\begin{document}$ M_\odot $\end{document} NSs can occur simultaneously in DANSs. This stems from the ability of the equation of state (EOS) for DM to be very soft at low density but very stiff at high density. It is well known that the IU-FSU and XS models are unable to produce a neutron star (NS) with a maximum mass greater than 2.0 \begin{document}$ M_\odot $\end{document}. However, by considering the IU-FSU and XS models for DANSs, there are interactions with DM that can produce a maximum mass greater than 2.0 \begin{document}$ M_\odot $\end{document} and a radius of 1.4 \begin{document}$ M_\odot $\end{document} NSs below 13.7 km. When considering a DANS, the difference between DM with chiral symmetry (DMC) and DM with meson exchange (DMM) becomes obvious when the central energy density of DM is greater than that of nuclear matter (NM). In this case, the DMC model with a DM mass of 1000 MeV can still produce a maximum mass greater than 2.0 \begin{document}$ M_\odot $\end{document} and a radius of a 1.4 \begin{document}$ M_\odot $\end{document} NS below 13.7 km. Additionally, although the maximum mass of the DANS using the DMM model is greater than 2.0 \begin{document}$ M_\odot $\end{document}, the radius of a 1.4 \begin{document}$ M_\odot $\end{document} NS can surpass 13.7 km. In the two-fluid system, the maximum mass of a DANS can be larger than 3.0 \begin{document}$ M_\odot $\end{document}. Consequently, the dimensionless tidal deformability \begin{document}$ \Lambda_{CP} $\end{document} of a DANS with 1.4 \begin{document}$ M_\odot $\end{document}, which increases with increasing maximum mass, may be larger than 800 when the radius of the 1.4 \begin{document}$ M_\odot $\end{document} DANS is approximately 13.0 km."> Dark matter with chiral symmetry admixed with hadronic matterin compact stars -
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