In addition to deepening the fundamental understanding of topology in condensed matter, they also offer new technological prospects [17] because of their striking associated features such as high conductivity, [15,18] chirality, [7,12] negative capacitance, [19][20][21][22] large electromechanical response, [10] or the possibility to design nanoelectronics based on domain walls of ferroelectrics. [23] However, the formation of these topological textures requires a delicate and precise balance between several factors, including mechanical and electrical boundary conditions [9,12] and the cooling rate the material is subject to or the amount of dc electric field it experiences. [9,11] Therefore, one may wonder if it is possible to find a physical handle that can create and stabilize them even when they are metastable, rather than the thermodynamically stable ground state. In other words, can such electric topological states be so-called hidden states? These latter cannot be accessed through ergodic processes (such as a gradual cooling of the system to give enough time to reach an equilibrium state) but rather by an excitation to break the ergodicity of the system in a complex manner. Such out-of-equilibrium hidden states have been previously generated using ultrafast optical pulses in many other materials such as, for example, i) a charge-density-wave state in a layered 1T-Ta(Se,S) 2 transition-metal dichalcogenide; [24] ii) a superconducting phase in the La 1.675 Eu 0.2 Sr 0.125 CuO 4 Mott-insulator; or iii) a ferroelectric phase in the quantum paraelectric SrTiO 3 . [25] Based on these results and the many recently predicted different states in a relaxor ferroelectric, [26] it is legitimate to wonder if electric topological states or defects can be created, stabilized, and tuned by applying a train of THz electric pulses starting from ground-state configurations that do not possess such topologies. If so, they will offer a rich playground for designing ultrafast neuromorphic computing [27][28][29][30] not only to emulate the behavior of the brain but also to accomplish such a feat at a picosecond scale. Moreover, understanding the mechanism leading to these complex topological structures, such as, for example, the nonlinearity of the atomic potential suggested for the emergence of the ferroelectric state in SrTiO 3 , [31] is highly desirable as it will provide a useful guideline for looking for more responsive materials.