“…The latter constitute an almost unexplored territory, ideal for investigations with AGATA coupled to light charged-particle detectors, using intense stable beams. For example, reactions such as 6,7 Li on 6,7 Li, 9 Be, 10,11 B, and 12,13 C targets, will lead, after a single proton evaporation, to the population of unbound states in 13 B, 15 C, 17,19 O, and 16,17 N, respectively. Shape coexistence occurs when different microscopic configurations correspond to similar binding energies, as illustrated by the wave functions of 0 + states in the neutron-rich krypton isotopes beyond N = 60 (left), where oblate and prolate shapes are expected to coexist.…”