Research/Sitter/MAGNDATA / 0.264_Fe3(PO4)2.mcif

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Spin lattice of Fe3(PO4)2Spin lattice of Fe3(PO4)2

Fe3(PO4)2

MAGNDATA entry 0.264 · 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 ≤ 44 K (−229 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21/c′ BNS 14.78
Parent space groupP 21/c No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 6.0137 · b 4.7727 · c 10.4052 Å · α 90° · β 90.94° · γ 90°
Transition44 K (−229 °C)
Measured at10.1 K
Magnetic ionsFe
Largest moment component4.31 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 21/c′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.500
Fe2Fe0.23750.98480.2821−4.31004.31
P1P0.26020.43270.1005
O1O0.27780.75470.1042
O2O0.25330.1810.4638
O3O0.07160.32450.182
O4O0.4680.28520.1627

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

J.K. Warner et al. J. MATER. CHEM. (1992) · doi:10.1039/JM9920200191

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.264_Fe3(PO4)2.mcif from MAGNDATA · entry page

sha256 of this copy: da3603201964420dff30b1d2c46cfc354f54b573d5096595ffe2d6404b6fae8b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.264_Fe3(PO4)2.mcif.