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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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149<br />

In addition to the cooling dynamics Figure 8 also shows the bleach recovery<br />

dynamics of core and different core-shells. The bleach recovery kinetics can be fitted multiexponentially<br />

with different time constants with τ 1 = 2.55 ps (45%), τ 2 = 27 ps (17%) and τ 3 =<br />

> 400 ps (38%) for CdSe core, τ 1 = 2.6 ps (30%), τ 2 = 30 ps (33%) and τ 3 = > 400 ps (37%)<br />

for CdSe/ZnTe3 core-shell and τ 1 = 3 ps (21.5%), τ 2 = 50 ps (32.5%) and τ 3 = > 400 ps (46%)<br />

for CdSe/ZnTe4 core-shell. It clearly hints at the multi-exponential nature of bleach recovery<br />

tell us that the charge carrier dynamics is governed by more than one process. The multiexponential<br />

nature of the dynamics can come from multiple sizes QD in addition to trapping<br />

dynamics of trap states. If the dynamics is dominated by only one lifetime contribution it<br />

could come from single dot contribution. However in the present case we have long<br />

component which contributes quite substantially (> 30%). Since under the present excitation<br />

conditions N

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