“…In πN elastic and charge exchange scattering, the excited states may have isospin I = 1/2 (N * ) and I = 3/2 (∆ * ). A large amount of data was analyzed by the groups at Karlsruhe-Helsinki (KH84) [10], Carnegie-Mellon (CM) [11] and at GWU [12]. The 1850 -2100 MeV mass region -where the missing resonances of the second excitation shell are predicted in most constituent quark models (see, e.g., [2,3,4,5,6,13,14]) -is dominated by the production of ∆ * resonances with spin-parity J P = 1/2 ± , 3/2 ± , 5/2 ± , 7/2 + ; nucleon resonances are difficult to establish in this mass range due to the overwhelming background from ∆ * resonances.…”