Research/Sitter/MAGNDATA / 2.112_TbFe6Ge6.mcif

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Spin lattice of Tb1Fe6Ge6Spin lattice of Tb1Fe6Ge6

Tb1Fe6Ge6

MAGNDATA entry 2.112 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 9 K (−264 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP c′ a 21′ BNS 29.101
Point groupm′m2′
Parent space groupC m c m No. 63
Spinscoplanar · net moment 35.16 μB per cell
Propagation[0 0 0] · [1 0 0] 2k
Cella 8.1293 · b 17.7319 · c 5.1188 Å · α 90° · β 90° · γ 90°
Transition9 K (−264 °C)
Measured at1.4 K
Magnetic ionsFe, Tb
Largest moment component5.19 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′ a 21′ →
Atom sites · 16 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb00.1220.255.1905.197.3398
Tb2Tb00.6280.253.603.65.0912
Ge1Ge0−0.0390.25
Ge2Ge00.4560.25
Ge3Ge00.7920.25
Ge4Ge00.29730.25
Ge5_1Ge0.34750.12570.25
Ge5_2Ge0.65250.87430.75
Ge6_1Ge0.84750.12430.25
Ge6_2Ge0.15250.87570.75
Fe1_1Fe0.250.2502.02002.02
Fe1_2Fe0.750.750.5−2.02002.02
Fe2_1Fe0.2509002.02002.02
Fe2_2Fe0.749100.5−2.02002.02
Fe3_1Fe0.74910.87670.25−2.02002.02
Fe3_2Fe0.25090.12330.752.02002.02

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. Zaharko et al. J. Magn. Magn. Mater. (1998) · doi:10.1016/S0304-8853(98)00148-6

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.112_TbFe6Ge6.mcif from MAGNDATA · entry page

sha256 of this copy: 9405e35bff8a0930ffbe6a01d7ca2119e8ed0e2c95da9087b020b76ad457b728
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.112_TbFe6Ge6.mcif.