Research/Sitter/MAGNDATA / 1.439_BaCoF4.mcif

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Spin lattice of BaCoF4Spin lattice of BaCoF4

BaCoF4

MAGNDATA entry 1.439 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 69.6 K (−204 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPb c a 21 BNS 29.105
Parent space groupA 21 a m No. 36
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 5.8519 · b 14.628 · c 8.4204 Å · α 90° · β 90° · γ 90°
Transition69.6 K (−204 °C)
Measured at4.7 K
Magnetic ionsCo
Largest moment component3.4 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 a 21 →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.46050.85220
Co1Co00.412703.4003.4
F1F0.19810.30180
F2F0.72710.33360
F3F0.32070.47180
F4F0.01120.92060

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

M. Eibschutz et al. PHYSICAL REVIEW B (1972) · doi:10.1103/PhysRevB.6.2677

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.439_BaCoF4.mcif from MAGNDATA · entry page

sha256 of this copy: 9d7fc2853a559b80ff52896dff6c44ae3d914c2ad5d9b4c4661162f007adc02f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.439_BaCoF4.mcif.