id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.1049 | An Interval Analysis Based Study for the Design and the Comparison of
3-DOF Parallel Kinematic Machines | This paper addresses an interval analysis based study that is applied to the
design and the comparison of 3-DOF parallel kinematic machines. Two design
criteria are used, (i) a regular workspace shape and, (ii) a kinetostatic
performance index that needs to be as homogeneous as possible throughout the
workspace. The ... | cs.RO | this paper addresses an interval analysis based study that is applied to the design and the comparison of 3dof parallel kinematic machines two design criteria are used i a regular workspace shape and ii a kinetostatic performance index that needs to be as homogeneous as possible throughout the workspace the interval an... | [['this', 'paper', 'addresses', 'an', 'interval', 'analysis', 'based', 'study', 'that', 'is', 'applied', 'to', 'the', 'design', 'and', 'the', 'comparison', 'of', '3dof', 'parallel', 'kinematic', 'machines', 'two', 'design', 'criteria', 'are', 'used', 'i', 'a', 'regular', 'workspace', 'shape', 'and', 'ii', 'a', 'kinetos... | [-0.14469761883936308, 0.031352192839679854, -0.07040781723977677, -0.0236179494491682, -0.11024722229882047, -0.18137719294313212, -0.04435138846185572, 0.439485511087395, -0.24199283518989023, -0.29710819209315653, 0.11785942443871293, -0.22457475261441592, -0.11353989889652565, 0.19236745834350585, -0.06246281383109... |
708.105 | Pulsars: Progress, Problems and Prospects | I survey recent successes in the application of relativistic MHD and
force-free electrodynamics to the modeling of the pulsars' rotational energy
loss mechanism as well as to the structure and emission characteristics of
Pulsar Wind Nebulae. I suggest that unsteady reconnection in the current sheet
separating the clo... | astro-ph | i survey recent successes in the application of relativistic mhd and forcefree electrodynamics to the modeling of the pulsars rotational energy loss mechanism as well as to the structure and emission characteristics of pulsar wind nebulae i suggest that unsteady reconnection in the current sheet separating the closed f... | [['i', 'survey', 'recent', 'successes', 'in', 'the', 'application', 'of', 'relativistic', 'mhd', 'and', 'forcefree', 'electrodynamics', 'to', 'the', 'modeling', 'of', 'the', 'pulsars', 'rotational', 'energy', 'loss', 'mechanism', 'as', 'well', 'as', 'to', 'the', 'structure', 'and', 'emission', 'characteristics', 'of', ... | [-0.09621664412940542, 0.14767024889743577, -0.011892307200986479, 0.10064908193010423, -0.08686575383568804, -0.06682977634171645, 0.027284885065423117, 0.377709597605798, -0.25904868121362395, -0.3169796838983893, 0.07649246784289264, -0.2749061024727093, -0.040121390475995014, 0.2436114346442951, -0.0112591375442894... |
708.1051 | Deconvolution by simulation | Given samples (x_1,...,x_m) and (z_1,...,z_n) which we believe are
independent realizations of random variables X and Z respectively, where we
further believe that Z=X+Y with Y independent of X, the problem is to estimate
the distribution of Y. We present a new method for doing this, involving
simulation. Experiments... | stat.CO | given samples x_1x_m and z_1z_n which we believe are independent realizations of random variables x and z respectively where we further believe that zxy with y independent of x the problem is to estimate the distribution of y we present a new method for doing this involving simulation experiments suggest that the metho... | [['given', 'samples', 'x_1x_m', 'and', 'z_1z_n', 'which', 'we', 'believe', 'are', 'independent', 'realizations', 'of', 'random', 'variables', 'x', 'and', 'z', 'respectively', 'where', 'we', 'further', 'believe', 'that', 'zxy', 'with', 'y', 'independent', 'of', 'x', 'the', 'problem', 'is', 'to', 'estimate', 'the', 'dist... | [-0.09739262582401612, 0.10221536768533822, -0.1116345302933561, 0.005800086871853897, -0.04776611314654084, -0.14208511757897213, 0.10382778165512718, 0.4121576298826507, -0.27097033988684416, -0.25498181028524414, 0.0676504250981712, -0.2808280227306698, -0.13921635449618666, 0.22981079508151328, -0.05369394879588591... |
708.1052 | Trace Anomaly Inflation in Brane Induced Gravity | In the present letter we find that Starobinsky's inflationary solution is
also valid in the Dvali-Gabadadze-Porrati (DGP) model where a 3-brane is
embedded in 5-dimensional Minkowski bulk. We show that such a solution is
typically not supported by the Self-Accelerated branch of the model, giving
therefore a natural s... | hep-th astro-ph gr-qc | in the present letter we find that starobinskys inflationary solution is also valid in the dvaligabadadzeporrati dgp model where a 3brane is embedded in 5dimensional minkowski bulk we show that such a solution is typically not supported by the selfaccelerated branch of the model giving therefore a natural selection of ... | [['in', 'the', 'present', 'letter', 'we', 'find', 'that', 'starobinskys', 'inflationary', 'solution', 'is', 'also', 'valid', 'in', 'the', 'dvaligabadadzeporrati', 'dgp', 'model', 'where', 'a', '3brane', 'is', 'embedded', 'in', '5dimensional', 'minkowski', 'bulk', 'we', 'show', 'that', 'such', 'a', 'solution', 'is', 'ty... | [-0.15791602030298427, 0.07682296617054625, -0.11959532449316038, 0.07591207175956745, -0.12212885274110656, -0.11801832197724205, -2.089754776342919e-05, 0.26274243166768235, -0.17761937315686066, -0.23618865938563097, 0.08277844480165329, -0.27391233027569556, -0.1678427619295881, 0.11948019285490247, -0.061329359776... |
708.1053 | Spatial distribution and galactic model parameters of cataclysmic
variables | The spatial distribution, galactic model parameters and luminosity function
of cataclysmic variables (CVs) in the solar neighbourhood have been determined
from a carefully established sample of 459 CVs. The sample contains all of the
CVs with distances computed from the Period-Luminosity-Colours (PLCs) relation
of CV... | astro-ph | the spatial distribution galactic model parameters and luminosity function of cataclysmic variables cvs in the solar neighbourhood have been determined from a carefully established sample of 459 cvs the sample contains all of the cvs with distances computed from the periodluminositycolours plcs relation of cvs which ha... | [['the', 'spatial', 'distribution', 'galactic', 'model', 'parameters', 'and', 'luminosity', 'function', 'of', 'cataclysmic', 'variables', 'cvs', 'in', 'the', 'solar', 'neighbourhood', 'have', 'been', 'determined', 'from', 'a', 'carefully', 'established', 'sample', 'of', '459', 'cvs', 'the', 'sample', 'contains', 'all',... | [-0.05585853629152272, 0.12417243394758351, -0.085538000453268, 0.12133400637461679, -0.09030546839774335, -0.05242721986500188, 0.09960221518010187, 0.4019996089538416, -0.16104613768850237, -0.35656447814723763, 0.04877856540854107, -0.3411081256882216, -0.028061898631746702, 0.22730426703212567, -0.06123399866135934... |
708.1054 | Shape restricted regression with random Bernstein polynomials | Shape restricted regressions, including isotonic regression and concave
regression as special cases, are studied using priors on Bernstein polynomials
and Markov chain Monte Carlo methods. These priors have large supports, select
only smooth functions, can easily incorporate geometric information into the
prior, and ... | math.ST stat.TH | shape restricted regressions including isotonic regression and concave regression as special cases are studied using priors on bernstein polynomials and markov chain monte carlo methods these priors have large supports select only smooth functions can easily incorporate geometric information into the prior and can be g... | [['shape', 'restricted', 'regressions', 'including', 'isotonic', 'regression', 'and', 'concave', 'regression', 'as', 'special', 'cases', 'are', 'studied', 'using', 'priors', 'on', 'bernstein', 'polynomials', 'and', 'markov', 'chain', 'monte', 'carlo', 'methods', 'these', 'priors', 'have', 'large', 'supports', 'select',... | [0.009252555543097042, -0.002346530250167545, -0.09654354123705172, 0.10951548343659909, -0.14266330424601895, -0.19453507701901696, -0.003021018768224535, 0.5045291539635274, -0.2637537581554343, -0.349446311781678, 0.12949872853034, -0.24460132881892915, -0.13273345829316274, 0.2335134809925162, -0.10379455100650652,... |
708.1055 | A Catalog of New M33 Star Clusters Based on the HST/WFPC2 Images | We present the result of a survey for star clusters in M33 using the
HST/WFPC2 archive images. We have found 104 star clusters, including 32 new
ones, in the images of 24 fields that were not included in the previous
studies. Combining these with previous data in the literature, we increase the
number of M33 star clu... | astro-ph | we present the result of a survey for star clusters in m33 using the hstwfpc2 archive images we have found 104 star clusters including 32 new ones in the images of 24 fields that were not included in the previous studies combining these with previous data in the literature we increase the number of m33 star clusters fo... | [['we', 'present', 'the', 'result', 'of', 'a', 'survey', 'for', 'star', 'clusters', 'in', 'm33', 'using', 'the', 'hstwfpc2', 'archive', 'images', 'we', 'have', 'found', '104', 'star', 'clusters', 'including', '32', 'new', 'ones', 'in', 'the', 'images', 'of', '24', 'fields', 'that', 'were', 'not', 'included', 'in', 'the... | [-0.02353157210764871, 0.10446533252994128, -0.10119571667955884, 0.08367316264680472, -0.07352991153720426, -0.02469380937814956, 0.08639751242137411, 0.4849229274478169, -0.1171698203767662, -0.3977089444863202, 0.03379971887397023, -0.343427736078179, -0.011119270254401308, 0.17147047124997852, -0.08303828778008251,... |
708.1056 | Suppression of Tunneling of Superconducting Vortices Caused by a Remote
Gate: Example of an Extended Object Tunneling | We discuss a recent experiment in which the resistance of a superconducting
film has been measured in magnetic field. A strong decrease of the
superconducting film resistance has been observed when a metallic gate is
placed above the film. We study how the magnetic coupling between vortices in a
thin superconducting ... | cond-mat.supr-con | we discuss a recent experiment in which the resistance of a superconducting film has been measured in magnetic field a strong decrease of the superconducting film resistance has been observed when a metallic gate is placed above the film we study how the magnetic coupling between vortices in a thin superconducting film... | [['we', 'discuss', 'a', 'recent', 'experiment', 'in', 'which', 'the', 'resistance', 'of', 'a', 'superconducting', 'film', 'has', 'been', 'measured', 'in', 'magnetic', 'field', 'a', 'strong', 'decrease', 'of', 'the', 'superconducting', 'film', 'resistance', 'has', 'been', 'observed', 'when', 'a', 'metallic', 'gate', 'is... | [-0.20722331091212237, 0.2027762351634865, -0.04151348253789311, 0.029787457794324422, 0.006198820855451344, -0.09943167473863347, 0.06753290488549898, 0.34864080184856044, -0.25008156660446373, -0.30782658243251426, -0.020200966181950258, -0.2801563624541537, -0.10666677111025882, 0.18603091102419636, -0.0126144970640... |
708.1057 | Dpes massless QCD have vacuum energy? | It is widely thought that this question has a positive answer, but we argue
that the support for this belief from both experiment and theory is weak or
nonexistent. We then list some of the ramifications of a negative answer.
| hep-ph hep-th | it is widely thought that this question has a positive answer but we argue that the support for this belief from both experiment and theory is weak or nonexistent we then list some of the ramifications of a negative answer | [['it', 'is', 'widely', 'thought', 'that', 'this', 'question', 'has', 'a', 'positive', 'answer', 'but', 'we', 'argue', 'that', 'the', 'support', 'for', 'this', 'belief', 'from', 'both', 'experiment', 'and', 'theory', 'is', 'weak', 'or', 'nonexistent', 'we', 'then', 'list', 'some', 'of', 'the', 'ramifications', 'of', 'a... | [-0.07909545279690064, 0.10064554966520518, -0.09210538535844534, 0.1671507827937603, -0.12027262181363767, -0.1700708256335929, 0.08002102133759763, 0.3812341546174139, -0.256691343896091, -0.26246553580276666, 0.12791061063762754, -0.2793210075236857, -0.256198789580958, 0.17678597056656145, -0.043680000118911266, -0... |
708.1058 | Non- and semi-parametric analysis of failure time data with missing
failure indicators | A class of estimating functions is introduced for the regression parameter of
the Cox proportional hazards model to allow unknown failure statuses on some
study subjects. The consistency and asymptotic normality of the resulting
estimators are established under mild conditions. An adaptive estimator which
achieves th... | math.ST stat.TH | a class of estimating functions is introduced for the regression parameter of the cox proportional hazards model to allow unknown failure statuses on some study subjects the consistency and asymptotic normality of the resulting estimators are established under mild conditions an adaptive estimator which achieves the mi... | [['a', 'class', 'of', 'estimating', 'functions', 'is', 'introduced', 'for', 'the', 'regression', 'parameter', 'of', 'the', 'cox', 'proportional', 'hazards', 'model', 'to', 'allow', 'unknown', 'failure', 'statuses', 'on', 'some', 'study', 'subjects', 'the', 'consistency', 'and', 'asymptotic', 'normality', 'of', 'the', '... | [-0.052227453475720005, -0.0003329548777209742, -0.1210444557660243, 0.11948070928797518, -0.035829205578601545, -0.1438231850206329, 0.03574311542079637, 0.36917987982783335, -0.2141615370729644, -0.2616958081183073, 0.16448555973342113, -0.22150819959413065, -0.16986152864665838, 0.21166284418493314, -0.1359715580842... |
708.1059 | Two non-commutative parameters and regular cosmological phase transition
in the semi-classical dilaton cosmology | We study cosmological phase transitions from modified equations of motion by
introducing two non-commutative parameters in the Poisson brackets, which
describes the initial- and future-singularity-free phase transition in the
soluble semi-classical dilaton gravity with a non-vanishing cosmological
constant. Accelerat... | gr-qc | we study cosmological phase transitions from modified equations of motion by introducing two noncommutative parameters in the poisson brackets which describes the initial and futuresingularityfree phase transition in the soluble semiclassical dilaton gravity with a nonvanishing cosmological constant accelerated expansi... | [['we', 'study', 'cosmological', 'phase', 'transitions', 'from', 'modified', 'equations', 'of', 'motion', 'by', 'introducing', 'two', 'noncommutative', 'parameters', 'in', 'the', 'poisson', 'brackets', 'which', 'describes', 'the', 'initial', 'and', 'futuresingularityfree', 'phase', 'transition', 'in', 'the', 'soluble',... | [-0.13315961907479773, 0.2002117511141545, -0.1053236858246641, 0.0468645394991014, -0.0724943996777896, -0.12317247011405588, -0.046880475135468364, 0.3067150259286993, -0.2741569631939961, -0.2505812986648245, 0.09053994185955229, -0.23449606624328428, -0.08209880368991031, 0.10512125279099026, 0.00454651240768187, -... |
708.106 | Coherent Electron Scattering Captured by an Attosecond Quantum
Stroboscope | The basic properties of atoms, molecules and solids are governed by electron
dynamics which take place on extremely short time scales. To measure and
control these dynamics therefore requires ultrafast sources of radiation
combined with efficient detection techniques. The generation of extreme
ultraviolet (XUV) attos... | physics.atom-ph | the basic properties of atoms molecules and solids are governed by electron dynamics which take place on extremely short time scales to measure and control these dynamics therefore requires ultrafast sources of radiation combined with efficient detection techniques the generation of extreme ultraviolet xuv attosecond 1... | [['the', 'basic', 'properties', 'of', 'atoms', 'molecules', 'and', 'solids', 'are', 'governed', 'by', 'electron', 'dynamics', 'which', 'take', 'place', 'on', 'extremely', 'short', 'time', 'scales', 'to', 'measure', 'and', 'control', 'these', 'dynamics', 'therefore', 'requires', 'ultrafast', 'sources', 'of', 'radiation'... | [-0.07966541403162476, 0.20420314283304228, -0.09052568202897839, 0.07163392682134527, -0.005201787981268478, -0.14491794072942102, -0.0033475314304190072, 0.48559409072069815, -0.2591894200905205, -0.3255368415181223, 0.04588896983790054, -0.27114398855626687, -0.045574959296282365, 0.26258529882482573, -0.00596099741... |
708.1061 | Nonparametric estimation of a distribution function under biased
sampling and censoring | This paper derives the nonparametric maximum likelihood estimator (NPMLE) of
a distribution function from observations which are subject to both bias and
censoring. The NPMLE is obtained by a simple EM algorithm which is an extension
of the algorithm suggested by Vardi (Biometrika, 1989) for size biased data.
