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TRIQS · Oct 23, 2023 · 55dc7eb · 55dc7eb
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diff --git a/.doctrees/environment.pickle b/.doctrees/environment.pickle
diff --git a/.doctrees/nbsphinx/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb b/.doctrees/nbsphinx/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb
@@ -166,8 +166,6 @@
     "* `plo_cfg = plo.cfg`: the name of the config file for constructing the PLOs (see below)\n",
     "* `n_l = 35`: the number of Legendre coefficients to measure the imaginary-time Green's function in. Too few resulting in a \"bumpy\" Matsubara self-energy, too many include simulation noise. See also https://doi.org/10.1103/PhysRevB.84.075145.\n",
     "* `dc_dmft = True`: using the DMFT occupations for the double counting is mandatory in CSC calculations. The DFT occupations are not well defined after the first density correction anymore\n",
-    "* `mu_gap_gb2_threshold = 0.05`: the system is treated as gapped if the lattice Green's function at tau=beta/2 goes below the threshold. Then solid_dmft uses MaxEnt to set the chemical potential in the middle of the gap\n",
-    "* `mu_gap_occ_deviation = 0.4`: additional condition for the above described procedure. Only uses MaxEnt if the occupation after a solver run deviates from the target occupation by this value\n",
     "\n",
     "Group [solver]:\n",
     "\n",

diff --git a/.doctrees/nbsphinx/tutorials/SVO_os_qe/tutorial.ipynb b/.doctrees/nbsphinx/tutorials/SVO_os_qe/tutorial.ipynb
@@ -2,7 +2,7 @@
  "cells": [
   {
    "cell_type": "markdown",
-   "id": "b59009ba",
+   "id": "9cef9972",
    "metadata": {},
    "source": [
     "*Disclaimer:*\n",
@@ -14,7 +14,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "aa682d3a",
+   "id": "e0c30c14",
    "metadata": {},
    "source": [
     "Hello and welcome to the first part of the tutorial for solid_dmft. Here we will guide to set up and run your first DMFT calculations. \n",
@@ -31,7 +31,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "b7262d18",
+   "id": "5b3cb91c",
    "metadata": {},
    "source": [
     "---\n",
@@ -50,7 +50,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "e5242272",
+   "id": "62fc1ef5",
    "metadata": {},
    "source": [
     "```\n",
@@ -69,7 +69,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "b2877448",
+   "id": "81da7f55",
    "metadata": {},
    "source": [
     "The meaning of the column names is the following:\n",
@@ -84,7 +84,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "9132829a",
+   "id": "0304e52b",
    "metadata": {},
    "source": [
     "## 2. Looking at the Metal-Insulator Transition\n",
@@ -110,7 +110,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "0d5e9f67",
+   "id": "cbd9421d",
    "metadata": {},
    "source": [
     "## 3. Refining the diagram\n",
@@ -127,7 +127,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "cac9219b",
+   "id": "2528c743",
    "metadata": {},
    "source": [
     "## 4. Plotting the spectral function\n",
@@ -151,7 +151,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "3e891f43",
+   "id": "7239970c",
    "metadata": {},
    "source": [
     "## 5 Visualizing the MIT\n",

diff --git a/.doctrees/tutorials/Ce2O3_csc_w90/tutorial.doctree b/.doctrees/tutorials/Ce2O3_csc_w90/tutorial.doctree
diff --git a/.doctrees/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.doctree b/.doctrees/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.doctree
diff --git a/_sources/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb.txt b/_sources/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb.txt
@@ -166,8 +166,6 @@
     "* `plo_cfg = plo.cfg`: the name of the config file for constructing the PLOs (see below)\n",
     "* `n_l = 35`: the number of Legendre coefficients to measure the imaginary-time Green's function in. Too few resulting in a \"bumpy\" Matsubara self-energy, too many include simulation noise. See also https://doi.org/10.1103/PhysRevB.84.075145.\n",
     "* `dc_dmft = True`: using the DMFT occupations for the double counting is mandatory in CSC calculations. The DFT occupations are not well defined after the first density correction anymore\n",
-    "* `mu_gap_gb2_threshold = 0.05`: the system is treated as gapped if the lattice Green's function at tau=beta/2 goes below the threshold. Then solid_dmft uses MaxEnt to set the chemical potential in the middle of the gap\n",
-    "* `mu_gap_occ_deviation = 0.4`: additional condition for the above described procedure. Only uses MaxEnt if the occupation after a solver run deviates from the target occupation by this value\n",
     "\n",
     "Group [solver]:\n",
     "\n",

