Research/Sitter/MAGNDATA / 0.1143_Fe4Nb2O9.mcif

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Spin lattice of Fe4Nb2O9Spin lattice of Fe4Nb2O9

Fe4Nb2O9

MAGNDATA entry 0.1143 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 87.5 K (−186 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2/c′ BNS 15.88
Point group2/m′
Parent space groupC 2/c No. 15
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 9.0861 · b 5.197 · c 14.234 Å · α 90° · β 91.29° · γ 90°
Transition87.5 K (−186 °C)
Measured at1.5 K
Magnetic ionsFe
Largest moment component4.675 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 C 2/c′ →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Nb1Nb0.0010.99960.6428
Fe1Fe0.83410.49850.69113.651−0.204−0.8633.776
Fe2Fe0.83580.50440.48524.6750.484−2.1515.2124
O1O0.8450.8210.0863
O2O0.6720.3550.0858
O3O0.9860.3280.0833
O4O00.7220.25
O5O0.1410.1450.25

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

Raktim Datta et al. PHYSICAL REVIEW B (2025) · doi:10.1103/9tgw-l1nj

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1143_Fe4Nb2O9.mcif from MAGNDATA · entry page

sha256 of this copy: 8b58905ef80675c2d780f176b6c251313c79e497ecf6e1b43faa2d32e3335d92
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1143_Fe4Nb2O9.mcif.