Solution to Set 5: Difference between revisions
m (→Problem 1) |
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<math>\Rightarrow m \ddot{U}_n = - k [2U_n - U_{n-1} - U_{n+1}] \;</math> | <math>\Rightarrow m \ddot{U}_n = - k [2U_n - U_{n-1} - U_{n+1}] \;</math> | ||
Eigenvector Value | Eigenvector Value for modes | ||
<math> | <math>u_m(t)=e^{i\omega t} u_m \;</math> | ||
< | <font color="blue">What does the subscript m stand for? Modes? [[User:KimberlyWynne|KimberlyWynne]] 03:36, 2 March 2009 (EST)</font> | ||
<math>\Rightarrow -m \omega ^2 \vec{u} = - k \mathbf{M} \vec{u} \;</math> | |||
Band Matrix | |||
<math> | |||
\mathbf{M} = \begin{vmatrix} | |||
2 & 1 & 0 & 0\\ | |||
1 & 2 & 1 & 0\\ | |||
0 & 1 & 2 & 1\\ | |||
0 & 0 & 1 & 2 | |||
\end{vmatrix} | |||
</math> | |||
<math>u_m (t) = e^{ik(na)- \omega t} \;</math> where <math>u_m \rightarrow u_n e^{ik(na)} \;</math> | |||
<math>\Rightarrow -m \omega ^2 \vec{u} = - k [2 - e^{ik \alpha} - e^{-ik \alpha}] \;</math> | |||
[[Image:Dispersionrelation.jpg]] | [[Image:Dispersionrelation.jpg]] |
Revision as of 04:36, 2 March 2009
I have no idea what I'm doing - KimberlyWynne 03:11, 2 March 2009 (EST)
Diatomic harmonic chain
Problem 1
Given:
- a chain of atoms
- with alternating masses and
- connected with elastic springs with constant
- moving only in the x-direction
Derive the dispersion relation for this chain
- Index for acoustic branch
- Index for optical branch
Potential Energy
Eigenvector Value for modes
What does the subscript m stand for? Modes? KimberlyWynne 03:36, 2 March 2009 (EST)
Band Matrix
where
Problem 2
Determine the speed of sound for this chain. What is the lowest frequency of long-wavelength sound corresponding to the optical branch?
From my lecture notes:
where = speed of sound
Problem 3
Sketch the motion of the atoms corresponding to the edge of the Brillouin zone, both for the optical and the acoustic branch.
Problem 4
Determine the Debye temperature for this system, and determine the form of the specific heat in the limits of high and low temperatures.
Problem 5
Consider low temperatures () and determine the wavelength of the most abundant phonons (Hint: note the analogy with Wien's Law!)