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Cupric Oxide Thin Films for Photovoltaic Applications

Published online by Cambridge University Press:  21 August 2013

Patrick J. M. Isherwood*
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
Biancamaria Maniscalco
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
Fabiana Lisco
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
Piotr M. Kaminski
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
Jake W. Bowers
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
John M. Walls
Affiliation:
CREST, School of Electrical, Electronic and Systems Engineering, Loughborough University, Loughborough, Leicestershire, LE11 3TU UK
*
*Email: P.J.M [email protected]
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Abstract

Cupric oxide thin films were sputtered onto soda-lime glass slides from a single pre-formed ceramic target using a radio-frequency power supply. The effects of oxygen partial pressure and substrate temperature on the optical, electrical and structural properties of the films were studied. It was found that increasing temperature resulted in increased crystallinity and crystal size but also increased film resistivity. The most conductive films were those deposited at room temperature. Increasing oxygen partial pressure was found to reduce resistivity dramatically. This is thought to be due to higher charge carrier concentrations resulting from increased copper vacancies. Increasing oxygen partial pressure causes an increase in the optical band gap from a minimum of 0.8eV up to a maximum of 1.42eV. Oxygen-rich films display reduced crystallinity, becoming increasingly amorphous with increased oxygen content. These results show that the optical, electrical and structural properties of sputtered cupric oxide films can be controlled by alteration of the deposition environment.

Type
Articles
Copyright
Copyright © Materials Research Society 2013 

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References

REFERENCES

Ginley, D. S. and Perkins, J. D., “Transparent Conductors”, Handbook of Transparent Conductors, ed. Ginely, D. S., Hosono, H. and Paine., D. C. (London: Springer, 2010) p. 126.Google Scholar
Ginley, D. S., “Nanoparticle Derived Contacts for Photovoltaic Cells,” Electrochemical Society Proceedings, vol. 99, no. 11, pp. 103110, 1999.Google Scholar
Granqvist, C. G., “Transparent conductors as solar energy materials: A panoramic review,” Solar Energy Materials and Solar Cells, vol. 91, no. 17, pp. 15291598, Oct. 2007.CrossRefGoogle Scholar
Dong, G., Zhang, M., Lan, W., Dong, P., and Yan, H., “Structural and physical properties of Mg-doped CuAlO2 thin films,” Vacuum, vol. 82, no. 11, pp. 13211324, Jun. 2008.CrossRefGoogle Scholar
Tate, J. et al. ., “Origin of p-type conduction in single-crystal CuAlO2,” Physical Review B, vol. 80, no. 16, pp. 18, Oct. 2009.CrossRefGoogle Scholar
Kawazoe, H., Yanagi, H., Ueda, K., and Hosono, H., “Transparent p-type conducting oxides: design and fabrication of pn heterojunctions,” MRS Bulletin, vol. 25, no. 8, pp. 2836, 2000.CrossRefGoogle Scholar
Scanlon, D. O., Godinho, K. G., Morgan, B. J., and Watson, G. W., “Understanding conductivity anomalies in Cu(I)-based delafossite transparent conducting oxides: Theoretical insights.,” The Journal of chemical physics, vol. 132, no. 2, p. 024707, Jan. 2010.CrossRefGoogle ScholarPubMed
Yanagi, H., Inoue, S.-ichiro, Ueda, K., Kawazoe, H., Hosono, H., and Hamada, N., “Electronic structure and optoelectronic properties of transparent p-type conducting CuAlO2,” Journal of Applied Physics, vol. 88, no. 7, pp. 41594163, 2000.CrossRefGoogle Scholar
Ingram, B. J. et al. ., “Transport and Defect Mechanisms in Cuprous Delafossites. 1. Comparison of Hydrothermal and Standard Solid-State Synthesis in CuAlO2,” Chemistry of Materials, vol. 16, no. 26, pp. 56165622, 2004.CrossRefGoogle Scholar
Wang, L., Han, K., Song, G., Yang, X., and Tao, M., “Characterization of electro-deposited CuO as a low-cost material for high-efficiency solar cells,” Nature, pp. 130133, 2006.Google Scholar
Wu, D., Zhang, Q., and Tao, M., “LSDA+U study of cupric oxide: Electronic structure and native point defects,” Physical Review B, vol. 73, no. 23, pp. 16, Jun. 2006.CrossRefGoogle Scholar
Peng, Y., Zhang, Z., Viet Pham, T., Zhao, Y., Wu, P., and Wang, J., “Density functional theory analysis of dopants in cupric oxide,” Journal of Applied Physics, vol. 111, no. 10, p. 103708, 2012.CrossRefGoogle Scholar
Lee, J.-H., “Effects of substrate temperature on electrical and optical properties ITO films deposited by r.f. magnetron sputtering,” Journal of Electroceramics, vol. 23, no. 2-4, pp. 554558, Jul. 2008.CrossRefGoogle Scholar
Leenheer, A., Perkins, J., van Hest, M., Berry, J., O’Hayre, R., and Ginley, D., “General mobility and carrier concentration relationship in transparent amorphous indium zinc oxide films,” Physical Review B, vol. 77, no. 11, p. 115215, Mar. 2008.CrossRefGoogle Scholar