Research/Sitter/MAGNDATA / 0.1146_Sr2DyRuO6.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Sr2Dy1Ru1O6Spin lattice of Sr2Dy1Ru1O6

Sr2Dy1Ru1O6

MAGNDATA entry 0.1146 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 25 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21/c BNS 14.75
Point group2/m
Parent space groupP 21/n No. 14
Spinscoplanar · net moment 0.7 μB per cell
Propagation[0 0 0] 1k
Cella 5.7774 · b 5.7948 · c 8.1848 Å · α 90° · β 90.18° · γ 90°
Transition25 K (−248 °C)
Measured at5 K
Magnetic ionsDy, Ru
Largest moment component4.91 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/c →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1Sr0.50350.51230.25
Dy1Dy00.504.910.3504.9225
Ru1Ru0.5001.94001.94
O1O0.22560.19170.9569
O2O0.31180.72710.9569
O3O0.41030.98420.2317

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

Rabia Pandi et al. J Mater Sci: Mater Electron (2025) · doi:10.1007/s10854-025-16069-z

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1146_Sr2DyRuO6.mcif from MAGNDATA · entry page

sha256 of this copy: 9c36f3c0338d6163eefa7d7216585fbcbacfe9f5db993d2fa369458718b2d75d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1146_Sr2DyRuO6.mcif.