id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.3635 | High redshift FRII radio sources: large-scale X-ray environment | We investigate the properties of the environment around 20 powerful radio
galaxies and quasars at redshifts between 0.45 and 1. Using XMM-Newton and
Chandra observations we probe the spatial distribution and the temperature of
the cluster gas. We find that more than 60 per cent of powerful radio sources
in the redshi... | astro-ph | we investigate the properties of the environment around 20 powerful radio galaxies and quasars at redshifts between 045 and 1 using xmmnewton and chandra observations we probe the spatial distribution and the temperature of the cluster gas we find that more than 60 per cent of powerful radio sources in the redshift ran... | [['we', 'investigate', 'the', 'properties', 'of', 'the', 'environment', 'around', '20', 'powerful', 'radio', 'galaxies', 'and', 'quasars', 'at', 'redshifts', 'between', '045', 'and', '1', 'using', 'xmmnewton', 'and', 'chandra', 'observations', 'we', 'probe', 'the', 'spatial', 'distribution', 'and', 'the', 'temperature'... | [-0.060240141554943304, 0.08366075349204692, -0.06692974238066847, 0.12171892678070305, -0.08686564086681808, -0.04657750559984137, 0.0650651510779766, 0.46456350760011794, -0.14064798679867785, -0.34293417744472515, 0.047314603314668, -0.2987862667554601, -0.01444462345068832, 0.22880949169102546, 0.027924172425300903... |
709.3636 | Detecting Neutrino Magnetic Moments with Conducting Loops | It is well established that neutrinos have mass, yet it is very difficult to
measure those masses directly. Within the standard model of particle physics,
neutrinos will have an intrinsic magnetic moment proportional to their mass. We
examine the possibility of detecting the magnetic moment using a conducting
loop. A... | hep-ex | it is well established that neutrinos have mass yet it is very difficult to measure those masses directly within the standard model of particle physics neutrinos will have an intrinsic magnetic moment proportional to their mass we examine the possibility of detecting the magnetic moment using a conducting loop accordin... | [['it', 'is', 'well', 'established', 'that', 'neutrinos', 'have', 'mass', 'yet', 'it', 'is', 'very', 'difficult', 'to', 'measure', 'those', 'masses', 'directly', 'within', 'the', 'standard', 'model', 'of', 'particle', 'physics', 'neutrinos', 'will', 'have', 'an', 'intrinsic', 'magnetic', 'moment', 'proportional', 'to',... | [-0.12232096838504747, 0.18463083811608763, -0.05857564131351742, 0.14684512725137677, -0.10603293820980701, -0.08314525176192054, 0.02778779572769496, 0.36924842234935845, -0.2610815724752306, -0.35595190712997504, 0.03553306633765969, -0.2464034660627042, -0.09397173230955796, 0.2112734869787436, 0.007308481695331834... |
709.3637 | \Lambda_{c} enhancement from strongly coupled quark-gluon plasma | We propose the enhancement of $\Lambda_{c}$ as a novel QGP signal in heavy
ion collisions at RHIC and LHC. Assuming a stable bound diquark state in the
strongly coupled QGP near the critical temperature, we argue that the direct
two-body collision between a $c$ quark and a $[ud]$ diquark would lead to an
enhanced $\L... | nucl-th | we propose the enhancement of lambda_c as a novel qgp signal in heavy ion collisions at rhic and lhc assuming a stable bound diquark state in the strongly coupled qgp near the critical temperature we argue that the direct twobody collision between a c quark and a ud diquark would lead to an enhanced lambda_c production... | [['we', 'propose', 'the', 'enhancement', 'of', 'lambda_c', 'as', 'a', 'novel', 'qgp', 'signal', 'in', 'heavy', 'ion', 'collisions', 'at', 'rhic', 'and', 'lhc', 'assuming', 'a', 'stable', 'bound', 'diquark', 'state', 'in', 'the', 'strongly', 'coupled', 'qgp', 'near', 'the', 'critical', 'temperature', 'we', 'argue', 'tha... | [-0.10434572733258514, 0.276819753896326, -0.1344439879248149, 0.09331666786626526, 0.017264438269848234, -0.16071971930730877, 0.05758320710234595, 0.32163558057980257, -0.21296660271420909, -0.20679533666815986, -0.09209806765063425, -0.33165027182863166, 0.013066426971194785, 0.05928929901179554, 0.09538935566467516... |
709.3638 | Dynamical Casimir Effect and the Black Body Spectrum | Creation of scalar massless particles in two-dimensional Minkowski
space-time--as predicted by the dynamical Casimir effect--is studied for the
case of a semitransparent mirror initially at rest, then accelerating for some
finite time, along a specified trajectory, and finally moving with constant
velocity. When the ... | quant-ph gr-qc hep-th math-ph math.MP | creation of scalar massless particles in twodimensional minkowski spacetimeas predicted by the dynamical casimir effectis studied for the case of a semitransparent mirror initially at rest then accelerating for some finite time along a specified trajectory and finally moving with constant velocity when the reflection a... | [['creation', 'of', 'scalar', 'massless', 'particles', 'in', 'twodimensional', 'minkowski', 'spacetimeas', 'predicted', 'by', 'the', 'dynamical', 'casimir', 'effectis', 'studied', 'for', 'the', 'case', 'of', 'a', 'semitransparent', 'mirror', 'initially', 'at', 'rest', 'then', 'accelerating', 'for', 'some', 'finite', 't... | [-0.1056854017502205, 0.22542904114871143, -0.08956501757810739, 0.040970284082811906, -0.05623886671352696, -0.19328004662506887, -0.0303326472271515, 0.33159648381512274, -0.20933312682023683, -0.2656726250969261, 0.0313252599126744, -0.30524570108007704, -0.08566623062270319, 0.19545067819258707, -0.0307195401318105... |
709.3639 | Fast Selection of Spectral Variables with B-Spline Compression | The large number of spectral variables in most data sets encountered in
spectral chemometrics often renders the prediction of a dependent variable
uneasy. The number of variables hopefully can be reduced, by using either
projection techniques or selection methods; the latter allow for the
interpretation of the select... | cs.LG stat.AP | the large number of spectral variables in most data sets encountered in spectral chemometrics often renders the prediction of a dependent variable uneasy the number of variables hopefully can be reduced by using either projection techniques or selection methods the latter allow for the interpretation of the selected va... | [['the', 'large', 'number', 'of', 'spectral', 'variables', 'in', 'most', 'data', 'sets', 'encountered', 'in', 'spectral', 'chemometrics', 'often', 'renders', 'the', 'prediction', 'of', 'a', 'dependent', 'variable', 'uneasy', 'the', 'number', 'of', 'variables', 'hopefully', 'can', 'be', 'reduced', 'by', 'using', 'either... | [-0.060657077544737, 0.03833923167635934, -0.12491251071536004, 0.0881379653163644, -0.09599818370409685, -0.131259084879529, 0.08484561588974351, 0.38188260813900665, -0.2678751193421041, -0.33252387636976477, 0.12057432726336022, -0.24439695792799715, -0.10934121341736944, 0.22524966242228628, -0.08927453966999008, 0... |
709.364 | Resampling methods for parameter-free and robust feature selection with
mutual information | Combining the mutual information criterion with a forward feature selection
strategy offers a good trade-off between optimality of the selected feature
subset and computation time. However, it requires to set the parameter(s) of
the mutual information estimator and to determine when to halt the forward
procedure. The... | cs.LG stat.AP | combining the mutual information criterion with a forward feature selection strategy offers a good tradeoff between optimality of the selected feature subset and computation time however it requires to set the parameters of the mutual information estimator and to determine when to halt the forward procedure these two c... | [['combining', 'the', 'mutual', 'information', 'criterion', 'with', 'a', 'forward', 'feature', 'selection', 'strategy', 'offers', 'a', 'good', 'tradeoff', 'between', 'optimality', 'of', 'the', 'selected', 'feature', 'subset', 'and', 'computation', 'time', 'however', 'it', 'requires', 'to', 'set', 'the', 'parameters', '... | [-0.0447930308908005, 0.0071644460652297475, -0.10428431420587003, 0.11667182793933213, -0.12898613988449248, -0.17821207923663998, 0.13210724730400697, 0.38741800315020714, -0.30008221263586377, -0.35270293083671916, 0.15297076571047963, -0.2678395703174722, -0.12466247644795872, 0.19848314963746816, -0.11124564398072... |
709.3641 | Representation of Functional Data in Neural Networks | Functional Data Analysis (FDA) is an extension of traditional data analysis
to functional data, for example spectra, temporal series, spatio-temporal
images, gesture recognition data, etc. Functional data are rarely known in
practice; usually a regular or irregular sampling is known. For this reason,
some processing ... | cs.NE | functional data analysis fda is an extension of traditional data analysis to functional data for example spectra temporal series spatiotemporal images gesture recognition data etc functional data are rarely known in practice usually a regular or irregular sampling is known for this reason some processing is needed in o... | [['functional', 'data', 'analysis', 'fda', 'is', 'an', 'extension', 'of', 'traditional', 'data', 'analysis', 'to', 'functional', 'data', 'for', 'example', 'spectra', 'temporal', 'series', 'spatiotemporal', 'images', 'gesture', 'recognition', 'data', 'etc', 'functional', 'data', 'are', 'rarely', 'known', 'in', 'practice... | [-0.05694508834071835, -0.04485554303539322, -0.11551484044458768, 0.13030241724226396, -0.09204901529104777, -0.12002811874137134, 0.013022934446092444, 0.39225885327402, -0.3029585958468709, -0.3152382273126293, 0.13607581104844105, -0.326375240283842, -0.22203959516608282, 0.21469908463296708, -0.07454685389057959, ... |
709.3642 | Functional Multi-Layer Perceptron: a Nonlinear Tool for Functional Data
Analysis | In this paper, we study a natural extension of Multi-Layer Perceptrons (MLP)
to functional inputs. We show that fundamental results for classical MLP can be
extended to functional MLP. We obtain universal approximation results that show
the expressive power of functional MLP is comparable to that of numerical MLP.
We... | cs.NE | in this paper we study a natural extension of multilayer perceptrons mlp to functional inputs we show that fundamental results for classical mlp can be extended to functional mlp we obtain universal approximation results that show the expressive power of functional mlp is comparable to that of numerical mlp we obtain c... | [['in', 'this', 'paper', 'we', 'study', 'a', 'natural', 'extension', 'of', 'multilayer', 'perceptrons', 'mlp', 'to', 'functional', 'inputs', 'we', 'show', 'that', 'fundamental', 'results', 'for', 'classical', 'mlp', 'can', 'be', 'extended', 'to', 'functional', 'mlp', 'we', 'obtain', 'universal', 'approximation', 'resul... | [-0.02893182384813654, -0.030669476927911072, -0.12144568718263302, 0.13266782125393892, -0.07986666968670385, -0.149416276130654, 0.06492443706160518, 0.42218771761004953, -0.2679560485392295, -0.31107627754581385, 0.02885947761730687, -0.23475509967612124, -0.30169844388662054, 0.23903926020627306, -0.073858575017630... |
709.3643 | Broad Line Emission in Low-Metallicity Blue Compact Dwarf Galaxies:
Evidence for Stellar Wind, Supernova and Possible AGN Activity | We present spectra of a large sample of low-metallicity blue compact dwarf
galaxies which exhibit broad components in their strong emission lines, mainly
in Hbeta, [O III]4959, 5007 and Halpha. Twenty-three spectra have been obtained
with the MMT, 14 of which show broad emission. The remaining 21 spectra with
broad e... | astro-ph | we present spectra of a large sample of lowmetallicity blue compact dwarf galaxies which exhibit broad components in their strong emission lines mainly in hbeta o iii4959 5007 and halpha twentythree spectra have been obtained with the mmt 14 of which show broad emission the remaining 21 spectra with broad emission have... | [['we', 'present', 'spectra', 'of', 'a', 'large', 'sample', 'of', 'lowmetallicity', 'blue', 'compact', 'dwarf', 'galaxies', 'which', 'exhibit', 'broad', 'components', 'in', 'their', 'strong', 'emission', 'lines', 'mainly', 'in', 'hbeta', 'o', 'iii4959', '5007', 'and', 'halpha', 'twentythree', 'spectra', 'have', 'been',... | [-0.009478048008697277, 0.07940355992283334, 0.03622064682475122, 0.11690577367130159, -0.12502347713558595, -0.11592841514026407, 0.04012949012050575, 0.5167473139410669, -0.09384598138329403, -0.339427294857292, 0.03457327040642585, -0.36753910721957006, 0.05725437814306299, 0.19237419316142967, -0.007988931398490835... |
709.3644 | Radio Source Heating in the ICM: The Example of Cygnus A | One of the most promising solutions for the cooling flow problem involves
energy injection from the central AGN. However it is still not clear how
collimated jets can heat the ICM at large scale, and very little is known
concerning the effect of radio lobe expansion as they enter into pressure
equilibrium with the su... | astro-ph | one of the most promising solutions for the cooling flow problem involves energy injection from the central agn however it is still not clear how collimated jets can heat the icm at large scale and very little is known concerning the effect of radio lobe expansion as they enter into pressure equilibrium with the surrou... | [['one', 'of', 'the', 'most', 'promising', 'solutions', 'for', 'the', 'cooling', 'flow', 'problem', 'involves', 'energy', 'injection', 'from', 'the', 'central', 'agn', 'however', 'it', 'is', 'still', 'not', 'clear', 'how', 'collimated', 'jets', 'can', 'heat', 'the', 'icm', 'at', 'large', 'scale', 'and', 'very', 'little... | [-0.07288669402949638, 0.12729349069331594, -0.08284804225825002, 0.10830876899224655, -0.14831617209443285, -0.09359858268043426, 0.052009024434477275, 0.44020486281373383, -0.2522490810468276, -0.3099106388635065, 0.09498566415795108, -0.27617574949388857, 0.0022585617086958664, 0.20306990613898068, 0.023683521019557... |
709.3645 | Stable First-order Particle-frame Relativistic Hydrodynamics for
Dissipative Systems | We propose a stable first-order relativistic dissipative hydrodynamic
equation in the particle frame (Eckart frame) for the first time. The equation
to be proposed was in fact previously derived by the authors and a collaborator
from the relativistic Boltzmann equation. We demonstrate that the equilibrium
state is st... | nucl-th hep-ph physics.flu-dyn | we propose a stable firstorder relativistic dissipative hydrodynamic equation in the particle frame eckart frame for the first time the equation to be proposed was in fact previously derived by the authors and a collaborator from the relativistic boltzmann equation we demonstrate that the equilibrium state is stable wi... | [['we', 'propose', 'a', 'stable', 'firstorder', 'relativistic', 'dissipative', 'hydrodynamic', 'equation', 'in', 'the', 'particle', 'frame', 'eckart', 'frame', 'for', 'the', 'first', 'time', 'the', 'equation', 'to', 'be', 'proposed', 'was', 'in', 'fact', 'previously', 'derived', 'by', 'the', 'authors', 'and', 'a', 'col... | [-0.0777971721538229, 0.09597206157745748, -0.186225797442248, 0.06217956521531295, -0.07894897903883602, -0.12697782512277184, -0.04033981858349473, 0.31069956167896345, -0.29328559784264097, -0.24815143496380188, 0.009726052185259305, -0.24888691849007114, -0.06457783524571668, 0.13904420366204093, -0.019266948842148... |
709.3646 | A convenient category of locally preordered spaces | As a practical foundation for a homotopy theory of abstract spacetime, we
extend a category of certain compact partially ordered spaces to a convenient
category of locally preordered spaces. In particular, we show that our new
category is Cartesian closed and that the forgetful functor to the category of
compactly ge... | math.AT | as a practical foundation for a homotopy theory of abstract spacetime we extend a category of certain compact partially ordered spaces to a convenient category of locally preordered spaces in particular we show that our new category is cartesian closed and that the forgetful functor to the category of compactly generat... | [['as', 'a', 'practical', 'foundation', 'for', 'a', 'homotopy', 'theory', 'of', 'abstract', 'spacetime', 'we', 'extend', 'a', 'category', 'of', 'certain', 'compact', 'partially', 'ordered', 'spaces', 'to', 'a', 'convenient', 'category', 'of', 'locally', 'preordered', 'spaces', 'in', 'particular', 'we', 'show', 'that', ... | [-0.13692587967798636, 0.08366361079051306, -0.06709799329390782, 0.15923104676409838, -0.15855835093054593, -0.07768752072986804, 0.014567007986714313, 0.42234735194136175, -0.41212108342401815, -0.11285566878423356, 0.09295500095794794, -0.1646101445770463, -0.12787406676726645, 0.20437162134208178, -0.21965293955515... |
709.3647 | A light non-standard Higgs boson: to be or not to be at a (Super) B
factory? | A light non-standard Higgs boson decaying mainly into $\tau^+\tau^-$ has not
been yet ruled out by LEP searches in several scenarios. We verify that, in the
context of the Next-to-Minimal-Supersymmetric Standard Model, a low-mass CP-odd
(mostly but not completely singlet-like) Higgs boson can couple strongly enough
t... | hep-ph | a light nonstandard higgs boson decaying mainly into tautau has not been yet ruled out by lep searches in several scenarios we verify that in the context of the nexttominimalsupersymmetric standard model a lowmass cpodd mostly but not completely singletlike higgs boson can couple strongly enough to downtype fermions to... | [['a', 'light', 'nonstandard', 'higgs', 'boson', 'decaying', 'mainly', 'into', 'tautau', 'has', 'not', 'been', 'yet', 'ruled', 'out', 'by', 'lep', 'searches', 'in', 'several', 'scenarios', 'we', 'verify', 'that', 'in', 'the', 'context', 'of', 'the', 'nexttominimalsupersymmetric', 'standard', 'model', 'a', 'lowmass', 'c... | [-0.06629122060564298, 0.32612136570050526, -0.07253179292954308, 0.18524332204833627, -0.11659127464027781, -0.27988095880535085, 0.07930732634390313, 0.3397717537039793, -0.2029986705104085, -0.23336531114029258, -0.0022572680777796592, -0.2932558585399468, 0.04968482406050163, 0.1703257273950026, 0.06638356197723433... |
709.3648 | On the Correlations, Selberg Integral and Symmetry of Sieve Functions in
Short Intervals | We study the arithmetic (real) function f=g*1, with g "essentially bounded"
and supported over the integers of [1,Q]. In particular, we obtain non-trivial
bounds, through f "correlations", for the "Selberg integral" and the "symmetry
integral" of f in almost all short intervals [x-h,x+h], N<x<2N, beyond the
"classica... | math.NT | we study the arithmetic real function fg1 with g essentially bounded and supported over the integers of 1q in particular we obtain nontrivial bounds through f correlations for the selberg integral and the symmetry integral of f in almost all short intervals xhxh nx2n beyond the classical level up to level of distributi... | [['we', 'study', 'the', 'arithmetic', 'real', 'function', 'fg1', 'with', 'g', 'essentially', 'bounded', 'and', 'supported', 'over', 'the', 'integers', 'of', '1q', 'in', 'particular', 'we', 'obtain', 'nontrivial', 'bounds', 'through', 'f', 'correlations', 'for', 'the', 'selberg', 'integral', 'and', 'the', 'symmetry', 'i... | [-0.15665166032849812, 0.12277989414287731, -0.08145226121414453, 0.0913889606599696, -0.020989234984153882, -0.12561557088629344, 0.05960657060641097, 0.32368105044588447, -0.2802522633719491, -0.2840568199473637, 0.06901368003163952, -0.2717398218461312, -0.1265757594293973, 0.20366988331079483, -0.052938751364126804... |
709.3649 | Spin and orbital angular momentum in gauge theories (I): QED and
determination of the angular momentum density | This two-paper series addresses and fixes the long-standing gauge invariance
problem of angular momentum in gauge theories. This QED part reveals: 1) The
spin and orbital angular momenta of electrons and photons can all be
consistently defined gauge invariantly. 2) These gauge-invariant quantities can
be conveniently... | hep-ph | this twopaper series addresses and fixes the longstanding gauge invariance problem of angular momentum in gauge theories this qed part reveals 1 the spin and orbital angular momenta of electrons and photons can all be consistently defined gauge invariantly 2 these gaugeinvariant quantities can be conveniently computed ... | [['this', 'twopaper', 'series', 'addresses', 'and', 'fixes', 'the', 'longstanding', 'gauge', 'invariance', 'problem', 'of', 'angular', 'momentum', 'in', 'gauge', 'theories', 'this', 'qed', 'part', 'reveals', '1', 'the', 'spin', 'and', 'orbital', 'angular', 'momenta', 'of', 'electrons', 'and', 'photons', 'can', 'all', '... | [-0.17544728344693836, 0.2646184248448669, -0.09215186688586743, 0.12014433754485672, -0.10835638840981915, -0.11140660927325052, -0.03530654878046255, 0.3484497656026026, -0.25880591203560577, -0.27104977474982994, -0.03869921939165406, -0.2438854133220811, -0.07654966530560033, 0.09314275151679469, -0.035796634849487... |
709.365 | A Support Theorem For The Radiation Fields On Asymptotically Euclidean
Manifolds | We prove a support theorem for the radiation fields on asymptotically
Euclidean manifolds with metrics which are warped products near infinity. It
generalizes to this setting the well known support theorem for the Radon
transform on n-dimensional Euclidean space.
