Bhabha's Irreducible Spin (32,12) Equation as a Basis of Strong-Interaction Symmetries

Abstract
It is demonstrated that Bhabha's irreducible relativistic equation describing a particle with two mass states, one of mass m and spin 32 and another of mass λm and spin ½, where λ is arbitrary, can be used as the basis of a covariant theory of strong-interaction symmetries which incorporates spin splitting in a dynamical fashion. Detailed consequences of the theory have been obtained for the nonrelativistic case. Some new mass relations, in addition to the well-known ones, are derived.

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