Enhancing low-temperature H<sub>2</sub>S sensing performance of SnO<sub>2</sub> quantum wires <i>via</i> transition metal doping and oxygen vacancy engineering
Doping impurity atoms into metal oxide semiconductors plays a crucial role in modulating both their electronic and chemical properties at active sites. Tin oxide (SnO<sub>2</sub>) quantum wires (QWs), with their large surface area and numerous exposed active sites, have shown significant potential as sensing materials for gas sensors. However, challenges such as unsatisfactory selectivity and detection limits (LODs) still hinder their performance. In this study, we explore the electronic interactions between transition metal atoms (V, Nb, or Ta) and sub-nm ultrathin SnO<sub>2</sub> QWs, while also introducing oxygen vacancies to enhance H<sub>2</sub>S sensing performance. The resulting tailored electronic structures lower the energy barrier for gas molecule adsorption and electron transport, promoting the activation of oxygen and accelerating surface reaction kinetics with H<sub>2</sub>S molecules. Notably, the Ta-doped SnO<sub>2</sub> QWs demonstrate significantly improved low-temperature H<sub>2</sub>S sensing, with a real LOD reaching sub-ppb level, surpassing most reported metal oxide-based sensors. This work provides new insights into the development of high-performance gas sensors through the rational manipulation of electronic structures.
Authors
- Jiazhen Zhang (ORCID: https://orcid.org/0000-0002-6905-7916)
- Kunming Yang
- Yi Tian (ORCID: https://orcid.org/0000-0003-0180-7482)
- Zhilong Song (ORCID: https://orcid.org/0000-0002-4755-7776)
- Weihao Fang
- Jia Yan (ORCID: https://orcid.org/0000-0001-7312-6323)
- Yue Kang
- Zhu Bingchen
Institutions
- Jiangsu University (CN)
- Jiangsu University of Science and Technology (CN)
Publication Details
- Journal
- Nanoscale
- Published
- 2025-01-01
- DOI
- https://doi.org/10.1039/d5nr02580j
- Citations
- 3
- Primary Topic
- Gas Sensing Nanomaterials and Sensors
- Type
- article
- Field-Weighted Citation Impact
- 2.19