Research/Sitter/MAGNDATA / 2.47_Y2SrCuFeO6.5.mcif

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Spin lattice of Y2SrCuFeO6.5Spin lattice of Y2SrCuFeO6.5

Y2SrCuFeO6.5

MAGNDATA entry 2.47 · 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 ≤ 255 K (−18 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP c′ c′ n BNS 56.369
Parent space groupI b a m No. 72
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] · [1 1 1] 2k
Cella 5.4081 · b 10.7111 · c 20.2412 Å · α 90° · β 90° · γ 90°
Transition255 K (−18 °C)
Measured at2 K
Magnetic ionsCu, Fe
Largest moment component1.56 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 P c′ c′ n →
Atom sites · 16 sites · CSV
siteelementxyzmambmc|m| (μB)
Y1_1Y0.20920.36190.1841
Y1_2Y0.79080.63810.8159
Sr1Sr0.20670.36570
Cu1_1Cu0.71680.38330.0981
Cu1_2Cu0.28320.61670.9019
Fe2_1Fe0.71680.38330.0981−1.561.3602.0696
Fe2_2Fe0.28320.61670.90191.561.3602.0696
O1O0.1960.10890
O2_1O00.50.1063
O2_2O00.50.8937
O3O0.500.25
O4O00.22250.25
O5_1O0.45650.25280.1079
O5_2O0.54350.74720.8921
O6_1O000.3558
O6_2O000.6442

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

R.K. Li et al. PHYSICAL REVIEW B (2000) · doi:10.1103/PhysRevB.62.14149

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.47_Y2SrCuFeO6.5.mcif from MAGNDATA · entry page

sha256 of this copy: 8f87bd5d75b676b658e449cf95ec591daf37654e6f8b0af0e5218f8033880b70
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.47_Y2SrCuFeO6.5.mcif.