################################################################################ # # TRIQS: a Toolbox for Research in Interacting Quantum Systems # # Copyright (C) 2011 by M. Aichhorn, L. Pourovskii, V. Vildosola # # TRIQS is free software: you can redistribute it and/or modify it under the # terms of the GNU General Public License as published by the Free Software # Foundation, either version 3 of the License, or (at your option) any later # version. # # TRIQS is distributed in the hope that it will be useful, but WITHOUT ANY # WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS # FOR A PARTICULAR PURPOSE. See the GNU General Public License for more # details. # # You should have received a copy of the GNU General Public License along with # TRIQS. If not, see . # ################################################################################ #from pytriqs.applications.dft.sumk_lda import * #from pytriqs.applications.dft.converters.wien2k_converter import * from sumk_lda import * from converters.wien2k_converter import * from pytriqs.archive import * #===================================================== #Basic input parameters: LDAFilename = 'SrVO3' U = 4.0 J = 0.6 Beta = 40 DC_type = 1 # DC type: 0 FLL, 1 Held, 2 AMF useBlocs = True # use bloc structure from LDA input useMatrix = False # True: Slater parameters, False: Kanamori parameters U+2J, U, U-J use_spinflip = False # use the full rotational invariant interaction? #===================================================== U=U-2*J HDFfilename = LDAFilename+'.h5' # Init the SumK class SK=SumkLDA(hdf_file='SrVO3.h5',use_lda_blocks=True) Norb = SK.corr_shells[0][3] l = SK.corr_shells[0][2] from solver_multiband import * #from pytriqs.applications.dft.solver_multiband import * S=SolverMultiBand(beta=Beta,n_orb=Norb,gf_struct=SK.gf_struct_solver[0],map=SK.map[0]) SK.put_Sigma([S.Sigma]) Gloc=SK.extract_G_loc() ar = HDFArchive('srvo3_Gloc.output.h5','w') ar['Gloc'] = Gloc[0] del ar