% IMPORTANT: The following is UTF-8 encoded. This means that in the presence % of non-ASCII characters, it will not work with BibTeX 0.99 or older. % Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or % “biber”. @PHDTHESIS{Sandt:993520, author = {Sandt, Roland}, othercontributors = {Spatschek, Robert and Svendsen, Bob}, title = {{M}echanics and microstructure modeling of the solid electrolyte $\mathrm{{L}i_7{L}a_3{Z}r_2{O}_{12}}$.}, school = {Rheinisch-Westfälische Technische Hochschule Aachen}, type = {Dissertation}, address = {Aachen}, publisher = {RWTH Aachen University}, reportid = {RWTH-2024-08796}, pages = {1 Online-Ressource : Illustrationen}, year = {2024}, note = {Veröffentlicht auf dem Publikationsserver der RWTH Aachen University; Dissertation, Rheinisch-Westfälische Technische Hochschule Aachen, 2024, Kumulative Dissertation}, abstract = {The efficient electrical energy storage is an important challenge of research, where many crucial topics like the usage of electrical vehicles are strongly related in the overall context of the proceeding climate change. Solid state batteries are suitable candidates for next-generation battery systems, and especially the solid state electrolyte $\mathrm{Li_7La_3Zr_2O_{12}}$ (LLZO) influences the ionic conductivity and the mechanical stability of the whole battery system. Therefore, a mechanical characterization and the understanding of microstructure formations of LLZO are necessary, and are in the scope of the present work. For that, established and novel developed approaches and scale bridging descriptions are used in the framework of the mechanical properties of LLZO.On the electronic scale, density functional theory (DFT) simulations allow the precise ab initio calculation of the mechanical properties of cubic LLZO, which is stabilized via co-substitutions of aluminium and tantalum. Here, prescreening methods, exploiting an electronic model, an artificial neural network and preliminary DFT calculations, determine energetically suitable substitution positions and therefore increase the efficiency of the productive computations. The directional properties of Young's modulus and shear modulus indicate an anisotropy of LLZO, however, the elastic properties of isotropic polycrystalline LLZO are not deviating much from the averaged outcomes. The resulting values of the lattice constants, elastic moduli and hardness show the influence of the co-substitutions, but overall the structural and mechanical properties of cubic LLZO are preserved. Realistic LLZO is a porous material, whose characteristics cannot be captured via DFT simulations, therefore a scale bridging description via a differential effective medium theory approach is used to investigate the influence of pores on the mechanical parameters. For a porosity of $10\,\\%$ in LLZO, a decay of $27\,\\%$ for Young's modulus is expected. The general agreement between the predicted and experimental values is good, allowing to use this model for consistency checks of experimental and theoretical outcomes. Depending on the doping level, the microstructure consists of a mixture of a tetragonal and a cubic phase, where the latter is beneficial due to its higher ionic conductivity. The formation of an equilibrated microstructure therefore has a strong influence on the overall electrochemical performance of this solid electrolyte material. Mechanical mismatches between the phases are expected to contribute to the spatial arrangement of the phases, which is difficult to assess with established modeling approaches. Therefore, a novel quantum annealing (QA) method for the determination of the equilibrium microstructure with long-range elastic interactions between coherent grains was developed. Comparisons with classical algorithms show that quantum annealing can accelerate the simulations drastically, even for huge system sizes with several thousands of grains, where conventional algorithms exhibit high computational demand. In order to simulate realistic LLZO microstructures, Voronoi tesselations are used to generate the grains. The QA method is demonstrated under consideration of systems with shear and tetragonal eigenstrains, whose resulting microstructures are additionally analyzed regarding applied tensile strains and random grain rotations. For the application of the developed QA approach to LLZO, the DFT results are used in order to formulate the eigenstrain. The resulting microstructures show the interplay between chemical and elastic contributions, where elastic effects favor a formation of ion conducting channels in doped LLZO.In materials science the physical properties at finite temperatures are of high interest, while so far the presented DFT and QA simulations of LLZO consider only ground state energies at $0\,\mathrm{K}$.Thermal expansion is a crucial issue in solid state batteries, which cannot be characterised via the presented QA microstructure equilibrations. Therefore, a QA method for the efficient sampling of finite temperature properties is developed, which shows high performance at low temperatures and operates at low computational demand. The performance of the approach is demonstrated using benchmarking scenarios of spin glasses and Ising chains. The QA sampling is very accurate where conventional approaches fail and therefore complements classical methods perfectly.}, cin = {525820 / 520000}, ddc = {620}, cid = {$I:(DE-82)525820_20160614$ / $I:(DE-82)520000_20140620$}, pnm = {BMBF 03XP0258C - MEET HiEnD III - Materials and Components to Meet High Energy Density Batteries (03XP0258C) / ZeDaBase-Batteriezelldatenbank (KW-BASF-6)}, pid = {G:(BMBF)03XP0258C / G:(HGF)KW-BASF-6}, typ = {PUB:(DE-HGF)11}, doi = {10.18154/RWTH-2024-08796}, url = {https://publications.rwth-aachen.de/record/993520}, }