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Homework Statement
Consider the following set of eigenstates of a spin-J particle:
<br /> |j,j > , ... , |j,m > , ... | j , -j ><br />
where
<br /> \hbar^2 j(j+1) , \hbar m<br />
are the eigenvalues of J^2 and Jz, respectively. Is it always possible to rotate these states into each other? i.e. given |j,m> and |j,m'>, is it always possible to find a unitary rotation operator U^j such that
<br /> |j,m' > = U^{(j)} |j, m >
***
Not too sure how to approach this problem, although given that
<br /> U^\dagger |j,m' > = U^\dagger U |j,m >
and
<br /> < j,m' | j,m > = \delta_{mm'}<br />
I would think that
<br /> < j,m' | U^\dagger | j,m' > = 0<br />
which doesn't seem right hence the answer would be no.
Also the fact that the rotation matrix times a given eigenstate is in general a linear combination of 2j+1 independent states of the form |j,m'> makes me doubtful as well.
Any help would be appreciated (this isn't an actual homework question but taken from a practice exam so feel free to go into as much detail as possible as that would be really helpful).