\begin{document}$ ^{208} $\end{document}Pb nucleus and its neighbors as daughters. The recently proposed universal cluster preformation formula has been established based on the concepts that underscore the influence of mass and charge asymmetry (\begin{document}$ \eta_A $\end{document} and \begin{document}$ \eta_Z $\end{document}), cluster mass \begin{document}$ A_c $\end{document}, and the Q-value, paving the way to quantify the energy contribution during preformation as well as during the tunneling process separately. The cluster-daughter interaction potential is obtained by folding the relativistic mean-field (RMF) densities with the recently developed microscopic R3Y using the NL\begin{document}$ 3^* $\end{document} and the phenomenological M3Y NN potentials to compare their adaptability. The penetration probabilities are calculated from the WKB approximation. With the inclusion of the new preformation probability \begin{document}$ P_0 $\end{document}, the predicted half-lives of the R3Y and M3Y interactions are in good agreement with the experimental data. Furthermore, a careful inspection reflects slight differences in the decay half-lives, which arise from their respective barrier properties. The \begin{document}$ P_0 $\end{document} for systems with double magic shell closure \begin{document}$ ^{208} $\end{document}Pb daughter are found to be an order of \begin{document}$ \approx 10^2 $\end{document} higher than those with neighboring Pb daughter nuclei. By exploring the contributions of the decay energy, the recoil effect of the daughter nucleus is evaluated, in contrast to several other conjectures. Thus, the centrality of the \begin{document}$Q$\end{document}-value in the decay process is demonstrated and redefined within the preformed cluster-decay model. Additionally, we have introduced a simple and intuitive set of criteria that governs the estimation of recoil energy in the cluster radioactivity."> Preformation probability and kinematics of cluster emission yielding Pb-daughters -
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