Elementary QED Processes II
Møller scattering, crossing symmetry, and the power of Feynman diagrams
🔗Course Connections
📚Prerequisites
Video Lecture
Lecture 25: Elementary Processes in QED (II) - MIT 8.323
Advanced QED processes and crossing symmetry (MIT QFT Course)
💡 Tip: Watch at 1.25x or 1.5x speed for efficient learning. Use YouTube's subtitle feature if available.
5.1 Møller Scattering (e⁻e⁻ → e⁻e⁻)
Electron-electron scattering has both t and u channel diagrams. The electrons are identical fermions, so we must antisymmetrize!
The minus sign comes from fermion exchange (Pauli exclusion principle).
Differential cross section:
5.2 Crossing Symmetry
Crossing relates different physical processes by analytic continuation in Mandelstam variables:
- e⁺e⁻ → μ⁺μ⁻ (s-channel)
- e⁻μ⁻ → e⁻μ⁻ (t-channel)
- e⁻μ⁺ → e⁺μ⁻ (u-channel)
Same amplitude function M(s,t,u) describes all three! Just evaluate in different kinematic regions.
5.3 Photon-Photon Scattering
Photons don't directly couple to each other (ℒint = -eψ̄γμψAμ), but they scatter via virtual electron loop!
This is a one-loop process - quantum correction to classical EM.
💡 Quantum Effects
Photon-photon scattering is pure quantum - no classical analog! It demonstrates:
- Virtual particles have real physical effects
- Nonlinear corrections to Maxwell's equations
- Vacuum polarization (vacuum acts like a medium)
🎯 Key Takeaways
- Møller scattering: Fermion antisymmetrization (Mt - Mu)
- Crossing symmetry: Related processes from same amplitude
- Photon-photon scattering: One-loop quantum effect
- Virtual particles: Contribute to real physical processes
- QED precision: Tree level + loops match experiments
- Next: Loop corrections and renormalization!