Research/Sitter/MAGNDATA / 0.1191_CuCoFe2O5.mcif

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Spin lattice of CuCoFe2O5Spin lattice of CuCoFe2O5

CuCoFe2O5

MAGNDATA entry 0.1191 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 77 K (−196 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2′/c′ BNS 15.89
Point group2′/m′
Parent space groupC m c m No. 63
Spinsnoncoplanar · net moment 14.187 μB per cell
Propagation[0 0 0] 1k
Cella 2.8866 · b 9.7493 · c 12.5235 Å · α 90° · β 90° · γ 90°
Transition77 K (−196 °C)
Measured at5 K
Magnetic ionsCo, Cu, Fe
Largest moment component2.1 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 C 2′/c′ →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu00.51750.2260.90−1.11.4213
Co1Co00.51750.2260.90−1.11.4213
Co2Co0000.91.1−2.12.5357
Cu2Cu0000.91.1−2.12.5357
Fe2Fe0000.91.1−2.12.5357
Fe3Fe0.50.76150.1149−0.9−1.12.12.5357
Co3Co0.50.76150.1149−0.9−1.12.12.5357
O1O0.50.6650.75
O2O00.09860.1409
O3O0.5−0.1470.0479

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

Leelashree Solaiappan et al. Chem. Mater. (2026) · doi:10.1021/acs.chemmater.6c00764

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1191_CuCoFe2O5.mcif from MAGNDATA · entry page

sha256 of this copy: 9301bd7ffe30eb412124205a1efa460b25e1a0f21bbbaba76c95e929a82ec902
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1191_CuCoFe2O5.mcif.