13–17 Sept 2021 Virtual Conference
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Co3+/La3+ cross-diffusion at the Li7La3Zr2O12 | LiCoO2 interface

15 Sept 2021, 15:50
20m
Room 13

Room 13

Oral Presentation E3. Anion and cation transport in materials for energy storage E3_Anion and cation transport in materials for energy storage

Speaker

Lukas Ladenstein (Graz University of Technology)

Description

Cubic Li7La3Zr2O12 (LLZO) garnets have attracted lots of attention in previous years as they show promising properties for Solid-state Li batteries (SSLB) as solid electrolyte including a high electrochemical stability of up to 6 V and a high ionic conductivity in the range of 1 mS cm-1.1 Despite of these favorable prerequisites, its current use in such devices is limited as high temperature treatment is required to form a good contact between LLZO and, e.g., LiCoO2 leading to a high interface resistance by the formation of interdiffusion layers.2
In this study, we present that Co does not only lead to Co diffusion into the LLZO lattice but further induces the formation of resistive interlayers, such as La2CoO4. Since Co is a transition metal, its incorporation could change, e.g., the band gap and, thus, the electrochemical stability window or ionic conduction.
Herein, we simulated the properties of the LLZO|LiCoO2 interface by incorporating Co from LiCoO2 powder into transparent Czochralski-grown Li6.4Ga0.2La3Zr2O12 single crystals over the gas phase at high temperatures. We noticed a color change of the crystals from yellow, orange to dark blue depending on the heating history. To investigate the role of incorporated Co in LLZO garnets, we applied a wide spectrum of techniques, such as UV-VIS, TOF-SIMS, SC-XRD, 57Emission Mößbauer spectroscopy or impedance spectroscopy.
For example, we found that the optical band gap decreases to 1.5 eV by the incorporation of 0.92 Co per formula unit. By conducting impedance analysis a significant change in the Li ion transport was revealed resulting in an increase of the activation energy Ea of 0.54 eV and a decreased room temperature ionic conductivity σ = 7.60 x 10-7 S cm-1 for dark blue LLZO compared to Ea = 0.30 eV and σ = 1.20 x 10-4 S cm-1 for pristine LLZO, respectively.

Speaker Country Austria

Author

Lukas Ladenstein (Graz University of Technology)

Co-authors

Mr Joseph Ring (2Vienna University of Technology, Institute of Chemical Technologies and Analytics, 1060 Wien, Austria) Mr Stefan Smetaczek (2Vienna University of Technology, Institute of Chemical Technologies and Analytics, 1060 Wien, Austria) Dr Markus Kubicek (2Vienna University of Technology, Institute of Chemical Technologies and Analytics, 1060 Wien, Austria) Dr Steffen Ganschow (Leibniz Institute for Crystal Growth (IKZ), 12489 Berlin, Germany) Dr Günther Redhammer (University of Salzburg, Department of Chemistry and Physics of Materials, 5020 Salzburg, Austria.) Dr Daniel Knez (Institute of Electron Microscopy andNanoanalysis and Graz Centre for Electron Microscopy, GrazUniversity of Technology, Graz 8010, Austria) Dr Gerald Kothleitner (Institute of Electron Microscopy andNanoanalysis and Graz Centre for Electron Microscopy, GrazUniversity of Technology, Graz 8010, Austria) Dr Iulian Dugulan (Fundamental Aspects Mat&Energy Group, Delft University of Technology, Mekelweg 15, 2629, JB Delft, the Netherlands) Dr Donald Siegel (Department of Physics, Mechanical Engineering Department, Materials Science and Engineering, Applied Physics Program, and University of Michigan Energy Institute, University of Michigan, Ann Arbor, MI 48109, USA) Dr Andreas Limbeck (Vienna University of Technology, Institute of Chemical Technologies and Analytics, 1060 Wien, Austria) Dr Jürgen Fleig (Vienna University of Technology, Institute of Chemical Technologies and Analytics, 1060 Wien, Austria) Dr Daniel Rettenwander (Graz University of Technology, Institute of Chemistry and Technology of Materials (NAWI Graz), Austria)

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