TY - JOUR
T1 - Quark model estimate of hidden-charm pentaquark resonances
AU - Hiyama, Emiko
AU - Hosaka, Atsushi
AU - Oka, Makoto
AU - Richard, Jean Marc
N1 - Funding Information:
The authors thank Prof.S. Takeuchi and Prof. M. Takizawa for valuable discussion. This work was supported by a JSPS-Japan-CNRS-France Joint Research Project and by the Grant-in-Aid for Scientific Research [Grants No. 25247036 and No. JP26400273(C)] from the Japan Society for the Promotion of Science.
Funding Information:
The authors thank Prof. S. Takeuchi and Prof. M. Takizawa for valuable discussion. This work was supported by a JSPS-Japan–CNRS-France Joint Research Project and by the Grant-in-Aid for Scientific Research [Grants No. 25247036 and No. JP26400273(C)] from the Japan Society for the Promotion of Science.
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/10/22
Y1 - 2018/10/22
N2 - A quark model, which reproduces the ground-state mesons and baryons, i.e., the threshold energies, is applied to the qqqcc configurations, where q is a light quark and c the charmed quark. In the calculation, several open channels are explicitly included such as J/ψ+N, ηc+N, Λc+D, etc. To distinguish genuine resonances and estimate their width, we employ the Gaussian expansion method supplemented by the real scaling method (stabilization). No resonance is found at the energies of the Pc(4380) and Pc(4450) pentaquarks. On the other hand, there is a sharp resonant state at 4690 MeV with a J=1/2- state and another one at 4920 MeV with a J=3/2- state which have a compact structure.
AB - A quark model, which reproduces the ground-state mesons and baryons, i.e., the threshold energies, is applied to the qqqcc configurations, where q is a light quark and c the charmed quark. In the calculation, several open channels are explicitly included such as J/ψ+N, ηc+N, Λc+D, etc. To distinguish genuine resonances and estimate their width, we employ the Gaussian expansion method supplemented by the real scaling method (stabilization). No resonance is found at the energies of the Pc(4380) and Pc(4450) pentaquarks. On the other hand, there is a sharp resonant state at 4690 MeV with a J=1/2- state and another one at 4920 MeV with a J=3/2- state which have a compact structure.
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U2 - 10.1103/PhysRevC.98.045208
DO - 10.1103/PhysRevC.98.045208
M3 - Article
AN - SCOPUS:85055861427
SN - 2469-9985
VL - 98
JO - Physical Review C
JF - Physical Review C
IS - 4
M1 - 045208
ER -