation of atoms in fewcycle laser pulses we established the general conclusion that differential elastic scattering and photorecombination cross sections of the target ion with em free electrons can be extracted accurately from lasergen... | [['by', 'analyzing', 'exact', 'theoretical', 'results', 'from', 'solving', 'the', 'timedependent', 'schrodinger', 'equation', 'of', 'atoms', 'in', 'fewcycle', 'laser', 'pulses', 'we', 'established', 'the', 'general', 'conclusion', 'that', 'differential', 'elastic', 'scattering', 'and', 'photorecombination', 'cross', 's... | [-0.0374503105516061, 0.1890576515944129, -0.06788086965962341, 0.07417546566270028, 0.003671183998724728, -0.13506284464301185, -0.0220886218006431, 0.4789418823019874, -0.2679181957636217, -0.2842322219882838, -0.03268621766097806, -0.33017778769135475, -0.04082200233119004, 0.24502374840232383, 0.07106401122673744, ... |
707.3158 | Quasiparticle mirages in the tunneling spectra of d-wave superconductors | We illustrate the importance of many-body effects in the Fourier transformed
local density of states (FT-LDOS) of d-wave superconductors from a model of
electrons coupled to an Einstein mode with energy Omega_0. For bias energies
significantly larger than Omega_0 the quasiparticles have short lifetimes due
to this co... | cond-mat.supr-con cond-mat.str-el | we illustrate the importance of manybody effects in the fourier transformed local density of states ftldos of dwave superconductors from a model of electrons coupled to an einstein mode with energy omega_0 for bias energies significantly larger than omega_0 the quasiparticles have short lifetimes due to this coupling a... | [['we', 'illustrate', 'the', 'importance', 'of', 'manybody', 'effects', 'in', 'the', 'fourier', 'transformed', 'local', 'density', 'of', 'states', 'ftldos', 'of', 'dwave', 'superconductors', 'from', 'a', 'model', 'of', 'electrons', 'coupled', 'to', 'an', 'einstein', 'mode', 'with', 'energy', 'omega_0', 'for', 'bias', '... | [-0.14233961030011613, 0.22319080543322392, -0.10751786968058409, 0.11569239797185443, -0.014708036575976708, -0.12320325117915461, 0.04185393229701033, 0.33858899876781523, -0.23890071935084176, -0.27476296887720286, -0.03063619360869929, -0.3070392264580483, -0.05815283634878491, 0.1856109426446157, 0.051294454863001... |
707.3159 | Rectification and nonlinear transport in chaotic dots and rings | We investigate the nonlinear current-voltage characteristic of mesoscopic
conductors and the current generated through rectification of an alternating
external bias. To leading order in applied voltages both the nonlinear and the
rectified current are quadratic. This current response can be described in
terms of seco... | cond-mat.mes-hall cond-mat.mtrl-sci | we investigate the nonlinear currentvoltage characteristic of mesoscopic conductors and the current generated through rectification of an alternating external bias to leading order in applied voltages both the nonlinear and the rectified current are quadratic this current response can be described in terms of second or... | [['we', 'investigate', 'the', 'nonlinear', 'currentvoltage', 'characteristic', 'of', 'mesoscopic', 'conductors', 'and', 'the', 'current', 'generated', 'through', 'rectification', 'of', 'an', 'alternating', 'external', 'bias', 'to', 'leading', 'order', 'in', 'applied', 'voltages', 'both', 'the', 'nonlinear', 'and', 'the... | [-0.2094970682748652, 0.1628657613573738, -0.045338394485623025, 0.026534516573791928, -0.042220233087097915, -0.14837529809822833, 0.007578843888298674, 0.36436585574887514, -0.31612816001251925, -0.25333226100710315, 0.033087325824596954, -0.28118695728077486, -0.16095682471535924, 0.18222471281215108, -0.01856116505... |
707.316 | Random Walks in Random Environments | Random walks provide a simple conventional model to describe various
transport processes, for example propagation of heat or diffusion of matter
through a medium. However, in many practical cases the medium is highly
irregular due to defects, impurities, fluctuations etc., and it is natural to
model this as random en... | math.PR math-ph math.MP | random walks provide a simple conventional model to describe various transport processes for example propagation of heat or diffusion of matter through a medium however in many practical cases the medium is highly irregular due to defects impurities fluctuations etc and it is natural to model this as random environment... | [['random', 'walks', 'provide', 'a', 'simple', 'conventional', 'model', 'to', 'describe', 'various', 'transport', 'processes', 'for', 'example', 'propagation', 'of', 'heat', 'or', 'diffusion', 'of', 'matter', 'through', 'a', 'medium', 'however', 'in', 'many', 'practical', 'cases', 'the', 'medium', 'is', 'highly', 'irre... | [-0.06840848925861744, 0.15168023484470866, -0.08414739799986472, 0.07456388749649974, -0.08357553663580039, -0.1659420995217134, 0.048705905005586386, 0.3963086256849258, -0.2436353974691655, -0.26903173656541135, 0.15074681188032082, -0.28261682332280375, -0.189820805030474, 0.20563137861210937, -0.113316037909299, 0... |
707.3161 | The Subaru/XMM-Newton Deep Survey (SXDS). IV. Evolution of Lya Emitters
from z=3.1 to 5.7 in the 1 deg^2 Field: Luminosity Functions and AGN | We present luminosity functions (LFs) and various properties of Lya emitters
(LAEs) at z=3.1, 3.7, and 5.7, in a 1 deg^2 sky of the Subaru/XMM-Newton Deep
Survey (SXDS) Field. We obtain a photometric sample of 858 LAE candidates based
on deep Subaru/Suprime-Cam imaging data, and a spectroscopic sample of 84
confirmed... | astro-ph | we present luminosity functions lfs and various properties of lya emitters laes at z31 37 and 57 in a 1 deg2 sky of the subaruxmmnewton deep survey sxds field we obtain a photometric sample of 858 lae candidates based on deep subarusuprimecam imaging data and a spectroscopic sample of 84 confirmed laes from subarufocas... | [['we', 'present', 'luminosity', 'functions', 'lfs', 'and', 'various', 'properties', 'of', 'lya', 'emitters', 'laes', 'at', 'z31', '37', 'and', '57', 'in', 'a', '1', 'deg2', 'sky', 'of', 'the', 'subaruxmmnewton', 'deep', 'survey', 'sxds', 'field', 'we', 'obtain', 'a', 'photometric', 'sample', 'of', '858', 'lae', 'candi... | [0.018499845855229444, 0.04961832526615569, -0.04406249824743478, 0.1534870144123683, -0.10739779852674435, -0.05650116606563522, 0.09379390624647585, 0.53423145290688, -0.005799286674044611, -0.3887651043628291, -0.012158822205793033, -0.3733602236764498, 0.014323243072412332, 0.19315536791566648, 0.03258661330275861,... |
707.3162 | Triple Higgs boson production in the Linear Collider | Triple Higgs boson production (3H) may provide essential information to
reconstruct the Higgs potential. We consider 3H-production in the International
Linear Collider (ILC) both in the Minimal Supersymmetric Standard Model (MSSM)
and in the general Two-Higgs-doublet Model (2HDM). We compute the total
cross-section f... | hep-ph | triple higgs boson production 3h may provide essential information to reconstruct the higgs potential we consider 3hproduction in the international linear collider ilc both in the minimal supersymmetric standard model mssm and in the general twohiggsdoublet model 2hdm we compute the total crosssection for the various 3... | [['triple', 'higgs', 'boson', 'production', '3h', 'may', 'provide', 'essential', 'information', 'to', 'reconstruct', 'the', 'higgs', 'potential', 'we', 'consider', '3hproduction', 'in', 'the', 'international', 'linear', 'collider', 'ilc', 'both', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'a... | [-0.08716609462982604, 0.21100919101050233, -0.0065936899510185415, 0.1966097799662516, -0.05375348011495492, -0.19512511702379454, 0.01726258078728009, 0.32837124209690055, -0.19952738931289501, -0.2545148238452025, 0.03024087502829991, -0.30863890343886097, -0.008529223986506585, 0.13999366677565492, 0.05192473693942... |
707.3163 | Intersection probabilities for a chordal SLE path and a semicircle | We derive a number of estimates for the probability that a chordal SLE path
in the upper half plane H intersects a semicircle centred on the real line. We
prove that if 0<kappa<8 and gamma:[0,infinity) to closure(H) is a chordal SLE
in H from 0 to infinity, then P(gamma[0,infinity) cap C(x;rx) neq emptyset)
asymp r^(... | math.PR | we derive a number of estimates for the probability that a chordal sle path in the upper half plane h intersects a semicircle centred on the real line we prove that if 0kappa8 and gamma0infinity to closureh is a chordal sle in h from 0 to infinity then pgamma0infinity cap cxrx neq emptyset asymp r4a1 where a2kappa and ... | [['we', 'derive', 'a', 'number', 'of', 'estimates', 'for', 'the', 'probability', 'that', 'a', 'chordal', 'sle', 'path', 'in', 'the', 'upper', 'half', 'plane', 'h', 'intersects', 'a', 'semicircle', 'centred', 'on', 'the', 'real', 'line', 'we', 'prove', 'that', 'if', '0kappa8', 'and', 'gamma0infinity', 'to', 'closureh', ... | [-0.11587897518277168, 0.0913879908019444, -0.06578216423653066, 0.01539051835052669, -0.06496235566772521, -0.1531735309883952, 0.07350726014375687, 0.3838823226541281, -0.2657213405109942, -0.16288917346671222, 0.12621947213169188, -0.3499067853987217, -0.08141624266747385, 0.17955535087920727, -0.033004960954189304,... |
707.3164 | The Symmetric Tensor Lichnerowicz Algebra and a Novel Associative
Fourier-Jacobi Algebra | Lichnerowicz's algebra of differential geometric operators acting on
symmetric tensors can be obtained from generalized geodesic motion of an
observer carrying a complex tangent vector. This relation is based upon
quantizing the classical evolution equations, and identifying wavefunctions
with sections of the symmetr... | math.DG gr-qc hep-th math.RT | lichnerowiczs algebra of differential geometric operators acting on symmetric tensors can be obtained from generalized geodesic motion of an observer carrying a complex tangent vector this relation is based upon quantizing the classical evolution equations and identifying wavefunctions with sections of the symmetric te... | [['lichnerowiczs', 'algebra', 'of', 'differential', 'geometric', 'operators', 'acting', 'on', 'symmetric', 'tensors', 'can', 'be', 'obtained', 'from', 'generalized', 'geodesic', 'motion', 'of', 'an', 'observer', 'carrying', 'a', 'complex', 'tangent', 'vector', 'this', 'relation', 'is', 'based', 'upon', 'quantizing', 't... | [-0.12151737689977339, 0.12052083354653807, -0.0842817744299726, 0.042940652395901814, -0.16909215375808131, -0.12585928606215951, -0.07888383082950726, 0.3387287811072933, -0.2786393747989868, -0.23188693840821478, 0.11240896047566758, -0.24296895146023395, -0.20398942023098773, 0.1712696459455697, -0.0975797189654089... |
707.3165 | Extinction Corrected Star Formation Rates Empirically Derived from
Ultraviolet-Optical Colors | Using a sample of galaxies from the Sloan Digital Sky Survey spectroscopic
catalog with measured star-formation rates (SFRs) and ultraviolet (UV)
photometry from the GALEX Medium Imaging Survey, we derived empirical linear
correlations between the SFR to UV luminosity ratio and the UV-optical colors
