Proceedings of the 4th International Conference on Nanostructures (ICNS4) 12-14 March, 2012, Kish Island, I.R. Iran Study of Te-enriched Cadmium Telluride Nano-Structured Thin Films at Cryogenic and Room Temperature Waqar A. Adil Syed1 Nazar Abbas Shah2, and M. Kamran2 1 Department of Physics, International Islamic University, Islamabad, Pakistan 2 Thin Films Technology Research Laboratory, Department of Physics COMSATS Institute of Information Technology, Islamabad 46000, Pakistan * Corresponding author Tel.: +92519049295; Fax: +92514442805. Cell: +923215105363 E-mail addresses: [email protected], [email protected] Abstract: Te-enriched Cadmium Telluride (CdTe) polycrystalline thin films were grown on corning glass substrate. The structural investigations performed by means of X-ray diffraction (XRD) technique showed that the deposited samples exhibit a polycrystalline structure with <111> as preferred orientation. Compositional study was taken by energy dispersive X-ray spectroscopy (EDX). Electrical properties of these samples were measured by Hall Effect. For the Te-enriched samples, the electrical resistivity dropped several orders of magnitude at room temperature. The deposited films also showed decreasing resistivity with increasing temperature, manifesting the semi conducting behaviour. Hall measurements at room temperature as well as at cryogenic temperature are discussed Keywords: Crystal structure; Optical microscopy; Thin films; Semiconductor; Vacuum coating Introduction Recent advances in the research of Cadmium 2CdTe ( s ) ⇔ 2Cd ( g ) + Te 2 ( g ) Telluride (CdTe) based solar cells [1-6], raised the The source CdTe dissociates into its elements (Cd interests in this highly efficient material for the use in and Te) at high temperature, and they recombine on thin film terrestrial photovoltaic applications [7-9]. the substrate surface, which is kept at a lower CdTe has a direct band gap of 1.5 eV at room temperature. The CSS system used in our experiment temperature, which is optimum for single junction is shown in Fig. 1. solar cell efficiency [6]. Wu et al [10] have reported CdTe / CdS solar cell with an efficiency of 16.5%. Because of its low sublimation temperature, CdTe polycrystalline films can be prepared by several techniques, such as thermal evaporation [11], close spaced sublimation (CSS). The closed space sublimation (CSS) technique is one of the various techniques that have produced encouraging results. Experimental The deposition of CdTe films is based on the reversible process at high temperature. 864 Thin films of cadmium telluride powder (99.99% pure) by Aldrich chemical company were placed on microscope slides of water-white glass substrates. Source material was put in the graphite boat as shown in Fig 1 (b), heated by a halogen lamp of Proceedings of the 4th International Conference on Nanostructures (ICNS4) 12-14 March, 2012, Kish Island, I.R. Iran 1000W, connected to the main power through the transmittance curves of as deposited film along temperature controller with K-type thermocouple. with Te-enriched samples for different periods of The substrate was fixed at a distance of about 5 mm from the source material. It was heated by a halogen lamp of 500 Watts, while the thermocouple was placed over the substrate to measure its temperature. Source and substrate temperatures were kept at 500oC and 400oC respectively. The chamber was evacuated at ∼ 10-4 mbar with the help of rotary pump and diffusion pump. s times. The resistivity of In the next step, Te was deposited on the top of CdTe thin films by successively varying Te mass evaporation in the graphite boat keeping the source o and substrate temperature at 200 and 100 C respectively. The vacuum of the system was ∼ 10-4 mbar. All the thin films were heat treated at 400oC sample 7 using Vander Pauw geometry was ~ 156 Ω-cm at room temperature, while the mobility and carrier concentration were about 129.3 cm2 V-1 s -1 and 3.09*1014 cm –3 respectively at room temperature using Hall Effect. for 30 minutes under the same vacuum. The silver It has been observed by Hall measurements that p- paste was used for making Ohmic contacts to type doping is achieved in Te-doped CdTe films perform Hall measurements. The samples denoted by 1-5 with successively varying Te content achieved prepared by CSS technique, which ensures the excess after tellurium depositing as shown in Table.1 by the of Te forms a part of the lattice, might create Cd above technique and the characterization of these vacancies, which increases the p-type doping. samples is described below. Results and Discussion 8 6x10 In the XRD patterns, the main reflections of samples according to fcc CdTe lattice. The data obtained for the lattice constant ‘a’ of the investigated samples series is 6.48-6.50Å, which agreed with the standard values of lattice constant (ASTM Cards 15-0770). During Te depositing, the in coming Te atoms collide 8 Resistivity at Room Temperature 5x10 Resistivity (Ωcm) are found similar to each other and can be indexed 8 4x10 8 3x10 8 2x10 8 1x10 0 1 with the cadmium telluride, replacing the Cd atom in 2 3 Sample Number 4 5 the lattice, resulting an increase in the lattice constant. Also the grains of the film became larger with the increase of Te content in the samples, which indicates that the crystallinity of the films can be improved by appropriate Te doping. Fig. 2. Shows Conclusion In this work, Te-doped CdTe films have been fabricated by the CSS technique. It is concluded on 865 Proceedings of the 4th International Conference on Nanostructures (ICNS4) 12-14 March, 2012, Kish Island, I.R. Iran the basis of the results of XRD, SEM and Hall measurements that the post deposition treatment [4] G. Fulop, M. Doty, P. Meyers, J. Betz and C. H. Liu, Appl. Phys. Lett.40 (1982) 327. [5] K. Yamaguchi, H. Matsumoto, N. Nakayama and S. strongly affects the morphology as well as electrical properties. The samples had large grains with a size ∼ 2 µm and the crystallite size can grow larger with appropriate Te doping. The refractive index was increased with the increase of Te doping. The transmission spectra showed a decrease of transmittance with an increasing level of Te doping. The band gap values are also affected by Te doping. The sheet resistance, dc electrical resistivity and activation energy of Te-doped samples have decreased, on the other hand the dark conductivity, mobility and carrier concentration have increased significantly compared to pure CdTe samples at cryogenic temperature. Acknowledgment The authors would like to thank Higher Education Commission (HEC), Pakistan, for financial support through the project 20-1187/R&D/09. References [1] J. G. Werthen, T. C. Anthony, R. H. Bube and A. L. Fahrenbruch, IEEE 16th Photovoltaic Specialists Conference Proceedings (1982) 1138. [2] Y. S. Tyan and E. A. Perez-Albuerne, IEEE 16th Photovoltaic Specialists Conference Proceedings (1982)794. [3] N. A. Shah, W. A. A. Syed, M. A. Atta, M. Ajmal, A. Ali and A. Maqsood, Nanoscience and Nanotechnology Letters, 1 (2009) 62. 866 Ikegami, Jpn. J. Appl. Phys. 15 (1976)1575. [6] N. A. Shah, A. Ali and A. Maqsood, Journal of Electronic Materials, 37 (2008) 145. [7] R. Chakrabarti, J. Dutta, A. B. Maity, S. Chaudhuri and A. K. Pal , Thin Solid Films 288 (1996)32. [8] J. Touskova, D. Kindl and J. Tousek , Thin Solid Films 293(1997) 272. [9] Y. L. Soo, S. Huang, Y. H. Kao and A.D. Compaan, J. Appl . Phys. 83 (1998) 4173. [10] A. Ali, N. A. Shah, A. K. S. Aqili, and A. 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