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Electric field gradients in Hg compounds: Molecular orbital (MO) analysis and comparison of 4-component and 2-component (ZORA) methods

机译:汞化合物中的电场梯度:分子轨道(MO)分析和4组分和2组分(ZORA)方法的比较

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摘要

We examine the performance of Density Functional Theory (DFT) approaches based on the Zeroth-Order Regular Approximation (ZORA) Hamiltonian (with and without inclusion of spin-orbit coupling) for predictions of electric field gradients (EFGs) at the heavy atom Hg nucleus. This is achieved by comparing with benchmark DFT and CCSD-T data (Arcisauskaite et al., Phys. Chem. Chem. Phys., 2012, 14, 2651-2657) obtained from 4-component Dirac-Coulomb Hamiltonian calculations. The investigated set of molecules comprises linear HgL2 (L = Cl, Br, I, CH3) and bent HgCl2 mercury compounds as well as the trigonal planar [HgCl3](-) system. In 4-component calculations we used the dyall. cv3z basis set for Hg, Br, I and the cc-pCVTZ basis set for H, C, Cl, whereas in ZORA calculations we used the QZ4P basis set for all the atoms. ZORA-4 reproduces the fully relativistic 4-component DFT reference values within 6% for all studied Hg compounds and employed functionals (BH&H, BP86, PBE0), whereas scalar relativistic (SR)-ZORA-4 results show deviations of up to 15%. Compared to our 4-component CCSD-T benchmark the BH&H functional performs best at both 4-component and ZORA levels. We furthermore observe that changes in the largest component of the diagonalised EFG tensor, V-zz, of linear HgCl2 show a slightly stronger dependence than the r(-3) scaling upon bond length r(Hg-Cl) alterations. The 4-component/BH&H V-zz value of -9.26 a. u. for a bent HgCl2 (+Cl-Hg-Cl = 120 degrees) is close to -9.60 a. u. obtained for the linear HgCl2 structure. Thus a point charge model for EFG calculations completely fails in this case. By means of a projection analysis of molecular orbital (MO) contributions to V-zz in terms of the atomic constituents, we conclude that this is due to the increased importance of the Hg 5d orbitals upon bending HgCl2 compared to the linear HgCl2 structure. Changing ligand leads to only minor changes in V-zz (from -9.60 a. u. (HgCl2) to -8.85 a. u. (HgI2) at the 4-component/BH&H level). This appears to be due to cancellation of contributions with opposite signs to V-zz arising from: (i) increasing electron donation from occupied ligand orbitals to the formally empty Hg 6p orbitals and (ii) an increasing bond length and a decreasing negative charge on the ligand along the series.
机译:我们研究了基于零阶正则逼近(ZORA)哈密顿量(有或没有自旋轨道耦合)的密度泛函理论(DFT)方法的性能,以预测重原子Hg核处的电场梯度(EFG)。 。通过与从4组分Dirac-Coulomb Hamilton计算获得的基准DFT和CCSD-T数据(Arcisauskaite等人,Phys。Chem。Chem。Phys。,2012,14,2651-2657)进行比较,即可实现这一点。研究的分子组包括线性HgL2(L = Cl,Br,I,CH3)和弯曲的HgCl2汞化合物以及三角平面[HgCl3](-)系统。在4分量计算中,我们使用了dyall。 Hg,Br,I的cv3z基础集和H,C,Cl的cc-pCVTZ基础集,而在ZORA计算中,我们对所有原子使用QZ4P基础集。 ZORA-4再现了所有研究的Hg化合物和使用的功能(BH&H,BP86,PBE0)的完全相对论4分量DFT参考值在6%之内,而标量相对论(SR)-ZORA-4结果显示偏差高达15% 。与我们的4分量CCSD-T基准相比,BH&H功能在4分量和ZORA级别上均表现最佳。我们进一步观察到,线性HgCl2的对角化EFG张量的最大分量V-zz的变化显示,对键长r(Hg-Cl)的变化比r(-3)缩放的依赖性要强一些。 4-分量/ BH&H V-zz值为-9.26 a。你弯曲的HgCl2(+ Cl-Hg-Cl = 120度)的值接近-9.60 a。你线性HgCl2结构获得。因此,在这种情况下,用于EFG计算的点费用模型完全失败。通过对原子原子方面对V-zz的分子轨道(MO)贡献的投影分析,我们得出结论,这是由于与线性HgCl2结构相比,HgCl2弯曲时Hg 5d轨道的重要性增加。改变配体只会导致V-zz的微小变化(在4组分/ BH&H水平下,从-9.60 a。u。(HgCl2)到-8.85 a。u。(HgI2)。这似乎是由于以下原因导致的对V-zz的相反符号的抵消:(i)从占据的配体轨道向正空的Hg 6p轨道的电子给体增加,以及(ii)键长增加,且负电荷降低系列中的配体。

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