“…In this way the E1 strength function of the one-neutron halo nucleus 11 Be can be explained using a simple two-body model with a Yukawa wave function (WF) for the initial state and plane waves in the final state [10,11]. However, for two-neutron halo nuclei, like 6 He, 11 Li, and 14 Be, a three-body picture is more appropriate but also more complicated. Microscopic three-cluster calculations of the E1 strength function were performed for, e.g., 6 He [9,12].…”