Condensed Matter
Condensed Matter in 29 chapters — from “Historical origins” to “The frontier”.
Chapters
- Historical origins
- The puzzle of heat in solids
- Einstein, 1907: a quantum solid
- Sound, waves, and the phonon precursor
- The puzzle of metals in 1900
- Drude: the right answer for the wrong reasons
- Sommerfeld: Fermi statistics restored
- Bloch, Wilson, and the birth of band theory
- How to read this book
- Lattices, reciprocal space, and the Brillouin zone
- Bravais lattices and crystal structures
- Reciprocal space
- The Brillouin zone
- Why reciprocal space?
- Miller indices
- Where this chapter fits
- Scattering and crystal-structure determination
- The scattering geometry
- The lattice sum: the Laue condition
- The Ewald construction
- The basis sum: structure factor and form factor
- Powder diffraction and a worked NaCl example
- What diffraction sees and what it does not
- Inelastic scattering: a preview
- Where this chapter fits
- The free electron gas
- Drude, carefully
- Sommerfeld: Fermi statistics restored
- Pauli paramagnetism
- Thermopower and the Mott formula
- What Sommerfeld still misses
- Heat capacity as the decisive test
- Where this chapter fits
- Bloch’s theorem
- The question, and why it’s hard
- Bloch’s theorem, stated three ways
- The proof, in two lines and then expanded
- Reading the Bloch state
- The empty-lattice construction: parabolas folded into the zone
- Nearly-free electrons and the opening of gaps
- Nearly-free electrons and band gaps
- From Bloch to a calculation
- The gap at the zone boundary
- Reading the gap formula
- Fermi surfaces, free and nearly-free
- Effective mass and band curvature
- Direct, indirect, and the semiconductor zoo
- Where this chapter fits
- Problems
- Tight binding and graphene
- The tight-binding picture
- Multiple orbitals per site
- Graphene: the structure
- Graphene: the tight-binding Hamiltonian
- Dirac cones
- Reading the Dirac Hamiltonian
- Where this chapter fits
- Problems
- Semiclassical dynamics and the Berry phase (I)
- The problem and the regime
- The standard semiclassical equations
- Bloch oscillations: the textbook equations applied
- The Berry phase, introduced geometrically
- Reading the anomalous velocity
- Worked example: cyclotron motion in copper
- Applications: three signatures of Berry curvature
- Where this chapter fits
- Problems
- Phonons in 1D
- The monatomic chain
- The diatomic chain
- Counting modes in 3D and the Brillouin zone
- Specific heat: the Debye model
- Counting modes and what's next
- Problems
- Specific heat
- The problem: Dulong–Petit and its failure
- Einstein's model
- Phonons as quanta: the formal derivation
- Debye's model
- Comparing to experiment
- Electron–phonon coupling
- Resistivity from electron-phonon scattering
- Problems
- Anharmonicity and thermal expansion
- The harmonic approximation and its failures
- The Grüneisen parameter
- Phonon-phonon scattering and thermal conductivity
- Magnetic response of atoms in solids: a first look
- Where this chapter fits
- Problems
- Second quantisationand the interacting electron gas
- Why first quantisation is not enough
- Creation and annihilation operators
- One-body and two-body operators
- The Hamiltonian of interacting electrons
- Dimensional analysis: what scales win?
- From Hubbard to Heisenberg: localised electrons
- Sign of the exchange: ferromagnet or antiferromagnet?
