“…With high breakdown strength, the nanocomposites can operate efficiently at both relatively low and high electric fields. It is found that the P(VDF-TrFE-CFE)-BNNSs-BST1/2/3 nanocomposite exhibits a giant Q of 100 MJ m –3 , Δ S of 310 kJ m –3 K –1 , and Δ T of 35 °C at an electric field of 200 MV m –1 , as shown in Figures c and S20, which not only surpass the pure ferroelectric polymer, but also exceed most inorganic ferroelectric materials. ,, The maximum electric field in the EC measurements is deliberately set at about half to the breakdown strength of the samples, which is predicted by the theoretical calculations of dielectric materials with a lifetime of 10 years . Concurrently, as shown in Figures a and S17a and c, under a relatively low electric field of 75 MV m –1 , a sizable ECE, that is, Q of 25 MJ m –3 , Δ S of 70 kJ m –3 K –1 , and Δ T of 8 °C, is obtained in the nanocomposites, which is ∼2 times superior to that of pristine P(VDF-TrFE-CFE), and comparable to the ECE generated in the P(VDF-TrFE-CFE)-BST1/2/3 binary nanocomposites.…”