Mass Structure of Axial Vector Types of Leptons and Fields

TL;DR

This paper classifies axial-vector leptons and fields based on C-symmetry, deriving equations linking their mass components to electromagnetic properties, and suggests the existence of truly neutral leptons with specific structural characteristics.

Contribution

It introduces a new classification of leptons considering C-noninvariance and derives equations connecting mass structure to electromagnetic moments within flavor symmetry.

Findings

All C-antisymmetrical leptons share the same anapole and electric dipole.

The mass structure relates to electromagnetic properties like charge radius.

The analysis supports the existence of truly neutral leptons with specific mass and field properties.

Abstract

A classification of currents with respect to C-operation admits the existence of C-noninvariant types of Dirac fermions. Among them one can meet an electroweakly charged C-antisymmetrical leptons, the mass of which includes the electric and weak components responsible for the existence of their anapole charge, charge radius and electric dipole moment. Such connections can constitute the paraleptons of axial-vector currents, for example, at the interactions with field of spinless nuclei of true neutrality. We derive the united equations which relate the structural parts of mass to anapole, charge radius and electric dipole of any truly neutral lepton in the framework of flavour symmetry. Thereby, they establish the C-odd nature of leptons and fields at the level of constancy law of the size implied from the multiplication of a weak mass of C-antisymmetrical lepton by its electric mass. Therefore, all leptons of C-antisymmetricality regardless of the difference in masses of an axial-vector character, have the same anapole with his radius as well as an equal electric dipole. Their analysis together with measured value of an electric dipole moment of lepton gives the right to interpret not only the existence of truly neutral types of leptons and fields but also the availability of mass structure in them as the one of earlier laboratory facts.