Vector Currents of Massive Neutrinos of an Electroweak Nature

TL;DR

This paper explores the unified electroweak structure of massive neutrinos, deriving equations linking their mass components to charge, charge radius, and magnetic moment, and discusses implications for neutrino universality and experimental limits.

Contribution

It introduces structural equations connecting neutrino mass components to electromagnetic properties based on fermion unification, highlighting neutrino universality and potential laboratory tests.

Findings

Neutrinos of vector nature share the same charge, charge radius, and magnetic moment regardless of mass.

Derived equations relate neutrino mass structure to electromagnetic characteristics.

Earlier measurements support a unified mass interaction model for neutrinos.

Abstract

The mass of an electroweakly interacting neutrino consists of the electric and weak parts responsible for the existence of its charge, charge radius, and magnetic moment. Such connections explain the formation of paraneutrinos, for example, at the polarized neutrino electroweak scattering by spinless nuclei. We derive the structural equations that relate the self-components of mass to charge, charge radius, and magnetic moment of each neutrino as a consequence of unification of fermions of a definite flavor. They indicate the availability of neutrino universality and require following its logic in a constancy law dependence of the size implied from the multiplication of a weak mass of neutrino by its electric mass. According to this principle, all Dirac neutrinos of a vector nature, regardless of the difference in their masses, have the same charge, an identical charge radius, as well as an equal magnetic moment. Thereby, the possibility appears of establishing the laboratory limits of weak masses of the investigated types of neutrinos. Finding estimates show clearly that the earlier measured properties of these particles may testify in favor of the unified mass structure of their interaction with any of the corresponding types of gauge fields.