  We describe the formation of superconducting states in graphene in the
presence of pseudo-Landau levels induced by strain, when time reversal symmetry
is preserved. We show that superconductivity in strained graphene is quantum
critical when the pseudo-Landau levels are completely filled, whereas at
partial fillings superconductivity survives at weak coupling. In the weak
coupling limit, the critical temperature scales \emph{linearly} with the
coupling strength and shows a sequence of quantum critical points as a function
of the filling factor that can be accessed experimentally. We argue that
superconductivity can be induced by electron-phonon coupling and that the
transition temperature can be controlled with the amount of strain and with the
filling fraction of the Landau levels.
