Where does the magnetic field in spin-orbit coupling come from?

Click For Summary

Discussion Overview

The discussion centers around the origins of the magnetic field in spin-orbit coupling, exploring both classical and quantum mechanical perspectives. Participants examine the implications of analyzing the problem from different reference frames, particularly the rest frame of the proton versus the electron, and critique standard derivations found in textbooks.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants argue that analyzing the magnetic field in the rest frame of the proton is valid, while others suggest that the electron's frame provides a clearer understanding due to the complexities involved with electron spin and velocity.
  • There is a contention regarding the validity of standard derivations of spin-orbit coupling, with some participants labeling them as inadequate or overly simplistic, while others defend the classical explanations involving Thomas precession.
  • One participant mentions that the Dirac equation in the proton's rest frame yields spin-orbit coupling for the electron, highlighting the quantum mechanical aspect of the discussion.
  • Some participants express frustration with the reliance on classical intuition to explain quantum effects, suggesting that this leads to confusion and misunderstandings among students.
  • There is a proposal that a legitimate calculation of spin-orbit coupling can be derived from the nonrelativistic limit of the Dirac equation, which can be simplified using Pauli spinors.
  • Others emphasize the importance of recognizing that spin-orbit coupling is fundamentally a quantum mechanical effect, countering claims that it can be adequately described using classical concepts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of spin-orbit coupling, with ongoing disagreements about the adequacy of classical versus quantum explanations and the effectiveness of standard derivations in textbooks.

Contextual Notes

Some participants note that the discussion is limited by the assumptions made in classical descriptions and the potential oversimplification of quantum mechanical concepts. There is also mention of the challenges faced by students when transitioning from classical to quantum frameworks.

alemsalem
Messages
173
Reaction score
5
the proton is stationary, and we're assuming there is no magnetic field in the rest frame of the proton. I know if we move to the rest frame of the electron there will be a magnetic field.
but shouldn't we be able to analyze it in the rest frame of the proton?
 
Physics news on Phys.org
It easier in the frame of the electron. Even in the frame of the proton, the easiest description would be "the electric field, if we would transfer it to the electron frame, has a magnetic component". In the proton rest frame, you have to consider electron spin, electron velocity and electric field at the same time.
 
The standard derivation of spin-orbit coupling is total horseradish. For a classical particle one can talk about its orbit, its centripetal acceleration, and the relativistic Thomas precession that will act on the spin. None of these classical concepts apply to the quantum mechanical Dirac wavefunction for a bound state. Quantum mechanics can only be done in a nonaccelerating frame.

Unfortunately, most books satisfy themselves with a one-line handwaving derivation, and even more unfortunately, most students fall for it. A legitimate calculation can be found, for example, in the old but excellent QM book by Schiff. His approach involves taking the nonrelativistic limit, in which the Dirac spinor can be replaced by a two-component Pauli spinor, assuming a central potential, and simplifying the resulting Hamiltonian.

One can also write down the exact solution for the bound states of a Dirac particle in a Coulomb potential and extract the spin-orbit term from that.
 
I don't remember it but a proton can be described by a localized current.and can be described by current j=∇×M,where M=mδ(x),m contains contribution from magnetic moment of proton.
this corresponds to vector potential
A=∫j(x')/|x-x'| d3x',apart from some constant.Now one can evaluate B by
B=∇×A.
 
The Dirac equation (in the rest frame of the proton) gives spin orbit coupling for the electron.
 
Bill_K said:
The standard derivation of spin-orbit coupling is total horseradish.

SO coupling is not an intrinsically QM effect. Hence the explanation with Thomas precession is classically correct and physically illuminating, I don't see why it is horseradish.
The standard derivation in QM is via the Dirac equation, but it is somehow a "shut up and calculate" approach and the significance of the terms arising is usually done via comparison with the classically limiting expressions.
 
SO coupling is not an intrinsically QM effect. Hence the explanation with Thomas precession is classically correct and physically illuminating, I don't see why it is horseradish.
Because the atom is an intrinsically QM system, and IMO it is downright harmful to pretend otherwise. In fact most of the confusion in students' minds about QM comes from their too-persistent image of little BBs in little well-defined orbits. Angular momentum exists classically too, but using a classical description of it on the atomic level in terms of little vectors, is not "illumination", just misleading.
The standard derivation in QM is via the Dirac equation, but it is somehow a "shut up and calculate" approach
This is not a ten-page calculation, more like ten lines. Even a small amount of calculation is sometimes looked down on, but that is the way the universe runs, not on intuition. :wink:
the significance of the terms arising is usually done via comparison with the classically limiting expressions.
:confused: When I see a term rxp·σ in the Hamiltonian I don't need to look at the classical limit to tell me that it represents spin-orbit coupling.
 
Last edited:
DrDu said:
SO coupling IS an intrinsically QM effect.
(My slight correction)

the significance of the terms arising is usually done via comparison with the classically limiting expressions.
Using classical 'intuition' to explain a quantum effect is the cause of most of the
'paradoxes' caused by too much talk and too little calculation.
 
I guess its good to see both ways of doing it, with keeping in mind that its actually QM not a classical effect
 
  • #10
Bill_K said:
Unfortunately, most books satisfy themselves with a one-line handwaving derivation, and even more unfortunately, most students fall for it. A legitimate calculation can be found, for example, in the old but excellent QM book by Schiff. His approach involves taking the nonrelativistic limit, in which the Dirac spinor can be replaced by a two-component Pauli spinor, assuming a central potential, and simplifying the resulting Hamiltonian.
Yeah, It is always annoying when a semi-classical explanation is half-heartedly used. I prefer it when the professor just says something like "there is a good explanation, but we don't have time to go into it now".

Also, although the explanation using spinors might not take many lines, I think that for students who are just starting to learn quantum mechanics, it might be a bit too much all at once to go into spinors and other stuff.
 

Similar threads

Replies
1
Views
3K
  • · Replies 19 ·
Replies
19
Views
2K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 19 ·
Replies
19
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
939
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K