Posmyk Katarzyna, Dyksik Mateusz, Surrente Alessandro, Zalewska Katarzyna, Śmiertka Maciej, Cybula Ewelina, Paritmongkol Watcharaphol, Tisdale William A, Plochocka Paulina, Baranowski Michał
Department of Experimental Physics, Faculty of Fundamental Problems of Technology, Wroclaw University of Science and Technology, 50-370 Wroclaw, Poland.
Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA.
Nanomaterials (Basel). 2023 Mar 21;13(6):1119. doi: 10.3390/nano13061119.
Two-dimensional van der Waals materials exhibit particularly strong excitonic effects, which causes them to be an exceptionally interesting platform for the investigation of exciton physics. A notable example is the two-dimensional Ruddlesden-Popper perovskites, where quantum and dielectric confinement together with soft, polar, and low symmetry lattice create a unique background for electron and hole interaction. Here, with the use of polarization-resolved optical spectroscopy, we have demonstrated that the simultaneous presence of tightly bound excitons, together with strong exciton-phonon coupling, allows for observing the exciton fine structure splitting of the phonon-assisted transitions of two-dimensional perovskite (PEA)2PbI4, where PEA stands for phenylethylammonium. We demonstrate that the phonon-assisted sidebands characteristic for (PEA)2PbI4 are split and linearly polarized, mimicking the characteristics of the corresponding zero-phonon lines. Interestingly, the splitting of differently polarized phonon-assisted transitions can be different from that of the zero-phonon lines. We attribute this effect to the selective coupling of linearly polarized exciton states to non-degenerate phonon modes of different symmetries resulting from the low symmetry of (PEA)2PbI4 lattice.
二维范德华材料表现出特别强的激子效应,这使其成为研究激子物理的一个极其有趣的平台。一个显著的例子是二维Ruddlesden-Popper钙钛矿,其中量子和介电限制与柔软、极性和低对称性晶格共同为电子和空穴相互作用创造了独特的背景。在这里,通过使用偏振分辨光谱,我们证明了紧密束缚激子的同时存在以及强激子-声子耦合,使得能够观察到二维钙钛矿(PEA)2PbI4(其中PEA代表苯乙铵)的声子辅助跃迁的激子精细结构分裂。我们证明,(PEA)2PbI4特有的声子辅助边带被分裂且呈线性偏振,模仿了相应零声子线的特征。有趣的是,不同偏振的声子辅助跃迁的分裂可能与零声子线的分裂不同。我们将这种效应归因于(PEA)2PbI4晶格的低对称性导致线性偏振激子态与不同对称性的非简并声子模式的选择性耦合。