A formal FeIII/V redox couple in an intercalation electrode

  • Hari Ramachandran
  • , Edward W. Mu
  • , Eder G. Lomeli
  • , Augustin Braun
  • , Masato Goto
  • , Kuan H. Hsu
  • , Jue Liu
  • , Zhelong Jiang
  • , Kipil Lim
  • , Grace M. Busse
  • , Brian Moritz
  • , Joshua J. Kas
  • , John Vinson
  • , John J. Rehr
  • , Jungjin Park
  • , Iwnetim I. Abate
  • , Yuichi Shimakawa
  • , Edward I. Solomon
  • , Wanli Yang
  • , William E. Gent
  • Thomas P. Devereaux, William C. Chueh

Research output: Contribution to journalArticlepeer-review

Abstract

Iron redox cycling between low-valent oxidation states of FeII and FeIII drives crucial processes in nature. The FeII/III redox couple charge compensates the cycling of lithium iron phosphate, a positive electrode (cathode) for lithium-ion batteries. High-valent iron redox couples, involving formal oxidation higher than FeIII, could deliver higher electrochemical potentials and energy densities. However, because of the instability of high-valent Fe electrodes, they have proven difficult to probe and exploit in intercalation systems. Here we report and characterize a formal FeIII/V redox couple by revisiting the charge compensation mechanism of (de)lithiation in Li4FeSbO6. Valence-sensitive experimental and computational core-level spectroscopy reveal a direct transition from FeIII (3d5) to a negative-charge-transfer FeV (3d5L2) ground state on delithiation, without forming FeIV, or oxygen dimers. We identify that the cation ordering in Li4FeSbO6 drives a templated phase transition to stabilize the unique FeV species and demonstrate that disrupting cation ordering suppresses the FeIII/V redox couple. Exhibiting resistance to calendar aging, high operating potential and low voltage hysteresis, the FeIII/V redox couple in Li4FeSbO6 provides a framework for developing sustainable, Fe-based intercalation cathodes for high-voltage applications.

Original languageEnglish
Pages (from-to)91-99
Number of pages9
JournalNature Materials
Volume25
Issue number1
DOIs
StatePublished - Jan 2026

Funding

Certain commercial equipment, instruments or materials are identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by the National Institute of Standards and Technology, nor does it imply that the materials or equipment identified are necessarily the best available for the purpose. This work was partially supported by the US Department of Energy (DOE), Office of Basic Energy Sciences, Division of Materials Sciences and Engineering (contract DE-AC02-76SF00515). H.R. was supported by the Stanford Knight-Hennessy Scholarship program. E.W.M. was supported by a National Science Foundation Graduate Research Fellowship under grant number 1656518. A part of the work by M.G. and Y.S. was supported by Grants-in-Aid for Scientific Research (numbers 20H00397, 23H05457 and 23K13814) from MEXT and by AdCORP (JPMJKB2304) and ASPIRE (JPMJAP2314) programs from JST, Japan. This research used resources of the Advanced Light Source, which is a DOE, Office of Science User Facility, under contract number DE-AC02-05CH11231. Use of the SSRL, SLAC National Accelerator Laboratory, is supported by the US DOE, Office of Science, Office of Basic Energy Sciences, under contract number DE-AC02-76SF00515. This research also used resources of the Advanced Photon Source, a US DOE, Office of Science User Facility, operated for the DOE, Office of Science, by the Argonne National Laboratory under contract number DE-AC02-06CH11357. Part of this work was performed at the Stanford Nano Shared Facilities (SNSF), supported by the National Science Foundation under award number ECCS-2026822. Neutron diffraction and neutron pair distribution function were conducted at the NOMAD beamline at ORNL’s Spallation Neutron Source, which was sponsored by the US DOE, Scientific User Facilities Division, Office of Basic Sciences. Computational work was performed on the Sherlock cluster at Stanford University and on resources of the National Energy Research Scientific Computing Center (NERSC), a DOE, Office of Science User Facility, using NERSC award number BES-ERCAP0027203. We thank G. Lee for experimental XAS/RIXS support at Advanced Light Source beamline 8.0.1.1; A. Yao for help in developing the electrode slurry coating method; J. Lee for assistance with the XRD capillary sample preparation and pouch cell preparation; S. Narasimhan, N. Liang and E. Kaeli for help in optimizing the pouch cell electrochemistry; M. Preefer and K. Stone for assistance with experiments at SSRL BL 11-3; N. Strange, K. Stone, Y. Wu, C. Troxel, Jr., and Z. Liang for assistance with experiments at SSRL BL 2-1; and A. Marks, A. Geslin, D. Rivera, D. Eum, D. Edelman, E. Choy, K. Harmon, N. Siemons, N. Liang, S. Wang, W. Thompson, X. Cui, F. Zhang, D. R. Black and J. L. Weaver for proofreading and suggestions on the paper.

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