Search results for "Variant"

showing 10 items of 1267 documents

THE OPERATOR PRODUCT EXPANSION OF THE QCD PROPAGATORS

1992

We bring together for the first time the coefficients in covariant gauges of all the condensates of dimension four or less in the operator product expansion (OPE) of the quark, gluon and ghost propagators. It is stressed that contrary to general belief the condensates do not enter the OPE of the propagators in gauge-invariant combinations like [Formula: see text] and 〈G2〉. The results are presented in arbitrary dimension to lowest order in the light quark masses for the SU (Nc) internal symmetry group. All terms which, through the equations of motion, may be viewed as being effectively of order αs are included. The importance of the equations of motion if one is to fulfill the Slavnov-Tayl…

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQCD vacuumGeneral Physics and AstronomyPropagatorEquations of motionAstronomy and AstrophysicsLattice QCDHigh Energy Physics::TheoryCovariant transformationOperator product expansionMathematical physicsModern Physics Letters A
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Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at s=13TeV

2018

The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye|<0.8) in proton–proton (pp) collisions at a centre-of-mass energy of s=13 TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at s=7 TeV or 13 TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσcc¯/dy|y=0=974±138(stat.)±140(syst.)±214(BR)μb and dσbb…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsHadronMultiplicity (mathematics)01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massCharm (quantum number)Nuclear Experiment010306 general physicsPhysics Letters B
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QCD generates the ϱ-resonance

1991

Abstract The question whether the asymptotic QCD amplitude contains potentially hadronic resonances is examined by a mathematically rigorous method, based on the theory of maximally converging sequences of polynomials and conformal mappings. It is shown that the extrapolated amplitude to the physical cut exhibits indeed a bump structure which corresponds to the ϱ-resonance.

Quantum chromodynamicsScattering amplitudeNuclear and High Energy PhysicsAmplitudeMathematical analysisConformal mapElementary particleInvariant massQuantum field theorySeries expansionAtomic and Molecular Physics and OpticsMathematicsMathematical physicsNuclear Physics B - Proceedings Supplements
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Electromagnetic lattice gauge invariance in two-dimensional discrete-time quantum walks

2018

International audience; Gauge invariance is one of the more important concepts in physics. We discuss this concept in connection with the unitary evolution of discrete-time quantum walks in one and two spatial dimensions, when they include the interaction with synthetic, external electromagnetic fields. One introduces this interaction as additional phases that play the role of gauge fields. Here, we present a way to incorporate those phases, which differs from previous works. Our proposal allows the discrete derivatives, that appear under a gauge transformation, to treat time and space on the same footing, in a way which is similar to standard lattice gauge theories. By considering two step…

Quantum informationHigh Energy Physics::Latticecurrent: conservation lawLattice field theoryFOS: Physical sciencescurrent: density01 natural sciences010305 fluids & plasmasrandom walksymbols.namesakeTheoretical physics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]electromagnetic field0103 physical sciencesunitarityinvariance: gaugeQuantum walkDirac equationcontinuum limitGauge theorydimension: 2010306 general physicsConserved currentComputingMilieux_MISCELLANEOUSQuantum walksPhysicsQuantum PhysicsSpacetimeUnitaritylattice field theoryInvariant (physics)[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]electromagneticDirac equationsymbolsgauge field theoryQuantum simulationQuantum Physics (quant-ph)transformation: gaugeLattice gauge theoriesPhysical Review A
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Renormalization group invariant matrix elements of Delta S = 2 and Delta I = 3/2 four fermion operators without quark masses

1999

We introduce a new parameterization of four-fermion operator matrix elements which does not involve quark masses and thus allows a reduction of systematic uncertainties. In order to simplify the matching between lattice and continuum renormalization schemes, we express our results in terms of renormalization group invariant B-parameters which are renormalization-scheme and scale independent. As an application of our proposal, matrix elements of DI=3/2 and SUSY DS =2 operators have been computed. The calculations have been performed using the tree-level improved Clover lattice action at two different values of the strong coupling constant (beta=6/g^2=6.0 and 6.2), in the quenched approximati…

QuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesWILSON FERMIONSQuenched approximationPartícules (Física nuclear)kaon decays gauge theory latticeLATTICE QCDRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKAON B-PARAMETERLattice (order)Mathematical physicsPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionSupersymmetryInvariant (physics)Renormalization groupFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Heavy quark diffusion in an overoccupied gluon plasma

