19 research outputs found

    Single-particle structure of the N = 20, 28 isotones within the dispersive optical model

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    The neutron single-particle characteristics of the N=20,28 N = 20, 28 isotones at 8<Z<30 8 < Z < 30 were calculated within the dispersive optical model. The global parameters of the spin-orbit and imaginary parts of the potential as well as surface absorption independent on neutron-proton asymmetry and increased diffuseness at large neutron excess were used in the calculations. The suitability of the global parameters to predict the evolution of the neutron single-particle structure of nuclei near the neutron drip line was investigated. The following results are in agreement with the available experimental data: the reduction of the particle-hole energy gaps, the degeneration of the 1f7/2 1f_{7/2} and 2p 2p states and then a change in the 1f7/2 1f_{7/2}, 2p3/2 2p_{3/2} level sequence and more rapid reduction of the 2p 2p-splitting in comparison with the 1f 1f-splitting with Z decreasing. The predictive power of the dispersive optical model with respect to neutron-rich nuclei is demonstrated

    Proton dispersive optical potential of even-even Sn isotopes with 100 ≤ A ≤ 132

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    Section III. Theory of Atomic Nucleus and Fundamental Interaction

    Proton dispersive optical potential of even-even Sn isotopes with 100 ≤ A ≤ 132

    No full text
    Section III. Theory of Atomic Nucleus and Fundamental Interaction

    Evolution of single-particle structure of silicon isotopes

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    New data on proton and neutron single-particle energies Enlj E_{nlj} of Si isotopes with neutron number N from 12 to 28 as well as occupation probabilities Nnlj N_{nlj} of single-particle states of stable isotopes 28, 30Si near the Fermi energy were obtained by the joint evaluation of the stripping and pick-up reaction data and excited state decay schemes of neighboring nuclei. The evaluated data indicate the following features of single-particle structure evolution: persistence of Z = 14 subshell closure with N increase, the new magicity of the number N = 16, and the conservation of the magic properties of the number N = 20 in Si isotopic chain. The features were described by the dispersive optical model. The calculation also predicts the weakening of N = 28 shell closure and demonstrates evolution of a bubble-like structure of the proton density distributions in neutron-rich Si isotopes

    Features of the proton single-particle spectra of Ni, Zn, and Ge isotopes near the proton drip-line

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    Section III. Theory of Atomic Nucleus and Fundamental Interaction
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