ICMUB (UMR CNRS 6302), Université de Bourgogne Franche-Comté-9 , Avenue Alain Savary-BP 47870, 21078 Dijon Cedex, France.
Department of Chemistry, Université de Sherbrooke , 2500, Bd de l'Université, J1K 2R1 Sherbrooke, Québec, Canada.
ACS Appl Mater Interfaces. 2018 Jan 10;10(1):992-1004. doi: 10.1021/acsami.7b16112. Epub 2017 Dec 19.
Low bandgap A-π-D copolymer, P(BdP-DEHT), consisting of alternating BOronDIPYrromethene (BODIPY) and thiophene units bridged by ethynyl linkers, and its porphyrin-enriched analogue, P(BdP/Por-DEHT), were prepared, and their optical and electrochemical properties were studied. P(BdP-DEHT) exhibits strong absorption in the 500-800 nm range with an optical bandgap of 1.74 eV. On the basis of cyclic voltammetry, the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy levels are evaluated to be -5.40 and -3.66 eV, respectively. After the anchoring of zinc(II) porphyrin on the BODIPY unit, P(BdP/Por-DEHT) displays broadened absorption, thanks to porphyrins, and the optical bandgap decreases to 1.59 eV because of extension of BODIPY conjugation. The resulting estimated HOMO and LUMO energy levels, respectively, move to -5.32 and -3.73 eV. After optimization of the P(BdP-DEHT) or P(BdP/Por-DEHT) to PCBM weight ratio to 1:2 in dichlorobenzene solution, the bulk heterojunction polymer solar cells show overall power conversion efficiencies (PCEs) of 3.03 and 3.86%, respectively. After solvent vapor annealing (SVA) treatment in CHCl for 40 s, the PCEs increased to 7.40% [V of 0.95 V, J of 12.77 mA/cm, and fill factor (FF) of 0.61 with energy loss of 0.79 eV] and 8.79% (V of 0.92 V, J of 14.48 mA/cm, and FF of 0.66 with energy loss of 0.67 eV). The increase in the PCE for P(BdP/Por-DEHT)-based devices is mainly attributed to the enhancement in J and FF, which may be related to the broader absorption spectra, lower band gap, and better charge transport of P(BdP/Por-DEHT) compared to P(BdP-DEHT). This could also be related to the optimized nanoscale morphology of the active layer for both efficient exciton dissociation and charge transport toward the electrodes and a balanced charge transport in the device, induced by the SVA treatment of the active layer.
低带隙 A-π-D 共聚物 P(BdP-DEHT)由交替的 BOronDIPYrromethene (BODIPY) 和噻吩单元通过乙炔基连接桥组成,以及其富含卟啉的类似物 P(BdP/Por-DEHT),被制备出来,并研究了它们的光学和电化学性质。P(BdP-DEHT)在 500-800nm 范围内表现出强烈的吸收,光学带隙为 1.74eV。基于循环伏安法,最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)能级分别评估为-5.40 和-3.66eV。在 BODIPY 单元上锚定锌(II)卟啉后,P(BdP/Por-DEHT)显示出由于卟啉的存在而拓宽的吸收,并且由于 BODIPY 共轭的扩展,光学带隙降低至 1.59eV。由此产生的估计 HOMO 和 LUMO 能级分别移动到-5.32 和-3.73eV。在二氯苯溶液中将 P(BdP-DEHT)或 P(BdP/Por-DEHT)优化至与 PCBM 的重量比为 1:2 后,体异质结聚合物太阳能电池分别显示出 3.03%和 3.86%的整体功率转换效率(PCE)。在 CHCl 中进行溶剂蒸气退火(SVA)处理 40s 后,PCE 增加到 7.40%[V 为 0.95V,J 为 12.77mA/cm,填充因子(FF)为 0.61,能量损失为 0.79eV]和 8.79%(V 为 0.92V,J 为 14.48mA/cm,FF 为 0.66,能量损失为 0.67eV)。基于 P(BdP/Por-DEHT)器件的 PCE 增加主要归因于 J 和 FF 的增强,这可能与 P(BdP/Por-DEHT)与 P(BdP-DEHT)相比具有更宽的吸收光谱、更低的带隙和更好的电荷输运有关。这也可能与活性层的 SVA 处理导致的活性层中高效激子解离和电荷输向电极以及器件中电荷输运的平衡有关。