Abstract
The J=0,1,2 NN¯ππ amplitudes are evaluated in the physical region of the two pions, t4μ2, and used in a dispersion-theoretic calculation of nucleon-nucleon two-pion exchange. Experimental input to the evaluations of the NN¯ππ amplitudes is via ππ phase shifts, πN scattering lengths, and πN phase shifts. The effect of varying the I=J=0 ππ phase shift within its present uncertainty is investigated. Experimentally determined nucleon electromagnetic form factors are used in the evaluation of the J=1 NN¯ππ amplitude. After adding π and ω exchange to the two-pion-exchange amplitude, the theoretical phase shifts are compared with phase-shift-analysis results. The calculated S01 potential is also shown and compared with the phenomenological one of Hamada and Johnston.