20.6% Efficiency Organic Solar Cells Enabled by Incorporating a Lower Bandgap Guest Nonfullerene Acceptor Without Open‐Circuit Voltage Loss

Y Yuanyuan Jiang K Kerui Liu (Beijing National Laboratory for Molecular Sciences CAS Key Laboratory of Organic Solids and State Key Laboratory of Polymer Physics and Chemistry Institute of Chemistry Chinese Academy of Sciences Beijing 100190 China) F Feng Liu G Guangliu Ran (School of Physics and Astronomy, Applied Optics Beijing Area Major Laboratory, Center for Advanced Quantum Studies) M Mengni Wang (CAS Key Laboratory of Nanosystem and Hierarchical Fabrication CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology Beijing 100190 P.R. China) T Tao Zhang R Renjie Xu (Center For Future Organic Optoelectronics Global Institute of Future Technology (GIFT) Shanghai Jiao Tong University Shanghai P. R. China) H Heng Liu W Wenkai Zhang (School of Physics and Astronomy, Applied Optics Beijing Area Major Laboratory, Center for Advanced Quantum Studies) Z Zhixiang Wei (CAS Key Laboratory of Nanosystems and Hierarchical Fabrication, National Center for Nanoscience and Technology) Y Yong Cui X Xinhui Lu (Department of Physics) J Jianhui Hou (State Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences) X Xiaozhang Zhu (Global Institute of Future Technology Shanghai Jiao Tong University Shanghai China)

Abstract

AbstractSimultaneously mitigating both photovoltage and photocurrent losses is crucial for organic solar cells (OSCs) to approach the Shockley–Queisser limit of ideal efficiency. Incorporating a narrower bandgap nonfullerene acceptor (NFA) as a guest component into the host donor:NFA system broadens the absorption spectrum. However, this can also increase the nonradiative decay rate according to the energy‐gap law. In this work, ternary OSCs are constructed by combining a narrow bandgap AQx‐2F (as host NFA) with a lower bandgap eC9 (as guest NFA), significantly enhancing photocurrent generation without compromising photovoltage. The addition of eC9 acts as a crystallization inducer, extending the crystallization period and increasing the ordered packing distance. This leads to suppressed trap states, elevated dielectric constant, prolonged exciton lifetime, balanced hole/electron transport, and reduced recombination loss. Consequently, the optimized D18:AQx‐2F:eC9 ternary OSCs achieve a champion power conversion efficiency (PCE) of 20.6% with a high open‐circuit voltage of 0.937 V, a short‐circuit current density of 27.2 mA cm−2 and a fill factor of 80.8%, as validated by an independently certified PCE of 20.0%, establishing a new benchmark for bulk heterojunction OSCs. This work demonstrates an effective method to simultaneously mitigate photovoltage and photocurrent losses, paving the way for high‐performance OSCs.

Article Details

Volume / Issue Vol. 37, Issue 17
Published April 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (14)

Y

Yuanyuan Jiang

K

Kerui Liu

Beijing National Laboratory for Molecular Sciences CAS Key Laboratory of Organic Solids and State Key Laboratory of Polymer Physics and Chemistry Institute of Chemistry Chinese Academy of Sciences Beijing 100190 China

F

Feng Liu

G

Guangliu Ran

School of Physics and Astronomy, Applied Optics Beijing Area Major Laboratory, Center for Advanced Quantum Studies

M

Mengni Wang

CAS Key Laboratory of Nanosystem and Hierarchical Fabrication CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology Beijing 100190 P.R. China

T

Tao Zhang

R

Renjie Xu

Center For Future Organic Optoelectronics Global Institute of Future Technology (GIFT) Shanghai Jiao Tong University Shanghai P. R. China

H

Heng Liu

W

Wenkai Zhang

School of Physics and Astronomy, Applied Optics Beijing Area Major Laboratory, Center for Advanced Quantum Studies

Z

Zhixiang Wei

CAS Key Laboratory of Nanosystems and Hierarchical Fabrication, National Center for Nanoscience and Technology

Y

Yong Cui

X

Xinhui Lu

Department of Physics

J

Jianhui Hou

State Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences

X

Xiaozhang Zhu

Global Institute of Future Technology Shanghai Jiao Tong University Shanghai China