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Related papers: Dynamical study of the pentaquark antidecuplet

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We present a systematic calculation of the axial charges and magnetic moments for the decuplet of hidden-charm molecular pentaquarks within the framework of the constituent quark model. Our findings reveal that the axial charges of these…

High Energy Physics - Phenomenology · Physics 2025-11-18 Hao-Song Li

We describe a realistic, renormalizable, supersymmetric ``quindecuplet'' model in which the top quark, left handed bottom quark, and up-type Higgs boson are composite, with a compositeness scale $\sim 1-3$ TeV. The top-Higgs Yukawa coupling…

High Energy Physics - Phenomenology · Physics 2009-10-28 Ann E. Nelson , Matthew J. Strassler

For the case of two light flavors we propose the stringy description of the system consisting of two heavy and three light quarks, with the aim of exploring the quark organization inside the system and its low-lying Born-Oppenheimer…

High Energy Physics - Phenomenology · Physics 2023-02-15 Oleg Andreev

We study spin 1/2 isoscalar and isovector candidates in both parity channels for the recently discovered \Theta^+(1540) pentaquark particle in quenched lattice QCD. Our analysis takes into account all possible uncertainties, such as…

High Energy Physics - Lattice · Physics 2010-02-03 F. Csikor , Z. Fodor , S. D. Katz , T. G. Kovacs

A schematic model for hadronic states, based on constituent quarks and antiquarks and gluon pairs, is discussed. The phenomenological interaction between quarks and gluons is QCD motivated. The obtained hadronic spectrum leads to the…

Nuclear Theory · Physics 2009-11-10 M. Nunez , S. Lerma , P. O. Hess , S. Jesgarz , O. Civitarese , M. Reboiro

We determine the baryon octet and decuplet masses as well as their wave functions in a covariant three-body Faddeev approach. We work in an approximation where irreducible three-body forces are neglected. In the two-body interactions we…

High Energy Physics - Phenomenology · Physics 2014-11-11 Helios Sanchis-Alepuz , Christian S. Fischer

The strange-anticharmed Pentaquark is a $uud\bar{c}s$ or $udd\bar{c}s$ five-quark baryon that is expected to be either a narrow resonance, or possibly even stable against strong and electromagnetic decay. We describe this hyperon here, its…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

We present an analysis of the newly observed pentaquark $P_c(4312)^+$ to shed light on its quantum numbers. To do that, the QCD sum rule approach is used. The measured mass of this particle is close to $\Sigma_c^{++}\bar{D}^-$ threshold and…

High Energy Physics - Phenomenology · Physics 2021-05-26 K. Azizi , Y. Sarac , H. Sundu

The Theta+(1540), recently observed at LEPS, DIANA and CLAS, is hypothesized to be an isotensor resonance. This implies the existence of a multiplet where the Theta++, Theta+ and Theta0 have isospin-violating strong decays, and the Theta+++…

High Energy Physics - Phenomenology · Physics 2014-11-17 Simon Capstick , Philip R. Page , Winston Roberts

By assuming a mass formula for the spectrum of the Y=2 pentaquarks, where the chromo-magnetic interaction plays a main role, and identifying the lightest state with the Theta^+(1540), we predict a spectrum in good agreement with the few I=0…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. Buccella , D. Falcone , F. Tramontano

The lightest hidden-bottom tetraquarks in the dynamical diquark model fill an $S$-wave multiplet consisting of 12 isomultiplets. We predict their masses and dominant bottomonium decay channels using a simple 3-parameter Hamiltonian that…

High Energy Physics - Phenomenology · Physics 2020-07-29 Jesse F. Giron , Richard F. Lebed

We study hidden-flavor pentaquarks, $Q\bar Q qqq$, based on a constituent quark-model with a standard quark-quark interaction that reproduces the low-energy meson and baryon spectra. We make use of dynamical correlations between the heavy…

High Energy Physics - Phenomenology · Physics 2022-07-07 H. Garcilazo , A. Valcarce

The masses of $uudd\bar s $, $uudd\bar d$ and $uuss\bar d$ pentaquarks are evaluated in a framework of both the Effective Hamiltonian approach to QCD and spinless Salpeter using the Jaffe--Wilczek diquark approximation and the string…

High Energy Physics - Phenomenology · Physics 2009-11-11 I. M. Narodetskii , C. Semay , B. Silvestre-Brac , Yu. A. Simonov , M. A. Trusov

We apply the dynamical diquark model to predict the spectrum of hidden-charm pentaquark states in both unflavored and open-strange sectors. Using only Hamiltonian parameters introduced in the tetraquark $S$- and $P$-wave multiplets, the…

High Energy Physics - Phenomenology · Physics 2021-12-23 Jesse F. Giron , Richard F. Lebed

In this work, we study the octaquark, which is composed of two baryons and one meson using a simple chromomagnetic model. First, we construct the wave function of the octaquark satisfying the Pauli exclusion principle in the flavor SU(3)…

High Energy Physics - Phenomenology · Physics 2025-04-07 Aaron Park

We use a theoretical model of the $\gamma ~d \to ~K^+ K^- ~n ~p $ reaction adapted to the experiment done at LEPS where a peak was observed and associated to the $\Theta^{+}(1540)$ pentaquark. The study shows that the method used in the…

Nuclear Theory · Physics 2011-11-10 A. Martínez Torres , E. Oset

We study properties of the pentaquark particle Theta+ with emphasis on the role of chiral symmetry. It is shown that when chiral force is sufficiently strong, the positive parity Theta+ may be realized with a lower mass relative to the…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Hosaka

In this article, we study the magnetic moment of the pentaquark $ \Theta^+(1540)$ as (scalar)diquark-(pseudoscalar)diquark-antiquark state with the QCD sum rules approach in the external electromagnetic field. Due to the special structure…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zhi-Gang Wang , Ri-Cong Hu

Given the existing empirical information about the exotic Theta+ baryon, we analyze possible properties of its SU(3)F-partners, paying special attention to the nonstrange member of the antidecuplet N*. The modified piN partial-wave analysis…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. I. Strakovsky , R. A. Arndt , Ya. I. Azimov , M. V. Polyakov , R. L. Workman

We show that the mass intervals among the pentaquark baryons $\Theta^{+}$, $N^{*}(1685)$ and $\Xi_{3/2}^{-}$ proposed to be the members of the SU(3) antidecuplet are exact integral multiples of the mass difference between a neutral pion and…

General Physics · Physics 2009-04-24 Tariq Ahmad Mir
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