Research/Sitter/MAGNDATA / 1.1.97_EuNi2As2.mcif
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| Magnetic group | I4221′(0,0,γ)-q00s |
| Point group | 4221′ |
| Parent space group | I 4/m m m No. 139 |
| Repeats every | 1.09 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.92] 1k |
| Cell | a 4.1015 · b 4.1015 · c 10.0466 Å · α 90° · β 90° · γ 90° |
| Transition | 15 K (−258 °C) |
| Measured at | 2 K |
| Magnetic ions | Eu |
| Largest moment component | 6.75 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Eu1_1 | Eu | 0 | 0 | 0 | ||||
| Ni1_1 | Ni | 0 | 0.5 | 0.25 | ||||
| As1_1 | As | 0 | 0 | 0.3683 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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.
W.T. Jin et al. PHYSICAL REVIEW B (2019) · doi:10.1103/PhysRevB.99.014425
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.97_EuNi2As2.mcif from MAGNDATA · entry page
sha256 of this copy: c4a5d79e9d53a51d36befaaea47be1fe0fc894f6eafc1c56f9b0d45d8948e632
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.97_EuNi2As2.mcif.