Quantum mechanics and Minimal coupling of Dirac field

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Discussion Overview

The discussion revolves around the coupling of the Dirac field to electric and magnetic fields within the framework of quantum mechanics and quantum field theory (QFT). Participants explore how minimal coupling is applied in a relativistic context, particularly focusing on the implications for the spin of particles like electrons and the nature of electric and magnetic dipole moments.

Discussion Character

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

Main Points Raised

  • One participant questions how the spin of an electron, which couples to the magnetic field in non-relativistic quantum mechanics, is resolved in a relativistic context where it seems to couple to both electric and magnetic fields.
  • Another participant suggests that minimal coupling leads to an interaction term of the form σμνFμν, which is relativistically invariant and reduces to S·B in the particle's rest frame, but not in a moving frame where additional interactions with the electric field arise.
  • A participant seeks clarification on whether σμνFμν reduces to just the magnetic field in the rest frame and questions if QFT implies that spin does not couple to the electric field in that frame.
  • Discussion includes the idea that coupling to the electric field would imply the particle has an electric dipole moment, which is said to violate parity conservation, with very small electric dipole moments predicted but not observed.
  • Another participant inquires whether the Dirac equation accounts for both electric and magnetic dipole moments, and if the suppression of electric dipole moments is necessary in quantum electrodynamics (QED).
  • It is noted that minimal coupling implies a magnetic dipole moment but not an electric dipole moment, with electric dipole moments arising from parity-violating particles in internal loops, as predicted by the Standard Model.

Areas of Agreement / Disagreement

Participants express differing views on the implications of minimal coupling and the role of electric dipole moments, with no consensus reached on whether the Dirac equation includes effects from both types of dipole moments or the necessity of suppression in QED.

Contextual Notes

Participants highlight the limitations of current understanding regarding the detection of electric dipole moments and the dependence on theoretical frameworks like the Standard Model and supersymmetry.

mtak0114
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Hi

I have a simple question:

We know from non-relativistic quantum mechanics that the spin of an electron couples only to the magnetic field, i.e. it processes around the magnetic field. How is this resolved in the relativistic context where it would seem that the spin should couple to both electric and magnetic fields? In particular how is this implied through minimal coupling which seems to be relativistically covariant where as the magnetic field isnt?

thanking you in advanced.
 
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mtak, You can either start by giving your particle a minimal coupling or else put in an anomalous moment by hand. Either way you wind up considering an interaction term of the form σμνFμν. As you point out, this is relativistically invariant and reduces to S·B in the particle's rest frame. Of course you're also right that this is not S·B in a frame in which the particle is moving. In fact in a moving frame there will be an additional interaction with the E field that looks like S·(v x E). Well you can't quantize the spin along two different directions, so the obvious thing to do is combine these two terms and write them together as S·Beff where Beff is the necessary linear combination of B and v x E. But Beff is also just the B field back in the particle's rest frame, so we just write it that way!
 
Thanks Bill

that makes sense, but is that assuming that F^{\mu\nu} is just the magnetic field {\bf B} in the rest frame otherwise I can't see how \sigma_{\mu\nu}F^{\mu\nu} reduces to such a term in the rest frame. Is it possible to see the converse, that QFT implies that spin does not couple in the rest frame to the electric field?
 
S·E would mean that the particle had an electric dipole moment, in contrast with a magnetic dipole moment. This violates parity conservation. Very small electric dipole moments are predicted by the Standard Model, and larger ones by other theories, but none has ever been observed.
 
So would it be correct to say that the Dirac equation includes effects due to both electric and magnetic dipole moments of the electron? but given that the former are not observed they are suppressed?

When one goes to QED however is such a suppression necessary or does the theory predict that the electric dipole moment is small?

do you have any good references which discuss this issue?
thanks again

Mark
 
mtak, Minimal coupling implies a magnetic dipole moment but no electric dipole moment. If electric dipole moments exist, they don't arise from the Dirac equation, rather from internal loops of parity-violating particles.

In the Standard Model the moments predicted in this way are far smaller than can be detected. Other theories like supersymmetry predict moments near the present detection threshold. For a reference, look for "Neutron electric dipole moment" and "Electron electric dipole moment" on Wikipedia. Almost all of the information you'll find will be experiment-oriented.
 

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