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Suppression of Edge Recombination in InAs/InGaAs DWELL Solar Cells

Published online by Cambridge University Press:  31 January 2011

Tingyi Gu ,
Mohamed A El-Emawy ,
Kai Yang ,
Andreas Atintz  and
Luke F Lester
Tingyi Gu
Affiliation:
tgu@unm.edu
Mohamed A El-Emawy
Affiliation:
mo1emawy@unm.edu, United States
Kai Yang
Affiliation:
kaiyang@chtm.unm.edu, University of New Mexico, Center for High Technology Materials, Albuquerque, New Mexico, United States
Andreas Atintz
Affiliation:
andreas@chtm.unm.edu, Unviersity of New Mexico, Center for High Technology Materials, Albuqueruqe, New Mexico, United States
Luke F Lester
Affiliation:
luke@chtm.unm.edu, United States
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Abstract

The InAs/InGaAs DWELL solar cell grown by MBE is a standard pin diode structure with six layers of InAs QDs embedded in InGaAs quantum wells placed within a 200-nm intrinsic GaAs region. The GaAs control wafer consists of the same pin configuration but without the DWELL structure. The typical DWELL solar cell exhibits higher short current density while maintaining nearly the same open-circuit voltage for different scales, and the advantage of higher short current density is more obvious in the smaller cells. In contrast, the smaller size cells, which have a higher perimeter to area ratio, make edge recombination current dominant in the GaAs control cells, and thus their open circuit voltage and efficiency severely degrade. The open-circuit voltage and efficiency under AM1.5G of the GaAs control cell decrease from 0.914V and 8.85% to 0.834V and 7.41%, respectively, as the size shrinks from 5*5mm2 to 2*2mm2, compared to the increase from 0.665V and 7.04% to 0.675V and 8.17%, respectively, in the DWELL solar cells. The lower open-circuit voltage in the smaller GaAs control cells is caused by strong Shockley-Read-Hall (SRH) recombination on the perimeter, which leads to a shoulder in the semi-logarithmic dark IV curve. However, despite the fact that the DWELL and GaAs control cells were processed simultaneously, the shoulders on the dark IV curve disappear in all the DWELL cells over the whole processed wafer. As has been discussed in previous research on transport in QDs, it is believed that the DWELL cells inhibit lateral diffusion current and thus edge recombination by collection first in the InGaAs quantum well and then trapping in the embedded InAs dots. This conclusion is further supported by the almost constant current densities of the different area DWELL devices as a function of voltage.

Keywords

semiconductingoptoelectronicself-assembly
Type
Research Article
Information
MRS Online Proceedings Library (OPL) , Volume 1210: Symposium Q – Photovoltaic Materials and Manufacturing Issues II , 2009 , 1210-Q02-07
Copyright
Copyright © Materials Research Society 2010

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References

1 Luque, A. Marti, A. and Cuadra, L. IEEE Trans. Elec. Dev. 50, 447 (2003).Google Scholar
2 Laghumavarapu, R. B. El-Emawy, M., Nuntawong, N. Moscho, A. Lester, L. F. and Huffaker, D. L., Appl. Phys. Lett. 91, 243115 (2007).Google Scholar
3 Hubbard, S. M. Cress, C. D. Bailey, C. G. Raffaelle, R. P. Bailey, S. G. and Wilt, D. M. Appl. Phys. Lett. 92, 123512 (2008).Google Scholar
4 Hubbard, S. M. Raffaelle, R. Robinson, R. Bailey, C. Wilt, D. Wolford, D. Maurer, W. and Bailey, S. Mater. Res. Soc. Symp. Proc. 1017-DD 13–11 (2007).Google Scholar
5 Stintz, A. Liu, G. T. Gray, A.L., Spillers, R., Delgado, S.M., and Malloy, K.J., J. Vac. Sci. Technol. B 18(3) 1496 (2000)Google Scholar
6 Liu, G.T. Stintz, A. Li, H. Malloy, K.J. and Lester, L.F. Electronics Letters, 35, 1163 (1999)Google Scholar
7 Raghavan, S. Rotella, P. Stintz, A. Fuchs, B. and Krishna, S. Appl. Phys. Lett. 81, 1369 (2002)Google Scholar
8 Popescu, D. P. Eliseev, P. G. Stintz, A. and Malloy, K. J. J. Appl. Phys. 94(4), 2454 (2003).Google Scholar
9 McIntosh, K. R. Ph.D. thesis University of New South Wales (2001).Google Scholar
10http://www.eis.na.baesystems.com/media_resources/ast_mast.htmGoogle Scholar
11 Kasap, S. O. Optoelectronics and Photonics: Principles and Practices; Prentice Hall: Englewood Cliffs, NJ, 262 (2006).Google Scholar
12 Abbott, M. D. Cotter, J. E. Trupke, T. and Bardos, R. A. Appl. Phys. Lett. 88, 114105 (2006).Google Scholar
13 Dodd, P. E. Stellwag, T. B. Melloch, M. R. and Lundstrom, M. S. IEEE Trans. Elec. Dev. 38, 1253–1261 (1991).Google Scholar
14 McIntosh, K. R. and Honsberg, C. B. 16th European Photovoltaic Solar Energy Conference, Glasgow, UK (2000).Google Scholar
15 Robinson, S. J. Wenham, S. R. Altermatt, P. P. Aberle, A. G. Heiser, G. and Green, M. A. J. Appl. Phys. 78, 4740–4754 (1995).Google Scholar
16 Shockley, W. and Read, W. T. Phys. Rev. 87, 835 (1952).Google Scholar