International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: editor@ijaiem.org Volume 3, Issue 9, September 2014 ISSN 2319 – 4847 EFFECT OF GAMMA – RAY ON STRUCTURAL AND OPTICAL PROPERTIES OF CADIMUM SULFIDE (CdS) THIN FILMS FAISAL HAMAD ANTAR Physics Department Education College for Pure Sciences, Anbar University ,Iraq ABSTRACT In this work, CdS thin films have been deposited onto the glass substrates by thermal evaporation technique in vacuum of the order of 10–5 mbar. at different thickness. The effect of gamma radiation from Co-60 by with ray dose 20 Mrad on the structural and optical properties of the CdS thin films was investigated. The crystal structure and orientation of the CdS thin films were investigated by X-ray diffraction (XRD) patterns. The optical transmittance measurements were recorded by using a double beam spectrophotometer. The XRD spectra indicate that the films are of polycrystalline structure before and after irradiation with a preferential growth of crystallites in the (002) plane. The grain size of crystallites was found to be in the range of 9-32 nm. After gamma irradiation, the result indicates that the intensity of XRD spectra and grain size of crystallites increases, while the optical energy gap decreases. Keywords: Thin films, Gamma radiation, Cadmium sulphide. 1. INTRODUCTION In recent years, the synthesis of chalcogenides has attracted significant interest and still is the subject of intense investigation owing to their important non-linear properties, luminescent properties and other important physical and chemical properties [1]. Among the wide band gap II-VI semiconductors cadmium sulphide (CdS) with its direct band gap of 2.42 eV at room temperature is a promising material and is applied in wide variety of fields such as solar cells [2,3]. Ionizing radiations such as X-rays, gamma-rays, beta particles, alpha particles, fission fragments, etc. are present in several fields that include industry, medicine, military, particle accelerator based research, nuclear power plants, etc. It is very much essential to ensure that the radiation levels in the environment surrounding these fields are within the permissible limit which can be determined by proper dosimeters [4]. CdS is one of the most extensively investigated semiconductors in thin film form and a large variety of deposition techniques have been utilized to obtain solar cell quality layers of CdS. These preparation techniques include dry process such as sputtering, physical vapor deposition, chemical vapor deposition, and molecular beam epitaxy(MBE)[5]-[8], and wet process such as electro-deposition, spray pyrolysis, successive ionic layer adsorption and reaction, and chemical bath deposition [9]-[12]. The aim of this work is to investigate the effect of Gamma irradiation on structural and optical properties of CdS thin films. 2. EXPERMENTAL The cleanness of the substrate surface plays a decisive influence on film growth and adhesion. The commercial glass substrates were washed with a detergent solution, acid and base solutions, after which they were ultrasonically cleaned in distilled water and finally dried. The CdS thin films were deposited on glass substrates (using 99.99 % pure CdS powder) by thermal evaporation technique in vacuum (CVD) at room temperature (300K) at a pressure of the order of 10-5 torr. Molybdenum boat was used to hold powdered sample. The distance from source to substrate is kept at 20 cm and the rate of deposition was 7 Å/sec. The samples thickness were 100 nm , 200 nm and 300 nm. was determined using thickness monitor ( Edward 306 ). Then the as deposited films exposed to gamma radiation dose. Structure of deposited CdS films was analyzed by X-ray diffractometer using Cukα radiation at a slow scanning rate in the 2θ range 20-60°, while the optical transmittance measurements were recorded by using a double beam spectrophotometer. 3. RESULTS AND DISCUSION 3.1 Structural properties Figures 1and 2 shows the X-ray diffraction pattern of the CdS thin films before and after irradiation by gamma radiation. X-ray diffraction studies showed that these films are well oriented with a preferential growth of crystallites in the (002) plane. XRD studies revealed that the crystallanity of these films was improved on irradiation with a gamma radiation. Volume 3, Issue 9, September 2014 Page 89 International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: editor@ijaiem.org Volume 3, Issue 9, September 2014 ISSN 2319 – 4847 There is also observed several dominant peaks represent to (100), (101), (110) and (112) plane are present with low intensities as compared to that of (002) plane. Figure 1: X-ray diffraction pattern of CdS thin films before irradiation prepared at different thickness (a) 100 nm, (b) 200 nm and (c) 300 nm. Figure 2: X-ray diffraction pattern of CdS thin films after irradiation prepared at different thickness (a) 100 nm, (b) 200 nm and (c) 300 nm. The average grain size of the prepared CdS thin films can be determined from the full width at half maximum (FWHM) of the prominent peak using Debye- Scherer formula [2]: (1) D hkl K /( cos ) where λ = 1.54Ǻ is the wavelength of the X-ray radiation, β is the FWHM in radians of the XRD peak and is the angle of diffraction. The crystallite sizes are summarized in the table 1 are found to be within the range 9- 32 nm. Table 1: XRD results for CdS thin films before and after irradiation. Sample Thickness 2θ Pla FWHM Gran ne Size Before 1 100 1.036 9 irradiati 26. 00 2 200 0.423 21 on 5 2 3 300 0. 