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Reactivity-matched synthesis of monodisperse Ag(In,Ga)S QDs with efficient luminescence
I-III-VI quantum dots (QDs) have gained widespread attention owing to their significant advantages of non-toxicity, large structural tolerance, and efficient photoluminescence potential. However, the disbalance of reactivity between the elements will result in undesired products and compromised opti...
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Published in: | Nanoscale 2024-07, Vol.16 (28), p.13654-13662 |
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Main Authors: | , , , , , , , , |
Format: | Article |
Language: | |
Online Access: | Get full text |
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Summary: | I-III-VI quantum dots (QDs) have gained widespread attention owing to their significant advantages of non-toxicity, large structural tolerance, and efficient photoluminescence potential. However, the disbalance of reactivity between the elements will result in undesired products and compromised optical properties. Reducing the activity of highly reactive group IB elements is the most common approach, but it will reduce the overall reactivity and lead to a wide dispersion of QD sizes. In this study, we propose a method to improve the overall reactivity of the reaction system using the highly active IIIA precursor InI
3
, which triggers rapid nucleation and promotes the formation of Ag(In,Ga)S
2
(AIGS) QDs, resulting in monodisperse particle size distributions and a significantly improved photoluminescence quantum yield (PLQY) (from 12% to 72%). Furthermore, narrow band edge emission is realized by coating a gallium sulfide (GaS
x
) shell on the basis of obtaining high-quality AIGS QDs. The core/shell QDs exhibit a 90% PLQY with a full width at half maximum (FWHM) of only 31 nm at 530 nm. This study provides a viable design strategy to synthesize monodisperse AIGS QDs with a narrow peak width and efficient luminescence, promoting the application of AIGS QDs in the field of luminescent displays.
We present a method of preparing highly efficient monodisperse Ag(In,Ga)S
2
, which suppresses the activity mismatch of multiple elements by using InI
3
. The PLQY value reaches 90% at 530 nm with an optimum FWHM of 31 nm by cladding the shell layer. |
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ISSN: | 2040-3364 2040-3372 |
DOI: | 10.1039/d4nr00804a |