<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mn>3872</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> production in relativistic heavy-ion collisions

Abstract

Heavy-ion collisions provide a unique opportunity to study the nature of X(3872) compared with electron-positron and proton-proton (antiproton) collisions. We investigate the centrality and momentum dependence of $X(3872)$ in heavy-ion collisions via the Langevin equation and instant coalescence model (LICM). When $X(3872)$ is treated as a compact tetraquark state, the tetraquarks are produced via the coalescence of heavy and light quarks near the quantum chromodynamic phase transition due to the restoration of the heavy quark potential at $T\ensuremath{\rightarrow}{T}_{c}$. In the molecular scenario, loosely bound $X(3872)$ is produced via the coalescence of ${D}^{0}\text{\ensuremath{-}}{\overline{D}}^{*0}$ mesons in a hadronic medium after kinetic freeze-out. We employ the LICM to explain both ${D}^{0}$ and $J/\ensuremath{\psi}$ production as a benchmark. Then we give predictions regarding $X(3872)$ production and the nuclear modification factor ${R}_{AA}^{X(3872)}$. We find that the total yield of tetraquark is several times larger than the molecular production in Pb-Pb collisions. Although the geometric size of the hadronic molecule is huge, the coalescence probability is small due to strict constraints on the relative momentum between ${D}^{0}$ and ${\overline{D}}^{*0}$ in the molecular Wigner function, which significantly suppresses the molecular yield.

Topics & Concepts