id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.1849 | Effects of Ox-LDL on Macrophages NAD(P)H Autofluorescence Changes by
Two-photon Microscopy | Ox-LDL uptakes by macrophage play a critical role in the happening of
atherosclerosis. Because of its low damage on observed cells and better
signal-to- background ratio, two-photon excitation fluorescence microscopy is
used to observe NAD(P)H autofluorescence of macrophage under difference
cultured conditions- bare ... | physics.bio-ph | oxldl uptakes by macrophage play a critical role in the happening of atherosclerosis because of its low damage on observed cells and better signalto background ratio twophoton excitation fluorescence microscopy is used to observe nadph autofluorescence of macrophage under difference cultured conditions bare cover glass... | [['oxldl', 'uptakes', 'by', 'macrophage', 'play', 'a', 'critical', 'role', 'in', 'the', 'happening', 'of', 'atherosclerosis', 'because', 'of', 'its', 'low', 'damage', 'on', 'observed', 'cells', 'and', 'better', 'signalto', 'background', 'ratio', 'twophoton', 'excitation', 'fluorescence', 'microscopy', 'is', 'used', 'to... | [-0.05386283063704026, 0.15419032415766792, -0.050305718242704314, 0.045046317660919974, 0.030104342928574047, -0.14746688670156716, 0.009357503498904407, 0.43809297113357304, -0.19102309572849877, -0.2960447523716802, 0.0784027546787826, -0.2936942495893095, -0.19248818182908695, 0.20340760614261658, -0.09591019870800... |
708.185 | Transport Properties of a spinon Fermi surface coupled to a U(1) gauge
field | With the organic compound $\kappa$-(BEDT-TTF)$_2$-Cu$_2$(CN)$_3$ in mind, we
consider a spin liquid system where a spinon Fermi surface is coupled to a U(1)
gauge field. Using the non-equilibrium Green's function formalism, we derive
the Quantum Boltzmann Equation (QBE) for this system. In this system, however,
one c... | cond-mat.str-el | with the organic compound kappabedtttf_2cu_2cn_3 in mind we consider a spin liquid system where a spinon fermi surface is coupled to a u1 gauge field using the nonequilibrium greens function formalism we derive the quantum boltzmann equation qbe for this system in this system however one cannot a priori assume the exis... | [['with', 'the', 'organic', 'compound', 'kappabedtttf_2cu_2cn_3', 'in', 'mind', 'we', 'consider', 'a', 'spin', 'liquid', 'system', 'where', 'a', 'spinon', 'fermi', 'surface', 'is', 'coupled', 'to', 'a', 'u1', 'gauge', 'field', 'using', 'the', 'nonequilibrium', 'greens', 'function', 'formalism', 'we', 'derive', 'the', '... | [-0.15729914360087027, 0.1733850927923398, -0.13125393558139645, 0.07214791599126179, -0.06541871782469232, -0.1336678125941741, 0.05596339719346917, 0.3327690422735062, -0.26610297153603807, -0.2493452390209456, 0.039336293025619605, -0.28078814168760846, -0.14682095908860038, 0.14878286264763668, 0.01278057629781321,... |
708.1851 | Atomic-like behaviors and orbital-related Luttinger liquid in carbon
nano-peapod quantum dots | We report influence of encapsulated C60 molecules on electron transport in
carbon-nanotube peapod quantum dots. We find atomic-like behaviors with doubly
degenerate electronic levels, which exist only around ground states, by single
electron spectroscopy measured at low back-gate voltages (Vbg). Correlation
with pres... | cond-mat.mtrl-sci | we report influence of encapsulated c60 molecules on electron transport in carbonnanotube peapod quantum dots we find atomiclike behaviors with doubly degenerate electronic levels which exist only around ground states by single electron spectroscopy measured at low backgate voltages vbg correlation with presence of nea... | [['we', 'report', 'influence', 'of', 'encapsulated', 'c60', 'molecules', 'on', 'electron', 'transport', 'in', 'carbonnanotube', 'peapod', 'quantum', 'dots', 'we', 'find', 'atomiclike', 'behaviors', 'with', 'doubly', 'degenerate', 'electronic', 'levels', 'which', 'exist', 'only', 'around', 'ground', 'states', 'by', 'sin... | [-0.156327783013694, 0.23965486525858362, 0.013107158982517918, 0.02273539583116109, 0.05826691353145326, -0.22844259826196056, 0.08822858339220646, 0.37864755926233146, -0.2634352010321773, -0.2928612009141474, -0.036677977810482376, -0.37170370577293776, -0.0751847927083051, 0.12936423568809854, 0.05815826682373881, ... |
708.1852 | Synthesis, characterization, and application of carbon cubes | Carbon nanotubes (CNTs) have attracted increasing attention because of their
unique structural, mechanical, and electronic properties. Surface chemistry
modifications are also useful and critical to manipulate the adsorptive
properties of CNTs and develop their potential of environmental application.
Therefore, the m... | cond-mat.mtrl-sci | carbon nanotubes cnts have attracted increasing attention because of their unique structural mechanical and electronic properties surface chemistry modifications are also useful and critical to manipulate the adsorptive properties of cnts and develop their potential of environmental application therefore the main objec... | [['carbon', 'nanotubes', 'cnts', 'have', 'attracted', 'increasing', 'attention', 'because', 'of', 'their', 'unique', 'structural', 'mechanical', 'and', 'electronic', 'properties', 'surface', 'chemistry', 'modifications', 'are', 'also', 'useful', 'and', 'critical', 'to', 'manipulate', 'the', 'adsorptive', 'properties', ... | [-0.06562774533617265, 0.1603995331460676, -0.00887274356717442, -0.023353693825985365, -0.005562005419257685, -0.1385643569395897, 0.08430575044719991, 0.5124470481635831, -0.2562951992213452, -0.34541277792172653, 0.06832647081654426, -0.3030773367838445, -0.11952856469714472, 0.12286357610017484, -0.0059045055659870... |
708.1853 | A Wide-Field View of Leo II -- A Structural Analysis Using the SDSS | Using SDSS I data, we have analysed the stellar distribution of the Leo II
dwarf spheroidal galaxy (distance of 233 kpc) to search for evidence of tidal
deformation. The existing SDSS photometric catalogue contains gaps in regions
of high stellar crowding, hence we filled the area at the centre of Leo II
using the DA... | astro-ph | using sdss i data we have analysed the stellar distribution of the leo ii dwarf spheroidal galaxy distance of 233 kpc to search for evidence of tidal deformation the existing sdss photometric catalogue contains gaps in regions of high stellar crowding hence we filled the area at the centre of leo ii using the daophot a... | [['using', 'sdss', 'i', 'data', 'we', 'have', 'analysed', 'the', 'stellar', 'distribution', 'of', 'the', 'leo', 'ii', 'dwarf', 'spheroidal', 'galaxy', 'distance', 'of', '233', 'kpc', 'to', 'search', 'for', 'evidence', 'of', 'tidal', 'deformation', 'the', 'existing', 'sdss', 'photometric', 'catalogue', 'contains', 'gaps... | [-0.08646057310692046, 0.03164080338755776, -0.07574028608106663, 0.052096518268459915, -0.12369167023732533, -0.07542493365258536, 0.08298777675514253, 0.4036462592058693, -0.14950438829056906, -0.3726339085665898, 0.042441003555641246, -0.3007324245420009, -0.0392640622607162, 0.15769892531466298, -0.0769523569045471... |
708.1854 | AKARI infrared imaging of reflection nebulae IC4954 and IC4955 | We present the observations of the reflection nebulae IC4954 and IC4955
region with the Infrared Camera (IRC) and the Far-Infrared Surveyor (FIS) on
board the infrared astronomical satellite AKARI during its performance
verification phase. We obtained 7 band images from 7 to 160um with higher
spatial resolution and h... | astro-ph | we present the observations of the reflection nebulae ic4954 and ic4955 region with the infrared camera irc and the farinfrared surveyor fis on board the infrared astronomical satellite akari during its performance verification phase we obtained 7 band images from 7 to 160um with higher spatial resolution and higher se... | [['we', 'present', 'the', 'observations', 'of', 'the', 'reflection', 'nebulae', 'ic4954', 'and', 'ic4955', 'region', 'with', 'the', 'infrared', 'camera', 'irc', 'and', 'the', 'farinfrared', 'surveyor', 'fis', 'on', 'board', 'the', 'infrared', 'astronomical', 'satellite', 'akari', 'during', 'its', 'performance', 'verifi... | [-0.03347250123999054, 0.0446334160333963, -0.08785840597861597, 0.06370277370988484, -0.07254235652039655, -0.020970999045853977, 0.036920550586056755, 0.46302700273043385, -0.1665725087596266, -0.3660414782372068, 0.09812845808987146, -0.33148926930865313, -0.03157183785823317, 0.17672045285527543, -0.045839532814181... |
708.1855 | CaII and NaI absorption signatures from the circumgalactic gas of the
Milky Way | We combine CaII/NaI absorption and HI 21 cm emission line measurements to
analyse the metal abundances, the distribution, the small-scale structure, and
the physical conditions of intermediate- and high-velocity gas in the Galactic
halo.
| astro-ph | we combine caiinai absorption and hi 21 cm emission line measurements to analyse the metal abundances the distribution the smallscale structure and the physical conditions of intermediate and highvelocity gas in the galactic halo | [['we', 'combine', 'caiinai', 'absorption', 'and', 'hi', '21', 'cm', 'emission', 'line', 'measurements', 'to', 'analyse', 'the', 'metal', 'abundances', 'the', 'distribution', 'the', 'smallscale', 'structure', 'and', 'the', 'physical', 'conditions', 'of', 'intermediate', 'and', 'highvelocity', 'gas', 'in', 'the', 'galac... | [-0.060103005525888875, 0.04003741074463024, -0.010606637114987653, 0.0762636693304076, -0.05255840646842604, -0.03616913709351245, 0.02138471050078378, 0.4582153177984497, -0.17240290223237345, -0.3182784198399852, 0.010615030135822427, -0.3047480863683364, 0.01556720121024067, 0.09680609470781158, 0.08731238420723993... |
708.1856 | Vortex Images and q-Elementary Functions | In the present paper problem of vortex images in annular domain between two
coaxial cylinders is solved by the q-elementary functions. We show that all
images are determined completely as poles of the q-logarithmic function, where
dimensionless parameter $q = r^2_2/r^2_1$ is given by square ratio of the
cylinder radi... | math-ph math.MP math.QA | in the present paper problem of vortex images in annular domain between two coaxial cylinders is solved by the qelementary functions we show that all images are determined completely as poles of the qlogarithmic function where dimensionless parameter q r2_2r2_1 is given by square ratio of the cylinder radii resulting s... | [['in', 'the', 'present', 'paper', 'problem', 'of', 'vortex', 'images', 'in', 'annular', 'domain', 'between', 'two', 'coaxial', 'cylinders', 'is', 'solved', 'by', 'the', 'qelementary', 'functions', 'we', 'show', 'that', 'all', 'images', 'are', 'determined', 'completely', 'as', 'poles', 'of', 'the', 'qlogarithmic', 'fun... | [-0.17499461178177675, 0.10473767398415428, -0.048561492955830315, 0.020173687521977478, -0.05104424931192981, -0.12211179751132552, -0.015892999822665985, 0.3843137212097645, -0.2803106978973304, -0.2767998383597548, 0.07922124800759611, -0.27272825329599526, -0.13080748152057814, 0.18811617741585338, -0.0483827810818... |
708.1857 | Simulation Results for U(1) Gauge Theory on Non-Commutative Spaces | We present numerical results for U(1) gauge theory in 2d and 4d spaces
involving a non-commutative plane. Simulations are feasible thanks to a mapping
of the non-commutative plane onto a twisted matrix model. In d=2 it was a
long-standing issue if Wilson loops are (partially) invariant under
area-preserving diffeomor... | hep-lat astro-ph hep-th | we present numerical results for u1 gauge theory in 2d and 4d spaces involving a noncommutative plane simulations are feasible thanks to a mapping of the noncommutative plane onto a twisted matrix model in d2 it was a longstanding issue if wilson loops are partially invariant under areapreserving diffeomorphisms we sho... | [['we', 'present', 'numerical', 'results', 'for', 'u1', 'gauge', 'theory', 'in', '2d', 'and', '4d', 'spaces', 'involving', 'a', 'noncommutative', 'plane', 'simulations', 'are', 'feasible', 'thanks', 'to', 'a', 'mapping', 'of', 'the', 'noncommutative', 'plane', 'onto', 'a', 'twisted', 'matrix', 'model', 'in', 'd2', 'it'... | [-0.14083134657790142, 0.18445586025910943, -0.0676086442422514, 0.09470946910452065, -0.03668820188919965, -0.12532956397830786, 0.04141722046034901, 0.36550530038055096, -0.21415933737482287, -0.2268700091160115, 0.12971357820175686, -0.25968618792269316, -0.15941867820526423, 0.14503444201647908, -0.0856704841972443... |
708.1858 | The Effelsberg-Bonn HI Survey (EBHIS) | The new L-band 7-feed-array at the 100-m telescope in Effelsberg will be used
to perform an unbiased fully sampled HI survey of the entire northern
hemisphere observing the galactic and extragalactic sky using simultaneously
two different backends.
