Kittel Chapter 7: Empty Lattice Approximation

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The "Empty Lattice Approximation" in Kittel's solid-state physics refers to treating an empty lattice as a periodic potential, allowing for the analysis of band structures in a simplified manner. This approximation is necessary to understand how free particle energy spectra can resemble band structures by shifting them along reciprocal lattice vectors. The key distinction between this approximation and the free electron gas model is that the former assumes a lattice exists, leading to band filling, while the latter does not involve a lattice and fills a Fermi sphere instead. Additionally, the empty lattice approximation lacks energy gaps, which raises questions about its representation of actual band structures. Overall, this discussion highlights the conceptual differences between these models in solid-state physics.
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[SOLVED] kittel chapter 7

Homework Statement


This question refers to Kittel's solid-state physics book. I have edition 8.

In this chapter, there is a section called the "Empty Lattice Approximation". Can someone explain what the title of that chapter means i.e. in what sense is that lattice empty, where is that used, why is that approximation necessary?


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The Attempt at a Solution

 
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I don't have Kittel in front of me, but I think he just means to treat empty space as a periodic potential (which it is...) with whatever period you want (say, 'a'). One can break up the free particle energy spectrum and shift it along reciprocal "lattice" vectors ((2 Pi)/a, or whatever) and get something that looks like a band structure for the free particle.
 
What is the difference between the empty lattice approximation and the free electron fermi gas?
 
anyone?
 
Help!
 
ehrenfest said:
What is the difference between the empty lattice approximation and the free electron fermi gas?

in the empty lattice approximation you pretend there is still a lattice so you get bands--bands determined by shifting the free electron dispersion through a reciprocal lattice vector--and you fill up the bands till you get the number of electrons you want.

in the free electron gas there is no lattice and you just fill up the fermi sphere till you get the number of electrons you want.
 
olgranpappy said:
in the empty lattice approximation you pretend there is still a lattice so you get bands--bands determined by shifting the free electron dispersion through a reciprocal lattice vector--and you fill up the bands till you get the number of electrons you want.

in the free electron gas there is no lattice and you just fill up the fermi sphere till you get the number of electrons you want.

So the empty lattice approximation IS the reduced zone scheme, correct? I guess, I just don't see at all how that represents the band structure because then the dispersion relation is continuous at the BZ boundary in the empty lattice approximation That is, it just bounces back and forth between the boundaries. I thought that the point of an energy band was that it the dispersion relation WAS NOT CONTINUOUS. What I am saying is that there are no energy gaps in the empty lattice approximation and isn't that what we are interested in?
 
Last edited:
I don't know what *we* are interested in. But, yes, in the empty lattice there are no gaps.
 

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