Table 3.4.3.6

Janovec, V.; Přívratská

doi:10.1107/97809553602060000645

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

pdf | chapter contents | chapter index | related articles

International Tables for Crystallography (2006). Vol. D. ch. 3.4, pp. 486-489

Table 3.4.3.6

V. Janovec^a ^* and J. Přívratská^b

^a Department of Physics, Technical University of Liberec, Hálkova 6, 461 17 Liberec 1, 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

Table 3.4.3.6 | top | pdf |
Ferroelastic domain pairs and twins with compatible walls

[F_1:] symmetry of $[{\bf S}_1]$ ; $[g_{1j}]$ : twinning operations; $[K_{1j}]$ : twinning group; Axis: axis of domain pair; Equation:^† direction of the axis; $[\varphi ]$ :^† disorientation angle; $[{\sf \overline J}_{1j} ]$ : symmetry of the twin pair; $[{\underline t}_{1j}^{\star}]$ : twinning operation; $[{\sf \overline T}_{1j}]$ : symmetry of the twin and wall, twin law of the twin; Classification: see Table 3.4.4.3.

	$[g_{1j} ]$	$[K_{1j}]$	Axis	Equation	Wall normals		$[\varphi]$	$[{\sf \overline J}_{1j}]$	$[\underline t^{\star}_{1j} ]$	$[{\sf\overline T}_{1j}]$	Classification
1	$[2^{\star}_z]$	$[2^{\star}_Z]$	$[[B\bar{1}0]]$	(a)			(1)	$[2^{\star}_z]$		1	$[{\rm AR}^{\star}]$
1	$[2^{\star}_z]$	$[2^{\star}_Z]$	$[[B\bar{1}0]]$	(a)			(1)	$[\underline2^{\star}_z]$	$[\underline2^{\star}_z]$	$[\underline2^{\star}_z]$	SI
1	$[m^{\star}_z]$	$[m^{\star}_z]$	$[[B\bar{1}0] ]$	(a)			(1)	$[{\underline m}^{\star}_z ]$	$[{\underline m}^{\star}_z ]$	$[{\underline m}^{\star}_z ]$	SI
1	$[m^{\star}_z]$	$[m^{\star}_z]$	$[[B\bar{1}0] ]$	(a)			(1)	$[m^{\star}_z]$		1	$[{\rm AR}^{\star}]$
$[\bar{1}]$	$[m^{\star}_z]$ , $[2^{\star}_z]$	$[2^{\star}_z/m^{\star}_z ]$	$[[B\bar{1}0]]$	(a)			(1)	$[2_z^{\star}/\underline{m}^{\star}_z]$	$[\underline{m}^{\star}_z ]$	$[\underline{m}^{\star}_z ]$	SR
$[\bar{1}]$	$[m^{\star}_z]$ , $[2^{\star}_z]$	$[2^{\star}_z/m^{\star}_z ]$	$[[B\bar{1}0]]$	(a)			(1)	$[\underline2^{\star}_z/m^{\star}_z]$	$[\underline2^{\star}_z]$	$[\underline2^{\star}_z]$	SR
	$[2^{\star}_x]$ , $[2^{\star}_y]$	$[2^{\star}_x2^{\star}_y2_z ]$					(2)	$[2^{\star}_x\underline2^{\star}_y\underline2_z ]$	$[\underline2^{\star}_y]$	$[\underline2^{\star}_y]$	SR
	$[2^{\star}_x]$ , $[2^{\star}_y]$	$[2^{\star}_x2^{\star}_y2_z ]$					(2)	$[\underline2^{\star}_x2^{\star}_y\underline2_z ]$	$[\underline2^{\star}_x]$	$[\underline2^{\star}_x]$	SR
	$[m^{\star}_x]$ , $[m^{\star}_y]$	$[m^{\star}_xm^{\star}_y2_z ]$					(2)	$[\underline{m}^{\star}_xm^{\star}_y\underline2_z ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	SR
	$[m^{\star}_x]$ , $[m^{\star}_y]$	$[m^{\star}_xm^{\star}_y2_z ]$					(2)	$[m^{\star}_x\underline{m}^{\star}_y\underline2_z ]$	$[\underline{m}^{\star}_y ]$	$[\underline{m}^{\star}_y ]$	SR
	$[4^{\star}_z]$ , $[4_z^{3 \star}]$	$[4^{\star}_z]$		(b)	$[\Bigl[]$		(3)	$[\underline2_z]$		1	$[{\rm A}\underline {\rm R}]$
	$[4^{\star}_z]$ , $[4_z^{3 \star}]$	$[4^{\star}_z]$		(b)	$[\Bigl[]$	$[[B\bar{1}0] ]$	(3)	$[\underline2_z ]$		1	$[{\rm A}\underline{\rm R}]$
	$[\bar4^{\star}_z ]$ , $[\bar4_z^{*3}]$	$[\bar{4}^{\star}_z ]$		(b)	$[\Bigl[]$		(3)	$[\underline2_z ]$		1	$[{\rm A}\underline{\rm R} ]$
	$[\bar4^{\star}_z ]$ , $[\bar4_z^{*3}]$	$[\bar{4}^{\star}_z ]$		(b)	$[\Bigl[]$	$[[B\bar{1}0] ]$	(3)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R} ]$
	,	$[6_{z}]$		(c)			(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	,	$[6_{z}]$		(c)		$[[B\bar{1}0]]$	(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	,			(c)			(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	,			(c)		$[[B\bar{1}0] ]$	(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	$[\bar3_z^5]$ , $[\bar6_z ]$	$[6_{z}/m_z]$		(c)			(4)	$[\underline2_z ]$		1	$[{\rm A}\underline{\rm R} ]$
	$[\bar3_z^5]$ , $[\bar6_z ]$	$[6_{z}/m_z]$		(c)		$[[B\bar{1}0]]$	(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	$[\bar3_z]$ , $[\bar6_z^5]$			(c)			(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R} ]$
	$[\bar3_z]$ , $[\bar6_z^5]$			(c)		$[[B\bar{1}0] ]$	(4)	$[\underline2_z]$		1	$[{\rm A}\underline{\rm R}]$
