ZnO:Sn Thin Films Gas Sensor For Detection of Ethanol

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ZnO:Sn Thin Films Gas Sensor For Detection of Ethanol Salah. Q. Hazaa*, Sabah. A. Salman**, Sura. J. Abbas** *Department of Physics, College of Education, Al- Mustansiriyah University **Department of Physics, College of Science, University of Diyala Iraq Abstract In this research, undoped ZnO and doped with Sn (ZnO:Sn) thin films with different weight percentages of (1, 3, 5)% have been prepared on pre-heated glass substrates up to (400 ) with average thickens (400 nm) by using Atmospheric Pressure Chemical Vapor Deposition (APCVD) technique. The effect of Sn-doping on structural properties and the ethanol vapor gas sensing has been investigated. The results of XRD showed that the all deposited films are polycrystalline hexagonal structure with a preferred orientation in the (002) direction, the doping with Sn does not change crystal structure of ZnO. The increase in the dopant concentration into the ZnO leads to an increase of the crystallite size of the films which is well known causes to increase the gas sensitivity. The effect of operating temperature on performance of the sensor material has been investigated and a choice of optimum temperature was made at around (200 C). Introduction Metal oxide semiconductor sensors have advantages of small size, low mass, good sensitivity and low cost, gas sensors based on the semiconducting metal-oxides such as SnO 2 and ZnO ]1-5[ have been Found to be very useful for detecting ethanol vapor. ZnO is one of the metal oxide semiconductors suitable for use in optoelectronic devices, as an alternative material to tin oxide and indium tin oxide. Pure zinc oxide is an intrinsic semiconductor with high electrical resistivity and adirect band gap of about (3.2 ev) at 298K ]6,7[ which is an n-type (II-VI) group compound with a wurtzite structure semiconductor. Zinc oxide thin films have a wide range of applications such as gas sensors, solar cell windows, and surface acoustic-wave devices [8-10]. Pure and doped ZnO films have been investigated as sensors for O 2 [11,12], H 2 [13], No x [14-15], and ethanol [16]. One of the requirements of the gas sensors is low power consumption, because the sensors need to work reliably and continuously. It is well known that the sensing mechanism of semiconducting oxide gas sensors is based on the surface reaction and a high surface volume ratio. The grain size and the porosity of the sensing material are the most important factors for high sensitivity and short response time sensors. Appropriate donor doping can produce the electronic defects that increase the influence of oxygen partial pressure on the conductivity. Nanto et al. showed that a lower operating temperature may be achieved by the doping effect, and a significant resistance change can be obtained in the doped ZnO rather than the undoped ZnO sensor, which results in a higher sensitivity [17]. The aim of this work is to www.ijaetmas.com Page 72

produce high-quality Sn doped ZnO thin films for gas sensor application by APCVD method. Special attention was paid to the influence of the operating temperature and dopant concentration. Experimental part Undoped and Sn-doped ZnO thin films are prepared on a heated (400 o C) glass substrate by atmospheric pressure chemical vapor deposition (APCVD) technique. The base material in the preparation of undoped zinc oxide thin films was zinc acetate dehydrate [Zn (CH 3 COO) 2 2H 2 O] high purity 99.9%, supplied by (B.D.H. Laboratory chemicals group, Poole England). The dopant source of tin is [Sncl 4.5H 2 O] high purity 99.9%, supplied by (B.D.H Chemicals Ltd Poole England). The thickness is calculated by weight difference method. The gas sensing properties were evaluated at various operating temperatures, from (27-300), by measuring the changes of resistance of the sensor in air and in ethanol gas. The sensitivity in the experiment was defined as (S=Ra/Rg) where Ra is the sample resistance measured in the ambient environment while Rg is that under the test gas. Results and discussion The crystal structure and orientation of the ZnO thin film of the ZnO and ZnO:Sn samples were investigated using X-ray diffraction (XRD) patterns. The X-ray diffraction patterns for all films are shown in Fig.1 which indicates that the films are of polycrystalline in nature and exhibit single phase hexagonal wurtzite structure with a (002) preferred orientations, which suggests that the film is aligned with the c-axis oriented perpendicularly to the substrate surface. Doped sample, showed that the intensity of (002) peak is increased and peak becomes sharper, this can be explained by improvement of crystallinity. This suggests that the grain size becomes larger. The crystallite size was calculated using the Scherrer s equation and the estimated values are presented in table 1. www.ijaetmas.com Page 73

Fig (1) XRD patterns of ZnO and ZnO:Sn thin films at different Sn concentration. Table (1): crystallite size as a function of Sn concentration Sn% 0 1 3 5 G nm 21.69 41.39 21.68 38.09 The sensitivity of the gas sensor is defined as the capability of the sensor to respond the presence of a given gas concentration. Mathematically, the sensitivity (S) is defined by the formula; (S= R g /R air ) for redactor gas, and (S= R air /R g ), for oxidator gas, where R g and R air is the resistance of the sensor after and before passing the gas and reaches the saturation [18]. Fig. 2 shows the variation of sensitivity of the ZnO:Sn sensor with operating temperature in the range (27 300). The sensitivity of the ZnO:Sn ethanol sensor increases with the operating temperature up to (200 ) which is attributed to increase of crystallinity of films (mobility carriers increased). When the operating temperature is above 200, the sensitivity of the films decreased. The exothermic effect in the surface reaction of the oxide film with ethanol is difficult to proceed with increasing operating temperature above (200 ), thus decreasing has shown an increase in sensitivity value as the doping percentage increase up to (5%) at operating temperature 200. Fig 2. Variation of sensitivity as function of operating www.ijaetmas.com Page 74

