Table 1.11.2.1

Dmitrienko, V. E.; Kirfel, A.; Ovchinnikova, E. N.

doi:10.1107/97809553602060000910

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

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International Tables for Crystallography (2013). Vol. D. ch. 1.11, p. 271

Table 1.11.2.1

V. E. Dmitrienko,^a ^* A. Kirfel^b and E. N. Ovchinnikova^c

^a A. V. Shubnikov Institute of Crystallography, Leninsky pr. 59, Moscow 119333, Russia,^bSteinmann Institut der Universität Bonn, Poppelsdorfer Schloss, Bonn, D-53115, Germany, and ^cFaculty of Physics, M. V. Lomonosov Moscow State University, Leninskie Gory, Moscow 119991, Russia
Correspondence e-mail: dmitrien@crys.ras.ru

Table 1.11.2.1 | top | pdf |
The indices $[\ell]$ of the screw-axis/glide-plane forbidden reflections ( $[n = 0, \pm 1, \pm 2,\ldots]$ ) and independent components of their tensorial structure factors $[F^{{\bf H}}_{jk}]$

Other components: $[F^{{\bf H}}_{yy}=-F^{{\bf H}}_{xx}]$ , $[F^{{\bf H}}_{zz}=0]$ , $[F^{{\bf H}}_{jk}=F^{{\bf H}}_{kj}]$ . The direction of the z axis is selected along the corresponding screw axes. The last column lists different types of polarization properties defined in Section 1.11.3.

$[\ell]$	$[F^{{\bf H}}_{xx}]$	$[F^{{\bf H}}_{xy}]$	$[F^{{\bf H}}_{xz}]$	$[F^{{\bf H}}_{yz}]$	Type
	0	0			I
$[3n\pm 1]$		$[\mp iF_1]$		$[\pm iF_2]$	II
$[3n\pm 1]$		$[\pm iF_1]$		$[\mp iF_2]$	II
$[4n\pm 1]$	0	0		$[\pm iF_1]$	I
			0	0	II
			0	0	II
$[4n\pm 1]$	0	0		$[\mp iF_1]$	I
			0	0	II
$[6n\pm 1]$	0	0		$[\pm iF_1]$	I
$[6n\pm 2]$		$[\pm iF_1]$	0	0	II
	0	0	0	0
$[3n\pm 1]$		$[\pm iF_1]$	0	0	II
	0	0	0	0
$[3n\pm 1]$		$[\mp iF_1]$	0	0	II
$[6n\pm 1]$	0	0		$[\mp iF_1]$	I
$[6n\pm 2]$		$[\mp iF_1]$	0	0	II
	0	0	0	0
	0			0	II