Search results for "Quark model"

showing 10 items of 207 documents

Predictions for the ${\vec{\Lambda }_b \rightarrow J/\psi ~ \Lambda (1405)}$ Λ b → J / ψ Λ ( 1405 ) decay

2015

We calculate the shape of the [Formula: see text] and [Formula: see text] invariant mass distributions in the [Formula: see text] and [Formula: see text] decays that are dominated by the [Formula: see text] resonance. The weak interaction part is the same for both processes and the hadronization into the different meson-baryon channels in the final state is given by symmetry arguments. The most important feature is the implementation of the meson-baryon final-state interaction using two chiral unitary models from different theoretical groups. Both approaches give a good description of antikaon-nucleon scattering data, the complex energy shift in kaonic hydrogen and the line shapes of [Formu…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonUnitarityKaonic hydrogenQuark modelHigh Energy Physics::PhenomenologyNuclear TheoryElementary particleWeak interaction7. Clean energyHadronizationTheoretical physicsInvariant massHigh Energy Physics::Experimentddc:530Nuclear ExperimentEngineering (miscellaneous)
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Exclusive non-leptonic charm baryon decays

1992

We present a spectator quark model calculation of the Cabibbo-enhanced non-leptonic decays of the lowest lying charm baryons Λc, Ξc and Ωc decaying into non-charm ground state baryons and mesons. We employ covariant quark model wave functions to describe the ground state baryons and mesons. They are obtained by boosting rest frame wave functions to equal velocity frames. The non-leptonic decay amplitudes are then obtained in terms of two wave function overlap parameters which we fit to the experimental data. We discuss general features of the flavour and helicity composition of the final states in the quark model approach. We emphasize thatW-exchange contributions are of crucial importance …

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Mesonmedia_common.quotation_subjectNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelRest frameLambda baryonAsymmetryCharm quarkSigma baryonNuclear physicsBaryonHigh Energy Physics::ExperimentNuclear ExperimentEngineering (miscellaneous)media_commonZeitschrift für Physik C Particles and Fields
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Semi-leptonic charm baryon decays in the relativistic spectator quark model

1991

We calculate the exclusive semi-leptonic charm baryon decays of the lowest lying charm baryon states into the ground state strangeness baryons using the covariant spectator quark model approach. We present results on rates,q 2- andE l -spectra as well as on the angular decay distribution in the cascade decay $$\Omega _c \to \Omega ( \to \Xi \pi ,\Lambda {\rm K})$$ .

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::PhenomenologyQuark modelStrangenessLambdaOmegaNuclear physicsBaryonHigh Energy Physics::ExperimentCovariant transformationCharm (quantum number)Nuclear ExperimentGround stateEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Quark model explanation of ϒ (10860)

2020

PhysicsParticle physicsQuark modelHadron Spectroscopy and Structure
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Physical observables in the decay Λb→Λc(→Λ+π)+τ−+ν̄τ

2015

We analyze the tauonic semileptonic baryon decays [Formula: see text] with particular emphasis on the lepton helicity flip contributions which vanish for zero lepton masses. We calculate the total rate, differential decay distributions, the longitudinal and transverse polarization components of the [Formula: see text] and the [Formula: see text], and the lepton-side forward-backward asymmetries. We use the covariant confined quark model to provide numerical results on these observables.

PhysicsParticle physicsQuark modelHigh Energy Physics::PhenomenologyкваркиHyperonForm factor (quantum field theory)ObservableHelicityBaryonбарионыполулептонные распады барионовCovariant transformationHigh Energy Physics::ExperimentLepton
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NN Interaction in Chiral Constituent Quark Models

2003

We review the actual state in the description of the nucleon-nucleon (NN) interaction by means of chiral constituent quark models. We present a series of relevant features that are nicely explained within the quark model framework.

PhysicsParticle physicsSeries (mathematics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFlavourQuark modelConstituent quarkState (functional analysis)Top quark condensateNuclear ExperimentNuclear theory
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Polarized Structure Functions and the Nucleon Spin

1995

The link between the light-cone momentum distributions of constituent quark models and their corresponding parton distributions is used to study the polarized structure functions g 1 of proton and neutron. The formalism allows to analyze the effects of the structure of the quark model wave function and thus we discuss the SU (6) breaking mechanism associated with the One Gluon Exchange and large D-state admixtures originated in pionic models. We analyze the contribution to these structure functions of the gluon polarization arising from the anomaly.

PhysicsParticle physicsSpin polarizationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuark modelConstituent quarkPartonGluonHigh Energy Physics::ExperimentNeutronNuclear ExperimentNucleonWave function
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The non-perturbative unquenched quark model

2017

In recent years states in the quarkonium spectrum not expected in the naive quark model have appeared and created a lot of interest. In the theoretical side the study of the effect of meson-meson thresholds in the spectrum have been performed in different approximations. In a quark model framework, and in the spirit of the Cornell model, when a meson-meson threshold is included, the coupling to all the quark-antiquark states have to be considered. In practice only the closest states are included perturbatively. In this contribution we will present a framework in which we couple quark-antiquark states with meson-meson states non-perturbatively, taking into account effectively the coupling to…

PhysicsParticle physicsTop quark010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999Quark modelNuclear TheoryHigh Energy Physics::PhenomenologyTop quark condensateQuarkonium01 natural sciencesBottom quark0103 physical sciencesB mesonHigh Energy Physics::ExperimentNon-perturbative010306 general physicsNuclear ExperimentX(3872)EPJ Web of Conferences
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Relic density of neutrinos with primordial asymmetries.

2008

We study flavor oscillations in the early Universe, assuming primordial neutrino-antineutrino asymmetries. Including collisions and pair processes in the kinetic equations, we not only estimate the degree of flavor equilibration, but for the first time also kinetic equilibration among neutrinos and with the ambient plasma. Typically, the restrictive big-bang nucleosynthesis bound on the nu(e)(nu) over bar (e) asymmetry indeed applies to all flavors as claimed in the previous literature, but fine-tuned initial asymmetries always allow for a large surviving neutrino excess radiation that may show up in precision cosmological data.

PhysicsParticle physicsmedia_common.quotation_subjectAstrophysics (astro-ph)Quark modelHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyFísicaAstrophysicsUniverseMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisNucleosynthesisAntimatterHigh Energy Physics::ExperimentNeutrinoLeptonmedia_commonPhysical review letters
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Watson’s theorem and theNΔ(1232)axial transition

2016

We present a new determination of the $N\mathrm{\ensuremath{\Delta}}$ axial form factors from neutrino induced pion production data. For this purpose, the model of Hernandez et al. [Phys. Rev. D 76, 033005 (2007)] is improved by partially restoring unitarity. This is accomplished by imposing Watson's theorem on the dominant vector and axial multipoles. As a consequence, a larger ${C}_{5}^{A}(0)$, in good agreement with the prediction from the off-diagonal Goldberger-Treiman relation, is now obtained.

PhysicsPionUnitarity010308 nuclear & particles physicsQuantum mechanics0103 physical sciencesQuark modelProduction (computer science)Neutrino010306 general physicsMultipole expansion01 natural sciencesNuclear theoryPhysical Review D
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