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Base doping optimization for radiation-hard Si, GaAs, and InP solar cells

机译:耐辐射的Si,GaAs和InP太阳能电池的基极掺杂优化

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It is shown that the nature of radiation-induced point defects and dopant interactions can cause a shift in the optimum base doping concentration for terrestrial and space solar cells. The base doping concentration has been optimized for high-efficiency Si, GaAs, and InP solar cells before and after electron irradiation. A combination of detailed carrier lifetime calculations and cell modeling is used to show that the optimum doping concentration for irradiated cells increases for InP cells, decreases for Si cells, and remains essentially unchanged for GaAs cells compared to their counterpart terrestrial cells. The optimum base doping for Si cells decreases from 8.94*10/sup 16/ cm/sup -3/ to approximately 6.6*10/sup 14/ cm/sup -1/ after 1-MeV electron irradiation. In the case of GaAs, the optimum base doping concentration remains at approximately 2*10/sup 17/ cm/sup -3/ for both irradiated and unirradiated cells. The InP base doping needs to be increased in the range of (2-6)*10/sup 17/ cm/sup -3/ from 2*10/sup 17/ cm/sup -3/ for radiation fluences in the range of 10/sup 15/ to 10/sup 16/ cm/sup -2/.
机译:结果表明,辐射诱发的点缺陷和掺杂剂相互作用的性质会导致地面和空间太阳能电池的最佳基础掺杂浓度发生变化。已针对电子辐照前后的高效Si,GaAs和InP太阳能电池优化了基本掺杂浓度。与详细的载流子寿命计算和电池建模相结合,可以证明与InP电池相比,被辐照电池的最佳掺杂浓度与InP电池相比有所降低,而与GaAs电池相比,其最佳掺杂浓度却基本保持不变。在1 MeV电子辐照后,Si电池的最佳基极掺杂从8.94 * 10 / sup 16 / cm / sup -3 /降至约6.6 * 10 / sup 14 / cm / sup -1 /。在GaAs的情况下,对于被照射的和未被照射的电池,最佳的基本掺杂浓度都保持在大约2×10 / sup 17 / cm / sup -3 /。 InP基本掺杂需要在(2-6)* 10 / sup 17 / cm / sup -3 /的范围内从2 * 10 / sup 17 / cm / sup -3 /的范围内增加, 10 / sup 15 /至10 / sup 16 / cm / sup -2 /。

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