Langevin equations

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The generalised Langevin equation can be considered as a mathematical rearrangement of the Liouville's theorem.

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 \frac{da(t)}{dt}= i\Omega a(t) - \int_0^t K(s) a(t-s) + F(t) ~ {\mathrm {d}}t}

where 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 a(t)} is a set of dynamical variables, 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 K(s)} is a damping function and 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 \Omega} is a frequency matrix.

See also[edit]

References[edit]

  1. Hazime Mori "Transport, Collective Motion, and Brownian Motion", Progress of Theoretical Physics 33 pp. 423-455 (1965)