English

Notes on Lagrangean and Hamiltonian Symmetries

High Energy Physics - Theory 2007-05-23 v1

Abstract

The Hamiltonization of local symmetries of the form δqA=\eaRaA(q,q˙)\delta q^A = \ea{R_a}^A(q,\dot q) or δqA=\ea˙RaA(q,q˙)\delta q^A = \dot\ea{R_a}^A (q,\dot q) for arbitrary Lagrangean model L(qA,q˙A)L(q^A,\dot q^A) is considered. We show as the initial symmetries are transformed in the transition from LL to first order action, and then to the Hamiltonian action SH=dτ(pAq˙AH0vαΦα)S_H=\int{\rm d}\tau(p_A\dot q^A-H_0-v^\alpha\Phi_\alpha), where Φα\Phi_\alpha are the all (first and second class) primary constraints. An exact formulae for local symmetries of SHS_H in terms of the initial generators RaA{R_a}^A and all primary constraints Φα\Phi_\alpha are obtained.

Keywords

Cite

@article{arxiv.hep-th/9412244,
  title  = {Notes on Lagrangean and Hamiltonian Symmetries},
  author = {A. A. Deriglazov},
  journal= {arXiv preprint arXiv:hep-th/9412244},
  year   = {2007}
}

Comments

7 pages, LaTeX

R2 v1 2026-07-22T15:53:08.288Z