1994
DOI: 10.1016/0370-2693(94)90205-4
|View full text |Cite
|
Sign up to set email alerts
|

Some remark on consistent anomalies in gauge theories

Abstract: The new method for solving the descent equations for gauge theories proposed in [1] is shown to be equivalent with that based on the "Russian formula". Moreover it allows to obtain in a closed form the expressions of the consistent anomalies in any space-time dimension.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
16
0

Year Published

1994
1994
2004
2004

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 31 publications
(16 citation statements)
references
References 31 publications
0
16
0
Order By: Relevance
“…In other word using the operator δ we can calculate the solution of the cohomology H(s mod d) if we know the solution of the cohomology H(s). Actually, as has been shown in [23], the cocycles obtained by the descent equations (3.4) turn out to be completely equivalent to those one based on the Russian formula.…”
Section: )mentioning
confidence: 70%
See 2 more Smart Citations
“…In other word using the operator δ we can calculate the solution of the cohomology H(s mod d) if we know the solution of the cohomology H(s). Actually, as has been shown in [23], the cocycles obtained by the descent equations (3.4) turn out to be completely equivalent to those one based on the Russian formula.…”
Section: )mentioning
confidence: 70%
“…In order to solve the tower (3.4) we shall make use of the following identity e δ s = (s + d)e δ , (3.8) which is a direct consequence of (3.7) (see [23]).…”
Section: )mentioning
confidence: 99%
See 1 more Smart Citation
“…The operator δ can be used to solve the descent equations (1.2). As it has been shown in [17,18,19] these solutions can be obtained from the equation…”
Section: Brst Symmetry For the Superstringmentioning
confidence: 99%
“…We can collect then, following [31], all the Ω G+N −p where the cocycle Ω G+N 0 , according to its zero form degree, depends only on the set of zero form variables (ω a bm , R a bmn , T a mn , θ a b , η a ) and their tangent space derivatives ∂ m . Taking into account that under the action of the operator δ the form degree and the ghost number are respectively raised and lowered by one unit and that in a space-time of dimension N a (N +1)form identically vanishes, it follows that eq.…”
Section: Weyl Invariant Scalar Field Lagrangiansmentioning
confidence: 99%