Computing Research Center, High Energy Accelerator Research Organization (KEK), Oho 1, Tsukuba, Ibaraki 305-0801, Japan.
J Chem Phys. 2013 Nov 14;139(18):184904. doi: 10.1063/1.4829046.
We studied equilibrium conformations of trivial-, 31-knot, and 51-knot ring polymers with finite chain length at their θ-conditions using a Monte Carlo simulation. The polymer chains treated in this study were composed of beads and bonds on a face-centered-cubic lattice respecting the excluded volume. The Flory's critical exponent ν in Rg ~ N(ν) relationship was obtained from the dependence of the radius of gyration, Rg, on the segment number of polymers, N. In this study, the temperatures at which ν equal 1∕2 are defined as θ-temperatures of several ring molecules. The θ-temperatures for trivial-, 31-knot, and 51-knot ring polymers are lower than that for a linear polymer in N ≤ 4096, where their topologies are fixed by their excluded volumes. The radial distribution functions of the segments in each molecule are obtained at their θ-temperatures. The functions of linear- and trivial-ring polymers have been found to be expressed by those of Gaussian and closed-Gaussian chains, respectively. At the θ-conditions, the excluded volumes of chains and the topological-constraints of trivial-ring polymers can be apparently screened by the attractive force between segments, and the <Rg(2)> values for trivial ring polymers are larger than the half of those for linear polymers. In the finite N region the topological-constraints of 31- and 51-knot rings are stronger than that of trivial-ring, and trajectories of the knotted ring polymers cannot be described as a closed Gaussian even though they are under θ-conditions.
我们使用蒙特卡罗模拟研究了在θ条件下具有有限链长的平凡、31 结和 51 结环聚合物的平衡构象。在这项研究中,处理的聚合物链由面心立方晶格上的珠子和键组成,同时尊重排除体积。从回转半径 Rg 与聚合物链段数 N 的依赖关系中得到 Flory 临界指数 ν 在 Rg~N(ν)关系中的值。在这项研究中,ν 等于 1∕2 的温度被定义为几个环分子的θ温度。在 N ≤ 4096 时,平凡、31 结和 51 结环聚合物的θ温度低于线性聚合物的θ温度,在这个范围内,它们的拓扑结构由排除体积固定。在各自的θ温度下,获得了每个分子中链段的径向分布函数。线性和平凡环聚合物的函数分别由高斯和封闭高斯链的函数表示。在θ条件下,链的排除体积和平凡环聚合物的拓扑约束可以通过链段之间的吸引力明显屏蔽,平凡环聚合物的<Rg(2)>值大于线性聚合物的一半。在有限的 N 区域中,31 结和 51 结环的拓扑约束比平凡环的强,即使在θ条件下,扭结环聚合物的轨迹也不能描述为封闭高斯。