The design of semiconductor catalysts with excellent photocatalytic properties, stability, recyclability, and good separation for the treatment of polluted water is still challenging. In this paper, the ZnO/TiO nano-thin films were fabricated using the magnetron sputtering technique and then heating the underlying ZnO layer and the upper TiO layer for their respective optimal heating time, i. e. heating ZnO for 3 h and heating TiO for 2 h. The as-prepared films were characterized. The results show that the preferred growth of TiO grains along the [001] axis, relatively large specific surface area, and increased amounts of surface oxygen vacancies (OVs) were induced to the heterojunction catalysts through this optimized heating strategy, which boosts the photocatalytic activity of ZnO/TiO nano-film. The degradation experiment inndicates that the ciprofloxacin (CIP) removal efficiency can reach 97.3% in 2 h duration, which was higher than that of the samples annealed for the same periods. Meanwhile, the prepared ZnO/TiO photocatalytic film exhibited favorable stability of 95.5% degradation efficiency after the fourth run and general applicability for the photodegradation of various contantains, whih removed 99.5% of ofloxacin (OFX) and 77.6% of tetracycline (TC) in 2 h and 94.1% of Rhodamine B (RhB) in 1 h. This work is expected to yields a novel insight into the production of heterojunction photocatalysts with excellen ability for photocatalytic degradation of pollutants in the practical industry.
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http://dx.doi.org/10.1016/j.chemosphere.2023.140392 | DOI Listing |
Chemosphere
January 2024
School of Mechanics and Engineering Science, Zhengzhou University, Zhengzhou 450001, China. Electronic address:
The design of semiconductor catalysts with excellent photocatalytic properties, stability, recyclability, and good separation for the treatment of polluted water is still challenging. In this paper, the ZnO/TiO nano-thin films were fabricated using the magnetron sputtering technique and then heating the underlying ZnO layer and the upper TiO layer for their respective optimal heating time, i. e.
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