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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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Figure 3: Panel A: Normalized kinetic traces photoexcited CdTe for different particle sizes<br />

at 610 nm (1S exciton position). Panel B: Plot of cooling time (growth kinetics at 1S exciton)<br />

vs particle size showing non-linear increment.<br />

To confirm the involvement of Auger mediated cooling processes we have carried<br />

quenching studies where the quenchers can selectively accept electrons or holes and then find<br />

out the effect of cooling dynamics of the lowest excitonic (1S 3/2 -1S e ) state. The quenchers<br />

can decouple electrons or holes selectively which eventually hinders the energy transfer from<br />

the electron to the hole. In the present studies we have used benzoquinone (BQ) as electron<br />

quencher and n-butyl amine (BA) as hole quencher. Figure 4 show the kinetic trace at 1S<br />

exciton position (monitored at 610 nm) of CdTe QD in absence of any quencher (Figure<br />

4.4a), in presence of electron quencher (BQ) (Figure 4.4b) and in presence of hole quencher<br />

(BA) (Figure 4.4c). In presence of BQ, it is expected that hot electron will be quenched. In

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