fig8
Figure 8. Schottky barrier formation at the dielectric-substrate interface enables electric field redistribution and enhanced BDS. (A) Cross-sectional STEM images of BCZTOD/BCZT//(1P) and BCZT/BCZTOD//(1P) heterostructures, accompanied by corresponding lattice ball-and-stick models; (B) Energy band diagram of the BCZT/BCZTOD//(1P) structure under forward bias, depicting the metal-semiconductor-dielectric configuration and the formation of a Schottky barrier at the interface. (C) Schematic illustration of Wrec in different types of P-E loops. High Wrec is achieved by suppressing the negative-side FE contribution, enabling improved ESP. BCZT: Ba0.7Ca0.3Zr0.2Ti0.8O3; BCZTOD: oxygen-deficient BCZT. This figure is quoted with permission from Sun et al.[88]. BDS: Dielectric breakdown strength; STEM: scanning transmission electron microscopy; ESP: energy storage performance; FE: ferroelectric; BCZT: 0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Ca0.3)TiO3; NSTO: Nb-doped SrTiO3.








