Tandem solar cell structures require a high‐performance wide band gap absorber as top cell. A possible candidate is CuGaSe 2 , with a fundamental band gap of 1.7 eV. However, a significant open‐circuit voltage deficit is often reported for wide band gap chalcopyrite solar cells like CuGaSe 2 . In this paper, we show that the open‐circuit voltage can be drastically improved in wide band gap p‐Cu(In,Ga)Se 2 and p‐CuGaSe 2 devices by improving the conduction band alignment to the n‐type buffer layer. This is accomplished by using Zn 1− x Sn x O y , grown by atomic layer deposition, as a buffer layer. In this case, the conduction band level can be adapted to an almost perfect fit to the wide band gap Cu(In,Ga)Se 2 and CuGaSe 2 materials. With an improved buffer band alignment for CuGaSe 2 absorbers, evaporated in a 3‐stage type process, we show devices exhibiting open‐circuit voltages up to 1017 mV, and efficiencies up to 11.9%. This is to the best of our knowledge the highest reported open‐circuit voltage and efficiency for a CuGaSe 2 device. Temperature‐dependent current‐voltage measurements show that the high open‐circuit voltage is explained by reduced interface recombination, which makes it possible to separate the influence of absorber quality from interface recombination in future studies. An enhancement of open‐circuit voltage and conversion efficiency in wide band gap Cu(In 1− x )Ga x Se 2 solar cells is achieved by implementing a conduction band matched Zn 1− x Sn x O y front contact, grown with atomic layer deposition. An open‐circuit voltage of 1017 mV and an efficiency of 11.9% is demonstrated for a CuGaSe 2 /Zn 1− x Sn x O y device, by reducing the interface recombination.
Record 1.0 V open‐circuit voltage in wide band gap chalcopyrite solar cells
Progress in photovoltaics ; 25 , 9
2017
Aufsatz (Zeitschrift)
Englisch
BKL: | 53.36 Energiedirektumwandler, elektrische Energiespeicher |
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