International
Tables for
Crystallography
Volume D
Physical properties of crystals
Edited by A. Authier

International Tables for Crystallography (2006). Vol. D. ch. 3.3, p. 430

Table 3.3.10.1 

Th. Hahna* and H. Klapperb

a Institut für Kristallographie, Rheinisch–Westfälische Technische Hochschule, D-52056 Aachen, Germany, and bMineralogisch-Petrologisches Institut, Universität Bonn, D-53113 Bonn, Germany
Correspondence e-mail:  hahn@xtal.rwth-aachen.de

Table 3.3.10.1 | top | pdf |
Examples of permissible twin boundaries for higher-order merohedral twins ([j]> 1)

  [\Sigma 3] growth and deformation twins of cubic crystals, twin mirror plane (111) (spinel law) [\Sigma 5] growth twins of tetragonal rare-earth sulfides (SmS1.9), twin mirror plane (120) [\Sigma 33] deformation twins of cubic galena (PbS), twin mirror plane (441)
Eigensymmetry [{\cal H}] [4/m{\bar 3}2/m] [4/m\,2/m\,2/m] [4/m{\bar 3}2/m]
Intersection symmetry [{\cal H}^\ast] [{\bar 3}2/m] parallel to [111] [4/m] parallel to [001] [2/m] parallel to [[1{\bar 1}0]]
Reduced composite symmetry [{\cal K}^\ast] [6'/m'_1({\bar 3})2/m\,2'/m'_3] [4/m\,2'/m'_1\,2'/m'_2] [2'/m'_1\,2/m\,2'/m'_2]
Permissible twin boundaries Three pairs of perpendicular planes Two pairs of perpendicular planes One pair of permissible planes
[m_1 = (111)] & [m_3 = (11{\bar 2})] [m_1 = (120)] & [({\bar 2}10)] [m_1 \,= \,(441)] & [m_2 \,= \,(11{\bar 8})]
[m_1 = (111)] & [m_3 = ({\bar 2}11)] [m_2 = (310)] & [({\bar 1}30)]  
[m_1 = (111)] & [m_3 = (1{\bar 2}1)]    
Reference system Cubic axes Tetragonal axes Cubic axes
The existence of this deformation twin is still in doubt (cf. Seifert, 1928[link]).
The intersection symmetry [{\cal H}^\ast] and the permissible boundaries are referred to the coordinate system of the eigensymmetry; the reduced composite symmetries [{\cal K}^\ast] are based on their own conventional coordinate system derived from the intersection symmetry [{\cal H}^\ast] plus the twin law (cf. Section 3.3.4[link]).