N-Heterocyclic carbene adducts to [Cp′FeI]2: synthesis and molecular and electronic structure

N-Heterocyclic carbene adducts to [Cp′FeI]2: synthesis and molecular and electronic structure
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N-杂环卡宾与 [Cpâ²FeI]2 的加合物:合成以及分子和电子结构

DOI:
10.1039/c5qi00235d
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发表时间:
2016
影响因子:
7
通讯作者:
M. D. Walter
M. D. Walter
中科院分区:
化学1区
文献类型:
--
作者:
M. Reiners;D. Baabe;K. Harms;M. Maekawa;C. G. Daniliuc;M. Freytag;P. G. Jones;M. D. Walter

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添加 N-杂环卡宾 (L = 1,3-二叔丁基咪唑-2-亚基 (ItBu)、1,3-二异丙基-4,5-二甲基咪唑-2-亚基 (IiPr2Me2)、1,3- 基咪唑-2-亚基 (IMes) 和1,3-二-(2,6-二异丙基苯基)咪唑-2-亚基 (IPr)) 与铁半夹心配合物 [Cp′FeI]2 (Cp′ = η5-1,2,4-(Me3C)3C5H2, 1) 形成中性 16VE 加合物 [Cp′FeI(L)] (2–5),产率中等至优异。这些复合物具有结构特征。 NHC 配体与 Fe(II) 原子牢固结合,因此在 NMR 和化学时间尺度上未观察到交换。起始材料1中的Fe(II)原子采用高自旋构型(S=2)并且在低温下弱反铁磁耦合。此外,与之前有关[(η5-C5Me5)FeCl(NHC)]系统的报道相反,其中Fe(II)原子呈现中间自旋(S = 1),在NHC配体配位时不会发生自旋态变化;固态磁化率和零场 57Fe 穆斯堡尔谱研究表明,配合物 2-5 中的 Fe(II) 原子保持其高自旋状态 (S = 2)。 B3LYP 理论水平的密度泛函理论 (DFT) 研究也同意化合物 2-5 的良好分离的 S = 2 基态。令人惊讶的是,对于 Fe(II) 高自旋体系,化合物 1-5 在穆斯堡尔谱中表现出缓慢的顺磁弛豫;这可以追溯到自旋-自旋和自旋-晶格弛豫过程,具有异常大的自旋-晶格弛豫势垒。提出了一个结构模型,将这些过程与晶体堆积效应联系起来。
Addition of N-heterocyclic carbenes (L = 1,3-di-tert-butylimidazol-2-ylidene (ItBu), 1,3-di-iso-propyl-4,5-dimethylimidazol-2-yildene (IiPr2Me2), 1,3-mesitylimidazol-2-yildene (IMes) and 1,3-di-(2,6-di-isopropylphenyl)imidazol-2-yildene (IPr)) to the iron half-sandwich complex [Cp′FeI]2 (Cp′ = η5-1,2,4-(Me3C)3C5H2, 1) forms the neutral, 16VE adducts [Cp′FeI(L)] (2–5) in moderate to excellent yields. These complexes were structurally characterised. The NHC ligand binds strongly to the Fe(II) atom, so that no exchange is observed on the NMR and chemical time scale. Fe(II) atoms in the starting material 1 adopt a high-spin configuration (S = 2) and are weakly antiferromagnetically coupled at low temperatures. Furthermore, in contrast to previous reports on related [(η5-C5Me5)FeCl(NHC)] systems, in which the Fe(II) atoms assume an intermediate spin (S = 1), no spin state change occurs upon coordination of the NHC ligand; the Fe(II) atoms in complexes 2–5 retain their high-spin state (S = 2) as shown by solid state magnetic susceptibility and zero-field 57Fe Mössbauer spectroscopy investigations. Density functional theory (DFT) studies at the B3LYP level of theory also agree with a well separated S = 2 ground state for compounds 2–5. Surprisingly for Fe(II) high-spin systems, compounds 1–5 exhibit slow paramagnetic relaxation in their Mössbauer spectra; this can be traced to spin–spin and spin–lattice relaxation processes with unusually large spin–lattice relaxation barriers. A structural model is proposed that associates these processes with crystal packing effects.
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