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, Schematic representation of the spontaneous symmetry breaking, p.40
, Convergence of the RHB energies in 20 Ne with the size of harmonic oscil, p.61
, Convergence of the AMP energies in 20 Ne with the number of discretization points in projection integral for even-positive spin-parities, p.62
, Convergence of the AMP energies in 20 Ne with the number of discretization points in projection integral for odd-negative spin-parities, p.63
, Convergence of the AMP and PNP energies in 20 Ne with the number of discretization points in projection integrals for even-positive spin-parities, vol.64
, Convergence of the AMP and PNP energies in 20 Ne with the number of discretization points in projection integrals for odd-negative spin-parities 65
, Convergence of the AMP and PNP energies of the 2 + 1 state in 20 Ne for a very large number of discretization points in projection integrals, p.67
Excitation energies of collective states in 20 Ne as a function of the number of considered norm overlap eigenstates ,
Self-consistent RHB binding energies of even-even 20?34 Ne isotopes, in the ? 2 ? ? 3 plane ,
, Intrinsic nucleon densities of 20 Ne. Densities corresponding to the selfconsistent minimum and to the symmetry-restored minimum are shown, p.75
, Angular momentum-, particle number-, and parity-projected energy surfaces of even-even 20?34 Ne isotopes for J ? = 0 + in the ? 2 ? ? 3 plane, p.76
, List of Figures LIST OF FIGURES
, Two-neutron separation energies of 22?34 Ne isotopes on SR-EDF and MREDF level in comparison with the experimental data, p.77
? 3 )| 2 of the ground states of 20?34 Ne isotopes in the ? 2 ? ? 3 plane, Amplitudes of collective wave functions squared |g ,
Ground-state deformation parameters ? 2 and ? 3 of 20?34 Ne isotopes on the SR-EDF and MR-EDF level ,
, Angular momentum-, particle number-, and parity-projected energy surfaces of even-even 20?34 Ne isotopes for J ? = 2 + in the ? 2 ? ? 3 plane, p.81
, Angular momentum-, particle number-, and parity-projected energy surfaces of even-even 20?34 Ne isotopes for J ? = 4 + in the ? 2 ? ? 3 plane, p.81
, 82 4.10 Angular momentum-, particle number-, and parity-projected energy surfaces of even-even 20?34 Ne isotopes for J ? = 3 ? in the ? 2 ? ? 3 plane, p.82
, in even-even 20?34 Ne isotopes compared with data, p.83
, Calculated low-energy spectra of 22,24 Ne and 32,34 Ne isotopes, p.84
? 3 )| 2 of the lowenergy levels in 22 Ne, Amplitudes of collective wave functions squared |g ,
? 3 )| 2 of the lowenergy levels in 24 Ne, Amplitudes of collective wave functions squared |g ,
? 3 )| 2 of the lowenergy levels in 32 Ne, Amplitudes of collective wave functions squared |g ,
86 4.17 Calculated low-energy spectrum of 20 Ne compared with the available experimental data and with predictions of two other theoretical models, Amplitudes of collective wave functions squared |g, p.88 ,
? 3 )| 2 of the lowenergy levels of 20 Ne, Amplitudes of collective wave functions squared |g ,
Characteristic intrinsic nucleon densities of collective states of the groundstate band and the K ? = 0 ? band in 20 Ne ,
, Self-consistent RHB energy surface and angular momentum-, particle numberand parity-projected energy surfaces of 12 C isotope in ? 2-? 3 plane, p.97
Potential energy curves of 12 C isotope as functions of axial quadrupole deformation ? 2 for parity-conserving (? 3 = 0) configurations, p.98 ,
3 Calculated low-energy spectrum of 12 C compared with the available experimental data ,
? 3 )| 2 of the lowenergy levels in 12 C, Amplitudes of collective wave functions squared |g ,
Characteristic intrinsic nucleon densities of the first three 0 + and 2 + collective states in 12 C ,
, , vol.18
, Properties of nuclear symmetries that are broken and restored within our calculation: rotational, particle number, and parity invariance, p.41
74 4.2 Calculated ground-state band spectroscopic quadrupole moments in the even-even 20?34 Ne isotopes, RHB values of deformation parameters, binding energies, and charge radii in ground states of 20?34 Ne isotopes ,