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My book gives a treatment of this problem for crystal vibrations, but I don't really understand it. It says: There is one allowed value of K per volume (2\pi/L)3. But at the same time it has just shown that Kx,Ky,Kz can take values ±2\pi/L which would certainly lead to more combinations of Kx,Ky,Kz within the volume confined by (2\pi/L)3. What am I misunderstanding.
Also: applying periodic boundary conditions yields the condition that Kx,Ky,Kz=±n2\pi/L, while fixed ends yielded K=n\pi/L, but my book says the two approaches yield identical results. How is that??
Also: applying periodic boundary conditions yields the condition that Kx,Ky,Kz=±n2\pi/L, while fixed ends yielded K=n\pi/L, but my book says the two approaches yield identical results. How is that??