Table 1.2.3.1

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

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International Tables for Crystallography (2006). Vol. D. ch. 1.2, p. 49

T. Janssen^a ^*

^a Institute for Theoretical Physics, University of Nijmegen, 6524 ED Nijmegen, The Netherlands
Correspondence e-mail: ted@sci.kun.nl

Table 1.2.3.1 | top | pdf |
Choices of $[{\bf k}]$ in the fundamental domain of [Pnma] and the elements of $[K_{\bf k}]$

$[{\bf k}]$	Wyckoff position	Elements
	a		$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
$[{{1}\over{2}}]$ 00	b		$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
0 $[{{1}\over{2}}]$ 0	e		$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
00 $[{{1}\over{2}}]$	c		$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
0 $[{{1}\over{2}}{{1}\over{2}}]$	g	E	$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
$[{{1}\over{2}} 0{{1}\over{2}}]$	d	E	$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
$[{{1}\over{2}} {{1}\over{2}} 0]$	f	E	$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
$[{{1}\over{2}}{{1}\over{2}}{{1}\over{2}}]$	h	E	$[m_{x}]$	$[m_{y}]$	$[m_{z}]$	$[\bar{1}]$	2_x	2_y	2_z
$[\xi]$ 00	i	E	$[m_{y}]$	$[m_{z}]$	2_x
$[\xi{{1}\over{2}} 0]$	k	E	$[m_{y}]$	$[m_{z}]$	2_x
$[\xi 0{{1}\over{2}}]$	j	E	$[m_{y}]$	$[m_{z}]$	2_x
$[\xi {{1}\over{2}}{{1}\over{2}}]$	l	E	$[m_{y}]$	$[m_{z}]$	2_x
$[0\eta 0]$	m	E	$[m_{x}]$	$[m_{z}]$	2_y
$[{{1}\over{2}}\eta 0]$	o	E	$[m_{x}]$	$[m_{z}]$	2_y
$[0\eta {{1}\over{2}}]$	n	E	$[m_{x}]$	$[m_{z}]$	2_y
$[{{1}\over{2}} \eta {{1}\over{2}}]$	p	E	$[m_{x}]$	$[m_{z}]$	2_y
$[00\zeta]$	q	E	$[m_{x}]$	$[m_{y}]$	2_z
$[{{1}\over{2}} 0\zeta]$	s	E	$[m_{x}]$	$[m_{y}]$	2_z
$[0{{1}\over{2}} \zeta]$	r	E	$[m_{x}]$	$[m_{y}]$	2_z
$[{{1}\over{2}}{{1}\over{2}}\zeta]$	t	E	$[m_{x}]$	$[m_{y}]$	2_z
$[0\eta\zeta]$	u	E	$[m_{x}]$
$[{{1}\over{2}}\eta\zeta]$	v	E	$[m_{x}]$
$[\xi 0 \zeta]$	w	E	$[m_{y}]$
$[\xi {{1}\over{2}} \zeta]$	x	E	$[m_{y}]$
$[\xi\eta 0]$	y	E	$[m_{z}]$
$[\xi\eta {{1}\over{2}}]$	z	E	$[m_{z}]$
$[\xi\eta\zeta]$	$[\alpha]$	E