Hostname: page-component-cd9895bd7-gvvz8 Total loading time: 0 Render date: 2024-12-27T01:33:13.639Z Has data issue: false hasContentIssue false

Nanostructured Silicon Oxide Dual-Function Layer in Amorphous Silicon Based Solar Cells

Published online by Cambridge University Press:  25 May 2012

Tining Su
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Baojie Yan
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Laura Sivec
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Guozhen Yue
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Jessica Owens-Mawson
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Jeffrey Yang
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Subhendu Guha
Affiliation:
United Solar Ovonic LLC, 1100 W Maple Rd, Troy, MI 48084, U.S.A.
Get access

Abstract

We report the results of using n-type hydrogenated nanocrystalline silicon oxide alloy (nc-SiOx:H) in hydrogenated nanocrystalline silicon (nc-Si:H) and amorphous silicon germanium alloy (a-SiGe:H) single-junction solar cells. We used VHF glow discharge to deposit nc-SiOx:H layers on various substrates for material characterizations. We also used VHF glow discharge to deposit the intrinsic layer in nc-Si:H solar cells. RF glow discharge was used for the deposition of the doped layers and the intrinsic layer in a-SiGe:H solar cells. Various substrates such as stainless steel (SS), Ag coated SS, and ZnO/Ag coated SS were used for different cell structures. We found that by using nc-SiOx:H to replace the ZnO and the a-Si:H n-layer in nc-Si:H solar cells, the cell structure is greatly simplified, while the cell performances remain nearly identical to those made using the conventional n-i-p structure on standard ZnO/Ag BR’s. Solar cells with nc-SiOx:H as the n layer directly deposited on textured Ag show similar quantum efficiency (QE) as the n-i-p cells on ZnO/Ag BRs. In both cases, QE is higher than that in the n-i-p cells made directly on Ag coated SS. This effect is probably caused by the shift of surface plasmon-polariton resonance frequency due to the difference in index of refraction of ZnO, nc-SiOx:H, and Si.

Type
Articles
Copyright
Copyright © Materials Research Society 2012

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Buehlmann, P., Bailat, J., Dominé, D., Billet, A., Meillaud, F., Feltrin, A., Ballif, C., and Appl. Phys. Lett. 91, 143505 (2007).CrossRefGoogle Scholar
Yan, B., Yue, G., Sivec, L., Yang, J., and Guha, S., Appl. Phys. Lett. 99, 113512 (2011).CrossRefGoogle Scholar
Lambertz, A., Grundler, T., and Finger, F., J. Appl. Phys. 109, 113109 (2011).CrossRefGoogle Scholar
Veneri, P. D., Mercaldo, L. V., and Usatii, I., Appl. Phys. Lett. 97, 023512 (2010).CrossRefGoogle Scholar
Cuony, P., Marending, M., Alexander, D. T. L., Boccard, M., Bugnon, G., Despeisse, M., and Ballif, C., Appl. Phys. Lett. 97, 213502 (2010).CrossRefGoogle Scholar
Banerjee, A., and Guha, S., J. Appl. Phys. 69, 1030 (1991).CrossRefGoogle Scholar
Banerjee, A., Yang, J., Hoffman, K., and Guha, S., Appl. Phys. Lett. 65, 472 (1994).CrossRefGoogle Scholar