Writing 〈${\mathit{R}}_{\mathit{N}}^{2}$〉= ${\mathit{AN}}^{2\ensuremath{\nu}}$(1+${\mathit{BN}}^{\mathrm{\ensuremath{-}}{\mathrm{\ensuremath{\Delta}}}_{1}}$+${\mathit{CN}}^{\mathrm{\ensuremath{-}}1}$+\ensuremath{\cdot}\ensuremath{\cdot}\ensuremath{\cdot}) for the mean square end-to-end length 〈${\mathit{R}}_{\mathit{N}}^{2}$〉 of a self-avoiding polymer chain of N links, we have calculated ${\mathrm{\ensuremath{\Delta}}}_{1}$ for the two-dimensional continuum case from a finite perturbation method based on the ground state of Edwards self-consistent solution which predicts the (exact) \ensuremath{\nu}=3/4 exponent. This calculation yields ${\mathrm{\ensuremath{\Delta}}}_{1}$=1/2. A finite-size scaling analysis of data generated for the continuum using a biased sampling Monte Carlo algorithm supports this value, as does a reanalysis of exact data for two-dimensional lattices. \textcopyright{} 1996 The American Physical Society.
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