Research/Sitter/MAGNDATA / 0.317_Ho2CoMnO6.mcif

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Spin lattice of Ho2CoMnO6Spin lattice of Ho2CoMnO6

Ho2CoMnO6

MAGNDATA entry 0.317 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 60 K (−213 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′/c′ BNS 14.79
Parent space groupP 21/c No. 14
Spinscollinear · net moment 11.68 μB per cell
Propagation[0 0 0] 1k
Cella 5.2192 · b 5.5636 · c 7.4522 Å · α 90° · β 89.77° · γ 90°
Transition60 K (−213 °C)
Measured at10 K
Magnetic ionsCo, Ho, Mn
Largest moment component2.8 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)
Ho1Ho0.01940.07240.2509
Co1Co0.500.50.840−2.82.9201
Mn1Mn0.5000.840−2.82.9201
O1O0.29990.31570.0518
O2O0.31980.29230.4451
O3O0.60470.96670.255

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

J. Blasco et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.96.024409

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.317_Ho2CoMnO6.mcif from MAGNDATA · entry page

sha256 of this copy: 6dcb5139aeae976b374139c3a1549c8e738f7f3e706e93f594373d170f755822
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.317_Ho2CoMnO6.mcif.