The survey will be extremely valuable for a broad range of research... | astro-ph | the new lband 7feedarray at the 100m telescope in effelsberg will be used to perform an unbiased fully sampled hi survey of the entire northern hemisphere observing the galactic and extragalactic sky using simultaneously two different backends the survey will be extremely valuable for a broad range of research topics s... | [['the', 'new', 'lband', '7feedarray', 'at', 'the', '100m', 'telescope', 'in', 'effelsberg', 'will', 'be', 'used', 'to', 'perform', 'an', 'unbiased', 'fully', 'sampled', 'hi', 'survey', 'of', 'the', 'entire', 'northern', 'hemisphere', 'observing', 'the', 'galactic', 'and', 'extragalactic', 'sky', 'using', 'simultaneous... | [-0.031348452892803406, 0.060096931085393004, -0.03985170176143738, 0.10440239608485966, -0.12452378637216827, -0.018488198350322373, 0.033453213150038366, 0.43591000115934836, -0.14855227502498855, -0.3249677981824634, 0.10383833906281383, -0.293265939868511, -0.03115443796528741, 0.22133930968467463, 0.05012461253778... |
708.1859 | Multiple-Description Coding by Dithered Delta-Sigma Quantization | We address the connection between the multiple-description (MD) problem and
Delta-Sigma quantization. The inherent redundancy due to oversampling in
Delta-Sigma quantization, and the simple linear-additive noise model resulting
from dithered lattice quantization, allow us to construct a symmetric and
time-invariant M... | cs.IT math.IT | we address the connection between the multipledescription md problem and deltasigma quantization the inherent redundancy due to oversampling in deltasigma quantization and the simple linearadditive noise model resulting from dithered lattice quantization allow us to construct a symmetric and timeinvariant md coding sch... | [['we', 'address', 'the', 'connection', 'between', 'the', 'multipledescription', 'md', 'problem', 'and', 'deltasigma', 'quantization', 'the', 'inherent', 'redundancy', 'due', 'to', 'oversampling', 'in', 'deltasigma', 'quantization', 'and', 'the', 'simple', 'linearadditive', 'noise', 'model', 'resulting', 'from', 'dithe... | [-0.14834134392440318, 0.04840085663774516, -0.10259106582562838, 0.06884362407228244, -0.04595670276267421, -0.22023485925314681, 0.07672800876200199, 0.4204374930834664, -0.30451999310936245, -0.22638820486608893, 0.1253131595021114, -0.2304560567012855, -0.19650488433827246, 0.13410354234943433, -0.10701423781790903... |
708.186 | Stable curved solitonic surfaces in nonholonomic frame | Assuming the stability of soliton surfaces of vanishing Ricci sectional
curvature of soliton metric in the nonholonomic frame, we find a solution for
the metric in the approximation of weak constant torsion curves with constant
Frenet curvature. The computation of the Riemann tensor of the soliton metric
shows that i... | physics.flu-dyn physics.plasm-ph | assuming the stability of soliton surfaces of vanishing ricci sectional curvature of soliton metric in the nonholonomic frame we find a solution for the metric in the approximation of weak constant torsion curves with constant frenet curvature the computation of the riemann tensor of the soliton metric shows that it do... | [['assuming', 'the', 'stability', 'of', 'soliton', 'surfaces', 'of', 'vanishing', 'ricci', 'sectional', 'curvature', 'of', 'soliton', 'metric', 'in', 'the', 'nonholonomic', 'frame', 'we', 'find', 'a', 'solution', 'for', 'the', 'metric', 'in', 'the', 'approximation', 'of', 'weak', 'constant', 'torsion', 'curves', 'with'... | [-0.24722912245326573, 0.08662490165895886, -0.12689625986321415, 0.07819161346673759, -0.1584943822481566, -0.13941521129777862, -0.08249155573753847, 0.36262993750472866, -0.2416137849866775, -0.18582954171838031, 0.07239339490835038, -0.26143010505992503, -0.1490738781945159, 0.16001824878363147, -0.0403788102890959... |
708.1861 | Origins of the Combinatorial Basis of Entropy | The combinatorial basis of entropy, given by Boltzmann, can be written $H =
N^{-1} \ln \mathbb{W}$, where $H$ is the dimensionless entropy, $N$ is the
number of entities and $\mathbb{W}$ is number of ways in which a given
realization of a system can occur (its statistical weight). This can be
broadened to give genera... | physics.class-ph | the combinatorial basis of entropy given by boltzmann can be written h n1 ln mathbbw where h is the dimensionless entropy n is the number of entities and mathbbw is number of ways in which a given realization of a system can occur its statistical weight this can be broadened to give generalized combinatorial or probabi... | [['the', 'combinatorial', 'basis', 'of', 'entropy', 'given', 'by', 'boltzmann', 'can', 'be', 'written', 'h', 'n1', 'ln', 'mathbbw', 'where', 'h', 'is', 'the', 'dimensionless', 'entropy', 'n', 'is', 'the', 'number', 'of', 'entities', 'and', 'mathbbw', 'is', 'number', 'of', 'ways', 'in', 'which', 'a', 'given', 'realizati... | [-0.1155196203409057, 0.14066653036111107, -0.10366448684546509, 0.06308320084476451, -0.09800756065248463, -0.19469804104515595, 0.06663458515264976, 0.30021225609081353, -0.3165180354899923, -0.2389499407408661, 0.06392572358998126, -0.2771974926924725, -0.10584662899828369, 0.1400311112379361, -0.1202757808232778, 0... |
708.1862 | Spectral methods and cluster structure in correlation-based networks | We investigate how in complex systems the eigenpairs of the matrices derived
from the correlations of multichannel observations reflect the cluster
structure of the underlying networks. For this we use daily return data from
the NYSE and focus specifically on the spectral properties of weight W_{ij} =
|C|_{ij} - \del... | physics.soc-ph | we investigate how in complex systems the eigenpairs of the matrices derived from the correlations of multichannel observations reflect the cluster structure of the underlying networks for this we use daily return data from the nyse and focus specifically on the spectral properties of weight w_ij c_ij delta_ij and diff... | [['we', 'investigate', 'how', 'in', 'complex', 'systems', 'the', 'eigenpairs', 'of', 'the', 'matrices', 'derived', 'from', 'the', 'correlations', 'of', 'multichannel', 'observations', 'reflect', 'the', 'cluster', 'structure', 'of', 'the', 'underlying', 'networks', 'for', 'this', 'we', 'use', 'daily', 'return', 'data', ... | [-0.11019595673043327, 0.08119168625176797, -0.04975057814132284, 0.06792760561958124, -0.057185081038777355, -0.12266487430842447, 0.05829763000662373, 0.4065747674776877, -0.26683181275540785, -0.2674482743478085, 0.12236265936835741, -0.32995286720341127, -0.1595714824272266, 0.11071013404562334, -0.0040017588226002... |
708.1863 | The Blazhko behavior of RV UMa | RV UMa is one of the most extensively studied RR Lyrae stars showing Blazhko
modulation. Its photometric observations cover more than 90 years. The
published photoelectric observations of RV UMa obtained at the Konkoly
Observatory (Kanyo, 1976) were re-considered and completed with previously
unpublished data. During... | astro-ph | rv uma is one of the most extensively studied rr lyrae stars showing blazhko modulation its photometric observations cover more than 90 years the published photoelectric observations of rv uma obtained at the konkoly observatory kanyo 1976 were reconsidered and completed with previously unpublished data during the time... | [['rv', 'uma', 'is', 'one', 'of', 'the', 'most', 'extensively', 'studied', 'rr', 'lyrae', 'stars', 'showing', 'blazhko', 'modulation', 'its', 'photometric', 'observations', 'cover', 'more', 'than', '90', 'years', 'the', 'published', 'photoelectric', 'observations', 'of', 'rv', 'uma', 'obtained', 'at', 'the', 'konkoly',... | [-0.14953439928763912, 0.14391728954159477, -0.10624777347770299, 0.06053005804156027, -0.14364239022271771, -0.1290802099176923, 0.11788942618818765, 0.38530537913019736, -0.17793345515841222, -0.3519836926225866, 0.10069565169952727, -0.28614612775815523, -0.08841023766801934, 0.26901885496682665, -0.0994692499660415... |
708.1864 | Results of the photometry of the spotted dM1-2e star EY Draconis | We have observed EY Draconis with the 24`` telescope of Konkoly Observatory
in Budapest for 64 nights. In the first obse rving season the star produced a
stable light curve for more than 60 rotation periods, however, the light curves
observe d in the next season and the spot modelling show clear evidence of the
evolu... | astro-ph | we have observed ey draconis with the 24 telescope of konkoly observatory in budapest for 64 nights in the first obse rving season the star produced a stable light curve for more than 60 rotation periods however the light curves observe d in the next season and the spot modelling show clear evidence of the evolution of... | [['we', 'have', 'observed', 'ey', 'draconis', 'with', 'the', '24', 'telescope', 'of', 'konkoly', 'observatory', 'in', 'budapest', 'for', '64', 'nights', 'in', 'the', 'first', 'obse', 'rving', 'season', 'the', 'star', 'produced', 'a', 'stable', 'light', 'curve', 'for', 'more', 'than', '60', 'rotation', 'periods', 'howev... | [-0.11123679436886133, 0.15328723388798113, -0.13128018607808786, 0.07833315747980536, -0.05810222127051516, -0.10825533065839078, 0.10885591859220188, 0.37659178460440174, -0.16577341808872667, -0.391932513310828, 0.13767965300543106, -0.3032913947790803, -0.08617116404506801, 0.2615387881047685, -0.0667265472075087, ... |
708.1865 | Metabolite essentiality elucidates robustness of Escherichia coli
metabolism | Complex biological systems are very robust to genetic and environmental
changes at all levels of organization. Many biological functions of Escherichia
coli metabolism can be sustained against single-gene or even multiple-gene
mutations by using redundant or alternative pathways. Thus, only a limited
number of genes ... | q-bio.MN physics.bio-ph q-bio.QM | complex biological systems are very robust to genetic and environmental changes at all levels of organization many biological functions of escherichia coli metabolism can be sustained against singlegene or even multiplegene mutations by using redundant or alternative pathways thus only a limited number of genes have be... | [['complex', 'biological', 'systems', 'are', 'very', 'robust', 'to', 'genetic', 'and', 'environmental', 'changes', 'at', 'all', 'levels', 'of', 'organization', 'many', 'biological', 'functions', 'of', 'escherichia', 'coli', 'metabolism', 'can', 'be', 'sustained', 'against', 'singlegene', 'or', 'even', 'multiplegene', '... | [-0.11393321163454834, 0.128113304026221, -0.020109824969465683, 0.0857529782693583, -0.017870762665751414, -0.12456442546840776, 0.07752253383106149, 0.3378646975795539, -0.24256918269362468, -0.2913184900355725, 0.07772318941114739, -0.23758660187129282, -0.22053427346379714, 0.19374998978139898, -0.08031202731329706... |
708.1866 | On the equivalence of the microcanonical and the canonical ensembles: a
geometrical approach | In this paper, we consider the volume enclosed by the microcanonical ensemble
in phase space as a statistical ensemble. This can be interpreted as an
intermediate image between the microcanonical and the canonical pictures. By
maintaining the ergodic hypothesis over this ensemble, that is, the
equiprobability of all ... | nlin.CD cond-mat.stat-mech stat.ME | in this paper we consider the volume enclosed by the microcanonical ensemble in phase space as a statistical ensemble this can be interpreted as an intermediate image between the microcanonical and the canonical pictures by maintaining the ergodic hypothesis over this ensemble that is the equiprobability of all its acc... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'volume', 'enclosed', 'by', 'the', 'microcanonical', 'ensemble', 'in', 'phase', 'space', 'as', 'a', 'statistical', 'ensemble', 'this', 'can', 'be', 'interpreted', 'as', 'an', 'intermediate', 'image', 'between', 'the', 'microcanonical', 'and', 'the', 'canonical', 'pictur... | [-0.05503295523576869, 0.16295447923313883, -0.15121565519322483, 0.09424771034852865, 0.06740388351949458, -0.041438930562504056, 0.060548513666463064, 0.3226983184697774, -0.2645229982379121, -0.2678660416343021, 0.030498521784603275, -0.25998786382623157, -0.09636736411671594, 0.1393045016722578, -0.0596709902670656... |
708.1867 | Remarks on symplectic twistor spaces | We consider some classical fibre bundles furnished with almost complex
structures of twistor type, deduce their integrability in some cases and study
\textit{self-holomorphic} sections of a \textit{symplectic} twistor space. With
these we define a moduli space of $\omega$-compatible complex structures. We
recall the ... | math.DG math.CV | we consider some classical fibre bundles furnished with almost complex structures of twistor type deduce their integrability in some cases and study textitselfholomorphic sections of a textitsymplectic twistor space with these we define a moduli space of omegacompatible complex structures we recall the theory of flag m... | [['we', 'consider', 'some', 'classical', 'fibre', 'bundles', 'furnished', 'with', 'almost', 'complex', 'structures', 'of', 'twistor', 'type', 'deduce', 'their', 'integrability', 'in', 'some', 'cases', 'and', 'study', 'textitselfholomorphic', 'sections', 'of', 'a', 'textitsymplectic', 'twistor', 'space', 'with', 'these'... | [-0.18553440099683507, 0.08605764131465152, -0.08893408909403157, 0.09452917364697977, -0.14664691100173657, -0.06186737287051902, -0.031190787429349626, 0.36639500022082044, -0.2774732614185034, -0.19702530435590757, 0.1239329659054978, -0.21479012865093675, -0.2324209654021381, 0.1901615267933005, -0.0941823581441093... |
708.1868 | The alternative model of the spherical oscillator | The quasiradial wave functions and energy spectra of the alternative model of
spherical oscillator on the $D$-dimensional sphere and two-sheeted hyperboloid
are found.
| quant-ph | the quasiradial wave functions and energy spectra of the alternative model of spherical oscillator on the ddimensional sphere and twosheeted hyperboloid are found | [['the', 'quasiradial', 'wave', 'functions', 'and', 'energy', 'spectra', 'of', 'the', 'alternative', 'model', 'of', 'spherical', 'oscillator', 'on', 'the', 'ddimensional', 'sphere', 'and', 'twosheeted', 'hyperboloid', 'are', 'found']] | [-0.11666462390238176, 0.10925103981128853, -0.06094479534532065, 0.10064165763880896, -0.05324159704310739, -0.09253193267985531, -0.10165776004609854, 0.3577735581354279, -0.15945029611010914, -0.20512602251508963, 0.07833609681414522, -0.2975344858739687, -0.15617753419539201, 0.2196206507050311, 0.03660747329653848... |
708.1869 | Broadcasting of continuous variable entanglement | We present a scheme for broadcasting of continuous variable entanglement. We
show how an initial two-mode squeezed state of the electromagnetic field shared
by two distant parties can be broadcasted into two nonlocal bipartite entangled
states. Our protocol uses a local linear amplifier and a beam splitter at each
en... | quant-ph | we present a scheme for broadcasting of continuous variable entanglement we show how an initial twomode squeezed state of the electromagnetic field shared by two distant parties can be broadcasted into two nonlocal bipartite entangled states our protocol uses a local linear amplifier and a beam splitter at each end we ... | [['we', 'present', 'a', 'scheme', 'for', 'broadcasting', 'of', 'continuous', 'variable', 'entanglement', 'we', 'show', 'how', 'an', 'initial', 'twomode', 'squeezed', 'state', 'of', 'the', 'electromagnetic', 'field', 'shared', 'by', 'two', 'distant', 'parties', 'can', 'be', 'broadcasted', 'into', 'two', 'nonlocal', 'bip... | [-0.19886237607857624, 0.22039879217018923, -0.13244918608046197, 0.01793687916421271, 0.03461686416541214, -0.2684358802031387, 0.07597230779696498, 0.41943498904054816, -0.2622854092775227, -0.22683076515140665, 0.04231890697975631, -0.2560638440893842, -0.07214417763344654, 0.18323176564019802, -0.024958858665611063... |
708.187 | Multifractal spectrum of phase space related to generalized
thermostatistics | We consider a self-similar phase space with specific fractal dimension $d$
being distributed with spectrum function $f(d)$. Related thermostatistics is
shown to be governed by the Tsallis formalism of the non-extensive statistics,
where the non-additivity parameter is equal to ${\bar\tau}(q)\equiv
1/\tau(q)>1$, and t... | cond-mat.stat-mech | we consider a selfsimilar phase space with specific fractal dimension d being distributed with spectrum function fd related thermostatistics is shown to be governed by the tsallis formalism of the nonextensive statistics where the nonadditivity parameter is equal to bartauqequiv 1tauq1 and the multifractal function tau... | [['we', 'consider', 'a', 'selfsimilar', 'phase', 'space', 'with', 'specific', 'fractal', 'dimension', 'd', 'being', 'distributed', 'with', 'spectrum', 'function', 'fd', 'related', 'thermostatistics', 'is', 'shown', 'to', 'be', 'governed', 'by', 'the', 'tsallis', 'formalism', 'of', 'the', 'nonextensive', 'statistics', '... | [-0.10867841106934335, 0.17659713212331687, -0.10154235366455934, 0.0773490456078075, -0.01846998476568483, -0.1609451156310783, 0.02625847657004164, 0.2891650037936303, -0.29993308077560576, -0.25117970516554505, 0.021007802384117917, -0.3203923123885797, -0.1103948270212169, 0.14979801372406476, -0.04239889457936824,... |
708.1871 | Gravitational Lorentz Violation and Superluminality via AdS/CFT Duality | A weak quantum mechanical coupling is constructed permitting superluminal
communication within a preferred region of a gravitating AdS_5 spacetime. This
is achieved by adding a spatially non-local perturbation of a special kind to
the Hamiltonian of a four-dimensional conformal field theory with a
weakly-coupled AdS ... | hep-th | a weak quantum mechanical coupling is constructed permitting superluminal communication within a preferred region of a gravitating ads_5 spacetime this is achieved by adding a spatially nonlocal perturbation of a special kind to the hamiltonian of a fourdimensional conformal field theory with a weaklycoupled ads dual s... | [['a', 'weak', 'quantum', 'mechanical', 'coupling', 'is', 'constructed', 'permitting', 'superluminal', 'communication', 'within', 'a', 'preferred', 'region', 'of', 'a', 'gravitating', 'ads_5', 'spacetime', 'this', 'is', 'achieved', 'by', 'adding', 'a', 'spatially', 'nonlocal', 'perturbation', 'of', 'a', 'special', 'kin... | [-0.1622264739981962, 0.15285653861621326, -0.09733231975149144, 0.10483286933209884, -0.1280497305560857, -0.19156638630802797, -0.011715974921839113, 0.2801641417112585, -0.1728837938691654, -0.2594653116984238, 0.11101615368491313, -0.2490885986960219, -0.14947849765817142, 0.1429504793298239, -0.06135200463626568, ... |
708.1872 | Probing new physics with flavor physics (and probing flavor physics with
new physics) | This is a written version of a series of lectures aimed at graduate students
and postdoctoral fellows in particle theory/string theory/particle experiment
familiar with the basics of the Standard Model. We begin with an overview of
flavor physics and its implications for new physics. We emphasize the "new
