Ti 1−x )O 3 (PZT) has been widely used for energy storage applications because of its excellent ferroelectric and piezoelectric properties compared to other Pb-based perovskite oxides like PbTiO 3 , PMN-PT and Pb-free systems like, BaTiO 3 , BiFeO 3 , etc [1][2][3][4]. The miniaturization and integration of PZT thin film based capacitors for the development of electronic devices are of particular interest for the better performance of the energy storage. It is observed that the efficiency of energy storage in thin films is about 30 times higher than that in bulk materials [5][6][7][8]. However, PZT thin films suffer Pb loss due to high volatile nature of PbO and oxygen vacancies during the processing temperature, leading to degradation of the polarization values with a high hysteresis loss [9][10][11].However, the properties of perovskite PZT thin films can be enhanced through the addition of dopants for a wide range of applications. Tailoring of the properties of PZT thin films by suppressing and promoting oxygen or cation vacancies using