TY - JOUR
T1 - Effect of synthesis methods on photoluminescent properties for CsPbBr3 nanocrystals
T2 - Hot injection method and conversion method
AU - Zhang, Fengying
AU - Chen, Junsheng
AU - Zhou, Ying
AU - He, Rongxing
AU - Zheng, Kaibo
PY - 2020
Y1 - 2020
N2 - Multiple facile synthetic strategies for all inorganic perovskite CsPbBr3 nanocrystals (NCs) have been established and developed, profiting from their excellent performance and great potential applied in the field of photonic and optoelectronic. Here, CsPbBr3 NCs were synthesized by both hot injection method (method 1) and conversion method (method 2), and the discrepancy of their photophysical properties is elucidated via the complementary studies between time-resolved photoluminescence (TRPL) and transient-absorption (TA) spectroscopy. We found that CsPbBr3 NCs prepared by conversion method exhibited lower PL quantum yield (QY), which was ascribed to the larger partition of the NCs being passivated from the quenchers from the deep trap states. On the other hand, we also observed different radiative recombination rates between two samples which should be due to various trapping/detrapping times prior to the radiative recombination of the charge carriers in two samples. These results provide better guidance for the development and improvement of synthesis methodology for perovskite NCs.
AB - Multiple facile synthetic strategies for all inorganic perovskite CsPbBr3 nanocrystals (NCs) have been established and developed, profiting from their excellent performance and great potential applied in the field of photonic and optoelectronic. Here, CsPbBr3 NCs were synthesized by both hot injection method (method 1) and conversion method (method 2), and the discrepancy of their photophysical properties is elucidated via the complementary studies between time-resolved photoluminescence (TRPL) and transient-absorption (TA) spectroscopy. We found that CsPbBr3 NCs prepared by conversion method exhibited lower PL quantum yield (QY), which was ascribed to the larger partition of the NCs being passivated from the quenchers from the deep trap states. On the other hand, we also observed different radiative recombination rates between two samples which should be due to various trapping/detrapping times prior to the radiative recombination of the charge carriers in two samples. These results provide better guidance for the development and improvement of synthesis methodology for perovskite NCs.
KW - Perovskite nanoparticles
KW - Radiative recombination
KW - Synthetic strategy
KW - Trap states
U2 - 10.1016/j.jlumin.2019.117023
DO - 10.1016/j.jlumin.2019.117023
M3 - Journal article
AN - SCOPUS:85077374159
SN - 0022-2313
VL - 220
JO - Journal of Luminescence
JF - Journal of Luminescence
M1 - 117023
ER -