physics fla... | hep-ph | this is a written version of a series of lectures aimed at graduate students and postdoctoral fellows in particle theorystring theoryparticle experiment familiar with the basics of the standard model we begin with an overview of flavor physics and its implications for new physics we emphasize the new physics flavor puz... | [['this', 'is', 'a', 'written', 'version', 'of', 'a', 'series', 'of', 'lectures', 'aimed', 'at', 'graduate', 'students', 'and', 'postdoctoral', 'fellows', 'in', 'particle', 'theorystring', 'theoryparticle', 'experiment', 'familiar', 'with', 'the', 'basics', 'of', 'the', 'standard', 'model', 'we', 'begin', 'with', 'an',... | [0.02066607362322622, 0.2317859493664538, -0.0675173596528387, 0.14305916683268594, -0.11610030324311194, -0.21332284510770644, 0.08578090337951752, 0.2547433693067763, -0.23233802543219292, -0.355364954261335, 0.09225219551114026, -0.3160727551898383, -0.05531735097236268, 0.17968739661525682, 0.010641218718691644, 0.... |
708.1873 | Systematics of String Loop Corrections in Type IIB Calabi-Yau Flux
Compactifications | We study the behaviour of the string loop corrections to the N=1 4D
supergravity Kaehler potential that occur in flux compactifications of IIB
string theory on general Calabi-Yau three-folds. We give a low energy
interpretation for the conjecture of Berg, Haack and Pajer for the form of the
loop corrections to the Ka... | hep-th | we study the behaviour of the string loop corrections to the n1 4d supergravity kaehler potential that occur in flux compactifications of iib string theory on general calabiyau threefolds we give a low energy interpretation for the conjecture of berg haack and pajer for the form of the loop corrections to the kaehler p... | [['we', 'study', 'the', 'behaviour', 'of', 'the', 'string', 'loop', 'corrections', 'to', 'the', 'n1', '4d', 'supergravity', 'kaehler', 'potential', 'that', 'occur', 'in', 'flux', 'compactifications', 'of', 'iib', 'string', 'theory', 'on', 'general', 'calabiyau', 'threefolds', 'we', 'give', 'a', 'low', 'energy', 'interp... | [-0.15153290531324112, 0.08269544128706911, -0.07570107236011502, 0.16146121923948692, -0.07817421525525038, -0.12246797194649629, 0.012212899054729325, 0.3106088278349489, -0.2011979030280867, -0.259804344473078, 0.08514431091778747, -0.2615954631597132, -0.2124536145642838, 0.15543749622781486, -0.10254034611040398, ... |
708.1874 | Point estimation with exponentially tilted empirical likelihood | Parameters defined via general estimating equations (GEE) can be estimated by
maximizing the empirical likelihood (EL). Newey and Smith [Econometrica 72
(2004) 219--255] have recently shown that this EL estimator exhibits desirable
higher-order asymptotic properties, namely, that its $O(n^{-1})$ bias is small
and tha... | math.ST q-fin.ST stat.TH | parameters defined via general estimating equations gee can be estimated by maximizing the empirical likelihood el newey and smith econometrica 72 2004 219255 have recently shown that this el estimator exhibits desirable higherorder asymptotic properties namely that its on1 bias is small and that biascorrected el is hi... | [['parameters', 'defined', 'via', 'general', 'estimating', 'equations', 'gee', 'can', 'be', 'estimated', 'by', 'maximizing', 'the', 'empirical', 'likelihood', 'el', 'newey', 'and', 'smith', 'econometrica', '72', '2004', '219255', 'have', 'recently', 'shown', 'that', 'this', 'el', 'estimator', 'exhibits', 'desirable', '... | [-0.0870420198707382, 0.06220169793840335, -0.10701943827754729, 0.11348029801682633, -0.07928243691057017, -0.16402084112473547, -0.010693544888516492, 0.3209179307554198, -0.26890045316086136, -0.3127417273130523, 0.09876360133934561, -0.264299892565261, -0.1890503217191882, 0.15937770046580788, -0.15784602827226665,... |
708.1875 | Blowups of Heterotic Orbifolds using Toric Geometry | Heterotic orbifold models are promising candidates for models with MSSM like
spectra. But orbifolds only correspond to a special place in moduli space, the
bigger picture is described by the moduli space of Calabi-Yau spaces. In this
talk we will make explicit connections between both points of view. To this end
we s... | hep-th | heterotic orbifold models are promising candidates for models with mssm like spectra but orbifolds only correspond to a special place in moduli space the bigger picture is described by the moduli space of calabiyau spaces in this talk we will make explicit connections between both points of view to this end we study bl... | [['heterotic', 'orbifold', 'models', 'are', 'promising', 'candidates', 'for', 'models', 'with', 'mssm', 'like', 'spectra', 'but', 'orbifolds', 'only', 'correspond', 'to', 'a', 'special', 'place', 'in', 'moduli', 'space', 'the', 'bigger', 'picture', 'is', 'described', 'by', 'the', 'moduli', 'space', 'of', 'calabiyau', '... | [-0.15226795037833418, 0.05143578631755013, -0.10028279521925883, 0.18151025462656753, -0.10610149305483157, -0.1912875427931015, 0.002007565149650365, 0.39513215139605007, -0.20180673038514405, -0.2528868011356174, 0.11286187439993653, -0.2644671808970584, -0.18690318446122595, 0.18213987744764074, -0.1620111265038321... |
708.1876 | Conductance quantization and snake states in graphene magnetic
waveguides | We consider electron waveguides (quantum wires) in graphene created by
suitable inhomogeneous magnetic fields. The properties of uni-directional snake
states are discussed. For a certain magnetic field profile, two spatially
separated counter-propagating snake states are formed, leading to conductance
quantization in... | cond-mat.mes-hall | we consider electron waveguides quantum wires in graphene created by suitable inhomogeneous magnetic fields the properties of unidirectional snake states are discussed for a certain magnetic field profile two spatially separated counterpropagating snake states are formed leading to conductance quantization insensitive ... | [['we', 'consider', 'electron', 'waveguides', 'quantum', 'wires', 'in', 'graphene', 'created', 'by', 'suitable', 'inhomogeneous', 'magnetic', 'fields', 'the', 'properties', 'of', 'unidirectional', 'snake', 'states', 'are', 'discussed', 'for', 'a', 'certain', 'magnetic', 'field', 'profile', 'two', 'spatially', 'separate... | [-0.2890585071827267, 0.3479514782883081, 0.006619263120799088, 0.05888757966093573, 0.004206033496587884, -0.18749435128205838, -0.04316261437648505, 0.4424185493194005, -0.2899935232365833, -0.27220179063870625, -0.04063483280376257, -0.24495963874619966, -0.10238959879943114, 0.16115235206305834, 0.02960624998691035... |
708.1877 | A nearly tight memory-redundancy trade-off for one-pass compression | Let $s$ be a string of length $n$ over an alphabet of constant size $\sigma$
and let $c$ and $\epsilon$ be constants with (1 \geq c \geq 0) and (\epsilon >
0). Using (O (n)) time, (O (n^c)) bits of memory and one pass we can always
encode $s$ in (n H_k (s) + O (\sigma^k n^{1 - c + \epsilon})) bits for all
integers (k... | cs.IT math.IT | let s be a string of length n over an alphabet of constant size sigma and let c and epsilon be constants with 1 geq c geq 0 and epsilon 0 using o n time o nc bits of memory and one pass we can always encode s in n h_k s o sigmak n1 c epsilon bits for all integers k geq 0 simultaneously on the other hand even with unlim... | [['let', 's', 'be', 'a', 'string', 'of', 'length', 'n', 'over', 'an', 'alphabet', 'of', 'constant', 'size', 'sigma', 'and', 'let', 'c', 'and', 'epsilon', 'be', 'constants', 'with', '1', 'geq', 'c', 'geq', '0', 'and', 'epsilon', '0', 'using', 'o', 'n', 'time', 'o', 'nc', 'bits', 'of', 'memory', 'and', 'one', 'pass', 'we... | [-0.2447168165214222, 0.22224216194539353, 0.08337064537530144, -0.03984848701145017, 0.03218471931069399, -0.3998732227375041, 0.11522264936421481, 0.33859152660739644, -0.2848545269333516, -0.31182844276298527, -0.008500197881302383, -0.34540160562567135, 0.020350890826968546, 0.07818302240964302, 0.00086086737509402... |
708.1878 | Room temperature triggered single-photon source in the near infrared | We report the realization of a solid-state triggered single-photon source
with narrow emission in the near infrared at room temperature. It is based on
the photoluminescence of a single nickel-nitrogen NE8 colour centre in a
chemical vapour deposited diamond nanocrystal. Stable single-photon emission
has been observe... | quant-ph | we report the realization of a solidstate triggered singlephoton source with narrow emission in the near infrared at room temperature it is based on the photoluminescence of a single nickelnitrogen ne8 colour centre in a chemical vapour deposited diamond nanocrystal stable singlephoton emission has been observed in the... | [['we', 'report', 'the', 'realization', 'of', 'a', 'solidstate', 'triggered', 'singlephoton', 'source', 'with', 'narrow', 'emission', 'in', 'the', 'near', 'infrared', 'at', 'room', 'temperature', 'it', 'is', 'based', 'on', 'the', 'photoluminescence', 'of', 'a', 'single', 'nickelnitrogen', 'ne8', 'colour', 'centre', 'in... | [-0.09890644053067965, 0.15794705736297596, -0.09643299642455162, -0.061354280414083334, 0.031103040884496478, -0.17864770535379648, 0.09279541074463367, 0.5426248352550254, -0.17776366791251716, -0.23670593943871274, 0.036526684389933, -0.2810619249468363, -0.005061632980109204, 0.26411455189160815, -0.016608371210720... |
708.1879 | Quantum random access memory | A random access memory (RAM) uses n bits to randomly address N=2^n distinct
memory cells. A quantum random access memory (qRAM) uses n qubits to address
any quantum superposition of N memory cells. We present an architecture that
exponentially reduces the requirements for a memory call: O(log N) switches
need be thro... | quant-ph | a random access memory ram uses n bits to randomly address n2n distinct memory cells a quantum random access memory qram uses n qubits to address any quantum superposition of n memory cells we present an architecture that exponentially reduces the requirements for a memory call olog n switches need be thrown instead of... | [['a', 'random', 'access', 'memory', 'ram', 'uses', 'n', 'bits', 'to', 'randomly', 'address', 'n2n', 'distinct', 'memory', 'cells', 'a', 'quantum', 'random', 'access', 'memory', 'qram', 'uses', 'n', 'qubits', 'to', 'address', 'any', 'quantum', 'superposition', 'of', 'n', 'memory', 'cells', 'we', 'present', 'an', 'archi... | [-0.2011694440916839, 0.20718086751517745, -0.011979835860506452, 0.03459481120572867, -0.053499897490396645, -0.29436897914950744, 0.1245039355590695, 0.3544560203780279, -0.2562764942307364, -0.27966123872032067, 0.03931747333880401, -0.24246870017036645, -0.12042776375275219, 0.1815839231442284, -0.13310140676119112... |
708.188 | Cram\'{e}r-type large deviations for samples from a finite population | Cram\'{e}r-type large deviations for means of samples from a finite
population are established under weak conditions. The results are comparable to
results for the so-called self-normalized large deviation for independent
random variables. Cram\'{e}r-type large deviations for the finite population
Student $t$-statist... | math.ST stat.TH | cramertype large deviations for means of samples from a finite population are established under weak conditions the results are comparable to results for the socalled selfnormalized large deviation for independent random variables cramertype large deviations for the finite population student tstatistic are also investi... | [['cramertype', 'large', 'deviations', 'for', 'means', 'of', 'samples', 'from', 'a', 'finite', 'population', 'are', 'established', 'under', 'weak', 'conditions', 'the', 'results', 'are', 'comparable', 'to', 'results', 'for', 'the', 'socalled', 'selfnormalized', 'large', 'deviation', 'for', 'independent', 'random', 'var... | [-0.025590098736178003, 0.18578016622499985, -0.07418259842829271, 0.19574487463317133, -0.04104360283500599, -0.11506621932229874, 0.08555450242817063, 0.3087641476992179, -0.2510118825699795, -0.26585111070678313, 0.12964185244742443, -0.3060369715941223, -0.025863175407390703, 0.29159509585323656, -0.081842737759209... |
708.1881 | The actual Rees--Sciama effect from the Local Universe | Observations of the Cosmic Microwave Background (CMB) have revealed an
unexpected quadrupole-octopole alignment along a preferred axis pointing toward
the Virgo cluster. We here investigate whether this feature can be explained in
the framework of the concordance model by secondary anisotropies produced by
the non-li... | astro-ph | observations of the cosmic microwave background cmb have revealed an unexpected quadrupoleoctopole alignment along a preferred axis pointing toward the virgo cluster we here investigate whether this feature can be explained in the framework of the concordance model by secondary anisotropies produced by the nonlinear ev... | [['observations', 'of', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'have', 'revealed', 'an', 'unexpected', 'quadrupoleoctopole', 'alignment', 'along', 'a', 'preferred', 'axis', 'pointing', 'toward', 'the', 'virgo', 'cluster', 'we', 'here', 'investigate', 'whether', 'this', 'feature', 'can', 'be', 'explained', '... | [-0.14195314848824486, 0.08039305836571214, -0.09677030703226597, 0.08825036597201708, -0.09023933917636273, -0.050765128472971925, 0.012377470058577202, 0.36585443486686353, -0.2376506672110505, -0.31421227222356773, 0.06343247176695692, -0.26845937706240564, -0.08838944918345756, 0.1786026818824961, 0.031868181546059... |
708.1882 | The role of symmetries in adiabatic quantum algorithms | Exploiting the similarity between adiabatic quantum algorithms and quantum
phase transitions, we argue that second-order transitions -- typically
associated with broken or restored symmetries -- should be advantageous in
comparison to first-order transitions. Guided by simple examples we construct
an alternative adia... | quant-ph | exploiting the similarity between adiabatic quantum algorithms and quantum phase transitions we argue that secondorder transitions typically associated with broken or restored symmetries should be advantageous in comparison to firstorder transitions guided by simple examples we construct an alternative adiabatic algori... | [['exploiting', 'the', 'similarity', 'between', 'adiabatic', 'quantum', 'algorithms', 'and', 'quantum', 'phase', 'transitions', 'we', 'argue', 'that', 'secondorder', 'transitions', 'typically', 'associated', 'with', 'broken', 'or', 'restored', 'symmetries', 'should', 'be', 'advantageous', 'in', 'comparison', 'to', 'fir... | [-0.11885575167222047, 0.15033641587919863, -0.06343248677685072, 0.09273485420884467, -0.050824865321383667, -0.18563325116901022, 0.07481355492123648, 0.3675074053474849, -0.2875989079794013, -0.3197467586540274, 0.0834866593591869, -0.24019442504320881, -0.15726225734688343, 0.20291464359401482, -0.00879433067074339... |
708.1883 | Limits on spin-dependent WIMP-nucleon cross-sections from the first
ZEPLIN-II data | The first underground data run of the ZEPLIN-II experiment has set a limit on
the nuclear recoil rate in the two-phase xenon detector for direct dark matter
searches. In this paper the results from this run are converted into the limits
on spin-dependent WIMP-proton and WIMP-neutron cross-sections. The minimum of
the... | astro-ph | the first underground data run of the zeplinii experiment has set a limit on the nuclear recoil rate in the twophase xenon detector for direct dark matter searches in this paper the results from this run are converted into the limits on spindependent wimpproton and wimpneutron crosssections the minimum of the curve for... | [['the', 'first', 'underground', 'data', 'run', 'of', 'the', 'zeplinii', 'experiment', 'has', 'set', 'a', 'limit', 'on', 'the', 'nuclear', 'recoil', 'rate', 'in', 'the', 'twophase', 'xenon', 'detector', 'for', 'direct', 'dark', 'matter', 'searches', 'in', 'this', 'paper', 'the', 'results', 'from', 'this', 'run', 'are',... | [-0.051859515024098884, 0.13359765292131412, -0.08289699208463973, 0.07802894431055148, 0.00040308721433046147, -0.057590111297791576, 0.07362621953300853, 0.2750881234871974, -0.15154469382963073, -0.36880209346982973, 0.04019006963388355, -0.37027323001356266, 0.10417478794315413, 0.24864251696532452, 0.0731272625514... |
708.1884 | Superconductivity without attraction in a quasi-one-dimensional metal | An array of one-dimensional conductors coupled by transverse hopping and
interaction is studied with the help of a variational wave function. This wave
function is devised as to account for one-dimensional correlation effects. We
show that under broad conditions our system possesses the superconducting
ground state e... | cond-mat.supr-con cond-mat.str-el | an array of onedimensional conductors coupled by transverse hopping and interaction is studied with the help of a variational wave function this wave function is devised as to account for onedimensional correlation effects we show that under broad conditions our system possesses the superconducting ground state even if... | [['an', 'array', 'of', 'onedimensional', 'conductors', 'coupled', 'by', 'transverse', 'hopping', 'and', 'interaction', 'is', 'studied', 'with', 'the', 'help', 'of', 'a', 'variational', 'wave', 'function', 'this', 'wave', 'function', 'is', 'devised', 'as', 'to', 'account', 'for', 'onedimensional', 'correlation', 'effect... | [-0.2093182095825406, 0.22467637965881815, -0.06539297383278608, 0.05317870482020745, -0.04757379339176363, -0.17250100776020968, 0.03754442701881219, 0.35758877898167285, -0.21778255255693305, -0.2528423847942447, 0.023711475523720896, -0.3167493459801855, -0.13087071190155777, 0.12034470791030409, 0.09507898005124714... |
708.1885 | Posterior convergence rates of Dirichlet mixtures at smooth densities | We study the rates of convergence of the posterior distribution for Bayesian
density estimation with Dirichlet mixtures of normal distributions as the
prior. The true density is assumed to be twice continuously differentiable. The
bandwidth is given a sequence of priors which is obtained by scaling a single
prior by ... | math.ST stat.TH | we study the rates of convergence of the posterior distribution for bayesian density estimation with dirichlet mixtures of normal distributions as the prior the true density is assumed to be twice continuously differentiable the bandwidth is given a sequence of priors which is obtained by scaling a single prior by an a... | [['we', 'study', 'the', 'rates', 'of', 'convergence', 'of', 'the', 'posterior', 'distribution', 'for', 'bayesian', 'density', 'estimation', 'with', 'dirichlet', 'mixtures', 'of', 'normal', 'distributions', 'as', 'the', 'prior', 'the', 'true', 'density', 'is', 'assumed', 'to', 'be', 'twice', 'continuously', 'differentia... | [-0.07413544568134416, 0.0717054103099861, -0.09885895717042413, 0.11302003773550193, -0.036270062520987155, -0.09173098125805458, 0.119929758794641, 0.34548537397023404, -0.279648173982842, -0.28547918846774284, 0.1219786090042555, -0.21146138711253915, -0.05390178116997986, 0.186911679419449, -0.10671410002378803, 0.... |
708.1886 | Quantitative Determination of Enhanced and Suppressed Transmission
through Subwavelength Slit Arrays in Silver Films | Measurement of the transmitted intensity from a coherent monomode light
source through a series of subwavelength slit arrays in Ag films, with varying
array pitch and number of slits, demonstrate enhancement (suppression) by as
much as a factor of 6 (9) when normalized to that of an isolated slit.
