David Loebbaka
Abstract
Using a previously discussed dynamical model, we show that the baryon octet and decuplet poles alone lead to a simple explanation of the observed parity-violating nonleptonic hyperon decay amplitudes, essentially without involving any unknown parameters, provided that the strong interactions are $\mathrm{SU}(3)$-invariant.
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Using a previously discussed dynamical model, we show that the baryon octet and decuplet poles alone lead to a simple explanation of the observed parity-violating nonleptonic hyperon decay amplitudes, essentially without involving any unknown parameters, provided that the strong interactions are $\mathrm{SU}(3)$-invariant.
Key concepts: Octet, Hyperon, Physics, Particle physics, Baryon, Parity (physics), Amplitude, Invariant (physics)