Search results for "electrodynamics"

showing 10 items of 820 documents

Pinch technique to all orders

2002

The generalization of the pinch technique to all orders in perturbation theory is presented. The effective Green's functions constructed with this procedure are singled out in a unique way through the full exploitation of the underlying Becchi-Rouet-Stora-Tyutin symmetry. A simple all-order correspondence between the pinch technique and the background field method in the Feynman gauge is established. Comment: 10 pages, 4 figures; one reference added, typos corrected; final version to match the pubblished one

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsBackground field methodFísicaGluonTheoretical physicssymbols.namesakeQuantum electrodynamicsRegularization (physics)PinchsymbolsFeynman diagramPhysical Review D
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Towards a consistent estimate of the chiral low-energy constants

2006

Guided by the large-N_C limit of QCD, we construct the most general chiral resonance Lagrangian that can generate chiral low-energy constants up to O(p^6). By integrating out the resonance fields, the low-energy constants are parametrized in terms of resonance masses and couplings. Information on those couplings and on the low-energy constants can be extracted by analysing QCD Green functions of currents both for large and small momenta. The chiral resonance theory generates Green functions that interpolate between QCD and chiral perturbation theory. As specific examples we consider the VAP and SPP Green functions.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciencesQCD[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Low energyCorrelation function[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum electrodynamicsQuantum mechanics0103 physical sciences1/NC expansion010306 general physicsChiral lagrangians
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One-loop renormalization of Resonance Chiral Theory: scalar and pseudoscalar resonances

2005

We consider the Resonance Chiral Theory with one multiplet of scalar and pseudoscalar resonances, up to bilinear couplings in the resonance fields, and evaluate its beta-function at one-loop with the use of the background field method. Thus we also provide the full set of operators that renormalize the theory at one loop and render it finite.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theoryScalar field theoryBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesRenormalizationPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsMultipletMathematical physicsJournal of High Energy Physics
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Gauge invariance of the deeply virtual Compton scattering amplitude

2000

We analyze in detail the problem of gauge invariance of the deeply virtual Compton scattering (DVCS) amplitude. Using twist-3 one-gluon exchange diagram contributions and the QCD equations of motion, we derive the general gauge invariant expression of the DVCS amplitude on a (pseudo)scalar particle (pion, ${\mathrm{He}}^{4}).$ Similarly to the case of deep inelastic scattering, the amplitude does not depend on the twist-3 quark-gluon correlations at the Born level. The contribution of the derived amplitude to the single-spin asymmetry with longitudinally polarized lepton is calculated.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyCompton scatteringInelastic scatteringDeep inelastic scattering01 natural sciencesScattering amplitudeAmplitudePionQuantum electrodynamics0103 physical sciencesHigh Energy Physics::ExperimentGauge theoryNuclear Experiment010306 general physicsPhysical Review D
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Heavy meson interquark potential

2011

The resolution of Dyson-Schwinger equations leads to the freezing of the QCD running coupling (effective charge) in the infrared, which is best understood as a dynamical generation of a gluon mass function, giving rise to a momentum dependence which is free from infrared divergences. We calculate the interquark potential for heavy mesons by assuming that it is given by a massive One Gluon Exchange potential and compare with phenomenologyical fits inspired by lattice QCD. We apply these potential forms to the description of quarkonia and conclude that, even though some aspects of the confinement mechanism are absent in the Dyson Schwinger formalism, the results for the spectrum are surprisin…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMesonInfraredHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLattice QCDEffective nuclear chargeHigh Energy Physics - ExperimentGluonHigh Energy Physics - PhenomenologyFormalism (philosophy of mathematics)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsNuclear Experiment
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New results on the spin structure function g1 of the proton and the deuteron from SMC

1998

Abstract New results from a measurement of the spin-dependent structure function g 1 p by the SMC are presented. A next-to-leading order QCD analysis of all published data is used to compute g 1 p at a fixed Q 2 of 10 GeV 2 . Two methods for the extrapolation towards x = 0 to determine the first moment are discussed. In both cases the violation of the Ellis-Jaffe sum rule is confirmed. Using the deuteron data in addition the Bjorken sum rule is tested.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsProtonDeuteriumQuantum electrodynamicsExtrapolationOrder (group theory)Function (mathematics)Sum rule in quantum mechanicsSpin structureAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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The pion polarisability from QCD sum rules

1994

Abstract The electromagnetic polarisability of charged pions, α E , has recently attracted both theoretical and experimental attention. Unfortunately the experimental results disagree with each other. We have investigated this polarisation via a QCD sum rule approach and find α E = 5.6 ± 0.5 × 10 −4 fm 3 , which is in agreement with one experiment and disagrees with the result of chiral perturbation theory.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesChiral perturbation theoryPionHigh Energy Physics::LatticeQuantum electrodynamicsSum rule in quantum mechanicsPhysics Letters B
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Gauge-invariant truncation scheme for the Schwinger-Dyson equations of QCD

2008

We present a new truncation scheme for the Schwinger-Dyson equations of QCD that respects gauge invariance at any level of the dressed loop expansion. When applied to the gluon self-energy, it allows for its non-perturbative treatment without compromising the transversality of the solution, even when entire sets of diagrams (most notably the ghost loops) are omitted, or treated perturbatively.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTransversalityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFeynman graphInvariant (physics)GluonHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Self-energyQuantum electrodynamicsGauge theoryQuantum field theoryMathematical physics
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The form factor of the pion in point-form of relativistic dynamics revisited

2003

The electromagnetic form factor of the pion is calculated in the "point-form" of relativistic quantum mechanics using simple, phenomenological wave functions. It is found that the squared charge radius of the pion is predicted one order of magnitude larger than the experimental value and the asymptotic behavior expected from QCD cannot be reproduced. The origin of these discrepancies is analyzed. The present results confirm previous ones obtained from a theoretical model and call for major improvements in the implementation of the "point-form" approach.

Quantum chromodynamicsPhysicsNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsPoint-form relativistic dynamicsForm factor (quantum field theory)Relativistic dynamicsFOS: Physical sciencesRelativistic quantum mechanics01 natural sciencesPion form factorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionCharge radiusQuantum electrodynamics0103 physical sciences010306 general physicsWave functionOrder of magnitude
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Collective dynamics in relativistic nuclear collisions

2014

Abstract I will review the current status of describing spacetime evolution of the relativistic nuclear collisions with fluid dynamics, and of determining the transport coefficients of strongly interacting matter. The fluid dynamical models suggest that shear viscosity to entropy density ratio of the matter is small. However, there are still considerable challenges in determining the transport coefficients, and especially their temperature dependence is still poorly constrained.

Quantum chromodynamicsPhysicsNuclear and High Energy Physicsta114Spacetime010308 nuclear & particles physicsStrong interaction01 natural sciencesPhysics::Fluid DynamicsViscosityEntropy densityQuantum electrodynamics0103 physical sciencesQuark–gluon plasmaFluid dynamicsCurrent (fluid)010306 general physicsNuclear Physics A
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