Research/Sitter/MAGNDATA / 0.972_HoPdIn.mcif

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Spin lattice of Ho1Pd1In1Spin lattice of Ho1Pd1In1

Ho1Pd1In1

MAGNDATA entry 0.972 · 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 ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 22 K (−251 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 6 2′ m′ BNS 189.225
Point group6m′2′
Parent space groupP 6 2 m No. 189
Spinscollinear · net moment 24.3 μB per cell
Propagation[0 0 0] 1k
Cella 7.6249 · b 7.6249 · c 3.7717 Å · α 90° · β 90° · γ 120°
Transition22 K (−251 °C)
Measured at1.5 K
Magnetic ionsHo
Largest moment component8.1 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 6 2′ m′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho0.591800008.18.1
Pd1Pd000
Pd2Pd0.33330.66670.5
In1In0.254900.5

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

L. Gondek et al. Journal of Magnetism and Magnetic Materials (2005) · doi:10.1016/j.jmmm.2004.08.002

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.972_HoPdIn.mcif from MAGNDATA · entry page

sha256 of this copy: dd2d5177d7086c26a62b6b0481078d2bef7c1708735e0f28dc02da3edcbdb4ef
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.972_HoPdIn.mcif.