Angular momentum of an electron

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Discussion Overview

The discussion revolves around the angular momentum of an electron in a hydrogen atom, specifically addressing the possibility of an electron being in a superposition of energy eigenstates while having different expectation values for the angular momentum components L_x and L_y. The conversation explores the implications of quantum mechanics and the measurement of angular momentum in this context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether an electron in a superposition of eigenstates of L_z can have different expectation values for L_x and L_y, suggesting a potential asymmetry.
  • Another participant asserts that due to the uncertainty principle, L_z and L_y cannot be measured simultaneously, but total angular momentum can be measured with precision.
  • A different viewpoint claims that if the quantum system is in a state with l=0, all angular momentum components can be measured with arbitrary precision.
  • One participant clarifies that the expectation value is not the result of a single measurement and discusses a specific exam problem involving a hydrogen atom's state, where they found different expectation values for L_x and L_y.
  • Another participant agrees that it is possible to obtain different expectation values for L_x and L_y, emphasizing that the operators are distinct and can yield different results.
  • A subsequent reply notes that while the theory treats x and y equally when choosing z as the reference axis, the specific state in question does not maintain this symmetry.
  • Another participant points out that only m=0 states exhibit symmetry about the z-axis, indicating that the presence of the |211⟩ state breaks this symmetry.

Areas of Agreement / Disagreement

Participants express differing views on the measurement of angular momentum components and the implications of superposition states. There is no consensus on whether the expectation values for L_x and L_y can be equal in the discussed scenario, as some argue for the possibility of differing values while others emphasize the symmetry in certain states.

Contextual Notes

The discussion highlights the complexities of measuring angular momentum in quantum mechanics, particularly regarding the conditions under which different expectation values may arise. The specific assumptions about the states and the definitions of angular momentum operators are critical to the arguments presented.

broegger
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Hi,

Say you have an electron in the hydrogen atom. Can this electron be in a state that is a superposition of the usual energyeigenstates (which are also eigenstates of L_z) AND have different expectation values for L_x and L_y? Are x and y symmetric in the sense that their expectation values are always equal in this situation?
 
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You can't measure the expectation value of L_z and L_y simultaneously cause of the uncertainty. You can only measure total angular momentum and L_y or total angu. mom. and L_z precisely.
 
You can measure them all (5) with arbitrary precision,if the quantum system is in a state with [itex]l=0[/itex].

Daniel.
 
Kruger said:
You can't measure the expectation value of L_z and L_y simultaneously cause of the uncertainty. You can only measure total angular momentum and L_y or total angu. mom. and L_z precisely.

No no, I think you misunderstand. The EXPECTATION value is not the result of a single measurement. This is what I mean: Can you have a particle in a state, which is a superposition of eigenstates of L_z, but which - at some point in time (say t=0) - has different EXPECTATION values for L_x and L_y.

The reason I'm asking is that I found just that in my exam the other day. The assignment was this:

In this problem we consider a hydrogen atom whose normalized stationary states is denoted [tex]|nlm\rangle[/tex], where n is the main quantum number and l and m is the quantum numbers belonging to L^2 and L_z, respectively. Consider a hydrogen atom described by the state:
[tex]|\psi\rangle=\frac1{\sqrt2}(|210\rangle + |211\rangle)[/tex]​

Answer these questions:

1. Blah blah
2. Blah blah
3. Blah blah
4. Calculate the expectation values of L_x and L_y in the state |psi>.

I got different answers for <L_x> and <L_y> (h/sqrt(2) and 0, respectively). Is this possible? When you choose z as reference axis the theory seems to treat x and y equally.
 
There's no problem whatsoever.The two operators are different (see their expressions as a function of the ladder operators),so it's obvious to get different expectation values.

Daniel.
 
Ok, thanks.
 
broegger said:
When you choose z as reference axis the theory seems to treat x and y equally.

That's right, but your specific state doesn't treat x and y equally. So, as dextercioby already pointed, there's no contradiction if you find different expectation values.
 
Choosing z as the reference axis doesn't necessarily treat x and y equally, it's
just a convention. Only m=0 states have symmetry about the z-axis. So <L_x> = <L_y> (= 0 I think) whenever m= 0, but since [tex]|211\rangle[/tex] is part of
the wavefunction, it doesn't have the symmetry.
 

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