Search results for "constituent"

showing 10 items of 130 documents

Stable heavy pentaquarks in constituent models

2017

It is shown that standard constituent quark models produce $(\bar c c qqq)$ hidden-charm pentaquarks, where $c$ denotes the charmed quark and $q$ a light quark, which lie below the lowest threshold for spontaneous dissociation and thus are stable in the limit where the internal $\bar c c$ annihilation is neglected. The binding is a cooperative effect of the chromoelectric and chromomagnetic components of the interaction, and it disappears in the static limit with a pure chromoelectric potential. Their wave function contains color sextet and color octet configurations for the subsystems and can hardly be reduced to a molecular state made of two interacting hadrons. These pentaquark states co…

QuarkNuclear and High Energy PhysicsParticle physicscolor: octetMesonHigh Energy Physics::LatticeNuclear TheoryHadronFOS: Physical sciencesConstituent quarkpentaquark: heavydissociation01 natural sciencesCharm quarkNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)color: sextet0103 physical sciencesNuclear Experiment010306 general physicsPhysicsAnnihilation010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyquark model: constituentchromoelectricstabilitylcsh:QC1-999PentaquarkBaryonHigh Energy Physics - Phenomenologychromomagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentlcsh:PhysicsPhysics Letters B
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Very Heavy Flavored Dibaryons

2020

We explore the possibility of very heavy dibaryons with three charm quarks and three beauty quarks, $bbbccc$, using a constituent model which should drive to the correct solution in the limit of hadrons made of heavy quarks. The six-body problem is treated rigorously, in particular taking into account the orbital, color and spin mixed-symmetry components of the wave function. Unlike a recent claim based on lattice QCD, no bound state is found below the lowest dissociation threshold.

QuarkParticle physicswave function[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryHigh Energy Physics::LatticeHadronLattice field theoryNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesdissociationspin01 natural sciencesCharm quarkquarkNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateheavy quark010306 general physicsWave functionconstituentNuclear ExperimentNuclear theoryPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theoryLattice QCDcolordibaryon: heavybound stateHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Elementary Particles and FieldsHigh Energy Physics::ExperimenthadroncharmPhysical Review Letters
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Quark gap equation with non-Abelian Ball-Chiu vertex

2018

The full quark-gluon vertex is a crucial ingredient for the dynamical generation of a constituent quark mass from the standard quark gap equation, and its non-transverse part may be determined exactly from the nonlinear Slavnov-Taylor identity that it satisfies. The resulting expression involves not only the quark propagator, but also the ghost dressing function and the quark-ghost kernel, and constitutes the non-abelian extension of the so-called "Ball-Chiu vertex", known from QED. In the present work we carry out a detailed study of the impact of this vertex on the gap equation and the quark masses generated from it, putting particular emphasis on the contributions directly related with t…

QuarkPhysics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyMultiplicative functionFOS: Physical sciencesPropagatorConstituent quark01 natural sciencesGluonHigh Energy Physics - PhenomenologyNonlinear systemHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentAbelian group010306 general physicsPion decay constantMathematical physicsPhysical Review D
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Docc¯nn¯bound states exist?

2007

The four-quark system $c\overline{c}n\overline{n}$ is studied in the framework of the constituent quark model. Using different types of quark-quark potentials, we solve the four-body Schr\"odinger equation by means of the hyperspherical harmonic formalism. Exploring the low laying ${J}^{\mathrm{PC}}$ states for different isospin configurations no four-quark bound states have been found. Of particular interest is the possible four-quark structure of the $X(3872)$. We rule out the possibility that this particle is a compact tetraquark system, unless additional correlations, either in the form of diquarks or at the level of the interacting potential, not considered in simple quark models do co…

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelConstituent quarkParticle identificationSchrödinger equationsymbols.namesakeIsospinQuantum mechanicsBound statesymbolsHigh Energy Physics::ExperimentTetraquarkMathematical physicsPhysical Review D
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Extended van Royen-Weisskopf formalism for lepton-antilepton meson decay widths within non-relativistic quark models

