Research/Sitter/MAGNDATA / 0.832_CeAuGe.mcif

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Spin lattice of CeAuGeSpin lattice of CeAuGe

CeAuGe

MAGNDATA entry 0.832 · 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 ≤ 10.2 K (−263 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC m c′ 21′ BNS 36.175
Point groupm′m2′
Parent space groupP 63 m c No. 186
Spinscollinear · net moment 4.24 μB per cell
Propagation[0 0 0] 1k
Cella 4.45781 · b 7.72115 · c 7.8547 Å · α 90° · β 90° · γ 90°
Transition10.2 K (−263 °C)
Measured at1.5 K
Magnetic ionsCe
Largest moment component1.06 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 c′ 21′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Ce1Ce000−1.06001.06
Au1Au00.33330.7871
Ge1Ge00.33330.2416

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

S. Shin et al. J. Magn. Magn. Mater. (2022) · doi:10.1016/j.jmmm.2022.169147

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.832_CeAuGe.mcif from MAGNDATA · entry page

sha256 of this copy: 1abd894794832b9e2a61fcd4d8d456897309e85d3868f4ef05b0e8a7d07968cc
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.832_CeAuGe.mcif.