Erratum: Three-cluster dynamics within an ab initio framework [Phys. Rev. C 88, 034320 (2013)]

Figure 7

Probability distribution of the main component of the ${}^4\mathrm{He}+n+n$ relative motion wave function for the $J^{\pi }T=0^{+}1$ ground state. The quantum numbers corresponding to this component are $S=L={\ell }_x={\ell }_y=0$. Here $r_{nn}=\sqrt{2}{\eta }_{nn}$ and $r_{\alpha ,nn}=\sqrt{3/4}{\eta }_{\alpha ,nn}$, respectively, are the distance between the two neutrons and the distance between the c.m. of ${}^4\mathrm{He}$ and that of the two neutrons.

Figure 8

Contour diagram of the probability distribution plotted in Fig. 7.

Figure 9

Same as Fig. 7 but for the second most important component. The quantum numbers corresponding to this component are $S=L={\ell }_x={\ell }_y=1$.