2010
DOI: 10.1103/physrevlett.104.055702
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Accurate Estimate of the Critical Exponentνfor Self-Avoiding Walks via a Fast Implementation of the Pivot Algorithm

Abstract: We introduce a fast implementation of the pivot algorithm for self-avoiding walks, which we use to obtain large samples of walks on the cubic lattice of up to 33x10{6} steps. Consequently the critical exponent nu for three-dimensional self-avoiding walks is determined to great accuracy; the final estimate is nu=0.587 597(7). The method can be adapted to other models of polymers with short-range interactions, on the lattice or in the continuum.

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Cited by 197 publications
(285 citation statements)
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“…By fitting the power-law in logarithmic scale, one can obtain the values of ν listed in Table 1. As a comparison, with the renormalization group theory and Monte Carlo simulation, an accurate value of ν = 0.588 has been obtained [41,42]. Our results are in good agreement with this prediction as well as with previous CMD, BD and DPD simulations [17,20,43,44].…”
Section: Static Propertiessupporting
confidence: 79%
“…By fitting the power-law in logarithmic scale, one can obtain the values of ν listed in Table 1. As a comparison, with the renormalization group theory and Monte Carlo simulation, an accurate value of ν = 0.588 has been obtained [41,42]. Our results are in good agreement with this prediction as well as with previous CMD, BD and DPD simulations [17,20,43,44].…”
Section: Static Propertiessupporting
confidence: 79%
“…Polymers below the transition are compact globules and their radius of gyration R scales with their length as R~N 1/3 . Much above the transition temperature, the only relevant inter-monomer interaction is excluded volume and R Ñ n SAW , where ν SAW 0.587 is the exponent of three-dimensional selfavoiding walks 35 . Once again, due to the tricritical nature of the transition, characterized by mean-field values of the exponents in three dimensions, at the transition point ISAW polymers behave as ideal chains, with the radius of gyration R scaling as the square root of the number of monomers (R~N 1/2 ).…”
Section: Resultsmentioning
confidence: 99%
“…Pictorial representation of a confined polymer as a string of DeGennes' blobs is the three-dimensional self-avoiding walk scaling exponent [53]. At the same time, the string of blobs can be viewed as being a two-dimensional self-avoiding walk, with the blobs being the effective monomeric units of the walk.…”
Section: Metric Propertiesmentioning
confidence: 99%