Abstract
We compute , and the topological susceptibility, defined at finite gradient flow time for two-flavour QCD. The use of three lattice spacings and pion masses between 192 and 500 MeV together with a careful error analysis allow to approach the continuum limit of the two-flavour theory despite significant auto-correlations. A comparison to results shows the size of sea quark effects in , with the topological susceptibility, and low energy observables such as and .
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