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Commit 4430d576 authored by Lars kleyn Winkel's avatar Lars kleyn Winkel
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Update 8_many_atoms_solutions.md

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### Subquestion 3
Density of states is given as $g(\omega) = \frac{dN}{d\omega} = \frac{dN}{dk}\frac{dk}{d\omega}$. We know $\frac{dN}{dk} = 2\frac{L}{2\pi} = \frac{L}{\pi}$ since we have 1D and positive and negative k-values. $\frac{dk}{d\omega}$ can be computed using the group velocity: $$\frac{dk}{d\omega} = \bigg(\frac{d\omega}{dk} \bigg)^{-1} = (v_g)^{-1}$$
Density of states is given as $g(\omega) = \frac{dN}{d\omega} = \frac{dN}{dk}\frac{dk}{d\omega}$. We know $\frac{dN}{dk} = \frac{L}{2\pi}$ since we have 1D. $\frac{dk}{d\omega}$ can be computed using the group velocity: $$\frac{dk}{d\omega} = \bigg(\frac{d\omega}{dk} \bigg)^{-1} = (v_g)^{-1}$$
## Exercise 2: the Peierls transition
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