Surface Reconstructions in II-VI Quantum Dots

Journal Article (2023)
Author(s)

Jordi Llusar (Basque Center for Materials, Applications and Nanostructures (BCMaterials))

I. Du Fosse (TU Delft - ChemE/Opto-electronic Materials)

Zeger Hens (Universiteit Gent)

Arjan Houtepen (TU Delft - ChemE/Opto-electronic Materials)

Ivan Infante (Basque Foundation for Science)

Research Group
ChemE/Opto-electronic Materials
Copyright
© 2023 Jordi Llusar, I. du Fossé, Zeger Hens, A.J. Houtepen, Ivan Infante
DOI related publication
https://doi.org/10.1021/acsnano.3c09265
More Info
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Publication Year
2023
Language
English
Copyright
© 2023 Jordi Llusar, I. du Fossé, Zeger Hens, A.J. Houtepen, Ivan Infante
Research Group
ChemE/Opto-electronic Materials
Issue number
2
Volume number
18
Pages (from-to)
1563-1572
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Abstract

Although density functional theory (DFT) calculations have been crucial in our understanding of colloidal quantum dots (QDs), simulations are commonly carried out on QD models that are significantly smaller than those generally found experimentally. While smaller models allow for efficient study of local surface configurations, increasing the size of the QD model will increase the size or number of facets, which can in turn influence the energetics and characteristics of trap formation. Moreover, core-shell structures can only be studied with QD models that are large enough to accommodate the different layers with the correct thickness. Here, we use DFT calculations to study the electronic properties of QDs as a function of size, up to a diameter of ∼4.5 nm. We show that increasing the size of QD models traditionally used in DFT studies leads to a disappearance of the band gap and localization of the HOMO and LUMO levels on facet-specific regions of the QD surface. We attribute this to the lateral coupling of surface orbitals and the formation of surface bands. The introduction of surface vacancies and their a posteriori refilling with Z-type ligands leads to surface reconstructions that widen the band gap and delocalize both the HOMO and LUMO. These results show that the surface geometry of the facets plays a pivotal role in defining the electronic properties of the QD.