Deriving Coulomb's Law with Virtual Photon Exchange Theory: Complete Explanation

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SUMMARY

The discussion focuses on deriving Coulomb's Law using the virtual photon exchange theory, emphasizing that a complete derivation can be achieved without perturbation theory. It highlights the use of the Coulomb gauge and the A°=0 gauge, where the inverse of the Laplacian (1/Δ) is constructed. The derivation leads to an interaction term represented as V ∼ ∫ d³x d³y (ρ(x)ρ(y)/|x-y|), confirming the relationship between charge density and electrostatic potential.

PREREQUISITES
  • Understanding of Coulomb's Law and electrostatic fields
  • Familiarity with virtual photon exchange theory
  • Knowledge of gauge theories, specifically Coulomb and A°=0 gauges
  • Basic concepts of differential equations and the Laplacian operator
NEXT STEPS
  • Study the derivation of the Poisson equation in electrostatics
  • Explore the mathematical properties of the Laplacian operator and its inverse
  • Learn about gauge invariance and its implications in quantum field theory
  • Investigate the role of virtual particles in quantum electrodynamics (QED)
USEFUL FOR

This discussion is beneficial for physicists, particularly those specializing in quantum field theory, as well as students and researchers interested in the mathematical foundations of electrostatics and gauge theories.

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How the virtual photon exchange theory be used to derive completely Coulombs Law related to electrostatic field? Complete derivation means derivation involving charges and distance
 
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http://www.scribd.com/doc/70796478/97/The-Coulomb-Potential
 
You don't need any virtual photons but you can derive Coulombs law w/o using perturbation theory. It's most transparent in
a) Coulomb gauge or in
b) A°=0 gauge plus fixing of the residual symmetry of time-independent transformations respecting A°=0.

In both cases it boils down to construct the inverse of the Laplacian 1/Δ; in Coulomb gauge this is due to the Poisson equation

\Delta A^0 = \rho

with

\Delta^{-1} \to k^{-2}

in k-space and

\Delta^{-1} \to |x|^{-1}

in x-space

This results in an interaction term

V \sim \int d^3x\,d^3y\,\frac{\rho(x)\,\rho(y)}{|x-y|}

Of course there are other interaction terms involving physical (transversal) photons as well.
 
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