Zn(O,OH) layers in chalcopyrite thin-film solar cells: Valence-band maximum versus composition

Zn(O,OH) layers deposited by the ion layer gas reaction (ILGAR) technique have the potential to replace the conventionally used CdS buffer layer in Cu ( In ( 1 − X ) Ga X ) ( S Y Se ( 1 − Y ) ) 2 -based thin-film solar cells. To avoid stability issues, the fraction of metastable Zn ( O H ) 2 should...

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Veröffentlicht in:Journal of applied physics 2005-09, Vol.98 (5), p.053702-053702-8
Hauptverfasser: Bär, M., Reichardt, J., Grimm, A., Kötschau, I., Lauermann, I., Rahne, K., Sokoll, S., Lux-Steiner, M. C., Fischer, Ch.-H., Weinhardt, L., Umbach, E., Heske, C., Jung, Ch, Niesen, T. P., Visbeck, S.
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Sprache:eng
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Zusammenfassung:Zn(O,OH) layers deposited by the ion layer gas reaction (ILGAR) technique have the potential to replace the conventionally used CdS buffer layer in Cu ( In ( 1 − X ) Ga X ) ( S Y Se ( 1 − Y ) ) 2 -based thin-film solar cells. To avoid stability issues, the fraction of metastable Zn ( O H ) 2 should be reduced in the final buffer layer. However, hydroxide-poor or -free ZnO "buffers" result in noncompetitive devices. We have therefore investigated the impact of different oxide/hydroxide ratios on the electronic band alignment at the absorber/buffer heterointerface. The surface composition as well as the position of the valence-band maximum (VBM) of respective ILGAR-Zn(O,OH) samples was determined by photoelectron spectroscopy. The position of the conduction-band minimum (CBM) was estimated using optical band gaps determined from optical reflection/transmission measurements. From the comparison of these VBM and CBM values with the respective values of the absorber surface, predictions are made in terms of valence- and conduction-band offsets at the crucial absorber/buffer interface. The results are compared with previous findings, and the drawn conclusions are correlated with the performance of respective solar cell devices.
ISSN:0021-8979
1089-7550
DOI:10.1063/1.2034650