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
Schr"{o}dinger 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.

生成讲解博客的中文版本

生成AI智能校验的中文版本