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Related papers: A pentaquark model of the negative parity Lambda(1…

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The masses of the negative parity 70-plet baryons are analyzed in large N_c QCD to order 1/N_c and to first order in SU(3) symmetry breaking. The existing experimental data are well reproduced and twenty new observables are predicted. The…

High Energy Physics - Phenomenology · Physics 2014-11-17 C. L. Schat , J. L. Goity , N. N. Scoccola

A number of candidate multiquark hadrons, i.e., particle resonances with substructures that are more complex than the quark-antiquark mesons and three-quark baryons that are prescribed in the textbooks, have recently been observed. In this…

High Energy Physics - Experiment · Physics 2017-08-02 Stephen Lars Olsen

Within an extended chiral constituent quark model, three- and five-quark structure of the $S_{01}$ resonance $\Lambda(1405)$ is investigated. Helicity amplitudes for the electromagnetic decays ($\Lambda(1405) \to \Lambda(1116)\gamma$,…

Nuclear Theory · Physics 2010-05-28 C. S. An , B. Saghai , S. G. Yuan , Jun He

In two recent papers, we used the hadro-quarkonium model to study the properties of hidden-charm and bottom tetraquarks and pentaquarks. Here, we extend the previous results and calculate the masses of heavy-quarkonium-kaon/hyperon systems.…

High Energy Physics - Phenomenology · Physics 2020-04-23 J. Ferretti , E. Santopinto

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

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

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

We study time correlation functions of operators representing heavy-light K-Lambda like systems at various relative distances r. The heavy quarks, one in each hadron, are treated as static. An anisotropic and asymmetric lattice is used with…

High Energy Physics - Lattice · Physics 2007-05-23 M. S. Cook , H. R. Fiebig

The quark-meson coupling (QMC) model, which has been successfully used to describe the properties of both infinite nuclear matter and finite nuclei, is applied to a systematic study of $\Lambda, \Sigma$ and $\Xi$ hypernuclei. Assumptions…

Nuclear Theory · Physics 2010-02-17 K. Tsushima , K. Saito , J. Haidenbauer , A. W. Thomas

Since the discovery of the $\Lambda(1405)$, it remains poorly described by conventional constituent quark models, and it is a candidate for having an "exotic" meson-baryon or "penta-quark" structure, similar to states recently reported in…

We study the possibility to bind eight quarks in a molecular hadronic system composed of two nucleons and an antikaon, with the quantum numbers of a hexaquark flavour, in particular with strangeness -1, isospin 1/2, parity -, baryonic…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Bicudo

We study the semileptonic decay of $\Lambda_c$ to $\nu l^+$ and $\Lambda(1405)$, where the $\Lambda(1405)$ is seen in the invariant mass distribution of $\pi \Sigma$. We perform the hadronization of the quarks produced in the reaction in…

High Energy Physics - Phenomenology · Physics 2016-01-27 N. Ikeno , E. Oset

Anti-decuplet penta-quark baryon is studied with the quenched anisotropic lattice QCD for accurate measurement of the correlator. Both the positive and negative parity states are studied using a non-NK type interpolating field with I=0 and…

High Energy Physics - Lattice · Physics 2017-08-23 N. Ishii , T. Doi , H. Iida , M. Oka , F. Okiharu , H. Suganuma

Stimulated by various experimental achievements, the study of Kbar N dynamics now enters a new phase. The two-body Kbar N interaction is largely constrained by recent experimental data, and the nature of the Lambda(1405) resonance is being…

Nuclear Theory · Physics 2013-02-08 Tetsuo Hyodo

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

The newly discovered exotic $\Theta$ baryon of mass 1540 MeV (and very small width) truly has a very low mass, if it is a pentaquark system of even parity. A schematic model in which the coherent interaction of $u\bar s$ and $d\bar s$ pairs…

Nuclear Theory · Physics 2014-11-18 Gerald A. Miller

We investigate the symmetry property and the stability of the heptaquark containing two identical heavy antiquarks using color-spin interaction. We construct the wave function of the heptaquark from the Pauli exclusion principle in the…

High Energy Physics - Phenomenology · Physics 2017-09-06 Aaron Park , Woosung Park , Su Houng Lee

We investigate the interaction of an antikaon ($K^-$) with the $^{6}$Li nucleus, described as an $\alpha + d$ cluster system. The study aims to explore the formation of the $\Lambda(1405)$ resonance through the $K^-d$ subsystem in the…

Nuclear Theory · Physics 2026-05-04 Ahmad Naderi Beni , Sajjad Marri

In this work, we carry out the study of heavy flavor pentatuarks with four heavy quarks, which have typical $QQQQ\bar q$ configuration. Within the Chromomagnetic Interaction model, the mass spectrum of these discussed $QQQQ\bar q$…

High Energy Physics - Phenomenology · Physics 2021-07-07 Hong-Tao An , Kan Chen , Zhan-Wei Liu , Xiang Liu

We generalize to five distinct flavors the flavor-spin hyperfine interaction introduced previously for four flavors and used in the study of $uudc\overline{c}$ pentaquark. As a particular case here we study the lowest states of the…

High Energy Physics - Phenomenology · Physics 2023-07-26 Fl. Stancu