表面光电压与光致发光联合研究钙钛矿/Rubrene双层薄膜上转换载流子动力学

Karunanantharajah Prashanthan, I. Levine, Emilio Gutiérrez-Partida, A. Musiienko, H. Hempel, K. Lips, T. Unold, M. Stolterfoht, T. Dittrich, Rowan W. MacQueen
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引用次数: 0

摘要

典型的钙钛矿驱动光子上转换器由卤化铅钙钛矿薄膜和小分子半导体湮灭剂(如rubrene)层合而成。这些系统表现出从近红外到可见光谱的三重态-三重态湮灭上转换,其中钙钛矿膜作为三重态增敏剂,而rubrene层作为湮灭剂和发射器[1,2]。这种上转换器的一个关键特征是,它去除了传统的激子三重态敏化剂,并用大块半导体薄膜的界面代替它,将钙钛矿中的自由电子和空穴转化为有机湮灭膜内的强束缚电子-空穴对(即激子)。该工艺是卤化铅钙钛矿在光伏领域之外的一种新兴应用,在光子学作用和混合半导体界面能量传导的基础研究方面都很有趣。本研究旨在利用瞬态表面光电压和光致发光方法的结合,对这些钙钛矿上转换器系统产生新的见解。瞬态表面光电压测量由短激光脉冲激发后载流子扩散、捕获和复合而产生的半导体薄膜堆的瞬态电极化。因此,它提供了洞察整个样品的净电荷分布以及各种载流子转移和重组过程的速率。光致发光,
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Carrier Dynamics in Upconverting Thin Film Perovskite/Rubrene Bilayers Studied by Combined Surface Photovoltage and Photoluminescence
A typical perovskite-driven photon upconverter consists of lead halide perovskite thin film layered with a small molecule semiconductor annihilator, such as rubrene. These systems exhibit triplet-triplet annihilation upconversion from the near-infrared to the visible spectrum, with the perovskite film acting as a triplet sensitizer while the rubrene layer functions as the annihilator and emitter [1, 2]. A key feature of this style of upconverter, which removes the conventional excitonic triplet sensitizer and replaces it with the interface of a bulk semiconductor film, is the conversion of free electrons and holes in the perovskite into strongly-bound electron-hole pairs (i.e. excitons) within the organic annihilator film. The process is an emerging application of lead halide perovskite beyond the photovoltaics space, and is interesting both in a photonics role, and as a fundamental investigation into energy transduction at hybrid semiconductor interfaces. This study aims to generate new insights into these perovskite upconverter systems using a combination of transient surface photovoltage and photoluminescence methods. Transient surface photovoltage measures the transient electrical polarization across a semiconductor film stack resulting from carrier diffusion, trapping and recombination following excitation by a short laser pulse. As such, it offers insight into the net charge distribution throughout the sample as well as the rates of various carrier transfer and recombination processes. Photoluminescence,
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