Foundations and Frontiers of QFT · Vol I
Quantum Field Theory in 20 chapters — from “Why Quantum Field Theory?” to “Effective Field Theory”.
Chapters
- Why Quantum Field Theory?
- A Subject Worth Its Difficulty
- The Klein Paradox: Relativistic Quantum Mechanics Breaks
- Dirac’s Sea and Its Trouble
- The Lamb Shift: An Experiment That Demands QFT
- The Vacuum Has Structure: The Casimir Effect
- Fields vs. Particles: A Preview
- The Road from Here
- Problems
- Chapter 1 Summary
- Classical Fields and the Mathematical Toolkit
- The Lagrangian Perspective, Revisited
- Special Relativity in the Notation We Will Use
- From Particles to Fields: Classical Field Theory
- Symmetries and Noether’s Theorem
- The Electromagnetic Field
- Dimensional Analysis in Field Theory
- Summary and Look Ahead
- Chapter 2 Summary
- Problems
- Groups and Representations
- Groups: What and Why
- Lie Groups and Lie Algebras
- Representations
- The Lorentz Group
- The Poincaré Group
- Summary and Look Ahead
- Problems
- Poincaré Invariance and One-Particle States
- What Is a One-Particle State?
- Wigner’s Strategy: Labels from Symmetries
- Boost, Stabilize, Classify: The Little Group Method
- Massive Particles and Spin
- Massless Particles and Helicity
- The Result: A Short List of Possible Particles
- Why Nature Picks What She Picks
- Summary and Look Ahead
- Problems
- Many-Particle States and Fock Space
- From One Particle to Many
- Occupation-Number Representation
- Creation and Annihilation Operators
- The Fock Space
- Working with Fock States: Some Examples
- What Fock Space Does and Does Not Give Us
- Summary and Look Ahead
- Problems
- Why Fields? From Particles to Fields
- What We Want: A Local, Lorentz-Invariant S-Matrix
- Why Creation and Annihilation Operators Alone Are Not Enough
- The Key Construction: Bundling Operators into a Field
- Microcausality and the Necessity of Antiparticles
- Spin-Statistics, Previewed
- Fields with Spin
- The Weinberg Perspective and What Comes Next
- Summary and Look Ahead
- Problems
- Canonical Quantization of the Free Scalar
- The Faster Route
- From Lagrangian to Hamiltonian for a Field
- Canonical Commutation Relations
- Mode Expansion of the Free Scalar
- The Hamiltonian and the Vacuum
- The Feynman Propagator
- The Casimir Effect, Finally
- Summary and Look Ahead
- Problems
- Quantum Mechanics as 0+1D QFT
- The Dictionary
- The Dimensional Reduction
- Computing the Oscillator Using the QFT Machinery
- Euclidean Time and Thermal Physics
- A First Look at the Renormalization Group
- The Climb of the Dimensional Ladder
- Summary and Look Ahead
- Problems
- Interactions and Perturbation Theory
- What Is an Interaction?
- The Interaction Picture
- The S-Matrix
- Wick’s Theorem, Starting from the Oscillator
- Feynman Diagrams: What They Are and Why They Exist
- Worked Example: Tree-Level Scattering in Phi-Fourth Theory
- The Path from Here to (g-2)
- Summary and Look Ahead
- Problems
- From Amplitudes to Observables
- The Disaster of Squaring a Delta Function
- Lorentz-Invariant Phase Space
- Master Formulas: Cross Sections and Decay Rates
- Fully Worked Example: Scalar-Scalar Scattering
- The Optical Theorem
- A Concrete Sketch of (g-2)
- Summary and Look Ahead
- Problems
- The Path Integral from Scratch
- Why a Second Formulation?
- The Core Idea: Sum Over Paths
- Time-Slicing: From Evolution Operator to Path Integral
- The Euclidean Path Integral
- The Harmonic Oscillator as a Worked Example
- From Quantum Mechanics to Field Theory
- The Generating Functional
- The Classical Limit
- Summary and Look Ahead
- Problems
- Path Integral and Canonical, Compared
- Two Languages, One Physics
- The Two-Point Function, In Both Formulations
- The Translation Dictionary
- When Each Formulation Is Better
- The Places Where the Equivalence Is Subtle
- A Worked Example: Phi-Fourth Tree-Level Amplitude, Redux
- Summary and Look Ahead
- Problems
- Symmetries in the Quantum Theory
- The Master Identity
- Schwinger-Dyson Equations: Classical Equations of Motion, Quantized
- Ward Identities: Noether’s Theorem Quantized
- Anomalies: When the Measure Fights Back
- Ward Identities in Action: QED, Previewed
- A First Encounter with the Anomaly, in 1+1D
- The End of Part III
- Summary and Look Ahead
- Problems
- First Loop Calculations
- What Is a Loop?
- The Tadpole Diagram
- What the Divergence Means
- Power Counting: Which Integrals Diverge?
- Regularization, Briefly
- The Program for Part IV
- Summary and Look Ahead
- Problems
- Regularization Methods Compared
- Why We Want Another Regulator
- Dimensional Regularization: The Idea
- Comparison with Hard Cutoff
- The Dimensional-Regularization Integral Formula
- Pauli-Villars, Briefly
- The Renormalization Scale
- A Subtlety: Chirality and Gamma-Five
- Summary and Look Ahead
- Problems
- The Loop Calculation Toolkit
- The One Master Integral
- Feynman Parameters
- Tensor Reductions
- Example: A One-Loop Vertex Correction
- A Preview: Multi-Loop Integrals
- Summary and Look Ahead
- Chapter 16 Summary
- Problems
- Renormalization of Phi-Fourth: Old School and New
- Two Views of Renormalization
- Counter-Terms and the Bare Lagrangian
- The One-Loop Calculation
- The Pattern of Divergences
- The Renormalization Conditions
- The Wilsonian Reframe
- Summary and Look Ahead
- Problems
- The Renormalization Group
- Why Parameters Run
- The Beta Function
- The Callan-Symanzik Equation
- Fixed Points and Universality
- Relevant, Marginal, and Irrelevant Operators
- Asymptotic Freedom: A Preview of QCD
- Summary and Look Ahead
- Problems
- Spontaneous Symmetry Breaking
- The Phenomenon
- The Simplest Example
- Goldstone’s Theorem, Derived
- The Non-Abelian Generalization
- The Higgs Mechanism
- Exceptions: No Goldstones in Low Dimensions
- Summary and Look Ahead
- Chapter 19 Summary
- Problems
- Effective Field Theory
- The Core Insight
- Fermi’s Theory as the Canonical Example
- Einstein Gravity as an Effective Field Theory
- The Decoupling Theorem
- EFT Matching: The Procedure
- The Standard Model as an EFT
- A Retrospective, and the View Forward
- Summary and Look Ahead
- Problems