Applica... | math.ST stat.TH | this paper derives the nonparametric maximum likelihood estimator npmle of a distribution function from observations which are subject to both bias and censoring the npmle is obtained by a simple em algorithm which is an extension of the algorithm suggested by vardi biometrika 1989 for size biased data application of t... | [['this', 'paper', 'derives', 'the', 'nonparametric', 'maximum', 'likelihood', 'estimator', 'npmle', 'of', 'a', 'distribution', 'function', 'from', 'observations', 'which', 'are', 'subject', 'to', 'both', 'bias', 'and', 'censoring', 'the', 'npmle', 'is', 'obtained', 'by', 'a', 'simple', 'em', 'algorithm', 'which', 'is'... | [-0.04357331448994663, -0.046950755284593346, -0.12870411086699057, 0.0930645975442175, -0.062077144776396025, -0.14683533342683625, 0.057994642360510586, 0.3891079975185038, -0.24754599933566032, -0.31705004200553416, 0.13070553772408386, -0.26522963762754337, -0.16699755687437867, 0.21404562537269345, -0.147024252096... |
708.1062 | Controlled-NOT for multiparticle qubits and topological quantum
computation based on parity measurements | We discuss a measurement-based implementation of a controlled-NOT (CNOT)
quantum gate. Such a gate has recently been discussed for free electron qubits.
Here we extend this scheme for qubits encoded in product states of two (or
more) spins-1/2 or in equivalent systems. The key to such an extension is to
find a feasib... | cond-mat.mes-hall quant-ph | we discuss a measurementbased implementation of a controllednot cnot quantum gate such a gate has recently been discussed for free electron qubits here we extend this scheme for qubits encoded in product states of two or more spins12 or in equivalent systems the key to such an extension is to find a feasible qubitparit... | [['we', 'discuss', 'a', 'measurementbased', 'implementation', 'of', 'a', 'controllednot', 'cnot', 'quantum', 'gate', 'such', 'a', 'gate', 'has', 'recently', 'been', 'discussed', 'for', 'free', 'electron', 'qubits', 'here', 'we', 'extend', 'this', 'scheme', 'for', 'qubits', 'encoded', 'in', 'product', 'states', 'of', 't... | [-0.19097247035720752, 0.23411285552629124, 0.001990988971166579, 0.050214404933545405, 0.054775587241497954, -0.30035864512319677, 0.08761167284267556, 0.3992567601547177, -0.19770493102259934, -0.26347770832340495, 0.03130312076038016, -0.24523382236033545, -0.09081574054185435, 0.25346497189769124, -0.03918817812076... |
708.1063 | Onset of ferromagnetism in low-doped GaMnAs | We develop a quantitatively predictive theory for impurity-band
ferromagnetism in the low-doping regime of GaMnAs and compare with experimental
measurements of a series of samples whose compositions span the transition from
paramagnetic insulating to ferromagnetic conducting behavior. The theoretical
Curie temperatur... | cond-mat.mtrl-sci cond-mat.mes-hall | we develop a quantitatively predictive theory for impurityband ferromagnetism in the lowdoping regime of gamnas and compare with experimental measurements of a series of samples whose compositions span the transition from paramagnetic insulating to ferromagnetic conducting behavior the theoretical curie temperatures de... | [['we', 'develop', 'a', 'quantitatively', 'predictive', 'theory', 'for', 'impurityband', 'ferromagnetism', 'in', 'the', 'lowdoping', 'regime', 'of', 'gamnas', 'and', 'compare', 'with', 'experimental', 'measurements', 'of', 'a', 'series', 'of', 'samples', 'whose', 'compositions', 'span', 'the', 'transition', 'from', 'pa... | [-0.08412195994236248, 0.20443268984923096, -0.036950295523847224, 0.025451100752956125, 0.02782760277680564, -0.11699288568963281, 0.10577844609754526, 0.36223107344302974, -0.2232470375745267, -0.3249301763678916, 0.010261945567331392, -0.3665386445428623, -0.049424475796528346, 0.19221449147177036, 0.033024758654913... |
708.1064 | Estimating a Polya frequency function_2 | We consider the non-parametric maximum likelihood estimation in the class of
Polya frequency functions of order two, viz. the densities with a concave
logarithm. This is a subclass of unimodal densities and fairly rich in general.
The NPMLE is shown to be the solution to a convex programming problem in the
Euclidean ... | math.ST stat.TH | we consider the nonparametric maximum likelihood estimation in the class of polya frequency functions of order two viz the densities with a concave logarithm this is a subclass of unimodal densities and fairly rich in general the npmle is shown to be the solution to a convex programming problem in the euclidean space a... | [['we', 'consider', 'the', 'nonparametric', 'maximum', 'likelihood', 'estimation', 'in', 'the', 'class', 'of', 'polya', 'frequency', 'functions', 'of', 'order', 'two', 'viz', 'the', 'densities', 'with', 'a', 'concave', 'logarithm', 'this', 'is', 'a', 'subclass', 'of', 'unimodal', 'densities', 'and', 'fairly', 'rich', '... | [-0.07337926991749555, 0.006991764620614026, -0.13414045647258246, 0.12037394655267178, -0.08124727446915983, -0.13730924469536712, 0.032378565260692486, 0.39305385145582733, -0.28138068083768025, -0.2676367923688096, 0.12654770521559058, -0.24560244304799958, -0.16225826632985962, 0.138169130664083, -0.144886872206543... |
708.1065 | A super Frobenius formula for the characters of Iwahori-Hecke algebras | We establish a super Frobenius formula for the characters of Iwahori-Hecke
algebras. We show that the Hall-Littlewood sypersymmetric function, up to
constant, generates the values of the irreducible characters of Iwahori-Hecke
algebras at the elements corresponding to cycle permutations. Our formula in
this article i... | math.RT math.QA | we establish a super frobenius formula for the characters of iwahorihecke algebras we show that the halllittlewood sypersymmetric function up to constant generates the values of the irreducible characters of iwahorihecke algebras at the elements corresponding to cycle permutations our formula in this article includes b... | [['we', 'establish', 'a', 'super', 'frobenius', 'formula', 'for', 'the', 'characters', 'of', 'iwahorihecke', 'algebras', 'we', 'show', 'that', 'the', 'halllittlewood', 'sypersymmetric', 'function', 'up', 'to', 'constant', 'generates', 'the', 'values', 'of', 'the', 'irreducible', 'characters', 'of', 'iwahorihecke', 'alg... | [-0.15702674239873887, 0.087765911830568, -0.047173060083084487, 0.08043060667431828, -0.07023358090188016, -0.09395441003990444, 0.00977419382384555, 0.2886614882133224, -0.33185929344459014, -0.1986634149300781, 0.07193179600448771, -0.25970690859989687, -0.18052946542474357, 0.19387572341683237, -0.12135183661752803... |
708.1066 | Observation of the first gravitational microlensing event in a sparse
stellar field : the Tago event | We report the observation of the first gravitational microlensing event in a
sparse stellar field, involving the brightest (V=11.4 mag) andclosest (~ 1 kpc)
source star to date. This event was discovered by an amateurastronomer, A.
Tago, on 2006 October 31 as a transient brightening, by ~4.5 mag during a ~15
day peri... | astro-ph | we report the observation of the first gravitational microlensing event in a sparse stellar field involving the brightest v114 mag andclosest 1 kpc source star to date this event was discovered by an amateurastronomer a tago on 2006 october 31 as a transient brightening by 45 mag during a 15 day period of a normal atyp... | [['we', 'report', 'the', 'observation', 'of', 'the', 'first', 'gravitational', 'microlensing', 'event', 'in', 'a', 'sparse', 'stellar', 'field', 'involving', 'the', 'brightest', 'v114', 'mag', 'andclosest', '1', 'kpc', 'source', 'star', 'to', 'date', 'this', 'event', 'was', 'discovered', 'by', 'an', 'amateurastronomer'... | [-0.11247337824866377, 0.12640671321407992, -0.05713463935724183, 0.0922548958943603, -0.12350653918535524, -0.05197820830838503, 0.09959921149939702, 0.36459454892052184, -0.17610589987535433, -0.38859328696806283, 0.12946408048423158, -0.3095733843315896, -0.0820316078153917, 0.24074722408077906, -0.06970077162558162... |
708.1067 | Interacting RNA polymerase motors on DNA track: effects of traffic
congestion and intrinsic noise on RNA synthesis | RNA polymerase (RNAP) is an enzyme that synthesizes a messenger RNA (mRNA)
strand which is complementary to a single-stranded DNA template. From the
perspective of physicists, an RNAP is a molecular motor that utilizes chemical
energy input to move along the track formed by a DNA. In many circumstances,
which are des... | physics.bio-ph q-bio.BM | rna polymerase rnap is an enzyme that synthesizes a messenger rna mrna strand which is complementary to a singlestranded dna template from the perspective of physicists an rnap is a molecular motor that utilizes chemical energy input to move along the track formed by a dna in many circumstances which are described in t... | [['rna', 'polymerase', 'rnap', 'is', 'an', 'enzyme', 'that', 'synthesizes', 'a', 'messenger', 'rna', 'mrna', 'strand', 'which', 'is', 'complementary', 'to', 'a', 'singlestranded', 'dna', 'template', 'from', 'the', 'perspective', 'of', 'physicists', 'an', 'rnap', 'is', 'a', 'molecular', 'motor', 'that', 'utilizes', 'che... | [-0.10261437532565806, 0.17966638750456296, -0.04264408754690255, 0.0729052121484107, 0.007866163901621249, -0.12185011664405465, 0.09347489608463082, 0.37737878745467196, -0.3008923400102592, -0.3130602113947999, 0.01710588134620793, -0.23576350532239304, -0.18242252691444463, 0.17525022638530086, -0.0670972451840232,... |
708.1068 | Capability of multi-detector analyses on supernova neutrinos | This paper has been withdrawn by the author, due to errors in the figures.
| hep-ph | this paper has been withdrawn by the author due to errors in the figures | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'errors', 'in', 'the', 'figures']] | [-0.10006661912692445, -0.020335858754281486, -0.11206320513572011, -0.06369040657799425, -0.08331371311630521, -0.012484078029436725, 0.002345973700617573, 0.32606036961078644, -0.25192813761532307, -0.4037838280200958, 0.12276170671352052, -0.34405405739588396, -0.15419600917292492, 0.09646940763507571, -0.3588278229... |
708.1069 | A comparison of the accuracy of saddlepoint conditional cumulative
distribution function approximations | Consider a model parameterized by a scalar parameter of interest and a
nuisance parameter vector. Inference about the parameter of interest may be
based on the signed root of the likelihood ratio statistic R. The standard
normal approximation to the conditional distribution of R typically has error
of order O(n^{-1/2... | stat.ME | consider a model parameterized by a scalar parameter of interest and a nuisance parameter vector inference about the parameter of interest may be based on the signed root of the likelihood ratio statistic r the standard normal approximation to the conditional distribution of r typically has error of order on12 where n ... | [['consider', 'a', 'model', 'parameterized', 'by', 'a', 'scalar', 'parameter', 'of', 'interest', 'and', 'a', 'nuisance', 'parameter', 'vector', 'inference', 'about', 'the', 'parameter', 'of', 'interest', 'may', 'be', 'based', 'on', 'the', 'signed', 'root', 'of', 'the', 'likelihood', 'ratio', 'statistic', 'r', 'the', 's... | [-0.08598188480604355, 0.04913356883178761, -0.07776505363219213, 0.1312531458196889, -0.055859052713835476, -0.13376594923447999, 0.0696783829743054, 0.3535701879413753, -0.24180119784503448, -0.34050840978289204, 0.11723043245871029, -0.25356010405528473, -0.09627036289340339, 0.16738192445070416, -0.0422207301868716... |
708.107 | Multivariate medians and measure-symmetrization | We discuss two research areas dealing respectively with (1) a class of
multivariate medians and (2) a symmetrization algorithm for probability
measures.
| math.ST stat.TH | we discuss two research areas dealing respectively with 1 a class of multivariate medians and 2 a symmetrization algorithm for probability measures | [['we', 'discuss', 'two', 'research', 'areas', 'dealing', 'respectively', 'with', '1', 'a', 'class', 'of', 'multivariate', 'medians', 'and', '2', 'a', 'symmetrization', 'algorithm', 'for', 'probability', 'measures']] | [-0.10734411569269882, 0.07024879300628196, -0.03111316009678624, 0.169329123317518, 0.020104762928729706, -0.19186611553992738, 0.05691268955442039, 0.43182475052096625, -0.21866327215155418, -0.2659535934217274, 0.16061288805212826, -0.3226948396980085, -0.1588240403004668, 0.22097450884228403, -0.12674846212294968, ... |
708.1071 | Statistical thinking: From Tukey to Vardi and beyond | Data miners (minors?) and neural networkers tend to eschew modelling, misled
perhaps by misinterpretation of strongly expressed views of John Tukey. I
discuss Vardi's views of these issues as well as other aspects of Vardi's work
in emision tomography and in sampling bias.