| math.AP | we prove a support theorem for the radiation fields on asymptotically euclidean manifolds with metrics which are warped products near infinity it generalizes to this setting the well known support theorem for the radon transform on ndimensional euclidean space | [['we', 'prove', 'a', 'support', 'theorem', 'for', 'the', 'radiation', 'fields', 'on', 'asymptotically', 'euclidean', 'manifolds', 'with', 'metrics', 'which', 'are', 'warped', 'products', 'near', 'infinity', 'it', 'generalizes', 'to', 'this', 'setting', 'the', 'well', 'known', 'support', 'theorem', 'for', 'the', 'radon... | [-0.08579245801919545, 0.0626970323948906, -0.08452322109578511, 0.16565022931302872, -0.08014195818358506, -0.10674037014205869, -0.010178325029137807, 0.3582485953871256, -0.2115206934678822, -0.1625840316693752, 0.21180338635801887, -0.3019424115952391, -0.17132391926283255, 0.2427421664007199, -0.1677829368183246, ... |
709.3651 | A further look into combinatorial orthogonality | Strongly quadrangular matrices have been introduced in the study of the
combinatorial properties of unitary matrices. It is known that if a (0,
1)-matrix supports a unitary then it is strongly quadrangular. However, the
converse is not necessarily true. In this paper, we fully classify strongly
quadrangular matrices ... | math.CO quant-ph | strongly quadrangular matrices have been introduced in the study of the combinatorial properties of unitary matrices it is known that if a 0 1matrix supports a unitary then it is strongly quadrangular however the converse is not necessarily true in this paper we fully classify strongly quadrangular matrices up to degre... | [['strongly', 'quadrangular', 'matrices', 'have', 'been', 'introduced', 'in', 'the', 'study', 'of', 'the', 'combinatorial', 'properties', 'of', 'unitary', 'matrices', 'it', 'is', 'known', 'that', 'if', 'a', '0', '1matrix', 'supports', 'a', 'unitary', 'then', 'it', 'is', 'strongly', 'quadrangular', 'however', 'the', 'co... | [-0.12856486158036604, 0.18501092124412336, -0.06040995719093012, 0.039982555857178095, -0.051853089370458134, -0.1912037377166221, -0.02687015902199896, 0.4007069849431878, -0.30552243014297836, -0.1972680370459651, 0.11633792175150408, -0.274055303869451, -0.18550886383007575, 0.11120101306502275, -0.0699746045738276... |
709.3652 | Massive vectors from projective-invariance breaking | A general affine connection has enough degrees of freedom to describe the
classical gravitational and electromagnetic fields in the metric-affine
formulation of gravity. The gravitational field is represented in the
Lagrangian by the symmetric part of the Ricci tensor and the classical
electromagnetic field can be re... | gr-qc hep-th math-ph math.MP | a general affine connection has enough degrees of freedom to describe the classical gravitational and electromagnetic fields in the metricaffine formulation of gravity the gravitational field is represented in the lagrangian by the symmetric part of the ricci tensor and the classical electromagnetic field can be repres... | [['a', 'general', 'affine', 'connection', 'has', 'enough', 'degrees', 'of', 'freedom', 'to', 'describe', 'the', 'classical', 'gravitational', 'and', 'electromagnetic', 'fields', 'in', 'the', 'metricaffine', 'formulation', 'of', 'gravity', 'the', 'gravitational', 'field', 'is', 'represented', 'in', 'the', 'lagrangian', ... | [-0.23228595526661816, 0.1779319460555576, -0.08369421408465424, 0.06399721090295693, -0.19972051959030512, -0.12654088927097845, -0.12239117211571372, 0.29446250486482933, -0.2506849661015156, -0.24870081328582472, 0.04840212734132188, -0.22722202876203682, -0.1752694734054186, 0.08425817024871343, -0.0396288016788298... |
709.3653 | Two Scenarios of the Quantum Critical Point | Two different scenarios of the quantum critical point (QCP), a
zero-temperature instability of the Landau state, related to the divergence of
the effective mass, are investigated. Flaws of the standard scenario of the
QCP, where this divergence is attributed to the occurrence of some second-order
phase transition, ar... | cond-mat.str-el | two different scenarios of the quantum critical point qcp a zerotemperature instability of the landau state related to the divergence of the effective mass are investigated flaws of the standard scenario of the qcp where this divergence is attributed to the occurrence of some secondorder phase transition are demonstrat... | [['two', 'different', 'scenarios', 'of', 'the', 'quantum', 'critical', 'point', 'qcp', 'a', 'zerotemperature', 'instability', 'of', 'the', 'landau', 'state', 'related', 'to', 'the', 'divergence', 'of', 'the', 'effective', 'mass', 'are', 'investigated', 'flaws', 'of', 'the', 'standard', 'scenario', 'of', 'the', 'qcp', '... | [-0.24458296379368555, 0.1957243787187556, -0.08824681263956193, 0.08529264705966373, -0.024033307617432192, -0.17475196757402858, 0.05719405399684451, 0.259073400360189, -0.26779764475006806, -0.2292043904724874, 0.03741714987095053, -0.3371610045923214, -0.17043381441188485, 0.14307137868416153, 0.0003819813657748072... |
709.3654 | VERITAS: Status and Latest Results | VERITAS is an atmospheric Cherenkov telescope array designed to study
astrophysi cal sources of very-high-energy gamma radiation. Located in southern
Arizona, USA, the array consists of four 12m-diameter imaging Cherenkov
telescopes. All four telescopes have been deployed at the basecamp of the
Whipple Observatory an... | astro-ph | veritas is an atmospheric cherenkov telescope array designed to study astrophysi cal sources of veryhighenergy gamma radiation located in southern arizona usa the array consists of four 12mdiameter imaging cherenkov telescopes all four telescopes have been deployed at the basecamp of the whipple observatory and began f... | [['veritas', 'is', 'an', 'atmospheric', 'cherenkov', 'telescope', 'array', 'designed', 'to', 'study', 'astrophysi', 'cal', 'sources', 'of', 'veryhighenergy', 'gamma', 'radiation', 'located', 'in', 'southern', 'arizona', 'usa', 'the', 'array', 'consists', 'of', 'four', '12mdiameter', 'imaging', 'cherenkov', 'telescopes'... | [-0.1392934110009338, 0.18525795275648282, -0.030781276706555807, 0.0330034366531952, -0.09793621520008389, -0.06466017469663073, -0.07156249919648257, 0.40818341411146764, -0.07641891772682602, -0.4166805683005903, 0.16008994681446032, -0.3384418212053542, -0.0948232731127457, 0.27114002187610475, -0.04111583428882138... |
709.3655 | Nonlinear paramagnetic magnetization in the mixed state of CeCoIn_5 | Torque and magnetization measurements in magnetic fields $H$ up to 14 T were
performed on CeCoIn$_5$ single crystals. The amplitude of the paramagnetic
torque shows an $H^{2.3}$ dependence in the mixed state and an $H^{2}$
dependence in the normal state. In addition, the mixed-state magnetizations for
both $H\paralle... | cond-mat.str-el | torque and magnetization measurements in magnetic fields h up to 14 t were performed on cecoin_5 single crystals the amplitude of the paramagnetic torque shows an h23 dependence in the mixed state and an h2 dependence in the normal state in addition the mixedstate magnetizations for both hparallel c and hparallel ab ax... | [['torque', 'and', 'magnetization', 'measurements', 'in', 'magnetic', 'fields', 'h', 'up', 'to', '14', 't', 'were', 'performed', 'on', 'cecoin_5', 'single', 'crystals', 'the', 'amplitude', 'of', 'the', 'paramagnetic', 'torque', 'shows', 'an', 'h23', 'dependence', 'in', 'the', 'mixed', 'state', 'and', 'an', 'h2', 'depen... | [-0.1593511434360629, 0.20768950053939728, -0.05496746434697083, -0.013138116684387482, -0.02675906064520989, -0.08654766415378877, 0.07835321804242475, 0.35317135456772075, -0.2526341321212905, -0.264829642724778, 0.034858125783059565, -0.3229033938830807, -0.04199568984054384, 0.21226949614162247, 0.07077700831943644... |
709.3656 | A simple construction of fermion measure term in U(1) chiral lattice
gauge theories with exact gauge invariance | In the gauge invariant formulation of U(1) chiral lattice gauge theories
based on the Ginsparg-Wilson relation, the gauge field dependence of the
fermion measure is determined through the so-called measure term. We derive a
closed formula of the measure term on the finite volume lattice. The Wilson
line degrees of fr... | hep-lat | in the gauge invariant formulation of u1 chiral lattice gauge theories based on the ginspargwilson relation the gauge field dependence of the fermion measure is determined through the socalled measure term we derive a closed formula of the measure term on the finite volume lattice the wilson line degrees of freedom tor... | [['in', 'the', 'gauge', 'invariant', 'formulation', 'of', 'u1', 'chiral', 'lattice', 'gauge', 'theories', 'based', 'on', 'the', 'ginspargwilson', 'relation', 'the', 'gauge', 'field', 'dependence', 'of', 'the', 'fermion', 'measure', 'is', 'determined', 'through', 'the', 'socalled', 'measure', 'term', 'we', 'derive', 'a'... | [-0.19405363661752753, 0.14440056210583893, -0.08634265861618294, 0.07795495361239796, -0.09651752917696375, -0.11410716455044949, 0.04337966007811656, 0.31228565615563353, -0.22757333204388802, -0.251748943732174, 0.0962914830027533, -0.24889217234555294, -0.11269933600671404, 0.10309651711655488, -0.04020008145377409... |
709.3657 | Observations of the high-frequency-peaked BL Lac object 1ES 1218+304
with VERITAS | The VERITAS collaboration has observed the high-frequency-peaked BL Lac
object 1ES 1218+304 using an array of several imaging Cherenkov telescopes
located at the Fred Lawrence Whipple Observatory in Southern Arizona. A
gamma-ray signal was detected with high significance for the observations taken
during several mont... | astro-ph | the veritas collaboration has observed the highfrequencypeaked bl lac object 1es 1218304 using an array of several imaging cherenkov telescopes located at the fred lawrence whipple observatory in southern arizona a gammaray signal was detected with high significance for the observations taken during several months in t... | [['the', 'veritas', 'collaboration', 'has', 'observed', 'the', 'highfrequencypeaked', 'bl', 'lac', 'object', '1es', '1218304', 'using', 'an', 'array', 'of', 'several', 'imaging', 'cherenkov', 'telescopes', 'located', 'at', 'the', 'fred', 'lawrence', 'whipple', 'observatory', 'in', 'southern', 'arizona', 'a', 'gammaray'... | [-0.06912790815676412, 0.21327365361245146, -0.05333563075926635, 0.14858081047761165, -0.14658019832906224, -0.12854206083612818, -0.028009427655037614, 0.5163344781725637, -0.07576879082367785, -0.45298400013557366, 0.10627317782153466, -0.3583436155271146, -0.011330140874751152, 0.2784485615369293, -0.05684229105921... |
709.3658 | A construction of the Glashow-Weinberg-Salam model on the lattice with
exact gauge invariance | We present a gauge-invariant and non-perturbative construction of the
Glashow-Weinberg-Salam model on the lattice, based on the lattice Dirac
operator satisfying the Ginsparg-Wilson relation. Our construction covers all
SU(2) topological sectors with vanishing U(1) magnetic flux and would be usable
for a description ... | hep-lat hep-ph hep-th | we present a gaugeinvariant and nonperturbative construction of the glashowweinbergsalam model on the lattice based on the lattice dirac operator satisfying the ginspargwilson relation our construction covers all su2 topological sectors with vanishing u1 magnetic flux and would be usable for a description of the baryon... | [['we', 'present', 'a', 'gaugeinvariant', 'and', 'nonperturbative', 'construction', 'of', 'the', 'glashowweinbergsalam', 'model', 'on', 'the', 'lattice', 'based', 'on', 'the', 'lattice', 'dirac', 'operator', 'satisfying', 'the', 'ginspargwilson', 'relation', 'our', 'construction', 'covers', 'all', 'su2', 'topological',... | [-0.1718312236517081, 0.1786867584813181, -0.10098786063228302, 0.09249150994010123, -0.10288760335162633, -0.10617165253900988, 0.04708268344915641, 0.28622813694413723, -0.21589933144016646, -0.26097897073532655, 0.06117022310852946, -0.2533847332792723, -0.12043841930443612, 0.12713392508788196, -0.02205359015071134... |
709.3659 | Observations of Mrk 421 and Mrk 501 in Spring 2006 with VERITAS | VERITAS, the Very Energetic Radiation Telescope Imaging Array System, is an
array of four imaging Atmospheric Cherenkov telescopes in southern Arizona. It
is sensitive to gamma rays at energies above 100 GeV. Here, we discuss the
results of observations of two well known VHE blazars, Markarian 421 and
Markarian 501, ... | astro-ph | veritas the very energetic radiation telescope imaging array system is an array of four imaging atmospheric cherenkov telescopes in southern arizona it is sensitive to gamma rays at energies above 100 gev here we discuss the results of observations of two well known vhe blazars markarian 421 and markarian 501 during sp... | [['veritas', 'the', 'very', 'energetic', 'radiation', 'telescope', 'imaging', 'array', 'system', 'is', 'an', 'array', 'of', 'four', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'in', 'southern', 'arizona', 'it', 'is', 'sensitive', 'to', 'gamma', 'rays', 'at', 'energies', 'above', '100', 'gev', 'here', 'we', 'di... | [-0.0742499838806381, 0.19152653054466515, -0.029970899455187733, 0.10515946521296758, -0.10772191454494788, -0.09219958882948215, -0.014971261033942262, 0.49375663362135574, -0.1434958385946306, -0.45375710080016, 0.12497196370477918, -0.2975473931397904, -0.04153286199824315, 0.26673419905964996, -0.00138297201372867... |
709.366 | Einstein's equations and the embedding of 3-dimensional CR manifolds | We prove several theorems concerning the connection between the local CR
embeddability of 3-dimensional CR manifolds, and the existence of algebraically
special Maxwell and gravitational fields. We reduce the Einstein equations for
spacetimes associated with such fields to a system of CR invariant equations on
a 3-di... | math.DG math.AP math.CV | we prove several theorems concerning the connection between the local cr embeddability of 3dimensional cr manifolds and the existence of algebraically special maxwell and gravitational fields we reduce the einstein equations for spacetimes associated with such fields to a system of cr invariant equations on a 3dimensio... | [['we', 'prove', 'several', 'theorems', 'concerning', 'the', 'connection', 'between', 'the', 'local', 'cr', 'embeddability', 'of', '3dimensional', 'cr', 'manifolds', 'and', 'the', 'existence', 'of', 'algebraically', 'special', 'maxwell', 'and', 'gravitational', 'fields', 'we', 'reduce', 'the', 'einstein', 'equations', ... | [-0.2328361041812051, 0.053447357540214874, -0.028974567177808948, 0.11688968579038087, -0.0930473350872023, -0.12813475110735267, -0.05846401643899516, 0.3118283916583173, -0.24957170579423252, -0.2284627164530958, 0.07651948567846009, -0.26222409744762903, -0.1524206765720414, 0.20075648193323237, -0.0296801904367649... |
709.3661 | Observation of LS I +61 303 with VERITAS | The high mass X-ray binary LS I +61 303 has been observed over several months
in 2006 and 2007 with the VERITAS array of imaging air-Cherenkov telescopes. A
signal of high energy gamma rays with energies above 350 GeV is detected in
several orbital cycles of the binary system. The detected flux of gamma rays is
stron... | astro-ph | the high mass xray binary ls i 61 303 has been observed over several months in 2006 and 2007 with the veritas array of imaging aircherenkov telescopes a signal of high energy gamma rays with energies above 350 gev is detected in several orbital cycles of the binary system the detected flux of gamma rays is strongly var... | [['the', 'high', 'mass', 'xray', 'binary', 'ls', 'i', '61', '303', 'has', 'been', 'observed', 'over', 'several', 'months', 'in', '2006', 'and', '2007', 'with', 'the', 'veritas', 'array', 'of', 'imaging', 'aircherenkov', 'telescopes', 'a', 'signal', 'of', 'high', 'energy', 'gamma', 'rays', 'with', 'energies', 'above', '... | [-0.14579557365337117, 0.20351280530695265, -0.028586979113662474, 0.05779351897385473, -0.031193303915922746, -0.08259303826623811, 0.038411536656964854, 0.4173802139165883, -0.21968502797692332, -0.4378511901013553, 0.09350245179442797, -0.31794062508897, 0.01670082973746153, 0.23000859493018092, -0.00047024984199267... |
709.3662 | Econophysics, Statistical Mechanics Approach to | This is a review article for Encyclopedia of Complexity and System Science,
to be published by Springer http://refworks.springer.com/complexity/. The paper
reviews statistical models for money, wealth, and income distributions
developed in the econophysics literature since late 1990s.
