Research/Sitter/MAGNDATA / 0.871_Pr2NiIrO6.mcif

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Spin lattice of Pr2Ni1Ir1O6Spin lattice of Pr2Ni1Ir1O6

Pr2Ni1Ir1O6

MAGNDATA entry 0.871 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 110 K (−163 °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
Spinscoplanar · net moment 4.06 μB per cell
Propagation[0 0 0] 1k
Cella 5.4697 · b 5.6718 · c 7.7852 Å · α 90° · β 90.01° · γ 90°
Transition110 K (−163 °C)
Measured at20 K
Magnetic ionsIr, Ni, Pr
Largest moment component1.65 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 · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni000.50.811.6501.8381
Ir1Ir0000.32−0.3200.4525
Pr1Pr0.01610.5610.7590.210.3500.4082
O1O0.09740.02610.26
O2O0.2010.2865−0.053
O3O0.1970.31050.547

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

C. Ritter et al. PHYSICAL REVIEW MATERIALS (2022) · doi:10.1103/PhysRevMaterials.6.084405

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.871_Pr2NiIrO6.mcif from MAGNDATA · entry page

sha256 of this copy: 3fa709dcce308eec5f6dc13cc8e828bdcb78c969a2e32597f68535b10aabe8aa
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.871_Pr2NiIrO6.mcif.