| math.ST stat.TH | data miners minors and neural networkers tend to eschew modelling misled perhaps by misinterpretation of strongly expressed views of john tukey i discuss vardis views of these issues as well as other aspects of vardis work in emision tomography and in sampling bias | [['data', 'miners', 'minors', 'and', 'neural', 'networkers', 'tend', 'to', 'eschew', 'modelling', 'misled', 'perhaps', 'by', 'misinterpretation', 'of', 'strongly', 'expressed', 'views', 'of', 'john', 'tukey', 'i', 'discuss', 'vardis', 'views', 'of', 'these', 'issues', 'as', 'well', 'as', 'other', 'aspects', 'of', 'vard... | [-0.04782428508180948, 0.04857353063388949, -0.030867099290758017, 0.11315991330359663, -0.11708082930584039, -0.19304815573351725, 0.05474126024083013, 0.3452491525205828, -0.3182759667813246, -0.3291061766268242, 0.16213959803073003, -0.30104555160782875, -0.14598369864480837, 0.13497282622293347, -0.2153704882200275... |
708.1072 | Deviation from $\Lambda$CDM: Pressure Parametrization | Most parametrizations for dark energy involve the equation of state $w$ of
the dark energy. In this work, we choose the pressure of the dark energy to
parametrize. As $p = constant$ essentially gives a cosmological constant, we
use the Taylor expansion around this behavior $p = -p_{0} + (1-a)p_{1} + ....$
to study th... | astro-ph gr-qc hep-ph | most parametrizations for dark energy involve the equation of state w of the dark energy in this work we choose the pressure of the dark energy to parametrize as p constant essentially gives a cosmological constant we use the taylor expansion around this behavior p p_0 1ap_1 to study the small deviations from the cosmo... | [['most', 'parametrizations', 'for', 'dark', 'energy', 'involve', 'the', 'equation', 'of', 'state', 'w', 'of', 'the', 'dark', 'energy', 'in', 'this', 'work', 'we', 'choose', 'the', 'pressure', 'of', 'the', 'dark', 'energy', 'to', 'parametrize', 'as', 'p', 'constant', 'essentially', 'gives', 'a', 'cosmological', 'consta... | [-0.11715604062536793, 0.10290819645352282, -0.09777383719828274, 0.07603687156638204, -0.11499090639048709, -0.110062669331551, 0.033157006681186, 0.2701476203326724, -0.2561488020376266, -0.3405716930467047, 0.03702242319827507, -0.29170866359613445, -0.03453019639403608, 0.17027025597513115, 0.032056995306016974, 0.... |
708.1073 | Errors Theory using Dirichlet Forms, Linear Partial Differential
Equations and Wavelets | We present an application of error theory using Dirichlet Forms in linear
partial differential equations (LPDE). We study the transmission of an
uncertainty on the terminal condition to the solution of the LPDE thanks to the
decomposition of the solution on a wavelets basis. We analyze the basic
properties and a part... | math.AP math.PR | we present an application of error theory using dirichlet forms in linear partial differential equations lpde we study the transmission of an uncertainty on the terminal condition to the solution of the lpde thanks to the decomposition of the solution on a wavelets basis we analyze the basic properties and a particular... | [['we', 'present', 'an', 'application', 'of', 'error', 'theory', 'using', 'dirichlet', 'forms', 'in', 'linear', 'partial', 'differential', 'equations', 'lpde', 'we', 'study', 'the', 'transmission', 'of', 'an', 'uncertainty', 'on', 'the', 'terminal', 'condition', 'to', 'the', 'solution', 'of', 'the', 'lpde', 'thanks', '... | [-0.122237737488318, -0.03192489885222107, -0.11689988885504696, 0.0659148076023811, -0.09973613880216502, -0.04583121641562917, 0.03393167394022338, 0.31609631492159307, -0.3321850092556232, -0.20797558809415653, 0.15830315478319207, -0.22957533115568834, -0.19640071907391152, 0.1943309688104842, -0.07624622758512253,... |
708.1074 | Model calculation of orientational effect of deformed aerogel on the
order parameter of superfluid 3He | Theory of Rainer and Vuorio of small objects in superfluid ^3He is applied
for calculation of the average orientational effect of a deformed aerogel on
the order parameter of 3He. The minimum deformation which stabilizes the
ordered state is evaluated both for specular and diffusive scattering of
quasiparticles by th... | cond-mat.dis-nn cond-mat.mes-hall | theory of rainer and vuorio of small objects in superfluid 3he is applied for calculation of the average orientational effect of a deformed aerogel on the order parameter of 3he the minimum deformation which stabilizes the ordered state is evaluated both for specular and diffusive scattering of quasiparticles by the th... | [['theory', 'of', 'rainer', 'and', 'vuorio', 'of', 'small', 'objects', 'in', 'superfluid', '3he', 'is', 'applied', 'for', 'calculation', 'of', 'the', 'average', 'orientational', 'effect', 'of', 'a', 'deformed', 'aerogel', 'on', 'the', 'order', 'parameter', 'of', '3he', 'the', 'minimum', 'deformation', 'which', 'stabili... | [-0.1373081252677366, 0.3228662625098458, -0.10111188610944037, 0.007569002395030111, 0.0008645852168019002, -0.06345601219576426, 0.058457814960722596, 0.29453067663752547, -0.212566051667986, -0.26870259176491973, 0.0034966879197432157, -0.3003677543109426, -0.05910632756198398, 0.11975899850949645, 0.019971887598960... |
708.1075 | N=4 superconformal Calogero models | We continue the research initiated in hep-th/0607215 and apply our method of
conformal automorphisms to generate various N=4 superconformal quantum
many-body systems on the real line from a set of decoupled particles extended
by fermionic degrees of freedom. The su(1,1|2) invariant models are governed by
two scalar p... | hep-th | we continue the research initiated in hepth0607215 and apply our method of conformal automorphisms to generate various n4 superconformal quantum manybody systems on the real line from a set of decoupled particles extended by fermionic degrees of freedom the su112 invariant models are governed by two scalar potentials o... | [['we', 'continue', 'the', 'research', 'initiated', 'in', 'hepth0607215', 'and', 'apply', 'our', 'method', 'of', 'conformal', 'automorphisms', 'to', 'generate', 'various', 'n4', 'superconformal', 'quantum', 'manybody', 'systems', 'on', 'the', 'real', 'line', 'from', 'a', 'set', 'of', 'decoupled', 'particles', 'extended... | [-0.14380437728602352, 0.15527374154895765, -0.055555415746319115, 0.029495310830674314, -0.06975292569647233, -0.17282961303902458, -0.07628095678736044, 0.2674819211251745, -0.21668179231053292, -0.2539218867002705, 0.04629653679836874, -0.32309858672060937, -0.16490007027019854, 0.12230226809480191, 0.00282253408371... |
708.1076 | Early evolution of transversally thermalized partons | The idea that the parton system created in relativistic heavy-ion collisions
(i) emerges in a state with transverse momenta close to thermodynamic
equilibrium and (ii) its evolution at early times is dominated by the
2-dimensional (transverse) hydrodynamics of the ideal fluid is investigated. It
is argued that this m... | nucl-th hep-ph nucl-ex | the idea that the parton system created in relativistic heavyion collisions i emerges in a state with transverse momenta close to thermodynamic equilibrium and ii its evolution at early times is dominated by the 2dimensional transverse hydrodynamics of the ideal fluid is investigated it is argued that this mechanism ma... | [['the', 'idea', 'that', 'the', 'parton', 'system', 'created', 'in', 'relativistic', 'heavyion', 'collisions', 'i', 'emerges', 'in', 'a', 'state', 'with', 'transverse', 'momenta', 'close', 'to', 'thermodynamic', 'equilibrium', 'and', 'ii', 'its', 'evolution', 'at', 'early', 'times', 'is', 'dominated', 'by', 'the', '2di... | [-0.1277081566252585, 0.2223430625965883, -0.1904980976150596, 0.10260495211495536, -0.009134925934004372, -0.1112474767523336, -0.08398808648906134, 0.31052147635611993, -0.2689910136355922, -0.2534377465891684, 0.014957987683311361, -0.27372211416990594, -0.005192539140839001, 0.0879708459472348, 0.025276862486297715... |
708.1077 | Green-Schwarz superstring from type IIB matrix model | We construct Green-Schwarz (GS) light-cone closed superstring theory from
type IIB matrix model. A GS light-cone string action is derived from two
dimensional N=8 U(n) noncommutative Yang-Mills (NCYM) by identifying
noncommutative scale with string scale. Supersymmetry transformation for the
light-cone gauge action i... | hep-th | we construct greenschwarz gs lightcone closed superstring theory from type iib matrix model a gs lightcone string action is derived from two dimensional n8 un noncommutative yangmills ncym by identifying noncommutative scale with string scale supersymmetry transformation for the lightcone gauge action is also derived f... | [['we', 'construct', 'greenschwarz', 'gs', 'lightcone', 'closed', 'superstring', 'theory', 'from', 'type', 'iib', 'matrix', 'model', 'a', 'gs', 'lightcone', 'string', 'action', 'is', 'derived', 'from', 'two', 'dimensional', 'n8', 'un', 'noncommutative', 'yangmills', 'ncym', 'by', 'identifying', 'noncommutative', 'scale... | [-0.11122770749319058, 0.21804011614563373, -0.054286255544194806, 0.19737530989536586, -0.09317173576698853, -0.2020327611038318, -0.013330382395249146, 0.3065306842756959, -0.16467330195009708, -0.19806214207066938, 0.057007598748000765, -0.26222692222262806, -0.2110481634664421, 0.009567637017999705, -0.056167959192... |
708.1078 | Nearly MDS expander codes with reduced alphabet size | Recently, Roth and Skachek proposed two methods for constructing nearly
maximum-distance separable (MDS) expander codes. We show that through the
simple modification of using mixed-alphabet codes derived from MDS codes as
constituent codes in their code designs, one can obtain nearly MDS codes of
significantly smalle... | cs.IT math.IT | recently roth and skachek proposed two methods for constructing nearly maximumdistance separable mds expander codes we show that through the simple modification of using mixedalphabet codes derived from mds codes as constituent codes in their code designs one can obtain nearly mds codes of significantly smaller alphabe... | [['recently', 'roth', 'and', 'skachek', 'proposed', 'two', 'methods', 'for', 'constructing', 'nearly', 'maximumdistance', 'separable', 'mds', 'expander', 'codes', 'we', 'show', 'that', 'through', 'the', 'simple', 'modification', 'of', 'using', 'mixedalphabet', 'codes', 'derived', 'from', 'mds', 'codes', 'as', 'constitu... | [-0.1531757846603106, 0.06624511695177905, -0.07821064269378909, 0.11269490096461156, 0.07327886639516158, -0.30909070676867045, 0.050794183983114256, 0.374484997628064, -0.3281676587488117, -0.30984565397274905, 0.1344221774318079, -0.24332790189133635, -0.10488375224943819, 0.2736200086676098, -0.10131874001295917, 0... |
708.1079 | Statistical inverse problems in active network tomography | The analysis of computer and communication networks gives rise to some
interesting inverse problems. This paper is concerned with active network
tomography where the goal is to recover information about quality-of-service
(QoS) parameters at the link level from aggregate data measured on end-to-end
network paths. The... | stat.ME | the analysis of computer and communication networks gives rise to some interesting inverse problems this paper is concerned with active network tomography where the goal is to recover information about qualityofservice qos parameters at the link level from aggregate data measured on endtoend network paths the estimatio... | [['the', 'analysis', 'of', 'computer', 'and', 'communication', 'networks', 'gives', 'rise', 'to', 'some', 'interesting', 'inverse', 'problems', 'this', 'paper', 'is', 'concerned', 'with', 'active', 'network', 'tomography', 'where', 'the', 'goal', 'is', 'to', 'recover', 'information', 'about', 'qualityofservice', 'qos',... | [-0.1544503260672361, -0.0065295574263677944, 0.00041567377939081944, 0.07425317193092024, -0.10071142761640854, -0.15982407112480015, 0.08507010430781389, 0.4297958647345637, -0.2760366638031629, -0.3394648648865588, 0.15152875715887662, -0.29704235988325095, -0.1735151803188093, 0.24041537379191533, -0.14757127853882... |
708.108 | Constraints on the range lambda of Yukawa-like modifications to the
Newtonian inverse-square law of gravitation from Solar System planetary
motions | In this paper we use the latest corrections to the Newton-Einstein secular
perihelion rates of some planets of the Solar System, phenomenologically
estimated with the EPM2004 ephemerides by the Russian astronomer E.V. Pitjeva,
to put severe constraints on the range parameter lambda characterizing the
Yukawa-like modi... | gr-qc astro-ph hep-ph physics.space-ph | in this paper we use the latest corrections to the newtoneinstein secular perihelion rates of some planets of the solar system phenomenologically estimated with the epm2004 ephemerides by the russian astronomer ev pitjeva to put severe constraints on the range parameter lambda characterizing the yukawalike modification... | [['in', 'this', 'paper', 'we', 'use', 'the', 'latest', 'corrections', 'to', 'the', 'newtoneinstein', 'secular', 'perihelion', 'rates', 'of', 'some', 'planets', 'of', 'the', 'solar', 'system', 'phenomenologically', 'estimated', 'with', 'the', 'epm2004', 'ephemerides', 'by', 'the', 'russian', 'astronomer', 'ev', 'pitjeva... | [-0.1045263611028696, 0.13216704979389296, -0.06604159491186674, 0.10659067259223244, -0.1342018507514774, -0.13599430021498626, 0.04512467367290175, 0.30263643208016083, -0.21403292480281136, -0.3595929561970418, 0.10825597676339141, -0.2728917135438263, -0.06558856167150787, 0.23877398084986629, -0.08639534079936964,... |
708.1081 | Quantifying Resonant Structure in NGC 6946 from Two-dimensional
Kinematics | We study the two-dimensional kinematics of the H-alpha-emitting gas in the
nearby barred Scd galaxy, NGC 6946, in order to determine the pattern speed of
the primary m=2 perturbation mode. The pattern speed is a crucial parameter for
constraining the internal dynamics, estimating the impact velocities of the
gravitat... | astro-ph | we study the twodimensional kinematics of the halphaemitting gas in the nearby barred scd galaxy ngc 6946 in order to determine the pattern speed of the primary m2 perturbation mode the pattern speed is a crucial parameter for constraining the internal dynamics estimating the impact velocities of the gravitational pert... | [['we', 'study', 'the', 'twodimensional', 'kinematics', 'of', 'the', 'halphaemitting', 'gas', 'in', 'the', 'nearby', 'barred', 'scd', 'galaxy', 'ngc', '6946', 'in', 'order', 'to', 'determine', 'the', 'pattern', 'speed', 'of', 'the', 'primary', 'm2', 'perturbation', 'mode', 'the', 'pattern', 'speed', 'is', 'a', 'crucial... | [-0.14367794335409387, 0.03164060922551811, -0.09923303993230667, 0.04144370252315915, -0.08269664530425963, -0.04019141264701958, 0.004178061787358889, 0.35348926044323226, -0.23977171376728537, -0.3059597250010649, 0.05384111985143255, -0.23599031477946977, -0.055395613866623, 0.16591329667764254, -0.0033735821418689... |
708.1082 | Q2237+0305 source structure and dimensions from light curves simulation | Assuming a two-component quasar structure model consisting of a central
compact source and an extended outer feature, we produce microlensing
simulations for a population of star-like objects in the lens galaxy. Such a
model is a simplified version of that adopted to explain the brightness
variations observed in Q095... | astro-ph | assuming a twocomponent quasar structure model consisting of a central compact source and an extended outer feature we produce microlensing simulations for a population of starlike objects in the lens galaxy such a model is a simplified version of that adopted to explain the brightness variations observed in q0957 schi... | [['assuming', 'a', 'twocomponent', 'quasar', 'structure', 'model', 'consisting', 'of', 'a', 'central', 'compact', 'source', 'and', 'an', 'extended', 'outer', 'feature', 'we', 'produce', 'microlensing', 'simulations', 'for', 'a', 'population', 'of', 'starlike', 'objects', 'in', 'the', 'lens', 'galaxy', 'such', 'a', 'mod... | [-0.08540988597195354, 0.03931964442401497, -0.10712934172867487, 0.0817850838222377, -0.06446522073949584, -0.07450355919233213, 0.014306369673081295, 0.37442975067878487, -0.21482417154712258, -0.34260378487373666, 0.07798850497703017, -0.2610838405003219, -0.03698764487678461, 0.2453854677075503, -0.0337415154294662... |
708.1083 | The Near-Infrared Broad Emission Line Region of Active Galactic Nuclei
-- I. The Observations | We present high quality (high signal-to-noise ratio and moderate spectral
resolution) near-infrared (near-IR) spectroscopic observations of 23 well-known
broad-emission line active galactic nuclei (AGN). Additionally, we obtained
simultaneous (within two months) optical spectroscopy of similar quality. The
near-IR br... | astro-ph | we present high quality high signaltonoise ratio and moderate spectral resolution nearinfrared nearir spectroscopic observations of 23 wellknown broademission line active galactic nuclei agn additionally we obtained simultaneous within two months optical spectroscopy of similar quality the nearir broad emission line sp... | [['we', 'present', 'high', 'quality', 'high', 'signaltonoise', 'ratio', 'and', 'moderate', 'spectral', 'resolution', 'nearinfrared', 'nearir', 'spectroscopic', 'observations', 'of', '23', 'wellknown', 'broademission', 'line', 'active', 'galactic', 'nuclei', 'agn', 'additionally', 'we', 'obtained', 'simultaneous', 'with... | [-0.033677373507306874, 0.08846854712638973, 0.0443537507731563, 0.0724014689007567, -0.043460711136332944, -0.13397167059871504, 0.10148374555318052, 0.5061694820467223, -0.14538450895124075, -0.3186454738283323, 0.052631301819307044, -0.31290460145498955, -0.008573015801544882, 0.1373370996513205, -0.0030471715323913... |
708.1084 | Densities for Ornstein-Uhlenbeck processes with jumps | We consider an Ornstein-Uhlenbeck process with values in R^n driven by a
L\'evy process (Z_t) taking values in R^d with d possibly smaller than n. The
L\'evy noise can have a degenerate or even vanishing Gaussian component.
