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Thickness-Dependent Physical Properties of Coevaporated Cu4SnS4 Films

DOI: 10.1155/2013/142029

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Abstract:

Cu4SnS4 films of different thicknesses were prepared by thermal coevaporation technique on glass substrates at a constant substrate temperature of 400°C. The layer thickness was varied in the range 0.25–1?μm. The composition analysis revealed that all the evaporated films were nearly stoichiometric. The XRD patterns indicated the presence of a strong (311) peak as the preferred orientation, following the orthorhombic crystal structure corresponding to Cu4SnS4 films. Raman analysis showed a sharp peak at 317?cm?1, also related to Cu4SnS4 phase. The optical transmittance spectra suggested that the energy band gap decreased from 1.47?eV to 1.21?eV with increase of film thickness. The hot-probe test revealed that the layers had p-type electrical conductivity. A decrease of electrical resistivity was observed with the rise of film thickness. 1. Introduction In recent years, extensive efforts have been made in finding novel and new semiconductors for application in energy conversion using the photovoltaic route. One such new material system is the Cu-Sn-S that contains inexpensive, nontoxic, and earth-abundant elements. This ternary system exhibited different stable phases such as Cu2SnS3, Cu2Sn3S7, Cu5Sn2S7, Cu4SnS4, and Cu10Sn2S13, that was reported by Wu et al. [1]. All these compounds are represented by the general formula I-IV-VI. Their optimum optical, thermal, and mechanical properties with appropriate energy band gap of these materials have attracted much attention for their applications in solar cells, sensor and other optoelectronic devices [2]. Cu4SnS4 is one such material that had an optimum energy band gap for solar energy conversion along with suitable properties [3, 4]. Hence, many researchers have attempted to grow thin films of this material using a variety of wet chemical methods such as chemical bath deposition [5] and electrodeposition [6]. However, to our knowledge, there were no attempts made to form Cu4SnS4 films using physical methods. Therefore, thermal coevaporation technique has been used in this study for the growth of Cu4SnS4 films. It is one of the best techniques because of the possibility of large-scale production, high quality of the grown layers, and minimum wastage of components. In previous work, we have shown that thin films of Cu4SnS4 could be obtained by coevaporating SnS and CuS powders [7]. In general, the physical properties of thin films strongly depend on the deposition technique and growth parameters as well as the film thickness [8]. Film thickness plays an important role in controlling the film properties unlike

