물리:복제_대칭_해

Differences

This shows you the differences between two versions of the page.

Link to this comparison view

Both sides previous revision Previous revision
물리:복제_대칭_해 [2023/09/05 15:46] – external edit 127.0.0.1물리:복제_대칭_해 [2026/09/27 16:05] (current) – [자유에너지 범함수] admin
Line 1: Line 1:
 ====자유에너지 범함수==== ====자유에너지 범함수====
-방금 본 것처럼 복제 대칭성이 있으면 $q_{\alpha\beta} = q$와 $m_{\alpha} = m$로 쓸 수 있다. 헬름홀츠 자유에너지는+[[물리:복제_트릭|복제 트릭]]에서 복제 대칭성이 있으면 $q_{\alpha\beta} = q$와 $m_{\alpha} = m$로 쓸 수 있다. [[물리:셰링턴-커크패트릭_모형|셰링턴-커크패트릭 모형]]의 헬름홀츠 자유에너지는
 \begin{align} \begin{align}
     -\beta [f] =& -\frac{\beta^2 J^2}{4n} \sum_{\alpha \neq \beta} q_{\alpha \beta}^2 - \frac{\beta J_0}{2n} \sum_{\alpha} m_{\alpha}^2 + \frac{\beta^2 J^2}{4} + \frac{1}{n} \ln \text{Tr}^{\prime} e^L \\     -\beta [f] =& -\frac{\beta^2 J^2}{4n} \sum_{\alpha \neq \beta} q_{\alpha \beta}^2 - \frac{\beta J_0}{2n} \sum_{\alpha} m_{\alpha}^2 + \frac{\beta^2 J^2}{4} + \frac{1}{n} \ln \text{Tr}^{\prime} e^L \\
  • 물리/복제_대칭_해.txt
  • Last modified: 2026/09/27 16:05
  • by admin