Abstract
We study pressurised self-avoiding ring polymers in two dimensions using Monte Carlo simulations, scaling arguments and Flory-type theories, through models which generalise the model of Leibler, Singh and Fisher (Phys. Rev. Lett. 59, 1989 (1987)). We demonstrate the existence of a thermodynamic phase transition at a non-zero scaled pressure \( \tilde{p}\) , where \( \tilde{p}\) = Np/4\( \pi\) , with the number of monomers N \( \rightarrow\) ∞ and the pressure p \( \rightarrow\) 0 , keeping \( \tilde{p}\) constant, in a class of such models. This transition is driven by bond energetics and can be either continuous or discontinuous. It can be interpreted as a shape transition in which the ring polymer takes the shape, above the critical pressure, of a regular N -gon whose sides scale smoothly with pressure, while staying unfaceted below this critical pressure. Away from these limits, we argue that the transition is replaced by a sharp crossover. The area, however, scales with N2 for all positive p in all such models, consistent with earlier scaling theories.
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Mitra, M.K., Menon, G.I. & Rajesh, R. Thermodynamic behaviour of two-dimensional vesicles revisited. Eur. Phys. J. E 35, 30 (2012). https://doi.org/10.1140/epje/i2012-12030-1
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DOI: https://doi.org/10.1140/epje/i2012-12030-1