Zhang Hongyun, Bao Changhua, Schüler Michael, Zhou Shaohua, Li Qian, Luo Laipeng, Yao Wei, Wang Zhong, Devereaux Thomas P, Zhou Shuyun
State Key Laboratory of Low-Dimensional Quantum Physics and Department of Physics, Tsinghua University, Beijing 100084, China.
Stanford Institute for Materials and Energy Sciences (SIMES), SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA.
Natl Sci Rev. 2021 Sep 16;9(5):nwab175. doi: 10.1093/nsr/nwab175. eCollection 2022 May.
Electron-phonon interaction and related self-energy are fundamental to both the equilibrium properties and non-equilibrium relaxation dynamics of solids. Although electron-phonon interaction has been suggested by various time-resolved measurements to be important for the relaxation dynamics of graphene, the lack of energy- and momentum-resolved self-energy dynamics prohibits direct identification of the role of specific phonon modes in the relaxation dynamics. Here, by performing time- and angle-resolved photoemission spectroscopy measurements on Kekulé-ordered graphene with folded Dirac cones at the Γ point, we have succeeded in resolving the self-energy effect induced by the coupling of electrons to two phonons at Ω = 177 meV and Ω = 54 meV, and revealing its dynamical change in the time domain. Moreover, these strongly coupled phonons define energy thresholds, which separate the hierarchical relaxation dynamics from ultrafast, fast to slow, thereby providing direct experimental evidence for the dominant role of mode-specific phonons in the relaxation dynamics.
电子 - 声子相互作用及相关的自能对于固体的平衡性质和非平衡弛豫动力学都至关重要。尽管各种时间分辨测量表明电子 - 声子相互作用对于石墨烯的弛豫动力学很重要,但缺乏能量和动量分辨的自能动力学使得无法直接确定特定声子模式在弛豫动力学中的作用。在这里,通过对在Γ点具有折叠狄拉克锥的凯库勒有序石墨烯进行时间和角度分辨光电子能谱测量,我们成功地解析了电子与能量为Ω = 177 meV和Ω = 54 meV的两种声子耦合所引起的自能效应,并揭示了其在时域中的动态变化。此外,这些强耦合声子定义了能量阈值,将分层弛豫动力学从超快、快速到慢速区分开来,从而为特定模式声子在弛豫动力学中的主导作用提供了直接的实验证据。