Research/Sitter/MAGNDATA / 0.286_Mn5Ge3.mcif

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Spin lattice of Mn5Ge3Spin lattice of Mn5Ge3

Mn5Ge3

MAGNDATA entry 0.286 · 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 ≤ 304 K (31 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63/m c′ m′ BNS 193.260
Parent space groupP 63/m c m No. 193
Spinscollinear · net moment 27.22 μB per cell
Propagation[0 0 0] 1k
Cella 7.184 · b 7.184 · c 5.053 Å · α 90° · β 90° · γ 120°
Transition304 K (31 °C)
Measured at60 K
Magnetic ionsMn
Largest moment component3.23 μB
MethodPolarised NSD

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 63/m c′ m′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Ge1Ge0.60300.25
Mn1Mn0.33330.66670001.961.96
Mn2Mn0.239700.25003.233.23

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

J.B. Forsyth et al. J. Phys.: Condens. Matter (1990) · doi:10.1088/0953-8984/2/11/014

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.286_Mn5Ge3.mcif from MAGNDATA · entry page

sha256 of this copy: f7fedec45bd593702dc2ee1b2c0fff053ac1e528301ac28757e230cb6b394d46
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.286_Mn5Ge3.mcif.