Research/Sitter/MAGNDATA / 1.1.21_Li2IrO3.mcif
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| Magnetic group | C2221′(α00)s00s |
| Point group | 2221′ |
| Parent space group | C c c m No. 66 |
| Repeats every | 1.75 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.57 0 0] 1k |
| Cell | a 5.9119 · b 8.4461 · c 17.8363 Å · α 90° · β 90° · γ 90° |
| Transition | 39.5 K (−234 °C) |
| Magnetic ions | Ir |
| Largest moment component | 1 μB |
| Method | MRXD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ir1_1 | Ir | 0.25 | 0.25 | 0.0836 | ||||
| Ir1_2 | Ir | −0.25 | −0.25 | −0.0836 | ||||
| Ir2_1 | Ir | 0.5 | 0.5 | 0.167 | ||||
| Ir2_2 | Ir | −0.5 | −0.5 | −0.167 | ||||
| Li1_1 | Li | 0 | 0.5 | 0.3333 | ||||
| Li1_2 | Li | 0 | −0.5 | −0.3333 | ||||
| Li2_1 | Li | 0.75 | 0.25 | 0.25 | ||||
| Li2_2 | Li | −0.75 | −0.25 | −0.25 | ||||
| Li3_1 | Li | 0.75 | 0.25 | 0.9167 | ||||
| Li3_2 | Li | −0.75 | −0.25 | −0.9167 | ||||
| Li4 | Li | 0.5 | 0.5 | 0.5 | ||||
| Li5 | Li | 0.5 | 0 | 0 | ||||
| O1_1 | O | 0.77 | 0.515 | 0.087 | ||||
| O1_2 | O | −0.77 | −0.515 | −0.087 | ||||
| O2_1 | O | 0.72 | 0.5 | 0.25 | ||||
| O2_2 | O | −0.72 | −0.5 | −0.25 | ||||
| O3 | O | 0 | 0.262 | 0 | ||||
| O4_1 | O | 0.49 | 0.262 | 0.163 | ||||
| O4_2 | O | −0.49 | −0.262 | −0.163 |
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. Biffin et al. PHYSICAL REVIEW LETTERS (2014) · doi:10.1103/PhysRevLett.113.197201
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.21_Li2IrO3.mcif from MAGNDATA · entry page
sha256 of this copy: 313c7324a7b2812af0c8def5e9f222a0ef79de0935f9b53fe449cb1351695b24
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.21_Li2IrO3.mcif.