Research/Sitter/MAGNDATA / 0.139_BiCrO3.mcif

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Spin lattice of BiCrO3Spin lattice of BiCrO3

BiCrO3

MAGNDATA entry 0.139 · source
s-wave compensated ferrimagnet
Opposite moments cancel, but the two sublattices aren't related by any symmetry, so the bands split like a ferromagnet's (s-wave).
Spin group ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 80 K (−193 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 1 BNS 2.4
Point group1
Parent space groupC 2/c No. 15
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 9.4519 · b 5.4741 · c 9.5767 Å · α 90° · β 108.55° · γ 90°
Transition80 K (−193 °C)
Measured at2 K
Magnetic ionsCr
Largest moment component2 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 1 →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Bi1_1Bi0.13340.21580.1313
Bi1_2Bi0.86660.21580.3687
Cr1_1Cr0.250.250.501.722.6249
Cr1_2Cr0.750.25001.722.6249
Cr2Cr00.7650.250−1.7−22.6249
O1_1O0.08730.2020.587
O1_2O0.91270.2020.913
O2_1O0.15570.5230.3649
O2_2O0.84430.5230.1351
O3_1O0.35750.5220.1596
O3_2O0.64250.5220.3404

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

C. Darie et al. Solid State Sciences (2010) · doi:10.1016/j.solidstatesciences.2008.12.004

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.139_BiCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 44f6ba5bd425ebda79265fd163f1a45f5be88c869b4f845a4f757f299a7fedfd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.139_BiCrO3.mcif.