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Method for optimizing the parameters of heterojunction photovoltaic cells based on crystalline silicon

A. V. SachenkoLashkaryov Institute of Semiconductor Physics, National Academy of Sciences, pr. Nauki 41, Kyiv, 03028, UkraineYu. V. KryuchenkoLashkaryov Institute of Semiconductor Physics, National Academy of Sciences, pr. Nauki 41, Kyiv, 03028, UkraineV. P. KostylyovLashkaryov Institute of Semiconductor Physics, National Academy of Sciences, pr. Nauki 41, Kyiv, 03028, UkraineI.O. SokolovskyiLashkaryov Institute of Semiconductor Physics, National Academy of Sciences, pr. Nauki 41, Kyiv, 03028, UkraineА. АбрамовA. V. BobylIoffe Physical–Technical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021, RussiaI. E. PanaĭottiIoffe Physical–Technical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021, RussiaE. I. TerukovIoffe Physical–Technical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021, Russia
2016en
ABI

Аннотация

An approach is proposed to calculate the optimal parameters of silicon-based heterojunction solar cells whose key feature is a low rate of recombination processes in comparison with direct-gap semiconductors. It is shown that at relatively low majority-carrier concentrations (N d ∼ 1015 cm–3), the excess carrier concentration can be comparable to or higher than N d . In this case, the efficiency η is independent of N d . At higher N d , the dependence η(N d ) is defined by two opposite trends. One of them promotes an increase in η with N d , and the other associated with Auger recombination leads to a decrease in η. The optimum value N d ≈ 2 × 1016 cm–3 at which η of such a cell is maximum is determined. It is shown that maximum η is 1.5–2% higher than η at 1015 cm–3.

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