Departamento de Química, Modulo 13, Universidad Autónoma de Madrid, 28049 Madrid, Spain.
Chemphyschem. 2013 May 10;14(7):1456-63. doi: 10.1002/cphc.201200974. Epub 2013 Mar 14.
Atomic autoionization following photoabsorption is a typical example of quantum interferences governed by electron-electron correlation. Coherence between direct photoionization and autoionization paths results in "Fano profiles", widely explored in atoms in the last 60 years. The advent of femto- and attosecond laser technology made time-resolved images of the delayed electron ejection in autoionization accessible, leading to the reemergence of such studies in atomic systems. The counterpart molecular phenomena show the richness, as well as the complexity, added by nuclear motion, which may proceed on similar time scales. However, Fano profiles are usually absent in measured molecular photoionization cross sections and an unequivocal parametrization of molecular autoionization signatures, similar to that introduced by Fano in atoms [U. Fano, Phys. Rev. 1961, 124, 1866] has not yet been achieved. In this work we introduce a simple semiclassical model that accounts for all the features observed in H2 photoionization and demonstrate that the interference structures observed in dissociative ionization spectra are almost exclusively due to the phase accumulated in the nuclear motion. Furthermore, we show that the temporal build-up of these structures in the energy-differential cross sections is also determined by nuclear motion. We validate our models by comparing with full-dimensional ab initio calculations solving the time-dependent Schrödinger equation.
原子光致自电离是电子关联控制的量子干涉的典型例子。直接光电离和自电离路径之间的相干导致了“Fano 轮廓”,这在过去 60 年中在原子中得到了广泛的研究。飞秒和阿秒激光技术的出现使得自电离中延迟电子发射的时间分辨图像变得可行,这导致了这种研究在原子系统中的重新出现。分子对应的现象显示了核运动带来的丰富性和复杂性,核运动可能在相似的时间尺度上进行。然而,在测量的分子光致电离截面中通常不存在 Fano 轮廓,并且尚未实现类似于原子中 Fano 引入的分子自电离特征的明确参数化[U. Fano,Phys. Rev. 1961, 124, 1866]。在这项工作中,我们引入了一个简单的半经典模型,该模型解释了 H2 光致电离中观察到的所有特征,并证明了在离解电离光谱中观察到的干涉结构几乎完全是由核运动中积累的相位引起的。此外,我们表明,这些结构在能量微分截面中的时间积累也由核运动决定。我们通过与求解含时薛定谔方程的全维从头计算进行比较来验证我们的模型。