Research/Sitter/MAGNDATA / 1.118_GdPO4.mcif

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Spin lattice of GdPO4Spin lattice of GdPO4

GdPO4

MAGNDATA entry 1.118 · 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 ≤ 0.8 K (−272 °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 21/n No. 14
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 13.25 · b 6.82 · c 12.634 Å · α 90° · β 104.06° · γ 90°
Transition0.8 K (−272 °C)
Measured at0.06 K
Magnetic ionsGd
Largest moment component6.57 μB
MethodNSD

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 · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Gd1Gd0.14130.1540.04976.5723.36.8935
P1P0.15240.17340.3049
O1O0.1245−0.00010.2191
O2O0.18960.32610.2522
O3O0.23770.11370.4069
O4O0.05960.20570.3559

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. Palacios et al. PHYSICAL REVIEW B (2014) · doi:10.1103/PhysRevB.90.214423

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.118_GdPO4.mcif from MAGNDATA · entry page

sha256 of this copy: c1c2bd1cfb684f795c702a55865da4bb66158fc998242646a7451c9febb2443e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.118_GdPO4.mcif.