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Generalized Formulation of the Density Functional Tight Binding-Based Restricted Ensemble Kohn-Sham Method with
1Department of Chemistry, Ulsan National Institute of Science and Technology (UNIST), 50 UNIST-gil, Ulju-gun, Ulsan 44919, South Korea.
We developed a new computational method combining density functional tight binding (DFTB) with state-interaction state-average spin-restricted ensemble-referenced Kohn-Sham (SI-SA-REKS or SSR) and long-range corrected (LC) functionals. This approach accurately models conical intersections, crucial for molecular dynamics simulations.
Area of Science:
- Computational Chemistry
- Quantum Chemistry
- Theoretical Chemistry
Background:
- Accurate modeling of excited states and conical intersections is vital for understanding photochemical processes.
- Existing methods like DFTB have limitations in describing multireference systems.
Purpose of the Study:
- To generalize the density functional tight binding (DFTB) approach by incorporating the state-interaction state-average spin-restricted ensemble-referenced Kohn-Sham (SI-SA-REKS or SSR) method.
- To include onsite correction (OC) and long-range corrected (LC) functionals for improved accuracy.
- To accurately describe conical intersections and excited-state dynamics.
Main Methods:
- Generalized formulation of LC-OC-DFTB/SSR method.
- Benchmarking against various DFTB calculation methods for excitation energies and conical intersection structures.
- Performing excited-state molecular dynamics simulations using the developed method.
Main Results:
- The LC-OC-DFTB/SSR method provides more accurate energies and analytic gradients for individual microstates.
- The multireference character of SSR correctly describes conical intersections.
- The onsite correction (OC) contribution to the LC functional is essential for obtaining accurate conical intersection geometries.
Conclusions:
- The developed LC-OC-DFTB/SSR method offers a significant improvement for calculating excited-state properties and conical intersections.
- This method is crucial for accurate molecular dynamics simulations of photochemical systems, such as molecular rotary motors.
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