首页> 外文期刊>The Journal of Chemical Physics >Ab initio calculations on low-lying electronic states of TeO_2 and Franck-Condon simulation of the (1)~1B_2 -X~1A_1,TeO_2 absorption spectrum including anharmonicity
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Ab initio calculations on low-lying electronic states of TeO_2 and Franck-Condon simulation of the (1)~1B_2 -X~1A_1,TeO_2 absorption spectrum including anharmonicity

机译:TeO_2的低电子态的从头算计算和(1)〜1B_2 <-X〜1A_1,TeO_2包括非谐性的吸收光谱的Franck-Condon模拟

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Ab initio calculations have been carried out on low-lying singlet and triplet states of TeO_2 at different levels of theory with basis sets of up to the augmented-polarized valence-quintuple-delta quality.Equilibrium geometrical parameters,harmonic vibrational frequencies,and relative electronic energies of the X ~1A_1,~1B_l,~1B_2,~1A_2,~3A_1,~3B_1,~3B_2,and ~3A_2 states of TeO_2 have been calculated.Potential energy functions (PEFs) of the X ~1A_1 and the (1) ~1B_2 states were computed at the complete-active-space self-consistent-field multireference configuration interaction level,with a basis set of augmented-polarized valence-quadruple-delta quality.Franck-Condon factors (FCFs) for the electronic transition between the X~1A_1 and (1)~1B_2 states of TeO_2 were calculated with the above-mentioned ab initio PEFs.The (1)~1B_2<-X ~1A_1 absorption spectrum of TeO_2 was simulated employing the computed FCFs,which include Duschinsky rotation and anharmonicity,and compared with the recently published laser-induced fluorescence (LIF) spectrum of Hullah and Brown [J.Mol.Spectrosc.200,261 (2000)].The ab initio results and spectral simulation reported here confirm the upper electronic state involved in the LIF spectrum to be the (1) ~1B_2 state of TeO_2 and also confirm the vibrational assignments of Hullah and Brown.However,our simulated spectrum suggests that the reported LIF spectrum from 345 to 406 nm represents only a portion of the full (1)~1B_2<- X~1A_1 absorption spectrum of TeO_2,which extends from ca.406 to 300 nm.Another dye other than the two used by Hullah and Brown is required to cover the 345-300 nm region of the LIF band.Ab initio calculations show strong configuration mixing of the (1)~1B_2 electronic surface with higher ~1B_2 states in a region of large TeO bond length (>=2.0 A) and OTeO bond angle (52=135.0~°).
机译:在不同理论水平上对TeO_2的低态单重态和三重态进行了从头算计算,基集最高为增强极化的价-五重体-δ质量。平衡几何参数,谐波振动频率和相对电子计算了TeO_2的X〜1A_1,〜1B_1,〜1B_2,〜1A_2,〜3A_1,〜3B_1,〜3B_2和〜3A_2态的能量.X〜1A_1和(1的势能函数(PEF) )〜1B_2状态是在完全活动空间自洽场多参考配置相互作用水平下计算的,具有增强极化价-四重-增量质量的基础集。弗兰克-康登因子(FCF)用于电子之间的跃迁用上述从头算PEFs计算出TeO_2的X〜1A_1和(1)〜1B_2状态。使用计算出的FCFs模拟TeO_2的(1)〜1B_2 <-X〜1A_1吸收光谱,包括Duschinsky旋转和非谐性,并与最近已发表的Hullah和Brown的激光诱导荧光(LIF)光谱[J.Mol.Spectrosc.200,261(2000)]。从头算的结果和光谱模拟证实,LIF光谱中涉及的上电子态为(1 )处于TeO_2的〜1B_2状态,也证实了Hullah和Brown的振动分配。但是,我们的模拟光谱表明,报告的345至406 nm的LIF光谱仅代表全部(1)〜1B_2 <-X〜1A_1 TeO_2的吸收光谱范围约为406至300 nm。除Hullah和Brown使用的两种染料外,还需要另一种染料覆盖LIF波段的345-300 nm区域。 (1)在TeO键长(> = 2.0 A)和OTeO键角(52 = 135.0〜°)较大的区域中〜1B_2的电子表面具有较高的〜1B_2状态。

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