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Compositional Tuning of Carrier Dynamics in Cs<sub>2</sub>Na<sub>1–<i>x</i></sub>Ag<sub><i>x</i></sub>BiCl<sub>6</sub> Double-Perovskite Nanocrystals

87

Citations

37

References

2020

Year

Abstract

We devised a hot-injection synthesis to prepare colloidal double-perovskite Cs<sub>2</sub>NaBiCl<sub>6</sub> nanocrystals (NCs). We also examined the effects of replacing Na<sup>+</sup> with Ag<sup>+</sup> cations by preparing and characterizing Cs<sub>2</sub>Na<sub>1-<i>x</i></sub> Ag <sub><i>x</i></sub> BiCl<sub>6</sub> alloy NCs with <i>x</i> ranging from 0 to 1. Whereas Cs<sub>2</sub>NaBiCl<sub>6</sub> NCs were not emissive, Cs<sub>2</sub>Na<sub>1-<i>x</i></sub> Ag <sub><i>x</i></sub> BiCl<sub>6</sub> NCs featured a broad photoluminescence band at ∼690 nm, Stokes-shifted from the respective absorption by ≥1.5 eV. The emission efficiency was maximized for low Ag<sup>+</sup> amounts, reaching ∼3% for the Cs<sub>2</sub>Na<sub>0.95</sub>Ag<sub>0.05</sub>BiCl<sub>6</sub> composition. Density functional theory calculations coupled with spectroscopic investigations revealed that Cs<sub>2</sub>Na<sub>1-<i>x</i></sub> Ag <sub><i>x</i></sub> BiCl<sub>6</sub> NCs are characterized by a complex photophysics stemming from the interplay of (i) radiative recombination via trapped excitons localized in spatially connected AgCl<sub>6</sub>-BiCl<sub>6</sub> octahedra; (ii) surface traps, located on undercoordinated surface Bi centers, behaving as phonon-assisted nonradiative decay channels; and (iii) a thermal equilibrium between trapping and detrapping processes. These results offer insights into developing double-perovskite NCs with enhanced optoelectronic efficiency.

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