Abstract <p>The single-particle structure of near-spherical superheavy nuclei from the region <i>Z</i> ≤ 126, <i>N</i> ≤ 246 and a hypothetical hyperheavy nucleus <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({}_{{308}}^{{472}}164\)</EquationSource> <!--BullPhys2670051Bespalova-m1--> </InlineEquation> was studied in the dispersive optical model. The calculation results correspond to the magic numbers <i>N</i> = 126, 148, 164, 178, 184, 228, and 246 and <i>Z</i> = 82, 92, 114, 120, and 126 and the double magicity of the <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({}_{{308}}^{{472}}164\)</EquationSource> <!--BullPhys2670051Bespalova-m2--> </InlineEquation> nucleus. The neutron density distribution shows depletion in the center (semibubble structure) at 164 ≤ <i>N</i> ≤ 178, and the proton density distribution shows depletion at <i>r</i> ≈ 2 fm at 114 ≤ <i>Z</i> ≤ 120. The proton density depletion of the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({}_{{308}}^{{472}}164\)</EquationSource> <!--BullPhys2670051Bespalova-m3--> </InlineEquation> nucleus affects almost the entire volume of the nucleus unlike in superheavy nuclei and increases toward the center of the nucleus starting from the periphery.</p>

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Single-Particle Structure of Superheavy Nuclei in the Dispersive Optical Model

  • O. V. Bespalova,
  • A. A. Klimochkina,
  • M. M. Mosunov

摘要

Abstract

The single-particle structure of near-spherical superheavy nuclei from the region Z ≤ 126, N ≤ 246 and a hypothetical hyperheavy nucleus \({}_{{308}}^{{472}}164\) was studied in the dispersive optical model. The calculation results correspond to the magic numbers N = 126, 148, 164, 178, 184, 228, and 246 and Z = 82, 92, 114, 120, and 126 and the double magicity of the \({}_{{308}}^{{472}}164\) nucleus. The neutron density distribution shows depletion in the center (semibubble structure) at 164 ≤ N ≤ 178, and the proton density distribution shows depletion at r ≈ 2 fm at 114 ≤ Z ≤ 120. The proton density depletion of the \({}_{{308}}^{{472}}164\) nucleus affects almost the entire volume of the nucleus unlike in superheavy nuclei and increases toward the center of the nucleus starting from the periphery.