Research/Sitter/MAGNDATA / 0.616_HoB2.mcif

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Spin lattice of HoB2Spin lattice of HoB2

HoB2

MAGNDATA entry 0.616 · 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 ≤ 15 K (−258 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/m′ BNS 12.62
Parent space groupP 6/m m m No. 191
Spinscollinear · net moment 6.745 μB per cell
Propagation[0 0 0] 1k
Cella 3.2849 · b 3.2849 · c 3.8183 Å · α 90° · β 90° · γ 120°
Transition15 K (−258 °C)
Measured at2 K
Magnetic ionsHo
Largest moment component5.31 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 C 2′/m′ →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho00004.165.316.7455
B1B0.33330.66670.5

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

N. Terada et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.094435

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.616_HoB2.mcif from MAGNDATA · entry page

sha256 of this copy: 8bd47d699917c2f47fa03437919156d7bda3936906a862f24dbedd17c78dae2a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.616_HoB2.mcif.