Under a controllability condition and an assumption on the L\'evy measure of
(Z_t), we prove... | math.PR math.AP | we consider an ornsteinuhlenbeck process with values in rn driven by a levy process z_t taking values in rd with d possibly smaller than n the levy noise can have a degenerate or even vanishing gaussian component under a controllability condition and an assumption on the levy measure of z_t we prove that the law of the... | [['we', 'consider', 'an', 'ornsteinuhlenbeck', 'process', 'with', 'values', 'in', 'rn', 'driven', 'by', 'a', 'levy', 'process', 'z_t', 'taking', 'values', 'in', 'rd', 'with', 'd', 'possibly', 'smaller', 'than', 'n', 'the', 'levy', 'noise', 'can', 'have', 'a', 'degenerate', 'or', 'even', 'vanishing', 'gaussian', 'compon... | [-0.09681720477105542, 0.20045697932503323, -0.08623772290196609, 0.012335522952691297, -0.0017879222498529336, -0.15545908058464358, 0.007556004576723684, 0.4027658159082586, -0.2635355960916389, -0.1471729735335843, 0.1356076914989072, -0.3046197584957223, -0.09529805948047644, 0.1622126667352859, -0.0903723148512654... |
708.1085 | Using data network metrics, graphics, and topology to explore network
characteristics | Yehuda Vardi introduced the term network tomography and was the first to
propose and study how statistical inverse methods could be adapted to attack
important network problems (Vardi, 1996). More recently, in one of his final
papers, Vardi proposed notions of metrics on networks to define and measure
distances betwe... | stat.ME | yehuda vardi introduced the term network tomography and was the first to propose and study how statistical inverse methods could be adapted to attack important network problems vardi 1996 more recently in one of his final papers vardi proposed notions of metrics on networks to define and measure distances between a net... | [['yehuda', 'vardi', 'introduced', 'the', 'term', 'network', 'tomography', 'and', 'was', 'the', 'first', 'to', 'propose', 'and', 'study', 'how', 'statistical', 'inverse', 'methods', 'could', 'be', 'adapted', 'to', 'attack', 'important', 'network', 'problems', 'vardi', '1996', 'more', 'recently', 'in', 'one', 'of', 'his... | [-0.08269656332118462, -0.02771764393814059, -0.10656589932733442, 0.10932830748749217, -0.0900105034092416, -0.17135966989853596, 0.09853537045372021, 0.3919277725791609, -0.2731873064830497, -0.328060727141722, 0.10063203266818656, -0.2603355047648546, -0.2699203212836732, 0.19234153261955678, -0.13791332141546583, 0... |
708.1086 | Recycling of quantum information: Multiple observations of quantum
systems | Given a finite number of copies of an unknown qubit state that have already
been measured optimally, can one still extract any information about the
original unknown state? We give a positive answer to this question and quantify
the information obtainable by a given observer as a function of the number of
copies in t... | quant-ph | given a finite number of copies of an unknown qubit state that have already been measured optimally can one still extract any information about the original unknown state we give a positive answer to this question and quantify the information obtainable by a given observer as a function of the number of copies in the e... | [['given', 'a', 'finite', 'number', 'of', 'copies', 'of', 'an', 'unknown', 'qubit', 'state', 'that', 'have', 'already', 'been', 'measured', 'optimally', 'can', 'one', 'still', 'extract', 'any', 'information', 'about', 'the', 'original', 'unknown', 'state', 'we', 'give', 'a', 'positive', 'answer', 'to', 'this', 'questio... | [-0.09539306892880371, 0.14223349566132779, -0.11536094974726438, 0.04136449723279968, -0.03163528718786048, -0.17727853736973234, 0.07213456885988957, 0.3348019898336913, -0.257702124863863, -0.32294067987906083, 0.12767895337892696, -0.2981794080630477, -0.05415635528042913, 0.15526947611942887, -0.07510159135396992,... |
708.1087 | Legendrian ribbons in overtwisted contact structures | We show that a null-homologous transverse knot K in the complement of an
overtwisted disk in a contact 3-manifold is the boundary of a Legendrian ribbon
if and only if it possesses a Seifert surface S such that the self-linking
number of K with respect to S satisfies $\sel(K,S)=-\chi(S)$. In particular,
every null-ho... | math.GT | we show that a nullhomologous transverse knot k in the complement of an overtwisted disk in a contact 3manifold is the boundary of a legendrian ribbon if and only if it possesses a seifert surface s such that the selflinking number of k with respect to s satisfies selkschis in particular every nullhomologous topologica... | [['we', 'show', 'that', 'a', 'nullhomologous', 'transverse', 'knot', 'k', 'in', 'the', 'complement', 'of', 'an', 'overtwisted', 'disk', 'in', 'a', 'contact', '3manifold', 'is', 'the', 'boundary', 'of', 'a', 'legendrian', 'ribbon', 'if', 'and', 'only', 'if', 'it', 'possesses', 'a', 'seifert', 'surface', 's', 'such', 'th... | [-0.31272631873606993, 0.11042076417636777, -0.0999911334165322, 0.038001574257949505, -0.10366577081262104, -0.238192575027345, 0.011822529627831393, 0.40724618857856637, -0.3253214023506609, -0.2601979667282042, 0.01731328591729404, -0.26025874706445845, -0.2080737913718387, 0.17654660241978784, -0.1613404050354235, ... |
708.1088 | Wobbles and other kink-breather solutions of the Sine Gordon model | We study various solutions of the Sine Gordon model in (1+1) dimensions. We
use the Hirota method to construct some of them and then show that the wobble,
discussed in detail by K\"alberman, is one of such solutions. We concentrate
our attention on a kink and its bound states with one or two breathers. We
study their... | hep-th cond-mat.other nlin.SI | we study various solutions of the sine gordon model in 11 dimensions we use the hirota method to construct some of them and then show that the wobble discussed in detail by kalberman is one of such solutions we concentrate our attention on a kink and its bound states with one or two breathers we study their stability a... | [['we', 'study', 'various', 'solutions', 'of', 'the', 'sine', 'gordon', 'model', 'in', '11', 'dimensions', 'we', 'use', 'the', 'hirota', 'method', 'to', 'construct', 'some', 'of', 'them', 'and', 'then', 'show', 'that', 'the', 'wobble', 'discussed', 'in', 'detail', 'by', 'kalberman', 'is', 'one', 'of', 'such', 'solution... | [-0.14261803920898172, 0.057873873997272715, -0.07242730380191158, 0.09391121859435872, -0.05795494495477113, -0.1245107880483071, 0.05068528793183052, 0.3865616811801576, -0.21584111819457677, -0.24896477955755675, 0.18288008080627252, -0.3171237256869467, -0.22143954405004884, 0.19931770459515974, -0.0120509341423813... |
708.1089 | Quantum criticality as a resource for quantum estimation | We address quantum critical systems as a resource in quantum estimation and
derive the ultimate quantum limits to the precision of any estimator of the
coupling parameters. In particular, if L denotes the size of a system and
\lambda is the relevant coupling parameters driving a quantum phase transition,
we show that... | quant-ph | we address quantum critical systems as a resource in quantum estimation and derive the ultimate quantum limits to the precision of any estimator of the coupling parameters in particular if l denotes the size of a system and lambda is the relevant coupling parameters driving a quantum phase transition we show that a pre... | [['we', 'address', 'quantum', 'critical', 'systems', 'as', 'a', 'resource', 'in', 'quantum', 'estimation', 'and', 'derive', 'the', 'ultimate', 'quantum', 'limits', 'to', 'the', 'precision', 'of', 'any', 'estimator', 'of', 'the', 'coupling', 'parameters', 'in', 'particular', 'if', 'l', 'denotes', 'the', 'size', 'of', 'a... | [-0.16410675094703378, 0.15093979382208575, -0.046844995336903034, 0.04119730507302159, 0.0016755037135923298, -0.17921852081074058, 0.08930125536623403, 0.3203688604391624, -0.22625055031581112, -0.2776345028063265, 0.09424519696094479, -0.27328697504110144, -0.13969418338160508, 0.2142446614414558, -0.013277446674879... |
708.109 | Fano resonances at light scattering by an obstacle | It is shown that elastic resonance scattering of light by a finite-size
obstacle with weak dissipation is analogous to quantum scattering by a
potential with quasi-discrete levels and exhibits Fano resonances. Localized
plasmons (polaritons), exited in the obstacle by the incident light, are
equivalent to the quasi-d... | cond-mat.other cond-mat.mes-hall cond-mat.soft physics.optics | it is shown that elastic resonance scattering of light by a finitesize obstacle with weak dissipation is analogous to quantum scattering by a potential with quasidiscrete levels and exhibits fano resonances localized plasmons polaritons exited in the obstacle by the incident light are equivalent to the quasidiscrete le... | [['it', 'is', 'shown', 'that', 'elastic', 'resonance', 'scattering', 'of', 'light', 'by', 'a', 'finitesize', 'obstacle', 'with', 'weak', 'dissipation', 'is', 'analogous', 'to', 'quantum', 'scattering', 'by', 'a', 'potential', 'with', 'quasidiscrete', 'levels', 'and', 'exhibits', 'fano', 'resonances', 'localized', 'plas... | [-0.11558504966436885, 0.2372358530726342, -0.055149824526160955, 0.09643937858054415, -0.0007252449076622725, -0.1772203603386879, -0.024078104312065987, 0.3562270383536816, -0.259295384241268, -0.28367182474117725, 0.011251272717490792, -0.3300430545862764, -0.1579700010595843, 0.18712920083082282, 0.0511181602015858... |
708.1091 | Semiclassical Limits of Quantum Affine Spaces | Semiclassical limits of generic multiparameter quantized coordinate rings A =
O_q(k^n) of affine spaces are constructed and related to A, for k an
algebraically closed field of characteristic zero and q a multiplicatively
antisymmetric matrix whose entries generate a torsionfree subgroup of k*. A
semiclassical limit ... | math.QA math.RA | semiclassical limits of generic multiparameter quantized coordinate rings a o_qkn of affine spaces are constructed and related to a for k an algebraically closed field of characteristic zero and q a multiplicatively antisymmetric matrix whose entries generate a torsionfree subgroup of k a semiclassical limit of a is a ... | [['semiclassical', 'limits', 'of', 'generic', 'multiparameter', 'quantized', 'coordinate', 'rings', 'a', 'o_qkn', 'of', 'affine', 'spaces', 'are', 'constructed', 'and', 'related', 'to', 'a', 'for', 'k', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'zero', 'and', 'q', 'a', 'multiplicatively', 'antis... | [-0.1839490258579801, 0.08724695957613557, -0.08618787999982667, 0.044672825020755744, -0.07472905522259841, -0.14270631357980001, -0.012750885917235664, 0.3091338717313424, -0.33446528011588916, -0.1797801578761476, 0.0754802870418829, -0.25383868136377946, -0.13069798482676884, 0.21966555749605984, -0.106933822598794... |
708.1092 | Spin-orbital Kondo decoherence by environmental effects in capacitively
coupled quantum dot devices | Strong correlation effects in a capacitively coupled double quantum-dot setup
were previously shown to provide the possibility of both entangling spin-charge
degrees of freedom and realizing efficient spin-filtering operations by static
gate-voltage manipulations. Motivated by the use of such a device for quantum
com... | cond-mat.mes-hall cond-mat.str-el | strong correlation effects in a capacitively coupled double quantumdot setup were previously shown to provide the possibility of both entangling spincharge degrees of freedom and realizing efficient spinfiltering operations by static gatevoltage manipulations motivated by the use of such a device for quantum computing ... | [['strong', 'correlation', 'effects', 'in', 'a', 'capacitively', 'coupled', 'double', 'quantumdot', 'setup', 'were', 'previously', 'shown', 'to', 'provide', 'the', 'possibility', 'of', 'both', 'entangling', 'spincharge', 'degrees', 'of', 'freedom', 'and', 'realizing', 'efficient', 'spinfiltering', 'operations', 'by', '... | [-0.1865283021709088, 0.17198823307274427, -0.07020837833845346, 0.0637342245651974, -0.045525895494616546, -0.18993439564298167, 0.07248843120807996, 0.35525552054760273, -0.22601820562859296, -0.31806752745245326, 0.027007064401466958, -0.2200361315817496, -0.15763421344082254, 0.22295479544965152, -0.000874520039002... |
708.1093 | Nuclear Star Clusters across the Hubble Sequence | Over the last decade, HST imaging studies have revealed that the centers of
most galaxies are occupied by compact, barely resolved sources. Based on their
structural properties, position in the fundamental plane, and spectra, these
sources clearly have a stellar origin. They are therefore called ``nuclear star
cluste... | astro-ph | over the last decade hst imaging studies have revealed that the centers of most galaxies are occupied by compact barely resolved sources based on their structural properties position in the fundamental plane and spectra these sources clearly have a stellar origin they are therefore called nuclear star clusters ncs or s... | [['over', 'the', 'last', 'decade', 'hst', 'imaging', 'studies', 'have', 'revealed', 'that', 'the', 'centers', 'of', 'most', 'galaxies', 'are', 'occupied', 'by', 'compact', 'barely', 'resolved', 'sources', 'based', 'on', 'their', 'structural', 'properties', 'position', 'in', 'the', 'fundamental', 'plane', 'and', 'spectr... | [-0.07675492157506818, 0.11780639733274893, -0.04384900658243449, 0.09953906613393365, -0.09769307285172987, -0.06752317721267866, 0.030154389512037562, 0.4573624785293207, -0.18776175520430693, -0.3159390292086891, 0.108129696423301, -0.33686934499435617, -0.11839417968093305, 0.2221838543936828, -0.042709305551703845... |
708.1094 | Threshold Resonant Structure of the 232Th Neutron-Induced Fission Cross
Section | The structures observed in the sub-threshold neutron-induced fission of
^{232}Th were investigated employing a recent developed model. Theoretical
single-particle excitations of a phenomenological two-humped barrier are
determined by solving a system of coupled differential equations for the motion
along the optimal ... | nucl-th | the structures observed in the subthreshold neutroninduced fission of 232th were investigated employing a recent developed model theoretical singleparticle excitations of a phenomenological twohumped barrier are determined by solving a system of coupled differential equations for the motion along the optimal fission pa... | [['the', 'structures', 'observed', 'in', 'the', 'subthreshold', 'neutroninduced', 'fission', 'of', '232th', 'were', 'investigated', 'employing', 'a', 'recent', 'developed', 'model', 'theoretical', 'singleparticle', 'excitations', 'of', 'a', 'phenomenological', 'twohumped', 'barrier', 'are', 'determined', 'by', 'solving... | [-0.1116957249800504, 0.19304586161333737, -0.018096947553798114, 0.07048318896438041, -0.003039168291333325, -0.11323238794903943, 0.04030267318876663, 0.32748421252068904, -0.20657889816983796, -0.3600109213926267, 0.022871401505590888, -0.33051555253344006, -0.02978785364602757, 0.20688952966408786, 0.06110034236629... |
708.1095 | Quantum turbulence in propagating superfluid vortex front | We present experimental, numerical and theoretical studies of a vortex front
propagating into a region of vortex-free flow of rotating superfluid 3He-B. We
show that the nature of the front changes from laminar through quasi-classical
turbulent to quantum turbulent with decreasing temperature. Our experiment
provides... | cond-mat.soft | we present experimental numerical and theoretical studies of a vortex front propagating into a region of vortexfree flow of rotating superfluid 3heb we show that the nature of the front changes from laminar through quasiclassical turbulent to quantum turbulent with decreasing temperature our experiment provides the fir... | [['we', 'present', 'experimental', 'numerical', 'and', 'theoretical', 'studies', 'of', 'a', 'vortex', 'front', 'propagating', 'into', 'a', 'region', 'of', 'vortexfree', 'flow', 'of', 'rotating', 'superfluid', '3heb', 'we', 'show', 'that', 'the', 'nature', 'of', 'the', 'front', 'changes', 'from', 'laminar', 'through', '... | [-0.19204806268320793, 0.25890757695570127, -0.10051881913191725, 0.012205016807672213, -0.04693521666772587, -0.06321480747830775, 0.021842198674423025, 0.30632737778144, -0.2768563269301481, -0.2368034705442866, 0.022505544564091436, -0.25086691263179806, -0.05352611089912579, 0.23027680057686628, 0.03878034703336301... |
708.1096 | Pseudo-Riemannian Jacobi-Videv Manifolds | We exhibit several families of Jacobi-Videv pseudo-Riemannian manifolds which
are not Einstein. We also exhibit Jacobi-Videv algebraic curvature tensors
where the Ricci operator defines an almost complex structure.