| q-fin.ST cond-mat.stat-mech physics.data-an physics.soc-ph stat.AP | this is a review article for encyclopedia of complexity and system science to be published by springer httprefworksspringercomcomplexity the paper reviews statistical models for money wealth and income distributions developed in the econophysics literature since late 1990s | [['this', 'is', 'a', 'review', 'article', 'for', 'encyclopedia', 'of', 'complexity', 'and', 'system', 'science', 'to', 'be', 'published', 'by', 'springer', 'httprefworksspringercomcomplexity', 'the', 'paper', 'reviews', 'statistical', 'models', 'for', 'money', 'wealth', 'and', 'income', 'distributions', 'developed', 'i... | [0.0036379986494365665, 0.023524218963252172, -0.14619984258509552, 0.09702874714922574, -0.1291511330443124, -0.10207071782658911, 0.012720872030412365, 0.27088560060494477, -0.24537013481474584, -0.3725407618201441, 0.1374286839111139, -0.30176954561223585, -0.1568278389879399, 0.1902044369942612, -0.2200646643889033... |
709.3663 | Observation of M87 with VERITAS | The giant radio galaxy M87 is the only extragalactic non-blazar object which
has been detected as a source of very high energy gamma-rays. It represents a
unique opportunity to study the phenomena of gamma-ray emission from a nearby
AGN. In this paper we report preliminary results from the observations of M87
taken w... | astro-ph | the giant radio galaxy m87 is the only extragalactic nonblazar object which has been detected as a source of very high energy gammarays it represents a unique opportunity to study the phenomena of gammaray emission from a nearby agn in this paper we report preliminary results from the observations of m87 taken with the... | [['the', 'giant', 'radio', 'galaxy', 'm87', 'is', 'the', 'only', 'extragalactic', 'nonblazar', 'object', 'which', 'has', 'been', 'detected', 'as', 'a', 'source', 'of', 'very', 'high', 'energy', 'gammarays', 'it', 'represents', 'a', 'unique', 'opportunity', 'to', 'study', 'the', 'phenomena', 'of', 'gammaray', 'emission'... | [-0.05752106041652726, 0.12251107266278717, -0.09121286105155275, 0.11480703655619885, -0.13216857122927067, -0.07636523872006977, 0.02794017209645277, 0.43367674057319594, -0.12411961676762177, -0.43384908219234325, 0.05514434588944874, -0.3574910962933235, -0.031113223413403116, 0.25549871278298875, -0.00258374409331... |
709.3664 | Connecting SLE and minisuperspace Liouville gravity | We show that Fokker-Planck equation for chordal SLE process under a simple
rescaling of the probability density can be traced to the minisuperspace
Wheeler-de Witt equation for boundary operator in 2d Liouville gravity.
Insertion of an operator, calculating SLE critical exponent, corresponds to
adding matter contribu... | hep-th math-ph math.MP | we show that fokkerplanck equation for chordal sle process under a simple rescaling of the probability density can be traced to the minisuperspace wheelerde witt equation for boundary operator in 2d liouville gravity insertion of an operator calculating sle critical exponent corresponds to adding matter contribution to... | [['we', 'show', 'that', 'fokkerplanck', 'equation', 'for', 'chordal', 'sle', 'process', 'under', 'a', 'simple', 'rescaling', 'of', 'the', 'probability', 'density', 'can', 'be', 'traced', 'to', 'the', 'minisuperspace', 'wheelerde', 'witt', 'equation', 'for', 'boundary', 'operator', 'in', '2d', 'liouville', 'gravity', 'i... | [-0.12881166898449392, 0.13318541237037462, -0.1399775945434445, 0.11784289142138062, -0.13618599343202445, -0.20038001608765243, -0.02712085996570654, 0.287367685570835, -0.28411906284868327, -0.2032632557001259, 0.054907711515337916, -0.28019334501311133, -0.16810499570381485, 0.20393791539888634, -0.0494907258574752... |
709.3665 | Nonlinear Elasticity, Fluctuations and Heterogeneity of Nematic
Elastomers | Liquid crystal elastomers realize a fascinating new form of soft matter that
is a composite of a conventional crosslinked polymer gel (rubber) and a liquid
crystal. These {\em solid} liquid crystal amalgams, quite similarly to their
(conventional, fluid) liquid crystal counterparts, can spontaneously partially
break ... | cond-mat.soft cond-mat.stat-mech | liquid crystal elastomers realize a fascinating new form of soft matter that is a composite of a conventional crosslinked polymer gel rubber and a liquid crystal these em solid liquid crystal amalgams quite similarly to their conventional fluid liquid crystal counterparts can spontaneously partially break translational... | [['liquid', 'crystal', 'elastomers', 'realize', 'a', 'fascinating', 'new', 'form', 'of', 'soft', 'matter', 'that', 'is', 'a', 'composite', 'of', 'a', 'conventional', 'crosslinked', 'polymer', 'gel', 'rubber', 'and', 'a', 'liquid', 'crystal', 'these', 'em', 'solid', 'liquid', 'crystal', 'amalgams', 'quite', 'similarly',... | [-0.19643608266892443, 0.28523240900051405, -0.1283102551178672, 0.012579366665704583, -0.09008901719244022, -0.1510008074237703, 0.025424801174722234, 0.3564302631057217, -0.3265591902345477, -0.22743929164425936, 0.05744164067391466, -0.2383070583055087, -0.21567614995910844, 0.08736990188117488, -0.01395622775635274... |
709.3666 | Experimental study on Gaussian-modulated coherent states quantum key
distribution over standard telecom fiber | In this paper, we present a fully fiber-based one-way Quantum Key
Distribution (QKD) system implementing the Gaussian-Modulated Coherent States
(GMCS) protocol. The system employs a double Mach-Zehnder Interferometer (MZI)
configuration in which the weak quantum signal and the strong Local Oscillator
(LO) go through ... | quant-ph | in this paper we present a fully fiberbased oneway quantum key distribution qkd system implementing the gaussianmodulated coherent states gmcs protocol the system employs a double machzehnder interferometer mzi configuration in which the weak quantum signal and the strong local oscillator lo go through the same fiber b... | [['in', 'this', 'paper', 'we', 'present', 'a', 'fully', 'fiberbased', 'oneway', 'quantum', 'key', 'distribution', 'qkd', 'system', 'implementing', 'the', 'gaussianmodulated', 'coherent', 'states', 'gmcs', 'protocol', 'the', 'system', 'employs', 'a', 'double', 'machzehnder', 'interferometer', 'mzi', 'configuration', 'in... | [-0.19828402557918293, 0.10128799415730155, -0.11120106757858372, 0.02260780752333107, -0.0026005763687532058, -0.20854021794278224, 0.09316122520998982, 0.4034053151880278, -0.26020585617339803, -0.2632652897172551, 0.059199791371638916, -0.23913107267815742, -0.1131626618849678, 0.22236335227595797, -0.10071648493987... |
709.3667 | Generalized sine-Gordon model and baryons in two-dimensional QCD | We consider the sl(3,C) affine Toda model coupled to matter (Dirac spinor)
(ATM) and through a gauge fixing procedure we obtain the classical version of
the generalized sl(3,C) sine-Gordon model (cGSG) which completely decouples
from the Dirac spinors. The GSG models are multifield extensions of the
ordinary sine-Gor... | hep-th | we consider the sl3c affine toda model coupled to matter dirac spinor atm and through a gauge fixing procedure we obtain the classical version of the generalized sl3c sinegordon model cgsg which completely decouples from the dirac spinors the gsg models are multifield extensions of the ordinary sinegordon model in the ... | [['we', 'consider', 'the', 'sl3c', 'affine', 'toda', 'model', 'coupled', 'to', 'matter', 'dirac', 'spinor', 'atm', 'and', 'through', 'a', 'gauge', 'fixing', 'procedure', 'we', 'obtain', 'the', 'classical', 'version', 'of', 'the', 'generalized', 'sl3c', 'sinegordon', 'model', 'cgsg', 'which', 'completely', 'decouples', ... | [-0.13686199660019827, 0.19473359725476466, -0.06728480449786074, 0.11825604727119589, -0.0888136853311272, -0.19328251614647565, -0.024524898036883104, 0.2842489680137913, -0.18889543170448855, -0.24433897195200696, 0.018400924650524727, -0.2800507694788155, -0.145425352268249, 0.11856444800925273, 0.03139384886341506... |
709.3668 | Fermions on one or fewer Kinks | We find the full spectrum of fermion bound states on a Z_2 kink. In addition
to the zero mode, there are int[2 m_f/m_s] bound states, where m_f is the
fermion and m_s the scalar mass. We also study fermion modes on the background
of a well-separated kink-antikink pair. Using a variational argument, we prove
that ther... | hep-th | we find the full spectrum of fermion bound states on a z_2 kink in addition to the zero mode there are int2 m_fm_s bound states where m_f is the fermion and m_s the scalar mass we also study fermion modes on the background of a wellseparated kinkantikink pair using a variational argument we prove that there is at least... | [['we', 'find', 'the', 'full', 'spectrum', 'of', 'fermion', 'bound', 'states', 'on', 'a', 'z_2', 'kink', 'in', 'addition', 'to', 'the', 'zero', 'mode', 'there', 'are', 'int2', 'm_fm_s', 'bound', 'states', 'where', 'm_f', 'is', 'the', 'fermion', 'and', 'm_s', 'the', 'scalar', 'mass', 'we', 'also', 'study', 'fermion', 'm... | [-0.16746162922319138, 0.25360308617654476, -0.0751543121995649, 0.10134617378464852, 0.0004916039302550031, -0.15814295160875777, 0.09776354821944477, 0.29912565894321436, -0.16896224720873917, -0.3075823953770327, 0.058248217920819766, -0.3311925751693321, -0.08093780797501707, 0.12167712273264322, 0.0668478287530667... |
709.3669 | Development of a thermal ionizer as ion catcher | An effective ion catcher is an important part of a radioactive beam facility
that is based on in-flight production. The catcher stops fast radioactive
products and emits them as singly charged slow ions. Current ion catchers are
based on stopping in He and H$_2$ gas. However, with increasing intensity of
the secondar... | nucl-ex | an effective ion catcher is an important part of a radioactive beam facility that is based on inflight production the catcher stops fast radioactive products and emits them as singly charged slow ions current ion catchers are based on stopping in he and h_2 gas however with increasing intensity of the secondary beam th... | [['an', 'effective', 'ion', 'catcher', 'is', 'an', 'important', 'part', 'of', 'a', 'radioactive', 'beam', 'facility', 'that', 'is', 'based', 'on', 'inflight', 'production', 'the', 'catcher', 'stops', 'fast', 'radioactive', 'products', 'and', 'emits', 'them', 'as', 'singly', 'charged', 'slow', 'ions', 'current', 'ion', ... | [-0.006433303883790763, 0.24180207439834098, -0.011769911316999544, 0.014340180227817554, 0.029403396897638837, -0.16434504599051758, 0.02959154810782315, 0.40994727191411784, -0.20926581053580676, -0.2768673015777798, 0.0823601218205618, -0.33531313781988703, 0.03899323896815379, 0.22045219256025222, -0.00823931370396... |
709.367 | Production and trapping of radioactive atoms at the TRI\muP facility | The structures for the TRI$\mu$P facility have been completed and
commissioned. At the facility radioactive nuclides are produced to study
fundamental interactions and symmetries. An important feature is the
possibility to trap radioactive atoms in order to obtain and hold a pure
substrate-free sample for precision m... | nucl-ex | the structures for the trimup facility have been completed and commissioned at the facility radioactive nuclides are produced to study fundamental interactions and symmetries an important feature is the possibility to trap radioactive atoms in order to obtain and hold a pure substratefree sample for precision measureme... | [['the', 'structures', 'for', 'the', 'trimup', 'facility', 'have', 'been', 'completed', 'and', 'commissioned', 'at', 'the', 'facility', 'radioactive', 'nuclides', 'are', 'produced', 'to', 'study', 'fundamental', 'interactions', 'and', 'symmetries', 'an', 'important', 'feature', 'is', 'the', 'possibility', 'to', 'trap',... | [-0.032131896299627406, 0.2509421922856527, -0.03013762173567399, 0.041775557044412236, 0.013731942746226349, -0.1929105879353911, 0.03488380826135588, 0.4146396334818955, -0.24258305319694168, -0.30018839402405245, 0.02873471859509552, -0.3251127995519415, 0.08875001545516806, 0.2059316469210736, 0.007276107481675608,... |
709.3671 | A fractal approach to the rheology of concentrated cell suspensions | Results on the rheological behavior of novel CHO cell suspensions in a large
range of concentrations are reported. The concentration dependent yield stress
and elastic plateau modulus are formalized in the context of fractal aggregates
under shear, and quite different exponents are found as compared to the case of
re... | cond-mat.soft | results on the rheological behavior of novel cho cell suspensions in a large range of concentrations are reported the concentration dependent yield stress and elastic plateau modulus are formalized in the context of fractal aggregates under shear and quite different exponents are found as compared to the case of red bl... | [['results', 'on', 'the', 'rheological', 'behavior', 'of', 'novel', 'cho', 'cell', 'suspensions', 'in', 'a', 'large', 'range', 'of', 'concentrations', 'are', 'reported', 'the', 'concentration', 'dependent', 'yield', 'stress', 'and', 'elastic', 'plateau', 'modulus', 'are', 'formalized', 'in', 'the', 'context', 'of', 'fr... | [-0.08295640783394907, 0.1895451328633458, -0.036583561031671055, 0.02356407766915816, -0.00394426372027799, -0.10561650162144157, 0.017569592567893227, 0.36671554056137506, -0.275368364789429, -0.289346371929088, 0.05233713915555874, -0.2550251341079561, -0.19430423897868965, 0.1761851842420992, -0.09596009328019585, ... |
709.3672 | Baryon Acoustic Oscillation Intensity Mapping as a Test of Dark Energy | The expansion of the universe appears to be accelerating, and the mysterious
anti-gravity agent of this acceleration has been called ``dark energy''. To
measure the dynamics of dark energy, Baryon Acoustic Oscillations (BAO) can be
used. Previous discussions of the BAO dark energy test have focused on direct
measurem... | astro-ph | the expansion of the universe appears to be accelerating and the mysterious antigravity agent of this acceleration has been called dark energy to measure the dynamics of dark energy baryon acoustic oscillations bao can be used previous discussions of the bao dark energy test have focused on direct measurements of redsh... | [['the', 'expansion', 'of', 'the', 'universe', 'appears', 'to', 'be', 'accelerating', 'and', 'the', 'mysterious', 'antigravity', 'agent', 'of', 'this', 'acceleration', 'has', 'been', 'called', 'dark', 'energy', 'to', 'measure', 'the', 'dynamics', 'of', 'dark', 'energy', 'baryon', 'acoustic', 'oscillations', 'bao', 'can... | [-0.10452953652665019, 0.153920719653368, -0.09327508526667952, 0.11083747501950711, -0.1276111345589161, -0.09292060442082584, 0.01045328850671649, 0.3630369725376368, -0.2121002527177334, -0.3510948490947485, 0.08303123276401311, -0.2666103708446026, -0.011554629372432828, 0.22074750795029105, 0.030479004170745613, 0... |
709.3673 | Gauss-Green theorem for weakly differentiable vector fields, sets of
finite perimeter, and balance laws | We analyze a class of weakly differentiable vector fields (\FF \colon \rn \to
\rn) with the property that (\FF\in L^{\infty}) and (\div \FF) is a Radon
measure. The primary focus of our investigation is to introduce a suitable
notion of the normal trace of any divergence-measure field $\FF$ over the
boundary of an ar... | math.AP | we analyze a class of weakly differentiable vector fields ff colon rn to rn with the property that ffin linfty and div ff is a radon measure the primary focus of our investigation is to introduce a suitable notion of the normal trace of any divergencemeasure field ff over the boundary of an arbitrary set of finite peri... | [['we', 'analyze', 'a', 'class', 'of', 'weakly', 'differentiable', 'vector', 'fields', 'ff', 'colon', 'rn', 'to', 'rn', 'with', 'the', 'property', 'that', 'ffin', 'linfty', 'and', 'div', 'ff', 'is', 'a', 'radon', 'measure', 'the', 'primary', 'focus', 'of', 'our', 'investigation', 'is', 'to', 'introduce', 'a', 'suitable... | [-0.12695804036689773, 0.09091485294041324, -0.10731142813593204, 0.031309569168918056, -0.04136403107002158, -0.09205007219947327, 0.059242813364749854, 0.2934561622027746, -0.2892885575582862, -0.2050498100618236, 0.11092242371266954, -0.27215399277386443, -0.07855344727217659, 0.18520640453446985, -0.100639212493500... |
709.3674 | Implication of Classical Black Hole Evaporation Conjecture to Floating
Black Holes | In Randall-Sundrum single-brane (RS-II) model, it was conjectured that there
is no static large black hole localized on the brane based on adS/CFT
correspondence. Here we consider the phase diagram of black objects in the
models extended from the RS-II model. We propose a scenario for the phase
