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Reciprocal Lattice


The reciprocal lattice of a full-rank point lattice L subset R^d is the point lattice

 L^*={g in R^d:g·v in Z for all v in L},

where g·v is the dot product. If the columns of an invertible matrix B form a basis of L, so that L=BZ^d, then

 L^*=(B^(-1))^TZ^d,

where the superscript T denotes the transpose. Indeed, g·v is an integer for every v in L iff B^Tg in Z^d. Taking the reciprocal twice gives (L^*)^*=L, and the covolumes satisfy covol(L^*)=1/covol(L). For example, the reciprocal of aZ^d, for a>0, is a^(-1)Z^d.

In solid-state physics, the reciprocal lattice is usually normalized as 2piL^*, so its defining condition is g·v in 2piZ and its basis matrix is 2pi(B^(-1))^T (Tong, p. 52).


See also

Brillouin Zone, Covolume, Point Lattice

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References

Barvinok, A. Math 669: Combinatorics, Geometry and Complexity of Integer Points. Lecture notes. Ann Arbor, MI: University of Michigan, 2011. https://sites.lsa.umich.edu/barvinok/wp-content/uploads/sites/1434/2025/05/latticenotes669.pdf.Lagarias, J. C.; Lenstra, H. W. Jr.; and Schnorr, C.-P. "Korkin-Zolotarev Bases and Successive Minima of a Lattice and Its Reciprocal Lattice." Combinatorica 10, 333-348, 1990. https://doi.org/10.1007/BF02128669.Tong, D. "Band Structure." In Lectures on Applications of Quantum Mechanics, pp. 52-56. https://www.damtp.cam.ac.uk/user/tong/aqm/solid2.pdf.

Cite this as:

Weisstein, Eric W. "Reciprocal Lattice." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/ReciprocalLattice.html

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