QED vs Point Charge of the Electron

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SUMMARY

The discussion centers on the implications of treating the electron as a point charge within Quantum Electrodynamics (QED). Participants highlight that the electron's charge-to-mass ratio approaches infinity, leading to divergences in electromagnetic self-energy. These divergences are addressed through the process of renormalization, which allows for the restoration of predictive power in the theory. The conversation also touches on the potential need for renormalization if the electron were treated as having a finite size, emphasizing the role of high-energy physics in these calculations.

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  • Understanding of Quantum Electrodynamics (QED)
  • Familiarity with the concept of renormalization in quantum field theory
  • Knowledge of perturbation theory and its applications
  • Basic principles of particle physics, including the nature of point particles
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  • Research the process of renormalization in Quantum Field Theory (QFT)
  • Explore the implications of high-energy physics on particle behavior
  • Study the differences between renormalizable and non-renormalizable theories
  • Investigate the structure of particles, including string theory concepts
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Physicists, students of theoretical physics, and researchers interested in the foundations of Quantum Electrodynamics and the implications of particle theory.

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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