CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES |
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Weak Electron-Phonon Coupling and Unusual Electron Scattering of Topological Surface States in Sb(111) by Laser-Based Angle-Resolved Photoemission Spectroscopy |
XIE Zhuo-Jin1, HE Shao-Long1**, CHEN Chao-Yu1, FENG Ya1, YI He-Mian1, LIANG Ai-Ji1, ZHAO Lin1, MOU Dai-Xiang1, HE Jun-Feng1, PENG Ying-Ying1, LIU Xu1, LIU Yan1, LIU Guo-Dong1, DONG Xiao-Li1, YU Li1, ZHANG Jun1, ZHANG Shen-Jin3, WANG Zhi-Min3, ZHANG Feng-Feng3, YANG Feng3, PENG Qin-Jun3, WANG Xiao-Yang3, CHEN Chuang-Tian3, XU Zu-Yan3, ZHOU Xing-Jiang1,2** |
1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190 2Collaborative Innovation Center of Quantum Matter, Beijing 100871 3Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190
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Cite this article: |
XIE Zhuo-Jin, HE Shao-Long, CHEN Chao-Yu et al 2014 Chin. Phys. Lett. 31 067305 |
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Abstract High-resolution laser-based angle-resolved photoemission (ARPES) measurements are carried out on Sb(111) single crystal. Two kinds of Fermi surface sheets are observed, which are derived from the topological surface states: one small hexagonal electron-like Fermi pocket around Γ point and the other six elongated lobes of hole-like Fermi pockets around the electron pocket. Clear Rashba-type band splitting due to the strong spin-orbit coupling is observed to be anisotropic in the momentum space. Our super-high-resolution ARPES measurements reveal no obvious kink in the surface band dispersions, indicating a weak electron-phonon interaction in the surface states. In particular, the electron scattering rate for these topological surface states is nearly a constant over a large energy window near the Fermi level that is unusual in terms of the conventional picture.
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Published: 26 May 2014
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PACS: |
73.20.-r
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(Electron states at surfaces and interfaces)
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79.60.-i
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(Photoemission and photoelectron spectra)
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71.20.-b
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(Electron density of states and band structure of crystalline solids)
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Abstract
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