\begin{document}$ 8\leqslant Z\leqslant128 $\end{document} and \begin{document}$ 8\leqslant N\leqslant251 $\end{document} in the framework of the WS-type model with RBFs correction. Simultaneously, the ground state deformations \begin{document}$ \beta_{2, \; 4, \; 6} $\end{document} and all parts in the WS-type mass formula are presented in this paper. Finally, we tabulated all calculated characteristics within the improved formula and linked them to https://github.com/lukeronger/NuclearData-LZU: nuclear binding energies, one-nucleon and two-nucleon separation energies (\begin{document}$ S_{\rm{n, \; p, \; 2n, \; 2p}} $\end{document}), \begin{document}$ \alpha $\end{document} and \begin{document}$ \beta $\end{document}-decay energies (\begin{document}$ Q_{\alpha} $\end{document} and \begin{document}$ Q_{\rm{\beta^-, \; \beta^+, \; EC}} $\end{document}), and the pairing gap \begin{document}$ \Delta_{\rm{n}} $\end{document} and \begin{document}$ \Delta_{\rm{p}} $\end{document}."> Basic characteristics of nuclear landscape by improved Weizsäcker-Skyrme-type nuclear mass model -
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