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四分量相对论核磁共振屏蔽理论:磁平衡规范包含原子轨道。

Four-component relativistic theory for nuclear magnetic shielding: magnetically balanced gauge-including atomic orbitals.

机构信息

Beijing National Laboratory for Molecular Sciences, Institute of Theoretical and Computational Chemistry, State College of Chemistry and Molecular Engineering, and Center for Computational Science and Engineering, Peking University, Beijing 100871, People's Republic of China.

出版信息

J Chem Phys. 2009 Dec 28;131(24):244113. doi: 10.1063/1.3283036.

Abstract

It is recognized only recently that the incorporation of the magnetic balance condition is absolutely essential for four-component relativistic theories of magnetic properties. Another important issue to be handled is the so-called gauge problem in calculations of, e.g., molecular magnetic shielding tensors with finite bases. It is shown here that the magnetic balance can be adapted to distributed gauge origins, leading to, e.g., magnetically balanced gauge-including atomic orbitals (MB-GIAOs) in which each magnetically balanced atomic orbital has its own local gauge origin placed on its center. Such a MB-GIAO scheme can be combined with any level of theory for electron correlation. The first implementation is done here at the coupled-perturbed Dirac-Kohn-Sham level. The calculated molecular magnetic shielding tensors are not only independent of the choice of gauge origin but also converge rapidly to the basis set limit. Close inspections reveal that (zeroth order) negative energy states are only important for the expansion of first order electronic core orbitals. Their contributions to the paramagnetism are therefore transferable from atoms to molecule and are essentially canceled out for chemical shifts. This allows for simplifications of the coupled-perturbed equations.

摘要

直到最近才认识到,对于四分量相对论磁性质理论,纳入磁平衡条件是绝对必要的。另一个需要处理的重要问题是计算有限基分子磁屏蔽张量时所谓的规范问题。本文表明,磁平衡可以适应分布式规范原点,从而导致例如具有各自局部规范原点的磁平衡包含原子轨道(MB-GIAO),其中每个磁平衡原子轨道都位于其中心。这种 MB-GIAO 方案可以与任何电子相关理论水平相结合。本文首次在耦合微扰狄拉克-科恩-肖姆(CPDK)水平上实现。计算得到的分子磁屏蔽张量不仅不依赖于规范原点的选择,而且还快速收敛到基组极限。仔细检查表明,(零阶)负能态仅对一阶电子核轨道的展开很重要。因此,它们对顺磁性质的贡献可以从原子转移到分子,并且对于化学位移基本上被抵消。这允许简化耦合微扰方程。

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