Prerequisites
Sources
Kittel, Introduction to Solid State Physics
Ashcroft and Mermin, Solid State Physics
Prerequisites and outcomes
This note assumes introductory quantum mechanics, thermodynamics, electromagnetism, and vectors. By the end, you should be able to move between lattice, phonon, band, and continuum models, identify the assumptions behind each model, and relate measurable transport or diffraction data to microscopic structure.
1. What condensed matter physics studies
Condensed matter physics explains how large collections of atoms and electrons produce the properties of solids, liquids, and structured materials. The central challenge is connecting microscopic interactions to collective behavior.
Core ideas
Crystal structure determines symmetry, defects, and many material properties.
Quasiparticles provide useful descriptions of collective excitations.
Band structure explains electrical and optical behavior.
Temperature, pressure, disorder, and fields can drive phase transitions.
2. Crystal structure
The lattice is an ideal periodic reference; a real crystal also has a basis and defects. Keep those roles separate when interpreting a diffraction or transport problem.
A crystal is described by a lattice and a basis. Primitive translation vectors generate equivalent points:
The reciprocal lattice is useful for diffraction and band theory. Constructive diffraction follows Bragg's law:
Real crystals contain vacancies, interstitials, substitutional impurities, dislocations, and grain boundaries. Defects can dominate diffusion, strength, conductivity, and optical response.
3. Phonons and thermal properties
Lattice vibrations are quantized as phonons with energy
At long wavelength, acoustic phonons behave like sound waves. Optical phonons occur when a unit cell has multiple atoms moving relative to one another. Heat capacity, thermal conductivity, and expansion depend on the phonon spectrum and scattering from boundaries, defects, and other phonons.
4. Electrons in solids
Periodic potentials split atomic levels into bands. The Fermi–Dirac distribution is
Materials are commonly classified by the relationship between the Fermi level and available states:
| Material | Electronic picture | Typical behavior |
|---|---|---|
| Metal | Partially filled band or overlapping bands | High electrical conductivity |
| Semiconductor | Small band gap | Conductivity increases with temperature or doping |
| Insulator | Large band gap | Very low ordinary conductivity |
For a simple carrier model,
Doping creates donors or acceptors and changes carrier concentration. In a magnetic field, moving charges experience the Lorentz force and can produce a Hall voltage.
5. Magnetism and phase transitions
Diamagnetism opposes an applied field; paramagnetism comes from unpaired moments; ferromagnetism supports spontaneous alignment. Antiferromagnets and ferrimagnets have ordered but opposing sublattices.
Superconductors exhibit zero DC resistance and magnetic flux expulsion below a critical temperature. Their behavior is limited by critical field, current, and temperature.
Near a continuous phase transition, fluctuations become important and macroscopic properties often follow power laws. Order parameters distinguish phases, while symmetry breaking explains why phases have different properties.
6. Problem-solving workflow
Identify the structure, carriers, or collective mode involved.
Decide whether a microscopic, band, lattice, or continuum model is appropriate.
State approximations such as low temperature, weak disorder, or parabolic bands.
Check dimensions and compare the result with the relevant energy or length scale.
Summary
Condensed matter physics is organized around structure, excitations, and collective behavior. Diffraction probes structure, transport probes motion, and thermodynamic or magnetic measurements reveal phases and transitions.