A new method is developed to combine the large-basis shell-model and Hartree-Fock methods. The Hartree-Fock method is used to obtain the absolute uncorrelated binding energies, a starting set of single-particle energies, and the single-particle radial wave functions. The shell model Hamiltonian is modified to remove the monopole terms and these are replaced by Hartree-Fock single-particle energies. The shell model is then used to calculate the ground-state correlation energy and the excited state spectrum. Applications are made to the nuclei ⁴⁷⁻⁻⁶⁰Ca. A detailed comparison is made for ⁴⁸Ca including the electron scattering data for ⁴⁸Ca.
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Brown et al. (1998) studied this question.
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