Background: The (spin and isospin zero) α-particle is an efficient projectile for the excitation of the isoscalar, natural-parity states of 12 C. Among those states that have pronounced α-cluster structure, the Hoyle state (0 + 2 state at 7.65 MeV) has been observed in many (α, α ) experiments while the second 2 + state of 12 C, predicted at E x ≈ 10 MeV as an excitation of the Hoyle state, has not been observed until a recent high-precision experiment of the α+ 12 C scattering at E α = 386MeV. A plausible reason is a strong population of the narrow 3 state in the (α, α ) spectra measured at E α = 240 and 386 MeV has been consistently confirmed by the present folding model + coupled channel analysis.