Abstract
Mn-rich cathodes balance performance and sustainability but suffer from limited cyclability due to Mn dissolution and cathode-to-anode crosstalk. The Jahn-Teller (J-T) effect of Mn3+ is often linked to the above phenomena, such as in spinel LiMn2O4. However, in typical voltage ranges, significant Mn3+ only appears near the end of discharge, highlighting the need to reassess its role in driving Mn dissolution, structural degradation, and battery performance. Here, the spinel cathode's degree of disorder is tailored to expand the Mn redox range, enabling segmentation into J-T active and less active voltage ranges. Cycling at segmented voltage windows reveals surface degradation mechanisms with and without the major J-T effect. Despite a stronger J-T effect below 3.6 V vs. Li/Li+, Mn dissolution is less significant than above 3.6 V. Expanding the cycling window to 2.0–4.3 V causes severe degradation as the J-T active range induces a tetragonal phase and Mn2+-rich surface, driving Mn dissolution and consuming Li-ion inventory in full cells. Reducing electrolyte acidity minimizes Mn3+ disproportionation, enabling a stable dopant-free Mn-only cathode with a 250 mAh g−1 specific capacity. These findings demonstrate that full cells using Mn-rich cathodes have the potential to avoid the notorious crosstalk problem through electrolyte engineering.
| Original language | English |
|---|---|
| Article number | 2501352 |
| Journal | Advanced Materials |
| Volume | 37 |
| Issue number | 34 |
| DOIs | |
| State | Published - Aug 28 2025 |
Funding
The work was supported by the National Science Foundation (DMR-2045570). This work used shared facilities at the Nanoscale Characterization and Fabrication Laboratory (NCFL), which is funded and managed by Virginia Tech's Institute for Critical Technology and Applied Science. Additional support is provided by the Virginia Tech National Center for Earth and Environmental Nanotechnology Infrastructure (NanoEarth), a member of the National Nanotechnology Coordinated Infrastructure (NNCI), supported by NSF (ECCS 1542100 and ECCS 2025151). F.L. acknowledges the NCFL Faculty Fellowship program. D.X. and F.L. thank Dr. Hongyu Wang at NCFL, Virginia Tech for helping with TEM measurements. This research used resources of the Advanced Photon Source and Center for Nanoscale Materials, an Office of Science User Facility operated for the U.S. Department of Energy (DOE) Office of Science by Argonne National Laboratory, and was supported by the U.S. DOE under Contract No. DE-AC02-06CH11357. The use of the Stanford Synchrotron Radiation Lightsource (SSRL), SLAC National Accelerator Laboratory, was supported by the US DOE, Office of Science, Office of Basic Energy Sciences, under contract no. DE-AC02-76SF00515. A portion of this research used resources at the High Flux Isotope Reactor, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The beam time was allocated to HB-2C WAND2 on proposal number IPTS-32663.1. The work was supported by the National Science Foundation (DMR‐2045570). This work used shared facilities at the Nanoscale Characterization and Fabrication Laboratory (NCFL), which is funded and managed by Virginia Tech's Institute for Critical Technology and Applied Science. Additional support is provided by the Virginia Tech National Center for Earth and Environmental Nanotechnology Infrastructure (NanoEarth), a member of the National Nanotechnology Coordinated Infrastructure (NNCI), supported by NSF (ECCS 1542100 and ECCS 2025151). F.L. acknowledges the NCFL Faculty Fellowship program. D.X. and F.L. thank Dr. Hongyu Wang at NCFL, Virginia Tech for helping with TEM measurements. This research used resources of the Advanced Photon Source and Center for Nanoscale Materials, an Office of Science User Facility operated for the U.S. Department of Energy (DOE) Office of Science by Argonne National Laboratory, and was supported by the U.S. DOE under Contract No. DE‐AC02‐06CH11357. The use of the Stanford Synchrotron Radiation Lightsource (SSRL), SLAC National Accelerator Laboratory, was supported by the US DOE, Office of Science, Office of Basic Energy Sciences, under contract no. DE‐AC02‐76SF00515. A portion of this research used resources at the High Flux Isotope Reactor, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The beam time was allocated to HB‐2C WAND on proposal number IPTS‐32663.1.
Keywords
- Mn dissolution
- Mn-based electrodes
- cation disorder
- high-energy Li-ion batteries
- spinel cathode