Solution to Set 5: Difference between revisions
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<math>\Rightarrow -m \omega ^2 \vec{u} = - k [2 - e^{ik \alpha} - e^{-ik \alpha}] \;</math> | <math>\Rightarrow -m \omega ^2 \vec{u} = - k [2 - e^{ik \alpha} - e^{-ik \alpha}] \;</math> | ||
<math>\omega (k) = 2 \sqrt{ \frac{k}{m} } |sin(ka)|</math> | |||
[[Image:Dispersionrelation.jpg]] | [[Image:Dispersionrelation.jpg]] | ||
Revision as of 04:42, 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!)