An imminent challenge of lead-free Bi 0.5 Na 0.5 TiO 3based (BNT) piezoceramics is that the giant piezoelectric constant (d 33 ) caused by the morphotropic phase boundary is incompatible with a high depolarization temperature (T d ) and ultralow temperature coefficient (T tc ) of the real-time d 33 , which severely hinders their industrial application in the field of elevated temperatures. Herein, a sandwich-structured 0.94Bi 0.5 Na 0.5 TiO 3 − 0 . 0 6 B a T i O 3 / 0 . 8 9 B i 0 . 5 N a 0 . 5 T i O 3 − 0 . 1 1 B a T i O 3 / 0.94Bi 0.5 Na 0.5 TiO 3 −0.06BaTiO 3 (SWS-6/11/6BT-y, where y refers to the weight fraction of the BNT-11BT solid solution) ceramic composite is engineered for mitigating the conflict between d 33 , T d and T tc . Following this strategy, ultrahigh T d near the Curie point (225 °C, close to that of the BNT-11BT layer) and relatively large d 33 (130 pC/N, close to that of the BNT-6BT layer) are simultaneously realized in a SWS-6/11/6BT-40%-Q ceramic composite. More importantly, the ultralow T tc (0.07%) of real-time d 33 is also achieved in this work. The structural heterogeneity yields the high piezoresponse, and the built-in field resulting from layer-type ceramic composites provides the driving force to promote the diffused ferroelectric−relaxor phase transition and the resultant ferroelectric order with high T d . The above synergistic contributions realize the remission of the d 33 −T d −T tc conflict in a sandwich-structural SWS-6/11/6BT-40% ceramic composite. Thus, our work provided a path for designing the BNT-based piezoceramics with potential for industrial applications.