Research/Sitter/MAGNDATA / 0.29_Er2Ti2O7.mcif
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| Magnetic group | I 41′/a m′ d BNS 141.554 |
| Point group | 4′/mm′m |
| Parent space group | F d 3m No. 227 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 10.0762 · b 10.0762 · c 10.0762 Å · α 90° · β 90° · γ 90° |
| Transition | 1.173 K (−272 °C) |
| Measured at | 0.05 K |
| Magnetic ions | Er |
| Largest moment component | 2.65 μB |
| Method | Neutron polarimetry |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Er1 | Er | 0 | 0 | 0 | 1.325 | 1.325 | −2.65 | 3.2456 |
| Ti1 | Ti | 0 | 0 | 0.5 | ||||
| O1 | O | 0.625 | 0.625 | 0.125 | ||||
| O2_1 | O | 0.58 | 0.875 | 0.875 | ||||
| O2_2 | O | 0.875 | 0.875 | 0.58 |
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. Poole et al. J. Phys.: Condens. Matter (2007) · doi:10.1088/0953-8984/19/45/452201
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.29_Er2Ti2O7.mcif from MAGNDATA · entry page
sha256 of this copy: 02990f6446dabc1da622f6c1762af7ebddb4bfba51d5208be222e7133c5c27c6
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.29_Er2Ti2O7.mcif.