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Spin lattice of Dy2Ti1O5Spin lattice of Dy2Ti1O5

Dy2Ti1O5

MAGNDATA entry 1.698 · 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 ≤ 1.7 K (−271 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21/c BNS 14.80
Point group2/m1′
Parent space groupP n m a No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1/2 0] 1k
Cella 10.344 · b 7.4228 · c 11.193 Å · α 90° · β 90° · γ 90°
Transition1.7 K (−271 °C)
Measured at0.3 K
Magnetic ionsDy
Largest moment component7.56 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 Pa 21/c →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy0.1160.1250.2254.70−7.568.9019
Dy2Dy0.1430.1250.559−60−4.927.7593
Ti1Ti0.2160.1250.854
O1O0.50.1250.091
O2O0.2440.1250.035
O3O0.2490.1250.741
O4O0.4850.1250.662
O5O0.2610.1250.368

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

J. Shamblin et al. PHYSICAL REVIEW B (2016) · doi:10.1103/PhysRevB.94.024413

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.698_Dy2TiO5.mcif from MAGNDATA · entry page

sha256 of this copy: b55fa05d36daeda91f9aa06b410277d1dbf9f265b6a35cdc9e4cb27ea64395a7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.698_Dy2TiO5.mcif.