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A parametrization of the lattice spacing () in terms of the bare coupling () for the SU(3) Yang–Mills theory with the Wilson gauge action is given in a wide range of~. The Yang–Mills gradient flow with respect to the flow time~ for the dimensionless observable, $t\frac{d}{dt}t^2\langle E(t)\rangle$, is utilized to determine the parametrization. With fine lattice spacings () and large lattice volumes ($N_{\rm s}=64128$), the discretization and finite-volume errors are significantly reduced to the same level as the statistical error.

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