Gohr Sebastian, Hrobárik Peter, Repiský Michal, Komorovský Stanislav, Ruud Kenneth, Kaupp Martin
Institut für Chemie, Theoretische Chemie/Quantenchemie, Technische Universität Berlin , Sekr. C7, Straße des 17. Juni 135, 10623 Berlin, Germany.
Department of Chemistry, Centre for Theoretical and Computational Chemistry (CTCC), UiT The Arctic University of Norway , 9037 Tromsø, Norway.
J Phys Chem A. 2015 Dec 24;119(51):12892-905. doi: 10.1021/acs.jpca.5b10996. Epub 2015 Dec 16.
The four-component matrix Dirac-Kohn-Sham (mDKS) implementation of EPR g- and hyperfine A-tensor calculations within a restricted kinetic balance framework in the ReSpect code has been extended to hybrid functionals. The methodology is validated for an extended set of small 4d(1) and 5d(1) MEXn systems, and for a series of larger Ir(II) and Pt(III) d(7) complexes (S = 1/2) with particularly large g-tensor anisotropies. Different density functionals (PBE, BP86, B3LYP-xHF, PBE0-xHF) with variable exact-exchange admixture x (ranging from 0% to 50%) have been evaluated, and the influence of structure and basis set has been examined. Notably, hybrid functionals with an exact-exchange admixture of about 40% provide the best agreement with experiment and clearly outperform the generalized-gradient approximation (GGA) functionals, in particular for the hyperfine couplings. Comparison with computations at the one-component second-order perturbational level within the Douglas-Kroll-Hess framework (1c-DKH), and a scaling of the speed of light at the four-component mDKS level, provide insight into the importance of higher-order relativistic effects for both properties. In the more extreme cases of some iridium(II) and platinum(III) complexes, the widely used leading-order perturbational treatment of SO effects in EPR calculations fails to reproduce not only the magnitude but also the sign of certain g-shift components (with the contribution of higher-order SO effects amounting to several hundreds of ppt in 5d complexes). The four-component hybrid mDKS calculations perform very well, giving overall good agreement with the experimental data.
ReSpect代码中,在受限动力学平衡框架内用于电子顺磁共振g张量和超精细A张量计算的四分量矩阵狄拉克-科恩-沙姆(mDKS)实现已扩展到杂化泛函。该方法在一组扩展的小4d(1)和5d(1) MEXn体系以及一系列具有特别大g张量各向异性的较大铱(II)和铂(III) d(7)配合物(S = 1/2)上得到了验证。评估了具有可变精确交换混合比例x(范围从0%到50%)的不同密度泛函(PBE、BP86、B3LYP-xHF、PBE0-xHF),并研究了结构和基组的影响。值得注意的是,精确交换混合比例约为40%的杂化泛函与实验结果的一致性最佳,并且明显优于广义梯度近似(GGA)泛函,特别是对于超精细耦合。与Douglas-Kroll-Hess框架内的单分量二阶微扰水平计算(1c-DKH)以及四分量mDKS水平的光速缩放进行比较,有助于深入了解高阶相对论效应对于这两种性质的重要性。在一些铱(II)和铂(III)配合物的更极端情况下,电子顺磁共振计算中广泛使用的自旋-轨道(SO)效应的领先阶微扰处理不仅无法再现某些g位移分量的大小,甚至无法再现其符号(在5d配合物中,高阶SO效应的贡献达到数百ppm)。四分量杂化mDKS计算表现非常出色,与实验数据总体上吻合良好。