Zeeman effect - spin orbit coupling

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Discussion Overview

The discussion revolves around the Zeeman effect, particularly focusing on the role of spin and orbital angular momentum in the splitting of energy levels in a magnetic field. Participants explore the historical context of the effect, the terminology used to describe the resulting states, and the implications of spin-orbit coupling in different elements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the total angular momentum orientations are degenerate until a magnetic field is applied, leading to the Zeeman effect.
  • Another participant explains that many educational resources simplify the Zeeman effect by focusing on orbital angular momentum, as it was historically studied before the concept of spin was introduced.
  • It is mentioned that excluding spin fails to explain the "anomalous Zeeman effect," which requires the inclusion of spin to account for observed phenomena.
  • A participant questions whether the three different energy levels resulting from the splitting of the 2p level in a magnetic field should be referred to as "states," similar to the terminology used for splitting of J levels.
  • Another participant emphasizes the importance of experimental observations, noting that selection rules in optical transitions may limit the visibility of spin splitting, particularly in lighter elements.
  • One participant asserts that the 2p level inherently consists of three different states with distinct m values, which become non-degenerate under an external magnetic field.

Areas of Agreement / Disagreement

Participants express differing views on the role of spin in the Zeeman effect and the terminology used to describe the resulting energy levels. There is no consensus on the implications of spin-orbit coupling across different elements, and the discussion remains unresolved regarding the terminology for the energy levels.

Contextual Notes

Some limitations include the historical context of the Zeeman effect, the dependence on definitions of states versus levels, and the unresolved implications of spin-orbit interaction in various atomic systems.

Chemist20
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As far as I know: the possible orientations that the total angular momentum can take (given my Mj) are degenerate. if we apply a magnetic field, degeneracy will be lost and different states arise. this is the zeeman effect

but when looking up on google for zeeman effect, a webpage used as an example the splitting of the ml values por p orbitals. hence it said that in a magnetic field, the three different orientations of the orbital angular momentum would not be degenerate and hence px py pz would have different energies.

What I don't get is why are they talking about orbital angular momentum without including the spin angular momentum and hence talking about L instead of J ?
 
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Many books and courses introduce the Zeeman effect using only orbital angular momentum because it's easier. It also follows the historical development because physicists started to study the Zeeman effect before they knew anything about spin.

Of course, if you don't include spin, you can't explain many actual examples of Zeeman splitting. People talked about the "normal Zeeman effect" (which did fit the orbital-only calculations) and the "anomalous Zeeman effect" (which didn't).

Then Uhlenbeck and Goudsmit "invented" spin, and it turned out to be what was needed to explain the "anomalous Zeeman effect."
 
jtbell said:
Many books and courses introduce the Zeeman effect using only orbital angular momentum because it's easier. It also follows the historical development because physicists started to study the Zeeman effect before they knew anything about spin.

Of course, if you don't include spin, you can't explain many actual examples of Zeeman splitting. People talked about the "normal Zeeman effect" (which did fit the orbital-only calculations) and the "anomalous Zeeman effect" (which didn't).

Then Uhlenbeck and Goudsmit "invented" spin, and it turned out to be what was needed to explain the "anomalous Zeeman effect."

great thanks!

so... when technically the 2p level splits into 3 different ones due to the interaction of the orbital angular momentum with the magnetic field, are these three different levels called "states"? because this is the term they use when they talking about splitting of the J levels.
 
You also have to take in mind what you actually observe in experiment. In an optical transition, e.g. in hydrogen atom from 1s to 2p there is a selection rule Delta S=0. So you will not observe the splitting of the spin but only the splitting of the orbital momentum. Only in heavier elements where spin orbit interaction is important, you will see the splitting due to spin.
 
Chemist20 said:
when technically the 2p level splits into 3 different ones due to the interaction of the orbital angular momentum with the magnetic field, are these three different levels called "states"? because this is the term they use when they talking about splitting of the J levels.

I would say that 2p consists of three different states to begin with, with different values of m (-1, 0, +1), and with different wave functions that contain different spherical harmonics. With no external magnetic field, these states are degenerate, that is, they have the same energy. An external magnetic field gives them different energies and removes the degeneracy.
 

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