Research/Sitter/MAGNDATA / 0.445_MnCoGe.mcif

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Spin lattice of MnCoGeSpin lattice of MnCoGe

MnCoGe

MAGNDATA entry 0.445 · 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 ≤ 345 K (72 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m′ a BNS 62.446
Parent space groupP n m a No. 62
Spinscollinear · net moment 16.68 μB per cell
Propagation[0 0 0] 1k
Cella 5.9192 · b 3.8132 · c 7.0621 Å · α 90° · β 90° · γ 90°
Transition345 K (72 °C)
Measured at1.2 K
Magnetic ionsCo, Mn
Largest moment component3.54 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 P n′ m′ a →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co0.15250.250.5832000.630.63
Mn1Mn0.03210.250.1988003.543.54
Ge1Ge0.77420.250.6204

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

X. Miao et al. PHYSICAL REVIEW MATERIALS (2020) · doi:10.1103/PhysRevMaterials.4.104407

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.445_MnCoGe.mcif from MAGNDATA · entry page

sha256 of this copy: 5160baf7ed7bcbcb4827c93196c3c945f1eaf3175251a931d26028e16871d454
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.445_MnCoGe.mcif.