Research/Sitter/MAGNDATA / 1.1.73_Tb2Ni3Si5.mcif
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| Magnetic group | Ibam1′(00γ)000s |
| Point group | mmm1′ |
| Parent space group | I b a m No. 72 |
| Repeats every | 1.26 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.794] 1k |
| Cell | a 9.544 · b 11.136 · c 5.6286 Å · α 90° · β 90° · γ 90° |
| Transition | 19.5 K (−254 °C) |
| Measured at | 13 K |
| Magnetic ions | Tb |
| Largest moment component | 6.55 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Tb1 | Tb | 0.2682 | 0.373 | 0 | ||||
| Ni1 | Ni | 0.1148 | 0.139 | 0 | ||||
| Ni2 | Ni | 0.5 | 0 | 0.25 | ||||
| Si1 | Si | 0.3467 | 0.131 | 0 | ||||
| Si2 | Si | 0 | 0.261 | 0.25 | ||||
| Si3 | Si | 0 | 0 | 0.25 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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.
A. Szytula et al. J. Phys.: Condens. Matter (1997) · doi:10.1088/0953-8984/9/31/017
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.73_Tb2Ni3Si5.mcif from MAGNDATA · entry page
sha256 of this copy: 0427d077ee19e6aadd920a12e72b5cec1f5c3c451675f7c48f068ddf5282d414
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.73_Tb2Ni3Si5.mcif.