Research/Sitter/MAGNDATA / 1.193_CrTe3.mcif
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| Magnetic group | PS 1 BNS 2.7 |
| Point group | 11′ |
| Parent space group | P 21/c No. 14 |
| Spins | collinear · net moment 0 μB per cell |
| Propagation | [1/2 1/2 1/2] 1k |
| Cell | a 15.76 · b 22.168 · c 23.036 Å · α 90° · β 118.46° · γ 90° |
| Transition | 55 K (−218 °C) |
| Measured at | 10 K |
| Magnetic ions | Cr |
| Largest moment component | 2.1 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cr1_1 | Cr | 0.004 | 0.2515 | 0.085 | 2.1 | 0.7 | 1.1 | 1.977 |
| Cr1_2 | Cr | 0.996 | 0.5015 | 0.165 | 2.1 | 0.7 | 1.1 | 1.977 |
| Cr2_1 | Cr | 0.011 | 0.1165 | 0.004 | −2.1 | −0.7 | −1.1 | 1.977 |
| Cr2_2 | Cr | 0.989 | 0.3665 | 0.246 | −2.1 | −0.7 | −1.1 | 1.977 |
| Te1_1 | Te | 0.1005 | 0.31 | 0.199 | ||||
| Te1_2 | Te | 0.8995 | 0.56 | 0.051 | ||||
| Te2_1 | Te | 0.1145 | 0.2995 | 0.0365 | ||||
| Te2_2 | Te | 0.8855 | 0.5495 | 0.2135 | ||||
| Te3_1 | Te | 0.139 | 0.0865 | 0.2165 | ||||
| Te3_2 | Te | 0.861 | 0.3365 | 0.0335 | ||||
| Te4_1 | Te | 0.1375 | 0.163 | 0.123 | ||||
| Te4_2 | Te | 0.8625 | 0.413 | 0.127 | ||||
| Te5_1 | Te | 0.1455 | 0.0295 | 0.0475 | ||||
| Te5_2 | Te | 0.8545 | 0.2795 | 0.2025 | ||||
| Te6_1 | Te | 0.3975 | 0.193 | 0.1325 | ||||
| Te6_2 | Te | 0.6025 | 0.443 | 0.1175 |
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.A. McGuire et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.95.144421
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.193_CrTe3.mcif from MAGNDATA · entry page
sha256 of this copy: 355c1083c8f75437d19d7546edd7312838ca3c6c076c7a51ad4891ceeaae68d3
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.193_CrTe3.mcif.