Abstract
The negative parity levels of odd-even nuclei with protons and neutrons in the 1f72 shell are calculated using the strong-coupling symmetric-rotator model including the Coriolis coupling between bands. The single-particle energy levels and wave functions in the deformed well are computed for a spin-orbit strength C=0.26ω0 which is consistent with the observed splitting in Ca41. The well-flattening parameter D is taken to be 0.06ω0 in the middle of the 1f72 shell and 0.035ω0 otherwise. The band-head energies are calculated from the appropriate summation over the occupied single-particle energy levels using ω0=41A13 MeV for the energy of the oscillator quantum. The moment of inertia is taken from the excitation energy of the first excited 2+ state of neighboring even-even nuclei assuming a rotational character for this state. The same value is used for all bands in any given nucleus. The matrix elements of the Coriolis coupling are computed from the single-particle wave functions. The final excitation spectra are obtained by diagonalizing the Coriolis coupling term with the rotational wave function based on the ten available particle or core excited states in the 1f2p shell. Energy levels and wave functions are calculated as a function of the deformation parameter β; the level spectrum for each individual nucleus is given for a tentative choice of β. The effect of a quenching of the Coriolis interaction on the calculated level spectrum is investigated. The computed level spectra for the nuclei (i) Sc43, Sc45, Sc47, (ii) Ca43, Ti45, V47, V49, V51, (iii) Ca45, Ti47, Cr49, Mn51, Mn53, and (iv) Ti49,

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