Quantum theory from Hamilton's Principle with imperfect information
| dc.creator | Hegseth, John | |
| dc.date | 2007-04-16 | |
| dc.date.accessioned | 2026-07-07T07:56:49Z | |
| dc.date.available | 2026-07-07T07:56:49Z | |
| dc.description | Many quantization schemes rely on analogs of classical mechanics where the connections with classical mechanics are indirect. In this work I propose a new and direct connection between classical mechanics and quantum mechanics where the quantum mechanical propagator is derived from a variational principle. This principle allows a physical system to have imperfect information, i.e., there is incomplete knowledge of the physical state, and many paths are allowed. | |
| dc.description | 4 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/0704.2078 | |
| dc.identifier | http://arxiv.org/abs/0704.2078 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/127452 | |
| dc.subject | Quantum Physics | |
| dc.title | Quantum theory from Hamilton's Principle with imperfect information | |
| dc.type | text |