原子在强磁场中的能谱特征

SPECTRUM CHARACTERISTICS OF AN ATOM IN A STRONG MAGNETIC FIELD

本文使用一种微扰法计算强磁场中的Na原子(m=-2,z宇称π=+)在强场混合区的能级位置和振子强度。理论能谱的一些特征可以较好地描述一些实验能谱的特征。对得到的能谱所做的傅里叶变换分析表明,除了传统的准朗道共振外(在零场电离阈附近间距近似为1.5ω_c,ω_c为电子迴旋频率),还存在有一系列大小与磁场强度无关的“共振”间距,与其他理论所给出的相一致,还从所用微扰法中的零级能量公式出发,对这些间距给予量子力学解释。

A perturbation method is used to evaluate the energy levels and oscillator strengths of sodium atoms (m=-2,π2=+)in a strong magnetic field. The main features of the calculated spectra which lie in the strong-field-mixing regime agree well with the corresponding experimental results. Besides the conventional quasi-Landau resonance with spacing equal to 1.5 ωc (ωc is the electron cyclotron frequency) near the zero field ionization limit, a series of resonance spacings are found and analysed using the zero order energy formula and the Fourier transform technique. The values of these spacings are in consistent with other theoretical results. Based on the perturbation method, a quantum mechanical explanation for the spacings is given. These resonance spacings are independent of the applied exernal magnetic field.