\begin{document}$ \phi\phi $\end{document}, \begin{document}$ D^0 $\end{document}\begin{document}$ D^0 $\end{document}, and \begin{document}$ K^+ $\end{document}\begin{document}$ K^+ $\end{document}. The squeezing effect suppresses the impact of transverse flow on the transverse source distribution and broadens the space-time rapidity distribution of the particle-emitting source, leading to an increase in the HBT radii, particularly in the out and longitudinal directions. This phenomenon becomes more significant for higher transverse pair momentum, resulting in a non-monotonic decrease in the HBT radii with increasing transverse pair momentum. The impact of the squeezing effect on the HBT radii is more pronounced for \begin{document}$ D^0 $\end{document}\begin{document}$ D^0 $\end{document} than for \begin{document}$ \phi\phi $\end{document}. Furthermore, this effect is also more significant for ϕϕ than for \begin{document}$ K^+ $\end{document}\begin{document}$ K^+ $\end{document}. The findings presented in this paper could offer fresh perspectives on investigating the squeezing effect."> Squeezing effect on three-dimensional Hanbury Brown-Twiss radii -
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