- Mean-field theory of the ferromagnet
- Spin waves: the Holstein–Primakoff approach
- Worked example: 1D Heisenberg ferromagnet
- Where this chapter fits
- Problems
- Screening and the RPA
- The problem: Coulomb is long-ranged
- The Lindhard function
- Screening in the RPA
- Two consequences: Friedel oscillations and plasmons
- When screening fails: the Hubbard model
- The Mott transition: band theory’s failure
- Worked example: half-filled Hubbard at large U gives Heisenberg
- Anderson localisation: insulators from disorder
- Where this chapter fits
- Problems
- Fermi liquid theory
- The puzzle
- Quasiparticles
- The spectral function
- Landau parameters
- Heavy fermions: Fermi liquid theory at the extreme
- Summary and bridge
- Electron-phonon coupling
- The coupling, derived
- The screened potential, in detail
- Three consequences
- Migdal's theorem and why this is tractable
- Where this chapter fits
- Problems
- Local moments and exchange
- Where local moments come from
- Exchange interaction
- The Heisenberg ferromagnet at the simplest level
- Itinerant electrons revisited: RPA, plasmons, and the Stoner instability
- Where this chapter fits
- Problems
- Antiferromagnets and spin waves
- The Néel state is not the ground state
- Antiferromagnetic spin waves
- Frustration: when Néel order isn't even classical
- Where this chapter fits
- Forward look: from magnon exchange to Cooper pairs
- Problems
- Itinerant magnetism and the Stoner criterion
- The puzzle: ferromagnetism in a metal
- The Stoner argument
- Stoner enhancement and Fermi liquid connection
- Spin fluctuations and quantum criticality
- Where this chapter fits
- A parallel instability: London electrodynamics and the Meissner effect
- Ginzburg–Landau theory
- Type I versus Type II superconductors
- Worked example: λ and ξ for lead
- Parallel with the Stoner instability
- Problems
- The Kondo effect
- The puzzle: rising resistivity at low T
- Why a logarithm: a phase-space argument
- The third-order calculation: where the log comes from
- Poor man's scaling
- The resistivity minimum
- Worked example: TK for Fe in Cu
- The Anderson model and Schrieffer–Wolff
- The Kondo lattice and heavy fermions
- Where this chapter fits
- Problems
- Ginzburg–Landau theory
- The order parameter
- The Landau free energy
- Spatial variations: the GL functional
- Two-component order parameters and superconductivity
- The Ginzburg criterion
- Interlude: the Anderson and Kondo problems
- The Schrieffer–Wolff transformation
- Three regimes: Kondo, Anderson, mixed valence
- Worked example: low-T crossover in heavy fermions
- Where this chapter fits
- Problems
- BCS superconductivity
- The Cooper instability
- The BCS Hamiltonian and gap equation
- The temperature-dependent gap and thermodynamics
- Tunnelling spectroscopy: the BCS density of states
- Coherence factors and the Hebel-Slichter peak
- Meissner effect
- The isotope effect
- Strong coupling: Eliashberg theory
- The Josephson effect and flux quantization
- Two superconductors connected weakly
- Flux quantization
- The SQUID: applications of the Josephson effect
- Where this chapter fits
- Problems
- Superfluidity
- Bose–Einstein condensation
- The Landau criterion
- The two-fluid model
- Charged bosons in a magnetic field: a preview of Landau levels
- Where this chapter fits
- Problems
- Charge density waves
- The Peierls instability
- The Kohn anomaly and 2kF phonon softening
- Pinning and sliding
- Interlude: the Hall effect as a probe of broken-symmetry order
- Semiclassical Hall effect in a band metal
- The anomalous Hall effect
- Worked example: the Hall coefficient of copper at 300 K
- Where this chapter fits
- Problems
- The integer quantum Hall effect
- Landau levels
- The Hall conductance and its quantisation
- The Laughlin argument
- The TKNN formula: Hall conductance from Kubo
- Worked example: the ν=1 plateau
- The role of disorder
- Where this chapter fits
- Problems
- The fractional quantum Hall effect
- Why interactions matter
- The Laughlin wavefunction
- Fractional charge
- Composite fermions
- The 5/2 state and non-Abelian statistics
- Where this chapter fits
- Problems
- Topological insulators
- Time reversal and Kramers pairs
- The Z2 invariant in 2D
- The Kane-Mele model
- The BHZ model and HgTe quantum wells
- Three-dimensional topological insulators
- Worked example: the Bi2Se3 surface state
- Beyond the basic TI
- Weyl and Diracsemimetals
- Berry phase and Berry curvature: a working toolkit
- Weyl points
- Berry monopoles
- Fermi arcs and bulk-boundary correspondence
- The chiral anomaly
- Dirac semimetals
- Where this chapter fits
- Problems
- The frontier
- Twisted bilayer graphene
- Spin liquids
- Strange metals and non-Fermi liquids
- Quantum simulation with cold atoms
- Topological superconductors
- Topological quantum computation
- Closing remarks