	$[2^{\star}_{xy} ]$ ,	$[4_z2_x2_{xy} ]$	$[[\bar{C}C2] ]$	(d)			(5)	$[2^{\star}_{xy}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{xy} ]$ ,	$[4_z2_x2_{xy} ]$	$[[\bar{C}C2] ]$	(d)		$[[1\bar{1}C]_e]$	(5)	$[\underline2^{\star}_{xy} ]$	$[\underline2^{\star}_{xy} ]$	$[\underline2^{\star}_{xy}]$	SI
	$[m^{\star}_{xy} ]$ , $[\bar4_z]$	$[\bar4_z2_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)			(5)	$[\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy}]$	SI
	$[m^{\star}_{xy} ]$ , $[\bar4_z]$	$[\bar4_z2_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)		$[[1\bar{1}C] ]$	(5)	$[m^{\star}_{xy}]$			$[{\rm AR}^{\star}]$
	$[2^{\star}_{x{^\prime}} ]$ ,		$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\bar1\sqrt{3}0]]$	(6)	$[2^{\star}_{x{^\prime}}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{x{^\prime}} ]$ ,		$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\sqrt{3}1C]_e ]$	(6)	$[\underline2^{\star}_{x{^\prime}}]$	$[\underline2^{\star}_{x{^\prime}} ]$	$[\underline2^{\star}_{x{^\prime}} ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ , $[\bar3_z^5]$	$[\bar{3}_zm_x ]$	$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\bar1\sqrt{3}0]_e ]$	(6)	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ , $[\bar3_z^5]$	$[\bar{3}_zm_x ]$	$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\sqrt{3}1C] ]$	(6)	$[m^{\star}_{x{^\prime}} ]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\sqrt{3}10]]$	(7)	$[2^{\star}_{y{^\prime}}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\bar1\sqrt{3}C]_e]$	(7)	$[\underline2^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}} ]$	SI
	$[m^{\star}_{y{^\prime}} ]$ , $[\bar6_z]$	$[\bar{6}_z2_xm_y ]$	$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\sqrt{3}10]_e ]$	(7)	$[\underline{m}^{\star}_{y{^\prime}}]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	SI
	$[m^{\star}_{y{^\prime}} ]$ , $[\bar6_z]$	$[\bar{6}_z2_xm_y ]$	$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\bar1\sqrt{3}C] ]$	(7)	$[m^{\star}_{y{^\prime}}]$		1	$[{\rm AR}^{\star}]$
$[2_{xy}]$	$[m^{\star}_{x} ]$ , $[\bar4_z^{3}]$	$[\bar4_zm_x2_{xy} ]$	$[[0C\bar{1}] ]$	(g)			(8)	$[\underline{m}^{\star}_{x} ]$	$[\underline{m}^{\star}_{x} ]$	$[\underline{m}^{\star}_{x}]$	SI
$[2_{xy}]$	$[m^{\star}_{x} ]$ , $[\bar4_z^{3}]$	$[\bar4_zm_x2_{xy} ]$	$[[0C\bar{1}] ]$	(g)			(8)	$[m^{\star}_{x}]$		1	$[{\rm AR}^{\star}]$
	$[m^{\star}_x]$ , $[2^{\star}_y]$	$[m^{\star}_x2^{\star}_ym_z ]$					(2)	$[\underline{m}^{\star}_x\underline2^{\star}_ym_z ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x\underline2^{\star}_ym_z ]$	SI
	$[m^{\star}_x]$ , $[2^{\star}_y]$	$[m^{\star}_x2^{\star}_ym_z ]$					(2)	$[m_x^{\star}2_y^{\star}m_z]$	$[\underline{m}^{\star}_x ]$		$[{\rm AR}^{\star}]$
$[m_{z}]$	, $[\bar4_z^3 ]$	$[4_z/m_{z}]$		(b)		$[[1B0]_{e0}]$	(3)				AI
	, $[\bar4_z^3 ]$	$[4_z/m_{z}]$		(b)		$[[B\bar{1}0]_{0e}]$	(3)				AI
	, $[\bar4_z]$			(b)		$[[1B0]_{e0}]$	(3)				AI
	, $[\bar4_z]$			(b)		$[[B\bar{1}0]_{0e}]$	(3)				AI
	, $[\bar6^5_z ]$	$[\bar6_{z}]$		(c)		$[[1B0]_{e0} ]$	(4)				AI
	, $[\bar6^5_z ]$	$[\bar6_{z}]$		(c)		$[[B\bar{1}0]_{0e} ]$	(4)				AI
	, $[\bar6_z]$	$[\bar6_z]$		(c)		$[[1B0]_{e0} ]$	(4)				AI
	, $[\bar6_z]$	$[\bar6_z]$		(c)		$[[B\bar{1}0]_{0e} ]$	(4)				AI
	$[\bar3_z]$ ,	$[6_{z}/m_z]$		(c)		$[[1B0]_{e0}]$	(4)				AI
	$[\bar3_z]$ ,	$[6_{z}/m_z]$		(c)		$[[B\bar{1}0]_{0e} ]$	(4)				AI
	$[\bar3_z^5]$ ,			(c)		$[[1B0]_{e0} ]$	(4)				AI
	$[\bar3_z^5]$ ,			(c)		$[[B\bar{1}0]_{0e} ]$	(4)				AI
	$[m^{\star}_{xy} ]$ ,	$[4_zm_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)			(5)	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	SI
	$[m^{\star}_{xy} ]$ ,	$[4_zm_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)		$[[1\bar{1}C]]$	(5)	$[m^{\star}_{xy}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{xy} ]$ , $[\bar4_z]$	$[\bar{4}_zm_x2_{xy} ]$	$[[\bar{C}C2]]$	(d)			(5)	$[2^{\star}_{xy}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{xy} ]$ , $[\bar4_z]$	$[\bar{4}_zm_x2_{xy} ]$	$[[\bar{C}C2]]$	(d)		$[[1\bar{1}C]_e]$	(5)	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	SI
