################################################################################ # # TRIQS: a Toolbox for Research in Interacting Quantum Systems # # Copyright (C) 2011 by M. Aichhorn # # 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 types import * import numpy from pytriqs.archive import * import pytriqs.utility.mpi as mpi from math import sqrt from converter_tools import * class HkConverter(ConverterTools): """ Conversion from general H(k) file to an hdf5 file that can be used as input for the SumKDFT class. """ def __init__(self, hk_filename, hdf_filename, dft_subgrp = 'dft_input', symmcorr_subgrp = 'dft_symmcorr_input', repacking = False): """ Init of the class. """ assert type(hk_filename)==StringType,"HkConverter: hk_filename must be a filename." self.hdf_file = hdf_filename self.dft_file = hk_filename self.dft_subgrp = dft_subgrp self.symmcorr_subgrp = symmcorr_subgrp self.fortran_to_replace = {'D':'E', '(':' ', ')':' ', ',':' '} # Checks if h5 file is there and repacks it if wanted: import os.path if (os.path.exists(self.hdf_file) and repacking): ConverterTools.repack(self) def convert_dmft_input(self, first_real_part_matrix = True, only_upper_triangle = False, weights_in_file = False): """ Reads the input files, and stores the data in the HDFfile """ # Read and write only on the master node if not (mpi.is_master_node()): return mpi.report("Reading input from %s..."%self.dft_file) # R is a generator : each R.Next() will return the next number in the file R = ConverterTools.read_fortran_file(self,self.dft_file,self.fortran_to_replace) try: energy_unit = 1.0 # the energy conversion factor is 1.0, we assume eV in files n_k = int(R.next()) # read the number of k points k_dep_projection = 0 SP = 0 # no spin-polarision SO = 0 # no spin-orbit charge_below = 0.0 # total charge below energy window is set to 0 density_required = R.next() # density required, for setting the chemical potential symm_op = 0 # No symmetry groups for the k-sum # the information on the non-correlated shells is needed for defining dimension of matrices: n_shells = int(R.next()) # number of shells considered in the Wanniers # corresponds to index R in formulas # now read the information about the shells: shells = [ [ int(R.next()) for i in range(4) ] for icrsh in range(n_shells) ] # reads iatom, sort, l, dim n_corr_shells = int(R.next()) # number of corr. shells (e.g. Fe d, Ce f) in the unit cell, # corresponds to index R in formulas # now read the information about the shells: corr_shells = [ [ int(R.next()) for i in range(6) ] for icrsh in range(n_corr_shells) ] # reads iatom, sort, l, dim, SO flag, irep # determine the number of inequivalent correlated shells and maps, needed for further reading [n_inequiv_shells, corr_to_inequiv, inequiv_to_corr] = ConverterTools.det_shell_equivalence(self,corr_shells) use_rotations = 0 rot_mat = [numpy.identity(corr_shells[icrsh][3],numpy.complex_) for icrsh in xrange(n_corr_shells)] rot_mat_time_inv = [0 for i in range(n_corr_shells)] # Representative representations are read from file n_reps = [1 for i in range(n_inequiv_shells)] dim_reps = [0 for i in range(n_inequiv_shells)] T = [] for icrsh in range(n_inequiv_shells): n_reps[icrsh] = int(R.next()) # number of representatives ("subsets"), e.g. t2g and eg dim_reps[icrsh] = [int(R.next()) for i in range(n_reps[icrsh])] # dimensions of the subsets # The transformation matrix: # is of dimension 2l+1, it is taken to be standard d (as in Wien2k) ll = 2*corr_shells[inequiv_to_corr[icrsh]][2]+1 lmax = ll * (corr_shells[inequiv_to_corr[icrsh]][4] + 1) T.append(numpy.zeros([lmax,lmax],numpy.complex_)) T[icrsh] = numpy.array([[0.0, 0.0, 1.0, 0.0, 0.0], [1.0/sqrt(2.0), 0.0, 0.0, 0.0, 1.0/sqrt(2.0)], [-1.0/sqrt(2.0), 0.0, 0.0, 0.0, 1.0/sqrt(2.0)], [0.0, 1.0/sqrt(2.0), 0.0, -1.0/sqrt(2.0), 0.0], [0.0, 1.0/sqrt(2.0), 0.0, 1.0/sqrt(2.0), 0.0]]) # Spin blocks to be read: n_spin_blocs = SP + 1 - SO # number of spins to read for Norbs and Ham, NOT Projectors # define the number of n_orbitals for all k points: it is the number of total bands and independent of k! n_orb = sum([ shells[ish][3] for ish in range(n_shells) ]) n_orbitals = numpy.ones([n_k,n_spin_blocs],numpy.int) * n_orb # Initialise the projectors: proj_mat = numpy.zeros([n_k,n_spin_blocs,n_corr_shells,max(numpy.array(corr_shells)[:,3]),max(n_orbitals)],numpy.complex_) # Read the projectors from the file: for ik in xrange(n_k): for icrsh in range(n_corr_shells): for isp in range(n_spin_blocs): # calculate the offset: offset = 0 no = 0 for i in range(n_shells): if (no==0): if ((shells[i][0]==corr_shells[icrsh][0]) and (shells[i][1]==corr_shells[icrsh][1])): no = corr_shells[icrsh][3] else: offset += shells[i][3] proj_mat[ik,isp,icrsh,0:no,offset:offset+no] = numpy.identity(no) # now define the arrays for weights and hopping ... bz_weights = numpy.ones([n_k],numpy.float_)/ float(n_k) # w(k_index), default normalisation hopping = numpy.zeros([n_k,n_spin_blocs,max(n_orbitals),max(n_orbitals)],numpy.complex_) if (weights_in_file): # weights in the file for ik in xrange(n_k) : bz_weights[ik] = R.next() # if the sum over spins is in the weights, take it out again!! sm = sum(bz_weights) bz_weights[:] /= sm # Grab the H for isp in range(n_spin_blocs): for ik in xrange(n_k) : no = n_orbitals[ik,isp] if (first_real_part_matrix): # first read all real components for given k, then read imaginary parts for i in xrange(no): if (only_upper_triangle): istart = i else: istart = 0 for j in xrange(istart,no): hopping[ik,isp,i,j] = R.next() for i in xrange(no): if (only_upper_triangle): istart = i else: istart = 0 for j in xrange(istart,no): hopping[ik,isp,i,j] += R.next() * 1j if ((only_upper_triangle)and(i!=j)): hopping[ik,isp,j,i] = hopping[ik,isp,i,j].conjugate() else: # read (real,im) tuple for i in xrange(no): if (only_upper_triangle): istart = i else: istart = 0 for j in xrange(istart,no): hopping[ik,isp,i,j] = R.next() hopping[ik,isp,i,j] += R.next() * 1j if ((only_upper_triangle)and(i!=j)): hopping[ik,isp,j,i] = hopping[ik,isp,i,j].conjugate() # keep some things that we need for reading parproj: things_to_set = ['n_shells','shells','n_corr_shells','corr_shells','n_spin_blocs','n_orbitals','n_k','SO','SP','energy_unit'] for it in things_to_set: setattr(self,it,locals()[it]) except StopIteration : # a more explicit error if the file is corrupted. raise "HK Converter : reading file dft_file failed!" R.close() # Save to the HDF5: ar = HDFArchive(self.hdf_file,'a') if not (self.dft_subgrp in ar): ar.create_group(self.dft_subgrp) things_to_save = ['energy_unit','n_k','k_dep_projection','SP','SO','charge_below','density_required', 'symm_op','n_shells','shells','n_corr_shells','corr_shells','use_rotations','rot_mat', 'rot_mat_time_inv','n_reps','dim_reps','T','n_orbitals','proj_mat','bz_weights','hopping', 'n_inequiv_shells', 'corr_to_inequiv', 'inequiv_to_corr'] for it in things_to_save: ar[self.dft_subgrp][it] = locals()[it] del ar