TY - JOUR
T1 - Bright Blue Emitting Cu-Doped Cs2ZnCl4Colloidal Nanocrystals
AU - Zhu, Dongxu
AU - Zaffalon, Matteo L.
AU - Pinchetti, Valerio
AU - Brescia, Rosaria
AU - Moro, Fabrizio
AU - Fasoli, Mauro
AU - Fanciulli, Marco
AU - Tang, Aiwei
AU - Infante, Ivan
AU - De Trizio, Luca
AU - Brovelli, Sergio
AU - Manna, Liberato
PY - 2020/7/14
Y1 - 2020/7/14
N2 - 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.
AB - 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.
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U2 - 10.1021/acs.chemmater.0c02017
DO - 10.1021/acs.chemmater.0c02017
M3 - Article
AN - SCOPUS:85092236894
SN - 0897-4756
VL - 32
SP - 5897
EP - 5903
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 13
ER -