Studies of the Temperature Dependence of the Structure and Magnetism of a Hexagonal-Bipyramidal Dysprosium(III) Single-Molecule Magnet

The hexagonal-bipyramidal lanthanide­(III) complex [Dy­(OtBu)­Cl­(18-C-6)]­[BPh4] (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...

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Veröffentlicht in:Inorganic chemistry 2022-01, Vol.61 (1), p.227-235
Hauptverfasser: Ding, You-Song, Blackmore, William J. A., Zhai, Yuan-Qi, Giansiracusa, Marcus J., Reta, Daniel, Vitorica-Yrezabal, Inigo, Winpenny, Richard E. P., Chilton, Nicholas F., Zheng, Yan-Zhen
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Sprache:eng
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Zusammenfassung:The hexagonal-bipyramidal lanthanide­(III) complex [Dy­(OtBu)­Cl­(18-C-6)]­[BPh4] (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–OtBu 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.
ISSN:0020-1669
1520-510X
DOI:10.1021/acs.inorgchem.1c02779