| math.DG | we exhibit several families of jacobividev pseudoriemannian manifolds which are not einstein we also exhibit jacobividev algebraic curvature tensors where the ricci operator defines an almost complex structure | [['we', 'exhibit', 'several', 'families', 'of', 'jacobividev', 'pseudoriemannian', 'manifolds', 'which', 'are', 'not', 'einstein', 'we', 'also', 'exhibit', 'jacobividev', 'algebraic', 'curvature', 'tensors', 'where', 'the', 'ricci', 'operator', 'defines', 'an', 'almost', 'complex', 'structure']] | [-0.2772099063373529, 0.10047887343199154, -0.10496350804057258, 0.10166749702050136, -0.19773251289286867, -0.16633302001998976, -0.2415239785153132, 0.4457743334082457, -0.26875663806612676, -0.19487322146932667, 0.11918370970166646, -0.2983669963880227, -0.27211661937718207, 0.1512662936718418, -0.07192698572404109,... |
708.1097 | Effects of the network structural properties on its controllability | In a recent paper, it has been suggested that the controllability of a
diffusively coupled complex network, subject to localized feedback loops at
some of its vertices, can be assessed by means of a Master Stability Function
approach, where the network controllability is defined in terms of the spectral
properties of... | cond-mat.dis-nn | in a recent paper it has been suggested that the controllability of a diffusively coupled complex network subject to localized feedback loops at some of its vertices can be assessed by means of a master stability function approach where the network controllability is defined in terms of the spectral properties of an ap... | [['in', 'a', 'recent', 'paper', 'it', 'has', 'been', 'suggested', 'that', 'the', 'controllability', 'of', 'a', 'diffusively', 'coupled', 'complex', 'network', 'subject', 'to', 'localized', 'feedback', 'loops', 'at', 'some', 'of', 'its', 'vertices', 'can', 'be', 'assessed', 'by', 'means', 'of', 'a', 'master', 'stability... | [-0.15428810206187493, 0.06611320609875332, -0.05087707591567026, 0.02840937538649482, -0.025162890862228105, -0.08454338373849168, 0.0012115530743081447, 0.391176630186079, -0.2737635147717336, -0.2951699171984649, 0.09769751874568022, -0.2586317236191067, -0.2345576693263391, 0.1220911975707049, -0.026292038813192885... |
708.1098 | Hydrostatic pressure study of pure and doped La1-xRxAgSb2 (R = Ce, Nd)
charge-density-wave compounds | The intermetallic compound LaAgSb2 displays two charge-density-wave (CDW)
transitions, which were detected with measurements of electrical resistivity
(rho), magnetic susceptibility, and X-ray scattering; the upper transition
takes place at T1 approx. 210 K, and it is accompanied by a large anomaly in
rho(T), whereas... | cond-mat.str-el cond-mat.other | the intermetallic compound laagsb2 displays two chargedensitywave cdw transitions which were detected with measurements of electrical resistivity rho magnetic susceptibility and xray scattering the upper transition takes place at t1 approx 210 k and it is accompanied by a large anomaly in rhot whereas the lower transit... | [['the', 'intermetallic', 'compound', 'laagsb2', 'displays', 'two', 'chargedensitywave', 'cdw', 'transitions', 'which', 'were', 'detected', 'with', 'measurements', 'of', 'electrical', 'resistivity', 'rho', 'magnetic', 'susceptibility', 'and', 'xray', 'scattering', 'the', 'upper', 'transition', 'takes', 'place', 'at', '... | [-0.15172218426039977, 0.26401189088081833, -0.01570413425089974, 0.01767153720720671, 0.018980332499589112, -0.12273829773196257, 0.1374706178492702, 0.31625583513717476, -0.24186677401588647, -0.3243142366637567, 0.03919734699964322, -0.3853210740010528, -0.052596005352040495, 0.1357681353236366, 0.07097714680261846,... |
708.1099 | Attosecond Control of Ionization Dynamics | Attosecond pulses can be used to initiate and control electron dynamics on a
sub-femtosecond time scale. The first step in this process occurs when an atom
absorbs an ultraviolet photon leading to the formation of an attosecond
electron wave packet (EWP). Until now, attosecond pulses have been used to
create free EWP... | physics.atom-ph | attosecond pulses can be used to initiate and control electron dynamics on a subfemtosecond time scale the first step in this process occurs when an atom absorbs an ultraviolet photon leading to the formation of an attosecond electron wave packet ewp until now attosecond pulses have been used to create free ewps in the... | [['attosecond', 'pulses', 'can', 'be', 'used', 'to', 'initiate', 'and', 'control', 'electron', 'dynamics', 'on', 'a', 'subfemtosecond', 'time', 'scale', 'the', 'first', 'step', 'in', 'this', 'process', 'occurs', 'when', 'an', 'atom', 'absorbs', 'an', 'ultraviolet', 'photon', 'leading', 'to', 'the', 'formation', 'of', '... | [-0.07113300536368643, 0.21047511635866437, -0.10852822355865951, 0.08092056047665415, 0.025739825207499727, -0.0955684752699228, 0.0475063765864639, 0.4884843772818004, -0.2793382049207726, -0.27834523170585596, -0.0063656199595800815, -0.2677334121458473, -0.09972787611022209, 0.2111069726937961, -0.02556857981628948... |
708.11 | Differential geometry of curves in Lagrange Grassmannians with given
Young diagram | Curves in Lagrange Grassmannians appear naturally in the intrinsic study of
geometric structures on manifolds. By a smooth geometric structure on a
manifold we mean any submanifold of its tangent bundle, transversal to the
fibers. One can consider the time-optimal problem naturally associate with a
geometric structur... | math.DG | curves in lagrange grassmannians appear naturally in the intrinsic study of geometric structures on manifolds by a smooth geometric structure on a manifold we mean any submanifold of its tangent bundle transversal to the fibers one can consider the timeoptimal problem naturally associate with a geometric structure the ... | [['curves', 'in', 'lagrange', 'grassmannians', 'appear', 'naturally', 'in', 'the', 'intrinsic', 'study', 'of', 'geometric', 'structures', 'on', 'manifolds', 'by', 'a', 'smooth', 'geometric', 'structure', 'on', 'a', 'manifold', 'we', 'mean', 'any', 'submanifold', 'of', 'its', 'tangent', 'bundle', 'transversal', 'to', 't... | [-0.22508667350116066, 0.04110028038979633, -0.11758295829969588, 0.0809168526892354, -0.12197004574989992, -0.11381284029728361, -0.03248711021809166, 0.3340298532750541, -0.3404758459650348, -0.2371220902457307, 0.08877338522172329, -0.21243904028282315, -0.19829882148887143, 0.19146358804994434, -0.1714762652025562,... |
708.1101 | Determination of localized conduction band-tail states distribution in
single phase undoped microcrystalline silicon | We report on the phototransport properties of microstructurally well
characterized plasma deposited highly crystallized microcrystalline silicon
films. The steady state photoconductivity was measured on a wide
microstructural variety of single-phase undoped microcrystalline silicon films
as a function of temperature ... | cond-mat.mtrl-sci | we report on the phototransport properties of microstructurally well characterized plasma deposited highly crystallized microcrystalline silicon films the steady state photoconductivity was measured on a wide microstructural variety of singlephase undoped microcrystalline silicon films as a function of temperature and ... | [['we', 'report', 'on', 'the', 'phototransport', 'properties', 'of', 'microstructurally', 'well', 'characterized', 'plasma', 'deposited', 'highly', 'crystallized', 'microcrystalline', 'silicon', 'films', 'the', 'steady', 'state', 'photoconductivity', 'was', 'measured', 'on', 'a', 'wide', 'microstructural', 'variety', '... | [-0.09360753726976892, 0.20833841811640766, -0.06402873173596915, -0.049226488777564775, 0.04304370543154776, -0.1368170020547856, 0.033591457624550396, 0.4585218083691494, -0.2406689170145847, -0.3119194668252021, 0.01514954978483729, -0.3499528145465743, -0.06798660255775883, 0.20284369260731056, 0.034070368637411114... |
708.1102 | Spectral geometry, homogeneous spaces, and differential forms with
finite Fourier series | Let G be a compact Lie group acting transitively on Riemannian manifolds M
and N. Let p be a G equivariant Riemannian submersion from M to N. We show that
a smooth differential form on N has finite Fourier series if and only if the
pull back has finite Fourier series on M
| math.AP | let g be a compact lie group acting transitively on riemannian manifolds m and n let p be a g equivariant riemannian submersion from m to n we show that a smooth differential form on n has finite fourier series if and only if the pull back has finite fourier series on m | [['let', 'g', 'be', 'a', 'compact', 'lie', 'group', 'acting', 'transitively', 'on', 'riemannian', 'manifolds', 'm', 'and', 'n', 'let', 'p', 'be', 'a', 'g', 'equivariant', 'riemannian', 'submersion', 'from', 'm', 'to', 'n', 'we', 'show', 'that', 'a', 'smooth', 'differential', 'form', 'on', 'n', 'has', 'finite', 'fourier... | [-0.2239736925177979, 0.13502233487747187, -0.16763886393768326, -0.06857852455017702, -0.20033409954312276, -0.19674476848493488, -0.0313258266849619, 0.38540704267204934, -0.2897694082052078, -0.21446593745418316, 0.09447451676505636, -0.3135611115480369, -0.09768561717948683, 0.21740548569656346, -0.1299327492081331... |
708.1103 | Normal and anti Meyer-Neldel rule in conductivity of highly crystallized
undoped microcrystalline silicon films | We have studied the electrical conductivity behavior of highly crystallized
undoped hydrogenated microcrystalline silicon films having different
microstructures. The dark conductivity is seen to follow Meyer Neldel rule
(MNR) in some films and anti MNR in others, which has been explained on the
basis of variation in ... | cond-mat.mtrl-sci | we have studied the electrical conductivity behavior of highly crystallized undoped hydrogenated microcrystalline silicon films having different microstructures the dark conductivity is seen to follow meyer neldel rule mnr in some films and anti mnr in others which has been explained on the basis of variation in the fi... | [['we', 'have', 'studied', 'the', 'electrical', 'conductivity', 'behavior', 'of', 'highly', 'crystallized', 'undoped', 'hydrogenated', 'microcrystalline', 'silicon', 'films', 'having', 'different', 'microstructures', 'the', 'dark', 'conductivity', 'is', 'seen', 'to', 'follow', 'meyer', 'neldel', 'rule', 'mnr', 'in', 's... | [-0.10408135752016999, 0.1551339995499363, -0.0773314418560215, 0.049976385059035865, -0.017038931825262463, -0.10303589354413722, 0.06481634877052093, 0.4081918837117224, -0.26502329916372125, -0.2980930885733587, 0.07207752465258417, -0.3231239809156877, -0.12921981253372183, 0.1380134409951881, -0.020697263671599072... |
708.1104 | Fractional composition of large crystallite grains: a unique
microstructural parameter to explain conduction behavior in single phase
undoped microcrystalline silicon | We have studied the dark conductivity of a broad microstructural range of
plasma deposited single phase undoped microcrystalline silicon films in a wide
temperature range (15 - 450K) to identify the possible transport mechanisms and
the interrelationship between film microstructure and electrical transport
behavior. ... | cond-mat.mtrl-sci | we have studied the dark conductivity of a broad microstructural range of plasma deposited single phase undoped microcrystalline silicon films in a wide temperature range 15 450k to identify the possible transport mechanisms and the interrelationship between film microstructure and electrical transport behavior differe... | [['we', 'have', 'studied', 'the', 'dark', 'conductivity', 'of', 'a', 'broad', 'microstructural', 'range', 'of', 'plasma', 'deposited', 'single', 'phase', 'undoped', 'microcrystalline', 'silicon', 'films', 'in', 'a', 'wide', 'temperature', 'range', '15', '450k', 'to', 'identify', 'the', 'possible', 'transport', 'mechani... | [-0.1038012044851767, 0.21359662952211997, -0.035682105219386744, -0.06506177027723893, 0.00193714366865937, -0.1301049158421599, 0.03443248246119104, 0.4631154659683957, -0.2772672734166862, -0.3553861773107201, 0.01613940571339547, -0.3101746136760057, -0.06598827721212398, 0.20629593371554758, 0.023030140103814614, ... |
708.1105 | Search for \bar{B}^0\to\Lambda_c^+\bar{\Lambda}_c^- decay at Belle | We search for the doubly charmed baryonic decay
$\bar{B}^0\to\Lambda_c^+\bar{\Lambda}_c^-$, in a data sample of $520\times10^6$
$B{\bar B}$ events accumulated at the $\Upsilon(4S)$ resonance with the Belle
detector at the KEKB asymmetric e^+e^- collider. We find no significant signal
and set an upper limit of ${\cal
... | hep-ex | we search for the doubly charmed baryonic decay barb0tolambda_cbarlambda_c in a data sample of 520times106 bbar b events accumulated at the upsilon4s resonance with the belle detector at the kekb asymmetric ee collider we find no significant signal and set an upper limit of cal bbarb0tolambda_cbarlambda_c62times105 at ... | [['we', 'search', 'for', 'the', 'doubly', 'charmed', 'baryonic', 'decay', 'barb0tolambda_cbarlambda_c', 'in', 'a', 'data', 'sample', 'of', '520times106', 'bbar', 'b', 'events', 'accumulated', 'at', 'the', 'upsilon4s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetric', 'ee', 'collider', ... | [-0.07986537996033553, 0.22826219983436008, -0.055822189947517184, 0.11519997786187257, -0.06991433701934475, -0.118244271812157, 0.11086065673917606, 0.2608763565327607, -0.18034442019301886, -0.2813507842046081, -0.04751935974562395, -0.4152960615488244, 0.056398997695057414, 0.1190554558883841, 0.09400930264325556, ... |
708.1106 | Additivity of Spin^c Quantization under Cutting | A G-equivariant spin^c structure on a manifold gives rise to a virtual
representation of the group G, called the spin^c quantization of the manifold.
We present a cutting construction for S^1-equivariant spin^c manifolds, and
show that the quantization of the original manifold is isomorphic to the direct
sum of the q... | math.DG | a gequivariant spinc structure on a manifold gives rise to a virtual representation of the group g called the spinc quantization of the manifold we present a cutting construction for s1equivariant spinc manifolds and show that the quantization of the original manifold is isomorphic to the direct sum of the quantization... | [['a', 'gequivariant', 'spinc', 'structure', 'on', 'a', 'manifold', 'gives', 'rise', 'to', 'a', 'virtual', 'representation', 'of', 'the', 'group', 'g', 'called', 'the', 'spinc', 'quantization', 'of', 'the', 'manifold', 'we', 'present', 'a', 'cutting', 'construction', 'for', 's1equivariant', 'spinc', 'manifolds', 'and',... | [-0.2149308966351794, 0.018636680050910293, -0.13835285340326947, 0.08062763810203133, -0.15371650421399286, -0.09170063914029629, 0.03906947969120334, 0.3134723623077591, -0.296280569021965, -0.24630195255596915, 0.06487382630751069, -0.23749917106969015, -0.18704916944412828, 0.13640758699991487, -0.14594179472803628... |
708.1107 | Functional analysis via extensions of the band depth | The notion of data depth has long been in use to obtain robust location and
scale estimates in a multivariate setting. The depth of an observation is a
measure of its centrality, with respect to a data set or a distribution. The
data depths of a set of multivariate observations translates to a
center-outward ordering... | stat.ME | the notion of data depth has long been in use to obtain robust location and scale estimates in a multivariate setting the depth of an observation is a measure of its centrality with respect to a data set or a distribution the data depths of a set of multivariate observations translates to a centeroutward ordering of th... | [['the', 'notion', 'of', 'data', 'depth', 'has', 'long', 'been', 'in', 'use', 'to', 'obtain', 'robust', 'location', 'and', 'scale', 'estimates', 'in', 'a', 'multivariate', 'setting', 'the', 'depth', 'of', 'an', 'observation', 'is', 'a', 'measure', 'of', 'its', 'centrality', 'with', 'respect', 'to', 'a', 'data', 'set', ... | [-0.04996068346812282, 0.03222409516394494, -0.11793663176570753, 0.08610329464260243, -0.08210548572512993, -0.10208548049355835, 0.03889050163994651, 0.38279766507100227, -0.25423841411338094, -0.3305655783353655, 0.1633974525801361, -0.30113160638445485, -0.08298756264090582, 0.193970755235357, -0.11295594975971364,... |
708.1108 | Linear Depenedences of Van Der Waals, Covalent and Valence Shell Radii
of Atoms of Groups 1a - 8a on their Bohr Radii | An earlier finding that the van der waals radii are related to their de
broglie wavelengths for some non-metallic elements has been extended here to
show that in fact, they vary linearly with the ground state bohr radii for all
the elements of groups 1a to 8 a. Similarly, the valence shell radii and the
covalent radi... | physics.gen-ph physics.chem-ph | an earlier finding that the van der waals radii are related to their de broglie wavelengths for some nonmetallic elements has been extended here to show that in fact they vary linearly with the ground state bohr radii for all the elements of groups 1a to 8 a similarly the valence shell radii and the covalent radii are ... | [['an', 'earlier', 'finding', 'that', 'the', 'van', 'der', 'waals', 'radii', 'are', 'related', 'to', 'their', 'de', 'broglie', 'wavelengths', 'for', 'some', 'nonmetallic', 'elements', 'has', 'been', 'extended', 'here', 'to', 'show', 'that', 'in', 'fact', 'they', 'vary', 'linearly', 'with', 'the', 'ground', 'state', 'bo... | [-0.12673888338758843, 0.19888908739202243, -0.0712468621474857, 0.048752845203645326, -0.037426030778858276, -0.12268217211073663, -0.008131502279346543, 0.3930259832995944, -0.2351425229904375, -0.28706924961547237, 0.06338431210419262, -0.3576471276381718, -0.06501664699213247, 0.20653703246041136, -0.00433642931082... |
708.1109 | The hook fusion procedure and its generalisations | The fusion procedure provides a way to construct new solutions to the
Yang-Baxter equation. In the case of the symmetric group the fusion procedure
has been used to construct diagonal matrix elements using a decomposition of
the Young diagram into its rows or columns. We present a new construction which
decomposes th... | math.RT math.CO | the fusion procedure provides a way to construct new solutions to the yangbaxter equation in the case of the symmetric group the fusion procedure has been used to construct diagonal matrix elements using a decomposition of the young diagram into its rows or columns we present a new construction which decomposes the dia... | [['the', 'fusion', 'procedure', 'provides', 'a', 'way', 'to', 'construct', 'new', 'solutions', 'to', 'the', 'yangbaxter', 'equation', 'in', 'the', 'case', 'of', 'the', 'symmetric', 'group', 'the', 'fusion', 'procedure', 'has', 'been', 'used', 'to', 'construct', 'diagonal', 'matrix', 'elements', 'using', 'a', 'decomposi... | [-0.08937935961676495, 0.090460342440222, -0.129392852990755, 0.02775537392590195, -0.13447630568806615, -0.1075210096873343, 0.0556062873479511, 0.3791979556104967, -0.29138872360544543, -0.25541457401322465, 0.08708391727613551, -0.218247455825497, -0.17782539284821333, 0.1560530440921762, -0.07867138833472771, -0.00... |
708.111 | Discovery of coherent millisecond X-ray pulsations in Aql X-1 | We report the discovery of an episode of coherent millisecond X-ray pulsation
in the neutron star low-mass X-ray binary Aql X-1. The episode lasts for
slightly more than 150 seconds, during which the pulse frequency is consistent
with being constant. No X-ray burst or other evidence of thermonuclear burning
activity ... | astro-ph | we report the discovery of an episode of coherent millisecond xray pulsation in the neutron star lowmass xray binary aql x1 the episode lasts for slightly more than 150 seconds during which the pulse frequency is consistent with being constant no xray burst or other evidence of thermonuclear burning activity is seen in... | [['we', 'report', 'the', 'discovery', 'of', 'an', 'episode', 'of', 'coherent', 'millisecond', 'xray', 'pulsation', 'in', 'the', 'neutron', 'star', 'lowmass', 'xray', 'binary', 'aql', 'x1', 'the', 'episode', 'lasts', 'for', 'slightly', 'more', 'than', '150', 'seconds', 'during', 'which', 'the', 'pulse', 'frequency', 'is... | [-0.09043701787231839, 0.22802738983673407, -0.03414982343965676, 0.11425021719333017, -0.15392678697244264, -0.0985274543898413, 0.13107397813291755, 0.43363776498299555, -0.19778960970943443, -0.3355005608056672, 0.08250345341948559, -0.2928600684521371, -0.020012897039123345, 0.2909701185199083, -0.04064309326640795... |
708.1111 | Probing for the Cosmological Parameters with PLANCK Measurement | We investigate the constraints on cosmological parameters especially for EoS
of dark energy, inflationary parameters, neutrino mass and curvature of
universe using simulated Planck data. Firstly we determine cosmological
parameters with current observations including ESSENCE, WMAP3, Boomerang-2K2,
CBI, VSA, ACBAR, SD... | astro-ph gr-qc hep-ph hep-th | we investigate the constraints on cosmological parameters especially for eos of dark energy inflationary parameters neutrino mass and curvature of universe using simulated planck data firstly we determine cosmological parameters with current observations including essence wmap3 boomerang2k2 cbi vsa acbar sdss lrg and 2... | [['we', 'investigate', 'the', 'constraints', 'on', 'cosmological', 'parameters', 'especially', 'for', 'eos', 'of', 'dark', 'energy', 'inflationary', 'parameters', 'neutrino', 'mass', 'and', 'curvature', 'of', 'universe', 'using', 'simulated', 'planck', 'data', 'firstly', 'we', 'determine', 'cosmological', 'parameters',... | [-0.10944696097177695, 0.12551936508604775, -0.062261518444521005, 0.14811876279181213, -0.1267203428359978, -0.14606109206280155, 0.02479070562576116, 0.32230227046335735, -0.17946587504249895, -0.3923259422475153, 0.056300524279423475, -0.2925185995340278, 0.018489849097440364, 0.2022318272269331, 0.04119818021394571... |
708.1112 | Weyl functions, inverse problem and special solutions for the system
auxiliary to the nonlinear optics equation | A Borg-Marchenko type uniqueness theorem (in terms of the Weyl function) is
obtained here for the system auxiliary to the N-wave equation. A procedure to
solve inverse problem is used for this purpose. The asymptotic condition on the
Weyl function, under which the inverse problem is uniquely solvable, is
completed by... | math-ph math.CA math.MP | a borgmarchenko type uniqueness theorem in terms of the weyl function is obtained here for the system auxiliary to the nwave equation a procedure to solve inverse problem is used for this purpose the asymptotic condition on the weyl function under which the inverse problem is uniquely solvable is completed by the new a... | [['a', 'borgmarchenko', 'type', 'uniqueness', 'theorem', 'in', 'terms', 'of', 'the', 'weyl', 'function', 'is', 'obtained', 'here', 'for', 'the', 'system', 'auxiliary', 'to', 'the', 'nwave', 'equation', 'a', 'procedure', 'to', 'solve', 'inverse', 'problem', 'is', 'used', 'for', 'this', 'purpose', 'the', 'asymptotic', 'c... | [-0.1545289679083462, 0.018259745781845183, -0.10450683587102913, 0.07492405987417727, -0.10611691221813946, -0.1443331623039044, 0.013005063608836602, 0.2727382360574077, -0.3076883360524388, -0.25907922432045727, 0.16171747064286404, -0.23814373875639455, -0.15187896419243485, 0.1868599727475906, -0.04188426305065114... |
708.1113 | Distribution of periodic torus orbits and Duke's theorem for cubic
fields | We study periodic torus orbits on spaces of lattices. Using the action of the
group of adelic points of the underlying tori, we define a natural equivalence
relation on these orbits, and show that the equivalence classes become
uniformly distributed. This is a cubic analogue of Duke's theorem about the
distribution o... | math.NT math.DS | we study periodic torus orbits on spaces of lattices using the action of the group of adelic points of the underlying tori we define a natural equivalence relation on these orbits and show that the equivalence classes become uniformly distributed this is a cubic analogue of dukes theorem about the distribution of close... | [['we', 'study', 'periodic', 'torus', 'orbits', 'on', 'spaces', 'of', 'lattices', 'using', 'the', 'action', 'of', 'the', 'group', 'of', 'adelic', 'points', 'of', 'the', 'underlying', 'tori', 'we', 'define', 'a', 'natural', 'equivalence', 'relation', 'on', 'these', 'orbits', 'and', 'show', 'that', 'the', 'equivalence', ... | [-0.22532987615300548, 0.09811769627655546, -0.12147463478434545, 0.09840992383925547, -0.05670583293112552, -0.08861146355296573, 0.03155277015314971, 0.3163458998832438, -0.2675013021271453, -0.21419885894681653, 0.09976505506564823, -0.2724103706064992, -0.13262684134225178, 0.24195672240522173, -0.12546252528539834... |
708.1114 | Integrability of a conducting elastic rod in a magnetic field | We consider the equilibrium equations for a conducting elastic rod placed in
a uniform magnetic field, motivated by the problem of electrodynamic space
tethers. When expressed in body coordinates the equations are found to sit in a
hierarchy of non-canonical Hamiltonian systems involving an increasing number
of vecto... | math-ph math.MP | we consider the equilibrium equations for a conducting elastic rod placed in a uniform magnetic field motivated by the problem of electrodynamic space tethers when expressed in body coordinates the equations are found to sit in a hierarchy of noncanonical hamiltonian systems involving an increasing number of vector fie... | [['we', 'consider', 'the', 'equilibrium', 'equations', 'for', 'a', 'conducting', 'elastic', 'rod', 'placed', 'in', 'a', 'uniform', 'magnetic', 'field', 'motivated', 'by', 'the', 'problem', 'of', 'electrodynamic', 'space', 'tethers', 'when', 'expressed', 'in', 'body', 'coordinates', 'the', 'equations', 'are', 'found', '... | [-0.19197660301186437, 0.16674150118657952, -0.050562626352612244, 0.04780837577621801, -0.08162836095981625, -0.13325907754521055, -0.03765986427939665, 0.3371794173516423, -0.28771905376609547, -0.24461359711481728, 0.06663536330957123, -0.25505572890144695, -0.12706419969319804, 0.1679664370716067, -0.02387169199849... |
708.1115 | Remark on fundamental groups and effective Diophantine methods for
hyperbolic curves | We discuss how non-commutative fundamental groups could eventually contribute
to algorithms for finding rational points on hyperbolic curves.
