  It is shown that the explicit calculation of the Wess-Zumino functional
pertaining to the breaking term of the Weyl symmetry for the Einstein-Hilbert
action allows to restore the Weyl symmetry by introducing the extra dilaton
field as Goldstone field. Adding the Wess-Zumino counter-term to the
Einstein-Hilbert action reproduces the usual Weyl invariant action used in
standard literature. Further consideration might confer to the Einstein-Hilbert
action a new status.
