From 19248514d1cd4b9505e14bedfa206c29fe568a88 Mon Sep 17 00:00:00 2001 From: Flatiron Jenkins Date: Wed, 27 Nov 2024 05:49:33 -0500 Subject: [PATCH] Generated documentation for ctseg/3.3.x jenkins-TRIQS-ctseg_J-3.3.x-57 79dc64ad8b14e2ac29afb44e553661ae175e1fa2 --- ctseg/3.3.x/_sources/algorithm_implementation/ctseg.rst.txt | 2 +- ctseg/3.3.x/algorithm_implementation/ctseg.html | 2 +- 2 files changed, 2 insertions(+), 2 deletions(-) diff --git a/ctseg/3.3.x/_sources/algorithm_implementation/ctseg.rst.txt b/ctseg/3.3.x/_sources/algorithm_implementation/ctseg.rst.txt index 7ac07c4fb5..62ca853e4e 100644 --- a/ctseg/3.3.x/_sources/algorithm_implementation/ctseg.rst.txt +++ b/ctseg/3.3.x/_sources/algorithm_implementation/ctseg.rst.txt @@ -26,7 +26,7 @@ Here :math:`\beta` is the inverse temperature, :math:`a` denote orbital indices, :math:`n_a \equiv \sum_{\sigma} n_{a\sigma}`, :math:`s_a^{\xi} \equiv \frac{1}{2} \sum_{\sigma \sigma'} \overline{c}_{a\sigma} \sigma_{\sigma \sigma'}^{\xi} c_{a \sigma'}` and :math:`\sigma^{\xi}` are the Pauli matrices. :math:`\overline{c}_{a\sigma}(\tau)` and :math:`c_{a\sigma}(\tau)` are the :math:`\beta`-antiperiodic Grassmann fields corresponding to the fermion -creation and annihilation operators on the impurity, respectively. The :math:`\epsilon_{a\sigma}` are orbital energies and :math:`mu` +creation and annihilation operators on the impurity, respectively. The :math:`\epsilon_{a\sigma}` are orbital energies and :math:`\mu` is the chemical potential. This action can be recast as diff --git a/ctseg/3.3.x/algorithm_implementation/ctseg.html b/ctseg/3.3.x/algorithm_implementation/ctseg.html index 3c63c23802..0c9b00be36 100644 --- a/ctseg/3.3.x/algorithm_implementation/ctseg.html +++ b/ctseg/3.3.x/algorithm_implementation/ctseg.html @@ -229,7 +229,7 @@

Double expansion\(n_a \equiv \sum_{\sigma} n_{a\sigma}\), \(s_a^{\xi} \equiv \frac{1}{2} \sum_{\sigma \sigma'} \overline{c}_{a\sigma} \sigma_{\sigma \sigma'}^{\xi} c_{a \sigma'}\) and \(\sigma^{\xi}\) are the Pauli matrices. \(\overline{c}_{a\sigma}(\tau)\) and \(c_{a\sigma}(\tau)\) are the \(\beta\)-antiperiodic Grassmann fields corresponding to the fermion -creation and annihilation operators on the impurity, respectively. The \(\epsilon_{a\sigma}\) are orbital energies and \(mu\) +creation and annihilation operators on the impurity, respectively. The \(\epsilon_{a\sigma}\) are orbital energies and \(\mu\) is the chemical potential.

This action can be recast as