论文标题

高对称性蒽的分子填料基序可促进热激活的单线裂变

High symmetry anthradithiophene molecular packing motifs promote thermally-activated singlet fission

论文作者

Mayonado, Gina, Vogt, Kyle T., Van Schenck, Jonathan D. B., Zhu, Liangdong, Anthony, John, Ostroverkhova, Oksana, Graham, Matt W.

论文摘要

当考虑最佳分子堆积以实现有机光伏材料中的电荷乘法时,分子间电荷转移(CT)耦合的细微变化可以强烈调节单重裂变。为了了解为什么某些包装形态更有利于通过三重态对(TT)形成充电乘法,我们测量了氟胞菌的四个单晶官能化衍生物的衍射限量瞬时吸收(TA)响应(TA)响应(TA)响应(TA):r = tes,tsbs,tsbs,tdms,tdms,tbdms,dif r-adt(dif r-adt)。 DIFTE-ADT和DIF TDMS-ADT均表现出2D砖砌堆积结构,DIF TSBS-ADT采用1D三明治 - herringbone填料结构,而DIF TBDMS-ADT则表现出1D扭曲的柱子堆积结构。当砖砌或扭曲的单晶被共同探测到平行于其电荷转移(CT)轴突起时,TA信号由Picsecond TimeCale上的上升组件(速率$ k_ {tt} $)归因于TT州人群。当探测到CT轴正交时,我们会以$ k_ {a} $恢复单元状态耗竭的下落动力学。上升与下降率估计TT编队效率,$ε_{tt} $ = $ k_ {tt}/k_a $相对于激子自我捕捞。 $ε_{tt} $范围从差异dift-adt的接近统一到dif tdms-adt中的84%。有趣的是,DIF TSB-ADT晶体仅表现出CT介导的自诱饵和单线状态耗竭的动力学。由于其较低的对称三明治人字填料的差异TSBS-ADT晶体的单裂裂变是高度的,导致$ S_1 $ to $ s_1 $ to CT-State Energy Eapination,比其他包装大约3倍。总的来说,这些结果突出了最佳的包装配置,可以增强或完全抑制CT介导的TT对形成。

When considering the optimal molecular packing to realize charge multiplication in organic photovoltaic materials, subtle changes in intermolecular charge transfer (CT) coupling can strongly modulate singlet fission. To understand why certain packing morphologies are more conducive to charge multiplication by triplet pair (TT) formation, we measure the diffraction-limited transient absorption (TA) response from four single-crystal functionalized derivatives of fluorinated anthradithiophene: diF R-ADT (R = TES, TSBS, TDMS, TBDMS). diF TES-ADT and diF TDMS-ADT both exhibit 2D brickwork packing structures, diF TSBS-ADT adopts a 1D sandwich-herringbone packing structure, and diF TBDMS-ADT exhibits a 1D twisted-columnar packing structure. When brickwork or twisted-columnar single crystals are resonantly probed parallel to their charge transfer (CT)-axis projections, the TA signal is dominated by a rising component on the picosecond timescale (rate $k_{TT}$) attributed to TT state population. When probed orthogonal to the CT-axis, we instead recover the falling TA kinetics of singlet state depletion at rate, $k_{A}$. The rising to falling rate ratio estimates the TT formation efficiency, $ε_{TT}$ = $k_{TT}/k_A$ relative to exciton self-trapping. $ε_{TT}$ ranged from near unity in diF TES-ADT to 84% in diF TDMS-ADT. Interestingly, diF TSBS-ADT crystals only manifest falling kinetics of CT-mediated self-trapping and singlet state depletion. Singlet fission is prohibitive in diF TSBS-ADT crystals owing to its lower symmetry sandwich herringbone packing that leads to $S_1$ to CT-state energy separation that is ~3x larger than in other packings. Collectively, these results highlight optimal packing configurations that either enhance or completely suppress CT-mediated TT-pair formation.

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