“…The resulting symmetry of the bound-exciton states is described by representations which are a direct product of the representation for Nb − (fully symmetric, 1 , or A 1 ) and one of the representations for the hole ( 4 or 56 ), i.e., just the same as that of the hole alone. At this point we do not know which of the three possible hole (and therefore exciton) states is lowest in energy (one of the two 4 states or the 56 state), but later we will see that the actual order is 4 , 56 , and 4 in order of ascending energies, with the former two states split by spin-orbit interaction, as depicted schematically in Fig. 3(b).…”