Erratum: Effects of a chiral three-nucleon force on nucleus-nucleus scattering [Phys. Rev. C 90, 051601(R) (2014)]

Figure 1

Revised version of Fig. 1 in the original paper. $k_F$ dependence of the nucleon single-particle potential in each spin-isospin channel at $E=70\mathrm{MeV}$: (a) ${}^1\mathrm{O}$, (b) ${}^1\mathrm{E}$, (c) ${}^3\mathrm{E}$, and (d) ${}^3\mathrm{O}$ channels. The circles, squares, and triangles stand for the results of the chiral two-nucleon force (2NF) + 3NF, chiral 2NF, and Bonn-B 2NF, respectively. The closed (open) symbols correspond to the real (imaginary) part of the single-particle potentials. For ${}^3\mathrm{O}$, the imaginary part is shifted down by 10 MeV.

Figure 2

Revised version of Fig. 2 in the original paper. The folding potential for the ${}^{16}\mathrm{O}\text{−}{}^{16}\mathrm{O}$ elastic scattering at 70 MeV/nucleon. The real and imaginary parts of the potential are shown in the upper and lower panels, respectively. The solid (dashed) curve represents the result with (without) the 3NF effects.

Figure 3

Revised version of Fig. 3 in the original paper. The differential cross sections of (a) the ${}^{16}\mathrm{O}\text{−}{}^{16}\mathrm{O}$ elastic scattering at 70 MeV/nucleon and (b) the ${}^{12}\mathrm{C}\text{−}{}^{12}\mathrm{C}$ elastic scattering at 85 MeV/nucleon as a function of the scattering angle in the center-of-mass system. The solid (dashed) line corresponds to the result of Melbourne interaction with (without) the 3NF corrections. The experimental data are taken from Refs. [3, 4].