International Conference on Global Trends in Engineering, Technology and Management (ICGTETM-2016) Microwave –assisted Synthesis of Sb- doped ZnO Nanostructures for Gas Sensor Application Yogita S. Patil#1, F.C. Raghuvanshi*2, M. Ramzan#3 I. D. Patil*4 # Department of Applied Science, Government College of Engineering, Jalgaon-425002, India. 2 3 4 Principal, Vidya Bharati Mahavidyalaya, Amravati, India. Department of Mechanical Engineering, MMANTC College of Engg., Malegaon, India. Professor& Head, Department of Biotechnology, SSBT’s College of Engg., Bambhori, Jalgaon, India. Abstract-- ZnO and Sb-doped ZnO nanostructures were size and shape has been strongly motivated and novel applications can be investigated dependent on their structural properties [7–10]. Among various semiconductor nanostructures, variety of nanostructures of ZnO has been investigated presenting it as richest family of nanostructures. It crystallizes in a wurtzite structure and exhibits n-type electrical conductivity [11]. ZnO nanomaterials with one-dimensional structure, such as nanowires or nanorods, are specifically attractive due to their tunable electronic and opto-electronic properties, and the potential applications in the nanoscale electronic and optoelectronic devices [12]. Window layer [13], varistor [14], gas sensor [15-17], etc., are the reported Keywords- Sb-doped ZnO, microwave assisted synthesis, applications. Researchers are now probing on this nanostructures, thick films. material as one of the alternative photoanode for dyesensitized solar cells [18-20]. Zinc oxide has proven I. INTRODUCTION: Zinc Oxide (ZnO) is a wide-band gap semiconductor itself as one of the competitive and promising metal oxide with wide range of optical and electronic candidates to replace expensive materials like CdS, applications. It’s an n-type semiconductor of wurtzite TiO2, GaN, SnO2, and In2O3 for applications such as structure with direct band gap of about 3.37eV at solar cells [21], photocatalysis [22], ultraviolet laser room temperature. Polycrystalline ZnO has found [23, 24], transparent conductive oxides [25], numerous applications such as related to surface spintronics [26], and gas sensors [27]. For gas sensor acoustic wave devices, piezoelectric devices, varistors, application, SnO2 has been the most investigated planar optical waveguides, transparent electrodes, UV material. However, ZnO is particularly applicable to photo detectors, facial powders, gas sensors, etc. Out gas sensors because of its typical properties such as of these applications of ZnO, gas sensor devices have resistivity control over the range 10−3 to 10−5 cm, the sensitivity to various gases, high chemical stability, high electrochemical stability, absence of toxicity, and and suitability for doping, non-toxicity and low cost [1, abundance in nature [28]. Zinc Oxide nanostructures 2]. ZnO films have attracted considerable attention could be synthesized by several techniques such as due to its high electrical conductivity, high infrared vapour deposition, oxidation, sputtering, and pulse reflectance and high visible transmittance. Low laser deposition. Several deposition methods have resistive zinc oxide films have been achieved by been used to grow undoped and doped ZnO films such doping with different group III elements like as Spray pyrolysis, evaporation, chemical vapour aluminium, boron, indium, gallium or with group VII deposition, magnetron sputtering, pulsed laser elements like fluorine(1). Due to the transparency in deposition, sol-gel technique, screen printing the visible range, high electrical stability, direct band technique [29]. gap (3.37 eV), absence of toxicity, abundance in nature, etc., ZnO is one of the versatile and technologically important material [6]. Controlled synthesis of semiconductor nanostructures in terms of synthesized using microwave assisted precipitation method. Thick films of prepared powders were fabricated using screen printing method. The X-ray diffraction studies show that the nanostructures are crystallized in the form of hexagonal Wurzite crystalline phase and Sb-doping does not change the structure of ZnO. The size of nanostructures decreases with increasing the Sb+3-doping. Field emission scanning electron microscope (FESEM ) images