Models of athermal self-avoiding fluid and polymerized vesicles have been investigated by Monte Carlo simulations. There is no evidence for crumpling of polymerized vesicles, and the squared radius of gyration is proportional to the number of monomers on the surface, R²{~}N. Fluid vesicles, on the other hand, exhibit a crumpled shape and R²{~}N0.8. We explain our model dynamics for fluid surfaces. The time-dependent mean-squared displacement r²(t) of a monomer on a fluid surface is {~}t0.8, whereas r²(t){~} {}t for polymerized vesicles. The corresponding configurational correlation times are {τ}{~}N for fluid and {τ}{~}N² for polymerized vesicles.
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Baumgärtner et al. (1990) studied this question.
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