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| Journal Article | PreJuSER-8552 |
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2009
Inst.
Woodbury, NY
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Please use a persistent id in citations: http://hdl.handle.net/2128/10452 doi:10.1103/PhysRevC.79.034309
Abstract: We have calculated the strength distributions of the isoscalar giant monopole resonance (ISGMR) in the even-A tin isotopes (A=112-124) that were recently measured in inelastic alpha scattering. The calculations were performed within two microscopic models: the quasiparticle random phase approximation (QRPA) and the quasiparticle time blocking approximation (QTBA), which is an extension of the QRPA including quasiparticle-phonon coupling. We used a self-consistent calculational scheme based on the Hartree-Fock+Bardeen-Cooper-Schrieffer approximation. Within the RPA the self-consistency is full. The single-particle continuum is also exactly included at the RPA level. The self-consistent mean field and the effective interaction are derived from the Skyrme energy functional. In the calculations, two Skyrme force parametrizations were used: T5 with a comparatively low value of the incompressibility modulus of infinite nuclear matter (K-infinity=202 MeV) and T6 with K-infinity=236 MeV. The T5 parametrization gives theoretical results for tin isotopes in good agreement with the experimental data including the resonance widths. The results of the ISGMR calculations in Zr-90, Sm-144, and Pb-208 performed with these Skyrme forces are discussed and compared with the experiment.
Keyword(s): J
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