Research/Sitter/MAGNDATA / 0.436_TbNi4Si.mcif

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Spin lattice of TbNi4SiSpin lattice of TbNi4Si

TbNi4Si

MAGNDATA entry 0.436 · 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 ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 37 K (−236 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m m′ m′ BNS 65.486
Parent space groupC m m m No. 65
Spinscollinear · net moment 17.32 μB per cell
Propagation[0 0 0] 1k
Cella 5.0481 · b 8.2048 · c 3.9422 Å · α 90° · β 90° · γ 90°
Transition37 K (−236 °C)
Measured at1.5 K
Magnetic ionsNi, Tb
Largest moment component8.66 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 m m′ m′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb00008.6608.66
Ni1Ni00.34030
Ni2Ni0.250.250.5
Si1Si0.500.5

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

A. Morozkin et al. Journal of Magnetism and Magnetic Materials (2014) · doi:10.1016/j.jmmm.2014.04.057

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.436_TbNi4Si.mcif from MAGNDATA · entry page

sha256 of this copy: d8cb8883db159e7e97c6e494115d0ff221be2ac73b42554dbc05e5107677cd23
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.436_TbNi4Si.mcif.