	$[m^{\star}_{x{^\prime}} ]$ ,		$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\bar1\sqrt{3}0]_e ]$	(6)	$[\underline{m}^{\star}_{x{^\prime}}]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ ,		$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\sqrt{3}1C] ]$	(6)	$[m^{\star}_{x{^\prime}}]$			$[{\rm AR}^{\star}]$
	$[2^{\star}_{x{^\prime}} ]$ , $[\bar3_z^5]$	$[\bar3_zm_x]$	$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\bar1\sqrt{3}0] ]$	(6)	$[2^{\star}_{x{^\prime}}]$			$[{\rm AR}^{\star}]$
	$[2^{\star}_{x{^\prime}} ]$ , $[\bar3_z^5]$	$[\bar3_zm_x]$	$[[\sqrt{3}C]$ , C, $[\bar4]]$	(e)		$[[\sqrt{3}1C]_e]$	(6)	$[\underline2^{\star}_{x{^\prime}}]$	$[\underline2^{\star}_{x{^\prime}}]$	$[\underline2^{\star}_{x{^\prime}}]$	SI
	$[m^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\sqrt{3}10]_e]$	(7)	$[\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	SI
	$[m^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\bar1\sqrt{3}C] ]$	(7)	$[m^{\star}_{y{^\prime}}]$			$[{\rm AR}^{\star}]$
	$[2^{\star}_{y{^\prime}} ]$ , $[\bar6_z]$	$[\bar{6}_zm_x2_y ]$	$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\sqrt{3}10] ]$	(7)	$[2^{\star}_{y{^\prime}}]$			$[{\rm AR}^{\star}]$
	$[2^{\star}_{y{^\prime}} ]$ , $[\bar6_z]$	$[\bar{6}_zm_x2_y ]$	$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\bar1\sqrt{3}C]_e ]$	(7)	$[\underline2^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}}]$	$[\underline2^{\star}_{y{^\prime}} ]$	SI
$[m_{xy}]$	$[2^{\star}_{x} ]$ , $[\bar4^3_z]$	$[\bar{4}_z2_xm_{xy} ]$	$[[0C\bar{1}]]$	(g)			(8)	$[2^{\star}_{x}]$			$[{\rm AR}^{\star}]$
$[m_{xy}]$	$[2^{\star}_{x} ]$ , $[\bar4^3_z]$	$[\bar{4}_z2_xm_{xy} ]$	$[[0C\bar{1}]]$	(g)			(8)	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{x}]$	$[\underline2^{\star}_{x}]$	SI
	$[m^{\star}_x]$ , $[m^{\star}_y]$	$[m^{\star}_xm^{\star}_ym_z ]$					(2)	$[\underline{m}^{\star}_xm^{\star}_ym_z ]$	$[\underline{m}^{\star}_x]$	$[\underline{m}^{\star}_x\underline2^{\star}_ym_z ]$	SR
	$[m^{\star}_x]$ , $[m^{\star}_y]$	$[m^{\star}_xm^{\star}_ym_z ]$					(2)	$[m^{\star}_x\underline{m}^{\star}_ym_z ]$	$[\underline{m}^{\star}_y]$	$[\underline2^{\star}_x\underline{m}^{\star}_ym_z ]$	SR
	$[4^{\star}_z]$ , $[4^{3 \star}_z]$	$[4^{\star}_z/m_z ]$		(b)	$[\Bigl[]$		(3)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	$[4^{\star}_z]$ , $[4^{3 \star}_z]$	$[4^{\star}_z/m_z ]$		(b)	$[\Bigl[]$	$[[B\bar{1}0]]$	(3)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	,	$[6_{z}/m_z]$		(c)			(4)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	,	$[6_{z}/m_z]$		(c)		$[[B\bar{1}0] ]$	(4)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	,			(c)			(4)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	,			(c)		$[[B\bar{1}0] ]$	(4)	$[\underline2_z/m_z]$			$[{\rm A}\underline {\rm R}]$
	$[m^{\star}_{xy} ]$ ,	$[4_z/m_zm_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)			(5)	$[2^{\star}_{xy}/\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	SR
	$[m^{\star}_{xy} ]$ ,	$[4_z/m_zm_xm_{xy} ]$	$[[\bar{C}C2]]$	(d)		$[[1\bar{1}C]]$	(5)	$[\underline2^{\star}_{xy}/m^{\star}_{xy} ]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	SR
	$[m^{\star}_{x{^\prime}} ]$ ,	$[\bar{3}_zm_x ]$	$[[\sqrt{3}CC\bar4] ]$	(e)		$[[\bar1\sqrt{3}0]]$	(6)	$[2^{\star}_{x{^\prime}}/\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}}]$	$[\underline{m}^{\star}_{x{^\prime}}]$	SR
	$[m^{\star}_{x{^\prime}} ]$ ,	$[\bar{3}_zm_x ]$	$[[\sqrt{3}CC\bar4] ]$	(e)		$[[\sqrt{3}1C]]$	(6)	$[\underline2^{\star}_{x{^\prime}}/m^{\star}_{x{^\prime}} ]$	$[\underline2^{\star}_{x{^\prime}} ]$	$[\underline2^{\star}_{x{^\prime}} ]$	SR
	$[m^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\sqrt{3}10] ]$	(7)	$[2^{\star}_{y{^\prime}}/\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}}]$	$[\underline{m}^{\star}_{y{^\prime}}]$	SR
	$[m^{\star}_{y{^\prime}} ]$ ,		$[[\bar{C}]$ , $[\sqrt{3}C]$ , $[\bar4]]$	(f)		$[[\bar1\sqrt{3}C]]$	(7)	$[\underline2^{\star}_{y{^\prime}}/m^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}} ]$	SR
	$[2^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[4^{\star}_z2_x2^{\star}_{xy} ]$			$[\Bigl[]$		(10)	$[2^{\star}_{xy}\underline2^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline2^{\star}_{x\bar{y}}]$	$[\underline2^{\star}_{x\bar{y}}]$	SR
