Microstructure and open-circuit voltage of n–i–p microcrystalline silicon solar cells

tions either analyzed in this paper or observed at low resolution by recording dispersed laser-induced fluorescence.. Nevertheless, there is no doubt that the two states linked by

and as an increase of capacitance over the geometrical value. The frequency dependence of the capacitance exhibits marked differences from a-Si:H and is proposed as a tool for

For sample B (i-layer on sputtered ZnO), the thickness of the amorphous incubation layer is in the range of hundreds of nanometers, while for sample C (n–i–p cell on sputtered ZnO)

As a further indication of both (a) a rather weak transport anisotropy and (b) a minor effect of structure on transport properties, one observes that (thick) n–i–p cell performance

This model reproduces most of the features of the complex microstructure of microcrystalline silicon: transition from amorphous to crystalline phase, conical shape of the

Cite this article as: Zouhair El Jouad, Linda Cattin, Mohammed Addou, Jean Christian Bernède, Open circuit voltage of organic photovoltaic cells using C 60 as acceptor: variation

In this report a 2D modeling of n-type interdigitated back contact (IBC) crystalline silicon (c-Si) solar cell structures is presented for two different types of the BSF and

In the 1960s-1970s, the geometry of solar cells for terrestrial applications remained circular due to the high cost of silicon wafer fabrication.. However, while keeping a