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Superconductivity in pressurized trilayer La4Ni3O10-δ single crystals.
Zhu, Yinghao; Peng, Di; Zhang, Enkang; Pan, Bingying; Chen, Xu; Chen, Lixing; Ren, Huifen; Liu, Feiyang; Hao, Yiqing; Li, Nana; Xing, Zhenfang; Lan, Fujun; Han, Jiyuan; Wang, Junjie; Jia, Donghan; Wo, Hongliang; Gu, Yiqing; Gu, Yimeng; Ji, Li; Wang, Wenbin; Gou, Huiyang; Shen, Yao; Ying, Tianping; Chen, Xiaolong; Yang, Wenge; Cao, Huibo; Zheng, Changlin; Zeng, Qiaoshi; Guo, Jian-Gang; Zhao, Jun.
Afiliación
  • Zhu Y; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Peng D; Shanghai Research Center for Quantum Sciences, Shanghai, China.
  • Zhang E; Shanghai Key Laboratory of Material Frontiers Research in Extreme Environments (MFree), Institute for Shanghai Advanced Research in Physical Sciences (SHARPS), Shanghai, China.
  • Pan B; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Chen X; College of Physics and Optoelectronic Engineering, Ocean University of China, Qingdao, China.
  • Chen L; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Ren H; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Liu F; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Hao Y; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Li N; Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Xing Z; Center for High Pressure Science and Technology Advanced Research, Shanghai, China.
  • Lan F; Center for High Pressure Science and Technology Advanced Research, Shanghai, China.
  • Han J; Center for High Pressure Science and Technology Advanced Research, Shanghai, China.
  • Wang J; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Jia D; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Wo H; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Gu Y; Center for High Pressure Science and Technology Advanced Research, Beijing, China.
  • Gu Y; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Ji L; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Wang W; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Gou H; State Key Laboratory of ASIC and System, School of Microelectronics, Fudan University, Shanghai, China.
  • Shen Y; Institute of Nanoelectronics and Quantum Computing, Fudan University, Shanghai, China.
  • Ying T; Center for High Pressure Science and Technology Advanced Research, Beijing, China.
  • Chen X; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Yang W; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Cao H; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Zheng C; Center for High Pressure Science and Technology Advanced Research, Shanghai, China.
  • Zeng Q; Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Guo JG; State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, China.
  • Zhao J; Shanghai Key Laboratory of Material Frontiers Research in Extreme Environments (MFree), Institute for Shanghai Advanced Research in Physical Sciences (SHARPS), Shanghai, China. zengqs@hpstar.ac.cn.
Nature ; 631(8021): 531-536, 2024 Jul.
Article en En | MEDLINE | ID: mdl-39020034
ABSTRACT
The pursuit of discovering new high-temperature superconductors that diverge from the copper-based model1-3 has profound implications for explaining mechanisms behind superconductivity and may also enable new applications4-8. Here our investigation shows that the application of pressure effectively suppresses the spin-charge order in trilayer nickelate La4Ni3O10-δ single crystals, leading to the emergence of superconductivity with a maximum critical temperature (Tc) of around 30 K at 69.0 GPa. The d.c. susceptibility measurements confirm a substantial diamagnetic response below Tc, indicating the presence of bulk superconductivity with a volume fraction exceeding 80%. In the normal state, we observe a strange metal behaviour, characterized by a linear temperature-dependent resistance extending up to 300 K. Furthermore, the layer-dependent superconductivity observed hints at a unique interlayer coupling mechanism specific to nickelates, setting them apart from cuprates in this regard. Our findings provide crucial insights into the fundamental mechanisms underpinning superconductivity, while also introducing a new material platform to explore the intricate interplay between the spin-charge order, flat band structures, interlayer coupling, strange metal behaviour and high-temperature superconductivity.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Nature Año: 2024 Tipo del documento: Article País de afiliación: China

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Nature Año: 2024 Tipo del documento: Article País de afiliación: China