ferroelectric materials, which are comprised of non-centrosymmetric unit cells, each possessing a switchable polarization of their electric dipole moment. Of the class of ferroelectric materials, perovskitestructured Bi 0.5 Na 0.5 TiO 3 (BNT)-based compounds have attracted worldwide research interest in recent years with the development of lead-free forms, [4] which have been deployed in a range of technological applications, including piezoelectric actuators, sensors, and dielectric capacitors. Each of these areas of utility is respectively attributed to their large electric field-induced strain, [5] high piezoelectric constant, and high specific energy. While earlier studies of the crystal structure and phase transitions of BNT have answered many questions, there still remain some key points that are controversial due to the complexity of NaO and BiO bonds, and the octahedral tilt in the unit cell. [6] Due to these unique structural properties, phase transitions in BNT, and its derivatives, can be induced by applied electric fields of 10s of kV cm −1 [7,8] which, in most cases, are indirectly represented by the electrical field-dependent bipolar current, polarization, or strain loops Electric-field-induced phase transitions in Bi 0.5 Na 0.5 TiO 3 -based relaxor ferroelectrics are essential to the control of their electrical properties and consequently in revolutionizing their dielectric and piezoelectric applications. However, fundamental understanding of these transitions is a long-standing challenge due to their complex crystal structures. Given the structural inhomogeneity at the nanoscale or sub-nanoscale in these materials, dielectric response characterization based on terahertz (THz) electromagnetic-probe beam fields is intrinsically coordinated to lattice dynamics during DC-biased poling cycles. The complex permittivity reveals the field-induced phase transitions to be irreversible. This profoundly counters the claim of reversibility, the conventional support for which is based upon the peak that is manifest in each of four quadrants of the current-field curves. The mechanism of this irreversibility is solely attributed to polar clusters in the transformed lattices. These represent an extrinsic factor, which is quiescent in the THz spectral domain.