Research/Sitter/MAGNDATA / 1.0.35_CsMnBr3.mcif

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Spin lattice of CsMnBr3Spin lattice of CsMnBr3

CsMnBr3

MAGNDATA entry 1.0.35 · 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 ≤ 8.3 K (−265 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 6 2′ m′ BNS 189.225
Parent space groupP 63/m m c No. 194
Spinscoplanar · net moment 0 μB per cell
Propagation[1/3 1/3 0] 1k
Cella 13.1792 · b 13.1792 · c 6.52 Å · α 90° · β 90° · γ 120°
Transition8.3 K (−265 °C)
Measured at4.5 K
Magnetic ionsMn
Largest moment component3 μB
MethodNSD

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 6 2′ m′ →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0003003
Cs1_1Cs0.333300.75
Cs1_2Cs0.666700.25
Cs1_3Cs0.33330.33330.25
Br1_1Br0.33330.82840.25
Br1_2Br0.17160.5050.25
Br1_3Br0.33330.5050.75
Br1_4Br0.4950.82840.75

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

Source

M. Eibschutz et al. AIP Conference Proceedings 10, 684 (1973) (1973) · doi:10.1063/1.2946992

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.35_CsMnBr3.mcif from MAGNDATA · entry page

sha256 of this copy: fdeab9f964e97c4f4f9779bdc2494c57e5f65007569680ea70f546dbb3eee681
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.35_CsMnBr3.mcif.