Research/Sitter/MAGNDATA / 0.589_NdCrO3.mcif

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Spin lattice of NdCrO3Spin lattice of NdCrO3

NdCrO3

MAGNDATA entry 0.589 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 224 K (−49 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21/m BNS 11.50
Parent space groupP b n m No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.425 · b 5.478 · c 7.694 Å · α 90° · β 90° · γ 90°
Transition224 K (−49 °C)
Measured at4.2 K
Magnetic ionsCr, Nd
Largest moment component2.21 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/m →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Nd1_1Nd0.490.4650.7500−1.31.3
Nd1_2Nd0.990.0350.25001.31.3
Cr1_1Cr0.5001.282.2102.5539
Cr1_2Cr00.50−1.28−2.2102.5539
O1_1O0.560.0250.75
O1_2O0.060.4750.25
O2_1O−0.2850.2920.05
O2_2O0.2150.2080.95

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. Solid State Communications (1967) · doi:10.1016/0038-1098(67)90001-4

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.589_NdCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: c4d9b35e524f9e51e53da73c893754fa1604245b4e07eaf9e177e53dcb4c78af
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.589_NdCrO3.mcif.