Pulsed-field gradient nuclear magnetic resonance (PFG-NMR) is a powerful tool for measuring the diffusion coefficient of lithium in solid electrolytes. In this study, the temperature dependence of the lithium diffusion coefficient in polycrystalline Li 0.29 La 0.57 TiO 3 (LLTO) is determined by carefully designed experiments. The microstructure of LLTO consists of randomly oriented grains and 90°d omains. The echo decay of the PFG is not linear, as predicted by the Stejskal−Tanner equation, but is curvilinear. The decay curves are analyzed with theoretical equations for randomly oriented crystals to provide evidence of two-dimensional diffusion of Li + ions in LLTO. The NMR and conductivity diffusion coefficients agree well with each other over a wide temperature range of 273−723 K and exhibit non-Arrhenius behavior. Since the timescale of the PFG-NMR diffusion coefficient corresponds to the bulk ionic conductivity, the origin of non-Arrhenius behavior is not the number of carriers but rather the change in the mobility of Li + ions in LLTO. Specifically, the activation energy of local Li + -ion hopping decreases at temperatures above 450 K. Herein, the results are discussed in comparison with other experimental data and molecular dynamics simulations.