In recent years, polymer solar cells (PSCs) have received a great deal of attention for their low cost, light weight, solution processing capability, and mechanical flexibility.
1,2The highest PSC power conversion efficiency (PCE) reported in literature is over 8%.3 The PCE of PSCs is proportional to the short circuit current density (J sc ), the open circuit voltage (V oc ) and the fill factor (FF). The J sc is largely affected by the light-absorption property of p-type polymers and the charge mobility of active layers. The V oc is closely related to the energy difference between the highest occupied molecular orbital (HOMO) of a p-type conjugated polymer and the lowest unoccupied molecular orbital (LUMO) of an n-type material, such as [6,6]-phenyl-C 71 -butyric acid methyl ester (PC 71 BM). The morphology of the active layer between two electrodes substantially influences the FF value. Thus low band gap polymers with suitable HOMO and LUMO energy levels should be employed for the fabrication of PSCs with high PCEs.
4One of the synthetic strategies for p-type polymers involves the combination of electron-donor (D) monomers with electron-acceptor (A) monomers to form alternating D-A polymers. Various D-A polymers have been actively investigated.5,6 Phenothiazine (PT) is a heterocyclic compound with high electron-donating ability, due to its electron-rich nitrogen and sulfur heteroatoms. Thus PT is an excellent molecular building block to achieve strong donating p-type conjugated polymers for photovoltaic devices.7,8 Recently we reported a PT-diketopyrrolopyrrole polymer (PPT-DPP) with an optical band gap (E opt g ) of 1.63 eV, and a HOMO energy level of −5.20 eV.9 The PCE of the PPT-DPP-based solar cells was 1.8%. Given this data, if an appropriate acceptor is combined with PT, the resulting copolymer Scheme 1. Synthetic routes to PPT-II and PPT-T-II.