核电子耦合的经典和半经典计算

D. W. Noid, F. Hartmann, M. Koszykowski
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引用次数: 0

摘要

制造伽马射线激光器的一个方面涉及储存在长寿命核异构体中的能量的快速释放。一种被提议的释放这种能量的方法是将同分异构体泵送到附近一个寿命较短的核激发态。这种激发态随后衰减为激光跃迁。本文用经典动力学方法考虑了核子和电子运动的动力学耦合,并计算了谱上的摄动。在我们的模型中,一个价态激发的质子作为一个独立的粒子利用伍兹-撒克逊势束缚在原子核上。电子被库仑势束缚在质子核和价质子核上。选择经典轨迹的初始条件为可分离哈密顿量的半经典状态。然后利用从经典轨迹中提取光谱信息的方法2来计算跃迁强度和频率。对于某些异构体,观察到非常强的耦合和混沌运动。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Classical and semiclassical calculation of nuclear-electron coupling
One aspect of making a gamma-ray laser concerns the rapid re lease of energy stored in a long-lived nuclear isomer. A proposed method for the release of this energy is to pump the isomerto a nearby, shorter-lived nuclear excited state. This excited state subsequently decays to a lasing transition. In this paper, we consider the dynamical coupling of the nucleon and electron motion using classical dynamics and calculate the perturbation on the spectra. In our model,1 a valence excited proton is bound as an independent particle to the nuclear core using a Woods-Saxon potential. The electron is bound to a core of protons and the valence proton by a Coulomb potential. Initial conditions for the classical trajectories were chosen to be semiclassical states of the separable Hamiltonian. A method2 to extract spectral information from classical trajectories is then used to calculate both transition intensities and frequencies. For some isomers, very strong coupling and chaotic motion were observed.
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