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首页> 外文期刊>Chemical Physics: A Journal Devoted to Experimental and Theoretical Research Involving Problems of Both a Chemical and Physical Nature >New propagator schemes for explicitly time-dependent hamiltonians: applications to the multiphoton dissociation dynamics of diatoms and quantum adiabatic processes
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New propagator schemes for explicitly time-dependent hamiltonians: applications to the multiphoton dissociation dynamics of diatoms and quantum adiabatic processes

机译:用于显着时间相关的哈密尔顿的新的传播器方案:在硅藻和量子绝热过程的多光子解离动力学中的应用

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摘要

Three different algorithms are proposed for studying the evolution of explicitly time-dependent Hamiltonians. In one case the propagator is constructed by making use of the Floquet states while in the other two cases, a split-operator based technique is used. Model applications to the problem of dissociation of diatoms in strong laser fields prove encouraging and our numerical experiments show that the threshold intensity of the laser field has unique relationship with the curvature of the potential of the dissociating diatoms. Adiabatically switched time-dependent split-operator based scheme is tested. This method encounters no difficulty even in the presence of tunneling or level crossings and can tackle fairly large changes or distortions in the Hamiltonian. All the eigenstates of the perturbed Hamiltonian at t = τ (large) are obtained from the corresponding eigenstates of the unperturbed Hamiltonian at t = 0 as the limit of continuous succession of eigenstates of the slowly changing H(t). The viability of this method is analysed with particular reference to the adiabatic passage of eigenstates of a harmonic oscillator to the appropriate eigenstates of a symmetric double well Hamiltonian.
机译:提出了三种不同的算法来研究显式时间相关的哈密顿量的演化。在一种情况下,传播器是通过使用Floquet状态构造的,而在其他两种情况下,则使用基于拆分运算符的技术。在强激光场中硅藻解离问题的模型应用证明是令人鼓舞的,我们的数值实验表明,激光场的阈值强度与离解硅藻的电势曲率具有独特的关系。测试了基于绝热切换的与时间有关的分裂算子的方案。即使存在隧道或平交道口,该方法也不会遇到任何困难,并且可以解决哈密顿量中相当大的变化或变形。从t = 0时未扰动的哈密顿量的相应本征态获得t =τ(大)处的扰动哈密顿量的所有本征态,作为缓慢变化的H(t)本征态连续连续的极限。分析该方法的可行性,尤其要参考谐波振荡器的本征态绝热传递到对称双阱哈密顿量的适当本征态。

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