Relativistic Quantum Field Theory I

Classical fields to canonical quantisation, path integrals and QED.

What this course covers

  • Quantum Field Theory as a Discipline
  • QFT as Quantum Mechanics with Infinite Degrees of Freedom
  • Building Intuition Through Examples and Practice
  • Connecting Formalism to Concrete Physical Problems
  • Principle of Locality
  • Fields as Mathematical Realization of Locality
  • Local Equations and Maxwell's Equations
  • Minkowski metric convention
  • Fields as infinite degrees of freedom
  • Lagrangian density and local action
  • Canonical momentum density and Hamiltonian density
  • Free scalar field theory
  • Definition of symmetry in field theory
  • Spacetime symmetries: translations and Lorentz invariance
  • Continuous vs. discrete symmetries
  • Infinitesimal form of continuous symmetries
  • Noether's theorem: symmetry implies conservation law
  • Global vs. local (gauge) symmetries
  • Noether's Theorem and Conserved Currents
  • Klein-Gordon Equation as Relativistic Wave Equation
  • Klein-Gordon Equation as Classical Field Equation
  • Difficulties of Relativistic Quantum Mechanics
  • Quantum Field Theory as the Resolution
  • Field Theory from Discrete Systems: Continuum Limit
  • Quantization of the Harmonic Oscillator
  • Klein-Gordon field quantization review
  • Canonical commutation relations
  • Commutation relations for mode operators
  • QFT as infinite harmonic oscillators
  • Hamiltonian in terms of mode operators
  • Zero-point energy divergence
  • Time independence of the Hamiltonian
  • Conserved momentum from spatial translation
  • Conserved currents and charges in classical field theory
  • Conserved charges as quantum operators
  • Conserved charge as a symmetry generator
  • Operator ordering ambiguity in quantum field theory
  • Proof of the generator relation for the restricted case
  • Time translation and the Hamiltonian as a generator
  • Finite symmetry transformations via exponentiation of charges
  • Propagator in non-relativistic quantum mechanics
  • No position operator in QFT
  • Lorentz covariance obstruction to localized states
  • Approximate position states via the field operator
  • Wave function analog in QFT
  • Two-point correlation functions G⁺ and G⁻
  • Retarded and advanced Green's functions
  • Feynman propagator G_F
  • Commutativity of fields at spacelike separation
  • Propagator and its two interpretations
  • Feynman propagator as time-ordered correlator
  • Poles of the propagator in momentum space
  • Contour prescriptions for retarded, advanced, and Feynman propagators
  • Iε prescription as an equivalent contour shift
  • General N-point vacuum correlation functions
  • Composite operators and ultraviolet divergences
  • S-matrix and scattering amplitude
  • LSZ theorem and correlation functions
  • Perturbation theory in the coupling constant
  • Naive perturbative expansion of correlation functions
  • Interaction picture
  • Path integral formulation of quantum mechanics
  • Path integral formulation of quantum mechanics
  • Mathematical definition of the path integral
  • Free particle as a Gaussian path integral
  • Generalization to multiple degrees of freedom
  • Path integral in quantum field theory
  • Field theory path integral measure D[φ]
  • Free scalar field theory as Gaussian path integral
  • Time-ordered correlation functions in the path integral
  • Path integral formula for correlation functions
  • Motivation for the generating functional
  • Generating function in one dimension
  • Recovering moments by differentiation
  • Generating functional Z[J] for path integrals
  • Functional derivative and its delta-function rule
  • n-point functions from Z[J] via functional derivatives
  • Z[J]/Z[0] as a time-ordered exponential
  • Power-series expansion of the time-ordered exponential
  • Harmonic oscillator as a worked example
  • Path integral master formula
  • Splitting action into free and interacting parts
  • Interacting correlators from free-theory correlators
  • Perturbative expansion in the interaction
  • Applying Wick's theorem to evaluate terms
  • Feynman diagrams as diagrammatic bookkeeping
  • Combinatorial (symmetry) factors
  • Disconnected and vacuum bubble diagrams
  • Feynman rules for λφ⁴ theory
  • Perturbative expansion of the interacting n-point function
  • Wick's theorem and Feynman diagrams as computational tools
  • Structure of diagrams for the numerator (star)
  • Vacuum diagrams and the denominator (star star)
  • Cancellation of vacuum bubbles in the ratio
  • Connected vs. disconnected Feynman diagrams
  • Momentum-space correlation functions and on-shell limit
  • Generalization to multiple interaction terms and multiple fields
  • LSZ reduction formula
  • Sign convention for initial vs. final state momenta
  • Truncation of external propagators
  • Field-strength renormalization constant Z
  • Motivation for the Dirac equation
  • Dirac's minimal requirement: plane-wave solutions
  • Clifford algebra conditions on Dirac matrices
  • Four-dimensional matrix representations of Dirac matrices
  • Dirac Equation and Spinor Space
  • Gamma Matrix Algebra (Clifford Algebra)
  • Hermiticity Properties of Gamma Matrices
