Lou Cancan, Guan Yurou, Cui Xingxia, Li Yafei, Zhou Xieyu, Yuan Qing, Mei Guangqiang, Jiao Chengxiang, Huang Kai, Hou Xuefeng, Cao Limin, Ji Wei, Novko Dino, Petek Hrvoje, Feng Min
School of Physics and Technology and Key Laboratory of Artificial Micro- and Nano-Structures of Ministry of Education, Wuhan University, Wuhan 430072, China.
Beijing Key Laboratory of Optoelectronic Functional Materials & Micro-Nano Devices, School of Physics, Renmin University of China, Beijing 100872, China.
Sci Adv. 2024 Oct 25;10(43):eado3470. doi: 10.1126/sciadv.ado3470. Epub 2024 Oct 23.
Scanning tunneling microscopy (STM) vibronic spectroscopy, which has provided submolecular insights into electron-vibration (vibronic) coupling, faces challenges when probing the pivotal low-frequency vibronic excitations. Because of eigenstate broadening on solid substrates, resolving low-frequency vibronic states demands strong decoupling. This work designs a type II band alignment in STM junction to achieve effective charge-transfer state decoupling. This strategy enables the successful identification of the lowest-frequency H(ω) (Raman-active H mode) vibronic excitation within single C molecules, which, despite being notably pronounced in electron transport of C single-molecule transistors, has remained hidden at submolecular level. Our results show that the observed H(ω) excitation is "anchored" to all molecules, irrespective of local geometry, challenging common understanding of structural definition of vibronic excitation governed by Franck-Condon principle. Density functional theory calculations reveal existence of molecule-substrate interfacial charge-transfer dipole, which, although overlooked previously, drives the dominant H(ω) excitation. This charge-transfer dipole is not specific but must be general at interfaces, influencing vibronic coupling in charge transport.
扫描隧道显微镜(STM)振动光谱学已在亚分子层面深入研究了电子 - 振动(振子)耦合,但在探测关键的低频振子激发时面临挑战。由于固体衬底上本征态的展宽,解析低频振子态需要强解耦。这项工作设计了一种STM结中的II型能带排列,以实现有效的电荷转移态解耦。该策略成功识别出单个C分子内最低频率的H(ω)(拉曼活性H模式)振子激发,尽管它在C单分子晶体管的电子输运中显著存在,但在亚分子层面一直未被发现。我们的结果表明,观察到的H(ω)激发与所有分子“相关”,与局部几何结构无关,这挑战了由弗兰克 - 康登原理主导的振子激发结构定义的普遍认知。密度泛函理论计算揭示了分子 - 衬底界面电荷转移偶极子的存在,尽管此前被忽视,但它驱动了主要的H(ω)激发。这种电荷转移偶极子并非特定存在,而是在界面普遍存在,影响电荷输运中的振子耦合。