has been attracted to ML research by many groups around the world. According to the recovery performance of ML, it is generally believed that ML materials can be divided into trap-controllable and self-recoverable two modes. [9,10] The trap-controllable ML is associated with the captured carriers in shallow and deep traps at around below the conduction band or above the valence band. It relies on the induced energy releasing for the captured carriers from the traps, and it occurs for a certain level of mechanical stress (or strain) energy which is sufficient to activate the captured carriers releasing from the traps to recombine with emission centers, resulting in the ML phenomenon after removal the excitation source. [11,12] Self-recoverable ML materials are a special kind of luminescent materials, whose ML intensity can be output stable optical signals under the consecutive compressing-releasing cycles, and do not require light excitation to charge carriers. [13,14] Previous studies have shown that the self-recoverable ML materials depend on the generation of local piezoelectric fields, which promotes the process of electron-hole recombination and realizes the self-recoverable ML process. [15][16][17][18] However, either trap-controllable or self-recoverable ML still leads to some shortcomings. Trap-controllable mode is the current mainstream way to achieve ML, but its preirradiation process and relatively poor repeatability seriously affect the performance and accuracy of stress sensing. Self-recoverable mode can be considered as Mechanoluminescence (ML) is a striking optical phenomenon that is achieved through mechanical to optical energy conversion. Here, a series of Li 1−x Na x NbO 3 : Pr 3+ (x = 0, 0.2, 0.5, 0.8, 1.0) ML materials have been developed. In particular, due to the formation of heterostructure, the synthesized Li 0.5 Na 0.5 NbO 3 : Pr 3+ effectively couples the trap structures and piezoelectric property to realize the highly repeatable ML performance without traditional preirradiation process. Furthermore, the ML performances measured under sunlight irradiation and preheating confirm that the ML properties of Li 0.5 Na 0.5 NbO 3 : Pr 3+ can be ascribed to the dual modes of luminescence mechanism, including both trap-controllable and self-recoverable modes. In addition, DFT calculations further confirm that the doping of Na + ions in LiNbO 3 leads to electronic modulations by the formation of the heterostructures, which optimizes the trap distributions and concentrations. These modulations improve the electron transfer efficiency to promote ML performances. This work has supplied significant references for future design and synthesis of efficient ML materials for broad applications.