Research/Sitter/MAGNDATA / 2.5_Mn3CuN.mcif

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Spin lattice of Mn3CuNSpin lattice of Mn3CuN

Mn3CuN

MAGNDATA entry 2.5 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 143 K (−130 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 4/n BNS 85.59
Point group4/m
Parent space groupP m 3m No. 221
Spinsnoncoplanar · net moment 2.1 μB per cell
Propagation[1/2 1/2 0] · [0 0 0] 2k
Cella 5.5239 · b 5.5239 · c 3.906 Å · α 90° · β 90° · γ 90°
Transition143 K (−130 °C)
Magnetic ionsMn
Largest moment component2.55 μB
MethodUnspecified neutron diffraction technique.

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 4/n →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu00.50
Mn1_1Mn0.750.750.5−2.55−1.270.22.8558
Mn1_2Mn000000.650.65
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

Fruchart, D. et al. Journal of the Physical Society of Japan (1978) · doi:10.1143/JPSJ.44.781

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.5_Mn3CuN.mcif from MAGNDATA · entry page

sha256 of this copy: 270b7e7448994020dfb97d644afa5f15a64944045cda123ed614fb7256e74a18
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.5_Mn3CuN.mcif.