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Related papers: Pentaquark baryons in SU(3) quark model

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In a previous work we have studied the isospin 1/2 lowest positive and negative parity states of the pentaquark $uudc\overline{c}$, in a constituent quark model with a linear confinement and an SU(4) flavor-spin hyperfine interaction and we…

High Energy Physics - Phenomenology · Physics 2021-11-04 Fl. Stancu

A brief review on some recent progresses in our understanding of multi-quark components in baryons is presented. The multi-quark components in baryons seem to be mainly in colored quark cluster configurations rather than in ``meson cloud''…

High Energy Physics - Phenomenology · Physics 2009-11-11 B. S. Zou

We 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. We fit our model to the known baryon spectrum and we predict the double…

Nuclear Theory · Physics 2019-04-29 Emmanuel Ortiz-Pacheco , Roelof Bijker , César Fernández-Ramírez

We calculate light-front wave functions of mesons, baryons and pentaquarks in a model including constituent mass (representing chiral symmetry breaking), harmonic confining potential, and 4-quark local interaction of 't Hooft type. The…

High Energy Physics - Phenomenology · Physics 2019-12-18 Edward Shuryak

The purported observation of a state $\Theta^+$ with strangeness S = +1 led to its quark model interpretation in terms of a pentaquark combination involving a triquark-diquark structure -- the Karliner-Lipkin model. In this work, the proper…

High Energy Physics - Phenomenology · Physics 2008-11-26 Swarup Kumar Majee , Amitava Raychaudhuri

The baryon structure is investigated in a covariant diquark-quark model. In this approach baryons emerge as relativistic bound states of a constituent quark and a $0^{+}$ or $1^{+}$ diquark. After solving the Bethe-Salpeter Equation for the…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Hellstern , R. Baürle , U. Zückert , R. Alkofer , H. Reinhardt

In the present talk, we report recent results on electromagnetic properties of the baryon decuplet within the SU(3) chiral quark-soliton model, taking into account the effects of explicit flavor SU(3) symmetry breaking. We focus on the…

High Energy Physics - Phenomenology · Physics 2019-02-11 June-Young Kim , Hyun-Chul Kim

In previous papers we developed the light front formulation for Hamiltonians and wave functions (WFs) for mesons and baryons, with both confinement and chiral symmetry breaking. For baryons limited to the lowest Fock component with three…

High Energy Physics - Phenomenology · Physics 2025-11-04 Nicholas Miesch , Edward Shuryak , Ismail Zahed

We examine the SU(3) symmetry breaking in hyperon semileptonic decays (HSD) by considering two typical sets of quark contributions to the spin content of the octet baryons: Set-1 with SU(3) flavor symmetry and Set-2 with SU(3) flavor…

High Energy Physics - Phenomenology · Physics 2009-11-07 Jian-Jun Yang

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

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

It is shown that standard constituent quark models produce $(\bar c c qqq)$ hidden-charm pentaquarks, where $c$ denotes the charmed quark and $q$ a light quark, which lie below the lowest threshold for spontaneous dissociation and thus are…

High Energy Physics - Phenomenology · Physics 2017-11-22 J. -M. Richard , A. Valcarce , J. Vijande

We propose a model for the recently discovered Theta^+ exotic KN resonance as a novel kind of a pentaquark with an unusual color structure: a color triplet (ud) diquark, coupled to a color anti-triplet (ud s-bar) triquark in a relative…

High Energy Physics - Phenomenology · Physics 2010-01-08 Marek Karliner , Harry J. Lipkin

We construct the complete set of positive parity pentaquarks, which correspond in the quark model to {\bar s} q^{Nc+1} states with one unit of orbital angular momentum L=1. In the large Nc limit they fall into the K=1/2 and K=3/2 irreps…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dan Pirjol , Carlos Schat

We construct a linear $SU(3)_L \times SU(3)_R$ parity doublet model for octet baryons. Our model employs the $(3,\bar{3}) + (\bar{3},3)$ and $(3,6) + (6,3)$ chiral representations while excluding the $(8,1) + (1,8)$ representation. Through…

High Energy Physics - Phenomenology · Physics 2026-02-16 Bikai Gao , Atsushi Hosaka

We present a generating functional producing quark wave functions of all Fock states in the octet, decuplet and antidecuplet baryons in the mean field approximation, both in the rest and infinite momentum frames. In particular, for the…

High Energy Physics - Phenomenology · Physics 2014-11-18 Dmitri Diakonov , Victor Petrov

Group theoretic method for the systematic study of five-quark states with meson-baryon ($q\bar{q}-q^3$) configuration is developed. The calculation of matrix elements of many body Hamiltonian is simplified by transforming the physical bases…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jialun Ping , Hongxia Huang , Chengrong Deng , Fan Wang , T. Goldman

We give a comprehensive review of concepts and numerical calculations for SU(2) and SU(3) baryonic systems which are considered as many body systems composed of three quarks coupled to a polarized Dirac sea by a Nambu--Jona-Lasinio like…

High Energy Physics - Phenomenology · Physics 2007-05-23 Th. Meissner , E. Ruiz Arriola , A. Blotz , K. Goeke

We propose a supersymmetric model of quark flavor symmetry based on SU(3)colorxSU(3)WxU(1)X x T' where T' (binary tetrahedral group) is a discrete flavor symmetry group. The third (heavy) generation of quarks are assigned to singlet…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sutapa Sen

Assuming that the recently observed $\Theta^+$ and $\Xi^{--}$ are members of an anti-decuplet of SU(3), decays to ground state baryons and mesons are calculated using an effective Lagrangian which incorporates chiral and SU(3) symmetry. We…

High Energy Physics - Phenomenology · Physics 2014-11-17 Thomas Mehen , Carlos Schat
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