0000000000585369

AUTHOR

Maxim Mai

showing 4 related works from this author

Weak decays of heavy hadrons into dynamically generated resonances

2016

In this paper, we present a review of recent works on weak decay of heavy mesons and baryons with two mesons, or a meson and a baryon, interacting strongly in the final state. The aim is to learn about the interaction of hadrons and how some particular resonances are produced in the reactions. It is shown that these reactions have peculiar features and act as filters for some quantum numbers which allow to identify easily some resonances and learn about their nature. The combination of basic elements of the weak interaction with the framework of the chiral unitary approach allow for an interpretation of results of many reactions and add a novel information to different aspects of the hadron…

QuarkNuclear and High Energy PhysicsParticle physicsFinal state interactionNuclear TheoryMesonNuclear TheoryHadronBaryon weak decaysFOS: Physical sciencesGeneral Physics and AstronomyHadronsLambda01 natural sciencesHeavy mesonNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)Nuclear Experiment010306 general physicsWave functionWeak interactions (Nuclear physics)PhysicsMesonic and baryonic resonances010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)State (functional analysis)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentProduction (computer science)International Journal of Modern Physics E
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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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Predictions for the Lambda(b) -> J/psi Lambda (1405) decay

2015

We calculate the shape of the pi Sigma and (K) over bar N invariant mass distributions in the Lambda(b) -> J/psi pi Sigma and Lambda(b) -> J/psi (K) over bar N decays that are dominated by the Lambda (1405) 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 pi Sig…

High Energy Physics::PhenomenologyNuclear TheoryFísicaHigh Energy Physics::ExperimentNuclear Experiment
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Predictions for the $\Lambda_b \to J/\psi ~ \Lambda(1405)$ decay

2015

We calculate the shape of the $\pi\Sigma$ and $\bar K N$ invariant mass distributions in the $\Lambda_b \to J/\psi\, \pi\Sigma$ and $\Lambda_b \to J/\psi \,\bar K N$ decays that are dominated by the $\Lambda(1405)$ 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 related by SU(3) symmetry. 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 …

High Energy Physics - PhenomenologyNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics::ExperimentNuclear ExperimentHigh Energy Physics - Experiment
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