X(3872)X(3872) production from reactions involving DD and D∗D^* mesons

preprint2014arXivOpen access

Abstract

In this proceeding we show the results found for the cross sections of the processes DˉD→πX(3872)\bar D D\toπX(3872), Dˉ∗D→πX(3872)\bar D^* D\to πX(3872) and Dˉ∗D∗→πX(3872)\bar D^* D^*\toπX(3872), information needed for calculations of the X(3872)X(3872) abundance in heavy ion collisions. Our formalism is based on the generation of X(3872)X(3872) from the interaction of the hadrons Dˉ0D∗0−c.c\bar D^0 D^{*0} - \textrm{c.c}, D−D∗+−c.cD^- D^{*+} - \textrm{c.c} and Ds−Ds∗+−c.cD^-_s D^{*+}_s - \textrm{c.c}. The evaluation of the cross section associated with processes having D∗D^* meson(s) involves an anomalous vertex, XDˉ∗D∗X\bar D^* D^*, which we have determined by considering triangular loops motivated by the molecular nature of X(3872)X(3872). We find that the contribution of this vertex is important. Encouraged by this finding we estimate the XDˉ∗D∗X\bar D^* D^* coupling, which turns out to be 1.95±0.221.95\pm 0.22. We then use it to obtain the cross section for the reaction Dˉ∗D∗→πX\bar D^* D^*\toπX and find that the XDˉ∗D∗X\bar D^* D^* vertex is also relevant in this case. We also discuss the role of the charged components of XX in the determination of the production cross sections.

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