	$[2^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[4^{\star}_z2_x2^{\star}_{xy} ]$			$[\Bigl[]$	$[[1\bar10]]$	(10)	$[\underline2^{\star}_{xy}2^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	SR
	$[m^{\star}_{x\bar{y}} ]$ , $[m^{\star}_{xy}]$	$[\bar{4}^{\star}_z2_xm^{\star}_{xy} ]$			$[\Bigl[]$		(10)	$[\underline{m}^{\star}_{xy}m^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy}]$	SR
	$[m^{\star}_{x\bar{y}} ]$ , $[m^{\star}_{xy}]$	$[\bar{4}^{\star}_z2_xm^{\star}_{xy} ]$			$[\Bigl[]$	$[[1\bar10]]$	(10)	$[m^{\star}_{xy}\underline{m}^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	SR
	$[2^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0] ]$	(9)	$[2^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline2^{\star}_{y{^\prime}}]$	$[\underline2^{\star}_{y{^\prime}} ]$	SR
	$[2^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10]]$	(9)	$[\underline2^{\star}_{x{^\prime}}2^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline2^{\star}_{x{^\prime}}]$	$[\underline2^{\star}_{x{^\prime}} ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0]]$	(9)	$[\underline{m}^{\star}_{x{^\prime}}m^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}}]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10]]$	(9)	$[{m}^{\star}_{x{^\prime}}\underline{m}^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}}]$	SR
$[2_{x\bar{y}}2_{xy}2_z ]$	$[m^{\star}_{x} ]$ , $[m^{\star}_{y}]$	$[{\bar 4}_z^\star m_x^\star 2_{xy} ]$			$[\Bigl[]$		(12)	$[\underline{m}^{\star}_{x}m^{\star}_{y}\underline2_z ]$	$[\underline{m}^{\star}_{x} ]$	$[\underline{m}^{\star}_{x}]$	SR
$[2_{x\bar{y}}2_{xy}2_z ]$	$[m^{\star}_{x} ]$ , $[m^{\star}_{y}]$	$[{\bar 4}_z^\star m_x^\star 2_{xy} ]$			$[\Bigl[]$		(12)	$[m^{\star}_{x}\underline{m}^{\star}_{y}\underline2_z ]$	$[\underline{m}^{\star}_{y} ]$	$[\underline{m}^{\star}_{y}]$	SR
$[2_{x\bar{y}}2_{xy}2_z ]$	$[2^{\star}_{xz} ]$ ,	$[4_z3_{p}2_{xy} ]$	$[[B2\bar{B}]]$	(h)			(11)	$[2^{\star}_{xz}]$		1	$[{\rm AR}^{\star}]$
$[2_{x\bar{y}}2_{xy}2_z ]$	$[2^{\star}_{xz} ]$ ,	$[4_z3_{p}2_{xy} ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1]]$	(11)	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	SI
$[2_{x\bar{y}}2_{xy}2_z ]$	$[m_{xz}^{\star} ]$ , $[\bar4_y]$	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)			(11)	$[\underline{m}_{xz}^{\star}]$	$[\underline{m}_{xz}^{\star}]$	$[\underline{m}_{xz}^{\star}]$	SI
$[2_{x\bar{y}}2_{xy}2_z ]$	$[m_{xz}^{\star} ]$ , $[\bar4_y]$	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1] ]$	(11)	$[m_{xz}^{\star}]$		1	$[{\rm AR}^{\star}]$
	$[m^{\star}_{x\bar{y}} ]$ , $[m^{\star}_{xy}]$	$[4^{\star}_zm_xm^{\star}_{xy} ]$			$[\Bigl[]$		(10)	$[m^{\star}_{x\bar{y}}\underline{m}^{\star}_{xy}\underline2_z ]$	$[\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy}]$	SR
	$[m^{\star}_{x\bar{y}} ]$ , $[m^{\star}_{xy}]$	$[4^{\star}_zm_xm^{\star}_{xy} ]$			$[\Bigl[]$	$[[1\bar10]]$	(10)	$[\underline{m}^{\star}_{x\bar{y}}{m}^{\star}_{xy}\underline2_z ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	SR
	$[2^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[\bar{4}^{\star}_zm_x2^{\star}_{xy} ]$			$[\Bigl[]$		(10)	$[2^{\star}_{xy}\underline2^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline2^{\star}_{x\bar{y}} ]$	$[\underline2^{\star}_{x\bar{y}} ]$	SR
	$[2^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[\bar{4}^{\star}_zm_x2^{\star}_{xy} ]$			$[\Bigl[]$	$[[1\bar10]]$	(10)	$[\underline2^{\star}_{xy}2^{\star}_{x\bar{y}}\underline2_z ]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy} ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0] ]$	(9)	$[\underline{m}^{\star}_{x{^\prime}}m^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10] ]$	(9)	$[{m}^{\star}_{x{^\prime}}\underline{m}^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	$[\underline{m}^{\star}_{y{^\prime}} ]$	SR
	$[2^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0] ]$	(9)	$[2^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline2^{\star}_{y{^\prime}} ]$	$[\underline2^{\star}_{y{^\prime}}]$	SR
