2022
DOI: 10.3390/nano12234300
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Photon-Energy-Dependent Reversible Charge Transfer Dynamics of Double Perovskite Nanocrystal-Polymer Nanocomposites

Abstract: Combining steady-state photoluminescence and transient absorption (TA) spectroscopy, we have investigated the photoinduced charge transfer dynamics between lead-free Mn-doped Cs2NaIn0.75Bi0.25Cl6 double perovskite (DP) nanocrystals (NCs) and conjugated poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylenevinylene] (MDMO-PPV). Upon ultraviolet-A excitation, the photoinduced absorption feature of DP NCs/MDMO-PPV nanocomposites disappeared, and the stimulated emission weakened in the TA spectrum. This was due t… Show more

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Cited by 3 publications
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“…In order to avoid interference, the TA kinetics at 440 and 570 nm had been considered as the intrinsic state and defect state in TA experiment. TA kinetic containing both SE and PIA features can be well fitted by the following biexponent decay formula 39 (2)…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…In order to avoid interference, the TA kinetics at 440 and 570 nm had been considered as the intrinsic state and defect state in TA experiment. TA kinetic containing both SE and PIA features can be well fitted by the following biexponent decay formula 39 (2)…”
Section: Resultsmentioning
confidence: 99%
“…In order to avoid interference, the TA kinetics at 440 and 570 nm had been considered as the intrinsic state and defect state in TA experiment. TA kinetic containing both SE and PIA features can be well fitted by the following biexponent decay formula f ( t ) = f 0 + p 1 exp ( t / τ PIA ) p 2 exp ( t / τ SE ) where τ PIA and τ SE were their lifetimes, and p 1 and p 2 were the corresponding weight factors, respectively. The single exponential decay function can be used to better fit the SE feature with only p 1 = 0.…”
Section: Resultsmentioning
confidence: 99%