Xiumei Xuab,
Haijiao Zhanga,
Chaozheng Hea,
Chunying Pua,
Yumin Lenga,
Genquan Lia,
Shujin Houa,
Yongsheng Zhu*a,
Ling Fu*a and
Geyu Lu*b
aCollege of Physics and Electronic Engineering, College of Chemistry and Pharmaceutical Engineering, College of Agriculture Engineering, Nanyang Normal University, Nanyang, 473061, China. E-mail: yongshengzhu0001@163.com; ful@nynu.edu.cn
bState Key Laboratory on Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, 2699 Qianjin Street, Changchun 130012, China
First published on 28th April 2016
In this work, a low-cost and environmentally friendly solvothermal route to the synthesis of indium oxide nanorod clusters was described in the presence of sodium chlorate and urea. The morphologies and structures of the as-prepared samples were characterized by X-ray powder diffraction (XRD), field emission scanning electron microscopy (FESEM), transmission electron microscopy (TEM), and high-resolution transmission electron microscopy (HRTEM). The results clearly revealed that the as-prepared indium oxide was composed of nanorods with a diameter of about 15 nm. The gas sensing properties of the as-prepared indium oxide samples were tested towards various gases. The indium oxide nanorod cluster based sensor showed high response and good selectivity toward NO2 at an operating temperature of 150 °C, giving a response of about 41 to 500 ppb.
Over the past decades, the design and development of gas sensors with high sensing performance has been a research hotspot. Thanks to the advances in nanotechnologies and synthetic methods, various kind of sensing materials, such as metal-oxide semiconductors,7–10 polymers,11,12 carbon nanotubes,13–15 active molecular plasmonics16 and their composite materials,17 have been developed and applied in gas sensors. Especially various kinds of metal oxides, such as ZnO, α-Fe2O3, WO3, In2O3, SnO2, NiO, etc. have been extensively investigated as sensing materials owing to their superior stability, low cost, and simplicity in preparation.
Metal oxides are the basis of functional materials that have tunable properties and important technological applications. Among them, as a very important wide-band-gap n-type semiconductor, In2O3 has been extensively studied for various applications, including window heaters, solar cells, liquid-crystal displays, and gas sensors for detection of CO, O3, Cl2, CO2, H2S, VOCs and NO2.18 Among most of the potential applications, the morphology and structure of the nanomaterials will undoubtedly play the pivotal role in determining their properties. The unique structures may show new properties and promising applications in many fields. Thus, over the past decades, several groups have synthesized In2O3 micro- and nanostructures with different morphologies by various preparation routes, including thermal evaporation,19,20 hydrothermal reaction,21 chemical coprecipitation22 and sol–gel method.23 Therefore, researchers are actively engaged in developing indium oxide nanostructures with different sizes and shapes in various applications, such as hollow microspheres, nanowires, nanobelts, nanotubes, nanocubes, nanofibers, nanosheets and complex hierarchical structures constructed with nanoscale building blocks.
Herein, we report a facile method for the preparation of In2O3 nanorod clusters by a simple solvothermal process. The diameter of In2O3 nanorod clusters was about 15 nm. Gas-sensing properties of the as-obtained In2O3 products are also investigated. The sensor based on the as-obtained In2O3 exhibited superior sensing performance to low concentration NO2 at 150 °C.
X-ray power diffraction (XRD) analysis was conducted on a Rigaku D/max-2500 X-ray diffractometer with Cu Kα1 radiation (λ = 1.540 Å) in the range of 20–70°. The mean crystallite size was calculated using the Debye–Scherer formula, D = 0.89λ/(βcos
θ), where λ is the X-ray wavelength, θ is the Bragg diffraction angle and β is the peak width at half maximum. The specific surface area was estimated using the Brunauer–Emmett–Teller (BET) equation based on the nitrogen adsorption isotherm obtained with a Micromeritics Gemini VII apparatus (Surface Area and Porosity System). Samples were degassed under vacuum at 200 °C for 4 h prior to the measurements. The pore size distribution was determined with the Barrett–Joyner–Halenda (BJH) method applied to the desorption branch of adsorption–desorption isotherm. Field emission scanning electron microscopy (FESEM) images were recorded on a JEOL JSM-7500F microscope operating at 15 kV. Transmission electron microscopy (TEM), selected-area electron diffraction (SAED), and high-resolution transmission electron microscopy (HRTEM) measurements were obtained on a JEOL JEM-2100 microscope operated at 200 kV.
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Fig. 1 (a) Schematic image of the In2O3 sensor and (b) ceramic tube images (without gas sensing materials), (c) structure of the gas sensor. |
The morphology of the samples was investigated by field emission scanning electron microscopy (FESEM). Fig. 3 shows typical FESEM images of the sample In2O3 at different magnification. The low magnification FESEM image (Fig. 3a) clearly displayed that the products are composed of nanorod clusters. No other morphologies can be found in Fig. 3a, which indicated the high uniformity of the as-obtained products. The detailed morphology information about In2O3 is presented in an enlarged-magnification FESEM (Fig. 3b–d), it can be observed that the diameter of nanorod clusters was about 15 nm.
