The 2d Heisenberg model --- or 2d O(3) model --- is popular in condensed matter physics, and in particle physics as a toy model for QCD. Along with other analogies, it shares with 4d Yang-Mills theories, and with QCD, the property that the configurations are divided in topological sectors. In the lattice regularisation the topological charge $Q$ can still be defined such that $Q in mathbb{Z}$. It has generally been observed, however, that the topological susceptibility $chi_{rm t} = langle Q^2 rangle / V$ does not scale properly in the continuum limit, i.e. that the quantity $chi_{rm t} xi^2$ diverges for $xi to infty$ (where $xi$ is the correlation length in lattice units). Here we address the question whether or not this divergence persists after the application of the Gradient Flow.
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