Research/Sitter/MAGNDATA / 0.588_PrCrO3.mcif

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Spin lattice of PrCrO3Spin lattice of PrCrO3

PrCrO3

MAGNDATA entry 0.588 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 239 K (−34 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m a′ BNS 62.448
Parent space groupP b n m No. 62
Spinscoplanar · net moment 2 μB per cell
Propagation[0 0 0] 1k
Cella 5.4503 · b 5.4799 · c 7.7154 Å · α 90° · β 90° · γ 90°
Transition239 K (−34 °C)
Measured at4.2 K
Magnetic ionsCr, Pr
Largest moment component2.46 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)
Pr1Pr−0.00740.03540.25000.50.5
Cr1Cr0.5002.46002.46
O1O0.0810.48310.25
O2O−0.2870.28960.0335

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. F. Bertaut et al. JOURNAL OF APPLIED PHYSICS (1966) · doi:10.1063/1.1708325

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.588_PrCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: e4a98a1a00f51cd016f0653f7952ca348555d8d14b8fef6236eb1ee30cd440db
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.588_PrCrO3.mcif.