show the change in morphology and size of nanostructures are changing with change in doping percentage of Sb+3. The UV- visible spectra shows the increase in band gap with increasing the Sb +3-doping percentage. The gas sensitivity of pure and Sb+3-doped ZnO nanostructures was studied. The gas sensitivity of the films was improved with the doping of 7% Sb+3 in ZnO. ISSN: 2231-5381 http://www.ijettjournal.org Page 645 International Conference on Global Trends in Engineering, Technology and Management (ICGTETM-2016) II. EXPERIMENTAL 2.1 Materials Zinc acetate (Zn (CH3COO) 2, H2O), antimony trichloride and sodium hydroxide from Loba Chemie (India) Pvt. Ltd. were used as precursor to synthesize ZnO nanostructure. The chemical reagents used were analytical reagent grade without further purification. All the glassware used in this experimental work was acid washed. Deionized water was used for sample preparation. 2.2 Synthesis of nanostructures: The ZnO nanostructures were synthesized in deionized water. In a typical experiment, 2g zinc acetate (Zn (CH3COO) 2, H2O), was dissolved in 110 ml deionized water and stirred magnetically until a homogeneous solution was obtained. Then 25 ml 2M sodium hydroxide (NaOH) was added drop by drop to above mixture. The stirring was continued for further 30 minutes after addition of 25 ml 2M NaOH to confirm that a white voluminous precipitate appeared. The solution was sonicated for 15 minutes in bath sonicator at 300 C and 52 KHz frequency. The milky suspension was irradiated in microwave for 2 minutes followed by air cooling, filtering and multiple washing with deionized water and absolute ethanol to remove impurities. The product was dried in hot air oven at 700 C for 24 hours. In case of preparing 5,7 and 9 % Sb+3-doped ZnO; an equivalent amount of antimony trichloride was added to the zinc acetate and the above procedure was repeated. 2.3 Thick Film Preparation The thixotropic paste was screen printed on glass substrate in desired patterns. Fluidity of the paste depends up on extent of organic part, which goes in its formulation i.e on solid to liquid ratio. Paste must exhibit a certain degree of yield such that after flow occurs under squeegee pressure, it should stiffen and remain in position to have sharp line defined patterns to be printed that should have thixotropic properties. In present process, thixotropic paste was formulated by mixing the synthesized ZnO powders with ethyl cellulose a temporary binder in a mixture of organic solvents such as butyl cellulose, butyl carbitol acetate and turpineol. The ratio of ZnO to ethyl cellulose was kept at 95:05. The ratio of inorganic to organic part was kept as 75:25 in formulating the pastes. The thixotropic pastes were screen printed on a glass substrate in desired patterns. The films prepared were fired at 500°C for 12 hr. Prepared thick films were called as pure ZnO and Sb-doped ZnO thick films. ISSN: 2231-5381 2.4 Characterization The X-ray diffraction (XRD) pattern of the powdered sample was recorded using X-ray diffractometer at room temperature. The crystallite size was estimated using the Scherer equation from full width at half maximum of the major XRD peak. The morphology, size and composition of nanostructure were determined by field emission scanning electron microscope (FESEM). The optical transmission/absorption spectra of nanostructure were recorded using UV-visible spectrophotometer. III. RESULTS AND DISCUSSION: 3.1 Morphological study The morphologies of prepared powder were investigated through field emission scanning electron microscope (FESEM). Fig. 1 shows some typical morphology of pure ZnO and ZnO doped with 5%, 7% and 9% Sb+3 respectively. It is observed that pure ZnO (Figure 1(a)), is in the form of flakes. ZnO flakes were randomly distributed. As the 5%, 7% and 9% Sb+3 was added to the reaction (Figure 1(b), 1(c), and 1(d)); the flakes became smaller and darker. The composition of the as-synthesized product was analysed by FESEM/EDAX. (a) (c) (b) (d) Fig. 1 FESEM images of (a) pure ZnO; (b) ZnO doped with 5% Sb+3; (c) ZnO doped with 7% Sb+3; (d) ZnO doped with 9% Sb+3 3.2 Structural study The crystallinity of grown nanoflakes was investigated by XRD pattern. Fig. 2 shows XRD patterns of pure and Sb+3-doped ZnO