By Christian Holm, Kurt Kremer, S. Auer, K. Binder, J.G. Curro, D. Frenkel, G.S. Grest, D.R. Heine, P.H. Hünenberger, L.G. MacDowell, M. Müller, P. Virnau

Soft topic technology is these days an acronym for an more and more very important classification of fabrics, which levels from polymers, liquid crystals, colloids as much as complicated macromolecular assemblies, protecting sizes from the nanoscale up the microscale. desktop simulations have confirmed as an crucial, if no longer the main robust, instrument to appreciate homes of those fabrics and hyperlink theoretical versions to experiments. during this first quantity of a small sequence famous leaders of the sphere evaluate complex themes and supply severe perception into the cutting-edge equipment and clinical questions of this full of life area of sentimental condensed topic research.

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**Example text**

The results for a local Onsager coefﬁcient are presented in Fig. 12 and are bracketed by the approximations for the weak and strong segregation limits. In Fig. 15 we corroborate that the results of the dynamic SCF calculations using the non-local Onsager coefﬁcient (Eq. 114) agree with the EPD using the local Onsager coefﬁcient (Eq. 126) for the ﬁeld W. As detailed in Sect. 5, however, the EPD calculations are computationally much less demanding. The growth rates for the dynamic SCF theory with local Onsager coefﬁcient are displayed in Fig.

Unfortunately, the lower critical dimension of isotropic Lifshitz points is not known [102]. Indeed, the experimentally observed phase behavior differs substantially from the mean-ﬁeld phase diagram. An example is shown in Fig. 6. The Lifshitz point is destroyed, the three phase coexistence region between the Fig. 5 Mean-ﬁeld phase diagram for a ternary symmetric A + B + AB blend as a function of the incompatibility parameter χN and the homopolymer volume fraction ΦH . The chain lengths of the copolymers is ﬁve times that of the homopolymers.

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