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Related papers: Decay properties of the $d^*(2380)$ hexaquark mult…

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The purpose of the present study was to explore the possibility of accommodating the $d^*(2380)$ and its flavor SU(3) partners in a diquark model. Proposing that $d^*(2380)$ is composed of three vector diquarks, its mass is calculated by…

Nuclear Theory · Physics 2019-04-15 Pan-Pan Shi , Fei Huang , Wen-Ling Wang

Experiments with intense photon and electron beams have the potential to provide access to nontrivial properties of the recently discovered $d^*(2380)$ hexaquark including its size, structure, magnetic moment, quadrupole and octupole…

Nuclear Theory · Physics 2019-07-31 M. Bashkanov , D. P. Watts , A. Pastore

The most fascinating dibaryon in the non-strange quark sector is $d^*(2380)$, which was reported by WASA-at-COSY Collaboration and confirmed by A2@MAMI Collaboration. The reported mass and width are $M\approx2.37$ GeV, $\Gamma\approx70$ MeV…

High Energy Physics - Phenomenology · Physics 2023-08-09 ManYing Pan , Xinmei Zhu , Jialun Ping

Hexaquarks constitute a natural extension of complex quark systems like also tetra- and pentaquarks do. To this end the current status of $d^*(2380)$ in both experiment and theory is shortly reviewed. Recent high-precision measurements in…

Nuclear Theory · Physics 2021-02-03 H. Clement , T. Skorodko

The LHCb has discovered two new states with preferred $J^P$ quantum numbers $3/2^-$ and $5/2^+$ from $\Lambda_b$ decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these…

High Energy Physics - Phenomenology · Physics 2016-01-27 Guan-Nan Li , Min He , Xiao-Gang He

We consider the mass splittings and strong decays of members of the lowest-lying pentaquark multiplet, which we take to be a parity-odd antidecuplet. We derive useful decompositions of the quark model wave functions that allow for easy…

High Energy Physics - Phenomenology · Physics 2015-06-25 Carl E. Carlson , Christopher D. Carone , Herry J. Kwee , Vahagn Nazaryan

Dynamical calculations are performed for all members of the flavor antidecuplet to which the pentaquark $\Theta^+$ belongs. The framework is a constituent quark model where the short-range interaction has a flavor-spin structure. From…

High Energy Physics - Phenomenology · Physics 2017-08-23 Fl. Stancu

Dynamical calculations are performed for all isomultiplets of the flavour antidecuplet to which the newly discovered pentaquark $\Theta^+$ belongs. The framework is a constituent quark model where the short-range interaction has a…

High Energy Physics - Phenomenology · Physics 2009-11-10 Fl. Stancu

To understand the nature of $X(2075)$ and $X(2085)$ observed by the BESIII collaboration in the $p\bar{\Lambda}$ system, we systematically investigate the possibility that these states are compact hexaquark with triquark-antitriquark…

High Energy Physics - Phenomenology · Physics 2026-03-11 Xuan-Heng Zhang , Sheng-Qi Zhang , Cong-Feng Qiao

Light and heavy pentaquarks are described within a constituent quark model based on a spin-flavor hyperfine interaction. In this model the lowest state acquires positive parity. The masses of the light antidecuplet members are calculated…

High Energy Physics - Phenomenology · Physics 2009-11-11 Fl. Stancu

In the light of the recent discovery of the $\Xi^{++}_{cc}$ by LHCb collaboration, we study the stable doubly heavy tetraquarks. These states are compact exotic hadrons which can be approximated as the diquark-anti-diquark correlations. In…

High Energy Physics - Phenomenology · Physics 2018-10-09 Ye Xing , Ruilin Zhu

Hexaquark wave function with the quantum numbers $I(J^P)=0(3^+)$, which might be relevant for $d^*(2380)$, is constructed under an assumption that this is composed only of $u,d$ quarks in an $S$-wave. By combining three diquarks of either…

High Energy Physics - Phenomenology · Physics 2020-11-04 Hungchong Kim , K. S. Kim , Makoto Oka

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

The structure of $d^*(2380)$ is re-studied with the single cluster structure in the chiral SU(3) quark model which has successfully been employed to explain the $N-N$ scattering data and the binding energy of deuteron. The binding behavior…

Nuclear Theory · Physics 2017-09-13 Qi-Fang Lü , Fei Huang , Yu-Bing Dong , Peng-Nian Shen , Zong-Ye Zhang

Baryons of the type Qqqqq-bar (where Q = c,b and q = u,d,s quarks) forming anti-decapenta (15)-plets with spin-parity one half-plus are predicted on simple theoretical considerations. The lightest members of these multiplets are explicitly…

High Energy Physics - Phenomenology · Physics 2010-03-11 Dmitri Diakonov

We presents an investigation of the $K^*(1680)$ state in its strong decays into two-body finial states within the flux-tube model and quark pair creation model. Since the charge conjugation parity is not conserved in the strange sector, the…

High Energy Physics - Phenomenology · Physics 2026-03-04 Samee Ullah , Ye Cao , Ming-Xiao Duan , Hai-Bing Fu , Qiang Zhao

Motivated by recent experimental evidence for apparent $cc\bar c \bar c$ states at LHCb, CMS and ATLAS, we consider how the mass spectrum and decays of such states can be used to discriminate among their possible theoretical…

High Energy Physics - Phenomenology · Physics 2023-11-28 Muhammad Naeem Anwar , Timothy J. Burns

In recent years there has been tremendous progress in the investigation of bound systems of quarks with multiplicities beyond the more usual two- and three-quark systems. Experimental and theoretical progress has been made in the four-,…

High Energy Physics - Phenomenology · Physics 2023-08-15 M. Bashkanov , D. P. Watts , G. Clash , M. Mocanu , M. Nicol

Heavy-light diquarks can be the building blocks of a rich spectrum of states which can accommodate some of the newly observed charmonium-like resonances not fitting a pure c-cbar assignment. We examine this possibility for hidden and open…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Maiani , F. Piccinini , A. D. Polosa , V. Riquer

We consider how the recent CMS measurements of the masses and quantum numbers of $X(6600)$, $X(6900)$ and $X(7100)$ can help to reveal the internal structure of these apparent $cc\bar{c}\bar{c}$ tetraquark states. The measured $J^{PC} =…

High Energy Physics - Phenomenology · Physics 2026-05-06 Muhammad Naeem Anwar , Timothy J. Burns
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