Schwinger-Dyson BRST-Symmetry and the Equivalence of Hamiltonian and Lagrangian Quantistion
arXiv:hep-th/9303027 · doi:10.1016/0370-2693(93)91035-L
Abstract
Implementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST-formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct consequence of the Fradkin-Vilkovisky theorem in Hamiltonian BRST quantisation.
10p, KUL-TF-93/08 and CERN- TH-6823/93
Cited by in corpus (10)
- Antibracket, Antifields and Gauge-Theory Quantization
- Odd Scalar Curvature in Anti-Poisson Geometry
- Generalized Lagrangian Master Equations
- On SU(2) anomaly and Majorana fermions
- Poisson structures in BRST-antiBRST invariant Lagrangian formalism
- From the BRST invariant Hamiltonian to the Field-Antifield Formalism
- A quantum field theoretical approach to the P vs. NP problem via the sign of the fermionic Quantum Monte Carlo
- The Batalin-Vilkovisky Field-Antifield Action for Systems with First-Class Constraints
- Schwinger--Dyson BRST symmetry and the Batalin--Vilkovisky Lagrangian Quantisation of Gauge Theories with Open or Reducible Gauge Algebras
- Batalin-Vilkovisky field-antifield quantisation of fluctuations around classical field configurations