Coupled coherent states method for tunneling dynamics: an interpretative study

Abstract Numerical solutions of the time-dependent Schrödinger equation based on the variational principle may offer physical insight that cannot be gained by a solution using fixed grids in position and momentum space. Here we focus on the tunneling dynamics in a quartic double-well and the use of classical, trajectory-guided coherent states to gain insight into the workings of the coupled coherent states method developed by Shalashilin and Child [J. Chem. Phys. 113, 10028 (2000)]. It is shown that over-the-barrier classical trajectories, alone, can accurately describe the tunneling effect.

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Publication Details

Journal
Journal of Physics Conference Series
Published
2024-11-01
DOI
https://doi.org/10.1088/1742-6596/2883/1/012005
Citations
1
Primary Topic
Quantum chaos and dynamical systems
Type
article
Field-Weighted Citation Impact
0.28
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article

Coupled coherent states method for tunneling dynamics: an interpretative study

Frank Großmann
1 citations
Journal of Physics Conference Series
Quantum chaos and dynamical systems
0.28
article

Coupled coherent states method for tunneling dynamics: an interpretative study

Frank Großmann
article en
1 citations

Abstract

Abstract Numerical solutions of the time-dependent Schrödinger equation based on the variational principle may offer physical insight that cannot be gained by a solution using fixed grids in position and momentum space. Here we focus on the tunneling dynamics in a quartic double-well and the use of classical, trajectory-guided coherent states to gain insight into the workings of the coupled coherent states method developed by Shalashilin and Child [J. Chem. Phys. 113, 10028 (2000)]. It is shown that over-the-barrier classical trajectories, alone, can accurately describe the tunneling effect.

Journal of Physics Conference SeriesVol. 2883(1)
Technische Universität Dresden (DE)
Sustainable cities and communities
Openalex Percentile: Top 43%
Quantum chaos and dynamical systems
0.28
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