Research/Sitter/MAGNDATA / 1.307_Mn5Si3.mcif
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| Magnetic group | PS 1 BNS 1.3 |
| Point group | 11′ |
| Parent space group | P 63/m c m No. 193 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 1/2 0] 1k |
| Cell | a 6.91 · b 11.9685 · c 4.814 Å · α 90° · β 90° · γ 90° |
| Transition | 66 K (−207 °C) |
| Measured at | 4.2 K |
| Magnetic ions | Mn |
| Largest moment component | 2.16 μB |
| Method | Neutron polarimetry |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1_1 | Mn | 0 | 0.3333 | 0 | −0.28 | 1.04 | −0.53 | 1.2004 |
| Mn1_2 | Mn | 0 | 0.6667 | 0.5 | 0.28 | −1.04 | 0.53 | 1.2004 |
| Mn1_3 | Mn | 0 | 0.6667 | 0 | 0.28 | −1.04 | 0.53 | 1.2004 |
| Mn1_4 | Mn | 0 | 0.3333 | 0.5 | −0.28 | 1.04 | −0.53 | 1.2004 |
| Mn2_1 | Mn | 0.236 | 0 | 0.25 | ||||
| Mn2_2 | Mn | 0.764 | 0 | 0.75 | ||||
| Mn2_3 | Mn | 0.882 | 0.118 | 0.25 | 0.11 | −2.16 | −0.79 | 2.3026 |
| Mn2_4 | Mn | 0.882 | 0.882 | 0.25 | −0.11 | 2.16 | 0.79 | 2.3026 |
| Mn2_5 | Mn | 0.118 | 0.882 | 0.75 | −0.65 | −0.13 | −1.73 | 1.8526 |
| Mn2_6 | Mn | 0.118 | 0.118 | 0.75 | 0.65 | 0.13 | 1.73 | 1.8526 |
| Si1_1 | Si | 0.5991 | 0 | 0.25 | ||||
| Si1_2 | Si | 0.4009 | 0 | 0.75 | ||||
| Si1_3 | Si | 0.7005 | 0.2995 | 0.25 | ||||
| Si1_4 | Si | 0.7005 | 0.7005 | 0.25 | ||||
| Si1_5 | Si | 0.2995 | 0.7005 | 0.75 | ||||
| Si1_6 | Si | 0.2995 | 0.2995 | 0.75 |
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.
P J Brown et al. J. Phys.: Condens. Matter (1992) · doi:10.1088/0953-8984/4/49/029
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.307_Mn5Si3.mcif from MAGNDATA · entry page
sha256 of this copy: 78366715ff5b5bd771dd75b83e0c43a68cfc10d1c699137ad0576c78d446737d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.307_Mn5Si3.mcif.