Calculating Energy Levels for Lattice Using Analytic Continuation?

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Discussion Overview

The discussion revolves around the calculation of energy levels for a lattice using band structure analysis, particularly focusing on the evaluation of the Bloch wave vector along the edges of the irreducible Brillouin zone. Participants explore the implications of calculating energy levels at boundary points versus arbitrary points within the zone, and the concept of analytic continuation in reconstructing band structures.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question why energy level calculations are typically performed only along the edges of the irreducible zone, such as the \Gamma - X - M path, rather than for arbitrary vectors within the zone.
  • Others suggest that the focus on boundary points is due to their significance in determining fundamental properties of materials, such as whether they are metals, semiconductors, or insulators, based on band gaps and the nature of the gaps (direct or indirect).
  • A participant mentions that it is possible to reconstruct the band structure from band eigenvalues at the \Gamma point, referencing a theorem related to k.p theory.
  • There is a discussion about the technique of analytic continuation, which requires a sufficient number of wave functions at the zone center to provide a decent approximation.

Areas of Agreement / Disagreement

Participants express differing views on the importance of calculating energy levels at boundary points versus within the zone. While some emphasize the significance of boundary calculations for understanding material properties, others raise questions about the limitations of this approach and the potential for exploring values within the zone.

Contextual Notes

There are unresolved questions regarding the accuracy and implications of using density-functional theory for band structure calculations, as well as the conditions under which analytic continuation can be effectively applied.

trogvar
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When energy levels for a lattice are constructed the Bloch wave vector is evaluated along the edges of the irruducible zone. Like \Gamma - X - M path for a square lattice.

I wonder why the calculation is NOT performed for values within the zone? And how the energy corresponding to an arbitrary vector within the zone but not laying at the boundary can be obtained from a band-gap diagrams (plotted for example in \Gamma - X - M coordinates)

Thanks in advance
 
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You're quite free to plot the band structure along any path you like. Much of the time we're only concerned about the behavior at the min and max of the bands, which only requires plotting in a few directions. You might want to know the band gaps, effective masses, and anisotropies near theses extrema. If, for some reason, you're especially concerned about what's happening off the band path, you'll just have to do a calculation of that system yourself (or call authors). Incidentally, there is a theorem that says it's possible to reconstruct the band structure from the band eigenvalues only at the gamma point. From k.p theory I think. You can look it up.
 
Thank you!

That's quite interesting that we can reconstruct the band structure from only information at \Gamma

Still people plot the diagrams in the particular paths along irreducible zones. You say

sam_bell said:
Much of the time we're only concerned about the behavior at the min and max of the bands, which only requires plotting in a few directions.

Why these are more important?

Thanks again
 
trogvar said:
Why these are more important?

These give you the most elementary information about the material such as whether it is a metal, semiconductor or insulator (determined by band gap, which is the energy difference between the maximum of the valence band and the minimum of the conduction band) and whether it has a direct or indirect gap (determined by whether the minimum and maximum occur at the same k-point). This is what the band structure is mainly used for. If calculated using the density-functional theory (usually the case) it would be risky trying to determine more subtle effects from the band structure due to the inaccuracies of the method.
 
trogvar said:
When energy levels for a lattice are constructed the Bloch wave vector is evaluated along the edges of the irruducible zone. Like \Gamma - X - M path for a square lattice.

I wonder why the calculation is NOT performed for values within the zone?
The \Gamma-point is at the zone center, and the \Gamma-X line, for instance, does span a region of reciprocal space "within the zone".
 
trogvar said:
That's quite interesting that we can reconstruct the band structure from only information at \Gamma

The technique is called analytic continuation, and it only works if you have a large number of wave functions at the center of zone. You get a decent approximation if you have 16 or more wave functions and all the coupling constants between them.
 

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