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Exploring highly-deformed ground states involving the second intruder orbit in Z>50 even-even nuclei

Tsunenori Inakura, Wataru Horiuchi, Shin'ichiro Michimasa, Masaomi Tanaka

Abstract

We present a systematic survey of even-even nuclei with $Z>50$ to identify where a very large prolate configuration driven by the second intruder orbit emerges. Within the energy density functional theory framework, we find in representative cases a pronounced prolate minimum at quadrupole deformation $β_2\approx$ 0.3--0.4. A characteristic feature of these minima is a local enhancement of the hexadecapole ($β_4$) component relative to nearby deformations, which is a clear fingerprint of the $β_2$--$β_4$ coupling expected for the second intruder orbit. Representative comparisons among three Skyrme interactions show a similar appearance of the highly deformed minimum and a local enhancement of $β_4$ at the prolate minimum, indicating qualitative robustness with respect to the interaction. The resulting maps highlight specific heavy nuclei where highly deformed ground states are anticipated.

Exploring highly-deformed ground states involving the second intruder orbit in Z>50 even-even nuclei

Abstract

We present a systematic survey of even-even nuclei with to identify where a very large prolate configuration driven by the second intruder orbit emerges. Within the energy density functional theory framework, we find in representative cases a pronounced prolate minimum at quadrupole deformation 0.3--0.4. A characteristic feature of these minima is a local enhancement of the hexadecapole () component relative to nearby deformations, which is a clear fingerprint of the -- coupling expected for the second intruder orbit. Representative comparisons among three Skyrme interactions show a similar appearance of the highly deformed minimum and a local enhancement of at the prolate minimum, indicating qualitative robustness with respect to the interaction. The resulting maps highlight specific heavy nuclei where highly deformed ground states are anticipated.

Paper Structure

This paper contains 10 sections, 12 figures.

Figures (12)

  • Figure 1: Quadrupole deformation parameters $|\beta_2|$ of even-even nuclei from proton dripline to $N=126$ of Te ($Z=52$) to Hg ($Z=80$) isotopes as a function of the neutron number. For visibility, the $|\beta_2|$ values of each isotope is shifted by $0.05\times (Z-52)$ and oblate shapes ($\beta_2<0$) are represented by open symbols.
  • Figure 2: Hexadecapole deformation parameters $\beta_4$ of even-even nuclei from proton dripline to $N=126$ of Te ($Z=52$) to Hg ($Z=80$) isotopes as a function of the neutron number. For visibility, the $\beta_4$ values of each isotope is shifted by $0.05\times (Z-52)$.
  • Figure 3: (a) Proton and (b) neutron single-particle energies (s.p.e) and (c) deformation energies of $^{166}$Nd as a function of quadrupole deformation parameter $\beta_2$. Blue solid and red dashed curves in the panels (a) and (b) present negative and positive parity single-particle levels, respectively. Thick dashed curves denote the proton and neutron chemical potentials. A vertical dotted line indicates the $\beta_2$ value of the ground state for a guide to the eye.
  • Figure 4: Same as Fig. \ref{['pec.config.166Nd']} but for $^{138}$Gd.
  • Figure 5: Deformation energy curve for $^{272}$No obtained from axial HFB calculations with the HFBTHO solver, using an axially deformed harmonic-oscillator basis truncated at $N_{\max}=14$. Octupole deformation ($\beta_3$) is not included.
  • ...and 7 more figures