In our previous papers we have proposed the peripheral orbit model by introducing a peripheral Regge trajectory in the direct channel. The radius and absorptivity of the orbit are related to Rea and Im a, respectively. The width of the orbit is introduced through the factor e(J, s) (O[exp(-2\IIJ/p)] as ReJ-->oo) and Ima. In this article the model is applied to exotic reactions into which no peripheral Regge trajectory can be introduced. The exotic forward reaction amplitudes are defined from their u-channel reaction amplitudes through analytic continuation. The imaginary parts of the exotic reaction amplitudes are shown to have non-peripheral components due to the analytic continuation of the factor e(J, s). The model is applied to n-p-tn°n, n-p->r;n, K+n--'>K0p and K-p--'>K 0 n. § l. Introduction In this article we discuss non-cliffractive two-body reactions. As is well known, the interaction between haclrons is strongly absorptive especially when the impact parameter of the collision is small. In spite of the strong absorption near the center, the interaction in the peripheral region is considerably transparent and an incoming hadron is assumed to revolve in a peripheral orbit around a target hadron if the interaction is attractive there. 1l' 'l In our pre,·ious papersn we have considered the reactions the u-channels of which are ec;:otic, i.e., x-p ;K_on and pj.J-->K-x-. The amplitudes of these re· actions receive contributions only from the resonances in the s-channel in the two component theory. 3l In this article we consider the reactions the u-channels of which are non-exotic, such as ;-:-jJ->7':071, ;-:-P->'ljn and J( n- > K 0j.J. The real parts of the amplitudes of these reactions receive contributions from the resonances in the u-channels. The model will be introduced in § 2 and will be applied to forward rr-j.J--+7r 0n, ;-:-p--+!Jn, x-n->K0p and x-p->K0n reactions at high energies (I tl <l.S(GeV)' and
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