Pronounced minima i... | physics.optics | measurement of the transmitted intensity from a coherent monomode light source through a series of subwavelength slit arrays in ag films with varying array pitch and number of slits demonstrate enhancement suppression by as much as a factor of 6 9 when normalized to that of an isolated slit pronounced minima in the tra... | [['measurement', 'of', 'the', 'transmitted', 'intensity', 'from', 'a', 'coherent', 'monomode', 'light', 'source', 'through', 'a', 'series', 'of', 'subwavelength', 'slit', 'arrays', 'in', 'ag', 'films', 'with', 'varying', 'array', 'pitch', 'and', 'number', 'of', 'slits', 'demonstrate', 'enhancement', 'suppression', 'by'... | [-0.12712103802706615, 0.18237030780138802, -0.04820511883008294, 0.013131644361627488, -0.005492310671667967, -0.15788449642630958, 0.017626160090523108, 0.46194502151670996, -0.23526112035116448, -0.3596855453839193, 0.028262709454533512, -0.327495522256608, -0.1077490327900575, 0.24484326732635964, 0.007342702056381... |
708.1887 | Study and characterization by magnetophonon resonance of the energy
structuring in GaAs/AlAs quantum-wire superlattices | We present the characterization of the band structure of GaAs/AlAs
quantum-wire 1D superlattices performed by magnetophonon resonance with pulsed
magnetic fields up to 35 T. The samples, generated by the "atomic saw method"
from original quantum-well 2D superlattices, underwent substantial
modifications of their ener... | cond-mat.mes-hall cond-mat.dis-nn | we present the characterization of the band structure of gaasalas quantumwire 1d superlattices performed by magnetophonon resonance with pulsed magnetic fields up to 35 t the samples generated by the atomic saw method from original quantumwell 2d superlattices underwent substantial modifications of their energy bands b... | [['we', 'present', 'the', 'characterization', 'of', 'the', 'band', 'structure', 'of', 'gaasalas', 'quantumwire', '1d', 'superlattices', 'performed', 'by', 'magnetophonon', 'resonance', 'with', 'pulsed', 'magnetic', 'fields', 'up', 'to', '35', 't', 'the', 'samples', 'generated', 'by', 'the', 'atomic', 'saw', 'method', '... | [-0.12943107138267873, 0.13196620272418577, -0.04625195325237979, 0.00928547020081682, 0.017544670961797237, -0.10373310472650533, 0.07879449159158336, 0.40781448328684716, -0.25854546174855525, -0.3271013320383667, 0.0261003576044816, -0.2716901401427262, -0.1099978909010719, 0.2067815448925973, 0.05349695339707509, 0... |
708.1888 | Statistical mechanics and thermodynamic limit of self-gravitating
fermions in D dimensions | We discuss the statistical mechanics of a system of self-gravitating fermions
in a space of dimension $D$. We plot the caloric curves of the self-gravitating
Fermi gas giving the temperature as a function of energy and investigate the
nature of phase transitions as a function of the dimension of space. We
consider st... | cond-mat.stat-mech | we discuss the statistical mechanics of a system of selfgravitating fermions in a space of dimension d we plot the caloric curves of the selfgravitating fermi gas giving the temperature as a function of energy and investigate the nature of phase transitions as a function of the dimension of space we consider stable sta... | [['we', 'discuss', 'the', 'statistical', 'mechanics', 'of', 'a', 'system', 'of', 'selfgravitating', 'fermions', 'in', 'a', 'space', 'of', 'dimension', 'd', 'we', 'plot', 'the', 'caloric', 'curves', 'of', 'the', 'selfgravitating', 'fermi', 'gas', 'giving', 'the', 'temperature', 'as', 'a', 'function', 'of', 'energy', 'an... | [-0.12981011753050464, 0.17882233168032155, -0.11809973737662546, 0.1197029656852618, 0.011809984379145036, -0.12322743390462394, 0.06997250250950231, 0.2633445667922048, -0.23343386715390238, -0.2858293383993792, 0.06825307462047449, -0.2618674551142402, -0.12647542956633023, 0.16059057305620264, -0.02124467168945864,... |
708.1889 | Zero temperature solutions of the Edwards-Anderson model in random
Husimi Lattices | We solve the Edwards-Anderson model (EA) in different Husimi lattices. We
show that, at T=0, the structure of the solution space depends on the parity of
the loop sizes. Husimi lattices with odd loop sizes have always a trivial
paramagnetic solution stable under 1RSB perturbations while, in Husimi lattices
with even ... | cond-mat.dis-nn cond-mat.stat-mech | we solve the edwardsanderson model ea in different husimi lattices we show that at t0 the structure of the solution space depends on the parity of the loop sizes husimi lattices with odd loop sizes have always a trivial paramagnetic solution stable under 1rsb perturbations while in husimi lattices with even loop sizes ... | [['we', 'solve', 'the', 'edwardsanderson', 'model', 'ea', 'in', 'different', 'husimi', 'lattices', 'we', 'show', 'that', 'at', 't0', 'the', 'structure', 'of', 'the', 'solution', 'space', 'depends', 'on', 'the', 'parity', 'of', 'the', 'loop', 'sizes', 'husimi', 'lattices', 'with', 'odd', 'loop', 'sizes', 'have', 'always... | [-0.14165254817951634, 0.21440301776485707, -0.08333730053973208, 0.06898429337888956, 0.0024423457655137863, -0.1464601431845053, 0.07234368324819682, 0.3900695329370058, -0.2417914222089061, -0.19680877102107025, 0.09766555020578907, -0.27098196708728844, -0.11502305168719233, 0.0958692927547879, 0.06254216801861058,... |
708.189 | On the design-consistency property of hierarchical Bayes estimators in
finite population sampling | We obtain a limit of a hierarchical Bayes estimator of a finite population
mean when the sample size is large. The limit is in the sense of ordinary
calculus, where the sample observations are treated as fixed quantities. Our
result suggests a simple way to correct the hierarchical Bayes estimator to
achieve design-c... | math.ST stat.TH | we obtain a limit of a hierarchical bayes estimator of a finite population mean when the sample size is large the limit is in the sense of ordinary calculus where the sample observations are treated as fixed quantities our result suggests a simple way to correct the hierarchical bayes estimator to achieve designconsist... | [['we', 'obtain', 'a', 'limit', 'of', 'a', 'hierarchical', 'bayes', 'estimator', 'of', 'a', 'finite', 'population', 'mean', 'when', 'the', 'sample', 'size', 'is', 'large', 'the', 'limit', 'is', 'in', 'the', 'sense', 'of', 'ordinary', 'calculus', 'where', 'the', 'sample', 'observations', 'are', 'treated', 'as', 'fixed',... | [-0.04918854356449293, 0.05021089104947781, -0.17117273144571013, 0.13112851441531492, -0.0711268626956122, -0.09945487281871274, 0.12076558111431568, 0.35728382422147614, -0.2709219490521048, -0.32066014482590716, 0.09617559674600336, -0.24784174850700716, -0.11846333944643113, 0.1684837509436827, -0.12295744542375599... |
708.1891 | Mapping the dark trajectory of the Bullet Cluster | We model the electrons/positrons produced by dark matter annihilations in the
colliding galaxy cluster system 1E0657-56 (the bullet cluster). These charged
particles, confined by the Magnetic field, clearly trace the path of the
bullet, which passes through the main cluster with a speed of 3000-5000 km/s.
Adding the ... | astro-ph hep-ph | we model the electronspositrons produced by dark matter annihilations in the colliding galaxy cluster system 1e065756 the bullet cluster these charged particles confined by the magnetic field clearly trace the path of the bullet which passes through the main cluster with a speed of 30005000 kms adding the effect of dar... | [['we', 'model', 'the', 'electronspositrons', 'produced', 'by', 'dark', 'matter', 'annihilations', 'in', 'the', 'colliding', 'galaxy', 'cluster', 'system', '1e065756', 'the', 'bullet', 'cluster', 'these', 'charged', 'particles', 'confined', 'by', 'the', 'magnetic', 'field', 'clearly', 'trace', 'the', 'path', 'of', 'the... | [-0.10256351735027931, 0.18429407346670948, -0.14206559152462253, 0.06271068508031381, -0.06277100129587816, -0.015867017905716554, 0.021463069465417085, 0.34078712137312267, -0.28055707825864157, -0.3419395020729539, -0.039188207393410696, -0.29295921230130817, 0.015614061573713945, 0.1657850141031898, 0.0817553653672... |
708.1892 | On rates of convergence for posterior distributions in
infinite-dimensional models | This paper introduces a new approach to the study of rates of convergence for
posterior distributions. It is a natural extension of a recent approach to the
study of Bayesian consistency. In particular, we improve on current rates of
convergence for models including the mixture of Dirichlet process model and the
rand... | math.ST stat.TH | this paper introduces a new approach to the study of rates of convergence for posterior distributions it is a natural extension of a recent approach to the study of bayesian consistency in particular we improve on current rates of convergence for models including the mixture of dirichlet process model and the random be... | [['this', 'paper', 'introduces', 'a', 'new', 'approach', 'to', 'the', 'study', 'of', 'rates', 'of', 'convergence', 'for', 'posterior', 'distributions', 'it', 'is', 'a', 'natural', 'extension', 'of', 'a', 'recent', 'approach', 'to', 'the', 'study', 'of', 'bayesian', 'consistency', 'in', 'particular', 'we', 'improve', 'o... | [-0.03713663317982785, 0.004264251024208286, -0.10911654013801705, 0.06633567316156669, -0.046335921809077266, -0.07986429497091607, 0.07916091695978221, 0.34609627175060187, -0.2944046689366752, -0.2603780364363708, 0.10128474739930508, -0.19888641336424784, -0.14459603049538353, 0.1931757330132479, -0.086654764494266... |
708.1893 | Sticky obstacles to intramolecular energy flow | Vibrational energy flows unevenly in molecules, repeatedly going back and
forth between trapping and roaming. We identify bottlenecks between diffusive
and chaotic behavior, and describe generic mechanisms of these transitions,
taking the carbonyl sulphide molecule OCS as a case study. The bottlenecks are
found to be... | nlin.CD physics.chem-ph | vibrational energy flows unevenly in molecules repeatedly going back and forth between trapping and roaming we identify bottlenecks between diffusive and chaotic behavior and describe generic mechanisms of these transitions taking the carbonyl sulphide molecule ocs as a case study the bottlenecks are found to be lowerd... | [['vibrational', 'energy', 'flows', 'unevenly', 'in', 'molecules', 'repeatedly', 'going', 'back', 'and', 'forth', 'between', 'trapping', 'and', 'roaming', 'we', 'identify', 'bottlenecks', 'between', 'diffusive', 'and', 'chaotic', 'behavior', 'and', 'describe', 'generic', 'mechanisms', 'of', 'these', 'transitions', 'tak... | [-0.19161817728819555, 0.19647936502945396, -0.04210847478131192, 0.11074586211001142, 0.03020873016334678, -0.1760546042208086, 0.11085821215978317, 0.37772167684804453, -0.31290795461258347, -0.23553416366574534, 0.03874748486723228, -0.298450069632708, -0.18321262958475895, 0.11766472520927589, 0.0075185996431269145... |
708.1894 | Cosmological Constraints on New Agegraphic Dark Energy | In this work, we consider the cosmological constraints on the new agegraphic
dark energy (NADE) proposed in arXiv:0708.0884, by using the observational data
of type Ia supernovae (SNIa), the shift parameter from cosmic microwave
background (CMB) and the baryon acoustic oscillation (BAO) peak from large
scale structur... | astro-ph gr-qc hep-th | in this work we consider the cosmological constraints on the new agegraphic dark energy nade proposed in arxiv07080884 by using the observational data of type ia supernovae snia the shift parameter from cosmic microwave background cmb and the baryon acoustic oscillation bao peak from large scale structures lss thanks t... | [['in', 'this', 'work', 'we', 'consider', 'the', 'cosmological', 'constraints', 'on', 'the', 'new', 'agegraphic', 'dark', 'energy', 'nade', 'proposed', 'in', 'arxiv07080884', 'by', 'using', 'the', 'observational', 'data', 'of', 'type', 'ia', 'supernovae', 'snia', 'the', 'shift', 'parameter', 'from', 'cosmic', 'microwav... | [-0.06735470911213594, 0.13041958871230758, -0.07071872672441509, 0.11997997058039285, -0.1390234285770634, -0.1356595025105445, 0.004230974393701831, 0.30801327745502366, -0.2512854192759697, -0.3376703401088946, 0.03734987315202002, -0.2832134609280313, -0.04995764957834757, 0.18751104297152496, -0.005879526208897118... |
708.1895 | Random telegraph noise from magnetic nanoclusters in the ferromagnetic
semiconductor (Ga,Mn)As | Measurements of the low frequency electrical noise in the ferromagnetic
semiconductor (Ga,Mn)As reveal an enhanced integrated noise at low temperature.
