In modern electronic systems and energy conversion, efficient capacitors with large energy densities are needed. Relaxor ferroelectrics show the potential to achieve those requirements. The lead-free relaxor ferroelectric 0.852(Na 1/2 Bi 1/2 TiO 3 )-0.028(BaTiO 3 )-0.12(K 1/2 Bi 1/2 TiO 3 ) is investigated exhibiting the behavior of a wide range of Na 1/2 Bi 1/2 TiO 3 -based relaxor systems. The criticality of this system is analyzed and a full electric field-temperature phase diagram is constructed. The energy storage performance is determined from polarization measurements in a wide temperature range. It is found that energy density and especially the efficiency is largely increased in the vicinity of the critical end point of the relaxor system. The concept of criticality is widely applicable to lead-based and lead-free relaxor ferroelectrics and therefore an important approach to increase energy storage performance in those systems.Modern electronics and electrical devices require for large energy storage and power output. [1][2][3] Batteries are the superior choice for energy storage, however, they suffer from their low power output due to the slow conversion from chemical energy to electrical energy. Capacitors on the other hand, exhibit large power outputs but suffer from their low energy storage capability. [4] To increase the energy storage density in ceramic capacitors mainly two classes of ferroelectrics are considered, i.e., relaxor ferroelectrics (REs) and antiferroelectrics (AFEs). [5] Both exhibit reversible electric field-induced phase transitions, which can increase the energy storage density. [6,7] The energy storage density (W total ) of ferroelectrics is usually determined from electric field-dependent polarization measurements using Equation (1). [8] where P max is the polarization at maximum electric field, E the applied electric field, and P the corresponding polarization during the charging process. To determine the recoverable energy storage density (W rec ), this is the energy released during the discharge process, the polarization during electric field decrease from maximum to zero has to be considered. W rec is calculated by Equation (2). [9] W rec ¼where P r denotes the remanent polarization. The difference between W total and W rec is the area enclosed by the polarization curve and describes the losses (W loss ). The efficiency (η) is given as the ratio between charging and discharging process, i.e., Equation (3). [9] ηEquations (1)-(3) demonstrate that in order to achieve high energy storage performance, the maximum polarization needs to be high and the remanent polarization low. In comparison with classical ferroelectrics, like barium titanate, REs and AFEs display those properties due to relaxor-ferroelectric and antiferroelectric-ferroelectric phase transitions. [5] REs feature different macroscopic properties whether they are in the nonergodic relaxor (NR) phase or the ergodic relaxor (ER) phase. In the temperature range of the ER phase, reversible phase transitions between the ...