Path Integral approach to kinematical browmian motion, due to random canonical transformation
| dc.creator | Tchoffo, M. | |
| dc.creator | Belinson, A. A. | |
| dc.date | 2006-04-21 | |
| dc.date.accessioned | 2026-07-07T07:11:25Z | |
| dc.date.available | 2026-07-07T07:11:25Z | |
| dc.description | The stochastization of the Jacobi second equality of classical mechanics, by Gaussian white noises for the Lagrangian of a particle in an arbitrary field is considered. The quantum mechanical Hamilton operator similar to that in Euclidian quantum theory is obtained. The conditional transition probability density of the presence of a Browmian particle is obtained with the help of the functional integral. The technique of factorisation of the solution of the Fokker-Planck equation is employed to evaluate the effective potential energy. | |
| dc.description | 13 pages, no figure | |
| dc.identifier | https://arxiv.org/abs/nlin/0604051 | |
| dc.identifier | http://arxiv.org/abs/nlin/0604051 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/111749 | |
| dc.subject | Exactly Solvable and Integrable Systems | |
| dc.title | Path Integral approach to kinematical browmian motion, due to random canonical transformation | |
| dc.type | text |