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Abstract
Lattice computations of the high-temperature topological susceptibility of QCD receive lattice-spacing corrections and suffer from systematics arising from the type and depth of gradient flow. We study the lattice spacing corrections to \[\chi _\mathrm {top}\] semi-analytically by exploring the behavior of discretized Harrington–Shepard calorons under the action of different forms of gradient flow. From our study we conclude that \[N_\tau = 6\] is definitely too small of a time extent to study the theory at temperatures of order \[4~T_\mathrm {c}\] and we explore how the amount of gradient flow influences the continuum extrapolation.
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1 Institut für Kernphysik (Theoriezentrum), Technische Universität Darmstadt, Darmstadt, Germany
2 Institut für Kernphysik (Theoriezentrum), Technische Universität Darmstadt, Darmstadt, Germany; Max-Planck-Institut für Quantenoptik, Garching, Germany