Related Experiment Video
Updated: May 26, 2025

Characterization of Thermal Transport in One-dimensional Solid Materials
Published on: January 26, 2014
Nonadiabatic Effects in the H + LiD(ν = 0, j = 0) → Li(2s) + HD Reaction Near Cold Collisions
Yuwen Bai1, Bayaer Buren2, Zijiang Yang3
1School of Strengthening Basic Disciplines, Shanxi Institute of Energy, Jinzhong 030600, China.
Abstract:
Nonadiabatic dynamic study of the H + LiD(ν = 0, j = 0) → Li(2s) + HD reaction is carried out using the time-dependent wave packet method in a collision energy range of 1-80 cm-1. The total integral cross section exhibits a partial wave resonance near 2 cm-1, corresponding to the opening of the J = 5 partial wave. The nonadiabatic coupling effects inhibit the reactivity, especially for the low-vibrational states. The rotational excitation of products is affected by nonadiabatic coupling effects. The maximum accessible rotational state of the products is higher when nonadiabatic effects are included than when they are omitted. At low collision energies, the product angular distributions are influenced by the resonances. Nonadiabatic results reveal a more pronounced backward scattering of the products than adiabatic results. As collision energy increases, the stripping mechanism gradually becomes dominant, and both adiabatic and nonadiabatic results exhibit significant forward-scattering characteristics.
More Related Videos
08:55High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy
Published on: October 9, 2020
08:42High-Sensitivity Nuclear Magnetic Resonance at Giga-Pascal Pressures: A New Tool for Probing Electronic and Chemical Properties of Condensed Matter under Extreme Conditions
Published on: October 10, 2014
Related Concept Videos
π Electron Effects on Chemical Shift: Overview
UV–Vis Spectroscopy: Molecular Electronic Transitions
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds
Molecular Orbital Theory II
The Born-Haber Cycle
Adiabatic Processes for an Ideal Gas