Research/Sitter/MAGNDATA / 0.31_HoMnO3.mcif

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Spin lattice of HoMnO3Spin lattice of HoMnO3

HoMnO3

MAGNDATA entry 0.31 · 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 ≤ 72 K (−201 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 63c′ m′ BNS 185.201
Point group6m′m′
Parent space groupP 63c m No. 185
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 6.1413 · b 6.1413 · c 11.4122 Å · α 90° · β 90° · γ 120°
Transition72 K (−201 °C)
Measured at60.9 K
Magnetic ionsMn
Largest moment component2.52 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 63c′ m′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho000.2731
Ho2Ho0.33330.66670.2306
Mn1Mn0.3224002.52002.52
O1O0.305400.16
O2O0.643300.3326
O3O000.4763
O4O0.33330.66670.017

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

A. Munoz et al. Chem. Mater. (2001) · doi:10.1021/cm0012264

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.31_HoMnO3.mcif from MAGNDATA · entry page

sha256 of this copy: 3014032f1283bac6c3505c9a91cd254ef9c6490700ed152c1df2a2ea730b7cc4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.31_HoMnO3.mcif.