SUMMARY
A Bravais lattice is defined by the equation R = la1 + ma2 + na3, where l, m, and n are integers. Lattices with a basis can be viewed as Bravais lattices with additional atoms at the lattice points, thus retaining primitive vectors. For instance, in cuprate superconductors, the CuO2 planes can be represented as a basis of copper and neighboring oxygen atoms, while the primitive vectors correspond to a square lattice. It is essential to distinguish between the lattice, which is a vector space of R, and the basis, as both are necessary to uniquely specify points within a crystal structure.
PREREQUISITES
- Understanding of Bravais lattices and their definitions
- Knowledge of crystal structures and periodicity
- Familiarity with primitive vectors in crystallography
- Basic concepts of electron density in crystal lattices
NEXT STEPS
- Study the properties of different Bravais lattices, including body-centered cubic (bcc) and face-centered cubic (fcc) structures
- Explore the concept of lattice basis and its implications in solid-state physics
- Learn about the mathematical representation of crystal structures using vector spaces
- Investigate the role of periodicity in defining crystal versus amorphous materials
USEFUL FOR
Students and professionals in materials science, solid-state physics, and crystallography, particularly those interested in the structural analysis of crystals and their electronic properties.