Dear EPW-team,
first of all congratulations to the refurbished, extended version of EPW. I was using EPW2.3
for quite some time as a benchmark for my own clutter of el-ph code, but the new version is
really a pleasure.
My question:
In the example for doped Diamond http://epw.org.uk/Documentation/B-dopedDiamond
in Fig. 3f) the phonon linewidths for the highest phonon mode is shown - randomized 50^3
Sobol k-points and a smearing of 100meV was used. I note \gamma:max~7meV around
the \Gamma point.
In the next Fig. 4, the same calculation is done with an homogeneous/unshifted 50^3 grid.
Here I note \gamma:max~11meV around the \Gamma point.
While I know that convergence with random meshes is much faster and a 50^3 homogenous
grid is far from convergence, I wonder why the discrepancy between both "integration method"
in the absolute value of the selfenergy is so large.
Is there a certain criterion (or empirical knowledge) on the convergence dependency
of Brillouin-zone integrations with randomized/homogenous meshes?
thanks for your effort!
Nicki
CAMd, DTU Lyngby
homogeneous vs. randomized k/q-mesh in BZ integration
Moderator: stiwari
Re: homogeneous vs. randomized k/q-mesh in BZ integration
Dear Nicki,
Thank you for your interest in EPW.
There are many things that can affect this.
1) Figure 3 from the tutorial was done with an old version of EPW (v~2).
2) The height and smoothness of the phonon self energy depends on
- the k-point grid on which it is integrated
- the smearing for the i\delta in the denominator (here 0.1 eV)
- the temperature at which the calculation is done (this affects the Fermi-Dirac and Bose-Einstein distribution functions)
3) The most likely reasons is the following: there are three ways of computing the im. part of Eq. (4) of the new EPW paper:
- taking the imaginary part directly
- computing it with \delta (you can show that this is analytically the same, however it will be numerically slightly different)
- you can use the "delta delta" approximation.
In any case, the reference for the new version of EPW is Fig. 5 of the new EPW paper. Note that the calculations are done at 300K.
Hope it helps,
Samuel
Thank you for your interest in EPW.
There are many things that can affect this.
1) Figure 3 from the tutorial was done with an old version of EPW (v~2).
2) The height and smoothness of the phonon self energy depends on
- the k-point grid on which it is integrated
- the smearing for the i\delta in the denominator (here 0.1 eV)
- the temperature at which the calculation is done (this affects the Fermi-Dirac and Bose-Einstein distribution functions)
3) The most likely reasons is the following: there are three ways of computing the im. part of Eq. (4) of the new EPW paper:
- taking the imaginary part directly
- computing it with \delta (you can show that this is analytically the same, however it will be numerically slightly different)
- you can use the "delta delta" approximation.
In any case, the reference for the new version of EPW is Fig. 5 of the new EPW paper. Note that the calculations are done at 300K.
Hope it helps,
Samuel
Prof. Samuel Poncé
Chercheur qualifié F.R.S.-FNRS / Professeur UCLouvain
Institute of Condensed Matter and Nanosciences
UCLouvain, Belgium
Web: https://www.samuelponce.com
Chercheur qualifié F.R.S.-FNRS / Professeur UCLouvain
Institute of Condensed Matter and Nanosciences
UCLouvain, Belgium
Web: https://www.samuelponce.com