Fliegl Heike, Sundholm Dage, Taubert Stefan, Jusélius Jonas, Klopper Wim
Institut für Nanotechnologie, Forschungszentrum Karlsruhe GmbH, Hermann-von-Helmholtz-Platz 1, D-76344 Eggenstein-Leopoldshafen, Germany.
J Phys Chem A. 2009 Jul 30;113(30):8668-76. doi: 10.1021/jp9029776.
The magnetically induced current densities for ring-shaped hydrocarbons are studied at the density functional theory (DFT) and second-order Møller-Plesset (MP2) levels using gauge-including atomic orbitals. The current densities are calculated using the gauge-including magnetically induced current approach. The calculations show that all studied hydrocarbon rings sustain strong diatropic and paratropic ring currents when exposed to an external magnetic field, regardless whether they are unsaturated or not. For nonaromatic rings, the strength of the paratropic current flowing inside the ring is as large as the diatropic one circling outside it, yielding a vanishing net ring current. For aromatic molecules, the diatropic current on the outside of the ring is much stronger than the paratropic one inside, giving rise to the net diatropic ring current that is typical for aromatic molecules. For antiaromatic molecules, the paratropic ring-current contribution inside the ring dominates. For homoaromatic molecules, the diatropic current circles at the periphery of the ring. The ring current is split at the CH(2) moiety; the main fraction of the current flow passes outside the CH(2) at the hydrogens, and some current flows inside the carbon atom. The diatropic current does not take the through-space short-cut pathway, whereas the paratropic current does take that route. Calculations of the ring-current profile show that the ring current of benzene is not transported by the pi electrons on both sides of the molecular ring. The strongest diatropic ring current flows on the outside of the ring and in the ring plane. A weaker paratropic current circles inside the ring with the largest current density in the ring plane. Due to the ring strain, small unconjugated and saturated hydrocarbon rings sustain a strong ring current which could be called ring-strain current. Nuclear magnetic shieldings calculated for 1,3,5-cycloheptatriene and homotropylium at the DFT and MP2 levels agree well with experimental values.
利用含规范原子轨道,在密度泛函理论(DFT)和二阶Møller-Plesset(MP2)水平上研究了环状碳氢化合物的磁感应电流密度。使用含规范磁感应电流方法计算电流密度。计算表明,所有研究的碳氢化合物环在外部磁场作用下都能维持强抗磁和顺磁环电流,无论它们是否不饱和。对于非芳香环,环内流动的顺磁电流强度与环外环绕的抗磁电流强度一样大,导致净环电流消失。对于芳香分子,环外的抗磁电流比环内的顺磁电流强得多,产生了芳香分子典型的净抗磁环电流。对于反芳香分子,环内的顺磁环电流贡献占主导。对于同芳香分子,抗磁电流在环的周边环绕。环电流在CH(2)部分分裂;电流的主要部分在氢原子处从CH(2)外部通过,一些电流在碳原子内部流动。抗磁电流不采用空间捷径路径,而顺磁电流采用该路径。环电流分布的计算表明,苯的环电流不是由分子环两侧的π电子传输的。最强的抗磁环电流在环的外部和环平面内流动。较弱的顺磁电流在环内环绕,在环平面内电流密度最大。由于环张力,小的非共轭和饱和碳氢化合物环维持着强环电流,可称为环张力电流。在DFT和MP2水平上为1,3,5-环庚三烯和高环庚三烯计算的核磁屏蔽与实验值吻合良好。