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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

Evidence for a narrow baryon state at 1528 +- 2.6(stat) +- 2.1(syst) MeV is presented in quasi-real photoproduction on a deuterium target through the decay channel p,K0 to p,pi+,pi-. The statistical significance of the peak in the p,K0…

High Energy Physics - Experiment · Physics 2019-08-14 Wolfgang Lorenzon

We investigate the production of the pentaquark $\Theta^+$ baryon via the $\gamma n\to K^-\Theta^+$ and $\gamma p\to \bar{K}^0 \Theta^+$ processes, focusing on the parity of the $\Theta^+$. Using the effective Lagrangians, we calculate the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Seung-Il Nam , Atsushi Hosaka , Hyun-Chul Kim

Recently several experiments have reported evidences for pentaquark $\Theta^+$. H1 experiment at HERA-B has also reported evidence for $\Theta_c$. $\Theta^+$ is interpreted as a bound state of an $\bar s$ with other four light quarks $udud$…

High Energy Physics - Phenomenology · Physics 2011-01-27 Xiao-Gang He , Xue-Qian Li

In chiral soliton models for baryons the computation of hadronic decay widths of baryon resonances is a long standing problem. For the three flavor Skyrme model I present a solution to this problem that satisfies large--$N_C$ consistency…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Weigel

The experimental signature of an S=+1 baryon of mass 1540 MeV and width 10-25 MeV has led to speculation that this is an exotic baryon consisting of 4 quarks and 1 antiquark lying at the top of a $\bar{10}$ SU(3) multiplet. The observed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Steven Golbeck , Mikhail Savrov

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

Several recent experiments have reported evidence for a narrow baryon resonance with positive strangeness ($\Theta^+$) at a mass of 1.54 GeV/$c^2$. Baryons with $S=+1$ cannot be conventional $qqq$ states and the reports have thus generated…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. R. Dzierba , D. Krop , M. Swat , A. P. Szczepaniak , S. Teige

Assuming that the recently observed $\Theta^+$ and $\Xi^{--}$ are members of an anti-decuplet of SU(3), decays to ground state baryons and mesons are calculated using an effective Lagrangian which incorporates chiral and SU(3) symmetry. We…

High Energy Physics - Phenomenology · Physics 2014-11-17 Thomas Mehen , Carlos Schat

The newly confirmed pentaquark state $P_c(4312)$ has been treated as a weakly bound $(\Sigma_c\bar{D})$ state by a well-established chiral constituent quark model and by a dynamical calculation on quark degrees of freedom where the quark…

High Energy Physics - Phenomenology · Physics 2020-05-20 Yubing Dong , Pengnian Shen , Fei Huang , Zongye Zhang

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

The exotic baryon $\Theta^+(uudd\bar{s})$ is studied with microscopic calculations in a quark model by using a method of antisymmetrized molecular dynamics(AMD). We predict narrow states, $J^\pi=1/2^+(I=0)$, $J^\pi=3/2^+(I=0)$, and…

High Energy Physics - Phenomenology · Physics 2017-08-23 Y. Kanada-En'yo , O. Morimatsu , T. Nishikawa

We review the current status of the exotic pentaquark baryons. After a brief look at experiments of both positive and negative results, we discuss theoretical methods to study the structure and reactions for the pentaquarks. First we…

High Energy Physics - Phenomenology · Physics 2008-11-26 Atsushi Hosaka

The existence of the $\Theta^+$ pentaquark requires a peculiar mechanism to explain its stability. Looking at quark clusters, notably diquark and triquark configurations, such a mechanism may be found in the color-magnetic interaction…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. J. Mulders , P. Jimenez Delgado

We estimate the decay rates of $\eta_c\rightarrow 2\gamma$, $\eta_c'\rightarrow 2\gamma$, and $J/\psi\rightarrow e^+ e^-$, $\psi^\prime\rightarrow e^+e^-$, by taking into account both relativistic and QCD radiative corrections. The decay…

High Energy Physics - Phenomenology · Physics 2009-10-28 Kuang-Ta Chao , Han-Wen Huang , Jing-Hua Liu , Jian Tang

The exclusive reaction $\gamma p \to \bar K^0 K^+ n$ was studied in the photon energy range between 1.6-3.8 GeV searching for evidence of the exotic baryon $\Theta^+(1540)\to nK^+$. The decay to $nK^+$ requires the assignment of strangeness…

High Energy Physics - Experiment · Physics 2010-04-06 M. Battaglieri , R. De Vita , V. Kubarovsky , L. Guo , G. S. Mutchler , P. Stoler , D. P. Weygand , the CLAS Collaboration

We study the decay of Theta+ in a non-relativistic quark model. The wave function of Theta+ is constructed for the two cases JP = 1/2+- as products of color, spin, flavor and orbital parts respecting total antisymmetrization among the four…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Hosaka , M. Oka , T. Shinozaki

Identifying the Roper N(1440) and N(1710) as the pentaquark octet and anti-decuplet, respectively, we analyze their main decay modes in the diquark picture. The ratio of the partial decay widths is largely consistent with the nearly ideal…

High Energy Physics - Phenomenology · Physics 2007-05-23 Deog Ki Hong

We used an effective Lagrangian approach to investigate the production of the anticharmed pentaquark state $P_{\bar{c}s}^{(*)-}$ with the minimal quark content $\bar{c}sudd$ in the $\Lambda_b^0$ decay and its decay into the $\Lambda…

High Energy Physics - Phenomenology · Physics 2025-01-27 Shi-Dong Liu , Xiao-Yun Wang , Xiao-Hai Liu , Gang Li

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