• Journal of Semiconductors
  • Vol. 42, Issue 10, 101607 (2021)
Liu Ye1, Weiyu Ye1, and Shiming Zhang1、2
Author Affiliations
  • 1Key Laboratory of Flexible Electronics (KLOFE) & Institute of Advanced Materials (IAM), Jiangsu National Synergetic Innovation Center for Advanced Materials (SICAM), Nanjing Tech University, Nanjing 211816, China
  • 2Jiangsu Seenbom Flexible Electronics Institute Co. Ltd., Nanjing 210043, China
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    DOI: 10.1088/1674-4926/42/10/101607 Cite this Article
    Liu Ye, Weiyu Ye, Shiming Zhang. Recent advances and prospects of asymmetric non-fullerene small molecule acceptors for polymer solar cells[J]. Journal of Semiconductors, 2021, 42(10): 101607 Copy Citation Text show less

    Abstract

    Recently, polymer solar cells developed very fast due to the application of non-fullerence acceptors. Substituting asymmetric small molecules for symmetric small molecule acceptors in the photoactive layer is a strategy to improve the performance of polymer solar cells. The asymmetric design of the molecule is very beneficial for exciton dissociation and charge transport and will also fine-tune the molecular energy level to adjust the open-circuit voltage (Voc) further. The influence on the absorption range and absorption intensity will cause the short-circuit current density (Jsc) to change, resulting in higher device performance. The effect on molecular aggregation and molecular stacking of asymmetric structures can directly change the microscopic morphology, phase separation size, and the active layer's crystallinity. Very recently, thanks to the ingenious design of active layer materials and the optimization of devices, asymmetric non-fullerene polymer solar cells (A-NF-PSCs) have achieved remarkable development. In this review, we have summarized the latest developments in asymmetric small molecule acceptors (A-NF-SMAs) with the acceptor–donor–acceptor (A–D–A) and/or acceptor–donor–acceptor–donor–acceptor (A–D–A–D–A) structures, and the advantages of asymmetric small molecules are explored from the aspects of charge transport, molecular energy level and active layer accumulation morphology.
    $ \mathrm{F}\mathrm{F}=\frac{{V}_{\mathrm{m}\mathrm{a}\mathrm{x}} {{J}}_{\mathrm{m}\mathrm{a}\mathrm{x}}}{V_{\mathrm{o}\mathrm{c}} J_{\mathrm{s}\mathrm{c}}}=\frac{{P}_{\mathrm{m}\mathrm{a}\mathrm{x}}}{V_{\mathrm{o}\mathrm{c}} J_{\mathrm{s}\mathrm{c}}} . $ (1)

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    $ \mathrm{P}\mathrm{C}\mathrm{E}=\frac{{P}_{\mathrm{m}\mathrm{a}\mathrm{x}}}{{P}_{\mathrm{i}\mathrm{n}}}=\frac{{V}_{\mathrm{m}\mathrm{a}\mathrm{x}} {J}_{\mathrm{m}\mathrm{a}\mathrm{x}}}{{P}_{\mathrm{i}\mathrm{n}}}=\frac{V_{\mathrm{o}\mathrm{c}} J_{\mathrm{s}\mathrm{c}} \mathrm{F}\mathrm{F}}{{P}_{\mathrm{i}\mathrm{n}}} . $ (2)

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    $ \mathrm{E}\mathrm{Q}\mathrm{E}=\frac{1240 J_{\mathrm{s}\mathrm{c}}}{{\lambda }{P}_{\mathrm{i}\mathrm{n}}}. $ (3)

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    Liu Ye, Weiyu Ye, Shiming Zhang. Recent advances and prospects of asymmetric non-fullerene small molecule acceptors for polymer solar cells[J]. Journal of Semiconductors, 2021, 42(10): 101607
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