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Related papers: A pentaquark picture of Lambda(1405)

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We study the stability of the pentaquarks uuddQbar, uudsQbar and udssQbar (Q = c, b, or t) of positive parity in a constituent quark model based on Goldstone boson exchange interaction between quarks. The pentaquark parity is the antiquark…

High Energy Physics - Phenomenology · Physics 2009-12-30 Fl. Stancu

We construct the complete set of positive parity pentaquarks, which correspond in the quark model to {\bar s} q^{Nc+1} states with one unit of orbital angular momentum L=1. In the large Nc limit they fall into the K=1/2 and K=3/2 irreps…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dan Pirjol , Carlos Schat

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

In a nonrelativistic potential quark model framework, we carry out a calculation of the mass spectrum for the low-lying $1S$ all-heavy pentaquark state by adopting the explicitly correlated Gaussian method. The obtained states are compact…

High Energy Physics - Phenomenology · Physics 2024-10-31 Zhi-Biao Liang , Feng-Xiao Liu , Xian-Hui Zhong

In this talk, multiquarks are studied microscopically in a standard quark model. In pure ground-state pentaquarks the short-range interaction is computed and it is shown to be repulsive. An additional quark-antiquark pair is then…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Bicudo

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 study the coupling of the Lambda(1520)= Lambda* resonance to the \bar K* vector meson and nucleon. This coupling is not directly measured from the resonance decay, but is expected to be important in hyperon production reactions, in…

High Energy Physics - Phenomenology · Physics 2014-11-18 T. Hyodo , Sourav Sarkar , A. Hosaka , E. Oset

Assuming that the recently observed hidden-charm pentaquark state, $P_c(4450)$, is of molecular nature as predicted in the unitary approach, we propose to study the decay of $\Xi^-_b\rightarrow J/\psi K^- \Lambda$ to search for the…

High Energy Physics - Phenomenology · Physics 2016-06-22 Hua-Xing Chen , Li-Sheng Geng , Wei-Hong Liang , Eulogio Oset , En Wang , Ju-Jun Xie

The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the first time into Lambda(1405) K, Lambda(1520) K, Sigma(1385) K, Lambda K*, and Sigma K*, are examined in a relativized quark pair creation…

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

The penta-quark(5Q) Theta^+(1540) is studied in anisotropic lattice QCD with renormalized anisotropy a_s/a_t=4 for a high-precision measurement. Both the positive and the negative parity 5Q baryons are studied using a non-NK type…

High Energy Physics - Lattice · Physics 2009-11-10 N. Ishii , T. Doi , H. Iida , M. Oka , F. Okiharu , H. Suganuma

Under the working hypothesis that the structure of a bound hadron is modified by its interactions with other hadrons, one may expect to see changes in carefully chosen observables. In the light of a recent proposal to measure the axial…

High Energy Physics - Phenomenology · Physics 2017-11-22 P. A. M. Guichon , A. W. Thomas

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 perform a five-body calculation for pentaquark $(q^4\bar{q})$ state of $\Lambda(1405)$ as well as the three-body calculations for the ground state baryons and the $\Lambda(1405)$, and two-body calculations for mesons. The hamiltonian,…

Nuclear Theory · Physics 2009-11-11 H. Nemura , C. Nakamoto

The pentaquark is studied in a simple model of confinement where the quarks and the antiquark are linked by flux tubes of minimal cumulated length, and the Coulomb-like interaction, the spin-dependent terms and the antisymmetrization…

High Energy Physics - Phenomenology · Physics 2014-11-20 Jean-Marc Richard

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

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

Decays of $\Lambda$ in nuclei, nonmesonic mode, are studied by using the $\Lambda N \to NN$ weak transition potential derived from the meson exchange mechanism and the direct quark mechanism. The decay rates are calculated both for the…

Nuclear Theory · Physics 2009-10-31 K. Sasaki , T. Inoue , M. Oka

We study the behavior with the number of colors (Nc) of the two poles associated to the Lambda(1405) resonance obtained dynamically within the chiral unitary approach. The leading order chiral meson-baryon interaction manifests a nontrivial…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tetsuo Hyodo , Daisuke Jido , Luis Roca

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

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