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I was trying to compute some electronic properties for Pd using SIESTA and VASP for some computer practicals in my university, specially focused on band structure and density of states (DOS) using LDA and GGA functionals. First of all, we run convergence tests: k-point grid and energy cut-off. After that, the relaxation of the cell and the band structure and DOS were calculated. One of my professors said that it was necessary to increase the number of k-points to run the DOS calculation.

Is there a reason for that? I have been reading on the internet but it seems to be a trick to obtain more accurate results.

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  • $\begingroup$ Why you don't ask to your professors? Normally, even after doing the convergence studies, I do the calculations with mesh-cut-off and k-point greater than the "converged" values. This is to guarantee better results. $\endgroup$
    – Camps
    May 25 at 12:32
  • $\begingroup$ In your question title you have mentioned band structure calculation. In the body, its mentioned DOS calculation. $\endgroup$
    – Thomas
    May 25 at 12:55
  • $\begingroup$ +1. Welcome to our new community and thank you so much for contributing your question here! We hope to see much more of you in the future !!! $\endgroup$ May 25 at 15:30
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This depends a lot on how the DOS is calculated. I don't know the options one has for this when using VASP or SIESTA, but I am aware of different approaches. The central problem is that you don't know which state at a certain k point is "connected" to some other state at another k point. When calculating a DOS you have to integrate over the Brillouin zone and therefore you have to somehow interpolate between the actually calculated k points. The eigenenergies of the states at the different k points may differ by more than what you might find reasonable for the energy-resolution of your DOS.

Two approaches:

  1. You could say that each state contributes to the "energy bin" it is directly related to and smoothen the DOS afterwards to get rid of the artifacts due to this finite sampling. In this case you somehow have to define a parameter controlling the smoothening and this has to be related to the fineness of the sampling in the Brillouin zone. Unfortunately the relationship between the k-point sampling and the smoothing is also not direct: The band dispersion may be very different for different bands and for different materials.

  2. You could assume a certain correspondence between the states at different k points and interpolate between the states in k space. This is the tetrahedron method. Unfortunately a naive approach may assume a wrong correspondence. For example if you just say that the i-th eigenvalue at some k point corresponds to the i-th eigenvalue at another k point, you ignore the possibility of band crossings. Your interpolation scheme would imply avoided crossings. To make this issue less severe you would also smoothen the DOS on the energy grid. And, of course, a finer k-point sampling would also reduce the significance of this issue.

In the end creating a nice DOS is a matter of different ingredients:

  1. The Brillouin zone integration scheme.
  2. The k-point sampling of the Brillouin zone.
  3. The fineness of the energy grid.
  4. The smoothing of the DOS.
  5. The dispersion of the bands.

A finer k-point sampling allows the generation of a higher-quality DOS. But you also have to control the other parameters.

I also described this landscape of different parameters in the documentation of the Fleur code. You can find there a few example plots demonstrating the effect of changing certain aspects of the DOS generation. Of course, the parametrization may be slightly different for other codes, but the general problem should be similar.

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  • $\begingroup$ +1. A great and detailed answer as always from Gregor! I've made a minor edit to improve the formatting of the hyperlink (no need to see a long URL, haha). $\endgroup$ May 25 at 15:32
  • $\begingroup$ Thank you Gregor for your detailed answer $\endgroup$
    – Paul Logan
    May 27 at 10:55

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