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Figure 3
Transformation of vector gM (in the direction η2) into vector gM′ by a magnitude of shear γ along the direction η1. Note that gM and gM′ have the same length and are in mirror symmetry with respect to the plane perpendicular to the K1 plane and the shear plane P.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 43| Part 6| December 2010| Pages 1426-1430
https://doi.org/10.1107/S0021889810037180
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