Skip to content
Snippets Groups Projects
Commit 60f0df3d authored by Kevin Choi's avatar Kevin Choi
Browse files

Added hint for exercise 1.1

parent a6cb1a40
No related branches found
No related tags found
No related merge requests found
...@@ -228,6 +228,10 @@ $\rightarrow \rho_{\rm R}(k)=\frac{L}{2\pi}$, which is lower than for the case o ...@@ -228,6 +228,10 @@ $\rightarrow \rho_{\rm R}(k)=\frac{L}{2\pi}$, which is lower than for the case o
Recall the eigenfrequencies of a diatomic vibrating chain in the lecture notes with 2 different masses (can be found below [here](#more-degrees-of-freedom-per-unit-cell)). Recall the eigenfrequencies of a diatomic vibrating chain in the lecture notes with 2 different masses (can be found below [here](#more-degrees-of-freedom-per-unit-cell)).
1. Find the magnitude of the group velocity near $k=0$ for the _acoustic_ branch. 1. Find the magnitude of the group velocity near $k=0$ for the _acoustic_ branch.
??? hint
Make use of Taylor series.
2. Show that the group velocity at $k=0$ for the _optical_ branch is zero. 2. Show that the group velocity at $k=0$ for the _optical_ branch is zero.
3. Derive an expression for the density of states $g(\omega)$ for the _acoustic_ branch and small $ka$. Make use of your expression of the group velocity in 1. 3. Derive an expression for the density of states $g(\omega)$ for the _acoustic_ branch and small $ka$. Make use of your expression of the group velocity in 1.
......
0% Loading or .
You are about to add 0 people to the discussion. Proceed with caution.
Please register or to comment