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A search for narrow Theta(1540)^+, a candidate for pentaquark baryon with positive strangeness, has been performed in an exclusive proton-induced reaction p+C(N) \to Theta^+ \bar{K}^0 + C(N) on carbon nuclei or quasifree nucleons at…

In the chiral quark soliton model the smallness of $\Theta^+$ width is due to the cancellation of the coupling constants which are of different order in $N_c$. We show that taking properly into account the flavor structure of relevant SU(3)…

High Energy Physics - Phenomenology · Physics 2016-09-06 Michal Praszalowicz

P-wave pentaquarks with strangeness +1, I=0 and J^P=1/2^+ are studied in the non-relativistic quark model with instanton induced interaction (III). We present their mass splittings and orbital-spin-isospin-color structures. It is found that…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tetsuya Shinozaki , Makoto Oka , Sachiko Takeuchi

Heavy baryon chiral perturbation theory for pentaquarks is applied beyond leading order. The mass splitting in the pentaquark anti-decuplet is calculated up to NNLO. An expansion in the coupling of pentaquarks to non-exotic baryons…

High Energy Physics - Phenomenology · Physics 2009-11-10 Vivek Mohta

We study the recently discovered Theta^+ baryon in the context of the perturbative chiral quark model. The basic configuration of the Theta^+ is set up as a pentaquark bound state, where the single particle wave functions are the ground…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Inoue , V. E. Lyubovitskij , Th. Gutsche , Amand Faessler

The strange-anticharmed Pentaquark is a uud(cbar)s or udd(cbar)s five-quark baryon that is expected to be either a narrow resonance, or possibly even stable against strong decay. We describe this hyperon here; its structure, binding energy…

High Energy Physics - Phenomenology · Physics 2008-02-03 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

We study the photoproduction of the exotic pentaquark Theta^+ baryon with the vector kaon, assuming that the quantum numbers of the Theta^+ to be J^P=3/2^(+-) and J^P=1/2^+. Scalar meson kappa(800)-exchange is also taken into account. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 Seung-Il Nam , Atsushi Hosaka , Hyun-Chul Kim

We study $np\to \Lambda\Theta^{+}$ and $np\to \Sigma^{0}\Theta^{+}$ processes for both of the positive and negative parities of the $\Theta^{+}$. Employing the effective chiral Lagrangians for the $KNY$ and $K^*NY$ interactions, we…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. I. Nam , A. Hosaka , H. -Ch. Kim

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

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

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

The recent experimental results of LHCb collaboration suggested the existence of pentaquark states with charmonium. To understand the structure of the states, a dynamical calculation of 5-quark systems with quantum numbers…

High Energy Physics - Phenomenology · Physics 2017-01-18 Gang Yang , Jialun Ping

We study the CP violating effects in the decay of $\eta\to\pi^+\pi^-\gamma$. We show that to have CP violation in the decay, one has to consider both linear and circular photon polarizations. In the standard model, the polarizations are…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. Q. Geng , J. N. Ng , T. H. Wu

The CP conserved non leptonic $K\to \pi \pi \pi$ decays are discussed within the chiral quark model, including chiral perturbation theory corrections. All amplitudes are parameterized in terms of quark and gluon condensate and the…

High Energy Physics - Phenomenology · Physics 2009-11-10 E. I. Lashin

We investigate medium modifications of the pentaquark $\Theta^+$ in dense medium, taking into account different parities of the exotic $\Theta^+$ baryon. We find that the chemical potential of the $\Theta^+$ is shifted in a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hyun-Chul Kim , Chang-Hwan Lee , Hee-Jung Lee

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, we measure their $ 3 \times 3 $ correlation matrix and obtain the…

High Energy Physics - Phenomenology · Physics 2017-08-23 Ting-Wai Chiu , Tung-Han Hsieh

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

In this study, pentaquark Pc(4380) composed of a baryon sigma_c and a D_* meson is considered. Pentaquark is as a bound state of two-body systems composed of a baryon and a meson. The calculated potential will be expanded and replaced in…

High Energy Physics - Phenomenology · Physics 2020-12-14 F. Chezani Sharahi , M. Monemzadeh

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
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