“…Charge-exchange reactions, however, can map the GT strength distributions over a wider range of excitation energies. A variety of charge-changing reactions can be employed, for example, A Z(p, n) A (Z+1) [423,171], A Z(n, p) A (Z − 1) [424], A Z(d, 2 He) A (Z − 1) [425], A Z( 3 He, t) A (Z + 1) [426][427][428][429], and A Z(t, 3 He) A (Z − 1) [430][431][432][433]. In chargeexchange reactions at beam energies exceeding 100 MeV/nucleon, the cross-section at low momentum transfer (small angles) is proportional to the B(GT ) transition strength [434][435][436]171,173].…”