Research PROGRESS IN PHOTOVOLTAICS: RESEARCH AND APPLICATIONS Prog. Photovolt: Res. Appl. 2004; 12:529–538 Published online 29 July 2004 in Wiley InterScience (www.interscimax.book118.com). DOI: 10.1002/pip.544 Shunt Types in Crystalline Silicon Solar Cells O. Breitenstein*,y , J. P. Rakotoniaina, M. H. Al Rifai and M. Werner Max Planck Institute of Microstructure Physics, Weinberg 2, D-06120 Halle, Germany Nine different types of shunt have been found in state-of-the-art mono- and multi- crystalline solar cells by lock-in thermography and identified by SEM investigation (including EBIC), TEM and EDX. These shunts differ by the type of their I–V char- acteristics (linear or nonlinear) and by their physical origin. Six shunt types are pro- cess-induced, and three are caused by grown-in defects of the material. The most important process-induced shunts are residues of the emitter at the edge of the cells, cracks, recombination sites at the cell edge, Schottky-type shunts below grid lines, scratches, and aluminum particles at the surface. The material-induced shunts are strong recombination sites at grown-in defects (e.g., metal-decorated small-angle grain boundaries), grown-in macroscopic Si3N4 inclusions, and inversion layers caused by microscopic SiC precipitates on grain boundaries crossing the wafer. Copyright # 2004 John Wiley & Sons, Ltd. key words: shunts; thermography; lock-in; silicon; monocrystalline; multicrystalline INTRODUCTION solar cell, as simulated by essentially one-dimensional models, is assumed to show a homogeneous current flow across the whole area, both under illumination and in the dark. In the traditional inter- I–V characteristics of solar cells all nonlinear currents belonged to the cell, and only pretation of ohmic current paths across the pn junction have been attributed to ‘shunts’. With the availibility of precision lock-in thermography techniques these shunts can be made visible, so in the following all bright features visible in thermography have been called ‘shunts’. However, by later investigations it has turned out that there are not only ohmic shunts, but also diode-like ones, e.g., caused by local recombination sites. So the question, what is a shunt and what belongs to the undisturbed cell, has a philosophical dimension: can, e.g., a region of lower crystal quality be called a shunt? This question is still under discussion, but throughout this work we will use the term ‘shunt’ for any position in a solar cell showing under forward or reverse-bias a dark-current contribution additional to the diffusion current. In this sense edge leakage currents are shunting currents, but a region of lower crystal quality, where only the saturation current density of the diffusion current is increased, is not. Future discussions will show whether this definition will survive or has to be replaced by a more precise one. *Correspondence to: O. Breite
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