For moderate localization, we find a 1/f normalized power spectrum density over
the entire range of temperatures studied (4.2K < T < 70K). However, for
stronger local... | cond-mat.mtrl-sci | measurements of the low frequency electrical noise in the ferromagnetic semiconductor gamnas reveal an enhanced integrated noise at low temperature for moderate localization we find a 1f normalized power spectrum density over the entire range of temperatures studied 42k t 70k however for stronger localization and a hig... | [['measurements', 'of', 'the', 'low', 'frequency', 'electrical', 'noise', 'in', 'the', 'ferromagnetic', 'semiconductor', 'gamnas', 'reveal', 'an', 'enhanced', 'integrated', 'noise', 'at', 'low', 'temperature', 'for', 'moderate', 'localization', 'we', 'find', 'a', '1f', 'normalized', 'power', 'spectrum', 'density', 'ove... | [-0.16846316069250508, 0.23670534978811367, 0.03795247571542859, 0.06005011652881394, 0.05666647526216978, -0.16354444487571565, 0.07690895761170767, 0.4220946277586781, -0.23102150467813623, -0.34459763797646276, -0.02550788331605798, -0.34599678040178, -0.06669045598911387, 0.15725606361556113, 0.02044113346242479, -... |
708.1896 | Resolvable designs with large blocks | Resolvable designs with two blocks per replicate are studied from an
optimality perspective. Because in practice the number of replicates is
typically less than the number of treatments, arguments can be based on the
dual of the information matrix and consequently given in terms of block
concurrences. Equalizing bloc... | math.ST stat.TH | resolvable designs with two blocks per replicate are studied from an optimality perspective because in practice the number of replicates is typically less than the number of treatments arguments can be based on the dual of the information matrix and consequently given in terms of block concurrences equalizing block con... | [['resolvable', 'designs', 'with', 'two', 'blocks', 'per', 'replicate', 'are', 'studied', 'from', 'an', 'optimality', 'perspective', 'because', 'in', 'practice', 'the', 'number', 'of', 'replicates', 'is', 'typically', 'less', 'than', 'the', 'number', 'of', 'treatments', 'arguments', 'can', 'be', 'based', 'on', 'the', '... | [-0.11233260823717835, 0.07447013118552585, -0.022188165529193928, 0.0663251225273505, -0.05245990623311349, -0.16641591984436524, 0.023627135033092023, 0.37278592046730374, -0.20619488394420063, -0.3047051378145662, 0.1790118018255512, -0.23414383790151652, -0.15056675223738183, 0.23188621429156284, -0.106178090403958... |
708.1897 | Morita classes of algebras in modular tensor categories | We consider algebras in a modular tensor category C. If the trace pairing of
an algebra A in C is non-degenerate we associate to A a commutative algebra
Z(A), called the full centre, in a doubled version of the category C. We prove
that two simple algebras with non-degenerate trace pairing are
Morita-equivalent if an... | math.CT hep-th math.QA | we consider algebras in a modular tensor category c if the trace pairing of an algebra a in c is nondegenerate we associate to a a commutative algebra za called the full centre in a doubled version of the category c we prove that two simple algebras with nondegenerate trace pairing are moritaequivalent if and only if t... | [['we', 'consider', 'algebras', 'in', 'a', 'modular', 'tensor', 'category', 'c', 'if', 'the', 'trace', 'pairing', 'of', 'an', 'algebra', 'a', 'in', 'c', 'is', 'nondegenerate', 'we', 'associate', 'to', 'a', 'a', 'commutative', 'algebra', 'za', 'called', 'the', 'full', 'centre', 'in', 'a', 'doubled', 'version', 'of', 'th... | [-0.175707690625828, 0.0918266944109804, -0.09108954740371158, 0.07849057476306236, -0.10944176302539145, -0.17711768820485535, -0.051837776651348366, 0.38963781697477434, -0.3625356552210894, -0.13436230801744387, 0.10705941795629073, -0.22696602400986754, -0.15412265031866015, 0.16783596331531064, -0.1296172702209429... |
708.1898 | On the dynamics of point vortices in a quantum gas confined in an
annular region | The dynamics of one and two pointlike vortices in a planar quantum gas of
spin-0 particles confined in an annular region is considered. New analytical
and numerical solutions are found. The concept of stationarity radius, related
to the doubly connected nature of the annulus, is defined. It is seen that the
existence... | cond-mat.stat-mech quant-ph | the dynamics of one and two pointlike vortices in a planar quantum gas of spin0 particles confined in an annular region is considered new analytical and numerical solutions are found the concept of stationarity radius related to the doubly connected nature of the annulus is defined it is seen that the existence of thes... | [['the', 'dynamics', 'of', 'one', 'and', 'two', 'pointlike', 'vortices', 'in', 'a', 'planar', 'quantum', 'gas', 'of', 'spin0', 'particles', 'confined', 'in', 'an', 'annular', 'region', 'is', 'considered', 'new', 'analytical', 'and', 'numerical', 'solutions', 'are', 'found', 'the', 'concept', 'of', 'stationarity', 'radi... | [-0.21363313676981002, 0.1600917068197608, -0.09041073355668534, 0.08298943405679893, -0.02755231778913488, -0.11142970319391073, -0.04538585083840493, 0.3312895243288949, -0.2131669380372235, -0.2719974270730745, 0.09475908624032552, -0.26860642272125307, -0.11194988384765263, 0.16049917517132903, -0.00727007123138416... |
708.1899 | A First Exposure to Statistical Mechanics for Life Scientists | Statistical mechanics is one of the most powerful and elegant tools in the
quantitative sciences. One key virtue of statistical mechanics is that it is
designed to examine large systems with many interacting degrees of freedom,
providing a clue that it might have some bearing on the analysis of the
molecules of livin... | q-bio.QM | statistical mechanics is one of the most powerful and elegant tools in the quantitative sciences one key virtue of statistical mechanics is that it is designed to examine large systems with many interacting degrees of freedom providing a clue that it might have some bearing on the analysis of the molecules of living ma... | [['statistical', 'mechanics', 'is', 'one', 'of', 'the', 'most', 'powerful', 'and', 'elegant', 'tools', 'in', 'the', 'quantitative', 'sciences', 'one', 'key', 'virtue', 'of', 'statistical', 'mechanics', 'is', 'that', 'it', 'is', 'designed', 'to', 'examine', 'large', 'systems', 'with', 'many', 'interacting', 'degrees', '... | [-0.05256496172073777, 0.0965159422322882, -0.13185990901635677, 0.10219510172098649, -0.11428491590601025, -0.1464736083522439, 0.023111063830385154, 0.32828449379991403, -0.2677843783311828, -0.34465330694660995, 0.0878077043862449, -0.29199216756405255, -0.19050519606098532, 0.23959531066657017, -0.11115343690087849... |
708.19 | Gegenbauer tau methods with and without spurious eigenvalues | It is proven that a class of Gegenbauer tau approximations to a 4th order
differential eigenvalue problem of hydrodynamic type provide real, negative and
distinct eigenvalues, as is the case for the exact solutions. This class of
Gegenbauer tau methods includes Chebyshev and Legendre Galerkin and `inviscid'
Galerkin ... | math.NA math.SP | it is proven that a class of gegenbauer tau approximations to a 4th order differential eigenvalue problem of hydrodynamic type provide real negative and distinct eigenvalues as is the case for the exact solutions this class of gegenbauer tau methods includes chebyshev and legendre galerkin and inviscid galerkin but doe... | [['it', 'is', 'proven', 'that', 'a', 'class', 'of', 'gegenbauer', 'tau', 'approximations', 'to', 'a', '4th', 'order', 'differential', 'eigenvalue', 'problem', 'of', 'hydrodynamic', 'type', 'provide', 'real', 'negative', 'and', 'distinct', 'eigenvalues', 'as', 'is', 'the', 'case', 'for', 'the', 'exact', 'solutions', 'th... | [-0.093516589815004, 0.01985953233929144, -0.09204004030260775, 0.10990600160762874, -0.12232276663805047, -0.17109708826368053, -0.04644839942662252, 0.3263527261817621, -0.3045721154453026, -0.2191163376439363, 0.11343643225263804, -0.25827481858432294, -0.15775810547638686, 0.20873780602123587, -0.03607818850626548,... |
708.1901 | On the number of support points of maximin and Bayesian optimal designs | We consider maximin and Bayesian $D$-optimal designs for nonlinear regression
models. The maximin criterion requires the specification of a region for the
nonlinear parameters in the model, while the Bayesian optimality criterion
assumes that a prior for these parameters is available. On interval parameter
spaces, it... | math.ST stat.TH | we consider maximin and bayesian doptimal designs for nonlinear regression models the maximin criterion requires the specification of a region for the nonlinear parameters in the model while the bayesian optimality criterion assumes that a prior for these parameters is available on interval parameter spaces it was obse... | [['we', 'consider', 'maximin', 'and', 'bayesian', 'doptimal', 'designs', 'for', 'nonlinear', 'regression', 'models', 'the', 'maximin', 'criterion', 'requires', 'the', 'specification', 'of', 'a', 'region', 'for', 'the', 'nonlinear', 'parameters', 'in', 'the', 'model', 'while', 'the', 'bayesian', 'optimality', 'criterion... | [-0.062004781317704455, 0.01885906657342526, -0.09311080760290397, 0.13634290909635483, -0.10343811723628435, -0.1459679594070747, 0.0853527008925147, 0.40992051861409484, -0.2247771750750213, -0.30713613657601946, 0.13470750114928673, -0.20896514438991917, -0.19074468902504907, 0.22482834361043982, -0.1275124284224022... |
708.1902 | Some Open Problems in Quantum Information Theory | Some open questions in quantum information theory (QIT) are described. Most
of them were presented in Banff during the BIRS workshop on Operator Structures
in QIT 11-16 February 2007. New material has been added in view of the recent
counter-examples to p-norm multiplicativity.
| quant-ph | some open questions in quantum information theory qit are described most of them were presented in banff during the birs workshop on operator structures in qit 1116 february 2007 new material has been added in view of the recent counterexamples to pnorm multiplicativity | [['some', 'open', 'questions', 'in', 'quantum', 'information', 'theory', 'qit', 'are', 'described', 'most', 'of', 'them', 'were', 'presented', 'in', 'banff', 'during', 'the', 'birs', 'workshop', 'on', 'operator', 'structures', 'in', 'qit', '1116', 'february', '2007', 'new', 'material', 'has', 'been', 'added', 'in', 'vi... | [-0.08975503434492059, 0.08807822098132483, -0.08062680219408384, 0.07328523513536121, -0.0868699366313427, -0.15846426620386367, 0.002694102331757719, 0.3619005986337745, -0.2504561620055113, -0.34935326575366565, 0.14784661729191972, -0.3559005784607211, -0.15318117502990158, 0.20294486220146335, -0.18593100694463002... |
708.1903 | On Edge-Disjoint Pairs Of Matchings | For a graph G, consider the pairs of edge-disjoint matchings whose union
consists of as many edges as possible. Let H be the largest matching among such
pairs. Let M be a maximum matching of G. We show that 5/4 is a tight upper
bound for |M|/|H|.
| cs.DM | for a graph g consider the pairs of edgedisjoint matchings whose union consists of as many edges as possible let h be the largest matching among such pairs let m be a maximum matching of g we show that 54 is a tight upper bound for mh | [['for', 'a', 'graph', 'g', 'consider', 'the', 'pairs', 'of', 'edgedisjoint', 'matchings', 'whose', 'union', 'consists', 'of', 'as', 'many', 'edges', 'as', 'possible', 'let', 'h', 'be', 'the', 'largest', 'matching', 'among', 'such', 'pairs', 'let', 'm', 'be', 'a', 'maximum', 'matching', 'of', 'g', 'we', 'show', 'that',... | [-0.21236982141086397, 0.1593730160570208, -0.0047354463468048166, 0.005206674874879103, -0.09272443324803038, -0.12258502465494453, 0.08887878592631364, 0.3197365894002166, -0.24252839925441336, -0.4138810730519447, 0.0684494804888171, -0.33891460664094764, -0.061485669793600733, 0.17290660187582227, -0.06454697200790... |
708.1904 | Triplet spin resonance of the Haldane compound with interchain coupling | Spin resonance absorption of the triplet excitations is studied
experimentally in the Haldane magnet PbNi2V2O8. The spectrum has features of
spin S=1 resonance in a crystal field, with all three components, corresponding
to transitions between spin sublevels, being observable. The resonance field is
temperature depen... | cond-mat.str-el | spin resonance absorption of the triplet excitations is studied experimentally in the haldane magnet pbni2v2o8 the spectrum has features of spin s1 resonance in a crystal field with all three components corresponding to transitions between spin sublevels being observable the resonance field is temperature dependent ind... | [['spin', 'resonance', 'absorption', 'of', 'the', 'triplet', 'excitations', 'is', 'studied', 'experimentally', 'in', 'the', 'haldane', 'magnet', 'pbni2v2o8', 'the', 'spectrum', 'has', 'features', 'of', 'spin', 's1', 'resonance', 'in', 'a', 'crystal', 'field', 'with', 'all', 'three', 'components', 'corresponding', 'to',... | [-0.18530549552065856, 0.2450517457427758, -0.041080663135896124, 0.048355185960635844, -0.046525264262325235, -0.12957019556897006, -0.00530581192692302, 0.3820349152359848, -0.19741534899844967, -0.30649491706204535, 0.012974996539538331, -0.29134842172039277, -0.03990769298803626, 0.15231366361481974, 0.100196841158... |
708.1905 | A random walk approximation to fractional Brownian motion | We present a random walk approximation to fractional Brownian motion where
the increments of the fractional random walk are defined as a weighted sum of
the past increments of a Bernoulli random walk.
| math.PR | we present a random walk approximation to fractional brownian motion where the increments of the fractional random walk are defined as a weighted sum of the past increments of a bernoulli random walk | [['we', 'present', 'a', 'random', 'walk', 'approximation', 'to', 'fractional', 'brownian', 'motion', 'where', 'the', 'increments', 'of', 'the', 'fractional', 'random', 'walk', 'are', 'defined', 'as', 'a', 'weighted', 'sum', 'of', 'the', 'past', 'increments', 'of', 'a', 'bernoulli', 'random', 'walk']] | [-0.13928580848556577, 0.2678623226273692, -0.11258503783381346, -0.008111099430331678, -0.08013156890361146, -0.10109098539264365, 0.09601454873512866, 0.43467051637443627, -0.3213185794425733, -0.12881026496038292, 0.13604379204017195, -0.26763462218822853, -0.1733737155569322, 0.09412691358363989, -0.102976192663790... |
708.1906 | Solving QCD evolution equations in rapidity space with Markovian Monte
Carlo | This work covers methodology of solving QCD evolution equation of the parton
distribution using Markovian Monte Carlo (MMC) algorithms in a class of models
ranging from DGLAP to CCFM. One of the purposes of the above MMCs is to test
the other more sophisticated Monte Carlo programs, the so-called Constrained
Monte Ca... | hep-ph | this work covers methodology of solving qcd evolution equation of the parton distribution using markovian monte carlo mmc algorithms in a class of models ranging from dglap to ccfm one of the purposes of the above mmcs is to test the other more sophisticated monte carlo programs the socalled constrained monte carlo cmc... | [['this', 'work', 'covers', 'methodology', 'of', 'solving', 'qcd', 'evolution', 'equation', 'of', 'the', 'parton', 'distribution', 'using', 'markovian', 'monte', 'carlo', 'mmc', 'algorithms', 'in', 'a', 'class', 'of', 'models', 'ranging', 'from', 'dglap', 'to', 'ccfm', 'one', 'of', 'the', 'purposes', 'of', 'the', 'abov... | [-0.04289678970895739, 0.13609633190917367, -0.1717536160370194, 0.15742993627126062, -0.04193881906944664, -0.09744691576401726, -0.02025897239389665, 0.3910256310820016, -0.25194810774664494, -0.3188359944948128, 0.10634442247027735, -0.23933483618350715, 0.0022772907107254537, 0.18833647993933253, 0.0406909645026346... |
708.1907 | Uncovering the Active Galactic Nuclei in Low-Ionization Nuclear
Emission-Line Regions with Spitzer | The impact of active galactic nuclei on low-ionization nuclear emission-line
regions (LINERs) remains a vigorous field of study. We present preliminary
results from a study of the mid-infrared atomic emission lines of LINERs with
the Spitzer Space Telescope. We assess the ubiquity and properties of AGN in
LINERs usin... | astro-ph | the impact of active galactic nuclei on lowionization nuclear emissionline regions liners remains a vigorous field of study we present preliminary results from a study of the midinfrared atomic emission lines of liners with the spitzer space telescope we assess the ubiquity and properties of agn in liners using this da... | [['the', 'impact', 'of', 'active', 'galactic', 'nuclei', 'on', 'lowionization', 'nuclear', 'emissionline', 'regions', 'liners', 'remains', 'a', 'vigorous', 'field', 'of', 'study', 'we', 'present', 'preliminary', 'results', 'from', 'a', 'study', 'of', 'the', 'midinfrared', 'atomic', 'emission', 'lines', 'of', 'liners', ... | [-0.004603594109781463, 0.06333437489487137, -0.018263994704318953, 0.11403390718476634, -0.08240090558140338, -0.030775006518616706, 0.09707266857104871, 0.5031051297636726, -0.08741759461692616, -0.26242319986082707, 0.051138935715278395, -0.31027436588855484, -0.04195961405676377, 0.18592481561229104, -0.01829300453... |
708.1908 | Complete enumeration of two-Level orthogonal arrays of strength $d$ with
$d+2$ constraints | Enumerating nonisomorphic orthogonal arrays is an important, yet very
difficult, problem. Although orthogonal arrays with a specified set of
parameters have been enumerated in a number of cases, general results are
extremely rare. In this paper, we provide a complete solution to enumerating
nonisomorphic two-level or... | math.ST stat.TH | enumerating nonisomorphic orthogonal arrays is an important yet very difficult problem although orthogonal arrays with a specified set of parameters have been enumerated in a number of cases general results are extremely rare in this paper we provide a complete solution to enumerating nonisomorphic twolevel orthogonal ... | [['enumerating', 'nonisomorphic', 'orthogonal', 'arrays', 'is', 'an', 'important', 'yet', 'very', 'difficult', 'problem', 'although', 'orthogonal', 'arrays', 'with', 'a', 'specified', 'set', 'of', 'parameters', 'have', 'been', 'enumerated', 'in', 'a', 'number', 'of', 'cases', 'general', 'results', 'are', 'extremely', '... | [-0.16491475653166363, 0.0924339866531588, -0.02133092850105453, 0.009022134249560705, -0.08218890186825781, -0.1731564174441777, 0.02772849720710789, 0.38986822851855335, -0.20124260444577982, -0.3109936909394637, 0.11023115954461386, -0.2465328556976018, -0.18177178560557086, 0.24585138862056813, -0.03736898001596218... |
708.1909 | Lower Bounds for the Complexity of the Voronoi Diagram of Polygonal
Curves under the Discrete Frechet Distance | We give lower bounds for the combinatorial complexity of the Voronoi diagram
of polygonal curves under the discrete Frechet distance. We show that the
Voronoi diagram of n curves in R^d with k vertices each, has complexity
Omega(n^{dk}) for dimension d=1,2 and Omega(n^{d(k-1)+2}) for d>2.
| cs.CG cs.CC | we give lower bounds for the combinatorial complexity of the voronoi diagram of polygonal curves under the discrete frechet distance we show that the voronoi diagram of n curves in rd with k vertices each has complexity omegandk for dimension d12 and omegandk12 for d2 | [['we', 'give', 'lower', 'bounds', 'for', 'the', 'combinatorial', 'complexity', 'of', 'the', 'voronoi', 'diagram', 'of', 'polygonal', 'curves', 'under', 'the', 'discrete', 'frechet', 'distance', 'we', 'show', 'that', 'the', 'voronoi', 'diagram', 'of', 'n', 'curves', 'in', 'rd', 'with', 'k', 'vertices', 'each', 'has', '... | [-0.14058520363340543, 0.12482798166659682, -0.11100791728253974, 0.058782549951290494, -0.039396967056618874, -0.15257251041746417, 0.11998642573869506, 0.378819789737463, -0.2373812043562878, -0.2314420337247294, 0.0356640417621536, -0.2807722692919332, -0.1519039042434807, 0.1934885192925237, -0.12134967415138732, 0... |
708.191 | Correlated behavior of conductance and phase rigidity in the transition
from the weak-coupling to the strong-coupling regime | We study the transmission through different small systems as a function of
the coupling strength $v$ to the two attached leads. The leads are identical
with only one propagating mode $\xi^E_C$ in each of them. Besides the
conductance $G$, we calculate the phase rigidity $\rho$ of the scattering wave
function $\Psi^E_... | cond-mat.other quant-ph | we study the transmission through different small systems as a function of the coupling strength v to the two attached leads the leads are identical with only one propagating mode xie_c in each of them besides the conductance g we calculate the phase rigidity rho of the scattering wave function psie_c in the interior o... | [['we', 'study', 'the', 'transmission', 'through', 'different', 'small', 'systems', 'as', 'a', 'function', 'of', 'the', 'coupling', 'strength', 'v', 'to', 'the', 'two', 'attached', 'leads', 'the', 'leads', 'are', 'identical', 'with', 'only', 'one', 'propagating', 'mode', 'xie_c', 'in', 'each', 'of', 'them', 'besides', ... | [-0.21554374638036256, 0.21721868961292312, -0.0620280013162249, 0.02227267832995864, -0.007543024800081805, -0.15427475902479051, 0.03476378537394576, 0.33359840527419155, -0.2769678898398931, -0.26695640014136224, 0.04679764556789362, -0.3077812093703788, -0.10209921169912488, 0.14647851810162146, 0.04714640420558673... |
708.1911 | Moduli Vacuum Bubbles Produced by Evaporating Black Holes | We consider a model with a toroidally compactified extra dimension giving
rise to a temperature-dependent 4d effective potential with one-loop
contributions due to the Casimir effect, along with a 5d cosmological constant.
