Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model
Recently, the LHCb Collaboration have updated their analysis of the resonant J/ψp mass spectrum in the decay Λb0→J/ψpK−. In the combined Run 1 and Run 2 LHCb data, three peaks are observed, with the former Pc(4450)+ state split into two narrow states, Pc(4440)+ and Pc(4457)+, having the masses M=(44...
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doaj-caa195f1b6a94355b3b6547344fdd8de2020-11-24T21:49:56ZengElsevierPhysics Letters B0370-26932019-06-01793365371Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark modelAhmed Ali0Alexander Ya. Parkhomenko1Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, GermanyDepartment of Theoretical Physics, P.G. Demidov Yaroslavl State University, Sovietskaya 14, 150003 Yaroslavl, RussiaRecently, the LHCb Collaboration have updated their analysis of the resonant J/ψp mass spectrum in the decay Λb0→J/ψpK−. In the combined Run 1 and Run 2 LHCb data, three peaks are observed, with the former Pc(4450)+ state split into two narrow states, Pc(4440)+ and Pc(4457)+, having the masses M=(4440.3±1.3−4.7+4.1) MeV and M=(4457.3±0.6−1.7+4.1) MeV, and decay widths Γ=(20.6±4.9+8.7−10.1) MeV and Γ=(6.4±2.0−1.9+5.7) MeV, respectively. In addition, a third narrow peak, Pc(4312)+, having the mass M=(4311.9±0.7−0.6+6.8) MeV and decay width Γ=(9.8±2.7−4.5+3.7) MeV is also observed. The LHCb analysis is not sensitive to broad J/ψp contributions like the former Pc(4380)+, implying that there could be more states present in the data. Also the spin-parity, JP, assignments of the states are not yet determined. We interpret these resonances in the compact diquark model as hidden-charm diquark-diquark-antiquark baryons, having the following spin and angular momentum quantum numbers: Pc(4312)+={c¯[cu]s=1[ud]s=0;LP=0,JP=3/2−}, the S-wave state, and the other two as P-wave states, with Pc(4440)+={c¯[cu]s=1[ud]s=0;LP=1,JP=3/2+} and Pc(4457)+={c¯[cu]s=1[ud]s=0;LP=1,JP=5/2+}. The subscripts denote the spins of the diquarks and LP=0,1 is the orbital angular momentum quantum number of the pentaquark. These assignments are in accord with the heavy-quark-symmetry selection rules for Λb-baryon decays, in which the spin S=0 of the light diquark [ud]s=0 is conserved. The masses of observed states can be accommodated in this framework and the two heaviest states have the positive parities as opposed to the molecular-like interpretations. In addition, we predict several more states in the J/ψp mass spectrum, and urge the LHCb Collaboration to search for them in their data.http://www.sciencedirect.com/science/article/pii/S0370269319303119 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Ahmed Ali Alexander Ya. Parkhomenko |
spellingShingle |
Ahmed Ali Alexander Ya. Parkhomenko Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model Physics Letters B |
author_facet |
Ahmed Ali Alexander Ya. Parkhomenko |
author_sort |
Ahmed Ali |
title |
Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model |
title_short |
Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model |
title_full |
Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model |
title_fullStr |
Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model |
title_full_unstemmed |
Interpretation of the narrow J/ψ p peaks in Λb → J/ψ p K− decay in the compact diquark model |
title_sort |
interpretation of the narrow j/ψ p peaks in λb → j/ψ p k− decay in the compact diquark model |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 |
publishDate |
2019-06-01 |
description |
Recently, the LHCb Collaboration have updated their analysis of the resonant J/ψp mass spectrum in the decay Λb0→J/ψpK−. In the combined Run 1 and Run 2 LHCb data, three peaks are observed, with the former Pc(4450)+ state split into two narrow states, Pc(4440)+ and Pc(4457)+, having the masses M=(4440.3±1.3−4.7+4.1) MeV and M=(4457.3±0.6−1.7+4.1) MeV, and decay widths Γ=(20.6±4.9+8.7−10.1) MeV and Γ=(6.4±2.0−1.9+5.7) MeV, respectively. In addition, a third narrow peak, Pc(4312)+, having the mass M=(4311.9±0.7−0.6+6.8) MeV and decay width Γ=(9.8±2.7−4.5+3.7) MeV is also observed. The LHCb analysis is not sensitive to broad J/ψp contributions like the former Pc(4380)+, implying that there could be more states present in the data. Also the spin-parity, JP, assignments of the states are not yet determined. We interpret these resonances in the compact diquark model as hidden-charm diquark-diquark-antiquark baryons, having the following spin and angular momentum quantum numbers: Pc(4312)+={c¯[cu]s=1[ud]s=0;LP=0,JP=3/2−}, the S-wave state, and the other two as P-wave states, with Pc(4440)+={c¯[cu]s=1[ud]s=0;LP=1,JP=3/2+} and Pc(4457)+={c¯[cu]s=1[ud]s=0;LP=1,JP=5/2+}. The subscripts denote the spins of the diquarks and LP=0,1 is the orbital angular momentum quantum number of the pentaquark. These assignments are in accord with the heavy-quark-symmetry selection rules for Λb-baryon decays, in which the spin S=0 of the light diquark [ud]s=0 is conserved. The masses of observed states can be accommodated in this framework and the two heaviest states have the positive parities as opposed to the molecular-like interpretations. In addition, we predict several more states in the J/ψp mass spectrum, and urge the LHCb Collaboration to search for them in their data. |
url |
http://www.sciencedirect.com/science/article/pii/S0370269319303119 |
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