2011/06/30 by J. Nieves, M. Pavon Valderrama, M. Pavón Valderrama · 6 citations
Mathematics · Physics and Astronomy · #Binding energy #Bound state #Energy (signal processing) #Isoscalar #Isovector #Mathematical analysis #Mathematical physics #Mathematics #Meson #Nuclear physics research studies #Nucleon #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quark #Upper and lower bounds #hep-ph #nucl-th
paper · pdf · doi:10.1103/physrevd.84.056015
21 pages, 3 figures; a sign error in the potential has been corrected and new predictions have been computed
arxiv created 2011/08/31 · openalex publication_date 2011/09/27 · arxiv updated 2015/05/28 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We discuss the possibility and the description of bound states between B and B* 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 DD* system and (iii) heavy quark symmetry. From these assumptions the binding energy of the possible BB* 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 3S1\ensuremath-3D1 state with a binding energy of 20 MeV and 6 MeV below threshold, respectively, and a positive C-parity 3P0 shallow state located almost at the BB* threshold. However, large uncertainties are generated as a consequence of the 1/mQ corrections from heavy quark symmetry. Finally, the newly discovered isovector Zb(10610) state can be easily accommodated within the present framework by a minor modification of the short-range dynamics.