Modifying the Fine Structure Constant to Incorporate Self-Energy Interactions?

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SUMMARY

The discussion centers on the fine structure constant and its relationship with self-energy interactions in quantum electrodynamics. Participants analyze the dimensionality of the fine structure constant, specifically how the ratio of Coulomb energy and the product of h-bar and speed of light results in a dimensionless quantity. The conversation explores whether the fine structure constant can be modified to incorporate self-energy effects, proposing a new definition of the fine structure constant, α'(s), that equates to the ratio of α(s) and the modified Mandelstam variable s. This suggests a potential avenue for further theoretical exploration in particle physics.

PREREQUISITES
  • Understanding of quantum electrodynamics (QED)
  • Familiarity with the fine structure constant (α)
  • Knowledge of Mandelstam variables in particle physics
  • Basic concepts of self-energy interactions
NEXT STEPS
  • Research the implications of modifying the fine structure constant in quantum field theory
  • Study the role of self-energy in quantum electrodynamics
  • Examine the mathematical framework of Mandelstam variables
  • Explore existing literature on the dimensional analysis of fundamental constants
USEFUL FOR

The discussion is beneficial for theoretical physicists, quantum field theorists, and researchers interested in the foundations of particle physics and the implications of modifying fundamental constants.

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How do (e^2)/(4Pi x epsilon x Planck constant x speed of light) cancel to give one and make the fine structure constant dimensionless?

thanks
 
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The Coulomb energy is V = e2/r, so e2 has dimensions of energy*length. On the other hand, h-bar*c = 197.5 MeV-f also has dimensions of energy*length, so the ratio of the two expressions is dimensionless.
 
Does anyone know if by making the fine structure a function of energy, can one capture the Lorentz force as proportional to:

[tex]\frac{\alpha(s)}{s}[/tex]

where s is a Mandelstam variable and [tex]\alpha[/tex] is the fine-structure constant?

Or does one have to resort to:

[tex]\frac{\alpha(s)}{s-\pi(s)}[/tex]

where [tex]\pi[/tex] is the electromagnetic interaction of the photon with itself (the self-energy)?

Can one modify the fine structure constant to incorporate [tex]\pi(s)[/tex] by defining the new fine structure constant [tex]\alpha'(s)[/tex] as the value that makes the following equation true:

[tex]\frac{\alpha'(s)}{s}=\frac{\alpha(s)}{s-\pi(s)}[/tex]
 

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