Phys. Rev. E 53, 5800 - 5807 (1996)

Bending-rigidity-driven transition and crumpling-point scaling of lattice vesicles

Download: PDF (158 kB) or Buy this Article (Use Article Pack) Export: BibTeX or EndNote (RIS)

E. Orlandini
Department of Physics, Theoretical Physics, University of Oxford, Oxford OX1 3NP, England

A. L. Stella
INFM-Dipartimento di Fisica e Sezione INFN, Università di Padova, I-35131 Padova, Italy

T. L. Einstein
Department of Physics, University of Maryland, College Park, Maryland 20742-4111

M. C. Tesi
Mathematical Institute, University of Oxford, Oxford OX1 3LB, England

I. Beichl
Computing and Applied Mathematics Laboratory, National Institute of Standards and Technology, Gaithersburg, Maryland 20899

F. Sullivan
Center for Computing Sciences, 17100 Science Drive, Bowie, Maryland 20715-4300

Received 11 August 1995

The crumpling transition of three-dimensional (3D) lattice vesicles subject to a bending fugacity ρ=exp(-κ/kBT) is investigated by Monte Carlo methods in a grand canonical framework. By also exploiting conjectures suggested by previous rigorous results, a critical regime with scaling behavior in the universality class of branched polymers is found to exist for ρ≳ρc. For ρ<ρc the vesicles undergo a first-order transition that has remarkable similarities to the line of droplet singularities of inflated 2D vesicles. At the crumpling point (ρ=ρc), which has a tricritical character, the average radius and the canonical partition function of vesicles with n plaquettes scale as nνc and nc, respectively, with νc=0.4825±0.0015 and θc=1.78±0.03. These exponents indicate a new class, distinct from that of branched polymers, for scaling at the crumpling point. © 1996 The American Physical Society.


©1996 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevE.53.5800
DOI: 10.1103/PhysRevE.53.5800
PACS: 64.60.Fr, 05.50.+q, 36.20.-r, 82.65.Dp

[ Abstract  |  Previous article  |  Next article  |  Issue 6 ]