	$[2^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10] ]$	(9)	$[\underline2^{\star}_{x{^\prime}}2^{\star}_{y{^\prime}}\underline2_z ]$	$[\underline2^{\star}_{x{^\prime}} ]$	$[\underline2^{\star}_{x{^\prime}} ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$	$[\bar{6}_zm_x2_y ]$				$[[\bar1\sqrt{3}0]_e ]$	(9)	$[\underline{m}^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}m_z ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}m_z ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$	$[\bar{6}_zm_x2_y ]$				$[[\sqrt{3}10] ]$	(9)	$[{m}^{\star}_{x{^\prime}}2^{\star}_{y{^\prime}}m_z ]$			$[{\rm AR}^{\star}]$
	$[m^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[4_z/m_zm_xm_{xy} ]$					(10)	$[2^{\star}_{xy}m^{\star}_{x\bar{y}}m_z ]$			$[{\rm AR}^{\star}]$
	$[m^{\star}_{x\bar{y}} ]$ , $[2^{\star}_{xy}]$	$[4_z/m_zm_xm_{xy} ]$				$[[1\bar10]_e]$	(10)	$[\underline2^{\star}_{xy}\underline{m}^{\star}_{x\bar{y}}m_z ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	$[\underline2^{\star}_{xy}\underline{m}^{\star}_{x\bar{y}}m_z ]$	SI
	$[m^{\star}_{y{^\prime}} ]$ , $[2^{\star}_{x{^\prime}}]$	$[\bar{6}_z2_xm_y ]$				$[[\bar1\sqrt{3}0] ]$	(9)	$[2^{\star}_{x{^\prime}}m^{\star}_{y{^\prime}}m_z ]$			$[{\rm AR}^{\star}]$
	$[m^{\star}_{y{^\prime}} ]$ , $[2^{\star}_{x{^\prime}}]$	$[\bar{6}_z2_xm_y ]$				$[[\sqrt{3}10]_e ]$		$[\underline{2}^{\star}_{x{^\prime}}\underline{m}^{\star}_{y{^\prime}}m_z ]$	$[\underline{m}_{y{^\prime}} ]$	$[\underline{2}^{\star}_{x{^\prime}}\underline{m}^{\star}_{y{^\prime}}m_z ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0]_e]$	(9)	$[\underline{m}^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}m_z ]$	$[\underline{m}^{\star}_{x{^\prime}} ]$	$[\underline{m}^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}m_z ]$	SI
	$[m^{\star}_{x{^\prime}} ]$ , $[2^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10] ]$	(9)	$[m^{\star}_{x{^\prime}}2^{\star}_{y{^\prime}}m_z ]$			$[{\rm AR}^{\star}]$
$[m_{x\bar{y}}m_{xy}2_z]$	$[2^{\star}_{x}]$ , $[2^{\star}_{y} ]$	$[\bar{4}^{\star}_z2^{\star}_xm_{xy}]$			$[\Bigl[]$		(12)	$[2^{\star}_{x}\underline2^{\star}_{y}\underline2_z ]$	$[\underline2^{\star}_{y}]$	$[\underline2^{\star}_{y}]$	SR
					$[\Bigl[]$			$[\underline2^{\star}_{x}2^{\star}_{y}\underline2_z ]$	$[\underline2^{\star}_{x} ]$	$[\underline2^{\star}_{x}]$	SR
$[m_{x\bar{y}}m_{xy}2_z ]$	$[m^{\star}_{xz} ]$ , $[\bar4_y]$	$[\bar{4}_z3_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)			(11)	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SI
$[m_{x\bar{y}}m_{xy}2_z ]$	$[m^{\star}_{xz} ]$ , $[\bar4_y]$	$[\bar{4}_z3_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1] ]$		$[m^{\star}_{xz}]$		1	$[{\rm AR}^{\star}]$
$[m_{x\bar{y}}m_{xy}2_z ]$	$[2^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)			(11)	$[2^{\star}_{xz}]$		1	$[{\rm AR}^{\star}]$
$[m_{x\bar{y}}m_{xy}2_z ]$	$[2^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1]_e]$	(11)	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz} ]$	SI
$[m_{x\bar{y}}2_{xy}m_z ]$	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy}(m^{\star}_{xz}) ]$	$[[B2\bar{B}]]$	(h)			(11)	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SI
$[m_{x\bar{y}}2_{xy}m_z ]$	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy}(m^{\star}_{xz}) ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1] ]$	(11)	$[m^{\star}_{xz}]$			$[{\rm AR}^{\star}]$
$[m_{x\bar{y}}2_{xy}m_z ]$	$[2^{\star}_{xz} ]$ , $[\bar4_y]$	$[m_z\bar{3}_{p}m_{xy}(2^{\star}_{xz}) ]$	$[[B2\bar{B}]]$	(h)			(11)	$[2^{\star}_{xz}]$		1	$[{\rm AR}^{\star}]$
$[m_{x\bar{y}}2_{xy}m_z ]$	$[2^{\star}_{xz} ]$ , $[\bar4_y]$	$[m_z\bar{3}_{p}m_{xy}(2^{\star}_{xz}) ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1]_e ]$	(11)	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	SI
	$[m^{\star}_{xy} ]$ , $[m^{\star}_{x\bar{y}}]$	$[4^{\star}_z/m_zm_xm^{\star}_{xy} ]$			$[\Bigl[]$		(10)	$[m^{\star}_{x\bar{y}}\underline{m}^{\star}_{xy}m_z ]$	$[\underline{m}^{\star}_{xy} ]$	$[\underline2^{\star}_{x\bar{y}}\underline{m}^{\star}_{xy}m_z ]$	SR
