Part II Overview

Canonical Quantization

From classical fields to quantum operators: Creating and annihilating particles

🎯 What You'll Learn

Canonical quantization is the bridge between classical and quantum field theory. We promote classical fields Ο†(x,t) to quantum operators Ο†Μ‚(x,t) that satisfy commutation relations, just like in quantum mechanics.

The revolutionary insight: particles are excitations of quantum fields! What we call "particles" are actually quanta - discrete energy bundles of the underlying field.

The Big Picture

In Part I, we studied classical fields described by Lagrangians. Now we quantize these fields to create a quantum theory. The process mirrors what you learned in quantum mechanics:

Quantum Mechanics

  • β€’ Observable: position x(t)
  • β€’ Quantize: x β†’ xΜ‚
  • β€’ Commutator: [xΜ‚, pΜ‚] = iℏ
  • β€’ States: |ψ⟩ in Hilbert space
  • β€’ Particles: Fixed number

Quantum Field Theory

  • β€’ Observable: field Ο†(x,t)
  • β€’ Quantize: Ο† β†’ Ο†Μ‚
  • β€’ Commutator: [Ο†Μ‚(x), Ο€Μ‚(y)] = iδ³(x-y)
  • β€’ States: |n,k⟩ in Fock space
  • β€’ Particles: Variable number!

Chapter Roadmap

πŸ”‘ Key Concepts

  • Fields become operators: Ο†(x,t) β†’ Ο†Μ‚(x,t)
  • Canonical commutation relations: [Ο†Μ‚(x), Ο€Μ‚(y)] = iδ³(x-y)
  • Particles are quanta: excitations of the quantum field
  • Fock space: states with definite particle number |n,k⟩
  • Creation operators Ò†k create particles with momentum k
  • Annihilation operators Γ’k destroy particles
  • Vacuum |0⟩: lowest energy state (not empty!)
  • Propagators: ⟨0|T{`Ο†Μ‚(x)Ο†Μ‚(y)`}|0⟩ describe particle propagation