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Analytical potential energy function for the electronic states 2^∏1/2 and 2^∏3/2 of O^x2 (x=+1, -1)
引用本文:吕 兵,令狐荣锋,周 勋,杨向东,朱正和,程新路.Analytical potential energy function for the electronic states 2^∏1/2 and 2^∏3/2 of O^x2 (x=+1, -1)[J].中国物理 B,2008,17(5):1738-1742.
作者姓名:吕 兵  令狐荣锋  周 勋  杨向东  朱正和  程新路
作者单位:School of Sciences, Guizhou Normal University, Guiyang 550001, China;Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China;School of Sciences, Guizhou Normal University, Guiyang 550001, China;School of Sciences, Guizhou Normal University, Guiyang 550001, China;Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China;Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China;Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China
基金项目:Project supported by the National Natural Science Foundation of China (Grant Nos 10574096 and 10676025), the Specialized Research Fund for the Doctoral Program of Higher Education of China (Grant No 20050610010), and the Scientific Research Foundation of
摘    要:The splitting of potential energy levels for ground state X^2∏g of O^x2 (x = +1,-1) under spin-orbit coupling (SOC) has been calculated by using the spin-orbit (SO) multi-configuration quasi-degenerate perturbation theory (SO-MCQDPT). Their Murrell-Sorbie (M S) potential functions are gained, and then the spectroscopic constants for electronic states 2^∏1/2 and 2^∏3/2 are derived from the M S function. The vertical excitation energies for O^x2 (x = +1,-1) are vO2+1^(2∏3/2→X^2∏1/2)] =195.652cm^-1, and vO2^-1(2^∏1/2 →X^2∏3/2)] =182.568cm^-1, respectively. All the spectroscopic data for electronic states 2^∏1/2 and 2^∏3/2 are given for the first time.

关 键 词:分子结构  势能函数  自旋轨道耦合  电子态
收稿时间:2007-05-31

Analytical potential energy function for the electronic states 2П1/2 and 2П3/2 of O2x(x=+1, --1)
Lü Bing,Linghu Rong-Feng,Zhou Xun,Yang Xiang-Dong,Zhu Zheng-He,Cheng Xin-Lu.Analytical potential energy function for the electronic states 2П1/2 and 2П3/2 of O2x(x=+1, --1)[J].Chinese Physics B,2008,17(5):1738-1742.
Authors:Lü Bing  Linghu Rong-Feng  Zhou Xun  Yang Xiang-Dong  Zhu Zheng-He  Cheng Xin-Lu
Institution:Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China; School of Sciences, Guizhou Normal University, Guiyang 550001, China; School of Sciences, Guizhou Normal University, Guiyang 550001, China;Institute of Atomic and Molecular Physics, Sichuan University, Chengdu 610065, China
Abstract:The splitting of potential energy levels for ground state X2πg of O2x(x=+1, -1) under spin--orbit coupling (SOC) has been calculated by using the spin--orbit (SO) multi-configuration quasi-degenerate perturbation theory (SO-MCQDPT). Their Murrell--Sorbie (M--S) potential functions are gained, and then the spectroscopic constants for electronic states 2π1/2 and 2π3/2 are derived from the M--S function. The vertical excitation energies for O2x(x=+1, -1) are \nu O2+1 (2π3/2→ X2π1/2)]=195.652cm-1, and \nu O2-1(2π1/2 →X2π3/2 )]=182.568cm-1, respectively. All the spectroscopic data for electronic states 2π1/2 and 2π3/2 are given for the first time.
Keywords:O2x(x=+1  -1)  molecular structure and potential function  Murrell--Sorbie function  spin--orbit coupling
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