Research/Sitter/MAGNDATA / 1.321_Ba2FeWO6.mcif

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Spin lattice of Ba2FeWO6Spin lattice of Ba2FeWO6

Ba2FeWO6

MAGNDATA entry 1.321 · 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 ¹1̄ × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 25 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPS 1 BNS 2.7
Parent space groupI 4/m No. 87
Spinscollinear · net moment 0 μB per cell
Propagation[0 1/2 1/2] 1k
Cella 5.7446 · b 11.4892 · c 16.2198 Å · α 90° · β 90° · γ 90°
Transition25 K (−248 °C)
Measured at10 K
Magnetic ionsFe
Largest moment component2.87 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 PS 1 →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba00.250.125
Fe1Fe000.25−0.612.87−1.773.4266
W1W000
O1O000.1205
O2_1O0.2390.11750
O2_2O0.7650.11950

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

A. Azad et al. Materials Research Bulletin (2002) · doi:10.1016/S0025-5408(02)00872-3

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.321_Ba2FeWO6.mcif from MAGNDATA · entry page

sha256 of this copy: 61991f9df98570b0f98f47be0875979f3d277a297f6ea1ea29b3029ca4c13962
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.321_Ba2FeWO6.mcif.