diagram consistent wit... | gr-qc | in randallsundrum singlebrane rsii model it was conjectured that there is no static large black hole localized on the brane based on adscft correspondence here we consider the phase diagram of black objects in the models extended from the rsii model we propose a scenario for the phase diagram consistent with the classi... | [['in', 'randallsundrum', 'singlebrane', 'rsii', 'model', 'it', 'was', 'conjectured', 'that', 'there', 'is', 'no', 'static', 'large', 'black', 'hole', 'localized', 'on', 'the', 'brane', 'based', 'on', 'adscft', 'correspondence', 'here', 'we', 'consider', 'the', 'phase', 'diagram', 'of', 'black', 'objects', 'in', 'the',... | [-0.14936372505067147, 0.06671383069215776, -0.0975014034978414, 0.16217808058797956, -0.06570640527834631, -0.18028973427613917, 0.04385118079307961, 0.28277092969223655, -0.11862578720798435, -0.2836272233127527, 0.07362949066757135, -0.2821416539580191, -0.15764233201410469, 0.15489334444043368, -0.08776226226393491... |
709.3675 | Length control of microtubules by depolymerizing motor proteins | In many intracellular processes, the length distribution of microtubules is
controlled by depolymerizing motor proteins. Experiments have shown that,
following non-specific binding to the surface of a microtubule, depolymerizers
are transported to the microtubule tip(s) by diffusion or directed walk and,
then, depoly... | physics.bio-ph cond-mat.stat-mech q-bio.SC | in many intracellular processes the length distribution of microtubules is controlled by depolymerizing motor proteins experiments have shown that following nonspecific binding to the surface of a microtubule depolymerizers are transported to the microtubule tips by diffusion or directed walk and then depolymerize the ... | [['in', 'many', 'intracellular', 'processes', 'the', 'length', 'distribution', 'of', 'microtubules', 'is', 'controlled', 'by', 'depolymerizing', 'motor', 'proteins', 'experiments', 'have', 'shown', 'that', 'following', 'nonspecific', 'binding', 'to', 'the', 'surface', 'of', 'a', 'microtubule', 'depolymerizers', 'are', ... | [-0.1133337915831735, 0.2256866231541491, -0.053337609108824, 0.0337213464835002, -0.03403064428895073, -0.1676934420471438, 0.06794677632383238, 0.4123679139973739, -0.29627066630667126, -0.2228185317467134, 0.03510371891659302, -0.25343673018804297, -0.1984614058455918, 0.18765946263178754, -0.04359619983006269, 0.03... |
709.3676 | Haagerup's Approximation Property and Relative Amenability | A finite von Neumann algebra $\mathcal{M}$ with a faithful normal trace $%
\tau $ has Haagerup's approximation property (relative to a von Neumann
subalgebra $\mathcal{N}$) if there exists a net $(\phi_{\alpha})_{\alpha\in
\Lambda}$ of normal completely positive ($\mathcal{N}$-bimodular) maps from
$\mathcal{M}$ to $\... | math.OA math.GR | a finite von neumann algebra mathcalm with a faithful normal trace tau has haagerups approximation property relative to a von neumann subalgebra mathcaln if there exists a net phi_alpha_alphain lambda of normal completely positive mathcalnbimodular maps from mathcalm to mathcalm that satisfy the subtracial condition ta... | [['a', 'finite', 'von', 'neumann', 'algebra', 'mathcalm', 'with', 'a', 'faithful', 'normal', 'trace', 'tau', 'has', 'haagerups', 'approximation', 'property', 'relative', 'to', 'a', 'von', 'neumann', 'subalgebra', 'mathcaln', 'if', 'there', 'exists', 'a', 'net', 'phi_alpha_alphain', 'lambda', 'of', 'normal', 'completely... | [-0.12956794181222758, 0.11782459057447399, -0.11953401328590248, 0.05901062055190484, -0.08193593876316183, -0.1918542231132667, -0.023701647783802342, 0.3342357597768217, -0.3569726532385234, -0.10218782037226183, 0.10586074604596492, -0.3041561398610112, -0.09095905539429476, 0.14898845642775058, -0.1433817479100393... |
709.3677 | Detailed description of accelerating, simple solutions of relativistic
perfect fluid hydrodynamics | In this paper we describe in full details a new family of recently found
exact solutions of relativistic, perfect fluid dynamics. With an ansatz, which
generalizes the well-known Hwa-Bjorken solution, we obtain a wide class of new
exact, explicit and simple solutions, which have a remarkable advantage as
compared to ... | nucl-th | in this paper we describe in full details a new family of recently found exact solutions of relativistic perfect fluid dynamics with an ansatz which generalizes the wellknown hwabjorken solution we obtain a wide class of new exact explicit and simple solutions which have a remarkable advantage as compared to presently ... | [['in', 'this', 'paper', 'we', 'describe', 'in', 'full', 'details', 'a', 'new', 'family', 'of', 'recently', 'found', 'exact', 'solutions', 'of', 'relativistic', 'perfect', 'fluid', 'dynamics', 'with', 'an', 'ansatz', 'which', 'generalizes', 'the', 'wellknown', 'hwabjorken', 'solution', 'we', 'obtain', 'a', 'wide', 'cla... | [-0.09624996162892785, 0.08726266725240678, -0.13736919076263104, 0.10159156544082529, -0.06081763097720865, -0.10764805247974717, -0.029150703735537648, 0.3200115062421761, -0.2421716951268116, -0.3189032656149581, 0.0774973296574899, -0.2257939309750397, -0.09936910365649965, 0.1855205800703306, -0.02440118421117614,... |
709.3678 | The spectral dimension of random brushes | We consider a class of random graphs, called random brushes, which are
constructed by adding linear graphs of random lengths to the vertices of Z^d
viewed as a graph. We prove that for d=2 all random brushes have spectral
dimension d_s=2. For d=3 we have {5\over 2}\leq d_s\leq 3 and for d\geq 4 we
have 3\leq d_s\leq ... | cond-mat.stat-mech | we consider a class of random graphs called random brushes which are constructed by adding linear graphs of random lengths to the vertices of zd viewed as a graph we prove that for d2 all random brushes have spectral dimension d_s2 for d3 we have 5over 2leq d_sleq 3 and for dgeq 4 we have 3leq d_sleq d | [['we', 'consider', 'a', 'class', 'of', 'random', 'graphs', 'called', 'random', 'brushes', 'which', 'are', 'constructed', 'by', 'adding', 'linear', 'graphs', 'of', 'random', 'lengths', 'to', 'the', 'vertices', 'of', 'zd', 'viewed', 'as', 'a', 'graph', 'we', 'prove', 'that', 'for', 'd2', 'all', 'random', 'brushes', 'hav... | [-0.15025888810799057, 0.24031203524542175, 0.007289378404883402, 0.012166689156271917, 0.0172602800219985, -0.24550252835199768, -0.032138022793723006, 0.44823256015245405, -0.1679101146458249, -0.19931362845402742, 0.12521887732353726, -0.3144454933104238, -0.15391474084130355, 0.08230348663424333, -0.051768448270325... |
709.3679 | Constraining the dark energy and smoothness-parameter with supernovae | The presence of inhomogeneities modifies the cosmic distances through the
gravitational lensing effect, and, indirectly, must affect the main
cosmological tests. Assuming that the dark energy is a smooth component, the
simplest way to account for the influence of clustering is to suppose that the
average evolution of... | astro-ph | the presence of inhomogeneities modifies the cosmic distances through the gravitational lensing effect and indirectly must affect the main cosmological tests assuming that the dark energy is a smooth component the simplest way to account for the influence of clustering is to suppose that the average evolution of the ex... | [['the', 'presence', 'of', 'inhomogeneities', 'modifies', 'the', 'cosmic', 'distances', 'through', 'the', 'gravitational', 'lensing', 'effect', 'and', 'indirectly', 'must', 'affect', 'the', 'main', 'cosmological', 'tests', 'assuming', 'that', 'the', 'dark', 'energy', 'is', 'a', 'smooth', 'component', 'the', 'simplest',... | [-0.09213060315966048, 0.14124041379110402, -0.0656731459770469, 0.08590938529920009, -0.09399491229633558, -0.1011606416826349, 0.06954496693394081, 0.3111047070788762, -0.2046654515456973, -0.36192875913313155, 0.0458506621634881, -0.28932106911248756, -0.03305798119635163, 0.17730909576969528, -0.00415617717415329, ... |
709.368 | Inequalities that Collectively Completely Characterize the Catalytic
Majorization Relation | For probability vectors x and y, the catalytic majorization relation x prec_T
y is defined to hold when there exists a probability vector z such that x
otimes z is majorized by y otimes z. In this paper, an infinite family of
functions is given such that, subject to some trivial restrictions, x prec_T y
if and only i... | quant-ph | for probability vectors x and y the catalytic majorization relation x prec_t y is defined to hold when there exists a probability vector z such that x otimes z is majorized by y otimes z in this paper an infinite family of functions is given such that subject to some trivial restrictions x prec_t y if and only if f_rx ... | [['for', 'probability', 'vectors', 'x', 'and', 'y', 'the', 'catalytic', 'majorization', 'relation', 'x', 'prec_t', 'y', 'is', 'defined', 'to', 'hold', 'when', 'there', 'exists', 'a', 'probability', 'vector', 'z', 'such', 'that', 'x', 'otimes', 'z', 'is', 'majorized', 'by', 'y', 'otimes', 'z', 'in', 'this', 'paper', 'an... | [-0.14888939633176235, 0.15591614234783605, -0.05073278664090371, 0.025802040240782614, -0.03363182362153242, -0.19458333058016358, 0.0741957036878961, 0.3915061959838968, -0.3361347340347277, -0.20612932805769082, 0.05597027934499685, -0.26282588020756337, -0.09946336707700107, 0.16469029229258506, -0.0901615874352470... |
709.3681 | Improved transfer matrix method without numerical instability | A new improved transfer matrix method (TMM) is presented. It is shown that
the method not only overcomes the numerical instability found in the original
TMM, but also greatly improves the scalability of computation. The new improved
TMM has no extra cost of computing time as the length of homogeneous scattering
regio... | cond-mat.mes-hall | a new improved transfer matrix method tmm is presented it is shown that the method not only overcomes the numerical instability found in the original tmm but also greatly improves the scalability of computation the new improved tmm has no extra cost of computing time as the length of homogeneous scattering region becom... | [['a', 'new', 'improved', 'transfer', 'matrix', 'method', 'tmm', 'is', 'presented', 'it', 'is', 'shown', 'that', 'the', 'method', 'not', 'only', 'overcomes', 'the', 'numerical', 'instability', 'found', 'in', 'the', 'original', 'tmm', 'but', 'also', 'greatly', 'improves', 'the', 'scalability', 'of', 'computation', 'the'... | [-0.10097787132671772, 0.04286928340279234, -0.09931199936172327, 0.0684679849132991, -0.061175163787526965, -0.14071436469347623, 0.02045612705226701, 0.36970548561583155, -0.24261557014706808, -0.2972250524908304, 0.07640838664090739, -0.25023782236549336, -0.18355611303092864, 0.2598209513399081, -0.0209885680636104... |
709.3682 | The Vcirc-sigma0 Relation of Galaxies | Courteau et al. (2007a) reported on the dependence of the ratio of a galaxy's
maximum circular velocity, Vcirc, to its central velocity dispersion, sigma0,
on morphology, or equivalently total light concentration. This Vcirc-sigma0
concentration relation, which involves details about the local and global
galaxy physi... | astro-ph | courteau et al 2007a reported on the dependence of the ratio of a galaxys maximum circular velocity vcirc to its central velocity dispersion sigma0 on morphology or equivalently total light concentration this vcircsigma0 concentration relation which involves details about the local and global galaxy physics poses a fun... | [['courteau', 'et', 'al', '2007a', 'reported', 'on', 'the', 'dependence', 'of', 'the', 'ratio', 'of', 'a', 'galaxys', 'maximum', 'circular', 'velocity', 'vcirc', 'to', 'its', 'central', 'velocity', 'dispersion', 'sigma0', 'on', 'morphology', 'or', 'equivalently', 'total', 'light', 'concentration', 'this', 'vcircsigma0'... | [-0.07186572923738924, 0.07580030811260696, -0.11058816212850313, 0.09632135691882232, -0.15576644395305603, -0.0900787594054472, 0.06412578246521729, 0.38518263965293215, -0.2100656131817097, -0.3790974689526828, 0.047222763976875554, -0.2840175894951379, -0.09462447194750388, 0.20451215111124502, -0.03128044162790670... |
709.3683 | Comparative study of nonlinear properties of EEG signals of a normal
person and an epileptic patient | Background: Investigation of the functioning of the brain in living systems
has been a major effort amongst scientists and medical practitioners. Amongst
the various disorder of the brain, epilepsy has drawn the most attention
because this disorder can affect the quality of life of a person. In this paper
we have rei... | physics.med-ph physics.data-an | background investigation of the functioning of the brain in living systems has been a major effort amongst scientists and medical practitioners amongst the various disorder of the brain epilepsy has drawn the most attention because this disorder can affect the quality of life of a person in this paper we have reinvesti... | [['background', 'investigation', 'of', 'the', 'functioning', 'of', 'the', 'brain', 'in', 'living', 'systems', 'has', 'been', 'a', 'major', 'effort', 'amongst', 'scientists', 'and', 'medical', 'practitioners', 'amongst', 'the', 'various', 'disorder', 'of', 'the', 'brain', 'epilepsy', 'has', 'drawn', 'the', 'most', 'atte... | [-0.05762681381460792, 0.11619631006553825, -0.10292609152063693, 0.08302527917933505, -0.06169421928416758, -0.14543001743785422, 0.019315397739089992, 0.4132936258561089, -0.16893853048565413, -0.2593585355805421, 0.06738560682765012, -0.2986044052287663, -0.27763795359978677, 0.23641105568775514, -0.1477066009719813... |
709.3684 | Hawking Radiation of Black p-Branes from Gravitational Anomaly | We investigate the Hawking radiation of black $p$-branes of superstring
theories using the method of anomaly cancelation, specially, we use the method
of [S. Iso, H. Umetsu and F. Wilczek, {\sl Phys. Rev. Lett.} {\bf 96}, 151302
(2006); {\sl Phys. Rev. D} {\bf 74}, 044017 (2006)]. The metrics of black
$p$-branes are ... | hep-th | we investigate the hawking radiation of black pbranes of superstring theories using the method of anomaly cancelation specially we use the method of s iso h umetsu and f wilczek sl phys rev lett bf 96 151302 2006 sl phys rev d bf 74 044017 2006 the metrics of black pbranes are spherically symmetric but not the schwarzs... | [['we', 'investigate', 'the', 'hawking', 'radiation', 'of', 'black', 'pbranes', 'of', 'superstring', 'theories', 'using', 'the', 'method', 'of', 'anomaly', 'cancelation', 'specially', 'we', 'use', 'the', 'method', 'of', 's', 'iso', 'h', 'umetsu', 'and', 'f', 'wilczek', 'sl', 'phys', 'rev', 'lett', 'bf', '96', '151302',... | [-0.11827209579620372, 0.07172547391167393, -0.04592921439885955, 0.024134886720114285, -0.11310915044612355, -0.11547370868286601, 0.03385663802080132, 0.3188991211216759, -0.12137269254200402, -0.28978198966080393, 0.0014866125968250412, -0.3139573774472983, -0.13553435362323565, 0.13855426013469696, -0.0954679759909... |
709.3685 | The Spin Density Matrix II: Application to a system of two quantum dots | This work is a sequel to our work "The Spin Density Matrix I: General Theory
and Exact Master Equations" (eprint arXiv:0708.0644 [cond-mat]). Here we
compare pure- and pseudo-spin dynamics using as an example a system of two
quantum dots, a pair of localized conduction-band electrons in an n-doped GaAs
semiconductor.... | cond-mat.str-el quant-ph | this work is a sequel to our work the spin density matrix i general theory and exact master equations eprint arxiv07080644 condmat here we compare pure and pseudospin dynamics using as an example a system of two quantum dots a pair of localized conductionband electrons in an ndoped gaas semiconductor purespin dynamics ... | [['this', 'work', 'is', 'a', 'sequel', 'to', 'our', 'work', 'the', 'spin', 'density', 'matrix', 'i', 'general', 'theory', 'and', 'exact', 'master', 'equations', 'eprint', 'arxiv07080644', 'condmat', 'here', 'we', 'compare', 'pure', 'and', 'pseudospin', 'dynamics', 'using', 'as', 'an', 'example', 'a', 'system', 'of', 't... | [-0.16193181869287057, 0.18334011865235084, -0.030772110655551473, 0.0549527658614376, -0.02969837372063769, -0.13109857002768963, 0.00934219287890771, 0.35598989401832437, -0.21385627279470643, -0.32635148061163183, -0.02170952343374859, -0.2739407219180391, -0.14142872778275634, 0.16439849570590095, 0.005018221421570... |
709.3686 | Curvature estimates for minimal submanifolds of higher codimension | We derive curvature estimates for minimal submanifolds in Euclidean space for
arbitrary dimension and codimension via Gauss map. Thus, Schoen-Simon-Yau's
results and Ecker-Huisken's results are generalized to higher codimension. In
this way we improve Hildebrandt-Jost-Widman's result for the Bernstein type
theorem.
