Gobeze Habtom B, Younus Muhammed, Turlington Michael D, Ahmed Sohel, Schanze Kirk S
Department of Chemistry, University of Texas at San Antonio, One UTSA Circle, San Antonio, TX 78249, USA.
Molecules. 2024 Jun 5;29(11):2678. doi: 10.3390/molecules29112678.
Diblock conjugated oligomers are π-conjugated molecules that contain two segments having distinct frontier orbital energies and HOMO-LUMO gap offsets. These oligomers are of fundamental interest to understand how the distinct π-conjugated segments interact and modify their excited state properties. The current paper reports a study of two series of diblock oligomers that contain oligothiophene (T) and 4,7-bis(2-thienyl)-2,1,3-benzothiadiazole (TBT) segments that are coupled by either ethynyl (-C≡C-) or -(-C≡C-)Pt(II)(PBu) acetylide linkers. In these structures, the T segment is electron rich (donor), and the TBT is electron poor (acceptor). The diblock oligomers are characterized by steady-state and time-resolved spectroscopy, including UV-visible absorption, fluorescence, fluorescence lifetimes, and ultrafast transient absorption spectroscopy. Studies are compared in several solvents of different polarity and with different excitation wavelengths. The results reveal that the (-C≡C-) linked oligomers feature a delocalized excited state that takes on a charge transfer (CT) character in more polar media. In the (-C≡C-)Pt(II)(PBu)-linked oligomers, there is weak coupling between the T and TBT segments. Consequently, short wavelength excitation selectively excites the T segment, which then undergoes ultrafast energy transfer (~1 ps) to afford a TBT-localized excited state.
双嵌段共轭低聚物是π共轭分子,包含两个具有不同前沿轨道能量和HOMO-LUMO能隙偏移的链段。这些低聚物对于理解不同的π共轭链段如何相互作用并改变其激发态性质具有重要的基础研究意义。本文报道了对两个系列双嵌段低聚物的研究,这些低聚物包含由乙炔基(-C≡C-)或 -(-C≡C-)Pt(II)(PBu)乙炔化物连接基偶联的低聚噻吩(T)和4,7-双(2-噻吩基)-2,1,3-苯并噻二唑(TBT)链段。在这些结构中,T链段是富电子的(供体),而TBT是缺电子的(受体)。双嵌段低聚物通过稳态和时间分辨光谱进行表征,包括紫外可见吸收、荧光、荧光寿命和超快瞬态吸收光谱。在几种不同极性的溶剂中以及不同激发波长下进行了研究比较。结果表明,(-C≡C-)连接的低聚物具有离域激发态,在极性更强的介质中呈现电荷转移(CT)特征。在(-C≡C-)Pt(II)(PBu)连接的低聚物中,T和TBT链段之间存在弱耦合。因此,短波长激发选择性地激发T链段,然后T链段经历超快能量转移(~1 ps)以产生TBT局域激发态。