Search results for " Integra"

showing 10 items of 2527 documents

Lattice QCD: A Brief Introduction

2014

A general introduction to lattice QCD is given. The reader is assumed to have some basic familiarity with the path integral representation of quantum field theory. Emphasis is placed on showing that the lattice regularization provides a robust conceptual and computational framework within quantum field theory. The goal is to provide a useful overview, with many references pointing to the following chapters and to freely available lecture series for more in-depth treatments of specifics topics.

PhysicsParticle physicsTheoretical physicssymbols.namesakeWilson loopLattice (order)Regularization (physics)Path integral formulationLattice field theorysymbolsLattice QCDQuantum field theoryDirac operator
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Determination of the top quark mass circa 2013: methods, subtleties, perspectives

2013

We present an up-to-date overview of the problem of top quark mass determination. We assess the need for precision in the top mass extraction in the LHC era together with the main theoretical and experimental issues arising in precision top mass determination. We collect and document existing results on top mass determination at hadron colliders and map the prospects for future precision top mass determination at e+e- colliders. We present a collection of estimates for the ultimate precision of various methods for top quark mass extraction at the LHC.

PhysicsParticle physicsTop quarkLarge Hadron ColliderPhysics and Astronomy (miscellaneous)HadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesComputer Science::Computers and SocietyHigh Energy Physics - ExperimentNonlinear Sciences::Chaotic DynamicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemsPhysics::Atomic and Molecular ClustersEngineering (miscellaneous)Particle Physics - PhenomenologyThe European Physical Journal C
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Statistical mechanics of the NLS models and their avatars

2006

“In Vishnuland what avatar? Or who in Moscow (Leningrad) towards the czar [1]”. The different manifestations (avatars) of the Nonlinear Schrodinger equation (NLS models) are described including both classical and quantum integrable cases. For reasons explained the sinh-Gordon and sine-Gordon models, which can be interpreted as covariant manifestations of the ‘repulsive’ and ‘attractive’ NLS models, respectively, are chosen as generic models for the statistical mechanics. It is shown in the text how the quantum and classical free energies can be calculated by a method of functional integration which uses the classical action-angle variables on the real line with decaying boundary conditions,…

PhysicsPartition function (statistical mechanics)symbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable SystemsIntegrable systemThermodynamic limitsymbolsCovariant transformationStatistical mechanicsQuantumNonlinear Schrödinger equationBethe ansatzMathematical physics
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Examples for Calculating Path Integrals

2001

We now want to compute the kernel K(b, a) for a few simple Lagrangians. We have already found for the one-dimensional case that $$\displaystyle{ K{\bigl (x_{2},t_{2};x_{1},t_{1}\bigr )} =\int _{ x(t_{1})=x_{1}}^{x(t_{2})=x_{2} }[dx(t)]\,\text{e}^{(\mathrm{i}/\hslash )S} }$$ (19.1) with $$\displaystyle{ S =\int _{ t_{1}}^{t_{2} }dt\,L(x,\dot{x};t)\;. }$$ First we consider a free particle, $$\displaystyle{ L = m\dot{x}^{2}/2\;, }$$ (19.2) and represent an arbitrary path in the form, $$\displaystyle{ x(t) =\bar{ x}(t) + y(t)\;. }$$ (19.3) Here, \(\bar{x}(t)\) is the actual classical path, i.e., solution to the Euler–Lagrange equation: $$\displaystyle{ \frac{\partial L} {\partial x}\Big\vert _{…

PhysicsPath (topology)CombinatoricsPath integral formulation
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Soliton rains in a fiber laser: An experimental study

2010

Rains of solitons constitute a class of nonlinear dynamics of dissipative soliton ensembles that we briefly reported in Opt. Express 17, 11776 (2009) from a fiber laser experiment. The existence of a relatively intense noisy background together with several tens of soliton pulses aggregated in a condensed soliton phase constitutes a necessary condition for their appearance. New soliton pulses form spontaneously from the background fluctuations and drift until they reach the condensed soliton phase. We here relate in detail the experimental conditions under which soliton rains manifest and their key features, describe related dynamics observed in their vicinity, and propose an explanation fo…

PhysicsPhase (waves)Key featuresLaserQuasi particlesAtomic and Molecular Physics and Opticslaw.inventionDissipative solitonNonlinear systemNonlinear Sciences::Exactly Solvable and Integrable SystemslawQuantum mechanicsSolitonA fibersNonlinear Sciences::Pattern Formation and SolitonsPhysical Review A
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A Rainich-like approach to the Killing-Yano tensors

