Generation of oxygen vacancies in ZnO nanorods/films and their effects on gas sensing properties
Introduction
Gas sensors based on metal oxides, such as SnO2, TiO2, and ZnO, have attracted much attention due to their high sensitivity, low cost, and simple fabrication [1], [2], [3]. Since Seiyama et al. [4] discovered that the adsorption and desorption of gases produced rapid and remarkable changes in the electrical conductivities of semiconductors, several studies of the utility of semiconducting metal oxide materials as gas sensors have been reported [5], [6], [7], [8]. ZnO is one of the most promising metal oxide materials for this purpose due to its thermal and chemical stability under standard operating environments, its high conductivity, and its non-toxic properties [8], [9], [10], [11], [12], [13], [14], [15], [16], [17]. ZnO gas sensors have been intensively investigated recently, and films have been fabricated in a variety of structures, including as single crystals, thick/thin amorphous films, nanorod arrays, and nanotube assemblies [14], [15], [16], [17]. The general gas sensing mechanism underlying metal oxide sensor function involves a resistance change through a reaction between the oxygen species () chemisorbed onto the metal oxide surface and the target gas molecules. Under ambient air conditions, the surface of a metal oxide material is covered with charged oxygen species that accept charge carriers (electrons) to form a depletion region on the surface. As these species react with reducing agents, oxygen species are desorbed from the surface and release the trapped electrons, which reduces the film thickness in the depletion region and, consequently, the resistance. As the surface coverage of adsorbed oxygen species increases, the gas sensing response is expected to increase as well. Although the surface oxygen species density usually varies with the surface area, however, the main factors that affect the adsorption of oxygen species are the surface atomic structures related to the exposed facets and the surface defect densities, including zinc and oxygen vacancies [9], [14], [18].
Oxygen vacancies are the predominant native defect present on metal oxide surfaces. Oxygen vacancies play an important role in metal oxide function, including ZnO, because they act as shallow donors with substitutional hydrogen atoms that exhibit n-type conductivity [19]. In addition, surface oxygen vacancies can present strong adsorption sites for oxidizing molecules. The surface oxygen vacancy density depends on the type of exposed facet of material [20]. For example, wurtzite ZnO nanorods have exposed surfaces with a top hexagonal plane corresponding to the polar (0 0 0 1) surface and side planes corresponding to the non-polar surfaces. In general, the top (0 0 0 1) surface has more oxygen vacancies than the side surfaces; hence the reactivity on the (0 0 0 1) surface is higher than on the side surfaces [21]. Recent gas sensing studies reported that varying the exposed facets, surface areas, or aspect ratios may be used to control the surface oxygen vacancies [9], [18], [22]. It is difficult, however, to claim that oxygen vacancies alone contributed to the enhanced sensing properties; possibly other factors could be involved during changing structures or surface areas, and thus a systematic analysis of the effects of oxygen vacancies is needed. Few studies have attempted to control the oxygen vacancies alone as a means for enhancing the sensing properties. The introduction of stable oxygen vacancies at a surface poses several challenges.
Nanomaterials, especially one-dimensional (1D) nanostructures, provide good sensing properties because of their high surface-to-volume ratio (resulting from a high nanostructure aspect ratio), which facilitates the adsorption of oxygen groups and rapid transport of charge carriers. Many reports have attempted to improve the gas sensing properties of a device by introducing 1D nanostructures [8], [9], [10], [11], [12], [13], [14], [15]. The effects of the nanostructures, however, are not yet fully understood because the gas sensing properties can vary with the crystal size, morphology, fabrication method, and applied processing steps. In most cases, the synthesis of nanostructures requires high temperatures or complicated processes. The reproducibility of nanostructure synthesis tends to be poor.
In this work, we fabricated ZnO nanorod arrays using a simple hydrothermal method and investigated the gas sensing properties of these arrays in comparison with the corresponding properties of a ZnO film. The responses of the ZnO gas sensors were found to improve upon introduction of the ZnO nanorod arrays, and the surface preparation was highly reproducible. The target gas tested here was ethanol, which reacts with oxygen to form CO2 and H2O. The ZnO structures were used to develop oxygen vacancy-containing ZnO gas sensors through application of a post-treatment process with H2O2 and annealing. These studies revealed the mechanism underlying the contributions of oxygen vacancies to the gas sensing properties. The generation of surface oxygen vacancies was confirmed by performing a variety of analyses. The analytic results and gas sensing properties were compared to establish the relationship between the oxygen vacancies and the responses of the ZnO gas sensors.
Section snippets
Experimental
ZnO-based gas sensors were fabricated by depositing two gold electrodes (0.7 cm × 0.4 cm) 1 mm apart onto a 2 cm × 1 cm quartz substrate. A 1 μm thick ZnO film was deposited onto a part of the substrate using RF sputtering. The gap between the two distinct gold electrodes acted as a sensing layer, and this region also acted as a seed layer for ZnO nanorod array growth to form the ZnO nanorod gas sensor. ZnO nanorod arrays were grown on the seed layers using an ammonia solution method. The precursor
Results and discussion
Fig. 1(a) schematically illustrates the procedure used to fabricate the ZnO-based gas sensors. The ZnO film and nanorod gas sensors were prepared by depositing a ZnO film and growing an array of ZnO nanorods on gold electrodes. Ag paste was used to connect the electrodes, and gold wires were used to transfer the electrical signals to the I–V measurement system. Fig. 1(b) and (c) presents cross-sectional SEM images of a ZnO film and an array of ZnO nanorods. A uniform 1 μm thick ZnO film was
Conclusions
We investigated the effects of the surface area and oxygen vacancies on the gas sensing properties of ZnO nanorods/films. The ZnO nanorod array gas sensors exhibited enhanced gas sensing properties, compared with the ZnO film, in the presence of ethanol gas. H2O2 pretreatment and annealing processes produced oxygen vacancies on the ZnO surface. The presence of the oxygen vacancies were confirmed by XPS and PL analyses and were found to shift the light absorption edge toward longer wavelengths.
Acknowledgment
This work was supported by the National Research Foundation of Korea (2013-R1A2A2A05-005344).
Wooseok Kim is currently a PhD student in chemical engineering at Pohang University of Science and Technology (POSTECH). He also received bachelor of science (BS) degree from chemical engineering at POSTECH in 2010 and started integrated course of master of science (MS) degree and PhD degree. His research activities focus on surface chemistry of ZnO and gas sensors.
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Wooseok Kim is currently a PhD student in chemical engineering at Pohang University of Science and Technology (POSTECH). He also received bachelor of science (BS) degree from chemical engineering at POSTECH in 2010 and started integrated course of master of science (MS) degree and PhD degree. His research activities focus on surface chemistry of ZnO and gas sensors.
Mingi Choi is currently a PhD student in chemical engineering at Pohang University of Science and Technology (POSTECH). He received bachelor of science (BS) degree from materials science and engineering at POSTECH in 2012 and started integrated course of master of science (MS) degree and PhD degree. His research activities focus on synthesis of TiO2 and applications in energy devices.
Kijung Yong is a professor in chemical engineering department at POSTECH. He obtained his PhD degree from chemical engineering at Carnegie Mellon University in 1997. His research interests are semiconductor nanowire growth and applications in energy, sensor and electronic devices, and he has published over 120 SCI journal papers.