Research/Sitter/MAGNDATA / 1.297_CuFe2(P2O7)2.mcif

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Spin lattice of CuFe2(P2O7)2Spin lattice of CuFe2(P2O7)2

CuFe2(P2O7)2

MAGNDATA entry 1.297 · 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 ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 15.5 K (−258 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPa 21/c BNS 14.80
Parent space groupP 21/n No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 13.1842 · b 5.1606 · c 31.2794 Å · α 90° · β 91.98° · γ 90°
Transition15.5 K (−258 °C)
Measured at1.4 K
Magnetic ionsCu, Fe
Largest moment component4.88 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 · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu0000−0.8300.83
Fe1Fe0.16720.24230.060−4.8804.88
P1P0.17720.27540.4526
P2P0.47490.25290.4156
O1O0.12260.20760.4933
O2O0.09510.28380.4152
O3O0.45950.99790.4398
O4O0.4340.47550.4411
O5O0.4350.22530.3711
O6O0.2540.08280.4411
O7O0.21770.55280.4567

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

N.E. Khayati et al. Solid State Sciences (2002) · doi:10.1016/S1293-2558(02)00015-8

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.297_CuFe2(P2O7)2.mcif from MAGNDATA · entry page

sha256 of this copy: 2f401532bb5255b7025abbe797e1728e9c2145a00f8a677b7eb8554811fd5846
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.297_CuFe2(P2O7)2.mcif.