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Description
The Bohr Hamiltonian [1,2] with a sextic potential, having two minima, a spherical and a deformed one separated by a barrier, was diagonalized in a basis of Bessel functions of the first kind [3]. The model, depending on the height of the potential barrier (Panels 1-4 of Figure 1 from [4]), can describe the well-known critical points from spherical vibrator to prolate / γ-unstable rotor if the barrier is very small / absent, a shape evolution as a function of the total angular momentum, respectively the shape coexistence and mixing phenomena once the barrier is gradually raised. Some preliminary applications of the model for 76Kr [4], 72,74,76Se [5], 96,98,100Mo [6], 74Ge, 74Kr [7] and 80Ge [8] revealed promising perspectives for future applications of the model to other nuclei known to manifest these phenomena.
1. A. Bohr, Mat. Fys. Medd. Dan. Vidensk. Selsk. 26 (1952) 14.
2. A. Bohr, B. R. Mottelson, Mat. Fys. Medd. Dan. Vidensk. Selsk. 27 (1953) 16.
3. R. Budaca, P. Buganu, A. I. Budaca, Phys. Lett. B 776 (2018) 26-31.
4. R. Budaca, A. I. Budaca, EPL 123 (2018) 42001.
5. R. Budaca, P. Buganu, A. I. Budaca, Nucl. Phys. A 990 (2019) 137-148.
6. R. Budaca, A. I. Budaca, P. Buganu, J. Phys. G: Nucl. Part. Phys. 46 (2019) 125102.
7. A. Ait Ben Mennana, R. Benjedi, R. Budaca, P. Buganu, Y. EL Bassem, A. Lahbas, M. Oulne, Phys. Scr. 96 (2021) 125306.
8. A. Ait Ben Mennana, R. Benjedi, R. Budaca, P. Buganu, Y. EL Bassem, A. Lahbas, M. Oulne, Phys. Rev. C 105 (2022) 034347.