Abstract

The radius of a nucleus is one of the important quantities in nuclear physics. Although there are many researches on ground-state properties of superheavy nuclei, researches on charge radii of superheavy nuclei are rare. In this article, nuclear root-mean-square (rms) charge radii of heavy and superheavy nuclei are extracted from the experimental $\ensuremath{\alpha}$-decay data. $\ensuremath{\alpha}$-decay calculations are performed within the generalized density-dependent cluster model, where $\ensuremath{\alpha}$-decay half-lives are evaluated using quasibound state wave functions. The charge distribution of daughter nuclei is determined in the double-folding model to reproduce the experimental $\ensuremath{\alpha}$-decay half-lives. The rms charge radius is then calculated using the resulting charge distribution. In addition, a simple formula is also proposed to calculate nuclear charge radii with the experimental $\ensuremath{\alpha}$-decay energies and half-lives. The formula is directly derived from the Wentzel-Kramers-Brillouin barrier penetration probability with some approximations. The two different methods show good agreement with the experimental data for even-even nuclei, and the deduced results are consistent with other theoretical models. Moreover, nuclear radii of heavy and superheavy nuclei with $Z=98$--116 are extracted from the $\ensuremath{\alpha}$-decay data, for which $\ensuremath{\alpha}$ decay is a unique tool to probe nuclear sizes at present. This is the first result on nuclear charge radii of superheavy nuclei based on the experimental $\ensuremath{\alpha}$-decay data.

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