Search results for "Quark model"

showing 10 items of 207 documents

Comments on "Neutron-proton mass difference in the chiral solitonic bag model"

1990

It is pointed out that the topological soliton bag is incompletely quantized in the papers of Durgut, Pak, and Yilmaz and of Wittman and Woloshyn, leading to results on the neutron-proton mass difference and other phenomena that are not implied by the model. The purpose of this paper is to clarify how and where their scheme goes wrong and to propose an alternative consistent scheme of quantization.

PhysicsQuantization (physics)Theoretical physicsQuantum mechanicsNuclear TheoryQuark modelElementary particleFermionSymmetry groupNucleonQuantum numberTopological defectPhysical review. D, Particles and fields
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Quark-model study of the hadron structure and the hadron-hadron interaction

2011

Recent results of hadron spectroscopy and hadron-hadron interaction within a quark model framework are reviewed. Higher order Fock space components are considered based on new experimental data on low-energy hadron phenomenology. The purpose of this study is to obtain a coherent description of the low-energy hadron phenomenology to constrain QCD phenomenological models and try to learn about low-energy realizations of the theory.

PhysicsQuantum chromodynamicsHistoryParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelHadronComputer Science ApplicationsEducationFock spaceHadron spectroscopyHigh Energy Physics::ExperimentNuclear ExperimentJournal of Physics: Conference Series
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The lowest-lying baryon masses in covariant SU(3)-flavor chiral perturbation theory

2010

We present an analysis of the baryon-octet and -decuplet masses using covariant SU(3)-flavor chiral perturbation theory up to next-to-leading order. Besides the description of the physical masses we address the problem of the lattice QCD extrapolation. Using the PACS-CS Collaboration data we show that a good description of the lattice points can be achieved at next-to-leading order with the covariant loop amplitudes and phenomenologically determined values for the meson-baryon couplings. Moreover, the extrapolation to the physical point up to this order is found to be better than the linear one given at leading-order by the Gell-Mann-Okubo approach. The importance that a reliable combinatio…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeLattice field theoryQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesLattice QCDBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Covariant transformationHigh Energy Physics::ExperimentQuantum field theoryNuclear Experiment
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Model calculations of the Sivers function satisfying the Burkardt sum rule

2009

9 pages, 4 figures.-- ISI article identifier:000266408300028.-- ArXiv pre-print avaible at:http://arxiv.org/abs/0811.1191

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryQuark modelFísicaFOS: Physical sciencesConstituent quarkFunction (mathematics)Variance (accounting)Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Statistical physicsSum rule in quantum mechanicsNuclear theoryPhysical Review D
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Identifying spin and parity of charmonia in flight with lattice QCD

2019

The spectrum of charmonium resonances contains a number of unanticipated states along with several conventional quark-model excitations. The hadrons of different quantum numbers $J^P$ appear in a fairly narrow energy band, where $J^P$ refers to the spin-parity of a hadron at rest. This poses a challenge for Lattice QCD studies of (coupled-channel) meson-meson scattering aimed at the determination of scattering amplitudes and resonance pole positions. A wealth of information for this purpose can be obtained from the lattice spectra in frames with nonzero total momentum. These are particularly dense since hadrons with different $J^P$ contribute to any given lattice irreducible representation.…

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)ddc:530High Energy Physics::PhenomenologyQuark modelLattice field theoryFOS: Physical sciencesLattice QCD530 PhysikQuantum number01 natural sciencesGood quantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Irreducible representationHadron spectroscopy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Strong magnetic fields in a nonlocal Polyakov chiral quark model

2018

We study the behavior of strongly interacting matter under an external constant magnetic field in the context of nonlocal chiral quark models that incorporate a coupling to the Polyakov loop. We find that at zero temperature the behavior of the quark condensates shows the expected magnetic catalysis effect, our predictions being in good quantitative agreement with lattice QCD results. On the other hand when the analysis is extended to the case of finite temperature our results show that nonlocal models naturally lead to the Inverse Magnetic Catalysis effect for both the chiral restoration and deconfinement transition temperatures.

PhysicsQuantum chromodynamicsQuarkCiencias Astronómicas010308 nuclear & particles physicsMagnetic catalysisPhysicsQC1-999High Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryQuark modelLattice QCD01 natural sciencesDeconfinementMagnetic fieldQuantum electrodynamics0103 physical sciencesNonlocal chiral quark models010306 general physicsCiencias ExactasQuantum chromodynamicsEPJ Web of Conferences
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Quark-model description of the NN*(1440) potential

2001

We derive a $NN^*$(1440) potential from a non-relativistic quark-quark interaction and a chiral quark cluster model for the baryons. By making use of the Born-Oppenheimer approximation we examine the most important features of this interaction in comparison to those obtained from meson-exchange models.

PhysicsQuarkBaryonNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyCluster (physics)FísicaHigh Energy Physics::Experiment
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Two-loop calculation of the anomalous dimension of the axial current with static heavy quarks

1992

Abstract A method to perform two-loop calculations in Eichten's effective field theory for heavy quarks is developed. The anomalous dimension of the axial current for static heavy quarks is calculated at two loops. For N = 3, we get γ A (2) = − 1 36 [ 127 2 +28ξ(2)−5N f ] . This result is very important to understand completely the physical significance of the lattice measurement of the decay constant of the B meson. The two-loop correction generated by γ A (2) turns out to be small, less than 1% for four quark flavours, so that the value of the decay constant of the B meson does not need in practice renormalization group improvement. As extra results, the self-energy renormalization consta…

PhysicsQuarkCoupling constantNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeQuark modelLattice field theoryHadronNuclear TheoryHigh Energy Physics::PhenomenologyFísicaGluonQuantum electrodynamicsB mesonHigh Energy Physics::Experiment
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Constituent quarks and parton distributions

1997

Abstract The high energy parton distribution when evolved to a low energy scale appears to indicate that a valence picture of hadron structure arises. We have developed a formalism based on a laboratory partonic description which connects the parton distributions with the momentum distributions of a quark model. The formalism uses Next to Leading Order evolution and has been defined to produce the right support for the parton distributions. In this scheme we have analyzed the polarized and unpolarized data and shown that well-known Quark Models lead to a qualitative description of the data. However, if one aims at a quantitative agreement, these conventional low energy models have to be cha…

PhysicsQuarkNuclear and High Energy PhysicsAngular momentumParticle physicsHigh Energy Physics::PhenomenologyQuark modelHadronConstituent quarkPartonRenormalization groupGluonNuclear physicsHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics A
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S-4 model for quarks and leptons with maximal atmospheric angle

2010

We consider a model for quark and lepton masses and mixings based on S-4 flavor symmetry. The model contains six Higgs doublets where three of them give mass to the leptons, and the other three gives mass to the quarks. Charged fermion and quark masses arise from renormalizable interactions while neutrino Majorana masses are generated through effective dimension five Weinberg operator. From the study of the minimization of the scalar potential we found a residual mu tau symmetry in the neutrino sector predicting zero reactor angle and maximal atmospheric angle and for the quark sector we found a four-zero texture. We give a fit of the mass hierarchies and mixing angles in the quark sector.

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesUp quarkHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsParticle Physics - PhenomenologyLepton
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