Search results for "Quantum electrodynamics."

showing 10 items of 797 documents

Génération et interfaçage de lumière à photon unique et contrôle de la dynamique atomique ultra-rapide pour l’information quantique

2010

We develop a robust and realistic mechanism for the generation of indistinguishable single-photon (SP) pulses with identical frequency and polarization. They are produced on demand from a coupled double-Raman atom-cavity system driven by a sequence of laser pump pulses. This scheme features a high efficiency, the ability to produce a sequence of narrow-band SP pulses with a delay determined only by the pump repetition rate, and simplicity of the system free from complications such as repumping process and environmental dephasing. We propose and analyze a simple scheme of parametric frequency conversion for optical quantum information in cold atomic ensembles. Its remarkable properties are m…

Quantum beatingsParametric interactionAtomic coherenceFour-wave-mixing processProcessus de mélange à quatre ondesCavity quantum electrodynamics[ PHYS.COND.CM-GEN ] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Single-photon generationCohérence atomiqueSelective excitationElectrodynamique quantique en cavitéExcitation sélective[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other][PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Conversion de fréquence quantiqueBattements quantiquesGénération de photons uniquesQuantum frequency conversionInteraction paramétrique
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Screening effects in Relativistic Models of Dense Matter at Finite Temperature

1998

We investigate screening effects of the medium on the potential interaction between two static 'charges' for different models of dense plasmas in the one-boson exchange approximation. The potential can exhibit an oscillatory behavior, which is related to the analytic structure of the corresponding boson propagators in the complex $q$-plane. We have first revisited the one-pion exchange in a nuclear medium. In addition to Friedel oscillations, which are associated to branch cuts in the $q$-plane, there appears another oscillatory component, which arises from a pole on the pion propagator. This pole is located appart from the axes, giving rise to an oscillating Yukawa-like potential. Therefor…

Quantum chromodynamicsPhysicsFriedel oscillationsCoupling constantParticle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyYukawa potentialPerturbative QCDPropagatorFísicaFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicssymbolsBosonDebye
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Gluon and ghost propagators in the Landau gauge: Deriving lattice results from Schwinger-Dyson equations

2008

We show that the application of a novel gauge invariant truncation scheme to the Schwinger-Dyson equations of QCD leads, in the Landau gauge, to an infrared finite gluon propagator and a divergent ghost propagator, in qualitative agreement with recent lattice data.

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaGluonHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Lattice (order)Quantum electrodynamicsGauge theoryQuantum field theory
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Gluon mass and freezing of the QCD coupling

2007

Infrared finite solutions for the gluon propagator of pure QCD are obtained from the gauge-invariant non-linear Schwinger-Dyson equation formulated in the Feynman gauge of the background field method. These solutions may be fitted using a massive propagator, with the special characteristic that the effective mass employed drops asymptotically as the inverse square of the momentum transfer, in agreement with general operator-product expansion arguments. Due to the presence of the dynamical gluon mass the strong effective charge extracted from these solutions freezes at a finite value, giving rise to an infrared fixed point for QCD.

Quantum chromodynamicsPhysicsHistoryParticle physicsBackground field methodInfrared fixed pointHigh Energy Physics::LatticeMomentum transferHigh Energy Physics::PhenomenologyFísicaPropagatorFOS: Physical sciencesComputer Science ApplicationsEducationGluonsymbols.namesakeHigh Energy Physics - PhenomenologyEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicssymbolsFeynman diagram
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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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