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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Critical phenomena ： ウィキペディア英語版 Critical phenomena In physics, critical phenomena is the collective name associated with the physics of critical points. Most of them stem from the divergence of the correlation length, but also the dynamics slows down. Critical phenomena include scaling relations among different quantities, power-law divergences of some quantities (such as the magnetic susceptibility in the ferromagnetic phase transition) described by critical exponents, universality, fractal behaviour, ergodicity breaking. Critical phenomena take place in second order phase transition, although not exclusively. The critical behavior is usually different from the mean-field approximation which is valid away from the phase transition, since the latter neglects correlations, which become increasingly important as the system approaches the critical point where the correlation length diverges. Many properties of the critical behavior of a system can be derived in the framework of the renormalization group. In order to explain the physical origin of these phenomena, we shall use the Ising model as a pedagogical example. ==The critical point of the 2D Ising model== Let us consider a $2D$ square array of classical spins which may only take two positions: +1 and −1, at a certain temperature $T$, interacting through the Ising classical Hamiltonian: : $H=\; -J\; \backslash sum\_\; S\_i\backslash cdot\; S\_j$ where the sum is extended over the pairs of nearest neighbours and $J$ is a coupling constant, which we will consider to be fixed. There is a certain temperature, called the Curie temperature or critical temperature, $T\_c$ below which the system presents ferromagnetic long range order. Above it, it is paramagnetic and is apparently disordered. At temperature zero, the system may only take one global sign, either +1 or -1. At higher temperatures, but below $T\_c$, the state is still globally magnetized, but clusters of the opposite sign appears. As the temperature increases, these clusters start to contain smaller clusters themselves, in a typical Russian dolls picture. Their typical size, called the correlation length, $\backslash xi$ grows with temperature until it diverges at $T\_c$. This means that the whole system is such a cluster, and there is no global magnetization. Above that temperature, the system is globally disordered, but with ordered clusters within it, whose size is again called ''correlation length'', but it is now decreasing with temperature. At infinite temperature, it is again zero, with the system fully disordered. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Critical phenomena」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.