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Revealing Gliding-Induced Structural Distortion in High-Nickel Layered Oxide Cathodes for Lithium-Ion Batteries.
Yu, Dongyan; Zeng, Guifan; Chen, Diancheng; Yan, Yawen; Zou, Yue; Liu, Qirui; Zhang, Kang; Fang, Kai; Xu, Juping; Yin, Wen; Hong, Yu-Hao; Qiu, Tian; Liao, Hong-Gang; Kuai, Xiaoxiao; Sun, Yang; Qiao, Yu; Sun, Shi-Gang.
Afiliação
  • Yu D; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Zeng G; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Chen D; School of MaterialsSun Yat-sen University, Shenzhen 518107, China.
  • Yan Y; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Zou Y; National Synchrotron Radiation Laboratory, IRFEL Innovation Center for Energy Chemistry, University of Science and Technology of China, Hefei ,Anhui 230026, China.
  • Liu Q; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Zhang K; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Fang K; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Xu J; Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, P.R. China.
  • Yin W; Spallation Neutron Source Science Center, Dongguan 523803, China.
  • Hong YH; Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, P.R. China.
  • Qiu T; Spallation Neutron Source Science Center, Dongguan 523803, China.
  • Liao HG; Fujian Science & Technology Innovation Laboratory for Energy Materials of China (Tan Kah Kee Innovation Laboratory), Xiamen 361005, PR China.
  • Kuai X; Huayou New Energy Technology (Quzhou) Co. LTD, QuZhou, Zhejiang 324000, P.R. China.
  • Sun Y; State Key Laboratory of Physical Chemistry of Solid Surfaces, Collaborative Innovation Center of Chemistry for Energy Materials (iChEM), Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, PR China.
  • Qiao Y; Innovation Research Institute in Advanced Electronic Chemicals of Quzhou, QuZhou,Zhejiang324000, P.R. China.
  • Sun SG; School of MaterialsSun Yat-sen University, Shenzhen 518107, China.
ACS Nano ; 18(40): 27654-27664, 2024 Oct 08.
Article em En | MEDLINE | ID: mdl-39323096
ABSTRACT
After charging to a high state-of-charge (SoC), layered oxide cathodes exhibit high capacities but suffer from gliding-induced structural distortions caused by deep Li depletion within alkali metal (AM) layers, especially for high-nickel candidates. In this study, we identify the essential structure of the detrimental H3 phase formed at high SoC to be an intergrowth structure characterized by random sequences of the O3 and O1 slabs, where the O3 slabs represent Li-rich layers and the O1 slabs denote Li-depleted (or empty) layers that glide from the O3 slabs. Moreover, we adopt two doping strategies targeting different doping sites to eliminate the formation of Li-vacant O1 slabs. First, we introduce direct transition metal (TM) pillars between TMO2 slabs achieved through dopants (e.g., Nb) positioned within AM layers, significantly improving the cycling stability. Second, we introduce indirect Li pillars achieved through dopants located at TM layers to adjust the Li-O bond strength. While this strategy can regulate the uniformity of Li at the slab level, it results in an uneven Li distribution at the particle scale, ultimately failing to enhance the electrochemical performance. Our established research strategy facilitates the realization of diverse pillars between TMO2 slabs through doping, thereby offering guidance for stabilizing high-capacity layered oxide cathodes at high SoC.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article