Simultaneous observables for hydrogen

In summary, there is a state with simultaneous eigenfunctions and eigenvalues of E, L^2, and L_z, but with an eigenvalue of zero for L_x. This state is represented by l=0 and m=0. For other states, there is no simultaneous eigenfunction and eigenvalue for L_x, L_y, L_z, and L^2. However, it is possible to transform a wavefunction representing an eigenstate of E, L^2, and L_z into another function that is an eigenstate of E, L^2, and L_x with the same eigenvalues for E and L^2, and an eigenvalue for L_x equal to the eigenvalue for L_z.
  • #1
bobred
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Homework Statement


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

Homework Equations



[itex]L^2[/itex] and [itex]L_z[/itex] 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 [itex]L_x,L_y,L_z[/itex] and [itex]L^2[/itex], but with eigenvalues equal to zero. This being the state with [itex]l=0[/itex] and [itex]m=0[/itex], so there are no definite non-zero values of [itex]E, L^2[/itex] and [itex]L_x[/itex]. For other states [itex]L_x,L_y,L_z[/itex] and [itex]L^2[/itex] do not commute.
 
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  • #2
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)]##
 
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  • #3
Thanks, z is an arbitrary choice.
 

FAQ: Simultaneous observables for hydrogen

1. What are simultaneous observables for hydrogen?

Simultaneous observables for hydrogen refer to physical quantities that can be measured simultaneously for a hydrogen atom without affecting each other. These include the energy, position, and momentum of the electron, as well as the spin and magnetic moment of the atom.

2. How are simultaneous observables for hydrogen related to the uncertainty principle?

The uncertainty principle states that certain pairs of observables, such as position and momentum, cannot be precisely measured at the same time. Therefore, simultaneous observables for hydrogen must be chosen carefully to minimize the uncertainty and obtain accurate measurements.

3. Why is it important to study simultaneous observables for hydrogen?

Studying simultaneous observables for hydrogen allows us to better understand the behavior of atoms and the fundamental laws of quantum mechanics. It also has practical applications in fields such as chemistry and materials science.

4. Can simultaneous observables for hydrogen be measured simultaneously in practice?

No, according to the uncertainty principle, simultaneous observables for hydrogen cannot be measured simultaneously with absolute precision. However, by carefully choosing the observables and minimizing the uncertainty, we can obtain measurements that are close to being simultaneous.

5. How do simultaneous observables for hydrogen differ from classical observables?

In classical mechanics, all observables can be measured simultaneously with absolute precision. In quantum mechanics, on the other hand, there is always some uncertainty due to the wave-like nature of particles. Therefore, simultaneous observables for hydrogen in quantum mechanics are limited by the uncertainty principle.

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