首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Kinetic-energy-angle differential distribution of photofragments in multiphoton above-threshold dissociation of D-2(+) by linearly polarized 400-nm intense laser fields: Effects of highly excited electronic states
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Kinetic-energy-angle differential distribution of photofragments in multiphoton above-threshold dissociation of D-2(+) by linearly polarized 400-nm intense laser fields: Effects of highly excited electronic states

机译:线性偏振400 nm强激光场对D-2(+)的多光子阈值以上解离的光碎片的动能角微分分布:高激发电子态的影响

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摘要

We have performed a detailed calculation of the double-differential angular-kinetic-energy distribution of photofragments in above threshold dissociation (ATD) of D-2(+) from initial vibrational-rotational levels v(i)=4,5 and J(i)=0,1 in an intense linearly polarized laser field of wavelength 400 nm and intensity 3x10(13) W/cm(2). The calculation used a time-independent close-coupling (CC) formalism with eight (ten) electronic states included in the basis-set expansion of the molecular wave function. The molecular electronic states included, apart from the two lowest 1s sigma(g) and 2p sigma(u) states, were 2p pi(+/-)(u), 2s sigma(g), 3p sigma(u), 3d sigma(g), 3d pi(+/-)(g), and 4f sigma(u). All the higher electronic states dissociate to the atomic state D(2l). A sufficient number of photon absorption channels, n=0-7, and molecular rotational quantum numbers J=0-11 were taken into account to ensure the convergence of the multiphoton ATD probability. Altogether 198 coupled channels had to be considered in the calculation. The calculations reveal signatures of significant ejection of the photodissociation fragments away from the laser polarization direction due to the inclusion of the higher excited electronic states. The ratio of the photofragments perpendicular to and along the polarization axis shows good quantitative agreement with the experimental result. The angular distributions show considerable structures depending on the relative kinetic energies of the photofragments, and the fragments with different kinetic energies show peaks at different dissociation angles.
机译:我们已经从初始振动旋转水平v(i)= 4,5和J( i)= 0,1在波长为400 nm,强度为3x10(13)W / cm(2)的强线性偏振激光场中。该计算使用了与时间无关的紧密耦合(CC)形式主义,其中八个(十)电子态包含在分子波函数的基集扩展中。除两个最低的1s sigma(g)和2p sigma(u)态外,包括的分子电子态分别为2p pi(+/-)(u),2s sigma(g),3p sigma(u),3d sigma (g),3d pi(+/-)(g)和4f sigma(u)。所有更高的电子态都离解为原子态D(2l)。为了确保多光子ATD概率的收敛,考虑了足够数量的光子吸收通道n = 0-7和分子旋转量子数J = 0-11。计算中必须考虑总共198个耦合通道。计算结果表明,由于包含了较高的激发电子态,光解离片段明显远离激光偏振方向喷射。垂直于偏振轴并沿着偏振轴的光碎片比例与实验结果具有良好的定量一致性。角分布显示取决于光碎片的相对动能的可观结构,并且具有不同动能的片段在不同的解离角处显示峰。

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