6533b835fe1ef96bd12a0012

RESEARCH PRODUCT

Resonances and the Weinberg-Tomozawa 56-baryon-35-meson interaction

Lorenzo Luis SalcedoCarmen Garcia-recioJuan Nieves

subject

PhysicsNuclear and High Energy PhysicsParticle physicsMesonIsoscalarNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesParity (physics)StrangenessBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateHigh Energy Physics::ExperimentInvariant massVector mesonNuclear Experiment

description

Vector meson degrees of freedom are incorporated into the Weinberg-Tomozawa (WT) meson-baryon chiral Lagrangian by using a scheme which relies on spin--flavor SU(6) symmetry. The corresponding Bethe-Salpeter approximation successfully reproduces previous SU(3)--flavor WT results for the lowest-lying s--wave negative parity baryon resonances, and it also provides some information on the dynamics of the heavier ones. Moreover, it also predicts the existence of an isoscalar spin-parity $\frac32^-$ $K^*N$ bound state (strangeness +1) with a mass around 1.7--1.8 GeV, unstable through $K^*$ decay. Neglecting d-wave KN decays, this state turns out to be quite narrow ($\Gamma \le 15$ MeV) and it might provide clear signals in reactions like $\gamma p \to \bar K^0 p K^+\pi^-$ by looking at the three body $p K^+\pi^-$ invariant mass.

https://doi.org/10.1140/epja/i2006-10203-9