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NSR database version of May 3, 2024.

Search: Author = K.Sugiura

Found 3 matches.

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2016NA24      Eur.Phys.J. A 52, 185 (2016)

H.Nakada, K.Sugiura, T.Inakura, J.Margueron

Can realistic interaction be useful for nuclear mean-field approaches?

NUCLEAR STRUCTURE 40,48,52,80Ca; calculated energy difference between p1s1/2 and sp0d3/2 states. Ca, Sn, Pb; calculated isotope shifts. M3Y-type semi-realistic interaction within mean-field approach. Compared with available data.

doi: 10.1140/epja/i2016-16185-y
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2014NA09      Prog.Theor.Exp.Phys. 2014, 033D02 (2014)

H.Nakada, K.Sugiura

Predicting magic numbers of nuclei with semi-realistic nucleon-nucleon interactions

NUCLEAR STRUCTURE N=6, 14, 16, 20, 28, 32, 34, 40, 50, 56, 58, 82, 90, 124, 126, 164, 184;Z=14, 16, 20, 28, 34, 38, 40, 50, 58, 64, 82, 92, 120, 124, 126; calculated nuclear properties, vanishing pair correlations in the spherical HFB regime; deduced magic numbers.

doi: 10.1093/ptep/ptu027
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2013NA17      Phys.Rev. C 87, 067305 (2013)

H.Nakada, K.Sugiura, J.Margueron

Tensor-force effects on single-particle levels and proton bubble structure around the Z or N=20 magic number

NUCLEAR STRUCTURE 34Si, 36S, 46Ar, 48Ca; calculated proton density distributions. Z=20, N=20-28, 40, 50; calculated single particle energy differences between 1s1/2 and 0d3/2 proton orbitals, tensor force effects. 34Si; possible proton bubble structure. Hartree-Fock (HF) and Hartree-Fock-Bogolyubov (HFB) calculations using semirealistic NN interactions including a realistic tensor force.

doi: 10.1103/PhysRevC.87.067305
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