First, why Field Theory?
- We need a consistent quantum treatment of relativistic particles.
- Our theory should be local and causal (since nature is).
- Our theory should allow for a dynamical number of particles.
With a QFT (Quantum …), we can treat all particles on the same footing, with a common framework (spin-statistics relation emerges). It becomes the language to formulate our most fundamental theory of nature. It also supports a consistent, low energy theory for quantum gravity (our next to last theory).
But, how do we build a QFT?
- Dynamics: Review Lagrangian and Hamiltonian mechanics and apply it to fields.
- Quantise: Implement canonical commutation relations.
- Interpret: Introduce Fock Space and identify familiar operators.
Before delving, check Conventions
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