Source code for gpaw.nlopt.linear

import numpy as np
from ase.units import Ha


[docs] def get_chi_tensor( nlodata, freqs=[1.0], eta=0.05, ftol=1e-4, Etol=1e-6, eshift=0.0, band_n=None, out_name=None): """ Calculate full linear susceptibility tensor for nonmagnetic semiconductors; array will be saved to disk if out_name is given. Parameters ---------- nlodata Data object of type NLOData. freqs Excitation frequency array (a numpy array or list). eta Broadening, a number or an array (default 0.05 eV). Etol, ftol Tolerance in energy and occupancy to consider degeneracy. eshift Bandgap correction. band_n List of bands in the sum (default 0 to nb). out_name If it is given: output filename. Returns ------- np.ndarray: Full linear susceptibility tensor (3, 3, nw). """ comm = nlodata.comm # Covert inputs in eV to Ha freqs = np.array(freqs) nw = len(freqs) w_lc = (freqs + 1j * eta) / Ha Etol /= Ha eshift /= Ha # Load the required data k_info = nlodata.distribute() if k_info: tmp = list(k_info.values())[0] nb = len(tmp[1]) if band_n is None: band_n = list(range(nb)) # Initialize the outputs sum_vvl = np.zeros((3, 3, nw), complex) # Do the calculations for _, (we, f_n, E_n, p_vnn) in k_info.items(): tmp = np.zeros((3, 3, nw), complex) for v1 in range(3): for v2 in range(v1, 3): sum_l = calc_chi( w_lc, f_n, E_n, p_vnn, [v1, v2], band_n, ftol, Etol, eshift=eshift) tmp[v1, v2] = sum_l tmp[v2, v1] = sum_l # Add it to previous with a weight sum_vvl += tmp * we comm.sum(sum_vvl) # Multiply prefactors (4pi from eps0, 8pi^3 from BZ) prefactor = 4 * np.pi / (2 * np.pi)**3 chi_vvl = prefactor * sum_vvl # Save it to the file if comm.rank == 0 and out_name is not None: tmp = chi_vvl.reshape(9, nw) lin = np.vstack((freqs, tmp)) np.save(out_name, lin) return chi_vvl
def calc_chi( w_l, f_n, E_n, p_vnn, pol_v, band_n=None, ftol=1e-4, Etol=1e-6, eshift=0): """ Loop over bands for computing the response Input: w_l Complex frequency array f_n Fermi levels E_n Energies p_vnn Momentum matrix elements pol_v Tensor element band_n Band list Etol, ftol Tol. in energy and fermi to consider degeneracy eshift Bandgap correction Output: sum_l Output sum value (array with length of w_l) """ # Initialize variables nb = len(f_n) if band_n is None: band_n = list(range(nb)) sum_l = np.zeros(w_l.size, complex) # Loop over bands for nni in band_n: for mmi in band_n: # Use TRS to reduce if mmi <= nni: continue fnm = f_n[nni] - f_n[mmi] Emn = E_n[mmi] - E_n[nni] + fnm * eshift if np.abs(fnm) < ftol or np.abs(Emn) < Etol: continue # *2 for real, /2 for TRS, *2 for m<n sum_l += 2 * fnm * np.real( p_vnn[pol_v[0], nni, mmi] * p_vnn[pol_v[1], mmi, nni]) \ / (Emn * (Emn**2 - w_l**2)) return sum_l