of blue sequence ... | astro-ph | using a sample of galaxies from the sloan digital sky survey spectroscopic catalog with measured starformation rates sfrs and ultraviolet uv photometry from the galex medium imaging survey we derived empirical linear correlations between the sfr to uv luminosity ratio and the uvoptical colors of blue sequence galaxies ... | [['using', 'a', 'sample', 'of', 'galaxies', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'spectroscopic', 'catalog', 'with', 'measured', 'starformation', 'rates', 'sfrs', 'and', 'ultraviolet', 'uv', 'photometry', 'from', 'the', 'galex', 'medium', 'imaging', 'survey', 'we', 'derived', 'empirical', 'linear', 'corr... | [0.054246241631715195, 0.03559384258949886, -0.07221872412154208, 0.1591389741586602, -0.12878731055711598, -0.02669567793364758, 0.11016241793581487, 0.5346089198213556, -0.10267392309868466, -0.3366733074512171, 0.02775677388695919, -0.3417775896823277, -0.006754587351789941, 0.2065863866872425, -0.06895380122587084,... |
707.3166 | Conformal Windows of SU(N) Gauge Theories, Higher Dimensional
Representations and The Size of The Unparticle World | We present the conformal windows of SU(N) supersymmetric and
nonsupersymmetric gauge theories with vector-like matter transforming according
to higher irreducible representations of the gauge group. We determine the
fraction of asymptotically free theories expected to develop an infrared fixed
point and find that it ... | hep-th hep-lat hep-ph | we present the conformal windows of sun supersymmetric and nonsupersymmetric gauge theories with vectorlike matter transforming according to higher irreducible representations of the gauge group we determine the fraction of asymptotically free theories expected to develop an infrared fixed point and find that it does n... | [['we', 'present', 'the', 'conformal', 'windows', 'of', 'sun', 'supersymmetric', 'and', 'nonsupersymmetric', 'gauge', 'theories', 'with', 'vectorlike', 'matter', 'transforming', 'according', 'to', 'higher', 'irreducible', 'representations', 'of', 'the', 'gauge', 'group', 'we', 'determine', 'the', 'fraction', 'of', 'asy... | [-0.06758703141383587, 0.18940103019215415, -0.09248193130023183, 0.10126832523943488, -0.0670663603683585, -0.1452597528272732, 0.02059515844594767, 0.32158580127565617, -0.192201470966167, -0.28665469429470636, 0.0776523823910866, -0.29682862409149274, -0.12132993529993981, 0.11741029667819945, -0.03476851408255914, ... |
707.3167 | Rational Tate classes | In despair, as Deligne (2000) put it, of proving the Hodge and Tate
conjectures, we can try to find substitutes. For abelian varieties in
characteristic zero, Deligne (1982) constructed a theory of Hodge classes
having many of the properties that the algebraic classes would have if the
Hodge conjecture were known. In... | math.AG math.NT | in despair as deligne 2000 put it of proving the hodge and tate conjectures we can try to find substitutes for abelian varieties in characteristic zero deligne 1982 constructed a theory of hodge classes having many of the properties that the algebraic classes would have if the hodge conjecture were known in this articl... | [['in', 'despair', 'as', 'deligne', '2000', 'put', 'it', 'of', 'proving', 'the', 'hodge', 'and', 'tate', 'conjectures', 'we', 'can', 'try', 'to', 'find', 'substitutes', 'for', 'abelian', 'varieties', 'in', 'characteristic', 'zero', 'deligne', '1982', 'constructed', 'a', 'theory', 'of', 'hodge', 'classes', 'having', 'ma... | [-0.15597642927120128, 0.06787129675762521, -0.1894986467772267, 0.12476869905755544, -0.11443834654572937, -0.1705197007033146, -0.03603121101494051, 0.2943086790839314, -0.34820042175965177, -0.26256710125340355, 0.09631647086417716, -0.19333363479365492, -0.13982037865142855, 0.19219903582707049, -0.2114180953345365... |
707.3168 | Wormholes in Maximal Supergravity | In this brief note, we reconsider the problem of finding Euclidean wormhole
solutions to maximal supergravity in d dimensions. We find that such solutions
exists for all d less than or equal to 9. However, we argue that, in
toroidally-compactified string theories, these saddle points never contribute
to the path inte... | hep-th | in this brief note we reconsider the problem of finding euclidean wormhole solutions to maximal supergravity in d dimensions we find that such solutions exists for all d less than or equal to 9 however we argue that in toroidallycompactified string theories these saddle points never contribute to the path integral beca... | [['in', 'this', 'brief', 'note', 'we', 'reconsider', 'the', 'problem', 'of', 'finding', 'euclidean', 'wormhole', 'solutions', 'to', 'maximal', 'supergravity', 'in', 'd', 'dimensions', 'we', 'find', 'that', 'such', 'solutions', 'exists', 'for', 'all', 'd', 'less', 'than', 'or', 'equal', 'to', '9', 'however', 'we', 'argu... | [-0.17033342335240118, 0.10008792278157282, -0.05450749530323914, 0.09192240803843431, -0.06932587361994333, -0.16738011339579575, 0.04972156069041895, 0.31604410339579253, -0.19844919848921044, -0.2691068496288998, 0.09368643946488321, -0.33784338153366533, -0.19719710332823784, 0.13209852762104543, -0.114799908320752... |
707.3169 | Traces on operator ideals and arithmetic means | This article - a part of a multipaper project investigating arithmetic mean
ideals - investigates the codimension of commutator spaces [I, B(H)] of
operator ideals on a separable Hilbert space, i.e., ``How many traces can an
ideal support?" We conjecture that the codimension can be only zero, one, or
infinity. Using ... | math.FA math.OA | this article a part of a multipaper project investigating arithmetic mean ideals investigates the codimension of commutator spaces i bh of operator ideals on a separable hilbert space ie how many traces can an ideal support we conjecture that the codimension can be only zero one or infinity using the arithmetic mean am... | [['this', 'article', 'a', 'part', 'of', 'a', 'multipaper', 'project', 'investigating', 'arithmetic', 'mean', 'ideals', 'investigates', 'the', 'codimension', 'of', 'commutator', 'spaces', 'i', 'bh', 'of', 'operator', 'ideals', 'on', 'a', 'separable', 'hilbert', 'space', 'ie', 'how', 'many', 'traces', 'can', 'an', 'ideal... | [-0.1298259146989156, 0.08460922015439838, -0.06320927146440133, 0.08633803122783064, -0.06397667736985171, -0.14989767728182368, -0.030717368086632817, 0.31169946496971906, -0.3259302825595324, -0.1499570389588674, 0.15973237177374988, -0.28327113829123285, -0.10958085069731356, 0.1838922831337326, -0.1184677224194344... |
707.317 | Inductive Definition and Domain Theoretic Properties of Fully Abstract | A construction of fully abstract typed models for PCF and PCF^+ (i.e., PCF +
"parallel conditional function"), respectively, is presented. It is based on
general notions of sequential computational strategies and wittingly consistent
non-deterministic strategies introduced by the author in the seventies.
Although the... | cs.LO | a construction of fully abstract typed models for pcf and pcf ie pcf parallel conditional function respectively is presented it is based on general notions of sequential computational strategies and wittingly consistent nondeterministic strategies introduced by the author in the seventies although these notions of stra... | [['a', 'construction', 'of', 'fully', 'abstract', 'typed', 'models', 'for', 'pcf', 'and', 'pcf', 'ie', 'pcf', 'parallel', 'conditional', 'function', 'respectively', 'is', 'presented', 'it', 'is', 'based', 'on', 'general', 'notions', 'of', 'sequential', 'computational', 'strategies', 'and', 'wittingly', 'consistent', 'n... | [-0.04582815945157828, 0.08361074052433408, -0.11272474416957504, 0.10270993403643464, -0.11269090239464039, -0.15141400569890762, 0.038018267315077646, 0.37810092373404786, -0.3357153868597544, -0.2488672884556128, 0.09228820918945727, -0.2270894678053329, -0.15127365418063973, 0.18467334252852366, -0.1350118043339909... |
707.3171 | Intrinsic Impurity in the High Temperature Superconductor
Bi_2Sr_2CaCu_2O$_{8+\delta}$ | The {}^{17}O NMR spectra of Bi_2Sr_2CaCu_2O$_{8+\delta}$ (Bi-2212) single
crystals were measured in the temperature range from 4 K to 200 K and magnetic
fields from 3 to 29 T, reported here principally at 8 T. The NMR linewidth of
the oxygen in the CuO_{2} plane was found to be magnetically broadened with the
tempera... | cond-mat.supr-con cond-mat.str-el | the 17o nmr spectra of bi_2sr_2cacu_2o_8delta bi2212 single crystals were measured in the temperature range from 4 k to 200 k and magnetic fields from 3 to 29 t reported here principally at 8 t the nmr linewidth of the oxygen in the cuo_2 plane was found to be magnetically broadened with the temperature dependence of a... | [['the', '17o', 'nmr', 'spectra', 'of', 'bi_2sr_2cacu_2o_8delta', 'bi2212', 'single', 'crystals', 'were', 'measured', 'in', 'the', 'temperature', 'range', 'from', '4', 'k', 'to', '200', 'k', 'and', 'magnetic', 'fields', 'from', '3', 'to', '29', 't', 'reported', 'here', 'principally', 'at', '8', 't', 'the', 'nmr', 'line... | [-0.1126331317183726, 0.27117245319069994, 0.014039305504411459, -0.042046949371476385, -0.001994526369825882, -0.1368323111851864, 0.11592260877437452, 0.3996684607337503, -0.2703872124911012, -0.35511023505207373, -0.03860529239618165, -0.4028874419081737, 0.03625548181726652, 0.18071626827175566, 0.06843248984283384... |
707.3172 | Equivariant orbifold structures on the projective line and integrable
hierarchies | Let $\CP^1_{k,m}$ be the orbifold structure on $\CP^1$ obtained via
uniformizing the neighborhoods of 0 and $\infty$ respectively by $z\mapsto z^k$
and $w\mapsto w^m.$ The diagonal action of the torus on the projective line
induces naturally an orbifold action on $\CP^1_{k,m}.$ In this paper we prove
that if k and m ... | math.SG math.AG | let cp1_km be the orbifold structure on cp1 obtained via uniformizing the neighborhoods of 0 and infty respectively by zmapsto zk and wmapsto wm the diagonal action of the torus on the projective line induces naturally an orbifold action on cp1_km in this paper we prove that if k and m are coprime then giventals predic... | [['let', 'cp1_km', 'be', 'the', 'orbifold', 'structure', 'on', 'cp1', 'obtained', 'via', 'uniformizing', 'the', 'neighborhoods', 'of', '0', 'and', 'infty', 'respectively', 'by', 'zmapsto', 'zk', 'and', 'wmapsto', 'wm', 'the', 'diagonal', 'action', 'of', 'the', 'torus', 'on', 'the', 'projective', 'line', 'induces', 'nat... | [-0.19541035263769163, 0.05705032474260505, -0.09781879740467497, 0.11372478505640318, -0.07635376865440739, -0.13767064865079182, 0.029403072294875942, 0.2514653407281615, -0.3435707350658013, -0.23178335245569595, 0.07781628057381397, -0.23821031255417013, -0.1846581531762339, 0.1626553063794952, -0.11156097974940572... |
707.3173 | Points on Shimura varieties over finite fields: the conjecture of
Langlands and Rapoport | We state an improved version of the conjecture of Langlands and Rapoport, and
we prove the conjecture for a large class of Shimura varieties. In particular,
we obtain the first proof of the (original) conjecture for Shimura varieties of
PEL-type.
