共查询到15条相似文献，搜索用时 31 毫秒
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采用CASSCF方法和6-311++(3df, 3pd)基组以及Cs对称性优化了乙基硫自由基和阳、阴离子3种分子的12个电子态的几何构型. 利用二级微扰方法(CASPT2)对这12个电子态做了单点能校正. 通过比较自由基与阴阳离子的能量, 得出了绝热电子亲和势和绝热电子电离能, 与实验结果在允许误差范围内基本一致. 相似文献
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采用CASSCF方法和ANO-S基组计算了FONO2分子及其阳离子的低能激发态, 并采用CASPT2方法进行能量校正. 预测了在低能激发态时FONO2分子的几何结构发生了很大变化, 从基态的平面构型转变为空间的几何构型. 然而在阳离子中没有发生相似的几何构型改变. 此外, 在分子的基态几何构型下, 设计并计算了相应阳离子的垂直离子势, 对分子的光电子谱给出了详细的解释. 相似文献
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使用CASSCF方法和ANO-L基组优化了HSO自由基的基态和3个低占据激发态的结构, 并采用包括更多电子动态相关能的CASPT2方法进行了单点能校正. 频率计算结果表明, 优化的4个几何为势能面上的稳定点. 通过电子结构的研究合理地解释了各个激发态相对于电子基态的结构变化. 相似文献
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光化学反应是最基本也是最重要的物理化学过程之一,在诸多领域有着广泛的应用。由于计算方法的限制以及光化学反应过程的错综复杂性,光化学反应机理的从头算研究是极具挑战性的国际前沿课题之一。本文综述了近20年来羰基化合物光化学反应机理从头算研究的一些进展,总结了羰基化合物电子激发态的特性和光化学反应过程的规律性,为深入研究光化学反应提供一些有用的信息。 相似文献
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采用全活化空间自洽场方法(CASSCF)研究了OClO阴离子7个低能电子态及其自由基的基态.为了进一步考虑动态电子相关效应,采用二级多组态微扰理论(CASPT2)获得更加可靠的能量值.此外,在ANO-L基组的基础上,在OClO自由基的电荷中心增加了为研究里德堡态所建立的1s1p1d的波函数,并应用多组态二级微扰理论(MS-CASPT2)方法获得了里德堡态的准确电子激发能. 相似文献
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采用全活化空间自洽场方法(CASSCF)研究了OClO阴离子7个低能电子态及其自由基的基态. 为了进一步考虑动态电子相关效应, 采用二级多组态微扰理论(CASPT2)获得更加可靠的能量值. 此外, 在ANO-L基组的基础上, 在OClO自由基的电荷中心增加了为研究里德堡态所建立的1s1p1d的波函数, 并应用多组态二级微扰理论(MS-CASPT2)方法获得了里德堡态的准确电子激发能. 相似文献
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在C2v对称性下,采用全活化空间自洽场(CASSCF)和多组态二级微扰理论(CASPT2)方法研究氰基铝(AlCN)及其阴阳离子的基态和低能激发态.在ANO-L基组水平下,计算了AlCN及其阴阳离子低能电子态的几何,组态及其相互作用系数,谐振频率,绝热激发能,垂直激发能和振子强度.在CASSCF/CASPT2理论水平下,计算得到AlCN的11Π电子态的绝热激发能为352.4kJ·mol-1,与实验值344.0kJ·mol-1符合得很好.另外,预测AlCN的跃迁X1Σ+→21Π发生在673.1kJ·mol-1.激发能和振子强度的计算为研究AlCN的吸收光谱提供理论指导. 相似文献
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采用CASPT2/CASSCF方法对HO2自由基进行统计算, 优化了三个电子态的稳定点几何构型, 得到详细的频率数据. 利用垂直激发计算确定了3个里德堡态、11个价电子态的电子结构以及在三种理论水平上(CASSCF, SS-CASPT2和MS-CASPT2)的能量信息. 计算中使用了ANO-L和ANO-L+基组, 验证了已知实验数据的同时, 通过与其它理论计算结果的对比, 揭示了应用弥散轨道系数对于该体系激发态研究的重要性. 相似文献
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Wen‐Zuo Li Fang Geng Yu‐Wei Pei Jian‐Bo Cheng Qing‐Zhong Li Bao‐An Gong 《International journal of quantum chemistry》2011,111(15):4373-4377
Some low‐lying states of HAlO+ and HOAl+ cations have been studied using the complete‐active‐space self‐consistent field (CASSCF) and multiconfiguration second‐order perturbation theory (CASPT2) methods with the contracted atomic natural orbital (ANO) basis sets. The geometries of all stationary points along the potential energy surfaces were optimized at the CASSCF/ANO and CASPT2/ANO levels. The ground and the first excited states of HAlO+ are predicted to be X2Π and A2Σ+ states, respectively. It was predicted that the ground state of HOAl+ is X2Σ+ state. The A2Π state of HOAl+ has unique imaginary frequency. A bent local minimum M1 was found along the 12A″ potential energy surface, and the A2Π state of HOAl+ should be the transition state of the isomerization reactions for M1 ? M1. The CASPT2/ANO potential energy curves of isomerization reactions were calculated as a function of HAlO bond angle. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2011 相似文献
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Wen‐Zuo Li Yu‐Wei Pei F.‐F. Geng Jian‐Bo Cheng Qing‐Zhong Li Bao‐An Gong 《International journal of quantum chemistry》2012,112(12):2499-2503
