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Prevailing Charge Order in Overdoped La_{2-x}Sr_{x}CuO_{4} beyond the Superconducting Dome.
Li, Qizhi; Huang, Hsiao-Yu; Ren, Tianshuang; Weschke, Eugen; Ju, Lele; Zou, Changwei; Zhang, Shilong; Qiu, Qingzheng; Liu, Jiarui; Ding, Shuhan; Singh, Amol; Prokhnenko, Oleksandr; Huang, Di-Jing; Esterlis, Ilya; Wang, Yao; Xie, Yanwu; Peng, Yingying.
Afiliação
  • Li Q; International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.
  • Huang HY; National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.
  • Ren T; Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.
  • Weschke E; Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin 14109, Germany.
  • Ju L; Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.
  • Zou C; International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.
  • Zhang S; International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.
  • Qiu Q; International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.
  • Liu J; Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.
  • Ding S; Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.
  • Singh A; National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.
  • Prokhnenko O; Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin 14109, Germany.
  • Huang DJ; National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.
  • Esterlis I; Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA.
  • Wang Y; Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.
  • Xie Y; Department of Chemistry, Emory University, Atlanta, Georgia 30322, USA.
  • Peng Y; Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.
Phys Rev Lett ; 131(11): 116002, 2023 Sep 15.
Article em En | MEDLINE | ID: mdl-37774302
ABSTRACT
The extremely overdoped cuprates are generally considered to be Fermi liquid metals without exotic orders, whereas the underdoped cuprates harbor intertwined states. Contrary to this conventional wisdom, using Cu L_{3}-edge and O K-edge resonant x-ray scattering, we reveal a charge order (CO) correlation in overdoped La_{2-x}Sr_{x}CuO_{4} (0.35≤x≤0.6) beyond the superconducting dome. This CO has a periodicity of ∼6 lattice units with correlation lengths of ∼20 lattice units. It shows similar in-plane momentum and polarization dependence and dispersive excitations as the CO of underdoped cuprates, but its maximum intensity differs along the c direction and persists up to 300 K. This CO correlation cannot be explained by the Fermi surface instability and its origin remains to be understood. Our results suggest that CO is prevailing in the overdoped metallic regime and requires a reassessment of the picture of overdoped cuprates as weakly correlated Fermi liquids.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article