| math.NT math.AG | we state an improved version of the conjecture of langlands and rapoport and we prove the conjecture for a large class of shimura varieties in particular we obtain the first proof of the original conjecture for shimura varieties of peltype | [['we', 'state', 'an', 'improved', 'version', 'of', 'the', 'conjecture', 'of', 'langlands', 'and', 'rapoport', 'and', 'we', 'prove', 'the', 'conjecture', 'for', 'a', 'large', 'class', 'of', 'shimura', 'varieties', 'in', 'particular', 'we', 'obtain', 'the', 'first', 'proof', 'of', 'the', 'original', 'conjecture', 'for',... | [-0.19744437949266286, -0.04688206985265424, -0.1844873777590692, 0.08895725444890559, -0.06778565589338541, -0.13353541268734262, -0.004081361507996917, 0.18926704507321118, -0.28090776661410927, -0.26940306527540087, 0.08793278204102535, -0.14539742495981045, -0.14804763244464994, 0.24870406477712095, -0.241986390599... |
707.3174 | A new characterization for the m-quasiinvariants of S_n and explicit
basis for two row hook shapes | In 2002, Feigin and Veselov defined the space of m-quasiinvariants for any
Coxeter group, building on earlier work of Chalykh and Veselov. While many
properties of those spaces were proven from this definition, an explicit
computation of a basis was only done in certain cases. In particular, Feigin
and Veselov comput... | math.CO | in 2002 feigin and veselov defined the space of mquasiinvariants for any coxeter group building on earlier work of chalykh and veselov while many properties of those spaces were proven from this definition an explicit computation of a basis was only done in certain cases in particular feigin and veselov computed bases ... | [['in', '2002', 'feigin', 'and', 'veselov', 'defined', 'the', 'space', 'of', 'mquasiinvariants', 'for', 'any', 'coxeter', 'group', 'building', 'on', 'earlier', 'work', 'of', 'chalykh', 'and', 'veselov', 'while', 'many', 'properties', 'of', 'those', 'spaces', 'were', 'proven', 'from', 'this', 'definition', 'an', 'explic... | [-0.11116732228547335, 0.05883941036481701, -0.08306634713274737, 0.03431600593418504, -0.04995184996320556, -0.06835294503641004, 0.032572183589218186, 0.34252459413061537, -0.2349421952404858, -0.25138356708921494, 0.1193159651971655, -0.19922903426534808, -0.17081582331253836, 0.21300851739166926, -0.102582466753422... |
707.3175 | Stacked OSTBC: Error Performance and Rate Analysis | It is well known, that the Alamouti scheme is the only space-time code from
orthogonal design achieving the capacity of a multiple-input multiple-output
(MIMO) wireless communication system with n_T=2 transmit antennas and n_R=1
receive antenna. In this work, we propose the n-times stacked Alamouti scheme
for n_T=2n ... | cs.IT math.IT | it is well known that the alamouti scheme is the only spacetime code from orthogonal design achieving the capacity of a multipleinput multipleoutput mimo wireless communication system with n_t2 transmit antennas and n_r1 receive antenna in this work we propose the ntimes stacked alamouti scheme for n_t2n transmit anten... | [['it', 'is', 'well', 'known', 'that', 'the', 'alamouti', 'scheme', 'is', 'the', 'only', 'spacetime', 'code', 'from', 'orthogonal', 'design', 'achieving', 'the', 'capacity', 'of', 'a', 'multipleinput', 'multipleoutput', 'mimo', 'wireless', 'communication', 'system', 'with', 'n_t2', 'transmit', 'antennas', 'and', 'n_r1'... | [-0.22289351125732232, 0.01689462281818107, 0.004233433487052474, -0.014562579814131652, -0.027420807926343427, -0.24374358185813366, 0.11341111024741435, 0.3801414467636579, -0.1901744835349134, -0.268692183254011, 0.09670821342548364, -0.26384757496750677, -0.19237124534415692, 0.19859044873072126, -0.093851485517243... |
707.3176 | Photocurrent Imaging of p-n Junctions and Local Defects in Ambipolar
Carbon Nanotube Transistors | We use scanning photocurrent microscopy (SPCM) to investigate the properties
of internal p-n junctions as well as local defects in ambipolar carbon nanotube
(CNT) transistors. Our SPCM images show strong signals near metal contacts
whose polarity and positions change depending on the gate bias. SPCM images
analyzed i... | cond-mat.mtrl-sci cond-mat.mes-hall | we use scanning photocurrent microscopy spcm to investigate the properties of internal pn junctions as well as local defects in ambipolar carbon nanotube cnt transistors our spcm images show strong signals near metal contacts whose polarity and positions change depending on the gate bias spcm images analyzed in conjunc... | [['we', 'use', 'scanning', 'photocurrent', 'microscopy', 'spcm', 'to', 'investigate', 'the', 'properties', 'of', 'internal', 'pn', 'junctions', 'as', 'well', 'as', 'local', 'defects', 'in', 'ambipolar', 'carbon', 'nanotube', 'cnt', 'transistors', 'our', 'spcm', 'images', 'show', 'strong', 'signals', 'near', 'metal', 'c... | [-0.14713750537743586, 0.05495011386261063, -0.08511762813173442, 0.0027775154521805234, -0.0037372814387910897, -0.18556208839193764, 0.08107220057839488, 0.46724895645295167, -0.26266976647699875, -0.34982961548181873, -0.011530933868521566, -0.2777346733580796, -0.1644867244208904, 0.22763493011653838, -0.0104641051... |
707.3177 | Towards a proof of the conjecture of Langlands and Rapoport | A conference talk discussing the conjecture of Langlands and Rapoport
concerning the structure of the points on a Shimura variety modulo a prime of
good reduction.
| math.NT math.AG | a conference talk discussing the conjecture of langlands and rapoport concerning the structure of the points on a shimura variety modulo a prime of good reduction | [['a', 'conference', 'talk', 'discussing', 'the', 'conjecture', 'of', 'langlands', 'and', 'rapoport', 'concerning', 'the', 'structure', 'of', 'the', 'points', 'on', 'a', 'shimura', 'variety', 'modulo', 'a', 'prime', 'of', 'good', 'reduction']] | [-0.2834684599477511, -0.04297048462411532, -0.21984270752335971, 0.07446933741896199, -0.1303505003810502, -0.1251181753244824, 0.05431816160965424, 0.1455443172643964, -0.2587583004855193, -0.32031340825443083, 0.09536997846757564, -0.2061531596655886, -0.15269545077955207, 0.244112455429366, -0.2044252993610616, 0.0... |
707.3178 | Vanishing theorems for toric polyhedra | A toric polyhedron is a reduced closed subscheme of a toric variety that are
partial unions of the orbits of the torus action. We prove vanishing theorems
for toric polyhedra. We also give a proof of the $E_1$-degeneration of Hodge to
de Rham type spectral sequence for toric polyhedra in any characteristic.
Finally, ... | math.AG | a toric polyhedron is a reduced closed subscheme of a toric variety that are partial unions of the orbits of the torus action we prove vanishing theorems for toric polyhedra we also give a proof of the e_1degeneration of hodge to de rham type spectral sequence for toric polyhedra in any characteristic finally we give a... | [['a', 'toric', 'polyhedron', 'is', 'a', 'reduced', 'closed', 'subscheme', 'of', 'a', 'toric', 'variety', 'that', 'are', 'partial', 'unions', 'of', 'the', 'orbits', 'of', 'the', 'torus', 'action', 'we', 'prove', 'vanishing', 'theorems', 'for', 'toric', 'polyhedra', 'we', 'also', 'give', 'a', 'proof', 'of', 'the', 'e_1d... | [-0.23751294601058204, -0.0191927709263779, -0.1425692497323903, 0.13267013579348308, -0.12317454492643712, -0.17755014850713668, -0.021801111101734615, 0.31100134190822404, -0.28793504881480386, -0.14258332245997965, 0.13476497311300287, -0.18289861620389045, -0.12305669789572084, 0.23178023304642428, -0.2329065797052... |
707.3179 | Combinatorial Aspects of Elliptic Curves | Given an elliptic curve C, we study here $N_k = #C(F_{q^k})$, the number of
points of C over the finite field F_{q^k}. This sequence of numbers, as k runs
over positive integers, has numerous remarkable properties of a combinatorial
flavor in addition to the usual number theoretical interpretations. In
particular we ... | math.CO math.NT | given an elliptic curve c we study here n_k cf_qk the number of points of c over the finite field f_qk this sequence of numbers as k runs over positive integers has numerous remarkable properties of a combinatorial flavor in addition to the usual number theoretical interpretations in particular we prove that n_k w_kq n... | [['given', 'an', 'elliptic', 'curve', 'c', 'we', 'study', 'here', 'n_k', 'cf_qk', 'the', 'number', 'of', 'points', 'of', 'c', 'over', 'the', 'finite', 'field', 'f_qk', 'this', 'sequence', 'of', 'numbers', 'as', 'k', 'runs', 'over', 'positive', 'integers', 'has', 'numerous', 'remarkable', 'properties', 'of', 'a', 'combi... | [-0.20672951420613875, 0.13138158459247887, -0.07736313778441399, 0.023748917629321416, -0.06926713660359382, -0.10670650068980952, 0.023843689070781694, 0.3116151207126677, -0.3121880882109205, -0.2573659342092772, 0.06377639803201116, -0.25245708477838585, -0.14868883725721388, 0.1985672128619626, -0.0718702931733181... |
707.318 | Two Trends of Composition Variation of Zircons and Their Significance in
Origin Discrimination | Zircons can crystallize in a wide range of physical and chemical conditions.
At the same time, they have high stability and durability. Therefore zircons
can grow and survive in a variety of geological processes. In addition, the
diffusivity of chemical compositions in their crystals is very low.
Consequently,we can ... | physics.geo-ph astro-ph cond-mat.mtrl-sci | zircons can crystallize in a wide range of physical and chemical conditions at the same time they have high stability and durability therefore zircons can grow and survive in a variety of geological processes in addition the diffusivity of chemical compositions in their crystals is very low consequentlywe can trace bac... | [['zircons', 'can', 'crystallize', 'in', 'a', 'wide', 'range', 'of', 'physical', 'and', 'chemical', 'conditions', 'at', 'the', 'same', 'time', 'they', 'have', 'high', 'stability', 'and', 'durability', 'therefore', 'zircons', 'can', 'grow', 'and', 'survive', 'in', 'a', 'variety', 'of', 'geological', 'processes', 'in', '... | [-0.05491852323813186, 0.18898449375842247, -0.09355703091057258, 0.01102390081641759, -0.04152079705348345, -0.04577457527301394, 0.05705801705533469, 0.42717042883287704, -0.3154294457140102, -0.33735380328870845, 0.08892860506888497, -0.2772225317986388, -0.13244007545875378, 0.1389286684465002, -0.06297205852090636... |
707.3181 | The Minerageny of Two Groups of Zircons from Plagioclase- Amphibolite of
Mayuan Group in Northern Fujian | Zircons can crystallize in a wide range of physical and chemical conditions.
At the same time, they have high stability and durability. Therefore zircons
can grow and survive in a variety of geological processes. In addition, the
diffusivity of chemical compositions in their crystals is very low.
Consequently,we can ... | physics.geo-ph astro-ph | zircons can crystallize in a wide range of physical and chemical conditions at the same time they have high stability and durability therefore zircons can grow and survive in a variety of geological processes in addition the diffusivity of chemical compositions in their crystals is very low consequentlywe can trace bac... | [['zircons', 'can', 'crystallize', 'in', 'a', 'wide', 'range', 'of', 'physical', 'and', 'chemical', 'conditions', 'at', 'the', 'same', 'time', 'they', 'have', 'high', 'stability', 'and', 'durability', 'therefore', 'zircons', 'can', 'grow', 'and', 'survive', 'in', 'a', 'variety', 'of', 'geological', 'processes', 'in', '... | [-0.031820546121175006, 0.1939025645976496, -0.13150751674421937, 0.0501405252825452, -0.0577010864136019, -0.06189031509875513, 0.03521104383351583, 0.4485839498522985, -0.30349768362026913, -0.33248063879976936, 0.08401811212617988, -0.26126678350071114, -0.1420621136465605, 0.17482563104954557, -0.06799613222949677,... |
707.3182 | Collider Signals of Gravitational Fixed Points | Recent studies have shown that the poor perturbative behavior of General
Relativity in the ultraviolet regime may be ameliorated by the existence of a
non-Gaussian fixed point which renders the theory asymptotically safe and
possibly non-perturbatively renormalizable. This results in a running of the
(effective) grav... | hep-ph hep-ex hep-th | recent studies have shown that the poor perturbative behavior of general relativity in the ultraviolet regime may be ameliorated by the existence of a nongaussian fixed point which renders the theory asymptotically safe and possibly nonperturbatively renormalizable this results in a running of the effective gravitation... | [['recent', 'studies', 'have', 'shown', 'that', 'the', 'poor', 'perturbative', 'behavior', 'of', 'general', 'relativity', 'in', 'the', 'ultraviolet', 'regime', 'may', 'be', 'ameliorated', 'by', 'the', 'existence', 'of', 'a', 'nongaussian', 'fixed', 'point', 'which', 'renders', 'the', 'theory', 'asymptotically', 'safe',... | [-0.13077528249935166, 0.20409312501066812, -0.07580122022108422, 0.14601764504087766, -0.04427253486111438, -0.13796377787653955, 0.01915994719070394, 0.3070457715075463, -0.18420201275543666, -0.2689111969623439, 0.02019214219942597, -0.2804924973551138, -0.10044665614223498, 0.12615517071551746, 0.03430405302536616,... |
