André Niebur, Eugen Klein, Rostyslav Lesyuk, Christian Klinke, Jannika Lauth
{"title":"Understanding the Optoelectronic Processes in Colloidal 2D Multi-Layered MAPbBr3 Perovskite Nanosheets: Funneling, Recombination and Self-Trapped Excitons","authors":"André Niebur, Eugen Klein, Rostyslav Lesyuk, Christian Klinke, Jannika Lauth","doi":"arxiv-2408.04571","DOIUrl":null,"url":null,"abstract":"Quasi two-dimensional (2D) colloidal synthesis made quantum confinement\nreadily accessible in perovskites, generating additional momentum in perovskite\nLED research and lasing. Ultrathin perovskite layers exhibit high exciton\nbinding energies and beneficial charge transport properties interesting for\nsolar cells. In 2D perovskites, the combination of layers with different\nthickness helps to direct charge carriers in a targeted manner toward thicker\nlayers with a smaller bandgap. However, detailed knowledge about the mechanisms\nby which excitons and charge carriers funnel and recombine in these structures\nis lacking. Here, we characterize colloidal 2D methylammonium lead bromide\n(MAPbBr3) Ruddlesden-Popper perovskites with a broad combination of layers (n =\n3 to 10, and bulk fractions with n > 10) in one stack by femtosecond transient\nabsorption spectroscopy and time-resolved photoluminescence, which gives\ncomprehensive insights into the complexity of funneling and recombination\nprocesses. We find that after photoexcitation second- and third-order processes\ndominate in MAPbBr3 nanosheets, which indicates exciton-exciton annihilation\n(EEA) and Auger recombination. Long-lived excitons in thin layers (e.g., n = 5,\nEb = 136 meV) funnel into high n with t = 10-50 ps, which decreases their\nexciton binding energy below kB T = 26 meV ( T = 300K) and leads to radiative\nrecombination. Parallel and consecutive funneling compete with exciton trapping\nprocesses, making funneling an excellent tool to overcome exciton self-trapping\nwhen high-quality n-n interfaces are present. Free charge carriers in high n\nregions on the other hand facilitate radiative recombination and EEA is\nbypassed, which is desirable for LED and lasing applications.","PeriodicalId":501304,"journal":{"name":"arXiv - PHYS - Chemical Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-08-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chemical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.04571","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
Quasi two-dimensional (2D) colloidal synthesis made quantum confinement
readily accessible in perovskites, generating additional momentum in perovskite
LED research and lasing. Ultrathin perovskite layers exhibit high exciton
binding energies and beneficial charge transport properties interesting for
solar cells. In 2D perovskites, the combination of layers with different
thickness helps to direct charge carriers in a targeted manner toward thicker
layers with a smaller bandgap. However, detailed knowledge about the mechanisms
by which excitons and charge carriers funnel and recombine in these structures
is lacking. Here, we characterize colloidal 2D methylammonium lead bromide
(MAPbBr3) Ruddlesden-Popper perovskites with a broad combination of layers (n =
3 to 10, and bulk fractions with n > 10) in one stack by femtosecond transient
absorption spectroscopy and time-resolved photoluminescence, which gives
comprehensive insights into the complexity of funneling and recombination
processes. We find that after photoexcitation second- and third-order processes
dominate in MAPbBr3 nanosheets, which indicates exciton-exciton annihilation
(EEA) and Auger recombination. Long-lived excitons in thin layers (e.g., n = 5,
Eb = 136 meV) funnel into high n with t = 10-50 ps, which decreases their
exciton binding energy below kB T = 26 meV ( T = 300K) and leads to radiative
recombination. Parallel and consecutive funneling compete with exciton trapping
processes, making funneling an excellent tool to overcome exciton self-trapping
when high-quality n-n interfaces are present. Free charge carriers in high n
regions on the other hand facilitate radiative recombination and EEA is
bypassed, which is desirable for LED and lasing applications.