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Gas Sensing Properties at Room Temperature of A Quartz Crystal Microbalance Coated with ZnO Nanorods
Tính nhạy khí ở nhiệt độ phòng của cảm biến vi cân tinh thể thạch anh được phủ thanh nano ZnO (For international authors, please make Vietnamese title “empty lines”. The secretary board may help you)

Le Thanh A1,2, Nguyen Van B1,*
1 Hanoi University of Science and Technology, No. 1, Dai Co Viet, Hai Ba Trung, Hanoi, Viet Nam
2 Viet Nam Atomic Energy Institute, No. 59, Ly Thuong Kiet, Hoan Kiem, Hanoi, Viet Nam


Abstract
Gas sensors based on a quartz crystal microbalance (QCM) coated with ZnO nanorods were developed for detection of NH3 at room temperature. Vertically well-aligned ZnO nanorods were synthesized by a novel wet chemical route at a low temperature of 90 ºC, which was used to grow the ZnO nanorods directly on the QCM for the gas sensor application. The morphology of the ZnO nanorods was examined by field-emission scanning electron microscopy (FE-SEM). The diameter and length of the nanorods were 100 nm and 3 µm, respectively. The QCM coated with the ZnO nanorods gas sensor showed excellent performance to NH3 gas. The frequency shift (Df) to 50 ppm NH3 at room temperature was about 9.1 Hz. It was found that the response and recovery times were varied with the ammonia concentration. The fabricated gas sensors showed good reproducibility and high stability. (from 100 to 150 words)
Keywords: QCM, ZnO nanorods, Gas sensing (from 3 to 5 keywords)
Tóm tắt (Abtract in Vietnamese)








Từ khóa (Keywords in Vietnamese):
(For international authors, please make Vietnamese abstract and key words “empty lines”. The secretary board may help you to translate it. Make sure that after adding Vietnamese title, abstract, and keywords, total page number do not exceed 6)

 


1. Introduction[*]

Refer page 4 for the detail format of article
 
In recent years, many semiconductor metal-oxide materials, such as SnO2, TiO2, CuO, and In2O3, have been used for gas sensors [1-5]. In these, the ZnO nanomaterial possesses certain unique properties, such as a direct band gap (3.37 eV), large exciton binding energy (60 meV), high thermal and chemical stability, transparence, biocompatibility, and wide electrical conductivity range [6-8]. Moreover, one-dimensional (1D) ZnO nanostructures have attracted much attention due to their large aspect ratio, which makes them a good candidate for gas sensing applications [9, 10]. Most gas sensors using semiconductor metal-oxide materials are based on the change in electrical conductivity with the composition of the surrounding gas atmosphere. Major challenges in conductivity-based gas sensors are the high operating temperature, poor gas selectivity, and unstableness. These sensors are based on the changes in electrical resistance of the materials upon gas adsorption. Thus, a high temperature is required for charge carriers of the semiconductor materials to overcome the activation energy barrier. Therefore, almost all conductivity-based gas sensors operate at high temperatures [2-4, 9,10].

