Ergodic hypothesis: Difference between revisions
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#[http://www.pnas.org/cgi/reprint/18/3/263 J. V. Neumann "Physical Applications of the Ergodic Hypothesis", PNAS '''18''' pp. 263-266 (1932)] | #[http://www.pnas.org/cgi/reprint/18/3/263 J. V. Neumann "Physical Applications of the Ergodic Hypothesis", PNAS '''18''' pp. 263-266 (1932)] | ||
#[http://www.pnas.org/cgi/reprint/18/3/279 G. D. Birkhoff and B. O. Koopman "Recent Contributions to the Ergodic Theory", PNAS '''18''' pp. 279-282 (1932)] | #[http://www.pnas.org/cgi/reprint/18/3/279 G. D. Birkhoff and B. O. Koopman "Recent Contributions to the Ergodic Theory", PNAS '''18''' pp. 279-282 (1932)] | ||
#Adrian Patrascioiu "The Ergodic-Hypothesis, A Complicated Problem in Mathematics and Physics", Los Alamos Science, '''15''' pp. 263- (1987) | #[http://library.lanl.gov/cgi-bin/getfile?15-18.pdf Adrian Patrascioiu "The Ergodic-Hypothesis, A Complicated Problem in Mathematics and Physics", Los Alamos Science, '''15''' pp. 263- (1987)] | ||
[[category: Computer simulation techniques]] | [[category: Computer simulation techniques]] |
Revision as of 12:03, 14 August 2007
The Ergodic hypothesis (Ref 1 and 2) essentially states that an ensemble average (i.e. Monte Carlo) of an observable, is equivalent to the time average, of an observable (i.e. molecular dynamics). i.e.
A restatement of the ergodic hypothesis is to say that all allowed states are equally probable.
See also
References
- George D. Birkhoff, "Proof of the Ergodic Theorem", PNAS 17 pp. 656-660 (1931)
- J. V. Neumann "Proof of the Quasi-ergodic Hypothesis", PNAS 18 pp. 70-82 (1932)
- J. V. Neumann "Physical Applications of the Ergodic Hypothesis", PNAS 18 pp. 263-266 (1932)
- G. D. Birkhoff and B. O. Koopman "Recent Contributions to the Ergodic Theory", PNAS 18 pp. 279-282 (1932)
- Adrian Patrascioiu "The Ergodic-Hypothesis, A Complicated Problem in Mathematics and Physics", Los Alamos Science, 15 pp. 263- (1987)