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On the algebraic structure of covariant anomalies and covariant Schwinger terms

Abstract

A cohomological characterization of covariant anomalies and covariant Schwinger terms in an anomalous Yang-Mills theory is formulated and w ill be geometrically interpreted. The BRS and anti-BRS transformations are defined as purely differential geometric objects. Finally the covariant descent equations are formulated within this context. (author).
Authors:
Publication Date:
Nov 19, 1992
Product Type:
Technical Report
Report Number:
UWThPh-1992-22
Reference Number:
SCA: 662100; PA: AIX-24:016907; SN: 93000944320
Resource Relation:
Other Information: PBD: 19 Nov 1992
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; YANG-MILLS THEORY; SCHWINGER TERMS; DIFFERENTIAL GEOMETRY; 662100; GENERAL THEORY OF PARTICLES AND FIELDS
OSTI ID:
10128409
Research Organizations:
Vienna Univ. (Austria). Inst. fuer Theoretische Physik
Country of Origin:
Austria
Language:
English
Other Identifying Numbers:
Other: ON: DE93615575; TRN: AT9200613016907
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
[8] p.
Announcement Date:
Jul 04, 2005

Citation Formats

Kelnhofer, G. On the algebraic structure of covariant anomalies and covariant Schwinger terms. Austria: N. p., 1992. Web.
Kelnhofer, G. On the algebraic structure of covariant anomalies and covariant Schwinger terms. Austria.
Kelnhofer, G. 1992. "On the algebraic structure of covariant anomalies and covariant Schwinger terms." Austria.
@misc{etde_10128409,
title = {On the algebraic structure of covariant anomalies and covariant Schwinger terms}
author = {Kelnhofer, G}
abstractNote = {A cohomological characterization of covariant anomalies and covariant Schwinger terms in an anomalous Yang-Mills theory is formulated and w ill be geometrically interpreted. The BRS and anti-BRS transformations are defined as purely differential geometric objects. Finally the covariant descent equations are formulated within this context. (author).}
place = {Austria}
year = {1992}
month = {Nov}
}