Research/Sitter/MAGNDATA / 3.20_TbMn2Ge2.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Tb1Mn2Ge2Spin lattice of Tb1Mn2Ge2

Tb1Mn2Ge2

MAGNDATA entry 3.20 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 26 K (−247 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 1 BNS 2.4
Point group1
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 30.4 μB per cell
Propagation[0 0 0] · [1 1 1] · [0 1/2 0] 3k
Cella 3.972 · b 7.944 · c 10.758 Å · α 90° · β 90° · γ 90°
Transition26 K (−247 °C)
Measured at4.2 K
Magnetic ionsMn, Tb
Largest moment component7.6 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 1 →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1_1Mn00.250.25002.32.3
Mn1_2Mn0.50.50.7500−2.32.3
Mn1_3Mn0.500.7500−2.32.3
Mn1_4Mn00.750.25002.32.3
Tb1_1Tb0002.46−4.927.69.3818
Tb1_2Tb0.50.750.5−2.464.927.69.3818
Ge1_1Ge000.3797
Ge1_2Ge0.50.750.8797
Ge1_3Ge000.6203
Ge1_4Ge0.50.750.1203

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

J. Leciejewicz et al. Solid State Communications (1984) · doi:10.1016/0038-1098(84)90587-8

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 3.20_TbMn2Ge2.mcif from MAGNDATA · entry page

sha256 of this copy: cf3eb438fc4d6cc32f56853aaa5022b9f7b9f79f37b42bbd9abe993a294f0632
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 3.20_TbMn2Ge2.mcif.