QED vs Point Charge of the Electron

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Discussion Overview

The discussion revolves around the implications of treating the electron as a point charge within the framework of Quantum Electrodynamics (QED). Participants explore the consequences of this assumption, particularly regarding the charge to mass ratio and the concept of renormalization in high-energy physics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that if the electron is a point charge, its charge to mass ratio approaches infinity, raising questions about how QED addresses this issue.
  • Renormalization is proposed as a method to handle divergences associated with a point particle's electromagnetic self-energy and charge.
  • One participant expresses uncertainty about the implications of renormalization, questioning whether knowledge of high-energy physics would eliminate the need for it.
  • Another participant suggests that if the electron had a finite size, it might change the need for renormalization.
  • There is a discussion about the role of ignorance in the divergences encountered in QFT and how introducing a cutoff can help manage these issues.
  • Concerns are raised about the reliability of sources discussing renormalization, specifically referencing Gerardus 't Hooft and his views on related topics.
  • A participant reflects on the historical context of QED and its dependence on the electron being treated as a point particle, linking it to Dirac's theories.

Areas of Agreement / Disagreement

Participants express differing views on the implications of treating the electron as a point charge and the necessity of renormalization, indicating that multiple competing perspectives remain unresolved.

Contextual Notes

Limitations include the dependence on assumptions about the electron's structure and the unresolved nature of high-energy physics. The discussion also highlights the complexity of renormalization and its implications in theoretical physics.

Buckeye
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If the electron is a point charge, then its' charge to mass ratio approaches infinity. How does the Standard Model (QED) deal with this?
 
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Buckeye said:
If the electron is a point charge, then its' charge to mass ratio approaches infinity. How does the Standard Model (QED) deal with this?

RENORMALIZATION

regards
marlon
 
Buckeye said:
If the electron is a point charge, then its' charge to mass ratio approaches infinity.

Excuse my ignorance but how so?
 
I would assume Buckeye is referring to the fact that a point particle has a divergent electromagnetic self energy. What has not been mentioned is that the charge of the electron also diverges. As marlon said, both these divergences are dealt with by first acknowledging our ignorance of the high energy physics and then by renormalizing both parameters at each order in perturbation theory. The predictive power of the theory is restored.
 
Physics Monkey said:
I would assume Buckeye is referring to the fact that a point particle has a divergent electromagnetic self energy. What has not been mentioned is that the charge of the electron also diverges. As marlon said, both these divergences are dealt with by first acknowledging our ignorance of the high energy physics and then by renormalizing both parameters at each order in perturbation theory. The predictive power of the theory is restored.
Question...does this then mean that, if we had knowledge (not ignorance) of the physics, we would do away with renormalization ? And, if so, what would replace renormalization ?
 
If we treat the electron as a charge with a finite size, do we need to renormalize?
 
Rade said:
Question...does this then mean that, if we had knowledge (not ignorance) of the physics, we would do away with renormalization ? And, if so, what would replace renormalization ?

Yes. The infinity comes about of our ignorance of the structure of the electron. That's why we make it a *point* particle. This comes down to saying that an electron can interact, as a WHOLE, and transmit arbitrary high momenta. It is the integration over these arbitrary high momenta which make quantities diverge in QFT. If the electron has a structure (say, a string or something else) then of course it will not be able to transmit higher momenta (= short wavelengths) than the size of its structure ; at higher momenta, we would start to see the effects of its structure (like happens for instance with a proton: you cannot have very high momentum transfer to a *proton*, because when you try to do so, you break up the proton: that's called deep inelastic scattering). What we do in renormalization, is to propose an arbitrary scale at which we cut off the momentum transfer to the electron (as if it had structure at this scale). It then turns out, in renormalizable theories, that the low-energy behaviour becomes independent of the exact value of this cutoff scale, as long as it is high enough. So we can just as well take its limit to infinity.
What happens then is that the *relationship* between low energy quantities remains unchanged.
In non-renormalizable theories, this doesn't happen: we depend for the low energy behaviour crucially on the details of the cutoff (of the arbitrary structure we introduced).
 
Buckeye said:
If we treat the electron as a charge with a finite size, do we need to renormalize?

Check out http://nobelprize.org/physics/laureates/1999/thooft-lecture.html if you want to know more on renormalization.

Trust me, the source is reliable:wink:

regards
marlon
 
Reliable? Famous perhaps, but also maybe cranky? It doesn't follow because somebody made a wonderful discovery back when, that he is today a reliable guide on controversial issues. Recall Dirac and his later life adventures.
 
  • #10
selfAdjoint said:
Reliable? Famous perhaps, but also maybe cranky? It doesn't follow because somebody made a wonderful discovery back when, that he is today a reliable guide on controversial issues. Recall Dirac and his later life adventures.

I was not talking in general terms here. In the case of Gerardus 't Hooft the situation is very clear. Well, perhaps not his visions on string theory but even with those i agree with him. But, this does not change much since we are talking about QED renormalization here

regards
marlon
 
  • #11
marlon said:
I was not talking in general terms here. In the case of Gerardus 't Hooft the situation is very clear. Well, perhaps not his visions on string theory but even with those i agree with him. But, this does not change much since we are talking about QED renormalization here
regards
marlon
I read 't Hooft's Nobel lecture and understand most of it. Now I'm wondering if QED moved in this direction because Dirac's theory depends on the electron and other particles to act or be point particles.
Yes, No or Option C?
 

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