Ergodic hypothesis: Difference between revisions
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A restatement of the ergodic hypothesis is to say that all allowed states are equally probable. | A restatement of the ergodic hypothesis is to say that all allowed states are equally probable. | ||
==See also== | |||
*[[Markov chain]] | |||
==References== | ==References== | ||
#[http://www.pnas.org/cgi/reprint/17/12/656 George D. Birkhoff, "Proof of the Ergodic Theorem", PNAS '''17''' pp. 656-660 (1931) ] | #[http://www.pnas.org/cgi/reprint/17/12/656 George D. Birkhoff, "Proof of the Ergodic Theorem", PNAS '''17''' pp. 656-660 (1931)] | ||
#[http://www.pnas.org/cgi/reprint/18/1/70 J. V. Neumann "Proof of the Quasi-ergodic Hypothesis", PNAS '''18''' pp. 70-82 (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)] | |||
#Adrian Patrascioiu "The Ergodic-Hypothesis, A Complicated Problem in Mathematics and Physics", Los Alamos Science, '''15''' pp. 263- (1987) | #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 12:01, 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, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \overline{O}_T} of an observable (i.e. molecular dynamics). i.e.
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \lim_{T \rightarrow \infty} \overline{O}_T (\{q_0(t)\},\{p_0(t)\}) = \langle O \rangle_\mu.}
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)