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Related papers: Constraints on widths of mixed pentaquark multiple…

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We examine several assignments of spin and parity for the pentaquark Theta+ state (J^P=1/2^{+,-}, 3/2^{+,-}) in connection with known baryon resonances. Assuming that the Theta+ belongs to an antidecuplet representation which mixes with an…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tetsuo Hyodo , Atsushi Hosaka

Recently, the tetraquark mixing framework has been proposed as a possible structure for the two light-meson nonets in the $J^P=0^+$ channel, the light nonet composed of $a_0(980)$, $K_0^*(700)$, $f_0(500)$, $f_0(980)$, and the heavy nonet…

High Energy Physics - Phenomenology · Physics 2022-12-28 Hungchong Kim , K. S. Kim

We consider hidden charm pentaquarks as hadroquarkonium states in a QCD inspired approach. Pentaquarks arise naturally as bound states of quarkonia excitations and ordinary baryons. The LHCb $P_c(4450)$ pentaquark is interpreted as a…

High Energy Physics - Phenomenology · Physics 2018-02-14 Michael I. Eides , Victor Yu. Petrov , Maxim V. Polyakov

The systematic large N_c limit within chiral perturbation provides an optimal eta-eta' mixing angle of about -27 degrees at leading order in p^2. In this frame, agreement with the data can be reached with higher order corrections of about…

High Energy Physics - Phenomenology · Physics 2010-01-15 C. Degrande , J. -M. Gerard

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

Some claim that there are two independent mixing angles ($\theta = 35.3^\circ$, $-54.7^\circ$) between $^3P_1$ and $^1P_1$ states of heavy-light mesons in heavy quark symmetric limit, and others claim there is only one ($\theta =…

High Energy Physics - Phenomenology · Physics 2010-12-09 Takayuki Matsuki , Toshiyuki Morii , Kohichi Seo

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

Based on the recent phenomenological analysis done by M. Mojzis, Eur. Phys. Jour. {\bf C2} (1998) 182, of $\pi N $ scattering within the framework of Heavy Baryon Chiral Perturbation Theory we predict, after a suitable unitarization of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Nieves , E. Ruiz Arriola

We discuss the implications of the suggested interpretation of the recently reported narrow pi N resonance (width \approx 25 MeV at 1680 MeV) as a pentaquark in the same multiplet as the Theta+. We consider a diquark-triquark pentaquark…

High Energy Physics - Phenomenology · Physics 2010-03-09 Marek Karliner , Harry J. Lipkin

In this article, we take the point of view that the pentaquark state $\Theta^+(1540)$ has negative parity, and choose the diquark-triquark type interpolating current to calculate the strong coupling constant $g_{\Theta NK}$ in the QCD sum…

High Energy Physics - Phenomenology · Physics 2009-11-11 Zhi-Gang Wang , Wei-Min Yang , Shao-Long Wan

We report on searches in deep inelastic $ep$ scattering for narrow baryonic states decaying into $\Xi^-\pi^-, \Xi^-\pi^+, \KS p$ and their charge conjugates, at centre-of-mass energies of 300 and 318 GeV. No signal for a new narrow baryonic…

High Energy Physics - Experiment · Physics 2007-05-23 J. E. Olsson

Theoretical predictions for the spectrum of heavy meson-baryon bound states are a fundamental tool for disentangling the nature of the different pentaquark states that have been observed in experimental facilities. Here we explore this…

High Energy Physics - Phenomenology · Physics 2025-01-17 Zi-Ying Yang , Fang-Zheng Peng , Mao-Jun Yan , Mario Sánchez Sánchez , Manuel Pavon Valderrama

Very recently, the LHCb collaboration has reported the new result about the hidden-charm pentaquarks: $P_c(4312)$ near the $\bar{D}\Sigma_c$ threshold, and $P_c(4440)$ and $P_c(4457)$ near $\bar{D}^*\Sigma_c$ threshold. We study the heavy…

High Energy Physics - Phenomenology · Physics 2019-04-02 Yuki Shimizu , Yasuhiro Yamaguchi , Masayasu Harada

We report on a study of the pentaquark Theta^+(1540), using a variety of different interpolating fields. We use Chirally Improved fermions in combination with Jacobi smeared quark sources to improve the signal and get reliable results even…

High Energy Physics - Lattice · Physics 2007-05-23 Dieter Hierl , Christian Hagen , Andreas Schaefer

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

The vertex corrections to the leptonic partial widths of the $Z$ induced by leptoquarks that couple leptons to the top quark are considered. We obtain stringent bounds on the parameter space of the masses and Yukawa couplings of these…

High Energy Physics - Phenomenology · Physics 2009-09-25 Gautam Bhattacharyya , John Ellis , K. Sridhar

We present a largely model independent analysis of the lighter Heavy Quarkonium Hybrids based on the strong coupling regime of Potential Non-Relativistic QCD (pNRQCD). We calculate the spectrum at leading order, including the mixing of…

High Energy Physics - Phenomenology · Physics 2017-07-19 Rubén Oncala , Joan Soto

States beyond those expected in the simple constituent quark model are now emerging. I focus on the scalar glueball and its mixing with states in the $q\bar{q}$ nonet, and also on correlations in Strong QCD that may form diquarks and seed…

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

We investigate the mass spectrum of the pentaquark baryon ($ udud \bar s $) in quenched lattice QCD with exact chiral symmetry. Using 3 different interpolating operators for $ \Theta $, we measure the $ 3 \times 3 $ correlation matrix and…

High Energy Physics - Phenomenology · Physics 2011-02-16 Ting-Wai Chiu , Tung-Han Hsieh

Using the exisiting experimental data for hyperon semileptonic decays and the flavor-singlet axial-vector charge $g_{A}^{(0)}$ from polarized deep inelastic scattering of the proton, we derive the decay width of the $\Theta^{+}$ pentaquark…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ghil-Seok Yang , Hyun-Chul Kim , Klaus Goeke