temperature at different concentration of Sn. Fig3.variation of sensitivity as concentration of Sn at 200 operating temperature. Conclusion Highly textured pure and Sn doped ZnO films were prepared by PACVD. Gas sensing investigation reveals that Sn-doping can enhance the sensing properties of ZnO films gas sensor efficiently. From the gas sensor characterization studies, it is clear that the ZnO:Sn can be used as an ethanol sensor effectively. The optimized operating temperature for the ZnO:Sn film is 200 and Tin concentration 5%. References [1]- B. P. J. D.Costello,, R. J.Ewen, N.Guernion, N. M. Ratcliffe, "Highly sensetive mixed oxide sensors for the detection of ethanol", Sens. Actuators, B 2002, 87, 207-210. [2]- D. F.Paraguay, M. Miki-Yoshida, J. Morales, J. Solis, L. W. Estrada, "Influence of Al, In, Cu, Fe and Sn dopants on the response of thin film ZnO gas sensor to ethanol vapor", Thin solid Films, 2000, 373, 137-140. [3]- p.ivanov, E. Llobet, X. Vilanova, J. Brezmes, J. Hubalek, X. Correig, "Development of high sensitivity ethanol gas sensors based on Pt-doped SnO2 surfaces. Sens", Actuators, B 2004, 99, 201-206. [4]- X. L. Cheng, H. Zhao, L.H.Huo, S. Gao, J. G. Zhao, "ZnO nanoparticulate thin film: Preparation, characterization and gas-sensing property", Sens. Actuators, B 2004, 102, 248-252. www.ijaetmas.com Page 75

] 5[- J.Tamaki, T.Maekawa, S.Matsushima, N.Miura, N.Yamazoe, "Ethanol gas sensing Properties of Pd-La2O3-In2O3 thick film element", Chem. Lett., 1990, 3, 477-480. ] 6[- W. Hirschwald et al.," Current Topics in Material Science", Amsterdam, North Holland 1981. ]7[- O.Madelung, "Data in Science and Technology: Semiconductors Other Than Group IV Elements and III-V Compounds,New York: Springer, 1992. [8]- M. Pacio, H. Juárez, G. Escalante, G. García, T. Díaz, E. Rosendo, "Study of (100) orientated ZnO films by APCVD system", Materials Science and Engineering: B, 174 (1 3) October (2010)38-41. [9]- S. Wu, R. Ro, and Z.X. Lin, "Rayleigh surface acoustic wave modes of (100) ZnO films on (111) diamond", Applied Physics Letters, 94 (2009) 032908-1 032908-3. [10]- M. Malekia, and S.M. Rozatib, Dependence of ZnO nanostructured thin films properties on growth temperature by APCVD method. Acta Physica Polonica,128(3) (2015) 367-373. [11]- G. Sberveglieri, S. Groppelli, P. Nelli, F.Quaranta, A. Valentini, L.Vasanelli, "Oxygen gas sensing characteristics for ZnO(Li) sputtered thin films", Sensors and Actuators B, 7 (1992) 747-751. [12]- T. Yamazaki, S. Wada, T. Noma, T. Suzuki, "Gas-sensing properties of ultrathin zinc oxide films", Sensors and Actuators B: Chemical, 14 (1 3) June (1993) 594-595. [13]- A. Trinchi, Y.X. Li, W. Wlodarski, S. Kaciulis, L. Pandolfi, S.P. Russo, J. Duplessis, S. Viticoli, "Investigation of sol gel prepared Ga Zn oxide thin films for oxygen gas sensing", Sensors and Actuators A: Physical, 108 (1 3) November (2003) 263-270. [14]- A. Pimentel, E. Fortunato, A. Gonçalves, A. Marques, H. Águas, L. PereiraA, I. Ferreira, R. Martins, "Polycrystalline intrinsic zinc oxide to be used in transparent electronic devices ",Thin Solid Films 487(1-2) (2005) 212-215. [15]- V. Musat, A.M. Rego, R. Monteiro, E. Fortunato, "Microstructure and gas-sensing properties of sol gel ZnO thin films", Thin Solid Films, 516 (2008) 1512 1515. [16]- W.P. Tai, J.H. Oh, "Humidity sensing behaviors of nanocrystalline Al-doped ZnO thin by sol gel process", Journal of Materials Science: Materials in Electronics, 13 (7) (2002)391 394. [17]- H. Nanto, T. Minami, S. Takata, "Zinc-oxide thin film ammonia gas sensor with high sensitivity and excellent selectivity", Journal of Applied Physics, 60 (1986)482-484. [18]- A. Mirzaei, K. Janghorban, B.Hashemi, A. Bonavita, M. Bonyani, S.G. Leonardi and G. Neri, Synthesis, "Characterization and gas sensing properties of Ag@α-Fe2O3 core shell nanocomposites", Nanomaterials 5(2015) 737-749. www.ijaetmas.com Page 76