Research/Sitter/MAGNDATA / 0.91_Rb2Fe2O(AsO4)2.mcif

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Spin lattice of Rb2Fe2O9As2Spin lattice of Rb2Fe2O9As2

Rb2Fe2O9As2

MAGNDATA entry 0.91 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 25 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m a′ BNS 62.448
Point groupm′m′m
Parent space groupP n m a No. 62
Spinsnoncoplanar · net moment 1.36 μB per cell
Propagation[0 0 0] 1k
Cella 8.5331 · b 5.7892 · c 18.611 Å · α 90° · β 90° · γ 90°
Transition25 K (−248 °C)
Measured at4 K
Magnetic ionsFe
Largest moment component3.1 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 n′ m a′ →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Rb1Rb0.88880.250.8628
Rb2Rb0.03790.250.2679
Fe1Fe0.28440.250.434703.103.1
Fe2Fe000.5−0.5−2.761.33.0915
As1As0.82040.250.6426
As2As0.67580.250.444
O1O1.0580.250.4375
O2O0.9610.250.576
O3O0.76660.01080.4785
O4O0.49230.250.4744
O5O0.70430.01270.6338
O6O0.68430.250.3556
O7O0.9130.250.7197

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

Garlea, V.O. et al. PHYSICAL REVIEW B (2014) · doi:10.1103/PhysRevB.89.014426

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.91_Rb2Fe2O(AsO4)2.mcif from MAGNDATA · entry page

sha256 of this copy: 9cdbbea32470cd56d93bc1ed28c42b1bf05c29f3d0d6d1b94751ed1573df0ba4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.91_Rb2Fe2O(AsO4)2.mcif.