Reversible Charge-Carrier Trapping Slows Förster Energy Transfer in CdSe/CdS Quantum-Dot Solids
Author(s) -
Federico Montanarella,
Margherita Biondi,
Stijn O. M. Hinterding,
Daniël Vanmaekelbergh,
Freddy T. Rabouw
Publication year - 2018
Publication title -
nano letters
Language(s) - Uncategorized
Resource type - Journals
SCImago Journal Rank - 4.853
H-Index - 488
eISSN - 1530-6992
pISSN - 1530-6984
DOI - 10.1021/acs.nanolett.8b02538
Subject(s) - photoexcitation , quantum dot , trapping , photoluminescence , charge carrier , excited state , ultrafast laser spectroscopy , chemical physics , materials science , molecular physics , relaxation (psychology) , förster resonance energy transfer , optoelectronics , chemistry , atomic physics , fluorescence , spectroscopy , physics , optics , psychology , ecology , social psychology , quantum mechanics , biology
The dynamics of photoluminescence (PL) from nanocrystal quantum dots (QDs) is significantly affected by the reversible trapping of photoexcited charge carriers. This process occurs after up to 50% of the absorption events, depending on the type of QD considered, and can extend the time between the photoexcitation and relaxation of the QD by orders of magnitude. Although many optoelectronic applications require QDs assembled into a QD solid, until now, reversible trapping has been studied only in (ensembles of) spatially separated QDs. Here, we study the influence of reversible trapping on the excited-state dynamics of CdSe/CdS core/shell QDs when they are assembled into close-packed "supraparticles". Time- and spectrally resolved photoluminescence (PL) measurements reveal competition among spontaneous emission, reversible charge-carrier trapping, and Förster resonance energy transfer between the QDs. While Förster transfer causes the PL to red-shift over the first 20-50 ns after excitation, reversible trapping stops and even reverses this trend at later times. We can model this behavior with a simple kinetic Monte Carlo simulation by considering that charge-carrier trapping leaves the QDs in a state with zero oscillator strength in which no energy transfer can occur. Our results highlight that reversible trapping significantly affects the energy and charge-carrier dynamics for applications in which QDs are assembled into a QD solid.
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