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Fig. 3 FESEM images of the as-synthesized In2O3: (a) a panoramic and (b) an enlarged of a part of samples. (c and d) High-magnification FESEM image of In2O3 nanorod clusters. |
Further detailed structural analysis of products was carried out using TEM. Fig. 4a shows the TEM image of representative In2O3 nanorod clusters. It can be seen that the size and shape of product were similar to those of the FESEM observations. A high-magnification TEM (Fig. 4b) image presents that the diameter of these nanorods was about 15 nm. The selected-area electron diffraction (SAED) pattern of an individual In2O3 nanorod (Fig. 4c) confirms that the as-synthesized products were polycrystalline in structure. The high-resolution transmission electron microscopy (HRTEM) image (inset of Fig. 4b) showed fringe distance of 0.292 nm, corresponding to the lattice distances of the (222) plane of cubic In2O3. Fig. 4d shows the high angle annular dark field (HAADF) image of the In2O3 sample and Fig. 4e and f show the corresponding EDX elemental mapping of In and O, respectively. It was observed that In and O are uniform and homogeneous.
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Fig. 5 Correlations between the gas response and response time to 0.5 ppm NO2 and the operating temperature for the sensor using the as-obtained In2O3. |
This tendency indicates that fast response can be obtained through increasing the operating temperature. However, when the operating temperature is too high, the gas response decreases sharply. The decrease of the response at higher temperatures may be attributed to the decrease in number of active sites for the adsorption of NO2. Since at high temperature larger amount of oxygen molecules dissociate and adsorb on the active sites, the free active sites for the adsorption of NO2 molecules can be sharply reduced the response to NO2 becomes smaller. Another possibility may be that at such higher temperature the rate of adsorption is lower as compared to desorption.23–25 Accordingly, considering two aspects including the larger gas response and faster response speed of the sensor to 0.5 ppm NO2, the optimum operating temperature for the sensor using the as-obtained In2O3 is believed to be 150 °C, which is applied in all the investigations hereinafter. The response transients of the In2O3 nanorod clusters sensor to 0.5 ppm NO2 was measured at 150 °C (Fig. 6), the response time and recovery time were about 50 s and 30 s, respectively. The four reversible cycles of the response curve indicated a stable and repeatable response characteristic, as shown in the inset of Fig. 6. It can be observed that the average response was 41 to 500 ppb NO2.
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Fig. 6 Response transients of the sensor to 0.5 ppm NO2 at 150 °C, the inset displaying four periods of response curve. |
The dynamic response resistances of the sensors based on In2O3 nanorod clusters (Fig. 7a) to different NO2 concentration were investigated at 150 °C. The resistance of the sensor increases upon exposure NO2, whereas it decreases upon the removal of NO2. Furthermore, the response of the sensor to NO2 increased with the increasing of the NO2 concentration. The sensor can detect 50 ppb NO2, and the response is about 4. The responses to 0.1, 0.2, 0.3, 0.4 and 0.5 ppm NO2 were about 7, 14, 20, 29 and 41, respectively. Even in ppb level of NO2 concentration (e.g. 50 ppb), the In2O3 nanorod clusters sensor shows an acceptable response from the view of the practical application. Many models have been proposed to describe the sensing behavior of metal oxides. When the process is mainly controlled by diffusion, the response of semiconductor oxide type gas sensor can be empirically represented as S = 1 + Ag(Pg)β, where Pg is the target gas partial pressure, which is directly proportional to the gas concentration, Ag is a prefactor, and β is the exponent on Pg.26,27 Generally, the exponent β has an ideal value of either 0.5 or 1, which is derived from the surface interaction between chemisorbed oxygen and reducing gas to n-type semiconductor.28,29 Fig. 7b shows a chart of the sensor response versus the NO2 concentration. The linear fitting was quite good, and the correlation coefficient R of the sensor fit curve was 0.998. A comparison between the sensing performances of the sensor and the literature reports30–36 is summarized in Table 1. From the table, it can be observed that the sensor based on the nanorod clusters In2O3 has a correspondingly higher gas response and lower working temperature.
Sensor material | NO2 concentration | Working temperature | Response | Reference |
---|---|---|---|---|
WO3 nanosheets | 0.1 ppm | 150 °C | ∼7 | 30 |
WO3 thin films | 10 ppm | 150 °C | ∼57 | 31 |
In2O3 microspheres | 20 ppm | 250 °C | ∼36 | 32 |
Zn-Doped In2O3 | 50 ppm | 300 °C | 821.7 | 33 |
Porous In2O3 | 50 ppm | 250 °C | 164 | 34 |
Fe-Doped In2O3 | 1 ppm | 150 °C | 71 | 35 |
In2O3 nanofibers | 100 ppm | 300 °C | 1.8 | 36 |
In2O3 nanorod clusters | 500 ppb | 150 °C | 41 | Present work |
Selectivity is an important parameter for gas sensor. Fig. 8 showed the cross-sensitivities of the sensor using the In2O3 nanorod clusters to various gases, including NH3, O3, H2S, CO, SO2, Cl2, and C2H5OH. It is clear that the In2O3 sensor exhibits the largest response to NO2 among the tested gases. Such result indicates that the sensor using the In2O3 nanostructure exhibits an excellent selectivity to NO2 against the other tested gases at the working temperature of 150 °C. For most semiconducting oxide type gas sensors, the change in resistance is primarily caused by the chemical adsorption and reaction of the gas molecules on the surface of the sensing material. The sensitivity of indium oxide towards NO2 is generally attributed to an adsorption effect. Indium oxide surfaces tend to strongly adsorb NO2, mostly as nitrato (NO3) species, which replace the oxygen at the surface, some of the NO2-related nitrato adsorbates are very stable with high binding energies. By first principles calculations,37,38 a high net charge transfer from the semiconductor to these adsorbates was determined, thus explaining the pronounced conductivity drop in the presence of NO2. In this work, this special In2O3 nanorod clusters will provide offer abundant active sites for diffusion, chemisorptions and reactions of NO2, then achieve high sensitivity. The more detailed reason and qualitative explanation need further investigation.
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