Anion Exchange and the Quantum-Cutting Energy Threshold in Ytterbium-Doped CsPb(Cl<sub>1- x</sub>Br <sub>x</sub>)<sub>3</sub> Perovskite Nanocrystals.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 30694072.
- Also identified by DOI 10.1021/acs.nanolett.8b05104.
- No licence information is recorded for this record.
- Because redistribution is not established, this page shows the abstract only. Follow the links below for the full text.
Abstract
Colloidal halide perovskite nanocrystals of CsPbCl<sub>3</sub> doped with Yb<sup>3+</sup> have demonstrated remarkably high sensitized photoluminescence quantum yields (PLQYs), approaching 200%, attributed to a picosecond quantum-cutting process in which one photon absorbed by the nanocrystal generates two photons emitted by the Yb<sup>3+</sup> dopants. This quantum-cutting process is thought to involve a charge-neutral defect cluster within the nanocrystal's internal volume. We demonstrate that Yb<sup>3+</sup>-doped CsPbCl<sub>3</sub> nanocrystals can be converted postsynthetically to Yb<sup>3+</sup>-doped CsPb(Cl<sub>1- x</sub>Br <sub>x</sub>)<sub>3</sub> nanocrystals without compromising the desired high PLQYs. Nanocrystal energy gaps can be tuned continuously from E<sub>g</sub> ≈ 3.06 eV (405 nm) in CsPbCl<sub>3</sub> down to E<sub>g</sub> ≈ 2.53 eV (∼490 nm) in CsPb(Cl<sub>0.25</sub>Br<sub>0.75</sub>)<sub>3</sub> while retaining a constant PLQY above 100%. Reducing E<sub>g</sub> further causes a rapid drop in PLQY, interpreted as reflecting an energy threshold for quantum cutting at approximately twice the energy of the Yb<sup>3+</sup><sup>2</sup>F<sub>7/2</sub> → <sup>2</sup>F<sub>5/2</sub> absorption threshold. These data demonstrate that very high quantum-cutting energy efficiencies can be achieved in Yb<sup>3+</sup>-doped CsPb(Cl<sub>1- x</sub>Br <sub>x</sub>)<sub>3</sub> nanocrystals, offering the possibility to circumvent thermalization losses in conventional solar technologies. The presence of water during anion exchange is found to have a deleterious effect on the Yb<sup>3+</sup> PLQYs but does not affect the nanocrystal shapes or morphologies, or even reduce the excitonic PLQYs of analogous undoped CsPb(Cl<sub>1- x</sub>Br <sub>x</sub>)<sub>3</sub> nanocrystals. These results provide valuable information relevant to the development and application of these unique materials for spectral-shifting solar energy conversion technologies.