Microscopic models of the 21+and 31+states in24Mg and28Si and their test by inelastic scattering analyses

Nesci, P; Morrison, I.; Amos, K.

doi:10.1088/0305-4616/5/3/009

Cited by 3 publications

(1 citation statement)

References 27 publications

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“…The single-particle bound-state wave functions that complete the nuclear density matrices are harmonic oscillator (HO), Woods-Saxon (WS), or as given by the SHF studies [8,9]. For the inelastic scattering calculations, the no-core shell model was used to define the transition OBDME for the excitation of the 2 + 1 state in 12 C. For 2 + 1 transitions in the sd-shell nuclei, however, only projected Hartree-Fock (PHF) studies [10,11] have been made in a large enough basis to suit. There is an inconsistency in using SHF wave functions with PHF transition OBDME, but we can only await SHF studies giving excitation spectra and transition OBDME.…”

Section: Introductionmentioning

confidence: 99%

Microscopic model analyses of proton scattering from 12C, 20Ne, 24Mg, 28Si and 40Ca

Kim,

Amos,

Karataglidis

et al. 2007

Preprint

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Differential cross sections and analyzing powers for elastic scattering from, and for inelastic proton scattering to a set of 2 + 1 states in, 12 C, 20 Ne, 24 Mg, 28 Si and 40 Ca, and for a set of energies between 35 to 250 MeV, have been analyzed. A g-folding model has been used to determine optical potentials and a microscopic distorted wave approximation taken to analyze the inelastic data. The effective nucleon-nucleon interactions used to specify the optical potentials have also been used as the transition operators in the inelastic scattering processes. Shell and large space Hartree-Fock models of structure have been used to describe the nuclear states.

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