Simultaneous observables for hydrogen

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SUMMARY

The discussion centers on the existence of quantum states with simultaneous non-zero eigenvalues for energy (E), total angular momentum squared (L²), and the x-component of angular momentum (Lₓ) in the context of the hydrogen atom. It is established that while L² and Lₓ commute with the Hamiltonian, states with l=0 and m=0 yield zero eigenvalues for these operators. The conversation suggests that transforming a wavefunction representing an eigenstate of E, L², and Lₓ into another eigenstate of E, L², and Lₓ with the same eigenvalues is feasible, challenging the notion of the z-axis being special in this context.

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Homework Statement


Is there a state that has definite non-zero values of E, L^2 and L_x

Homework Equations



L^2 and L_z commute with the Hamiltonian so we can find eigenfunctions for these

The Attempt at a Solution


I would say that there is a state with simultaneous eigenfunctions of L_x,L_y,L_z and L^2, but with eigenvalues equal to zero. This being the state with l=0 and m=0, so there are no definite non-zero values of E, L^2 and L_x. For other states L_x,L_y,L_z and L^2 do not commute.
 
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Hello.

Something to think about. Should the z axis be special in the hydrogen atom? That is, if there exist states with definite non-zero eigenvalues of ##E, L^2,## and ##L_z##, why shouldn't there exist states with definite non-zero eigenvalues of ##E, L^2,## and ##L_x##?

Suppose you had a wavefunction ##\psi(r, \theta, \phi)## that represents an eigenstate of ##E, L^2,## and ##L_z##. Can you think of how you could transform ##\psi(r, \theta, \phi)## into another function ##\psi'(r, \theta, \phi)##that would be an eigenstate of ##E, L^2,## and ##L_x## with the same eigenvalues for ##E## and ## L^2## and with an eigenvalue of ##L_x## equal to the eigenvalue that ##\psi## had for ##L_z##?

[Edit: It might be easier to think in terms of Cartesian coordinates ##\psi(x, y, z)]##
 
Last edited:
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Thanks, z is an arbitrary choice.
 

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