Abstract
The effect of real and effective three-nucleon forces on the excitation spectra and wave functions has been studied for nuclei occurring at the beginning as well as the end of the 1s0d shell. The effects of these three-body terms are compared to those of a phenomenological mass-dependent two-nucleon interaction which has been fitted to describe excitation spectra for nuclei in the whole shell. The Glasgow shell-model code has been extended to incorporate a general three-body term in the effective hamiltonian.
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