“…For such quantum numbers, the totally symmetric [6] orbital state is forbidden and therefore we expect a strong short-range repulsion induced by the Pauli principle. Such channels include BB ′ (S, I) = N ∆(1, 1), N ∆(2, 2), ∆∆(2, 3), ∆∆(3, 2), (∆Σ + ∆Σ * )(2, 5 2 ), ∆Σ * (3, 3 2 ), ∆Σ * (3, 5 2 ), and so on. On the other hand, many combinations of quantum numbers, particularly with lower spins, appear both in the [33] and [51] SU (6) sf representations.…”