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Related papers: Pentaquark Decay Width in QCD Sum Rules

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In a diquark-diquark-antiquark picture of the pentaquark we study the decay $\Theta \to K^{+} n$ within the framework of QCD sum rules. After evaluation of the relevant three-point function, we extract the coupling $g_{\Theta nK}$ which is…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. S. Navarra , M. Nielsen , R. Rodrigues da Silva

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 calculate the widths of the various pentaquarks in a relativistic model in which the pentaquark is considered to be composed of a scalar diquark and a spin 1/2 triquark. We consider both positive and negative parity for the pentaquark.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hu Li , C. M. Shakin , Xiangdong Li

The pentaquark width is calculated in QCD sum rules. Result for $\Gamma_{\Theta}$ show, that $\Gamma_{\Theta}$ can vary in the region less than 1$MeV$. The main conclusion is, that if pentaquark is genuine states then sum rules really…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. G. Oganesian

We study the pentaquark $uudd\bar s$ with $J=3/2$ and I=1 ($\Theta^{++}$) in the QCD sum rule approach. We derive the QCD sum rules for positive and negative parity states of the pentaquark. The QCD sum rule predicts that there exists…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tetsuo Nishikawa , Yoshiko Kanada-En'yo , Osamu Morimatsu , Yoshihiko Kondo

For tetraquarks of the form $T[(\bar{Q}q)(Q\bar{q})]$ we give sum rules for their decay coupling constants, taking into account the SU(3) symmetry breaking interactions to first order.

High Energy Physics - Phenomenology · Physics 2013-04-05 V. Gupta , G. Sánchez-Colón , S. Rajpoot

It is shown, that the small decay width of $\Theta^+ = uudd\bar{s}$ baryon is suppressed by chirality violation. It is shown that $\Theta^+$ decay width $\Gamma$ is proportional to $\alpha^2_s < 0 | \bar{q} q | 0 >^2$, for any pentaquark…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. G. Oganesian

Assuming the two diquark structure for the pentaquark state as advocated in the Jaffe-Wilczek model, we study the strong decays of light and heavy parity-even pentaquark states using the light-front quark model in conjunction with the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua

The pentaquark width is calculated in QCD sum rules. The higher dimension operators contribution is accounted. It is shown, that $\Gamma_{\Theta}$ should be very small, less than $1Mev$.

High Energy Physics - Phenomenology · Physics 2008-11-26 A. G. Oganesian

We use QCD sum rules to study the possible existence of a \Theta c(3250) charmed pentaquark. We consider the contributions of condensates up to dimension-10 and work at leading order in \alpha_s. We obtain m(\Theta c) = (3.21 +/- 0.13) GeV,…

High Energy Physics - Phenomenology · Physics 2013-10-30 R. M. Albuquerque , S. H. Lee , M. Nielsen

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

The analysis of the sum rules (for two differentchoices of 5-quark currents) indicate that to explain experimental results it is necessary to have some one-particle lower state (and pentaquark is a reliable candidate to this state) while…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. G. Oganesian

We analyse the decay $\Theta_s(1/2^+)\to NK$ in a non-relativistic Fock space description using three and five constituent quarks for the nucleon and the pentaquark, respectively. Following Jaffe and Wilczek \cite{jw}, we assume that…

High Energy Physics - Phenomenology · Physics 2009-11-11 Dmitri Melikhov

We calculate the width of the Theta(1540) pentaquark in a relativistic model in which the pentaquark is considered to be composed of a scalar diquark and a spin 1/2 triquark. We consider both positive and negative parity for the pentaquark.…

High Energy Physics - Phenomenology · Physics 2011-07-19 Hu Li , C. M. Shakin , Xiangdong Li

The pentaquark state of $\Theta^{+}(uudd\bar{s})$ has been observed to decay with two decay modes: $\Theta^+\to n K^+$ and $\Theta^+ \to p K^0$. The decay probability ratio of the two decay modes is studied with general symmetry…

High Energy Physics - Phenomenology · Physics 2008-11-26 Xun Chen , Yajun Mao , Bo-Qiang Ma

In this work we study the Theta(1540) in the framework of QCD sum rules based on (ud)^2\bar{s} diquark clustering as suggested by Jaffe and Wilczek. Within errors, the mass of the pentaquark is compatible with the experimentally measured…

High Energy Physics - Phenomenology · Physics 2009-11-10 Markus Eidemuller

Pentaquark baryons $\Theta^{+}$ and $\Xi^{--}$ are studied in the dual gravity theory of QCD in which simple mass formulae of pentaquarks are derived in the Maldacena prototype model for supersymmetric QCD and a more realistic model for…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Bando , T. Kugo , A. Sugamoto , S. Terunuma

We analyse the width of the $\theta(\frac12^+)$ pentaquark assuming that it is a bound state of two extended spin-zero $ud$-diquarks and the $\bar s$ antiquark (the Jaffe-Wilczek scenario). The width obtained when the size parameters of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Melikhov , S. Simula , B. Stech

In this work, we study the properties of the pseudoscalar hidden-charm tetraquark states by analyzing their two-body strong decays via the QCD sum rules based on rigorous quark-hadron duality. We take into account the vacuum condensates up…

High Energy Physics - Phenomenology · Physics 2026-05-05 Yu-Hang Xu , Zhi-Gang Wang

The mass and meson-current coupling of the diquark-antidiquark states with the quantum numbers $J^{P}=0^{+}$ and quark contents $Z_{q}=[cq][\bar {b} \bar q ]$ and $Z_{s}=[cs][\bar {b} \bar s]$ are calculated using two-point QCD sum rule…

High Energy Physics - Phenomenology · Physics 2017-02-22 S. S. Agaev , K. Azizi , H. Sundu
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