Superspace Unitary Operator in Superfield Approach to Non-Abelian Gauge Theory with Dirac Fields

TL;DR

This paper derives the superspace unitary operator within the superfield approach to non-Abelian gauge theory with Dirac fields, providing explicit expressions without external Hermitian conjugation constraints, enhancing the BRST formalism framework.

Contribution

It introduces a novel derivation of the superspace unitary operator in non-Abelian gauge theory, avoiding external Hermitian conjugation conditions, and connects it with the horizontality condition and gauge invariant restriction.

Findings

Explicit expressions for the SUSP unitary operator derived.

Application of HC and GIR expressed via SUSP operators.

No external Hermitian conjugation imposed on parameters or fields.

Abstract

Within the framework of augmented version of the superfield approach to Becchi-Rouet-Stora-Tyutin (BRST) formalism, we derive the superspace unitary operator (and its Hermitian conjugate) in the context of four (3 + 1)-dimensional (4D) interacting non-Abelian 1-form gauge theory with Dirac fields. The ordinary 4D non-Abelian theory, defined on the flat 4D Minkowski spacetime manifold, is generalized onto a (4, 2)-dimensional supermanifold which is parameterized by the spacetime bosonic coordinates x^\mu (with \mu = 0, 1, 2, 3) and a pair of Grassmannian variables (\theta, \bar\theta) which satisfy the standard relationships: \theta^2 = {\bar\theta}^2 = 0, \theta\,\bar\theta + \bar\theta\,\theta = 0. Various consequences of the application of the above superspace (SUSP) unitary operator (and its Hermitian conjugate) are discussed. In particular, we obtain the results of the application of horizontality condition (HC) and gauge invariant restriction (GIR) in the language of the above SUSP operators. One of the novel results of our present investigation is the derivation of explicit expressions for the SUSP unitary operator (and its Hermitian conjugate) without imposing any Hermitian conjugation condition from outside on the parameters and (super)fields of the supersymmetric version of our 4D interacting non-Abelian 1-form theory with Dirac fields.