Abstract

We study three-body systems composed of ${D}^{(*)}$, ${B}^{(*)}$, and ${\overline{B}}^{(*)}$ in order to look for possible bound states or resonances. In order to solve the three-body problem, we use the fixed center approach for the Faddeev equations considering that the ${B}^{*}{\overline{B}}^{*}(B\overline{B})$ are clusterized systems, generated dynamically, which interact with a third particle $D({D}^{*})$ whose mass is much smaller than the two-body bound states forming the cluster. In the $D{B}^{*}{\overline{B}}^{*}$, ${D}^{*}{B}^{*}{\overline{B}}^{*}$, $DB\overline{B}$, and ${D}^{*}B\overline{B}$ systems with $I=1/2$, we found clear bound state peaks with binding energies typically a few tens MeV and more uncertain broad resonant states about ten MeV above the threshold with widths of a few tens MeV.

Highlights

  • The heavy flavor sector has gained renewed attention in the last years by the hadron physics community, in part spurred by the wide increase of experimental results

  • In Ref. [59] it was justified that heavy quark symmetry implies that the value of the cutoff is independent of the heavy flavor, up to corrections of order Oð1=mQÞ, with mQ the mass of the heavy quark

  • We have investigated theoretically the three-body interactions DBÃB Ã, DBÃB Ã, DBB, and DÃBBtaking into account dynamical models for the DðÃÞBðÃÞ, DðÃÞBðÃÞ and BÃB ÃðBB Þ subsystems studied in previous works

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Summary

INTRODUCTION

The heavy flavor sector (both open and hidden) has gained renewed attention in the last years by the hadron physics community, in part spurred by the wide increase of experimental results (see Ref. [1] for a recent review). The three-body problem can be drastically simplified when two of the particles form a bound cluster which is not much altered by the interaction with the third particle In such a case one can resort to the so-called fixed center approximation (FCA) to the Faddeev equations [34,35,36,37,38]. In the present work we analyze the DBÃB Ã, DÃBÃB Ã, DBB , and DÃBBsystems with I 1⁄4 1=2 to look for possible bound and/or resonant three-body states In this case, the use of the FCA to evaluate the three-body scattering amplitude is suitable and appropriate since the BBand BÃB Ã systems in isospin I 1⁄4 0 were found to bind [13], forming states of mass about 10450 and 10 550 MeV, respectively. Since the I 1⁄4 1 amplitude is nonresonant one could expect a priori that the I 1⁄4 0 interaction will prevail, helping to bind the three-body state

THEORETICAL FRAMEWORK
RESULTS
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SUMMARY
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