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

International Tables for Crystallography (2013). Vol. D, ch. 3.4, p. 507

Figure 3.4.3.2 

V. Janoveca* and J. Přívratskáb

aInstitute of Physics, Academy of Sciences of the Czech Republic, Na Slovance 2, CZ-18221 Prague 8, Czech Republic, and bDepartment of Mathematics and Didactics of Mathematics, Technical University of Liberec, Hálkova 6, 461 17 Liberec 1, Czech Republic
Correspondence e-mail:  janovec@fzu.cz

[Figure 3.4.3.2]
Figure 3.4.3.2

Non-transposable domain pairs. (a) The parent phase with symmetry [G=6_z/m_z] is represented by a dotted hexagon and the three ferroelastic single-domain states with symmetry [F_1=F_2=F_3=2_z/m_z] are depicted as drastically squeezed hexagons. (b) Domain pair [({\bf S}_1,{\bf S}_2) ] and transposed domain pair [({\bf S}_2,{\bf S}_1)]. There exists no operation from the group [6_z/m_z] that would exchange domain states [{\bf S}_1] and [{\bf S}_2], i.e. that would transform one domain pair into a transposed domain pair.