C-invariance Criterion for the Gauge Field

To each type of gauge boson corresponds a kind of current. Therefore, the photon and other boson leptonic currents include both vector C-even and axial-vector C-odd components. In these circumstances, it seems possible to separate all gauge bosons into the two classes. The first of them consists of C-invariant vector bosons. They are of course the mediate bosons of vector $(V)$ types of interactions. We include in this class the vector photons $\gamma^{V}$ and weak $W^{\pm}$-bosons. A new example of the first group may be weak vector $Z^{\pm}$-bosons. To the second class apply the axial-vector C-noninvariant bosons. They come forward as the mediate bosons of axial-vector $(A)$ types of interactions. A beautiful example is weak $Z^{0}(W^{0})$-bosons and new axial-vector photons $(\gamma^{A})$ having the Coulomb nature. Recognizing this behavior of the mediate bosons and accepting its ideas about that a classification of elementary particles and currents with respect to C-operation [1] is compatible with gauge invariance, we would change our presentations about matter fields. Without such a changing, the unified field theory construction of elementary particles still remains not quite in line with nature.\\[4pt] [1] R.S. Sharafiddinov, Bull. Am. Phys. Soc. 57, KA.00069 (2012).