| math.DG | we derive curvature estimates for minimal submanifolds in euclidean space for arbitrary dimension and codimension via gauss map thus schoensimonyaus results and eckerhuiskens results are generalized to higher codimension in this way we improve hildebrandtjostwidmans result for the bernstein type theorem | [['we', 'derive', 'curvature', 'estimates', 'for', 'minimal', 'submanifolds', 'in', 'euclidean', 'space', 'for', 'arbitrary', 'dimension', 'and', 'codimension', 'via', 'gauss', 'map', 'thus', 'schoensimonyaus', 'results', 'and', 'eckerhuiskens', 'results', 'are', 'generalized', 'to', 'higher', 'codimension', 'in', 'thi... | [-0.08859717891563808, 0.05255680867029648, -0.034122749770942484, 0.11797988282112208, -0.08680417892327041, -0.14352343260849776, -0.00890675657673886, 0.3223356892428312, -0.21556410433013776, -0.22192094857363323, 0.1031125245162433, -0.21962239509938578, -0.16983199162457727, 0.27680048415755953, -0.17564227079090... |
709.3687 | Nonlinear Dynamics of the Parker Scenario for Coronal Heating | The Parker or field line tangling model of coronal heating is studied
comprehensively via long-time high-resolution simulations of the dynamics of a
coronal loop in cartesian geometry within the framework of reduced
magnetohydrodynamics (RMHD). Slow photospheric motions induce a Poynting flux
which saturates by drivi... | astro-ph physics.plasm-ph physics.space-ph | the parker or field line tangling model of coronal heating is studied comprehensively via longtime highresolution simulations of the dynamics of a coronal loop in cartesian geometry within the framework of reduced magnetohydrodynamics rmhd slow photospheric motions induce a poynting flux which saturates by driving an a... | [['the', 'parker', 'or', 'field', 'line', 'tangling', 'model', 'of', 'coronal', 'heating', 'is', 'studied', 'comprehensively', 'via', 'longtime', 'highresolution', 'simulations', 'of', 'the', 'dynamics', 'of', 'a', 'coronal', 'loop', 'in', 'cartesian', 'geometry', 'within', 'the', 'framework', 'of', 'reduced', 'magneto... | [-0.15299074311466895, 0.2511784638370744, -0.0019423158483603737, 0.12569176780245797, -0.05683917036308016, -0.07843879104567923, -0.03716794058806443, 0.3775720694322187, -0.26476495127821176, -0.32894530845606146, 0.04135165202917027, -0.21981181931190288, -0.061036295304474596, 0.2422250929631317, 0.02444714088744... |
709.3688 | Some Impacts of Lorentz Violation on Cosmology | The impact of Lorentz violation on the dynamics of a scalar field is
investigated. In particular, we study the dynamics of a scalar field in the
scalar-vector-tensor theory where the vector field is constrained to be unity
and time like. By taking a generic form of the scalar field action, a
generalized dynamical equ... | hep-th | the impact of lorentz violation on the dynamics of a scalar field is investigated in particular we study the dynamics of a scalar field in the scalarvectortensor theory where the vector field is constrained to be unity and time like by taking a generic form of the scalar field action a generalized dynamical equation fo... | [['the', 'impact', 'of', 'lorentz', 'violation', 'on', 'the', 'dynamics', 'of', 'a', 'scalar', 'field', 'is', 'investigated', 'in', 'particular', 'we', 'study', 'the', 'dynamics', 'of', 'a', 'scalar', 'field', 'in', 'the', 'scalarvectortensor', 'theory', 'where', 'the', 'vector', 'field', 'is', 'constrained', 'to', 'be... | [-0.19181479563635281, 0.14933117334144566, -0.1045564979031755, 0.06707699022338014, -0.09915472407980512, -0.17030996984605878, -0.03714221120896457, 0.26442829810320306, -0.23187961382334868, -0.2649918188176611, 0.06753106409108595, -0.251775392153136, -0.1652952057432712, 0.14301975722899476, 0.05218208177065404, ... |
709.3689 | Static Deadlock Detection in MPI Synchronization Communication | It is very common to use dynamic methods to detect deadlocks in MPI programs
for the reason that static methods have some restrictions. To guarantee high
reliability of some important MPI-based application software, a model of MPI
synchronization communication is abstracted and a type of static method is
devised to e... | cs.DC | it is very common to use dynamic methods to detect deadlocks in mpi programs for the reason that static methods have some restrictions to guarantee high reliability of some important mpibased application software a model of mpi synchronization communication is abstracted and a type of static method is devised to examin... | [['it', 'is', 'very', 'common', 'to', 'use', 'dynamic', 'methods', 'to', 'detect', 'deadlocks', 'in', 'mpi', 'programs', 'for', 'the', 'reason', 'that', 'static', 'methods', 'have', 'some', 'restrictions', 'to', 'guarantee', 'high', 'reliability', 'of', 'some', 'important', 'mpibased', 'application', 'software', 'a', '... | [-0.1282635518287695, 0.00723008155068337, -0.0972752329966455, 0.11387404874180218, -0.0818961602422634, -0.24349413442370646, 0.029430097516845253, 0.3923622430393509, -0.2769404476252841, -0.3431587833972051, 0.12399985080164876, -0.22427375450748585, -0.13549350292172307, 0.20537759524350072, -0.05722334454128263, ... |
709.369 | Pioneer anomaly: a drift in the proper time of the spacecraft | A relativistic theory is proposed to explain the anomalous accelerations of
Pioneer 10/11, Galileo and Ulysses spacecrafts. The theory points out at the
limitations of the weak field approximation and proposes a drift in the proper
time of the spacecraft outside the framework of general relativity. The theory
yields ... | physics.gen-ph | a relativistic theory is proposed to explain the anomalous accelerations of pioneer 1011 galileo and ulysses spacecrafts the theory points out at the limitations of the weak field approximation and proposes a drift in the proper time of the spacecraft outside the framework of general relativity the theory yields a very... | [['a', 'relativistic', 'theory', 'is', 'proposed', 'to', 'explain', 'the', 'anomalous', 'accelerations', 'of', 'pioneer', '1011', 'galileo', 'and', 'ulysses', 'spacecrafts', 'the', 'theory', 'points', 'out', 'at', 'the', 'limitations', 'of', 'the', 'weak', 'field', 'approximation', 'and', 'proposes', 'a', 'drift', 'in'... | [-0.14067387532886771, 0.13999508892560059, -0.11692719819236173, 0.06035303415340041, -0.10527017513059721, -0.07462620283693983, 0.05490081069455232, 0.32766985952249966, -0.2520485965177871, -0.3052071945860274, 0.041997140655243986, -0.25777765954293874, -0.09931725378759125, 0.1910770475175098, -0.0824500113011314... |
709.3691 | Negative reflection in a Faraday chiral medium | The four wavenumbers associated with planewave propagation in a Faraday
chiral medium (FCM) with relatively huge magnetoelectric coupling give rise to
enhanced possibilities for negative-phase-velocity propagation and therefore
negative refraction. They can also give rise to the phenomenon of negative
reflection. In ... | physics.optics | the four wavenumbers associated with planewave propagation in a faraday chiral medium fcm with relatively huge magnetoelectric coupling give rise to enhanced possibilities for negativephasevelocity propagation and therefore negative refraction they can also give rise to the phenomenon of negative reflection in particul... | [['the', 'four', 'wavenumbers', 'associated', 'with', 'planewave', 'propagation', 'in', 'a', 'faraday', 'chiral', 'medium', 'fcm', 'with', 'relatively', 'huge', 'magnetoelectric', 'coupling', 'give', 'rise', 'to', 'enhanced', 'possibilities', 'for', 'negativephasevelocity', 'propagation', 'and', 'therefore', 'negative'... | [-0.1976268443097247, 0.25615137165980895, -0.04997448003055846, 0.025421187054456736, -0.16622373063071835, -0.11812651489020848, -0.004361973575702528, 0.4296312869140288, -0.2578990772003081, -0.26942257689902693, 0.02598807910917236, -0.2751402965769535, -0.17711195098122628, 0.20616388370896258, 0.0434538956231823... |
709.3692 | Deadlock Detection in Basic Models of MPI Synchronization Communication
Programs | A model of MPI synchronization communication programs is presented and its
three basic simplified models are also defined. A series of theorems and
methods for deciding whether deadlocks will occur among the three models are
given and proved strictly. These theories and methods for simple models'
deadlock detection a... | cs.DC | a model of mpi synchronization communication programs is presented and its three basic simplified models are also defined a series of theorems and methods for deciding whether deadlocks will occur among the three models are given and proved strictly these theories and methods for simple models deadlock detection are th... | [['a', 'model', 'of', 'mpi', 'synchronization', 'communication', 'programs', 'is', 'presented', 'and', 'its', 'three', 'basic', 'simplified', 'models', 'are', 'also', 'defined', 'a', 'series', 'of', 'theorems', 'and', 'methods', 'for', 'deciding', 'whether', 'deadlocks', 'will', 'occur', 'among', 'the', 'three', 'model... | [-0.12148064599846894, 0.053020267494011133, -0.0917315549662325, 0.11880280415501164, -0.07369635284603017, -0.23614021993400353, 0.059905378648765245, 0.40053544966972565, -0.2843058897510358, -0.3628393751364084, 0.18714264043352022, -0.21893449056214132, -0.10355765848389809, 0.24726935612687947, -0.071920719419447... |
709.3693 | Algorithm of Static Deadlock Detection in MPI Synchronization
Communication Sequential Model | Detecting deadlocks in MPI synchronization communication programs is very
difficult and need building program models. All complex models are based on
sequential models. The sequential model is mapped into a set of character
strings and its deadlock detection problem is translated into an equivalent
multi-queue string... | cs.DC | detecting deadlocks in mpi synchronization communication programs is very difficult and need building program models all complex models are based on sequential models the sequential model is mapped into a set of character strings and its deadlock detection problem is translated into an equivalent multiqueue string matc... | [['detecting', 'deadlocks', 'in', 'mpi', 'synchronization', 'communication', 'programs', 'is', 'very', 'difficult', 'and', 'need', 'building', 'program', 'models', 'all', 'complex', 'models', 'are', 'based', 'on', 'sequential', 'models', 'the', 'sequential', 'model', 'is', 'mapped', 'into', 'a', 'set', 'of', 'character... | [-0.17738980164082022, 0.028732720532279928, -0.08760671949014068, 0.11246391401509755, -0.08629650655202567, -0.2317800418729894, 0.06845939698629082, 0.3959926816634834, -0.3225496887927875, -0.3518237694585696, 0.12776309486129322, -0.21424276719801127, -0.11064419022994115, 0.16668332382570952, -0.0781134710041806,... |
709.3694 | The coupling of dynamics and molecular chemistry in galaxies | While the best tracer of the molecular component and its dynamics in galaxies
is the CO molecule, which excitation is revealed by its isotopic and
(2-1)/(1-0) ratios, the denser gas is revealed by molecules such as HCN, HNC,
HCO+ or CN, which are now widely used to probe star formation regions, or to
quantify the imp... | astro-ph | while the best tracer of the molecular component and its dynamics in galaxies is the co molecule which excitation is revealed by its isotopic and 2110 ratios the denser gas is revealed by molecules such as hcn hnc hco or cn which are now widely used to probe star formation regions or to quantify the impact of the nucle... | [['while', 'the', 'best', 'tracer', 'of', 'the', 'molecular', 'component', 'and', 'its', 'dynamics', 'in', 'galaxies', 'is', 'the', 'co', 'molecule', 'which', 'excitation', 'is', 'revealed', 'by', 'its', 'isotopic', 'and', '2110', 'ratios', 'the', 'denser', 'gas', 'is', 'revealed', 'by', 'molecules', 'such', 'as', 'hcn... | [-0.022603069994084794, 0.08433861696070147, -0.015756705830910524, 0.06179899487844003, -0.0195423804390992, -0.059430582416725566, 0.050167668433607614, 0.43119226709889075, -0.18300972048083108, -0.339029487965656, 0.044474039378167664, -0.2510569317637957, -0.06664585312736665, 0.13213011735288674, -0.0182781597539... |
709.3695 | Observations of 1ES 0647+250 and 1ES 0806+524 with VERITAS | Observations of the blazars 1ES 0647+250 and 1ES 0806+524 with VERITAS are
reported here. These objects are among the favoured candidate extragalactic
sources in the very high-energy regime due to the presence of high-energy
electrons and adequate seed photons. The presence of high-energy electrons is
established fro... | astro-ph | observations of the blazars 1es 0647250 and 1es 0806524 with veritas are reported here these objects are among the favoured candidate extragalactic sources in the very highenergy regime due to the presence of highenergy electrons and adequate seed photons the presence of highenergy electrons is established from the loc... | [['observations', 'of', 'the', 'blazars', '1es', '0647250', 'and', '1es', '0806524', 'with', 'veritas', 'are', 'reported', 'here', 'these', 'objects', 'are', 'among', 'the', 'favoured', 'candidate', 'extragalactic', 'sources', 'in', 'the', 'very', 'highenergy', 'regime', 'due', 'to', 'the', 'presence', 'of', 'highenerg... | [-0.01968879789182562, 0.16760811571601744, -0.056973485981736995, 0.17704729398675378, -0.10608099285010363, -0.08597714215105662, 0.018717954820879033, 0.453632916552386, -0.1254687589261841, -0.3969480196196883, 0.024111273526385472, -0.3265556048707568, 0.02506157942973306, 0.2629149664290524, -0.02090647295288787,... |
709.3696 | DAFNE Status and Upgrade Plans | The Frascati Phi-factory DAFNE has successfully completed experimental runs
for the three main detectors, KLOE, FINUDA and DEAR. The best peak luminosity
achieved so far is 1.6x10^32 cm-2s-1, while the best daily integrated
luminosity is 10 pb-1. At present the DAFNE team is preparing an upgrade of the
collider based... | physics.acc-ph | the frascati phifactory dafne has successfully completed experimental runs for the three main detectors kloe finuda and dear the best peak luminosity achieved so far is 16x1032 cm2s1 while the best daily integrated luminosity is 10 pb1 at present the dafne team is preparing an upgrade of the collider based on the novel... | [['the', 'frascati', 'phifactory', 'dafne', 'has', 'successfully', 'completed', 'experimental', 'runs', 'for', 'the', 'three', 'main', 'detectors', 'kloe', 'finuda', 'and', 'dear', 'the', 'best', 'peak', 'luminosity', 'achieved', 'so', 'far', 'is', '16x1032', 'cm2s1', 'while', 'the', 'best', 'daily', 'integrated', 'lum... | [-0.03617240545194013, 0.09277456381210232, -0.08647235859948468, 0.05484895708729479, -0.06330509332334061, -0.12989085597401284, -0.04123766003709556, 0.42199098444487676, -0.07704781180146678, -0.3759730668010538, 0.10875835830586995, -0.35391239627791815, 0.09623865771993816, 0.22935655899345875, 0.0048993328728540... |
709.3697 | On the harmonic oscillator on the Lobachevsky plane | We introduce the harmonic oscillator on the Lobachevsky plane with the aid of
the potential $V(r)=(a^2\omega^2/4)sinh(r/a)^2$ where $a$ is the curvature
radius and $r$ is the geodesic distance from a fixed center. Thus the potential
is rotationally symmetric and unbounded likewise as in the Euclidean case. The
eigenv... | math-ph math.MP | we introduce the harmonic oscillator on the lobachevsky plane with the aid of the potential vra2omega24sinhra2 where a is the curvature radius and r is the geodesic distance from a fixed center thus the potential is rotationally symmetric and unbounded likewise as in the euclidean case the eigenvalue equation leads to ... | [['we', 'introduce', 'the', 'harmonic', 'oscillator', 'on', 'the', 'lobachevsky', 'plane', 'with', 'the', 'aid', 'of', 'the', 'potential', 'vra2omega24sinhra2', 'where', 'a', 'is', 'the', 'curvature', 'radius', 'and', 'r', 'is', 'the', 'geodesic', 'distance', 'from', 'a', 'fixed', 'center', 'thus', 'the', 'potential', ... | [-0.1571021186883408, 0.06424603014712847, -0.08795792653072107, 0.028275494362062573, -0.07787392962476404, -0.09382629041453894, -0.026417574130552762, 0.3138026422997819, -0.2540174117665502, -0.21556478715207003, 0.10496528267188446, -0.3319044135558077, -0.1284171908038751, 0.16575587263531227, -0.0148765377912528... |
709.3698 | Miscellaneous Applications of Quons | This paper deals with quon algebras or deformed oscillator algebras, for
which the deformation parameter is a root of unity. We show the interest of
such algebras for fractional supersymmetric quantum mechanics, angular momentum
theory and quantum information. More precisely, quon algebras are used for (i)
a realizat... | quant-ph math-ph math.MP | this paper deals with quon algebras or deformed oscillator algebras for which the deformation parameter is a root of unity we show the interest of such algebras for fractional supersymmetric quantum mechanics angular momentum theory and quantum information more precisely quon algebras are used for i a realization of a ... | [['this', 'paper', 'deals', 'with', 'quon', 'algebras', 'or', 'deformed', 'oscillator', 'algebras', 'for', 'which', 'the', 'deformation', 'parameter', 'is', 'a', 'root', 'of', 'unity', 'we', 'show', 'the', 'interest', 'of', 'such', 'algebras', 'for', 'fractional', 'supersymmetric', 'quantum', 'mechanics', 'angular', 'm... | [-0.12892858287444026, 0.1356233269308168, -0.062137239308345436, 0.09052209958715346, -0.10179388750399841, -0.18457273473285396, -0.05891634613312412, 0.3225689355726584, -0.2887672805550075, -0.1492291199778769, 0.11493791052656673, -0.25479826091392205, -0.1809159530128472, 0.16344778517049063, -0.13471460992949877... |
709.3699 | Flatness-based pre-compensation of laser diodes | A physical nonlinear dynamical model of a laser diode is considered. We
propose a feed-forward control scheme based on differential flatness for the
design of input-current modulations to compensate diode distortions. The goal
is to transform without distortion a radio-frequency current modulation into a
light modula... | math.OC | a physical nonlinear dynamical model of a laser diode is considered we propose a feedforward control scheme based on differential flatness for the design of inputcurrent modulations to compensate diode distortions the goal is to transform without distortion a radiofrequency current modulation into a light modulation le... | [['a', 'physical', 'nonlinear', 'dynamical', 'model', 'of', 'a', 'laser', 'diode', 'is', 'considered', 'we', 'propose', 'a', 'feedforward', 'control', 'scheme', 'based', 'on', 'differential', 'flatness', 'for', 'the', 'design', 'of', 'inputcurrent', 'modulations', 'to', 'compensate', 'diode', 'distortions', 'the', 'goa... | [-0.15113665121136588, 0.096625797881786, -0.07467139602031851, 0.0301928805413635, -0.0870489390106516, -0.17743008169986496, 0.03409776786928264, 0.4115241028661473, -0.28491222052416354, -0.2721273533168008, 0.10515244832469067, -0.24355645516489663, -0.15134957241250224, 0.24392735580992206, -0.08825378496267865, 0... |
709.37 | Orientation dependence of the optical spectra in graphene at high
frequencies | On the basis of the Kubo formula we evaluated the optical conductivity of a
graphene sheet. The full behavior of frequency as well as temperature
dependence of the optical conductivity is presented. We show that the
anisotropy of conductivity can be significantly enhanced at high frequencies.
