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Spin lattice of Cu1.94Mn1.06BO5Spin lattice of Cu1.94Mn1.06BO5

Cu1.94Mn1.06BO5

MAGNDATA entry 0.322 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 92 K (−181 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′/c′ BNS 14.79
Parent space groupP 21/c No. 14
Spinscoplanar · net moment 7.724 μB per cell
Propagation[0 0 0] 1k
Cella 3.1385 · b 9.4002 · c 12.0204 Å · α 90° · β 92.27° · γ 90°
Transition92 K (−181 °C)
Measured at2 K
Magnetic ionsCu, Mn
Largest moment component1.93 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 21′/c′ →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn000
Cu1Cu0000.090−0.440.4526
Mn2Mn0.500.5
Cu2Cu0.500.50.600.971.1202
Mn3Mn0.06380.98770.279
Cu3Cu0.06380.98770.279−0.2300.910.9474
Mn4Mn0.5760.73240.3785−1.930−1.912.661
Cu4Cu0.5760.73240.3785
B1B0.40570.2640.367
O1O0.00380.09530.1454
O2O0.14920.87250.4118
O3O0.46610.11870.3654
O4O0.60910.65970.5369
O5O0.64190.83320.2337

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

E. Moshkina et al. Journal of Physics: Condensed Matter (2017) · doi:10.1088/1361-648X/aa7020

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.322_Cu1.94Mn1.06BO5.mcif from MAGNDATA · entry page

sha256 of this copy: 491b3a64e4e95d981291a9fb0e120f6cedc4313c7ef9625ab14f7dc1293b3351
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.322_Cu1.94Mn1.06BO5.mcif.