In order to search the dynamics to form the nucleon and the Roper resonance, a threechannel model consisting of rcN, u-N and the third channel is adopted, where the last channel is not specified explicitly. By adjusting elastic and. transition forces, this model is able to reproduce the nucleon mass, the rcN coupling constant, the phase shift and inelasticity up to 1440 MeV in C. M. energy fairly well, and the bending of the Argand loop near the top of the circle. In this situation, the pure elastic parts (the decoupled amplitudes) of the rcN and the third channels have bound states with nearly the same energy near the rcN threshold; the u-N channel has a resonance and is ~eakly coupled to rcN, but it causes large inelasticity in the low energy region and the bending of the Argand loop. The dynamical importance of the rcN and the other channels on the formation of the nucleon may be nearly equivalent. § 1. Introduction Recently, rcN phase shift analyses are much improved up to 2.2 Bev in invariantmass. 1 ),2)We may ragard these results not only as a tool to search new resonances and determine their parameters, but also as a clue to investigate the dynamics of the nucleon and low-lying resonances. A few years a'go, the zero of the P ll phase shift near the threshold and the existence of a resonance in P ll state were suggested by Roper,S) and these results have been confirmed in recent analyses. 4 ) Another interesting feature is found in the P ss phase shift which arises far above 90° and seems to pass 180°. These features of the P ll and PS3 phase shifts were quite unexpected from the Chew-Low reciprocal bootstrap modeP) in which the nucleon and the (3, 3)-resonqnce are regarded as the composite states of the rcN system constructed by the long range forces from the exchange of themselves.In this paper, we concentrate our' attention on the P ll state. It is possible to reproduce the phase shift qualitatively up to the Roper resonance region by adopting a model in which, in addition to the composite state of rcN, another channel forms one more compos'ite with the same quantum numbers as the nucleon. Then, the nucleon and the Roper resonance can be interpret~d as a mixture of these two composites. On the basis of the above picture, various works have been done. 6 ) ... 14) Some of them 9 ) ... 14) adopted multichannel models, and others 6 ) ..... S) . performed single channel calculations introducing a CDD pole or an elementary particle in the intermediate state in order to recover the equivalence with. multichannel situation. However, these works deal with only rather qualitative discussion and the dynamical understanding of the true situation is still not at