Degeneracy of a 2-dimensional isotropic Harmonic Oscillator

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silverwhale
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Homework Statement


The Hamiltonian is given by:
[tex]H = \frac{1}{2} \sum_{i=1,2}[p_i^2 + q_i^2][/tex]
We define the following operators:
[tex]J = \frac{1}{2} (a_1^+ a_1 + a_2^+ a_2)[/tex]
[tex]J_1 = \frac{1}{2} (a_2^+ a_1 + a_1^+ a_2)[/tex]
[tex]J = \frac{i}{2} (a_2^+ a_1 - a_1^+ a_2)[/tex]
[tex]J = \frac{1}{2} (a_1^+ a_1 - a_2^+ a_2)[/tex]

I have shown previosly that [tex]\textbf{J}^2=J_1^2 + J_2^2 + J_3^2 = J(J+1)[/tex]

The question: Using this result (the one above), discuss what is the degeneracy of the eigenvalues of H.

Homework Equations


[tex]H = 2J + 1[/tex]
[tex]\textbf{J}^2=J_1^2 + J_2^2 + J_3^2 = J(J+1)[/tex]

The Attempt at a Solution


I thought just saying that [tex][H, \textbf{J}^2] = 0[/tex] would be enough to say that the eigenvalues of H are degenerate with respect to the eigenstates of [tex]\textbf{J}^2[/tex]. But I am not sure if this is enough, can I calculate the degeneracy of the eigenvalues of H just using the equations found above?
 
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One makes an analogy to angular momentum. So one does something like
$$J_{\pm} = J_1 \pm i J_2 $$
and find that
$$[J_+, J_3] = J_+ $$
$$[J_-, J_3] = -J_- $$
One also finds that ##[J_3, J^2] = 0## so one can give the eigenvalues of ##J^2## and ##J_3## a separate quantum number, so the eigenvalues of the two operators are ##j(j+1)## and ##m##, respectively.
So from this we obtain $$J_3J_+\mid j m \rangle = (m+1) J_+\mid j m \rangle $$
$$ J_+\mid j m \rangle = \alpha_{jm+}\mid j m+1 \rangle$$
and similiarly for ##J_-##. Also since ##[J_\pm, J^2] = 0##, one gets that ##J_\pm\mid j m \rangle## has the same energy eigenvalue as ##\mid j m \rangle##
To find the degeneracy one calculates ##\left| J_\pm\mid j m \rangle\right|^2 = |\alpha_{jm\pm}|^2## and notice that if one tries to exceed a particular range of ##m## one just gets ##\alpha=0##. So there is a finite range of ##m## with the same energy. Let me know if that helps.
 
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