The new mechanism for intermediate- and short-range nucleon-nucleon interaction
arXiv:nucl-th/9912074 · doi:10.1088/0954-3899/27/9/301
Abstract
Arguments against the traditional Yukawa-type approach to intermediate- and short-range interaction due to scalar-isoscalar meson exchange are presented. Instead of the Yukawa mechanism for intermediate-range attraction some new approach based on formation of the symmetric six-quark bag in the state dressed due to strong coupling to , and fields are suggested. These new mechanism offers a strong intermediate-range attraction which replaces the effective -exchange (or excitation of two isobars in the intermediate state) in traditional force models. A similar mechanism with vector -meson production in the intermediate six-quark state is expected to lead to a strong short-range spin-orbital nonlocal interaction in the system, which may resolve the long-standing puzzle of the spin-orbit force in baryons and in two-baryon systems. Illustrative examples are developed which demonstrate clearly how well the suggested new model can reproduce data. Strong interrelations have been shown to exist between the proposed microscopic model and the one-component Moscow potential developed by the authors previously and also with some hybrid models and the one-term separable Tabakin potential. The new implications of the proposed model for nuclear physics are discussed.
56 pages, 10 Postscript figures, corrected formulas and figures
References in corpus (7)
- Exchange in the NN Interaction within the Chiral Unitary Approach
- Low energy n+t scattering and the NN forces
- Investigation of the Exclusive 3He(e,e'pp)n Reaction
- One-loop Reggeon-Reggeon-gluon vertex at arbitrary space-time dimension
- Nucleon-nucleon scattering in a chiral constituent quark model
- The piNN vertex function in a meson-theoretical model
- Hadronic Invariant Mass Spectrum in B -> X_u l nu Decay with Lepton Energy Cut
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