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Related papers: A pentaquark picture of Lambda(1405)

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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

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

A relativistic constituent quark model is used to calculate the semileptonic beta decay of nucleons and hyperons. The parameters of the model, namely, the constituent quark mass and the confinement scale, are fixed by a previous calculation…

High Energy Physics - Phenomenology · Physics 2011-08-17 Felix Schlumpf

In some models, exotic baryons with strangeness and anticharm or antibeauty should exist and even be stable against strong decay. We consider the stability of such possible exotic baryons, which in the constituent quark picture are called…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. B. Lichtenberg

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

Five-quark (5Q) picture of Lambda(1405) is studied using quenched lattice QCD with an exotic 5Q operator of N\bar{K} type. To discreminate mere N\bar{K} and \Sigma\pi scattering states, Hybrid Boundary Condition (HBC), a flavor-dependent…

High Energy Physics - Lattice · Physics 2008-11-26 Noriyoshi Ishii , Takumi Doi , Makoto Oka , Hideo Suganuma

The weak $\Lambda N\to NN$ transition is studied in the valence quark model approach. The quark component of the two baryon system is described in the quark cluster model and the weak transition potential is calculated by evaluating the…

High Energy Physics - Phenomenology · Physics 2016-09-01 Takashi Inoue , Sachiko Takeuchi , Makoto Oka

It is pointed out that the previously suggested interpretation of the hidden-charm pentaquarks $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$ as molecular bound states of $\Sigma_c \bar D$ and $\Sigma_c \bar D^*$ baryon-meson pairs gives rise to…

High Energy Physics - Phenomenology · Physics 2019-08-28 M. B. Voloshin

In a diquark-diquark-antiquark picture of the pentaquark we study the decay $\Theta \rightarrow K^{+} n$ within the framework of QCD sum rules. After evaluation of the relevant three-point function, we extract the coupling $g_{\Theta nK}$…

High Energy Physics - Phenomenology · Physics 2009-11-11 M. Eidemüller , F. S. Navarra , M. Nielsen , R. Rodrigues da Silva

There are different assumptions on the substructure of the pentaquarks $P_c(4380)$ and $P_c(4450)$, newly founded in $J/\psi N $ invariant mass by the LHCb collaboration, giving consistent mass results with the experimental observations.…

High Energy Physics - Phenomenology · Physics 2018-08-01 K. Azizi , Y. Sarac , H. Sundu

Light and heavy pentaquarks are described within a constituent quark model based on a spin-flavor hyperfine interaction. In this model the lowest state acquires positive parity. The masses of the light antidecuplet members are calculated…

High Energy Physics - Phenomenology · Physics 2009-11-11 Fl. Stancu

Assuming the two diquark structure for the pentaquark state as advocated in the Jaffe-Wilczek model, there exist exotic parity-even anti-sextet and parity-odd triplet heavy pentaquark baryons. The theoretical estimate of charmed and bottom…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hai-Yang Cheng , Chun-Khiang Chua , Chien-Wen Hwang

The fully-charm and -bottom pentaquarks, \emph{i.e.} $cccc\bar{c}$ and $bbbb\bar{b}$, with spin-parity quantum numbers $J^P=\frac{1}{2}^-$, $\frac{3}{2}^-$ and $\frac{5}{2}^-$, are investigated within a Lattice-QCD inspired quark model,…

High Energy Physics - Phenomenology · Physics 2022-07-20 Gang Yang , Jialun Ping , Jorge Segovia

For almost 50 years the structure of the Lambda(1405) resonance has been a mystery. Even though it contains a heavy strange quark and has odd parity, its mass is lower than any other excited spin-1/2 baryon. Dalitz and co-workers speculated…

We aim to construct quark hadron physics based on QCD. First, using lattice QCD, we study mass spectra of positive-parity and negative-parity baryons in the octet, the decuplet and the singlet representations of the SU(3) flavor. In…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. Suganuma , N. Ishii , H. Matsufuru , Y. Nemoto , T. T. Takahashi

The nature of the $ \Lambda(1405) $ has been a puzzle for decades, whether it is a standard three-quark baryon, a hybrid baryon or a baryon-meson molecule. More information on the decay channels of this particle and its strong, weak and…

High Energy Physics - Phenomenology · Physics 2018-03-13 K. Azizi , B. Barsbay , H. Sundu

Within an extended chiral constituent quark model, three- and five-quark structure of the $S_{01}$ resonance $\Lambda(1405)$ is investigated with respect to the coupling constants $g^2_{\Lambda^* \pi \Sigma}$ and $g^2_{\Lambda^* \bar{K}…

Nuclear Theory · Physics 2011-07-28 Chunsheng An , Bijan Saghai

In this article, we take the point of view that the pentaquark state $\Theta^+(1540)$ has negative parity, and choose the diquark-triquark type interpolating current to calculate the strong coupling constant $g_{\Theta NK}$ in the QCD sum…

High Energy Physics - Phenomenology · Physics 2009-11-11 Zhi-Gang Wang , Wei-Min Yang , Shao-Long Wan

We consider the mass splittings and strong decays of members of the lowest-lying pentaquark multiplet, which we take to be a parity-odd antidecuplet. We derive useful decompositions of the quark model wave functions that allow for easy…

High Energy Physics - Phenomenology · Physics 2015-06-25 Carl E. Carlson , Christopher D. Carone , Herry J. Kwee , Vahagn Nazaryan

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