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Resonances and chaos in the collinear collision system (He, H_2~+) and its isotopic variants

机译:共线碰撞系统(He,H_2〜+)及其同位素变体中的共振和混沌

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The collinear atom-diatom collision system provides one of the simplest instances of chaotic or irregular scattering. Classically, irregular scattering is manifest in the sensitive dependence of post-collision variables on initial conditions, and quantally, in the appearance of a dense spectrum of dynamical resonances. We examine the influence of kinematic factors on such dynamical resonances in collinear (He, H_2~+) collisions by computing the transition state spectra for collinear (He,HD~+) and (He, DH~+) collisions using the time-dependent quantum mechanical approach. The nearest neighbor spacing distribution P(s) and the spectral rigidity Δ_3(L) for these resonances suggest that the dynamics is predominantly irregular for collinear (He,HD~+) and predominantly regular for collinear (He, DH~+). These findings are reinforced by a significantly larger "correlation hole" in ensemble averaged survival probability < < P(t) > > values for collinear (He, HD~+) than for collinear (He,DH~+). In addition we have also examined measures of classical chaos through the dependence of the final vibrational action, n_f, on the initial vibrational phase φ_i of the diatom, and Poincare surfaces-of-section. They show that (He, HD~+) collisions are partly chaotic over the entire energy range (0-2.78 eV) while (He, DH~+) collisions, in contrast, are highly regular at collision energies below the classical threshold for reaction. Above the threshold, the scattering remains regular for initial vibrational states v = 0 and 1 of DH~+.
机译:共线原子-硅藻碰撞系统提供了混沌或不规则散射的最简单实例之一。传统上,不规则散射表现为碰撞后变量对初始条件的敏感依赖性,而定量地表现为密集的动态共振谱。通过使用时间相关性计算共线(He,HD〜+)和(He,DH〜+)碰撞的跃迁状态谱,我们研究了运动因素对共线(He,H_2〜+)碰撞中这种动态共振的影响量子力学方法。这些共振的最近邻居间距分布P(s)和光谱刚度Δ_3(L)表明,对于共线(He,HD〜+),动力学主要是不规则的;对于共线(He,DH〜+),动力学主要是规则的。共线(He,HD〜+)的集合平均生存概率P(t)值比共线(He,DH〜+)显着更大的“相关孔”加强了这些发现。此外,我们还通过最终振动作用n_f依赖于硅藻的初始振动相位φ_i和Poincare截面表面来研究经典混沌的度量。他们显示(He,HD〜+)碰撞在整个能量范围(0-2.78 eV)内部分混乱,而(He,DH〜+)碰撞则在碰撞能量低于经典反应阈值时高度规则。在阈值以上,对于DH〜+的初始振动状态v = 0和1,散射保持规则。

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