Surface Effects on Block Copolymer Melts Above the Order-Disorder Transition: Linear Theory of Equilibrium Properties and the Kinetics of Surface-Induced Ordering

K. Binder, Harry L. Risch, S. Stepanow
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引用次数: 11

Abstract

A phenomenological theory is developed for static and dynamic aspects ofsurface- induced ordering of symmetrical block copolymers taking fluctuation corrections into account, but, considering conditions where the bulk block copolymer melt is still disordered, and a lin- earized version of the resulting Ginzburg-Landau type equation suffices. Both the semi-infinite geometry and symmetrical films of thickness 2L are treated, applying the same boundary con- ditions as used previously for a treatment of wetting in polymer blends, assuming short range surface forces and a long Wavelength approximation. For the static order parameter profile in thin film geometry, We derive an oscillatory convergence of both amplitude and phase to the corre- sponding properties of the semi-infinite systems, because terms of order exp(-2L/f+) cos(2Lq*) enter, f+ being the correlation length and = 21r/q* the Wave~length of lamellar ordering. It is shown that the conservation of the number of monomers of the two species, Which can be expressed as a global constraint on the order parameter, leads to a non-linear equation for the phase expressed in terms of the amplitude, When one considers the kinetics of ordering. Both numerical and approximate analytical treatments are given to describe the evolution of the considered systems towards equilibrium.
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嵌段共聚物熔体在有序-无序过渡之上的表面效应:平衡性质的线性理论和表面诱导有序的动力学
在考虑波动修正的情况下,为对称嵌段共聚物表面诱导有序的静态和动态方面发展了一种现象学理论,但是,考虑到大块嵌段共聚物熔体仍然无序的条件,并且由此产生的金兹堡-朗道型方程的线性化版本就足够了。在处理厚度为2L的半无限几何和对称薄膜时,采用与先前用于处理聚合物共混物润湿相同的边界条件,假设短距离表面力和长波长近似。对于薄膜几何中的静态序参量分布,由于阶项exp(- 2l /f+) cos(2Lq*)进入,其中f+为相关长度,= 21r/q*为层状有序的波长度,我们推导出振幅和相位对半无限系统相应性质的振荡收敛。结果表明,当考虑有序化动力学时,两种单体数量的守恒性(可表示为对有序参数的全局约束)导致以振幅表示的相的非线性方程。给出了数值和近似解析处理来描述所考虑的系统向平衡的演化。
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