Research/Sitter/MAGNDATA / 1.133_CuSb2O6.mcif

CuSb₂O₆

MAGNDATA entry 1.133 · source

noncollinear antiferromagnet

All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).

ordered ≤ 8.7 K (−264 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	P_a 2₁/c BNS 14.80
Point group	2/m1′
Parent space group	P 2₁/n No. 14
Spins	coplanar · net moment 0 μ_B per cell
Propagation	[1/2 0 1/2] 1k
Cell	a 9.2698 · b 4.637 · c 18.5862 Å · α 90° · β 91.12° · γ 90°
Transition	8.7 K (−264 °C)
Measured at	2 K
Magnetic ions	Cu
Largest moment component	0.49 μ_B
Method	NSD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P_a 2₁/c →

Atom sites · 5 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Cu1	Cu	0	0	0	−0.15	0.49	0	0.5124
Sb1	Sb	0.0006	0.008	0.1669
O1	O	0.1565	0.2983	0.0008
O2	O	0.1495	0.3176	0.1646
O3	O	0.3494	0.7085	0.1624

Moment components are along the crystal axes a, b, c (μ_B), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

B. Gibson et al. Journal of Magnetism and Magnetic Materials (2004) · doi:10.1016/j.jmmm.2003.12.006

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.133_CuSb2O6.mcif from MAGNDATA · entry page

sha256 of this copy: bccb326da95bf9a915d198737ef5f31b858be2b8de780d09a505f886aa73283f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.133_CuSb2O6.mcif.