Research/Sitter/MAGNDATA / 1.279_Ho2Cu2O5.mcif
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| Magnetic group | Pa 21 BNS 4.10 |
| Parent space group | P n a 21 No. 33 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 1/2 0] 1k |
| Cell | a 10.8096 · b 6.9924 · c 12.4735 Å · α 90° · β 90° · γ 90° |
| Transition | 13 K (−260 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Cu, Ho |
| Largest moment component | 7.8 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ho1_1 | Ho | 0.208 | 0.1135 | 0 | −4.4 | 1 | 7.8 | 9.0111 |
| Ho1_2 | Ho | 0.708 | 0.1365 | 0 | 4.4 | 1 | −7.8 | 9.0111 |
| Ho2_1 | Ho | 0.0424 | 0.113 | 0.3303 | −4.4 | −1 | 7.8 | 9.0111 |
| Ho2_2 | Ho | 0.5424 | 0.137 | 0.3303 | 4.4 | −1 | −7.8 | 9.0111 |
| Cu1_1 | Cu | 0.9902 | 0.331 | 0.115 | −0.8 | 0 | 0 | 0.8 |
| Cu1_2 | Cu | 0.4902 | 0.919 | 0.115 | 0.8 | 0 | 0 | 0.8 |
| Cu2_1 | Cu | 0.261 | 0.332 | 0.217 | −0.8 | 0 | 0 | 0.8 |
| Cu2_2 | Cu | 0.761 | 0.918 | 0.217 | 0.8 | 0 | 0 | 0.8 |
| O1_1 | O | 0.173 | 0.363 | 0.359 | ||||
| O1_2 | O | 0.673 | 0.887 | 0.359 | ||||
| O2_1 | O | 0.324 | 0.356 | 0.066 | ||||
| O2_2 | O | 0.824 | 0.894 | 0.066 | ||||
| O3_1 | O | 0.124 | 0.16 | 0.169 | ||||
| O3_2 | O | 0.624 | 0.09 | 0.169 | ||||
| O4_1 | O | 0.427 | 0.388 | 0.263 | ||||
| O4_2 | O | 0.927 | 0.862 | 0.263 | ||||
| O5_1 | O | 0.426 | 0.115 | 0.479 | ||||
| O5_2 | O | 0.926 | 0.135 | 0.479 |
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.
J.L. Garcia-Muoz et al. Phys. Rev. B (1991) · doi:10.1103/PhysRevB.44.4716
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.279_Ho2Cu2O5.mcif from MAGNDATA · entry page
sha256 of this copy: 8216c82447637fcbc8dfec7e6b668ed499e290fdf3a353fa627537e004c443a2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.279_Ho2Cu2O5.mcif.