Department of Chemistry, Faculty of Sciences, Okayama University, Tsushima-naka 3-1-1, Okayama-Shi, Okayama-ken, 700-8530, Japan.
J Mol Model. 2010 May;16(5):965-74. doi: 10.1007/s00894-009-0603-1. Epub 2009 Oct 23.
Spin-restricted DFT (X3LYP and B3LYP) and ab initio (MP2(fc) and CCSD(fc)) calculations in conjunction with the Aug-CC-pVDZ and Aug-CC-pVTZ basis sets were performed on a series of hydrogen bonded complexes PN...HX (X = F, Cl, Br) to examine the variations of their equilibrium gas phase structures, energetic stabilities, electronic properties, and vibrational characteristics in their electronic ground states. In all cases the complexes were predicted to be stable with respect to the constituent monomers. The interaction energy (Delta E) calculated using a super-molecular model is found to be in this order: PN...HF > PN...HCl > PN...HBr in the series examined. Analysis of various physically meaningful contributions arising from the Kitaura-Morokuma (KM) and reduced variational space self-consistent-field (RVS-SCF) energy decomposition procedures shows that the electrostatic energy has significant contribution to the over-all interaction energy. Dipole moment enhancement (Delta mu) was observed in these complexes expected of predominant dipole-dipole electrostatic interaction and was found to follow the trend PN...HF > PN...HCl > PN...HBr at the CCSD level. However, the DFT (X3LYP and B3LYP) and MP2 levels less accurately determined these values (in this order HF < HCl < HBr). Examination of the harmonic vibrational modes reveals that the PN and HX bands exhibit characteristic blue- and red shifts with concomitant bond contraction and elongation, respectively, on hydrogen bond formation. The topological or critical point (CP) analysis using the static quantum theory of atoms in molecules (QTAIM) of Bader was considered to classify and to gain further insight into the nature of interaction existing in the monomers PN and HX, and between them on H-bond formation. It is found from the analysis of the electron density rho ( c ), the Laplacian of electron charge density nabla(2)rho(c), and the total energy density (H ( c )) at the critical points between the interatomic regions that the interaction N...H is indeed electrostatic in origin (rho(c) > 0, nabla(2)rho(c) > 0 and H(c) > 0 at the BCP) whilst the bonds in PN (rho(c) > 0, nabla(2)rho(c) > 0 and H(c) < 0) and HX ((rho(c) > 0, nabla(2)rho(c) < 0 and H(c) < 0)) are predominantly covalent. A natural bond orbital (NBO) analysis of the second order perturbation energy lowering, E((2)), caused by charge transfer mechanism shows that the interaction N...H is n(N) --> BD*(HX) delocalization.
采用自旋限制密度泛函理论(X3LYP 和 B3LYP)和从头算(MP2(fc) 和 CCSD(fc))方法,结合 Aug-CC-pVDZ 和 Aug-CC-pVTZ 基组,对一系列氢键复合物 PN...HX(X = F、Cl、Br)进行了计算,以研究它们在电子基态下平衡气相结构、能量稳定性、电子性质和振动特性的变化。在所有情况下,复合物均被预测相对于组成单体是稳定的。使用超分子模型计算的相互作用能(Delta E)按以下顺序排列:在研究的系列中,PN...HF > PN...HCl > PN...HBr。对源于 Kitaura-Morokuma(KM)和简化变分空间自洽场(RVS-SCF)能量分解程序的各种具有物理意义的贡献的分析表明,静电能对整体相互作用能有显著贡献。在这些复合物中观察到偶极矩增强(Delta mu),这是主要的偶极-偶极静电相互作用的预期结果,并且在 CCSD 水平下遵循 PN...HF > PN...HCl > PN...HBr 的趋势。然而,DFT(X3LYP 和 B3LYP)和 MP2 水平不太准确地确定了这些值(HF < HCl < HBr)。对谐振振动模式的研究表明,在氢键形成时,PN 和 HX 带分别表现出特征的蓝移和红移,同时伴随着键的收缩和伸长。采用 Bader 的原子在分子中的静态量子理论(QTAIM)对拓扑或临界点(CP)进行分析,以对单体 PN 和 HX 之间以及它们在氢键形成时的相互作用进行分类和进一步深入了解。通过分析原子间区域的电子密度 rho(c)、电子电荷密度的拉普拉斯算子 nabla(2)rho(c)和总能量密度(H(c)),发现 N...H 相互作用确实是静电起源的(在 BCP 处 rho(c) > 0,nabla(2)rho(c) > 0 和 H(c) > 0),而 PN(rho(c) > 0,nabla(2)rho(c) > 0 和 H(c) < 0)和 HX((rho(c) > 0,nabla(2)rho(c) < 0 和 H(c) < 0)中的键主要是共价的。通过电荷转移机制引起的二阶微扰能降低 E((2))的自然键轨道(NBO)分析表明,N...H 相互作用是 n(N) --> BD*(HX) 离域。