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. 2024 Mar 13;29(6):1263.
doi: 10.3390/molecules29061263.

State-to-State Quantum Dynamics Study of Intramolecular Isotope Effects on Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D Reaction

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State-to-State Quantum Dynamics Study of Intramolecular Isotope Effects on Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D Reaction

Hongtai Xu et al. Molecules. .

Abstract

The dynamic mechanisms and intramolecular isotope effects of the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction are studied at the state-to-state level using the time-dependent wave packet method on a high-quality potential energy surface. This reaction can proceed along the indirect pathway that features a barrier and a deep well or the smooth direct pathway. The reaction probabilities, total and state-resolved integral cross sections, and differential cross sections are analyzed in detail. The calculated dynamics results show that both of the products are mainly formed by the dissociation of a collinear HBeD intermediate when the collision energy is slightly larger than the threshold. As the collision energy increases, the BeH + D channel is dominated by the direct abstraction process, whereas the BeD + H channel mainly follows the complex-forming mechanism.

Keywords: integral cross section; intramolecular isotope effect; quantum dynamics; time-dependent wave packet.

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Conflict of interest statement

The authors declare no conflicts of interest.

Figures

Figure 1
Figure 1
Indirect and direct pathways of the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction.
Figure 2
Figure 2
Total reaction probabilities of the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction as a function of collision energy at four particle waves (J = 0, 30, 60, and 80).
Figure 3
Figure 3
Opacity functions of the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction at the collision energy of 2.0, 2.5, 3.0, and 4.0 eV.
Figure 4
Figure 4
Total ICSs of the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction and the BeH/BeD branching ratio as a function of collision energy.
Figure 5
Figure 5
Ro-vibrationally resolved ICSs of the BeH + D channel at (a) 2.5 and (b) 4.0 eV collision energy and the BeD + H channel at (c) 2.5 and (d) 4.0 eV for the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction.
Figure 6
Figure 6
Total DCSs of t the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD + H/D reaction as a function of collision energy.
Figure 7
Figure 7
Rotationally resolved DCSs of the BeH + D channel at (a) 2.5 and (b) 4.0 eV collision energy and the BeD + H channel at (c) 2.5 and (d) 4.0 eV at v′ = 0 for the Be(1S) + HD (v0 = 2, j0 = 0) → BeH/BeD (v′ = 0, j′) + H/D reaction.

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