Research/Sitter/MAGNDATA / 0.487_ErCr2Si2.mcif

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Spin lattice of ErCr2Si2Spin lattice of ErCr2Si2

ErCr2Si2

MAGNDATA entry 0.487 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 2.4 K (−271 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI m′ m′ 2 BNS 44.232
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 10.48 μB per cell
Propagation[0 0 0] 1k
Cella 3.895 · b 3.895 · c 10.632 Å · α 90° · β 90° · γ 90°
Transition2.4 K (−271 °C)
Measured at2 K
Magnetic ionsCr, Er
Largest moment component5.24 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 I m′ m′ 2 →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Er1Er0005.24005.24
Cr1Cr00.50.2500−1.351.35
Si1Si000.3888

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

O. Moze et al. Eur. Phys. J. B (2003) · doi:10.1140/epjb/e2004-00006-4

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.487_ErCr2Si2.mcif from MAGNDATA · entry page

sha256 of this copy: 3c29632fc3aabb572778e465229b6063461d57b3a3ab2e8ba4150c2ed6595cec
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.487_ErCr2Si2.mcif.