Research/Sitter/MAGNDATA / 0.329_RbMnF4.mcif
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| Magnetic group | P 1 BNS 2.4 |
| Parent space group | P 21/a No. 14 |
| Spins | collinear · 1 nodal planes · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 7.7865 · b 7.7447 · c 5.9968 Å · α 90° · β 90.43° · γ 90° |
| Transition | 3.7 K (−269 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Mn |
| Largest moment component | 1.97 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1_1 | Mn | 0 | 0 | 0 | 1.97 | 1.97 | 1.03 | 2.9652 |
| Mn1_2 | Mn | 0.5 | 0.5 | 0 | −1.97 | −1.97 | −1.03 | 2.9652 |
| Mn2_1 | Mn | 0.5 | 0 | 0 | 1.97 | 1.97 | 1.03 | 2.9652 |
| Mn2_2 | Mn | 0 | 0.5 | 0 | −1.97 | −1.97 | −1.03 | 2.9652 |
| F1_1 | F | 0.9997 | 0.2409 | 0.1001 | ||||
| F1_2 | F | 0.5003 | 0.7409 | 0.8999 | ||||
| F2_1 | F | 0.262 | 0.0156 | 0.9166 | ||||
| F2_2 | F | 0.238 | 0.5156 | 0.0834 | ||||
| F3_1 | F | 0.0489 | 0.9384 | 0.2833 | ||||
| F3_2 | F | 0.4511 | 0.4384 | 0.7167 | ||||
| F4_1 | F | 0.9472 | 0.56 | 0.2854 | ||||
| F4_2 | F | 0.5528 | 0.06 | 0.7146 | ||||
| Rb1_1 | Rb | 0.746 | 0.294 | 0.483 | ||||
| Rb1_2 | Rb | 0.754 | 0.794 | 0.517 |
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.
M.C. Moron et al. J. Phys.:Condens. Matter (1993) · doi:10.1088/0953-8984/5/28/007
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.329_RbMnF4.mcif from MAGNDATA · entry page
sha256 of this copy: 8c5eb9fefab82a398f921719fc8ccf12348b8156d9e4e657414b3b7578537ddb
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.329_RbMnF4.mcif.