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Random energy model : ウィキペディア英語版
Random energy model

In statistical physics of disordered systems, the random energy model is a toy model of a system with quenched disorder. It concerns the statistics of a system of N particles, such that the number of possible states for the systems grow as 2^N, while the energy of such states is a Gaussian stochastic variable. The model has an exact solution. Its simplicity makes this model suitable for pedagogical introduction of concepts like quenched disorder and replica symmetry.
==Comparison with other disordered systems==
The r-spin Infinite Range Model, in which all r-spin sets interact with a random, independent, identically distributed interaction constant, becomes the Random-Energy Model in a suitably defined r\to\infty limit.
More precisely, if the Hamiltonian of the model is defined by

H(\sigma)=\sum_\sigma_\cdots\sigma_,

where the sum runs over all distinct sets of r indices, and, for each such set, \, J_ is an independent Gaussian variable of mean 0 and variance J^2r!/(2 N^), the Random-Energy model is recovered in the r\to\infty limit.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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