Department of Chemistry, University of Southern California , Los Angeles, California 90089, United States.
J Am Chem Soc. 2016 Jan 20;138(2):617-27. doi: 10.1021/jacs.5b10550. Epub 2016 Jan 6.
Singlet fission is a process in which a singlet exciton converts into two triplet excitons. To investigate this phenomenon, we synthesized two covalently linked 5-ethynyl-tetracene (ET) dimers with differing degrees of intertetracene overlap: BET-X, with large, cofacial overlap of tetracene π-orbitals, and BET-B, with twisted arrangement between tetracenes exhibits less overlap between the tetracene π-orbitals. The two compounds were crystallographically characterized and studied by absorption and emission spectroscopy in solution, in PMMA and neat thin films. The results show that singlet fission occurs within 1 ps in an amorphous thin film of BET-B with high efficiency (triplet yield: 154%). In solution and the PMMA matrix the S1 of BET-B relaxes to a correlated triplet pair (1)(T1T1) on a time scale of 2 ps, which decays to the ground state without forming separated triplets, suggesting that triplet energy transfer from (1)(T1T1) to a nearby chromophore is essential for producing free triplets. In support of this hypothesis, selective excitation of BET-B doped into a thin film of diphenyltetracene (DPT) leads to formation of the (1)(T1T1) state of BET-B, followed by generation of both DPT and BET-B triplets. For the structurally cofacial BET-X, an intermediate forms in <180 fs and returns to the ground state more rapidly than BET-B. First-principles calculations predict a 2 orders of magnitude faster rate of singlet fission to the (1)(T1T1) state in BET-B relative to that of crystalline tetracene, attributing the rate increase to greater coupling between the S1 and (1)(T1T1) states and favorable energetics for formation of the separated triplets.
单线态裂变是一个单线态激子转化为两个三线态激子的过程。为了研究这一现象,我们合成了两个通过共价键连接的具有不同程度并五苯重叠的 5-乙炔基并五苯(ET)二聚体:BET-X,具有大的、共面的并五苯π轨道重叠,而 BET-B 则表现出扭曲排列,其并五苯π轨道之间的重叠较小。这两种化合物在结晶上进行了表征,并通过吸收和发射光谱在溶液中、在 PMMA 中和在纯薄膜中进行了研究。结果表明,在 BET-B 的非晶态薄膜中,单线态裂变在 1 ps 内发生,效率很高(三重态产率:154%)。在溶液和 PMMA 基质中,BET-B 的 S1 在 2 ps 时间尺度上弛豫到相关的三重态对(1)(T1T1),然后没有形成分离的三重态而回到基态,这表明从(1)(T1T1)到附近发色团的三重态能量转移对于产生游离三重态至关重要。为了支持这一假设,选择性地激发掺杂在二苯基并五苯(DPT)薄膜中的 BET-B 会导致 BET-B 的(1)(T1T1)状态的形成,然后产生 DPT 和 BET-B 的三重态。对于结构共面的 BET-X,中间态在<180 fs 内形成,并比 BET-B 更快地回到基态。第一性原理计算预测,相对于晶体并五苯,BET-B 中单线态裂变到(1)(T1T1)态的速率快 2 个数量级,这归因于 S1 和(1)(T1T1)态之间的耦合增强以及形成分离三重态的有利能态。