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Monte Carlo simulations and self-consistent field theory applied to calculations of density profiles in A1BA2 triblock copolymer melts

机译:蒙特卡罗模拟和自洽场理论用于计算A1BA2三嵌段共聚物熔体的密度分布

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摘要

Using two complementary numerical methods, the lattice Monte Carlo simulations with parallel tempering and self-consistent field theory, we investigate the distribution of Al, B, and A2 segments in the lamellar nanostructure of A1BA2 triblock copolymer melts. While the lattice Monte Carlo method is in principle exact, it is limited by a variety of factors, such as finite size effects, long relaxation times required to reach the thermal equilibrium and geometry of the underlying lattice. It is also limited to chains consisting of relatively few segments. The self-consistent field theory, on the other hand, is free of the above limitations, but it is a mean-field approach which does not take into account the thermal fluctuations. Therefore we confront the results obtained from the two above methods and draw conclusions concerning both the comparison of the two methods and the localization of the Al segments in the B domain with increasing length of the Al block. For Monte Carlo simulations we employ two types of chains, 2-32-30 and 1-16-15, and for the self-consistent field theory we use the corresponding values of the thermodynamic incompatibility parameter, XN.
机译:使用两种互补的数值方法,采用平行回火和自洽场论的点阵蒙特卡洛模拟,我们研究了Al,B和A2链段在A1BA2三嵌段共聚物熔体的层状纳米结构中的分布。尽管晶格蒙特卡罗方法在原理上是精​​确的,但它受到多种因素的限制,例如有限的尺寸效应,达到热平衡所需的较长的弛豫时间以及底层晶格的几何形状。它也仅限于由相对较少的段组成的链。另一方面,自洽场理论不受上述限制,但它是一种不考虑热波动的均值场方法。因此,我们面对了从上述两种方法获得的结果,并得出了关于两种方法的比较以及随着Al嵌段长度的增加在B域中Al片段的定位的结论。对于蒙特卡洛模拟,我们使用两种类型的链:2-​​32-30和1-16-15,对于自洽场论,我们使用热力学不相容性参数XN的相应值。

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