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Spin lattice of Ni0.85Cu0.15Cr2O4Spin lattice of Ni0.85Cu0.15Cr2O4

Ni0.85Cu0.15Cr2O4

MAGNDATA entry 0.894 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 85 K (−188 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2′/c′ BNS 15.89
Point group2′/m′
Parent space groupI 41/a m d No. 141
Spinscoplanar · net moment 10.4 μB per cell
Propagation[0 0 0] 1k
Cella 8.0565 · b 8.3129 · c 8.5384 Å · α 90° · β 90° · γ 90°
Transition85 K (−188 °C)
Measured at2 K
Magnetic ionsCr, Cu, Ni
Largest moment component1.88 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 C 2′/c′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni0.1250.1250.125−1.88001.88
Cu1Cu0.1250.1250.125−1.88001.88
Cr1_1Cr0.50.50.51.2301.832.2049
Cr1_2Cr0.250.50.251.230−1.832.2049
O1_1O0.25570.26150.2676
O1_2O0.2557−0.0115−0.0176

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

M. Reehuis et al. PHYSICAL REVIEW B? (2015) · doi:10.1103/PhysRevB.91.024407

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.894_Ni0.85Cu0.15Cr2O4.mcif from MAGNDATA · entry page

sha256 of this copy: ef11dd11ca81b845016f7a6187b4b891d810ee339d59b8c37ec0dbecc20b053a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.894_Ni0.85Cu0.15Cr2O4.mcif.