The forms of the effective potential at low and high temperatures indicates a
possibility for t... | hep-th gr-qc hep-ph | we consider a model with a toroidally compactified extra dimension giving rise to a temperaturedependent 4d effective potential with oneloop contributions due to the casimir effect along with a 5d cosmological constant the forms of the effective potential at low and high temperatures indicates a possibility for the for... | [['we', 'consider', 'a', 'model', 'with', 'a', 'toroidally', 'compactified', 'extra', 'dimension', 'giving', 'rise', 'to', 'a', 'temperaturedependent', '4d', 'effective', 'potential', 'with', 'oneloop', 'contributions', 'due', 'to', 'the', 'casimir', 'effect', 'along', 'with', 'a', '5d', 'cosmological', 'constant', 'th... | [-0.11195164795847978, 0.1765985423875472, -0.06881151480627233, 0.07500191714366052, -0.06679625350469892, -0.14524306619656835, 0.04853386235319906, 0.2919723489018076, -0.1539162891058719, -0.3337049211154957, 0.051312706723431314, -0.3054926083423197, -0.061084190104606646, 0.17402061500928503, -0.06087662687340688... |
708.1912 | Distinguishing the Littlest Higgs model with T-parity from supersymmetry
at the LHC using trileptons | We analyse hadronically quiet trilepton signatures in the T-parity conserving
Littlest Higgs model and in R-parity conserving supersymmetry at the Large
Hadron Collider. We identify the regions of the parameter space where such
signals can reveal the presence of these new physics models above the Standard
Model backg... | hep-ph | we analyse hadronically quiet trilepton signatures in the tparity conserving littlest higgs model and in rparity conserving supersymmetry at the large hadron collider we identify the regions of the parameter space where such signals can reveal the presence of these new physics models above the standard model background... | [['we', 'analyse', 'hadronically', 'quiet', 'trilepton', 'signatures', 'in', 'the', 'tparity', 'conserving', 'littlest', 'higgs', 'model', 'and', 'in', 'rparity', 'conserving', 'supersymmetry', 'at', 'the', 'large', 'hadron', 'collider', 'we', 'identify', 'the', 'regions', 'of', 'the', 'parameter', 'space', 'where', 's... | [-0.07228539965417184, 0.22789768014155642, -0.013335234059256986, 0.2364088416256955, -0.09111584686923405, -0.2421426544634914, -0.016571455205438995, 0.28368097520105434, -0.23882022214882095, -0.31617726842072646, 0.021028937016036624, -0.3120517782657079, -0.038138544895279576, 0.08614748517956428, 0.0226250991395... |
708.1913 | Uniformly root-$N$ consistent density estimators for weakly dependent
invertible linear processes | Convergence rates of kernel density estimators for stationary time series are
well studied. For invertible linear processes, we construct a new density
estimator that converges, in the supremum norm, at the better, parametric, rate
$n^{-1/2}$. Our estimator is a convolution of two different residual-based
kernel esti... | math.ST stat.TH | convergence rates of kernel density estimators for stationary time series are well studied for invertible linear processes we construct a new density estimator that converges in the supremum norm at the better parametric rate n12 our estimator is a convolution of two different residualbased kernel estimators we obtain ... | [['convergence', 'rates', 'of', 'kernel', 'density', 'estimators', 'for', 'stationary', 'time', 'series', 'are', 'well', 'studied', 'for', 'invertible', 'linear', 'processes', 'we', 'construct', 'a', 'new', 'density', 'estimator', 'that', 'converges', 'in', 'the', 'supremum', 'norm', 'at', 'the', 'better', 'parametric'... | [-0.04479194782851707, 0.017817540205128136, -0.10570881333588326, 0.1516232126676995, 0.01769304254816638, -0.13987555413965194, 0.0051277616940852665, 0.4480859984954198, -0.2669976017482224, -0.15012226159137393, 0.17802048038085183, -0.26935083351083217, -0.1187769150331853, 0.23589275936995233, -0.0834259633196606... |
708.1914 | Global versus Local Aspects of Critical Collapse | This thesis deals with critical collapse of a massless scalar field coupled
to Einstein's equations in spherical symmetry. The system is numerically
investigated from both global and local points of view using a characteristic
slicing and radial compactification. We find that the critical exponent that
characterizes ... | gr-qc | this thesis deals with critical collapse of a massless scalar field coupled to einsteins equations in spherical symmetry the system is numerically investigated from both global and local points of view using a characteristic slicing and radial compactification we find that the critical exponent that characterizes the d... | [['this', 'thesis', 'deals', 'with', 'critical', 'collapse', 'of', 'a', 'massless', 'scalar', 'field', 'coupled', 'to', 'einsteins', 'equations', 'in', 'spherical', 'symmetry', 'the', 'system', 'is', 'numerically', 'investigated', 'from', 'both', 'global', 'and', 'local', 'points', 'of', 'view', 'using', 'a', 'characte... | [-0.1438698345872084, 0.10689743296555292, -0.13772952832166374, 0.11341499346974498, -0.060404285165954134, -0.12942867697763843, -0.011958211805004166, 0.3402683117610556, -0.18034219434580853, -0.2175619589757731, 0.0771299339872881, -0.29560524940529126, -0.13912467417047963, 0.1841465739752934, 0.00723678817970740... |
708.1915 | Consistently Solving the Simplicity Constraints for Spinfoam Quantum
Gravity | We give an independent derivation of the Engle-Pereira-Rovelli spinfoam model
for quantum gravity which recently appeared in [arXiv:0705.2388]. Using the
coherent state techniques introduced earlier in [arXiv:0705.0674], we show that
the EPR model realizes a consistent imposition of the simplicity constraints
impleme... | gr-qc hep-th | we give an independent derivation of the englepereirarovelli spinfoam model for quantum gravity which recently appeared in arxiv07052388 using the coherent state techniques introduced earlier in arxiv07050674 we show that the epr model realizes a consistent imposition of the simplicity constraints implementing general ... | [['we', 'give', 'an', 'independent', 'derivation', 'of', 'the', 'englepereirarovelli', 'spinfoam', 'model', 'for', 'quantum', 'gravity', 'which', 'recently', 'appeared', 'in', 'arxiv07052388', 'using', 'the', 'coherent', 'state', 'techniques', 'introduced', 'earlier', 'in', 'arxiv07050674', 'we', 'show', 'that', 'the',... | [-0.12664850475266576, 0.10654649861990424, -0.143886790194727, 0.05059027743149311, -0.08196414517674674, -0.1682644491777458, 0.010208016826196554, 0.27723623573423384, -0.18954960782913136, -0.24784009071423652, 0.014369364149194765, -0.19339949455350003, -0.18908679662668643, 0.18824792801937523, -0.098017162673096... |
708.1916 | Non-Minimal Inflation on the Warped DGP Brane | We construct an inflation model with inflaton non-minimally coupled to
gravity on a warped DGP brane. Using an exponential potential, we calculate
scalar power spectrum, spectral index and the running of the spectral index. We
show that for a suitable range of non-minimal coupling it is possible to exit
the inflation... | hep-th | we construct an inflation model with inflaton nonminimally coupled to gravity on a warped dgp brane using an exponential potential we calculate scalar power spectrum spectral index and the running of the spectral index we show that for a suitable range of nonminimal coupling it is possible to exit the inflationary phas... | [['we', 'construct', 'an', 'inflation', 'model', 'with', 'inflaton', 'nonminimally', 'coupled', 'to', 'gravity', 'on', 'a', 'warped', 'dgp', 'brane', 'using', 'an', 'exponential', 'potential', 'we', 'calculate', 'scalar', 'power', 'spectrum', 'spectral', 'index', 'and', 'the', 'running', 'of', 'the', 'spectral', 'index... | [-0.16875501835866916, 0.161199761038998, -0.09482015885243361, 0.09853750580143904, -0.1548132930924608, -0.19403866194294428, -0.016147190223405647, 0.3408470343935981, -0.20880604816854678, -0.30253678502049297, 0.0936380788017149, -0.22019416484346782, -0.13590501113371414, 0.14084358369952746, -0.02719578455964272... |
708.1917 | The Early Years of String Theory: A Personal Perspective | This article surveys some of the highlights in the development of string
theory through the first superstring revolution in 1984. The emphasis is on
topics in which the author was involved, especially the observation that
critical string theories provide consistent quantum theories of gravity and the
proposal to use ... | hep-th hep-ph | this article surveys some of the highlights in the development of string theory through the first superstring revolution in 1984 the emphasis is on topics in which the author was involved especially the observation that critical string theories provide consistent quantum theories of gravity and the proposal to use stri... | [['this', 'article', 'surveys', 'some', 'of', 'the', 'highlights', 'in', 'the', 'development', 'of', 'string', 'theory', 'through', 'the', 'first', 'superstring', 'revolution', 'in', '1984', 'the', 'emphasis', 'is', 'on', 'topics', 'in', 'which', 'the', 'author', 'was', 'involved', 'especially', 'the', 'observation', '... | [-0.1327627063954189, 0.15750760102884903, -0.1154354183010817, 0.10271072121817738, -0.08184393248595898, -0.10878404888564781, 0.019249110957682735, 0.25577095586566195, -0.18302865125118725, -0.2839235602427394, 0.08011651007766504, -0.2638437342379362, -0.20270073627151788, 0.18649105622523254, -0.08981679802039458... |
708.1918 | Quantum state tomography using a single apparatus | The density matrix of a two-level system (spin, atom) is usually determined
by measuring the three non-commuting components of the Pauli vector. This
density matrix can also be obtained via the measurement data of two commuting
variables, using a single apparatus. This is done by coupling the two-level
system to a mo... | quant-ph cond-mat.stat-mech | the density matrix of a twolevel system spin atom is usually determined by measuring the three noncommuting components of the pauli vector this density matrix can also be obtained via the measurement data of two commuting variables using a single apparatus this is done by coupling the twolevel system to a mode of radia... | [['the', 'density', 'matrix', 'of', 'a', 'twolevel', 'system', 'spin', 'atom', 'is', 'usually', 'determined', 'by', 'measuring', 'the', 'three', 'noncommuting', 'components', 'of', 'the', 'pauli', 'vector', 'this', 'density', 'matrix', 'can', 'also', 'be', 'obtained', 'via', 'the', 'measurement', 'data', 'of', 'two', '... | [-0.16599060001626478, 0.22045010703706505, -0.04475908607771966, 0.006786993742854524, 0.002783784548034974, -0.13503668144081546, 0.036385754865091456, 0.32331534066295203, -0.2755791911014677, -0.2842148053501032, 0.05547838293395079, -0.2748901927019511, -0.06421756578312643, 0.1587515569609318, 0.02663276642478541... |
708.1919 | Metrics for sparse graphs | Recently, Bollob\'as, Janson and Riordan introduced a very general family of
random graph models, producing inhomogeneous random graphs with $\Theta(n)$
edges. Roughly speaking, there is one model for each {\em kernel}, i.e., each
symmetric measurable function from $[0,1]^2$ to the non-negative reals,
although the de... | math.CO math.PR | recently bollobas janson and riordan introduced a very general family of random graph models producing inhomogeneous random graphs with thetan edges roughly speaking there is one model for each em kernel ie each symmetric measurable function from 012 to the nonnegative reals although the details are much more complicat... | [['recently', 'bollobas', 'janson', 'and', 'riordan', 'introduced', 'a', 'very', 'general', 'family', 'of', 'random', 'graph', 'models', 'producing', 'inhomogeneous', 'random', 'graphs', 'with', 'thetan', 'edges', 'roughly', 'speaking', 'there', 'is', 'one', 'model', 'for', 'each', 'em', 'kernel', 'ie', 'each', 'symmet... | [-0.1290525115792718, 0.12015497396617357, -0.0415523187035606, 0.09222982858517463, -0.105394650659193, -0.14478627271714004, 0.029342845125352426, 0.41059454288606567, -0.2620075411498444, -0.3095845457538707, 0.11675877645466777, -0.3067678217972277, -0.2005494857563436, 0.14612015414447438, -0.1319475913477461, 0.0... |
708.192 | Ultralong-range radiative excitation transfer between quantum dots in a
planar microcavity | We study the system of two quantum dots lying on the central plane of a
planar semiconductor microcavity. By solving the full Maxwell problem, we
demonstrate that the rate of resonant excitation transfer between the two dots
decays as $d^{-1/2}$ as a function of the distance $d$ at long distance. This
very long-range... | cond-mat.mes-hall cond-mat.other | we study the system of two quantum dots lying on the central plane of a planar semiconductor microcavity by solving the full maxwell problem we demonstrate that the rate of resonant excitation transfer between the two dots decays as d12 as a function of the distance d at long distance this very longrange mechanism is d... | [['we', 'study', 'the', 'system', 'of', 'two', 'quantum', 'dots', 'lying', 'on', 'the', 'central', 'plane', 'of', 'a', 'planar', 'semiconductor', 'microcavity', 'by', 'solving', 'the', 'full', 'maxwell', 'problem', 'we', 'demonstrate', 'that', 'the', 'rate', 'of', 'resonant', 'excitation', 'transfer', 'between', 'the',... | [-0.1772656655094276, 0.16605419259932305, -0.01900521960730354, 0.06799236811930313, 0.013943869268728627, -0.17159411939274932, 0.014122317331687858, 0.3804354263986978, -0.2947365041925675, -0.2851923680760794, -0.006914146673969097, -0.2930072143053015, -0.13119308587370648, 0.1830164449911687, 0.08103122389357952,... |
708.1921 | Cartesian Bicategories II | The notion of cartesian bicategory, introduced by Carboni and Walters for
locally ordered bicategories, is extended to general bicategories. It is shown
that a cartesian bicategory is a symmetric monoidal bicategory.
| math.CT | the notion of cartesian bicategory introduced by carboni and walters for locally ordered bicategories is extended to general bicategories it is shown that a cartesian bicategory is a symmetric monoidal bicategory | [['the', 'notion', 'of', 'cartesian', 'bicategory', 'introduced', 'by', 'carboni', 'and', 'walters', 'for', 'locally', 'ordered', 'bicategories', 'is', 'extended', 'to', 'general', 'bicategories', 'it', 'is', 'shown', 'that', 'a', 'cartesian', 'bicategory', 'is', 'a', 'symmetric', 'monoidal', 'bicategory']] | [-0.1343300368358952, 0.13014688595168053, -0.014128406081468828, 0.20044593446542538, -0.15822940836510352, -0.134344132346732, -0.07487817463134566, 0.4495765376956232, -0.3862644143162235, -0.10046109109516105, -0.027570814495125124, -0.08197920469026412, -0.0934467089752997, 0.050320624103469234, -0.341202622700122... |
708.1922 | Cross Curvature Flow on Locally Homogenous Three-manifolds (I) | Chow and Hamilton introduced the cross curvature flow on closed 3-manifolds
with negative or positive sectional curvature. In this paper, we study the
negative cross curvature flow in the case of locally homogenous metrics on
3-manifolds. In each case, we describe the long time behavior of the solutions
of the corres... | math.DG | chow and hamilton introduced the cross curvature flow on closed 3manifolds with negative or positive sectional curvature in this paper we study the negative cross curvature flow in the case of locally homogenous metrics on 3manifolds in each case we describe the long time behavior of the solutions of the corresponding ... | [['chow', 'and', 'hamilton', 'introduced', 'the', 'cross', 'curvature', 'flow', 'on', 'closed', '3manifolds', 'with', 'negative', 'or', 'positive', 'sectional', 'curvature', 'in', 'this', 'paper', 'we', 'study', 'the', 'negative', 'cross', 'curvature', 'flow', 'in', 'the', 'case', 'of', 'locally', 'homogenous', 'metric... | [-0.24113323349716528, 0.06291011023941397, -0.06465134579899176, 0.06086631494196448, -0.052971692149580085, -0.13682046776883444, -0.08995996613960432, 0.34228110450478094, -0.2365583375300597, -0.2124715472729701, 0.08871605402113483, -0.3340030972195684, -0.17216665650067745, 0.1420612850375825, -0.1135346568628864... |
708.1923 | Some graph properties determined by edge zeta functions | Stark and Terras introduced the edge zeta function of a finite graph in 1996.
