Research/Sitter/MAGNDATA / 1.1.6_TbMnO3.mcif
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| Magnetic group | Pbnm1′(0,β,0)s00s |
| Point group | mmm1′ |
| Parent space group | P b n m No. 62 |
| Repeats every | 3.7 cells along b (not a whole number: that's what incommensurate means) |
| Propagation | [0 0.27 0] 1k |
| Cell | a 5.297 · b 5.831 · c 7.403 Å · α 90° · β 90° · γ 90° |
| Transition | 41 K (−232 °C) |
| Measured at | 35 K |
| Magnetic ions | Mn, Tb |
| Largest moment component | 2.9 μB |
| Method | Phase I. Below 28K a second phase (phase II) exists with a cycloidal spin arrangement. |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Tb1 | Tb | −0.028 | 0.072 | 0.25 | ||||
| Mn1 | Mn | 0.5 | 0 | 0 | ||||
| O1 | O | 0.097 | 0.46 | 0.25 | ||||
| O2 | O | −0.296 | 0.337 | 0.056 |
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.
M. Kenzelmann et al. PHYSICAL REVIEW LETTERS (2005) · doi:10.1103/PhysRevLett.95.087206
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.6_TbMnO3.mcif from MAGNDATA · entry page
sha256 of this copy: 2de27d2484f9637f8255cb51c20265cf4200f885a1e09e70d96f116c855732d9
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.6_TbMnO3.mcif.