| math.NT math.AG | we discuss how noncommutative fundamental groups could eventually contribute to algorithms for finding rational points on hyperbolic curves | [['we', 'discuss', 'how', 'noncommutative', 'fundamental', 'groups', 'could', 'eventually', 'contribute', 'to', 'algorithms', 'for', 'finding', 'rational', 'points', 'on', 'hyperbolic', 'curves']] | [-0.17768595233145687, 0.1102272348685397, -0.15978287532925606, 0.16176333454334074, -0.15332563542243507, -0.16491817817505863, 0.13126875936157173, 0.3913884965909852, -0.3207153288854493, -0.22661022796011013, 0.08148495426091056, -0.27145195757556295, -0.24254107180361947, 0.342253881196181, -0.226196785353952, -0... |
708.1116 | A variant of the Recoil Growth algorithm to generate multi-polymer
systems | The Recoil Growth algorithm, proposed in 1999 by Consta et al., is one of the
most efficient algorithm available in the literature to sample from a
multi-polymer system. Such problems are closely related to the generation of
self-avoiding paths. In this paper, we study a variant of the original Recoil
Growth algorith... | cs.CE cond-mat.stat-mech | the recoil growth algorithm proposed in 1999 by consta et al is one of the most efficient algorithm available in the literature to sample from a multipolymer system such problems are closely related to the generation of selfavoiding paths in this paper we study a variant of the original recoil growth algorithm where we... | [['the', 'recoil', 'growth', 'algorithm', 'proposed', 'in', '1999', 'by', 'consta', 'et', 'al', 'is', 'one', 'of', 'the', 'most', 'efficient', 'algorithm', 'available', 'in', 'the', 'literature', 'to', 'sample', 'from', 'a', 'multipolymer', 'system', 'such', 'problems', 'are', 'closely', 'related', 'to', 'the', 'genera... | [-0.06847246856761909, 0.046910183546945046, -0.08307662758847524, 0.061457255861610854, -0.1225984894004095, -0.12262095035472458, 0.08599663101277664, 0.35305212734591795, -0.2732704839457698, -0.3398040655248482, 0.0878408965473106, -0.21434671000081942, -0.17809238820550366, 0.23076341976198034, -0.1012451708906355... |
708.1117 | The cosine law at the atomic scale: Toward realistic simulations of
Knudsen diffusion | We propose to revisit the diffusion of atoms in the Knudsen regime in terms
of a complex dynamical reflection process. By means of molecular dynamics
simulation we emphasize the asymptotic nature of the cosine law of reflection
at the atomic scale, and carefully analyze the resulting strong correlations in
the reflec... | cond-mat.stat-mech nlin.CD | we propose to revisit the diffusion of atoms in the knudsen regime in terms of a complex dynamical reflection process by means of molecular dynamics simulation we emphasize the asymptotic nature of the cosine law of reflection at the atomic scale and carefully analyze the resulting strong correlations in the reflection... | [['we', 'propose', 'to', 'revisit', 'the', 'diffusion', 'of', 'atoms', 'in', 'the', 'knudsen', 'regime', 'in', 'terms', 'of', 'a', 'complex', 'dynamical', 'reflection', 'process', 'by', 'means', 'of', 'molecular', 'dynamics', 'simulation', 'we', 'emphasize', 'the', 'asymptotic', 'nature', 'of', 'the', 'cosine', 'law', ... | [-0.1536671471219781, 0.12633988686970302, -0.10886717497647463, 0.0372032972699454, -0.04286304945228519, -0.05177507672847791, 0.053192234526459985, 0.358803148739613, -0.3142570243984625, -0.26197371852921914, 0.06974748435691204, -0.2608099483199172, -0.14294284517661884, 0.14663559364175405, 0.00941208279998666, 0... |
708.1118 | Flavour symmetry breaking and meson masses | The axial-vector Ward-Takahashi identity is used to derive mass formulae for
neutral pseudoscalar mesons. Flavour symmetry breaking entails non-ideal
flavour content for these states. Adding that the \eta^\prime is not a
Goldstone mode, exact chiral-limit relations are developed from the identity.
They connect the dr... | nucl-th hep-ex hep-lat hep-ph nucl-ex | the axialvector wardtakahashi identity is used to derive mass formulae for neutral pseudoscalar mesons flavour symmetry breaking entails nonideal flavour content for these states adding that the etaprime is not a goldstone mode exact chirallimit relations are developed from the identity they connect the dressedquark pr... | [['the', 'axialvector', 'wardtakahashi', 'identity', 'is', 'used', 'to', 'derive', 'mass', 'formulae', 'for', 'neutral', 'pseudoscalar', 'mesons', 'flavour', 'symmetry', 'breaking', 'entails', 'nonideal', 'flavour', 'content', 'for', 'these', 'states', 'adding', 'that', 'the', 'etaprime', 'is', 'not', 'a', 'goldstone',... | [-0.13229392818442878, 0.23371417751273504, -0.0846115331183557, 0.12341616962014045, -0.10114070173518883, -0.12910597959878564, 0.03922326284348322, 0.3085920586539754, -0.19995453230496069, -0.2414839540517236, 0.048776376520781296, -0.3018469388286273, -0.09507755925323567, 0.10333187915063624, 0.05016536670522871,... |
708.1119 | Spiral Disk Opacity from Occulting Galaxy Pairs in the Sloan Digital Sky
Survey | A spiral galaxy partially ovelapping a more distant elliptical offers an
unique opportunity to measure the dust extinction in the foreground spiral.
From the Sloan Digital Sky Survey DR4 spectroscopic sample, we selected 83
occulting galaxy pairs and measured disk opacity over the redshift range z =
0.0-0.2 with th... | astro-ph | a spiral galaxy partially ovelapping a more distant elliptical offers an unique opportunity to measure the dust extinction in the foreground spiral from the sloan digital sky survey dr4 spectroscopic sample we selected 83 occulting galaxy pairs and measured disk opacity over the redshift range z 0002 with the goal to d... | [['a', 'spiral', 'galaxy', 'partially', 'ovelapping', 'a', 'more', 'distant', 'elliptical', 'offers', 'an', 'unique', 'opportunity', 'to', 'measure', 'the', 'dust', 'extinction', 'in', 'the', 'foreground', 'spiral', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'dr4', 'spectroscopic', 'sample', 'we', 'selected', ... | [-0.0453478867162226, 0.04413377732568834, -0.09030563429515395, 0.09085100166706575, -0.12788769117453033, -0.003968813392437167, 0.03009334110034009, 0.44953328516748214, -0.2162181586606635, -0.3324204342739864, 0.03850341164895023, -0.30087121528883776, -0.03329453715433677, 0.19451488681810183, -0.0413883355673816... |
708.112 | Molecular gas in high-velocity clouds: revisited scenario | We report a new search for 12CO(1-0) emission in high-velocity clouds (HVCs)
performed with the IRAM 30 m telescope. This search was motivated by the recent
detection of cold dust emission in the HVCs of Complex C. Despite a spatial
resolution which is three times better and sensitivity twice as good compared
to prev... | astro-ph | we report a new search for 12co10 emission in highvelocity clouds hvcs performed with the iram 30 m telescope this search was motivated by the recent detection of cold dust emission in the hvcs of complex c despite a spatial resolution which is three times better and sensitivity twice as good compared to previous studi... | [['we', 'report', 'a', 'new', 'search', 'for', '12co10', 'emission', 'in', 'highvelocity', 'clouds', 'hvcs', 'performed', 'with', 'the', 'iram', '30', 'm', 'telescope', 'this', 'search', 'was', 'motivated', 'by', 'the', 'recent', 'detection', 'of', 'cold', 'dust', 'emission', 'in', 'the', 'hvcs', 'of', 'complex', 'c', ... | [-0.05777484015373266, 0.11800185227839158, 0.006236154335162159, 0.05713723562914022, -0.013883237409764075, -0.06595338383330858, 0.053068933247446916, 0.43554430238565, -0.1479028333279886, -0.3367340067736081, 0.05870755429833247, -0.26709067361869376, 0.018148905496658534, 0.13754299281087393, 0.02383762457435137,... |
708.1121 | Next-to-leading order corrections in exclusive meson production | We analyze in detail the size of next-to-leading order corrections to hard
exclusive meson production within the collinear factorization approach.
Corrections to the cross section are found to be huge at small xB and
substantial in typical fixed-target kinematics. With the models we take for
nucleon helicity-flip dis... | hep-ph | we analyze in detail the size of nexttoleading order corrections to hard exclusive meson production within the collinear factorization approach corrections to the cross section are found to be huge at small xb and substantial in typical fixedtarget kinematics with the models we take for nucleon helicityflip distributio... | [['we', 'analyze', 'in', 'detail', 'the', 'size', 'of', 'nexttoleading', 'order', 'corrections', 'to', 'hard', 'exclusive', 'meson', 'production', 'within', 'the', 'collinear', 'factorization', 'approach', 'corrections', 'to', 'the', 'cross', 'section', 'are', 'found', 'to', 'be', 'huge', 'at', 'small', 'xb', 'and', 's... | [-0.09268542320378834, 0.20431234219688035, -0.08342747074285788, 0.16448081337148324, -0.029186782077886164, -0.10729031410578284, -0.0019350002098473765, 0.3841014248540714, -0.2325151756827143, -0.24409098847813548, -0.023762286746031827, -0.3434814607719004, 0.05956774798964727, 0.10281870909827939, 0.0504141635499... |
708.1122 | Bose-Einstein study of position-momentum correlations of charged pions
in hadronic Z0 decays | A study of Bose-Einstein correlations in pairs of identically charged pions
produced in e+e- annihilations at the Z0 peak has been performed for the first
time assuming a non-static emitting source. The results are based on the high
statistics data obtained with the OPAL detector at LEP. The correlation
functions hav... | hep-ex | a study of boseeinstein correlations in pairs of identically charged pions produced in ee annihilations at the z0 peak has been performed for the first time assuming a nonstatic emitting source the results are based on the high statistics data obtained with the opal detector at lep the correlation functions have been a... | [['a', 'study', 'of', 'boseeinstein', 'correlations', 'in', 'pairs', 'of', 'identically', 'charged', 'pions', 'produced', 'in', 'ee', 'annihilations', 'at', 'the', 'z0', 'peak', 'has', 'been', 'performed', 'for', 'the', 'first', 'time', 'assuming', 'a', 'nonstatic', 'emitting', 'source', 'the', 'results', 'are', 'based... | [-0.09875646538777752, 0.17696542795645948, -0.11117926209457156, 0.11714425875614679, 0.012193664320863334, -0.07571280146198935, -0.032605720063571465, 0.40796453177799225, -0.20771513449265652, -0.3235882708116047, -0.031013894016735707, -0.3725411761302076, 0.08186417958666352, 0.16188101198535176, 0.08158855070203... |
708.1123 | Dynamical glass transition: critical temperature T_c and memory kernel
in MD-simulated Ni_{0.8}Zr_{0.2} | We use molecular dynamics computer simulations to investigate a critical
temperature T_c for a dynamical glass transition as proposed by the
mode-coupling theory (MCT) of dense liquids in a glass forming
Ni_{0.8}Zr_{0.2}-system. The critical temperature T_c are analyzed from
different quantities and checked the consi... | cond-mat.mtrl-sci cond-mat.stat-mech | we use molecular dynamics computer simulations to investigate a critical temperature t_c for a dynamical glass transition as proposed by the modecoupling theory mct of dense liquids in a glass forming ni_08zr_02system the critical temperature t_c are analyzed from different quantities and checked the consistency of the... | [['we', 'use', 'molecular', 'dynamics', 'computer', 'simulations', 'to', 'investigate', 'a', 'critical', 'temperature', 't_c', 'for', 'a', 'dynamical', 'glass', 'transition', 'as', 'proposed', 'by', 'the', 'modecoupling', 'theory', 'mct', 'of', 'dense', 'liquids', 'in', 'a', 'glass', 'forming', 'ni_08zr_02system', 'the... | [-0.09704430092126132, 0.20037338198162616, -0.1118106541223824, 0.030825461943168195, 0.0321684174798429, -0.12297226907801814, 0.06589410990825854, 0.302297028452158, -0.24061598716303706, -0.22242736800573767, 0.11758335749735124, -0.2944227711716667, -0.1034179611201398, 0.1271752244606614, 0.05189699409476816, 0.0... |
708.1124 | Warp diffusion in accretion discs: a numerical investigation | In this paper we explore numerically the evolution of a warped accretion
disc. Here, we focus here on the regime where the warp evolves diffusively. By
comparing the numerical results to a simple diffusion model, we are able to
determine the diffusion coefficient of the warp, $\alpha_2$, as a function of
the relevant... | astro-ph | in this paper we explore numerically the evolution of a warped accretion disc here we focus here on the regime where the warp evolves diffusively by comparing the numerical results to a simple diffusion model we are able to determine the diffusion coefficient of the warp alpha_2 as a function of the relevant disc param... | [['in', 'this', 'paper', 'we', 'explore', 'numerically', 'the', 'evolution', 'of', 'a', 'warped', 'accretion', 'disc', 'here', 'we', 'focus', 'here', 'on', 'the', 'regime', 'where', 'the', 'warp', 'evolves', 'diffusively', 'by', 'comparing', 'the', 'numerical', 'results', 'to', 'a', 'simple', 'diffusion', 'model', 'we'... | [-0.10892100621851722, 0.12586329766822704, -0.04558985648510678, 0.06681333959649702, -0.07643622833457157, -0.08548081584333383, -0.03377941624551256, 0.35605472903307916, -0.2561100240458142, -0.2827991329595915, 0.11967551856996961, -0.23788297862804436, -0.12820608781771148, 0.1877224427929565, -0.0200754131135120... |
708.1125 | N=2 supersymmetric unconstrained matrix GNLS hierarchies are consistent | We develop a pseudo-differential approach to the N=2 supersymmetric
unconstrained matrix (k|n,m)-Generalized Nonlinear Schroedinger hierarchies and
prove consistency of the corresponding Lax-pair representation
(nlin.SI/0201026). Furthermore, we establish their equivalence to the
integrable hierarchies derived in the... | nlin.SI hep-th math-ph math.MP | we develop a pseudodifferential approach to the n2 supersymmetric unconstrained matrix knmgeneralized nonlinear schroedinger hierarchies and prove consistency of the corresponding laxpair representation nlinsi0201026 furthermore we establish their equivalence to the integrable hierarchies derived in the superalgebraic ... | [['we', 'develop', 'a', 'pseudodifferential', 'approach', 'to', 'the', 'n2', 'supersymmetric', 'unconstrained', 'matrix', 'knmgeneralized', 'nonlinear', 'schroedinger', 'hierarchies', 'and', 'prove', 'consistency', 'of', 'the', 'corresponding', 'laxpair', 'representation', 'nlinsi0201026', 'furthermore', 'we', 'establi... | [-0.12325948110576403, 0.06984285888744526, -0.04628745425429385, 0.17714867008834193, -0.1287620703381944, -0.176753210669415, -0.01684928912732561, 0.3363430890238891, -0.3051313186474776, -0.25720390570113216, 0.10726604278207268, -0.2688557773954787, -0.21075128738657903, 0.08830761259137573, -0.0854044968767439, 0... |
708.1126 | Janus particles with coupled electric and magnetic moments make a
disordered magneto-electric medium | We demonstrate that by combining permanent electric and magnetic moments in
particles, it is possible to realize a new type of medium that allows for a
cross-correlation between electric and magnetic properties of matter, known as
magnetoelectric coupling. Magnetoelectric materials have so far been restricted
to syst... | cond-mat.mtrl-sci | we demonstrate that by combining permanent electric and magnetic moments in particles it is possible to realize a new type of medium that allows for a crosscorrelation between electric and magnetic properties of matter known as magnetoelectric coupling magnetoelectric materials have so far been restricted to systems th... | [['we', 'demonstrate', 'that', 'by', 'combining', 'permanent', 'electric', 'and', 'magnetic', 'moments', 'in', 'particles', 'it', 'is', 'possible', 'to', 'realize', 'a', 'new', 'type', 'of', 'medium', 'that', 'allows', 'for', 'a', 'crosscorrelation', 'between', 'electric', 'and', 'magnetic', 'properties', 'of', 'matter... | [-0.1880739748541435, 0.25191311715637066, -0.021919195582582193, 0.010462499988286501, -0.12949227868706326, -0.11225962652613154, 0.0001355766302863644, 0.46556522848814813, -0.2615882122931494, -0.3173763063651594, 0.021150689615751617, -0.26780137787219166, -0.18560896171733143, 0.18104080665084024, 0.0585944123449... |
708.1127 | Coincidence measurement of residues and light particles in the reaction
56Fe+p at 1 GeV per nucleon with SPALADIN | The spallation of $^{56}$Fe in collisions with hydrogen at 1 A GeV has been
studied in inverse kinematics with the large-aperture setup SPALADIN at GSI.
