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Wavefunctions for Traveling Electrons

One can easily see that this solution satisfies the boundary conditions [Pg.356]

Putting this back into the Schrodinger wave equation, [Pg.356]

Recall in the previous treatment where we allowed only standing waves, we found energy eigenvalues given by [Pg.356]

Clearly, emplo)fing periodic boundary conditions produces a different set of energy levels however, it will also produce a different density of states. Since E = h k = (2ti/L) h. [Pg.356]

Thus the voliune associated with each energy state in fc-space is 2tt/L). The minimum energy configuration is a Fermi sphere with radius fcmax- The volume of this sphere in fc-space is (4n/3)fc ax- Th number of electrons that can be accommodated is [Pg.356]


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