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. 2021 Mar 24;15(4):7216–7225. doi: 10.1021/acsnano.1c00481

Figure 3.

Figure 3

(a–c) Three (de)trapping regimes that CdSe NPLs may experience: (a) no trapping, (b) fast trapping–detrapping cycling, and (c) irreversible trapping. (d) Calculated lifetime of the slow delay component τslow, normalized to the trap recombination lifetime τT, and (e) fractional trap PL IT/Itot, as a function of trapping probability Pt and detrapping probability Pdt. The dotted lines in (d) and (e) are contours of the calculated average number of trapping events N prior to recombination. (f) Configuration–coordinate diagram, illustrating exciton and trap emission. (g) Zoom-in of the diagram displayed in panel (f), indicating the energy barriers for trapping ΔEtrap# and detrapping ΔEdetrap. As the single-NPL trap-PL fwhm appears to be independent of the peak energy (Figure S3; Extended Data), the difference in the equilibrium Q among trap states is negligible; that is, the trap states are spaced vertically, not horizontally, in the coordinate diagram.