Research/Sitter/MAGNDATA / 1.0.19_Cs2CoU3F16.mcif

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Spin lattice of Cs2CoU3F16Spin lattice of Cs2CoU3F16

Cs2CoU3F16

MAGNDATA entry 1.0.19 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 3.5 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63/m c′ m′ BNS 193.260
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 6.18 μB per cell
Propagation[1/3 1/3 0] · [0 0 0] 1k
Cella 23.9673 · b 23.9673 · c 13.006 Å · α 90° · β 90° · γ 120°
Transition3.5 K (−270 °C)
Measured at1.5 K
Magnetic ionsCo, U
Largest moment component1.7 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 P 63/m c′ m′ →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
U1_1U0.27670.55330.2500−0.910.91
U1_2U0.27670.88670.25000.910.91
Cs1Cs0.11110.22220.059
F1_1F0.05850.1170.25
F1_2F0.05850.45030.25
F2_1F000.25
F2_2F00.33330.25
F3_1F0.29320.58630.4114
F3_2F0.29320.91970.4114
F4_1F0.18410.36830.1563
F4_2F0.18410.70160.1563
Co1_1Co000001.71.7
Co1_2Co00.3333000−1.71.7

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

V.V. Klepov et al. J. Am. Chem. Soc. (2019) · doi:10.1021/jacs.9b00345

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.19_Cs2CoU3F16.mcif from MAGNDATA · entry page

sha256 of this copy: bd8b4b6877cc11f994fd217cd75b391c99de355477369b79f4da5f4b4279035d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.19_Cs2CoU3F16.mcif.