期刊
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
卷 136, 期 19, 页码 7026-7037出版社
AMER CHEMICAL SOC
DOI: 10.1021/ja5017014
关键词
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资金
- JSPS [20550130, 24550162]
- MEXT [23110723]
- Shorai Foundation for Science and Technology
- Hyogo Science and Technology Association
- Grants-in-Aid for Scientific Research [26410093, 20550130, 24550162, 23550015] Funding Source: KAKEN
We present a comprehensive study of the synthesis, heat capacity, crystal structures, UV-vis-NIR and mid-IR spectra, DFT calculations, and magnetic and electrical properties of a one-dimensional (1D) rhodium(I)-semiquinonato complex, [Rh(3,6-DBSQ-4,5-(MeO)(2))(CO)(2)](infinity) (3), where 3,6-DBSQ4,5-(MeO)(2)(center dot-) represents 3,6-di-tert-butyl-4,5-climethoxy-1,2-benzosemiquinonato radical anion. The compound 3 comprises neutral ID chains of complex molecules stacked in a staggered arrangement with short Rh-Rh distances of 3.0796(4) and 3.1045(4) angstrom at 226 K and exhibits unprecedented bistable multifunctionality with respect to its magnetic and conductive properties in the temperature range of 228-207 K. The observed bistability results from the thermal hysteresis across a first-order phase transition, and the transition accompanies the exchange of the interchain C-H center dot center dot center dot O hydrogen-bond partners between the semiquinonato ligands. The strong overlaps of the complex molecules lead to unusually strong ferromagnetic interactions in the low-temperature (LT) phase. Furthermore, the magnetic interactions in the 1D chain drastically change from strongly ferromagnetic in the LT phase to antiferromagnetic in the room-temperature (RT) phase with hysteresis. In addition, the compound 3 exhibits long-range antiferromagnetic ordering between the ferromagnetic chains and spontaneous magnetization because of spin canting (canted antiferromagnetism) at a transition temperature T-N of 14.2 K. The electrical conductivity of 3 at 300 K is 4.8 X 10(-4) S cm(-1), which is relatively high despite Rh not being in a mixed-valence state. The temperature dependence of electrical resistivity also exhibits a clear hysteresis across the first-order phase transition. Furthermore, the ferromagnetic LT phase can be easily stabilized up to RT by the application of a relatively weak applied pressure of 1.4 kbar, which reflects the bistable characteristics and demonstrates the simultaneous control of multifiinctionality through external perturbation.
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