707.3183 | Ferromagnetism as a universal feature of nanoparticles of the otherwise
nonmagnetic oxides | Room-temperature ferromagnetism has been observed in the nanoparticles (7 -
30 nm dia) of nonmagnetic oxides such as CeO2, Al2O3, ZnO, In2O3 and SnO2. The
saturated magnetic moments in CeO_2 and Al_2O_3 nanoparticles are comparable to
those observed in transition metal doped wide band semiconducting oxides. The
other... | cond-mat.mtrl-sci | roomtemperature ferromagnetism has been observed in the nanoparticles 7 30 nm dia of nonmagnetic oxides such as ceo2 al2o3 zno in2o3 and sno2 the saturated magnetic moments in ceo_2 and al_2o_3 nanoparticles are comparable to those observed in transition metal doped wide band semiconducting oxides the other oxide nanop... | [['roomtemperature', 'ferromagnetism', 'has', 'been', 'observed', 'in', 'the', 'nanoparticles', '7', '30', 'nm', 'dia', 'of', 'nonmagnetic', 'oxides', 'such', 'as', 'ceo2', 'al2o3', 'zno', 'in2o3', 'and', 'sno2', 'the', 'saturated', 'magnetic', 'moments', 'in', 'ceo_2', 'and', 'al_2o_3', 'nanoparticles', 'are', 'compar... | [-0.08383912598809565, 0.25577809527428363, 0.023699197314558624, 0.02479037591512865, 0.02964051779429245, -0.1701199734348833, 0.09350932651844726, 0.4802018154676505, -0.21338121764023613, -0.33107522834004377, -0.01786478501414572, -0.397710701553371, -0.08633275195501569, 0.14834967328741502, 0.0344573962868844, -... |
707.3184 | A Raman spectroscopic study of zircons on micro-scale and Its
significance in explaining the origin of zircons | The magmatic and metamorphic zircons were investigated with Raman spectrum
microprobe analysis. We found notable differences between these two kinds of
zircons exhibited by the variation trend of Raman peak intensity from core to
rim of a crystal. In magmatic zircons, the intensity and the ratio H/W of Raman
spectrum... | physics.geo-ph astro-ph physics.chem-ph | the magmatic and metamorphic zircons were investigated with raman spectrum microprobe analysis we found notable differences between these two kinds of zircons exhibited by the variation trend of raman peak intensity from core to rim of a crystal in magmatic zircons the intensity and the ratio hw of raman spectrum peaks... | [['the', 'magmatic', 'and', 'metamorphic', 'zircons', 'were', 'investigated', 'with', 'raman', 'spectrum', 'microprobe', 'analysis', 'we', 'found', 'notable', 'differences', 'between', 'these', 'two', 'kinds', 'of', 'zircons', 'exhibited', 'by', 'the', 'variation', 'trend', 'of', 'raman', 'peak', 'intensity', 'from', '... | [-0.05264992026980133, 0.18371952116646936, -0.09161059902264522, -0.004562465824069573, -0.010437516551942312, -0.0679849059291679, 0.06864417836369648, 0.4319794994414217, -0.3043660076882143, -0.3215638222335675, 0.06660087479985079, -0.32332925896088666, -0.11672789983388682, 0.15650769788039184, -0.036547321409403... |
707.3185 | Random generation of finitely generated subgroups of a free group | We give an efficient algorithm to randomly generate finitely generated
subgroups of a given size, in a finite rank free group. Here, the size of a
subgroup is the number of vertices of its representation by a reduced graph
such as can be obtained by the method of Stallings foldings. Our algorithm
randomly generates a... | math.GR math.CO | we give an efficient algorithm to randomly generate finitely generated subgroups of a given size in a finite rank free group here the size of a subgroup is the number of vertices of its representation by a reduced graph such as can be obtained by the method of stallings foldings our algorithm randomly generates a subgr... | [['we', 'give', 'an', 'efficient', 'algorithm', 'to', 'randomly', 'generate', 'finitely', 'generated', 'subgroups', 'of', 'a', 'given', 'size', 'in', 'a', 'finite', 'rank', 'free', 'group', 'here', 'the', 'size', 'of', 'a', 'subgroup', 'is', 'the', 'number', 'of', 'vertices', 'of', 'its', 'representation', 'by', 'a', '... | [-0.12390086950607977, 0.14453466598576398, -0.09805134862614007, -0.013330985634546147, -0.025833480210059274, -0.06575365632701413, 0.08864451237654282, 0.38150616801517495, -0.3023769947684417, -0.3332270337604144, 0.08844200067490465, -0.2646489149369931, -0.07137834812293492, 0.18657411129403292, -0.10182054792491... |
707.3186 | Kinematic and stiffness analysis of the Orthoglide, a PKM with simple,
regular workspace and homogeneous performances | The Orthoglide is a Delta-type PKM dedicated to 3-axis rapid machining
applications that was originally developed at IRCCyN in 2000-2001 to meet the
advantages of both serial 3-axis machines (regular workspace and homogeneous
performances) and parallel kinematic architectures (good dynamic performances
and stiffness)... | cs.RO | the orthoglide is a deltatype pkm dedicated to 3axis rapid machining applications that was originally developed at irccyn in 20002001 to meet the advantages of both serial 3axis machines regular workspace and homogeneous performances and parallel kinematic architectures good dynamic performances and stiffness this mach... | [['the', 'orthoglide', 'is', 'a', 'deltatype', 'pkm', 'dedicated', 'to', '3axis', 'rapid', 'machining', 'applications', 'that', 'was', 'originally', 'developed', 'at', 'irccyn', 'in', '20002001', 'to', 'meet', 'the', 'advantages', 'of', 'both', 'serial', '3axis', 'machines', 'regular', 'workspace', 'and', 'homogeneous'... | [-0.15745836270721875, 0.07679464517308301, -0.06297915845521186, -0.05197342798132204, -0.16602920971988505, -0.1741845753644348, -0.06234587731964175, 0.4292680538308464, -0.26565292277863545, -0.2862996294264265, 0.10033142319968504, -0.20898204529045247, -0.10869344697015262, 0.1689216746078608, -0.1133245047837446... |
707.3187 | The barnes G function and its relations with sums and products of
generalized Gamma convolution variables | We give a probabilistic interpretation for the Barnes G-function which
appears in random matrix theory and in analytic number theory in the important
moments conjecture due to Keating-Snaith for the Riemann zeta function, via the
analogy with the characteristic polynomial of random unitary matrices. We show
that the ... | math.PR | we give a probabilistic interpretation for the barnes gfunction which appears in random matrix theory and in analytic number theory in the important moments conjecture due to keatingsnaith for the riemann zeta function via the analogy with the characteristic polynomial of random unitary matrices we show that the mellin... | [['we', 'give', 'a', 'probabilistic', 'interpretation', 'for', 'the', 'barnes', 'gfunction', 'which', 'appears', 'in', 'random', 'matrix', 'theory', 'and', 'in', 'analytic', 'number', 'theory', 'in', 'the', 'important', 'moments', 'conjecture', 'due', 'to', 'keatingsnaith', 'for', 'the', 'riemann', 'zeta', 'function', ... | [-0.12334352360597549, 0.15188396796370848, -0.13168503845977875, 0.07372962074880382, -0.05605860210898268, -0.10815149718426338, 0.03208668652801056, 0.31144819164094123, -0.33001238163134067, -0.1991609070691785, 0.06613575896774312, -0.22897214443024733, -0.2404522281513329, 0.19993467698449569, -0.0351094026722810... |
707.3188 | The cubic nonlinear Schr\"odinger equation in two dimensions with radial
data | We establish global well-posedness and scattering for solutions to the
mass-critical nonlinear Schr\"odinger equation $iu_t + \Delta u = \pm |u|^2 u$
for large spherically symmetric L^2_x(\R^2) initial data; in the focusing case
we require, of course, that the mass is strictly less than that of the ground
state. As a... | math.AP | we establish global wellposedness and scattering for solutions to the masscritical nonlinear schrodinger equation iu_t delta u pm u2 u for large spherically symmetric l2_xr2 initial data in the focusing case we require of course that the mass is strictly less than that of the ground state as a consequence we deduce tha... | [['we', 'establish', 'global', 'wellposedness', 'and', 'scattering', 'for', 'solutions', 'to', 'the', 'masscritical', 'nonlinear', 'schrodinger', 'equation', 'iu_t', 'delta', 'u', 'pm', 'u2', 'u', 'for', 'large', 'spherically', 'symmetric', 'l2_xr2', 'initial', 'data', 'in', 'the', 'focusing', 'case', 'we', 'require', ... | [-0.15142046558229547, 0.07049234575640999, -0.04656215776738368, 0.07137129081192574, -0.06376406301401163, -0.1405386634121992, -0.0051354820987111645, 0.3169690027734951, -0.21617733148955984, -0.2209284377039263, 0.16420574463830379, -0.3188122634138716, -0.0633421910338496, 0.14431825825258304, 0.00404054454386488... |
707.3189 | Fusion Algebras of Logarithmic Minimal Models | We present explicit conjectures for the chiral fusion algebras of the
logarithmic minimal models LM(p,p') considering Virasoro representations with
no enlarged or extended symmetry algebra. The generators of fusion are
countably infinite in number but the ensuing fusion rules are quasi-rational in
the sense that the ... | hep-th cond-mat.stat-mech math-ph math.MP | we present explicit conjectures for the chiral fusion algebras of the logarithmic minimal models lmpp considering virasoro representations with no enlarged or extended symmetry algebra the generators of fusion are countably infinite in number but the ensuing fusion rules are quasirational in the sense that the fusion o... | [['we', 'present', 'explicit', 'conjectures', 'for', 'the', 'chiral', 'fusion', 'algebras', 'of', 'the', 'logarithmic', 'minimal', 'models', 'lmpp', 'considering', 'virasoro', 'representations', 'with', 'no', 'enlarged', 'or', 'extended', 'symmetry', 'algebra', 'the', 'generators', 'of', 'fusion', 'are', 'countably', '... | [-0.10272212110935373, 0.11170609197783671, -0.07016937306803966, 0.04685341345958729, -0.09159124413941135, -0.1409846617629692, 0.00997755928249891, 0.37314116257599533, -0.2814760510671012, -0.19691982599807548, 0.11581493000787227, -0.2462350096177072, -0.14545194095377117, 0.1505428298039639, -0.06150479576391901,... |
707.319 | Electromagnetism and perfect fluids interplay in multidimensional
spacetimes | We consider fields in (D>2)-dimensional spacetime, whose potential is r-form
(skew-symmetric tensor of rank r), the field tensor F being its exterior
derivative and the Lagrangian, a function of the quadratic invariant I of this
tensor. It is shown that vector field (r=1) describes electromagnetic field
only for D=4.... | gr-qc | we consider fields in d2dimensional spacetime whose potential is rform skewsymmetric tensor of rank r the field tensor f being its exterior derivative and the lagrangian a function of the quadratic invariant i of this tensor it is shown that vector field r1 describes electromagnetic field only for d4 in particular for ... | [['we', 'consider', 'fields', 'in', 'd2dimensional', 'spacetime', 'whose', 'potential', 'is', 'rform', 'skewsymmetric', 'tensor', 'of', 'rank', 'r', 'the', 'field', 'tensor', 'f', 'being', 'its', 'exterior', 'derivative', 'and', 'the', 'lagrangian', 'a', 'function', 'of', 'the', 'quadratic', 'invariant', 'i', 'of', 'th... | [-0.22317754031186376, 0.1413342996555216, -0.05720441688043887, -0.008797361081301728, -0.0945755822419682, -0.1544989850207725, -0.11398416134967085, 0.3020069031154408, -0.23216355160317, -0.21748272708671934, 0.06322707179659869, -0.22976824702585444, -0.1810277648626224, 0.0640659068218049, -0.0049818495398058615,... |
707.3191 | Toward Coupling Flow Driven and Magnetically Driven Dynamos | Most large scale dynamo research for astrophysical rotators focuses on
interior flow driven helical dynamos (FDHDs), but larger scale coronal fields
most directly influence observations. It is thus important to understand the
relationship between coronal and interior fields. Coronal field relaxation is
actually a typ... | astro-ph physics.plasm-ph | most large scale dynamo research for astrophysical rotators focuses on interior flow driven helical dynamos fdhds but larger scale coronal fields most directly influence observations it is thus important to understand the relationship between coronal and interior fields coronal field relaxation is actually a type of ma... | [['most', 'large', 'scale', 'dynamo', 'research', 'for', 'astrophysical', 'rotators', 'focuses', 'on', 'interior', 'flow', 'driven', 'helical', 'dynamos', 'fdhds', 'but', 'larger', 'scale', 'coronal', 'fields', 'most', 'directly', 'influence', 'observations', 'it', 'is', 'thus', 'important', 'to', 'understand', 'the', ... | [-0.16432782094463283, 0.28907518919339775, -0.027209064629298788, 0.12793490315906386, -0.11724069563619105, -0.0965177757642397, -0.014614445405041284, 0.365713571165259, -0.27795305918301094, -0.3256521704507635, 0.08181893634808032, -0.18717431897257872, -0.09618522218223793, 0.22975563022790227, 0.0205065803073927... |
707.3192 | Zeeman-type dragging in the Kerr--Newman and NUT spacetimes | In this communication we discuss two distinct Zeeman-type gravitomagnetic
effects deserving attention since they can be easily characterized in their
exact form, not via approximation procedures. Some observations are also made
on gravitoelectric effects.
