In this work we evaluate the $X(3872)$ to $ \psi (2S) $ yield ratio ($N_X/N_{ \psi(2S)}$) in Pb Pb collisions, taking into account the interactions of the $\psi (2S) $ and $ X(3872)$ states with light mesons in the hadron gas formed at the late stages of these collisions. We employ an effective Lagrangian approach to estimate the thermally-averaged cross sections for the production and absorption of the $\psi(2S)$ and use them in the rate equation to determine the time evolution of $N_{ \psi(2S)}$. The multiplicity of these states at the end of mixed phase is obtained from the coalescence model. The multiplicity of $X(3872)$, treated as a bound state of $(D\bar D^{ *} + c.c.)$ and also as a compact tetraquark, was already calculated in previous works. Knowing these yields, we derive predictions for the ratio ($N_X/N_{ \psi(2S)}$) as a function of the centrality, of the center-of-mass energy and of the charged hadron multiplicity measured at midrapidity $[dN_{ ch}/d\eta \,(\eta<0.5)]$. Finally, we make predictions for this ratio in Pb Pb collisions at $\sqrt{ s_{ NN}} = 5.02$ TeV to be measured by the ALICE Collaboration in the Run 3.
Categories: hep-ph nucl-th