Affiliation:
1. IEK-5 Photovoltaik Forschungszentrum Jülich GmbH 52425 Jülich Germany
2. Faculty of Electrical Engineering and Information Technology RWTH Aachen University 52062 Aachen Germany
Abstract
Due to its high transparency, silicon carbide can replace amorphous silicon as a front contact material in crystalline silicon solar cells. Herein, first a look at doping in nc‐SiC:H with different deposition techniques is taken. Then, the influence of various deposition conditions for hot wire chemical vapor deposition‐prepared nc‐SiC:H is investigated. Both the electrical conductivity and the optical bandgap increase simultaneously for a multitude of deposition parameters. Combining a high filament temperature of the catalytic filament, a high hydrogen dilution of the precursor gas and an overall low total gas flow, conductivities of 0.38 S cm−1 in combination with an optical bandgap of 3.2 eV can be achieved. In the last section, a closer look into the dependencies of the layer thicknesses of the two different nc‐SiC:H layers applied in solar cells on the cell performance is taken. While the layer with conducting properties only has minor influences on cell properties, a trade‐off between passivation and fill factor is identified for the passivating nc‐SiC:H layer. For thicker layers, the passivating nc‐SiC:H layer achieves a very high implied open‐circuit voltage above 740 mV, but the fill factor starts to degrade due to a very low conductance of the layer.
Subject
Electrical and Electronic Engineering,Energy Engineering and Power Technology,Atomic and Molecular Physics, and Optics,Electronic, Optical and Magnetic Materials
Cited by
2 articles.
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