From 9f4c74a0324579c0c35a59c28c5d4c1a549953d9 Mon Sep 17 00:00:00 2001 From: Li Huang Date: Wed, 30 Nov 2022 01:12:58 +0800 Subject: [PATCH] update docs --- docs/src/examples/sigma.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/docs/src/examples/sigma.md b/docs/src/examples/sigma.md index 94d70072..e47e926f 100644 --- a/docs/src/examples/sigma.md +++ b/docs/src/examples/sigma.md @@ -113,7 +113,7 @@ open("sigma.data", "w") do fout end ``` -The calculated results are displayed in **Fig.1**. **Fig.1(a)** and **(b)** show the real and imaginary parts of the real frequency self-energy function, respectively. Near the Fermi level, Re``\Sigma(\omega)`` exhibits quasi-linear behavior, with which the quasiparticle weight ``Z`` and effective mass of electron ``m^*`` can be easily evaluated. As for the imaginary part, Im``\Sigma(0)`` is finite, which indicates that the electron-electron scattering is not trivial. **Fig.1(c)** shows the ``\alpha``-dependent ``\chi^{2}``. The vertical bar in this figure indicates the optimal ``\alpha`` is around 2.15. In **Fig.(d)**, the reproduced and raw self-energy functions are compared. It is apparent that they are consistent with each other. +The calculated results are displayed in **Fig.1**. **Fig.1(a)** and **(b)** show the real and imaginary parts of the real frequency self-energy function, respectively. Near the Fermi level, Re``\Sigma(\omega)`` exhibits quasi-linear behavior, with which the quasiparticle weight ``Z`` and effective mass of electron ``m^*`` can be easily evaluated. As for the imaginary part, Im``\Sigma(0)`` is finite, which indicates that the electron-electron scattering is not trivial. **Fig.1(c)** shows the ``\alpha``-dependent ``\chi^{2}``. The vertical bar in this figure indicates the optimal ``\alpha`` is around ``10^{2.154}``. In **Fig.(d)**, the reproduced and raw self-energy functions are compared. It is apparent that they are consistent with each other. ![T_E1.png](../assets/T_E1.png)