The edge zeta function is the reciprocal of a polynomial in twice as many
variables as edges in the graph and can be computed in polynomial time. We look
at graph properties which we can determine using the edge zeta function. In
particular... | math.CO math.NT | stark and terras introduced the edge zeta function of a finite graph in 1996 the edge zeta function is the reciprocal of a polynomial in twice as many variables as edges in the graph and can be computed in polynomial time we look at graph properties which we can determine using the edge zeta function in particular the ... | [['stark', 'and', 'terras', 'introduced', 'the', 'edge', 'zeta', 'function', 'of', 'a', 'finite', 'graph', 'in', '1996', 'the', 'edge', 'zeta', 'function', 'is', 'the', 'reciprocal', 'of', 'a', 'polynomial', 'in', 'twice', 'as', 'many', 'variables', 'as', 'edges', 'in', 'the', 'graph', 'and', 'can', 'be', 'computed', '... | [-0.20677740832369002, 0.10355343744004988, -0.1440409264342754, 0.07728742323003111, -0.11473457210583014, -0.1113183402438771, 0.061127289385042805, 0.3686904227888247, -0.3274941402048154, -0.3034128969016854, 0.08693771384423599, -0.2314169818781457, -0.20326475149354423, 0.13086599068779867, -0.05635825105512269, ... |
708.1924 | The Absolute, Relative and Multi-Wavelength Calibration of the Pierre
Auger Observatory Fluorescence Detectors | Absolute calibration of the Pierre Auger Observatory fluorescence detectors
uses a 375 nm light source at the telescope aperture. This end-to-end technique
accounts for the combined effects of all detector components in a single
measurement. The relative response has been measured at wavelengths of 320,
337, 355, 380... | astro-ph | absolute calibration of the pierre auger observatory fluorescence detectors uses a 375 nm light source at the telescope aperture this endtoend technique accounts for the combined effects of all detector components in a single measurement the relative response has been measured at wavelengths of 320 337 355 380 and 405 ... | [['absolute', 'calibration', 'of', 'the', 'pierre', 'auger', 'observatory', 'fluorescence', 'detectors', 'uses', 'a', '375', 'nm', 'light', 'source', 'at', 'the', 'telescope', 'aperture', 'this', 'endtoend', 'technique', 'accounts', 'for', 'the', 'combined', 'effects', 'of', 'all', 'detector', 'components', 'in', 'a', ... | [-0.06037568087597973, 0.1199137200688472, -0.10660603411923178, 0.036692564082751816, -0.01905626772719695, -0.11481931226587565, 0.020216668264169367, 0.45401723114926307, -0.1889273855590918, -0.3910562072414905, 0.11699540510517926, -0.3477358242237299, -0.005607670020373141, 0.23946933937831552, -0.057661537042834... |
708.1925 | Frobenius Objects in Cartesian Bicategories | Maps (left adjoint arrows) between Frobenius objects in a cartesian
bicategory B are precisely comonoid homomorphisms and, for A Frobenius and any
T in B, map(B)(T,A) is a groupoid.
| math.CT | maps left adjoint arrows between frobenius objects in a cartesian bicategory b are precisely comonoid homomorphisms and for a frobenius and any t in b mapbta is a groupoid | [['maps', 'left', 'adjoint', 'arrows', 'between', 'frobenius', 'objects', 'in', 'a', 'cartesian', 'bicategory', 'b', 'are', 'precisely', 'comonoid', 'homomorphisms', 'and', 'for', 'a', 'frobenius', 'and', 'any', 't', 'in', 'b', 'mapbta', 'is', 'a', 'groupoid']] | [-0.1776547199946695, 0.1003235714243991, -0.03432617383077741, 0.11435081292958264, -0.11777272853734237, -0.18768173491116613, -0.022033084416761994, 0.41536252573132515, -0.4411571214108595, -0.16731503243292017, 0.02424275182420388, -0.24477244368089096, -0.061008935794234276, 0.09700132434123329, -0.23811638132402... |
708.1926 | Probing non-Riemannian spacetime geometry | The equations of motion for matter in non-Riemannian spacetimes are derived
via a multipole method. It is found that only test bodies with microstructure
couple to the non-Riemannian spacetime geometry. Consequently it is impossible
to detect spacetime torsion with the satellite experiment Gravity Probe B,
contrary t... | gr-qc astro-ph | the equations of motion for matter in nonriemannian spacetimes are derived via a multipole method it is found that only test bodies with microstructure couple to the nonriemannian spacetime geometry consequently it is impossible to detect spacetime torsion with the satellite experiment gravity probe b contrary to some ... | [['the', 'equations', 'of', 'motion', 'for', 'matter', 'in', 'nonriemannian', 'spacetimes', 'are', 'derived', 'via', 'a', 'multipole', 'method', 'it', 'is', 'found', 'that', 'only', 'test', 'bodies', 'with', 'microstructure', 'couple', 'to', 'the', 'nonriemannian', 'spacetime', 'geometry', 'consequently', 'it', 'is', '... | [-0.12828796085921326, 0.10685233075944882, -0.13236810607870794, 0.0725696370190115, -0.1654913999351128, -0.16144235503315083, -0.10019712242350545, 0.33374646618821713, -0.19040073601985877, -0.30864510551657315, 0.06522980461968987, -0.2831225666955535, -0.16146633749441155, 0.18978607815356469, -0.1001878934824523... |
708.1927 | Stochastic bounds for two-layer loss systems | This paper studies multiclass loss systems with two layers of servers, where
each server at the first layer is dedicated to a certain customer class, while
the servers at the second layer can handle all customer classes. The routing of
customers follows an overflow scheme, where arriving customers are
preferentially ... | math.PR | this paper studies multiclass loss systems with two layers of servers where each server at the first layer is dedicated to a certain customer class while the servers at the second layer can handle all customer classes the routing of customers follows an overflow scheme where arriving customers are preferentially direct... | [['this', 'paper', 'studies', 'multiclass', 'loss', 'systems', 'with', 'two', 'layers', 'of', 'servers', 'where', 'each', 'server', 'at', 'the', 'first', 'layer', 'is', 'dedicated', 'to', 'a', 'certain', 'customer', 'class', 'while', 'the', 'servers', 'at', 'the', 'second', 'layer', 'can', 'handle', 'all', 'customer', ... | [-0.177709063932222, 0.09850470981367228, -0.011446286344532078, 0.03215961801470257, -0.07524829431107112, -0.23125206737798484, 0.15926137615800448, 0.36105021291101974, -0.3047105418712211, -0.3163133790658321, 0.10476270994695369, -0.31415775463877554, -0.06702577530328806, 0.16722065335488878, -0.10497958825241464... |
708.1928 | Microtubule dynamics depart from wormlike chain model | Thermal shape fluctuations of grafted microtubules were studied using high
resolution particle tracking of attached fluorescent beads. First mode
relaxation times were extracted from the mean square displacement in the
transverse coordinate. For microtubules shorter than 10 um, the relaxation
times were found to foll... | q-bio.BM | thermal shape fluctuations of grafted microtubules were studied using high resolution particle tracking of attached fluorescent beads first mode relaxation times were extracted from the mean square displacement in the transverse coordinate for microtubules shorter than 10 um the relaxation times were found to follow an... | [['thermal', 'shape', 'fluctuations', 'of', 'grafted', 'microtubules', 'were', 'studied', 'using', 'high', 'resolution', 'particle', 'tracking', 'of', 'attached', 'fluorescent', 'beads', 'first', 'mode', 'relaxation', 'times', 'were', 'extracted', 'from', 'the', 'mean', 'square', 'displacement', 'in', 'the', 'transvers... | [-0.09475070166397172, 0.20918716391988368, -0.09787509179199641, 0.0334470964054454, -0.025453369598835707, -0.1228166785846763, -0.07673979319965923, 0.3879044841764108, -0.29616839408804224, -0.2871215364034727, 0.04125485064369574, -0.2739773421583451, -0.10398442751974007, 0.19021607505625449, -0.00259854431914271... |
708.1929 | Rank-based estimation for all-pass time series models | An autoregressive-moving average model in which all roots of the
autoregressive polynomial are reciprocals of roots of the moving average
polynomial and vice versa is called an all-pass time series model. All-pass
models are useful for identifying and modeling noncausal and noninvertible
autoregressive-moving average... | math.ST stat.TH | an autoregressivemoving average model in which all roots of the autoregressive polynomial are reciprocals of roots of the moving average polynomial and vice versa is called an allpass time series model allpass models are useful for identifying and modeling noncausal and noninvertible autoregressivemoving average proces... | [['an', 'autoregressivemoving', 'average', 'model', 'in', 'which', 'all', 'roots', 'of', 'the', 'autoregressive', 'polynomial', 'are', 'reciprocals', 'of', 'roots', 'of', 'the', 'moving', 'average', 'polynomial', 'and', 'vice', 'versa', 'is', 'called', 'an', 'allpass', 'time', 'series', 'model', 'allpass', 'models', 'a... | [-0.06188456203517878, 0.022022239078069106, -0.10508412839725423, 0.09700156641332035, -0.03458604828701315, -0.18184516100913414, 0.024586286842295677, 0.3904513550014832, -0.23050579679811484, -0.2751362922275041, 0.15589742441203955, -0.27571462276272285, -0.1535544618168193, 0.18462329875860906, -0.095033916604951... |
708.193 | A Two-Parameter Family of Infinite-Dimensional Diffusions in the Kingman
Simplex | The aim of the paper is to introduce a two-parameter family of
infinite-dimensional diffusion processes X(alpha,theta) related to Pitman's
two-parameter Poisson-Dirichlet distributions PD(alpha,theta). The diffusions
X(alpha,theta) are obtained in a scaling limit transition from certain finite
Markov chains on partit... | math.PR | the aim of the paper is to introduce a twoparameter family of infinitedimensional diffusion processes xalphatheta related to pitmans twoparameter poissondirichlet distributions pdalphatheta the diffusions xalphatheta are obtained in a scaling limit transition from certain finite markov chains on partitions of natural n... | [['the', 'aim', 'of', 'the', 'paper', 'is', 'to', 'introduce', 'a', 'twoparameter', 'family', 'of', 'infinitedimensional', 'diffusion', 'processes', 'xalphatheta', 'related', 'to', 'pitmans', 'twoparameter', 'poissondirichlet', 'distributions', 'pdalphatheta', 'the', 'diffusions', 'xalphatheta', 'are', 'obtained', 'in'... | [-0.05371072811069967, 0.14330051579001404, -0.060057955490668384, 0.09655030888830798, -0.04058441646131022, -0.11983218017662761, 0.04934395464960706, 0.3221178797849, -0.298433026289705, -0.192813989986193, 0.0951015552694524, -0.2699917752749924, -0.15511137280347093, 0.19736789685319606, -0.11068523778658122, 0.05... |
708.1931 | Searching for targets on a model DNA: Effects of inter-segment hopping,
detachment and re-attachment | For most of the important processes in DNA metabolism, a protein has to reach
a specific binding site on the DNA. The specific binding site may consist of
just a few base pairs while the DNA is usually several millions of base pairs
long. How does the protein search for the target site? What is the most
efficient mec... | cond-mat.stat-mech q-bio.BM | for most of the important processes in dna metabolism a protein has to reach a specific binding site on the dna the specific binding site may consist of just a few base pairs while the dna is usually several millions of base pairs long how does the protein search for the target site what is the most efficient mechanism... | [['for', 'most', 'of', 'the', 'important', 'processes', 'in', 'dna', 'metabolism', 'a', 'protein', 'has', 'to', 'reach', 'a', 'specific', 'binding', 'site', 'on', 'the', 'dna', 'the', 'specific', 'binding', 'site', 'may', 'consist', 'of', 'just', 'a', 'few', 'base', 'pairs', 'while', 'the', 'dna', 'is', 'usually', 'sev... | [-0.10060515387690273, 0.1342324714168328, -0.018282481514174363, 0.10206379123231053, -0.0434346431065431, -0.16209954409378355, 0.13014962755400558, 0.38565291379546296, -0.2581137907354097, -0.2813278181028777, 0.06660136807356672, -0.2572759532594475, -0.14857640524780186, 0.22483287984906727, 0.011458492966304565,... |
708.1932 | Derivation of the quantum probability law from minimal non-demolition
measurement | One more derivation of the quantum probability rule is presented in order to
shed more light on the versatile aspects of this fundamental law. It is shown
that the change of state in minimal quantum non-demolition measurement, also
known as ideal measurement, implies the probability law in a simple way.
Namely, the v... | quant-ph | one more derivation of the quantum probability rule is presented in order to shed more light on the versatile aspects of this fundamental law it is shown that the change of state in minimal quantum nondemolition measurement also known as ideal measurement implies the probability law in a simple way namely the very requ... | [['one', 'more', 'derivation', 'of', 'the', 'quantum', 'probability', 'rule', 'is', 'presented', 'in', 'order', 'to', 'shed', 'more', 'light', 'on', 'the', 'versatile', 'aspects', 'of', 'this', 'fundamental', 'law', 'it', 'is', 'shown', 'that', 'the', 'change', 'of', 'state', 'in', 'minimal', 'quantum', 'nondemolition'... | [-0.10908929883347203, 0.11776947004332518, -0.14013076168795427, 0.06608414606035998, -0.09295607976615429, -0.19597424424563845, 0.11281344724042962, 0.28349175120393433, -0.24562107625106971, -0.2680971109246214, 0.05004021010672053, -0.22965574386219184, -0.14019601171215376, 0.23205600050588449, -0.101379570352534... |
708.1933 | On the well posedness of Robinson Trautman Maxwell solutions | We show that the so called Robinson-Trautman-Maxwell equations do not
constitute a well posed initial value problem. That is, the dependence of the
solution on the initial data is not continuous in any norm built out from the
initial data and a finite number of its derivatives. Thus, they can not be used
to solve for... | gr-qc | we show that the so called robinsontrautmanmaxwell equations do not constitute a well posed initial value problem that is the dependence of the solution on the initial data is not continuous in any norm built out from the initial data and a finite number of its derivatives thus they can not be used to solve for solutio... | [['we', 'show', 'that', 'the', 'so', 'called', 'robinsontrautmanmaxwell', 'equations', 'do', 'not', 'constitute', 'a', 'well', 'posed', 'initial', 'value', 'problem', 'that', 'is', 'the', 'dependence', 'of', 'the', 'solution', 'on', 'the', 'initial', 'data', 'is', 'not', 'continuous', 'in', 'any', 'norm', 'built', 'out... | [-0.08478739097093542, 0.06112347338348627, -0.13571917724766536, 0.08024991515170161, -0.13337767599150538, -0.07991397108417005, 0.020663826307281852, 0.3518102743973335, -0.2981673607913156, -0.2625548431649804, 0.20874816796858794, -0.25991120062147577, -0.08637534696608781, 0.2170033104737134, -0.06128790891186023... |
708.1934 | A fully solvable equilibrium self-assembly process: fine tuning the
clusters size and the connectivity in patchy particle systems | Self-assembly is the mechanism that controls the formation of well defined
structures from disordered pre-existing parts. Despite the importance of
self-assembly as a manufacturing method and the increasingly large number of
experimental realizations of complex self-assembled nano aggregates,
theoretical predictions ... | cond-mat.soft | selfassembly is the mechanism that controls the formation of well defined structures from disordered preexisting parts despite the importance of selfassembly as a manufacturing method and the increasingly large number of experimental realizations of complex selfassembled nano aggregates theoretical predictions are lagg... | [['selfassembly', 'is', 'the', 'mechanism', 'that', 'controls', 'the', 'formation', 'of', 'well', 'defined', 'structures', 'from', 'disordered', 'preexisting', 'parts', 'despite', 'the', 'importance', 'of', 'selfassembly', 'as', 'a', 'manufacturing', 'method', 'and', 'the', 'increasingly', 'large', 'number', 'of', 'exp... | [-0.08396420530819644, 0.18409599062232745, -0.09009338889847554, 0.029743828464277266, -0.05185580315412067, -0.1230794836578536, 0.037978340505755374, 0.3790738151541778, -0.29930712947610855, -0.3139027955365323, 0.03323805726973833, -0.23677882627539693, -0.25211145864644396, 0.15265959561414397, 0.0107832730559277... |
708.1935 | Testing modified gravity with globular cluster velocity dispersions | Globular clusters (GCs) in the Milky Way have characteristic velocity
dispersions that are consistent with the predictions of Newtonian gravity, and
may be at odds with Modified Newtonian Dynamics (MOND). We discuss a modified
gravity (MOG) theory that successfully predicts galaxy rotation curves, galaxy
cluster mass... | astro-ph gr-qc | globular clusters gcs in the milky way have characteristic velocity dispersions that are consistent with the predictions of newtonian gravity and may be at odds with modified newtonian dynamics mond we discuss a modified gravity mog theory that successfully predicts galaxy rotation curves galaxy cluster masses and velo... | [['globular', 'clusters', 'gcs', 'in', 'the', 'milky', 'way', 'have', 'characteristic', 'velocity', 'dispersions', 'that', 'are', 'consistent', 'with', 'the', 'predictions', 'of', 'newtonian', 'gravity', 'and', 'may', 'be', 'at', 'odds', 'with', 'modified', 'newtonian', 'dynamics', 'mond', 'we', 'discuss', 'a', 'modifi... | [-0.07479396871375767, 0.11748194260184061, -0.2093407479580492, 0.16725967946377668, -0.1602345742010088, -0.14677955253811723, -0.07408631036947058, 0.39238227470354603, -0.17182834775779735, -0.3429383144459941, -0.0687658869925971, -0.2558775789316066, -0.07189610451883213, 0.24432267281226813, -0.04285764220509339... |
708.1936 | Gas phase sorting of nanoparticles | We discuss Stark deflectometry of micro-modulated molecular beams for the
enrichment of biomolecular isomers as well as single-wall carbon nanotubes and
we demonstrate the working principle of this idea with fullerenes. The sorting
is based on the species-dependent polarizability-to-mass ratio $\alpha/m$. The
device ... | quant-ph cond-mat.mtrl-sci physics.atm-clus physics.bio-ph physics.chem-ph | we discuss stark deflectometry of micromodulated molecular beams for the enrichment of biomolecular isomers as well as singlewall carbon nanotubes and we demonstrate the working principle of this idea with fullerenes the sorting is based on the speciesdependent polarizabilitytomass ratio alpham the device is compatible... | [['we', 'discuss', 'stark', 'deflectometry', 'of', 'micromodulated', 'molecular', 'beams', 'for', 'the', 'enrichment', 'of', 'biomolecular', 'isomers', 'as', 'well', 'as', 'singlewall', 'carbon', 'nanotubes', 'and', 'we', 'demonstrate', 'the', 'working', 'principle', 'of', 'this', 'idea', 'with', 'fullerenes', 'the', '... | [-0.09225571244447069, 0.09630081210299536, -0.038382842459461906, 0.014756316454925885, 0.007322066576417648, -0.09963209569369527, 0.07384786308940613, 0.4793747328221798, -0.22559207358977856, -0.34062590994731046, 0.027243974138841484, -0.2029437408817819, -0.07644786727685256, 0.14615801151023444, -0.0485967311330... |
708.1937 | The asymptotic geometry of right-angled Artin groups, I | We study atomic right-angled Artin groups -- those whose defining graph has
no cycles of length less than five, and no separating vertices, separating
edges, or separating vertex stars. We show that these groups are not
quasi-isometrically rigid, but that an intermediate form of rigidity does hold.
