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The strange pentaquarks with hidden heavy quark pair ($q^3c\bar c$ and $q^3b \bar b$) are investigated by the coupled-channel quark cluster model. Two types of the $q^3$ color-octet configurations are found to provide the attraction, which…

High Energy Physics - Phenomenology · Physics 2025-07-29 Sachiko Takeuchi , Alessandro Giachino , Makoto Takizawa , Elena Santopinto , Makoto Oka

We reconsider the relationship between the bound state and the SU(3) rigid rotator approaches to strangeness in chiral soliton models. For non-exotic $S=-1$ baryons the bound state approach matches for small $m_K$ onto the rigid rotator…

High Energy Physics - Phenomenology · Physics 2017-08-23 Igor R. Klebanov , Peter Ouyang

Inspired by $P_c(4380)$ and $P_c(4450)$ recently observed by LHCb, a QCD sum rule investigation is performed, by which they can be identified as exotic hidden-charm pentaquarks composed of an anti-charmed meson and a charmed baryon. Our…

High Energy Physics - Phenomenology · Physics 2015-10-21 Hua-Xing Chen , Wei Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

QCD-motivated models for hadrons predict an assortment of "exotic" hadrons that have structures that are more complex then the quark-antiquark mesons and three-quark baryons of the original quark-parton model. These include pentaquark…

High Energy Physics - Experiment · Physics 2015-06-19 Stephen Lars Olsen

The three pentaquark states, $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$, discovered by the LHCb Collaboration in 2019, can be arranged into a complete heavy quark spin symmetry multiplet of hadronic molecules of…

High Energy Physics - Phenomenology · Physics 2022-10-12 Ya-Wen Pan , Tian-Wei Wu , Ming-Zhu Liu , Li-Sheng Geng

I develop an extension of the usual three-flavor quark model to four flavors (u, d, s and c), and discuss the classification of pentaquark states with hidden charm. This work is motivated by the recent observation of such states by the LHCb…

Nuclear Theory · Physics 2017-11-02 Roelof Bijker

The effective strange quark and antiquark masses are estimated from the chiral soliton approach (CSA) results for the spectrum of exotic and nonexotic baryons. There are problems when one tries to project results of the CSA on the simple…

High Energy Physics - Phenomenology · Physics 2013-09-11 Vladimir B. Kopeliovich

We study the weak decay of the $\Lambda_b$ baryon into $J/\psi\ \phi\ \Lambda$, a process that is particularly well suited to analyze the physics of some of the recently observed or theoretically predicted exotic hadrons, as one expects to…

High Energy Physics - Phenomenology · Physics 2020-10-06 Volodymyr Magas , Àngels Ramos , Rahul Somasundaram , Júlia Tena Vidal

QCD-motivated models for hadrons predict an assortment of "exotic" hadrons that have structures that are more complex than the quark-antiquark mesons and three-quark baryons of the original quark-parton model. These include pentaquark…

High Energy Physics - Experiment · Physics 2014-12-10 Stephen Lars Olsen

The field of exotic spectroscopy is extremely rich and productive. Several observations and searches for pentaquark states have been performed in the last 4 years, starting from the LHCb observation in 2015. This is still quite a recent…

High Energy Physics - Experiment · Physics 2019-06-24 Lorenzo Capriotti

The hidden-charm pentaquark states $P_{c\bar{c}}\left(4312\right)^+$, $P_{c\bar{c}}\left(4380\right)^+$, $P_{c\bar{c}}\left(4440\right)^+$, and $P_{c\bar{c}}\left(4457\right)^+$, all with isospin $I = 1/2$, were discovered by the LHCb…

High Energy Physics - Phenomenology · Physics 2025-08-19 Nora Brambilla , Abhishek Mohapatra , Antonio Vairo

The LHCb collaboration has recently observed three narrow pentaquark states --- the $P_c(4312)$, $P_c(4440)$, and $P_c(4457)$ ---that are located close to the $\bar{D} \Sigma_c$ and $\bar{D}^* \Sigma_c$ thresholds. Among the so-far proposed…

High Energy Physics - Phenomenology · Physics 2020-08-05 Ya-Wen Pan , Ming-Zhu Liu , Fang-Zheng Peng , Mario Sánchez Sánchez , Li-Sheng Geng , Manuel Pavon Valderrama

In the framework of one-pion-exchange (OPE) model, we study the hidden-charm and charm-strange molecular pentaquark systems composed of a heavy baryon $(\Sigma_c, \Sigma_c^*)$ and a vector meson $(\bar{K}^*, \bar{D}^*)$, where the S-D…

High Energy Physics - Phenomenology · Physics 2016-08-09 Rui Chen , Xiang Liu , Shi-Lin Zhu

The hidden charm pentaquark state $P_c(4450)$ observed recently by the LHCb collaboration may be of molecular nature, as advocated by some unitary approaches that also predict pentaquark partners in the strangeness $S=-1$ sector. In this…

High Energy Physics - Phenomenology · Physics 2016-09-21 A. Feijoo , V. K. Magas , A. Ramos , E. Oset

We briefly review the formulation of chiral quark soliton model and explain the difference and similarities with the Skyrme model. Next, we apply the model to calculate non-exotic and exotic mass spectra. We concentrate on large $N_{c}$…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Praszalowicz , K. Goeke

The LHCb collaboration have recently updated their analysis of the resonant $J/\psi p$ mass spectrum in the decay $\Lambda_b^0 \to J/\psi p K^-$, making use of their combined Run 1 and Run 2 data. In the updated analysis, three narrow…

High Energy Physics - Phenomenology · Physics 2020-01-08 Ahmed Ali , Ishtiaq Ahmed , M. Jamil Aslam , Alexander Ya. Parkhomenko , Abdur Rehman

The properties of pentaquarks containing a heavy anti-quark and strange quarks are studied in the bound state picture. In the flavor SU(3) limit, there are many pentaquark states with the same binding energy. When the SU(3) symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-28 Chi-Keung Chow

We study the spectrum of the isoscalar pentaquark $udsc\overline{c}$, of either positive or negative parity, in a constituent quark model with linear confinement and a flavor-spin hyperfine interaction previously extended to SU(4) and used…

High Energy Physics - Phenomenology · Physics 2021-08-17 Fl. Stancu

The pentaquark states, $P_{c}(4312)$, $P_{c}(4440)$ and $P_{c}(4457)$, could be nicely arranged into a multiplet of seven molecules of $\bar{D}^{(\ast)}\Sigma_{c}^{(\ast)}$ dictated by heavy quark spin symmetry. However, the spins of…

High Energy Physics - Phenomenology · Physics 2021-02-10 Ming-Zhu Liu , Ya-Wen Pan , Li-Sheng Geng

The past seventeen years have witnessed tremendous progress on the experimental and theoretical explorations of the multiquark states. The hidden-charm and hidden-bottom multiquark systems were reviewed extensively in [Phys. Rept. 639…

High Energy Physics - Phenomenology · Physics 2019-06-11 Yan-Rui Liu , Hua-Xing Chen , Wei Chen , Xiang Liu , Shi-Lin Zhu