2002

The Rainich problem for the Killing-Yano tensors posed by Collinson \cite{col} is solved. In intermediate steps, we first obtain the necessary and sufficient conditions for a 2+2 almost-product structure to determine the principal 2--planes of a skew-symmetric Killing-Yano tensor and then we give the additional conditions on a symmetric Killing tensor for it to be the square of a Killing-Yano tensor.We also analyze a similar problem for the conformal Killing-Yano and the conformal Killing tensors. Our results show that, in both cases, the principal 2--planes define a maxwellian structure. The associated Maxwell fields are obtained and we outline how this approach is of interest in studying …

PhysicsPhysics and Astronomy (miscellaneous)GeodesicFirst integralsStructure (category theory)FOS: Physical sciencesConformal mapGeneral Relativity and Quantum Cosmology (gr-qc)Square (algebra)General Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyKilling tensorTensorMathematics::Differential GeometryMathematical physics
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A diffusion Monte Carlo study of small para-Hydrogen clusters

2007

Abstract An improved Monte Carlo diffusion model is used to calculate the ground state energies and chemical potentials of parahydrogen clusters of three to forty molecules, using two different p-H2-p-H2 interactions. The improvement is due to three-body correlations in the importance sampling, to the time step adjustment and to a better estimation of statistical errors. In contrast to path-integral Monte Carlo results, this method predicts no magic clusters other than that with thirteen molecules.

PhysicsPhysicsQC1-999FOS: Physical sciencesGeneral Physics and AstronomyFísica36.40.-cTime stepSpin isomers of hydrogenMolecular physicsmolecular clusterspara-hydrogen clusters67.40.db61.46.bcCluster (physics)Physics::Atomic and Molecular ClustersMoleculeDiffusion Monte CarloPhysics - Atomic and Molecular ClustersAtomic and Molecular Clusters (physics.atm-clus)Ground stateImportance samplingPath integral Monte Carlo
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The CZT X-ray imager on AXO

2001

DSRI has initiated a development program of CZT X-ray and gamma ray detectors employing strip readout techniques. A dramatic improvement of the energy response was found operating the detectors as so-called drift detectors. For the electronic readout, modern ASIC chips were investigated. Modular design and the low power electronics will make large area detectors using the drift strip method feasible. The performance of a prototype CZT system will be presented and discussed. One such detector system has been proposed for future space missions: The X-Ray Imager (XRI) on the Atmospheric X-ray Observatory (AXO), which is a mission proposed to the Danish Small Satellite Program and is dedicated …

PhysicsPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaDetectorAstrophysics::Instrumentation and Methods for AstrophysicsModular designSpace explorationOpticsApplication-specific integrated circuitObservatoryLow-power electronicsSatellitebusinessEnergy (signal processing)
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Classical and Quantum Nonultralocal Systems on the Lattice

1997

We classify nonultralocal Poisson brackets for 1-dimensional lattice systems and describe the corresponding regularizations of the Poisson bracket relations for the monodromy matrix. A nonultralocal quantum algebras on the lattices for these systems are constructed. For some class of such algebras an ultralocalization procedure is proposed. The technique of the modified Bethe-Anzatz for these algebras is developed and is applied to the nonlinear sigma model problem.

PhysicsPoisson bracketNonlinear systemPure mathematicsNonlinear Sciences::Exactly Solvable and Integrable SystemsSigma modelPoisson manifoldLattice (order)Quantum mechanicsMonodromy matrixQuantumPoisson algebra
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Monte Carlo calculation of dose rate distributions around the Walstam CDC.K-type137Cs sources

2001

Basic dosimetric data for the Walstam CDC.K-type low dose rate 137Cs sources in water have been calculated using Monte Carlo techniques. These sources, CDC.K1 -K3 and CDC.K4, are widely used in a range of applicators and moulds for the treatment of intracavitary and superficial cancers. Our purpose is to improve existing data about these sources using the Monte Carlo simulation code GEANT3. Absolute dose rate distributions in water have been calculated around these sources and are presented as conventional 2D Cartesian look-up tables. Also the AAPM Task Group 43 formalism for dose calculation has been applied. The calculated dose rate constant for the CDC.K1-K3 source is A = 1.106 +/- 0.001…

PhysicsPolynomial regressionModels StatisticalRadiological and Ultrasound TechnologyRadiotherapy Planning Computer-AssistedMonte Carlo methodSievert integrallaw.inventionComputational physicsCesium RadioisotopeslawAnisotropyHumansDosimetryRadiology Nuclear Medicine and imagingCartesian coordinate systemStatistical physicsLow dose rateRadiometryDose rateAnisotropyMonte Carlo MethodAlgorithmsSoftwarePhysics in Medicine and Biology
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