Crystal Structures

A crystal is invariant under translation by a lattice vector.

The crystal lattice is a set of mathematical points defined by:

rn = n1a1 + n2a2 + n3a3 n1, n2, n3 integer

The vectors a1, a2, a3 define the unit cell. Atoms inside the unit cell are called thebasis.

= +

Crystal Symmetries

1) Translation Bravais Lattices (14 in 3D, 5 in 2D; fcc, bcc,…)

2) Point OperationsPoint Groups ( 32 in 3D, 10 in 2D; rotation, mirror)

1) + 2)Space Groups (230 in 3D, 17 in 2D; crystal structures)

Reciprocal lattice  Diffractionpattern  Fourier transform of the lattice

The reciprocal lattice consists of the vectors Ghkl defined by:

Ghkl = hg1 + kg2 + lg3 h, k, l integer (Miller indices)

g1= 2/Va2a3 for all permutations: 1,2,3 2,3,1 3,1,2 V = a1(a2a3)

The (hkl) define the lattice planes which produce a diffraction peak (Bragg, Laue).

Ghkl is perpendicular to the planes(hkl). Its length is given by theinverseof theplane spacing dhkl: |Ghkl| = 2/dhkl

Square brackets denote the direction [hkl] which is perpendicular to the planes (hkl).

Brillouin zone = Unit cell in reciprocal space (k-space).

Usually one chooses the Wigner-Seitz construction for the Brillouin zone, wherek=(000) is at the center and the surface planes are half way to the nearest reciprocal lattice points. More on that in Lecture 10.

Crystal Structure and Bonding

Covalent: Diamond; Binary compounds: Zincblende (cubic), Wurtzite (hexagonal)

Directional bonds determine the geometry, e.g. tetrahedral for sp3 bonding.

Surface: Re-bonding (= “reconstruction”) minimizes the density of broken bonds.

See Lecture 6 for the intricate structures formed at silicon surfaces.

Ionic: NaCl for ralkali  rhalogen CsCl for ralkali  rhalogen

Optimize the Coulomb (Madelung) energy for a given size of the ions.

Surface: Charge neutrality to avoid infinite Coulomb energy: NaCl(100)

Metallic, Molecular: fcc, hcp

Isotropic bonding favors close-packed structures (12 neighbors)

Two close-packed structures: face centered cubic (fcc) = abcabc stacking

hexagonal close packed (hcp) = ababab stacking

Surface: Also dense packing, i.e. fcc(111), hcp(0001) (four indices: a1, a2, a3, c)

Stacking of Close-Packed Layers

a abcaba

Low Index Planes for a Cubic Lattice

Covalent

IonicMetallic

NaCl structure:fcc structure:

CsCl structurebcc structure

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