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Electron-rotation coupling in UV photodissociation of aligned diatomics

Yan Rong LiuSchool of Physics and Information Technology, Shaanxi Normal University, Xi'an 710119, ChinaVictor KimbergInternational Research Center of Spectroscopy and Quantum Chemistry, Siberian Federal University – IRC SQC, 660041 Krasnoyarsk, RussiaYong WuCenter for Applied Physics and Technology, Peking University, Beijing 100084, ChinaJianguo WangInstitute of Applied Physics and Computational Mathematics, Beijing 100088, ChinaOriol VendrellTheoretical Chemistry, Institute of Physical Chemistry, Heidelberg University, 69120 Heidelberg, GermanySong Bin ZhangSchool of Physics and Information Technology, Shaanxi Normal University, Xi'an 710119, China
2022en
ABI

Аннотация

We investigate the effect of electron-rotation coupling ($\mathbf{R}\ensuremath{-}\mathrm{\ensuremath{\Omega}}$ coupling) on fs UV photodissociation dynamics of aligned diatomic molecules. We consider the showcase of ground-state $\mathrm{Mg}{\mathrm{H}}^{+}$ (${}^{1}{\mathrm{\ensuremath{\Sigma}}}^{+}$) pumped by an fs IR pulse, which initiates rotational dynamics leading to field-free molecular alignment. A time-delayed fs UV pulse probes the degree of alignment of the rotational wave packet in the framework of photodissociation spectroscopy. The molecular alignment correlates directly with the angular distribution of the photofragments in the dissociative ${}^{1}\mathrm{\ensuremath{\Pi}}$ state, as it is shown in our simulations comparing the cases when the $\mathbf{R}\ensuremath{-}\mathrm{\ensuremath{\Omega}}$ coupling is included and ignored. We show how the angular distribution of the photofragment is strongly affected by the $\mathbf{R}\ensuremath{-}\mathrm{\ensuremath{\Omega}}$ coupling at various delay times with specific molecular alignment. It was shown that increases of the fs UV pulse intensity and the degree of alignment enhance the effect of $\mathbf{R}\ensuremath{-}\mathrm{\ensuremath{\Omega}}$ coupling on the angular distribution of the photofragments. On the contrary, an increase of the initial temperature tends to reduce the effect of $\mathbf{R}\ensuremath{-}\mathrm{\ensuremath{\Omega}}$ coupling, which is explained by the fact that such an effect turns smaller as the increasing of magnetic state $|{\mathrm{M}}_{0}|$ for each initial rotational state ${\mathrm{J}}_{0}$; furthermore, higher excited rotational state ${\mathrm{J}}_{0}$ contains more magnetic states ${\mathrm{M}}_{0}$, and the results have been averaged over all degenerated ${\mathrm{M}}_{0}$ states.

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