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Research Article

Switching Optimally Balanced Fe–N Interaction Enables Extremely Stable Energy Storage

Zhenzhen Zhao1, Wei Zhang1 ( ), Miao Liu1, Dong Wang2, Xiyang Wang3, Lirong Zheng4, Xu Zou1, Zizhun Wang1, Dabing Li5, Keke Huang6, Weitao Zheng1( )
Key Laboratory of Mobile Materials MOE, and School of Materials Science & Engineering, and Electron Microscopy Center, and International Center of Future Science, Jilin University, Changchun 130012, China
State Key Laboratory of Chem/Bio-Sensing and Chemometrics, Provincial Hunan Key Laboratory for Graphene Materials and Devices, College of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, China
Department of Mechanical and Mechatronics Engineering, University of Waterloo, Waterloo Canada
Beijing Synchrotron Radiation Facility, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
State Key Laboratory of Inorganic Synthesis and Preparative Chemistry, College of Chemistry, Jilin University, Changchun 130012, China
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Abstract

The interaction between electrode materials and charge carriers is one of the central issues dominating underlying energy storage mechanisms. To address the notoriously significant volume changes accompanying intercalation or formation of alloy/compounds, we aim to introduce and utilize a weak, reversible Fe–N interaction during the (de)intercalation of ammonium ions (NH4+) within iron(Ⅲ) hexacyanoferrate (FeHCF), inspired by manipulating the electrostatic adsorption between N and Fe in the early stages of ammonia synthesis (Bosch-Harber Process, Chemical Engineering) and steel nitriding processes (Metal Industry). Such strategy of switching well-balanced Fe–N interaction is confirmed in between the nitrogen of ammonium ions and high-spin Fe in FeHCF, as observed by using X-ray absorption spectroscopy. The resulting material provided an extremely stable energy storage (58 mAh g−1 after 10000 cycles at current density of 1 A g−1) as well as high-rate performance (23.6 mAh g−1 at current density of 10 A g−1).

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Cite this article:
Zhao Z, Zhang W, Liu M, et al. Switching Optimally Balanced Fe–N Interaction Enables Extremely Stable Energy Storage. Energy & Environmental Materials, 2023, 6(2). https://doi.org/10.1002/eem2.12342

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Received: 25 October 2021
Revised: 21 December 2021
Published: 24 December 2021
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