342 27 After irradiati on 1 2 3 Volume 3, Issue 9, September 2014 100 200 300 26. 5 00 2 0.559 0.345 0.333 16 26 32 Page 90 International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: editor@ijaiem.org Volume 3, Issue 9, September 2014 ISSN 2319 – 4847 3.2 Optical properties Absorbance measurements are performed at room temperature in the range of 300 – 1100 nm to obtain information on the optical properties of the CdS thin films obtained at different thickness values. Figures 3 and 4 shows the transmittance as a function of wavelength of the CdS thin films before and after irradiation. The CdS films have high transmittance of about 70 to 80% in the UV-Vis-NIR regions. From the figures we can see that as the thickness increase the transmittance decrease. Also the transmittance decreases after irradiation. The small decreases in transmittance after irradiation may be due to increase in the grain size of these films. Figure 3: transmittance as a function of wavelength of the CdS thin films (A) before and, (B) after irradiation From optical absorption spectrum of CdS the band gap was calculated using the Tauc relation [13]. We plotted (αhw)2 versus hν as shown in figures 4 and 5. Where α is the absorption coefficient and hν is the photon energy. Tauc relation connecting the α, hν and optical band gap Eg takes the form: h A( h E ) g m …….(2) The direct band gap values were determined by extrapolating the linear portion of these plots to the energy axis. Where m=1/2 for a direct band gap material, 2 for an indirect band gap material and 3/2 for a forbidden –direct energy gap. As can be seen in Figuer 5, after irradiation the band gap energy is decreasing. The band gap energies of CdS thin films are given in table 2. Table 2: The bandgap energies for CdS thin films before and after irradiation. Eg (eV) Eg (eV) Sample Thickness Before After (nm) irradiation irradiation 1 100 2.42 2.42 2 200 2.38 2.37 3 300 2.36 2.33 Figure 4: Optical energy gap of CdS thin films before irradiation prepared at nm and (c) 300nm. Volume 3, Issue 9, September 2014 different thickness (a) 100 nm, (b) 200 Page 91 International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: editor@ijaiem.org Volume 3, Issue 9, September 2014 Figure 5: Optical energy gap of CdS thin films after irradiation prepared at different thickness and (c) 300 nm. ISSN 2319 – 4847 (a) 100 nm, (b) 200 nm 4. CONCLUSION CdS are synthesized through thermal evaporation technique in vacuum at different thickness. The x-ray diffraction pattern shows that CdS thin film is polycrystalline with a hexagonal structure before and after irradiation by gamma radiation and the intensity increase after irradiation. The grain size of crystallites was found to be in the range of 9-32 nm. The transmittance and optical band gap energies of the prepared CdS thin films decreases after irradiation. REFRENCES [1] D. K. Dwivedi, Dyashankar, M. Dubey, " Synthesis Structural and Optical Characterization of CdS Nanoparticles " Journal of Ovonic Research Vol. 6, No. 1, February, pp.57-62 (2010). [2] D. Saikia, P. K. Gogol, P. K. Saikia," Structural and Optical Properties of nanostructured CdS Thin Films Deposited at Different Preparative Conditions," Chalcogenide Letters Vol. 7, 2010, pp. 317 – 324 [3] K. Ravichandran and P. Philominathan," Comparative Study on Structural and Optical Properties of CdS Films fabricated by Three Different Low-cost Techniques" Applied Surface Science, 255 , pp. 5736–5741, 2009. [4] Manisha Mohil and G. Anil Kumar "Gamma Radiation Induced Effects in TeO2 Thin Films" Journal of Nano- and Electronic Physics, Vol. 5 , pp. 02018 (1-3), 2013. [5] K. Yamaguchi, T. Yoshida, D. Lincot and H. Minoura," Mechanistic Study of Chemical Deposition of ZnS Thin Films from Aqueous Solutions Containing Zinc Acetate and Thioacetamide by Comparison with Homogeneous Precipitation," J. Phys. Chem. B, 107, pp.387-397, 2003. [6] H. Khallaf, I. O. Oladeji and L. Chow,"Optimization of Chemical Bath Deposited CdS Thin Films using Nitrilotriacetic Acid as a Complexing Agent," Thin Solid Films, 516, pp.5967-5973, 2008. [7] N. Barreau, S. Marsillac, J. C. Bernede, T. B. Nasrallah and S. Belgacem, "Optical Properties of Wide Band Gap Indium Sulphide Thin Films Obtained by Physical Vapor Deposition," Phys. Status. Solidi A, 184, pp.179-186, 2001. [8] F. Zhenyi, C. Yichao, H. Yongliang, Y. Yaoyuan, D. Yanping, Y. Zewn, T. Hongchang, Y. Hogfao and W. Heming, " CVD Growth of Bulk Polycrystalline ZnS and its Optical Properties, " J. Cryst. Growth, pp.1707-1710, 2002. [9] G. Machado, D. N. Guerra, D. Leinen, J. R. Ramos- Barrado, R. E. Marotti and E. A. Dalchiele, "Indium Doped Zinc Oxide Thin Films Obtained by Electro-deposition," Thin Solid Films, 490, pp.124-131, 2005. [10] K. Ravichandran and P. Philominathan, "Investigations on Microstructural and Optical Properties of CdS Films Fabricated by a Low-cost, Simplified Spray Technique using Perfume Atomizer for Solar Cell Applications," Sol. Energy, 82, pp.1062-1066, 2008. [11] M. Kundakci, A. Ates, A. Astam and M. Yildirim, "Structural, Optical and Electrical Properties of CdS, Cd0.5In0.5S and In 2S3 Thin Films Grown by SILAR Method," Physica E, 40, pp.600-605, 2008. [12] R. Sahraei, G. M. Aval and A. Goudarzi, "Compositional, Structural, and Optical Study of Nanocrystalline ZnS Thin Films Prepared by a New Chemical Bath Deposition Route," J. Alloys Compd.,466, pp.488-492, 2008. [13] Tauc, "Amorphous & Liquid Semiconductors," New York: Plenum, p.159,1974. Volume 3, Issue 9, September 2014 Page 92