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Quantum dynamics with Lanczos subspace propagation: Application to a laser-driven molecular system

机译:Lanczos子空间传播的量子动力学:在激光驱动分子系统中的应用

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Two Lanczos subspace propagation techniques are discussed in this work and compared with the Chebyshev method applied to the original Hamiltonian matrix. Both procedures involve the use of a reduced propagator in the Lanczos subspace to calculate the solution to the time-dependent Schrodinger equation but differ in the way the propagator is evaluated. The LSC (Lanczos subspace Chebyshev) expresses the propagator in terms of Chebyshev polynomials that are functions of the tridiagonal Hamiltonian matrix in the Lanczos space. In contrast, the LSV (Lanczos subspace variational) is implemented by solving the eigenproblem in the Lanczos subspace and then performing a variational expansion of the propagator in the M-dimensional eigenvector space. Although the LSV is the same as the reduced propagator scheme proposed by Park and Light, in the present study the LSV is implemented as a one-step long-time propagator. As a numerical example, the interaction of a molecule with a strong laser pulse is investigated. The Hamiltonian is explicitly time dependent in this case, and thus the stationary formalism is employed in this work to solve the time-dependent Schrodinger equation. Application of either the LSC or LSV yields a wave function in the M-dimensional Lanczos subspace. Nonetheless, the transition amplitudes computed from this wave function are in excellent agreement with those calculated by direct application of the Chebyshev method in the original space used to define the Hamiltonian matrix. (C) 1998 John Wiley & Sons, Inc. [References: 25]
机译:本文讨论了两种Lanczos子空间传播技术,并与应用于原始哈密顿矩阵的Chebyshev方法进行了比较。两种方法都涉及在Lanczos子空间中使用简化的传播子来计算与时间相关的Schrodinger方程的解,但是传播子的评估方式有所不同。 LSC(Lanczos子空间Chebyshev)用Chebyshev多项式表示传播子,该多项式是Lanczos空间中三对角哈密顿矩阵的函数。相反,LSV(Lanczos子空间变分)是通过解决Lanczos子空间中的本征问题,然后在M维特征向量空间中执行传播子的变分展开来实现的。尽管LSV与Park and Light提出的简化传播器方案相同,但在本研究中,LSV被实现为一个一步的长时间传播器。作为数值示例,研究了分子与强激光脉冲的相互作用。在这种情况下,哈密顿量显着地与时间有关,因此在该工作中采用平稳形式来求解与时间有关的薛定inger方程。 LSC或LSV的应用都会在M维Lanczos子空间中产生波动函数。但是,从该波函数计算出的跃迁幅度与在定义哈密顿矩阵的原始空间中直接应用切比雪夫方法计算出的跃迁幅度非常吻合。 (C)1998 John Wiley&Sons,Inc. [参考:25]

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