2010
DOI: 10.1063/1.3372732
|View full text |Cite
|
Sign up to set email alerts
|

BRST detour quantization: Generating gauge theories from constraints

Abstract: We present the Becchi–Rouet–Stora–Tyutin (BRST) cohomologies of a class of constraint (super) Lie algebras as detour complexes. By interpreting the components of detour complexes as gauge invariances, Bianchi identities, and equations of motion, we obtain a large class of new gauge theories. The pivotal new machinery is a treatment of the ghost Hilbert space designed to manifest the detour structure. Along with general results, we give details for three of these theories which correspond to gauge invariant spi… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
4
0

Year Published

2010
2010
2018
2018

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 10 publications
(4 citation statements)
references
References 83 publications
0
4
0
Order By: Relevance
“…These include relativistic and constant curvature spinning particles, the hydrogen atom with spin and other SO(d, 2) invariant conformal models [15]. Its worldline BRST operator can be treated using the detour methods of [16]. This yields an equivalent, reduced BRST operator…”
Section: First Quantized Dirac Equationmentioning
confidence: 99%
“…These include relativistic and constant curvature spinning particles, the hydrogen atom with spin and other SO(d, 2) invariant conformal models [15]. Its worldline BRST operator can be treated using the detour methods of [16]. This yields an equivalent, reduced BRST operator…”
Section: First Quantized Dirac Equationmentioning
confidence: 99%
“…See for instance[38] for the BRST quantization of several worldline models 10. Recall that the ghosts γi and βi are bosonic.…”
mentioning
confidence: 99%
“…in [9]) [11], [12], [13], [20], [22], including the BRST-BFV approach, e.g., in [14]- [19]. For MAS, the problem of field-theoretic description has not been solved completely, except for: massless constrained MS and MAS tensor fields on Minkowsky space, R 1.d−1 , as the elements of irreducible representations of gl(d)-algebra, in terms of multiforms [23] on a base of BRST detour quantization techniques [24], with Einstein operator for the equations of motion; constrained bosonic MAS fields with 2 group indices: Lagrangians for massless HS fields on Minkowsky and for massive HS fields on AdS spaces have been considered respectively in [25], [26], whereas the massless fields at the level of the equations of motion in a frame-like formulation were studied in [27].…”
Section: Introductionmentioning
confidence: 99%