Research/Sitter/MAGNDATA / 0.108_Mn3Ir.mcif

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Spin lattice of Mn3IrSpin lattice of Mn3Ir

Mn3Ir

MAGNDATA entry 0.108 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 960 K (687 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupR 3m′ BNS 166.101
Point group3m′
Parent space groupP m 3m No. 221
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 3.77 · b 3.77 · c 3.77 Å · α 90° · β 90° · γ 90°
Transition960 K (687 °C)
Measured at300 K
Magnetic ionsMn
Largest moment component2 μB
MethodNSD

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 R 3m′ →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Ir1Ir000
Mn1Mn00.50.52−1−12.4495

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

I. Tomeno et al. Journal of Applied Physics (1999) · doi:10.1063/1.371298

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.108_Mn3Ir.mcif from MAGNDATA · entry page

sha256 of this copy: 28d119b570d463e654480f47370a78028ac340b96315cb6645acd517ab0fd844
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.108_Mn3Ir.mcif.