Search results for " ELECTRODYNAMICS"

showing 10 items of 813 documents

Massive quarks in NLO dipole factorization for DIS : Longitudinal photon

2021

In this work, we will present the first complete calculation of the one-loop longitudinal photon-to-quark-antiquark light cone wave function, with massive quarks. The quark masses are renormalized in the pole mass scheme. The result is used to calculate the next-to-leading order correction to the high energy Deep Inelastic Scattering longitudinal structure function on a dense target in the dipole factorization framework. For massless quarks the next-to-leading order correction was already known to be sizeable, and our result makes it possible to evaluate it also for massive quarks.

QuarkParticle physicsPhotonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryQUANTUM ELECTRODYNAMICSFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)FactorizationLight coneINFINITE-MOMENTUM0103 physical sciencesSCATTERINGPICTURE010306 general physicsWave functionPhysics010308 nuclear & particles physicskvarkitLIGHT-FRONT QCDHigh Energy Physics::PhenomenologyDeep inelastic scatteringINVARIANCEMassless particleDipoleHigh Energy Physics - PhenomenologykvanttiväridynamiikkaHigh Energy Physics::ExperimentBK EVOLUTION
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Light-Front Interpretation of Proton Generalized Polarizabilities

2009

We extend the recently developed formalism to extract light-front quark charge densities from nucleon form factor data to the deformations of these quark charge densities when applying an external electric field. We show that the resulting induced polarizations can be extracted from proton generalized polarizabilities. The available data for the generalized electric polarizabilitiy of the proton yield a pronounced structure in its induced polarization at large transverse distances, which will be pinned down by forthcoming high precision virtual Compton scattering experiments.

QuarkPhysicsElastic scatteringNuclear TheoryProtonNuclear TheoryCompton scatteringFOS: Physical sciencesGeneral Physics and AstronomyCharge densityNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PolarizabilityElectric fieldQuantum electrodynamicsAtomic physicsNucleonPhysical Review Letters
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Finite-size scaling of vector and axial current correlators

2002

Using quenched chiral perturbation theory, we compute the long-distance behaviour of two-point functions of flavour non-singlet axial and vector currents in a finite volume, for small quark masses, and at a fixed gauge-field topology. We also present the corresponding predictions for the unquenched theory at fixed topology. These results can in principle be used to measure the low-energy constants of the chiral Lagrangian, from lattice simulations in volumes much smaller than one pion Compton wavelength. We show that quenching has a dramatic effect on the vector correlator, which is argued to vanish to all orders, while the axial correlator appears to be a robust observable only moderately …

QuarkPhysicsNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParticle Physics - LatticeObservableCompton wavelengthHigh Energy Physics - LatticePionLattice (order)Quantum electrodynamicsScaling
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On the Pauli-Villars regularisation scheme in the NJL model

1993

Abstract We consider the Nambu-Jona-Lasinio model with a Pauli-Villars cutoff. We point out that previous attempts to use this regularisation have not been consistent and it is shown that if used correctly this approach yields very reasonable values for the cutoff parameter and quark condensate when we demand that ƒπ is fixed to its experimental value. Finally it is argued that because of its covariance and smooth nature this regularisation scheme has significant advantages over other regulators on the market.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryStrong interactionElementary particleCovariancesymbols.namesakePauli exclusion principleRegularization (physics)Quantum electrodynamicssymbolsApplied mathematicsCutoffGauge theoryPhysics Letters B
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Nucleon matrix elements from lattice QCD with all-mode-averaging and a domain-decomposed solver: An exploratory study

2017

We study the performance of all-mode-averaging (AMA) when used in conjunction with a locally deflated SAP-preconditioned solver, determining how to optimize the local block sizes and number of deflation fields in order to minimize the computational cost for a given level of overall statistical accuracy. We find that AMA enables a reduction of the statistical error on nucleon charges by a factor of around two at the same cost when compared to the standard method. As a demonstration, we compute the axial, scalar and tensor charges of the nucleon in $N_f=2$ lattice QCD with non-perturbatively O(a)-improved Wilson quarks, using O(10,000) measurements to pursue the signal out to source-sink sepa…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Scalar (physics)FOS: Physical sciencesCharge (physics)Lattice QCDComputational Physics (physics.comp-ph)Solver01 natural sciencesMatrix (mathematics)High Energy Physics - Lattice13. Climate actionQuantum electrodynamics0103 physical scienceslcsh:QC770-798ddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityTensor010306 general physicsNucleonPhysics - Computational PhysicsNuclear Physics B
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Relativistic constituent quark model with infrared confinement

