Nickel Oxide Hole‐Selective Heterocontact for Silicon Solar Cells: Role of SiOx Interlayer on Device Performance
Solar RRL, 2019•Wiley Online Library
Carrier‐selective contact‐based silicon heterojunction solar cells are fabricated using nickel
oxide (NiOx) as a hole‐selective layer by thermal evaporation. The highest power
conversion efficiency of≈ 15.20% with a chemically grown SiOx interlayer is achieved from
a Ag/ITO/NiOx/n‐Si/LiFx/Al cell structure in comparison with≈ 12.43% without SiOx. The
cells without and with the SiOx layer are analyzed by considering crucial parameters for
conversion efficiency, such as minority carriers' diffusion lengths, lifetimes, recombination …
oxide (NiOx) as a hole‐selective layer by thermal evaporation. The highest power
conversion efficiency of≈ 15.20% with a chemically grown SiOx interlayer is achieved from
a Ag/ITO/NiOx/n‐Si/LiFx/Al cell structure in comparison with≈ 12.43% without SiOx. The
cells without and with the SiOx layer are analyzed by considering crucial parameters for
conversion efficiency, such as minority carriers' diffusion lengths, lifetimes, recombination …
Carrier‐selective contact‐based silicon heterojunction solar cells are fabricated using nickel oxide (NiOx) as a hole‐selective layer by thermal evaporation. The highest power conversion efficiency of ≈15.20% with a chemically grown SiOx interlayer is achieved from a Ag/ITO/NiOx/n‐Si/LiFx/Al cell structure in comparison with ≈12.43% without SiOx. The cells without and with the SiOx layer are analyzed by considering crucial parameters for conversion efficiency, such as minority carriers' diffusion lengths, lifetimes, recombination resistance, and density of interface defect states at the NiOx/n‐Si junction, by studying the dark/light current density–voltage, quantum efficiency, impedance, and parallel conductance characteristics. Device analysis provides evidence for the cell's open‐circuit voltage and short‐circuit current enhancement with the SiOx interlayer. This is due to an improvement in minority carrier lifetimes from ≈8.6 to ≈48.27 μs (photo‐conductance decay analysis), which is also estimated from ≈7.45 to ≈49.20 μs by impedance spectra analysis, increased minority carrier diffusion length from ≈171 to ≈952 μm, and decreased rear surface recombination velocity from ≈1106 to ≈170 cm s−1 (quantum efficiency analysis). These investigations reveal that engineering the n‐Si/LiFx interface by the SiOx interlayer is more important than the NiOx/n‐Si interface because of a thin unintentionally grown SiOx layer during NiOx evaporation simultaneously mediating silicon surface passivation.
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