Moment and the Larmor precession

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Discussion Overview

The discussion revolves around the concept of Larmor precession, particularly focusing on the definition and application of magnetic moment in the context of a single electron in a magnetic field. Participants explore the implications of using classical definitions in quantum scenarios and question the validity of the Larmor equation under these conditions.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant discusses the definition of magnetic moment as related to current and surface area, questioning its applicability when an electron's trajectory changes due to a magnetic field.
  • Another participant expresses uncertainty about the validity of Larmor precession at the quantum level, particularly for a single electron orbiting a nucleus.
  • A different participant notes that they have only used the Larmor equation in classical contexts and questions its relevance to the scenario of a unique electron.

Areas of Agreement / Disagreement

Participants generally express uncertainty regarding the application of Larmor precession to a single electron and whether the classical definitions and equations hold in this quantum context. Multiple competing views remain on the validity of the Larmor equation in such scenarios.

Contextual Notes

There are limitations regarding the assumptions made about the classical versus quantum treatment of Larmor precession, and the discussion does not resolve whether the Larmor equation is applicable in the case of a unique electron.

enigmation
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Hi,

In the Larmor precession, we tend to define the magnetic moment as the current multiplied by the surface (for an electron rotating around a nucleus), sometimes this moment is defined (generally) as the sum of the vectoriel products of half of the position vector and the charge times the velocity. But once we apply a magnetic field for the case of a unique electron, the "magnetic moment" starts rotating around the z-axis and the trajectory of the electron is no longer a circle. Now the obvious thing is that there is no average "current", because there is no loop (the electron starts to move in a quite different circular paths and never comes back to an earlier position), so the definition of the magnetic moment that uses the current is not correct in the Larmor precession, unless we consider that the electron period of rotation around the nucleus is negligible with respect to the Larmor period, which gives quite the same trajectory when there is no magnetic field. The problem in general is, are we still allowed to use the magnetic moment in, the Newton second law (the moment appears in the couple) and then deduce the famous larmor equation by substituting the angular momentum by the gyromagnetic relation? And what is the exact definition of the magnetic moment? To sum up, do you think that there are some circumstances (time scale for example) at which there is a problematic in the Larmor equation that gives the precession the magnetic moment?Thank you,
 
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enigmation said:
But once we apply a magnetic field for the case of a unique electron
I am not sure that Larmor precession makes sense at that level. I have only ever treated Larmor precession in the classical limit. Is it a valid equation at the quantum level?
 
Dale said:
I am not sure that Larmor precession makes sense at that level. I have only ever treated Larmor precession in the classical limit. Is it a valid equation at the quantum level?

I mean when there is a unique electron orbiting a fixed nucleus.
 
Yes, that is what I understood that you meant. I have never used the Larmor equation to describe a unique electron orbiting a fixed nucleus. I have only used it under the usual classical limit to model the expectation of a large number of spins. I am not sure that it applies to your scenario.
 

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