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Leading-order relativistic effects on nuclear magnetic resonance Shielding tensors

机译:相对论对核磁共振的影响屏蔽张量

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We present perturbational ab initio calculations of the nuclear-spin-dependent relativistic corrections to the nuclear magnetic resonance shielding tensors that constitute,together with the other relativistic terms reported by us earlier,the full leading-order perturbational set of results for the one-electron relativistic contributions to this observable,based on the (Breit-)Pauli Hamiltonian.These contributions are considered for the U_2X (X=O,S,Se,Te,Po) and HX (X=F,Cl,Br,I,At) molecules,as well as the noble gas (Ne,Ar,Kr,Xe,Rn) atoms.The corrections are evaluated using the relativistic and magnetic operators as perturbations on an equal footing,calculated using analytical linear and quadratic response theory applied on top of a nonrelativistic reference state provided by self-consistent field calculations.The ~1H and heavy-atom nuclear magnetic shielding tensors are compared with four component,nearly basis-set-limit Dirac-Hartree-Fock calculations that include positronic excitations,as well as available literature data.Besides the easy interpretability of the different contributions in terms of familiar nonrelativistic concepts,the accuracy of the present perturbational scheme is striking for the isotropic part of the shielding tensor,for systems including elements up to Xe.
机译:我们介绍对核磁共振屏蔽张量的依赖于核自旋的相对论校正的微扰从头计算,这些校正与我们先前报道的其他相对论项一起构成了单电子的完整前导微扰结果集。基于(Breit-)Pauli Hamiltonian的相对论贡献.U_2X(X = O,S,Se,Te,Po)和HX(X = F,Cl,Br,I,At分子以及稀有气体(Ne,Ar,Kr,Xe,Rn)原子。使用相对论和磁算子以等基础上的扰动对校正进行评估,并使用顶部应用的分析线性和二次响应理论进行计算自相干场计算提供的非相对论参考状态。将〜1H和重原子核磁屏蔽张量与包括正电子激发在内的四个分量的基本组极限Dirac-Hartree-Fock计算进行比较除了对熟悉的非相对论概念而言不同贡献的易于解释性之外,对于包括张量不超过Xe的系统,本次扰动方案的精度对于屏蔽张量的各向同性部分也是惊人的。

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