LaCoO 3 -materials have received considerable attention due to their novel magnetic properties [1][2][3] and mixed ionicelectronic conductivity at elevated temperatures leading to exciting applications such as electrodes in solid oxide fuel cells [4] and oxygen permeable membranes.[5] Perovskites such as LaCoO 3 and related materials like LaAlO 3 undergo a displacive phase transition from a paraelastic cubic perovskite with space group Pm 3m at high temperatures to a ferroelastic rhombohedral perovskite with space group R 3c. [6][7][8][9][10] Toughening of the materials is particularly beneficial for membrane applications. Ferroelastic domain switching in LaCoO 3 -materials under mechanical load may increase the fracture toughness of the materials.[11] Microstructure investigations of the ferroelastic domains and switching mechanisms in LaCoO 3 -materials are therefore interesting in order to understand the materials′ mechanical behavior. In this work we report a detailed transmission electron microscopy (TEM) analysis of the ferroelastic domains in LaCoO 3 -based materials. In addition to the well known ferroelastic domains formed by deformation twinning in rhombohedral perovskites, a monoclinic structure is observed by TEM in LaCoO 3 -based materials. The second order improper paraelastic to ferroelastic phase transition in LaCoO 3 -materials doubles the periodicity along the threefold axis, which becomes the unique axis of the rhombohedral ferroelastic state. The phase transition results in the well known deformation twinning (ferroelastic twin domain [12]