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Crumpled-to-tubule transition and shape transformations of a model of self-avoiding spherical meshwork
This paper analyzes a new self-avoiding (SA) meshwork model using the canonical Monte Carlo simulation technique on lattices that consist of connection-fixed triangles. The Hamiltonian of this model includes a self-avoiding potential and a pressure term. The model identifies a crumpled-to-tubule (CT...
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Published in: | arXiv.org 2013-12 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | This paper analyzes a new self-avoiding (SA) meshwork model using the canonical Monte Carlo simulation technique on lattices that consist of connection-fixed triangles. The Hamiltonian of this model includes a self-avoiding potential and a pressure term. The model identifies a crumpled-to-tubule (CT) transition between the crumpled and tubular phases. This is a second-order transition, which occurs when the pressure difference between the inner and outer sides of the surface is close to zero. We obtain the Flory swelling exponents \(\nu_{{\rm R}^2}(=\!D_f/2)\) and \(\bar{\nu}_{\rm v}\) corresponding to the mean square radius of gyration \(R_g^2\) and enclosed volume \(V\), where \(D_f\) is the fractal dimension. The analysis shows that \(\bar{\nu}_{\rm v}\) at the transition is almost identical to the one of the smooth phase of previously reported SA model which has no crumpled phase. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1312.1408 |