SUMMARY
The discussion focuses on determining the action corresponding to photon emission during an electron transition within Feynman's path integral formulation. Participants clarify that the first-order diagram involves an incoming electron with momentum p and an outgoing electron with momentum (p-k), alongside a photon with momentum k. The action S related to this process does not exist as a standalone entity; instead, it arises from the perturbation expansion of the classical action, primarily through the minimal coupling term (##j_{\mu} A^{\mu}##) that links the electron field to the Maxwell field.
PREREQUISITES
- Understanding of Feynman's path integral formulation
- Knowledge of quantum electrodynamics (QED)
- Familiarity with perturbation theory in quantum mechanics
- Basic concepts of Lagrangian mechanics and action principles
NEXT STEPS
- Study the minimal coupling term in quantum electrodynamics
- Explore perturbation theory applications in QED
- Investigate the role of Feynman diagrams in particle interactions
- Learn about the classical action and its derivation in field theory
USEFUL FOR
Physicists, particularly those specializing in quantum mechanics and quantum field theory, as well as students seeking to deepen their understanding of photon emission processes and Feynman's path integral approach.