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Spray-driven halide exchange in solid-state CsPbX 3 nanocrystal films.

R I Sánchez-AlarcónJ Noguera-GomezVladimir S ChirvonyH Pashaei AdlPablo P BoixG Alarcón-FloresJuan P Martínez-PastorR Abargues
Published in: Nanoscale (2022)
CsPbI 3 perovskite nanocrystals (NCs) are promising building blocks for photovoltaics and optoelectronics. However, they exhibit an essential drawback in the form of phase stability: α-phase, with a ∼1.80 eV bandgap, can easily experience a phase transition to a non-radiative orthorhombic δ-phase in an ambient environment. This leads to the need to carry out the CsPbI 3 -based device fabrication in an inert atmosphere, which is technologically inconvenient and expensive. One of the most successful approaches proposed to overcome this problem is synthesizing mixed halide CsPbBr 3- x I x NCs to improve the stability of the α-phase perovskite structure. However, the formation of high-quality thin films of CsPbBr 3- x I x NCs with high PLQY is challenging owing to the degradation of their optical properties after deposition on a substrate. This work presents spray coating to carry out a solid-state anion exchange in CsPbBr 3 NCs thin films at ambient conditions with low-demanding reaction conditions. This constitutes a novel open-air and annealing-free technology to manufacture CsPbBr 3- x I x NC thin films with high optical quality and record high photoluminescence quantum yields (PLQY) based on spray-driven halide (Br - to I - ) anion exchange in a solid-state phase. Besides, tunable emission wavelengths between 520 and 670 nm can be obtained from CsPbBr 3- x I x NC films using accurate tuning volumes of HI solution sprayed over the initial surface of CsPbBr 3 film to provide the halide exchange. The optical quality of the halide-exchanged PNCs films remains practically identical to that of initial Br-containing layers, with a remarkable PLQY enhancement after anion exchange, from ∼61% for CsPbBr 3 thin films emitting at 520 nm to ∼84% for mixed halide CsPbBr 3- x I x film emitting at 640 nm. The huge potential of the system is confirmed by demonstrating a low-threshold amplified spontaneous emission.
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