Neutron single-particle strength in silicon isotopes: Constraining the driving forces of shell evolution
arXiv:1504.02329 · doi:10.1103/PhysRevC.91.041302
Abstract
Shell evolution is studied in the neutron-rich silicon isotopes 36,38,40 Si using neutron single-particle strengths deduced from one-neutron knockout reactions. Configurations involving neutron excita- tions across the N = 20 and N = 28 shell gaps are quantified experimentally in these rare isotopes. Comparisons with shell model calculations show that the tensor force, understood to drive the col- lective behavior in 42 Si with N = 28, is already important in determining the structure of 40 Si with N = 26. New data relating to cross-shell excitations provide the first quantitative support for repulsive contributions to the cross-shell T = 1 interaction arising from three-nucleon forces.
References in corpus (11)
- Nuclear magic numbers: new features far from stability
- Magic numbers in exotic nuclei and spin-isospin properties of {\it NN} interaction
- Novel features of nuclear forces and shell evolution in exotic nuclei
- Three-body forces and the limit of oxygen isotopes
- Collapse of the N=28 shell closure in Si
- Shape transitions in exotic Si and S isotopes and tensor-force-driven Jahn-Teller effect
- A new effective interaction for shell model calculations in the sdpf valence space
- The merging of the islands of inversion at N=20 and N=28
- Discovery of the shape coexisting 0+ state in 32Mg by a two neutron transfer reaction
- Three-body monopole corrections to the realistic interactions
- MOMDIS: a Glauber model computer code for knockout reactions
Cited by in corpus (4)
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- The calculation of single-nucleon energies of nuclei by considering two-body effective interaction, n(k,rho), and a Hartree-Fock inspired scheme