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| <math>\Rightarrow m \omega^2 = k [2 - (e^{ika} + e^{-ika}] \;</math> | | <math>\Rightarrow m \omega^2 = k [2 - (e^{ika} + e^{-ika}] \;</math> |
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| <math>\Rightarrow \omega^2 = \frac{2k}{m} [1 - cos(ka)] = \;</math> | | <math>\Rightarrow \omega^2 = \frac{2k}{m} [1 - cos(ka)] \;</math> |
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| | <math>\Rightarrow \omega^2 = \frac{\Delta k}{m} \frac{1}{2} [1 - cos(ka)] \;</math> |
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| | <math>\Rightarrow \omega^2 = \frac{\Delta k}{m} sin^{2}(\frac{ka}{2}) \;</math> |
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| | <math>\Rightarrow \omega (k) = 2 \sqrt{ \frac{k}{m} } |sin(\frac{ka}{2})| \;</math> |
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| [[Image:Dispersionrelation.jpg]] | | [[Image:Dispersionrelation.jpg]] |
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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
Potential Energy
Eigenvectors of Modes A and B (defined arbitrarily)
Band Matrix
where
= distance on some coordinate system
Derive and get:
- Index
for optical branch
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!)