Impact of N-substitution of a carbazole unit on molecular packing and charge transport of DPP-carbazole copolymers

被引:16
作者
Chen, Shaoyun [1 ,2 ,3 ]
Sun, Bin [1 ,2 ]
Hong, Wei [1 ,2 ]
Yan, Zhuangqing [1 ,2 ]
Aziz, Hany [4 ]
Meng, Yuezhong [3 ]
Hollinger, Jon [5 ]
Seferos, Dwight S. [5 ]
Li, Yuning [1 ,2 ]
机构
[1] Univ Waterloo, Dept Chem Engn, Waterloo, ON N2L 3G1, Canada
[2] Waterloo Inst Nanotechnol, Waterloo, ON N2L 3G1, Canada
[3] Sun Yat Sen Univ, State Key Lab Optoelect Mat & Technol, Key Lab Law Carbon Chem & Energy Conservat Guangd, Guangzhou 510275, Guangdong, Peoples R China
[4] Univ Waterloo, Waterloo Inst Nanotechnol, Dept Elect & Comp Engn, Waterloo, ON N2L 3G1, Canada
[5] Univ Toronto, Dept Chem, Toronto, ON M5S 3H6, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
POLYMER SOLAR-CELLS; HIGH-MOBILITY; SIDE-CHAINS; FILM; SEMICONDUCTOR;
D O I
10.1039/c3tc31753f
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Two diketopyrrolopyrrole (DPP)-carbazole (Cz) based pi-conjugated copolymers, PDBTCz-H (P1) and PDBTCz-Me (P2), were designed and synthesized to study the effects of N-substitution of the carbazole unit on the molecular ordering, main chain conjugation, and charge transport properties of these polymers. It was found that the existence of hydrogen bonding interaction between the N-H group in the carbazole unit and the C=O group in the DPP unit has a significant impact on the UV absorption, crystallinity, thin film morphology, as well as charge transport characteristics of P1. The hydrogen bonding is a very competitive force with the is pi-pi stacking interaction, leading to the more twisted backbone structure and poorer molecular ordering of P1 in the solid state. Although the crystallinity of the P1 thin films could be somewhat improved by thermal annealing, the polymer main chains of P1 remain rather twisted and less conjugated in comparison with P2. The poorer main chain conjugation of P1 caused by the hydrogen bonding led to a dramatic drop in charge transport performance in organic thin film transistors (OTFTs). The highest hole mobility achieved for P1 is 8.9 x 10(-3) cm(2) V-1 s(-1), which is almost two orders of magnitude lower than that of P2 (0.53 cm(2) V-1 s(-1)).
引用
收藏
页码:1683 / 1690
页数:8
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