2017
DOI: 10.1039/c6cp08770a
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Do grain boundaries dominate non-radiative recombination in CH3NH3PbI3perovskite thin films?

Abstract: Here, we examine grain boundaries (GBs) with respect to non-GB regions (grain surfaces (GSs) and grain interiors (GIs)) in high-quality micrometer-sized perovskite CHNHPbI (or MAPbI) thin films using high-resolution confocal fluorescence-lifetime imaging microscopy in conjunction with kinetic modeling of charge-transport and recombination processes. We show that, contrary to previous studies, GBs in our perovskite MAPbI thin films do not lead to increased recombination but that recombination in these films hap… Show more

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Cited by 168 publications
(189 citation statements)
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“…As a result, the grain size and compactness of the MAPbI 3 film are improved after solvent annealing, which is consisted with the film morphology. Compact films with larger grain sizes decrease the number of grain boundaries and density of defects, which are favorable to improve the photovoltaic performance . In addition, ZnO nanorods passivated with a thin Al 2 O 3 layer improve charge collection in the PSCs, which is confirmed by the transient PL spectra of different perovskite films and J – V curves shown in Figure k,l.…”
Section: Pscs With Zno Nanorods Etmsmentioning
confidence: 63%
“…As a result, the grain size and compactness of the MAPbI 3 film are improved after solvent annealing, which is consisted with the film morphology. Compact films with larger grain sizes decrease the number of grain boundaries and density of defects, which are favorable to improve the photovoltaic performance . In addition, ZnO nanorods passivated with a thin Al 2 O 3 layer improve charge collection in the PSCs, which is confirmed by the transient PL spectra of different perovskite films and J – V curves shown in Figure k,l.…”
Section: Pscs With Zno Nanorods Etmsmentioning
confidence: 63%
“…This points to GBs either efficiently mediating nonradiative recombination or that charge carriers are simply deflected, which has been previously proposed. [ 5,44 ] As the focused excitation remains, we observe similar spatial redistribution of PL to what occurs in the single crystal (see Video S3 in the Supporting Information), establishing the light‐induced ionic defect migration. As the excitation is switched back to defocused mode (PL 1 ), we can confirm that PL remains significantly reduced exclusively for the grain that is excited (Figure 3c).…”
Section: Resultsmentioning
confidence: 99%
“…Interestingly, when the DS additive was used under the same conditions, the J sc , V oc , and FF increase to 22.48 mA cm −2 , 1.103 V, and 0.742, respectively, yielding a PCE as high as 18.40%, the highest reported so far for F‐PSCs. The significantly larger J sc and FF are attributed to good crystallinity and large grain size, resulting in effective charge transport and less carrier recombination at grain boundaries . We fabricated MAPbI 3 –DS solar cells on both flexible and rigid substrates using identical condition, including the spin‐coating procedure, annealing temperature and time, etc.…”
Section: The Key J–v Parameters Of the F‐pscsmentioning
confidence: 99%