Both first-principles and tight-binding electronic structure total energy calculations require integrals of wavefunctions and/or eigenvalues over the Brillouin zone. Thus, in the NRL tight-binding formalism the total energy of a crystal is given by
where the sum is over the occupied states of the system at the wave vector k in the first Brillouin zone. In practice the integral must be approximated by a sum over selected k-points in the Brillouin zone:
where the (lattice dependent) weights wi and points ki are chosen to reproduce the integral as accurately as possible. Common meshes are the so-called "regular" k-point meshes, where the points are equally spaced from the origin, and the "special" k-point mesh of Monkhorst and Pack, which offsets the regular mesh from the origin to reduce the number of k-points needed. In a wide variety of lattices, the original special k-point method must be modified (Mehl et al.) to properly account for the symmetry of the lattice.The links below take you to predefined k-point meshes for several common lattices. We list both regular and special k-point meshes, and take the symmetry of the lattice into account to minimize the computational work. Each set of k-points is also cross referenced to the appropriate entries in the Crystal Lattice Structures database.
The k-point database
Cubic Systems | Other Systems |
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face-centered cubic lattices | Hexagonal Lattices |
body-centered cubic lattices | |
simple cubic lattices |
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