Research/Sitter/MAGNDATA / 0.265_Mn3(Co0.61Mn0.39)N.mcif

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Spin lattice of Mn3(Co0.61Mn0.39)NSpin lattice of Mn3(Co0.61Mn0.39)N

Mn3(Co0.61Mn0.39)N

MAGNDATA entry 0.265 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 260 K (−13 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupR 3 BNS 148.17
Parent space groupP m 3 m No. 221
Spinsnoncoplanar · net moment 12.63 μB per cell
Propagation[0 0 0] 1k
Cella 5.4682 · b 5.4682 · c 6.6972 Å · α 90° · β 90° · γ 120°
Transition260 K (−13 °C)
Measured at5 K
Magnetic ionsCo, Mn
Largest moment component1.79 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 R 3 →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0.500−1.4100.211.4256
Mn2Mn000001.791.79
Co1Co000001.791.79
N1N000.5

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

Y. Sun et al. PHYSICAL REVIEW MATERIALS (2019) · doi:10.1103/PhysRevMaterials.3.024409

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.265_Mn3(Co0.61Mn0.39)N.mcif from MAGNDATA · entry page

sha256 of this copy: aa34f3a92b919a953af43aac4d9bc000f18b1a5f2d311f11ed8bd63db970b84d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.265_Mn3(Co0.61Mn0.39)N.mcif.