Abstract
Understanding and mitigating filament formation, short-circuit and solid electrolyte fracture is necessary for advanced all-solid-state batteries. Here, we employ a coupled far-field high-energy diffraction microscopy and tomography approach for assessing the chemo-mechanical behaviour for dense, polycrystalline garnet (Li7La3Zr2O12) solid electrolytes with grain-level resolution. In situ monitoring of grain-level stress responses reveals that the failure mechanism is stochastic and affected by local microstructural heterogeneity. Coupling high-energy X-ray diffraction and far-field high-energy diffraction microscopy measurements reveals the presence of phase heterogeneity that can alter local chemo-mechanics within the bulk solid electrolyte. These local regions are proposed to be regions with the presence of a cubic polymorph of LLZO, potentially arising from local dopant concentration variation. The coupled tomography and FF-HEDM experiments are combined with transport and mechanics modelling to illustrate the degradation of polycrystalline garnet solid electrolytes. The results showcase the pathways for processing high-performing solid-state batteries.
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Data availability
Data presented in this study are available from the corresponding authors upon request.
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Acknowledgements
This work was supported by the National Science Foundation under grant nos. 2140376, 2140472, and 1847029. We acknowledge the Vanderbilt Institute of Nanoscience and Engineering (VINSE) for access to their shared characterization facilities. P.P.M. acknowledges support in part from the National Science Foundation (award no. 2041499). 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. This research was carried out in part at the Oak Ridge National Laboratory, managed by UT–Battelle, for the US DOE under contract DE-AC05-00OR22725. M.B.D. was also supported in part by Alvin M. Weinberg Fellowship at the Oak Ridge National Laboratory. Notice: This manuscript has been authored by UT–Battelle under contract no. DE-AC0500OR22725 with the US DOE. The United States Government retains and the publisher, by accepting the article for publication, acknowledges that the United States Government retains a non-exclusive, paid-up, irrevocable, world-wide license to publish or reproduce the published form of this manuscript, or allow others to do so, for the United States Government purposes. The US DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan (https://www.energy.gov/downloads/doe-public-access-plan).
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M.B.D. and K.B.H. conceived the concept and idea. M.B.D. and W.Z. performed the synchrotron imaging and diffraction experiments. J-S.P., J.A. and P.K. performed the synchrotron measurements and helped with the analysis. M.B.D. completed the image processing and analysis from the synchrotron experiments. B.S.V. and P.P.M. carried out the modelling efforts. M.D. and K.B.H. wrote the manuscript. The manuscript was edited by all the authors.
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Extended data
Extended Data Fig. 1 Evaluating the presence of trace phases in sintered LLZO pellets.
(a) High resolution, X-Ray diffraction patterns from specified locations of an LLZO pellet. (b) Spatially resolved high resolution XRD map of the LLZO pellet. (c) Spatially resolved XRD map zoomed to the anticipated location of the low-structure factor peak corresponding to < 141 > plane in the 230 space group LLZO.
Extended Data Fig. 2 Correlating grain-level mechanics to the bulk microstructure.
(a) Difference in the pore structure of a hot-spot neighbourhood between the pristine and the failed sample. The structure represents the modification of pore network between pristine and the failed sample. The scale bar in the figure is 100 μm (b) Depth averaged Δporosity values for identical sub-volume sizes taken at a hot spot region (right) and other (unstrained) regions of the bulk pellet. The porosity difference is calculated between the pristine and the failed sample. The scale bar in the figure is 10 μm. (c) Difference in porosity values tracked over the hot-spot and cold-spots for each step plotted as a box plot. Additionally, the average porosity difference over the entire pellet between each step is overlayed and connected by a solid line. As the sample undergoes degradation with cycling, the hot-/cold- neighbourhoods clearly show very high variance in the porosity change compared to the bulk sample value.
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Supplementary Figs. 1–28 and details on data analysis.
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Dixit, M.B., Vishugopi, B.S., Zaman, W. et al. Polymorphism of garnet solid electrolytes and its implications for grain-level chemo-mechanics. Nat. Mater. 21, 1298–1305 (2022). https://doi.org/10.1038/s41563-022-01333-y
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DOI: https://doi.org/10.1038/s41563-022-01333-y
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