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High resolution vacuum ultraviolet pulsed field ionization photoelectron band for OCS+(X-2 Pi): An experimental and theoretical study

机译:用于OCS +(X-2 Pi)的高分辨率真空紫外脉冲场电离光电子能带:实验和理论研究

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摘要

The vacuum ultraviolet pulsed field ionization photoelectron (PFI-PE) band for OCS+(X (2) Pi) in the energy region of 11.09-11.87 eV has been measured using high resolution monochromatized synchrotron radiation, The ionization energies (IEs) for the formation of the (0,0,0) X (2) Pi(3/2) and (0,0,0) (2) Pi(1/2) states of OCS+ are determined to be 11.1831+/-0.0005 and 11.2286+/-0.0005 eV, respectively, yielding a value of 367+/-1.2 cm(-1) for the spin-orbit splitting. Using the internally contracted multireference configuration interaction approach, three-dimensional potential energy functions (PEFs) for the OCS+(X (2) Pi) state have been generated and used in the variational Renner-Teller calculations of the vibronic states. The energies of all vibronic states (J=P) for J=1/2, 3/2, 5/2, and 7/2 have been computed in the energy range of approximate to 4000 cm(-1) above the IE[OCS+(X (2) Pi(3/2))] for the assignment of the experimental spectrum. By a minor modification of the nb initio PEFs, good correlations are found between the experimental and theoretical Renner-Teller structures. Similar to the PFI-PE bands for CO2+(X (2) Pi(g)) and CS2+(X (2) Pi(g)), weak transitions have been detected in the PFI-PE band for OCS+(X (2) Pi), which are forbidden in the Franck-Condon approximation. The nonvanishing single-photon ionization cross sections involving the excitation of the bending vibrational modes of OCS+, CO2+, and CS2+, in their ground electronic states are attributed to the symmetries of the geometry-dependent electronic transition dipole operator components. (C) 1998 American Institute of Physics. [S0021-9606(98)00415-2]. [References: 46]
机译:使用高分辨率的单色同步加速器辐射测量了能量域为11.09-11.87 eV的OCS +(X(2)Pi)的真空紫外脉冲场电离光电子(PFI-PE)谱带,用于形成的电离能(IEs)确定OCS +的(0,0,0)X(2)Pi(3/2)和(0,0,0)(2)Pi(1/2)的状态分别为11.1831 +/- 0.0005和11.2286 +/- 0.0005 eV,分别为自旋轨道分裂产生367 +/- 1.2 cm(-1)的值。使用内部收缩的多参考配置交互方法,已经生成了OCS +(X(2)Pi)状态的三维势能函数(PEF),并将其用于振动态的Renner-Teller变分计算。对于J = 1 / 2、3 / 2、5 / 2和7/2的所有振动状态(J = P)的能量已经在IE []上方大约4000 cm(-1)的能量范围内进行了计算。 OCS +(X(2)Pi(3/2))]用于分配实验光谱。通过对nb起始PEF的较小修改,可以在实验和理论的Renner-Teller结构之间找到良好的相关性。与CO2 +(X(2)Pi(g))和CS2 +(X(2)Pi(g))的PFI-PE谱带相似,在OCS +(X(2))的PFI-PE谱带中检测到弱过渡Pi),这在Franck-Condon近似中是禁止的。在其基态电子状态下,涉及OCS +,CO2 +和CS2 +的弯曲振动模式激发的不消失的单光子电离截面归因于与几何相关的电子跃迁偶极子算符的对称性。 (C)1998美国物理研究所。 [S0021-9606(98)00415-2]。 [参考:46]

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