Rotating eigenstates of J operator into each other?

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SUMMARY

The discussion centers on the feasibility of rotating eigenstates of a spin-J particle, specifically whether a unitary rotation operator \( U^{(j)} \) can transform one eigenstate \( |j,m\rangle \) into another \( |j,m'\rangle \). The participants conclude that while constructing a unitary operator is theoretically possible, the resulting states may not correspond to the desired eigenstates due to the nature of rotation matrices, which typically yield superpositions of multiple states. The consensus leans towards the idea that such rotations do not always yield direct transformations between eigenstates.

PREREQUISITES
  • Understanding of quantum mechanics, specifically spin systems
  • Familiarity with unitary operators and their properties
  • Knowledge of rotation matrices in quantum mechanics
  • Concept of eigenstates and eigenvalues in the context of angular momentum
NEXT STEPS
  • Research the properties of unitary operators in quantum mechanics
  • Learn about the mathematical formulation of rotation operators, particularly \( U = e^{-i\theta \hat{\mathbf{n}} \cdot \mathbf{J}} \)
  • Explore the implications of superposition in quantum state transformations
  • Investigate the relationship between rotation matrices and eigenstate transformations in Hilbert space
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This discussion is beneficial for quantum mechanics students, physicists specializing in angular momentum, and researchers exploring the mathematical foundations of quantum state transformations.

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Homework Statement



Consider the following set of eigenstates of a spin-J particle:

<br /> |j,j &gt; , ... , |j,m &gt; , ... | j , -j &gt;<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&#039; &gt; = U^{(j)} |j, m &gt;

***

Not too sure how to approach this problem, although given that
<br /> U^\dagger |j,m&#039; &gt; = U^\dagger U |j,m &gt;
and
<br /> &lt; j,m&#039; | j,m &gt; = \delta_{mm&#039;}<br />
I would think that
<br /> &lt; j,m&#039; | U^\dagger | j,m&#039; &gt; = 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).
 
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What do you mean by rotation? I think it is always possible to construct such a unitary operator. One could just do it explicitly.

U = \mathbf{I} - \mid j, m \rangle \langle j, m \mid - \mid j, m&#039; \rangle \langle j, m&#039; \mid + \mid j, m&#039; \rangle \langle j, m \mid - \mid j, m \rangle \langle j, m&#039; \mid

I think the above would work. But do you consider that a rotation? I suppose one might consider all special unitary operators to be rotations in a sense (rotations in the Hilbert space). However I don't know if you mean rotations as in rotations in 3D space, that is ## U = e^{-i\theta \hat{\mathbf{n}} \cdot \mathbf{J}} ##. If this is what you mean, then I'm not sure of the answer. I know such rotations will often result in superpositions of m states, which is not what you want.
 
Last edited:
Rotation is a bit of a misnomer indeed. I think unitary transformation is what is meant here. I'll try your first suggestion (just need to check it's indeed unitary) but it looks good to me. Thanks.
 

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