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Different emissive states in the bulk and at the surface of methylammonium lead bromide perovskite revealed by two-photon micro-spectroscopy and lifetime measurements
Author(s) -
Khadga Jung Karki,
Mohamed Abdellah,
Wei Zhang,
Tönu Pullerits
Publication year - 2016
Publication title -
apl photonics
Language(s) - English
Resource type - Journals
ISSN - 2378-0967
DOI - 10.1063/1.4948645
Subject(s) - exciton , photoluminescence , photovoltaics , perovskite (structure) , materials science , spectroscopy , optoelectronics , charge carrier , band gap , molecular physics , atomic physics , chemistry , condensed matter physics , physics , photovoltaic system , crystallography , ecology , biology , quantum mechanics
Two photon photoluminescence (2PPL) from single crystals of methyl ammonium lead bromide (CH3NH3PbBr3, MAPbBr3) is studied. We observe two components in the 2PPL spectra, which we assign to the photoluminescence (PL) from the carrier recombination at the band edge and the recombination due to self-trapping of excitons. The PL Stokes shift of self-trapped excitons is about 100 meV from the band-gap energy. Our measurements show that about 15% of the total PL from regions about 40 μm deep inside the crystal is due to the emission from self-trapped exciton. This contribution increases to about 20% in the PL from the regions close to the surface. Time resolved measurements of 2PPL show that the PL due to band-edge recombination has a life time of about 8 ns while the PL lifetime of self-trapped excitons is in the order of 100 ns. Quantification of self-trapped excitons in the materials used in photovoltaics is important as such excitons hinder charge separation. As our results also show that an appreciable fraction of photo-generated carriers get trapped, the results are important in rational design of photovoltaics. On the other hand, our results also show that the self-trapped excitons broaden the emission spectrum, which may be useful in designing broadband light emitting devices

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