Spin orbit coupling/orbital degeneracy

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Discussion Overview

The discussion revolves around spin-orbit coupling and its implications for energy levels in atomic orbitals, particularly focusing on the 2S and 2P states, as well as the behavior of these states in systems with varying electron counts. Participants explore the relationships between quantum numbers and the effects of electron configuration on energy degeneracy.

Discussion Character

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

Main Points Raised

  • One participant questions whether the 2S0 and 2P0 states have the same energy, similar to the 2S1/2 and 2P1/2 states.
  • Another participant clarifies that the subscript 1/2 refers to total angular momentum J, which is limited to L+1/2 and L-1/2, and notes that a D orbital can only have J values of 3/2 or 5/2.
  • A participant raises concerns about the validity of the quantum number assignments for even versus odd numbers of electrons, specifically questioning the existence of 2S0 as a single orbital.
  • There is a discussion about the Zeeman effect and its differences for even and odd electron configurations, with a participant expressing confusion about the spin of S orbitals in even electron systems.
  • Another participant references the appropriate use of quantum numbers for single electrons outside closed subshells and inquires about the treatment of closed shells or multi-electron systems in fine structure calculations.
  • A participant discusses the commutation of the spin-orbit Hamiltonian with various operators and the implications for quantum numbers used to label states in the presence of spin-orbit interaction.
  • There is a clarification regarding the term "unperturbed hydrogenic wavefunctions," with participants discussing its meaning in the context of simplified models without spin-orbit coupling.
  • One participant humorously acknowledges a mistake in their previous statement regarding the half-integer nature of j for single electron orbitals.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of quantum numbers for even versus odd electron configurations, and there is no consensus on the existence or treatment of certain states like 2S0. The discussion remains unresolved regarding the implications of spin-orbit coupling on energy levels.

Contextual Notes

Limitations include the dependence on the definitions of quantum numbers and the unresolved nature of how to treat multi-electron systems in relation to fine structure calculations.

granpa
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disregarding the hyperfine structure and the lamb shift for the moment, spin orbit coupling says that 2S1/2 and 2P1/2 have the same energy. do 2S0 and 2P0 have the same energy?

if 2P splits into 3/2 and 1/2 does the 3D orbital split into 5/2, 3/2, and 1/2 and the 4F orbital into 7/2, 5/2, 3/2, and 1/2? google gets plenty of hits but they only talk about 2P.this is just my own personal interest but you can move it to homework if you are so inclined.
 
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The subscript1/2 is the total J=L+S (QM addition). That limits J to L+1/2 and L-1/2.
There is no 0 subscrlpt for one electron.
A D orbital (L=2) can have only 3/2 or 5/2.
An F orbital (L=3) can have only 5/2 or 7/2.
The G...
 
thank you for responding.

the web says that those numbers only hold if the number of electrons is odd. I was wondering what happens if the number of electrons is even. that is why I asked about 2S0.
 
"the web says" is a pretty non specific statement, why not state where you read it? Maybe you have misunderstood something?

Which atoms are you considering?

nLj referes to single electron-orbitals, a single electron orbital can not have j = half integer. 2So does not exists as single orbital, are you suggesting 2So to be notation for what??
 
because I read it on many sites. they all say the same thing. that the formula only works of odd number of electrons. I'll try to find the exact source.
 
Last edited:
I know that the zeeman effect is different for even and odd and all the sites talk about 2P1/2 and 2S1/2. maybe I assumed it was different. if the number of electrons was even then why would the S orbital have spin 1/2?
 
from the web:
The nlj quantum numbers are, then, again appropriate for a single electron outside closed subshells.

so what do I use for closed shells or nonclosed shells with more than one electron? especially for calculating fine structure.
 
https://www.physicsforums.com/showthread.php?t=114363

They are still valid. But that's not the point. The point is whether the *perturbation* hamiltonian commutes with these operators. One finds that the spin orbit hamiltonian commutes with L^2, S^2, J^2 and J_z, but not with L_z and S_z. Therefore, m_s and m_l are not good quantum numbers but must be replaced by m_j and j. So the states of definite energy when the spin-orbit interaction are taken into account are the states labelled by the quantum numbers l,s,j, m_j (instead of the usual l,m_l,s,m_s that one uses to label the unperturbed hydrogenic wavefunctions).

unperturbed hydrogenic wavefunctions?
 
http://www.pha.jhu.edu/~rt19/hydro/node9.html

http://www.pha.jhu.edu/~rt19/hydro/img194.gif
 
Last edited by a moderator:
  • #10
yes what about them, and what about the picture? what do you want?
 
  • #11
I thought others might find it helpful.
 
  • #12
but you explicit ask "unperturbed hydrogenic wavefunctions?"
 
  • #13
that was 3 days ago. I figured you just weren't going to answer.

I guess that 'unperturbed hydrogenic wavefunction' just means the simplified hydrogen model without taking spin-orbit coupling into account? or does it mean something else completely?
 
  • #14
yes, that is correct.
 
  • #15
malawi_glenn said:
nLj referes to single electron-orbitals, a single electron orbital can not have j = half integer.
?? L is an integer and S= 1/2 so j must be a half integer for a single electron orbital
 
  • #16
nrqed said:
?? L is an integer and S= 1/2 so j must be a half integer for a single electron orbital

LOL correct, i did too many "not" in one sentence ;-) Sorry
 

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