Lorentz-Covariant Quantization of Massive Non-Abelian Gauge Fields in The Hamiltonian Path-Integral Formalism
Su, Jun-Chen
arXiv, 0506101 / Harvested from arXiv
Text on arXiv
The massive non-Abelian gauge fields are quantized Lorentz-covariantly in the Hamiltonian path-integral formalism. In the quantization, the Lorentz condition, as a necessary constraint, is introduced initially and incorporated into the massive Yang-Mills Lagrangian by the Lagrange multiplier method so as to make each temporal component of a vector potential to have a canonically conjugate counterpart. The result of this quantization is confirmed by the quantization performed in the Lagrangian path-integral formalism by applying the Lagrange multiplier method which is shown to be equivalent to the Faddeev-Popov approach.
Publié le : 2005-06-13
Classification:  High Energy Physics - Theory,  Mathematical Physics 
@article{0506101,
     author = {Su, Jun-Chen},
     title = {Lorentz-Covariant Quantization of Massive Non-Abelian Gauge Fields in
  The Hamiltonian Path-Integral Formalism},
     journal = {arXiv},
     volume = {2005},
     number = {0},
     year = {2005},
     language = {en},
     url = {http://dml.mathdoc.fr/item/0506101}
}

Su, Jun-Chen. Lorentz-Covariant Quantization of Massive Non-Abelian Gauge Fields in
  The Hamiltonian Path-Integral Formalism. arXiv, Tome 2005 (2005) no. 0, . http://gdmltest.u-ga.fr/item/0506101/