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Ubiquitous coexisting electron-mode couplings in high-temperature cuprate superconductors.
Yan, Hongtao; Bok, Jin Mo; He, Junfeng; Zhang, Wentao; Gao, Qiang; Luo, Xiangyu; Cai, Yongqing; Peng, Yingying; Meng, Jianqiao; Li, Cong; Chen, Hao; Song, Chunyao; Yin, Chaohui; Miao, Taimin; Chen, Yiwen; Gu, Genda; Lin, Chengtian; Zhang, Fengfeng; Yang, Feng; Zhang, Shenjin; Peng, Qinjun; Liu, Guodong; Zhao, Lin; Choi, Han-Yong; Xu, Zuyan; Zhou, X J.
Afiliação
  • Yan H; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Bok JM; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • He J; Department of Physics, Pohang University of Science and Technology, Pohang 37673, Korea.
  • Zhang W; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Gao Q; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Luo X; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Cai Y; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Peng Y; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Meng J; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Li C; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Chen H; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Song C; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Yin C; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Miao T; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Chen Y; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Gu G; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Lin C; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhang F; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Yang F; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhang S; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Peng Q; National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Liu G; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Zhao L; Condensed Matter Physics, Materials Science Division of Brookhaven National Laboratory, Upton, NY 11973-5000.
  • Choi HY; Max Planck Institute for Solid State Research, D-70569 Stuttgart, Germany.
  • Xu Z; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
  • Zhou XJ; Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China.
Proc Natl Acad Sci U S A ; 120(43): e2219491120, 2023 Oct 24.
Article em En | MEDLINE | ID: mdl-37851678
ABSTRACT
In conventional superconductors, electron-phonon coupling plays a dominant role in generating superconductivity. In high-temperature cuprate superconductors, the existence of electron coupling with phonons and other boson modes and its role in producing high-temperature superconductivity remain unclear. The evidence of electron-boson coupling mainly comes from angle-resolved photoemission (ARPES) observations of [Formula see text]70-meV nodal dispersion kink and [Formula see text]40-meV antinodal kink. However, the reported results are sporadic and the nature of the involved bosons is still under debate. Here we report findings of ubiquitous two coexisting electron-mode couplings in cuprate superconductors. By taking ultrahigh-resolution laser-based ARPES measurements, we found that the electrons are coupled simultaneously with two sharp modes at [Formula see text]70meV and [Formula see text]40meV in different superconductors with different dopings, over the entire momentum space and at different temperatures above and below the superconducting transition temperature. These observations favor phonons as the origin of the modes coupled with electrons and the observed electron-mode couplings are unusual because the associated energy scales do not exhibit an obvious energy shift across the superconducting transition. We further find that the well-known "peak-dip-hump" structure, which has long been considered a hallmark of superconductivity, is also omnipresent and consists of "peak-double dip-double hump" finer structures that originate from electron coupling with two sharp modes. These results provide a unified picture for the [Formula see text]70-meV and [Formula see text]40-meV energy scales and their evolutions with momentum, doping and temperature. They provide key information to understand the origin of these energy scales and their role in generating anomalous normal state and high-temperature superconductivity.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article País de afiliação: China

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article País de afiliação: China