Density of states free electron gas

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Discussion Overview

The discussion centers on the density of states (DOS) for a free electron gas, exploring the implications of boundary conditions and the geometry of the material. Participants examine theoretical frameworks and historical references related to the topic.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Historical

Main Points Raised

  • One participant outlines the procedure for determining the density of states by applying periodic boundary conditions to a cube of side L, noting that this results in one state per volume of 2π/L³.
  • Another participant raises a question about the assumption of a cubic geometry, suggesting the need to consider alternative shapes, such as a ball of metal.
  • A participant references a theorem attributed to Sommerfeld, proposing that the boundary conditions become negligible in the limit as volume approaches infinity.
  • Another participant mentions a proof by W. Ledermann from 1944, indicating that it is discussed in a review paper from 1993.
  • One participant speculates that Ashcroft and Mermin may also mention the theorem related to boundary conditions and density of states.
  • There is a question about who originally proposed the theorem, with a participant indicating they will check the relevant literature.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the implications of boundary conditions on the density of states and the historical attribution of the theorem, indicating that multiple competing views remain without a clear consensus.

Contextual Notes

Participants note limitations related to the assumptions of geometry and boundary conditions, as well as the historical context of the theorem's development, which remains unresolved.

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For a free electron gas the procedure for determining the density of states is as follows.
Apply periodic boundary conditions to the free electron waves over a cube of side L. This gives us that there is one state per volume 2\pi/L3=2\pi/V
And from there we can find the number of states at a given energy E by multiplying by the volume of a sphere at E in k space.
One big problem with this is however: Why do we assume that material is necessarily a cube? What if we worked with a ball of metal?
 
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There is a theorem, I think by Sommerfeld, that the boundary becomes unimportant in determining e.g. the DOS in the limit V->infinity
 
I thought that the proof is in an article by a guy named W. Ledermann, published in 1944.

http://rspa.royalsocietypublishing.org/content/182/991/362.full.pdf

I actualy found it mentioned in a review paper from 1993:
http://www.jstor.org/discover/10.2307/52288?uid=3739728&uid=2&uid=4&uid=3739256&sid=21102824926163

Do you know something about Sommerfeld writing something along the same lines?
 
I think Ashcroft Mermin may mention the theorem.
 
I am pretty sure they do. But who is the first to come with it?
I'll check the book.
 

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