Equivalence of Hamiltonian and Lagrangian Path Integral Quantization: Effective Gauge Theories
arXiv:hep-ph/9308201 · doi:10.1103/PhysRevD.49.1988
Abstract
The equivalence of correct Hamiltonian and naive Lagrangian (Faddeev--Popov) path integral quantization (Matthews's theorem) is proven for gauge theories with arbitrary effective interaction terms. Effective gauge-boson self-interactions and effective interactions with scalar and fermion fields are considered. This result becomes extended to effective gauge theories with higher derivatives of the fields.
14 pages LaTeX, BI-TP 93/40, August 1993
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- The new modified Vlasov equation for the systems with dissipative processes
- An Analysis of the First Order Form of Gauge Theories
- Non-Trivial Ghosts and Second Class Constraints
- Generalized Standard Model with higher-order derivatives under Rotor Mechanism and its Quantization