The photon absorption de... | cond-mat.mes-hall | on the basis of the kubo formula we evaluated the optical conductivity of a graphene sheet the full behavior of frequency as well as temperature dependence of the optical conductivity is presented we show that the anisotropy of conductivity can be significantly enhanced at high frequencies the photon absorption depends... | [['on', 'the', 'basis', 'of', 'the', 'kubo', 'formula', 'we', 'evaluated', 'the', 'optical', 'conductivity', 'of', 'a', 'graphene', 'sheet', 'the', 'full', 'behavior', 'of', 'frequency', 'as', 'well', 'as', 'temperature', 'dependence', 'of', 'the', 'optical', 'conductivity', 'is', 'presented', 'we', 'show', 'that', 'th... | [-0.1611383998560371, 0.1699355075567719, -0.04467228747093837, -0.015138158008619744, -0.06729870459965949, -0.09097049596456398, 0.04203063997489805, 0.44610892808534036, -0.284830228951653, -0.23856026137546274, 0.06488522915578383, -0.2870149675842005, -0.0807449804007552, 0.2393229222707166, 0.041521000767389724, ... |
709.3701 | Controlled coupling of counterpropagating whispering-gallery modes by a
single Rayleigh scatterer: a classical problem in a quantum optical light | We present experiments where a single subwavelength scatterer is used to
examine and control the back-scattering induced coupling between
counterpropagating high-Q modes of a microsphere resonator. Our measurements
reveal the standing wave character of the resulting symmetric and antisymmetric
eigenmodes, their unbal... | quant-ph | we present experiments where a single subwavelength scatterer is used to examine and control the backscattering induced coupling between counterpropagating highq modes of a microsphere resonator our measurements reveal the standing wave character of the resulting symmetric and antisymmetric eigenmodes their unbalanced ... | [['we', 'present', 'experiments', 'where', 'a', 'single', 'subwavelength', 'scatterer', 'is', 'used', 'to', 'examine', 'and', 'control', 'the', 'backscattering', 'induced', 'coupling', 'between', 'counterpropagating', 'highq', 'modes', 'of', 'a', 'microsphere', 'resonator', 'our', 'measurements', 'reveal', 'the', 'stan... | [-0.17372640417042104, 0.16839501148017197, -0.09605484643902679, 0.03915173230335939, -0.08195397780917875, -0.14505797032532947, 0.0389741653177355, 0.3961054648381549, -0.25924887382969647, -0.25959145692600444, 0.02100643930448727, -0.2650621420183739, -0.18282973056949384, 0.18278380181918574, 0.03346412907529912,... |
709.3702 | The Chow rings of the algebraic groups E_6, E_7, and E_8 | We determine the Chow rings of the complex algebraic groups of the
exceptional type E_6, E_7, and E_8, giving the explicit generators represented
by the pull-back images of Schubert varieties of the corresponding flag
varieties. This is a continuation of the work of R. Marlin on the computation
of the Chow rings of S... | math.AT math.AG | we determine the chow rings of the complex algebraic groups of the exceptional type e_6 e_7 and e_8 giving the explicit generators represented by the pullback images of schubert varieties of the corresponding flag varieties this is a continuation of the work of r marlin on the computation of the chow rings of so_n spin... | [['we', 'determine', 'the', 'chow', 'rings', 'of', 'the', 'complex', 'algebraic', 'groups', 'of', 'the', 'exceptional', 'type', 'e_6', 'e_7', 'and', 'e_8', 'giving', 'the', 'explicit', 'generators', 'represented', 'by', 'the', 'pullback', 'images', 'of', 'schubert', 'varieties', 'of', 'the', 'corresponding', 'flag', 'v... | [-0.21991387168566387, -0.0749808367372801, -0.10769433518250783, 0.035886050942353906, -0.13676289790620408, -0.13373094338923694, -0.00814556377629439, 0.27812089214722313, -0.29535557413473723, -0.185706738345325, 0.1416692723132049, -0.1880513442866504, -0.15409175124019384, 0.18941128640125196, -0.1903270023312264... |
709.3703 | Decay Rates for Spherical Scalar Waves in the Schwarzschild Geometry | The Cauchy problem is considered for the scalar wave equation in the
Schwarzschild geometry. Using an integral spectral representation we derive the
exact decay rate for solutions of the Cauchy problem with spherical symmetric
initial data, which is smooth and compactly supported outside the event
horizon.
| gr-qc | the cauchy problem is considered for the scalar wave equation in the schwarzschild geometry using an integral spectral representation we derive the exact decay rate for solutions of the cauchy problem with spherical symmetric initial data which is smooth and compactly supported outside the event horizon | [['the', 'cauchy', 'problem', 'is', 'considered', 'for', 'the', 'scalar', 'wave', 'equation', 'in', 'the', 'schwarzschild', 'geometry', 'using', 'an', 'integral', 'spectral', 'representation', 'we', 'derive', 'the', 'exact', 'decay', 'rate', 'for', 'solutions', 'of', 'the', 'cauchy', 'problem', 'with', 'spherical', 'sy... | [-0.13953773746185977, 0.006944842811524564, -0.10369489773723256, 0.1288483210525516, -0.12166246123935866, -0.08036119630560279, -0.10277975544981334, 0.30177651013693085, -0.2727894126386989, -0.18230209778994322, 0.19026335335144287, -0.28156988577836234, -0.08924912709904753, 0.1867339617177925, -0.005993725237203... |
709.3704 | Multiscale expansion and integrability properties of the lattice
potential KdV equation | We apply the discrete multiscale expansion to the Lax pair and to the first
few symmetries of the lattice potential Korteweg-de Vries equation. From these
calculations we show that, like the lowest order secularity conditions give a
nonlinear Schroedinger equation, the Lax pair gives at the same order the
Zakharov an... | math-ph math.MP | we apply the discrete multiscale expansion to the lax pair and to the first few symmetries of the lattice potential kortewegde vries equation from these calculations we show that like the lowest order secularity conditions give a nonlinear schroedinger equation the lax pair gives at the same order the zakharov and shab... | [['we', 'apply', 'the', 'discrete', 'multiscale', 'expansion', 'to', 'the', 'lax', 'pair', 'and', 'to', 'the', 'first', 'few', 'symmetries', 'of', 'the', 'lattice', 'potential', 'kortewegde', 'vries', 'equation', 'from', 'these', 'calculations', 'we', 'show', 'that', 'like', 'the', 'lowest', 'order', 'secularity', 'con... | [-0.11659315538903077, 0.050724562190041164, -0.0853625045535897, 0.0932209803790286, -0.13543668956549812, -0.11590118577325906, -0.05824330702855967, 0.2761766293450542, -0.3303726163517306, -0.23087051353565807, 0.06885979351574097, -0.32443569908323494, -0.1672387638979632, 0.08076305994831458, 0.060594008817081005... |
709.3705 | First Steps in Tropical Intersection Theory | We establish first parts of a tropical intersection theory. Namely, we define
cycles, Cartier divisors and intersection products between these two (without
passing to rational equivalence) and discuss push-forward and pull-back. We do
this first for fans in R^n and then for "abstract" cycles that are fans
locally. Wi... | math.AG math.CO | we establish first parts of a tropical intersection theory namely we define cycles cartier divisors and intersection products between these two without passing to rational equivalence and discuss pushforward and pullback we do this first for fans in rn and then for abstract cycles that are fans locally with regard to a... | [['we', 'establish', 'first', 'parts', 'of', 'a', 'tropical', 'intersection', 'theory', 'namely', 'we', 'define', 'cycles', 'cartier', 'divisors', 'and', 'intersection', 'products', 'between', 'these', 'two', 'without', 'passing', 'to', 'rational', 'equivalence', 'and', 'discuss', 'pushforward', 'and', 'pullback', 'we'... | [-0.19938624838418137, 0.07211532516481534, -0.08396317144498637, 0.0998286717453308, -0.044962732555115056, -0.10207035913042826, 0.06364959729867285, 0.3764119168922101, -0.3652099648822252, -0.21046315030870985, 0.1363628345417267, -0.27897218104502924, -0.20420795516429902, 0.17944694184283536, -0.18251375824991256... |
709.3706 | Static friction on the fly: velocity depinning transitions of lubricants
in motion | The dragging velocity of a model solid lubricant confined between sliding
periodic substrates exhibits a phase transition between two regimes,
respectively with quantized and with continuous lubricant center-of-mass
velocity. The transition, occurring for increasing external driving force F_ext
acting on the lubrican... | cond-mat.mtrl-sci cond-mat.other | the dragging velocity of a model solid lubricant confined between sliding periodic substrates exhibits a phase transition between two regimes respectively with quantized and with continuous lubricant centerofmass velocity the transition occurring for increasing external driving force f_ext acting on the lubricant displ... | [['the', 'dragging', 'velocity', 'of', 'a', 'model', 'solid', 'lubricant', 'confined', 'between', 'sliding', 'periodic', 'substrates', 'exhibits', 'a', 'phase', 'transition', 'between', 'two', 'regimes', 'respectively', 'with', 'quantized', 'and', 'with', 'continuous', 'lubricant', 'centerofmass', 'velocity', 'the', 't... | [-0.20361276226201847, 0.24256699696834227, -0.10017483705853664, -0.04054812118648416, -0.05143711383192284, -0.18288196707415638, 0.07391774265442577, 0.3929904867144464, -0.2558875554557709, -0.2516273740064172, 0.019085812633314613, -0.2837194117346724, -0.14871532362388465, 0.1609219299285736, 0.024934806103718656... |
709.3707 | An Invitation to Random Schroedinger operators | This review is an extended version of my mini course at the Etats de la
recherche: Operateurs de Schroedinger aleatoires at the Universite Paris 13 in
June 2002, a summer school organized by Frederic Klopp. These lecture notes try
to give some of the basics of random Schroedinger operators. They are meant for
nonspec... | math-ph math.MP | this review is an extended version of my mini course at the etats de la recherche operateurs de schroedinger aleatoires at the universite paris 13 in june 2002 a summer school organized by frederic klopp these lecture notes try to give some of the basics of random schroedinger operators they are meant for nonspecialist... | [['this', 'review', 'is', 'an', 'extended', 'version', 'of', 'my', 'mini', 'course', 'at', 'the', 'etats', 'de', 'la', 'recherche', 'operateurs', 'de', 'schroedinger', 'aleatoires', 'at', 'the', 'universite', 'paris', '13', 'in', 'june', '2002', 'a', 'summer', 'school', 'organized', 'by', 'frederic', 'klopp', 'these', ... | [-0.07641635688532215, 0.10709368755002895, -0.15611623540686337, 0.12508262024493888, -0.11779632264425835, -0.1522862189807571, -0.04289987569418139, 0.252231442482951, -0.11353172288121034, -0.34535428799258977, 0.13522290863926548, -0.32503412410807914, -0.1740074981457721, 0.13089228930095068, -0.17624908845680645... |
709.3708 | B meson excitations with chirally improved light quarks | We present our latest results for the excitations of static-light mesons on
both quenched and unquenched lattices, where the light quarks are simulated
using the chirally improved (CI) lattice Dirac operator.
