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Related papers: Theta++ from QCD sum rule

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Exotic penta-quark baryon with strangeness +1, \Theta^+, is studied in the QCD sum rule approach. We derive sum rules for the positive and negative parity baryon states with J=1/2 and I=0. It is found that the standard values of the QCD…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jun Sugiyama , Takumi Doi , Makoto Oka

We study $IJ^P=0{3/2}^\pm$ and $1{3/2}^\pm$ pentaquark states with $S=+1$ in the QCD sum rule approach. The QCD sum rule for positive parity states and that for negative parity are independently derived. The sum rule suggests that there…

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

The QCD sum rule for the pentaquark $\Theta^+$, first analyzed by Sugiyama, Doi and Oka, is reanalyzed with a phenomenological side that explicitly includes the contribution from the two-particle reducible kaon-nucleon intermediate state.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Su Houng Lee , Hungchong Kim , Youngshin Kwon

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

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

QCD sum rule is applied to the pentaquark spectroscopy. It is concluded that no positive parity state is seen in low energy region, while there may exist negative parity states at around 1.5 GeV. Choice of interpolating local operators and…

High Energy Physics - Phenomenology · Physics 2017-08-23 Makoto Oka

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

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

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

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

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

We study pentaquark $\Theta^{+} (I=0,J=1/2)$ in the QCD sum rules emphasizing that we can not extract any properties of the pentaquark outside of the Borel window. To find the appropriate Borel window, we prepare a favorable set up of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Toru Kojo , Daisuke Jido , Arata Hayashigaki

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

We perform a QCD sum rule analysis for the pentaquark baryon Theta^+ with the non-interacting $KN$ contribution treated carefully. The coupling of the Theta^+ current to the $KN$ state is evaluated by applying the soft kaon theorem and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Youngshin Kwon , Atsushi Hosaka , Su Houng Lee

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

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

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

The QCD sum rule method is formulated for the strangeness +1 pentaquark baryon with isospin I=0 and spin-parity J^P = 3/2^\pm. The spin-3/2 states are considered to be narrower than the spin-1/2 ones, and thus may provide a natural…

High Energy Physics - Phenomenology · Physics 2014-11-18 P. Gubler , D. Jido , T. Kojo , T. Nishikawa , M. Oka

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

In this article, we study the $J^{PC}=0^{++}$ and $2^{++}$ $QQ\bar{Q}\bar{Q}$ tetraquark states with the QCD sum rules, and obtain the predictions $M_{X(cc\bar{c}\bar{c},0^{++})} =5.99\pm0.08\,\rm{GeV}$, $M_{X(cc\bar{c}\bar{c},2^{++})}…

High Energy Physics - Phenomenology · Physics 2017-07-03 Zhi-Gang Wang
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