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氟化对茚并二噻吩并噻吩受体堆积、电子结构、端基重分布及太阳能电池光伏响应的影响

Fluorination Effects on Indacenodithienothiophene Acceptor Packing and Electronic Structure, End-Group Redistribution, and Solar Cell Photovoltaic Response.

作者信息

Aldrich Thomas J, Matta Micaela, Zhu Weigang, Swick Steven M, Stern Charlotte L, Schatz George C, Facchetti Antonio, Melkonyan Ferdinand S, Marks Tobin J

机构信息

Flexterra Corporation , 8025 Lamon Avenue , Skokie , Illinois 60077 , United States.

出版信息

J Am Chem Soc. 2019 Feb 20;141(7):3274-3287. doi: 10.1021/jacs.8b13653. Epub 2019 Feb 7.

Abstract

Indacenodithienothiophene (IDTT)-based postfullerene electron acceptors, such as ITIC (2,2'-[[6,6,12,12-tetrakis(4-hexylphenyl)-6,12-dihydrodithieno[2,3- d:2',3'- d']-s-indaceno[1,2- b:5,6- b']dithiophene-2,8-diyl]-bis[methylidyne(3-oxo-1 H-indene-2,1(3 H)-diylidene)]]bis[propanedinitrile]), have become synonymous with high power conversion efficiencies (PCEs) in bulk heterojunction (BHJ) polymer solar cells (PSCs). Here we systematically investigate the influence of end-group fluorination density and positioning on the physicochemical properties, single-crystal packing, end-group redistribution propensity, and BHJ photovoltaic performance of a series of ITIC variants, ITIC- nF ( n = 0, 2, 3, 4, and 6). Increasing n from 0 → 6 contracts the optical bandgap, but only marginally lowers the LUMO for n > 4. This yields enhanced photovoltaic short-circuit current density and good open-circuit voltage, so that ITIC-6F achieves the highest PCE of the series, approaching 12% in blends with the PBDB-TF donor polymer. Single-crystal diffraction reveals that the ITIC- nF molecules cofacially interleave with ITIC-6F having the shortest π-π distance of 3.28 Å. This feature together with ZINDO-level computed intermolecular electronic coupling integrals as high as 57 meV, and B3LYP/DZP-level reorganization energies as low as 147 meV, rival or surpass the corresponding values for fullerenes, ITIC-0F, and ITIC-4F, and track a positive correlation between the ITIC- nF space-charge limited electron mobility and n. Finally, a heretofore unrecognized solution-phase redistribution process between the 2-(3-oxo-indan-1-ylidene)-malononitrile-derived end-groups (EGs) of IDTT-based NFAs, i.e., EG-IDTT-EG + EG-IDTT-EG ⇌ 2 EG-IDTT-EG, with implications for the entire ITIC PSC field, is identified and mechanistically characterized, and the effects on PSC performance are assessed.

摘要

基于茚并二噻吩并噻吩(IDTT)的后富勒烯电子受体,如ITIC(2,2'-[[6,6,12,12-四(4-己基苯基)-6,12-二氢二噻吩并[2,3-d:2',3'-d']-s-茚并[1,2-b:5,6-b']二噻吩-2,8-二基]-双[亚甲基(3-氧代-1H-茚-2,1(3H)-二亚基)]]双[丙二腈]),已成为体异质结(BHJ)聚合物太阳能电池(PSC)中高功率转换效率(PCE)的代名词。在此,我们系统地研究了端基氟化密度和位置对一系列ITIC变体ITIC-nF(n = 0、2、3、4和6)的物理化学性质、单晶堆积、端基重新分布倾向以及BHJ光伏性能的影响。将n从0增加到6会使光学带隙收缩,但对于n > 4时,仅略微降低最低未占分子轨道(LUMO)。这导致光伏短路电流密度增强且开路电压良好,因此ITIC-6F在与PBDB-TF供体聚合物的共混物中实现了该系列中的最高PCE,接近12%。单晶衍射表明,ITIC-nF分子共面交错排列,ITIC-6F的最短π-π距离为3.28 Å。这一特征与高达57 meV的ZINDO水平计算的分子间电子耦合积分以及低至147 meV的B3LYP/DZP水平重组能一起,与富勒烯、ITIC-0F和ITIC-4F的相应值相当或超过这些值,并追踪了ITIC-nF空间电荷限制电子迁移率与n之间的正相关关系。最后,我们确定并从机理上表征了基于IDTT的非富勒烯受体(NFA)的2-(3-氧代茚-1-亚基)-丙二腈衍生端基(EG)之间一种此前未被认识的溶液相重新分布过程,即EG-IDTT-EG + EG-IDTT-EG ⇌ 2 EG-IDTT-EG,该过程对整个ITIC PSC领域具有重要意义,并评估了其对PSC性能的影响。

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