Zolnhofer Eva M, Opalade Adedamola A, Jackson Timothy A, Heinemann Frank W, Meyer Karsten, Krzystek J, Ozarowski Andrew, Telser Joshua
Department of Chemistry and Pharmacy, Inorganic Chemistry, Friedrich-Alexander University Erlangen-Nürnberg (FAU), 91058 Erlangen, Germany.
Department of Chemistry, University of Kansas, 1567 Irving Hill Road, Lawrence, Kansas 66045, United States.
Inorg Chem. 2021 Dec 6;60(23):17865-17877. doi: 10.1021/acs.inorgchem.1c02471. Epub 2021 Nov 1.
Octahedral coordination complexes of the general formula -[MX(RECHCHER)] (M = Ti, V, Cr, Mn; E = N, P; R = alkyl, aryl) are a cornerstone of both coordination and organometallic chemistry, and many of these complexes are known to have unique electronic structures that have been incompletely examined. The -[CrCl(dmpe)] complex (dmpe = MePCHCHPMe), originally reported by Girolami and co-workers in 1985, is a rare example of a six-coordinate d system with an = 1 (spin triplet) ground state, as opposed to the high-spin ( = 2, spin quintet) state. The ground-state properties of = 1 systems are challenging to study using conventional spectroscopic methods, and consequently, the electronic structure of -[CrCl(dmpe)] has remained largely unexplored. In this present work, we have employed high-frequency and -field electron paramagnetic resonance (HFEPR) spectroscopy to characterize the ground-state electronic structure of -[CrCl(dmpe)]. This analysis yielded a complete set of spin Hamiltonian parameters for this = 1 complex: = +7.39(1) cm, = +0.093(1) ( = 0.012), and = [1.999(5), 2.00(1), 2.00(1)]. To develop a detailed electronic structure description for -[CrCl(dmpe)], we employed both classical ligand-field theory and quantum chemical theory (QCT) calculations, which considered all quintet, triplet, and singlet ligand-field states. While the high density of states suggests an unexpectedly complex electronic structure for this "simple" coordination complex, both the ligand-field and QCT methods were able to reproduce the experimental spin Hamiltonian parameters quite nicely. The QCT computations were also used as a basis for assigning the electronic absorption spectrum of -[CrCl(dmpe)] in toluene.
通式为-[MX(RECHCHER)](M = Ti、V、Cr、Mn;E = N、P;R = 烷基、芳基)的八面体配位络合物是配位化学和有机金属化学的基石,已知其中许多络合物具有尚未得到充分研究的独特电子结构。-[CrCl(dmpe)]络合物(dmpe = MePCHCHPMe)最初由吉罗拉米及其同事于1985年报道,是具有S = 1(自旋三重态)基态的六配位d体系的罕见例子,与高自旋(S = 2,自旋五重态)状态相反。对于S = 1体系的基态性质,使用传统光谱方法进行研究具有挑战性,因此,-[CrCl(dmpe)]的电子结构在很大程度上仍未被探索。在本工作中,我们采用了高频和高场电子顺磁共振(HFEPR)光谱来表征-[CrCl(dmpe)]的基态电子结构。该分析得出了这个S = 1络合物的一整套自旋哈密顿参数:g = +7.39(1) cm⁻¹,D = +0.093(1) cm⁻¹(E/D = 0.012),以及A = [1.999(5), 2.00(1), 2.00(1)] cm⁻¹。为了对-[CrCl(dmpe)]进行详细的电子结构描述,我们采用了经典配体场理论和量子化学理论(QCT)计算,其中考虑了所有的五重态、三重态和单重态配体场状态。虽然态密度表明这个“简单”配位络合物具有意想不到的复杂电子结构,但配体场和QCT方法都能够很好地重现实验自旋哈密顿参数。QCT计算还被用作确定-[CrCl(dmpe)]在甲苯中的电子吸收光谱的基础。