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The impact of non-adiabatic effects on reaction dynamics: a study based on the adiabatic and non-adiabatic potential energy surfaces of CaH 2

The two-state non-adiabatic potential energy matrices of the CaH 2 + system are calculated via a diabatization approach by using a neural network model. Subsequently, the adiabatic and non-adiabatic potential energy surfaces (PESs) are constructed based on these non-adiabatic potential energy matric...

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Published in:Physical chemistry chemical physics : PCCP 2023-08, Vol.25 (34), p.22744-22754
Main Authors: He, Di, Li, Wentao, Li, Quanjiang, Chen, Shenghui, Wang, Li, Liu, Yanli, Wang, Meishan
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creator He, Di
Li, Wentao
Li, Quanjiang
Chen, Shenghui
Wang, Li
Liu, Yanli
Wang, Meishan
description The two-state non-adiabatic potential energy matrices of the CaH 2 + system are calculated via a diabatization approach by using a neural network model. Subsequently, the adiabatic and non-adiabatic potential energy surfaces (PESs) are constructed based on these non-adiabatic potential energy matrices. Furthermore, based on the adiabatic and non-adiabatic PESs, the Ca + (4s 2 S) + H 2 (X 1 Σ+g) → H( 2 S) + CaH + (X 1 Σ + ) reaction is studied using the time-dependent wave packet method. Comparative analysis of the experimental and theoretical integral reaction cross-sections (ICSs) indicates that the maximum deviation between the results obtained from the adiabatic PES and the corresponding experimental value is 12.7 bohr 2 ; in contrast, the maximum discrepancy between the theoretical result derived from the non-adiabatic PES and the experimental value is merely 0.42 bohr 2 . The potential well along the reaction path acts as a ‘filter’, selectively guiding intermediates with longer lifetimes in the potential well back to the reactant channel. This phenomenon indicates that the non-adiabatic effects significantly influence the reaction dynamics of the CaH 2 + system.
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Subsequently, the adiabatic and non-adiabatic potential energy surfaces (PESs) are constructed based on these non-adiabatic potential energy matrices. Furthermore, based on the adiabatic and non-adiabatic PESs, the Ca + (4s 2 S) + H 2 (X 1 Σ+g) → H( 2 S) + CaH + (X 1 Σ + ) reaction is studied using the time-dependent wave packet method. Comparative analysis of the experimental and theoretical integral reaction cross-sections (ICSs) indicates that the maximum deviation between the results obtained from the adiabatic PES and the corresponding experimental value is 12.7 bohr 2 ; in contrast, the maximum discrepancy between the theoretical result derived from the non-adiabatic PES and the experimental value is merely 0.42 bohr 2 . The potential well along the reaction path acts as a ‘filter’, selectively guiding intermediates with longer lifetimes in the potential well back to the reactant channel. 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title The impact of non-adiabatic effects on reaction dynamics: a study based on the adiabatic and non-adiabatic potential energy surfaces of CaH 2
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