Research/Sitter/MAGNDATA / 0.612_Cu2OSO4.mcif

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Spin lattice of Cu2OSO4Spin lattice of Cu2OSO4

Cu2OSO4

MAGNDATA entry 0.612 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 19.7 K (−253 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2/m BNS 12.58
Parent space groupC 2/m No. 12
Spinscoplanar · net moment 1.56 μB per cell
Propagation[0 0 0] 1k
Cella 9.355 · b 6.312 · c 7.628 Å · α 90° · β 122.29° · γ 90°
Transition19.7 K (−253 °C)
Measured at1.5 K
Magnetic ionsCu
Largest moment component0.86 μB
MethodNPD and 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 2/m →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu0.250.2500.83−0.470.30.8566
Cu2Cu0.072400.21800.8600.86
S1S0.10190.50.316
O1O0.20550.50.2235
O2O0.29300.45
O3O0.152500.021
O4O0.4940.18920.245

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. Y. Favre et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.094422

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.612_Cu2OSO4.mcif from MAGNDATA · entry page

sha256 of this copy: 4124d9284f91d472504f42f4732553c6626fbf4f2f019364e3e9f3c84706f187
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.612_Cu2OSO4.mcif.