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Related papers: Diquarks, Pentaquarks and Dibaryons

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Based on the flavor SU(3) symmetry, we classify all the possible pentaquark baryons made of four quarks and one antiquark. In particular, we present possible multiplets of pentaquarks, their interactions with mesons, and the mass relations…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hungchong Kim , Yongseok Oh

By using of vector diquark ideas in the chiral limit diquark correlations in the relativistic region and imposing HF interactions between quarks in a vector diquark we calculated the mass of two multiquark states (Theta pentaquark and H…

High Energy Physics - Phenomenology · Physics 2007-08-07 Alireza Haghpayma

We study the SU(3) group structure of pentaquark baryons which are made of four quarks and one antiquark. The pentaquark baryons form {1}, {8}, {10}, {10}-bar, {27}, and {35} multiplets in SU(3) quark model. First, the flavor wave functions…

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

In this paper, we consider an exotic baryon (pentaquark) as a bound state of two-particle systems composed of a baryon (nucleon) and a meson.We used a baryon - meson picture to reduce a complicated five-body problem to a simple two-body…

High Energy Physics - Phenomenology · Physics 2016-07-19 Majid Monemzadeh , Narges Tazimi , Shahnaz Babaghodrat

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

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The five-quark amplitudes for the low-lying pentaquarks including the u,d,s-quarks are calculated. The poles of these amplitudes…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. M. Gerasyuta , V. I. Kochkin

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

By using of vector diquark ideas in the chiral limit diquark correlations in the relativistic region and imposing HF interactions between quarks in a vector diquark we calculated the mass of H-dibaryon, also by using of tunneling method we…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alireza Haghpayma

We discuss the mass splittings for the $S$-wave triply heavy pentaquark states with the $QQQq\bar{q}$ $(Q=b,c;q=u,d,s)$ configuration which is a mirror structure of $Q\bar{Q}qqq$. The latter configuration is related with the nature of…

High Energy Physics - Phenomenology · Physics 2019-02-01 Shi-Yuan Li , Yan-Rui Liu , Yu-Nan Liu , Zong-Guo Si , Jing Wu

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

Masses of the ground-state teraquarks composed from heavy $c$ and $b$ quarks and antiquarks are calculated in the diquark-antidiquark picture in the framework of the relativistic quark model based on the quasipotential approach. The…

High Energy Physics - Phenomenology · Physics 2021-01-12 R. N. Faustov , V. O. Galkin , E. M. Savchenko

Roles of instanton induced interactions (III) in the masses of pentaquark baryons, Theta^+ (J=1/2 and 3/2) and Xi^{--}, and a dibaryon, H, are discussed using the MIT bag model in the negative parity case. It is shown that the two-body…

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

We give a review of the calculations of the masses of tetraquarks with two and four heavy quarks in the framework of the relativistic quark model based on the quasipotential approach and QCD. The diquark-antidiquark picture of heavy…

High Energy Physics - Phenomenology · Physics 2021-04-21 R. N. Faustov , V. O. Galkin , E. M. Savchenko

A diquark model is used to investigate single charmed baryons. In this model, baryon is composed of two diquarks and an antiquark. Masses of lowest lying states with $J^P= 1/2 ^ \pm$ are obtained. Some masses are smaller than other…

High Energy Physics - Phenomenology · Physics 2008-08-13 Q. W. Wang

QCD instantons are known to produce deeply bound diquarks which may be used as building blocks in the formation of multiquark states, in particular pentaquarks and dibaryons. We suggest a simple model in which the lowest scalar diquark (and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Edward Shuryak , Ismail Zahed

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

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 pentaquarks are exotic baryons formed of four quarks and an antiquarks. Their existence has been discussed in the literature over the last 30 years or more, first in connection with kaon nucleon scattering data. The subject has been…

High Energy Physics - Phenomenology · Physics 2016-09-06 Fl. Stancu

QCD instantons are known to produce deeply bound diquarks. We study whether it may be used as building blocks in the formation of multiquark states, in particular pentaquarks and dibaryons. A simple model is presented in which the lowest…

High Energy Physics - Phenomenology · Physics 2016-09-06 E. V. Shuryak

We study the group structure of baryon anti-decuplet containing the $\Theta^+$. We derive the SU(3) mass relations among the pentaquark baryons in the anti-decuplet, when there is either no mixing or ideal mixing with the pentaquark octet,…

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