perovskites, this is provided by the longrange correlation of B-site (Ti 4+ ) cation displacements. This correlation encompasses also strains up to the microscale, and is embodied by the appearance of ferroelectric domains. [3] Upon field cycling, as needed for charging-discharging the capacitor, ferroelectric domains switch in the direction of the applied field, thereby dissipating the associated elastic energy as heat. These losses are one of the main origins of the low recoverable energy density in this class of materials. [4] One often pursued strategy to increase the recoverable energy density of ceramic capacitors is thus to avoid elasticity-driven losses by disembodying electric charge from elastic strain through the disruption of the long-range correlation of Ti 4+ displacements. [2] When BTO is substituted at the perovskite B-site, in fact, the correlation of TiOTi chains is broken; [5] consequently, ferroelectric domains cease to permeate the whole lattice and are rather confined to nanoscale polar regions, whose size, correlation and distribution depends on substituent type and concentration. [6] The absence of longrange strain correlation limits the losses associated with elastic energy and slims down the polarization-electric field (P-E) hysteresis loop, thereby increasing the recoverable energy density, [2] provided that the achievable polarization at the maximum