SUMMARY
The global U(1) invariance of the Dirac Lagrangian corresponds to different conserved quantities depending on the specific Lagrangian in use. For charged particles, this typically represents charge conservation, while for uncharged particles like neutrinos, it corresponds to neutrino number conservation. The hermiticity of the Hamiltonian can break this symmetry, particularly in cases where the Lagrangian does not support U(1) symmetry, such as when dealing with real scalar fields. In the context of the Standard Model, the relevant invariants include lepton number and baryon number, each associated with separate U(1) symmetries.
PREREQUISITES
- Understanding of Dirac Lagrangian and its formulation
- Knowledge of U(1) symmetry in quantum field theory
- Familiarity with the concept of hermitian operators in quantum mechanics
- Basic principles of particle physics, including lepton and baryon numbers
NEXT STEPS
- Study the implications of U(1) symmetry in quantum field theories
- Explore the role of hermitian operators in quantum mechanics
- Investigate the differences between Dirac and Majorana mass terms
- Review Srednicki's text on quantum field theory for deeper insights
USEFUL FOR
Particle physicists, theoretical physicists, and students studying quantum field theory who are interested in the implications of symmetries in Lagrangian formulations.