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Facile thermochemical conversion of FeOOH nanorods to ZnFe(2)O(4) nanorods for high-rate lithium storage

We successfully prepared ZnFe(2)O(4) nanorods (ZFO-NRs) by a simple thermochemical reaction of FeOOH nanorods with Zn(NO(3))(2) to use as an anode material in lithium-ion batteries. The FeOOH nanorod shape was well maintained after conversion into ZFO-NR with the formation of porous structures. The...

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Detalles Bibliográficos
Autores principales: Park, Yiseul, Oh, Misol, Lee, Yebin, Park, Hyunwoong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9066156/
https://www.ncbi.nlm.nih.gov/pubmed/35521298
http://dx.doi.org/10.1039/c9ra03600h
Descripción
Sumario:We successfully prepared ZnFe(2)O(4) nanorods (ZFO-NRs) by a simple thermochemical reaction of FeOOH nanorods with Zn(NO(3))(2) to use as an anode material in lithium-ion batteries. The FeOOH nanorod shape was well maintained after conversion into ZFO-NR with the formation of porous structures. The nanorod structure and porous morphology facilitate Li(+) transport, improve the reaction rates owing to the larger contact area with the electrolyte, and reduce the mechanical stress during lithiation/delithiation. The ZFO-NR electrode exhibited a reversible capacity of 725 mA h g(−1) at 1 A g(−1) and maintained a capacity of 668 mA h g(−1) at 2 A g(−1); these capacities are much higher and more stable than those of ZFO nanoparticles prepared by a hydrothermal method (ZFO-HT) (216 and 117 mA h g(−1) at 1 and 2 A g(−1), respectively). Although ZFO-NRs exhibited high, stable capacities at moderate current densities for charging and discharging, the capacity rapidly decreased under fast charging/discharging conditions (>4 A g(−1)). However, carbonized ZFO-NR (C/ZFO-NR) exhibited an improved reversible capacity and rate capability resulting from an increased conductivity compared with ZFO-NRs. The specific capacity of C/ZFO-NRs at 1 A g(−1) was 765 mA h g(−1); notably, a capacity of 680 mA h g(−1) was maintained at 6 A g(−1).