Band structure of Ni: Difference between revisions
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==Input | ==Input file == | ||
* | *ni_lcao.py | ||
<pre> | <pre> | ||
from gpaw import GPAW, FermiDirac | from gpaw import GPAW, FermiDirac | ||
from ase import Atoms | from ase import Atoms | ||
Line 66: | Line 63: | ||
calc.get_potential_energy() | calc.get_potential_energy() | ||
ef = calc.get_fermi_level() | |||
calc.write('band_harris.gpw') | calc.write('band_harris.gpw') | ||
# Extract eigenenergies into a file for plotting with some external package | |||
import numpy as np | |||
calc = GPAW('band_harris', txt=None) | calc = GPAW('band_harris', txt=None) | ||
eps_skn = np.array([[calc.get_eigenvalues(k,s) | eps_skn = np.array([[calc.get_eigenvalues(k,s) | ||
for k in range(80)] | for k in range(80)] | ||
for s in range(2)]) - | for s in range(2)]) - ef | ||
f = open('bands.dat', 'w') | |||
for n in range(10): | for n in range(10): | ||
for k in range(80): | for k in range(80): | ||
print k, eps_skn[0, k, n], eps_skn[1, k, n] | print >>f, k, eps_skn[0, k, n], eps_skn[1, k, n] | ||
print | print >>f | ||
</pre> | </pre> | ||
==Run job | ==Run job in parallel== | ||
* Run band structure calculations in parallel using 8 cores on ulam: | |||
mpirun -np 8 gpaw-python_openmpi ni_lcao.py | |||
==Plot the results== | ==Plot the results== | ||
* | * Reproduce the figure below using [http://www.gnuplot.info/ gnuplot] or transfer data to your Windows PC via sftp and use Origin: | ||
<pre> | <pre> | ||
gnuplot> plot " | gnuplot> plot "bands.dat" using 1:2 with lines title "Spin up", "bands.dat" using 1:3 with lines title "Spin down" | ||
</pre> | </pre> |
Latest revision as of 12:30, 16 November 2014
Input file
- ni_lcao.py
from gpaw import GPAW, FermiDirac from ase import Atoms from ase.io import read, write from gpaw import GPAW, PoissonSolver, MixerSum from ase.structure import bulk # ------------------------------------------------------------- # Bulk configuration # ------------------------------------------------------------- a = 3.5249 atoms = bulk('Ni', 'fcc', a=a) atoms.center() write('system.traj', atoms) for a in atoms: if a.symbol == 'Ni': a.magmom = 0.6 # Make self-consistent calculation and save results calc = GPAW(h=0.18, mode='lcao', xc='PBE', basis='dzp', kpts=(8,8,8), occupations=FermiDirac(width=0.05, maxiter=2000), mixer=MixerSum(beta=0.010, nmaxold=8, weight=100.0), poissonsolver=PoissonSolver(eps=1e-12), txt='band_sc.txt') atoms.set_calculator(calc) atoms.get_potential_energy() calc.write('band_sc.gpw') # Calculate band structure along Gamma-X from ase.dft.kpoints import ibz_points, get_bandpath points = ibz_points['fcc'] G = points['Gamma'] X = points['X'] kpts, x, X = get_bandpath([G, X], atoms.cell, 80) calc = GPAW('band_sc.gpw', mode='lcao', xc='PBE', basis='dzp', kpts=kpts, txt='band_harris.txt', fixdensity=True, parallel={'domain': 1}, usesymm=None, convergence={'bands': 'all'}) if calc.input_parameters['mode'] == 'lcao': calc.scf.reset() calc.get_potential_energy() ef = calc.get_fermi_level() calc.write('band_harris.gpw') # Extract eigenenergies into a file for plotting with some external package import numpy as np calc = GPAW('band_harris', txt=None) eps_skn = np.array([[calc.get_eigenvalues(k,s) for k in range(80)] for s in range(2)]) - ef f = open('bands.dat', 'w') for n in range(10): for k in range(80): print >>f, k, eps_skn[0, k, n], eps_skn[1, k, n] print >>f
Run job in parallel
- Run band structure calculations in parallel using 8 cores on ulam:
mpirun -np 8 gpaw-python_openmpi ni_lcao.py
Plot the results
- Reproduce the figure below using gnuplot or transfer data to your Windows PC via sftp and use Origin:
gnuplot> plot "bands.dat" using 1:2 with lines title "Spin up", "bands.dat" using 1:3 with lines title "Spin down"