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A medium-entropy transition metal oxide cathode for high-capacity lithium metal batteries

The limited capacity of the positive electrode active material in non-aqueous rechargeable lithium-based batteries acts as a stumbling block for developing high-energy storage devices. Although lithium transition metal oxides are high-capacity electrochemical active materials, the structural instabi...

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Detalles Bibliográficos
Autores principales: Pei, Yi, Chen, Qing, Wang, Meiyu, Zhang, Pengjun, Ren, Qingyong, Qin, Jingkai, Xiao, Penghao, Song, Li, Chen, Yu, Yin, Wen, Tong, Xin, Zhen, Liang, Wang, Peng, Xu, Cheng-Yan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9579144/
https://www.ncbi.nlm.nih.gov/pubmed/36257951
http://dx.doi.org/10.1038/s41467-022-33927-0
Descripción
Sumario:The limited capacity of the positive electrode active material in non-aqueous rechargeable lithium-based batteries acts as a stumbling block for developing high-energy storage devices. Although lithium transition metal oxides are high-capacity electrochemical active materials, the structural instability at high cell voltages (e.g., >4.3 V) detrimentally affects the battery performance. Here, to circumvent this issue, we propose a Li(1.46)Ni(0.32)Mn(1.2)O(4-x) (0 < x < 4) material capable of forming a medium-entropy state spinel phase with partial cation disordering after initial delithiation. Via physicochemical measurements and theoretical calculations, we demonstrate the structural disorder in delithiated Li(1.46)Ni(0.32)Mn(1.2)O(4-x), the direct shuttling of Li ions from octahedral sites to the spinel structure and the charge-compensation Mn(3+)/Mn(4+) cationic redox mechanism after the initial delithiation. When tested in a coin cell configuration in combination with a Li metal anode and a LiPF(6)-based non-aqueous electrolyte, the Li(1.46)Ni(0.32)Mn(1.2)O(4-x)-based positive electrode enables a discharge capacity of 314.1 mA h g(−1) at 100 mA g(−1) with an average cell discharge voltage of about 3.2 V at 25 ± 5 °C, which results in a calculated initial specific energy of 999.3 Wh kg(−1) (based on mass of positive electrode’s active material).