Quantum Field Theory I
From free fields to Feynman diagrams, loops and renormalisation
About this course
Canonical quantisation of scalar, Dirac and electromagnetic fields, the S-matrix and Feynman rules, tree-level QED processes, and one-loop renormalisation through to the running coupling and the anomalous magnetic moment.
What you will be able to do
- Quantise free scalar, Dirac and electromagnetic fields and derive their propagators
- Derive Feynman rules from Wick's theorem and the S-matrix
- Calculate tree-level cross sections for Compton scattering and electron-positron annihilation
- Apply crossing, unitarity and the optical theorem to scattering amplitudes
- Regularise and renormalise one-loop divergences and compute the running coupling
What this course covers
- Five borrowed premises and the hour's question
- Relativistic energy-momentum relation and its two roots
- Energy cost of confinement and the reduced Compton wavelength
- Pair-production threshold from halving the box
- Particle number is not conserved; charge is
- The quantum field as the forced object
- Causality preserved by cancellation, not prohibition
- Course outlook: the field's law via stationary action
- The Interaction Picture
- The Cut Is a Choice: Particles Depend on the Split
- Time-Ordering and the Exponential Approximation
- Linear Coupling: One Switching Priced
- Three Assumptions Behind 'Free at Both Ends'
- Ordering Costs More Than a Phase for Non-Linear Couplings
- The S-Matrix and What It Actually Says
- The divergent loop sum introduced
- Volume of shells in four-dimensional momentum space
- Pricing one term: the cancellation of sixteen against sixteen
- The superficial degree of divergence
- Nested-diagram failure of the naive count
- Exact cancellation and the list of two divergent shapes
- The bracket that decides renormalisability
- Why two Feynman diagrams are required
- Gauge test: two diagrams form one object
- Compton wavelength shift (kinematics)
- Classical radius as a length from charge and mass
- Klein-Machina differential cross-section
- Forward-direction identity at all energies
- Total cross-section, Thomson limit, and numerical result
- Feynman diagram enumeration for electron-positron annihilation
- Conservation laws and rest-mass non-conservation
- Angular distribution of the squared amplitude
- Annihilation cross-section and its energy dependence
- The R-ratio: a dimensionless count of quark charges
- Quark color: three copies per charge from the R-ratio staircases
- Residual excess and what the calculation leaves open
- Regularization: the cost of stopping a divergent sum
- Scheme-dependence: the gap between two stopping methods
- Separation of the answer into two brackets
- Scheme-independence of the energy-dependent bracket
- Symmetry breaking by a sharp cutoff: the rename test
- The unabsorbed bracket and the next problem
- Normal ordering and the contraction of two fields
- The contraction as a propagator with time-ordering signature
- Wick's theorem: pairing expansion for many fields
- Counting complete pairings: the double-factorial ladder
- Feynman diagrams as classes of pairings
- The full theorem away from the vacuum: incomplete pairings
- Disconnected diagrams and vacuum cancellation
- The Action as a Single Number for a Field History
- Stationary Action and Which History the Field Takes
- Deriving the Euler–Lagrange Field Equation
- Relativistic Dispersion Relation as a Derived Result
- Noether's Theorem: Symmetry Yields a Conserved Current and Charge
- Symmetry Breaking, Current Ambiguity, and the Classical Charge's Limits
- Counting terms: splitting four legs into pairs
- Three invariants on one kinematic plane
- Reality and complexity of the amplitude
- Unitarity bound and the circle in the complex plane
- The unitarity ceiling on cross-section
- Optical theorem: forward amplitude encodes total cross-section
- Interconnection of channels via the total width
- The unmeasured split: written-down value vs. instrument reading
- Written-down value's dependence on stopping point
- Spending one measurement: stopping point leaves all predictions
- Three theories, one curve: parallel shift under stopping-point change
- The same move applied to the charge
- Counting purchased measurements: renormalizability
- Written-down values are scheme-dependent, not merely unknown
- What this hour settles and what it hands on
- Field as a collection of independent modes
- Quantizing one harmonic oscillator: zero-point energy
- Particles as ladder rungs; indistinguishability from the ladder
- Vacuum energy divergence
- Boundary dependence makes vacuum energy observable
- Casimir effect — finite attractive pressure between plates
- What the Casimir measurement does and does not prove
- Dimensional analysis of the coupling constant
- Vertex factor and the half-cancellation
- Rate as a slope over a continuum of end states
- Identical-particle factor of one-half
- Phase-space measure after conservation conditions
- Four-factor decay rate and dimensional ledger
- Three readings of the decay rate and limits of first-order perturbation theory
- The running coupling: charge depends on distance
- Vacuum polarization as the screening mechanism
- The beta function: rate of running per decade
- Particle thresholds and slope steps
- Reading the particle count from the curve
- The quark contribution: calculated vs. measured blocks
- Recovery of the collider R-ratio and the Landau pole
- Causality as a commutator condition
- Normalization of the equal-time commutator
- Commutator as a difference of two amplitudes
- Lorentz boost reversing spacelike separations
- Commutator behaviour inside vs outside the light cone
- The Feynman propagator: time-ordered amplitude and pole prescription
- Propagator outside the light cone and limits of the result
- Five given foundations of the calculation
- The anomalous magnetic moment and its measurement
- The one-loop vertex correction: the central derivation
- Mass independence of the one-loop result
- Higher-order corrections and the perturbative ladder
- What limits the comparison: the charge measured elsewhere
- The even perturbative ladder and its spacing
- Borrowed results and the spin-half setup
- Energy of the spin-half field and the reversed-order problem
- The anti-commutator repair and its cost: negative-length states
- The causality test: bracket of fields outside the light cone
- Odd vs. even amplitude combinations and bracket selection
- The spin-statistics connection: the two-by-two table
- Exclusion principle as a consequence of the anti-commutator
- The electromagnetic operator's universal singularity
- Redundancy versus symmetry
- Gauge fixing and residual freedom
- Polarisation count on the light cone
- Cavity counting as independent verification
- Gauge-fixed propagator and the gauge parameter
- Measurement over algebra as an epistemic principle
- Five foundational loans from prior hours
- Experimental measurement of the Lamb shift
- Degeneracy of hydrogen 2S and 2P½ levels in the Dirac formula
- Vacuum jitter shifts only the level that reaches the nucleus
- The basic unit of the Lamb shift calculation
- Logarithmic structure of the jitter sum and the objection answered
- Vacuum charge screening lowers the shifted level
- Anomalous magnetic moment contributions to both levels
- The full one-loop Lamb shift ledger and its result
- What remains in the half-percent gap
- Cross-check via the ground-state Lamb shift ratio
- Why a radio receiver, not a spectrograph
Syllabus
Free Fields
- L1 · Why Fields Are Forced
- L2 · The Classical Field and Its Action
- L3 · Quantising the Free Scalar
- L4 · Causality and the Propagator
- L5 · The Dirac Field, Quantised
- L6 · The Electromagnetic Field, Quantised
Interactions and Feynman Rules
- L7 · Interactions and the S-Matrix
- L8 · Wick's Theorem and the Feynman Rules
- L9 · The First Diagram, End to End
Tree-Level Processes
- L10 · Compton Scattering
- L11 · Electron-Positron Annihilation
- L12 · Crossing, Unitarity, the Optical Theorem
Loops and Renormalisation
- L13 · Loops, and Where the Infinity Comes From
- L14 · Regularisation
- L15 · Renormalisation, and What “Measured” Means
- L16 · The Running Coupling
- L17 · The Anomalous Magnetic Moment
- L18 · The Lamb Shift, and What the Vacuum Does