Research/Sitter/MAGNDATA / 2.64_DyCrO3.mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | P 21′/m′ BNS 11.54 |
| Parent space group | P b n m No. 62 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] · [1/2 1/2 0] 2k |
| Cell | a 10.526 · b 11.04 · c 7.552 Å · α 90° · β 90° · γ 90° |
| Transition | 2.16 K (−271 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Cr, Dy |
| Largest moment component | 9.36 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cr1_1 | Cr | 0.25 | 0 | 0 | 0 | 0 | 2.76 | 2.76 |
| Cr1_2 | Cr | 0 | 0.25 | 0 | 0 | 0 | −2.76 | 2.76 |
| Cr1_3 | Cr | 0.75 | 0 | 0 | 0 | 0 | 2.76 | 2.76 |
| Cr1_4 | Cr | 0.5 | 0.25 | 0 | 0 | 0 | −2.76 | 2.76 |
| Dy1_1 | Dy | 0.994 | 0.0325 | 0.25 | 9.36 | −2.47 | 0 | 9.6804 |
| Dy1_2 | Dy | 0.494 | 0.0325 | 0.25 | −9.36 | 2.47 | 0 | 9.6804 |
| Dy1_3 | Dy | 0.756 | 0.2825 | 0.25 | −4.58 | −8.53 | 0 | 9.6818 |
| Dy1_4 | Dy | 0.744 | 0.2175 | 0.75 | 4.58 | 8.53 | 0 | 9.6818 |
| O1_1 | O | 0.2995 | 0.016 | 0.75 | ||||
| O1_2 | O | 0.5495 | 0.234 | 0.25 | ||||
| O1_3 | O | 0.7005 | 0.984 | 0.25 | ||||
| O1_4 | O | 0.9505 | 0.266 | 0.75 | ||||
| O2_1 | O | 0.348 | 0.15 | 0.05 | ||||
| O2_2 | O | 0.598 | 0.1 | 0.95 | ||||
| O2_3 | O | 0.652 | 0.85 | 0.55 | ||||
| O2_4 | O | 0.902 | 0.4 | 0.45 |
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.
E.F. Bertaut et al. J. Physique (1968) · doi:10.1051/jphys:0196800290106700
Cite the original paper and MAGNDATA, not this mirror.
⬇ 2.64_DyCrO3.mcif from MAGNDATA · entry page
sha256 of this copy: beaeacce7f9bf05a50e5bbbd7dd62e4fa049d9a5e2212c66c6998a9ea6dc21a2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.64_DyCrO3.mcif.