| gr-qc | in this communication we discuss two distinct zeemantype gravitomagnetic effects deserving attention since they can be easily characterized in their exact form not via approximation procedures some observations are also made on gravitoelectric effects | [['in', 'this', 'communication', 'we', 'discuss', 'two', 'distinct', 'zeemantype', 'gravitomagnetic', 'effects', 'deserving', 'attention', 'since', 'they', 'can', 'be', 'easily', 'characterized', 'in', 'their', 'exact', 'form', 'not', 'via', 'approximation', 'procedures', 'some', 'observations', 'are', 'also', 'made', ... | [-0.17919055591611302, 0.18119221314897432, -0.07889603491982117, 0.1664292125736692, -0.14137024667990558, -0.15533890931264444, 0.018429870491244775, 0.4755765911301269, -0.24158023779883103, -0.28888838891597357, 0.13267651181805, -0.23213282443911715, -0.215588728130302, 0.20744802200180643, -0.06773421858601711, -... |
707.3193 | Nariai--Bertotti--Robinson spacetimes as a building material for one-way
wormholes with horizons, but without singularity | We discuss the problem of wormholes from the viewpoint of gluing together two
Reissner--Nordstr\"om-type universes while putting between them a segment of
the Nariai-type world (in both cases there are also present electromagnetic
fields as well as the cosmological constant). Such a toy wormhole represents an
example... | gr-qc | we discuss the problem of wormholes from the viewpoint of gluing together two reissnernordstromtype universes while putting between them a segment of the nariaitype world in both cases there are also present electromagnetic fields as well as the cosmological constant such a toy wormhole represents an example of oneway ... | [['we', 'discuss', 'the', 'problem', 'of', 'wormholes', 'from', 'the', 'viewpoint', 'of', 'gluing', 'together', 'two', 'reissnernordstromtype', 'universes', 'while', 'putting', 'between', 'them', 'a', 'segment', 'of', 'the', 'nariaitype', 'world', 'in', 'both', 'cases', 'there', 'are', 'also', 'present', 'electromagnet... | [-0.1685288175149768, 0.09426541736842033, -0.07247340263587967, 0.09665145522932399, -0.09047581910217216, -0.16978489736288363, 0.013990461026792819, 0.3604028129001271, -0.23046840029496277, -0.28173049248948273, 0.09415923072824711, -0.3035242702056355, -0.10616786100567793, 0.1943651745974455, -0.03772461734149816... |
707.3194 | T-odd asymmetries in radiative top-quark decays | We study the angular distribution of the charged lepton in the top-quark
decay into a bottom quark and a W boson which subsequently decays into
\ell\nu_{\ell}, when a hard gluon is radiated off. The absorptive part of the t
\to bWg decay amplitudes, which gives rise to T-odd asymmetries in the
distribution, is calcul... | hep-ph | we study the angular distribution of the charged lepton in the topquark decay into a bottom quark and a w boson which subsequently decays into ellnu_ell when a hard gluon is radiated off the absorptive part of the t to bwg decay amplitudes which gives rise to todd asymmetries in the distribution is calculated at the on... | [['we', 'study', 'the', 'angular', 'distribution', 'of', 'the', 'charged', 'lepton', 'in', 'the', 'topquark', 'decay', 'into', 'a', 'bottom', 'quark', 'and', 'a', 'w', 'boson', 'which', 'subsequently', 'decays', 'into', 'ellnu_ell', 'when', 'a', 'hard', 'gluon', 'is', 'radiated', 'off', 'the', 'absorptive', 'part', 'of... | [-0.0632773635806153, 0.2942458767589037, -0.13976785976609046, 0.1683605477945613, -0.0369482786672843, -0.13334676018589503, 0.050643857261589306, 0.308211567823763, -0.23216989839921234, -0.21230376055222247, -0.021970501748615173, -0.33966550397892276, 0.08421590904910843, 0.11806148455732247, 0.12151259289111023, ... |
707.3195 | Galilean geometry of motions | In this paper we show that Galilean group is a matrix Lie group and find its
structure. Then provide the invariants of special Galilean geometry of motions,
by Olver's method of moving coframes, we also find the corresponding
$\{e\}-$structure.
| math.DG | in this paper we show that galilean group is a matrix lie group and find its structure then provide the invariants of special galilean geometry of motions by olvers method of moving coframes we also find the corresponding estructure | [['in', 'this', 'paper', 'we', 'show', 'that', 'galilean', 'group', 'is', 'a', 'matrix', 'lie', 'group', 'and', 'find', 'its', 'structure', 'then', 'provide', 'the', 'invariants', 'of', 'special', 'galilean', 'geometry', 'of', 'motions', 'by', 'olvers', 'method', 'of', 'moving', 'coframes', 'we', 'also', 'find', 'the',... | [-0.159451675386383, 0.07433347478926851, -0.15108859457839757, 0.01095227207033298, -0.10666614430598341, -0.06688610426126382, -0.006565442482660262, 0.4036472363349719, -0.3037650384582006, -0.26064861334191686, 0.10701789167554428, -0.1845902680264165, -0.2585248564704297, 0.14085342564981262, -0.10215254378719972,... |
707.3196 | Effect of Soft Modes on the Shear Viscosity of Quark Matter | We calculate shear viscosity of the quark matter at finite temperature and
density. If we assume that the quark interacts with the soft mode, which is a
collective mode of quark-antiquark pair, the self energy of the quark is
calculated by using the quasi-particle random phase approximation. It is shown
that its imag... | hep-ph | we calculate shear viscosity of the quark matter at finite temperature and density if we assume that the quark interacts with the soft mode which is a collective mode of quarkantiquark pair the self energy of the quark is calculated by using the quasiparticle random phase approximation it is shown that its imaginary pa... | [['we', 'calculate', 'shear', 'viscosity', 'of', 'the', 'quark', 'matter', 'at', 'finite', 'temperature', 'and', 'density', 'if', 'we', 'assume', 'that', 'the', 'quark', 'interacts', 'with', 'the', 'soft', 'mode', 'which', 'is', 'a', 'collective', 'mode', 'of', 'quarkantiquark', 'pair', 'the', 'self', 'energy', 'of', '... | [-0.12328786829925212, 0.3064858931432332, -0.1353572856149952, 0.04995866767938965, -0.07726548123000536, -0.06538366251586636, 0.04099967073041114, 0.297340110560094, -0.27610552230896046, -0.24609749106890408, 0.017766674149258078, -0.29354938636880273, -0.039325244801719325, 0.12498570796225436, 0.04415465309477049... |
707.3197 | Phase diagram for the one-dimensional Hubbard-Holstein model: A
density-matrix renormalization group study | Phase diagram of the Hubbard-Holstein model in the coexistence of
electron-electron and electron-phonon interactions has been theoretically
obtained with the density-matrix renormalization group method for
one-dimensional (1D) systems, where an improved warm-up (the recursive sweep)
procedure has enabled us to calcul... | cond-mat.str-el cond-mat.supr-con | phase diagram of the hubbardholstein model in the coexistence of electronelectron and electronphonon interactions has been theoretically obtained with the densitymatrix renormalization group method for onedimensional 1d systems where an improved warmup the recursive sweep procedure has enabled us to calculate various c... | [['phase', 'diagram', 'of', 'the', 'hubbardholstein', 'model', 'in', 'the', 'coexistence', 'of', 'electronelectron', 'and', 'electronphonon', 'interactions', 'has', 'been', 'theoretically', 'obtained', 'with', 'the', 'densitymatrix', 'renormalization', 'group', 'method', 'for', 'onedimensional', '1d', 'systems', 'where... | [-0.15467306518008653, 0.16687389458970195, -0.05163873198652665, 0.07461909414109558, -0.009526561626730717, -0.18795939068284448, 0.06509688885703888, 0.4053427513101942, -0.24319599091700494, -0.23085413655036524, 0.022101470208663033, -0.3058700570326349, -0.12835257841841866, 0.14614214404639214, 0.098336811379763... |
707.3198 | Growth-optimal portfolios under transaction costs | This paper studies a portfolio optimization problem in a discrete-time
Markovian model of a financial market, in which asset price dynamics depend on
an external process of economic factors. There are transaction costs with a
structure that covers, in particular, the case of fixed plus proportional
costs. We prove th... | q-fin.PM math.OC math.PR | this paper studies a portfolio optimization problem in a discretetime markovian model of a financial market in which asset price dynamics depend on an external process of economic factors there are transaction costs with a structure that covers in particular the case of fixed plus proportional costs we prove that there... | [['this', 'paper', 'studies', 'a', 'portfolio', 'optimization', 'problem', 'in', 'a', 'discretetime', 'markovian', 'model', 'of', 'a', 'financial', 'market', 'in', 'which', 'asset', 'price', 'dynamics', 'depend', 'on', 'an', 'external', 'process', 'of', 'economic', 'factors', 'there', 'are', 'transaction', 'costs', 'wi... | [-0.12831852811059968, 0.048624512252275716, -0.11412814533447518, 0.0847245771807388, -0.044140583650647276, -0.13242418915672483, 0.16620503135103112, 0.38827226003723253, -0.2899766803043438, -0.20496020382087604, 0.1650398888581834, -0.28947205596840847, -0.181132193645645, 0.16417612307294108, -0.1460666783615107,... |
707.3199 | Review of diffraction at HERA and Tevatron | We present and discuss the recent results on diffraction from the HERA and
Tevatron experiments.
| hep-ph | we present and discuss the recent results on diffraction from the hera and tevatron experiments | [['we', 'present', 'and', 'discuss', 'the', 'recent', 'results', 'on', 'diffraction', 'from', 'the', 'hera', 'and', 'tevatron', 'experiments']] | [0.0310300067688028, 0.08219936549042663, -0.11653570185105006, 0.0290959099928538, -0.062358799452583, 0.012091910474312802, 0.06440886822529138, 0.4375211000442505, -0.1558978104343017, -0.23215059315164885, 0.13081022423381608, -0.4396565990522504, -0.11452010969320933, 0.27489588807026544, 0.07126722956697146, 0.17... |
707.32 | Enhancing single-molecule photostability by optical feedback from
quantum-jump detection | We report an optical technique that yields an enhancement of single-molecule
photostability, by greatly suppressing photobleaching pathways which involve
photoexcitation from the triplet state. This is accomplished by dynamically
switching off the excitation laser when a quantum-jump of the molecule to the
triplet st... | quant-ph physics.chem-ph physics.optics | we report an optical technique that yields an enhancement of singlemolecule photostability by greatly suppressing photobleaching pathways which involve photoexcitation from the triplet state this is accomplished by dynamically switching off the excitation laser when a quantumjump of the molecule to the triplet state is... | [['we', 'report', 'an', 'optical', 'technique', 'that', 'yields', 'an', 'enhancement', 'of', 'singlemolecule', 'photostability', 'by', 'greatly', 'suppressing', 'photobleaching', 'pathways', 'which', 'involve', 'photoexcitation', 'from', 'the', 'triplet', 'state', 'this', 'is', 'accomplished', 'by', 'dynamically', 'swi... | [-0.11989533996328394, 0.174479279983411, -0.06209962912637027, -0.02126245626664542, 0.020710492050869667, -0.13134075379236898, 0.1130771876196377, 0.41669214356868983, -0.27701681764162284, -0.3277567544694435, 0.0020430381087824068, -0.2538126681713348, -0.084643917792338, 0.19941468542798402, 0.015263977510101617,... |
707.3201 | Evidence for a breakdown of the Isobaric Multiplet Mass Equation: A
study of the A=35, T=3/2 isospin quartet | Mass measurements on radionuclides along the potassium isotope chain have
been performed with the ISOLTRAP Penning trap mass spectrometer. For 35K
T1/2=178ms) to 46K (T1/2=105s) relative mass uncertainties of 2x10-8 and better
have been achieved. The accurate mass determination of 35K (dm=0.54keV) has
been exploited ... | nucl-ex | mass measurements on radionuclides along the potassium isotope chain have been performed with the isoltrap penning trap mass spectrometer for 35k t12178ms to 46k t12105s relative mass uncertainties of 2x108 and better have been achieved the accurate mass determination of 35k dm054kev has been exploited to test the isob... | [['mass', 'measurements', 'on', 'radionuclides', 'along', 'the', 'potassium', 'isotope', 'chain', 'have', 'been', 'performed', 'with', 'the', 'isoltrap', 'penning', 'trap', 'mass', 'spectrometer', 'for', '35k', 't12178ms', 'to', '46k', 't12105s', 'relative', 'mass', 'uncertainties', 'of', '2x108', 'and', 'better', 'hav... | [-0.028523279752610535, 0.17168475840607603, -0.06625140998794725, 0.05042709716398156, -0.004760225938463753, -0.13307969952989934, 0.013186673231592233, 0.3844717429725058, -0.11312705260625631, -0.3508883447555656, 0.05570367335652312, -0.3078492041959455, 0.08035454707163753, 0.2417601261739478, 0.02243363850919360... |
707.3202 | Stability in the instantaneous Bethe-Salpeter formalism:
harmonic-oscillator reduced Salpeter equation | A popular three-dimensional reduction of the Bethe-Salpeter formalism for the
description of bound states in quantum field theory is the Salpeter equation,
derived by assuming both instantaneous interactions and free propagation of all
bound-state constituents. Numerical (variational) studies of the Salpeter
equation... | hep-ph nucl-th | a popular threedimensional reduction of the bethesalpeter formalism for the description of bound states in quantum field theory is the salpeter equation derived by assuming both instantaneous interactions and free propagation of all boundstate constituents numerical variational studies of the salpeter equation with con... | [['a', 'popular', 'threedimensional', 'reduction', 'of', 'the', 'bethesalpeter', 'formalism', 'for', 'the', 'description', 'of', 'bound', 'states', 'in', 'quantum', 'field', 'theory', 'is', 'the', 'salpeter', 'equation', 'derived', 'by', 'assuming', 'both', 'instantaneous', 'interactions', 'and', 'free', 'propagation',... | [-0.11998681094224468, 0.12536878973872356, -0.09779510297110015, 0.115380622508759, -0.0651357655116389, -0.1496910126076947, 0.02846270546032084, 0.2970413516018668, -0.21973808823105204, -0.298371700329128, 0.0457135180065585, -0.30049071669305577, -0.10187388159703978, 0.16276639830802792, 0.04485786299156989, 0.08... |
707.3203 | Geo-neutrinos and Earth's interior | The deepest hole that has ever been dug is about 12 km deep. Geochemists
analyze samples from the Earth's crust and from the top of the mantle.
