few gw metadata

meta_info/nomad_meta_info/exciting.nomadmetainfo.json

@@ -1048,7 +1048,7 @@
     }, {
       "description": "Linearization prefactor",
       "dtypeStr": "f",
-      "name": "x_exciting_GW_qp_linearization_prefactor",
+      "name": "x_exciting_gw_qp_linearization_prefactor",
       "shape": [
         "number_of_spin_channels",
         "number_of_eigenvalues_kpoints",
@@ -1060,7 +1060,7 @@
     }, {
       "description": "diagonal matrix elements of the exchange self-energy",
       "dtypeStr": "f",
-      "name": "x_exciting_GW_self_energy_x",
+      "name": "x_exciting_gw_self_energy_x",
       "shape": [
         "number_of_spin_channels",
         "number_of_eigenvalues_kpoints",
@@ -1073,7 +1073,7 @@
     }, {
       "description": "diagonal matrix elements of the correlation self-energy",
       "dtypeStr": "f",
-      "name": "x_exciting_GW_self_energy_c",
+      "name": "x_exciting_gw_self_energy_c",
       "shape": [
         "number_of_spin_channels",
         "number_of_eigenvalues_kpoints",
@@ -1086,7 +1086,7 @@
     }, {
       "description": "Treatment of the integrable singular terms in the calculation of the self energy. Values: 'mpb' - Auxiliary function method by S. Massidda, M. Posternak, and A. Baldereschi, PRB 48, 5058 (1993); 'crg' - Auxiliary function method by P. Carrier, S. Rohra, and A. Goerling, PRB 75, 205126 (2007).",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_self_energy_singularity_treatment",
+      "name": "x_exciting_gw_self_energy_singularity_treatment",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1094,7 +1094,7 @@
     },  {
       "description": "Models for the correlation self-energy analytical continuation: 'pade' -  Pade's approximant (by H. J. Vidberg and J. W. Serence, J. Low Temp. Phys. 29, 179 (1977)); 'mpf' -  Multi-Pole Fitting (by H. N Rojas, R. W. Godby and R. J. Needs, Phys. Rev. Lett. 74, 1827 (1995)); 'cd' - contour deformation; 'ra' - real axis",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_self_energy_c_analytical_continuation",
+      "name": "x_exciting_gw_self_energy_c_analytical_continuation",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1102,7 +1102,7 @@
     }, {
       "description": "Frequency integration grid type for the correlational self energy: 'eqdis' - equidistant frequencies from 0 to freqmax; 'gaulag' - Gauss-Laguerre quadrature from 0 to infinity; 'gauleg' - Gauss-Legendre quadrature from 0 to freqmax; 'gaule2' (default) - double Gauss-Legendre quadrature from 0 to freqmax and from freqmax to infinity.",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_frequency_grid_type",
+      "name": "x_exciting_gw_frequency_grid_type",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1110,7 +1110,7 @@
     },   {
       "description": "Model used to calculate the dinamically-screened Coulomb potential: 'rpa' - Full-frequency random-phase approximation; 'ppm' - Godby-Needs plasmon-pole model Godby and Needs, Phys. Rev. Lett. 62, 1169 (1989); 'ppm_hl' - Hybertsen and Louie, Phys. Rev. B 34, 5390 (1986); 'ppm_lh' - von der Linden and P. Horsh, Phys. Rev. B 37, 8351 (1988); 'ppm_fe' - Farid and Engel, Phys. Rev. B 47,15931 (1993); 'cdm' - Contour deformation method, Phys. Rev. B 67, 155208 (2003).)",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_screened_Coulomb",
+      "name": "x_exciting_gw_screened_Coulomb",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1118,7 +1118,23 @@
     }, {
       "description": "Option for treating the core states in the GW calculation: all - All electron calculation; val - Valence electron only calculation; vab - Core electrons are excluded from the mixed product basis; xal - All electron treatment of the exchange self-energy only",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_core_treatment",
+      "name": "x_exciting_gw_core_treatment",
+      "shape": [],
+      "superNames": [
+        "section_method"
+      ]
+    },  {
