摘要
本文依据多通道量子亏损理论对Ar原子J=0的高激发态结构进行了理论分析,确定了基本结构参量,得到Lu-Fano图和全部分立态能位、通道混合系数,预言了自电离共振结构。
According to the multichannel quantum defect theory (MQDT), we were engaged in the theoretical analysis for the J=0 even-parity and odd-parity states of the argon atom. For two Rydberg series3p^5 (2p_3/2~0)np,3p^5(2P_1/2~0)np anp 3p^5(2P_3/2~0)nd, 3p^5(2P_1/2~0)ns, we have determined the MQDT parameters by fitting the experimental energy level data and the experimental value of oscillator stregth in the discrete states. With these parameters as input, according to the basic equation of MQDT, we have obtained the Lu-Fano plots, the energy levels of all discrete states and the mixing coefficients of the channels, and predicted the autoionization resonance structure.
出处
《吉林大学自然科学学报》
CSCD
1991年第4期62-66,共5页
Acta Scientiarum Naturalium Universitatis Jilinensis
基金
国家教育委员会博士点基金
关键词
氩原子
高激发态
MQDT
自电离共振
Ar atom, highly excited states, multichannel quantum defect theory