4.8 Article

Bulk heterojunction perovskite solar cells incorporated with p-type low optical gap conjugated polymers

Journal

NANO ENERGY
Volume 93, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.nanoen.2021.106907

Keywords

Perovskite solar cells; Bulk heterojunction device structure; Low optical gap conjugated polymer; Efficiency; Stability and photocurrent hysteresis

Funding

  1. National Science Foundation, USA [ECCS/EPMD1903303]

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This study presents high-performance perovskite solar cells (PSCs) based on a composite of perovskite and a low optical gap conjugated polymer. The composite film exhibits enhanced charge carrier mobility, larger crystal sizes, and suppressed non-radiation charge carrier recombination. Additionally, a photo-induced charge transfer occurs within the composite film, leading to improved power conversion efficiency (PCE) of the PSCs. The un-encapsulated PSCs also demonstrate enhanced stability and reduced photocurrent hysteresis compared to those based on pristine perovskite films.
Perovskite solar cells (PSCs) as alternative cost-effective solar technology have drawn great concentrations in both academic and industrial sectors in the past years. Through the film morphological manipulation of perovskite photoactive layers and generic interfacial engineering, efficient PSCs have been reported. However, intrinsic unbalanced charge transport within the perovskite photoactive layer, which restricted further boost device performance of PSCs, was not fully addressed. In this study, we report high-performance bulk heterojunction (BHJ) PSCs based on the composites composed of n-type Cs(0.15)FA(0.85)PbI(3) (where FA is formamidinium, HC(NH2)(2)) incorporated with p-type low optical gap conjugated polymer. Compared to pristine Cs(0.15)FA(0.85)PbI(3) thin film, the BHJ composite thin film possesses enhanced and balanced charge carrier mobilities, enlarged crystal sizes, and suppressed non-radiation charge carrier recombination. Most importantly, a photo-induced charge transfer occurs within the BHJ composite thin film. As a result, the BHJ PSCs exhibit a power conversion efficiency (PCE) of 21.08%. In addition, un-encapsulated BHJ PSCs possess remarkably enhanced stability (as they retain 80% of their initial PCE after similar to 200 days in ambient conditions) and diminished photocurrent hysteresis (photocurrent hysteresis index of 0.012) compared to those based on pristine Cs(0.15)FA(0.85)PbI(3) thin film. All these results demonstrate that the PSCs with a BHJ device structure are one of the facile ways to approach high-performance PSCs.

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