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Hydrogen-iodine scattering. II. Rovibronic analysis and collisional dynamics
Nicole Weike1, Wolfgang Eisfeld1, Kevin M Dunseath2
1Theoretische Chemie, Universität Bielefeld, Postfach 100131, D-33501 Bielefeld, Germany.
This study analyzes H + I collisions using a new spin-orbit coupled potential energy model. It examines bound states, scattering processes, and resonances, providing insights into chemical dynamics.
Area of Science:
- Chemical Physics
- Quantum Mechanics
- Molecular Dynamics
Background:
- Accurate potential energy models are crucial for understanding chemical reaction dynamics.
- Spin-orbit coupling significantly influences the behavior of heavy-atom systems like H + I.
Purpose of the Study:
- To analyze bound and quasi-bound states in H + I collisions using a novel spin-orbit coupled diabatic potential energy model.
- To investigate elastic and inelastic scattering processes and the role of resonances in H + I collisions.
- To compare calculations using a full diabatic model with approximations based on single adiabatic states.
Main Methods:
- Utilized a recently developed spin-orbit coupled diabatic potential energy model for HI.
- Performed thorough analysis of ro-vibronic bound and quasi-bound states.
- Computed elastic and inelastic scattering cross sections and thermal rates up to 12,500 cm⁻¹.
- Analyzed resonances by their energy, width, lifetime, and decay probabilities.
Main Results:
- The spin-orbit coupled diabatic model accurately describes complex dynamics in H + I collisions.
- Calculations revealed detailed properties of bound and quasi-bound states.
- Resonances were identified and characterized, influencing thermal rates.
- Decay probabilities of high-energy resonances were studied for photodissociation branching ratios.
Conclusions:
- The developed potential energy model is effective for studying H + I scattering dynamics.
- Resonances play a significant role in the thermal rates and photodissociation branching ratios.
- Approximations using single adiabatic states were evaluated against the full diabatic model.
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