Abstract
Brueckner-Hartree-Fock calculations on $^{16}\mathrm{O}$ are presented using a one-boson-exchange potential, which includes the $\ensuremath{\Delta}(1236)$ resonance in all partial waves. The repulsive effect from the explicit treatment of the $\ensuremath{\Delta}$ is considerably weaker than for the nuclear matter system. This density dependence of the repulsion leads to $\mathrm{NN}$ interactions, which may describe the energies of finite nuclei as well as of nuclear matter.
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