Some low‐lying states of the HAlS+ and HSAl+ cations have been studied for the first time by large‐scale theoretical calculations using three methods: complete active space self‐consistent field (CASSCF), complete active second‐order perturbation theory (CASPT2), and density functional theory Becke's three‐parameter hybrid function with the nonlocal correlation of Lee–Yang–Parr (B3LYP) with the contracted atomic natural orbital (ANO‐L) and cc‐pVTZ basis sets. The geometries of all stationary points along the potential energy surfaces (PESs) were optimized at the CASSCF/ANO‐L and B3LYP/cc‐pVTZ levels. The ground and the first excited states of linear HAlS+ are predicted to be X2Π and A2Σ+ states, respectively. For the linear HSAl+ structure, the first excited state is A2Σ+. The X2Π state of linear HSAl+ is a second‐order saddle point, because it has two imaginary frequencies. Two bent global minima M1 and M2 were found along the 12A′ and 12A″ PESs, respectively. The CASPT2/ANO‐L potential energy curves of isomerization reactions were calculated as a function of HAlS bond angle. According to our calculations, the ground‐state HAlS+ is linear, whereas the ground‐state HSAl+ is bent. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2011 相似文献
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Wen‐Zuo Li Jian‐Bo Cheng Qing‐Zhong Li Bao‐An Gong Jia‐Zhong Sun 《International journal of quantum chemistry》2010,110(14):2683-2688
Geometries, frequencies, and energies of the 12B1, 12A2, 12B2, 22B1, 22B2, and 12A1, of the C6H5Br+ ion were calculated by using CASSCF and CASPT2 methods in conjunction with an ANO‐RCC basis. The CASPT2//CASSCF adiabatic excitation energies and CASPT2 relative energies for the six states are in good agreement with experiment. The X, A, B, C, and D electronic states of the C6H5Br+ ion were assigned to be X2B1, A2A2, B2B2, C2B1, and D2B2 based on the CASSCF and CASPT2 calculations. The assignment on the D state of the C6H5Br+ ion is different from the previously published works. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010 相似文献
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Wen‐Zuo Li Jian‐Bo Cheng Qing‐Zhong Li Bao‐An Gong Jia‐Zhong Sun 《Journal of computational chemistry》2010,31(7):1397-1401
The HBO+ and HOB+ cations have been reinvestigated using the CASSCF and CASPT2 methods in conjunction with the contracted atomic natural orbital (ANO) basis sets. The geometries of all stationary points in the potential energy surfaces were optimized at the CASSCF/ANO and CASPT2/ANO levels. The ground and the first excited states of HBO+ are predicted to be X2Π and A2Σ+ states, respectively. It was predicted that the ground state of HOB+ is X2Σ+ state. The A2Π state of HOB+ has unique imaginary frequency. A bending local minimum M1 was found for the first time along the 12A′′ potential energy surface and the A2Π state of HOB+ should be the transition state of the isomerization reactions for M1? M1. The CASPT2/ANO potential energy curves (PECs) of isomerization reactions were calculated as functions of the HBO bond angle. Many of the CASSCF and CASPT2 calculated results were different from the previously published QCISD(T) results. © 2009 Wiley Periodicals, Inc. J Comput Chem, 2010 相似文献
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The ground state (S0) geometry of the firefly luciferin (LH2) was optimized by both DFT B3LYP and CASSCF methods. The vertical excitation energies (Tv) of three low-lying states (S1, S2, and S3) were calculated by TD-DFT B3LYP//CASSCF method. The S1 geometry was optimized by CASSCF method. Its Tv and the transition energy (Te) were calculated by MS-CASPT2//CASSCF method. Both the TD-DFT and MS-CASPT2 calculated S1 state Tv values agree with the experimental one. The IPEA shift greatly affects the MS-CASPT2 calculated Tv values. Some important excited states of LH2 and oxyluciferin (oxyLH2) are charge-transfer states and have more than one dominant configuration, so for deeply researching the firefly bioluminescence, the multireference calculations are desired. 相似文献