Converting Between K-Space Sum and Integral for Macroscopic Solids"

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SUMMARY

The discussion focuses on converting between k-space sums and integrals in the context of macroscopic solids under periodic boundary conditions. It establishes that the k-space states fill a volume of (2π/L)³, leading to a density of V/(2π)³. To count the number of states with wavevector k < k0, one can intuitively multiply the volume of a cube with radius k0, which translates mathematically to the equation ∑_k = (V/(2π)³) ∫d³k. Additionally, for slowly varying test functions, delta functions can be replaced by their density, reinforcing the relationship between sums and integrals.

PREREQUISITES
  • Understanding of k-space and wavevector concepts
  • Familiarity with periodic boundary conditions in solid-state physics
  • Knowledge of integral calculus and delta functions
  • Basic principles of statistical mechanics
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  • Study the application of periodic boundary conditions in solid-state physics
  • Learn about the mathematical properties of delta functions in integrals
  • Explore the implications of k-space density in quantum mechanics
  • Investigate the role of slowly varying test functions in physics
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Physicists, materials scientists, and students studying solid-state physics who are interested in the mathematical frameworks of k-space and its applications in macroscopic systems.

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How is it exactly i convert between a k-space sum an integral?
Assume that we have some macroscopic solid. Periodic boundary conditions leads to kx,ky,kz = 2π/L, so each k-space state fills a volume (2π/L)3 or has a density of V/(2π)3. To then count for instance the number of state with wavevector k<k0, what do you then do?
Intuitively I would multiply the volume of a cube of radius k0, but how does this translate into an integral exactly?
 
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##∑_k=\frac{V}{(2\pi)^3}∫d^3k##
 
You can also write the sum as an integral over a sum of delta functions.
For slowly varying test functions, the delta functions may then be replaced by their density ##V/(2\pi)^3##.
 

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