Sidler Dominik, Ruggenthaler Michael, Rubio Angel
Max Planck Institute for the Structure and Dynamics of Matter and Center for Free-Electron Laser Science, Luruper Chaussee 149, Hamburg 22761, Germany.
The Hamburg Center for Ultrafast Imaging, Luruper Chaussee 149, Hamburg 22761, Germany.
J Chem Theory Comput. 2023 Dec 12;19(23):8801-8814. doi: 10.1021/acs.jctc.3c00092. Epub 2023 Nov 16.
The first numerically exact simulation of a full ab initio molecular quantum system (HD) under strong ro-vibrational coupling to a quantized optical cavity mode in thermal equilibrium is presented. Theoretical challenges in describing strongly coupled systems of mixed quantum statistics (bosons and Fermions) are discussed and circumvented by the specific choice of our molecular system. Our numerically exact simulations highlight the absence of zero temperature for the strongly coupled matter and light subsystems, due to cavity-induced noncanonical conditions. Furthermore, we explore the temperature dependency of light-matter quantum entanglement, which emerges for the ground state but is quickly lost already in the deep cryogenic regime. This is in contrast to predictions from the Jaynes-Cummings model, which is the standard starting point to model collective strong-coupling chemistry phenomenologically. Moreover, we find that the fluctuations of matter remain modified by the quantum nature of the thermal and vacuum-field fluctuations for significant temperatures, e.g., at ambient conditions. These observations (loss of entanglement and coupling to quantum fluctuations) have implications for the understanding and control of polaritonic chemistry and materials science, since a semiclassical theoretical description of light-matter interaction becomes reasonable, but the typical (classical) canonical equilibrium assumption for the nuclear subsystem remains violated. This opens the door for quantum fluctuation-induced stochastic resonance phenomena under vibrational strong coupling, which have been suggested as a plausible theoretical mechanism to explain the experimentally observed resonance phenomena in the absence of periodic driving that has not yet been fully understood.
首次展示了在热平衡状态下,一个完整的从头算分子量子系统(HD)与量子化光学腔模式发生强旋转振动耦合时的数值精确模拟。讨论了描述混合量子统计(玻色子和费米子)强耦合系统时的理论挑战,并通过我们对分子系统的特定选择加以规避。我们的数值精确模拟突出了由于腔诱导的非规范条件,强耦合物质和光子系统不存在零温度。此外,我们探索了光与物质量子纠缠的温度依赖性,这种纠缠在基态出现,但在深低温状态下很快就会消失。这与Jaynes-Cummings模型的预测形成对比,该模型是从现象学角度模拟集体强耦合化学的标准起点。此外,我们发现,在显著温度下,例如在环境条件下,物质的涨落仍会受到热场涨落和真空场涨落量子性质的影响。这些观察结果(纠缠的丧失以及与量子涨落的耦合)对极化子化学和材料科学的理解与控制具有重要意义,因为光与物质相互作用的半经典理论描述变得合理,但核子系统典型的(经典)正则平衡假设仍然不成立。这为振动强耦合下量子涨落诱导的随机共振现象打开了大门,这一现象被认为是一种合理的理论机制,可以解释在尚未完全理解的无周期驱动情况下实验观察到的共振现象。