Nenavath Swathi, Duvva Naresh, Kaswan Ram R, Lim Gary N, D'Souza Francis, Giribabu Lingamallu
Polymers and Functional Materials Division, CSIR-Indian Institute of Chemical Technology, Tarnaka, Hyderabad 500007, Telangana, India.
Academy of Scientific and Innovative Research (AcSIR), Ghaziabad 201002, India.
J Phys Chem A. 2023 Aug 17;127(32):6779-6790. doi: 10.1021/acs.jpca.3c04141. Epub 2023 Aug 4.
Donor-acceptor systems in which a donor phenanthroimidazole (PhI) is directly connected to a BODIPY acceptor () and separated by an ethynyl bridge between PhI and BODIPY () have been designed, synthesized, and characterized by various spectroscopic and electrochemical techniques. Optical absorption and H NMR characteristics of both dyads with those of constituent individuals suggest that there exists a minimum π-π interaction between phenanthroimidazole and BODIPY. Quenched emission of both the dyads was observed when excited either at phenthaoimidazole absorption maxima or at BODIPY absorption maxima in all three investigated solvents. The detailed spectral analysis provided evidence for an intramolecular photoinduced excitation energy transfer (PEnT) from the singlet excited state of phenanthroimidazole to BODIPY and photoinduced electron transfer (PET) from the ground state of phenanthroimidazole to BODIPY. Transient absorption studies suggest that charge-separated species (PhI - BODIPY) are generated at a rate constant of (1.16 ± 0.01) × 10 s for the dyads and (5.15 ± 0.03) × 10 s and for whereas energy transfer rate constants were much higher and were on the order of (1.1 ± 0.02) × 10 s and (1.6 ± 0.02) × 10 s for and , respectively, signifying their usefulness in light energy harvesting applications.
设计、合成了供体 - 受体体系,其中供体菲咯咪唑(PhI)直接与BODIPY受体相连,并通过菲咯咪唑和BODIPY之间的乙炔桥隔开,并用各种光谱和电化学技术对其进行了表征。两种二元化合物与组成它们的单体的光吸收和氢核磁共振特征表明,菲咯咪唑和BODIPY之间存在最小的π - π相互作用。在所有三种研究的溶剂中,当在菲咯咪唑吸收最大值或BODIPY吸收最大值处激发时,都观察到了两种二元化合物的猝灭发射。详细的光谱分析为从菲咯咪唑的单重激发态到BODIPY的分子内光致激发能量转移(PEnT)以及从菲咯咪唑的基态到BODIPY的光致电子转移(PET)提供了证据。瞬态吸收研究表明,对于二元化合物 ,电荷分离物种(PhI - BODIPY)以(1.16 ± 0.01)× 10 s的速率常数生成,对于 则为(5.15 ± 0.03)× 10 s,而能量转移速率常数要高得多,对于 和 分别约为(1.1 ± 0.02)× 10 s和(1.6 ± 0.02)× 10 s,这表明它们在光能收集应用中的有用性。