Abstract
The calculation of bound states of relativistic subfermion fields within the framework of generalized Bargmann-Wigner equations is extended to the case of broken isospin symmetry. The investigation is performed for the two-particle sector of non-linearSU(2)×U(1) spinor-isospinor field models. In particular, the procedure is applied to composite vector bosons corresponding to a composite-particle description of electroweak gauge bosons as two-fermion bound states of microscopic subfermion fields.
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