2001

The classical van Royen-Weisskopf formula for the decay width of a meson into a lepton-antilepton pair is modified in order to include non-zero quark momentum contributions within the meson as well as relativistic effects. Besides, a phenomenological electromagnetic density for quarks is introduced. The meson wave functions are obtained from two different models: a chiral constituent quark model and a quark potential model including instanton effects. The modified van Royen-Weisskopf formula is found to improve systematically the results for the widths, giving an overall good description of all known decays.

QuarkPhysicsNuclear and High Energy PhysicsInstantonParticle physicsMesonNuclear Theory010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyConstituent quarkFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Formalism (philosophy of mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsRelativistic quantum chemistryWave functionLepton
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Study of the strongΣb→ΛbπandΣb*→Λbπin a nonrelativistic quark model

2011

We present results for the strong widths corresponding to the $\Sigma_b\to \Lambda_b\, \pi$ and $\Sigma_b^{*}\to \Lambda_b\, \pi$ decays. We apply our model in Ref. Phys. Rev. D 72, 094022 (2005) where we previously studied the corresponding transitions in the charmed sector. Our non-relativistic constituent quark model uses wave functions that take advantage of the constraints imposed by heavy quark symmetry. Partial conservation of axial current hypothesis allows us to determine the strong vertices from an analysis of the axial current matrix elements.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelConstituent quarkSigmaLambda01 natural sciencesSymmetry (physics)Matrix (mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsWave functionPhysical Review D
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Parton distributions in a constituent quark scenario

1999

A simple picture of the constituent quark as a composite system of point-like partons is used to construct the unpolarized and polarized parton distributions by a convolution between constituent quark momentum distributions and constituent quark structure functions. We achieve good agreement with experiments in the unpolarized, as well as, in the polarized case. When our results are compared with similar calculations using non-composite constituent quarks, the accord with the experiments of the present scheme is impressive. We conclude that DIS data are consistent with a low energy scenario dominated by composite constituents of the nucleon.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeStructure functionNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesConstituent quarkFísicaPartonConvolutionMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Simple (abstract algebra)High Energy Physics::ExperimentNucleon
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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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Helicity-dependent generalized parton distributions and composite constituent quarks

2004

An approach, recently proposed to calculate the nucleon generalized parton distributions (GPDs) in a constituent quark model (CQM) scenario, in which the constituent quarks are taken as complex systems, is used to obtain helicity-dependent GPDs. They are obtained from the wave functions of the non relativistic CQM of Isgur and Karl, convoluted with the helicity-dependent GPDs of the constituent quarks themselves. The latter are modelled by using the polarized structure functions of the constituent quark, the double distribution representation of GPDs, and a phenomenological constituent quark form factor. The present approach permits to access a kinematical range corresponding to both the Do…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeMomentum transferQuark modelHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Constituent quarkFOS: Physical sciencesFísicaPartonHelicityNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nucleon
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Relativity and constituent quark structure in model calculations of parton distributions

2004

According to recent studies, Parton Distribution Functions (PDFs) and Generalized Parton Distributions (GPDs) can be evaluated in a Constituent Quark Model (CQM) scenario, considering the constituent quarks as composite objects. In here, a fully covariant model for a system of two particles, together with its non relativistic limit, are used to calculate PDFs and GPDs. The analysis permits to realize that by no means the effects of Relativity can be simulated taking into account the structure of the constituent particles, the two effects being independent and necessary for a proper description of available high energy data in terms of CQM.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryStructure (category theory)Constituent quarkFOS: Physical sciencesPartonPartícules (Física nuclear)Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyTheory of relativityDistribution functionHigh Energy Physics - Phenomenology (hep-ph)Covariant transformationFísica nuclearLimit (mathematics)Nuclear Experiment
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