Freedman-Townsend vertex from Hamiltonian BRST cohomology
arXiv:hep-th/0003192 · doi:10.1088/0264-9381/17/9/310
Abstract
Consistent interactions among a set of two-form gauge fields in four dimensions are derived along a Hamiltonian cohomological procedure. It is shown that the deformation of the BRST charge and BRST-invariant Hamiltonian for the free model leads to the Freedman-Townsend interaction vertex. The resulting interaction deforms both the gauge transformations and reducibility relations, but not the algebra of gauge transformations.
Latex 2.09, 16 pages, some errors in a few formulas corrected, two more references added, main conclusions and results unaffected, the final form to appear in Class. Quantum Grav
References in corpus (2)
Cited by in corpus (5)
- Seiberg-Witten maps from the point of view of consistent deformations of gauge theories
- Hamiltonian BRST deformation of a class of n-dimensional BF-type theories
- Note on two-dimensional nonlinear gauge theories
- Lagrangian cohomological couplings among vector fields and matter fields
- PT-symmetry breaking hamiltonian interactions in BF models