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Related papers: Narrow Pentaquark States in a Quark Model with Ant…

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

High Energy Physics - Phenomenology · Physics 2009-11-10 Y. Kanada-En'yo , O. Morimatsu , T. Nishikawa

A dynamical calculation of pentaquark systems with quark contents $uudd\bar{s}$ is performed in the framework of quark delocalization color screening model with the help of resonating group method. The effective potentials between baryon…

High Energy Physics - Phenomenology · Physics 2019-08-14 Xuejie Liu , Hongxia Huang , Jialun Ping

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

Evidence for a narrow baryon state is found in quasi-real photoproduction on a deuterium target through the decay channel p K^0_S --> p pi^+ pi^-. A peak is observed in the p K^0_S invariant mass spectrum at 1528 +/- 2.6 (stat) +/-2.1…

High Energy Physics - Experiment · Physics 2012-08-03 HERMES Collaboration , A. Airapetian

If Jaffe and Wilczek's diquark picture for $\Theta_5$ pentaquark is correct, there should also exist a $SU_F$(3) pentaquark octet and singlet with no orbital excitation between the diquark pair, hence $J^P={1/2}^-$. These states are lighter…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Zhang , Y. -R. Liu , P. -Z. Huang , W. -Z. Deng , X. -L. Chen , Shi-Lin Zhu

A model recently introduced by Jaffe and Wilczek based on the quarks being dynamically bound into diquarks has been used to predict that the recently observed exotic baryons (pentaquarks) fall into a nearly ideally mixed combination of an…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas D. Cohen

We propose a collective stringlike model of pentaquarks with the geometry of an equilateral tetrahedron in which the four quarks are located at the four corners and the antiquark in its center. The nonplanar equilibrium configuration is a…

High Energy Physics - Phenomenology · Physics 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

We examine the decays of nonstrange baryons to the final states $\Delta\pi$, $N\rho$, $N\eta$, $N\eta^\prime$, $N\omega$, $N1/2^+(1440)\pi$, and $\Delta3/2^+(1600)\pi$, in a relativized pair-creation($^3P_0$) model which has been developed…

Nuclear Theory · Physics 2014-11-18 Simon Capstick , Winston Roberts

The narrow width of the exotic narrow baryon resonance $\Theta^+$ might be explained by mixing between the two nearly degenerate states that arise in models with two diquarks and an antiquark. The only open $\Theta^+$ decay channel is $KN$.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Marek Karliner , Harry J. Lipkin

We have investigated negative-parity uudd\bar{s} pentaquarks by employing a quark model with the meson exchange and the effective gluon exchange as qq and q\bar{q} interactions. The system for the five quarks is dynamically solved; the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sachiko Takeuchi , Kiyotaka Shimizu

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

SVD-2 experiment data have been analyzed to search for an exotic baryon state, the $\Theta^+$-baryon, in a $pK^0_s$ decay mode at $70 GeV/c$ on IHEP accelerator. The reaction $pA \to pK^0_s+X$ with a limited multiplicity was used in the…

High Energy Physics - Experiment · Physics 2012-08-27 SVD Collaboration

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 discuss the properties of the pentaquark in a collective stringlike model with a nonplanar configuration of the four quarks and the antiquark. In an application to the mass spectrum of exotic Theta baryons, we find that the ground state…

High Energy Physics - Phenomenology · Physics 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

We study the five-quark system $uudd{\bar s}$ in the standard non-relativistic quark model by solving the scattering problem. Using the Gaussian Expansion Method (GEM), we perform the almost precise multi-quark calculations by treating a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Emiko Hiyama , Hideo Suganuma , Masayasu Kamimura

The properties of the Theta^{+} and Xi^{--}_{3/2} exotic baryons have been investigated in the framework of diquark- diquark-antiquark system. A model for diquark suggested in an analogy with the quasi-particle in a crystal lattice has been…

High Energy Physics - Phenomenology · Physics 2014-11-18 A. Bhattacharya , B. Chakrabarti , S. Mani , S. N. Banerjee

The 1/N expansion for exotic baryons is developed, and applied to the masses, meson couplings and decay widths. Masses and widths of the 27 and 35 pentaquark states in the same tower as the Theta+ are related by spin-flavor symmetry. The 27…

High Energy Physics - Phenomenology · Physics 2009-11-10 Elizabeth Jenkins , Aneesh V. Manohar

Recent experimental evidence for the Theta^+(1540) has given rise to much theoretical interest in exotic baryons. The Theta^+ is a baryon that has strangeness S=+1, meaning that it contains an anti-strange quark. Thus it cannot be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Margaret E Wessling

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 color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a schematic study of the masses of the $J^P=1^+$ tetraquarks in the anti-decuplet representation. After diagonalizing the mass matrix, we find…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ying Cui , Xiao-Lin Chen , Wei-Zhen Deng , Shi-Lin Zhu
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