The renormalization of the periodic potential is investigated in the framew
ork of the Euclidean one-component scalar field theory by means of the diff
erential RG approach. Some known results about the sine-Gordon model are re
covered in an extremely simple manner. There are two phases: an ordered one
with asymptotical freedom and a disordered one where the model is nonrenor
malizable and trivial. The order parameter of the periodicity, the winding
number, indicates spontaneous symmetry breaking in the ordered phase where
the fundamental group symmetry is broken and the solitons acquire dynamical
stability. It is argued that the periodicity and the convexity are such st
rong constraints on the effective potential that it always becomes flat. Th
is flattening is reproduced by integrating out the RG equation.