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NEGF-mulp.py
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NEGF-mulp.py
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#!/usr/bin/env python
#
# NEGF-mulp.py is a sclipt to obtain the phonon transmission function
# for each k-point by using the hessian file in ALAMODE.
#
#
# Copyright (c) 2018 Yuto Tanaka
#
"""
--- How to use ---
$ python NEGF-mulp.py --negf=(prefix)_negf.in --hessian=(prefix).hessian (--nt=1)
You can skip the --nt option, which is specify the number of thread.
The default value is the thread limit on you environment.
"""
import argparse
import time
import multiprocessing as mp
from multiprocessing import Pool
import numpy as np
import numpy.linalg as LA
import mod_dymat as dymat
usage = "usage: %prog [options]"
parser = argparse.ArgumentParser(usage=usage)
parser.add_argument("--negf", help="negf file")
parser.add_argument("--hessian", help="hessian file")
parser.add_argument("--nt", help="hessian file",
type=int, default=mp.cpu_count())
cm = 3634.87331806918 # convert to cm^{-1}
def surface_green(nat, OMG_s, D_s):
N_atom = 3 * nat
ep_s = OMG_s - (D_s[:N_atom, :N_atom])
ep = OMG_s - (D_s[:N_atom, :N_atom])
alpha = (D_s[:N_atom, N_atom:])
beta = (D_s[N_atom:, :N_atom])
G_0 = LA.inv(ep_s)
norm_G = 1.0
while norm_G > criterion:
ep_inv = LA.inv(ep)
a = np.dot(ep_inv, alpha)
b = np.dot(ep_inv, beta)
ep_s -= np.dot(alpha, b)
ep -= np.dot(beta, a) + np.dot(alpha, b)
alpha = np.dot(alpha, a)
beta = np.dot(beta, b)
G = LA.inv(ep_s)
norm_G = LA.norm(G - G_0)
G_0 = G
return G
def transmission(i, nat):
omega = i * grid
omega2 = (omega)**2 + 1e-10
OMG = omega2 * (1 + delta*1j)
# Frequency
OMG_c = OMG * np.identity(9 * nat, dtype=np.complex128)
OMG_s = OMG * np.identity(3 * nat, dtype=np.complex128)
# coupling term in dynamical matrix
D_lc = np.conjugate(D_cl.T)
D_rc = np.conjugate(D_cr.T)
# Surface Green's function
G_l = surface_green(nat, OMG_s, D_s[::-1, ::-1])[::-1, ::-1]
G_r = surface_green(nat, OMG_s, D_s)
# Self energy
Self_l = np.dot(D_cl, np.dot(G_l, D_lc))
Self_r = np.dot(D_cr, np.dot(G_r, D_rc))
# Green's function in the scattering ragion
G_c = LA.inv(OMG_c - D_c - (Self_l + Self_r))
G_c_her = np.conjugate(G_c.T)
# Gamma (spectral density)
Gamma_l = (Self_l - np.conjugate(Self_l.T)) * 1j
Gamma_r = (Self_r - np.conjugate(Self_r.T)) * 1j
return omega * cm, np.trace(np.dot(Gamma_l, np.dot(G_c, np.dot(Gamma_r, G_c_her)))).real
def generate_qmesh(kpoint, tran_direct):
num_q = kpoint[0] * kpoint[1] * kpoint[2]
q = np.zeros([num_q, 3])
var_idx = [i for i, x in enumerate(tran_direct) if x == 0]
fix_idx = [i for i, x in enumerate(tran_direct) if x == 1][0]
bz = [[], [], []]
bz[fix_idx].append(0.0)
for i in var_idx:
dq = 1 / (kpoint[i] + 1)
qx = -0.5 + dq
xx = 0.5 - dq * 0.01
while qx < xx:
bz[i].append(qx)
qx += dq
q_count = 0
for i in range(kpoint[0]):
for j in range(kpoint[1]):
for k in range(kpoint[2]):
q[q_count] = np.array([bz[0][i], bz[1][j], bz[2][k]])
q_count += 1
return q, var_idx
def get_qpoint(qmesh, revec):
return qmesh[0] * revec[0] + qmesh[1] * revec[1] + qmesh[2] * revec[2]
def wrapper_transmission(args):
return transmission(*args)
def main():
# grobalization
global delta, criterion, grid
global D_c, D_s, D_cl, D_cr
start = time.time()
options = parser.parse_args()
if options.negf:
negf_file = options.negf
else:
print("negf file is not selected.")
if options.hessian:
hessian_file = options.hessian
else:
print("hessian file is not selected.")
if options.nt:
num_thread = options.nt
print("The number of thread : " + str(num_thread))
if num_thread > mp.cpu_count():
print("The number of thread specified by you is larger \
than the thread limit on your environment.")
exit(1)
prefix = negf_file.split('.')[0]
# read negf file
x_bohr, k_atom, nat, mass, lavec, univec, revec, tran_direct, kpoint, \
cutoff, delta, freq_max, criterion, step = dymat.read_negf(negf_file)
# supercell infomation
lmn = dymat.supercell(lavec, univec)
# shift parameter
dymat.make_shift_list(lmn)
# atoms in unitcell atom_uc = [1, ..., nat_unitcell]
atom_uc = dymat.atom_in_unitcell(x_bohr, univec, nat)
nat_uc = len(atom_uc) # number of atoms in unit cell
# considerable atom pairs for fcs
pairs = dymat.generate_pairs(atom_uc, x_bohr, lavec, univec, nat, cutoff)
# mapping equivalant atom in unit cell
map_uc = dymat.mapping(x_bohr, univec, atom_uc, nat, lmn)
# atomic mass in uni tcell
mass_uc = dymat.mass_in_unitcell(mass, k_atom, atom_uc)
# store fcs matrix
fcs = dymat.store_all_fcs(hessian_file, atom_uc,
nat_uc, pairs, map_uc, mass_uc)
# obtain k-point in 1st BZ and transport direction index
qmesh, var_idx = generate_qmesh(kpoint, tran_direct)
q_count = 0
freq_max /= cm
grid = float(freq_max) / step
wrap = [[s, nat_uc] for s in range(step)]
for i in range(kpoint[var_idx[0]]):
for j in range(kpoint[var_idx[1]]):
outfile = prefix + ".tran" + str(i) + "_" + str(j)
print(outfile)
tran_data = np.zeros([step, 2])
q = get_qpoint(qmesh[q_count], revec)
q_count += 1
# Dynamical matrix
D_c, D_s, D_cl, D_cr = dymat.generate_dynamical_matrix(
fcs, q, nat_uc, univec, tran_direct)
p = Pool(num_thread)
Tran = p.map(wrapper_transmission, wrap)
p.close()
tran_data = np.array(Tran)
np.savetxt(outfile, tran_data, delimiter=' ')
print(time.time() - start, "seconds")
if __name__ == "__main__":
main()