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The pentaquarks are exotic baryons formed of four quarks and an antiquarks. Their existence has been discussed in the literature over the last 30 years or more, first in connection with kaon nucleon scattering data. The subject has been…

High Energy Physics - Phenomenology · Physics 2016-09-06 Fl. Stancu

This is the second of two companion papers in which we continue to develop the construction of the doubly heavy pentaquark systems using the gauge/string duality. In this paper, we propose a stringy description of the $Q\bar Qqqq$ system in…

High Energy Physics - Phenomenology · Physics 2024-02-05 Oleg Andreev

We predict exotic doubly heavy--strange pentaquarks with minimal quark content $u\bar d sQQ'$ ($QQ'=cc,bc,bb$) within a coupled-channel unitary framework where the interaction is derived from an extension of the local hidden gauge approach…

High Energy Physics - Phenomenology · Physics 2026-05-26 Albert Feijoo , Eulogio Oset

We analyze the decay modes of the three $[\frac 12\frac 12^-]_{S=0,1}$ and $[\frac 12\frac 32^-]_{S=1}$ non-strange pentaquarks with hidden charm and bottom, predicted by holographic QCD in the heavy quark limit. In leading order, the…

High Energy Physics - Phenomenology · Physics 2022-01-05 Yizhuang Liu , Maciej A. Nowak , Ismail Zahed

Hidden-charm pentaquark-like $P_{\psi s}^\Lambda(4459)^0$ and $P_{\psi s}^\Lambda(4338)$ resonances are studied in a constituent quark model as molecular meson-baryon structures. Such states are found in the $J^P(I)=\frac{1}{2}^-(0)$…

High Energy Physics - Phenomenology · Physics 2023-02-22 Pablo G. Ortega , David R. Entem , Francisco Fernandez

In light of the recently observed resonance states $P_{\psi s}^{\Lambda}(4338)^0$ and $P_{cs}(4459)^0$ by LHCb Collaboration in $J/\psi\Lambda$ decay channel, we perform a systematical study of all possible hidden-heavy pentaquarks with…

High Energy Physics - Phenomenology · Physics 2023-12-21 Wen-Xuan Zhang , Chang-Le Liu , Duojie Jia

The $J/\psi p$ signals at 4380 MeV and 4450 MeV which were seen by the LHCb collaboration in the decay $\Lambda^0_b\to K^-J/\psi p$ are discussed following the hypothesis of the existence of diquark-diquark-antiquark composite states. The…

High Energy Physics - Phenomenology · Physics 2017-11-30 V. V. Anisovich , M. A. Matveev , J. Nyiri , A. V. Sarantsev , A. N. Semenova

A recent analysis by the LHCb collaboration suggests the existence of three narrow pentaquark-like states --- the $P_c(4312)$,$P_c(4440)$ and $P_c(4457)$ --- instead of just one in the previous analysis (the $P_c(4450)$). The closeness of…

High Energy Physics - Phenomenology · Physics 2019-06-26 Ming-Zhu Liu , Ya-Wen Pan , Fang-Zheng Peng , Mario Sanchez Sanchez , Li-Sheng Geng , Atsushi Hosaka , Manuel Pavon Valderrama

Inspired by the observed $X(2900)$, we study systematically the mass spectra of the ground pentaquark states with the $qqqq\bar{Q}$ ($Q=c,b$; $q=n,s$; $n=u,d$) configuration in the framework of the Chromomagnetic Interaction model. We…

High Energy Physics - Phenomenology · Physics 2022-02-22 Hong-Tao An , Kan Chen , Xiang Liu

The LHCb collaboration has recently announced the discovery of two hidden-charm pentaquark states with also strange quark content, $P_{cs}(4338)$ and $P_{cs}(4459)$; its analysis points towards having both hadrons isospin equal to zero and…

High Energy Physics - Phenomenology · Physics 2023-11-03 Gang Yang , Jialun Ping , Jorge Segovia

The masses of cryptoexotic pentaquarks with hidden beauty are estimated phenomenologically using the results by the LHCb collaboration which discovered recently the cryptoexotic pentaquarks with hidden charm. The expected masses of the…

High Energy Physics - Phenomenology · Physics 2017-07-10 Vladimir Kopeliovich , Irina Potashnikova

The observation of the two states $P_c(4380)$ and $P_c(4445)$ [Phys.Rev.Lett. 115 (2015) 072001] solids the existence of the pentaquark state in Nature. In this work, we study the spectrum of the pentaquark states including one or two heavy…

High Energy Physics - Phenomenology · Physics 2020-02-26 Ben-Teng Zhang , Jun-Shuai Wang , Yong-Liang Ma

Using the Thomas-Fermi quark model, a collective, spherically symmetric density of states is created to represent a gas of interacting fermions with various degeneracies at zero temperature. Over a family of multi-pentaquarks, color…

We discuss a realisation of the pentaquark structure proposed by Jaffe and Wilczek within a simple quark model with colour-spin contact interactions and coloured harmonic confinement, which accurately describes the $\Delta-N$ splitting. In…

High Energy Physics - Phenomenology · Physics 2015-07-27 J. J. Dudek

The pentaquark $P_c^+(4450)$ recently discovered by LHCb has been interpreted as a bound state of $\Psi(2S)$ and nucleon. The charmonium-nucleon interaction which provides the binding mechanism is given, in the heavy quark limit, in terms…

High Energy Physics - Phenomenology · Physics 2016-09-21 I. A. Perevalova , M. V. Polyakov , P. Schweitzer

We propose a collective stringlike model of pentaquarks with the geometry of an equilateral tetrahedron in which the four quarks are located at the four corners and the antiquark in its center. The nonplanar equilibrium configuration is a…

High Energy Physics - Phenomenology · Physics 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

We identify essential differences between the pentaquark and chiral soliton models of \10bar$_5$ and {\bf 8}$_5$ pentaquarks and conventional {\bf 8}$_3$ states, which are experimentally measurable. We show how the decays of $\Xi_5$ states…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. E. Close , J. J. Dudek

The LHCb Collaboration has observed two types of hidden-charm pentaquark states $P_{\psi}^N$ and $P_{\psi s}^{\Lambda}$ since 2015. In this work, we predict two other types of hidden-charm pentaquark states $P_{\psi s}^{\Sigma}(4367)$ and…

High Energy Physics - Phenomenology · Physics 2025-02-11 Hao-Song Li , Tao Li

The nature of the $P_{c}(4312)$, $P_c(4440)$ and $P_c(4457)$ pentaquarks is a fascinating theoretical question. Within the molecular picture their more usual interpretation is that of $I=\tfrac{1}{2}$ $\bar{D} \Sigma_c$ and $\bar{D}^*…

High Energy Physics - Phenomenology · Physics 2024-10-22 Fang-Zheng Peng , Mao-Jun Yan , Mario Sánchez Sánchez , Manuel Pavon Valderrama

We generalize to five distinct flavors the flavor-spin hyperfine interaction introduced previously for four flavors and used in the study of $uudc\overline{c}$ pentaquark. As a particular case here we study the lowest states of the…

High Energy Physics - Phenomenology · Physics 2023-07-26 Fl. Stancu