Abstract

We show that the assumption of dropping meson masses together with conventional many-body effects, implemented in the relativistic Dirac-Brueckner formalism, explains nuclear saturation. We use a microscopic model for correlated 2π2\pi exchange and include the standard many-body effects on the in-medium pion propagation, which initially increase the attractive nucleon-nucleon (NNNN) potential with density. For the vector meson exchanges in both the ππ\pi\pi and NNNN sector, we assume Brown-Rho scaling which---in concert with `chiral' ππ\pi\pi contact interactions---reduces the attraction at higher densities.Comment: 5 pages REVTeX, 2 eps-figures included, submitted to Phys. Rev. Let

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    Last time updated on 01/04/2019