diff --git a/searchindex.js b/searchindex.js
diff --git a/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.html b/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.html
@@ -679,8 +679,6 @@ <h3>Input files for CSC DMFT calculations<a class="headerlink" href="#Input-file
 <li><p><code class="docutils literal notranslate"><span class="pre">plo_cfg</span> <span class="pre">=</span> <span class="pre">plo.cfg</span></code>: the name of the config file for constructing the PLOs (see below)</p></li>
 <li><p><code class="docutils literal notranslate"><span class="pre">n_l</span> <span class="pre">=</span> <span class="pre">35</span></code>: the number of Legendre coefficients to measure the imaginary-time Green’s function in. Too few resulting in a “bumpy” Matsubara self-energy, too many include simulation noise. See also <a class="reference external" href="https://doi.org/10.1103/PhysRevB.84.075145" rel="noopener noreferrer" target="_blank">https://doi.org/10.1103/PhysRevB.84.075145</a>.</p></li>
 <li><p><code class="docutils literal notranslate"><span class="pre">dc_dmft</span> <span class="pre">=</span> <span class="pre">True</span></code>: using the DMFT occupations for the double counting is mandatory in CSC calculations. The DFT occupations are not well defined after the first density correction anymore</p></li>
-<li><p><code class="docutils literal notranslate"><span class="pre">mu_gap_gb2_threshold</span> <span class="pre">=</span> <span class="pre">0.05</span></code>: the system is treated as gapped if the lattice Green’s function at tau=beta/2 goes below the threshold. Then solid_dmft uses MaxEnt to set the chemical potential in the middle of the gap</p></li>
-<li><p><code class="docutils literal notranslate"><span class="pre">mu_gap_occ_deviation</span> <span class="pre">=</span> <span class="pre">0.4</span></code>: additional condition for the above described procedure. Only uses MaxEnt if the occupation after a solver run deviates from the target occupation by this value</p></li>
 </ul>
 <p>Group [solver]:</p>
 <ul class="simple">

diff --git a/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb b/tutorials/PrNiO3_csc_vasp_plo_cthyb/tutorial.ipynb
@@ -166,8 +166,6 @@
     "* `plo_cfg = plo.cfg`: the name of the config file for constructing the PLOs (see below)\n",
     "* `n_l = 35`: the number of Legendre coefficients to measure the imaginary-time Green's function in. Too few resulting in a \"bumpy\" Matsubara self-energy, too many include simulation noise. See also https://doi.org/10.1103/PhysRevB.84.075145.\n",
     "* `dc_dmft = True`: using the DMFT occupations for the double counting is mandatory in CSC calculations. The DFT occupations are not well defined after the first density correction anymore\n",
-    "* `mu_gap_gb2_threshold = 0.05`: the system is treated as gapped if the lattice Green's function at tau=beta/2 goes below the threshold. Then solid_dmft uses MaxEnt to set the chemical potential in the middle of the gap\n",
-    "* `mu_gap_occ_deviation = 0.4`: additional condition for the above described procedure. Only uses MaxEnt if the occupation after a solver run deviates from the target occupation by this value\n",
     "\n",
     "Group [solver]:\n",
     "\n",

diff --git a/tutorials/SVO_os_qe/tutorial.ipynb b/tutorials/SVO_os_qe/tutorial.ipynb
@@ -2,7 +2,7 @@
  "cells": [
   {
    "cell_type": "markdown",
-   "id": "b59009ba",
+   "id": "9cef9972",
    "metadata": {},
    "source": [
     "*Disclaimer:*\n",
@@ -14,7 +14,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "aa682d3a",
+   "id": "e0c30c14",
    "metadata": {},
    "source": [
     "Hello and welcome to the first part of the tutorial for solid_dmft. Here we will guide to set up and run your first DMFT calculations. \n",
@@ -31,7 +31,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "b7262d18",
+   "id": "5b3cb91c",
    "metadata": {},
    "source": [
     "---\n",
@@ -50,7 +50,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "e5242272",
+   "id": "62fc1ef5",
    "metadata": {},
    "source": [
     "```\n",
@@ -69,7 +69,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "b2877448",
+   "id": "81da7f55",
    "metadata": {},
    "source": [
     "The meaning of the column names is the following:\n",
@@ -84,7 +84,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "9132829a",
+   "id": "0304e52b",
    "metadata": {},
    "source": [
     "## 2. Looking at the Metal-Insulator Transition\n",
@@ -110,7 +110,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "0d5e9f67",
+   "id": "cbd9421d",
    "metadata": {},
    "source": [
     "## 3. Refining the diagram\n",
@@ -127,7 +127,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "cac9219b",
+   "id": "2528c743",
    "metadata": {},
    "source": [
     "## 4. Plotting the spectral function\n",
@@ -151,7 +151,7 @@
   },
   {
    "cell_type": "markdown",
-   "id": "3e891f43",
+   "id": "7239970c",
    "metadata": {},
    "source": [
     "## 5 Visualizing the MIT\n",