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首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Electronic structure of a weakly antiferromagnetically coupled Mn IIMnIII Model relevant to manganese proteins: A combined EPR, ~(55)Mn-ENDOR, and DFT study
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Electronic structure of a weakly antiferromagnetically coupled Mn IIMnIII Model relevant to manganese proteins: A combined EPR, ~(55)Mn-ENDOR, and DFT study

机译:与锰蛋白有关的弱反铁磁耦合Mn IIMnIII模型的电子结构:EPR,〜(55)Mn-ENDOR和DFT的组合研究

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摘要

An analysis of the electronic structure of the [Mn~(II)Mn ~(III)(μ-OH)-(μ-piv)_2(Me_3tacn) _2](ClO_4)_2 (PivOH) complex is reported. It displays features that include: (i) a ground 1/2 spin state; (ii) a small exchange (J) coupling between the two Mn ions; (iii) a mono-μ-hydroxo bridge, bis-μ-carboxylato motif; and (iv) a strongly coupled, terminally bound N ligand to the MnIII. All of these features are observed in structural models of the oxygen evolving complex (OEC). Multifrequency electron paramagnetic resonance (EPR) and electron nuclear double resonance (ENDOR) measurements were performed on this complex, and the resultant spectra simulated using the Spin Hamiltonian formalism. The strong field dependence of the ~(55)Mn-ENDOR constrains the ~(55)Mn hyperfine tensors such that a unique solution for the electronic structure can be deduced. Large hyperfine anisotropy is required to reproduce the EPR/ENDOR spectra for both the Mn ~(II) and Mn~(III) ions. The large effective hyperfine tensor anisotropy of the Mn~(II), a d~5 ion which usually exhibits small anisotropy, is interpreted within a formalism in which the fine structure tensor of the Mn~(III) ion strongly perturbs the zero-field energy levels of the Mn~(II)Mn~(III) complex. An estimate of the fine structure parameter (d) for the Mn~(III) of-4 cm~(-1) was made, by assuming the intrinsic anisotropy of the Mn~(II) ion is small. The magnitude of the fine structure and intrinsic (onsite) hyperfine tensor of the Mn~(III) is consistent with the known coordination environment of the Mn~(III) ion as seen from its crystal structure. Broken symmetry density functional theory (DFT) calculations were performed on the crystal structure geometry. DFT values for both the isotropic and the anisotropic components of the onsite (intrinsic) hyperfine tensors match those inferred from the EPR/ENDOR simulations described above, to within 5%. This study demonstrates that DFT calculations provide reliable estimates for spectroscopic observables of mixed valence Mn complexes, even in the limit where the description of a well isolated S = 1/2 ground state begins to break down.
机译:报道了[Mn〜(II)Mn〜(III)(μ-OH)-(μ-piv)_2(Me_3tacn)_2](ClO_4)_2(PivOH)配合物的电子结构分析。它显示的功能包括:(i)地面1/2旋转状态; (ii)两个Mn离子之间的小交换(J)耦合; (iii)单-μ-羟基桥,双-μ-羧基基序; (iv)与MnIII牢固偶联,末端结合的N配体。所有这些特征都在析氧复合物(OEC)的结构模型中观察到。在该复合物上进行了多频电子顺磁共振(EPR)和电子核双共振(ENDOR)测量,并使用自旋哈密顿方程式模拟了所得光谱。 〜(55)Mn-ENDOR的强场相关性限制了〜(55)Mn超细张量,因此可以推导电子结构的唯一解。为了再现Mn〜(II)和Mn〜(III)离子的EPR / ENDOR光谱,需要较大的超细各向异性。 Mn〜(II)的大有效超精细张量各向异性,通常表现出较小各向异性的ad〜5离子,在形式主义中得到了解释,其中Mn〜(III)离子的精细结构张量强烈干扰了零场能-(II)Mn-(III)配合物的水平。通过假设Mn〜(II)离子的固有各向异性较小,对Mn〜(III)的精细结构参数(d)进行了估算,结果为-4 cm〜(-1)。从其晶体结构来看,Mn〜(III)的精细结构和本征(现场)超精细张量的大小与Mn〜(III)离子的已知配位环境一致。对晶体结构的几何形状进行了破碎的对称密度泛函理论(DFT)计算。现场(本征)超精细张量的各向同性和各向异性分量的DFT值与上述EPR / ENDOR模拟推断的值相差不超过5%。这项研究表明,即使在分离良好的S = 1/2基态的描述开始破裂的极限范围内,DFT计算也可为混合价Mn配合物的光谱观察提供可靠的估计。

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