$\Lambda\bar\Lambda$ final-state interaction in the reactions $e^+e^-\to \phi\Lambda \bar \Lambda$ and $e^+e^- \to \eta\Lambda \bar \Lambda$

Near-threshold $\Lambda\bar\Lambda$ mass spectra for the reactions $e^+e^- \to \eta\Lambda\bar\Lambda$ and $e^+e^- \to \phi\Lambda\bar\Lambda$ are investigated with an emphasis on the role played by the interaction in the $\Lambda\bar\Lambda$ system. A variety of $\Lambda\bar\Lambda$ potential models is employed that have been established in the analysis of data on $p\bar p\to \Lambda\bar\Lambda$ in the past. It is shown that the near-threshold enhancement observed for the two $e^+e^-$ reactions can be reproduced by considering the $\Lambda\bar\Lambda$ final-state interaction in the partial waves suggested by the helicity-angle analysis of the experiments. For $e^+e^- \to \eta\Lambda\bar\Lambda$ the same $\Lambda\bar\Lambda$ $S$-wave interaction as in $e^+e^- \to \Lambda\bar\Lambda$ is relevant and with it a consistent description of the pertinent measurements can be achieved. It is pointed out that a nonzero threshold cross section as observed for the latter reaction is not supported by the new $\eta\Lambda\bar\Lambda$ data.