2. Experimental

For fabrication of the QCM device, both-side polished AT-cut quartz crystal plates with dimensions of 25 × 20 mm2 and thickness of 300 μm were used. Two circular electrodes with diameters of 12 and 6 mm were deposited on both sides of the quartz plate by sputtering method and were patterned by the lithography technique. The circular electrodes were composed of a 40 nm Cr under-layer surface and a top 100 nm Au layer.
Vertically aligned ZnO nanorods were directly grown on the Au electrode of the QCM device by a wet chemical route. ZnO nanorods form by the hydrolysis of zinc nitrate in water in the presence of HMTA. The chemical reactions for the formation of the ZnO nanorods on ZnO-coated substrates are [26].
3. Results and disscution
Fig. 2 shows a photograph and the resonant characteristics of the as-fabricated QCM device using AT-cut quartz crystal plate as a precursor substrate. The AT-cut quartz crystal is well known as a piezoelectric material suitable for the QCM due to its high sensitivity to mass change on the surface. The resonant frequency (fo) in this work was evaluated from the conductance peak. It has been observed that the conductance versus frequency curve shows a fundamental resonance peak at 5.48 MHz (Fig. 2b). The ZnO nanorods were then grown on one side of the Au electrode-coated QCM by the wet chemical route. Fig. 3 shows SEM images of the top-view (3a) and side-view (3b) of as-grown ZnO nanorods on the Au electrode of the QCM. The morphology of the ZnO nanorods with a hexagonal structure was vertically well-aligned and uniformly distributed on the Au electrode of the QCM. This shows that the exposed area of the sensing layer was remarkably enhanced compared with the sensing layer of the ZnO nanowires [1]. The average diameter and length of ZnO nanorods were around 100 nm and 3 mm, respectively. In comparison with the ZnO nanowires that were first synthesized by evaporating high purity zinc pellets at 900 ºC and were then distributed on the QCM [2], the wet chemical route has many advantages such as low cost, low temperature operation, high preferred orientation, and environmental friendliness. This method can also directly grow ZnO nanorods with high uniform distribution on a large area.
Table 1. The main components of fresh cassava
Main components
Composition base on dry weight (%, w/w)
Water concentration
58.6 - 59.9
Starch
28 - 31
Fig. 5a shows the response transients of the ZnO nanorod-coated QCM sensor to switching-on and off of the NH3 gas-flow with different concentrations (50, 100, and 200 ppm) at room temperature (25 ºC). In the first stage, the sensor flushed a reference air gas flow of 15 sccm to obtain a baseline. The sensor was then exposed to a NH3 gas flow of 15 sccm with a certain concentration, which leads to frequency response until a steady stage was reached, indicating maximum adsorption of NH3 gas onto the QCM sensor. The NH3 gas flow was finally replaced by the air gas flow and the sensor returned back to its baseline. In this experiment, the flow rate of the diluted ammonia gas and dry air was fixed at 15 sccm. Hence, in the gas sensing chamber, the flow and pressure were ensured to be constant. The change in resonant frequency of a QCM (∆f) can be related to the change in mass (∆m) due to the adsorption of NH3 gas.

 
Fig. 1. SEM images of ZnO nanorods grown by wet chemical bath deposition: (a) top-view and (b) side-view. (Figure’s colors are black and white only)


4. Conclusion
Vertically well-aligned ZnO nanorods were successfully grown on the Au electrode of QCM by the wet chemical bath deposition method. The ZnO nanorods were uniformly distributed on the substrate with a diameter and height of 100 nm and 3 mm, respectively. The sensor based on QCM coated with ZnO nanorods showed good interaction with ammonia and could detect low concentration of several tens of parts per million. The magnitude of the response of the fabricated sensor was directly proportional to the concentration of the ammonia. The result indicated the reproducible and reversible performance of the sensor.
Acknowledgments
This work was supported by the application-oriented basic research program.
References
[1]       X. Du, S.M. George, Thickness dependence of sensor response for CO gas sensing by tin oxide films grown using atomic layer deposition, Sens. Actuators B 135 (2008) 152-160.
[2]       Y.Z. Wang, B.L. Chu, Structural and optical properties of ZnO thin films on (111) CaF2 substrates grown by magnetron sputtering, Superlattices Microstruct. 44 (2008) 54–61.
[3]       P.A. Lieberzeit, A. Rehman, B. Najafi, F.L. Dickert, Real-life application of a QCM-based e-nose: quantitative characterization of different plant-degradation processes, Anal. Bioanal. Chem. 391 (2008) 2897–2903.
[4]       X. Du, S.M. George, Thickness dependence of sensor response for CO gas sensing by tin oxide films grown using atomic layer deposition, Sens. Actuators B 135 (2008) 152-160.
[5]       Y.Z. Wang, B.L. Chu, Structural and optical properties of ZnO thin films on (111) CaF2 substrates grown by magnetron sputtering, Superlattices Microstruct. 44 (2008) 54–61.
[6]       P.A. Lieberzeit, A. Rehman, B. Najafi, F.L. Dickert, Real-life application of a QCM-based e-nose: quantitative characterization of different plant-degradation processes, Anal. Bioanal. Chem. 391 (2008) 2897–2903.


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[*] Corresponding author:  Tel.: (+84) 912.345.678
Email: jst@hust.edu.vn