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    Laser-assisted dynamic interference in double ionization of helium

    Qiubo Meng1, Mingxuan Li2,3, Sizuo Luo2,3,*, Dajun Ding2,3,†, Liang-You Peng4,5, and Wei-Chao Jiang1,‡

    • 1Institute of Quantum Precision Measurement, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
    • 2Institute of Atomic and Molecular Physics, Jilin University, Changchun 130012, China
    • 3Jilin Provincial Key Laboratory of Applied Atomic and Molecular Spectroscopy, Jilin University, Changchun 130012, China
    • 4State Key Laboratory for Mesoscopic Physics and Collaborative Innovation Center of Quantum Matter, School of Physics, Peking University, Beijing 100871, China
    • 5Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China

    • *Contact author: luosz@jlu.edu.cn
    • †Contact author: dajund@jlu.edu.cn
    • ‡Contact author: jiang.wei.chao@szu.edu.cn

    Phys. Rev. A 113, 043122 – Published 17 April, 2026

    DOI: https://doi.org/10.1103/w5ls-g47d

    Abstract

    We theoretically study the double ionization of helium atom induced by an ultrashort extreme ultraviolet (XUV) pulse with the photon energy above the double-ionization threshold in the presence of an infrared (IR) laser pulse. By numerically solving the reduced-dimensional time-dependent Schrödinger equation (TDSE), we obtain the joint energy spectra of the two photoelectrons, in which peak splittings are observed both in the main band where one XUV photon is absorbed and in the sidebands where additional IR photons are either absorbed or emitted. A simple laser-assisted dynamic interference (LADI) model, based on the strong-field approximation (SFA) and neglecting the electron-electron correlation, accurately reproduces the numerical TDSE results regarding the peak splittings in the total energy spectra. Additionally, peak-splitting structures arising from the dynamic multiphoton interference (DMPI) mechanism are identified in the joint energy spectra. The DMPI is revealed by excluding the key LADI phase term in the SFA formula. We find that the DMPI is sensitive to the energy sharing between the two photoelectrons, and its contribution to peak splitting is likely smeared out in the total energy spectrum.

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