Cu-Doped Cs <sub>3</sub> Sb <sub>2</sub> Cl <sub>9</sub> Nanocrystals: Revisiting the Low Bandgap of Cs <sub>2</sub> CuSbCl <sub>6</sub> Double Perovskites

Lead-free halide double perovskite Cs<sub>2</sub>CuSbCl<sub>6</sub> nanocrystals have recently been reported to have a low bandgap of 1.66 eV. In this work, we show that the optical absorption spectra and X-ray diffraction patterns previously attributed to Cs<sub>2</sub>CuSbCl<sub>6</sub> can rather be explained with Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>:Cu: X-ray absorption spectroscopy identifies [CuCl<sub>3</sub>]<sup>-</sup> trigonal pyramids, with Cu<sup>2+</sup> possibly replacing two Cs<sup>+</sup> sites. The broad low-energy optical absorption is then assigned to localized electronic transitions at copper dopants within the Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> lattice, which do not affect the wide bandgap. Ab initio calculations suggest that Cs<sub>2</sub>CuSbCl<sub>6</sub> is thermodynamically unstable with respect to decomposition to Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>, in line with the low reproducibility of Cs<sub>2</sub>CuSbCl<sub>6</sub> observed in its synthesis.

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Journal
ACS Materials Letters
Published
2025-10-10
DOI
https://doi.org/10.1021/acsmaterialslett.5c01043
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Cu-Doped Cs 3 Sb 2 Cl 9 Nanocrystals: Revisiting the Low Bandgap of Cs 2 CuSbCl 6 Double Perovskites

David F. Macías-Pinilla, Quinten A. Akkerman, Federica Bertolotti, Simone Virga et al.
ACS Materials Letters
Perovskite Materials and Applications
article

Cu-Doped Cs 3 Sb 2 Cl 9 Nanocrystals: Revisiting the Low Bandgap of Cs 2 CuSbCl 6 Double Perovskites

David F. Macías-Pinilla, Quinten A. Akkerman, Federica Bertolotti, Simone Virga, Nicola Dengo, Francesco Giannici, Fei He, Alessandro Longo
article en

Abstract

Lead-free halide double perovskite Cs<sub>2</sub>CuSbCl<sub>6</sub> nanocrystals have recently been reported to have a low bandgap of 1.66 eV. In this work, we show that the optical absorption spectra and X-ray diffraction patterns previously attributed to Cs<sub>2</sub>CuSbCl<sub>6</sub> can rather be explained with Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>:Cu: X-ray absorption spectroscopy identifies [CuCl<sub>3</sub>]<sup>-</sup> trigonal pyramids, with Cu<sup>2+</sup> possibly replacing two Cs<sup>+</sup> sites. The broad low-energy optical absorption is then assigned to localized electronic transitions at copper dopants within the Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> lattice, which do not affect the wide bandgap. Ab initio calculations suggest that Cs<sub>2</sub>CuSbCl<sub>6</sub> is thermodynamically unstable with respect to decomposition to Cs<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>, in line with the low reproducibility of Cs<sub>2</sub>CuSbCl<sub>6</sub> observed in its synthesis.

ACS Materials LettersVol. 7(11)
University of Insubria (IT), European Synchrotron Radiation Facility (FR), Istituto di Astrofisica Spaziale e Fisica cosmica di Palermo (IT), Ludwig-Maximilians-Universität München (DE), University of Palermo (IT)
European Synchrotron Radiation Facility
Openalex Percentile: Top 72%
Perovskite Materials and Applications
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