Coincidences of residues with low-center-of-mass kinetic energy light particles
and fragments have been measured allowing the decomposition of the total
reaction cro... | nucl-ex | the spallation of 56fe in collisions with hydrogen at 1 a gev has been studied in inverse kinematics with the largeaperture setup spaladin at gsi coincidences of residues with lowcenterofmass kinetic energy light particles and fragments have been measured allowing the decomposition of the total reaction crosssection in... | [['the', 'spallation', 'of', '56fe', 'in', 'collisions', 'with', 'hydrogen', 'at', '1', 'a', 'gev', 'has', 'been', 'studied', 'in', 'inverse', 'kinematics', 'with', 'the', 'largeaperture', 'setup', 'spaladin', 'at', 'gsi', 'coincidences', 'of', 'residues', 'with', 'lowcenterofmass', 'kinetic', 'energy', 'light', 'parti... | [-0.04993402215768583, 0.15861994712225472, -0.12788620106706125, 0.09788248048474392, 0.0010588625738212917, -0.11337941848323681, -0.0362477513437625, 0.3953715694214528, -0.20775233513559216, -0.33657708157164357, 0.018503796073491684, -0.31475241396886605, 0.03777411355210158, 0.16390545986553964, 0.068225671739007... |
708.1128 | Calculations of the Exciton Coupling Elements Between the DNA Bases
Using the Transition Density Cube Method | Excited states of the of the double-stranded DNA model
(A)$_{12}\cdot$(T)_{12} were calculated in the framework of the exciton theory.
The off-diagonal elements of the exciton matrix were calculated using the
transition densities and ideal dipole approximation associated with the lowest
energy $\pi\pi^{*}$ excitation... | cond-mat.soft | excited states of the of the doublestranded dna model a_12cdott_12 were calculated in the framework of the exciton theory the offdiagonal elements of the exciton matrix were calculated using the transition densities and ideal dipole approximation associated with the lowest energy pipi excitations of the individual nucl... | [['excited', 'states', 'of', 'the', 'of', 'the', 'doublestranded', 'dna', 'model', 'a_12cdott_12', 'were', 'calculated', 'in', 'the', 'framework', 'of', 'the', 'exciton', 'theory', 'the', 'offdiagonal', 'elements', 'of', 'the', 'exciton', 'matrix', 'were', 'calculated', 'using', 'the', 'transition', 'densities', 'and',... | [-0.09767160237754217, 0.1772809671154162, -0.06872809879788039, 0.07069781310185119, 0.08864490214634586, -0.06028056614990304, 0.041735958105565664, 0.3454408297936122, -0.24305942111757692, -0.3052261633764919, -0.01113823364249657, -0.31624045325359246, -0.08063407554417043, 0.10938357347035194, 0.11336646445865349... |
708.1129 | Experimental realization of a quantum game on a one-way quantum computer | We report the first demonstration of a quantum game on an all-optical one-way
quantum computer. Following a recent theoretical proposal we implement a
quantum version of Prisoner's Dilemma, where the quantum circuit is realized by
a 4-qubit box-cluster configuration and the player's local strategies by
measurements p... | quant-ph | we report the first demonstration of a quantum game on an alloptical oneway quantum computer following a recent theoretical proposal we implement a quantum version of prisoners dilemma where the quantum circuit is realized by a 4qubit boxcluster configuration and the players local strategies by measurements performed o... | [['we', 'report', 'the', 'first', 'demonstration', 'of', 'a', 'quantum', 'game', 'on', 'an', 'alloptical', 'oneway', 'quantum', 'computer', 'following', 'a', 'recent', 'theoretical', 'proposal', 'we', 'implement', 'a', 'quantum', 'version', 'of', 'prisoners', 'dilemma', 'where', 'the', 'quantum', 'circuit', 'is', 'real... | [-0.136013243726433, 0.11290621155007272, -0.10487462278201007, 0.006666854407021039, -0.008054378025536968, -0.20780899146095264, 0.11649522529969122, 0.39818580418305344, -0.22355731486256214, -0.28621937821857457, 0.04626478296758737, -0.19861625563786472, -0.18505961799907478, 0.24022961981583732, -0.09116817258168... |
708.113 | Complex Datasets and Inverse Problems. Tomography, Networks and Beyond | This book is a collection of papers dedicated to the memory of Yehuda Vardi.
Yehuda was the chair of the Department of Statistics of Rutgers University when
he passed away unexpectedly on January 13, 2005. On October 21--22, 2005, some
150 leading scholars from many different fields, including statistics,
telecommuni... | math.ST stat.TH | this book is a collection of papers dedicated to the memory of yehuda vardi yehuda was the chair of the department of statistics of rutgers university when he passed away unexpectedly on january 13 2005 on october 2122 2005 some 150 leading scholars from many different fields including statistics telecommunications bio... | [['this', 'book', 'is', 'a', 'collection', 'of', 'papers', 'dedicated', 'to', 'the', 'memory', 'of', 'yehuda', 'vardi', 'yehuda', 'was', 'the', 'chair', 'of', 'the', 'department', 'of', 'statistics', 'of', 'rutgers', 'university', 'when', 'he', 'passed', 'away', 'unexpectedly', 'on', 'january', '13', '2005', 'on', 'oct... | [-0.05160113448392223, 0.07589296328186403, -0.04365067529206056, 0.08253498398044848, -0.10796608303478232, -0.144359679815921, 0.017339496125993826, 0.36126687555584347, -0.25371967150379765, -0.3955053318839534, 0.17566384268751933, -0.3386038686131382, -0.15961260041605668, 0.24574195953872585, -0.1156301661481739,... |
708.1131 | Global attraction to solitary waves for Klein-Gordon equation with mean
field interaction | We consider a U(1)-invariant nonlinear Klein-Gordon equation in dimension one
or larger, self-interacting via the mean field mechanism. We analyze the
long-time asymptotics of finite energy solutions and prove that, under certain
generic assumptions, each solution converges (as time goes to infinity) to the
two-dimen... | math-ph math.MP | we consider a u1invariant nonlinear kleingordon equation in dimension one or larger selfinteracting via the mean field mechanism we analyze the longtime asymptotics of finite energy solutions and prove that under certain generic assumptions each solution converges as time goes to infinity to the twodimensional set of a... | [['we', 'consider', 'a', 'u1invariant', 'nonlinear', 'kleingordon', 'equation', 'in', 'dimension', 'one', 'or', 'larger', 'selfinteracting', 'via', 'the', 'mean', 'field', 'mechanism', 'we', 'analyze', 'the', 'longtime', 'asymptotics', 'of', 'finite', 'energy', 'solutions', 'and', 'prove', 'that', 'under', 'certain', '... | [-0.14269024851731957, 0.13735247551153104, -0.08021261602019271, 0.08395268644827107, -0.07418662458347777, -0.13962264904752375, -0.02497892005989949, 0.28138226258258026, -0.30539339616894723, -0.206750138203303, 0.09200424304697663, -0.30314464564124743, -0.12068974796682597, 0.14506767900971074, 0.0215180782973766... |
708.1132 | Peculiar acceleration | It has been proposed recently to observe the change in cosmological redshift
of distant galaxies or quasars with the next generation of large telescope and
ultra-stable spectrographs (the so-called Sandage-Loeb test). Here we
investigate the possibility of observing the change in peculiar velocity in
nearby clusters ... | astro-ph | it has been proposed recently to observe the change in cosmological redshift of distant galaxies or quasars with the next generation of large telescope and ultrastable spectrographs the socalled sandageloeb test here we investigate the possibility of observing the change in peculiar velocity in nearby clusters and gala... | [['it', 'has', 'been', 'proposed', 'recently', 'to', 'observe', 'the', 'change', 'in', 'cosmological', 'redshift', 'of', 'distant', 'galaxies', 'or', 'quasars', 'with', 'the', 'next', 'generation', 'of', 'large', 'telescope', 'and', 'ultrastable', 'spectrographs', 'the', 'socalled', 'sandageloeb', 'test', 'here', 'we',... | [-0.09298311297090785, 0.12931496741109957, -0.10082117095589638, 0.06793989550938169, -0.15021491491095593, -0.051026008792862454, 0.014413946736303548, 0.39878628971756147, -0.22356049075562467, -0.3317126713653085, 0.04546067578923358, -0.26536050079370377, -0.08241271379313642, 0.19097368622208716, -0.0101994390047... |
708.1133 | The quasiparticle spectral function in doped graphene | We calculate the real and imaginary electron self-energy as well as the
quasiparticle spectral function in doped graphene taking into account
electron-electron interaction in the leading order dynamically screened Coulomb
coupling. Our theory provides the basis for calculating {\it all} one-electron
properties of ext... | cond-mat.mes-hall cond-mat.dis-nn | we calculate the real and imaginary electron selfenergy as well as the quasiparticle spectral function in doped graphene taking into account electronelectron interaction in the leading order dynamically screened coulomb coupling our theory provides the basis for calculating it all oneelectron properties of extrinsic gr... | [['we', 'calculate', 'the', 'real', 'and', 'imaginary', 'electron', 'selfenergy', 'as', 'well', 'as', 'the', 'quasiparticle', 'spectral', 'function', 'in', 'doped', 'graphene', 'taking', 'into', 'account', 'electronelectron', 'interaction', 'in', 'the', 'leading', 'order', 'dynamically', 'screened', 'coulomb', 'couplin... | [-0.12924078577146916, 0.12642374274494883, -0.09964724109446692, 0.1186805901189263, -0.0014921751354340014, -0.15428593115123745, 0.06894250177768069, 0.37717201460439426, -0.2187352908959428, -0.2867674993780943, -0.09518034054877257, -0.38156063525149453, -0.15910957767986333, 0.1720006402254432, 0.0881949452335362... |
708.1134 | Quantum transport in semiconductor quantum dot superlattices:
electron-phonon resonances and polaron effects | Electron transport in periodic quantum dot arrays in the presence of
interactions with phonons was investigated using the formalism of
nonequilibrium Green's functions. The self-consistent Born approximation was
used to model the self-energies. Its validity was checked by comparison with
the results obtained by direc... | cond-mat.mes-hall | electron transport in periodic quantum dot arrays in the presence of interactions with phonons was investigated using the formalism of nonequilibrium greens functions the selfconsistent born approximation was used to model the selfenergies its validity was checked by comparison with the results obtained by direct diago... | [['electron', 'transport', 'in', 'periodic', 'quantum', 'dot', 'arrays', 'in', 'the', 'presence', 'of', 'interactions', 'with', 'phonons', 'was', 'investigated', 'using', 'the', 'formalism', 'of', 'nonequilibrium', 'greens', 'functions', 'the', 'selfconsistent', 'born', 'approximation', 'was', 'used', 'to', 'model', 't... | [-0.1339176949650909, 0.16750796295915885, -0.08476769777189475, 0.08838928041036408, -0.002356071383334123, -0.1056439861541805, 0.03527012600366456, 0.3554866308859812, -0.21883231511291784, -0.28665447327045673, -0.0031584641300679115, -0.3085098317227302, -0.09987364601208053, 0.19723256884847218, 0.060679308004462... |
708.1135 | Charge transport in arrays of PbSe nanocrystals | We report electrical transport measurements of arrays of PbSe nanocrystals
forming the channels of field effect transistors. We measure the current in
these devices as a function of source-drain voltage, gate voltage and
temperature. Annealing is necessary to observe measurable current after which a
simple model of h... | cond-mat.mes-hall | we report electrical transport measurements of arrays of pbse nanocrystals forming the channels of field effect transistors we measure the current in these devices as a function of sourcedrain voltage gate voltage and temperature annealing is necessary to observe measurable current after which a simple model of hopping... | [['we', 'report', 'electrical', 'transport', 'measurements', 'of', 'arrays', 'of', 'pbse', 'nanocrystals', 'forming', 'the', 'channels', 'of', 'field', 'effect', 'transistors', 'we', 'measure', 'the', 'current', 'in', 'these', 'devices', 'as', 'a', 'function', 'of', 'sourcedrain', 'voltage', 'gate', 'voltage', 'and', '... | [-0.1560732194910354, 0.2049573125919645, -0.0188797280141266, 0.009382980469636983, 0.05702485844759816, -0.1667407633305141, 0.12907128937744036, 0.3906269935527589, -0.26458634385589236, -0.3433540338286903, -0.01186819652822323, -0.3243936520842154, -0.0791334619223163, 0.19344676980640876, 0.010448289109484815, 0.... |
708.1136 | Spatial effects on the speed and reliability of protein-DNA search | Strong experimental and theoretical evidence shows that transcription factors
and other specific DNA-binding proteins find their sites using a two-mode
search: alternating between 3D diffusion through the cell and 1D sliding along
the DNA. We consider the role spatial effects in the mechanism on two different
scales.... | q-bio.BM | strong experimental and theoretical evidence shows that transcription factors and other specific dnabinding proteins find their sites using a twomode search alternating between 3d diffusion through the cell and 1d sliding along the dna we consider the role spatial effects in the mechanism on two different scales first ... | [['strong', 'experimental', 'and', 'theoretical', 'evidence', 'shows', 'that', 'transcription', 'factors', 'and', 'other', 'specific', 'dnabinding', 'proteins', 'find', 'their', 'sites', 'using', 'a', 'twomode', 'search', 'alternating', 'between', '3d', 'diffusion', 'through', 'the', 'cell', 'and', '1d', 'sliding', 'al... | [-0.10537091644321818, 0.14366081928431124, -0.01293286975904754, 0.09357178033323868, -0.05427939838604865, -0.15498733533001163, 0.10233796448957902, 0.40581458779449414, -0.25425897168404443, -0.33035950989621443, 0.04838418483907334, -0.26270591628612816, -0.20742116933660126, 0.20550823656035724, 0.040408844685482... |
708.1137 | Quantum Walks on a Random Environment | Quantum walks are considered in a one-dimensional random medium characterized
by static or dynamic disorder. Quantum interference for static disorder can
lead to Anderson localization which completely hinders the quantum walk and it
is contrasted with the decoherence effect of dynamic disorder having strength
W, wher... | quant-ph cond-mat.dis-nn | quantum walks are considered in a onedimensional random medium characterized by static or dynamic disorder quantum interference for static disorder can lead to anderson localization which completely hinders the quantum walk and it is contrasted with the decoherence effect of dynamic disorder having strength w where a q... | [['quantum', 'walks', 'are', 'considered', 'in', 'a', 'onedimensional', 'random', 'medium', 'characterized', 'by', 'static', 'or', 'dynamic', 'disorder', 'quantum', 'interference', 'for', 'static', 'disorder', 'can', 'lead', 'to', 'anderson', 'localization', 'which', 'completely', 'hinders', 'the', 'quantum', 'walk', '... | [-0.14844805561956398, 0.2829065102650558, -0.06739717629757158, 0.053877939095920216, 0.007118542388803801, -0.2525111985278829, 0.047916272225105486, 0.38926493557055997, -0.2851251490528182, -0.18548432832621797, 0.03620345637496865, -0.2827757797298991, -0.1632516962898971, 0.129593419345875, -0.017855745626195352,... |
708.1138 | Progressive star formation in the young SMC cluster NGC 602 | NGC 602 is a young stellar cluster located in a peripheral region of the
Small Magellanic Cloud known as the wing. Far from the main body of the galaxy
and abutting the Magellanic Bridge, the SMC's wing is characterized by low gas
and stellar content. With deep optical imaging from the Advanced Camera for
Surveys (AC... | astro-ph | ngc 602 is a young stellar cluster located in a peripheral region of the small magellanic cloud known as the wing far from the main body of the galaxy and abutting the magellanic bridge the smcs wing is characterized by low gas and stellar content with deep optical imaging from the advanced camera for surveys acs aboar... | [['ngc', '602', 'is', 'a', 'young', 'stellar', 'cluster', 'located', 'in', 'a', 'peripheral', 'region', 'of', 'the', 'small', 'magellanic', 'cloud', 'known', 'as', 'the', 'wing', 'far', 'from', 'the', 'main', 'body', 'of', 'the', 'galaxy', 'and', 'abutting', 'the', 'magellanic', 'bridge', 'the', 'smcs', 'wing', 'is', '... | [-0.03660838310389732, 0.15321130130650795, -0.06891506576731717, 0.08398243921116984, -0.11299307277162586, -0.021247327777604432, 0.03542838279765605, 0.4485597131658072, -0.16280506845461046, -0.3973407853384223, 0.07746624396482514, -0.24409596623568716, -0.04552132010165244, 0.19140622931885096, -0.081475756014502... |
708.1139 | The Quantum Hydrodynamics of the Sutherland Model | We show that the form of the chiral condition found by Abanov et al., in the
quantum hydrodyamics of the Sutherland model arises because there are two
distinct inner products with respect to which the chiral Hamitonian hermitian,
but only one with respect to which the full, non-chiral, Hamiltonian is
hermitian.
