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Bohr Hamiltonian with a deformation-dependent mass term for the Kratzer potential

Dennis BonatsosInstitute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos,” GR-15310 Aghia Paraskevi, Attiki, GreeceP. E. GeorgoudisInstitute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos,” GR-15310 Aghia Paraskevi, Attiki, GreeceN. MinkovInstitute of Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, 72 Tzarigrad Road, 1784 Sofia, BulgariaD. PetrellisInstitute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos,” GR-15310 Aghia Paraskevi, Attiki, GreeceC. QuesnePhysique Nucléaire Théorique et Physique Mathématique, Université Libre de Bruxelles, Campus de la Plaine CP229,Boulevard du Triomphe, B-1050 Brussels, Belgium
2013en
ABI

Аннотация

The deformation-dependent mass Kratzer model is constructed by considering the Kratzer potential in a Bohr Hamiltonian, in which the mass is allowed to depend on the nuclear deformation, and solving it by using techniques of supersymmetric quantum mechanics (SUSYQM), involving a deformed shape invariance condition. Analytical expressions for spectra and wave functions are derived for separable potentials in the cases of $\ensuremath{\gamma}$-unstable nuclei, axially symmetric prolate deformed nuclei, and triaxial nuclei, implementing the usual approximations in each case. Spectra and $B(E2)$ transition rates are compared to experimental data. The dependence of the mass on the deformation, dictated by SUSYQM for the potential used, moderates the increase of the moment of inertia with deformation, removing a main drawback of the model.

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