Anomalous Electric Charge of a Neutrino of True Neutrality

Any dipole arises as a result of a kind of charge. Therefore, if each neutrino having a C-even or a C-odd charge possesses a mass of a vector $(V)$ or an axial-vector $(A)$ nature, from the point of view of mass-charge duality [1], the steadiness of an axial-vector electric charge distribution in all C-noninvariant leptons $(l^{A}=e^{A},$ $\mu^{A},$ $\tau^{A}, ...)$ must be accepted as the intralepton harmony of axial-vector types of forces. Then it is possible, for example, to present the anapole $(i=1)$ and electric dipole $(i=2)$ form factors $G_{il^{A}}$ depending on the momentum transfer square $q^{2}$ in the form $$G_{il^{A}}(q^{2})=g_{il^{A}}(0)+R_{il^{A}}(q^{2})+\Phi_{il^{A}}(\vec{q^{2}})+..., \eqno(1)$$ where $g_{il^{A}}$ define the static anapole and electric dipole, $R_{il^{A}}$ characterize the dependence of form factors $G_{il^{A}}$ on the lepton axial-vector radius. The functions $\Phi_{il^{A}}$ describe the anomalous behavior of axial-vector currents. Thus, a neutrino of true neutrality similarly to all other the axial-vector leptons must possess the anomalous electric charge of C-noninvariant nature. Such a type of charge says about the existence in neutrino of a kind of inertial mass.\\[4pt] [1] R.S. Sharafiddinov, Bull. Am. Phys. Soc. 59(5), T1.00009 (2014).