Search results for " ELECTRODYNAMICS"

showing 10 items of 813 documents

Finite-size Scaling of Meson Propagators

2001

Using quenched chiral perturbation theory we compute meson correlation functions at finite volume and fixed gauge field topology. We also present the corresponding analytical predictions for the unquenched theory at fixed gauge field topology. These results can be used to measure the low-energy parameters of the chiral Langrangian from lattice simulations in volumes much smaller than one pion Compton wavelength.

PhysicsNuclear and High Energy PhysicsFinite volume methodChiral perturbation theoryMesonHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesPropagatorFísicaParticle Physics - LatticeCompton wavelengthPionHigh Energy Physics - LatticeQuantum electrodynamicsGauge theoryScaling
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Description of sub-barrier heavy ion fusion in a semiclassical quantum tunneling model

1996

In this paper we apply the semiclassical method based on the Feynman path integral formalism to sub-barrier fusion of heavy nuclei. Cross sections are calculated and compared to experimental data and to coupled-channel calculations for different mass systems: 32S124Mg, 58Ni164Ni, and 16O1208Pb. The semiclassical method and coupled-channel calculations give comparable results. It is found that the coupling produces a renormalization of the barrier that is responsible for the enhancement of sub-barrier fusion cross sections and a dissipative force along the classical tunneling path.

PhysicsNuclear and High Energy PhysicsFusionQuantum mechanicsQuantum electrodynamicsSemiclassical physicsFísica nuclearHeavy ionQuantum tunnellingPhysical Review C
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Nonperturbative gluon and ghost propagators for d=3 Yang-Mills theory

2010

We study a manifestly gauge-invariant set of Schwinger-Dyson equations to determine the non-perturbative dynamics of the gluon and ghost propagators in d = 3 Yang-Mills theory. The use of the well-known Schwinger mechanism, in the Landau gauge leads to the dynamical generation of a mass for the gauge boson (gluon in d = 3), which, in turn, gives rise to an infrared finite gluon propagator and ghost dressing function. The propagators obtained from the numerical solution of these nonperturbative equations are in very good agreement with the results of SU(2) lattice simulations. We would like to thank A. Cucchieri and T. Mendes for kindly making their lattice results available to us, and for t…

PhysicsNuclear and High Energy PhysicsGauge bosonHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyPropagatorLie groupYang–Mills theoryGluonHigh Energy Physics::TheoryQuantum electrodynamicsGauge theoryQuantum field theory
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Gauge coupling instability and dynamical mass generation in N=1 three-dimensional supersymmetric QED

1999

Using superfield Dyson-Schwinger equations, we compute the infrared dynamics of the semi-amputated full vertex, corresponding to the effective running gauge coupling, in N-flavor N51 three-dimensional supersymmetric QED. It is shown that the presence of a supersymmetry-preserving mass for the matter multiplet stabilizes the infrared gauge coupling against oscillations present in the massless case, and we therefore infer that the massive vacuum is thus selected at the level of the ~quantum! effective action. We further demonstrate that such a mass can indeed be generated dynamically in a self-consistent way by appealing to the superfield Dyson-Schwinger gap equation for the full matter propa…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyPropagatorFísicaSupersymmetryVertex (geometry)Massless particleHigh Energy Physics::TheorySupersymmetric gauge theoryQuantum electrodynamicsMultipletEffective actionMathematical physics
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Multigluon correlations in JIMWLK

2012

We discuss applications of the JIMWLK renormalization group equation to multigluon correlations in high energy collisions. This includes recent progress in computing the energy dependence of higher point Wilson line correlators from the JIMWLK renormalization group equation. We find that the large Nc approximation used so far in the phenomenological literature is not very accurate. On the other hand a Gaussian finite Nc approximation is surprisingly close to the full result. We also discuss correlations at large rapidity separations, relevant for the "ridge" correlations observed in experiments.

