SU(6) Extension of the Weinberg-Tomozawa Meson-Baryon Lagrangian

Abstract

A consistent SU(6) extension of the Weinberg-Tomozawa meson-baryon chiral Lagrangian is constructed which incorporates vector meson and baryon decuplet degrees of freedom. The corresponding Bethe-Salpeter approximation predicts the existence of an isoscalar spin-parity ${3/2}^{-}$ $K^{\ast }N$ bound state (strangeness +1) with a mass around 1.7--1.8GeV. It is the highest hypercharge state of an antidecuplet SU(3) representation and it is unstable through $K^{\ast }$ decay. The estimated width of this state (neglecting d-wave $KN$ decay) turns out to be small ($\Gamma \le 15$MeV). Clear signals of this resonance would be found in reactions like $\gamma p\to {\bar{K}}^{0}p{K}^{+}{\pi }^{-}$ by looking at the three body $p{K}^{+}{\pi }^{-}$ invariant mass.

5 pages, REVTex, 1 Figure, discussion and references added

References in corpus (3)

• Big Bang Nucleosynthesis (in "The Review of Particle Properties" 2004)
• Baryonic Resonances from Baryon Decuplet-Meson Octet Interaction
• Large Nc Weinberg-Tomozawa interaction and negative parity s--wave baryon resonances

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