Research/Sitter/MAGNDATA / 0.868_Pr2NiIrO6.mcif

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Spin lattice of Pr2Ni1Ir1O6Spin lattice of Pr2Ni1Ir1O6

Pr2Ni1Ir1O6

MAGNDATA entry 0.868 · 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 2.4 μB per cell
Propagation[0 0 0] 1k
Cella 5.4702 · b 5.6648 · c 7.7853 Å · α 90° · β 90.07° · γ 90°
Transition110 K (−163 °C)
Measured at20 K
Magnetic ionsIr, Ni
Largest moment component1.5 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)
Ir1Ir000−0.1−0.300.3162
Pr1Pr0.0110.56330.75
Ni1Ni000.50.61.501.6155
O1O0.09470.02620.237
O2O0.1910.2890.964
O3O0.1960.2970.555

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

T. Ferreira et al. PHYSICAL REVIEW MATERIALS (2021) · doi:10.1103/PhysRevMaterials.5.064408

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.868_Pr2NiIrO6.mcif from MAGNDATA · entry page

sha256 of this copy: 5f04a9ecb68797e282f43381c9f0fb531660828b5d1cddd301385495bc93da00
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.868_Pr2NiIrO6.mcif.