Abstract:We study hidden-charm pentaquarks in the baryon-meson molecule picture within the framework of the constituent quark model, considering all the possible quark configurations for the ground state. The strong decays of the Pc(4312), Pc(4440), and Pc(4457) resonances are investigated. It is found that pentaquark states of all quark configurations in the model can decay through the N J/ψ channel, but only five pentaquark states may decay dominantly in open-charm modes. The partial decay widths in the pηc channel a… Show more
“…c hadronic molecules dictated by HQSS presents itself, which has later been corroborated by many studies [13][14][15][16][17]. Although at present the molecular interpretation is the most favored one [13][14][15][16][17][18][19][20][21][22][23][24], there exist other explanations, e.g., hadro-charmonium [25], compact pentaquark states [26][27][28][29][30][31][32][33], virtual states [34] or double triangle singularities [35]. See Refs.…”
The three pentaquark states, P c (4312), P c (4440), and P c (4457), discovered by the LHCb Collaboration in 2019, can be nicely arranged into a multiplet of D( * ) Σ ( * ) c of seven molecules dictated by heavy quark spin
“…c hadronic molecules dictated by HQSS presents itself, which has later been corroborated by many studies [13][14][15][16][17]. Although at present the molecular interpretation is the most favored one [13][14][15][16][17][18][19][20][21][22][23][24], there exist other explanations, e.g., hadro-charmonium [25], compact pentaquark states [26][27][28][29][30][31][32][33], virtual states [34] or double triangle singularities [35]. See Refs.…”
The three pentaquark states, P c (4312), P c (4440), and P c (4457), discovered by the LHCb Collaboration in 2019, can be nicely arranged into a multiplet of D( * ) Σ ( * ) c of seven molecules dictated by heavy quark spin
This work presents an analysis of a hidden charmed pentaquark candidate state with double strange quark in its quark content. The investigation is performed in two parts, which provide the mass prediction of the considered state and its partial decay width for the Pcss → Ξ 0 J/ψ channel. For the analyses, two-point and three-point QCD sum rule methods are applied to get the mass and the width, respectively. The mass for this candidate state is obtained as mP css = 4600 ± 155 MeV with corresponding current coupling constant λP css = (0.81 ± 0.21) × 10 −3 GeV 6 . These results are used in the analysis of the partial width of this state for the decay Pcss → Ξ 0 J/ψ. For this decay, the width is obtained as Γ = 9.52 ± 2.85 MeV. These results may shed light on the future experimental searches in which such types of states are probed and may provide information to discriminate between such possible observations.
“…MeV, respectively. After the P c states were discovered, many groups tried to explain their structures within the molecular states assumption [3][4][5][6][7][8][9][10][11][12][13][14][15]. Meanwhile, other explanations were also tried, such as hadro-charmonium [16], compact pentaquark states [17][18][19][20][21][22][23][24], virtual states [25] and triangle singularities [26].…”
We study the magnetic moments and transition magnetic moments of P c and P cs states in the molecular picture. We first revisit the magnetic moments of P c states as the S wave molecular states without coupled channel effects. The coupled channel effects and the D wave contributions are then investigated carefully. The coupled channel effects contribute to the change of 0.1 ∼ 0.4 nuclear magneton µ N for most cases while the D wave only induces the variation of less than 0.03 µ N . In addition, we obtain the transition magnetic moments between different P c states and the related electromagnetic decay widths of P ′ c → P c γ. The magnetic moments of P cs are much different for the assumption of spin being 1/2 and 3/2. The study of electromagnetic properties will help us disclose further the structure of these unconventional states.
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