Importance of Out-of-State Spin–Orbit Coupling for Slow Magnetic Relaxation in Mononuclear FeII Complexes

Two mononuclear high-spin FeII complexes with trigonal planar ([FeII(N(TMS)2)2(PCy3)] (1) and distorted tetrahedral ([FeII(N(TMS)2)2(depe)] (2) geometries are reported (TMS = SiMe3, Cy = cyclohexyl, depe = 1,2-bis(diethylphosphino)ethane). The magnetic properties of 1 and 2 reveal the profound effec...

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Published inJournal of the American Chemical Society Vol. 133; no. 40; pp. 15806 - 15809
Main Authors Lin, Po-Heng, Smythe, Nathan C, Gorelsky, Serge I, Maguire, Steven, Henson, Neil J, Korobkov, Ilia, Scott, Brian L, Gordon, John C, Baker, R. Tom, Murugesu, Muralee
Format Journal Article
LanguageEnglish
Published American Chemical Society 12.10.2011
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Summary:Two mononuclear high-spin FeII complexes with trigonal planar ([FeII(N(TMS)2)2(PCy3)] (1) and distorted tetrahedral ([FeII(N(TMS)2)2(depe)] (2) geometries are reported (TMS = SiMe3, Cy = cyclohexyl, depe = 1,2-bis(diethylphosphino)ethane). The magnetic properties of 1 and 2 reveal the profound effect of out-of-state spin–orbit coupling (SOC) on slow magnetic relaxation. Complex 1 exhibits slow relaxation of the magnetization under an applied optimal dc field of 600 Oe due to the presence of low-lying electronic excited states that mix with the ground electronic state. This mixing re-introduces orbital angular momentum into the electronic ground state via SOC, and 1 thus behaves as a field-induced single-molecule magnet. In complex 2, the lowest-energy excited states have higher energy due to the ligand field of the distorted tetrahedral geometry. This higher energy gap minimizes out-of-state SOC mixing and zero-field splitting, thus precluding slow relaxation of the magnetization for 2.
ISSN:0002-7863
1520-5126
DOI:10.1021/ja203845x