Xi Hong-Wei, Huang Ming-Bao, Chen Bo-Zhen, Li Wen-Zuo
College of Chemistry and Chemical Engineering, Graduate School, Chinese Academy of Sciences, P.O. Box 4588, Beijing 100049, People's Republic of China.
J Phys Chem A. 2005 Oct 13;109(40):9149-55. doi: 10.1021/jp0524835.
Complete active space self-consistent field (CASSCF) and multiconfiguration second-order perturbation theory (CASPT2) calculations with an atomic natural orbital basis were performed for the 1(2)A'', 1(2)A', 2(2)A', 2(2)A'', and 3(2)A' (X2E, A2A1, and B2E) states of the CH3F+ ion. The 1(2)A'' state is predicted to be the ground state, and the C(s)-state energy levels are different from those of the CH3Cl+ ion. The 2(2)A' (A2A1) state is predicted to be repulsive, and the calculated adiabatic excitation energies for 2(2)A'' and 3(2)A' are very close to the experimental value for the B state. The CASPT2//CASSCF potential energy curves (PECs) were calculated for F-loss dissociation from the five C(s) states and H-loss dissociation from the 1(2)A'', 1(2)A', and 2(2)A'' states. The electronic states of the CH3+ and CH2F+ ions as the dissociation products were carefully determined by checking the energies and geometries of the asymptote products, and appearance potentials for the two ions in different states are predicted. The F-loss PEC calculations for CH3F+ indicate that F-loss dissociation occurs from the 1(2)A'', 1(2)A', and 2(2)A' states [all correlating with CH3+(X1A1')], which supports the experimental observations of direct dissociation from the X and A states, and that direct F-loss dissociation can occur from the two Jahn-Teller component states of B2E, 2(2)A'' and 3(2)A' [correlating with CH3+(1(3)A'') and CH3+(1(3)A'), respectively]. Some aspects of the 3(2)A' Cl-loss PEC of the CH3Cl+ ion are inferred on the basis of the calculation results for CH3F+. The H-loss PEC calculations for CH3F+ indicate that H-loss dissociation occurs from the 1(2)A'', 1(2)A', and 2(2)A'' states [correlating with CH2F+(1(3)A''), CH2F+(X1A1), and CH2F+(1(1)A''), respectively], which supports the observations of direct dissociation from the X and B states. As the 2(2)A' H-loss PEC of CH3Cl+, the 2(2)A' H-loss PEC of CH3F+ does not lead to H + CH2X+, but the PECs of the two ions represent different types of reactions.
采用原子自然轨道基组,对CH₃F⁺离子的1(²)A″、1(²)A′、2(²)A′、2(²)A″和3(²)A′(X²E、A²A₁和B²E)态进行了完全活性空间自洽场(CASSCF)和多组态二阶微扰理论(CASPT2)计算。预测1(²)A″态为基态,且C(s)态的能级与CH₃Cl⁺离子的不同。预测2(²)A′(A²A₁)态具有排斥性,计算得到的2(²)A″和3(²)A′态的绝热激发能与B态的实验值非常接近。计算了从五个C(s)态的F损失解离以及从1(²)A″、1(²)A′和2(²)A″态的H损失解离的CASPT2//CASSCF势能曲线(PEC)。通过检查渐近产物的能量和几何结构,仔细确定了作为解离产物的CH₃⁺和CH₂F⁺离子的电子态,并预测了不同态下两种离子的出现势。CH₃F⁺的F损失PEC计算表明,F损失解离发生在1(²)A″、1(²)A′和2(²)A′态[均与CH₃⁺(X¹A₁′)相关],这支持了从X态和A态直接解离的实验观察结果,并且直接F损失解离可以从B²E的两个Jahn-Teller分量态2(²)A″和3(²)A′发生[分别与CH₃⁺(¹³A″)和CH₃⁺(¹³A′)相关]。基于CH₃F⁺的计算结果,推断了CH₃Cl⁺离子3(²)A′态Cl损失PEC的一些方面。CH₃F⁺的H损失PEC计算表明,H损失解离发生在1(²)A″、1(²)A′和2(²)A″态[分别与CH₂F⁺(¹³A″)、CH₂F⁺(X¹A₁)和CH₂F⁺(¹¹A″)相关],这支持了从X态和B态直接解离的观察结果。与CH₃Cl⁺的2(²)A′态H损失PEC一样,CH₃F⁺的2(²)A′态H损失PEC不会导致H + CH₂X⁺,但两种离子的PEC代表不同类型的反应。