Erukhimovich I Y
Moscow State University, Moscow 119899, Russia.
Eur Phys J E Soft Matter. 2005 Dec;18(4):383-406. doi: 10.1140/epje/e2005-00054-5. Epub 2005 Dec 13.
The statistical theory of microphase separation in the ternary ABC triblock copolymers is presented and the corresponding phase diagrams are built both for the linear and miktoarm copolymers. For this purpose the Leibler weak segregation theory in molten diblock copolymers is generalized to multi-component monodisperse block copolymers with due regard for the 2nd shell harmonics contributions defined in the paper. The Hildebrand approximation for the chi-parameters is used. The physical meaning of this and alternative choices for the chi-parameters is discussed. The symmetric A(f)B(1-2f)C(f) copolymers with the middle block non-selective with respect to the side ones are shown to undergo the continuous ODT not only into the lamellar phase but also, instead, into various non-conventional cubic phases (depending on the middle block composition it could be the simple cubic, face-centered cubic or non-centrosymmetric phase, which reveals the symmetry of I4(1) 32 space group No. 214 first predicted to appear in molten block copolymers). For asymmetric linear ABC copolymers a region of compositions is found where the weakly segregated gyroid (double gyroid) phase exists between the planar hexagonal and lamellar or one of the non-conventional cubic phases up to the very critical point. In contrast, the miktoarm (star) ABC block copolymers with one of its arm non-selective with respect to the two others are shown to reveal a pronounced tendency towards strong segregation, which is preceded by increase of stability of the conventional BCC phase and a peculiar weakly segregated BCC phase (BCC(3)), where the dominant harmonics belong to the 3rd coordination sphere of the reciprocal lattice. The validity region of the developed theory is discussed and outlined in the composition triangles both for linear and miktoarm copolymers. We present also the list of the 2nd shell harmonics (SAXS reflections) allowed and prohibited in some of the non-conventional morphologies due to the weak segregation considerations and comparison of our results with the preceding SCFT treatment of the ABC copolymers by Matsen.
本文提出了三元ABC三嵌段共聚物微相分离的统计理论,并构建了线性和星型共聚物的相应相图。为此,将熔融二嵌段共聚物中的莱布勒弱分离理论推广到多组分单分散嵌段共聚物,并考虑了本文中定义的第二壳层谐波贡献。使用了希尔德布兰德对χ参数的近似。讨论了χ参数的这种选择和其他选择的物理意义。结果表明,中间嵌段对两侧嵌段无选择性的对称A(f)B(1-2f)C(f)共聚物不仅会连续发生到层状相的ODT转变,还会发生到各种非常规立方相的转变(取决于中间嵌段的组成,可能是简单立方相、面心立方相或非中心对称相,这首次揭示了预测会出现在熔融嵌段共聚物中的I4(1) 32空间群(编号214)的对称性)。对于不对称线性ABC共聚物,发现了一个组成区域,在该区域中,弱分离的螺旋状(双螺旋状)相存在于平面六方相和层状相或其中一种非常规立方相之间,直至非常接近临界点。相比之下,其中一个臂对另外两个臂无选择性的星型(miktoarm)ABC嵌段共聚物表现出明显的强烈分离趋势,在此之前,常规体心立方相和一种特殊的弱分离体心立方相(BCC(3))的稳定性会增加,其中主导谐波属于倒易晶格的第三配位球。讨论并在组成三角形中概述了所发展理论在线性和星型共聚物中的适用范围。我们还列出了由于弱分离考虑在一些非常规形态中允许和禁止的第二壳层谐波(小角X射线散射反射),并将我们的结果与Matsen之前对ABC共聚物的自洽场理论处理进行了比较。