Among Bi alkali metal titanate piezoceramics [1][2][3][4][5][6][7][8][9][10], (Bi 0.5 Na 0.5 )TiO 3 (BNT) is a typical system that has been known for many years. Its structure was identified as ABO 3 perovskite with rhombohedral symmetry. However, it was long ago concluded that, due to its properties, it was not viable to compete with Pb(Zr,Ti)O 3 (PZT)-based ceramics. Not surprisingly, it did not draw much attention until the toxicity of the PZT oxide became a critical environmental issue. In particular, Pb and Pb oxide processing and waste disposal are harmful to the environment. Restrictions have been imposed on the use of hazardous substances; however, PZT-based ceramics have been an exception because substitute materials have not been available. In light of this situation, Pb-free materials have been rigorously studied. Thus far, none of the currently available Pb-free materials has shown properties comparable to those of PZT.BNT is such a Pb-free material frequently mentioned in the literature. However, there are still ambiguities in the characteristics of BNT itself because most of the research piling up on BNT has been based solid solutions with morphotropic phase boundary (MPB) compositions which are expected to have a similar success to PZT solid solutions [11][12][13][14][15][16][17][18][19][20][21][22][23][24]. As expected, high properties have been obtained but the values themselves have been below expectations as compared with PZT. In particular, key properties such as the piezoelectric coefficient (d 33 ) and the depolarization temperature (T d ) are not good enough to replace PZT. To be able to improve the BNT properties, it is necessary to understand the end members of solid solutions. Here, T d is a unique property in BNT, not observed in PZT, but acting as a counterpart of the Curie temperature (T c ) of PZT, which has been observed to be