Swathi K, Sujith Meleppatt, Divya P S, P Merin Varghese, Delledonne Andrea, Phan Huu D K Andrea, Di Maiolo Francesco, Terenziani Francesca, Lapini Andrea, Painelli Anna, Sissa Cristina, Thomas K George
Dipartimento di Scienze Chimiche, della Vita e della Sostenibilità Ambientale, Università di Parma Parco Area delle Scienze 17A 43124 Parma Italy
School of Chemistry, Indian Institute of Science Education and Research Thiruvananthapuram (IISER TVM) Vithura Thiruvananthapuram 695 551 India
Chem Sci. 2023 Jan 13;14(8):1986-1996. doi: 10.1039/d2sc05206g. eCollection 2023 Feb 22.
The phenomenon of excited-state symmetry breaking is often observed in multipolar molecular systems, significantly affecting their photophysical and charge separation behavior. As a result of this phenomenon, the electronic excitation is partially localized in one of the molecular branches. However, the intrinsic structural and electronic factors that regulate excited-state symmetry breaking in multibranched systems have hardly been investigated. Herein, we explore these aspects by adopting a joint experimental and theoretical investigation for a class of phenyleneethynylenes, one of the most widely used molecular building blocks for optoelectronic applications. The large Stokes shifts observed for highly symmetric phenyleneethynylenes are explained by the presence of low-lying dark states, as also established by two-photon absorption measurements and TDDFT calculations. In spite of the presence of low-lying dark states, these systems show an intense fluorescence in striking contrast to Kasha's rule. This intriguing behavior is explained in terms of a novel phenomenon, dubbed "symmetry swapping" that describes the inversion of the energy order of excited states, , the swapping of excited states occurring as a consequence of symmetry breaking. Thus, symmetry swapping explains quite naturally the observation of an intense fluorescence emission in molecular systems whose lowest vertical excited state is a dark state. In short, symmetry swapping is observed in highly symmetric molecules having multiple degenerate or quasi-degenerate excited states that are prone to symmetry breaking.
激发态对称性破缺现象在多极分子体系中经常被观察到,这对其光物理和电荷分离行为有显著影响。由于这种现象,电子激发部分定域在分子的一个分支中。然而,调节多分支体系中激发态对称性破缺的内在结构和电子因素几乎未被研究。在此,我们通过对一类亚苯基乙炔进行联合实验和理论研究来探索这些方面,亚苯基乙炔是光电子应用中使用最广泛的分子构建单元之一。高度对称的亚苯基乙炔所观察到的大斯托克斯位移是由低能暗态的存在所解释的,这也通过双光子吸收测量和含时密度泛函理论计算得以证实。尽管存在低能暗态,但这些体系与卡沙规则形成鲜明对比,呈现出强烈的荧光。这种有趣的行为可以用一种被称为“对称性互换”的新现象来解释,该现象描述了激发态能量顺序的反转,即由于对称性破缺而发生的激发态互换。因此,对称性互换很自然地解释了在最低垂直激发态为暗态的分子体系中观察到的强烈荧光发射。简而言之,在具有多个简并或准简并激发态且易于发生对称性破缺的高度对称分子中观察到了对称性互换。