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穆斯堡尔、电子顺磁共振和密度泛函理论研究合成的 S = 1/2 Fe(III)-O-Fe(IV)=O 配合物。Fe(IV)=O 位点的超交换介导的自旋转变。

Mössbauer, electron paramagnetic resonance, and density functional theory studies of synthetic S = 1/2 Fe(III)-O-Fe(IV)═O complexes. Superexchange-mediated spin transition at the Fe(IV)═O site.

机构信息

Department of Chemistry, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA.

出版信息

Inorg Chem. 2010 Sep 20;49(18):8310-22. doi: 10.1021/ic100870v.

DOI:10.1021/ic100870v
PMID:20795646
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC2957120/
Abstract

Previously we have characterized two high-valent complexes [LFe(IV)(μ-O)(2)Fe(III)L], 1, and [LFe(IV)(O)(μ-O)(OH) Fe(IV)L], 4. Addition of hydroxide or fluoride to 1 produces two new complexes, 1-OH and 1-F. Electron paramagnetic resonance (EPR) and Mössbauer studies show that both complexes have an S = 1/2 ground state which results from antiferromagnetic coupling of the spins of a high-spin (S(a) = 5/2) Fe(III) and a high-spin (S(b) = 2) Fe(IV) site. 1-OH can also be obtained by a 1-electron reduction of 4, which has been shown to have an Fe(IV)═O site. Radiolytic reduction of 4 at 77 K yields a Mössbauer spectrum identical to that observed for 1-OH, showing that the latter contains an Fe(IV)═O. Interestingly, the Fe(IV)═O moiety has S(b) = 1 in 4 and S(b) = 2 in 1-OH and 1-F. From the temperature dependence of the S = 1/2 signal we have determined the exchange coupling constant J (ℋ = JS(a)·S(b) convention) to be 90 ± 20 cm(-1) for both 1-OH and 1-F. Broken-symmetry density functional theory (DFT) calculations yield J = 135 cm(-1) for 1-OH and J = 104 cm(-1) for 1-F, in good agreement with the experiments. DFT analysis shows that the S(b) = 1 → S(b) = 2 transition of the Fe(IV)═O site upon reduction of the Fe(IV)-OH site to high-spin Fe(III) is driven primarily by the strong antiferromagnetic exchange in the (S(a) = 5/2, S(b) = 2) couple.

摘要

先前,我们已经对两个高价络合物[LFe(IV)(μ-O)(2)Fe(III)L],1 和[LFe(IV)(O)(μ-O)(OH) Fe(IV)L],4 进行了特征描述。向 1 中添加氢氧化物或氟化物会生成两个新的络合物,1-OH 和 1-F。电子顺磁共振(EPR)和穆斯堡尔研究表明,这两个络合物都具有 S = 1/2 的基态,这是由高自旋(S(a) = 5/2)Fe(III)和高自旋(S(b) = 2)Fe(IV)位点的反铁磁耦合导致的。1-OH 也可以通过 4 的 1 电子还原得到,这已经表明 4 具有 Fe(IV)═O 位点。在 77 K 下对 4 进行辐射还原会产生与 1-OH 观察到的相同的穆斯堡尔光谱,表明后者含有 Fe(IV)═O。有趣的是,在 4 中 Fe(IV)═O 部分的 S(b) = 1,而在 1-OH 和 1-F 中 S(b) = 2。根据 S = 1/2 信号的温度依赖性,我们确定 1-OH 和 1-F 的交换耦合常数 J(HS = JS(a)·S(b) 约定)分别为 90 ± 20 cm(-1)。破对称密度泛函理论(DFT)计算得出,对于 1-OH,J = 135 cm(-1),对于 1-F,J = 104 cm(-1),与实验结果吻合较好。DFT 分析表明,Fe(IV)-OH 位点还原为高自旋 Fe(III)时,Fe(IV)═O 位点的 S(b) = 1→S(b) = 2 跃迁主要由(S(a) = 5/2,S(b) = 2)偶对中的强反铁磁交换驱动。

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