Introduction to Condensed Matter Physics
Many-body methods for superconductors, magnets and topological matter
About this course
The many-body treatment of solids — second quantisation, Fermi liquids, screening and electron-phonon coupling — applied to superconductivity, magnetism, phase transitions and the renormalisation group, localisation, and quantum Hall and topological phases.
What you will be able to do
- Use second quantisation and the tight-binding model to describe electrons in solids, including graphene
- Explain Fermi-liquid quasiparticles and compute screening from linear response
- Derive the BCS gap and use Ginzburg–Landau theory to describe vortices and Josephson junctions
- Analyse phase transitions with order parameters, critical exponents and the renormalisation group
- Explain the quantum Hall effects and topological insulators in terms of the Berry phase
What this course covers
- Fock Space and Occupation-Number Representation
- Creation, Annihilation Operators and Pauli Algebra
- Jellium Hamiltonian
- Hartree-Fock Energy of the Electron Gas
- The Exchange Hole
- Correlation Energy and Its Numerical Values
- Two-Site Hubbard Model and Mott Localization
- Cooper's Problem: Bound State for Any Attraction
- BCS Ground State and the Gap Equation
- BCS Wave Function and Particle-Number Superposition
- Bogoliubov Quasiparticles and the Density of States
- Condensation Energy and the Critical Field
- Heat Capacity Jump and Coherence Length
- Full Worked Example: Aluminum from λ to Four Measurements
- Exchange interaction: Coulomb plus antisymmetry
- The Heisenberg Hamiltonian and ferromagnetic ground state
- Holstein-Primakoff bosons and spin-wave dispersion
- Bloch's T^(3/2) law and Mermin-Wagner theorem
- Antiferromagnetic spin waves and limits of the Heisenberg model
- Stoner criterion for itinerant ferromagnetism
- EuO worked example: exchange constants to TC, D, and moment loss
- Anderson Localization and the Transfer Matrix
- Dimensionality Dependence of Localization
- Scaling Theory of Localization and the Beta Function
- Mott's Criterion for the Metal–Insulator Transition
- Variable-Range Hopping and Finite-Temperature Localization
- The Mott Insulator and the Hubbard Dimer Gap
- Worked Example: Phosphorus in Silicon
- Landau mean-field critical exponents
- Failure of mean-field below four dimensions
- Onsager's exact 2D Ising solution
- Monte Carlo simulation and Binder cumulant
- Scaling relations and universality classes
- Ginzburg criterion and mean-field validity
- Van der Waals fluid as a mean-field critical point
- Tight-binding Hamiltonian and Bloch diagonalization
- 1D chain: band, effective mass, and density of states
- Square lattice: band, van Hove singularity, and Fermi surface
- Graphene: two-band Hamiltonian and Dirac cone
- Graphene as a semi-metal: DOS and gate-controlled carriers
- SSH chain: alternating bonds, bulk gap, and topological edge states
- Graphene worked example: numbers from one hopping
- Landau Levels and Filling Factor
- Integer Quantum Hall Effect and Disorder
- Laughlin's Gauge Argument for Exact Quantization
- Chiral Edge States and Zero Longitudinal Resistance
- Fractional Quantum Hall Effect and Laughlin's Wave Function
- Worked Example: GaAs Hall Bar from Density to Plateaus
- Topological Nature of the Quantized Hall Conductance
- Ginzburg-Landau Free Energy Functional
- Kappa and the Type-I / Type-II Boundary
- The Vortex: Topology, Flux Quantum, and Line Energy
- GL Theory: Scope, Limits, and Place in Condensed Matter
- Lower and Upper Critical Fields and Abrikosov's Lattice
- Josephson Effect and AC Voltage–Frequency Relation
- Worked Example: NbTi MRI Magnet
- Coarse graining and the renormalization group idea
- Exact decimation of the Ising chain
- Fixed points, critical points, and universality
- Exponents as formulas in y_T and y_H
- Gaussian fixed point and the upper critical dimension
- Universality classes and superfluid helium
- End-to-end worked example: 2D Ising by Migdal–Kadanoff
- Fermi Liquid: Adiabatic Continuity Premise
- Thermal Mass from Heat Capacity
- Quasiparticle Lifetime: ε² Phase-Space Argument
- Luttinger's Theorem: Fermi Surface Volume
- Landau Parameters and Fermi Liquid Responses
- T² Resistance and Kadowaki–Woods Ratio
- Worked Example: Sodium's Thermal Mass Decomposed
- Berry Phase and Berry Curvature
- Quantization of Berry Phase and the Chern Number
- SSH Chain and Winding Number
- Bulk-Boundary Correspondence as a General Principle
- Chern Number and the Quantum Anomalous Hall Effect
- Z₂ Topological Insulators and Bulk-Boundary Correspondence
- Polyacetylene as a Worked Topological Example
- Thomas-Fermi Screening and Screened Coulomb Interaction
- Lindhard Function and the 2k_F Kink
- Friedel Oscillations from the 2k_F Kink
- Plasma Oscillations and Plasmon Dispersion
- Kubo Formula: Linear Response as a Correlation Function
- Kramers-Kronig Relations and the F-Sum Rule
- Sodium Worked Example: Screening, Friedel, and Plasmon
- Hubbard Model at Half Filling and the Mott Gap
- The Kondo Effect: Logarithm and Resistance Minimum
- Kondo Temperature from Poor-Man Scaling
- Heavy Fermions and the Kadowaki-Woods Ratio
- Cuprate Phase Diagram and the Universal Superconducting Dome
- Open Problems: Pseudogap and Quantum Criticality
- Course Synthesis: Fourteen Numbers and Three Habits
- Electron-phonon coupling overview and lambda
- Bloch-Grüneisen phonon resistivity
- Fröhlich's phonon-mediated electron attraction
- The polaron: electron dressed in phonons
- Migdal's theorem and the hidden small parameter
- Peierls instability and lattice dimerization
- McMillan's formula: lambda to T_c
Syllabus
Many-Body Foundations
- L1 · Second Quantisation and the Many-Body Problem
- L2 · The Tight-Binding Model and Graphene
- L3 · Fermi Liquids and Quasiparticles
- L4 · Linear Response, Screening and Plasmons
- L5 · Phonons, Electron-Phonon Coupling and Polarons
Superconductivity
- L6 · BCS Theory of Superconductivity
- L7 · Ginzburg-Landau Theory, Vortices and Josephson Junctions
Magnetism and Phase Transitions
- L8 · Magnetism: Exchange, the Heisenberg Model and Spin Waves
- L9 · Phase Transitions, Order Parameters and Critical Exponents
- L10 · The Renormalisation Group and Universality
Disorder, Topology and Strong Correlation
- L11 · Disorder, Localisation and the Mott Transition
- L12 · The Quantum Hall Effects
- L13 · Topological Insulators and Berry Phase
- L14 · Strongly Correlated Matter, and the Close