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