Research/Sitter/MAGNDATA / 0.342_Tb3Ge5.mcif
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| Magnetic group | F d d 2 BNS 43.224 |
| Parent space group | F d d 2 No. 43 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 5.742 · b 17.226 · c 13.682 Å · α 90° · β 90° · γ 90° |
| Transition | 17 K (−256 °C) |
| Measured at | 4.2 K |
| Magnetic ions | Tb |
| Largest moment component | 9.29 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Tb1 | Tb | 0 | 0 | 0 | 0 | 0 | 9.29 | 9.29 |
| Tb2 | Tb | 0.7692 | 0.0799 | 0.2557 | 1.51 | 2.76 | −7.8 | 8.4106 |
| Ge1 | Ge | 0 | 0 | 0.4444 | ||||
| Ge2 | Ge | 0.7977 | 0.0663 | 0.654 | ||||
| Ge3 | Ge | 0.749 | 0.0858 | 0.8346 |
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.
P. Schobinger-Papamantellos et al. Journal of the Less-Common Metals (1989) · doi:10.1016/0022-5088(89)90386-X
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.342_Tb3Ge5.mcif from MAGNDATA · entry page
sha256 of this copy: 675f2eb2326cf073ffe7a51af7f25abaa032fdbe514d77b703be72254a31df2d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.342_Tb3Ge5.mcif.