[gpaw-users] Inaccuracies in phonon dispersion calculation
Jens Jørgen Mortensen
jjmo at dtu.dk
Fri Nov 10 07:18:40 CET 2017
On 11/07/2017 03:20 AM, Holden Parks wrote:
> Hi Jens,
>
> Thank you for the reply. I've tried running the plane-wave
> calculations with your suggested cutoff but haven't seen an
> improvement. I've confirmed that inaccuracies in the forces are the
> cause of the problem in the dispersions, as I've run the same
> calculation with the Brennan potential (part of the ASAP calculator)
> and the problematic features aren't present (I've attached it here).
> Do you have any thoughts on how I should move forward?
I got a nice looking phonon dispersion with a 7x7x7 cell and these
parameters:
calc = GPAW(symmetry={'point_group': False},
mode='lcao',
basis='szp(dzp)',
convergence={'density': 1e-7},
xc='PBE',
occupations=FermiDirac(0.01))
the important thing being a more tight convergence (I think).
Jens Jørgen
>
> -Holden
>
> On Fri, Nov 3, 2017 at 2:37 AM, Jens Jørgen Mortensen <jjmo at dtu.dk
> <mailto:jjmo at dtu.dk>> wrote:
>
> On 10/31/2017 11:19 PM, Holden Parks via gpaw-users wrote:
>
> Dear GPAW users,
>
> I am having a problem calculating the phonon dispersion for
> bulk diamond silicon. This calculation is performed in ase,
> and I at first suspected that something was wrong with the
> implementation. However, the example with aluminum using EMT
> on the ase manual works perfectly, so I believe my problem is
> that I am incorrectly calculating the force constants with my
> calculator.
>
> I've been calculating phonon dispersion curves for silicon
> with a variety of supercell and k-point sizes, grid spacing
> values, and displacement (delta) values. I've also tried a
> using GGA xc functionals rather than LDA, and turned
> point-group symmetry off. However, there are nonzero (and
> imaginary frequencies) at the gamma point, and the acoustic
> dispersion curves don't degenerate where they're expected
> (between the gamma and W points and between the L and gamma
> points). I've attached an example dispersion plot and the code
> I used to generate it.
>
> Any suggestions at this point would be extremely helpful.
> Thank you!
>
>
> Try running your calculation in plane-wave mode. Instead of
> h=0.16, use something like:
>
> calc = GPAW(..., mode=PW(300), ...)
>
> and remember to do "from gpaw import PW". This should give you
> better forces.
>
> Jens Jørgen
>
> -Holden
>
> ---------------------
>
> from ase.build import bulk
> from ase.dft.kpoints import ibz_points, bandpath
> from ase.phonons import Phonons
> from gpaw import GPAW, FermiDirac
> import numpy as np
>
> # Setup crystal and EMT calculator
> atoms = bulk('Si', 'diamond', a=5.477)
> calc = GPAW(kpts=(2, 2, 2),
> symmetry={'point_group': False},
> h=0.16,
> xc='PBE',
> occupations=FermiDirac(0.01))
>
> ph = Phonons(atoms, calc, supercell=(4, 4, 4), delta=0.05)
> ph.run()
>
> # Read forces and assemble the dynamical matrix
> ph.read(acoustic=True)
>
> High-symmetry points in the Brillouin zone
> G = [0, 0, 0]
> X = [0.5, 0, 0.5]
> W = [0.5,0.25,0.75]
> L = [0.5, 0.5, 0.5]
>
> point_names = ['$\Gamma$', 'X', 'W', 'L', '$\Gamma$']
> path = [G, X, W, L, G]
>
> # Band structure in meV
> freq_conv = 2.41798902*(10**14)
> path_kc, q, Q = bandpath(path, atoms.cell, 100)
> omega_kn = freq_conv*ph.band_structure(path_kc)/(10**12)
>
>
> import matplotlib.pyplot as plt
> plt.figure(1, (8, 6))
> plt.axes([.1, .07, .67, .85])
>
> for n in range(len(omega_kn[0])):
> omega_n = omega_kn[:, n]
> plt.plot(q, omega_n, 'k-', lw=2)
>
> plt.xticks(Q, point_names, fontsize=18)
> plt.yticks(fontsize=18)
> plt.xlim(q[0], q[-1])
> plt.ylabel("Frequency ($\mathrm{THz}$)", fontsize=22)
> plt.grid('on')
>
> plt.show()
>
>
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