We deduce from thi... | math.GR math.MG | we study atomic rightangled artin groups those whose defining graph has no cycles of length less than five and no separating vertices separating edges or separating vertex stars we show that these groups are not quasiisometrically rigid but that an intermediate form of rigidity does hold we deduce from this that two at... | [['we', 'study', 'atomic', 'rightangled', 'artin', 'groups', 'those', 'whose', 'defining', 'graph', 'has', 'no', 'cycles', 'of', 'length', 'less', 'than', 'five', 'and', 'no', 'separating', 'vertices', 'separating', 'edges', 'or', 'separating', 'vertex', 'stars', 'we', 'show', 'that', 'these', 'groups', 'are', 'not', '... | [-0.18187415920741234, 0.21521540743051445, -0.1034162943251431, 0.06199127335081964, -0.10872290357947349, -0.18618949979233246, 0.003881121405477946, 0.48843968100845814, -0.2863802695646882, -0.2351720671635121, 0.07949634139270832, -0.3408199629280716, -0.12061307613815492, 0.16978440259505684, -0.11036313123380144... |
708.1938 | Magnetic flows on Sol-manifolds: dynamical and symplectic aspects | We consider magnetic flows on compact quotients of the 3-dimensional solvable
geometry Sol determined by the usual left-invariant metric and the
distinguished monopole. We show that these flows have positive Liouville
entropy and therefore are never completely integrable. This should be compared
with the known fact t... | math.DS math.SG | we consider magnetic flows on compact quotients of the 3dimensional solvable geometry sol determined by the usual leftinvariant metric and the distinguished monopole we show that these flows have positive liouville entropy and therefore are never completely integrable this should be compared with the known fact that th... | [['we', 'consider', 'magnetic', 'flows', 'on', 'compact', 'quotients', 'of', 'the', '3dimensional', 'solvable', 'geometry', 'sol', 'determined', 'by', 'the', 'usual', 'leftinvariant', 'metric', 'and', 'the', 'distinguished', 'monopole', 'we', 'show', 'that', 'these', 'flows', 'have', 'positive', 'liouville', 'entropy',... | [-0.18992142704815637, 0.1621973529324384, -0.0426751839020002, 0.09284849319302327, -0.1033769113322099, -0.16323323901397763, -0.09031383475083225, 0.3746050230146926, -0.2877892931394371, -0.17284369995288643, 0.13342255357520677, -0.2739872703857628, -0.17932601508764942, 0.20561443886685152, -0.10285174277507597, ... |
708.1939 | Effect of Charged Scalar Loops on Photonic Decays of a Fermiophobic
Higgs | Higgs bosons with very suppressed couplings to fermions ("Fermiophobic Higgs
bosons", h_f) can decay to two photons (\gamma\gamma) with a branching ratio
significantly larger than that expected for the Standard Model Higgs boson for
m_{h_f}<150 GeV. Such a particle would give a clear signal at the LHC and can
arise i... | hep-ph | higgs bosons with very suppressed couplings to fermions fermiophobic higgs bosons h_f can decay to two photons gammagamma with a branching ratio significantly larger than that expected for the standard model higgs boson for m_h_f150 gev such a particle would give a clear signal at the lhc and can arise in the two higgs... | [['higgs', 'bosons', 'with', 'very', 'suppressed', 'couplings', 'to', 'fermions', 'fermiophobic', 'higgs', 'bosons', 'h_f', 'can', 'decay', 'to', 'two', 'photons', 'gammagamma', 'with', 'a', 'branching', 'ratio', 'significantly', 'larger', 'than', 'that', 'expected', 'for', 'the', 'standard', 'model', 'higgs', 'boson',... | [-0.08184034697696235, 0.36525342814084666, -0.003517430789211643, 0.18219984488705365, -0.07080579070792159, -0.2834535740037388, 0.02074618376443319, 0.3329024516986074, -0.20929478403701987, -0.2618347120941312, -0.03547987111117343, -0.3024500237830053, 0.022949161103743815, 0.15367199831411557, 0.09317640201014545... |
708.194 | H\"older forms and integrability of invariant distributions | We prove an inequality for H\"older continuous differential forms on compact
manifolds in which the integral of the form over the boundary of a sufficiently
small, smoothly immersed disk is bounded by a certain multiplicative convex
combination of the volume of the disk and the area of its boundary. This
inequality h... | math.DS math.CA | we prove an inequality for holder continuous differential forms on compact manifolds in which the integral of the form over the boundary of a sufficiently small smoothly immersed disk is bounded by a certain multiplicative convex combination of the volume of the disk and the area of its boundary this inequality has nat... | [['we', 'prove', 'an', 'inequality', 'for', 'holder', 'continuous', 'differential', 'forms', 'on', 'compact', 'manifolds', 'in', 'which', 'the', 'integral', 'of', 'the', 'form', 'over', 'the', 'boundary', 'of', 'a', 'sufficiently', 'small', 'smoothly', 'immersed', 'disk', 'is', 'bounded', 'by', 'a', 'certain', 'multipl... | [-0.18596980288834988, 0.06866906036072393, -0.0833198634446463, 0.06226680198688856, -0.049515954078654355, -0.0819741323628707, -0.018173868691060437, 0.3110562643687268, -0.3080350179044367, -0.19936742031386176, 0.1601606479312465, -0.24949543772138727, -0.12864704505603725, 0.25166215195582764, -0.1187713014694310... |
708.1941 | Predicting Solar Flares by Data Assimilation in Avalanche Models. I.
Model Design and Validation | Data assimilation techniques, developed in the last two decades mainly for
weather prediction, produce better forecasts by taking advantage of both
theoretical/numerical models and real-time observations. In this paper, we
explore the possibility of applying the data-assimilation techniques known as
4D-VAR to the pre... | astro-ph | data assimilation techniques developed in the last two decades mainly for weather prediction produce better forecasts by taking advantage of both theoreticalnumerical models and realtime observations in this paper we explore the possibility of applying the dataassimilation techniques known as 4dvar to the prediction of... | [['data', 'assimilation', 'techniques', 'developed', 'in', 'the', 'last', 'two', 'decades', 'mainly', 'for', 'weather', 'prediction', 'produce', 'better', 'forecasts', 'by', 'taking', 'advantage', 'of', 'both', 'theoreticalnumerical', 'models', 'and', 'realtime', 'observations', 'in', 'this', 'paper', 'we', 'explore', ... | [-0.06033606779307038, 0.11260496408180015, -0.06067540196402531, 0.12319409345772805, -0.03130295213417239, -0.07328690275538802, 0.03271984052497871, 0.3598675134458712, -0.2247633762502422, -0.374031423729667, 0.11472757116661385, -0.23521661915860714, -0.1385579926466432, 0.23372243428422648, -0.06771648666434278, ... |
708.1942 | Circumstellar Magnetic Field Diagnostics from Line Polarization | Given that dynamically significant magnetic fields in at least some massive
stars have now been measured, our contribution addresses the question, to what
extent can fields be directly detected in circumstellar gas? The question
speaks directly to the very interesting topic of line-driving physics coupled
with magnet... | astro-ph | given that dynamically significant magnetic fields in at least some massive stars have now been measured our contribution addresses the question to what extent can fields be directly detected in circumstellar gas the question speaks directly to the very interesting topic of linedriving physics coupled with magnetized p... | [['given', 'that', 'dynamically', 'significant', 'magnetic', 'fields', 'in', 'at', 'least', 'some', 'massive', 'stars', 'have', 'now', 'been', 'measured', 'our', 'contribution', 'addresses', 'the', 'question', 'to', 'what', 'extent', 'can', 'fields', 'be', 'directly', 'detected', 'in', 'circumstellar', 'gas', 'the', 'q... | [-0.10165690398378278, 0.15838311466730523, -0.04138712794519961, 0.09145291766736238, -0.12335633939816332, -0.12077362010521549, -0.011778276166593542, 0.3830526690949135, -0.2848315327855929, -0.31041014900107927, 0.030280676685815335, -0.25256439417182486, -0.07911316378099122, 0.19927660126847271, -0.0163387628509... |
708.1943 | On the Hopf-Schur group of a field | Let k be any field. We consider the Hopf-Schur group of k, defined as the
subgroup of the Brauer group of k consisting of classes that may be represented
by homomorphic images of Hopf algebras over k. We show here that twisted group
algebras and abelian extensions of k are quotients of cocommutative and
commutative H... | math.QA math.RT | let k be any field we consider the hopfschur group of k defined as the subgroup of the brauer group of k consisting of classes that may be represented by homomorphic images of hopf algebras over k we show here that twisted group algebras and abelian extensions of k are quotients of cocommutative and commutative hopf al... | [['let', 'k', 'be', 'any', 'field', 'we', 'consider', 'the', 'hopfschur', 'group', 'of', 'k', 'defined', 'as', 'the', 'subgroup', 'of', 'the', 'brauer', 'group', 'of', 'k', 'consisting', 'of', 'classes', 'that', 'may', 'be', 'represented', 'by', 'homomorphic', 'images', 'of', 'hopf', 'algebras', 'over', 'k', 'we', 'sho... | [-0.2532002353253438, 0.12947137458922015, -0.09550540174175169, -0.03648772598940341, -0.12847662926411507, -0.14481389114018722, -0.007626988320160158, 0.3857324065534955, -0.4046650107220276, -0.20955682981797716, 0.11622693766503758, -0.21121860158236064, -0.11381540870649222, 0.20759925888563246, -0.09131621347605... |
708.1944 | Statics and dynamics of a cylindrical droplet under an external body
force | We study the rolling and sliding motion of droplets on a corrugated substrate
by Molecular Dynamics simulations. Droplets are driven by an external body
force (gravity) and we investigate the velocity profile and dissipation
mechanisms in the steady state. The cylindrical geometry allows us to consider
a large range ... | cond-mat.soft | we study the rolling and sliding motion of droplets on a corrugated substrate by molecular dynamics simulations droplets are driven by an external body force gravity and we investigate the velocity profile and dissipation mechanisms in the steady state the cylindrical geometry allows us to consider a large range of dro... | [['we', 'study', 'the', 'rolling', 'and', 'sliding', 'motion', 'of', 'droplets', 'on', 'a', 'corrugated', 'substrate', 'by', 'molecular', 'dynamics', 'simulations', 'droplets', 'are', 'driven', 'by', 'an', 'external', 'body', 'force', 'gravity', 'and', 'we', 'investigate', 'the', 'velocity', 'profile', 'and', 'dissipat... | [-0.16285222556865858, 0.20578262676189663, -0.09528052213484656, -0.012956912901174433, -0.032019026507762914, -0.09894704064744675, 0.004944482929781525, 0.32982261622781883, -0.2640388696440523, -0.30141634646591225, 0.06354306391607635, -0.25403863904465473, -0.05926025214515805, 0.19547654759183436, -0.01677163611... |
708.1945 | Fossil Groups in the Sloan Digital Sky Survey | A search for fossil groups in the Sloan Digital Sky Survey was performed
using virtual observatory tools. A cross-match of the positions of all SDSS
Luminous Red Galaxies (with r < 19 and measured spectroscopic redshifts) with
sources in the ROSAT All-Sky Survey catalog resulted in a list of elliptical
galaxies with ... | astro-ph | a search for fossil groups in the sloan digital sky survey was performed using virtual observatory tools a crossmatch of the positions of all sdss luminous red galaxies with r 19 and measured spectroscopic redshifts with sources in the rosat allsky survey catalog resulted in a list of elliptical galaxies with extended ... | [['a', 'search', 'for', 'fossil', 'groups', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'was', 'performed', 'using', 'virtual', 'observatory', 'tools', 'a', 'crossmatch', 'of', 'the', 'positions', 'of', 'all', 'sdss', 'luminous', 'red', 'galaxies', 'with', 'r', '19', 'and', 'measured', 'spectroscopic', 'redshifts... | [-0.06678370401395235, 0.06840339709645299, -0.05000153082371579, 0.07585566017435731, -0.08908536856055377, -0.0050254910340987325, 0.1149656742840536, 0.4268994348226335, -0.06540704367125011, -0.40987984545704886, 0.07549647774866335, -0.4016980157989099, 0.05304868353208102, 0.22287673835789187, 0.00489943374065667... |
708.1946 | Vector and Axial Nucleon Form Factors:A Duality Constrained
Parameterization | We present new parameterizations of vector and axial nucleon form factors. We
maintain an excellent descriptions of the form factors at low momentum
transfers, where the spatial structure of the nucleon is important, and use the
Nachtman scaling variable xi to relate elastic and inelastic form factors and
impose quar... | hep-ex nucl-ex | we present new parameterizations of vector and axial nucleon form factors we maintain an excellent descriptions of the form factors at low momentum transfers where the spatial structure of the nucleon is important and use the nachtman scaling variable xi to relate elastic and inelastic form factors and impose quarkhadr... | [['we', 'present', 'new', 'parameterizations', 'of', 'vector', 'and', 'axial', 'nucleon', 'form', 'factors', 'we', 'maintain', 'an', 'excellent', 'descriptions', 'of', 'the', 'form', 'factors', 'at', 'low', 'momentum', 'transfers', 'where', 'the', 'spatial', 'structure', 'of', 'the', 'nucleon', 'is', 'important', 'and'... | [-0.08952010268191422, 0.23915317014084703, -0.048678632572212756, 0.14307609770912677, -0.07889282754867484, -0.054157658896752094, 0.0708101927390308, 0.364282952733618, -0.20900541729174724, -0.278331332833023, -0.012636908568105752, -0.3070218889392856, -0.03157404621124716, 0.15838934316236833, 0.10062087073754099... |
708.1947 | Vitaly Ginzburg and High Temperature Superconductivity: Personal
Reminiscences | I offer some personal reminiscences from the period of 1976-1983, when I was
a M. Sc. and then a Ph.D. student in Vitaly L. Ginzburg's High Temperature
Superconductivity group at the P.N. Lebedev Institute in Moscow
| cond-mat.supr-con | i offer some personal reminiscences from the period of 19761983 when i was a m sc and then a phd student in vitaly l ginzburgs high temperature superconductivity group at the pn lebedev institute in moscow | [['i', 'offer', 'some', 'personal', 'reminiscences', 'from', 'the', 'period', 'of', '19761983', 'when', 'i', 'was', 'a', 'm', 'sc', 'and', 'then', 'a', 'phd', 'student', 'in', 'vitaly', 'l', 'ginzburgs', 'high', 'temperature', 'superconductivity', 'group', 'at', 'the', 'pn', 'lebedev', 'institute', 'in', 'moscow']] | [-0.09265324845910072, 0.13632726557552816, -0.14081795892811247, 0.011058657190629415, -0.10473972566957984, -0.21911652769361223, 0.08533321171998978, 0.28790942441139905, -0.17930750814599117, -0.30118111965379546, 0.0715941082885755, -0.3259295312421662, -0.10112504655761378, 0.14345164697484247, -0.131223461457661... |
708.1948 | Chaoticity Parameter Lambda in Hanbury-Brown Twiss Interferometry | In Hanbury-Brown-Twiss interferometry measurements using identical bosons,
the chaoticity parameter lambda has been introduced phenomenologically to
represent the momentum correlation function at zero relative momentum. It is
useful to study an exactly solvable problem in which the lambda parameter and
its dependence... | hep-ph nucl-th quant-ph | in hanburybrowntwiss interferometry measurements using identical bosons the chaoticity parameter lambda has been introduced phenomenologically to represent the momentum correlation function at zero relative momentum it is useful to study an exactly solvable problem in which the lambda parameter and its dependence on th... | [['in', 'hanburybrowntwiss', 'interferometry', 'measurements', 'using', 'identical', 'bosons', 'the', 'chaoticity', 'parameter', 'lambda', 'has', 'been', 'introduced', 'phenomenologically', 'to', 'represent', 'the', 'momentum', 'correlation', 'function', 'at', 'zero', 'relative', 'momentum', 'it', 'is', 'useful', 'to',... | [-0.14517933961543988, 0.21551800777156035, -0.11698965771480443, 0.07874841684416095, -0.010888804853002124, -0.11491655828431249, 0.03028091231380847, 0.3445816047806689, -0.23815392903151347, -0.25687620548055845, 0.022912683385979148, -0.297608092760152, -0.03273226659883686, 0.15412409943924782, 0.0401650426503112... |
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