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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Defects in lamellar diblock copolymers: Chevron- and Omega-shaped tilt boundaries
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Defects in lamellar diblock copolymers: Chevron- and Omega-shaped tilt boundaries

机译:层状二嵌段共聚物的缺陷:雪佛龙形和欧米茄形的倾斜边界

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摘要

The lamellar phase in diblock copolymer systems appears as a result of a competition between molecular and entropic forces, which selects a preferred periodicity of the lamellae. Grain boundaries are formed when two grains of different orientations meet. We investigate the case where the lamellae meet symmetrically with respect to the interface. The form of the interface strongly depends on the angle, theta, between the normals of the grains. When this angle is small, the lamellae transform smoothly from one orientation to the other, creating the chevron morphology. As theta increases, a gradual transition is observed to an omega morphology characterized by a protrusion of the lamellae along the interface between the two phases. We present a theoretical approach to find these tilt boundaries in two-dimensional systems, based on a Ginzburg-Landau expansion of the free energy, which describes the appearance of Iamellae. Close to the tips at which lamellae from different grains meet, these lamellae are distorted. To find this distortion for small angles, we use a phase variation ansatz in which one assumes that the wave vector of the bulk lamellar phase depends on the distance from the interface. Minimization of the free energy gives an expression for the order parameter phi(x,y). The results describe the chevron morphology very well. For larger angles, a different approach is used. We linearize phi around its bulk value phi(L) and expand the free energy to second order in their difference. Minimization of the free energy results in a linear fourth-order differential equation for the distortion held, with proper constraints, similar to the Mathieu equation. The calculated monomer profile and line tension agree qualitatively with transmission electron microscope experiments, and with full numerical solution of the same problem. [References: 24]
机译:二嵌段共聚物体系中的层状相是分子力和熵力之间竞争的结果,这选择了薄片的优选周期性。当两个不同方向的晶粒相遇时会形成晶界。我们研究了薄片相对于界面对称相遇的情况。界面的形式在很大程度上取决于晶粒法线之间的角度θ。当此角度较小时,薄片会从一个方向平滑过渡到另一个方向,从而形成人字形形态。随着θ增加,观察到逐渐转变为Ω形貌,其特征在于薄片沿着两个相之间的界面突出。我们基于自由能的金兹堡-兰道展开描述了Iamellae的外观,提出了一种在二维系统中找到这些倾斜边界的理论方法。接近来自不同颗粒的薄片相遇的尖端,这些薄片变形了。为了找到小角度的这种畸变,我们使用相位变化ansatz,其中假设体层状相的波矢量取决于距界面的距离。自由能的最小化给出了阶数参数phi(x,y)的表达式。结果很好地描述了人字形。对于较大的角度,可以使用其他方法。我们围绕其体积值phi(L)线性化phi,并将自由能的差扩展为二阶。自由能的最小化会导致线性失真的四阶微分方程,具有适当的约束,类似于Mathieu方程。计算得到的单体轮廓和线张力与透射电子显微镜实验在质量上吻合,并且与相同问题的完整数值解吻合。 [参考:24]

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