PhysicsNuclear and High Energy PhysicsHigh energyNuclear Theoryta114010308 nuclear & particles physicsGaussianFOS: Physical sciencesRenormalization group01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencessymbolsRapidity010306 general physicsNuclear theoryLine (formation)Mathematical physicsNuclear Physics A
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Coulomb corrections to the three-body correlation function in high-energy heavy ion reactions

1998

Starting from an asymptotically correct three-body Coulomb wave-function, we determine the effect of Coulomb final state interaction on the three-particle Bose-Einstein correlation function of similarly charged particles. We numerically estimate that the Riverside approximation is not precise enough to determine the three-body Coulomb correction factor in the correlation function, if the characteristic HBT radius parameter is 5 - 10 fm, which is the range of interest in high-energy heavy ion physics.

PhysicsNuclear and High Energy PhysicsHigh energyRange (particle radiation)Particle physicsFOS: Physical sciencesState (functional analysis)RadiusCharged particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Correlation functionQuantum electrodynamicsCoulombHeavy ion
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GAUGE-HIGGS UNIFICATION MODELS WITH COSET SPACE DIMENSIONAL REDUCTION SCHEME

2009

We investigate the gauge-Higgs unification models within the scheme of the coset space dimensional reduction, beginning with two types of set up; fourteen-dimensional gauge theory with simple gauge groups and ten-dimensional gauge theory with direct product gauge groups. We found some phenomenologically acceptable models through an exhaustive search for the candidates of the coset spaces, the gauge group in higher dimension, and fermion representation.

PhysicsNuclear and High Energy PhysicsIntroduction to gauge theoryQuantum gauge theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsBRST quantizationHigh Energy Physics::TheoryTheoretical physicsHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theoryQuantum electrodynamicsGauge anomalyGauge symmetryInternational Journal of Modern Physics A
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A theoretical approach to pionic atoms and the problem of anomalies

1993

Abstract We have constructed a theoretical optical potential for pionic atoms based on the first- and second-order terms of a many-body expansion on the number of ph excitations. The p-wave parts are very much influenced by the medium polarization. The quenching at large densities produced by this phenomenon, together with the one from the Lorentz-Lorenz effect, and modifications over standard potentials due to the isospin dependence, lead to a new potential which produces notoriously improved results in the problem of anomalies. A clearer definition of this problem is proposed as the inability of standard potentials to reproduce simultaneously the data for light and heavy nuclei. Finally a…

PhysicsNuclear and High Energy PhysicsIsospinQuantum electrodynamicsQuantum mechanicsPolarization (waves)Optical potentialNuclear Physics A
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Isospin-invariant Skyrme energy-density-functional approach with axial symmetry

2014

We develop the isospin-invariant Skyrme-EDF method by considering local densities in all possible isospin channels and proton-neutron (p-n) mixing terms as mandated by the isospin symmetry. The EDF employed has the most general form that depends quadratically on the isoscalar and isovector densities. We test and benchmark the resulting p-n EDF approach, and study the general properties of the new scheme by means of the cranking in the isospin space. We extend the existing axial DFT solver HFBTHO to the case of isospin-invariant EDF approach with all possible p-n mixing terms. Explicit expressions have been derived for all the densities and potentials that appear in the isospin representatio…

PhysicsNuclear and High Energy PhysicsIsovectorNuclear Theoryta114IsoscalarNuclear TheoryFOS: Physical sciencesSolverNuclear Theory (nucl-th)isospintiheysIsospinPairingQuantum electrodynamicsQuantum mechanicsCoulombSymmetry breakingAxial symmetryNuclear ExperimentPhysical review C
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Factorization and resummation for jet broadening

2011

Jet broadening is an event-shape variable probing the transverse momenta of particles inside jets. It has been measured precisely in e+e- annihilations and is used to extract the strong coupling constant. The factorization of the associated cross section at small values of the broadening is afflicted by a collinear anomaly. Based on an analysis of this anomaly, we present the first all-order expressions for jet-broadening distributions, which are free of large perturbative logarithms in the two-jet limit. Our formulae reproduce known results at next-to-leading logarithmic order but also extend to higher orders.

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLogarithm010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciences01 natural sciencessymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationQuantum electrodynamics0103 physical sciencesWeierstrass factorization theoremEffective field theorysymbolsAnomaly (physics)Resummation010306 general physicsPHYSICS LETTERS B
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