Crystal Structure

Key idea: H3 Solid State Physics: Crystal Structure — key ideas and exam-focused notes on bonding, crystal structures, conduction models, and band ideas.

  • Advanced Physics
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Learning objectives

  • Use advanced reference material to reinforce mathematical, optical, material, and modern-physics models.

Atoms, ions or molecules in a crystal occupy positions with long-range periodic order. A lattice describes that repeating translational pattern; a basis identifies the particle or group attached to each lattice point. A unit cell is a repeating three-dimensional region that generates the crystal structure by translation.

Common structure descriptions include:

  • simple cubic (SC),
  • body-centred cubic (BCC),
  • face-centred cubic (FCC), and
  • hexagonal close-packed (HCP).
Simple-cubic and body-centred-cubic cells both have eight shared corner sites. Simple cubic contains one atom per cell, coordination number 6 and packing fraction 0.524. BCC adds one whole central atom, giving two atoms per cell, coordination number 8 and packing fraction 0.680.
Count the fraction of each boundary atom belonging to one cell; a corner contributes one eighth.

Simple cubic

The conventional simple-cubic cell has lattice sites at its eight corners. Each corner is shared by eight cells, so it contributes 1/8 of an atom to one cell: 8 × (1/8) = 1 atom per cell.

  • Coordination number: 6.
  • Nearest neighbours touch along a cube edge, so a = 2r.
  • Packing fraction: π/6 ≈ 0.524, or about 52.4%.

Naturally occurring alpha-polonium is the standard elemental example of simple-cubic packing.

Body-centred cubic

A BCC cell has the same eight shared corner sites plus one whole lattice point at the body centre, giving 8 × (1/8) + 1 = 2 atoms per cell.

  • Coordination number: 8.
  • Nearest neighbours touch along a body diagonal, so square root of 3 a = 4r.
  • Packing fraction: π square root of 3/8 ≈ 0.680, or about 68.0%.

Alpha-iron at room temperature is a familiar BCC metal. A crystal with one species at the corners and a different species at the centre, such as CsCl, is not a BCC Bravais lattice: translating by half a body diagonal exchanges unlike species. It is described by a simple-cubic Bravais lattice with a two-particle basis.

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Course and syllabus information
Course
Advanced Physics
Edition
Advanced Physics