Search results for "Constituent quark"

showing 10 items of 85 documents

Determination of quadrupole strengths in the γ∗p→Δ(1232) transition at Q2=0.20(GeV/c)2

2007

Abstract We report new precise p ( e → , e ′ p ) π 0 measurements at the peak of the Δ + ( 1232 ) resonance at Q 2 = 0.20 ( GeV / c ) 2 performed at the Mainz Microtron (MAMI). The new data are sensitive to both the electric (E2) and the Coulomb (C2) quadrupole amplitudes of the γ ∗ N → Δ transition. They yield precise quadrupole to dipole amplitude ratios: CMR = ( − 5.09 ± 0.28 stat + sys ± 0.30 model ) % and EMR = ( − 1.96 ± 0.68 stat + sys ± 0.41 model ) % for M 1 + 3 / 2 = ( 39.57 ± 0.75 stat + sys ± 0.40 model ) ( 10 −3 / m π + ) . The new results are in disagreement with Constituent Quark Model predictions and in qualitative agreement with models that account for mesonic contributions…

Nuclear physicsPhysicsNuclear and High Energy PhysicsDipoleAmplitudeQuark modelHadronQuadrupoleCoulombConstituent quarkHigh Energy Physics::ExperimentNuclear ExperimentMicrotronPhysics Letters B
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Double parton correlations and constituent quark models: a light front approach to the valence sector

2014

An explicit evaluation of the double parton distribution functions (dPDFs), within a relativistic Light-Front approach to constituent quark models, is presented. dPDFs encode information on the correlations between two partons inside a target and represent the non-perturbative QCD ingredient for the description of double parton scattering in proton-proton collisions, a crucial issue in the search of new Physics at the LHC. Valence dPDFs are evaluated at the low scale of the model and the perturbative scale of the experiments is reached by means of QCD evolution. The present results show that the strong correlation effects present at the scale of the model are still sizable, in the valence r…

Particle physicsNuclear and High Energy PhysicsNuclear TheoryPhysics beyond the Standard ModelConstituent quarkFOS: Physical sciencesParton01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhenomenological ModelsPhysicsQuantum chromodynamicsValence (chemistry)Large Hadron Collider010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyDistribution functionParton ModelPhenomenological Models Parton Model
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LHCb pentaquarks in constituent quark models

2016

The recently discovered $P_c(4380)^+$ and $P_c(4450)^+$ states at LHCb have masses close to the $\bar D\Sigma_c^*$ and $\bar D^*\Sigma_c$ thresholds, respectively, which suggest that they may have significant meson-baryon molecular components. We analyze these states in the framework of a constituent quark model which has been applied to a wide range of hadronic observables, being the model parameters, therefore, completely constrained. The $P_c(4380)^+$ and $P_c(4450)^+$ are studied as molecular states composed by charmed baryons and open charm mesons. Several bound states with the proper binding energy are found in the $\bar D\Sigma_c^*$ and $\bar D^*\Sigma_c$ channels. We discuss the pos…

Particle physicsNuclear and High Energy PhysicsPotential modelsMesonStrong interactionHadronBinding energyNuclear TheoryConstituent quarkFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Condensed Matter::Superconductivity0103 physical sciencesBound state010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPentaquarklcsh:QC1-999Models of strong interactionsCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentHeavy quarkonialcsh:PhysicsPhysics Letters B
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Baryon Properties with Three-Quark Forces

1987

The Constituent Quark Model (CQM) is very useful for the description of many baryon properties, leading to a fair agreement with the experimental data, especially in the case of the baryon spectrum 1) and of the electromagnetic processes involving baryons2,3). The model is based on a non relativistic QCD-inspired dynamics, which includes a confinement potential and a spin-dependent short-range part, the so called hyperfine interaction4,1). The confinement potential contains as its major part a harmonic oscillator (h.o.) interaction, which has however a too degenerate spectrum with respect to the experimental one and leads to an unreasonable damping of the form factors even at moderate momen…

PhysicsBaryonMomentumQuarkTheoretical physicsBasis (linear algebra)Degenerate energy levelsForm factor (quantum field theory)Constituent quarkHarmonic oscillator
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Three-body forces in the quark model

2008

The constituent quark model has been very useful for the description of many physical properties of baryons, achieving in most cases a fair agreement with the experimental data 1 The model is based on a non relativistic QCD-inspired dynamics including a harmonic oscillator (h.o.) confinement potential and a spin dependent (hyperfine) interaction. The use of Lovelace coordinates p, ~ avoides any problem with the center of mass motion, while the h.o. potential provides a simple basis for ana ly t ica l calculations, which is a very important feature for many applications, like the evaluation of form factors and Meson Exchange Currents 2. On the other hand the h.o. spectrum is too degenerate w…

PhysicsBody forceQuantum chromodynamicsBaryonQuarkParticle physicsMesonQuantum electrodynamicsQuark modelConstituent quarkHarmonic oscillator
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Lowest- Q2 measurement of the γp → Δ reaction: Probing the pionic contribution

