 Solution

A Wilsonian renormalization group step first splits the field into slow and fast Fourier modes and integrates out the shell $\Lambda /b<|k|<\Lambda$. It then rescales coordinates, or momenta, to restore the cutoff to $\Lambda$, and finally rescales the field to normalize the kinetic term. The resulting local effective free energy has the same allowed operators with changed coefficients. Repeating the operation therefore composes maps on the set of couplings and defines a renormalization-group flow.