Search results for "FIX"

showing 10 items of 1335 documents

Screened potential and quarkonia properties at high temperatures

2009

We perform a quark model calculation of the quarkonia b (b) over bar and c (c) over bar spectra using smooth and sudden string breaking potentials. The screening parameter is scale dependent and can be related to an effective running gluon mass that has a finite infrared fixed point. A temperature dependence for the screening mass is motivated by lattice QCD simulations at finite temperature. Qualitatively different results are obtained for quarkonia properties close to a critical value of the deconfining temperature when a smooth or a sudden string breaking potential is used. In particular, with a sudden string breaking potential quarkonia radii remain almost independent of the temperature…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryInfrared fixed pointScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelFísicaFOS: Physical sciencesLattice QCDCritical valueGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Critical point (thermodynamics)Nuclear ExperimentPhenomenology (particle physics)The European Physical Journal A
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The distribution of the rotational transition strength in warm nuclei studied through γ-ray correlations

1995

Abstract The study of damping of rotational motion applying te rotational plane mapping (RPM) method is presented and discussed. The aim of this technique is to extract the distribution of the rotational transition strength from an analysis of the shape of the “central valley” of two- and three-dimensional γ-ray spectra. The method is applied to a triple γ-coincidence data set of 162,163Tm nuclei formed in 37Cl+130Te reactions. The rotational transition strength is obtained as a function of rotational frequency for selected regions of entry states, and the width is found to be rather constant and approximately equal to 80 keV. This value is significantly smaller than the value predicted the…

PhysicsNuclear reactionNuclear and High Energy PhysicsRotation around a fixed axisRotational transitionRotational temperatureRotational–vibrational spectroscopyAtomic physicsResidualRotational partition functionSpectral lineNuclear Physics A
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Second-Order Phase Transition Induced by Deterministic Fluctuations in Aperiodic Eight-State Potts Models

1999

We investigate the influence of aperiodic modulations of the exchange interactions between nearest-neighbour rows on the phase transition of the two-dimensional eight-state Potts model. The systems are studied numerically through intensive Monte Carlo simulations using the Swendsen-Wang cluster algorithm for different aperiodic sequences. The transition point is located through duality relations, and the critical behaviour is investigated using FSS techniques at criticality. While the pure system exhibits a first-order transition, we show that the deterministic fluctuations resulting from the aperiodic coupling distribution are liable to modify drastically the physical properties in the nei…

PhysicsPhase transitionStatistical Mechanics (cond-mat.stat-mech)Monte Carlo methodDuality (optimization)FOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksFixed pointCondensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic MaterialsTransition pointAperiodic graphStatistical physicsCondensed Matter - Statistical MechanicsPotts model
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An intrinsic characterization of 2+2 warped spacetimes

2010

We give several equivalent conditions that characterize the 2+2 warped spacetimes: imposing the existence of a Killing-Yano tensor $A$ subject to complementary algebraic restrictions; in terms of the projector $v$ (or of the canonical 2-form $U$) associated with the 2-planes of the warped product. These planes are principal planes of the Weyl and/or Ricci tensors and can be explicitly obtained from them. Therefore, we obtain the necessary and sufficient (local) conditions for a metric tensor to be a 2+2 warped product. These conditions exclusively involve explicit concomitants of the Riemann tensor. We present a similar analysis for the conformally 2+2 product spacetimes and give an invaria…

PhysicsPure mathematicsRiemann curvature tensorPhysics and Astronomy (miscellaneous)Degenerate energy levelsFOS: Physical sciencesProduct metricGeneral Relativity and Quantum Cosmology (gr-qc)Fixed pointGeneral Relativity and Quantum Cosmologylaw.inventionsymbols.namesakeProjectorlawsymbolsTensorAlgebraic numberInvariant (mathematics)
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Multiplicity of positive solutions for a degenerate nonlocal problem with p-Laplacian

2021

Abstract We consider a nonlinear boundary value problem with degenerate nonlocal term depending on the L q -norm of the solution and the p-Laplace operator. We prove the multiplicity of positive solutions for the problem, where the number of solutions doubles the number of “positive bumps” of the degenerate term. The solutions are also ordered according to their L q -norms.

