In 1938, Stueckelberg introduced a scalar field which makes an Abelian gauge theory
massive but preserves gauge invariance. The Stueckelberg mechanism is the introduction of …

We construct a non-Abelian gauge theory of chiral 2-forms (self-dual gauge fields) in 6
dimensions with a spatial direction compactified on a circle of radius R. It has the following …

Taking the simple examples of an Abelian 1-form gauge theory in two (1+ 1)-dimensions, a 2-
form gauge theory in four (3+ 1)-dimensions and a 3-form gauge theory in six (5+ 1) …

We show that the Becchi-Rouet-Stora-Tyutin (BRST)/anti-BRST invariant (3+ 1)-dimensional
two-form gauge theory has further nilpotent symmetries (dual BRST/anti-dual BRST) that …

We establish the connection between the generating functional for the first class theories
and the generating functional for the second class theories using the finite field dependent …

We demonstrate Yokoyama gaugeon formalism for the Abelian one-form gauge (Maxwell)
as well as for Abelian two-form gauge theory in the very special relativity (VSR) framework …

We do a perturbative calculation of the anomalous chromomagnetic dipole moment (CMDM)
of quarks at one-loop, considering the effect of a small mass of the gluon. We find partial …

A proof of renormalizability of the theory of the dynamical non-Abelian two-form is given
using the Zinn-Justin equation. Two previously unknown symmetries of the quantum action …

It is shown that the four (3+ 1)-dimensional (4D) free Abelian 2-form gauge theory provides
an example of (i) a class of field theoretical models for the Hodge theory, and (ii) a possible …

We prove that there is no power-counting renormalizable nonabelian generalization of the
abelian topological mass mechanism in four dimensions. The argument is based on the …