	$[m^{\star}_{xy} ]$ , $[m^{\star}_{x\bar{y}}]$	$[4^{\star}_z/m_zm_xm^{\star}_{xy} ]$			$[\Bigl[]$	$[[1\bar10]]$	(10)	$[\underline{m}^{\star}_{x\bar{y}}{m}^{\star}_{xy}m_z ]$	$[\underline{m}^{\star}_{x\bar{y}} ]$	$[\underline{m}^{\star}_{x\bar{y}}\underline{2}^{\star}_{xy}m_z ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\bar1\sqrt{3}0] ]$	(9)	$[\underline{m}^{\star}_{x{^\prime}}m^{\star}_{y{^\prime}}m_z ]$	$[\underline{m}^{\star}_{x{^\prime}}]$	$[\underline{m}^{\star}_{x{^\prime}}\underline2^{\star}_{y{^\prime}}m_z ]$	SR
	$[m^{\star}_{x{^\prime}} ]$ , $[m^{\star}_{y{^\prime}}]$					$[[\sqrt{3}10] ]$	(9)	$[m^{\star}_{x'}\underline{m}^{\star}_{y'}m_z ]$	$[\underline{m}^{\star}_{y'}]$	$[\underline{2}^{\star}_{x'}\underline{m}^{\star}_{y'}m_z ]$	SR
$[m_{xy}m_{\bar{x}y}m_z ]$	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)			(11)	$[2^{\star}_{xz}/\underline{m}^{\star}_{xz} ]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SR
$[m_{xy}m_{\bar{x}y}m_z ]$	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$	$[[B2\bar{B}]]$	(h)		$[[\bar{1}B1]]$	(11)	$[\underline2^{\star}_{xz}/m^{\star}_{xz} ]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz} ]$	SR
	$[2^{\star}_{xz} ]$ ,	$[4_z3_{p}2_{xy} ]$					(13)	$[2^{\star}_{xz}]$		1	$[{\rm AR}^{\star}]$
	$[2^{\star}_{xz} ]$ ,	$[4_z3_{p}2_{xy} ]$				$[[\bar101]_e ]$	(13)	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	SI
	$[m^{\star}_{xz} ]$ , $[\bar{4}_y]$	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SI
	$[m^{\star}_{xz} ]$ , $[\bar{4}_y]$	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101]]$	(13)	$[m^{\star}_{xz}]$			$[{\rm AR}^{\star}]$
$[\bar{4}_z]$	$[m^{\star}_{xz} ]$ , $[\bar4_y]$	$[\bar{4}_z3_{p}m_{xy} ]$					(13)	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SI
$[\bar{4}_z]$	$[m^{\star}_{xz} ]$ , $[\bar4_y]$	$[\bar{4}_z3_{p}m_{xy} ]$				$[[\bar101]]$	(13)	$[m^{\star}_{xz}]$			$[{\rm AR}^{\star}]$
$[\bar{4}_z]$	$[2^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[2^{\star}_{xz}]$			$[{\rm AR}^{\star}]$
$[\bar{4}_z]$	$[2^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101]_e ]$	(13)	$[\underline2_{xz}^{\star}]$	$[\underline2_{xz}^{\star}]$	$[\underline2_{xz}^{\star}]$	SI
	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[2^{\star}_{xz}/\underline{m}^{\star}_{xz} ]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SR
	$[m^{\star}_{xz} ]$ ,	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101]]$	(13)	$[\underline2^{\star}_{xz}/m^{\star}_{xz} ]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}]$	SR
$[4_z2_x2_{xy} ]$	$[2^{\star}_{xz} ]$ , $[2^{\star}_{x\bar{z}}]$	$[4_z3_{p}2_{xy} ]$			$[\Bigl[]$		(13)	$[2^{\star}_{xz}\underline2^{\star}_{x\bar{z}}\underline2_{y} ]$	$[\underline2^{\star}_{\bar{x}z} ]$	$[\underline2^{\star}_{\bar{x}z} ]$	SR
$[4_z2_x2_{xy} ]$	$[2^{\star}_{xz} ]$ , $[2^{\star}_{x\bar{z}}]$	$[4_z3_{p}2_{xy} ]$			$[\Bigl[]$	$[[\bar101]]$	(13)	$[\underline2^{\star}_{xz}2^{\star}_{x\bar{z}}\underline2_y ]$	$[\underline2^{\star}_{xz} ]$	$[\underline2^{\star}_{xz} ]$	SR
$[4_z2_x2_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{x\bar{z}}]$	$[m_z\bar{3}_{p}m_{xy} ]$			$[\Bigl[]$		(13)	$[\underline{m}^{\star}_{xz}m^{\star}_{x\bar{z}}\underline2_y ]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SR
$[4_z2_x2_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{x\bar{z}}]$	$[m_z\bar{3}_{p}m_{xy} ]$			$[\Bigl[]$	$[[\bar101]]$	(13)	$[m^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}\underline2_y ]$	$[\underline{m}^{\star}_{x\bar{z}}]$	$[\underline{m}^{\star}_{x\bar{z}}]$	SR
$[4_zm_xm_{xy} ]$	$[m^{\star}_{x\bar{z}} ]$ , $[2^{\star}_{xz}]$	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[2^{\star}_{xz}m^{\star}_{x\bar{z}}m_y ]$			$[{\rm AR}^{\star}]$
$[4_zm_xm_{xy} ]$	$[m^{\star}_{x\bar{z}} ]$ , $[2^{\star}_{xz}]$	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101]_e ]$	(13)	$[\underline2^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	$[\underline2^{\star}_{xz}]$	$[\underline2^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	SI
