Abstract

In the framework of heavy baryon chiral perturbation theory, we give thIn the framework of heavy baryon chiral perturbation theory, we give the chiral expansion for the πNππN\pi N \to \pi \pi N threshold amplitudes D1D_1 and D2D_2 to quadratic order in the pion mass. The theoretical results agree within one standard deviation with the empirical values. We also derive a relation between the two threshold amplitudes of the reaction πNππN\pi N \to \pi \pi N and the ππ\pi \pi S--wave scattering lengths, a00a_0^0 and a02a_0^2, respectively, to order O(Mπ2){\cal O}(M_\pi^2). We show that there are uncertainties mostly related to resonance excitation which make an accurate determination of the ππ\pi \pi scattering length a00a_0^0 from the ππN\pi \pi N threshold amplitudes at present very difficult. The situation is different in the ππ\pi \pi isospin two final state. Here, the chiral series converges and one finds a02=0.031±0.007a_0^2 = -0.031 \pm 0.007 consistent with the one--loop chiral perturbation theory prediction.Comment: 30 pp, LaTeX file, uses epsf, 6 figures (appended), corrections in sections 5 and 6, conclusions unchange

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    Last time updated on 11/12/2019