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Spin lattice of FeF3(H2O)2H2OSpin lattice of FeF3(H2O)2H2O

FeF3(H2O)2H2O

MAGNDATA entry 1.157 · 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 ¹4/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 20 K (−253 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPb 21/c BNS 14.81
Point group2/m1′
Parent space groupP 4/n No. 85
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 7.80949 · b 7.80949 · c 7.753338 Å · α 90° · β 90° · γ 90°
Transition20 K (−253 °C)
Measured at1.8 K
Magnetic ionsFe
Largest moment component3.23 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 21/c →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.250.250.42593.23003.23
F1F0.250.250.1764
O11O0.250.750.25
O1_1O0.85270.97690.0707
O1_2O0.52310.85270.0707
F2_1F0.85270.97690.0707
F2_2F0.52310.85270.0707
H11_1H0.17770.92040.3645
H11_2H0.57960.17770.3645
H1_1H0.34810.7840.18
H1_2H0.7160.34810.18
H2_1H0.031500
H2_2H0.50.03150

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

G. Nenert et al. Dalton Trans. (2015) · doi:10.1039/c5dt02242h

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.157_FeF3(H2O)2H2O.mcif from MAGNDATA · entry page

sha256 of this copy: 5e610683f033d9070cbbf146954f402e47e142f5678a8d6c66edb8c962f3ecd1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.157_FeF3(H2O)2H2O.mcif.