Superfluorescent Multicomponent Nanocrystal Superlattices from Lead Halide Perovskite Nanocubes
Ihor Cherniukh a, b, Gabriele Rainò a, b, Taras Sekh a, b, Thilo Stöferle c, Max Burian d, Alex Travesset e, Modestos Athanasiou f, Andreas Manoli f, Rohit John a, b, Yevhen Shynkarenko a, b, Denys Naumenko g, Heinz Amenitsch g, Grigorios Itskos f, Rolf Erni h, Rainer Mahrt c, Maryna Bodnarchuk a, b, Maksym Kovalenko a, b
a Department of Chemistry and Applied Biosciences, Institute of Inorganic Chemistry, ETH Zürich, Zürich, Switzerland
b Laboratory of Thin Films and Photovoltaics, Empa — Swiss Federal Laboratories for Materials Science and Technology, Ueberlandstrasse, 129, Dübendorf, Switzerland
c IBM Research Europe — Zurich, Säumerstrasse, 4, Rüschlikon, Switzerland
d Swiss Light Source, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland
e Department of Physics and Astronomy and Ames Laboratory, Iowa State University, Ames, 50011 Iowa, United States
f Experimental Condensed Matter Physics Laboratory, Department of Physics, University of Cyprus, 1678 Nicosia, Cyprus
g Institute of Inorganic Chemistry, Graz University of Technology, Stremayrgasse, 9, Graz, Austria
h Electron Microscopy Center, Empa — Swiss Federal Laboratories for Materials Science and Technology, Ueberlandstrasse, 129, Dübendorf, Switzerland
Cesium lead halide perovskite nanocrystals, owing to high oscillator strength of bright triplet excitons, long coherence times and minimal inhomogeneous broadening of emission lines, are promising building blocks for creating superlattice structures that exhibit collective phenomena in their optical spectra. Thus far, only single-component superlattices with the simple cubic packing have been devised from these nanocrystals, which have been shown to exhibit superfluorescence – a collective emission resulting in a burst of photons with ultrafast radiative decay (ca. 20 ps) that could be tailored for use in ultrabright (quantum) light sources [1]. However, far broader structural engineerability of superlattices, required for programmable tuning of the collective emission and for building a theoretical framework can be envisioned from the recent advancements in colloidal science. We show that co-assembly of cubic and spherical steric-stabilized nanocrystals is experimentally possible and that the cubic shape of perovskite nanocrystals leads to a vastly different outcome compared to all-spherical systems. Five superlattice structures have been obtained: novel AB2, ABO3, ABO6, besides expected NaCl or common to all-sphere assemblies AlB2 superlattices [2,3]. In binary ABO3 and ABO6 superlattices, larger spherical nanocrystals occupy the A sites and smaller cubic CsPbBr3 nanocrystals reside on the B and O sites. Targeted substitution of B-site nanocubes by truncated cuboid PbS nanocrystals leads to the exclusive formation of ternary perovskite-type ABO3 superlattice. Truncated cuboid PbS NCs can occupy A-sites in binary ABO3, NaCl, and AlB2 SLs with smaller CsPbBr3 nanocubes. All synthesized superlattices exhibit a high degree of orientational ordering of the CsPbBr3 nanocubes. We also demonstrate the effect of superlattice structure on the collective optical properties.
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