Seismology can reconstruct the density profile throughout all Earth, but not
its composition. In this respect, our planet is mainly unexplored.
Geo-neutrinos, the antineutrin... | physics.geo-ph astro-ph hep-ph nucl-ex nucl-th | the deepest hole that has ever been dug is about 12 km deep geochemists analyze samples from the earths crust and from the top of the mantle seismology can reconstruct the density profile throughout all earth but not its composition in this respect our planet is mainly unexplored geoneutrinos the antineutrinos from the... | [['the', 'deepest', 'hole', 'that', 'has', 'ever', 'been', 'dug', 'is', 'about', '12', 'km', 'deep', 'geochemists', 'analyze', 'samples', 'from', 'the', 'earths', 'crust', 'and', 'from', 'the', 'top', 'of', 'the', 'mantle', 'seismology', 'can', 'reconstruct', 'the', 'density', 'profile', 'throughout', 'all', 'earth', '... | [-0.05139781572563829, 0.1901766777653369, -0.06710775428622036, 0.06311665596881748, -0.07607509305219781, -0.012708246458346157, 0.06321639043135946, 0.3092841251929796, -0.2625594093111265, -0.32136578864328186, 0.13262175736732756, -0.3204983402853162, -0.09572193097761449, 0.2238040760682981, -0.03325331415920184,... |
707.3204 | Emergence of the NMSGUT | We trace the emergence of the ``New Minimal'' supersymmetric SO(10) GUT
(NMSGUT) out of the debris created by our demonstration that the MSGUT is
falsified by the data. The NMSGUT is based on ${\bf{210\oplus 10\oplus
120\oplus 126\oplus {\bar {126}}}}$ Higgs system. It has only spontaneous CP
violation and Type I see... | hep-ph | we trace the emergence of the new minimal supersymmetric so10 gut nmsgut out of the debris created by our demonstration that the msgut is falsified by the data the nmsgut is based on bf210oplus 10oplus 120oplus 126oplus bar 126 higgs system it has only spontaneous cp violation and type i seesaw with only 24 real superp... | [['we', 'trace', 'the', 'emergence', 'of', 'the', 'new', 'minimal', 'supersymmetric', 'so10', 'gut', 'nmsgut', 'out', 'of', 'the', 'debris', 'created', 'by', 'our', 'demonstration', 'that', 'the', 'msgut', 'is', 'falsified', 'by', 'the', 'data', 'the', 'nmsgut', 'is', 'based', 'on', 'bf210oplus', '10oplus', '120oplus',... | [-0.10155875701746493, 0.20941375866127404, -0.015570509474527854, 0.12504163206849964, -0.10449165654200945, -0.16778069867872522, 0.0645581773028171, 0.25696027335300115, -0.2060928163010199, -0.32982345812184655, 0.08798804558648711, -0.2688926598924843, -0.07695776037293377, 0.13357893056930362, 0.00563800072417484... |
707.3205 | Neutrality and Many-Valued Logics | In this book, we consider various many-valued logics: standard, linear,
hyperbolic, parabolic, non-Archimedean, p-adic, interval, neutrosophic, etc. We
survey also results which show the tree different proof-theoretic frameworks
for many-valued logics, e.g. frameworks of the following deductive calculi:
Hilbert's sty... | cs.LO cs.AI | in this book we consider various manyvalued logics standard linear hyperbolic parabolic nonarchimedean padic interval neutrosophic etc we survey also results which show the tree different prooftheoretic frameworks for manyvalued logics eg frameworks of the following deductive calculi hilberts style sequent and hyperseq... | [['in', 'this', 'book', 'we', 'consider', 'various', 'manyvalued', 'logics', 'standard', 'linear', 'hyperbolic', 'parabolic', 'nonarchimedean', 'padic', 'interval', 'neutrosophic', 'etc', 'we', 'survey', 'also', 'results', 'which', 'show', 'the', 'tree', 'different', 'prooftheoretic', 'frameworks', 'for', 'manyvalued',... | [-0.11751352755981646, 0.060346636500830206, -0.13746842867724454, 0.17593325294441525, -0.2342676631572425, -0.14384788601617715, 0.057246111917671316, 0.3496717002026286, -0.33121512582300194, -0.21721566738976036, 0.04972875146580872, -0.26753164037395116, -0.0674612307268533, 0.17809183156536001, -0.201858230208040... |
707.3206 | A random walker on a ratchet potential: Effect of a non Gaussian noise | We analyze the effect of a colored non Gaussian noise on a model of a random
walker moving along a ratchet potential. Such a model was motivated by the
transport properties of motor proteins, like kinesin and myosin. Previous
studies have been realized assuming white noises. However, for real situations,
in general w... | cond-mat.stat-mech cond-mat.other | we analyze the effect of a colored non gaussian noise on a model of a random walker moving along a ratchet potential such a model was motivated by the transport properties of motor proteins like kinesin and myosin previous studies have been realized assuming white noises however for real situations in general we could ... | [['we', 'analyze', 'the', 'effect', 'of', 'a', 'colored', 'non', 'gaussian', 'noise', 'on', 'a', 'model', 'of', 'a', 'random', 'walker', 'moving', 'along', 'a', 'ratchet', 'potential', 'such', 'a', 'model', 'was', 'motivated', 'by', 'the', 'transport', 'properties', 'of', 'motor', 'proteins', 'like', 'kinesin', 'and', ... | [-0.09207167568021134, 0.15757242511179237, -0.06755934086948877, 0.07000270205049883, -0.03184528381670596, -0.17405297016709675, 0.050164717801829385, 0.3909784761242202, -0.27460459372425666, -0.24450218822562791, 0.08537068501492719, -0.2910977949495198, -0.2337606569568886, 0.23346762949997774, -0.0952929034485619... |
707.3207 | Index theory for actions of compact Lie groups on C*-algebras | We study the index theory for actions of compact Lie groups on C*-algebras
with an emphasis on principal actions. Given an invariant semifinite trace on
the C*-algebra we obtain semifinite spectral triples. For circle actions we
consider the relation to the dual Pimsner-Voiculescu sequence. On the way we
show that th... | math.KT math.OA | we study the index theory for actions of compact lie groups on calgebras with an emphasis on principal actions given an invariant semifinite trace on the calgebra we obtain semifinite spectral triples for circle actions we consider the relation to the dual pimsnervoiculescu sequence on the way we show that the notions ... | [['we', 'study', 'the', 'index', 'theory', 'for', 'actions', 'of', 'compact', 'lie', 'groups', 'on', 'calgebras', 'with', 'an', 'emphasis', 'on', 'principal', 'actions', 'given', 'an', 'invariant', 'semifinite', 'trace', 'on', 'the', 'calgebra', 'we', 'obtain', 'semifinite', 'spectral', 'triples', 'for', 'circle', 'act... | [-0.13724652307462834, 0.08698027350779046, -0.09161875154527407, 0.09217266587629205, -0.10719728248474734, -0.08720955902355768, 0.01448212969782097, 0.48688666336238384, -0.27245072251747526, -0.19493594163260053, 0.15210562837975367, -0.26459923903975224, -0.11251104631949038, 0.2008097902354267, -0.204329322077452... |
707.3208 | Amplification of gravitational waves signal in Michelson
coherent-squeezed interferometer | Gravitational waves reaching a Michelson interferometer are expected to
induce a very small change in the length of its arms causing a phase shift
between them, but it is very difficult to observe the extremely small phase
shift signals produced. In the present letter we show that the gravitational
waves signal could... | gr-qc | gravitational waves reaching a michelson interferometer are expected to induce a very small change in the length of its arms causing a phase shift between them but it is very difficult to observe the extremely small phase shift signals produced in the present letter we show that the gravitational waves signal could be ... | [['gravitational', 'waves', 'reaching', 'a', 'michelson', 'interferometer', 'are', 'expected', 'to', 'induce', 'a', 'very', 'small', 'change', 'in', 'the', 'length', 'of', 'its', 'arms', 'causing', 'a', 'phase', 'shift', 'between', 'them', 'but', 'it', 'is', 'very', 'difficult', 'to', 'observe', 'the', 'extremely', 'sm... | [-0.20013497363916546, 0.24344648550844417, -0.08052302051391218, 0.0633031305133617, -0.06876959737958445, -0.14288986256088382, 0.031090241648936236, 0.33897179447161324, -0.2692215078211618, -0.2935133664253748, 0.05761063811896404, -0.254587806885734, -0.10160051036989258, 0.2113708292585124, -0.02282275762350398, ... |
707.3209 | Commensurability effects for fermionic atoms trapped in 1D optical
lattices | Fermionic atoms in two different hyperfine states confined in optical
lattices show strong commensurability effects due to the interplay between the
atomic density wave (ADW) ordering and the lattice potential. We show that
spatially separated regions of commensurable and incommensurable phases can
coexist. The comme... | cond-mat.str-el | fermionic atoms in two different hyperfine states confined in optical lattices show strong commensurability effects due to the interplay between the atomic density wave adw ordering and the lattice potential we show that spatially separated regions of commensurable and incommensurable phases can coexist the commensurab... | [['fermionic', 'atoms', 'in', 'two', 'different', 'hyperfine', 'states', 'confined', 'in', 'optical', 'lattices', 'show', 'strong', 'commensurability', 'effects', 'due', 'to', 'the', 'interplay', 'between', 'the', 'atomic', 'density', 'wave', 'adw', 'ordering', 'and', 'the', 'lattice', 'potential', 'we', 'show', 'that'... | [-0.22359085041615698, 0.2878908854003789, -0.01931674828908096, 0.04509662580676377, 0.05127873377771013, -0.11971240661417444, 0.07350414448107283, 0.41631796480053, -0.29647944163944984, -0.25492103829876417, -0.003581447900311711, -0.26766448541052845, -0.09693303298101658, 0.12150323745380673, 0.06766219575163429,... |
707.321 | Applications of the change-of-rings spectral sequence to the computation
of Hochschild cohomology | We consider the change-of-rings spectral sequence as it applies to Hochschild
cohomology, obtaining a description of the differentials on the first page
which relates it to the multiplicative stucture on cohomology. Using this
information, we are able to completely describe the cohomology structure of
monogenic algeb... | math.KT | we consider the changeofrings spectral sequence as it applies to hochschild cohomology obtaining a description of the differentials on the first page which relates it to the multiplicative stucture on cohomology using this information we are able to completely describe the cohomology structure of monogenic algebras as ... | [['we', 'consider', 'the', 'changeofrings', 'spectral', 'sequence', 'as', 'it', 'applies', 'to', 'hochschild', 'cohomology', 'obtaining', 'a', 'description', 'of', 'the', 'differentials', 'on', 'the', 'first', 'page', 'which', 'relates', 'it', 'to', 'the', 'multiplicative', 'stucture', 'on', 'cohomology', 'using', 'thi... | [-0.09190799220911382, 0.004766546333363901, -0.11915415949188173, 0.1317357619040801, -0.1173008839522178, -0.10586867683256666, -0.0034932681097416206, 0.3525710281605522, -0.3403685990041898, -0.2569741797555859, 0.1375535364165747, -0.19756170248923202, -0.19348170711503673, 0.19711562934874868, -0.1781353431288153... |
707.3211 | Asymptotic behavior and orbital stability of galactic dynamics in
relativistic scalar gravity | The Nordstr\"om-Vlasov system is a relativistic Lorentz invariant
generalization of the Vlasov-Poisson system in the gravitational case. The
asymptotic behavior of solutions and the non-linear stability of steady states
are investigated. It is shown that solutions of the Nordstr\"om-Vlasov system
with energy grater o... | math-ph math.MP | the nordstromvlasov system is a relativistic lorentz invariant generalization of the vlasovpoisson system in the gravitational case the asymptotic behavior of solutions and the nonlinear stability of steady states are investigated it is shown that solutions of the nordstromvlasov system with energy grater or equal to t... | [['the', 'nordstromvlasov', 'system', 'is', 'a', 'relativistic', 'lorentz', 'invariant', 'generalization', 'of', 'the', 'vlasovpoisson', 'system', 'in', 'the', 'gravitational', 'case', 'the', 'asymptotic', 'behavior', 'of', 'solutions', 'and', 'the', 'nonlinear', 'stability', 'of', 'steady', 'states', 'are', 'investiga... | [-0.18532418754755714, 0.09065605735599573, -0.09281390793797262, 0.10858374529184317, -0.042432815354879735, -0.10098680486586296, -0.034314394243202116, 0.25320285546400073, -0.22676991462654802, -0.2749934525070888, 0.11966986763554643, -0.2651180445023303, -0.0932850034974454, 0.18014153841452427, -0.01243286694944... |
707.3212 | Signature of chirality in scanning-probe imaging of charge flow in
graphene | We theoretically propose to directly observe the chiral nature of charge
carriers in graphene mono- and bilayers within a controlled scattering
experiment. The charge located on a capacitively coupled scanning probe
microscope (SPM) tip acts as a scattering center with controllable position on
the graphene sheet. Una... | cond-mat.mes-hall | we theoretically propose to directly observe the chiral nature of charge carriers in graphene mono and bilayers within a controlled scattering experiment the charge located on a capacitively coupled scanning probe microscope spm tip acts as a scattering center with controllable position on the graphene sheet unambiguou... | [['we', 'theoretically', 'propose', 'to', 'directly', 'observe', 'the', 'chiral', 'nature', 'of', 'charge', 'carriers', 'in', 'graphene', 'mono', 'and', 'bilayers', 'within', 'a', 'controlled', 'scattering', 'experiment', 'the', 'charge', 'located', 'on', 'a', 'capacitively', 'coupled', 'scanning', 'probe', 'microscope... | [-0.15529307324689726, 0.14234317336419788, -0.10709618265200563, -0.0008041807019910892, 0.006386482720302434, -0.16393798806493273, 0.09744898763195682, 0.37407022743571955, -0.3059213042587918, -0.28218611469101, -0.04777488794115161, -0.3367748381022145, -0.16074656271727897, 0.13998096215366504, 0.0319380105919196... |
707.3213 | Demonstration of Temporal Distinguishability of Three and Four Photons
with Asymmetric Beam Splitter | By using an asymmetric beam splitter, we observe the generalized
Hong-Ou-Mandel effects for three and four photons, respectively. Furthermore,
we can use this generalized Hong-Ou-Mandel interferometer to characterize
temporal distinguishability.