$[\bar{4}_z2_xm_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{x\bar{z}}]$	$[\bar{4}_z3_{p}m_{xy} ]$			$[\Bigl[]$		(13)	$[\underline{m}^{\star}_{xz}m^{\star}_{x\bar{z}}\underline2_y ]$	$[\underline{m}^{\star}_{xz}]$	$[\underline{m}^{\star}_{xz}]$	SR
$[\bar{4}_z2_xm_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{x\bar{z}}]$	$[\bar{4}_z3_{p}m_{xy} ]$			$[\Bigl[]$	$[[\bar101]]$	(13)	$[m^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}\underline2_y ]$	$[\underline{m}^{\star}_{x\bar{z}} ]$	$[\underline{m}^{\star}_{x\bar{z}} ]$	SR
$[\bar{4}_zm_x2_{xy} ]$	$[m_{x\bar{z}}^{\star} ]$ , $[2_{xz}^{\star}]$	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[2^{\star}_{xz}m^{\star}_{x\bar{z}}m_y ]$			$[{\rm AR}^{\star}]$
$[\bar{4}_zm_x2_{xy} ]$	$[m_{x\bar{z}}^{\star} ]$ , $[2_{xz}^{\star}]$	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101]]$	(13)	$[\underline2^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	$[\underline{m}^{\star}_{x\bar{z}}]$	$[\underline2^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	SR
$[\bar{4}_z2_xm_{xy} ]$	$[2^{\star}_{xz} ]$ , $[2^{\star}_{x\bar{z}}]$	$[m_z\bar{3}_{p}m_{xy} ]$					(13)	$[2^{\star}_{xz}2^{\star}_{x\bar{z}}2_y ]$	$[\underline2^{\star}_{x\bar{z}}]$	$[\underline2^{\star}_{x\bar{z}}]$	SR
$[\bar{4}_z2_xm_{xy} ]$	$[2^{\star}_{xz} ]$ , $[2^{\star}_{x\bar{z}}]$	$[m_z\bar{3}_{p}m_{xy} ]$				$[[\bar101] ]$	(13)	$[\underline2^{\star}_{xz}\underline{2}^{\star}_{x\bar{z}}2_y ]$	$[\underline{2}^{\star}_{x\bar{z}} ]$	$[\underline2^{\star}_{xz}\underline{2}^{\star}_{x\bar{z}}2_y ]$	SI
$[4_z/m_zm_xm_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{\bar{x}z}]$	$[m_z\bar{3}_{p}m_{xy} ]$			$[\Bigl[]$		(13)	$[\underline{m}^{\star}_{xz}m^{\star}_{\bar{x}z}m_y ]$	$[\underline{m}^{\star}_{xz} ]$	$[\underline{m}^{\star}_{xz}\underline{2}^{\star}_{\bar{x}z}m_y ]$	SR
$[4_z/m_zm_xm_{xy} ]$	$[m^{\star}_{xz} ]$ , $[m^{\star}_{\bar{x}z}]$	$[m_z\bar{3}_{p}m_{xy} ]$			$[\Bigl[]$	$[[\bar101]]$	(13)	$[m^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	$[\underline{m}^{\star}_{x\bar{z}} ]$	$[\underline2^{\star}_{xz}\underline{m}^{\star}_{x\bar{z}}m_y ]$	SR
$[3_{p}]$	$[2^{\star}_{x} ]$ ,	$[2_z 3_{p}]$	$[[01\bar1]]$				(14)	$[2^{\star}_x]$			$[{\rm AR}^{\star}]$
$[3_{p}]$	$[2^{\star}_{x} ]$ ,	$[2_z 3_{p}]$	$[[01\bar1]]$				(14)	$[\underline2^{\star}_x]$	$[\underline2^{\star}_x]$	$[\underline2^{\star}_x]$	SI
$[3_{p}]$	$[m^{\star}_{x} ]$ , $[\bar3_r]$	$[m_z \bar3_{p} ]$	$[[01\bar1]]$				(14)	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	SI
$[3_{p}]$	$[m^{\star}_{x} ]$ , $[\bar3_r]$	$[m_z \bar3_{p} ]$	$[[01\bar1]]$				(14)	$[m^{\star}_x ]$			$[{\rm AR}^{\star}]$
$[3_{p}]$	$[2^{\star}_{xy} ]$ ,	$[4_z 3_{p} 2_{xy} ]$	$[[1\bar10]]$				(14)	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	SI
$[3_{p}]$	$[2^{\star}_{xy} ]$ ,	$[4_z 3_{p} 2_{xy} ]$	$[[1\bar10]]$				(14)	$[2^{\star}_{xy}]$			$[{\rm AR}^{\star}]$
$[3_{p}]$	$[m^{\star}_{xy} ]$ , $[\bar4_y]$	$[\bar4_z3_{p}m_{xy} ]$	$[[1\bar10]]$				(14)	$[m^{\star}_{xy}]$			$[{\rm AR}^{\star}]$
$[3_{p}]$	$[m^{\star}_{xy} ]$ , $[\bar4_y]$	$[\bar4_z3_{p}m_{xy} ]$	$[[1\bar10]]$				(14)	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	SI
$[\bar3_{p}]$	$[m^{\star}_{x} ]$ ,	$[m_z\bar3_{p} ]$	$[[01\bar1]]$				(14)	$[2^{\star}_x/\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	SR
$[\bar3_{p}]$	$[m^{\star}_{x} ]$ ,	$[m_z\bar3_{p} ]$	$[[01\bar1]]$				(14)	$[\underline2^{\star}_x/m^{\star}_x]$	$[\underline2^{\star}_x ]$	$[\underline2^{\star}_x]$	SR
$[\bar3_{p}]$	$[m^{\star}_{xy} ]$ ,	$[m_z\bar3_{p}m_{xy} ]$	$[[1\bar10]]$				(14)	$[\underline2^{\star}_{xy}/m^{\star}_{xy} ]$	$[\underline2^{\star}_{xy}]$	$[\underline2^{\star}_{xy}]$	SR
$[\bar3_{p}]$	$[m^{\star}_{xy} ]$ ,	$[m_z\bar3_{p}m_{xy} ]$	$[[1\bar10]]$				(14)	$[2^{\star}_{xy}/\underline{m}^{\star}_{xy} ]$	$[\underline{m}^{\star}_{xy}]$	$[\underline{m}^{\star}_{xy}]$	SR
$[3_{p} 2_{x\bar{y}} ]$	$[2^{\star}_{x} ]$ , $[2^{\star}_{yz}]$	$[4_z3_{p} 2_{xy} ]$	$[[01\bar1]]$				(14)	$[2^{\star}_x\underline2^{\star}_{yz}\underline2_{y\bar{z}} ]$	$[\underline2^{\star}_{yz} ]$	$[\underline2^{\star}_{yz} ]$	SR
