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Interlinking the Fe doping concentration, optoelectronic properties, and photocatalytic performance of ZnO nanostructures

Amugul EsbergenovaCenter for Development of Nanotechnology at the National University of Uzbekistan, University Str. 4, 100174, Tashkent, UzbekistanMirabbos HojamberdievInstitut für Chemie, Technische Universität Berlin, Straße des 17. Juni 135, 10623, Berlin, GermanyZukhra C. KadirovaUzbekistan-Japan Innovation Center of Youth, University Street 2B, 100095, Tashkent, UzbekistanYuichi SugaiDepartment of Earth Resources Engineering, Kyushu University, 744 Motooka, Fukuoka, 8190395, JapanShavkat MamatkulovInstitute of Material Sciences of the Academy of Sciences of the Republic of Uzbekistan, Chingiz Aytmatov 2b, 100084, Tashkent, UzbekistanR.R. JalolovDepartment of Physics, National University of Uzbekistan, Tashkent, Uzbekistan, University Str. 4, 100174, Tashkent, UzbekistanDebin KongCollege of New Energy, Research Center for Advanced Chemical Engineering and Energy Materials, China University of Petroleum (East China), 266580, Qingdao, PR ChinaXin QinCollege of New Energy, Research Center for Advanced Chemical Engineering and Energy Materials, China University of Petroleum (East China), 266580, Qingdao, PR ChinaShahlo DaminovaDepartment of General and Inorganic Chemistry, Faculty of Chemistry, National University of Uzbekistan, University Street 4, 100174, Tashkent, UzbekistanOlim RuzimuradovDepartment of Natural and Mathematic Sciences, Turin Polytechnic University in Tashkent, Kichik Halqa Yo'li 17, 100095, Tashkent, UzbekistanUlugbek ShaislamovCenter for Development of Nanotechnology at the National University of Uzbekistan, University Str. 4, 100174, Tashkent, Uzbekistan
Current Applied Physicsjournal2024en
ABI

Аннотация

Doping is one of the effective strategies to modulate the optoelectronic properties and photocatalytic activity of photocatalysts . In this study, the effect of Fe doping (0–10 %) on morphology, optical and electronic properties, and photocatalytic activity of ZnO nanostructures is studied. The X-ray diffraction analysis shows that >5 % Fe doping, ZnFe 2 O 4 is segregated as a secondary phase. The crystalline size decreases from 50.8 nm to 21.4 nm and the micro-strain increases with increasing the Fe concentration. The Fe doping-induced electronic restructuring facilitates visible light absorption through the O 2p → Fe 3d transition and the suppression of charge recombination by efficiently trapping conduction band electrons. Density functional theory (DFT) calculations are employed to unravel the underlying electronic changes induced by Fe doping in ZnO. The formation of shallow donor levels below the conduction band originates from the Fe 3d state. Photoluminescence spectra of pristine and Fe-doped ZnO nanostructures show characteristic emission peaks at approximately 384 nm and 570 nm, indicating the recombination of free excitons and oxygen interstitial defects, respectively. The results of the photocatalytic activity tests confirm that the 1 % Fe-doped ZnO nanostructures can exhibit the highest efficiency compared to the heavily doped ZnO nanostructures. The high efficiency in photocatalytic activity of 1 % Fe-doped ZnO nanostructures is ascribed to the modulated electronic structure and defect density . The adsorption affinity of methylene blue and water molecules to the surfaces of pristine and Fe-doped ZnO is simulated using the Monte-Carlo method. This study emphasizes the importance of controlling the dopant concentration to enhance the photocatalytic activity of various photocatalysts . • Fe-doped ZnO nanostructures are synthesized as visible-light-active photocatalyst. • >3 % Fe doping leads to the formation of a secondary phase ZnFe 2 O 4 . • DFT calculations confirm the formation of a shallow donor level. • ZnO doped with 1 % Fe exhibits the highest photocatalytic activity. • Fe impurity states enhance visible light absorption and suppress the recombination.

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