4.8 Article

Thick-Shell CuInS2/ZnS Quantum Dots with Suppressed Blinking and Narrow Single-Particle Emission Line Widths

Journal

NANO LETTERS
Volume 17, Issue 3, Pages 1787-1795

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.nanolett.6b05118

Keywords

Core/shell quantum dot; copper indium sulfide; photoluminescence line width; single-dot spectroscopy; suppressed blinking

Funding

  1. Center for Advanced Solar Photophysics (CASP), an Energy Frontier Research Center - the U.S. Department of Energy, Office of Science, Basic Energy Sciences
  2. Chemical Sciences, Biosciences and Geosciences Division, Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy

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Quantum dots (QDs) of ternary I-II-VI2 com-pounds such as CuInS2 and CuInSe2 have been actively investigated as heavy-metal-free alternatives to cadmium- and lead-containing semiconductor nanomaterials. One serious limitation of these nanostructures, however, is a large photoluminescence (PL) line width (typically >300 meV), the origin of which is still not fully understood. It remains even unclear whether the observed broadening results from considerable sample heterogeneities (due, e.g., to size polydispersity) or is an unavoidable intrinsic property of individual QDs. Here, we answer this question by conducting single particle measurements on a new type of CuInS2 (CIS) QDs with an especially thick ZnS shell. These QDs show a greatly enhanced photostability compared to core-only or thin-shell samples and, importantly, exhibit a strongly suppressed PL blinking at the single-dot level. Spectrally resolved measurements reveal that the single-dot, room-temperature PL line width is much narrower (down to,similar to 60 meV) than that of the ensemble samples. To explain this distinction, we invoke a model wherein PL from CIS QDs arises from radiative recombination of a delocalized band-edge electron and a localised hole residing on a Cu-related defect and also account for the effects of electron hole Coulomb coupling. We show that random positioning of the emitting center in the QD can lead to more than 300 meV variation in the PL energy, which represents at least one of the reasons for large PL broadening of the ensemble samples. These results suggest that in addition to narrowing size dispersion, future efforts on tightening the emission spectra of these QDs might also attempt decreasing the positional heterogeneity of the emitting centers.

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