Deriving the existence of bound states from the X(3872) and Heavy Quark Symmetry
arXiv:1106.0600 · doi:10.1103/PhysRevD.84.056015
Abstract
We discuss the possibility and the description of bound states between and mesons. We argue that the existence of such a bound state can be deduced from (i) the weakly bound X(3872) state, (ii) certain assumptions about the short range dynamics of the system and (iii) heavy quark symmetry. From these assumptions the binding energy of the possible bound states is determined, first in a theory containing only contact interactions which serves as a straightforward illustration of the method, and then the effects of including the one pion exchange potential are discussed. In this latter case three isoscalar states are predicted: a positive and negative C-parity state with a binding energy of and below threshold respectively, and a positive C-parity shallow state located almost at the threshold. However, large uncertainties are generated as a consequence of the corrections from heavy quark symmetry. Finally, the newly discovered isovector state can be easily accommodated within the present framework by a minor modification of the short range dynamics.
21 pages, 3 figures; a sign error in the potential has been corrected and new predictions have been computed
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