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Achieving a high-performance sodium-ion pouch cell by regulating intergrowth structures in a layered oxide cathode with anionic redox

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Abstract

In P2-type layered transition metal (TM) oxides, which are typical cathode materials for Na-ion batteries, the presence of Li within the TM layer could lead to the formation of specific Na–O–Li configurations that trigger additional oxygen redox at high charging voltages. However, the prismatic-type (P-type) to octahedral-type (O-type) phase transition and irreversible TM migration could be simultaneously aggravated in high state of charge, resulting in structural distortion. Here we demonstrate that excessive desodiation of P2-Na0.67Li0.1Fe0.37Mn0.53O2 (NLFMO) induces the formation of neighbouring O-type stacking faults with an intergrowth structure (that is, interlacing of O- and P-type layers), which leads to out-of-lattice Li migration and irreversible oxygen loss. We show that, by controlling the depth of charge to tailor the intergrowth structure, a P-type stacking state can be uniformly interspersed between the O-type stacking state, thereby avoiding neighbouring O-type stacking faults. Adjusting the O/P intergrowth structure leads to both reversible migration of Li/TM ions and reversible anionic redox in the NLFMO cathode. We thereby achieve a high-performance pouch cell (with an energy density of 165 W h kg−1 based on the entire weight of the cell) with both cationic and anionic redox activities.

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Fig. 1: Structural characterization of NLFMO and ARR demonstration.
Fig. 2: Characterization of P2–OP4–O2 intergrowth structures in NLFMO.
Fig. 3: Analysis of the TM–O covalent environment variation in NLFMO.
Fig. 4: Influence of the behaviour of doped Li on the local structure/environment of NLFMO.
Fig. 5: Evolution of the local oxygen environment.
Fig. 6: Reversible cycling of the NLFMO cathode in full cells.

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All data supporting the findings in this study are available within the paper and the Supplementary Information. Source data are provided with this paper.

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Acknowledgements

This work was partially supported by the National Natural Science Foundation of China (grant nos. 22021001, 22179111, 22109186, 52250402, 52025025 and 22288102), the Ministry of Science and Technology of China (grant no. 2021YFA1201900), the Basic Research Program of Tan Kah Kee Innovation Laboratory (grant no. RD2021070401), the Principal Fund from Xiamen University (grant no. 20720210015), the Fundamental Research Funds for the Central Universities (grant no. 20720220010) and the Beijing Natural Science Foundation (grant no. Z190010). H.L. and J.C. acknowledge support from the US National Science Foundation under grant no. DMR-1809372. This research used resources of the Advanced Photon Source, a US Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under contract no. DE-AC02-06CH11357. H.L. and J.C. were supported by the National Science Foundation under grant no. DMR-1809372. G.-L.X. and K.A. thank the Clean Vehicle Consortium, US–China Clean Energy Research Centre (CERC-CVC2) for support. This research also employed the resources of the Shanghai Synchrotron Radiation Facility BL11B, BL14B1 and BL02B02 beamline stations (SSRF, under contract nos. 2021-SSRF-PT-017208, 2022-SSRF-PT-019758 and 2022-SSRF-PT-021637), the Hefei National Synchrotron Radiation Laboratory (NSRL-USTC, under contract nos. 2021-HLS-PT-004529, 2021-HLS-PT-004156 and 2021-HLS-PT-004241), the Beijing Synchrotron Radiation Laboratory 1W1B, 4B9A, 4B7B, 3W1B and 4B9B beamline stations (under contract nos. 2021-BEPC-PT-005771, 2021-BEPC-PT-005765, 2021-BEPC-PT-005760 and 2022-BEPC-PT-006478) and the China Spallation Neutron Source (CSNS, under contract nos. P1621080200036 and P1621122000008). The authors appreciate the help from D. Wong, C. Schulz and M. Bartkowiak for RIXS characterization (proposal info: 221-11099-ST) at beamline U41-PEAXIS of BESSY II, Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin, Germany. We thank W. He (Chimie du Solide-Energie, Collège de France, France), L. Pan (Hokkaido University, Japan), C. Li (East China Normal University) and J. Serrano Sevillano (CIC energiGUNE, Spain) for help with and discussion on in situ XRD, Mossbäuer characterization, ssNMR and the FAULTS program.

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Contributions

X.W. and Y. Qiao contributed to the design of the research and performed the experimental data analysis. X.W. conducted the materials synthesis, electrochemistry and cell performance. Q.Z. and L.G. conducted the STEM experiments and related data analysis. H.L. and J.C. conducted the soft XAS experiments. C.Z. conducted the hard XAS experiments with the help of C.-J.S. and I.H. X.W. and Y.T. conducted the analysis of XAS results. B.Z., G.Z. and Y.T. helped to conduct the XRD experiment and FAULTS simulation. H.L., Z.H. and Y.X. conducted the ND/nPDF experiments and related data analysis. H.Z. and S.Z. conducted the TiMS/DEMS and HR-TEM experiment, respectively. Q.W. conducted the RIXS experiments and related data analysis. Y.S. conducted the DFT calculations and MD simulations. Y. Qiao conducted the analysis of Fe-MS and ssNMR characterizations. Y.S., Q.W., G.-L.X., L.G. and Y. Qiao supervised the work. All authors discussed the results and co-wrote and commented on the manuscript.

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Correspondence to Yang Sun, Qingsong Wang, Gui-Liang Xu, Lin Gu or Yu Qiao.

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Wang, X., Zhang, Q., Zhao, C. et al. Achieving a high-performance sodium-ion pouch cell by regulating intergrowth structures in a layered oxide cathode with anionic redox. Nat Energy 9, 184–196 (2024). https://doi.org/10.1038/s41560-023-01425-2

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