Canonical Quantization
From classical fields to quantum operators: Creating and annihilating particles
πCourse Connections
π― 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 ΟΜ(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] = iβ
- β’ States: |Οβ© in Hilbert space
- β’ Particles: Fixed number
Quantum Field Theory
- β’ Observable: field Ο(x,t)
- β’ Quantize: Ο β ΟΜ
- β’ Commutator: [ΟΜ(x), ΟΜ(y)] = iδ³(x-y)
- β’ States: |n,kβ© in Fock space
- β’ Particles: Variable number!
Chapter Roadmap
1. Quantization Procedure
Canonical commutation relations, promoting fields to operators, equal-time commutators
2. Free Scalar Field
Mode expansion, creation/annihilation operators, vacuum energy, normal ordering
3. Fock Space & Particle States
Multi-particle states, occupation number basis, creation/annihilation algebra
4. Propagators & Green's Functions
Feynman propagator, time-ordering, causality, i prescription
5. Quantizing the Dirac Field
Fermionic anticommutators, Pauli exclusion, spinor modes, antiparticles
6. Spin-Statistics Theorem
Why bosons commute and fermions anticommute, connection to spin
7. Photon Field Quantization
Gauge fixing, polarization vectors, transverse modes, QED vacuum
π Key Concepts
- Fields become operators: Ο(x,t) β ΟΜ(x,t)
- Canonical commutation relations: [ΟΜ(x), ΟΜ(y)] = iδ³(x-y)
- Particles are quanta: excitations of the quantum field
- Fock space: states with definite particle number |n,kβ©
- Creation operators Γ’β k create particles with momentum k
- Annihilation operators Γ’k destroy particles
- Vacuum |0β©: lowest energy state (not empty!)
- Propagators: β¨0|T{`ΟΜ(x)ΟΜ(y)`}|0β© describe particle propagation