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Autoionization distribution of atomic high doubly excited states: A 'breathing spheres' approach

机译:原子高双激发态的自电离分布:“呼吸球”方法

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By means of a time-dependent method, we have calculated final ionic state distributions after the decay of laser-prepared atomic high doubly excited, mutually penetrating NLnl states. The calculation is simplified by using two nondispersive radial wave-packet wave functions with the initial condition [r(1)](NL)< [r(2)](nl) at (t = 0). Two decay processes have been investigated. The first is the autoionization of high doubly excited states (DES) with N less than or equal to n. Within our model it is described by two electrons moving like two "breathing" charge clouds exchanging energy until one of them escapes. The second decay process is the photoionization of the inner electron (N greater than or equal to 2n including E(N)less than or equal to 0), which leaves the final ion in a high Rydberg state. Our results are compared with data from experiments, in which DES an laser-prepared using isolated core excitation. [S1050-2947(99)00404-7]. [References: 25]
机译:通过与时间有关的方法,我们已经计算出在激光制备的原子高双激发,互穿的NLnl态衰变之后的最终离子态分布。通过使用两个初始时间为[r(1)](NL)<[r(2)](nl)(t = 0)的非分散径向波包波函数简化了计算。已经研究了两种衰减过程。第一个是N小于或等于n的高双激发态(DES)的自电离。在我们的模型中,两个电子像两个“呼吸”的电荷云一样交换能量,直到其中一个逸出,从而描述了这种情况。第二个衰减过程是内部电子的光电离(N大于或等于2n,包括E(N)小于或等于0),使最终离子处于高Rydberg态。我们的结果与实验数据进行了比较,在实验中,DES是使用隔离的磁芯激发制备的激光。 [S1050-2947(99)00404-7]。 [参考:25]

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