Structural and electrical properties of polycrystalline CuGaSe2 thin films have been studied by changing the Ga/Cu ratio in the films. CuGaSe2 thin films with various Ga/Cu ratio were grown over Mo-coated soda-lime glass substrates. With the increase of Ga content in CuGaSe2, morphology of the films was found to deteriorate which is associated with the smaller grain size and the appearance of impurity phases presumably due to the phase transition from the chalcopyrite structure to the defect-related phase on the surface of the films. Properties of the Ga poor films were affected by the Cu rich secondary phases. Electrical properties of the films were strongly influenced by the structural properties and degraded with increasing the Ga/Cu ratio in the film. Device performances, fabricated with the corresponding CuGaSe2 films, were found to be correlated with the Ga/Cu ratio in the films and consistent with the observed structural and electrical properties. 1. Introduction Chalcopyrite Cu(In,Ga)Se2, abbreviated as CIGS, is one of the most promising materials to realize high-efficiency, low-cost thin film solar cell. Efficiency of 19.9% has already been achieved for the CIGS-based solar cell [1]. As the ideal CIGS bandgap for highest conversion efficiency is speculated theoretically to be around 1.4?eV [2], CuGaSe2 ( ) with a bandgap of 1.68?eV [3] can be considered as a leading material to enable the highest possible efficiency. Moreover, the large band gap makes the CuGaSe2, an ideal absorber material for the top cell in a photovoltaic tandem device together with CuInSe2 as the bottom cell absorber [4]. However, so far, CuGaSe2 solar cells with a CdS buffer have achieved efficiency of around 9.3% for thin film [5] and 9.7% for single crystal solar cells [6]. Therefore, a better understanding of the material properties of CuGaSe2 is needed to realize efficiency beyond the current level. The electrical, optical, and microstructural properties of CIGS films are dominated by the various intrinsic defects originated from the off stoichiometry of the film composition [7–9]. Moreover, deviation from the ideal stoichiometry during growth of this material is reported to contain some secondary phases preferably segregated on the surface of the film. Particularly, formation of the Cu(In,Ga)3Se5, Cu(In,Ga)2Se3.5, and so forth phases on the surface of the slightly Cu-poor film (Ga/Cu-rich) and Cu-Se related secondary phase in the Cu-rich film is a commonly observed phenomenon in CIGS material grown by various methods [10, 11] and reported to have significant impact on
References
[1]
I. Repins, M. A. Contreras, B. Egaas et al., “19.9%-efficient ZnO/CdS/CuInGaSe2 solar cell with 81.2% fill factor,” Progress in Photovoltaics, vol. 16, no. 3, pp. 235–239, 2008.
[2]
W. Shockley and H. Queisser, “Detailed balance limit of efficiency of p-n junction solar cells,” Journal of Applied Physics, vol. 32, no. 3, pp. 510–519, 1961.
[3]
S. Chichibu, T. Mizutani, K. Murakami et al., “Band gap energies of bulk, thin-film, and epitaxial layers of CuInSe2 and CuGaSe2,” Journal of Applied Physics, vol. 83, no. 7, pp. 3678–3689, 1998.
[4]
S. Nishiwaki, S. Siebentritt, P. Walk, and M. Ch. Lux-Steiner, “A stacked chalcopyrite thin-film tandem solar cell with 1.2 V open-circuit voltage,” Progress in Photovoltaics, vol. 11, no. 4, pp. 243–248, 2003.
[5]
V. Nadenau, D. Hariskos, and H. W. Schock, “CuGaSe2 based thin film solar cells with improved performance,” in Proceedings of the 14th European Photovoltaic Solar Energy Conference, H. S. Stephens, Ed., vol. 85, pp. 1250–1253, Bedford, UK, 1997.
[6]
M. Saad, H. Riazi, E. Bucher, and M. Ch. Lux-Steiner, “CuGaSe2 solar cells with 9.7% power conversion efficiency,” Applied Physics A, vol. 62, no. 2, pp. 181–185, 1996.
[7]
M. M. Islam, T. Sakurai, S. Ishizuka et al., “Effect of Se/(Ga+In) ratio on MBE grown Cu(In,Ga)Se2 thin film solar cell,” Journal of Crystal Growth, vol. 311, no. 7, pp. 2212–2214, 2009.
[8]
R. Noufi, R. Axton, C. Herrington, and S. K. Deb, “Electronic properties versus composition of thin films of CuInSe2,” Applied Physics Letters, vol. 45, no. 6, pp. 668–670, 1984.
[9]
M. M. Islam, A. Uedono, S. Ishibashi et al., “Impact of Cu/III ratio on the near-surface defects in polycrystalline CuGaSe2 thin films,” Applied Physics Letters, vol. 98, no. 11, Article ID 112105, 2011.
