Komasa Jacek
Faculty of Chemistry, A. Mickiewicz University, Grunwaldzka 6, 60-780, Poznań, Poland.
Phys Chem Chem Phys. 2008 Jun 21;10(23):3383-9. doi: 10.1039/b803548b. Epub 2008 May 8.
A class of doubly excited electronic states of the hydrogen molecule is reported. The states are of Sigma(-) symmetry and are located ca. 200,000 cm(-1) above the ground state and about 75,000 cm(-1) above the ionization threshold. The electronic wave functions employed to described these states have been expanded in the basis of exponentially correlated Gaussian (ECG) functions with the nonlinear parameters variationally optimized. The lowest (3)Sigma and (1)Sigma states dissociate into hydrogen atoms in the n = 2 state, whereas the lowest (3)Sigma and (1)Sigma states have H(n = 2) and H(n = 3) as the dissociation products. All the four states are attractive and accommodate vibrational levels. The location of the vibrational energy levels has been determined by solving the radial Schrödinger equation within the Born-Oppenheimer approximation.
报道了一类氢分子的双激发电子态。这些态具有Σ(-)对称性,位于基态上方约200,000厘米⁻¹处,且在电离阈值上方约75,000厘米⁻¹处。用于描述这些态的电子波函数已在指数相关高斯(ECG)函数的基础上展开,其非线性参数通过变分法进行了优化。最低的(3)Σ和(1)Σ态解离为处于n = 2态的氢原子,而最低的(3)Σ和(1)Σ态以H(n = 2)和H(n = 3)作为解离产物。所有这四个态都是吸引性的且容纳振动能级。振动能级的位置已通过在玻恩 - 奥本海默近似下求解径向薛定谔方程来确定。