We use single-cluster Monte Carlo simulations to study the role of topological defects in the three-dimensional classical Heisenberg model on simple cubic lattices of size up to . By applying reweighting techniques to time series generated in the vicinity of the approximate infinite volume transition point , we obtain clear evidence that the temperature derivative of the average defect density behaves qualitatively like the specific heat, i.e., both observables are finite in the infinite volume limit. This is in contrast to results by Lau and Dasgupta [{\em Phys. Rev./} {\bf B39} (1989) 7212] who extrapolated a divergent behavior of at from simulations on lattices of size up to . We obtain weak evidence that scales with the same critical exponent as the specific heat.As a byproduct of our simulations, we obtain a very accurate estimate for the ratio of the specific-heat exponent with the correlation-length exponent from a finite-size scaling analysis of the energy.

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