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Temperature dependent radiative and non-radiative recombination dynamics in CdSe–CdTe and CdTe–CdSe type II hetero nanoplatelets
Author(s) -
Riccardo Scott,
Sebastian Kickhöfel,
Oliver Schoeps,
Artsiom Antanovich,
Anatol Prudnikau,
Andrey Chuvilin,
U. Woggon,
Mikhail Artemyev,
Alexander W. Achtstein
Publication year - 2016
Publication title -
physical chemistry chemical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.053
H-Index - 239
eISSN - 1463-9084
pISSN - 1463-9076
DOI - 10.1039/c5cp06623a
Subject(s) - photoluminescence , cadmium telluride photovoltaics , radiative transfer , exciton , quantum yield , laser linewidth , quantum dot , chemistry , spontaneous emission , recombination , materials science , atomic physics , molecular physics , optoelectronics , condensed matter physics , physics , laser , optics , biochemistry , gene , fluorescence
We investigate the temperature-dependent decay kinetics of type II CdSe-CdTe and CdTe-CdSe core-lateral shell nanoplatelets. From a kinetic analysis of the photoluminescence (PL) decay and a measurement of the temperature dependent quantum yield we deduce the temperature dependence of the non-radiative and radiative lifetimes of hetero nanoplates. In line with the predictions of the giant oscillator strength effect in 2D we observe a strong increase of the radiative lifetime with temperature. This is attributed to an increase of the homogeneous transition linewidth with temperature. Comparing core only and hetero platelets we observe a significant prolongation of the radiative lifetime in type II platelets by two orders in magnitude while the quantum yield is barely affected. In a careful analysis of the PL decay transients we compare different recombination models, including electron hole pairs and exciton decay, being relevant for the applicability of those structures in photonic applications like solar cells or lasers. We conclude that the observed biexponential PL decay behavior in hetero platelets is predominately due to spatially indirect excitons being present at the hetero junction and not ionized e-h pair recombination.

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