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A two-scale approach to electron correlation in multiconfigurational perturbation theory
Pooria Farahani1, Daniel Roca-Sanjuán, Francesco Aquilante
1Department of Chemistry - Ångström, The Theoretical Chemistry Programme, Uppsala University, P. O. Box 518, SE-751 20, Uppsala, Sweden.
This study introduces a new computational method for large molecules, reducing computational cost by treating active sites with high accuracy and the environment with less demanding methods. This approach efficiently calculates dynamic electron correlation effects.
Area of Science:
- Computational Chemistry
- Quantum Chemistry
- Theoretical Chemistry
Background:
- Calculating dynamic electron correlation in large molecular systems is computationally intensive.
- Accurate treatment of electron correlation is crucial for understanding molecular behavior.
Purpose of the Study:
- To develop a computationally efficient method for calculating dynamic electron correlation in large molecular systems.
- To enable accurate electronic structure calculations for complex molecules.
Main Methods:
- A new approach based on multiconfigurational second-order perturbation theory (CASPT2) is proposed.
- The method partitions the system into an active site and an environment.
- Dynamic correlation is calculated at the CASPT2 level for the active site, while the environment is treated with lower computational cost.
Main Results:
- The new method offers substantial savings in storage and computational demands compared to full CASPT2 calculations for large systems.
- Approximation introduces small errors, which are outweighed by the computational benefits.
- The scheme provides a hierarchical approach to electron correlation.
Conclusions:
- The proposed method provides a computationally feasible way to study dynamic electron correlation in large molecular systems.
- This hierarchical approach allows for treating different molecular scales with appropriate levels of theory.
- The method is particularly beneficial when static correlation is adequately handled for the entire system.
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