Research/Sitter/MAGNDATA / 0.697_SmCrO3.mcif

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Spin lattice of SmCrO3Spin lattice of SmCrO3

SmCrO3

MAGNDATA entry 0.697 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 37 K (−236 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m′ a BNS 62.446
Parent space groupP b n m No. 62
Spinsnoncoplanar · net moment 0.4 μB per cell
Propagation[0 0 0] 1k
Cella 5.3634 · b 5.4911 · c 7.6337 Å · α 90° · β 90° · γ 90°
Transition37 K (−236 °C)
Measured at25 K
Magnetic ionsCr, Sm
Largest moment component2.86 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 n′ m′ a →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Cr1Cr0.50000.22.862.867
Sm1Sm0.00940.03310.250.10.400.4123
O1O−0.08470.47670.25
O2O0.29760.29490.0447

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

T. Sau et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.103.144418

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.697_SmCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 1e586ffdec39b88023ef653ab0d1fc8c0c5ce9b20e257a48fc475759518dfe58
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.697_SmCrO3.mcif.