Finite element models of different laterally extended polymer solar cells were applied in order to investigate current pathways and dissipative losses in organic solar cells, especially in the presence of local shunt defects. The models are of purely resistive nature, as this is sufficient to describe the effects under consideration. Remarkable agreement was found between the experimental and calculated thermography results in defect-free solar cells. All this provides a further step towards a quantitative description of the losses in defect-free and defective solar cells.
Extended AbstractWe constructed finite element models of different laterally extended polymer solar cells in order to investigate current pathways and dissipative losses in organic solar cells, especially in the presence of local shunt defects. The models are of purely resistive nature, as this is sufficient to describe the effects under consideration.The model calculations yield the spatial distribution of the current densities, potentials and the according resistive losses. In defect-free solar cells, the current density and loss patterns cover the entire area of the transparent electrode (ITO). In the close vicinity of the shunt defects, the current density exhibits large maxima leading to respective maxima in the power loss. On the other hand, non-negligible currents are spread out covering the entire area of the devices, running along the electric potential gradient.The current density mainly contributes to the resistive loss density of the device. The loss, in turn, is a consequence of the delicate interplay between the individual layer properties, namely the resistivities and layer thicknesses in combination, also in the presence of locally concentrated defects. Furthermore, the dissipative loss patterns are the origin of respective heat patterns, which are visible in dark lock-in thermography imaging experiments. Thermographic imaging is excellently suitable to represent the aforementioned losses under operating conditions [1][2][3]. Remarkable agreement was found between the experimental and calculated thermography results in defect-free solar cells. (cf. Figs. 1,2) All this provides a further step towards a quantitative description of the losses in defect-free and defective solar cells.