“…The actual pathway from a metastable state to an equilibrium state depends upon intrinsic and external agitations, which can include the rate of the temperature changes, thermal activation of domain wall displacements and an application of magnetic fields. Depending upon these factors, various scenarios of the temperature evolution of the domain structure can take place: (i) a jump-like DS transition can occur in the domain size and period that corresponds to a higher (or lower) temperature [29]; (ii) continuous changes of the domain geometry and size occur when the DS slowly passes through the chain of equilibrium states [31]; finally, (iii) the coexistence of two domain structures can exist characterized by different domain shapes, sizes and periods [28]. In general, the main magnetic parameters that determine the equilibrium domain size and period are the domain wall width d = (A/K) 1/2 and the characteristic length l c = r/4pM S 2 , where r = 4(AK) 1/2 is the domain wall energy surface density and A is the exchange constant.…”