In this work, bromide ions (Br–) on
the conjugated
polyelectrolytes (CPEs) were converted to tetrafluoroborate (BF4
–) or hexafluorophosphate (PF6
–) ions through anion exchange. The three CPEs
(PFN-Br, PFN-BF4, and PFN-PF6) were utilized
solely for surface modification of zinc oxide nanocrystals (ZnO NCs).
The ionic groups on CPEs can form permanent dipoles to facilitate
charge injection from ZnO NCs to cesium lead bromide (CsPbBr3) NC emitters, therefore promoting luminescent properties of inverted
perovskite light-emitting diodes (PeLEDs). The experimental results
reveal that ZnO NC films were smoothened by CPEs that allowed flat
deposition of the perovskite active layers; moreover, the improved
contact between ZnO and perovskite layers was beneficial for reducing
leakage current, as verified in the dark current measurement of devices.
In addition, the incorporation of CPEs helped to passivate the defects
of ZnO NC films and prolong the carrier lifetime of CsPbBr3 NCs. PeLEDs based on different CPEs were then constructed and evaluated.
The device based on PFN-Br showed the highest brightness and current
efficiency, and the one based on PFN-BF4 exhibited better
current efficiency over PFN-Br under the low current density below
160 mA/cm2. This is the first report using fluorene-based
CPEs with Br–, BF4
–, or PF6
– groups to modify the properties
of ZnO and CsPbBr3 NCs for the construction of inverted
PeLEDs so far. Our experiments explored new kinds of CPEs on the surface
modification of ZnO NCs and device performance of PeLEDs.
Hole transport layers (HTLs) with high conductivity, charge extraction ability, and carrier transport capability are highly important for fabricating perovskite solar cells (PSCs) with high power conversion efficiency and device stability. Low interfacial recombination between the HTL and perovskite absorber is also crucial to the device performance of PSCs. In this work, we developed a three-stage method to prepare NiOx nanoflakes as the HTL in the inverted PSCs. Due to the addition of the nanoflake layer, the deposited perovskite films with larger grain sizes and fewer boundaries were obtained, implying higher photogenerated current and fill factors in our PSCs. Meanwhile, the downshifted valence band of the NiOx HTL improved hole extraction from the perovskite absorber and open-circuit voltages of PSCs. The optimized device based on the NiOx nanoflakes showed the highest efficiency of 14.21% and a small hysteresis, which outperformed the NiOx thin film as the HTL. Furthermore, the device maintained 83% of its initial efficiency after 60 days of storage. Our results suggest that NiOx nanoflakes provide great potential for constructing PSCs with high efficiency and long-term stability.
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