“…Phase transition materials possess the ability to reversibly convert their physical or chemical properties accompanied by the structural transformation between different stable states, which usually endows them with various features such as ferroelectric (FE), − ferroelastic (FA), − ferromagnetic, ferrotoroidicity, dielectric switching, − and nonlinear optical (NLO) switching. − Therefore, these materials have been extensively utilized in energy storage, data storage, signal processing, photoelectric devices, mechanical switches, piezoelectric actuators, transducers, etc . − In thermally induced phase transitions, elevating temperature generally triggers the rotational or vibrational motions of those movable components, thereby inducing disordered–ordered or displacement phase transitions. − These motions typically favor pseudosymmetry and lead to high symmetry in the high-temperature phase (HTP), while decreasing the temperature leads to freezing motions and thereby inducing temperature symmetry-breaking (TSB) phase transitions, which are common in phase transitions with normal symmetry breaking. − On the contrary, an inverse temperature symmetry-breaking (ITSB) phase transition refers to a decrease in lattice symmetry upon heating, which is infrequent in phase transition materials. , For example, Rochelle salt, as a typical ITSB phase transition material, undergoes a ferroelectric phase transition from low-temperature phase (LTP) orthorhombic P 2 1 2 1 2 1 to HTP monoclinic P 2 1 upon a heating process. The ITSB phase transition results in the formation of polar, noncentrical, or chiral structures at a higher temperature, imparting the material unique physical properties under higher temperatures, i.e.…”