Spherical Harmonic Hydrogen Wavefunction

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Homework Help Overview

The discussion revolves around the physical interpretation of spherical harmonics, specifically Ylm, in the context of quantum mechanics and angular momentum. The original poster questions why a spherically symmetric Ylm cannot represent a system with non-zero angular momentum.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to reconcile the concept of spherical symmetry with the implications of angular momentum, questioning whether classical ideas are being applied too rigidly.
  • Some participants explore the definition of spherical symmetry and its relation to angular momentum, discussing how changes in physical properties upon rotation indicate a lack of symmetry.
  • Further inquiries are made regarding the nature of the wave-function and its implications for probability distributions in quantum mechanics.

Discussion Status

The discussion is ongoing, with participants providing insights and clarifications regarding the relationship between spherical symmetry and angular momentum. There is an exploration of the transition from classical to quantum interpretations, particularly concerning the nature of the wave-function and probability distributions.

Contextual Notes

Participants are grappling with the implications of quantum mechanics on classical concepts, particularly in the context of angular momentum and the interpretation of spherical harmonics. The original poster expresses confusion about the physical meaning of spherical symmetry in relation to angular momentum states.

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Homework Statement



Give a physical explanation of why a spherically symmetric Ylm cannot describe the state of a system with non-zero angular momentum.

Homework Equations





The Attempt at a Solution




I was thinking that if Ylm is spherically symmetric then the particle is equally likely to be found in any direction. But if it has non-zero angular momentum then it is rotating therefore it\'s probability to be found at a particular angle should change with time. But then I thought: assume l=0. Then the particle doesn't have angular momentum. Even so, the spherical harmonic shouldn\'t be spherically symmetric, should it? Surely if it\'s not rotating round the nucleus then there should be a particular direction where it is certain (or v likely) to be found..?

Or am i taking classical ideas too far?

What would you say?
Tanks!
 
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Look at the form of the l=0 spherical harmonic. It's constant.
 
Thanks but that doesn\'t help. I knew that already, as is clear from my post :)

I\'m trying to understand it physically...
 
Well, think about the idea of "spherically symmetric". Spherically symmetric means that upon rotations, the system's properties do not change. However, if something does have an angular momentum, then one can distinguish a change in a physical system upon rotation. For example, the rotation of an object in a classical orbit has an angular momentum and since the angular momentum is defined by a certain direction, it is no longer spherically symmetric. If you do the typical thing and define the angular momentum in the z-direction with objects orbiting in the xy-plane, the system will change upon any rotation that is not simply in the orbital plane.

So if you have an angular momentum, spherical symmetry no longer holds.
 
Well that\'s basically what i said in my first post..but my question is: why do you have spherical symmetry when l=0. Surely if it is not orbiting, its at a given point - in which case the probability to find it in all directions shouldn't be the same!
 
bon said:
Well that\'s basically what i said in my first post..but my question is: why do you have spherical symmetry when l=0. Surely if it is not orbiting, its at a given point - in which case the probability to find it in all directions shouldn't be the same!

Ahh, I see what you mean. Yes this is where the classical concept of an orbit needs to be abandoned. It doesn't make sense to talk about an electron orbiting a proton, for example. The electron doesn't have a well-defined orbit so that you could say "yes the electron is right there!". Remember, you're not solving for an orbit or equations of motion; you're solving for the wave-function so a lot of classical ideas no longer apply. If you were solving for an orbit, then it would make no sense for something with no angular momentum to be spherically symmetric. However you're solving for probabilities which means the probability distribution for finding the particle is spherically symmetric.
 
Thank you!
 

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