Bright Blue Emitting Cu-Doped Cs2ZnCl4Colloidal Nanocrystals

Dongxu Zhu, Matteo L. Zaffalon, Valerio Pinchetti, Rosaria Brescia, Fabrizio Moro, Mauro Fasoli, Marco Fanciulli, Aiwei Tang, Ivan Infante*, Luca De Trizio, Sergio Brovelli, Liberato Manna

*Corresponding author for this work

Research output: Contribution to JournalArticleAcademicpeer-review

Abstract

We report here the synthesis of undoped and Cu-doped Cs2ZnCl4 nanocrystals (NCs) in which we could tune the concentration of Cu from 0.7 to 7.5%. Cs2ZnCl4 has a wide band gap (4.8 eV), and its crystal structure is composed of isolated ZnCl4 tetrahedra surrounded by Cs+ cations. According to our electron paramagnetic resonance analysis, in 0.7 and 2.1% Cu-doped NCs the Cu ions were present in the +1 oxidation state only, while in NCs at higher Cu concentrations we could detect Cu(II) ions (isovalently substituting the Zn(II) ions). The undoped Cs2ZnCl4 NCs were non emissive, while the Cu-doped samples had a bright intragap photoluminescence (PL) at â2.6 eV mediated by band-edge absorption. Interestingly, the PL quantum yield was maximum (â55%) for the samples with a low Cu concentration ([Cu] ≤ 2.1%), and it systematically decreased when further increasing the concentration of Cu, reaching 15% for the NCs with the highest doping level ([Cu] = 7.5%). The same (â2.55 eV) emission band was detected under X-ray excitation. Our density functional theory calculations indicated that the PL emission could be ascribed only to Cu(I) ions: These ions promote the formation of trapped excitons, through which an efficient emission takes place. Overall, these Cu-doped Cs2ZnCl4 NCs, with their high photo- A nd radio-luminescence emission in the blue spectral region that is free from reabsorption, are particularly suitable for applications in ionizing radiation detection.

Original languageEnglish
Pages (from-to)5897-5903
Number of pages7
JournalChemistry of Materials
Volume32
Issue number13
Early online date5 Jun 2020
DOIs
Publication statusPublished - 14 Jul 2020

Funding

We acknowledge S. Lauciello for help with the SEM-EDS measurement and M. Prato for performing the XPS analysis. D.Z. acknowledges a scholarship from the China Scholarship Council (CSC) (201807090085). We also acknowledge funding from the programme for research and Innovation Horizon 2020 (2014-2020) under the Marie Skl̷odowska-Curie Grant Agreement COMPASS No. 691185. Financial support from the Italian Ministry of University and Research (MIUR) through grant “Dipartimenti di Eccellenza - 2017 Materials For Energy” is acknowledged. The computational work was carried out on the Dutch national e-infrastructure with the support of SURF cooperative.

FundersFunder number
Innovation Horizon 2020
Horizon 2020 Framework Programme691185
Ministero dell’Istruzione, dell’Università e della Ricerca
China Scholarship Council201807090085

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