The field-induced, spontaneous, and isothermal transition from glassy state to long-range-ordered ferroic state in two physically parallel ferroic glasses (relaxor and strain glass) have been reviewed from the aspect of experimental characteristics. The similarities and differences between these two ferroic glasses from macroscopic to microscopic properties have been summarized. In addition, some interesting phenomena that deserve further investigations have been pointed out.1 Introduction Ferroic materials possess two or more orientation states of a physical property with the same energy and these orientation states can be switched by an external field [1, 2]. Ferroelastics with spontaneous strain (e), ferroelectrics with spontaneous polarization (P) and ferromagnets with spontaneous magnetization (M) are the three best-known classes of primary ferroics [1,2]. Quenched randomness or defects in ferroic systems generally give rise to the frustration in a ferroic property such as strain, polarization, or magnetization; and thus result in the disordered glass-like states in ferroic materials, such as strain glass in ferroelastics (shape-memory alloys) [3], relaxor in ferroelectrics [4], and spin glass in ferromagnets [5]. These disordered states are generally termed as "ferroic glass" [6].There are three distinct states in ferroic materials with respect to their order parameter: a high-temperature parent phase with order parameter equal to zero (austenite or parent phase, paraelectric state, and paramagnetic state), a lowtemperature ferroic state with long-range-ordered order parameter (martensite or ferroelastic state, ferrolectric state, and ferromagnetic state), and a low-temperature glassy state (strain glass, relaxor, and spin glass) with a frozen and frustrated local order of the order parameter. The transitions