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Condensed Matter Physics

Condensed matter physics asks what happens when you bring 10²³ atoms together and let them settle. The answer is almost never the sum of the parts — order, rigidity, conduction, and magnetism are collective properties that no single atom possesses.

FIG_002
Ekconductionvalence
EgE_g
Band theory: a filled valence band and an empty conduction band, split by a forbidden gap Eg.

The starting point is structure. Most solids are crystals — atoms arranged on a periodic lattice — and that periodicity is the single fact from which nearly everything else follows. Choose a unit cell and a basis, and the reciprocal lattice hands you the natural language for waves inside the solid.

Periodicity reshapes the electrons. In a periodic potential the allowed energies collect into bands separated by gaps, and where the last electrons land — mid-band or at a band edge — decides whether a material is a metal, an insulator, or a semiconductor.

FIG_003
vv
λ\lambda
A phonon: a quantized lattice vibration travelling through the atoms, each bobbing about its rest position.

The lattice itself is never still. Its atoms vibrate in collective normal modes, and quantizing those modes gives phonons — the particle-like carriers of sound and heat that also scatter electrons and set a metal's resistance.

Before bands, the crudest model already carries a metal a long way: treat the conduction electrons as a free gas. Pauli exclusion stacks them into momentum space up to the Fermi energy, and the heat capacity, magnetism, and transport of a metal all trace back to what happens at that surface.

FIG_001
a1a_1
a2a_2
A crystal is a lattice: identical atoms repeat with perfect periodicity, and one unit cell tiles the whole solid.
FIG_004
kxkzky
kFk_F
The free-electron Fermi sphere: states fill momentum space up to kF, and the surface governs the metal.

From this foundation the subject fans out: semiconductors and the doped junctions that make devices, dielectrics and ferroelectrics, and the several distinct origins of magnetism in solids.

FIG_005
NS
B=0B = 0
Superconductivity: a superconductor expels magnetic flux (B = 0 inside), levitating a magnet by the Meissner effect.

The dramatic finale is superconductivity — below a critical temperature, electrons bind into Cooper pairs, resistance vanishes, and the material expels magnetic flux entirely, a purely quantum effect made visible at human scale.

Throughout, one move recurs: find the symmetry, count the states, and let the collective behavior emerge. The course follows Kittel, Ashcroft & Mermin, and Simon, ending in the low-dimensional physics of nanostructures and graphene.

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