nanoflakes. Sharp intense peaks are obtained for ZnO nanoflakes. The peaks at scattering angles (2θ) of 31.4, 33.2, 35.1, 46.3, 55.4, 61.6 and 66.6 deg. corresponding to the reflection http://www.ijettjournal.org Page 646 International Conference on Global Trends in Engineering, Technology and Management (ICGTETM-2016) from (100), (101), (002), (102), (110), (103),(112), (201) crystal planes respectively are observed. These are associated with the hexagonal wurtzite structure of ZnO. As can be seen, pure ZnO has hexagonal Wurtzite structure and no peaks attributable to possible impuries are observed [30].The Sb+3-doped ZnO nanostructures have similar XRD patterns to that of pure ZnO and there are no characteristic peaks for separate phases of ZnO and Sb2O3. The average particle sizes, D were calculated by Debye Scherer’s formula [31], D=0.9λ/Bcosϴ Where λ is the wavelength of radition, B is full-widthat half- maxima in radians and ϴ is characteristic Xray radition.The average particle sizes of the nanostructures for pure, 5% Sb+3, 7% Sb+3, and 9% Sb+3 are about 29, 18, 12, 6 nm respectively. The particle size decreases with increasing the percentage of Sb-doping. Fig.3 UV-vis absorption spectra (a)Pure ZnO,(b)5% Sb +3doped,(c)7% Sb+3-doped,(d)9% Sb+3-doped 4. Gas Sensing Properties 4.1 Current-voltage characteristics of pure ZnO Figure (a) shows I-V characteristics of pure ZnO thick film which indicates ohmic contact. I-V Characteristics of Pure ZnO 1.20E-05 1.00E-05 8.00E-06 6.00E-06 Current (pA) 4.00E-06 2.00E-06 0.00E+00 -30 -20 -10 0 10 20 -2.00E-06 -4.00E-06 -6.00E-06 -8.00E-06 Voltage (V) Fig.2 XRD for (a)Pure ZnO,(b)5% Sb+3-doped,(c)7% Sb+3doped,(d)9% Sb+3doped 3.3 Optical property To study the optical quality of nanoflakes; optical absorption investigations were carried out. The pure ZnO with absorption maxima 357nm shows a blue shift relative to bulk ZnO with aborption peak of 384nm that can be due to the size effect of nanocrystalline ZnO. ISSN: 2231-5381 Fig.4(a) shows I-V characteristics of pure ZnO at room temperature. 4. 2 Gas respnce for pure and Sb+3 doped ZnO thick films The gas response of the sensor was defied as the ratio of the change in conductance of a sample upon exposure to the target gas to the original conductance in air. Figure 4(b) shows the gas responses of ZnO thick films to 300 ppm for LPG, NH3,CO2, H2, Cl2 gases. Figure 4(b) also indicates that 7% Sb+3-doped ZnO have maximum gas response (493) to 300 ppm NH 3, whereas pure, 5% Sb+3 doped, 9% Sb+3-doped has minimum gas response to NH3 gas. The higher response of 7% Sb+3- doped ZnO nanostructure upon exposure to NH3 may be attributed to the decrease in http://www.ijettjournal.org Page 647 30 International Conference on Global Trends in Engineering, Technology and Management (ICGTETM-2016) concentration of oxygen adsorbents ( Oad2- ) and a resulting increase in concentration of electron. The gas response was mainly dependent upon two factors. The first was the amount of active sites for oxygen and the reducing gases on the surface of the sensor materials. V. [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] Fig. 4 (b) Gas responses of (a) Pure ZnO,(b) 5% Sb+3-doped,(c) 7% Sb+3-doped,(d) 9% Sb+3-doped ZnO thick films. [12] [13] IV. CONCLUSION: It can be concluded, from the above discussion, that pure and Sb+3-doped nano ZnO can be successfully synthesized by microwave assisted method. Surface roughness and smoothness morphology was clearly observed in FESEM which shows ZnO nanoflakes and hexagonal wurtzite structure. The average particle sizes of the nanostructures for pure, 5% Sb+3, 7% Sb+3, and 9% Sb+3 are about 29, 18, 12, 6 nm respectively. The particle size decreases with increasing the percentage of Sb-doping. The thick films are successfully prepared on glass substrate, The I-V characteristics of pure ZnO thick film indicates ohmic contact. The gas sensing characteristics are studied for pure and Sb+3-doped ZnO, 7% sb+3- doped ZnO shows gas response to NH3 gas for 300 ppm at 200 oC. [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] ISSN: 2231-5381 REFERENCES K. L. Chopra, S. Major and D. K. Pandya, Thin Solid Films, 1983, Vol. 102, Iss.1, 1-96.Chandrakant Dighavkar Arch. 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