How to Solve the Eigenfunctions of a Rigid Rotator in a Weak Electric Field?

hokhani
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Homework Statement



Consider the Hamiltonian for a rigid rotator, constrained to rotate in xy plane and with moment of inertia I and electric dipole moment\mu in the plane, as H_0=\frac{L_z^2}{2I}. Then suppose that a constant and weak external electric field,E, in the direction of x is applied so the perturbation is H'=-\mu E cos (\phi).

Homework Equations



The eigenfunctions of H_0 are double degenerate and the degeneracy is not removed even in high orders of perturbation. How should I solve it? could anyone please help me?

The Attempt at a Solution

 
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The problem statement doesn't include a question.

Have you calculated ##\langle m' | H' | m \rangle##? And found it to be always zero for ##m'\neq m##?
 
The degenerate eigenfunctions are |m\rangle=\frac{1}{\sqrt {2\pi}} e^(im\phi) and |-m\rangle=\frac{1}{\sqrt {2\pi}} e^(-im\phi) and \langle -m|cos(\phi)|m\rangle =0 (ms are integer). Hence all the elements of perturbation matrix between degenerate kets would be zero.
 
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I made a quick calculation, and it seems indeed that the degeneracy is not lifted. How is that a problem? The field still shifts the levels.
 
Could you please give me your solution? Or at least, how much does the electric field move the levels?
 
You should calculate ##\langle m' | H' | m \rangle## yourself. Rewriting ##\cos \phi## in terms of exponentials helps in evaluating the integrals.
 
DrClaude said:
You should calculate ##\langle m' | H' | m \rangle## yourself. Rewriting ##\cos \phi## in terms of exponentials helps in evaluating the integrals.
Ok, it is very easy to calculate it:
\langle m' | H' | m \rangle=-\frac{\mu E}{2}(\delta(m',m+1)+\delta(m',m-1))
Making the H' matrix on the two degenerate kets, m and -m, we observe that all the four matrix elements are zero. Could you please tell me what is my mistake?
 
I'm sorry, but the I don't understand what question you are trying to answer.
 
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