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Transition from strong-field sequential to nonsequential double ionization at near-infrared wavelengths and low intensities

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Abstract

Within a quantum-mechanical model, we investigate strong-field double ionization of a model helium atom by near-infrared, linearly polarized laser pulses at intensities far below the recollision threshold. The quantum simulations show a clear mechanism change from sequential to nonsequential double ionization (NSDI) as the laser intensity increases. For NSDI, the two-electron correlated momentum distribution exhibits a strong final-state Coulomb repulsion effect for high-energy photoelectrons, but absent for low-energy photoelectrons. This repulsion effect is ascribed to field double ionization from doubly-excited states populated by recollision of the first ionized electron when it returns to the parent ion. Such recollision-induced excited states are absent at ultraviolet wavelengths due to the very low returning kinetic energies, resulting to the absence of final-state repulsion effect in NSDI.

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Funding

National Natural Science Foundation of China (11674257, 11604248); Program for Distinguished Middle-aged and Young Innovative Research Team in Higher Education of Hubei, China (No. T201806); Natural Science Foundation of Hubei (2014CFB578).

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Correspondence to Qing Liao.

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Liu, K., Qin, M., Li, Q. et al. Transition from strong-field sequential to nonsequential double ionization at near-infrared wavelengths and low intensities. Opt Quant Electron 50, 364 (2018). https://doi.org/10.1007/s11082-018-1620-z

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