Since the discovery of ferroelectric (FE) properties in HfO 2 -based materials, [1] numerous advantages, such as simple structures, strong binding energy between oxygen and transition metal ions, large bandgap (%5.3-5.7 eV), and compatibility with current complementary metal-oxide semiconductor technologies, led to extensive research that focused on potential diverse applications, such as FE memory, ferroelectric field-effect transistors (Fe-FETs), pyroelectric sensors, and energy harvesters. Meanwhile, from the material survey of FEs, it is conventional that the structural phase transition induced by a compositional change plays a special role in obtaining excellent piezoelectric and dielectric properties. [2][3][4][5][6][7][8][9] The phase boundary known as morphotropic phase boundary (MPB) separates regions of different symmetries by varying their composition in FEs. [2][3][4][5][6][7][8][9] In fact, when different structural phases are almost degenerated near the MPB, rotations of polarization occur in response to external electric fields instead of a change in the magnitude of polarization. [5] Consequently, materials exhibit maximum piezoelectric and dielectric responses near the MPB, as several phases coexist, and there is nearly no energy barrier separating them. The MPB has garnered significant practical interest, because the variable that drives the transition (i.e., compositions) is inherent. Therefore, it provides an alternative approach to boost the dielectric constant ϵ r without degrading the bandgap. MPB ceramics are the basis of a wide range of piezoelectric and dielectric technologies, such as high-k materials, sensors, actuators, smart systems, ultrasound generation, and sensing and underwater acoustics. These applications motivated researchers to investigate the existence of MPB in the novel promising ceramic compounds, e.g., PbHfO 3 -PbTiO 3 -Pb(Mg 1/3 Nb 2/3 )O 3 , [10,11] lead-free BiFeO 3 -BaTiO 3 , [12,13] Pb(In 1/