Crystal Vibrations: Impurity in a monoatomic chain

Perses
Messages
14
Reaction score
0

Homework Statement



Hello everyone, I'm a bit stuck on this particular problem and i was hoping somebody could give me a couple tips or hints!

"consider a linear monoatomic chain where all atoms have a mass M except one which has a small mass m. The force constant is C."
First I'm asked to write the equation of motion for the relevant atoms. Then, I'm asked to solve it assuming a displacement function for atom n in the form of

Un = Aexp(-ax)exp(i((omega)t - Kx))

Let the chain be:

vs-2 -- vs-1 --- u --- vs --- vs+1

where u is the impurity

The Attempt at a Solution



I'm currently lost at the beginning of the problem, finding the equation of motion. What i first thought was to treat this almost like it were the case of a diatomic chain.

Mdvs/dt = C(vs+1 + u - 2vs)

mdu/dt = C(vs-1 + vs - 2u)

however, upon continuing in the problem I'm not sure that this is correct. Could anyone offer any advice as to how i should start this problem?
 
Physics news on Phys.org
Your notation is a little distracting. Simply call the displacement of the n'th atom (from its equilibrium position) u_n. Let the impurity be at n=k.

Secondly. you've made a mistake in constructing your equation of motion, which is a second order linear DE (not first order).

See that you should get something more like :

m_n \ddot{u_n} = c(u_{n+1} -2u_n+u_{n-1})

From here, I'm not sure what's the best approach. One possibility is to Fourier transform to k-space and hope the equations become decoupled. Odds are they will. Also, you will likely find that the solution in k-space is the FT of the localized wavepacket provided to you.
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top