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In this work we investigate the consequences of the Jaffe and Wilczek diquark model in the framework of QCD sum rules. An analysis of the Theta^+(1540) as (ud)^2\bar{s} state shows that the mass of the pentaquark is compatible with the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Markus Eidemuller

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

We consider a $[ud]^2\bar{s}$ current in the QCD sum rule framework to study the mass of the recently observed pentaquark state $\Theta^+(1540)$, obtaining good agreement with the experimental value. We also study the mass of the pentaquark…

High Energy Physics - Phenomenology · Physics 2015-06-25 R. D. Matheus , F. S. Navarra , M. Nielsen , R. Rodrigues da Silva , S. H. Lee

We construct QCD sum rules for the anti-charmed pentaquark $\Theta_c (3099)$, recently reported at HERA. The sum rules are constructed similarly with the $\Theta^+ (1540)$ sum rules using the anti-charmed analogue of the $\Theta^+$…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hungchong Kim , Su Houng Lee , Yongseok Oh

In this article, we study the magnetic moment of the pentaquark state $ \Theta^+(1540)$ as diquark-diquark-antiquark ($[ud][ud]\bar{s}$) state in the framework of the light-cone QCD sum rules approach. The numerical results indicate the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-Gang Wang , Shao-Long Wan , Wei-Min Yang

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 masses of pentaquarks $uudd\bar s$ are calculated within the framework of a semirelativistic effective QCD Hamiltonian, using a diquark picture. This approximation allows a correct treatment of the confinement, assumed here to be…

High Energy Physics - Phenomenology · Physics 2009-11-10 C. Semay , F. Brau , B. Silvestre-Brac

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 consider the $\Theta^+(1540)$ pentaquark in the string model that correctly reproduces the linear Regge trajectories for the case of orbital excitations of light $q\bar q$ mesons and $qqq$ baryons. Assuming (and arguing in favour of) the…

High Energy Physics - Phenomenology · Physics 2009-11-11 M. I. Krivoruchenko , B. V. Martemyanov , Amand Faessler , C. Fuchs

We consider a $[ud]^2\bar{s}$ current, in the finite-density QCD sum rule approach, to investigate the scalar and vector self-energies of the recently observed pentaquark state $\Theta^+(1540)$, propagating in nuclear mater. We find that,…

Nuclear Theory · Physics 2009-11-10 F. S. Navarra , M. Nielsen , K. Tsushima

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 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

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

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

According to QCD, there exists a broken dynamical supersymmetry between an antiquark and a diquark. This supersymmetry can be used to relate the mass of a pentaquark to the mass of an antibaryon by replacing two antiquarks in an antibaryon…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg

The masses of $uudd\bar s $ and $uudd\bar d$ pentaquarks are evaluated in a framework of the Effective Hamiltonian approach to QCD using the Jaffe-Wilczek $[ud]^2\bar q$ approximation. The mass of the $[ud]^2\bar s$ state is found to be…

High Energy Physics - Phenomenology · Physics 2015-06-25 I. M. Narodetskii , Yu. A. Simonov , M. A. Trusov , A. I. Veselov

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

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 study the magnetic moment of the pentaquark state $ \Theta^+(1540)$ with the QCD sum rules approach in the external electromagnetic field. The numerical results indicate the magnetic moment of the pentaquark state $…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-Gang Wang , Wei-Min Yang , Shao-Long Wan

The QCD sum rule technique is employed to investigate pentaquark states with strangeness S = +1 and IJ^P = 0,1/2^\pm, 1,1/2^\pm, 0,3/2^\pm, 1,3/2^\pm. Throughout the calculation, emphasis is laid on the establishment of a valid Borel…

High Energy Physics - Phenomenology · Physics 2010-01-15 P. Gubler , D. Jido , T. Kojo , T. Nishikawa , M. Oka

Additional broader I=0 states in the KN channel near $\Theta^+$(1540) are expected in many models, making the absence of any signature in the K$^+$-deuteron scattering data even more puzzling. In an ideal "three-body" picture the $\Theta$…

High Energy Physics - Phenomenology · Physics 2009-11-10 Shmuel Nussinov
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