ABSTRACT:Early stages of phase separation in liquid mixtures of polystyrene (PS) and poly(methylphenylsiloxane) were studied by light scattering. Measurements were made at four concentrations less than 60 wt% PS and at several temperatures in the two-phase region. The time (t) dependence of maximum intensity of scattered light /m and the corresponding wave number km did not obey the Cahn theory but could be represented by power-laws: Imoc. A phase separation of polymer systems upon quenching starts from a homogeneous state and proceeds through a series of heterogeneous states, as is the case with the liquid-gas phase transition in one-component systems or with liquid-liquid or solid-solid phase separation in two-component systems of small molecules. The process can be divided into two main stages, early and late, depending on the degree of time evolution. 1 At the early stages, there occur dominant concentration fluctuations in a homogeneous phase (mother phase or matrix), and these lead to the birth of new phases (daughter phases). At the late stages, called the coarsening process, 2 the size and number of daughter phases change accompanying neither nucleation of new phases nor variation in composition, and the gradual aggregation of daughter phases occurs by what is called the coalescence 1 or Ostwald Ripening mechanism.3.4 Finally, the entire system settles down to a macroscopic two-phase state.The early stage proceeds either by spinodal decomposition (SD) or by nucleation and growth. 5 The former takes place spontaneously without energy barriers when the system is brought into an unstable region, since any concentration fluctuation over a certain range of wave lengths reduces the free energy of the unstable system. The latter starts when the system enters into a metastable region, in which the system is unstable only for seldom-occurring sufficiently large concentration fluctuations. Thus, in this, there is an energy barrier for the nucleation of a new phase, but once it is formed, the new phase grows rapidly by diffusion.Spinodal decomposition was first formulated by Hillert 6 and Cahn (Cahn theory) 7 based on a linear mean field theory for concentration fluctuations. 8 In the framework of a mean field approximation, the Cahn theory was modified by Cook, 9 Langer, 10 -12 and Abraham 13 • 14 to take non-linear effects into account, and extended to polymer blends by de Gennes with the tube modelY On the other hand, Binder 16 and Kawasaki and Ohta 17 have developed new approaches to spinodal decomposition by using modern theories of phase transition.Recently, many experimental studies have been 225