The complete solution of the Hamilton-Jacobi equation in Quantum Mechanics
| dc.creator | Ferraro, Rafael | |
| dc.date | 1996-07-17 | |
| dc.date.accessioned | 2026-07-07T06:13:54Z | |
| dc.date.available | 2026-07-07T06:13:54Z | |
| dc.description | An ordinary unambiguous integral representation for the finite propagator of a quantum system is found by starting of a privileged skeletonization of the functional action in phase space, provided by the complete solution of the Hamilton-Jacobi equation. This representation allows to regard the propagator as the sum of the contributions coming from paths where the momenta generated by the complete solution of the Hamilton-Jacobi equation are conserved -as it does happen on the classical trajectory-, but are not restricted to having the classical values associated with the boundary conditions for the original coordinates. | |
| dc.description | 8 pages (TeX manuscript) | |
| dc.identifier | https://arxiv.org/abs/quant-ph/9607013 | |
| dc.identifier | http://arxiv.org/abs/quant-ph/9607013 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/93268 | |
| dc.subject | Quantum Physics | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | The complete solution of the Hamilton-Jacobi equation in Quantum Mechanics | |
| dc.type | text |