Extended BRST invariance (BRST plus anti-BRST invariances) provides in principle a natural way of introducing the complete gauge fixing structure associated to a gauge field theory in the minimum representation of the algebra. However, as it happens in topological Yang Mills theory, not all gauge fixings can be obtained from a symmetrical extended BRST algebra, where antighosts belong to the same representation of the Lorentz group of the corresponding ghosts. We show here that, at non interacting level, a simple field redefinition makes it possible to start with an extended BRST algebra with symmetric ghost antighost spectrum and arrive at the gauge fixing action of topological Yang Mills theory
AbstractThe antifield-BRST formalism and the various cohomologies associated with it are surveyed an...
We present the mathematical considerations which determine all gauge invariant ac-tions and anomaly ...
We report on the nonlocal gauge invariant operator of dimension two, F 1/D^2 F. We are able to local...
The Sp(2)-gauge fixing of N = 1 super-Yang-Mills is considered here. We thereby apply the triplectic...
In this short note we extend the results of Alfaro and Damgaard on the origin of antifields to theor...
The classical formal equivalence upon a redefinition of the gauge connection between Chern-Simons th...
A superspace formulation for the Batalin Vilkovisky formalism (also called field-antifield quantizat...
We consider possible superfield representations of extended BRST symmetry for general gauge theories...
We show that it is possible to formulate the most general first-class gauge algebra of the operator ...
We continue the study of finite BRST–antiBRST transformations for general gauge theories in Lagrangi...
AbstractWe continue the study of finite BRST–antiBRST transformations for general gauge theories in ...
General structure of BRST-invariant constraint algebra is established, in its commutator and antibra...
We generalize the method of superfield Lagrangian BRST quantization in the part of the gauge-fixing ...
In order to construct a gauge-invariant two-point function in a Yang-Mills theory, we propose the us...
We completely compute the local BRST cohomology $H(s|d)$ of the combined Yang-Mills-2-form system co...
AbstractThe antifield-BRST formalism and the various cohomologies associated with it are surveyed an...
We present the mathematical considerations which determine all gauge invariant ac-tions and anomaly ...
We report on the nonlocal gauge invariant operator of dimension two, F 1/D^2 F. We are able to local...
The Sp(2)-gauge fixing of N = 1 super-Yang-Mills is considered here. We thereby apply the triplectic...
In this short note we extend the results of Alfaro and Damgaard on the origin of antifields to theor...
The classical formal equivalence upon a redefinition of the gauge connection between Chern-Simons th...
A superspace formulation for the Batalin Vilkovisky formalism (also called field-antifield quantizat...
We consider possible superfield representations of extended BRST symmetry for general gauge theories...
We show that it is possible to formulate the most general first-class gauge algebra of the operator ...
We continue the study of finite BRST–antiBRST transformations for general gauge theories in Lagrangi...
AbstractWe continue the study of finite BRST–antiBRST transformations for general gauge theories in ...
General structure of BRST-invariant constraint algebra is established, in its commutator and antibra...
We generalize the method of superfield Lagrangian BRST quantization in the part of the gauge-fixing ...
In order to construct a gauge-invariant two-point function in a Yang-Mills theory, we propose the us...
We completely compute the local BRST cohomology $H(s|d)$ of the combined Yang-Mills-2-form system co...
AbstractThe antifield-BRST formalism and the various cohomologies associated with it are surveyed an...
We present the mathematical considerations which determine all gauge invariant ac-tions and anomaly ...
We report on the nonlocal gauge invariant operator of dimension two, F 1/D^2 F. We are able to local...