References

[1]  D. Wu, C. R. Knowles, and L. Y. Chang, “Copper-tin sulphides in the system Cu–Sn–S,” Mineralogical Magazine, vol. 50, no. 2, pp. 323–325, 1986.
[2]  G. Marcano, D. B. Bracho, C. Rincón, G. S. Pérez, and L. Nieves, “On the temperature dependence of the electrical and optical properties of Cu2GeSe3,” Journal of Applied Physics, vol. 88, no. 2, pp. 822–828, 2000.
[3]  D. Avellaneda, M. T. S. Nair, and P. K. Nair, “Cu2SnS3 and Cu4SnS4 thin films via chemical deposition for photovoltaic application,” Journal of the Electrochemical Society, vol. 157, no. 6, pp. D346–D352, 2010.
[4]  Q. Chen, X. Dou, Y. Ni, S. Cheng, and S. Zhuang, “Study and enhance the photovoltaic properties of narrow-bandgap Cu2SnS3 solar cell by p-n junction interface modification,” Journal of Colloid and Interface Science, vol. 376, no. 1, pp. 327–330, 2012.
[5]  A. Kassim, T. W. Tee, A. M. Sharif et al., “Influence of bath temperature and pH value on properties of chemically deposited Cu4SnS4 thin films,” Journal of the Chilean Chemical Society, vol. 54, no. 4, pp. 345–348, 2009.
[6]  K. Anuar, W. T. Tan, S. Atan et al., “Effects of electrolytes concentration on the chemically deposited Cu4SnS4 thin films,” Asian Journal of Chemistry, vol. 22, no. 1, pp. 222–232, 2010.
[7]  V. P. G. Vani, R. W. Miles, and K. T. R. Reddy, “Preparation and properties of Cu4SnS4 thin films,” Journal of Optoelectronic Engineering, vol. 3, pp. 1–5, 2013.
[8]  D.-A. Luh, T. Miller, J. J. Paggel, and T.-C. Chiang, “Large electron-phonon coupling at an interface,” Physical Review Letters, vol. 88, no. 25 I, pp. 2568021–2568024, 2002.
[9]  C. M. Wei and M. Y. Chou, “Theory of quantum size effects in thin Pb(111) films,” Physical Review B, vol. 66, Article ID 233408, 4 pages, 2002.
[10]  T. Valla, M. Kralj, A. ?iber et al., “Oscillatory electron-phonon coupling in ultra-thin silver films on V(100),” Journal of Physics Condensed Matter, vol. 12, no. 28, pp. L477–L482, 2000.
[11]  O. Pfennigstorf, A. Petkova, H. L. Guenter, and M. Henzler, “Conduction mechanism in ultrathin metallic films,” Physical Review B, vol. 65, no. 4, Article ID 045412, 8 pages, 2002.
[12]  B. G. Orr, H. M. Jaeger, and A. M. Goldman, “Transition-temperature oscillations in thin superconducting films,” Physical Review Letters, vol. 53, no. 21, pp. 2046–2049, 1984.
[13]  F. Lai, M. Li, H. Wang et al., “Optical scattering characteristic of annealed niobium oxide films,” Thin Solid Films, vol. 488, no. 1-2, pp. 314–320, 2005.
[14]  R. Brüggemann, P. Reinig, and M. H?lling, “Thickness dependence of optical scattering and surface roughness in microcrystalline silicon,” Thin Solid Films, vol. 427, no. 1-2, pp. 358–361, 2003.
[15]  H. Kim, J. S. Horwitz, G. Kushto et al., “Effect of film thickness on the properties of indium tin oxide thin films,” Journal of Applied Physics, vol. 88, no. 10, pp. 6021–6025, 2000.
[16]  Z. Qiao, R. Latz, and D. Mergel, “Thickness dependence of In2O3?:?Sn film growth,” Thin Solid Films, vol. 466, no. 1-2, pp. 250–258, 2004.
[17]  M. T. S. Nair, C. Lopéz-Mata, O. GomezDaza, and P. K. Nair, “Copper tin sulfide semiconductor thin films produced by heating SnS–CuS layers deposited from chemical bath,” Semiconductor Science and Technology, vol. 18, no. 8, pp. 755–759, 2003.
[18]  B. E. Warren, X-Ray Diffraction, Dover, New York, NY, USA, 1990.
[19]  J. Tauc, Amorphous and Liquid Semiconductors, J. Tauc, Ed., chapter 4, Plenum, London, UK, 1974.
[20]  C. D. Lokhande, A. U. Ubale, and P. S. Patil, “Thickness dependent properties of chemically deposited Bi2S3 thin films,” Thin Solid Films, vol. 302, no. 1-2, pp. 1–4, 1997.
[21]  S. Ilican, Y. Caglar, and M. Caglar, “Preparation and characterization of ZnO thin films deposited by sol-gel spin coating method,” Journal of Optoelectronics and Advanced Materials, vol. 10, no. 10, pp. 2578–2583, 2008.
[22]  N. Kumar, U. Parihar, R. Kumar, K. J. Patel, C. J. Panchal, and N. Padha, “Effect of film thickness on optical properties of tin selenide thin films prepared by thermal evaporation for photovoltaic applications,” American Journal of Materials Science, vol. 2, pp. 41–45, 2012.
[23]  M. Patel, I. Mukhopadhyay, and A. Ray, “Structural, optical and electrical properties of spray-deposited CZTS thin films under a non-equilibrium growth condition,” Journal of Physics D, vol. 45, Article ID 445103, 10 pages, 2012.
[24]  K. L. Chopra, Thin Film Phenomena, McGraw-Hill, New York, NY, USA, 1969.

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