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Studies of the Temperature Dependence of the Structure and Magnetism of a Hexagonal-Bipyramidal Dysprosium(III) Single-Molecule Magnet
[Image: see text] The hexagonal-bipyramidal lanthanide(III) complex [Dy(O(t)Bu)Cl(18-C-6)][BPh(4)] (1; 18-C-6 = 1,4,7,10,13,16-hexaoxacyclooctadecane ether) displays an energy barrier for magnetization reversal (U(eff)) of ca. 1000 K in a zero direct-current field. Temperature-dependent X-ray diffra...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9632936/ https://www.ncbi.nlm.nih.gov/pubmed/34939782 http://dx.doi.org/10.1021/acs.inorgchem.1c02779 |
Sumario: | [Image: see text] The hexagonal-bipyramidal lanthanide(III) complex [Dy(O(t)Bu)Cl(18-C-6)][BPh(4)] (1; 18-C-6 = 1,4,7,10,13,16-hexaoxacyclooctadecane ether) displays an energy barrier for magnetization reversal (U(eff)) of ca. 1000 K in a zero direct-current field. Temperature-dependent X-ray diffraction studies of 1 down to 30 K reveal bending of the Cl–Ln–O(t)Bu angle at low temperature. Using ab initio calculations, we show that significant bending of the O–Dy–Cl angle upon cooling from 273 to 100 K leads to a ca. 10% decrease in the energy of the excited electronic states. A thorough exploration of the temperature and field dependencies of the magnetic relaxation rate reveals that magnetic relaxation is dictated by five mechanisms in different regimes: Orbach, Raman-I, quantum tunnelling of magnetization, and Raman-II, in addition to the observation of a phonon bottleneck effect. |
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