Physical-Vapor-Deposited Metal Oxide Thin Films for pH Sensing Applications: Last Decade of Research Progress

Sensors (Basel). 2023 Sep 30;23(19):8194. doi: 10.3390/s23198194.

Abstract

In the last several decades, metal oxide thin films have attracted significant attention for the development of various existing and emerging technological applications, including pH sensors. The mandate for consistent and precise pH sensing techniques has been increasing across various fields, including environmental monitoring, biotechnology, food and agricultural industries, and medical diagnostics. Metal oxide thin films grown using physical vapor deposition (PVD) with precise control over film thickness, composition, and morphology are beneficial for pH sensing applications such as enhancing pH sensitivity and stability, quicker response, repeatability, and compatibility with miniaturization. Various PVD techniques, including sputtering, evaporation, and ion beam deposition, used to fabricate thin films for tailoring materials' properties for the advanced design and development of high-performing pH sensors, have been explored worldwide by many research groups. In addition, various thin film materials have also been investigated, including metal oxides, nitrides, and nanostructured films, to make very robust pH sensing electrodes with higher pH sensing performance. The development of novel materials and structures has enabled higher sensitivity, improved selectivity, and enhanced durability in harsh pH environments. The last decade has witnessed significant advancements in PVD thin films for pH sensing applications. The combination of precise film deposition techniques, novel materials, and surface functionalization strategies has led to improved pH sensing performance, making PVD thin films a promising choice for future pH sensing technologies.

Keywords: metal oxide; pH sensor; sensitivity; thin film.

Publication types

  • Review

Grants and funding

The authors would like to acknowledge the support provided by Tenaga Nasional Berhad (TNB) and UNITEN through the Ministry of Higher Education of Malaysia (MOHE) for the support given with the HICoE grant for this research with the code 2022003HICOE at the iRMC of Universiti Tenaga Nasional (UNITEN), and the BOLD Refresh Postdoctoral Fellowships under the project code of J510050002-IC-6 BOLDREFRESH2025-Centre of Excellence and Dato’ Low Tuck Kwong International Energy Transition Grant under the project code of 202203005ETG. The authors also appreciate the academic support from the School of Science, Edith Cowan University, Australia, and the School of Engineering, Technology, Central Queensland University Australia, Melbourne, VIC 3000, Australia.