Lead-free ceramics (1-x)NaNbO 3 -xLiTaO 3 were synthesized by an ordinary solid-state reaction method. Rietveld analysis reveals that the crystal structure changes from one orthorhombic phase with Pbcm space group to another orthorhombic phase with P222 1 space group when increasing x. The morphotropic phase boundary between two different orthorhombic symmetries is formed at 0.14 < x < 0.18. Excess LiTaO 3 causes an abnormal grain growth behavior. The pure NaNbO 3 presents four current peaks in the I-E loop, indicating electric-field-induced transitions. A low LiTaO 3 doping induces ferroelectricity in the initially antiferroelectric (AFE) NaNbO 3 . Enhanced ferroelectricity is obtained at x ¼ 0.02-0.12. The addition of LiTaO 3 makes the ceramics undergo a transition from an antiferroelectricity dominant to a ferroelectricity dominant phase state. The optimum d 33 , k p , Q m , and P r values of 46 pC/N, 18.3%, 1333, and 27.1 mC cm À2 are obtained when x equals 0.12, and the ceramic exhibits good temperature stability because of its high T C . In 1949, Matthias grew sodium niobate (NaNbO 3 ) crystals and found them to be ferroelectric (FE) at room temperature [7], but then Vousden rejected the ferroelectric-