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Spin lattice of DyCrO4Spin lattice of DyCrO4

DyCrO4

MAGNDATA entry 0.372 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹4/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 19 K (−254 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/c BNS 15.87
Parent space groupI 41/a No. 88
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.0148 · b 5.0148 · c 11.3037 Å · α 90° · β 90° · γ 90°
Transition19 K (−254 °C)
Measured at1.2 K
Magnetic ionsCr, Dy
Largest moment component9.67 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 C 2′/c →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy00.250.6259.67009.67
Cr1Cr00.250.1250.99000.99
O1_1O0.24370.60910.5486
O1_2O0.14090.49370.7986

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

A.J.D. santos-Garcia et al. Journal of Physics: Conference Series (2014) · doi:10.1088/1742-6596/549/1/012021

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.372_DyCrO4.mcif from MAGNDATA · entry page

sha256 of this copy: 4a42a2025a439014ef1156bd9d30173de38c102d01c54c973a89ffd8cf6fb051
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.372_DyCrO4.mcif.