Lieb and kagome lattices exhibit two-dimensional topological insulator behavior with ${\mathbb{Z}}_2$ topological classification when considering spin-orbit coupling. In this study, we used a general tight-binding Hamiltonian with a morphological control parameter $\theta$ to describe the Lieb ($\theta =\pi /2$), kagome ($\theta =2\pi /3$), and transition lattices ($\pi /2<\theta <2\pi /3$) while considering intrinsic spin-orbit (ISO) coupling. We systematically investigated the effects of shear and uniaxial strains, applied along different crystallographic directions, on the electronic spectrum of these structures. Our findings reveal that these deformations can induce topological phase transitions by modifying the structural lattice angle associated with the interconversibility process between Lieb and kagome, the amplitude of the strain, and the magnitude of the ISO coupling. These transitions are confirmed by the evolution of Berry curvature and by changes in the Chern number when the gap closes. Additionally, by analyzing hypothetical strain scenarios in which the hopping and ISO coupling parameters remain intentionally unchanged, our results demonstrate that the strain-induced phase transitions arise from changes in the hopping and ISO coupling parameters.

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• Flat bands
• Geometric & topological phases
• Strain
• Topological phase transition
• Kagome lattice
• Topological materials