$[3_{p} 2_{x\bar{y}} ]$	$[2^{\star}_{x} ]$ , $[2^{\star}_{yz}]$	$[4_z3_{p} 2_{xy} ]$	$[[01\bar1]]$				(14)	$[\underline2^{\star}_x2^{\star}_{yz}\underline2_{y\bar{z}} ]$	$[\underline2^{\star}_x]$	$[\underline2^{\star}_x]$	SR
$[3_{p} 2_{x\bar{y}} ]$	$[m^{\star}_{x} ]$ , $[m^{\star}_{yz}]$	$[m_z\bar3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[\underline{m}^{\star}_xm_{yz}^{\star}\underline2_{y\bar{z}} ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x ]$	SR
$[3_{p} 2_{x\bar{y}} ]$	$[m^{\star}_{x} ]$ , $[m^{\star}_{yz}]$	$[m_z\bar3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[m^{\star}_x\underline{m}^{\star}_{yz}\underline2_{y\bar{z}} ]$	$[\underline{m}^{\star}_{yz}]$	$[\underline{m}^{\star}_{yz}]$	SR
$[3_{p} m_{x\bar{y}} ]$	$[2^{\star}_{x} ]$ , $[m^{\star}_{yz}]$	$[\bar4_z3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[m^{\star}_{yz}m_{y\bar{z}}2^{\star}_x ]$		$[m_{y\bar{z}}]$	$[{\rm AR}^{\star}]$
$[3_{p} m_{x\bar{y}} ]$	$[2^{\star}_{x} ]$ , $[m^{\star}_{yz}]$	$[\bar4_z3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[\underline{m}_{yz}m_{y\bar{z}}\underline2^{\star}_x ]$	$[\underline{m}_{yz} ]$	$[\underline{m}_{yz}m_{y\bar{z}}\underline2^{\star}_x ]$	SI
$[3_{p} m_{x\bar{y}} ]$	$[m^{\star}_x]$ , $[2^{\star}_{yz}]$	$[m_z\bar3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[\underline{m}^{\star}_x\underline2^{\star}_{yz}m_{y\bar{z}} ]$	$[\underline{m}^{\star}_x ]$	$[\underline{m}^{\star}_x\underline2^{\star}_{yz}m_{y\bar{z}} ]$	SI
$[3_{p} m_{x\bar{y}} ]$	$[m^{\star}_x]$ , $[2^{\star}_{yz}]$	$[m_z\bar3_{p}m_{xy} ]$	$[[01\bar1]]$				(14)	$[m^{\star}_x2^{\star}_{yz}m_{y\bar{z}} ]$		$[m_{y\bar{z}}]$	$[{\rm AR}^{\star}]$
$[\bar3_{p}m_{x\bar{y}}]$	$[m^{\star}_x]$ , $[m^{\star}_{yz} ]$	$[m_z \bar3_{p}m_{xy}]$	$[[01\bar1]]$				(14)	$[\underline{m}^{\star}_xm^{\star}_{yz}m_{y\bar{z}} ]$	$[\underline{m}^{\star}_x]$	$[\underline{m}^{\star}_x\underline2^{\star}_{yz}m_{y\bar{z}} ]$	SR
$[\bar3_{p}m_{x\bar{y}}]$	$[m^{\star}_x]$ , $[m^{\star}_{yz} ]$	$[m_z \bar3_{p}m_{xy}]$	$[[01\bar1]]$				(14)	$[m^{\star}_x\underline{m}^{\star}_{yz}m_{y\bar{z}} ]$	$[\underline{m}^{\star}_{yz}]$	$[\underline2^{\star}_x\underline{m}^{\star}_{yz}m_{y\bar{z}} ]$	SR

^† Equations for directions of axes and shear angle $[\varphi]$ : $[\matrix{\pmatrix{a &f &e \cr f &b &d \cr e &d &c \cr}\quad\quad\quad\quad\quad\quad\quad\quad\quad\hfill& \pmatrix{a & d & 0 \cr d & b & 0 \cr 0 & 0 & c \cr}\hfill& \pmatrix{a & 0 & 0 \cr 0 & b & d \cr 0 & d & c \cr}\hfill\cr (a)\quad [001]\quad[1 {{\displaystyle d}\over{\displaystyle e}} 0]\hfill & (b)\quad [\bar1 \alpha 0]\quad [\alpha10]\hfill & (d)\quad[110] \quad [1\bar1 {{\displaystyle 2d}\over{\displaystyle a-b}}]\hfill\cr &\alpha={{\displaystyle 2d+\sqrt{(a-b)^2+4d^2}}\over{\displaystyle a-b}}\hfill& (e)\quad[\bar1\sqrt30]\quad [\sqrt31{{\displaystyle 4d}\over{\displaystyle b-a}}]\hfill\cr & (c)\quad[\bar1 \beta 0] \quad [\beta 10]\hfill& (f)\quad[\sqrt310]\quad [\bar1\sqrt3{{\displaystyle 4\sqrt3}\over{\displaystyle 3(a-b)}}]\hfill\cr & \beta={{\displaystyle(a-b)+2\sqrt{3}d+4\sqrt{(a-b)^2+4d^2}}\over{\displaystyle \sqrt3(a-b)-2d}}\hfill &\cr&&&\cr(1)\quad 2 \sqrt{d^2+e^2}\hfill & (2)\quad 2|d|\hfill & (5)\quad \sqrt{(a-b)^2+2d^2}\hfill\cr &(3)\quad {{1}\over{2}}\sqrt{(a-b)^2+4d^2}\hfill &(6)\quad {{\sqrt3}\over{2}}\sqrt{(a-b)^2+4d^2}\hfill\cr &(4)\quad {{\sqrt3}\over{2}}\sqrt{(a-b)^2+4d^2}\hfill & (7)\quad 2|d|\hfill\cr &&&\cr &&&\cr\pmatrix{a & b & -d \cr b & a & d \cr -d & d & c \cr}\hfill & \pmatrix{a & 0 & 0 \cr 0 & b & 0 \cr 0 & 0 & c \cr}\hfill & \pmatrix{a & d & 0 \cr d & a & 0 \cr 0 & 0 & c \cr}\hfill\cr (g)\quad[100]\quad[0\bar1 {{\displaystyle d}\over{\displaystyle b}}]\hfill & &(h)\quad[101]\quad[\bar1 {{\displaystyle 2d}\over{\displaystyle c-d}}1]\hfill\cr &&&\cr (8)\quad 2\sqrt{a^2+b^2}\hfill & (9)\quad {{\sqrt3}\over{2}} |a-b|\hfill & (11)\quad \sqrt{(a-c)^2+2d^2}\hfill\cr &(10)\quad|a-b|\hfill &(12)\quad 2|d|\hfill\cr &&&\cr &&&\cr\pmatrix{a & 0 & 0 \cr 0 & a & 0 \cr 0 & 0 & c \cr}\hfill&\pmatrix{a & d & d \cr d & a & d \cr d & d & a \cr}\hfill &\cr(13)\quad |a-c|\hfill & (14)\quad 2\sqrt2 |d|\hfill &\cr} ]$