Research/Sitter/MAGNDATA / 0.1038_CeAu0.5Cu0.5Ge.mcif

Ce₁Au_0.5Cu_0.5Ge₁

MAGNDATA entry 0.1038 · 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 ≤ 15.1 K (−258 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	C m c′ m′ BNS 63.463
Point group	m′m′m
Parent space group	P 6₃/m m c No. 194
Spins	collinear · net moment 2.32 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 4.3936 · b 7.8815 · c 4.3936 Å · α 90° · β 120° · γ 90°
Transition	15.1 K (−258 °C)
Measured at	1.5 K
Magnetic ions	Ce
Largest moment component	1.16 μ_B
Method	NPD

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′ m′ →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Ce1	Ce	0	0	0	0	0	1.16	1.16
Au1	Au	0.6667	0.25	0.3333
Cu1	Cu	0.6667	0.25	0.3333
Ge1	Ge	0.3333	0.25	0.6667

Moment components are along the crystal axes a, b, c (μ_B), 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

⬇ 0.1038_CeAu0.5Cu0.5Ge.mcif from MAGNDATA · entry page

sha256 of this copy: 81e5040b633fdee8d0a1aa3d4bbc0396cefe27e76155265d4fe828c8ee0aa5fc
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1038_CeAu0.5Cu0.5Ge.mcif.

Ce1Au0.5Cu0.5Ge1

Symmetry

Source

Original file

Ce₁Au_0.5Cu_0.5Ge₁