Stavretis Shelby E, Atanasov Mihail, Podlesnyak Andrey A, Hunter Seth C, Neese Frank, Xue Zi-Ling
Department of Chemistry, The University of Tennessee , Knoxville, Tennessee 37996, United States.
Max Planck Institute for Chemical Energy Conversion , Stiftstraße 34-36, D-45470 Mülheim an der Ruhr, Germany.
Inorg Chem. 2015 Oct 19;54(20):9790-801. doi: 10.1021/acs.inorgchem.5b01505. Epub 2015 Oct 2.
Zero-field splitting (ZFS) parameters of nondeuterated metalloporphyrins [Fe(TPP)X] (X = F, Br, I; H₂TPP = tetraphenylporphyrin) have been directly determined by inelastic neutron scattering (INS). The ZFS values are D = 4.49(9) cm⁻¹ for tetragonal polycrystalline [Fe(TPP)F], and D = 8.8(2) cm⁻¹, E = 0.1(2) cm⁻¹ and D = 13.4(6) cm⁻¹, E = 0.3(6) cm⁻¹ for monoclinic polycrystalline [Fe(TPP)Br] and [Fe(TPP)I], respectively. Along with our recent report of the ZFS value of D = 6.33(8) cm⁻¹ for tetragonal polycrystalline [Fe(TPP)Cl], these data provide a rare, complete determination of ZFS parameters in a metalloporphyrin halide series. The electronic structure of [Fe(TPP)X] (X = F, Cl, Br, I) has been studied by multireference ab initio methods: the complete active space self-consistent field (CASSCF) and the N-electron valence perturbation theory (NEVPT2) with the aim of exploring the origin of the large and positive zero-field splitting D of the ⁶A₁ ground state. D was calculated from wave functions of the electronic multiplets spanned by the d⁵ configuration of Fe(III) along with spin–orbit coupling accounted for by quasi degenerate perturbation theory. Results reproduce trends of D from inelastic neutron scattering data increasing in the order from F, Cl, Br, to I. A mapping of energy eigenvalues and eigenfunctions of the S = 3/2 excited states on ligand field theory was used to characterize the σ- and π-antibonding effects decreasing from F to I. This is in agreement with similar results deduced from ab initio calculations on CrX₆³⁻ complexes and also with the spectrochemical series showing a decrease of the ligand field in the same directions. A correlation is found between the increase of D and decrease of the π- and σ-antibonding energies e(λ)(X) (λ = σ, π) in the series from X = F to I. Analysis of this correlation using second-order perturbation theory expressions in terms of angular overlap parameters rationalizes the experimentally deduced trend. D parameters from CASSCF and NEVPT2 results have been calibrated against those from the INS data, yielding a predictive power of these approaches. Methods to improve the quantitative agreement between ab initio calculated and experimental D and spectroscopic transitions for high-spin Fe(III) complexes are proposed.
通过非弹性中子散射(INS)直接测定了非氘代金属卟啉[Fe(TPP)X](X = F、Br、I;H₂TPP = 四苯基卟啉)的零场分裂(ZFS)参数。对于四方多晶[Fe(TPP)F],ZFS值为D = 4.49(9) cm⁻¹;对于单斜多晶[Fe(TPP)Br]和[Fe(TPP)I],ZFS值分别为D = 8.8(2) cm⁻¹、E = 0.1(2) cm⁻¹以及D = 13.4(6) cm⁻¹、E = 0.3(6) cm⁻¹。连同我们最近报道的四方多晶[Fe(TPP)Cl]的ZFS值D = 6.33(8) cm⁻¹,这些数据提供了卤化金属卟啉系列中ZFS参数罕见的完整测定。通过多参考从头算方法研究了[Fe(TPP)X](X = F、Cl、Br、I)的电子结构:完全活性空间自洽场(CASSCF)和N电子价态微扰理论(NEVPT2),目的是探索⁶A₁基态大的正零场分裂D的起源。D是根据Fe(III)的d⁵构型所跨越的电子多重态的波函数计算得出的,同时考虑了由准简并微扰理论处理的自旋 - 轨道耦合。结果重现了非弹性中子散射数据中D的趋势,按F、Cl、Br到I的顺序增加。利用配体场理论对S = 3/2激发态的能量本征值和本征函数进行映射,以表征从F到I时σ和π反键效应的降低。这与对CrX₆³⁻配合物的从头算计算得出的类似结果一致,也与在相同方向上显示配体场降低的光谱化学序列一致。发现从X = F到I的系列中,D的增加与π和σ反键能e(λ)(X)(λ = σ、π)的降低之间存在相关性。使用基于角重叠参数的二阶微扰理论表达式对这种相关性进行分析,使实验推导的趋势合理化。已根据INS数据对CASSCF和NEVPT2结果中的D参数进行了校准,从而得出了这些方法的预测能力。提出了改善高自旋Fe(III)配合物从头算计算的D与实验D以及光谱跃迁之间定量一致性的方法。