“…[ 135 ] Achieving multiple functions of morphology optimization, surface passivation, and moisture resistance, conjugated polymer materials have significant potential to become a facile and universal strategy to enhance device performance and long‐term stability. [ 136–138 ]…”
Figure 3. The impact of MABr treatment on the scanning electron microscopy (SEM) images of film morphology (MAPbI 3 films a) without and b) with MABr treatment), c) ultraviolet-visible (UV-vis) absorption spectra, and d) XRD patterns of the perovskite films. Reproduced with permission. [61] Copyright 2016, Springer Nature. e) Schematic illustration and f) SEM images of the molecule-passivated RP/3D heterostructure. Reproduced with permission. [115] Copyright 2018, Royal Society of Chemistry. g) Schematic representation of the 1D/3D heterostructure evidenced by solid-state NMR proximity measurements. Reproduced with permission. [40] Copyright 2019, Springer Nature. h) Secondary-ion mass spectrometry (SIMS) measurement of interdiffusion-grown MAPbI 3 films on indium tin oxide (ITO) glass. Reproduced with permission.
“…[ 135 ] Achieving multiple functions of morphology optimization, surface passivation, and moisture resistance, conjugated polymer materials have significant potential to become a facile and universal strategy to enhance device performance and long‐term stability. [ 136–138 ]…”
Figure 3. The impact of MABr treatment on the scanning electron microscopy (SEM) images of film morphology (MAPbI 3 films a) without and b) with MABr treatment), c) ultraviolet-visible (UV-vis) absorption spectra, and d) XRD patterns of the perovskite films. Reproduced with permission. [61] Copyright 2016, Springer Nature. e) Schematic illustration and f) SEM images of the molecule-passivated RP/3D heterostructure. Reproduced with permission. [115] Copyright 2018, Royal Society of Chemistry. g) Schematic representation of the 1D/3D heterostructure evidenced by solid-state NMR proximity measurements. Reproduced with permission. [40] Copyright 2019, Springer Nature. h) Secondary-ion mass spectrometry (SIMS) measurement of interdiffusion-grown MAPbI 3 films on indium tin oxide (ITO) glass. Reproduced with permission.
“…Figure 1a shows the structure of PTAA/FAPbI 3 /TiO 2 sample, where the thickness of the ETL TiO 2 , the light harvester layer FAPbI 3 PQDs, and the HTL PTAA doped by tris(pentafluorophenyl)borane is~50 nm,~160 nm, and~40 nm, respectively. As shown in Figure 1b [25,33,34], respectively, which are in favor of the charge transfer. From the TEM image of the pure FAPbI 3 PQDs (Figure 1c), we found the PQDs have an average size of about 15 nm.…”
Section: Methodsmentioning
confidence: 87%
“…The FAPbI 3 PQDs were synthesized according to the recent report [25]. For fabrication of the PTAA/FAPbI 3 /TiO 2 sample, a 50 nm compact hydrothermal TiO 2 layer was deposited above the quartz substrate.…”
Section: Methodsmentioning
confidence: 99%
“…Compared with MAPbI 3 , FAPbI 3 is superior in light absorption characteristics [17][18][19][20][21] and thermal stability [21,22]. In particular, FAPbI 3 can be fabricated as quantum dots (QDs) which possess proper phase structure and crystalline orientation without the need of high temperature annealing [23][24][25]. Relative to bulk or thin-film perovskite materials, perovskite QDs (PQDs) possess high crystallinity during synthesis and exhibit unique features such as tunable bandgaps [26,27] and high quantum yield [28][29][30][31], which contribute to PV applications.…”
Section: Introductionmentioning
confidence: 99%
“…Relative to bulk or thin-film perovskite materials, perovskite QDs (PQDs) possess high crystallinity during synthesis and exhibit unique features such as tunable bandgaps [26,27] and high quantum yield [28][29][30][31], which contribute to PV applications. The corresponding PSCs made of FAPbI 3 PQDs have been demonstrated to exhibit reasonable high PCEs [25,32]. However, the investigation of CT processes to reveal the intrinsic transfer time and efficiency is still lacking, which hinders the clarification of the important factors limiting the PCEs.…”
In this work, the ultrafast transient absorption spectroscopy (TAs) was utilized to first investigate the charge transfer from the emerging FAPbI3 (FA = CH(NH2)2) perovskite quantum dots (PQDs) to charge transport layers. Specifically, we compared the TAs in pure FAPbI3 PQDs, PQDs grown with both electron and hole transfer layers (ETL and HTL), and PQDs with only ETL or HTL. The TA signals induced by photoexcited electrons decay much faster in PQDs samples with the ETL (~20 ps) compared to the pure FAPbI3 PQDs (>1 ns). These results reveal that electrons can effectively transport between coupled PQDs and transfer to the ETL (TiO2) at a time scale of 20 ps, much faster than the bimolecular charge recombination inside the PQDs (>1 ns), and the electron transfer efficiency is estimated to be close to 100%. In contrast, the temporal evolution of the TA signals in the PQDs with and without HTL exhibit negligible change, and no substantive hole transfer to the HTL (poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine], PTAA) occurs within 1 ns. The much slower hole transfer implies the further potential of increasing the overall photo-carrier conversion efficiency through enhancing the hole diffusion length and fine-tuning the coupling between the HTL and PQDs.
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