Research/Sitter/MAGNDATA / 1.459_CeFe3(BO3)4.mcif

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Spin lattice of CeFe3(BO3)4Spin lattice of CeFe3(BO3)4

CeFe3(BO3)4

MAGNDATA entry 1.459 · 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 ¹3̄¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 29 K (−244 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupCc 2 BNS 5.16
Parent space groupR 3 2 No. 155
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 3/2] 1k
Cella 9.6023 · b 9.6023 · c 15.2626 Å · α 90° · β 90° · γ 120°
Transition29 K (−244 °C)
Measured at3.7 K
Magnetic ionsCe, Fe
Largest moment component4.82 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 Cc 2 →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Ce1Ce0000.2540.12700.22
Fe1_1Fe0.5525004.822.4104.1742
Fe1_2Fe00.552504.822.4104.1742
O1_1O0.856600.25
O1_2O00.85660.25
O2_1O0.589200.25
O2_2O00.58920.25
O3_1O0.44990.14280.2596
O3_2O0.85720.30710.2596
O3_3O0.69290.55010.2596
B1B000.25
B2_1B0.447300.25
B2_2B00.44730.25

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

S. Hayashida et al. PHYSICAL REVIEW B (2018) · doi:10.1103/PhysRevB.98.224405

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.459_CeFe3(BO3)4.mcif from MAGNDATA · entry page

sha256 of this copy: abadd75cb7517e7f827b62f68bcf39f0bd91dd300ce1d9fe73cef0cf07dcecd7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.459_CeFe3(BO3)4.mcif.