From a7a00543664bc7e5cfb3056e4816b8d7e232739b Mon Sep 17 00:00:00 2001 From: Yuichi Motoyama Date: Tue, 19 Mar 2024 14:16:07 +0900 Subject: [PATCH] added description of ds1 --- doc/en/dla/users-manual/output.rst | 4 ++++ doc/jp/dla/users-manual/output.rst | 5 +++++ 2 files changed, 9 insertions(+) diff --git a/doc/en/dla/users-manual/output.rst b/doc/en/dla/users-manual/output.rst index ba712cb..8d6ea4c 100644 --- a/doc/en/dla/users-manual/output.rst +++ b/doc/en/dla/users-manual/output.rst @@ -221,6 +221,10 @@ For precise analysis, we need to take into account not only the statistical erro :math:`\displaystyle \chi^{zz}(\vec{k}, \omega=0) = \beta N_s \left[\left\langle (\tilde{m}_K^z)^2 \right\rangle - \left\langle \tilde{m}_K^z \right\rangle^2 \right]` +``ds1`` + The derivative of the "magnetization" (``amzu``) with respect to the temperature. + + :math:`\displaystyle T\frac{\partial \left\langle \tilde{m}^z \right\rangle}{\partial T} = -\beta\frac{\partial \left\langle \tilde{m}^z \right\rangle}{\partial\beta}` ``wi2`` The winding number. diff --git a/doc/jp/dla/users-manual/output.rst b/doc/jp/dla/users-manual/output.rst index 965355d..11e807d 100644 --- a/doc/jp/dla/users-manual/output.rst +++ b/doc/jp/dla/users-manual/output.rst @@ -217,6 +217,11 @@ NOTICE: 一般にモンテカルロ法では, 比熱や感受率など, サン :math:`\displaystyle \chi^{zz}(\vec{k}, \omega=0) = \beta N_s \left[\left\langle (\tilde{m}_K^z)^2 \right\rangle - \left\langle \tilde{m}_K^z \right\rangle^2 \right]` +``ds1`` + 「磁化 ``amzu`` 」の温度微分. + + :math:`\displaystyle T\frac{\partial \left\langle \tilde{m}^z \right\rangle}{\partial T} = -\beta\frac{\partial \left\langle \tilde{m}^z \right\rangle}{\partial\beta}` + ``wi2`` ワインディングナンバー.