Research/Sitter/MAGNDATA / 0.648_(Ho0.8Mn0.2)MnO3.mcif

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Spin lattice of (Ho0.8Mn0.2)MnO3Spin lattice of (Ho0.8Mn0.2)MnO3

(Ho0.8Mn0.2)MnO3

MAGNDATA entry 0.648 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 76 K (−197 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n m′ a′ BNS 62.447
Parent space groupP n m a No. 62
Spinscollinear · net moment 7.36 μB per cell
Propagation[0 0 0] 1k
Cella 5.6329 · b 7.3908 · c 5.2461 Å · α 90° · β 90° · γ 90°
Transition76 K (−197 °C)
Measured at40 K
Magnetic ionsHo, Mn
Largest moment component2.2 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 n m′ a′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho0.07830.250.9834−2.02002.02
Mn1Mn0.07830.250.9834−2.02002.02
Mn2Mn000.52.2002.2
O1O0.46190.250.1059
O2O0.31830.05340.6983

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. Donni et al. Journal of Alloys and Compounds (2021) · doi:10.1016/j.jallcom.2020.158230

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.648_(Ho0.8Mn0.2)MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: a5fa81697771610c33f3a451da27e76326e7b2e19c2c24423aa8f83b7feb50cd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.648_(Ho0.8Mn0.2)MnO3.mcif.