2020

We extract the heavy-quark diffusion coefficient \kappa and the resulting momentum broadening in a far-from-equilibrium non-Abelian plasma. We find several features in the time dependence of the momentum broadening: a short initial rapid growth of , followed by linear growth with time due to Langevin-type dynamics and damped oscillations around this growth at the plasmon frequency. We show that these novel oscillations are not easily explained using perturbative techniques but result from an excess of gluons at low momenta. These oscillation are therefore a gauge invariant confirmation of the infrared enhancement we had previously observed in gauge-fixed correlation functions. We argue that…

QuarkNuclear and High Energy PhysicsNuclear Theorynucl-thhep-latFOS: Physical sciencesLattice QCDhiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)fysikk0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsPlasmonParticle Physics - PhenomenologyPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]010308 nuclear & particles physicsOscillationComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)Particle Physics - Latticehep-phLattice QCDPlasmaInvariant (physics)GluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsNuclear Physics - TheoryQuark–gluon plasmaQuark-Gluon Plasmalcsh:QC770-798
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Scalar K pi form factor and light quark masses

2006

5 páginas, 2 figuras, 2 tablas.-- PACS numbers: 12.15.Ff, 14.65.Bt, 11.55.Hx.-- arXiv:hep-ph/0605095v2

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeScalar (mathematics)Nuclear TheoryFOS: Physical sciencesStrangenessAstrophysicsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle decayHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - LatticeInvariant massNuclear ExperimentQuantum chromodynamicsPhysicsCabibbo–Kobayashi–Maskawa matrixAstrophysics (astro-ph)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Electromagnetic structure of few-nucleon ground states

2015

Experimental form factors of the hydrogen and helium isotopes, extracted from an up-to-date global analysis of cross sections and polarization observables measured in elastic electron scattering from these systems, are compared to predictions obtained in three different theoretical approaches: the first is based on realistic interactions and currents, including relativistic corrections (labeled as the conventional approach); the second relies on a chiral effective field theory description of the strong and electromagnetic interactions in nuclei (labeled $\chi$EFT); the third utilizes a fully relativistic treatment of nuclear dynamics as implemented in the covariant spectator theory (labeled…

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryDegrees of freedom (physics and chemistry)FOS: Physical sciencescharge and magnetic radiiElectromagnetic properties01 natural sciences7. Clean energychiral effective field theoryNuclear Theory (nucl-th)Momentum0103 physical sciencesEffective field theoryCovariant transformationNuclear Experiment (nucl-ex)010306 general physicsform factorsNuclear ExperimentIsotopes of heliumPhysics010308 nuclear & particles physicselectric quadrupole and magnetic dipole momentslight nucleiGluoncharge and magnetic radii; chiral effective field theory; covariant spectator theory; electric quadrupole and magnetic dipole moments; form factors; light nuclei; Nuclear and High Energy Physicscovariant spectator theoryFew-nucleon ground statesNucleonJournal of Physics G: Nuclear and Particle Physics
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Spectroscopy of doubly charmed baryons

2004

We study the mass spectrum of baryons with two and three charmed quarks. For double charm baryons the spin splitting is found to be smaller than standard quark-model potential predictions. This splitting is not influenced either by the particular form of the confining potential or by the regularization taken for the contact term of the spin-spin potential. We consistently predict the spectra for triply charmed baryons.

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryFOS: Physical sciencesSpectral lineCharm quarkHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Invariant massSpectroscopyNuclear ExperimentPhysicsQuark modelHigh Energy Physics::PhenomenologyFísicaBaryonCharmed baryonsHigh Energy Physics - PhenomenologyRegularization (physics)Mass spectrumHigh Energy Physics::Experiment
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Pion radiative weak decays in nonlocal chiral quark models

2010

We analyze the radiative pion decay pi+ -> e+ nu_e gamma within nonlocal chiral quark models that include wave function renormalization. In this framework we calculate the vector and axial-vector form factors FV and FA at q^2=0 --where q^2 is the (e+ ��_e) squared invariant mass-- and the slope a of FV(q^2) at q^2 -> 0. The calculations are carried out considering different nonlocal form factors, in particular those taken from lattice QCD evaluations, showing a reasonable agreement with the corresponding experimental data. The comparison of our results with those obtained in the (local) NJL model and the relation of FV and a with the form factor in pi^0 -> gamma* gamma decays are d…

QuarkNuclear and High Energy PhysicsParticle physicsWave function renormalizationHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)RenormalizationPionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio model0103 physical sciencesInvariant mass010306 general physicsPhysics010308 nuclear & particles physicsQuark modelHigh Energy Physics::PhenomenologyFísicaLattice QCDPion radiative weak decaysNonlocal quark modelsHigh Energy Physics - PhenomenologyFísica nuclearHigh Energy Physics::Experiment
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