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Which Algorithm Best Propagates the Meyer-Miller-Stock-Thoss Mapping Hamiltonian for Non-Adiabatic Dynamics?
Lauren E Cook1, Johan E Runeson2, Jeremy O Richardson2
1Department of Chemistry, University College London, Christopher Ingold Building, London WC1H 0AJ, U.K.
This study compares three algorithms for simulating quantum-classical dynamics using the Meyer-Miller-Stock-Thoss (MMST) Hamiltonian. The Momentum Integral (MInt) algorithm is rigorously symplectic, while the Split-Liouvillian (SL) offers comparable accuracy at lower cost.
Area of Science:
- Quantum Chemistry
- Computational Chemistry
- Chemical Physics
Background:
- Mixed quantum-classical dynamics simulations are crucial for understanding chemical processes.
- The Meyer-Miller-Stock-Thoss (MMST) Hamiltonian and spin-mapping approaches are common for these simulations.
- Efficient and accurate numerical algorithms are needed for integrating the equations of motion.
Purpose of the Study:
- To compare the performance of three time-propagation algorithms for the MMST Hamiltonian: Momentum Integral (MInt), Split-Liouvillian (SL), and Degenerate Eigenvalue (DE).
- To analyze accuracy, energy conservation, symplecticity, Liouville's theorem adherence, and computational cost.
- To provide guidance for selecting appropriate algorithms in future mapping-variable simulations.
Main Methods:
- Implementation and comparison of MInt, SL, and DE algorithms for the MMST Hamiltonian.
- Evaluation of individual trajectory accuracy and correlation functions.
- Assessment of conserved quantities (energy, symplecticity, Liouville's theorem) and computational expense.
Main Results:
- The MInt algorithm is the only rigorously symplectic method among those tested.
- The SL algorithm achieves comparable accuracy to MInt but with reduced computational cost.
- The DE algorithm exhibits poor energy conservation, even at small timesteps, due to its inherent approximation.
Conclusions:
- The choice of algorithm significantly impacts the accuracy, conservation properties, and efficiency of mixed quantum-classical simulations.
- The SL algorithm presents a favorable balance of accuracy and computational cost.
- The DE algorithm's limitations in energy conservation warrant caution in its application.
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