  • Lorentz Covariance of Field Equations
  • Lorentz Transformation of the Vector Field
  • Spinor Field Transformation Law and the Matrix S(Λ)
  • Covariance Condition: S γ^μ S⁻¹ = Λ^μ_ν γ^ν
  • Infinitesimal Lorentz Transformations and the Spinor Generator σ^{μν}
  • Dirac equation plane wave solutions
  • Rest-frame method for U and V
  • Lorentz-boost method for general momentum
  • Algebraic shortcut using (K̸)² = K²
  • Normalization and orthogonality of spinors
  • Explicit spinor components in Dirac representation
  • Non-relativistic limit of Dirac spinors
  • Ultra-relativistic limit and linear dependence of U and V
  • Spinor projection operators
  • Failure of canonical commutator quantization for Dirac field
  • Canonical anti-commutation relations for Dirac field
  • Self-consistency of the anti-commutation relation
  • Mode expansion of the Dirac field
  • Anti-commutation relations for mode operators
  • Positive-definite Hamiltonian from anti-commutation
  • Conserved charge and particle/anti-particle interpretation
  • Fermionic harmonic oscillator
  • Pauli exclusion principle from anti-commutation
  • Spin-statistics theorem
  • Dirac spinor Lorentz transformation
  • Reducing spinor components under Lorentz symmetry
  • Chiral (Weyl) representation of gamma matrices
  • Left- and right-handed chiral spinors
  • Mass as the reason for four-component spinors
  • Gamma-5 matrix and its properties
  • Chiral projection operators P_L and P_R
  • Lorentz invariance of chiral subspaces via γ^5
  • Discrete symmetries: P, T, and C
  • Quantum implementation via unitary operators
  • Time reversal requires an anti-unitary operator
  • Anti-linear operators and their properties
  • Anti-unitary operators
  • Unitary implementation of P, T, C in scalar QFT
  • Intrinsic parity phases: scalars vs. pseudo-scalars
  • Action of parity on creation/annihilation operators
  • Grassmann variables and anti-commutativity
  • Taylor expansion of Grassmann functions
  • Differentiation of Grassmann variables
  • Integration rules for Grassmann variables
  • Gaussian integrals over real Grassmann variables
  • Complex Grassmann variables
  • Gaussian integrals over complex Grassmann variables
  • Generating functional with linear source terms
  • Two-point function from Grassmann generating functional
  • Dirac field as Grassmann-valued field
  • Path integral for the Dirac field
  • Classical Maxwell Lagrangian
  • Maxwell Equations from Euler-Lagrange
  • Current Conservation from Antisymmetry
  • Gauge Symmetry of the Maxwell Action
  • Lorenz gauge action and equation of motion
  • Polarization vectors for the gauge field
  • Canonical quantization of the gauge field
  • Negative-norm states from timelike polarization
  • Too many degrees of freedom in naive quantization
  • Path integral formulation and the propagator kernel
  • Non-invertibility of the Maxwell kernel due to gauge symmetry
  • Gauge fixing in the path integral via delta functional
  • Physical Hilbert space: eliminating unphysical states
  • QED Lagrangian construction
  • U(1) global symmetry and Noether current
  • Coupling fermions to photons via J_mu
  • Electric charge as coupling constant
  • Covariant derivative D_mu
  • Local (gauge) symmetry of QED
  • Gauge principle as a dynamical principle
  • Gauge symmetry in all fundamental interactions
  • Relativistic cross section: setup and requirements
  • Cross section defined via transition probability and incident flux
  • S-matrix element and scattering amplitude M_{αβ}
  • Squaring the delta function: spacetime volume V·T
  • Single-particle state normalisation with plane waves
  • Lorentz-invariant phase space (LIPS) measure dμ
  • Final relativistic cross section formula σ_{αβ} = |M|²/4Σ · dμ
  • Mandelstam variable s and the kinematic factor Σ
  • Centre-of-mass frame and momentum p_{CM}
  • Differential cross section for 2→2 scattering in the CM frame
  • Particle decay rate Γ and lifetime
  • Spin sums: averaging over initial and summing over final polarisations
  • E⁺E⁻ annihilation as a particle discovery tool
  • Discovery of the J/ψ and charm quark evidence
  • R-ratio and evidence for quark color
  • Feynman amplitude for e⁺e⁻ → B B̄
  • Spin averaging and summing for unpolarized cross section
  • Squaring the amplitude and taking the complex conjugate
  • Trace trick for evaluating spin sums
  • Spin-sum completeness relations for Dirac spinors
  • Cross section divergence at threshold velocity
  • Crossing symmetry between related processes
  • Momentum relabeling between crossed processes
  • Wave functions for particles vs. antiparticles (u vs. v spinors)
  • Spin-sum identity restoring crossing for unpolarized amplitudes
  • Field-theoretic origin of crossing symmetry
  • Tree-level diagrams in QED
  • Loop diagrams and free momentum integration
  • UV divergences from loop integrals
  • Divergences as signals of unknown short-distance physics
  • Vacuum fluctuations from loop diagrams
  • Bare vs. physical parameters
  • Electron self-energy and mass renormalization
  • Field renormalization
  • Charge renormalization and gauge symmetry preservation
  • Anomalous magnetic moment of the electron

