Density of states free electron gas

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SUMMARY

The density of states for a free electron gas is determined by applying periodic boundary conditions to free electron waves within a cubic volume of side L, resulting in one state per volume of 2π/L³ or 2π/V. The number of states at a specific energy E can be calculated by considering the volume of a sphere in k-space. A significant consideration is the assumption of a cubic geometry; however, as noted by Sommerfeld, the boundary conditions become negligible as the volume approaches infinity. This theorem is further discussed in W. Ledermann's 1944 paper.

PREREQUISITES
  • Understanding of periodic boundary conditions in quantum mechanics
  • Familiarity with the concept of density of states (DOS)
  • Knowledge of k-space and its significance in solid-state physics
  • Awareness of historical contributions to quantum theory, particularly by Sommerfeld and Ledermann
NEXT STEPS
  • Research the implications of periodic boundary conditions on density of states calculations
  • Study the theorem by Sommerfeld regarding boundary conditions in infinite volumes
  • Examine W. Ledermann's 1944 article on the density of states
  • Review Ashcroft and Mermin's textbook for insights on density of states and related theorems
USEFUL FOR

Physicists, materials scientists, and students studying solid-state physics who are interested in the theoretical foundations of electron behavior in materials.

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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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