| quant-ph | by using an asymmetric beam splitter we observe the generalized hongoumandel effects for three and four photons respectively furthermore we can use this generalized hongoumandel interferometer to characterize temporal distinguishability | [['by', 'using', 'an', 'asymmetric', 'beam', 'splitter', 'we', 'observe', 'the', 'generalized', 'hongoumandel', 'effects', 'for', 'three', 'and', 'four', 'photons', 'respectively', 'furthermore', 'we', 'can', 'use', 'this', 'generalized', 'hongoumandel', 'interferometer', 'to', 'characterize', 'temporal', 'distinguisha... | [-0.1464255099495252, 0.17360493716599498, -0.1464626015474399, 0.11000827120539422, 0.006105827043453852, -0.19889319532861313, 0.0027128400358681875, 0.5085863674680392, -0.23433049451559781, -0.2996586394185821, -0.05916429511271417, -0.2698574798181653, -0.15110545828938485, 0.2032190313562751, -0.06255778909350435... |
707.3214 | The quantum solvation, adiabatic versus nonadiabatic, and Markovian
versus non-Markovian nature of electron transfer rate processes | In this work, we revisit the electron transfer rate theory, with particular
interests in the distinct quantum solvation effect, and the characterizations
of adiabatic/nonadiabatic and Markovian/non-Markovian rate processes. We first
present a full account for the quantum solvation effect on the electron
transfer in D... | physics.chem-ph | in this work we revisit the electron transfer rate theory with particular interests in the distinct quantum solvation effect and the characterizations of adiabaticnonadiabatic and markoviannonmarkovian rate processes we first present a full account for the quantum solvation effect on the electron transfer in debye solv... | [['in', 'this', 'work', 'we', 'revisit', 'the', 'electron', 'transfer', 'rate', 'theory', 'with', 'particular', 'interests', 'in', 'the', 'distinct', 'quantum', 'solvation', 'effect', 'and', 'the', 'characterizations', 'of', 'adiabaticnonadiabatic', 'and', 'markoviannonmarkovian', 'rate', 'processes', 'we', 'first', 'p... | [-0.10986317951309806, 0.16293865242429698, -0.051479632920042304, 0.049224357124245825, -0.002710845028050244, -0.14766101914457977, 0.08517917630650725, 0.35916772903253635, -0.27934970424044875, -0.24847592297010124, -0.01026245709663878, -0.2536222464373956, -0.14235961851198226, 0.18325554483647769, -0.02709708978... |
707.3215 | Many-Body Separability of Warm Qubits | We analyze the separability of the joint state of a collection of two-level
systems at finite temperature T. The fact that only separable states are found
in the neighborhood of their thermal equilibrium state guarantees that
decoherence will destroy any initially arranged entanglement in a finite time.
| quant-ph cond-mat.stat-mech | we analyze the separability of the joint state of a collection of twolevel systems at finite temperature t the fact that only separable states are found in the neighborhood of their thermal equilibrium state guarantees that decoherence will destroy any initially arranged entanglement in a finite time | [['we', 'analyze', 'the', 'separability', 'of', 'the', 'joint', 'state', 'of', 'a', 'collection', 'of', 'twolevel', 'systems', 'at', 'finite', 'temperature', 't', 'the', 'fact', 'that', 'only', 'separable', 'states', 'are', 'found', 'in', 'the', 'neighborhood', 'of', 'their', 'thermal', 'equilibrium', 'state', 'guarant... | [-0.20161522087700506, 0.23873464769109132, -0.11688581623255889, 0.03144195699628363, 0.057120768947804226, -0.1531713946345956, 0.08034389000386, 0.35386980110977556, -0.27686128206551075, -0.21271156670248254, 0.06505757916540383, -0.2952096701223165, -0.010471686604432762, 0.08626094662604179, -0.027598612010478973... |
707.3216 | Complex cobordism and algebraic topology | This is a historical survey, beginning where Atiyah and Sullivan leave off...
| math.HO math.KT | this is a historical survey beginning where atiyah and sullivan leave off | [['this', 'is', 'a', 'historical', 'survey', 'beginning', 'where', 'atiyah', 'and', 'sullivan', 'leave', 'off']] | [-0.08838956686668098, 0.17004014815514287, -0.19668924358362952, 0.17645268375054002, -0.2879997257065649, -0.17511512366278717, 0.08447848287566255, 0.28413033702721197, -0.3035739337404569, -0.23481512100746235, 0.1850982578471303, -0.3183190201719602, -0.1364162415266037, 0.1432034926644216, -0.23975891705291966, -... |
707.3217 | Soft ideals and arithmetic mean ideals | This article investigates the soft-interior and the soft-cover of operator
ideals. These operations, and especially the first one, have been widely used
before, but making their role explicit and analyzing their interplay with the
arithmetic mean operations is essential for the study of the multiplicity of
traces (se... | math.FA math.OA | this article investigates the softinterior and the softcover of operator ideals these operations and especially the first one have been widely used before but making their role explicit and analyzing their interplay with the arithmetic mean operations is essential for the study of the multiplicity of traces see arxiv07... | [['this', 'article', 'investigates', 'the', 'softinterior', 'and', 'the', 'softcover', 'of', 'operator', 'ideals', 'these', 'operations', 'and', 'especially', 'the', 'first', 'one', 'have', 'been', 'widely', 'used', 'before', 'but', 'making', 'their', 'role', 'explicit', 'and', 'analyzing', 'their', 'interplay', 'with'... | [-0.11758462851004745, 0.11944371078915773, -0.09778796869537068, 0.11290594995658063, -0.034265438910504736, -0.08818052209982717, 0.014570631950024377, 0.3758267501162158, -0.3247258206312027, -0.2845247332834535, 0.17995799233602292, -0.2831930863671005, -0.1432486166867117, 0.18417039573778984, -0.1094991486924873,... |
707.3218 | Satellite Luminosities in Galaxy Groups | Halo model interpretations of the luminosity dependence of galaxy clustering
assume that there is a central galaxy in every sufficiently massive halo, and
that this central galaxy is very different from all the others in the halo. The
halo model decomposition makes the remarkable prediction that the mean
luminosity o... | astro-ph | halo model interpretations of the luminosity dependence of galaxy clustering assume that there is a central galaxy in every sufficiently massive halo and that this central galaxy is very different from all the others in the halo the halo model decomposition makes the remarkable prediction that the mean luminosity of th... | [['halo', 'model', 'interpretations', 'of', 'the', 'luminosity', 'dependence', 'of', 'galaxy', 'clustering', 'assume', 'that', 'there', 'is', 'a', 'central', 'galaxy', 'in', 'every', 'sufficiently', 'massive', 'halo', 'and', 'that', 'this', 'central', 'galaxy', 'is', 'very', 'different', 'from', 'all', 'the', 'others',... | [-0.06549305118040362, 0.11801843882942768, -0.11457230723381304, 0.15732834645007787, -0.08996408749371768, -0.03285467358665508, 0.0021973113700943557, 0.40891321523670565, -0.11416490911792049, -0.3921485418453813, 0.025383646128976946, -0.3085517110466434, -0.003485857920819207, 0.21025652701979486, -0.026908104618... |
707.3219 | Unitarity and real properties of the neutral meson complex | The proof of the Khalfin Theorem for neutral meson complex is analyzed. It is
shown that the unitarity of the time evolution operator for the total system
under considerations assures that the Khalfin's Theorem holds. The consequences
of this Theorem for the neutral mesons system are discussed: it is shown, eg.,
that... | hep-ph | the proof of the khalfin theorem for neutral meson complex is analyzed it is shown that the unitarity of the time evolution operator for the total system under considerations assures that the khalfins theorem holds the consequences of this theorem for the neutral mesons system are discussed it is shown eg that diagonal... | [['the', 'proof', 'of', 'the', 'khalfin', 'theorem', 'for', 'neutral', 'meson', 'complex', 'is', 'analyzed', 'it', 'is', 'shown', 'that', 'the', 'unitarity', 'of', 'the', 'time', 'evolution', 'operator', 'for', 'the', 'total', 'system', 'under', 'considerations', 'assures', 'that', 'the', 'khalfins', 'theorem', 'holds'... | [-0.13094889148888542, 0.20249205786444827, -0.08341011325522008, 0.11600597778162333, -0.021882918865481268, -0.15883085209998987, -0.002054778560661449, 0.31353337342242993, -0.25430885137443593, -0.20091698030121402, 0.07159357387600411, -0.26207531268937057, -0.15008457324573557, 0.15307264879881266, 0.007535209391... |
707.322 | First-principles modeling of BaCeO_{3}: structure and stabilization of O
vacancies by Pd-doping | We use first-principles density functional theory (DFT) calculations to
investigate the ground state structures of both BaCeO_{3} (BC) and Pd-doped BC
(BCP). The relaxed structures match closely with recent experimental scattering
studies, and also provide a local picture of how the BC perovskite lattice
accommodates... | cond-mat.mtrl-sci | we use firstprinciples density functional theory dft calculations to investigate the ground state structures of both baceo_3 bc and pddoped bc bcp the relaxed structures match closely with recent experimental scattering studies and also provide a local picture of how the bc perovskite lattice accommodates pd both stoic... | [['we', 'use', 'firstprinciples', 'density', 'functional', 'theory', 'dft', 'calculations', 'to', 'investigate', 'the', 'ground', 'state', 'structures', 'of', 'both', 'baceo_3', 'bc', 'and', 'pddoped', 'bc', 'bcp', 'the', 'relaxed', 'structures', 'match', 'closely', 'with', 'recent', 'experimental', 'scattering', 'stud... | [-0.1071000423970389, 0.14442105977906142, -0.04850997298123181, 0.022140506589953025, 0.02054341396669278, -0.137207775401908, 0.07700773345218417, 0.447020854012252, -0.28759828850895436, -0.2463487849344273, 0.04143727782417324, -0.2978211681417248, -0.1519257206771825, 0.07839627169242532, 0.04113974944092669, 0.01... |
707.3221 | Continuous Time Random Walks (CTRWs): Simulation of continuous
trajectories | Continuous time random walks have been developed as a straightforward
generalisation of classical random walk processes. Some 10 years ago, Fogedby
introduced a continuous representation of these processes by means of a set of
Langevin equations [H. C. Fogedby, Phys. Rev. E 50 (1994)]. The present work is
devoted to ... | physics.data-an physics.chem-ph | continuous time random walks have been developed as a straightforward generalisation of classical random walk processes some 10 years ago fogedby introduced a continuous representation of these processes by means of a set of langevin equations h c fogedby phys rev e 50 1994 the present work is devoted to a detailed dis... | [['continuous', 'time', 'random', 'walks', 'have', 'been', 'developed', 'as', 'a', 'straightforward', 'generalisation', 'of', 'classical', 'random', 'walk', 'processes', 'some', '10', 'years', 'ago', 'fogedby', 'introduced', 'a', 'continuous', 'representation', 'of', 'these', 'processes', 'by', 'means', 'of', 'a', 'set... | [-0.08896320697426809, 0.14063865324141275, -0.07376583621666676, -0.03120740246467135, -0.07537415715485392, -0.11304284003235295, 0.1129623197222417, 0.38699880645046353, -0.22586267244097002, -0.2625332806836551, 0.07322678069623423, -0.22542020898889487, -0.15656994076603106, 0.19768588732547637, -0.071716560063962... |
