Abstract

Using the Batalin, Fradkin and Tyutin approach, the second-class higher derivative Maxwell–Chern–Simons–Proca model is converted into a mixed constrained one and then, the Hamiltonian path integral of the resulting mixed constrained system is constructed. The Hamiltonian path integral takes a manifestly Lorentz covariant form.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call