Woloszczuk Sebastian, Mineart Kenneth P, Spontak Richard J, Banaszak Michal
Faculty of Physics, Adam Mickiewicz University, 61-614 Poznan, Poland.
Department of Chemical & Biomolecular Engineering, North Carolina State University, Raleigh, North Carolina 27695, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2015 Jan;91(1):010601. doi: 10.1103/PhysRevE.91.010601. Epub 2015 Jan 13.
While ABC triblock copolymers are known to form a plethora of dual-mode (i.e., order-on-order) nanostructures, bicomponent ABA triblock copolymers normally self-assemble into single morphologies at thermodynamic incompatibility levels up to the strong-segregation regime. In this study, we employ on-lattice Monte Carlo simulations to examine the phase behavior of molecularly asymmetric A(1)BA(2) copolymers possessing chemically identical endblocks differing significantly in length. In the limit of superstrong segregation, interstitial micelles composed of the minority A(2) endblock are observed to arrange into two-dimensional hexagonal arrays along the midplane of B-rich lamellae in compositionally symmetric (50:50 A:B) copolymers. Simulations performed here establish the coupled molecular-asymmetry and incompatibility conditions under which such micelles form, as well as the temperature dependence of their aggregation number. Beyond an optimal length of the A(2) endblock, the propensity for interstitial micelles to develop decreases, and the likelihood for colocation of both endblocks in the A(1)-rich lamellae increases. Interestingly, the strong-segregation theory of Semenov developed to explain the formation of free micelles by diblock copolymers accurately predicts the onset of interstitial micelles confined at nanoscale dimensions between parallel lamellae.
虽然已知ABC三嵌段共聚物会形成大量双模式(即有序-有序)纳米结构,但在热力学不相容程度达到强分离状态时,双组分ABA三嵌段共聚物通常会自组装成单一形态。在本研究中,我们采用晶格蒙特卡罗模拟来研究分子不对称的A(1)BA(2)共聚物的相行为,该共聚物的化学性质相同的端基在长度上有显著差异。在超强分离的极限情况下,观察到由少数A(2)端基组成的间隙胶束在组成对称(50:50 A:B)的共聚物中沿着富B片层的中平面排列成二维六边形阵列。这里进行的模拟确定了形成这种胶束的分子不对称和不相容耦合条件,以及它们聚集数的温度依赖性。超过A(2)端基的最佳长度后,间隙胶束形成的倾向降低,且两个端基在富A(1)片层中共存的可能性增加。有趣的是,为解释二嵌段共聚物形成自由胶束而发展的谢苗诺夫强分离理论准确地预测了在平行片层之间纳米尺度范围内受限的间隙胶束的出现。