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The shape of the electric dipole function determines the sub-picosecond dynamics of anharmonic vibrational polaritons

机译:电偶极子功能的形状决定了anharmonic振动极化子的亚皮秒动态

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Vibrational strong coupling has emerged as a promising route for manipulating the reactivity of molecules inside infrared cavities. We develop a full-quantum methodology to study the unitary dynamics of a single anharmonic vibrational mode interacting with a quantized infrared cavity field. By comparing multi-configurational time-dependent Hartree simulations for an intracavity Morse oscillator with an equivalent formulation of the problem in Hilbert space, we describe for the first time the essential role of permanent dipole moments in the femtosecond dynamics of vibrational polariton wavepackets. We classify molecules into three general families according to the shape of their electric dipole function d(e)(q) along the vibrational mode coordinate q. For polar species with a positive slope of the dipole function at equilibrium, an initial diabatic light-matter product state without vibrational or cavity excitations evolves into a polariton wavepacket with a large number of intracavity photons for interaction strengths at the conventional onset of ultrastrong coupling. This buildup of the cavity photon amplitude is accompanied by an effective lengthening of the vibrational mode that is comparable with a laser-induced vibrational excitation in free space. In contrast, polar molecules with a negative slope of the dipole function experience an effective mode shortening, under equivalent coupling conditions. We validate our predictions using realistic ab initio ground state potentials and dipole functions for HF and CO2 molecules. We also propose a non-adiabatic state preparation scheme to generate vibrational polaritons with molecules near infrared nanoantennas for the spontaneous radiation of infrared quantum light.
机译:振动强耦合作为操纵红外空腔中分子反应性的有希望的途径。我们开发了一种全量子方法,以研究与量化红外腔场相互作用的单一Anharmonic振动模式的单一动态。通过比较Hilbert Space的问题的岩性摩尔斯振荡器的多配置时间依赖的Hartree模拟,我们首次描述了振动极化振动波动的飞秒动态中永久偶极矩的基本作用。我们根据沿着振动模式坐标Q的电偶极子功能D(e)(e)(e)(q)的形状将分子分为三个一般家族。对于具有偶极斜率的极性物质,在平衡下,没有振动或腔激励的初始型式淡出产品状态在具有大量腔内光子的极性孔波袋中,用于在传统的超字耦合开始处的相互作用强度。腔光子幅度的这种堆积伴随着振动模式的有效延长,该振动模式与自由空间中的激光诱导的振动激发相当。相反,在等效耦合条件下,具有偶极子功能的负斜率的极性分子经历有效模式缩短。我们使用逼真的AB Initio地电电位和偶极功能来验证我们的预测,用于HF和CO2分子。我们还提出了一种非绝热状态制备方案,以产生具有近红外纳米环绕的分子的振动极性官,用于红外量子光的自发辐射。

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