Charged particle and virtual photons

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Discussion Overview

The discussion revolves around the quantum-level understanding of forces acting on a charged particle, specifically in the context of a lead ion moving through a dipole magnet in the LHC. Participants explore whether the interaction can be described using the concept of virtual photons and how different frames of reference and gauge choices affect this interpretation.

Discussion Character

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

Main Points Raised

  • One participant describes experiencing a sideways force due to a dipole magnet and questions how this can be understood at the quantum level, specifically through interactions with virtual photons.
  • Another participant suggests that while the magnetic field is described in the lab frame, the particle's frame alters the perceived charge densities, leading to a net force. They note that the concept of virtual photons is contentious and varies among physicists.
  • A third participant expresses interest in how quantum field theory (QFT) would address the deflection of an electron in a dipole magnet, referencing classical explanations as a starting point.
  • A later reply discusses the relevance of frame changes and gauge choices in QFT, suggesting that in the particle's frame and appropriate gauge, virtual particles may not be present, while in another gauge, virtual photons could be considered as gauge bosons.

Areas of Agreement / Disagreement

Participants express differing views on the utility and validity of the virtual photon concept in explaining the forces on charged particles, indicating that there is no consensus on this topic.

Contextual Notes

The discussion highlights the complexities involved in interpreting quantum interactions, including the dependence on frame of reference and gauge choice, which remain unresolved.

xaratustra
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Imagine I am sitting on a lead ion and fly happily through the LHC tube :approve:. Suddenly I feel an strong force pushing me sideways to the left. A physicist sitting in the lab frame tells me later, that I have been going through a dipole magnet yoke with field lines from top to bottom.

How do I understand the force which is dragging me on the quantum level? Is it possible to describe this with collisions with virtual photos? If yes, then why to the left and not some other directions?
 
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Let's start classically to see something interesting. The magnetic field is described in the lab frame, but if you look for a description of what is happening to the particle in the particle frame, the relativistic frame change will alter the charge densities in the currents that cause the B field. In the particle frame, it sees a net charge on the left and right that pushes it left. Now you asked for a field theoretic answer, not a classical one, but my point is that the question is the same as asking for an interpretation of the source of electric field. That is indeed often described in terms of virtual photons, but the whole concept of virtual photons seems very contentious. On another thread, I asked exactly this question, and it seems that it depends on who you put it to as to whether or not the virtual photon concept is a good one here.
 
Thanks. Indeed I was interested in the field theoretical approach. How would QFT deal with the deflection of say an electron going through a dipole magnet?

The classical version seems to be well explained, using the Liénard-Wiechert and the E. M. Pucell explanation e.g. http://physics.weber.edu/schroeder/mrr/MRRtalk.html" .
 
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Right, that clarifies the role of frame changes. But frame changes are still relevant in QFT-- and so is the choice of a gauge. I believe that in the frame of the charge, and in the appropriate gauge, there are no virtual particles there-- just the Coulomb potential of the length-contracted charge density. But in a different gauge, the virtual photons show up as gauge bosons. So I'm not an expert, but it seems to me that the scenario you describe is not so different from two interacting stationary charges, and whether you treat that in a gauge where invoking virtual photons would be useful, seems to be up to you.
 

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