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Laser Control of Photodissociation Process in Diatomic Molecule

机译:双原子分子光解离过程的激光控制

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In this work, we first aim to realize the complete laser-induced photodissociation of the OH molecule, and then intend to control the wavepacket generated on the continuum state, i.e., to achieve the laser control of the above-threshold dissociation (ATD) spectrum. To numerically solve the Schrodinger equation, we adopt the split operator method (SOM), which conserves the norm of the state vector, and can treat both discrete and continuum states simultaneously and correctly. This photodissociation process induced by the multiphoton absorption involves the ATD spectrum due to the continuum-continuum transition by the intense electric field. First, we investigate the detailed mechanism of the complete photodissociation with the one-color laser pulse by changing the laser parameters. Then, we investigate the control of the ATD spectrum by using the two-color laser field, where we focus on the role of the relative phase and position of two laser pulses. To analyze the population of both discrete and continuum states involved in the resultant wavepacket, we show the effective method by means of the quasicontinuum state on the Morse potential obtained by numerically diagonalizing the Fourier grid Hamiltonian (FGH.).
机译:在这项工作中,我们首先旨在实现OH分子的完全激光诱导的光解离,然后打算控制在连续状态下生成的波包,即实现上述阈值解离(ATD)光谱的激光控制。为了对Schrodinger方程进行数值求解,我们采用了分裂算子方法(SOM),它保留了状态向量的范数,并且可以同时正确地处理离散状态和连续状态。多光子吸收引起的这种光解离过程涉及ATD光谱,这是由于强电场引起的连续-连续跃迁。首先,我们通过改变激光参数来研究与单色激光脉冲完全光解离的详细机理。然后,我们研究了使用双色激光场对ATD光谱的控制,我们重点研究了两个激光脉冲的相对相位和位置的作用。为了分析结果波包中涉及的离散态和连续态的总体,我们通过对傅里叶网格哈密顿量(FGH。)进行对角线化获得的莫尔斯电势,通过准连续谱态展示了一种有效的方法。

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