Research/Sitter/MAGNDATA / 1.573_FeSO4.mcif

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Spin lattice of FeSO4Spin lattice of FeSO4

FeSO4

MAGNDATA entry 1.573 · 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 ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 14 K (−259 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPc 21/c BNS 14.82
Parent space groupP b n m No. 62
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 1/2 0] 1k
Cella 9.59 · b 17.43 · c 6.804 Å · α 90° · β 90° · γ 90°
Transition14 K (−259 °C)
Measured at4.2 K
Magnetic ionsFe
Largest moment component4.11 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 Pc 21/c →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1_1Fe0003.574.1105.444
Fe1_2Fe0.250.250−3.57−4.1105.444
S1_1S0.4940.1680.75
S1_2S0.7440.0820.25
O1_1O0.1360.19250.75
O1_2O0.3860.05750.25
O2_1O0.4750.07250.75
O2_2O0.7250.17750.25
O3_1O0.15650.0630.071
O3_2O0.40650.1870.929

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. Kirfel et al. phys. stat. sol. (a) (1977) · doi:10.1002/pssa.2210400210

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.573_FeSO4.mcif from MAGNDATA · entry page

sha256 of this copy: aa9196ea4e229578996b3496782355733bf2c92a88fbf2c5b8e04f6b0372365b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.573_FeSO4.mcif.