2022
DOI: 10.1016/j.cej.2021.133373
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Colorful, time-dependent carbon dot-based afterglow with ultralong lifetime

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Cited by 55 publications
(40 citation statements)
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“…The RTP of P3CA@BA has no excitation wavelength-dependent characteristics, indicating that the composite has only a single emission center, which is different from B-doped carbon dots. [45][46][47][48] In addition, Figure S17 shows two excited peaks at 263 and nm contributing to the RTP emission of P3CA@BA at 408 nm, which is in agreement with the absorption peaks of P3CA. Consequently, it can be concluded that the persistent RTP of P3CA@BA mainly comes from the excitation of the guest molecule itself, followed by the decay process: ISC of singlet excitons, and radiative transition of triplet excitons (Figure S18).…”
Section: Methodssupporting
confidence: 79%
“…The RTP of P3CA@BA has no excitation wavelength-dependent characteristics, indicating that the composite has only a single emission center, which is different from B-doped carbon dots. [45][46][47][48] In addition, Figure S17 shows two excited peaks at 263 and nm contributing to the RTP emission of P3CA@BA at 408 nm, which is in agreement with the absorption peaks of P3CA. Consequently, it can be concluded that the persistent RTP of P3CA@BA mainly comes from the excitation of the guest molecule itself, followed by the decay process: ISC of singlet excitons, and radiative transition of triplet excitons (Figure S18).…”
Section: Methodssupporting
confidence: 79%
“…The RTP of P3CA@BA has no excitation wavelength-dependent characteristics, indicating that the composite has only a single emission center, which is different from B-doped carbon dots. [45][46][47][48] In addition, Figure S17 shows two excited peaks at 263 and 299 nm contributing to the RTP emission of P3CA@BA at 408 nm, which is in agreement with the absorption peaks of P3CA. Consequently, it can be concluded that the persistent RTP of P3CA@BA mainly comes from the excitation of the guest molecule itself, followed by the decay process: ISC of singlet excitons, and radiative transition of triplet excitons (Figure S18).…”
Section: Zuschriftensupporting
confidence: 79%
“…C–B bonds can effectively decrease the Δ E ST value, promoting a reverse intersystem crossover (RISC) from the triplet state (T 1 ) to the lowest singlet state (S 1 ) . This indicates that, in comparison with GQDs 2 -6/PVA, GQDs 2 -6/B 2 O 3 composites are more likely to have effective ISC, exhibiting a longer phosphorescent life . The GQDs 2 -6/B 2 O 3 composite shows an excitation-wavelength-independent fluorescence characteristic with a maximum emission at 412 nm (Figure j); for the phosphorescent spectra in Figure k, excitation-independent afterglow emission peaks can be ascribed to the RTP emission, confirming the afterglow is due to RTP, not a thermally activated delayed fluorescence (TADF).…”
Section: Results and Discussionmentioning
confidence: 99%