Solution to Set 5: Difference between revisions

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(Adding to Problem 1 Solution)
Line 16: Line 16:
* Index<math>\alpha = 2\;</math> for optical branch
* Index<math>\alpha = 2\;</math> for optical branch


Potential Energy <math>U = 1, 2, 3, ... N \;</math>
Potential Energy <math>U = 1, 2, 3, ... n \;</math>


<math>U \cong \frac{1}{2} k \sum_{n} (U_n - U_{n-1}) \;</math>
<math>U \cong \frac{1}{2} k \sum_{n} (U_n - U_{n-1}) \;</math>


Eigenvectors
<math>\Rightarrow m \ddot{u}_n = - k [2U_n - U_{n-1} - U_{n+1}] \;</math>
 
Eigenvector Value
 
<math>u(t)=e^{i\omega t} u_n \;</math>


[[Image:Dispersionrelation.jpg]]
[[Image:Dispersionrelation.jpg]]

Revision as of 04:16, 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
  • Index for optical branch

Potential Energy

Eigenvector Value

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!)