dorsal/arxiv
View SchemaA generalized form of Hamilton's principle
| Authors | John Hegseth |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0505214 |
| URL | https://arxiv.org/abs/quant-ph/0505214 |
Abstract
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. I identify this variational principle as a generalized form of Hamilton's principle. This proposed variational principle is unusual because the physical system is allowed to have imperfect information, i.e., there is incomplete knowledge of the physical state. Two distribution functionals over possible generalized momentum paths a[p(t)] and generalized coordinates paths b[q(t)] are defined. A generalized action is defined that corresponds to a contraction of a[p(t)], b[q(t)], and a matrix of the action evaluated at all possible p and q paths. Hamilton's principle is the extremization of the generalized action over all possible distributions. The normalization of the two distributions allows their values to be negative and they are shown to be the real and imaginary parts of the complex amplitude. The amplitude in the Feynman path integral is shown to be an optimal vector that extremizes the generalized action. This formulation is also shown to be directly applicable to statistical mechanics and I show how irreversible behavior and the micro-canonical ensemble follows immediately.
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"abstract": "Many quantization schemes rely on analogs of classical mechanics where the\nconnections with classical mechanics are indirect. In this work I propose a new\nand direct connection between classical mechanics and quantum mechanics where\nthe quantum mechanical propagator is derived from a variational principle. I\nidentify this variational principle as a generalized form of Hamilton\u0027s\nprinciple. This proposed variational principle is unusual because the physical\nsystem is allowed to have imperfect information, i.e., there is incomplete\nknowledge of the physical state. Two distribution functionals over possible\ngeneralized momentum paths a[p(t)] and generalized coordinates paths b[q(t)]\nare defined. A generalized action is defined that corresponds to a contraction\nof a[p(t)], b[q(t)], and a matrix of the action evaluated at all possible p and\nq paths. Hamilton\u0027s principle is the extremization of the generalized action\nover all possible distributions. The normalization of the two distributions\nallows their values to be negative and they are shown to be the real and\nimaginary parts of the complex amplitude. The amplitude in the Feynman path\nintegral is shown to be an optimal vector that extremizes the generalized\naction. This formulation is also shown to be directly applicable to statistical\nmechanics and I show how irreversible behavior and the micro-canonical ensemble\nfollows immediately.",
"arxiv_id": "quant-ph/0505214",
"authors": [
"John Hegseth"
],
"categories": [
"quant-ph"
],
"title": "A generalized form of Hamilton\u0027s principle",
"url": "https://arxiv.org/abs/quant-ph/0505214"
},
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