\begin{document}$\sqrt{s_{_{NN}}}=7.77$\end{document} GeV. Given the sizable error of the fourth-order cumulant measured in the experiments, the calculation of MEM shows that with the increasing fourth-order cumulant, there is another peak in the distribution function developed in the region of the large baryon number. This unnaturalness observed in the reconstructed distribution function could in turn be used to constrain the cumulants measured in the experiments."> Reconstruction of baryon number distributions -
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