4.8 Review

Blue Light Emitting Defective Nanocrystals Composed of Earth-Abundant Elements

Journal

ANGEWANDTE CHEMIE-INTERNATIONAL EDITION
Volume 59, Issue 2, Pages 860-867

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/anie.201911436

Keywords

defect states; DFT calculations; fast lifetime; photoluminescence; ternary nanocrystal

Funding

  1. Department of Energy (DOE), Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DE-FG02-07ER46454]
  2. Department of Defense, Air Force Office of Scientific Research, National Defense Science and Engineering Graduate (NDSEG) Fellowship [32 CFR 168a]
  3. National Science Scholarship
  4. U.S. Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DE-FG02- 07ER46454]
  5. National Science Foundation [ACI-1053575, 1541959]
  6. MRSEC Program of the National Science Foundation [DMR-1419807]
  7. Office of Science of the US DOE [DE-AC02-05CH11231]

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Copper-based ternary (I-III-VI) chalcogenide nanocrystals (NCs) are compositionally-flexible semiconductors that do not contain lead (Pb) or cadmium (Cd). Cu-In-S NCs are the dominantly studied member of this important materials class and have been reported to contain optically-active defect states. However, there are minimal reports of In-free compositions that exhibit efficient photoluminescence (PL). Here, we report a novel solution-phase synthesis of approximate to 4 nm defective nanocrystals (DNCs) composed of copper, aluminum, zinc, and sulfur with approximate to 20 % quantum yield and an attractive PL maximum of 450 nm. Extensive spectroscopic characterization suggests the presence of highly localized electronic states resulting in reasonably fast PL decays (approximate to 1 ns), large vibrational energy spacing, small Stokes shift, and temperature-independent PL linewidth and PL lifetime (between room temperature and approximate to 5 K). Furthermore, density functional theory (DFT) calculations suggest PL transitions arise from defects within a CuAl5S8 crystal lattice, which supports the experimental observation of highly-localized states. The results reported here provide a new material with unique optoelectronic characteristics that is an important analog to well-explored Cu-In-S NCs.

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