Research/Sitter/MAGNDATA / 1.865_Ba2YbFeO5.mcif

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Spin lattice of Ba2Yb1Fe1O5Spin lattice of Ba2Yb1Fe1O5

Ba2Yb1Fe1O5

MAGNDATA entry 1.865 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 9.8 K (−263 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21/c BNS 14.80
Point group2/m1′
Parent space groupP 21/c No. 14
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 24.9253 · b 6.01762 · c 15.5748 Å · α 90° · β 92.198° · γ 90°
Transition9.8 K (−263 °C)
Measured at1.8 K
Magnetic ionsFe, Yb
Largest moment component4.01 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 Pa 21/c →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.07450.24610.0074
Ba2Ba0.05720.24980.2511
YbYb0.43510.25340.1170.40.062.962.9723
FeFe0.45670.24380.37790.920.224.014.0856
O1O0.4360.2680.2632
O2O0.16060.22790.2204
O3O0.11560.05220.3687
O4O0.25970.0330.1326
O5O0.24380.52110.1439

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

V. Hardy et al. Phys. Rev. B (2025) · doi:10.1103/xdgh-1vr4

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.865_Ba2YbFeO5.mcif from MAGNDATA · entry page

sha256 of this copy: 0ea62374165e5a96a4fa485806797bcbc159e01a9803f85de1ce02e405d05548
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.865_Ba2YbFeO5.mcif.