2009

We refine the relativistic constituent quark model developed in our previous papers to include the confinement of quarks. It is done, first, by introducing the scale integration in the space of alpha-parameters, and, second, by cutting this scale integration on the upper limit which corresponds to an infrared cutoff. In this manner one removes all possible thresholds presented in the initial quark diagram. The cutoff parameter is taken to be the same for all physical processes. We adjust other model parameters by fitting the calculated quantities of the basic physical processes to available experimental data. As an application, we calculate the electromagnetic form factors of the pion and t…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsQuark modelHadronNuclear TheoryConstituent quarkFOS: Physical sciencesOmega baryon01 natural sciencesHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesHigh Energy Physics::ExperimentColor confinement010306 general physics
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Fitting strategies to extract the axial charge of the nucleon from lattice QCD

2014

We report on a comparison of several fit methods used for the extraction of the nucleon axial charge gA from lattice QCD with two dynamical flavours of O(a) improved Wilson quarks. We use plateau fits, summed operator insertions (the summation method) and a new “midpoint” method to investigate contributions from excited states that affect the determination of gA. We also present a method to perform correlated fits when the standard estimator for the inverse of the covariance matrix becomes unstable.

QuarkPhysicsParticle physicsCovariance matrixHigh Energy Physics::LatticeOperator (physics)Quantum electrodynamicsEstimatorInverseCharge (physics)Lattice QCDNucleonProceedings of 31st International Symposium on Lattice Field Theory LATTICE 2013 — PoS(LATTICE 2013)
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Is the spectrum of highly excited mesons purely coulombian?

2008

We show that a static central potential may provide a precise description of highly excited light unflavoured mesons. Due to string breaking this potential becomes of chromoelectric type at sufficiently large quark-antiquark distances giving rise to a coulombian spectrum. The same conclusion can be inferred for any other meson sector through a straightforward extension of our analysis.

QuarkPhysicsParticle physicsMesonHigh Energy Physics::LatticeSpectrum (functional analysis)Nuclear TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesFísicaType (model theory)String theoryString (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Excited stateQuantum electrodynamicsHigh Energy Physics::ExperimentSymmetry breaking
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Abelian dominance and the dual Meissner effect in local unitary gauges in SU(2) gluodynamics

2007

Performing highly precise Monte-Carlo simulations of SU(2) gluodynamics, we observe for the first time Abelian dominance in the confining part of the static potential in local unitary gauges such as the F12 gauge. We also study the flux-tube profile between the quark and antiquark in these local unitary gauges and find a clear signal of the dual Meissner effect. The Abelian electric field is found to be squeezed into a flux tube by the monopole supercurrent. This feature is the same as that observed in the non-local maximally Abelian gauge. These results suggest that the Abelian confinement scenario is gauge independent. Observing the important role of space-like monopoles in the Polyakov g…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Magnetic monopoleFOS: Physical sciencesGluonHigh Energy Physics::TheoryHigh Energy Physics - LatticeMeissner effectQuantum electrodynamicsAbelian groupSpecial unitary groupMathematical physics
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Laurent series expansion of a class of massive scalar one-loop integrals toO(ε2)

2005

We use dimensional regularization to calculate the O({epsilon}{sup 2}) expansion of all scalar one-loop one-, two-, three-, and four-point integrals that are needed in the calculation of hadronic heavy quark production. The Laurent series up to O({epsilon}{sup 2}) is needed as input to that part of the next-to-next-to-leading order corrections to heavy flavor production at hadron colliders where the one-loop integrals appear in the loop-by-loop contributions. The four-point integrals are the most complicated. The O({epsilon}{sup 2}) expansion of the three- and four-point integrals contains in general polylogarithms up to Li{sub 4} and functions related to multiple polylogarithms of maximal …

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsDimensional regularizationQuantum electrodynamicsLaurent seriesHigh Energy Physics::PhenomenologyHadronScalar (mathematics)Series expansionMathematical physicsPhysical Review D
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