Semi-flexible interacting self-avoiding trails on the square lattice
arXiv:1210.7983 · doi:10.1016/j.physa.2012.12.019
Abstract
Self-avoiding walks self-interacting via nearest neighbours (ISAW) and self-avoiding trails interacting via multiply-visited sites (ISAT) are two models of the polymer collapse transition of a polymer in dilute solution. On the square lattice it has been established numerically that the collapse transition of each model lies in a different universality class. It has been shown that by adding stiffness to the ISAW model a second low temperature phase eventuates and a more complicated phase diagram ensues with three types of transition that meet at a multi-critical point. For large enough stiffness the collapse transition becomes first-order. Interestingly, a phase diagram of a similar structure has been seen to occur in an extended ISAT model on the triangular lattice without stiffness. It is therefore of interest to see the effect of adding stiffness to the ISAT model. We have studied by computer simulation a generalised model of self-interacting self-avoiding trails on the square lattice with a stiffness parameter added. Intriguingly, we find that stiffness does not change the order of the collapse transition for ISAT on the square lattice for a very wide range of stiffness weights. While at the lengths considered there are clear bimodal distributions for very large stiffness, our numerical evidence strongly suggests that these are simply finite-size effects associated with a crossover to a first-order phase transition at infinite stiffness.
13 pages, 9 figures. arXiv admin note: substantial text overlap with arXiv:1210.7196
References in corpus (5)
- Freezing and Collapse of Flexible Polymers on Regular Lattices in Three Dimensions
- Collapse Transition of Two-Dimensional Flexible and Semiflexible Polymers
- Collapse transition of self-avoiding trails on the square lattice
- Identification of a polymer growth process with an equilibrium multi-critical collapse phase transition: the meeting point of swollen, collapsed and crystalline polymers
- Weighting of topologically different interactions in a model of two-dimensional polymer collapse