4.6 Article

Phase diagram of flexible polymers with quenched disordered charged monomers

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ELSEVIER
DOI: 10.1016/j.physa.2022.127787

Keywords

Diluted polymer; Phase diagram; Phase transitions; Microcanonical analysis; Quenched disorder; ReplicaexchangeWang-Landau

Funding

  1. CNPq [RED -00458-16]
  2. FAPEMIG

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Recent advances in Generalized Ensemble simulations and microcanonical analysis have shown the significant role of electrostatic interactions in structural transitions of polymer models. In this study, a bead-spring polymer model with randomly distributed charged monomers interacting via a screened Coulomb potential was proposed. It was found that the coil-globule and globular-solid transitions were second and first order for the entire concentration range. However, above a concentration threshold of 80%, the electrostatic repulsion hindered the formation of solid and liquid globules, leading to the formation of liquid pearl-necklace and solid helical structures instead.
Recent advances in Generalized Ensemble simulations and microcanonical analysis allowed the investigation of structural transitions in polymer models over a broad range of local bending and torsion strengths. It is reasonable to argue that electrostatic interactions play a significant role in stabilizing and mediating structural transitions in polymers. We propose a bead-spring polymer model with randomly distributed charged monomers interacting via a screened Coulomb potential. By combining the Replica Exchange Wang-Landau (REWL) method with energy-dependent monomer updates, we constructed the hyperphase diagram as a function of temperature (T) and charged monomer concentration (77). The coil-globule and globular-solid transitions are second and first order for the entire concentration range. However, above a concentration threshold of 77 = 80%, electrostatic repulsion hinders the formation of solid and liquid globules, and the interplay between enthalpic and entropic interactions leads to the formation of liquid pearl-necklace and solid helical structures. The probability distribution, P(E, T), indicates that at high 77, the pearl-necklace liquid phase freezes into a stable solid helix-like structure with a free energy barrier higher than the freezing globule transition at low 77.

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