ELSEVIER Solar Energy Materials and Solar Cells 41/42 (1996) 485-492
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Solution of the ZnO/p contact problem in a-Si:H solar
cells
M. Kubon, E. Boehmer, F. Siebke, B. Rech, C. Beneking, H. Wagner
Forschungszentrum Jiilich GmbH, ISI-PI~, D-52425 Jiilich, Germany
Abstract
This paper addresses the problem of preparing a good p-layer contact with zinc oxide as
TCO. Our approach was to deposit pin cells with different p-layer recipes on ZnO coated
SnO2:F and on uncoated SnO2:F in one run, in order to obtain a direct comparison of the
interface properties of the two TCO materials under the condition of as equal as possible
surface morphology. The pin cells prepared on the ZnO surface exhibit a lower fill factor
(FF). Our experiments demonstrate that the hydrogen interaction with the ZnO surface
plays the most decisive role for the ZnO/p contact. We explain the observed effects using a
band diagram of the ZnO/p interface and show that the accumulation layer at the ZnO
surface -- caused by atomic hydrogen in the plasma -- is responsible for the low FF in pin
cells. Based on this model the contact problem is solved by introducing a/xc-n-Si intralayer
between ZnO and p-layer resulting in an identical high FF on both ZnO and SnO 2
substrates.
1. Introduction
In order to obtain further improvement in stabilized efficiency of a-Si:H solar
cells, growing attention is being paid to the transparent conductive oxide (TCO)
material that forms the front electrode. Especially the TCO/p contact properties
and their influence on solar cell parameters have been the object of a number of
investigations.
Fluorine doped SnO 2 is a well known material for TCO films, exhibiting
favourable surface textures which enhance the conversion efficiency. However,
SnO 2 is reduced during the early stages of solar cell deposition, leading to
additional absorption [1]. In contrast, aluminum or boron doped ZnO shows higher
transparency in the visible range and higher plasma stability [2], but ZnO/p
contact problems have been reported [3]. Especially free hydrogen in the plasma
has a negative influence on the ZnO surface [4].
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