QED, chapter 4 P&S page 125 (Coulomb Potential)

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SUMMARY

The discussion centers on the properties of Dirac spinors in quantum electrodynamics (QED), specifically in chapter 4 of the text. The equation $$\bar u(p') \gamma^i u(p) = u^\dagger(p') \gamma^0 \gamma^i u(p)$$ is established as a fundamental relationship. When the momentum vectors are equal (##p = p'##), the identity $$u^\dagger(p) u(p) = 2m \xi^\dagger \xi$$ is utilized to derive properties of the spinors. The query focuses on determining the form of the spinor ##u(p)## when the momentum ##\vec{p}## is zero.

PREREQUISITES
  • Understanding of Dirac spinors and their properties
  • Familiarity with quantum electrodynamics (QED)
  • Knowledge of gamma matrices and their algebra
  • Basic concepts of relativistic quantum mechanics
NEXT STEPS
  • Study the derivation of Dirac spinors in QED
  • Learn about the implications of momentum space in quantum field theory
  • Explore the role of gamma matrices in particle physics
  • Investigate the physical interpretation of spinors at rest (##\vec{p}=0##)
USEFUL FOR

This discussion is beneficial for theoretical physicists, students of quantum mechanics, and anyone studying quantum field theory, particularly those focusing on the properties of fermions in QED.

Pouramat
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Homework Statement
In section Coulomb Potential stated that: "You can easily verify that the other terms mentioned below vanish if ##p = p' = o##"
which we are working in nonrelativistic limit
Relevant Equations
$$\bar u(p') \gamma^i u(p)$$
$$\bar u(p') \gamma^i u(p) = u^\dagger(p') \gamma^0 \gamma^i u(p)$$
if ##p = p'## we can use
$$u^\dagger(p) u(p) = 2m \xi^\dagger \xi$$
but how can we conclude the statement?
 
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What is ##u(p)## when ##\vec{p}=0## ?
 

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