[10]
A. J. Nelson, A. B. Swartzlander, J. R. Tuttle, R. Noufi, R. Patel, and H. Hochst, “Photoemission investigation of the electronic structure at polycrystalline CuInSe2 thin-film interfaces,” Journal of Applied Physics, vol. 74, no. 9, pp. 5757–5760, 1993.
[11]
P. Fons, S. Niki, A. Yamada, and H. Oyanagi, “Direct observation of the Cu2-xSe phase of Cu-rich epitaxial CuInSe2 grown on GaAs (001),” Journal of Applied Physics, vol. 84, no. 12, pp. 6926–6928, 1998.
[12]
M. M. Islam, T. Sakurai, A. Yamada et al., “Determination of Cu(In1-xGax)3Se5 defect phase in MBE grown Cu(In1-xGax)Se2 thin film by Rietveld analysis,” Solar Energy Materials & Solar Cells, vol. 95, no. 1, pp. 231–234, 2011.
[13]
D. Schmid, M. Ruckh, F. Grunwald, and H. W. Schock, “Chalcopyrite/defect chalcopyrite heterojunctions on the basis of CuInSe2,” Journal of Applied Physics, vol. 73, no. 6, pp. 2902–2909, 1993.
[14]
K. Sakurai, R. Hunger, N. Tsuchimochi et al., “Properties of CuInGaSe2 solar cells based upon an improved three-stage process,” Thin Solid Films, vol. 431-432, pp. 6–10, 2003.
[15]
J. R. Tuttle, D. S. Albin, and R. Noufi, “Thoughts on the microstructure of polycrystalline thin film CuInSe2 and its impact on material and device performance,” Solar Cells, vol. 30, no. 1–4, pp. 21–38, 1991.
[16]
M. M. Islam, A. Yamada, T. Sakurai, et al., “Cu-dependent phase transition in polycrystalline CuGaSe2 thin films grown by three-stage process,” Journal of Applied Physics, vol. 110, Article ID 014903, 5 pages, 2011.
[17]
U. Rau and H. W. Schock, “Electronic properties of Cu(In,Ga)Se2 heterojunction solar cells-recent achievements, current understanding, and future challenges,” Applied Physics A, vol. 69, no. 2, pp. 131–147, 1999.
[18]
R. Klenk, T. Walter, H. W. Schock, and D. Cahen, “A model for the successful growth of polycrystalline films of CuInSe2 by multisource physical vacuum evaporation,” Advanced Materials, vol. 5, no. 2, pp. 114–119, 1993.
[19]
T. Schlenker, M. Luis Valero, H. W. Schock, and J. H. Werner, “Grain growth studies of thin Cu(In, Ga)Se2 films,” Journal of Crystal Growth, vol. 264, no. 1–3, pp. 178–183, 2004.
[20]
R. Caballero, S. Siebentritt, K. Sakurai, C. A. Kaufmann, H. W. Schock, and M. Ch. Lux-Steiner, “Effect of Cu excess on three-stage CuGaSe2 thin films using in-situ process controls,” Thin Solid Films, vol. 515, no. 15, pp. 5862–5866, 2007.
[21]
S. Nishiwaki, N. Kohara, T. Negami, H. Miyake, and T. Wada, “Microstructure of Cu(In,Ga)Se2 films deposited in low Se vapor pressure,” Japanese Journal of Applied Physics, vol. 38, no. 5, pp. 2888–2892, 1999.
[22]
J. C. Mikkelsen Jr., “Ternary phase relations of the chalcopyrite compound CuGaSe2,” Journal of Electronic Materials, vol. 10, no. 3, pp. 541–558, 1981.
[23]
J. R. Tuttle, M. Contreras, M. H. Bode et al., “Structure, chemistry, and growth mechanisms of photovoltaic quality thin-film Cu(In,Ga)Se2 grown from a mixed-phase precursor,” Journal of Applied Physics, vol. 77, no. 1, pp. 153–161, 1995.
[24]
M. Chen, Z. L. Pei, X. Wang et al., “Intrinsic limit of electrical properties of transparent conductive oxide films,” Journal of Physics D, vol. 33, no. 20, pp. 2538–2548, 2000.
[25]
T. Negami, N. Kohara, M. Nishitani, and T. Wada, “Preparation of ordered vacancy chalcopyrite-type CuIn3Se5 thin films,” Japanese Journal of Applied Physics, vol. 33, no. 9, pp. L1251–L1253, 1994.
[26]
V. Nadenau, G. Lippold, U. Rau, and H. W. Schock, “Sodium induced secondary phase segregations in CuGaSe2 thin films,” Journal of Crystal Growth, vol. 233, no. 1-2, pp. 13–21, 2001.