| cond-mat.str-el cond-mat.mes-hall hep-th | we show that the form of the chiral condition found by abanov et al in the quantum hydrodyamics of the sutherland model arises because there are two distinct inner products with respect to which the chiral hamitonian hermitian but only one with respect to which the full nonchiral hamiltonian is hermitian | [['we', 'show', 'that', 'the', 'form', 'of', 'the', 'chiral', 'condition', 'found', 'by', 'abanov', 'et', 'al', 'in', 'the', 'quantum', 'hydrodyamics', 'of', 'the', 'sutherland', 'model', 'arises', 'because', 'there', 'are', 'two', 'distinct', 'inner', 'products', 'with', 'respect', 'to', 'which', 'the', 'chiral', 'ham... | [-0.13030455318745227, 0.17015328970737756, -0.02234144225716591, -0.019608532625716178, -0.06053807392716408, -0.14206857718527316, -0.06664641855750233, 0.3410555797070265, -0.22694301499053837, -0.26954462747322394, 0.062344162312801925, -0.27549035333096983, -0.21257066749036313, 0.12677321335766464, -0.04746223563... |
708.114 | Liquid elasticity length, universal dynamic crossovers and glass
transition | We discuss two main universal dynamic crossovers in a liquid that correspond
to relaxation times of 1 ps and 10^{-7}--10^{-6} s. We introduce the concept of
liquid elasticity length $d_{\rm el}$. At room temperature, $d_{\rm el}$ is
several \AA in water and increases to 0.01 mm in honey and 1 mm in tar. We
discuss th... | cond-mat.dis-nn | we discuss two main universal dynamic crossovers in a liquid that correspond to relaxation times of 1 ps and 107106 s we introduce the concept of liquid elasticity length d_rm el at room temperature d_rm el is several aa in water and increases to 001 mm in honey and 1 mm in tar we discuss that on temperature decrease d... | [['we', 'discuss', 'two', 'main', 'universal', 'dynamic', 'crossovers', 'in', 'a', 'liquid', 'that', 'correspond', 'to', 'relaxation', 'times', 'of', '1', 'ps', 'and', '107106', 's', 'we', 'introduce', 'the', 'concept', 'of', 'liquid', 'elasticity', 'length', 'd_rm', 'el', 'at', 'room', 'temperature', 'd_rm', 'el', 'is... | [-0.15239743110159357, 0.22087947386458065, -0.04670519149460068, -0.002195291743246895, 0.03230764615970353, -0.16074050713161175, 0.011653231199350998, 0.3078598980580203, -0.24828139033563662, -0.2967899489555169, 0.10015243116790909, -0.3300910373359467, -0.07783338282906423, 0.109750328310342, 1.3744299808009105e-... |
708.1141 | The periodic standing-wave approximation: post-Minkowski computation | The periodic standing wave method studies circular orbits of compact objects
coupled to helically symmetric standing wave gravitational fields. From this
solution an approximation is extracted for the strong field, slowly
inspiralling motion of black holes and binary stars. Previous work on this
model has dealt with ... | gr-qc | the periodic standing wave method studies circular orbits of compact objects coupled to helically symmetric standing wave gravitational fields from this solution an approximation is extracted for the strong field slowly inspiralling motion of black holes and binary stars previous work on this model has dealt with nonli... | [['the', 'periodic', 'standing', 'wave', 'method', 'studies', 'circular', 'orbits', 'of', 'compact', 'objects', 'coupled', 'to', 'helically', 'symmetric', 'standing', 'wave', 'gravitational', 'fields', 'from', 'this', 'solution', 'an', 'approximation', 'is', 'extracted', 'for', 'the', 'strong', 'field', 'slowly', 'insp... | [-0.14101050333669468, 0.07369803265189052, -0.07714911431120419, 0.06731128313373312, -0.11007240450484042, -0.12969808049083498, -0.030675667092227233, 0.31938945845359507, -0.24007182535628632, -0.29933467852125256, 0.079084436282637, -0.26359492276581176, -0.12674967077364047, 0.2195271027277322, 0.0061488912949882... |
708.1142 | Extracting signatures of quantum criticality in the finite-temperature
behavior of many-body systems | We face the problem of detecting and featuring footprints of quantum
criticality in the finite-temperature behavior of quantum many-body systems.
Our strategy is that of comparing the phase diagram of a system displaying a
T=0 quantum phase transition with that of its classical limit, in order to
single out the genui... | cond-mat.stat-mech | we face the problem of detecting and featuring footprints of quantum criticality in the finitetemperature behavior of quantum manybody systems our strategy is that of comparing the phase diagram of a system displaying a t0 quantum phase transition with that of its classical limit in order to single out the genuinely qu... | [['we', 'face', 'the', 'problem', 'of', 'detecting', 'and', 'featuring', 'footprints', 'of', 'quantum', 'criticality', 'in', 'the', 'finitetemperature', 'behavior', 'of', 'quantum', 'manybody', 'systems', 'our', 'strategy', 'is', 'that', 'of', 'comparing', 'the', 'phase', 'diagram', 'of', 'a', 'system', 'displaying', '... | [-0.13322450122864815, 0.18294080080042405, -0.11026945993707979, 0.07922519107115239, -0.008444220054747877, -0.1509832126074677, 0.057379028699681936, 0.34526950182230326, -0.2525885547786547, -0.2607151580635536, 0.07669470014665368, -0.3072137084022265, -0.16440649575174193, 0.19145571810578735, 0.03992415742324711... |
708.1143 | The anomalous Hall Effect and magnetoresistance in the layered
ferromagnet Fe_{1/4}TaS_2: the inelastic regime | The large magnetic anisotropy in the layered ferromagnet Fe_{1/4}TaS_2 leads
to very sharp reversals of the magnetization $\bf M$ at the coercive field. We
have exploited this feature to measure the anomalous Hall effect (AHE),
focussing on the AHE conductivity $\sigma^A_{xy}$ in the inelastic regime. At
low temperat... | cond-mat.str-el cond-mat.mes-hall | the large magnetic anisotropy in the layered ferromagnet fe_14tas_2 leads to very sharp reversals of the magnetization bf m at the coercive field we have exploited this feature to measure the anomalous hall effect ahe focussing on the ahe conductivity sigmaa_xy in the inelastic regime at low temperature t 550 k sigmaa_... | [['the', 'large', 'magnetic', 'anisotropy', 'in', 'the', 'layered', 'ferromagnet', 'fe_14tas_2', 'leads', 'to', 'very', 'sharp', 'reversals', 'of', 'the', 'magnetization', 'bf', 'm', 'at', 'the', 'coercive', 'field', 'we', 'have', 'exploited', 'this', 'feature', 'to', 'measure', 'the', 'anomalous', 'hall', 'effect', 'a... | [-0.19967145561771113, 0.1921102318809039, -0.05896239632540205, 0.022046300408701543, -0.09004372629024607, -0.11100781285439772, 0.035951606401749235, 0.3260895854593078, -0.29015024648861415, -0.29932272542102994, 0.008637112173357908, -0.3286135081095692, -0.1542619122475934, 0.1918737315661215, 0.03901188269764467... |
708.1144 | Effects of Axion-Photon Mixing on Gamma-Ray Spectra from Magnetized
Astrophysical Sources | Astrophysical gamma-ray sources come in a variety of sizes and
magnetizations. We deduce general conditions under which gamma-ray spectra from
such sources would be significantly affected by axion-photon mixing. We show
that, depending on strength and coherence of the magnetic field, axion
couplings down to ~ 1/(10**... | astro-ph hep-ph | astrophysical gammaray sources come in a variety of sizes and magnetizations we deduce general conditions under which gammaray spectra from such sources would be significantly affected by axionphoton mixing we show that depending on strength and coherence of the magnetic field axion couplings down to 11013 gev can give... | [['astrophysical', 'gammaray', 'sources', 'come', 'in', 'a', 'variety', 'of', 'sizes', 'and', 'magnetizations', 'we', 'deduce', 'general', 'conditions', 'under', 'which', 'gammaray', 'spectra', 'from', 'such', 'sources', 'would', 'be', 'significantly', 'affected', 'by', 'axionphoton', 'mixing', 'we', 'show', 'that', 'd... | [-0.13095855197819475, 0.2843031088203078, -0.011450668633382285, 0.1691606014359117, -0.0976402752318256, -0.10017444201894389, 0.05118132435951297, 0.3928809200221573, -0.21827051212357088, -0.3805009219973199, 0.02158115322626985, -0.2725569375200581, -0.0064572224603212285, 0.24943576330311937, 0.038444923208528804... |
708.1145 | The prevalence of FRI radio quasars | We present deep, multi-VLA-configuration radio images for a set of 18
quasars, having redshifts between 0.36 and 2.5, from the 7C quasar survey.
Approximately one quarter of these quasars have FRI-type twin-jet structures
and the remainder are a broad range of wide angle tail, fat double, classical
double, core-jet a... | astro-ph | we present deep multivlaconfiguration radio images for a set of 18 quasars having redshifts between 036 and 25 from the 7c quasar survey approximately one quarter of these quasars have fritype twinjet structures and the remainder are a broad range of wide angle tail fat double classical double corejet and hybrid source... | [['we', 'present', 'deep', 'multivlaconfiguration', 'radio', 'images', 'for', 'a', 'set', 'of', '18', 'quasars', 'having', 'redshifts', 'between', '036', 'and', '25', 'from', 'the', '7c', 'quasar', 'survey', 'approximately', 'one', 'quarter', 'of', 'these', 'quasars', 'have', 'fritype', 'twinjet', 'structures', 'and', ... | [-0.03655921850907456, 0.07766897241938217, -0.017703413600423212, 0.17522420067488664, -0.14929733179060037, -0.10417008513970108, 0.02968760229615045, 0.5208331662647683, -0.10174214175645391, -0.33912049185741566, 0.09553603991727617, -0.2929757036718315, -0.006768430666676883, 0.22351343103138538, 0.012566471199408... |
708.1146 | Stochastic Knapsack Problem Revisited: Switch-Over Policies and Dynamic
Pricing | The stochastic knapsack has been used as a model in wide ranging applications
from dynamic resource allocation to admission control in telecommunication. In
recent years, a variation of the model has become a basic tool in studying
problems that arise in revenue management and dynamic/flexible pricing; and it
is in t... | q-fin.PR math.OC math.PR | the stochastic knapsack has been used as a model in wide ranging applications from dynamic resource allocation to admission control in telecommunication in recent years a variation of the model has become a basic tool in studying problems that arise in revenue management and dynamicflexible pricing and it is in this co... | [['the', 'stochastic', 'knapsack', 'has', 'been', 'used', 'as', 'a', 'model', 'in', 'wide', 'ranging', 'applications', 'from', 'dynamic', 'resource', 'allocation', 'to', 'admission', 'control', 'in', 'telecommunication', 'in', 'recent', 'years', 'a', 'variation', 'of', 'the', 'model', 'has', 'become', 'a', 'basic', 'to... | [-0.1078360454845548, 0.010720874808293625, -0.10911393474216444, 0.06686712724214461, -0.09771821762088441, -0.13079997662278095, 0.14757778338601907, 0.39912274858173336, -0.3205542986410378, -0.29291158877856976, 0.1981165735450417, -0.2310248512747514, -0.15008585008853761, 0.20739481726960435, -0.12207848077000928... |
708.1147 | Influence of polymer-pore interactions on translocation | We investigate the influence of polymer-pore interactions on the
translocation dynamics using Langevin dynamics simulations. An attractive
interaction can greatly improve translocation probability. At the same time, it
also increases translocation time slowly for weak attraction while exponential
dependence is observ... | cond-mat.soft cond-mat.stat-mech | we investigate the influence of polymerpore interactions on the translocation dynamics using langevin dynamics simulations an attractive interaction can greatly improve translocation probability at the same time it also increases translocation time slowly for weak attraction while exponential dependence is observed for... | [['we', 'investigate', 'the', 'influence', 'of', 'polymerpore', 'interactions', 'on', 'the', 'translocation', 'dynamics', 'using', 'langevin', 'dynamics', 'simulations', 'an', 'attractive', 'interaction', 'can', 'greatly', 'improve', 'translocation', 'probability', 'at', 'the', 'same', 'time', 'it', 'also', 'increases'... | [-0.16472335687947567, 0.19182685821493856, -0.1266852306555495, 0.07598301060686542, 0.003927040683642567, -0.1507867501570365, 0.02517329451737103, 0.4193244658972699, -0.29433169524680386, -0.2616318572807621, -0.0078035393826294324, -0.27610539592936767, -0.1028616438863111, 0.16280768476825141, 0.0632463739010262,... |
708.1148 | Automorphisms and derivations of free Poisson algebras in two variables | Let P be a free Poisson algebra in two variables over a field of
characteristic zero. We prove that the automorphisms of P are tame and that the
locally nilpotent derivations of P are triangulable.
| math.RA math.SG | let p be a free poisson algebra in two variables over a field of characteristic zero we prove that the automorphisms of p are tame and that the locally nilpotent derivations of p are triangulable | [['let', 'p', 'be', 'a', 'free', 'poisson', 'algebra', 'in', 'two', 'variables', 'over', 'a', 'field', 'of', 'characteristic', 'zero', 'we', 'prove', 'that', 'the', 'automorphisms', 'of', 'p', 'are', 'tame', 'and', 'that', 'the', 'locally', 'nilpotent', 'derivations', 'of', 'p', 'are', 'triangulable']] | [-0.25800635662994215, 0.1802165654887046, -0.16818176924384065, -0.007466564859662737, -0.093454296035426, -0.16956662107259035, -0.05659572490091835, 0.33491259887814523, -0.40177118820803503, -0.15840462685695716, 0.04899107510157462, -0.24708543526274818, -0.09315428429482771, 0.20256774752799953, -0.11805955448320... |
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