+      "description": "Type of volume averaging for the dynamically screened Coulomb potential: isotropic - Simple averaging along a specified direction using only diagonal components of the dielectric tensor; anisotropic - Anisotropic screening by C. Freysoldt et al., CPC 176, 1-13 (2007)",
+      "dtypeStr": "C",
+      "name": "x_exciting_gw_screened_coulomb_volume_average",
+      "shape": [],
+      "superNames": [
+        "section_method"
+      ]
+    },  {
+      "description": "Exchange-correlation functional of the ground-state calculation.",
+      "dtypeStr": "C",
+      "name": "x_exciting_gw_starting_point",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1127,33 +1143,56 @@
       "description": "Number of poles used in the analytical continuation.",
       "dtypeStr": "i",
       "kindStr": "type_dimension",
-      "name": "x_exciting_GW_self_energy_c_number_of_poles",
+      "name": "x_exciting_gw_self_energy_c_number_of_poles",
       "shape": [],
       "superNames": [
         "section_method"
       ]
     }, {
-      "description": "Number of empty states to be used to calculate the correlation self energy.",
+      "description": "Cut-off parameter for the truncation of the expansion of the plane waves in the interstitial region.",
+      "dtypeStr": "f",
+      "name": "x_exciting_gw_mixed_basis_gmax",
+      "shape": [],
+      "superNames": [
+        "section_method"
+      ]
+    }, {
+      "description": "Eigenvalue threshold below which the egenvectors are discarded in the construction of the radial basis set.",
+      "dtypeStr": "f",
+      "name": "x_exciting_gw_mixed_basis_tolerance",
+      "shape": [],
+      "superNames": [
+        "section_method"
+      ]
+    }, {
+      "description": "Maximum l value used for the radial functions within the muffin-tin",
       "dtypeStr": "i",
-      "name": "x_exciting_GW_self_energy_c_empty_states",
+      "name": "x_exciting_gw_mixed_basis_lmax",
       "shape": [],
       "superNames": [
         "section_method"
       ]
     }, {
-      "description": "Gives the number of eigenvalues, see eigenvalues_values.",
+      "description": "Auxillary basis set used for non-local operators: mixed - mixed basis set, Kotani and Schilfgaarde, Solid State Comm. 121, 461 (2002).",
+      "dtypeStr": "C",
+      "name": "x_exciting_gw_basis_set",
+      "shape": [],
+      "superNames": [
+        "section_method"
+      ]
+    }, {
+      "description": "Number of empty states to be used to calculate the correlation self energy.",
       "dtypeStr": "i",
-      "kindStr": "type_dimension",
-      "name": "number_of_eigenvalues",
+      "name": "x_exciting_gw_self_energy_c_empty_states",
       "shape": [],
       "superNames": [
-        "section_eigenvalues"
+        "section_method"
       ]
     }, {
       "description": "Number of empty states used to compute the polarizability P",
       "dtypeStr": "i",
       "kindStr": "type_dimension",
-      "name": "x_exciting_GW_polarizability_empty_states",
+      "name": "x_exciting_gw_polarizability_empty_states",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1161,7 +1200,7 @@
     }, {
       "description": "GW methodology: exciting test variable",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_type_test",
+      "name": "x_exciting_gw_type_test",
       "shape": [],
       "superNames": [
         "section_method"
@@ -1169,7 +1208,7 @@
     }, {
       "description": "GW methodology: G0W0; ev-scGW: (eigenvalues self-consistent GW) – Phys.Rev.B 34, 5390 (1986); qp-scGW: (quasi-particle self-consistent GW) – Phys. Rev. Lett. 96, 226402 (2006)  scGW0: (self-consistent G with fixed W0) – Phys.Rev.B 54, 8411 (1996); scG0W: (self-consistent W with fixed G0); scGW: (self-consistent GW) – Phys. Rev. B 88, 075105 (2013)",
       "dtypeStr": "C",
-      "name": "x_exciting_GW_type",
+      "name": "x_exciting_gw_type",
       "shape": [],
       "superNames": [
         "section_method"