Karunanantharajah Prashanthan, I. Levine, Emilio Gutiérrez-Partida, A. Musiienko, H. Hempel, K. Lips, T. Unold, M. Stolterfoht, T. Dittrich, Rowan W. MacQueen
{"title":"Carrier Dynamics in Upconverting Thin Film Perovskite/Rubrene Bilayers Studied by Combined Surface Photovoltage and Photoluminescence","authors":"Karunanantharajah Prashanthan, I. Levine, Emilio Gutiérrez-Partida, A. Musiienko, H. Hempel, K. Lips, T. Unold, M. Stolterfoht, T. Dittrich, Rowan W. MacQueen","doi":"10.29363/nanoge.hopv.2022.063","DOIUrl":null,"url":null,"abstract":"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,","PeriodicalId":128519,"journal":{"name":"Proceedings of the International Conference on Hybrid and Organic Photovoltaics","volume":"83 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-04-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the International Conference on Hybrid and Organic Photovoltaics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.29363/nanoge.hopv.2022.063","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
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,