In this contribution, we report on our study of the properties of the Wilson flow and on the calculation of the topological susceptibility of gauge theories for . The Wilson flow is shown to scale according to the quadratic Casimir operator of the gauge group, as was already observed for , and the commonly used scales and are obtained for a large interval of the inverse coupling for each probed value of . The continuum limit of the topological susceptibility is computed and we conjecture that it scales with the dimension of the group. The lattice measurements performed in the Yang-Mills theories by several independent collaborations allow us to test this conjecture and to obtain a universal large- limit of the rescaled topological susceptibility.

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