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Robust α-Fe(2)O(3)@TiO(2) Core–Shell Structures With Tunable Buffer Chambers for High-Performance Lithium Storage

α-Fe(2)O(3) has high potential energy storage capacity and can serve as a green and low-cost anode material for lithium-ion batteries. However, α-Fe(2)O(3) suffers large volume expansion and pulverization. Based on DFT calculations, TiO(2) can effectively maintain the integrity of the crystal struct...

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Detalles Bibliográficos
Autores principales: Pian, Chunyuan, Peng, Weichao, Ren, Haoyu, Ma, Chao, Su, Yun, Ti, Ruixia, Chen, Xiuyu, Zhu, Lixia, Liu, Jingjing, Sun, Xinzhi, Wang, Bin, Niu, Bingxuan, Wu, Dapeng
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9021487/
https://www.ncbi.nlm.nih.gov/pubmed/35464221
http://dx.doi.org/10.3389/fchem.2022.866369
Descripción
Sumario:α-Fe(2)O(3) has high potential energy storage capacity and can serve as a green and low-cost anode material for lithium-ion batteries. However, α-Fe(2)O(3) suffers large volume expansion and pulverization. Based on DFT calculations, TiO(2) can effectively maintain the integrity of the crystal structure during the discharge/charge process. Well-defined cubic α-Fe(2)O(3) is coated with a TiO(2) layer using the hydrothermal method with the assistance of oxalic acid surface treatment, and then α-Fe(2)O(3)@TiO(2) with tunable buffer chambers is obtained by altering the hydrochloric acid etching time. With the joint efforts of the buffer chamber and the robust structure of the TiO(2) layer, α-Fe(2)O(3)@TiO(2) alleviates the expansion of α-Fe(2)O(3) during the discharge/charge process. The optimized sample (FT-1h) achieves good cycling performance. The reversible specific capacity remains at 893.7 mA h g(-1), and the Coulombic efficiency still reaches up to 98.47% after 150 cycles at a current density of 100 mA g(−1). Furthermore, the reversible specific capacity can return to 555.5 mA h g(−1) at 100 mA g(−1) after cycling at a high current density. Hence, the buffer chamber and the robust TiO(2) layer can effectively improve the cycling stability and rate performance of α-Fe(2)O(3).