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This assumption is probably justified for the polymer blend in the late stage of SD, but it is only approximately true for a bicontinuous microemulsion. For the latter, one may take A ≈ d. More precisely, the spectral function we introduced contains three length scales, although there may be some relations among them in real systems.
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25
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note
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Scattering intensity in eq 14 should be expressed not only as a function of q but also as a function of time, t, for the polymer mixture; the phase separation of the system is a non-equilibrium process, and thus, a time-dependent process. Since, in the present study, the time evolution of the phase-separated structure is not the central issue, and we discuss the scattering intensity at a fixed time for the polymer blend, we simply write the scattering only as a function of q.
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