| hep-lat | we present our latest results for the excitations of staticlight mesons on both quenched and unquenched lattices where the light quarks are simulated using the chirally improved ci lattice dirac operator | [['we', 'present', 'our', 'latest', 'results', 'for', 'the', 'excitations', 'of', 'staticlight', 'mesons', 'on', 'both', 'quenched', 'and', 'unquenched', 'lattices', 'where', 'the', 'light', 'quarks', 'are', 'simulated', 'using', 'the', 'chirally', 'improved', 'ci', 'lattice', 'dirac', 'operator']] | [-0.07726890078535484, 0.3069530451490033, -0.058121144741533265, 0.08686017990112305, 0.009619730089100139, -0.09241827961898619, 0.12739589139668933, 0.43990501893624184, -0.08312136295341677, -0.15513775846169842, 0.039103326102298115, -0.3763791919956284, -0.060631061393407085, 0.08069000897868987, 0.10457378562967... |
709.3709 | On vortices and solitons in Goldstone and abelian-Higgs models | In the present work we discuss non-linear physics problems such as
Nielsen-Olesen strings, superconducting bosonic straight strings and static
vortex rings. We start with a toy model. We search for antiperiodic solitons of
the Goldstone model on a circle. Such models provide the basis as well as
useful hints for furt... | hep-ph | in the present work we discuss nonlinear physics problems such as nielsenolesen strings superconducting bosonic straight strings and static vortex rings we start with a toy model we search for antiperiodic solitons of the goldstone model on a circle such models provide the basis as well as useful hints for further rese... | [['in', 'the', 'present', 'work', 'we', 'discuss', 'nonlinear', 'physics', 'problems', 'such', 'as', 'nielsenolesen', 'strings', 'superconducting', 'bosonic', 'straight', 'strings', 'and', 'static', 'vortex', 'rings', 'we', 'start', 'with', 'a', 'toy', 'model', 'we', 'search', 'for', 'antiperiodic', 'solitons', 'of', '... | [-0.11905813769202578, 0.1253429352470874, -0.07981722352717795, 0.0824499994374906, -0.07612523924606511, -0.14144665347451524, 0.0051543814560422035, 0.36776697607946734, -0.21767194294036693, -0.29200096639022544, 0.12669563556840557, -0.2591924070840395, -0.13535369889327337, 0.17779107873582473, -0.019815055374449... |
709.371 | Bidding Strategy with Forecast Technology Based on Support Vector
Machine in Electrcity Market | The participants of the electricity market concern very much the market price
evolution. Various technologies have been developed for price forecast. SVM
(Support Vector Machine) has shown its good performance in market price
forecast. Two approaches for forming the market bidding strategies based on SVM
are proposed... | q-fin.GN physics.data-an | the participants of the electricity market concern very much the market price evolution various technologies have been developed for price forecast svm support vector machine has shown its good performance in market price forecast two approaches for forming the market bidding strategies based on svm are proposed one is... | [['the', 'participants', 'of', 'the', 'electricity', 'market', 'concern', 'very', 'much', 'the', 'market', 'price', 'evolution', 'various', 'technologies', 'have', 'been', 'developed', 'for', 'price', 'forecast', 'svm', 'support', 'vector', 'machine', 'has', 'shown', 'its', 'good', 'performance', 'in', 'market', 'price... | [-0.06352208160972894, 0.010232815720601795, -0.12355496106458079, 0.12518713338367796, -0.1066245083725944, -0.18634648846712001, 0.08490038804287456, 0.4470496582846666, -0.20403766912436977, -0.26670445595896736, 0.18651060592359142, -0.31243388293330204, -0.09947697173794444, 0.21345161681169086, -0.128432457882565... |
709.3711 | Mott-Hubbard versus charge-transfer behavior in LaSrMnO4 studied via
optical conductivity | Using spectroscopic ellipsometry, we study the optical conductivity
sigma(omega) of insulating LaSrMnO4 in the energy range of 0.75-5.8 eV from 15
to 330 K. The layered structure gives rise to a pronounced anisotropy. A
multipeak structure is observed in sigma_1^a(omega) (2, 3.5, 4.5, 4.9, and 5.5
eV), while only one... | cond-mat.str-el | using spectroscopic ellipsometry we study the optical conductivity sigmaomega of insulating lasrmno4 in the energy range of 07558 ev from 15 to 330 k the layered structure gives rise to a pronounced anisotropy a multipeak structure is observed in sigma_1aomega 2 35 45 49 and 55 ev while only one peak is present at 56 e... | [['using', 'spectroscopic', 'ellipsometry', 'we', 'study', 'the', 'optical', 'conductivity', 'sigmaomega', 'of', 'insulating', 'lasrmno4', 'in', 'the', 'energy', 'range', 'of', '07558', 'ev', 'from', '15', 'to', '330', 'k', 'the', 'layered', 'structure', 'gives', 'rise', 'to', 'a', 'pronounced', 'anisotropy', 'a', 'mul... | [-0.125256043026819, 0.17637588005203342, -0.0011181799977553958, 0.05561383618295541, -0.03031822885767147, -0.12308741025517944, 0.1278824992613787, 0.3972754656900706, -0.2653877245577538, -0.37757297080908886, -0.012507935830098413, -0.3292012009878393, -0.05264868493421105, 0.11531485579337142, 0.09098574540900349... |
709.3712 | Long term hard X-ray variability of the anomalous X-ray pulsar 1RXS
J170849.0-400910 discovered with INTEGRAL | We report on a multi-band high-energy observing campaign aimed at studying
the long term spectral variability of the Anomalous X-ray Pulsar (AXP) 1RXS
J170849.0-400910, one of the magnetar candidates. We observed 1RXS
J170849.0-400910 in Fall 2006 and Spring 2007 simultaneously with Swift/XRT, in
the 0.1-10 keV energ... | astro-ph | we report on a multiband highenergy observing campaign aimed at studying the long term spectral variability of the anomalous xray pulsar axp 1rxs j1708490400910 one of the magnetar candidates we observed 1rxs j1708490400910 in fall 2006 and spring 2007 simultaneously with swiftxrt in the 0110 kev energy range and with ... | [['we', 'report', 'on', 'a', 'multiband', 'highenergy', 'observing', 'campaign', 'aimed', 'at', 'studying', 'the', 'long', 'term', 'spectral', 'variability', 'of', 'the', 'anomalous', 'xray', 'pulsar', 'axp', '1rxs', 'j1708490400910', 'one', 'of', 'the', 'magnetar', 'candidates', 'we', 'observed', '1rxs', 'j17084904009... | [-0.057960600288974685, 0.08561206312286992, -0.07985810264078684, 0.14026303132616935, -0.14290776701153132, -0.08069694759829561, 0.08943675029499441, 0.48854170035022176, -0.18102067423345478, -0.4203022073723318, 0.13215473439461414, -0.3558003962213217, 0.0070218050837978834, 0.2605869103757332, -0.032936898290717... |
709.3713 | Existence, uniqueness and approximation for stochastic Schrodinger
equation: the Poisson case | In quantum physics, recent investigations deal with the so-called "quantum
trajectory" theory. Heuristic rules are usually used to give rise to
"stochastic Schrodinger equations" which are stochastic differential equations
of non-usual type describing the physical models. These equations pose tedious
problems in term... | math.PR math-ph math.MP quant-ph | in quantum physics recent investigations deal with the socalled quantum trajectory theory heuristic rules are usually used to give rise to stochastic schrodinger equations which are stochastic differential equations of nonusual type describing the physical models these equations pose tedious problems in terms of mathem... | [['in', 'quantum', 'physics', 'recent', 'investigations', 'deal', 'with', 'the', 'socalled', 'quantum', 'trajectory', 'theory', 'heuristic', 'rules', 'are', 'usually', 'used', 'to', 'give', 'rise', 'to', 'stochastic', 'schrodinger', 'equations', 'which', 'are', 'stochastic', 'differential', 'equations', 'of', 'nonusual... | [-0.10766404817394655, 0.03321049292571843, -0.10191065432094358, 0.10811877121109162, -0.12692343668434128, -0.15152661231796033, 0.006875779578092925, 0.27257523755542934, -0.29183790766120216, -0.2655637861984172, 0.11824330748942007, -0.24316779029523505, -0.1932279263374171, 0.18155464157662837, -0.099710233734342... |
709.3714 | Quasinormal Modes and Late-Time Tails of Canonical Acoustic Black Holes | In this paper, we investigate the evolution of classical wave propagation in
the canonical acoustic black hole by numerical method and discuss the details
of tail phenomenon. The oscillating frequency and damping time scale both
increase with the angular momentum $l$. For the lower $l$, numerical results
show the low... | gr-qc | in this paper we investigate the evolution of classical wave propagation in the canonical acoustic black hole by numerical method and discuss the details of tail phenomenon the oscillating frequency and damping time scale both increase with the angular momentum l for the lower l numerical results show the lowest wkb ap... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'evolution', 'of', 'classical', 'wave', 'propagation', 'in', 'the', 'canonical', 'acoustic', 'black', 'hole', 'by', 'numerical', 'method', 'and', 'discuss', 'the', 'details', 'of', 'tail', 'phenomenon', 'the', 'oscillating', 'frequency', 'and', 'damping', 'time', 'sc... | [-0.15113260871611345, 0.13112649323347098, -0.07954197860537814, 0.09868784706132153, -0.0884159765421198, -0.0762600212392266, 0.04244145229369259, 0.33855550967825526, -0.2571862391032016, -0.30412950030026525, 0.0775441905813447, -0.23505525805581456, -0.12648424339026976, 0.21989436552692682, 0.000515350746214748,... |
709.3715 | Criteria for homotopic maps to be so along monotone homotopies | The state spaces of machines admit the structure of time. A homotopy theory
respecting this additional structure can detect machine behavior unseen by
classical homotopy theory. In an attempt to bootstrap classical tools into the
world of abstract spacetime, we identify criteria for classically homotopic,
monotone ma... | math.AT | the state spaces of machines admit the structure of time a homotopy theory respecting this additional structure can detect machine behavior unseen by classical homotopy theory in an attempt to bootstrap classical tools into the world of abstract spacetime we identify criteria for classically homotopic monotone maps of ... | [['the', 'state', 'spaces', 'of', 'machines', 'admit', 'the', 'structure', 'of', 'time', 'a', 'homotopy', 'theory', 'respecting', 'this', 'additional', 'structure', 'can', 'detect', 'machine', 'behavior', 'unseen', 'by', 'classical', 'homotopy', 'theory', 'in', 'an', 'attempt', 'to', 'bootstrap', 'classical', 'tools', ... | [-0.1578956385844827, 0.08972560855084642, -0.10562071515661146, 0.11242216306014194, -0.13849771755437057, -0.1845880649259521, 0.03890917482333155, 0.41925365465382736, -0.3678815011866391, -0.20333363017998635, 0.11107278921020527, -0.24041609646648995, -0.15531629767372376, 0.16318316988828074, -0.1418067722167406,... |
709.3716 | Numerical Improvement of the Discrete Element Method applied to Shear of
Granular Media | We present a detailed analysis of the bounds on the integration step in
Discrete Element Method (DEM) for simulating collisions and shearing of
granular assemblies. We show that, in the numerical scheme, the upper limit for
the integration step, usually taken from the average time $t_c$ of one contact,
is in fact not... | cond-mat.mtrl-sci | we present a detailed analysis of the bounds on the integration step in discrete element method dem for simulating collisions and shearing of granular assemblies we show that in the numerical scheme the upper limit for the integration step usually taken from the average time t_c of one contact is in fact not sufficient... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'the', 'bounds', 'on', 'the', 'integration', 'step', 'in', 'discrete', 'element', 'method', 'dem', 'for', 'simulating', 'collisions', 'and', 'shearing', 'of', 'granular', 'assemblies', 'we', 'show', 'that', 'in', 'the', 'numerical', 'scheme', 'the', 'upper', 'limit'... | [-0.0853842196069778, 0.09988625165586258, -0.11048861148376618, 0.07363700590400596, -0.01324613117462685, -0.07099298973222293, 0.06371477829769344, 0.3578436727290072, -0.23467218994553532, -0.2969038049810596, 0.11984644802625201, -0.24232632614251587, -0.11252049583614984, 0.23499008258729573, 0.004568183400307691... |
709.3717 | Fermions with spin 1/2 as global SO(3) vortices | In this paper we show that the nontrivial fundamental group $\pi_1 SO(3)
={\Bbb Z}_2$ for the group SO(3) of global proper rotations of a
four-dimensional Euclidian space (when a spin structure is introduced
preliminarily in that space) implies always fermions as global SO(3) vortices,
while bosons can be reduced to ... | hep-th gr-qc | in this paper we show that the nontrivial fundamental group pi_1 so3 bbb z_2 for the group so3 of global proper rotations of a fourdimensional euclidian space when a spin structure is introduced preliminarily in that space implies always fermions as global so3 vortices while bosons can be reduced to trivial lines contr... | [['in', 'this', 'paper', 'we', 'show', 'that', 'the', 'nontrivial', 'fundamental', 'group', 'pi_1', 'so3', 'bbb', 'z_2', 'for', 'the', 'group', 'so3', 'of', 'global', 'proper', 'rotations', 'of', 'a', 'fourdimensional', 'euclidian', 'space', 'when', 'a', 'spin', 'structure', 'is', 'introduced', 'preliminarily', 'in', '... | [-0.21210732753770273, 0.21344002108776666, -0.07141708771957726, 0.05095995040076067, -0.11137788052685925, -0.09005110239090978, -0.0004249358164207613, 0.3909861046637668, -0.2632953699708718, -0.1729848852197899, 0.11421189308510024, -0.19193910532554642, -0.14492290364731042, 0.12225599119775608, -0.06586552339560... |
709.3718 | Electronic correlations and disorder in transport through
one-dimensional nanoparticle arrays | We analyze and clarify the transport properties of a one-dimensional metallic
nanoparticle array with interaction between charges restricted to charges
placed in the same conductor. We study the threshold voltage, the I-V curves
and the potential drop through the array and their dependence on the array
parameters inc... | cond-mat.mes-hall cond-mat.str-el | we analyze and clarify the transport properties of a onedimensional metallic nanoparticle array with interaction between charges restricted to charges placed in the same conductor we study the threshold voltage the iv curves and the potential drop through the array and their dependence on the array parameters including... | [['we', 'analyze', 'and', 'clarify', 'the', 'transport', 'properties', 'of', 'a', 'onedimensional', 'metallic', 'nanoparticle', 'array', 'with', 'interaction', 'between', 'charges', 'restricted', 'to', 'charges', 'placed', 'in', 'the', 'same', 'conductor', 'we', 'study', 'the', 'threshold', 'voltage', 'the', 'iv', 'cur... | [-0.14600266336958903, 0.12355386236539254, -0.04803567505381906, -0.0008863020965901131, -0.023763661119095884, -0.16179788388455144, 0.09800559406479199, 0.4096002841057877, -0.26080156093797624, -0.31252254535241103, 0.07376192822210634, -0.2990922562372035, -0.12140997244195881, 0.2068908036020823, -0.0078622944927... |
709.3719 | Implementation of the Random Forest Method for the Imaging Atmospheric
Cherenkov Telescope MAGIC | The paper describes an application of the tree classification method Random
Forest (RF), as used in the analysis of data from the ground-based gamma
telescope MAGIC. In such telescopes, cosmic gamma-rays are observed and have to
be discriminated against a dominating background of hadronic cosmic-ray
particles. We des... | astro-ph | the paper describes an application of the tree classification method random forest rf as used in the analysis of data from the groundbased gamma telescope magic in such telescopes cosmic gammarays are observed and have to be discriminated against a dominating background of hadronic cosmicray particles we describe the a... | [['the', 'paper', 'describes', 'an', 'application', 'of', 'the', 'tree', 'classification', 'method', 'random', 'forest', 'rf', 'as', 'used', 'in', 'the', 'analysis', 'of', 'data', 'from', 'the', 'groundbased', 'gamma', 'telescope', 'magic', 'in', 'such', 'telescopes', 'cosmic', 'gammarays', 'are', 'observed', 'and', 'h... | [-0.047428832813581026, 0.11530465778628465, -0.05876801292052363, 0.08972784535069535, -0.0598293521284762, -0.12049986416990362, 0.027489123452168952, 0.4147115540091354, -0.224539302916515, -0.32415508438134566, 0.0916236710358909, -0.2768129241459145, -0.11646438343911478, 0.2870535975838504, -0.041404077100871815,... |
709.372 | Magnetoresistance in an all-manganite heterostructure | We study the magnetic and transport properties of all-manganite
heterostructures consisting of ferromagnetic metallic electrodes separated by
an antiferromagnetic barrier. We find that the magnetic ordering in the barrier
is influenced by the relative orientation of the electrodes magnetization
producing a large diff... | cond-mat.str-el cond-mat.mtrl-sci | we study the magnetic and transport properties of allmanganite heterostructures consisting of ferromagnetic metallic electrodes separated by an antiferromagnetic barrier we find that the magnetic ordering in the barrier is influenced by the relative orientation of the electrodes magnetization producing a large differen... | [['we', 'study', 'the', 'magnetic', 'and', 'transport', 'properties', 'of', 'allmanganite', 'heterostructures', 'consisting', 'of', 'ferromagnetic', 'metallic', 'electrodes', 'separated', 'by', 'an', 'antiferromagnetic', 'barrier', 'we', 'find', 'that', 'the', 'magnetic', 'ordering', 'in', 'the', 'barrier', 'is', 'infl... | [-0.25796790864052516, 0.19534683362767932, 0.025964773739022867, -0.020062315775014994, -0.024791542144625315, -0.10129256843190108, 0.04416021168996979, 0.4285323940217495, -0.2903265680652112, -0.3473329920587795, -0.06317409707865279, -0.26711236451353343, -0.08881059853093964, 0.19335672128945589, 0.07067312223038... |
709.3721 | Millimeter observations of HCM6A, a gravitationally lensed Lyman alpha
emitting galaxy at z=6.56 | The gravitationally lensed Lyman-alpha emitting galaxy, HCM6A, detected by Hu
et al. (2002) at z=6.56 behind the Abell 370 cluster was observed with the
MAMBO-2 array of bolometers at 1.2mm wavelength. The galaxy was not detected
down to 1.08 mJy (3 sigma), but the depth of the observations and the lens
