Fermi Surface squashed by potentials

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SUMMARY

The discussion centers on the behavior of the Fermi surface in relation to potentials, specifically using the potential function V(x,y) = A cos(x) cos(y). It is established that a half-filled Brillouin zone leads to a Fermi surface that is affected by energy shifts near the zone boundaries. As the energy bands lower due to perturbations, the Fermi surface shifts to higher k values, indicating a change in the surface's geometry in reciprocal space. This behavior is crucial for understanding the effects of strong potentials on the Fermi surface, which may even extend into the second Brillouin zone.

PREREQUISITES
  • Understanding of Brillouin zones and Fermi surfaces
  • Familiarity with the Nearly Free Electron Model
  • Knowledge of perturbation theory in solid-state physics
  • Basic concepts of reciprocal space and potential functions
NEXT STEPS
  • Study the implications of perturbation theory on band structure in solid-state physics
  • Explore the characteristics of the Nearly Free Electron Model in greater detail
  • Investigate the effects of periodic potentials on electronic properties
  • Learn about the mathematical treatment of Fermi surfaces in reciprocal space
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Physicists, materials scientists, and students studying solid-state physics, particularly those interested in electronic band structure and the effects of potentials on Fermi surfaces.

unscientific
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Taken from my textbook:

fermisea1.png


My understanding is that:

  • One valence electron, 2 spin states -> Half-filled Brillouin zone
  • Seeking inspiration from "Nearly Free Electron Model": gaps open up at zone boundaries
  • States nearer to zone boundaries get pushed down in energy further

Since a fermi surface is a surface of constant energy in k-space, shouldn't the surfaces nearer to the zone boundaries that get pushed down in energies get repelled even more? It seems that surfaces nearer to the boundaries get closer even! Why are the fermi seas like these below?

fermisea2.png
 
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Take a simple potential with this symmetry as an example: ##V(x,y)=A \cos(x)\cos(y)##. Can you find a direction along which the potential is constant? To which lines do these directions in reciprocal space? What happens at the cell boundary?
 
DrDu said:
Take a simple potential with this symmetry as an example: ##V(x,y)=A \cos(x)\cos(y)##. Can you find a direction along which the potential is constant? To which lines do these directions in reciprocal space? What happens at the cell boundary?
cosxcosy.png


The surfaces of constant potential are the circles* about (0,0). Given this is the fermi surface, these surfaces are the reciprocal space. Still doesn't answer my question about "pushed down in energy -> decrease in radius, squashed inwards"?
 
bumpp
 
Sorry, I was on the wrong track and had no time to think about your problem recently. Now I think I understand the behaviour. Near the BZ boundary, the lower energy band will be lowered as compared to the free electron case, so the Fermi surface will be shifted to higher k values. At stronger potentials, it will even protrude into the second BZ or even farther.
 
DrDu said:
Sorry, I was on the wrong track and had no time to think about your problem recently. Now I think I understand the behaviour. Near the BZ boundary, the lower energy band will be lowered as compared to the free electron case, so the Fermi surface will be shifted to higher k values. At stronger potentials, it will even protrude into the second BZ or even farther.

I get the downward shift in energy due to a perturbation. Why will the fermi surface be shifted to higher k values?
 
The fermi surface is a surface of constant energy. If the levels split, this constant energy value will be reached at higher values of k. Think of an irregularly shaped plate: where the rim is lower, soup will ooze out more.
 

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