Contribution of the pre-ionized H and the ionized H subsystems to the HHG Spectra of H in intense laser fields
arXiv:1712.01596 · doi:10.1088/1361-6455/aaafb1
Abstract
Contributions of the pre-ionized H (PI-H) and ionized H subsystems of the two-electron H system to its high-order harmonic generation in 8-cycle -like ultrafast intense laser pulses are calculated and analyzed based on the solution of the time-dependent Schrödinger equation (TDSE) for the one-dimensional two-electronic H system with fixed nuclei. The laser pulses have nm wavelengths and , 5, 1 \&\ 5 Wcm intensities. It is found that at the two lower intensities, the PI-H subsystem dominantly produces the HHG spectra. While, at the two higher intensities, both PI-H and ionized H subsystems contribute comparably to the HHG spectra. In the H subsystem, the symmetry of the populations of H(I) and H(II) regions (left and right regions of H subsystem) is broken by increasing the laser intensity. Complex patterns and even harmonics also appear at these two higher intensities. For instance, at Wcm intensity and = 532 nm, the even harmonics are appeared near cut-off region. Interestingly, at Wcm intensity and = 390 nm, the even harmonics replaced by the odd harmonics with red shift. At = 390 \&\ 532 nm and intensity, the two-electron cutoffs corresponding to nonsequential double-recombination (NSDR) with maximum return kinetic energy of 4.70 are detected. The HHG spectra of the whole H system obtained with and without nuclear dynamics treated classically are approximately similar. However, at Wcm intensity and = 532 nm, if we take into account nuclear dynamics, the even harmonics which are appeared near cutoff region, replaced by the odd harmonics with blue shift.
12 pages, 10 figures
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