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- W2324805506 abstract "The proton density distribution of $^{206}mathrm{Hg}$ is calculated in the framework of the Skyrme-Hartree-Fock approach with the SLy5, SLy5 + T, and SLy5 + ${mathrm{T}}_{w}$ interactions. It is shown that the central density drops strongly with the SLy5 and SLy5 + T interactions due to the vacancy of the $3{s}_{1/2}$ orbital. This means that the density depression in the interior of the nucleus is not so much influenced by the tensor force of the SLy5 + T interaction. However, with the SLy5 + ${mathrm{T}}_{w}$ interaction the bubble structure does not exist because the tensor force effect of this interaction leads to the inversion between the single-proton states $3{s}_{1/2}$ and $1{h}_{11/2}$ $(3{s}_{1/2}ensuremath{-}1{h}_{11/2}$ inversion) so that the $3{s}_{1/2}$ state is fully occupied by protons. In addition, a detailed discussion on the antibubble effect from the pairing interaction is performed by using the Skyrme-Hartree-Fock-Bogoliubov approach. It is found that a proton bubble structure in $^{206}mathrm{Hg}$ is unlikely to appear because of the paring correlation." @default.
- W2324805506 created "2016-06-24" @default.
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- W2324805506 date "2015-01-08" @default.
- W2324805506 modified "2023-10-17" @default.
- W2324805506 title "Effect of a tensor force on the proton bubble structure ofHg206" @default.
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- W2324805506 doi "https://doi.org/10.1103/physrevc.91.017302" @default.
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