“…For example, for 2/5 and 2/3, which both map into n = 2 of composite fermions, we have a fully spin polarized state (2, 0) (with γ = 1) and a spin singlet state (1, 1) (with γ = 0). To take another example, 6/13 and 6/11 map into n = 6, where we have four possible states (6, 0), (5, 1), (4,2) and (3,3), with γ = 1, 2/3, 1/3, and 0, respectively. One expects at most one transition at 2/5 and 2/3 and three at 6/13 and 6/11.…”