O. Shito
Abstract
A quark-diquark model of baryons is adopted to describe nonleptonic decays of hyperons. Parity-violating and parity-conserving decays are assumed to rise, respectively, through weak and weak-strong sequential decays of the constituent strange quark or diquark of baryons. A simple way is shown to explain most features of both decays.
OpenAlex reports 2 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
A quark-diquark model of baryons is adopted to describe nonleptonic decays of hyperons. Parity-violating and parity-conserving decays are assumed to rise, respectively, through weak and weak-strong sequential decays of the constituent strange quark or diquark of baryons. A simple way is shown to explain most features of both decays.
Key concepts: Diquark, Physics, Hyperon, Particle physics, Baryon, Parity (physics), Quark, Nuclear physics