Research/Sitter/MAGNDATA / 0.1152_Bi2CoO2F4.mcif

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Spin lattice of Bi2Co1O2F4Spin lattice of Bi2Co1O2F4

Bi2Co1O2F4

MAGNDATA entry 0.1152 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
Structure · 10 properties
Magnetic groupP c′ a′ 21 BNS 29.103
Point groupm′m′2
Parent space groupP 21 a b No. 29
Spinscoplanar · net moment 2.8 μB per cell
Propagation[0 0 0] 1k
Cella 5.4317 · b 5.4313 · c 16.348 Å · α 90° · β 90° · γ 90°
Measured at5 K
Magnetic ionsCo
Largest moment component2.37 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 c′ a′ 21 →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Bi1Bi0.0060.010.078
Bi2Bi0.5080.0090.5767
Co1Co00.980.7480.7−2.3702.4712
F1F0.2070.290.7847
F2F0.8050.1980.2712
F3F0.0240.9280.873
F4F0.5190.9330.374
O1O0.2520.2410.9941
O2O0.7430.2540.4991

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

Euan A. S. Scott et al. Chem. Mater. (2022) · doi:10.1021/acs.chemmater.2c02745

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1152_Bi2CoO2F4.mcif from MAGNDATA · entry page

sha256 of this copy: 856ce3a54dca1b931405ddfa6eeacaa4ee0cfe43748641c6ab4826062749595f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1152_Bi2CoO2F4.mcif.