  We review the Lorentz integral transform coupled-cluster method for the
calculation of the electric dipole polarizability. We benchmark our results
with exact hyperspherical harmonics calculations for 4He and then we move to a
heavier nucleus studying 16O. We observe that the implemented chiral
nucleon-nucleon interaction at next-to-next-to-next-to-leading order
underestimates the electric dipole polarizability.
