Research/Sitter/MAGNDATA / 0.447_MnCoGeB0.05.mcif

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Spin lattice of MnCoGeB0.05Spin lattice of MnCoGeB0.05

MnCoGeB0.05

MAGNDATA entry 0.447 · 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 ≤ 260 K (−13 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 9 properties
Magnetic groupP 63/m m′ c′ BNS 194.270
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 5.46 μB per cell
Propagation[0 0 0] 1k
Cella 4.067 · b 4.067 · c 5.284 Å · α 90° · β 90° · γ 120°
Transition260 K (−13 °C)
Magnetic ionsCo, Mn
Largest moment component2.01 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 63/m m′ c′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Ge1Ge0.33330.66670.25
Mn1Mn000002.012.01
Co1Co0.33330.66670.75000.720.72

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

⬇ 0.447_MnCoGeB0.05.mcif from MAGNDATA · entry page

sha256 of this copy: d4838d736654551f5354dfa0f8b00436247a97e917e7829219a94e926f0450c5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.447_MnCoGeB0.05.mcif.