707.3222 | When is g_{tt} g_{rr} = -1? | The Schwarzschild metric, its Reissner-Nordstrom-de Sitter generalizations to
higher dimensions, and some further generalizations all share the feature that
g_{tt} g_{rr}=-1 in Schwarzschild-like coordinates. In this pedagogical note we
trace this feature to the condition that the Ricci tensor (and stress-energy
tens... | gr-qc hep-th | the schwarzschild metric its reissnernordstromde sitter generalizations to higher dimensions and some further generalizations all share the feature that g_tt g_rr1 in schwarzschildlike coordinates in this pedagogical note we trace this feature to the condition that the ricci tensor and stressenergy tensor in a solution... | [['the', 'schwarzschild', 'metric', 'its', 'reissnernordstromde', 'sitter', 'generalizations', 'to', 'higher', 'dimensions', 'and', 'some', 'further', 'generalizations', 'all', 'share', 'the', 'feature', 'that', 'g_tt', 'g_rr1', 'in', 'schwarzschildlike', 'coordinates', 'in', 'this', 'pedagogical', 'note', 'we', 'trace... | [-0.16383269555600627, 0.08620625715359763, -0.10141104579504047, 0.05511556648222419, -0.15821855355031966, -0.14854291516600088, -0.09916206929344862, 0.3365326585092892, -0.24670593214354344, -0.14421087443562491, 0.0917114912465747, -0.30445464646133286, -0.14923486098026237, 0.09039050492130973, -0.099729484500130... |
707.3223 | The Circumstellar Structure and Excitation Effects around the Massive
Protostar Cepheus A HW 2 | We report SMA 335 GHz continuum observations with angular resolution of
~0.''3, together with VLA ammonia observations with ~1'' resolution toward Cep
A HW 2. We find that the flattened disk structure of the dust emission observed
by Patel et al. is preserved at the 0.''3 scale, showing an elongated structure
of ~$0.... | astro-ph | we report sma 335 ghz continuum observations with angular resolution of 03 together with vla ammonia observations with 1 resolution toward cep a hw 2 we find that the flattened disk structure of the dust emission observed by patel et al is preserved at the 03 scale showing an elongated structure of 06 size 450 au peaki... | [['we', 'report', 'sma', '335', 'ghz', 'continuum', 'observations', 'with', 'angular', 'resolution', 'of', '03', 'together', 'with', 'vla', 'ammonia', 'observations', 'with', '1', 'resolution', 'toward', 'cep', 'a', 'hw', '2', 'we', 'find', 'that', 'the', 'flattened', 'disk', 'structure', 'of', 'the', 'dust', 'emission... | [-0.05794951545751289, 0.09057569722301186, -0.012019244196949995, 0.01704412925517328, -0.03287923154802394, -0.11375005957561583, -0.0066665868106031275, 0.45209188676542705, -0.18908908666923033, -0.37259716116033537, 0.09301017863302878, -0.24940269530685455, -0.07340574269428064, 0.1282771113948156, 0.001696921938... |
707.3224 | Tight-binding modeling of charge migration in DNA devices | Long range charge transfer experiments in DNA oligomers and the subsequently
measured -- and very diverse -- transport response of DNA wires in solid state
experiments exemplifies the need for a thorough theoretical understanding of
charge migration in DNA-based natural and artificial materials. Here we present
a rev... | q-bio.GN cond-mat.soft q-bio.OT | long range charge transfer experiments in dna oligomers and the subsequently measured and very diverse transport response of dna wires in solid state experiments exemplifies the need for a thorough theoretical understanding of charge migration in dnabased natural and artificial materials here we present a review of tig... | [['long', 'range', 'charge', 'transfer', 'experiments', 'in', 'dna', 'oligomers', 'and', 'the', 'subsequently', 'measured', 'and', 'very', 'diverse', 'transport', 'response', 'of', 'dna', 'wires', 'in', 'solid', 'state', 'experiments', 'exemplifies', 'the', 'need', 'for', 'a', 'thorough', 'theoretical', 'understanding'... | [-0.07321109378007146, 0.1100834673365616, -0.05468511762933768, 0.06519008437718017, -0.030120458437262902, -0.1534711963649155, 0.06428990928974117, 0.41661891597798284, -0.2704073382370478, -0.3226436626680471, 0.024626422486961723, -0.28171069363897727, -0.16461239747788606, 0.19386341470075125, 0.00409525035101236... |
707.3225 | Gluon contributions to the pion mass and light cone momentum fraction | We calculate the matrix elements of the gluonic contributions to the
energy-momentum tensor for a pion of mass 600 < Mpi < 1100 MeV in quenched
lattice QCD. We find that gluons contribute (37 +/- 8 +/- 12)% of the pion's
light cone momentum. The bare matrix elements corresponding to the trace
anomaly contribution to ... | hep-lat hep-ph | we calculate the matrix elements of the gluonic contributions to the energymomentum tensor for a pion of mass 600 mpi 1100 mev in quenched lattice qcd we find that gluons contribute 37 8 12 of the pions light cone momentum the bare matrix elements corresponding to the trace anomaly contribution to the pion mass are als... | [['we', 'calculate', 'the', 'matrix', 'elements', 'of', 'the', 'gluonic', 'contributions', 'to', 'the', 'energymomentum', 'tensor', 'for', 'a', 'pion', 'of', 'mass', '600', 'mpi', '1100', 'mev', 'in', 'quenched', 'lattice', 'qcd', 'we', 'find', 'that', 'gluons', 'contribute', '37', '8', '12', 'of', 'the', 'pions', 'lig... | [-0.06715803471161053, 0.27432838188688036, -0.09035734126737224, 0.1031500564327871, -0.053066336734991636, -0.028245854238048197, 0.012484465222223661, 0.34777844125055707, -0.20490609608241356, -0.24297076326329262, -0.007775744622631464, -0.3715170740149915, -0.010974386404268444, 0.07471505114808678, 0.10956182832... |
707.3226 | Invariants of Closed 3-Manifolds via Nullhomotopic Filling Dehn Spheres | We provide a calculus for the presentation of closed 3-manifolds via
nullhomotopic filling Dehn spheres and we use it to define an invariant of
closed 3-manifolds by applying the state-sum machinery. As a potential
application of this invariant, we show how to get lower bounds for the Matveev
complexity of P2-irreduc... | math.GT | we provide a calculus for the presentation of closed 3manifolds via nullhomotopic filling dehn spheres and we use it to define an invariant of closed 3manifolds by applying the statesum machinery as a potential application of this invariant we show how to get lower bounds for the matveev complexity of p2irreducible clo... | [['we', 'provide', 'a', 'calculus', 'for', 'the', 'presentation', 'of', 'closed', '3manifolds', 'via', 'nullhomotopic', 'filling', 'dehn', 'spheres', 'and', 'we', 'use', 'it', 'to', 'define', 'an', 'invariant', 'of', 'closed', '3manifolds', 'by', 'applying', 'the', 'statesum', 'machinery', 'as', 'a', 'potential', 'appl... | [-0.19981055618508867, 0.09587485429648568, -0.13304978504004938, 0.14873038208277553, -0.11926862793533426, -0.18054049832158184, 0.06030525643329479, 0.351106995814725, -0.26095519122961713, -0.28943533438110824, 0.09876037031828769, -0.21933225900130837, -0.2002743087589471, 0.2500578314065933, -0.16982014273832502,... |
707.3227 | Direct and reverse log-Sobolev inequalities in $\mu$-deformed
Segal-Bargmann analysis | Both direct and reverse log-Sobolev inequalities, relating the Shannon
entropy with a $\mu$-deformed energy, are shown to hold in a family of
$\mu$-deformed Segal-Bargmann spaces. This shows that the $\mu$-deformed energy
of a state is finite if and only if its Shannon entropy is finite. The direct
inequality is a ne... | math-ph math.MP | both direct and reverse logsobolev inequalities relating the shannon entropy with a mudeformed energy are shown to hold in a family of mudeformed segalbargmann spaces this shows that the mudeformed energy of a state is finite if and only if its shannon entropy is finite the direct inequality is a new result while the r... | [['both', 'direct', 'and', 'reverse', 'logsobolev', 'inequalities', 'relating', 'the', 'shannon', 'entropy', 'with', 'a', 'mudeformed', 'energy', 'are', 'shown', 'to', 'hold', 'in', 'a', 'family', 'of', 'mudeformed', 'segalbargmann', 'spaces', 'this', 'shows', 'that', 'the', 'mudeformed', 'energy', 'of', 'a', 'state', ... | [-0.06060243019485686, 0.13190311356293444, -0.14674943321020595, 0.11829680738360035, -0.08547304131534715, -0.14351831524577363, 0.034614486594773855, 0.32495455158911396, -0.3214063631210303, -0.17548986700122918, 0.1434139276828481, -0.2883700244190381, -0.09501404502114516, 0.2258029752071725, -0.06899586509580151... |
707.3228 | 1- Brane Sources for the Lightcone Worldsheet: Q-branion - {\bar
Q}-branion Scattering to One Loop | This paper extends the study, initiated by Rozowsky and Thorn [1], of gauge
fields in interaction with Dirac fields living on separated parallel 1-branes.
In a lightcone description, replacing static point sources by 1-brane sources
allows p^+ conservation to be maintained in their presence, which simplifies
the ligh... | hep-th | this paper extends the study initiated by rozowsky and thorn 1 of gauge fields in interaction with dirac fields living on separated parallel 1branes in a lightcone description replacing static point sources by 1brane sources allows p conservation to be maintained in their presence which simplifies the lightcone quantiz... | [['this', 'paper', 'extends', 'the', 'study', 'initiated', 'by', 'rozowsky', 'and', 'thorn', '1', 'of', 'gauge', 'fields', 'in', 'interaction', 'with', 'dirac', 'fields', 'living', 'on', 'separated', 'parallel', '1branes', 'in', 'a', 'lightcone', 'description', 'replacing', 'static', 'point', 'sources', 'by', '1brane',... | [-0.14542744973761157, 0.1930260765822787, -0.09797981010713414, 0.08475261160364266, -0.059674812407762394, -0.08407900426034615, 0.06896392551510978, 0.3574474059164013, -0.15618253512965405, -0.23340228874711136, -0.019565722200900828, -0.26019225366126547, -0.1342404653163006, 0.07893647585411136, -0.03598454009796... |
707.3229 | Leibniz seminorms for "Matrix algebras converge to the sphere" | In an earlier paper of mine relating vector bundles and Gromov-Hausdorff
distance for ordinary compact metric spaces, it was crucial that the Lipschitz
seminorms from the metrics satisfy a strong Leibniz property. In the present
paper, for the now non-commutative situation of matrix algebras converging to
the sphere ... | math.OA hep-th math.MG | in an earlier paper of mine relating vector bundles and gromovhausdorff distance for ordinary compact metric spaces it was crucial that the lipschitz seminorms from the metrics satisfy a strong leibniz property in the present paper for the now noncommutative situation of matrix algebras converging to the sphere or to o... | [['in', 'an', 'earlier', 'paper', 'of', 'mine', 'relating', 'vector', 'bundles', 'and', 'gromovhausdorff', 'distance', 'for', 'ordinary', 'compact', 'metric', 'spaces', 'it', 'was', 'crucial', 'that', 'the', 'lipschitz', 'seminorms', 'from', 'the', 'metrics', 'satisfy', 'a', 'strong', 'leibniz', 'property', 'in', 'the'... | [-0.13427693963127868, 0.07419059170671315, -0.08493655447715096, 0.13941063791429414, -0.13567883295840338, -0.12476391018249262, -0.018740786388744005, 0.4012182034215981, -0.3389876191714372, -0.150483478252825, 0.11785263004467676, -0.2504194172648923, -0.1478704345654136, 0.2098073757663229, -0.16092810427587956, ... |
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