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A. N. Bezbakh

Publications and source records attributed to A. N. Bezbakh.

2 recordsLinked to original sources

Quasiparticle structure and $α$-decay scheme of nuclei along alpha-decay chain of $^{288}$Mc

Recent experiments on $α$-decay of odd-odd superheavy nuclei give an important information on the structure of the low-lying states of these nuclei. For this reason it is interesting to calculate the excitation spectra of these superheavy nuclei and compare the results with the experimental data. The aim of this work is to calculate the excitation energies of the two-quasiparticle states of nuclei belonging to the $α$-decay chain of $^{288}$Mc. The approximation of the noninteracting quasiparticles based on the Woods-Saxon single particle potentials is used. Different sets of deformation parameters are considered. The spectra of the low-lying two-quasiparticle states are calculated. The $α$-decay spectra of nuclei belonging to the $α$-decay chain of $^{288}$Mc are obtained and compared with the experimental data. A possibility of the $E1$ transitions in $^{276}$Mt and $^{272}$Bh following $α$-decay of $^{288}$Mc is considered. It is shown that the E1 transitions in $^{276}$Mt can be related to the transition $π[505]9/2\rightarrowπ[615]11/2$. In $^{272}$Bh the $E1$ transition can be related to the neutron single quasiparticle states.

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Level-density parameters in superheavy nuclei

We systematically study the nuclear level densities of superheavy nuclei, including odd systems, using the single-particle energies obtained with the Woods-Saxon potential diagonalization. Minimization over many deformation parameters for the global minima - ground states and the "imaginary water flow" technique on many deformation energy grids for the saddle points, including nonaxial shapes has been applied. The level density parameters are calculated by fitting the obtained results with the standard Fermi gas expression. The total potential energy and shell correction dependencies of the level-density parameter are analyzed and compared at the ground state and saddle point. These parameters are compared with the results of the phenomenological expression. As shown, this expression should be modified for the saddle points, especially for small excitation energy. The ratio of the level-density parameter at the saddle point to that at the ground state is shown to be crucial for the survival probability of the heavy nucleus.

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