The model for self-dual chiral bosons as a Hodge theory
arXiv:1109.3001 · doi:10.1140/epjc/s10052-011-1759-2
Abstract
We consider (1+1) dimensional theory for a single self-dual chiral boson as classical model for gauge theory. Using Batalin-Fradkin-Vilkovisky (BFV) technique the nilpotent BRST and anti BRST symmetry transformations for this theory have been studied. In this model other forms of nilpotent symmetry transformations like co-BRST and anti co-BRST which leave the gauge-fixing part of the action invariant, are also explored. We show that the nilpotent charges for these symmetry transformations satisfy the algebra of de Rham cohomological operators in differential geometry. The Hodge decomposition theorem on compact manifold is also studied in the context of conserved charges.
19 pages, No figures, Revtex, Final version to appear in EPJC
References in corpus (2)
Cited by in corpus (9)
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- Finite BRST transformation and constrained systems
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- (Anti-)chiral Superfield Approach to Nilpotent Symmetries: Self-Dual Chiral Bosonic Theory
- Gauged Floreanini-Jackiw type chiral boson and its BRST quantization
- A Quantum Mechanical Example for Hodge Theory
- Modified gauge unfixing formalism and gauge symmetries in the non-commutative chiral bosons theory
- Quantum gauge symmetry of reducible gauge theory
- Noncommutative Gauge Theories: Model for Hodge theory