Abstract
We have established a new convergent scheme to treat analytically nucleon–nucleon interactions from a chiral effective field theory. The Kaplan–Savage–Wise (KSW) amplitudes are resummed to fulfill the unitarity or right-hand cut to all orders below pion production threshold. This is achieved by matching order by order in the KSW power counting the general expression of a partial wave with resummed unitarity cut, with the inverses of the KSW amplitudes. As a result, a new convergent and systematic KSW expansion is derived for an on-shell interacting kernel R in terms of which the partial waves are computed. The agreement with data for the S-waves is fairly good up to laboratory energies around 350 MeV and clearly improves and reestablishes the phenomenological success of the KSW amplitudes when treated within this scheme.
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