Research/Sitter/MAGNDATA / 1.864_Ba2TbFeO5.mcif

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Spin lattice of Ba2Tb1Fe1O5Spin lattice of Ba2Tb1Fe1O5

Ba2Tb1Fe1O5

MAGNDATA entry 1.864 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 14 K (−259 °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/n No. 14
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 25.3043 · b 6.08178 · c 15.5904 Å · α 90° · β 92.4029° · γ 90°
Transition14 K (−259 °C)
Measured at1.6 K
Magnetic ionsFe, Tb
Largest moment component8.31 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 Pa 21/c →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.07930.26110.0117
Ba2Ba0.05830.25470.2535
TbTb0.43560.25040.11298.310.13−0.038.3123
FeFe0.45780.23420.37994.051.960.184.4962
O1O0.43850.26540.2625
O2O0.15750.23090.2119
O3O0.11340.060.3792
O4O0.26210.04950.1442
O5O0.23790.54370.136

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

⬇ 1.864_Ba2TbFeO5.mcif from MAGNDATA · entry page

sha256 of this copy: 9e4ba04dd854c79258cde2f434b6ec99dee80a508b22338a83f571db2975c44f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.864_Ba2TbFeO5.mcif.