Research/Sitter/MAGNDATA / 1.232_CuMnSb.mcif

CuMnSb

MAGNDATA entry 1.232 · source

antiferromagnet

No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.

Spin group ¹3̄¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 34.3 K (−239 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	C_c c BNS 9.40
Parent space group	F 4 3 m No. 216
Spins	collinear · net moment 0 μ_B per cell
Propagation	[1/2 1/2 1/2] 1k
Cell	a 12.19 · b 12.19 · c 12.19 Å · α 90° · β 90° · γ 90°
Transition	34.3 K (−239 °C)
Measured at	4 K
Magnetic ions	Mn
Largest moment component	2.53 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 C_c c →

Atom sites · 3 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Cu1	Cu	0	0	0
Mn1	Mn	0.125	0.125	0.125	2.53	1.39	2.53	3.8385
Sb1	Sb	0.375	0.375	0.375

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

A. Regnat et al. Physical Review Materials (2018) · doi:10.1103/PhysRevMaterials.2.054413

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.232_CuMnSb.mcif from MAGNDATA · entry page

sha256 of this copy: ab435cf61618d41894034ed5a316ae7b160ab04bd1886cf27104558cd81373f2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.232_CuMnSb.mcif.