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In three dimensions, again only discrete values of k are allowed. This time the volume of k-space per allowed state is
\[ \Delta k^{3}=\Delta k_{x}\Delta k_{y}\Delta k_{z}=\frac{2\pi}{L_{x}}\frac{2\pi}{L_{y}}\frac{2\pi}{L_{z}}=\frac{8\pi^{3}}{V} \nonumber \]
where V is the volume of the material.
In summary, the k-space occupied per state is
Table \(\PageIndex{1}\): The k-space occupied per state in 1, 2 and 3 dimensions.
| 1-d | \(\Delta k=\frac{2\pi}{L}\) |
| 2-d | \(\Delta k^{2}=\frac{4\pi^{2}}{A}\) |
| 3-d | \(\Delta k^{3}=\frac{8\pi^{3}}{V}\) |
This page titled 2.13: Periodic boundary conditions in 3-D was last modified on Sun, 22 May 2022 21:20:09 GMT and is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Marc Baldo (MIT OpenCourseWare) via source content that was edited to the style and standards of the LibreTexts platform.
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