Author(s)
| Allaman, Héloïse (EPFL, Lausanne, LPTP) ; Ekhterachian, Majid (EPFL, Lausanne, LPTP) ; Nardi, Filippo (EPFL, Lausanne, LPTP) ; Rattazzi, Riccardo (EPFL, Lausanne, LPTP ; New York U., CCPP ; CERN) ; Stelzl, Stefan (EPFL, Lausanne, LPTP) |
Abstract
| We study tetraquarks in large $N$ QCD with heavy quarks, in the domain where non-relativistic quantum mechanics offers an adequate approximation. Within the regime of validity of the Born-Oppenheimer approximation, we systematically study and explicitly construct tetraquark states. At leading order in the $1/N$ expansion, the bound spectrum consists of free mesons, while the $1/N$ corrections give rise to a Born-Oppenheimer potential that can bind the mesons into tetraquarks. We find two different types of tetraquarks, each endowed with distinct color-spatial wavefunctions. These states arise in the presence of an $\mathcal{O}(N)$ mass hierarchy between the quarks and the antiquarks. We provide a quantitative argument indicating that only for such a hierarchy is the ground state of the system a tetraquark. We discuss what the extrapolation of our results to realistic values of the parameters may imply for the QCD tetraquark states. |