Shu Zheng, Liu Mingqing, Hu Shilin, Chen Jing
Opt Express. 2020 Apr 13;28(8):11165-11174. doi: 10.1364/OE.390564.
We have performed a comparison study of the Rydberg-state excitation of model molecules (1π and 1π states) in different laser fields by the approaches of time-dependent Schrödinger equation and a fully quantum-mechanical model, and both simulations show good accordance. It is found that the peak structure of the Rydberg-state population vs laser intensity becomes pronounced for longer laser pulses due to the stronger interference effect between the subwave packets released in different optical cycles, and the locations of the intensity-dependent peaks closely satisfy the multi-photon resonant transition condition. In addition, it is demonstrated that the populations of the Rydberg states possessing the identical parity oscillate in an inverse manner with increasing laser intensity for different initial states (1π and 1π), and the aforementioned distinct phenomenon is attributed to the additional phase introduced by the symmetry of 1π state with respect to that of 1π state.
我们通过含时薛定谔方程方法和全量子力学模型,对不同激光场中模型分子(1π和1π态)的里德堡态激发进行了比较研究,两种模拟结果吻合良好。研究发现,由于不同光学周期中释放的子波包之间更强的干涉效应,对于更长的激光脉冲,里德堡态布居数与激光强度关系的峰值结构变得更加明显,且强度依赖峰的位置紧密满足多光子共振跃迁条件。此外,研究表明,对于不同的初始态(1π和1π),具有相同宇称的里德堡态布居数随激光强度增加呈相反方式振荡,上述独特现象归因于1π态相对于1π态的对称性引入的附加相位。