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arXiv 2304.02461cond-mat.mtrl-sciphysics.chem-ph
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Ruddlesden-Popper 碘化锡中的多激子量子动力学

Many-Exciton Quantum Dynamics in a Ruddlesden-Popper Tin Iodide

Esteban Rojas Gatjens, Hao Li, Alejandro Vega Flick, Daniele Cortecchia, Annamaria Petrozza, Eric R. Bittner, Ajay Ram Srimath Kandada, Carlos Silva Acuña

AI总结:

本研究利用相干二维电子光谱,揭示了锡基与铅基Ruddlesden-Popper金属卤化物在激子量子动力学上的显著差异,发现锡基材料因晶格静态无序导致激子局域化,具有更高的EID速率及特有的低结合能双激子态。

摘要:

我们利用相干二维电子光谱学,研究了原型 Ruddlesden-Popper 金属卤化物(RPMH),即 \ce{(PEA)2SnI4}(PEA = phenylethylammine)中的多体激子相互作用。在这些系统中观察到的三阶极化的光学退相干时间由激子多体相互作用和晶格涨落决定。我们研究了激发诱导退相干(EID),并观察到与之前报道的铅类似物 \ce{(PEA)2PbI4} 相比,随着激发密度的增加,其对退相干时间的贡献显著减少。令人惊讶的是,我们发现 \ce{(PEA)2SnI4} 中的 EID 相互作用参数比 \ce{(PEA)2PbI4} 高出四个数量级。EID 速率的增加可能是由于锡衍生物中更强烈的静态无序晶格引起的激子局域化。多个间距紧密的激子态的观察,以及随着布居时间增加谱线宽度的展宽(光谱扩散),支持了这一观点,这表明相对于高度动态的铅卤化物,其具有静态无序结构。此外,我们发现激子非线性相干线型显示了在铅系统中未观察到的低结合能(<10\\,meV)双激子态的证据。我们基于随机散射理论对线型进行了建模,该理论考虑了与非稳态暗背景激子布居的相互作用。我们的研究提供了锡基和铅基 RPMHs 之间激子量子动力学差异的证据,并将它们与激子-激子相互作用强度和晶体结构的静态无序方面联系起来。

英文摘要:

We present a study on the many-body exciton interactions in a prototype Ruddlesden-Popper metal halide (RPMH), namely \ce{(PEA)2SnI4} (PEA = phenylethylammine), using coherent two-dimensional electronic spectroscopy. The optical dephasing times of the third-order polarization observed in these systems are determined by exciton many-body interactions and lattice fluctuations. We investigate the excitation-induced dephasing (EID) and observe a significant reduction of the contribution to the dephasing time with increasing excitation density as compared to its lead counterpart \ce{(PEA)2PbI4}, which we have previously reported [A.~R.~Srimath~Kandada~\textit{et~al.}, J.\ Chem.\ Phys.\ \textbf{153}, 164706 (2020)]. Surprisingly, we find that the EID interaction parameter is four orders of magnitude higher in \ce{(PEA)2SnI4} than that in \ce{(PEA)2PbI4}. This increase in the EID rate may be due to exciton localization arising from a more strongly statically disordered lattice in the tin derivative. This is supported by the observation of multiple closely spaced exciton states and the broadening of the linewidth with increasing population time (spectral diffusion), which suggests a static disordered structure relative to the highly dynamic lead-halide. Additionally, we find that the exciton nonlinear coherent lineshape shows evidence of a biexcitonic state with low binding energy ($<10$\,meV) not observed in the lead system. We model the lineshapes based on a stochastic scattering theory that accounts for the interaction with a non-stationary population of dark background excitations. Our study provides evidence of differences in the exciton quantum dynamics between tin- and lead-based RPMHs and links them to the exciton-exciton interaction strength and the static disorder aspect of the crystalline structure.

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