4.6 Article

Ionization of HCCI Neutral and Cations by Strong Laser Fields Simulated With Time Dependent Configuration Interaction

期刊

FRONTIERS IN CHEMISTRY
卷 10, 期 -, 页码 -

出版社

FRONTIERS MEDIA SA
DOI: 10.3389/fchem.2022.866137

关键词

HCCI plus; iodoacetylene cation; strong field ionization; coherent superposition; time-dependent configuration interaction; pump-probe

资金

  1. National Science Foundation [CHE1856437]
  2. U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES) [DE-SC0020994]
  3. U.S. Department of Energy (DOE) [DE-SC0020994] Funding Source: U.S. Department of Energy (DOE)

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This study investigates the coherent superposition of the X and A cations in neutral iodoacetylene through strong field ionization, and explores the orbital and angular dependence in the generation of cations and dications. It is found that the frequency of charge oscillation depends on the energy separation between the X and A states, while the ionization rates are affected by the polarization direction, carrier envelope phase, and initial phase of the superposition.
Strong field ionization of neutral iodoacetylene (HCCI) can produce a coherent superposition of the X and A cations. This superposition results in charge migration between the CC pi orbital and the iodine pi-type lone pair which can be monitored by strong field ionization with short, intense probe pulses. Strong field ionization of the X and A states of HCCI cation was simulated with time-dependent configuration interaction using singly ionized configurations and singly excited, singly ionized configurations (TD-CISD-IP) and an absorbing boundary. Studies with static fields were used to obtain the 3-dimensional angular dependence of instantaneous ionization rates by strong fields and the orbitals involved in producing the cations and dications. The frequency of charge oscillation is determined by the energy separation of the X and A states; this separation can change depending on the direction and strength of the field. Furthermore, fields along the molecular axis can cause extensive mixing between the field-free X and A configurations. For coherent superpositions of the X and A states, the charge oscillations are characterized by two frequencies-the driving frequency of the laser field of the probe pulse and the intrinsic frequency due to the energy separation between the X and A states. For linear and circularly polarized pulses, the ionization rates show marked differences that depend on the polarization direction of the pulse, the carrier envelope phase and initial phase of the superposition. Varying the initial phase of the superposition at the beginning of the probe pulse is analogous to changing the delay between the pump and probe pulses. The charge oscillation in the coherent superposition of the X and A states results in maxima and minima in the ionization yield as a function of the superposition phase.

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