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Quasi-type II CuInS(2)/CdS core/shell quantum dots

Ternary chalcopyrite CuInS(2) quantum dots (QDs) have been extensively studied in recent years as an alternative to conventional QDs for solar energy conversion applications. However, compared with the well-established photophysics in prototypical CdSe QDs, much less is known about the excited prope...

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Detalles Bibliográficos
Autores principales: Wu, Kaifeng, Liang+, Guijie, Kong, Degui, Chen, Jinquan, Chen, Zheyuan, Shan, Xinhe, McBride, James R., Lian, Tianquan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Royal Society of Chemistry 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5975837/
https://www.ncbi.nlm.nih.gov/pubmed/29910880
http://dx.doi.org/10.1039/c5sc03715h
Descripción
Sumario:Ternary chalcopyrite CuInS(2) quantum dots (QDs) have been extensively studied in recent years as an alternative to conventional QDs for solar energy conversion applications. However, compared with the well-established photophysics in prototypical CdSe QDs, much less is known about the excited properties of CuInS(2) QDs. In this work, using ultrafast spectroscopy, we showed that both conduction band (CB) edge electrons and copper vacancy (V(Cu)) localized holes were susceptible to surface trappings in CuInS(2) QDs. These trap states could be effectively passivated by forming quasi-type II CuInS(2)/CdS core/shell QDs, leading to a single-exciton (with electrons delocalized among CuInS(2)/CdS CB and holes localized in V(Cu)) half lifetime of as long as 450 ns. Because of reduced electron–hole overlap in quasi-type II QDs, Auger recombination of multiple excitons was also suppressed and the bi-exciton lifetime was prolonged to 42 ps in CuInS(2)/CdS QDs from 10 ps in CuInS(2) QDs. These demonstrated advantages, including passivated trap states, long single and multiple exciton lifetimes, suggest that quasi-type II CuInS(2)/CdS QDs are promising materials for photovoltaic and photocatalytic applications.