Impact of Ca2+, Ce3+ codoping on ZnSnO3-SnO2 heterostructure for dielectric, optoelectronic and solar cell applications

No Thumbnail Available
Authors
Taha, Taha Abdel Mohaymen
Alshammari, Alhulw H.
Sanad, Moustafa M.S.
Elsherif, Sara S.
Eraky, Mostafa S.
Alenad, Asma M.
El-Nasser, Karam S.
Hamdeh, Hussein H.
Advisors
Issue Date
2024-01-01
Type
Article
Keywords
Zinc stannate , Lanthanide doping , Dielectric , Optoelectronic , P-N junction
Research Projects
Organizational Units
Journal Issue
Citation
Taha T. A., Alshammari, A. H., Sanad M. M. M., Elsherif, S. S., Eraky, M. S., Alenad, A. M., El-Nasser, K. S., & Hamdeh, H. H. (2024). Impact of Ca2+, Ce3+ codoping on ZnSnO3-SnO2 heterostructure for dielectric, optoelectronic and solar cell applications. Journal of Electroanalytical Chemistry, 952. https://doi.org/10.1016/j.jelechem.2023.117955.
Abstract

We have successfully prepared a new mixed oxide system of Sn-rich ZTO (ZnSn2O5). The impact of coupling Ca2+ and Ce3+ inside the lattice of ZnSn2O5 on the dielectric, optical, and photoelectric conduction properties was investigated. In this regard, the co-precipitation technique was used to prepare three samples of ZTO, Ca-ZTO, and Ca/Ce-ZTO. The samples have been investigated by X-ray diffractometer (XRD), Fourier transform infrared (FTIR), field emission scanning electron microscope (FESEM), X-ray photoelectron spectrophotometer (XPS), and an energy dispersive X-ray spectrometer (EDS). The XRD pattern detected phases that highly interfere as a heterostructured compound. The pristine ZTO particles demonstrate a mixture of two morphologies, hexagonal and quasi-spherical shapes, with particle size distributions of 0.25–1.5 µm, resulting in significant porosity between these particles. Meanwhile, the particles of Ca/Ce-doped ZTO have a homogenous morphology as spherical shape and exhibit larger density, particle size distribution range of 1–2 µm. The dielectric constant as a function of frequency or wavelength is increased with the applied temperature (32 to 140 °C) for both pure and Ca/Ce-ZTO samples. Clearly, Ca/Ce-ZTO displays higher absorption in visible light and the estimated band gaps of ZTO, Ca-ZTO, and Ca/Ce-ZTO are equal to 1.58,1.56 and 1.48 eV, respectively. The pristine ZTO showed a stronger n-type effect than Ca and Ca/Ce-doped ZTO samples. The shift from n-type to being close to N-P junction by multiple doping induces the application of these heterostructured materials as buffering layers in energy conversion applications like thin film solar cells and light emitting diodes.

Table of Contents
Description
Part of special issue, 6th International Symposium on Electrochemistry, South Africa
Publisher
Elsevier
Journal
Journal of Electroanalytical Chemistry
Book Title
Series
PubMed ID
ISSN
1572-6657
1873-2569
EISSN