amplification... | astro-ph | the gravitationally lensed lymanalpha emitting galaxy hcm6a detected by hu et al 2002 at z656 behind the abell 370 cluster was observed with the mambo2 array of bolometers at 12mm wavelength the galaxy was not detected down to 108 mjy 3 sigma but the depth of the observations and the lens amplification allow us to impr... | [['the', 'gravitationally', 'lensed', 'lymanalpha', 'emitting', 'galaxy', 'hcm6a', 'detected', 'by', 'hu', 'et', 'al', '2002', 'at', 'z656', 'behind', 'the', 'abell', '370', 'cluster', 'was', 'observed', 'with', 'the', 'mambo2', 'array', 'of', 'bolometers', 'at', '12mm', 'wavelength', 'the', 'galaxy', 'was', 'not', 'de... | [0.00015349226827637697, 0.0692063321006665, -0.023183381656566873, 0.09662138007339448, -0.10563740239609988, -0.04500866885511921, 0.04499634547914283, 0.46911089059610206, -0.019485648764739148, -0.3736659583802789, 0.031014871124707265, -0.3122317993189566, 0.06374839771365842, 0.1998153049909235, 0.001658813704032... |
709.3722 | Substructures in lens galaxies: PG1115+080 and B1555+375, two fold
configurations | We study the anomalous flux ratio which is observed in some four-image lens
systems, where the source lies close to a fold caustic. In this case two of the
images are close to the critical curve and their flux ratio should be equal to
unity, instead in several cases the observed value differs significantly. The
most ... | astro-ph | we study the anomalous flux ratio which is observed in some fourimage lens systems where the source lies close to a fold caustic in this case two of the images are close to the critical curve and their flux ratio should be equal to unity instead in several cases the observed value differs significantly the most plausib... | [['we', 'study', 'the', 'anomalous', 'flux', 'ratio', 'which', 'is', 'observed', 'in', 'some', 'fourimage', 'lens', 'systems', 'where', 'the', 'source', 'lies', 'close', 'to', 'a', 'fold', 'caustic', 'in', 'this', 'case', 'two', 'of', 'the', 'images', 'are', 'close', 'to', 'the', 'critical', 'curve', 'and', 'their', 'f... | [-0.1340614070684941, 0.08599320449468167, -0.035515502433464005, 0.11853349253139112, -0.039851772911679836, -0.12974390256176913, 0.001134655517132128, 0.36223200097012875, -0.18378475089314214, -0.3744726573297782, 0.08581973527979792, -0.2908087495774661, -0.07350062159115514, 0.193441961788855, -0.0224962880538396... |
709.3723 | Pulsating travelling fronts: Asymptotics and homogenization regimes | This paper is concerned with some nonlinear propagation phenomena for
reaction-advection-diffusion equations with Kolmogrov-Petrovsky-Piskunov (KPP)
type nonlinearities in general periodic domains or in infinite cylinders with
oscillating boundaries. Having a variational formula for the minimal speed of
propagation i... | math.AP | this paper is concerned with some nonlinear propagation phenomena for reactionadvectiondiffusion equations with kolmogrovpetrovskypiskunov kpp type nonlinearities in general periodic domains or in infinite cylinders with oscillating boundaries having a variational formula for the minimal speed of propagation involving ... | [['this', 'paper', 'is', 'concerned', 'with', 'some', 'nonlinear', 'propagation', 'phenomena', 'for', 'reactionadvectiondiffusion', 'equations', 'with', 'kolmogrovpetrovskypiskunov', 'kpp', 'type', 'nonlinearities', 'in', 'general', 'periodic', 'domains', 'or', 'in', 'infinite', 'cylinders', 'with', 'oscillating', 'bou... | [-0.16220412577178833, 0.10742606219188883, -0.015819148438976745, 0.05637922649907138, -0.057457802138464936, -0.08504649432044539, 0.01660373550346437, 0.32173960936311, -0.28637118812776724, -0.2484690729766429, 0.12140886380112241, -0.2797004956973054, -0.1587969006248355, 0.20237689648194523, -0.06350472403129846,... |
709.3724 | Effect of the long-range interaction in transport through
one-dimensional nanoparticle arrays | We analyze the effect of the long-range interaction on the transport
properties through ordered and disordered one-dimensional metallic nanoparticle
arrays. We discuss how the threshold voltage, the I-V curves and the voltage
drop through the array are modified as compared to the case in which
interactions are restri... | cond-mat.mes-hall cond-mat.str-el | we analyze the effect of the longrange interaction on the transport properties through ordered and disordered onedimensional metallic nanoparticle arrays we discuss how the threshold voltage the iv curves and the voltage drop through the array are modified as compared to the case in which interactions are restricted to... | [['we', 'analyze', 'the', 'effect', 'of', 'the', 'longrange', 'interaction', 'on', 'the', 'transport', 'properties', 'through', 'ordered', 'and', 'disordered', 'onedimensional', 'metallic', 'nanoparticle', 'arrays', 'we', 'discuss', 'how', 'the', 'threshold', 'voltage', 'the', 'iv', 'curves', 'and', 'the', 'voltage', '... | [-0.15509665771241998, 0.19664842823840445, -0.024212184265707037, 0.06968811645492679, 0.013834955820129835, -0.14218263483053306, 0.05094792439194862, 0.4105797653173795, -0.2517813413942349, -0.30670693164574914, 0.022924392582353903, -0.3786090497960686, -0.1387252955173608, 0.12596886209576041, 0.03036145926944300... |
709.3725 | Tsunami generation by dynamic displacement of sea bed due to dip-slip
faulting | In classical tsunami-generation techniques, one neglects the dynamic sea bed
displacement resulting from fracturing of a seismic fault. The present study
takes into account these dynamic effects. Earth's crust is assumed to be a
Kelvin-Voigt material. The seismic source is assumed to be a dislocation in a
viscoelasti... | physics.ao-ph physics.comp-ph physics.flu-dyn physics.geo-ph | in classical tsunamigeneration techniques one neglects the dynamic sea bed displacement resulting from fracturing of a seismic fault the present study takes into account these dynamic effects earths crust is assumed to be a kelvinvoigt material the seismic source is assumed to be a dislocation in a viscoelastic medium ... | [['in', 'classical', 'tsunamigeneration', 'techniques', 'one', 'neglects', 'the', 'dynamic', 'sea', 'bed', 'displacement', 'resulting', 'from', 'fracturing', 'of', 'a', 'seismic', 'fault', 'the', 'present', 'study', 'takes', 'into', 'account', 'these', 'dynamic', 'effects', 'earths', 'crust', 'is', 'assumed', 'to', 'be... | [-0.1213954880306151, 0.13086875867246922, -0.11938174177307338, 0.08593818568212466, -0.07052421043997845, -0.0804033274020571, -0.023664984903586782, 0.3223018267447442, -0.2783275544643402, -0.2756176464325559, 0.10371000328785286, -0.2581227057390904, -0.16850648608998256, 0.19292040844241867, -0.02025221695348752,... |
709.3726 | Higgs-Boson Mass Limit within the Randall-Sundrum Model | Perturbative unitarity for $\wlwl$ scattering is discussed within the
Randall-Sundrum model. It is shown that the exchange of massive 4D Kaluza-Klein
gravitons leads to amplitudes growing linearly with the CM energy squared.
Summing over KK gravitons up to a scale $\lbar$ and testing unitarity at
$\rts=\lbar$, one fi... | hep-ph | perturbative unitarity for wlwl scattering is discussed within the randallsundrum model it is shown that the exchange of massive 4d kaluzaklein gravitons leads to amplitudes growing linearly with the cm energy squared summing over kk gravitons up to a scale lbar and testing unitarity at rtslbar one finds that unitarity... | [['perturbative', 'unitarity', 'for', 'wlwl', 'scattering', 'is', 'discussed', 'within', 'the', 'randallsundrum', 'model', 'it', 'is', 'shown', 'that', 'the', 'exchange', 'of', 'massive', '4d', 'kaluzaklein', 'gravitons', 'leads', 'to', 'amplitudes', 'growing', 'linearly', 'with', 'the', 'cm', 'energy', 'squared', 'sum... | [-0.10671200680676414, 0.2585225850627974, -0.07682168673518179, 0.14660819987820592, -0.07916882105014655, -0.1634629521976485, 0.03963438840109183, 0.2669131918280686, -0.20885482307274414, -0.2846483663184742, 0.07950043572697701, -0.29192414393832605, -0.00467816922748678, 0.1619204518785917, 0.04560507601262395, 0... |
709.3727 | Transdet: a matched-filter based algorithm for transit detection -
application to simulated COROT light curves | We present a matched-filter based algorithm for transit detection and its
application to simulated COROT light curves. This algorithm stems from the work
by Bord\'e, Rouan & L\'eger (2003). We describe the different steps we intend
to take to discriminate between planets and stellar companions using the three
photome... | astro-ph | we present a matchedfilter based algorithm for transit detection and its application to simulated corot light curves this algorithm stems from the work by borde rouan leger 2003 we describe the different steps we intend to take to discriminate between planets and stellar companions using the three photometric bands pro... | [['we', 'present', 'a', 'matchedfilter', 'based', 'algorithm', 'for', 'transit', 'detection', 'and', 'its', 'application', 'to', 'simulated', 'corot', 'light', 'curves', 'this', 'algorithm', 'stems', 'from', 'the', 'work', 'by', 'borde', 'rouan', 'leger', '2003', 'we', 'describe', 'the', 'different', 'steps', 'we', 'in... | [-0.07742967538846036, 0.07964691217186758, -0.13068253679407968, 0.08351744508577717, -0.12995150258971586, -0.0835686558443639, 0.12471537185160236, 0.3710688287495739, -0.19238248516081108, -0.38944489374342894, 0.0938166335884792, -0.26291896321862523, -0.18013162077663258, 0.23593466030951177, -0.11552649527891642... |
709.3728 | Coherent states and global entanglement in an N qubit system | We consider an $N$ qubit system and show that in the symmetric subspace,
$\mathbb{S}$ a state is not globally entangled, iff it is a coherent state. It
is also proven that in the orthogonal complement $\mathbb{S}_{\bot}$ all states
are globally entangled.
| quant-ph | we consider an n qubit system and show that in the symmetric subspace mathbbs a state is not globally entangled iff it is a coherent state it is also proven that in the orthogonal complement mathbbs_bot all states are globally entangled | [['we', 'consider', 'an', 'n', 'qubit', 'system', 'and', 'show', 'that', 'in', 'the', 'symmetric', 'subspace', 'mathbbs', 'a', 'state', 'is', 'not', 'globally', 'entangled', 'iff', 'it', 'is', 'a', 'coherent', 'state', 'it', 'is', 'also', 'proven', 'that', 'in', 'the', 'orthogonal', 'complement', 'mathbbs_bot', 'all', ... | [-0.20597516582347453, 0.21712305770815873, -0.07813431187532842, 0.018376833174261264, 0.03149538930738345, -0.206695889797993, -0.03875402859412134, 0.43685735370963813, -0.27243096521124244, -0.09263202282600105, 0.13069267254904843, -0.28178399717435243, -0.13158578066504562, 0.17891749520786107, -0.043245757895056... |
709.3729 | Localising the H.E.S.S. Galactic Centre point source | Observations by the H.E.S.S. system of imaging atmospheric Cherenkov
telescopes provide the most sensitive measurements of the Galactic Centre
region in the energy range 150 GeV - 30 TeV. The vicinity of the kinetic centre
of our galaxy harbours numerous objects which could potentially accelerate
particles to very hi... | astro-ph | observations by the hess system of imaging atmospheric cherenkov telescopes provide the most sensitive measurements of the galactic centre region in the energy range 150 gev 30 tev the vicinity of the kinetic centre of our galaxy harbours numerous objects which could potentially accelerate particles to very high energi... | [['observations', 'by', 'the', 'hess', 'system', 'of', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'provide', 'the', 'most', 'sensitive', 'measurements', 'of', 'the', 'galactic', 'centre', 'region', 'in', 'the', 'energy', 'range', '150', 'gev', '30', 'tev', 'the', 'vicinity', 'of', 'the', 'kinetic', 'centre', ... | [-0.06727756637195914, 0.09535269000994023, -0.0398494669757152, 0.13055907615386791, -0.12512049898452593, -0.09769561955847351, 0.07334936022795316, 0.399325347358182, -0.194544288761898, -0.4102729209251491, 0.04967211445169997, -0.32037426647598627, 0.054144565008138704, 0.2300077488035553, -0.02524886969203987, -0... |
709.373 | Interaction and ablation of fall-back disks in isolated neutron stars | An analysis of ablation processes is made for a fall-back disk with inner and
outer radii external to the neutron-star light cylinder. The calculated
ablation rate leads, with certain other assumptions, to a simple expression
relating the inner radius and mean mass per unit area of any long-lived
fall-back disk. Expr... | astro-ph | an analysis of ablation processes is made for a fallback disk with inner and outer radii external to the neutronstar light cylinder the calculated ablation rate leads with certain other assumptions to a simple expression relating the inner radius and mean mass per unit area of any longlived fallback disk expressions fo... | [['an', 'analysis', 'of', 'ablation', 'processes', 'is', 'made', 'for', 'a', 'fallback', 'disk', 'with', 'inner', 'and', 'outer', 'radii', 'external', 'to', 'the', 'neutronstar', 'light', 'cylinder', 'the', 'calculated', 'ablation', 'rate', 'leads', 'with', 'certain', 'other', 'assumptions', 'to', 'a', 'simple', 'expre... | [-0.14142123543224627, 0.16467044403382008, -0.05392547560658193, 0.09733457049834683, -0.10357698262904329, -0.10898923472209711, 0.005690054046672138, 0.4261559644864515, -0.2640265012442162, -0.32975511134348134, 0.12029381899040832, -0.24715247341299976, -0.03871796296138053, 0.2964369886263151, -0.0631404400737297... |
709.3731 | The Nature of Running Penumbral Waves Revealed | We seek to clarify the nature of running penumbral (RP) waves: are they
chromospheric trans-sunspot waves or a visual pattern of upward-propagating
waves? Full Stokes spectropolarimetric time series of the photospheric Si I
10827 \AA line and the chromospheric He I 10830 \AA multiplet were inverted
using a Milne-Eddi... | astro-ph | we seek to clarify the nature of running penumbral rp waves are they chromospheric transsunspot waves or a visual pattern of upwardpropagating waves full stokes spectropolarimetric time series of the photospheric si i 10827 aa line and the chromospheric he i 10830 aa multiplet were inverted using a milneeddington atmos... | [['we', 'seek', 'to', 'clarify', 'the', 'nature', 'of', 'running', 'penumbral', 'rp', 'waves', 'are', 'they', 'chromospheric', 'transsunspot', 'waves', 'or', 'a', 'visual', 'pattern', 'of', 'upwardpropagating', 'waves', 'full', 'stokes', 'spectropolarimetric', 'time', 'series', 'of', 'the', 'photospheric', 'si', 'i', '... | [-0.14826443546232493, 0.2055738917664284, 0.002528641566373956, 0.11682074770043768, -0.15221784737728097, -0.08528500711990465, -0.02180156538516338, 0.4813367579378845, -0.23577263173373306, -0.31382526350481543, 0.041850010522680614, -0.2699905121288098, -0.08433666035467896, 0.14919215054353974, 0.0512208866832010... |
709.3732 | Compact objects in globular clusters | Globular clusters have long been known to contain large excesses of a variety
of objects formed through dynamical processes. The past few years have seen a
dramatic increase in our knowledge about these systems.
| astro-ph | globular clusters have long been known to contain large excesses of a variety of objects formed through dynamical processes the past few years have seen a dramatic increase in our knowledge about these systems | [['globular', 'clusters', 'have', 'long', 'been', 'known', 'to', 'contain', 'large', 'excesses', 'of', 'a', 'variety', 'of', 'objects', 'formed', 'through', 'dynamical', 'processes', 'the', 'past', 'few', 'years', 'have', 'seen', 'a', 'dramatic', 'increase', 'in', 'our', 'knowledge', 'about', 'these', 'systems']] | [-0.10309126386966776, 0.09106520850978353, -0.09207830632872441, 0.07432952271226574, -0.06422333032413222, -0.010807604874785551, 0.019014990943319657, 0.43408558977877393, -0.23772783621269114, -0.43892038635471287, 0.10779154838596963, -0.2917980939588126, -0.09451066182159326, 0.22444072768420859, -0.0620540389243... |
709.3733 | The world-sheet description of A and B branes revisited | We give a manifest supersymmetric description of A and B branes on Kahler
manifolds using a completely local N=2 superspace formulation of the
world-sheet nonlinear sigma-model in the presence of a boundary. In particular,
we show that an N=2 superspace description of type A boundaries is possible, at
least when the ... | hep-th | we give a manifest supersymmetric description of a and b branes on kahler manifolds using a completely local n2 superspace formulation of the worldsheet nonlinear sigmamodel in the presence of a boundary in particular we show that an n2 superspace description of type a boundaries is possible at least when the backgroun... | [['we', 'give', 'a', 'manifest', 'supersymmetric', 'description', 'of', 'a', 'and', 'b', 'branes', 'on', 'kahler', 'manifolds', 'using', 'a', 'completely', 'local', 'n2', 'superspace', 'formulation', 'of', 'the', 'worldsheet', 'nonlinear', 'sigmamodel', 'in', 'the', 'presence', 'of', 'a', 'boundary', 'in', 'particular'... | [-0.14633993726998273, 0.12467333919508153, -0.06673760904404934, 0.08883766100124114, -0.0977401236846748, -0.17207216156535957, -0.0212787107252147, 0.3243953652016007, -0.20518482259317938, -0.23540130001262272, 0.11938102667030906, -0.23975923207431737, -0.20921355666648042, 0.10758258566885062, -0.1329321856472161... |
709.3734 | Hadronic decays of the tau lepton into K K pion modes within Resonance
Chiral Theory | Tau decays into hadrons have a twofold interest: On the one hand, they are a
clean environment for studying the hadronization of the left-handed current of
QCD, while, on the other side, provide relevant dynamical information of the
resonances that mediate these processes. Within an effective field theory-like
framew... | hep-ph | tau decays into hadrons have a twofold interest on the one hand they are a clean environment for studying the hadronization of the lefthanded current of qcd while on the other side provide relevant dynamical information of the resonances that mediate these processes within an effective field theorylike framework namely... | [['tau', 'decays', 'into', 'hadrons', 'have', 'a', 'twofold', 'interest', 'on', 'the', 'one', 'hand', 'they', 'are', 'a', 'clean', 'environment', 'for', 'studying', 'the', 'hadronization', 'of', 'the', 'lefthanded', 'current', 'of', 'qcd', 'while', 'on', 'the', 'other', 'side', 'provide', 'relevant', 'dynamical', 'info... | [-0.08427080844893403, 0.181120199706208, -0.1134798759351606, 0.10148467289729286, -0.06674856370638894, -0.11932372188539771, 0.05892019851497658, 0.3256014223170021, -0.20802030596558166, -0.2303663661622483, 0.04583490591637952, -0.3395885548432884, -0.07401514651213327, 0.1715563941423012, 0.0781263559712502, 0.03... |
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