Solution to Set 5: Difference between revisions

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Line 63: Line 63:
<math>\Rightarrow m \omega^2 = k [2 - (e^{ika}  + e^{-ika}] \;</math>
<math>\Rightarrow m \omega^2 = k [2 - (e^{ika}  + e^{-ika}] \;</math>


<math>\Rightarrow \omega^2 = \frac{2k}{m} [1 - cos(ka)] = \;</math>
<math>\Rightarrow \omega^2 = \frac{2k}{m} [1 - cos(ka)] \;</math>
 
<math>\Rightarrow \omega^2 = \frac{\Delta k}{m} \frac{1}{2} [1 - cos(ka)] \;</math>
 
<math>\Rightarrow \omega^2 = \frac{\Delta k}{m} sin^{2}(\frac{ka}{2}) \;</math>
 
<math>\Rightarrow \omega (k) = 2 \sqrt{ \frac{k}{m} } |sin(\frac{ka}{2})| \;</math>
 
[[Image:Dispersionrelation.jpg]]
[[Image:Dispersionrelation.jpg]]



Revision as of 05:52, 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

Chainatoms.jpg

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

Dispersionrelation.jpg

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!)