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Topological Effects in Vibronically Coupled DegenerateElectronic States: A Case Study on Nitrate and Benzene Radical Cation

机译:振动耦合简并的拓扑效应电子态:以硝酸根和苯自由基为例

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摘要

We carry out detailed investigation for topological effects of two molecular systems, NO3 radical and C6H6+ (Bz+) radical cation, where the dressed adiabatic, dressed diabatic, and adiabatic-via-dressed diabatic potential energy curves (PECs) are generated employing ab initio calculated adiabatic and diabatic potential energy surfaces (PESs). We have implemented beyond Born–Oppenheimer (BBO) theory for constructing smooth, single-valued, and continuous diabatic PESs for five coupled electronic states [J. Phys. Chem. A>2017,121, 6314–6326]. In the case of NO3 radical, the nonadiabatic coupling terms (NACTs) among the low-lying five electronic states, namely, X̃2A2 (12B2), A~2E″ (12A2 and 12B1), and B~2E′ (12A1 and 22B2), bear the signature of Jahn–Teller (JT) interactions, pseudo JT (PJT) interactions, and accidental conical intersections (CIs). Similarly, Bz+ radical cation also exhibits JT, PJT, and accidental CIs in the interested domain of nuclear configuration space. In order to generate dressed PECs, two components of degenerate in-plane asymmetric stretching modes are selectivelychosen for both the molecular species (Q3x–Q3y pair for NO3 radical and Q16x–Q16y pair for Bz+ radical cation). The JTcoupling between the electronic states is essentially originated throughthe asymmetric stretching normal mode pair, where the coupling elementsexhibit symmetric and nonlinear functional behavior along Q3x and Q16x normal modes.
机译:我们对两个分子系统NO3自由基和C6H6 + (Bz + )自由基阳离子的拓扑效应进行了详细的研究,其中,穿好绝热,穿好绝热和绝热-使用从头算出的绝热和绝热势能面(PES)生成通孔拟合的绝热势能曲线(PEC)。我们已经超越了Born–Oppenheimer(BBO)理论,为五个耦合电子态构建平滑,单值和连续的非绝热PES [J.物理化学A > 2017年, 121,6314-6326]。在NO3自由基的情况下,低位五个电子状态之间的非绝热耦合项(NACT),即 X ̃ 2 A2 '(1 2 B2),A〜 2 E''(1 2 A2和1 2 B1)和B〜 2 E'(1 2 A1和2 2 B2)具有Jahn-Teller(JT)交互,伪JT(PJT)交互和意外圆锥形交叉(CI)的签名。同样,Bz + 自由基阳离子在核构型空间的感兴趣域中也显示出JT,PJT和偶然的CI。为了生成修饰的PEC,退化的面内非对称拉伸模式的两个分量被选择性地选择选择两种分子种类(NO3自由基的Q3x–Q3y对和Bz + 自由基阳离子的Q16x–Q16y对)。日本电信电子状态之间的耦合本质上是通过非对称拉伸正模对,其中耦合元素沿Q3x和Q 16 x 正常模式呈现对称和非线性功能行为。

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