The increase of the dielectric permittivity with an electric field and enhanced energy storage properties make antiferroelectrics very attractive for high-power electronic applications needed in emerging green energy technologies and neuromorphic computing platforms. Their exceptional functional properties are closely related to the electric field-induced antiferroelectric\ensuremath{\leftrightarrow}ferroelectric phase transition, which can be driven toward a critical end point by manipulation with an external electric field. The critical fluctuation of physical properties at the critical end point in ferroelectrics is a promising approach to improve their functional properties. Here, we demonstrate the existence of two critical end points in antiferroelectric ceramics with a ferroelectric-antiferroelectric-paraelectric phase sequence, using the model system ${\mathrm{Pb}}_{0.99}{\mathrm{Nb}}_{0.02}{[{({\mathrm{Zr}}_{0.57}{\mathrm{Sn}}_{0.43})}_{0.92}{\mathrm{Ti}}_{0.08}]}_{0.98}{\mathrm{O}}_{3}$. The critical fluctuation of the dielectric permittivity in the proximity of the antiferroelectric-to-paraelectric critical end point is responsible for the strong enhancement of the dielectric tunability (by a factor of $>2$) measured at $\ensuremath{\approx}395$ K. The enhancement of the energy storage density at $\ensuremath{\approx}370$ K is related to the proximity of the ferroelectric-to-antiferroelectric critical end point. These findings open possibilities for material design and pave the way for the next generation of high-energy storage materials.