2012
DOI: 10.1007/s00601-012-0413-3
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The N = 16 Spherical Shell Closure in 24O

Abstract: The unbound excited states of the neutron drip-line isotope 24 O have been investigated via the 24 O(p,p ) 23 O+n reaction in inverse kinematics at a beam energy of 62 MeV/nucleon. The decay energy spectrum of 24 O * was reconstructed from the momenta of 23 O and the neutron. The spinparity of the first excited state, observed at Ex = 4.65 ± 0.14 MeV, was determined to be J π = 2 + from the angular distribution of the cross section. Higher-lying states were also observed. The quadrupole transition parameter … Show more

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Cited by 3 publications
(3 citation statements)
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“…For both the RMF and RHF theories, the meson masses and the meson-nucleon coupling strengths in the effective Hamiltonian (2) define the effective interactions (also referred to as effective Lagrangians); these are determined by fitting the bulk properties of nuclear matter and observable nuclei, such as 16 O, 40 Ca, 48 Ca, 56 Ni, 132 Sn, 208 Pb, and so on. More than that, the modeling of nuclear in-medium effects is also essential for an accurate description of nuclear properties; these are evaluated by considering the nonlinear self-couplings of mesons [113][114][115]120,121] or introducing the density dependence into the meson-nucleon coupling strengths [116][117][118][119]122].…”
Section: Effective Lagrangian and In-medium Effectsmentioning
confidence: 99%
See 1 more Smart Citation
“…For both the RMF and RHF theories, the meson masses and the meson-nucleon coupling strengths in the effective Hamiltonian (2) define the effective interactions (also referred to as effective Lagrangians); these are determined by fitting the bulk properties of nuclear matter and observable nuclei, such as 16 O, 40 Ca, 48 Ca, 56 Ni, 132 Sn, 208 Pb, and so on. More than that, the modeling of nuclear in-medium effects is also essential for an accurate description of nuclear properties; these are evaluated by considering the nonlinear self-couplings of mesons [113][114][115]120,121] or introducing the density dependence into the meson-nucleon coupling strengths [116][117][118][119]122].…”
Section: Effective Lagrangian and In-medium Effectsmentioning
confidence: 99%
“…This has greatly enriched nuclear science [1][2][3][4][5][6]. In contrast to the stable nuclei, numerous nuclear phenomena have been observed in the unstable nuclei, including the dilute matter distributions, the halo structure [7][8][9][10]; the emergence of new magicity and the disappearance of traditional magic shells [11][12][13][14][15][16][17][18]; and the occurrence of the central density depression, the bubble-like structure [19][20][21][22][23][24][25][26][27][28][29][30][31][32]; etc. These observations challenge our conventional understanding of nuclear physics.…”
Section: Introductionmentioning
confidence: 99%
“…Unstable nuclei far from the stability line in nuclear chart exhibit plenty of novel phenomena, for instance the emergence of new magic shells and the disappearance of the conventional ones [1][2][3][4][5][6][7], the island of inversion [8][9][10], and the dilute matter distributions -halo structures [11][12][13], which are attracting the interests of many researchers in the fields of nuclear physics and related disciplines. While enriching the knowledge of nuclear physics, the emergence of novelties in unstable nuclei has also subverted our traditional understanding of atomic nuclei.…”
Section: Introductionmentioning
confidence: 99%