4.8 Article

Colloidal Synthesis Path to 2D Crystalline Quantum Dot Superlattices

Journal

ACS NANO
Volume 15, Issue 2, Pages 2251-2262

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.0c07202

Keywords

self-assembly; oriented attachment; nanocrystal superlattices; quantum dots; CdSe

Funding

  1. National Science Foundation, Division of Materials Research (DMR) [DMR-1808151]
  2. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Materials Sciences and Engineering Division [DEAC02-05-CH11231, KC3103]
  3. NIH [S10OD023532]
  4. Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy [DE-AC02-05CH11231]
  5. Kavli Philomathia Graduate Student Fellowship

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By combining colloidal nanocrystal synthesis, self-assembly, and solution phase epitaxial growth techniques, a method for preparing high-quality single dot thick atomically attached quantum dot superlattices with good uniformity has been developed. The ability to independently tune the size and material of the quantum dot core, shell, QD-QD distance, and matrix material allows for control over various properties depending on specific applications.
By combining colloidal nanocrystal synthesis, self-assembly, and solution phase epitaxial growth techniques, we developed a general method for preparing single dot thick atomically attached quantum dot (QD) superlattices with high-quality translational and crystallographic orientational order along with state-of-the-art uniformity in the attachment thickness. The procedure begins with colloidal synthesis of hexagonal prism shaped core/shell QDs (e.g., CdSe/CdS), followed by liquid subphase self-assembly and immobilization of superlattices on a substrate. Solution phase epitaxial growth of additional semiconductor material fills in the voids between the particles, resulting in a QD-in-matrix structure. The photoluminescence emission spectra of the QD-in-matrix structure retains characteristic 0D electronic confinement. Importantly, annealing of the resulting structures removes inhomogeneities in the QD-QD inorganic bridges, which our atomistic electronic structure calculations demonstrate would otherwise lead to Anderson-type localization. The piecewise nature of this procedure allows one to independently tune the size and material of the QD core, shell, QD-QD distance, and the matrix material. These four choices can be tuned to control many properties (degree of quantum confinement, quantum coupling, band alignments, etc.) depending on the specific applications. Finally, cation exchange reactions can be performed on the final QD-in-matrix, as demonstrated herein with a CdSe/CdS to HgSe/HgS conversion.

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