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Abstract
Doping has been widely used to control the charge carrier concentration in organic semiconductors. However, in conjugated polymers, n-doping is often limited by the tradeoff between doping efficiency and charge carrier mobilities, since dopants often randomly distribute within polymers, leading to significant structural and energetic disorder. Here, we screen a large number of polymer building block combinations and explore the possibility of designing n-type conjugated polymers with good tolerance to dopant-induced disorder. We show that a carefully designed conjugated polymer with a single dominant planar backbone conformation, high torsional barrier at each dihedral angle, and zigzag backbone curvature is highly dopable and can tolerate dopant-induced disorder. With these features, the designed diketopyrrolopyrrole (DPP)-based polymer can be efficiently n-doped and exhibit high n-type electrical conductivities over 120 S cm−1, much higher than the reference polymers with similar chemical structures. This work provides a polymer design concept for highly dopable and highly conductive polymeric semiconductors.
In conjugated polymers, n-doping is often limited by the tradeoff between doping efficiency and charge carrier mobilities, since dopants often randomly distribute within polymers, leading to significant structural and energetic disorder. Here, the authors screen a large number of polymer building block combinations and explore the possibility of designing n-type conjugated polymers with good tolerance to dopant-induced disorder.
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1 Peking University, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); Peking University, Beijing National Laboratory for Molecular Science, College of Chemistry and Molecular Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); South-Central University for Nationalities, Key Laboratory of Catalysis and Energy Materials Chemistry of Ministry of Education & Hubei Key Laboratory of Catalysis and Materials Science, Hubei R&D Center of Hyperbranched Polymers Synthesis and Applications, Wuhan, China (GRID:grid.412692.a) (ISNI:0000 0000 9147 9053)
2 Peking University, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); Peking University, Beijing National Laboratory for Molecular Science, College of Chemistry and Molecular Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
3 Peking University, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
4 The University of Southern Mississippi, Center for Optoelectronic Materials and Devices, School of Polymer Science and Engineering, Hattiesburg, USA (GRID:grid.267193.8) (ISNI:0000 0001 2295 628X)
5 Hong Kong Baptist University, Department of Physics, Institute of Advanced Materials, Hong Kong SAR, China (GRID:grid.221309.b) (ISNI:0000 0004 1764 5980)
6 Beijing Normal University, Key Laboratory of Theoretical and Computational Photochemistry of Ministry of Education, College of Chemistry, Beijing, China (GRID:grid.20513.35) (ISNI:0000 0004 1789 9964)
7 Peking University, Beijing National Laboratory for Molecular Science, College of Chemistry and Molecular Engineering, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
8 Beijing Normal University, Key Laboratory of Theoretical and Computational Photochemistry of Ministry of Education, College of Chemistry, Beijing, China (GRID:grid.20513.35) (ISNI:0000 0004 1789 9964); Chinese Academy of Sciences, Laboratory of Theoretical and Computational Nanoscience, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309)