Research/Sitter/MAGNDATA / 0.1122_KTb3F10.mcif

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Spin lattice of K1Tb3F10Spin lattice of K1Tb3F10

K1Tb3F10

MAGNDATA entry 0.1122 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
Structure · 10 properties
Magnetic groupI m′ m′ m BNS 71.536
Point groupm′m′m
Parent space groupF m 3 m No. 225
Spinscoplanar · net moment 102.955 μB per cell
Propagation[0 0 0] 1k
Cella 11.6645 · b 11.6645 · c 11.6645 Å · α 90° · β 90° · γ 90°
Measured at1.5 K
Magnetic ionsTb
Largest moment component5.3 μB
MethodNSD and NPD

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 I m′ m′ m →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1_1Tb0.241000−5.305.3
Tb1_2Tb000.2413.8−3.805.374
K1K0.250.250.25
F1_1F0.11180.11180.1118
F1_2F0.88820.11180.8882
F2_1F0.50.16650.1665
F2_2F0.16650.16650.5
F2_3F0.83350.16650.5

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

O. Demortier et al. PHYSICAL REVIEW MATERIALS (2025) · doi:10.1103/PhysRevMaterials.9.056201

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1122_KTb3F10.mcif from MAGNDATA · entry page

sha256 of this copy: 730fe310dbc565e0619d3a1a6d75d889969cc16f4b329737f0a3c9fe78cc3f7e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1122_KTb3F10.mcif.