Research/Sitter/MAGNDATA / 1.99_CsCoCl3(D2O)2.mcif

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Spin lattice of CsCoCl3(D2O)2Spin lattice of CsCoCl3(D2O)2

CsCoCl3(D2O)2

MAGNDATA entry 1.99 · 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 ≤ 3.4 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPb c c n BNS 56.372
Point groupmmm1′
Parent space groupP c c a No. 54
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1/2 0] 1k
Cella 8.889 · b 14.236 · c 11.313 Å · α 90° · β 90° · γ 90°
Transition3.4 K (−270 °C)
Measured at1.3 K
Magnetic ionsCo
Largest moment component2.4 μB
MethodNPD

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 Pb c c n →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Cs1Cs0.2500.15
Co1Co00.2390.250.702.42.5
Cl1Cl0.250.250.15
Cl2Cl0.0870.1150.391
O1O0.0650.3640.363
D1D0.0270.3370.444
D2D0.1660.3380.383

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

A.L.M. Bongaarts et al. PHYSICAL REVIEW B (1972) · doi:10.1103/PhysRevB.6.2669

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.99_CsCoCl3(D2O)2.mcif from MAGNDATA · entry page

sha256 of this copy: cb0a7164d98f4ecd935b57ce1d29da97ff5fe4efe07ebf47c9ae0485a097c87f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.99_CsCoCl3(D2O)2.mcif.