PhysicsQA299.6-433sign-changing coefficientmultiple fixed pointsNonlocal problemsp-LaplacianDegenerate energy levels35j2035j25Settore MAT/05 - Analisi Matematica35q74p-LaplacianMultiplicity (chemistry)AnalysisMathematical physicsAdvances in Nonlinear Analysis
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Renormalization-scheme ambiguity and perturbation theory near a fixed point

1984

We consider the perturbative calculation of critical exponents in massless, renormalizable theories having a nontrivial fixed point. In conventional perturbation theory, all results depend on the arbitrary renormalization scheme used. We show how to resolve this problem, following the "principle of minimal sensitivity" approach. At least three orders of perturbation theory are required for quantitative results. We give scheme-independent criteria for determining the presence or absence of a fixed point in $n\mathrm{th}$ order, and discuss the conditions under which perturbative results might be reliable. As illustrations we discuss QED with many flavors, and ${({\ensuremath{\varphi}}^{4})}_…

PhysicsRenormalizationMassless particleScheme (mathematics)Quantum electrodynamicsOrder (ring theory)Perturbation theory (quantum mechanics)Sensitivity (control systems)Fixed pointCritical exponentMathematical physicsPhysical Review D
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General Solution for Self-Gravitating Spherical Null Dust

1997

We find the general solution of equations of motion for self-gravitating spherical null dust as a perturbative series in powers of the outgoing matter energy-momentum tensor, with the lowest order term being the Vaidya solution for the ingoing matter. This is done by representing the null-dust model as a 2d dilaton gravity theory, and by using a symmetry of a pure 2d dilaton gravity to fix the gauge. Quantization of this solution would provide an effective metric which includes the back-reaction for a more realistic black hole evaporation model than the evaporation models studied previously.

PhysicsShock waveHigh Energy Physics - TheoryNuclear and High Energy PhysicsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyQuantization (physics)High Energy Physics::TheoryGeneral Relativity and Quantum CosmologyClassical mechanicsSolution of equationsHigh Energy Physics - Theory (hep-th)DilatonHawking radiationGauge fixing
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Low-energy fixed points of random Heisenberg models

2002

The effect of quenched disorder on the low-energy and low-temperature properties of various two- and three-dimensional Heisenberg models is studied by a numerical strong disorder renormalization group method. For strong enough disorder we have identified two relevant fixed points, in which the gap exponent, omega, describing the low-energy tail of the gap distribution, P(Delta) ~ Delta^omega is independent of disorder, the strength of couplings and the value of the spin. The dynamical behavior of non-frustrated random antiferromagnetic models is controlled by a singlet-like fixed point, whereas for frustrated models the fixed point corresponds to a large spin formation and the gap exponent …

PhysicsStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsInfrared fixed pointFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Type (model theory)Fixed pointRenormalization groupCondensed Matter - Disordered Systems and Neural NetworksOmegaExponentCondensed Matter::Strongly Correlated ElectronsRandomnessCondensed Matter - Statistical MechanicsSpin-½Mathematical physics
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Kinetic Roughening in Slow Combustion of Paper

2001

Results of experiments on the dynamics and kinetic roughening of one-dimensional slow-combustion fronts in three grades of paper are reported. Extensive averaging of the data allows a detailed analysis of the spatial and temporal development of the interface fluctuations. The asymptotic scaling properties, on long length and time scales, are well described by the Kardar-Parisi-Zhang (KPZ) equation with short-range, uncorrelated noise. To obtain a more detailed picture of the strong-coupling fixed point, characteristic of the KPZ universality class, universal amplitude ratios, and the universal coupling constant are computed from the data and found to be in good agreement with theory. Below …

PhysicsStatistical Mechanics (cond-mat.stat-mech)PhysicspaperCrossoverFOS: Physical sciencesGeneral Physics and AstronomyDisordered Systems and Neural Networks (cond-mat.dis-nn)Fixed pointRenormalization groupCondensed Matter - Disordered Systems and Neural NetworksKinetic energyNoise (electronics)AmplitudeCondensed Matter::Statistical MechanicsStatistical physicsinterface dynamicsslow combustionkinetic rougheningConstant (mathematics)ScalingCondensed Matter - Statistical MechanicsPhysical Review Letters
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A New Non-stationary Channel Model Based on Drifted Brownian Random Paths

2014

This paper utilizes Brownian motion (BM) processes with drift to model mobile radio channels under non-stationary conditions. It is assumed that the mobile station (MS) starts moving in a semi-random way, but subject to follow a given direction. This moving scenario is modelled by a BM process with drift (BMD). The starting point of the movement is a fixed point in the two-dimensional (2D) propagation area, while its destination is a random point along a predetermined drift. To model the propagation area, we propose a non-centred one-ring scattering model in which the local scatterers are uniformly distributed on a ring that is not necessarily centred on the MS. The semi-random movement of …

PhysicsStochastic processMobile stationAutocorrelationSpectral densityPoint (geometry)Statistical physicsFixed pointRandom variableBrownian motion
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