Understanding Electron Mass in Classical and Quantum Electrodynamics

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SUMMARY

The discussion focuses on the distinctions between mechanical, electromagnetic, and observed electron mass within classical and quantum electrodynamics. It highlights the divergence of classical electron self-energy and the implications of mass-renormalization, runaway solutions, and preacceleration. The participants emphasize that assuming a point-like electron leads to unjustified conclusions regarding its mass and electromagnetic energy. Key references include Weisskopf's paper and Schwebers' book on relativistic quantum theory.

PREREQUISITES
  • Understanding of classical electron theory
  • Familiarity with quantum electrodynamics (QED)
  • Knowledge of mass-renormalization concepts
  • Basic principles of electromagnetic theory
NEXT STEPS
  • Read Weisskopf's paper on quantum electrodynamics
  • Study Schwebers' "Introduction to Relativistic Quantum Theory"
  • Explore the implications of Poynting's theorem for point-like particles
  • Investigate the concept of runaway solutions in classical electrodynamics
USEFUL FOR

Physicists, researchers in theoretical physics, and students studying classical and quantum electrodynamics who seek to deepen their understanding of electron mass and self-energy concepts.

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Consider classical electron theory. Distinguish between the mechanical, electromagnetic, and observed electron mass. What is the degree of divergence of the classical electron self-energy?
What are the roles of mass-renormalization, runaway solutions, and preacceleration in classical electron theory?
What is the degree of divergence of the electron self-energy in quantum electrodynamics?
 
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catlike,
I think that in classical theory, the divergence occurs only if you postulate that Poynting expressions are valid for point-like particle. But that is not justified.

If you assume it is point-like, there is no good reason to suppose its mass has anything to do with electromagnetic energy.
I do not know much of the quantum theory, but it is discussed by Weisskopf in the paper

http://prola.aps.org/abstract/PR/v56/i1/p72_1

and also in Schwebers book Introduction to Relativistic Quantum Theory.

J.
 

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