Abstract

We study the role of arbitrary (finite) anticanonical transformations in the field–antifield formalism and the gauge-fixing procedure based on the use of these transformations. The properties of the generating functionals of the Green functions subjected to finite anticanonical transformations are considered.

Highlights

  • The field–antifield formalism [1,2], summarizing numerous attempts to find correct quantization rules for various types of gauge models [3,4,5,6,7], is a powerful covariant quantization method which can be applied to arbitrary gauge invariant systems

  • We study the role of arbitrary anticanonical transformations in the field–antifield formalism and the gauge-fixing procedure based on the use of these transformations

  • It is an important property that the antibracket is preserved under the anticanonical transformations which are dual to canonical transformations for a Poisson bracket

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Summary

Introduction

The field–antifield formalism [1,2], summarizing numerous attempts to find correct quantization rules for various types of gauge models [3,4,5,6,7], is a powerful covariant quantization method which can be applied to arbitrary gauge invariant systems This method is based on the fundamental principle of BRST invariance [8,9] and has a rich new geometry [10]. We extend the use of anticanonical transformations in the field–antifield formalism from the infinitesimal level to the finite one, and we explore a gauge-fixing procedure for general gauge theories, based on arbitrary anticanonical transformations in an action being a proper solution to the quantum master equation with fixed boundary condition. C (2015) 75:270 erating functionals of the Green functions for a gauge system formulated in any two admissible gauges with the help of finite field-dependent BRST transformations

Field–antifield formalism
Infinitesimal anticanonical transformations
Finite anticanonical transformation
Solution to the basic equation
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