Research/Sitter/MAGNDATA / 1.320_Sr2FeWO6.mcif

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Spin lattice of Sr2FeWO6Spin lattice of Sr2FeWO6

Sr2FeWO6

MAGNDATA entry 1.320 · 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 ≤ 35 K (−238 °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 groupP 21/n No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[0 1/2 1/2] 1k
Cella 5.648 · b 11.2176 · c 15.8724 Å · α 90° · β 89.99° · γ 90°
Transition35 K (−238 °C)
Measured at10 K
Magnetic ionsFe
Largest moment component3.63 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 · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1_1Sr0.99760.49440.3755
Sr1_2Sr0.50240.74440.8745
Fe1_1Fe0.500.25−3.630.391.243.8555
Fe1_2Fe00.250−3.630.391.243.8555
W1_1W0.500
W1_2W00.250.25
O1_1O0.280.13050.0103
O1_2O0.220.38050.2397
O2_1O0.2410.3890.0155
O2_2O0.2590.6390.2346
O3_1O0.04950.25350.3695
O3_2O0.45050.50350.8805

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

⬇ 1.320_Sr2FeWO6.mcif from MAGNDATA · entry page

sha256 of this copy: f519f16b57411c9b69023c8e6e4af688ff2578ddbd97fabd2222ec8da23cce18
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.320_Sr2FeWO6.mcif.