arXiv:1907.06093·v2·High Energy Physics — Phenomenology
Spin-parities of the and in the One-Boson-Exchange Model
Ming-Zhu Liu🇨🇳 · Tian-Wei Wu🇨🇳 · Mario Sánchez Sánchez🇫🇷 · Manuel Pavon Valderrama🇨🇳 · Li-Sheng Geng🇨🇳 · Ju-Jun Xie🇨🇳
Abstract
The LHCb collaboration has recently observed three pentaquark peaks, the , and . They are very close to a pair of heavy baryon-meson thresholds, with the located below the threshold, and the and located and below the one. The spin-parities of these three states have not been measured yet. In this work we assume that the is a bound state, while the and are bound states of unknown spin-parity, where we notice that the consistent description of the three pentaquarks in the one-boson-exchange model can indeed determine the spin and parities of the later, i.e. of the two molecular candidates. For this determination we revisit first the one-boson-exchange model, which in its original formulation contains a short-range delta-like contribution in the spin-spin component of the potential. We argue that it is better to remove these delta-like contributions because, in this way, the one-boson-exchange potential will comply with the naive expectation that the form factors should not have a significant impact in the long-range part of the potential (in particular the one-pion-exchange part). Once this is done, we find that it is possible to consistently describe the three pentaquarks, to the point that the and can be predicted from the within a couple of MeV with respect to their experimental location. In addition the so-constructed one-boson-exchange model predicts the preferred quantum numbers of the and molecular pentaquarks to be and , respectively.
Comments: 21 pages, 1 figure, 8 tables; discusses relation with EFT results; corresponds with published version