论文标题
振动偏振子增强分子非线性吸收的空腔分子动力学模拟
Cavity molecular dynamics simulations of vibrational polariton enhanced molecular nonlinear absorption
论文作者
论文摘要
最近的实验已经观察到,在集体振动强耦合(VSC)条件下,可以在光学Fabry-Perrot微腔内修饰分子的化学和光物理性能,而理论上目前尚不对这种修饰进行理解。为了了解这种空腔诱导现象的起源,一些最近的研究集中在腔环境对分子子系统非线性光学响应的影响上。在这里,我们使用最近提出的用于经典腔分子动力学(CAVMD)模拟的方案来数值研究在光脉冲激发后这种VSC条件下液体二氧化碳的线性和非线性响应。我们发现,将强烈的激发脉冲应用于较低的杂化光态状态,即下极化子(LP),可以导致总体分子非线性吸收,从而相对于腔外的激发,可以增强多达两个数量级。这种极化增强的多光子吸收也会在强照明下引起超短LP寿命(0.2 PS)。与通常的极性弛豫过程不同,在当前的机制下,极化能量直接转移到了单一激发的振动暗状态的流动过程中,LP将能量直接转移到较高的振动激发的黑暗状态的歧管上;这些高度激发的黑暗状态随后放松到具有数十ps的寿命。由于本机制本质上是通用的,因此我们期望在不同的分子系统和不同体积的空腔中观察到这些数值预测。
Recent experiments have observed that the chemical and photophysical properties of molecules can be modified inside an optical Fabry-Perot microcavity under collective vibrational strong coupling (VSC) conditions, and such modification is currently not well understood by theory. In an effort to understand the origin of such cavity induced phenomena, some recent studies have focused on the effect of the cavity environment on the nonlinear optical response of the molecular subsystem. Here, we use a recently proposed protocol for classical cavity molecular dynamics (CavMD) simulations to numerically investigate the linear and nonlinear response of liquid carbon dioxide under such VSC conditions following an optical pulse excitation. We find that applying a strong pulse of excitation to the lower hybrid light-matter state, i.e., the lower polariton (LP), can lead to an overall molecular nonlinear absorption which is enhanced by up to two orders of magnitude relative to the excitation outside the cavity. This polariton-enhanced multiphoton absorption also causes an ultrashort LP lifetime (0.2 ps) under strong illumination. Unlike usual polariton relaxation processes -- whereby polaritonic energy transfers directly to the manifold of singly excited vibrational dark states -- under the present mechanism, the LP transfers energy directly to the manifold of higher vibrationally excited dark states; these highly excited dark states subsequently relax to the manifold of singly excited states with a lifetime of tens of ps. Because the present mechanism is generic in nature, we expect these numerical predictions to be experimentally observed in different molecular systems and in cavities with different volumes.