Abstract
It is shown that the presence of the additional symmetry discussed in [1] induces additional gauge fields, which can be held responsible for strong interactions of nucleons. In the spontaneous breaking of the symmetry of a vacuum the particles corresponding to these fields acquire masses. The latter are estimated. It is noted that in a special case the given theory goes over to the Weinberg-Salam theory describing weak and electromagnetic interactions of leptons.
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A. N. Kushnirenko, Izv. Vyssh. Uchebn. Zaved., Fiz., No. 5, 19 (1982).
A. N. Kushnirenko, Preprint No. 1, Inst. Probl. Mater. Akad. Nauk Ukr. SSR, Kiev (1969); Izv. Vyssh. Uchebn. Zaved., Fiz., No. 5, 40 (1971); Izv. Vyssh. Uchebn. Zaved., Fiz., No. 11, 48 (1972); Introduction to Quantum Field Theory [in Russian], Vysshaya Shkola, Moscow (1971); Preprint No. 7 [in Russian], Inst. Probl. Mater, Akad. Nauk Ukr. SSR, Kiev (1975); Preprint No. 2 [in Russian], Inst. Probl, Mater. Akad. Nauk Ukr. SSR, Kiev (1976); Conference Proceedings, Smolenice (1975), pp. 133–245.
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Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 7, pp. 84–88, July, 1982.
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Kushnirenko, A.N. Unified theory of weak, strong, and electromagnetic interactions: Spontaneous breaking of the symmetry of a vacuum. Soviet Physics Journal 25, 659–663 (1982). https://doi.org/10.1007/BF00911801
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DOI: https://doi.org/10.1007/BF00911801