Research/Sitter/MAGNDATA / 0.354_TbCrO3.mcif
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| Magnetic group | P n′ m′ a BNS 62.446 |
| Parent space group | P b n m No. 62 |
| Spins | collinear · 2 nodal planes · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 5.291 · b 5.513 · c 7.557 Å · α 90° · β 90° · γ 90° |
| Transition | 158 K (−115 °C) |
| Measured at | 77 K |
| Magnetic ions | Cr, Tb |
| Largest moment component | 2.55 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Tb1 | Tb | 0.489 | 0.436 | 0.75 | ||||
| Cr1 | Cr | 0.5 | 0 | 0 | 0 | 0 | 2.55 | 2.55 |
| O1 | O | 0.596 | 0.03 | 0.75 | ||||
| O2 | O | 0.697 | 0.301 | 0.049 |
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:10.1016/0022-3697(67)90238-7
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.354_TbCrO3.mcif from MAGNDATA · entry page
sha256 of this copy: 32e783a25105e7f561ce041e4d1a970b0392e49883b544c2b309a474eab3cfe0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.354_TbCrO3.mcif.