Research/Sitter/MAGNDATA / 0.866_Pr2NiIrO6.mcif

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Spin lattice of Pr2Ni1Ir1O6Spin lattice of Pr2Ni1Ir1O6

Pr2Ni1Ir1O6

MAGNDATA entry 0.866 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 103 K (−170 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21/c BNS 14.75
Point group2/m
Parent space groupP 21/n’ No. 14
Spinsnoncoplanar · net moment 4.6 μB per cell
Propagation[0 0 0] 1k
Cella 5.4764 · b 5.6794 · c 7.8046 Å · α 90° · β 90.02° · γ 90°
Transition103 K (−170 °C)
Measured at3 K
Magnetic ionsIr, Ni, Pr
Largest moment component2.3 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 · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni000.502.302.3
Ir2Ir000.5
Ir1Ir0001.301.62.0612
Ni2Ni000
Pr1Pr0.98730.44250.25010.93000.93
O1O0.08860.02860.248
O2O0.1960.28560.9608
O3O0.2920.80340.9431

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

P. Kayser et al. Acta Materialia (2021) · doi:10.1016/j.actamat.2021.116684

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.866_Pr2NiIrO6.mcif from MAGNDATA · entry page

sha256 of this copy: c52c1cb2d62c34878eeabf764d3fa729d41b119f38875dfc842a30fa8fc6ad6c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.866_Pr2NiIrO6.mcif.