Syllabus

  1. Lectures

    1. Lecture 1: Classical Field Theories and Principle of Locality
    2. Lecture 2: Symmetries and Conservation Laws
    3. Lecture 3: Why Quantum Field Theory
    4. Lecture 4: Canonical Quantization of a Free Scalar Field Theory
    5. Lecture 5: Complex Scalar Field Theory and Anti-Particle
    6. Lecture 6: Propagators and Green Functions
    7. Lecture 7: Interacting Theories and S-Matrix
    8. Lecture 8: Path Integral Formalism for Non-Relativistic Quantum Mechanics
    9. Lecture 9: Path Integral Formalism for QFT; Computation of Time-Ordered Correlation Functions
    10. Lecture 10: Time-Ordered Correlation Functions in Field Theory
    11. Lecture 11: Computation of Correlation Functions in Perturbation Theory and Feynman Diagrams
    12. Lecture 12: More on Perturbation Theory and Feynman Diagrams
    13. Lecture 13: Introducing the Dirac Equation
    14. Lecture 14: Lorentz Covariance of the Dirac Equation
    15. Lecture 15: Classical Solutions of Dirac Equations
    16. Lecture 16: Quantization of the Dirac Theory
    17. Lecture 17: Chiral and Majorana Spinors
    18. Lecture 18: Discrete Symmetries
    19. Lecture 19: Path Integrals of Fermions
    20. Lecture 20: Maxwell Theory and its Canonical Quantization
    21. Lecture 21: Quantum Maxwell Theory (continued)
    22. Lecture 22: Quantum Electrodynamics
    23. Lecture 23: Cross Section and Decay Rate
    24. Lecture 24: Elementary Processes in QED (I)
    25. Lecture 25: Elementary Processes in QED (II)
    26. Lecture 26: Quantum Fluctuations and Renormalization