Research/Sitter/MAGNDATA / 2.62_TbCrO3.mcif
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| Magnetic group | P m′ n′ 21 BNS 31.127 |
| Parent space group | P b n m No. 62 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 1/2 0] · [0 0 0] 2k |
| Cell | a 5.291 · b 11.026 · c 7.557 Å · α 90° · β 90° · γ 90° |
| Transition | 3.05 K (−270 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Cr, Tb |
| Largest moment component | 7.76 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Tb1_1 | Tb | 0.989 | 0.032 | 0.25 | 7.76 | 3.17 | 0 | 8.3825 |
| Tb1_2 | Tb | 0.489 | 0.218 | 0.75 | −7.76 | 3.17 | 0 | 8.3825 |
| Tb1_3 | Tb | 0.011 | 0.968 | 0.75 | −7.76 | −3.17 | 0 | 8.3825 |
| Tb1_4 | Tb | 0.511 | 0.282 | 0.25 | 7.76 | −3.17 | 0 | 8.3825 |
| Cr1_1 | Cr | 0.5 | 0 | 0 | 0 | 0 | 2.85 | 2.85 |
| Cr1_2 | Cr | 0 | 0.25 | 0 | 0 | 0 | −2.85 | 2.85 |
| O1_1 | O | 0.096 | 0.235 | 0.25 | ||||
| O1_2 | O | 0.596 | 0.015 | 0.75 | ||||
| O1_3 | O | 0.904 | 0.765 | 0.75 | ||||
| O1_4 | O | 0.404 | 0.485 | 0.25 | ||||
| O2_1 | O | 0.697 | 0.1505 | 0.049 | ||||
| O2_2 | O | 0.197 | 0.0995 | 0.951 | ||||
| O2_3 | O | 0.303 | 0.8495 | 0.549 | ||||
| O2_4 | O | 0.803 | 0.4005 | 0.451 |
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. Phys. Chem. Solids (1967) · doi:10.1016/0038-1098(67)90276-1
Cite the original paper and MAGNDATA, not this mirror.
⬇ 2.62_TbCrO3.mcif from MAGNDATA · entry page
sha256 of this copy: 3effce61f5282590c0442cd4f29c7f8b52808e1f2b0235b9a49251f804a6241e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.62_TbCrO3.mcif.