2006

To determine nonspherical angular momentum amplitudes in hadrons at long ranges (low Q^2), data were taken for the p(\vec{e},e'p)\pi^0 reaction in the Delta region at Q^2=0.060 (GeV/c)^2 utilizing the magnetic spectrometers of the A1 Collaboration at MAMI. The results for the dominant transition magnetic dipole amplitude and the quadrupole to dipole ratios at W=1232 MeV are: M_{1+}^{3/2} = (40.33 +/- 0.63_{stat+syst} +/- 0.61_{model}) (10^{-3}/m_{\pi^+}),Re(E_{1+}^{3/2}/M_{1+}^{3/2}) = (-2.28 +/- 0.29_{stat+syst} +/- 0.20_{model})%, and Re(S_{1+}^{3/2}/M_{1+}^{3/2}) = (-4.81 +/- 0.27_{stat+syst} +/- 0.26_{model})%. These disagree with predictions of constituent quark models but are in reaso…

PhysicsDipoleAngular momentumNuclear and High Energy PhysicsPionHadronQuadrupoleLattice (group)Constituent quarkHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentMagnetic dipoleThe European Physical Journal A
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Measurements of mass-dependent azimuthal anisotropy in central p + Au, d + Au, and He3 + Au collisions at sNN=200 GeV

2018

We present measurements of the transverse- momentum dependence of elliptic flow v2 for identified pions and (anti)protons at midrapidity (|η|<0.35), in 0%–5% central p+Au and He3+Au collisions at sNN=200 GeV. When taken together with previously published measurements in d+Au collisions at sNN=200 GeV, the results cover a broad range of small-collision-system multiplicities and intrinsic initial geometries. We observe a clear mass-dependent splitting of v2(pT) in d+Au and He3+Au collisions, just as in large nucleus-nucleus (A+A) collisions, and a smaller splitting in p+Au collisions. Both hydrodynamic and transport model calculations successfully describe the data at low pT (<1.5GeV/c), but …

PhysicsLarge Hadron Collider010308 nuclear & particles physicsNuclear TheoryHadronElliptic flowConstituent quarkMultiplicity (mathematics)Kinetic energy01 natural sciencesNuclear physicsPion0103 physical sciencesNuclear Experiment010306 general physicsAnisotropyPhysical Review C
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A covariant constituent-quark formalism for mesons

2014

Using the framework of the Covariant Spectator Theory (CST) [1] we are developing a covariant model formulated in Minkowski space to study mesonic structure and spectra. Treating mesons as effective $q\bar{q}$ states, we focused in [2] on the nonrelativistic bound-state problem in momentum space with a linear confining potential. Although integrable, this kernel has singularities which are difficult to handle numerically. In [2] we reformulate it into a form in which all singularities are explicitely removed. The resulting equations are then easier to solve and yield accurate and stable solutions. In the present work, the same method is applied to the relativistic case, improving upon the r…

PhysicsMesonsIntegrable systemMesonNuclear TheoryNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyConstituent quarkPosition and momentum spaceNuclear Theory (nucl-th)High Energy Physics - PhenomenologyCovariant spectator theoryHigh Energy Physics - Phenomenology (hep-ph)SingularityMinkowski spaceCovariant transformationGravitational singularityConfinementMathematical physics
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Generalized polarizabilities of the proton in a constituent quark model revisited

2001

We study low-energy virtual Compton scattering off the proton within the framework of a nonrelativistic constituent quark model. The Compton tensor is divided into two separately gauge-invariant contributions. The first consists of the groundstate propagation in the direct and crossed channels together with an appropriately chosen term to satisfy gauge invariance. The residual part contains the relevant structure information characterized by the so-called generalized polarizabilities. We discuss two different schemes to obtain the generalized polarizabilities from the residual term. Explicit predictions for the generalized polarizabilities are presented for the Isgur-Karl model. Our results…

PhysicsNuclear and High Energy PhysicsNuclear TheoryProtonStructure (category theory)Compton scatteringConstituent quarkFOS: Physical sciencesResidualNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsBibliographyTensorGauge theory
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Effect of higher orbital angular momenta in the baryon spectrum

2001

We have performed a Faddeev calculation of the baryon spectrum for the chiral constituent quark model including higher orbital angular momentum states. We have found that the effect of these states is important, although a description of the baryon spectrum of the same quality as the one given by including only the lowest-order configurations can be obtained. We have studied the effect of the pseudoscalar quark-quark interaction on the relative position of the positive- and negative-parity excitations of the nucleon as well as the effect of varying the strength of the color-magnetic interaction.

PhysicsNuclear and High Energy PhysicsParticle physicsAngular momentumNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesConstituent quarkAzimuthal quantum numberNuclear Theory (nucl-th)BaryonTotal angular momentum quantum numberQuantum electrodynamicsAngular momentum couplingOrbital angular momentum of lightNucleonPhysical Review C
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