Li Tao E
Department of Physics and Astronomy, University of Delaware, Newark, Delaware 19716, USA.
J Chem Phys. 2024 Aug 14;161(6). doi: 10.1063/5.0209212.
Vibrational polaritons form in a planar Fabry-Pérot microcavity when a vibrational mode of a layer of molecules is near resonant with an infrared cavity mode. Here, dispersion relations of vibrational polaritons are studied when the molecular density distribution breaks the macroscopic translational symmetry along the cavity mirror plane. Both perturbative theory and numerical calculations show that, if a homogeneous in-plane molecular distribution is modulated by sinusoidal fluctuations, in addition to a pair of upper and lower polariton branches, a discrete number of side polariton branches may emerge in the polariton dispersion relation. Moreover, for a periodic Gaussian in-plane density distribution, only two, yet significantly broadened polariton branches exist in the spectra. This polariton linewidth broadening is caused by the scattering between cavity modes at neighboring in-plane frequencies due to the symmetry breaking, which is distinguished from known origins of polariton broadening such as the homogeneous broadening of molecules, the cavity loss, or the large energetic disorder of molecules. Associated with the broadened polariton branches, under the periodic Gaussian in-plane inhomogeneity, a significant number of the vibrational strong coupling eigenstates contain a non-zero contribution from the cavity photon mode at zero in-plane frequency, blurring the distinction between the bright and the dark modes. Looking forward, our theoretical investigation should facilitate the experimental exploration of vibrational polaritons with patterned in-plane molecular density distributions.
当分子层的振动模式与红外腔模接近共振时,振动极化激元在平面法布里 - 珀罗微腔中形成。在此,研究了分子密度分布沿腔镜平面破坏宏观平移对称性时振动极化激元的色散关系。微扰理论和数值计算均表明,如果均匀的面内分子分布受到正弦波动调制,那么除了一对上下极化激元分支外,在极化激元色散关系中可能会出现离散数量的侧极化激元分支。此外,对于周期性高斯面内密度分布,光谱中仅存在两个但显著展宽的极化激元分支。这种极化激元线宽展宽是由于对称性破缺导致相邻面内频率处的腔模之间的散射引起的,这与已知的极化激元展宽起源不同,如分子的均匀展宽、腔损耗或分子的大能量无序。与展宽的极化激元分支相关,在周期性高斯面内不均匀性下,大量的振动强耦合本征态在零面内频率处包含来自腔光子模的非零贡献,模糊了亮模和暗模之间的区别。展望未来,我们的理论研究应有助于对具有图案化面内分子密度分布的振动极化激元进行实验探索。