SU(4)F×SU(4)Csynthesis of strong, weak, and electromagnetic interactions

Abstract

The gauge group ${[\mathrm{SU}{\mathrm{}\left(2\right)\mathrm{}}_L\times \mathrm{SU}{\mathrm{}\left(2\right)\mathrm{}}_R]}_F\times \mathrm{SU}{\mathrm{}\left(4\right)\mathrm{}}_C$ is extended to $\mathrm{SU}{\mathrm{}\left(4\right)\mathrm{}}_F\times \mathrm{SU}{\mathrm{}\left(4\right)\mathrm{}}_C$ and the emergence of the low-energy symmetry $\mathrm{SU}{\mathrm{}\left(2\right)\mathrm{}}_L\times \mathrm{SU}{\mathrm{}\left(2\right)\mathrm{}}_R\times \mathrm{U}{\mathrm{}\left(1\right)\mathrm{}}_L\times \mathrm{U}{\mathrm{}\left(1\right)\mathrm{}}_R$ is discussed.