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This research advances the theoretical modeling of dissipative quantum dynamics in molecule-cavity systems, specifically addressing how cavity losses and molecular rotation influence nonadiabatic processes. By comparing key mathematical frameworks like the Lindblad master equation with stochastic Schrödinger approaches, it offers a more efficient computational path for simulating light-induced conical intersections in Na2 molecules. These insights are critical for refining quantum simulations of photonic materials where dissipation cannot be ignored.
Light-induced nonadiabatic dissipative quantum dynamics of the Na2 molecule
arXiv:2606.15292v1 Announce Type: new Abstract: Strong light-matter coupling between molecules and optical or plasmonic cavity modes has emerged as a promising platform for advancing photonics, materials science, and chemistry. However, optical cavities and plasmonic resonators in particular are inherently lossy systems characterized by finite photon lifetimes. Accurate theoretical descriptions of molecular dynamics under strong coupling therefore require a proper treatment of cavity losses. In this work, we compare three theoretical approaches for modeling dissipative molecule-cavity dynamics within a realistic parameter regime: the Lindblad master equation, the stochastic Schr\"odinger equation, and the non-Hermitian Schr\"odinger equation. As an example, we consider the two lowest energy state of Na2 molecule coupled to a cavity mode and analyze the time evolution of the excited-state population and the mean photon number. Our results demonstrate that the stochastic Schr\"odinger equation provides an accurate and computationally efficient alternative to the Lindblad master equation, while the non-Hermitian Schr\"odinger approach is found to be applicable only within a limited range of conditions. Furthermore, we show that inclusion of molecular rotation leads to rotational-vibrational-photonic coupling and gives rise to pronounced nonadiabatic dynamics through light-induced conical intersections. These findings highlight the importance of both dissipation and rotational degrees of freedom for a realistic description of molecular dynamics in strongly coupled molecule-cavity systems.
Abstract:Strong light-matter coupling between molecules and optical or plasmonic cavity modes has emerged as a promising platform for advancing photonics, materials science, and chemistry. However, optical cavities and plasmonic resonators in particular are inherently lossy systems characterized by finite photon lifetimes. Accurate theoretical descriptions of molecular dynamics under strong coupling therefore require a proper treatment of cavity losses. In this work, we compare three theoretical approaches for modeling dissipative molecule-cavity dynamics within a realistic parameter regime: the Lindblad master equation, the stochastic Schrödinger equation, and the non-Hermitian Schrödinger equation. As an example, we consider the two lowest energy state of Na2 molecule coupled to a cavity mode and analyze the time evolution of the excited-state population and the mean photon number. Our results demonstrate that the stochastic Schrödinger equation provides an accurate and computationally efficient alternative to the Lindblad master equation, while the non-Hermitian Schrödinger approach is found to be applicable only within a limited range of conditions. Furthermore, we show that inclusion of molecular rotation leads to rotational-vibrational-photonic coupling and gives rise to pronounced nonadiabatic dynamics through light-induced conical intersections. These findings highlight the importance of both dissipation and rotational degrees of freedom for a realistic description of molecular dynamics in strongly coupled molecule-cavity systems.
Quantum Physics (quant-ph); Atomic and Molecular Clusters (physics.atm-clus)
arXiv:2606.15292 [quant-ph]
(or arXiv:2606.15292v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2606.15292 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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