Research/Sitter/MAGNDATA / 0.75_Cr2WO6.mcif

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Spin lattice of Cr2WO6Spin lattice of Cr2WO6

Cr2WO6

MAGNDATA entry 0.75 · 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 ¹4/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 45 K (−228 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ n m BNS 58.395
Point groupm′mm
Parent space groupP 42/m n m No. 136
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.582 · b 4.582 · c 8.87 Å · α 90° · β 90° · γ 90°
Transition45 K (−228 °C)
Magnetic ionsCr
Largest moment component1 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 n′ n m →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Cr1Cr000.33450101
W1W000
O1O0.3030.3030
O2O0.3060.3060.34

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. Zhu et al. PHYSICAL REVIEW LETTERS (2014) · doi:10.1103/PhysRevLett.113.076406

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.75_Cr2WO6.mcif from MAGNDATA · entry page

sha256 of this copy: 4c33b3aba35a07af27aaae2cd8f3c7a7138edac0178d417f36b532b4d4dd373e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.75_Cr2WO6.mcif.