view article
Figure 4
(a) Detail of a misindexed image, with incorrect reciprocal-space basis vectors a*′ and c*′ shown in the inset. Although all observed reflections are spanned by this basis, no reflections are observed when h′ + l′ is an odd number. (b) Corrected basis after application of the algorithm in §2.5[link]. New basis vectors are chosen such that a* = b*′, b* = a*′ + c*′, c* = a*′ − c*′. The reader will note that the new Miller indices are given by h = k′, k = (h′ + l′)/2, l = (h′ − l′)/2. The matrix transforming the Miller indices is the inverse transpose of the matrix transforming the basis vectors.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 37| Part 3| May 2004| Pages 399-409
doi:10.1107/S0021889804005874
Follow J. Appl. Cryst.
Sign up for e-alerts
E-alerts
Follow J. Appl. Cryst. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS