International Journal of Chemistry Research



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International Journal of Chemistry Research Vol 1, Issue 1, 2010 Research Article DEPOSITION AND CHARACTERIZATION OF MnS THIN FILMS BY CHEMICAL BATH DEPOSITION METHOD ANUAR KASSIM*, HO SOON MIN Department of Chemistry, Faculty of Science, University Putra Malaysia, 43400 Serdang, Selangor, Malaysia Email: anuar@science.upm.edu.my Received: 18 April 2010, Revised and Accepted: 01 May 2010 ABSTRACT The chemical bath deposition technique was used to deposit MnS thin films onto indium tin oxide glass substrate. During the deposition, manganese sulphate and thiourea were supplied Mn 2+ and S 2 ions, respectively. X ray diffraction and atomic force microscopy were used to investigate the structural and morphological properties of films, respectively. The band gap energy was determined using UV VIS spectrophotometer. The influence of bath temperature was investigated to determine the best conditions for deposition process. The deposited films showed cubic structure of MnS. The highest peak observed was (200) plane. The number of peaks referred to MnS increased as the bath temperature was increased from 35 to 65 C based on the XRD patterns. For the films deposited at lower bath temperature, the grains were small and thinner films to be formed. Conversely, for the films prepared at higher bath temperature, the grains were larger and thicker films to be formed. From the optical properties analysis, the band gap energy was to be dependent on the bath temperature. Keywords: Chemical bath deposition, Manganese sulphide, Thin films, X ray diffraction. INTRODUCTION Recently, extensive research has been devoted to prepare various kinds of semiconductor thin films such as MoSe2 1, CdSe 2, ZnS 3, CuS 4, Cd1 xfexse 5 and Cu4SnS4 6 by using several deposition methods. Manganese sulphide thin films have been used in variety of applications such as solar cells, sensor, photoconductors, optical mass memories and solar selective coatings. Over the past few years, many methods such as radio frequency sputtering 7, hydrothermal 8, SILAR 9 and chemical bath deposition method 10 13 have been used to prepare manganese sulphide thin films. Among various deposition methods, chemical bath deposition method has been identified as simple and low cost thin films deposition method with many advantages. Up to date, chemical bath deposition method has been successfully used to deposit various thin films including PbS 14, CdTe 15, ZnSe 16, CdS 17, Ni4S3 18 and As2S3 19. Chemical bath deposition method is based on the controlled precipitation from solution of a compound on a suitable substrate. The substrates are immersed either in an alkaline or acidic solution which containing the metal ion, chalcogenide source and a complexing agent. The present work reports the preparation and characterization of MnS thin films onto indium tin oxide glass substrates using chemical bath deposition method. The chemical bath contains manganese sulphate and thiourea which provide Mn 2+ and S 2 ions, respectively. It is the first time, we report the influence of bath temperature (35 to 65 C) on the MnS thin films in the presence of triethanolamine as a complexing agent. The results of the investigation on structural and morphological properties of thin films have been carried out by using X ray diffraction and atomic force microscopy, respectively. The band gap energy and absorption properties were determined using UV VIS spectrophotometer. MATERIALS AND METHODS All the chemicals used for the deposition were analytical grade reagents and all the solutions were prepared in deionised water (Alpha Q Millipore). The manganese sulphide thin films were prepared from an alkaline bath using aqueous solutions of manganese sulphate [MnSO4] and thiourea [SC(NH2)2] acted as a source of Mn 2+ and S 2 ions, respectively. The triethanolamine was served as a complexing agent to chelate with Mn 2+ to obtain Mn TEA complex solution. The indium tin oxide (ITO) glass was used as the substrate for the chemical bath deposition of MnS thin films. Before deposition, the ITO glass was degreased with ethanol for 15 min. Then, ultrasonically cleaned with distilled water for another 15 min and dried in desiccators. Deposition of MnS thin films was carried out using following procedure. 30 ml of manganese sulphate (1 M) was complexed with 5 ml of concentrated triethanolamine solution. To this, 30 ml of thiourea (1 M) was added slowly to the reaction mixture. The ph was adjusted to 11 by adding drop wise ammonia/ammonium chloride (buffer solution). The cleaned ITO glass substrate was immersed vertically into beaker. In order to determine the best conditions for the deposition process, the films were deposited at different bath temperatures, ranging from 35 to 65 C. During deposition process, the beaker was kept undisturbed. After the completion of deposition (7 h), the glass substrate was removed, washed several times with distilled water and dried naturally in desiccators for further characterization. The structure of the films was monitored by X ray diffraction (XRD) with a Philips PM 11730 diffractometer equipped with a CuKα (λ=0.15418 nm) radiation source. Data were collected by step scanning from 20 to 70 with a step size of 0.05 (2θ). The surface morphology, thickness and roughness were examined by recording atomic force microscopy images with a Q Scope 250 in contact mode with a commercial Si3N4 cantilever. Values of root mean square (RMS) roughness were calculated from the height values in the atomic force microscopy images using the commercial software. The optical properties of the film were measured with a Perkin Elmer UV/Vis Lambda 20 Spectrophotometer in the wavelength range of 300 to 800 nm. The film coated indium tin oxide glass was placed across the sample radiation pathway while the uncoated indium tin oxide glass was put across the reference path. From the analyses of absorption spectra, the band gap energy (Eg) was determined. RESULTS AND DISCUSSION The crystallographic properties have been investigated by X ray diffraction (XRD) technique using CuK α radiation. Fig. 1 shows X ray diffraction patterns of MnS thin films deposited at different bath temperatures. The films deposited at 35 C show only single peak at 2=34.1 corresponds to (200) plane. However, the number of peaks attributed to MnS increased to two and three peaks as the bath temperature is increased to 45, 55 and 65 C, respectively. These results confirm that the deposition at higher bath temperature proved more favourable as the intensities of peaks corresponding to MnS increase. The peaks obtained are in good agreement with the Joint Committee on Powder Diffraction

Standards values belonging to the MnS 20 (Reference code: 00 065 2919) cubic structure. The lattice parameter values are a=b=c=5.22 Å. It is observed from Fig. 1 that the highest peak obtained corresponds to (200) plane. As the bath temperature is increased from 35 to 65 C, the intensity of the peak corresponding to (200) plane increased, indicating that increasing bath temperature increases the crystallinity of thin films. On the other hand, the presence of the indium tin oxide 21 (JCPDS reference No.: 01 089 4597) peaks in the XRD patterns are because of the glass substrate used during deposition. Four peaks occurred at 2θ values of 21.3, 37.4, 60.5 and 65.2 corresponding to (211), (411), (622) and (543) planes were obtained. The peaks marked with solid diamonds are associated with reflections of the cubic structure of MnS and those marked with open diamonds can be ascribed to the cubic structure of indium tin oxide. Fig 1: X ray diffraction patterns of MnS thin films deposited at different bath temperatures [ 35 C 45 C (c) 55 C (d) 65 C ( In1.875O3Sn0.125, MnS) Atomic force microscopy (AFM) is a useful method analysis of the surface topography of the thin films. Fig. 2, Fig. 3, Fig. 4 and Fig. 5 show the AFM images of MnS thin films deposited on indium tin oxide substrates at various bath temperatures and the scanning area is 20 μm x20 μm. Fig. 2, 3, 4 and 5 show the twodimensional while Fig. 2, 3, 4 and 5 display threedimensional AFM images of MnS thin films deposited at 35, 45, 55 and 65 C, respectively. The films deposited at 35 C show incomplete grain coverage and low appearance of small grains (average grain size = 1 μm) over the substrate surface. The films deposition process on a substrate depends on the formation of nucleation sites and subsequent growth of the films from these centres. The films deposited at higher bath temperature (45, 55 and 65 C) indicate better morphology compared to the films deposited at lower bath temperature (35 C). The grains show complete coverage over the substrate surface. The grains size increases with increasing bath temperature. For the films prepared at 45 and 55 C, the size of each grain differs from each other, varying from 1.5 2 μm, indicating irregular growth rate of the grains. The orientation of grain growth is also irregular as can be noticed from the specific increase of grain size at different areas of the substrate. On the other hand, the films prepared at 65 C have the largest grains (average grain size = 2.5 μm) compared to the other films. During this stage, small grains agglomerate together to form larger grains. The film thickness was measured using atomic force microscopy method. It can be observed that the thickness values of the thin films deposited at 35, 45, 55 and 65 C are 971, 1314, 1542 and 2066 nm, respectively, indicating that the thickness increased as the bath temperature is increased. On the other hand, root mean square (RMS) roughness is defined as the standard deviation of the surface height profile from the average height, is the most commonly reported measurement of surface roughness 22. The films prepared at 35 C have smoother surface (103 nm) due to the smaller grains size while the films deposited at 65 C have rougher surface (139 nm) because of the films consist of irregularly shaped grains. The surface roughness values of the films deposited at 45 and 55 C are 121 and 132 nm, respectively. It can be said that the surface roughness increases with increasing bath temperatures. Therefore, we can conclude that the MnS thin films grown on different bath temperatures obtained different surface roughness and thickness values. Fig. 2: Two dimensional and three dimensional atomic force microscopy images of MnS thin films deposited at 35 C 2

Fig 3: Two dimensional and three dimensional atomic force microscopy images of MnS thin films deposited at 45 C Fig 4: Two dimensional and three dimensional atomic force microscopy images of MnS thin films deposited at 55 C Fig 5: Two dimensional and three dimensional atomic force microscopy images of MnS thin films deposited at 65 C In order to determine the band gap of thin films, the equation of Stern 23 was used. ( hv E ) n/ 2 [ k g ] A = (1) hv where v is the frequency, h is the Planck s constant, k equals a constant while n carries the value of either 1 or 4. The n value is 1 for a direct gap material and 4 for indirect gap material. Fig. 6 indicates the variation of (Ahν) 2 versus hν for MnS thin films deposited at various bath temperatures. The direct band gap values are measured by extrapolating the straight line portion over the hν axis. It is seen 3

that the band gap values are decrease (3.05, 3.0, 2.95 and 2.75 ev) when the bath temperature is increased from 35 to 65 C. At higher bath temperature, the enhancement in crystallinity of the films leads to larger grains and also contributes to reduction in the band gap of the materials. The band gap of MnS thin films obtained in this work is close with that reported by Pathan et al. 9 and Agbo and Ezema 13. ( ( ( ( Fig 6: Plot of (Ahv) 2 versus hv band gap for MnS thin films deposited at different bath temperatures [ 35 C 45 C (c) 55 C (d) 65 C] CONCLUSION The MnS thin films could be chemically deposited by using manganese sulphate and thiourea in the presence of triethanolamine as a complexing agent during deposition process. Based on XRD results, the thin films produced were polycrystalline in nature. The intensity of the (200) peak showed a significant increased as the bath temperature was increased from 35 to 65 C. As expected, the crystallinity of the thicker films was better and more XRD peaks were observed. According to AFM images, the sizes of the grains and film thickness as well as surface roughness were noticed to increase as the bath temperature was increased. From the optical properties analysis, the band gap energy was to be dependent on the bath temperature. ACKNOWLEDGEMENT The authors would like to thank the Department of Chemistry, Universiti Putra Malaysia for the provision of laboratory facilities and MOSTI for the National Science Fellowship. REFERENCES 1. Delphine SM, Jayachandran M, Sanjeeviraja C. Pulsed electrodeposition and characterization of molybdenum diselenide thin film. Mater Res Bull 2005; 40: 135 147. 2. Suthan NJ, Jayachandran M, Perumal K, Sanjeeviraja C. Structural and optical properties of electron beam evaporated CdSe thin films. Bull Mater Sci 2007; 30: 547 551. 3. Kassim A, Nagalingam S, Tee TW, Karrim N, Haron MJ, Min HS. A cyclic voltammetric synthesis of ZnS thin films using triethanolamine as a complexing agent. An Univ Bucuresti 2009; 18: 59 66. 4. Zhuge FW, Li XM, Gao XD, Gan XY, Zhou FL. Synthesis of stable amorphous Cu2S thin film by successive ion layer adsorption and reaction method. Mater Lett 2009; 63: 652 654. 5. Ju ZG, Lu YM, Zhang JY, Shan CX, Zhao DX, Zhang ZZ, Li BH, Yao B, Shen DZ. Metal organic chemical vapour deposition growth of Cd1 xfexse thin films. Appl Surf Sci 2008; 255: 3332 3335. 6. Anuar K, Zulkefly K, Atan S, Md Jelas H, Tan WT, Ho SM, Saravanan N. Effects of deposition potential on Cu4SnS4 thin films prepared by electrodeposition technique. Arabian J Sci Eng 2010; 35: 83 92. 7. Oidor Juarez I, Garcia Jimenez P, Torres Delgado G, Castanedo Perez R, Jimenez Sandoval O, Chao B, Jimenez Sandoval S. Substrate temperature effects on the growth and properties of γ MnS thin films grown by rf sputtering. Mater Res Bull 2002; 37: 1749 1754. 8. Zhang Y, Wang H, Wang B, Yan H, Yoshimura M. Lowtemperature hydrothermal synthesis of pure metastable γ 4

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