Why Is the Density of States the Same in Both Real and Reciprocal Space?

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SUMMARY

The density of states in both real space and reciprocal space is defined by the formula 1 / (4∏³). This equivalence arises from periodic boundary conditions in a cubic box of size L, leading to the relationship kx=nx*2pi/L. The volume occupied by a state in k-space is (2pi/L)³, resulting in the same density of states when considering the factor of 2 for electron spin. This conclusion is supported by the principles outlined in Ashcroft and Mermin's work.

PREREQUISITES
  • Understanding of periodic boundary conditions in quantum mechanics
  • Familiarity with k-space and its implications in solid-state physics
  • Knowledge of the density of states concept
  • Basic grasp of electron spin and its effects on state occupancy
NEXT STEPS
  • Explore the derivation of density of states in different dimensional systems
  • Study the implications of periodic boundary conditions in quantum mechanics
  • Learn about the reciprocal lattice and its applications in solid-state physics
  • Investigate the formula g(E)dE = 2g(k)dk/∇_k E(k) for further insights into density of states
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Physicists, materials scientists, and students studying solid-state physics who seek to understand the relationship between real and reciprocal space in the context of electron states and density of states.

Dr_Pill
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In my text:

The number of states per unit volume of the real space & the reciprocal space is given by


1 / (4∏³)

No further explanation is given.

How do you get to this 4∏³

And how come the density of states is the same in real space & reciprocal space?

I think this is incorrect, they should be the reversed version of each other.

Thx in advance
 
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Consider a cubic box of size L. Then periodic boundary conditions imply that kx=nx*2pi/L where nx=0,1,2,3,... The same follows for ky and kz.
Now you can see that in k-space a state with a given k occupies a k-space volume of (2pi/L)^3. Then the number of states per unit volume is (1/V) L^3 * 2 /(2pi)^3 and you get that result. The factor of 2 comes from the fact that the electron has 2 distinct values for the z component of the spin. Note that if you consider a rectangular box you would obtain an identical conclusion.
 
I have attached a figure from Ashcroft and Mermin.

Do this. In the case of 2D, take the reciprocal lattice and you draw a circle or radius k from the center.

How many electrons states you would have in that area encircled in k-space? If you can figure this out, you can easily find the answer you are looking for. Also, in the case of electrons, there are 2 electrons allowed for each state (spin).

If all else fails, you can use this formula. g(E)dE = 2g(k)dk/\nabla_k E(k)
 

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