Calculating Energy Levels for Lattice Using Analytic Continuation?

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SUMMARY

The discussion centers on calculating energy levels for a lattice using analytic continuation, specifically evaluating the Bloch wave vector along the edges of the irreducible zone, such as the \Gamma - X - M path for a square lattice. Participants highlight the importance of focusing on the min and max of the bands, which provide critical information about the material's classification as a metal, semiconductor, or insulator, determined by the band gap. The conversation also touches on the ability to reconstruct the band structure from eigenvalues at the \Gamma point, emphasizing the necessity of having a sufficient number of wave functions for accurate analytic continuation.

PREREQUISITES
  • Understanding of Bloch wave vectors and their role in solid-state physics
  • Familiarity with band structure diagrams and band gaps
  • Knowledge of density-functional theory (DFT) and its limitations
  • Concept of analytic continuation in quantum mechanics
NEXT STEPS
  • Research the implications of band gaps in determining material properties
  • Learn about the k.p theory and its application in band structure reconstruction
  • Explore advanced techniques in density-functional theory for improved accuracy
  • Investigate methods for calculating wave functions in solid-state systems
USEFUL FOR

Physicists, materials scientists, and researchers involved in solid-state physics, particularly those focused on band structure analysis and energy level calculations in crystalline materials.

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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