2020
DOI: 10.1103/physrevlett.125.102502
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Shape Coexistence at Zero Spin in Ni64 Driven by the Monopole Tensor Interaction

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Cited by 30 publications
(20 citation statements)
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“…where e is the unit charge; e p (e n ) denotes proton (neutron) effective charge induced by inmedium (or core-polarization) effects; and R 0 stands for the radius parameter of the droplet model (spherical background) (see [73] for some detailed explanation). The relations in Equations ( 18) and ( 19) worked very well in many works, for instance [64,[69][70][71]. Figure 14c,d shows the T-plot for the original interaction, where the PES is shown by using β 2 and γ as coordinates (see Figure 14a).…”
Section: Shape Coexistence In 154 Smmentioning
confidence: 75%
See 1 more Smart Citation
“…where e is the unit charge; e p (e n ) denotes proton (neutron) effective charge induced by inmedium (or core-polarization) effects; and R 0 stands for the radius parameter of the droplet model (spherical background) (see [73] for some detailed explanation). The relations in Equations ( 18) and ( 19) worked very well in many works, for instance [64,[69][70][71]. Figure 14c,d shows the T-plot for the original interaction, where the PES is shown by using β 2 and γ as coordinates (see Figure 14a).…”
Section: Shape Coexistence In 154 Smmentioning
confidence: 75%
“…Type-II shell evolution occurs in various cases, especially in a number of shape coexistence cases, providing deformed states with stronger deformation, lower excitation energies, and more stabilities. It is an appearance of the monopole-quadrupole interplay and plays crucial roles in various phenomena including the first-order quantum phase transition (Zr isotopes [65][66][67]), the second-order quantum phase transition (Sn isotopes [68]), the multiple even-odd quantum phase transitions (Hg isotopes [69]), as well as the raising of the intruder band due to the suppression of the type-II shell evolution (lighter Ni isotopes [64,70]). As the involvement of the monopole interaction in this manner had not been recognized, type-II shell evolution appears to be among the emerging concepts of nuclear structure.…”
Section: Short Summary Of This Sectionmentioning
confidence: 99%
“…Let us take an example. Figure 12 [59] depicts the PES of 66 Ni with the same Hamiltonian as in Fig. 10.…”
Section: Tplot Analysismentioning
confidence: 99%
“…Type II shell evolution occurs in various cases, especially in a number of shape coexistence cases, providing deformed states with stronger deformation, lower excitation energies and more stabilities. It is an appearance of the monopolequadrupole interplay, and plays crucial roles in various phenomena including the first order phase transition (Zr isotopes [61][62][63]), the second order phase transition (Sn isotopes [64]), the multiple even-odd phase transitions (Hg isotopes [65]) as well as the raising of the intruder band due to the suppression of the type II shell evolution (lighter Ni isotopes [59,66]). As the involvement of the monopole interaction in this manner had not been recognized, Type II shell evolution appears to be among the emerging concepts of nuclear structure.…”
Section: E Short Summary Of Sec IIImentioning
confidence: 99%
“…Tentative spin assignments are shown by open symbols. Data are taken from the ENSDF database[34][35][36][37]. See text for details.…”
mentioning
confidence: 99%