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Minimizing Current and Voltage Losses to Reach 25% Efficient Monolithic Two-Terminal Perovskite–Silicon Tandem Solar Cells AITranslate

Stanford University; Arizona State University; Stanford University; Arizona State University; Stanford University; Stanford University; Stanford University; Stanford University; Stanford University; Arizona State University; University of Colorado
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Publisher: ACS
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Abstract AITranslate

The rapid rise in efficiency and tunable bandgap of metal-halide perovskites makes them highly attractive for use in tandems on silicon. Recently we demonstrated a perovskite–silicon monolithic two-terminal tandem with 23.6% power conversion efficiency. Here, we present work on optical optimization to improve light harvesting that includes thinning out the top transparent electrode to reduce front-surface reflection and parasitic absorption; introducing metal fingers to minimize series resistance losses; and further minimizing reflection loss with a polydimethylsiloxane (PDMS) stamp with random, pyramidal texture. Additionally, to reduce voltage loss while achieving current matching, we employ poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine] (PTAA) as a hole transport material instead of NiOx and a wider 1.68 eV bandgap perovskite composition. These optimizations boost the open-circuit voltage to 1.77 V and the short-circuit current density to 18.4 mA/cm2, culminating in a 25% efficient perovskite–silicon tandem with a 1 cm2 active area.

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DOI:https://doi.org/10.1021/acsenergylett.8b01201

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Citation Information:

The rapid rise in efficiency and tunable bandgap of metal-halide perovskites makes them highly attractive for use in tandems on silicon. Recently we demonstrated a perovskite–silicon monolithic two-terminal tandem with 23.6% power conversion efficiency. Here, we present work on optical optimization to improve light harvesting that includes thinning out the top transparent electrode to reduce front-surface reflection and parasitic absorption; introducing metal fingers to minimize series resistance losses; and further minimizing reflection loss with a polydimethylsiloxane (PDMS) stamp with random, pyramidal texture. Additionally, to reduce voltage loss while achieving current matching, we employ poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine] (PTAA) as a hole transport material instead of NiOx and a wider 1.68 eV bandgap perovskite composition. These optimizations boost the open-circuit voltage to 1.77 V and the short-circuit current density to 18.4 mA/cm2, culminating in a 25% efficient perovskite–silicon tandem with a 1 cm2 active area.

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GB/T 7714-2015 [1] Kevin A. Bush, Salman Manzoor, Kyle Frohna, et al. ACS Energy Letters, 2018(3). DOI:10.1021/acsenergylett.8b01201.
MLA [1] Kevin A. Bush, et al., ACS Energy Letters, no. 3, 2018, https://doi.org/10.1021/acsenergylett.8b01201.
APA [1] Kevin A. Bush, Salman Manzoor, Kyle Frohna, Zhengshan J. Yu, James A. Raiford, Axel F. Palmstrom, HsinPing Wang, Rohit Prasanna, Stacey F. Bent, Zachary C. Holman, & Michael D. McGehee. (2018). ACS Energy Letters(3). https://doi.org/10.1021/acsenergylett.8b01201
IEEE [1] Kevin A. Bush, Salman Manzoor, Kyle Frohna, Zhengshan J. Yu, James A. Raiford, Axel F. Palmstrom, HsinPing Wang, Rohit Prasanna, Stacey F. Bent, Zachary C. Holman, and Michael D. McGehee, ACS Energy Letters, no. 3, 2018, doi: 10.1021/acsenergylett.8b01201.