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

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We test a pentaquark model of the negative parity hyperon Lambda(1405). We use a model where valence four quarks and one antiquark move in a potential relativistically and interact with each other and themselves through gluon and NG boson.…

High Energy Physics - Phenomenology · Physics 2007-08-20 Takashi Inoue

We study a pentaquark model of the negative parity hyperon Lambda(1405). We choose a specific quark configuration for trial, and use the perturbative chiral quark model extended to four quarks and one anti-quark system. We calculate a…

High Energy Physics - Phenomenology · Physics 2009-11-11 Takahi Inoue

We investigate the negative-parity baryon spectra in quenched lattice QCD. We employ the anisotropic lattice with standard Wilson gauge and O(a) improved Wilson quark actions at three values of lattice spacings with renormalized anisotropy…

High Energy Physics - Lattice · Physics 2009-11-10 Y. Nemoto , N. Nakajima , H. Matsufuru , H. Suganuma

$\Lambda(1405)$ is one of the interesting particles with its unclear structure and distinct properties. It has a light mass compared to its non-strange counterpart, despite the strange quark it carries. This situation puts the investigation…

High Energy Physics - Phenomenology · Physics 2023-10-26 K. Azizi , Y. Sarac , H. Sundu

We review briefly recent studies of the Lambda(1405) spectrum in Lattice QCD. Ordinary three-quark pictures of the Lambda(1405) in quenched Lattice QCD fail to reproduce the mass of the experimental value, which seems to support the…

High Energy Physics - Lattice · Physics 2007-05-23 Y. Nemoto , N. Nakajima , H. Matsufuru , H. Suganuma

We study negative-parity baryon spectra in quenched anisotropic lattice QCD. The negative-parity baryons are measured as the parity partner of the ground-state baryons. In addition to the flavor octet and decuplet baryons, we pay much…

High Energy Physics - Lattice · Physics 2009-11-10 Y. Nemoto , N. Nakajima , H. Matsufuru , H. Suganuma

Low-lying $\Lambda$ baryons with spin 1/2 are analyzed in two-flavor lattice QCD. In order to extract two low-lying states for each parity, we construct $2 \times 2$ cross correlators from flavor SU(3) ``octet'' and ``singlet'' baryon…

High Energy Physics - Lattice · Physics 2011-03-10 Toru T. Takahashi , Makoto Oka

The mechanism for the formation of the $\Lambda(1405)$ resonance is studied in a chiral quark model that includes quark-meson as well as contact (four point) interactions. The negative-parity $S$-wave scattering amplitudes for strangeness…

Nuclear Theory · Physics 2022-07-13 B. Golli , H. Osmanović , S. Širca

The low mass of the $\Lambda(1405)$ hyperon with $j^P = 1/2^-$, which is higher than the ground state $\Lambda(1116)$ mass by 290 MeV, is difficult to understand in quark models. We analyze the hyperon spectrum in the bound state approach…

Nuclear Theory · Physics 2015-06-03 Yongseok Oh

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

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 light-quark sector of the Lambda(1405) baryon is examined in the context of the recent discovery of a dominant antikaon-nucleon composition at low quark masses. Further evidence for this interpretation of the Lambda(1405) is presented,…

High Energy Physics - Lattice · Physics 2017-03-30 Jonathan M. M. Hall , Waseem Kamleh , Derek B. Leinweber , Benjamin J. Menadue , Benjamin J. Owen , Anthony W. Thomas

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

The Lambda(1405) baryon resonance plays an outstanding role in various aspects in hadron and nuclear physics. It has been considered that the Lambda(1405) resonance is generated by the attractive interaction of the antikaon and the nucleon,…

Nuclear Theory · Physics 2011-11-11 Tetsuo Hyodo , Daisuke Jido

Weak radiative hyperon decays are considered in the framework of a quark model. The phenomenological model includes 1-quark transitions with the effective $sd\gamma$-vertex and 2-quark ones with the W-exchange $s+u\to u+d+\gamma$ and turns…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. N. Dubovik , V. S. Zamiralov , S. N. Lepshokov

The properties of the Lambda(1405) resonance are key ingredients for determining the antikaon-nucleon interaction in strangeness nuclear physics, and the novel internal structure of the Lambda(1405) is of great interest in hadron physics,…

High Energy Physics - Phenomenology · Physics 2016-08-24 Yuki Kamiya , Kenta Miyahara , Shota Ohnishi , Yoichi Ikeda , Tetsuo Hyodo , Eulogio Oset , Wolfram Weise

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

We have investigated uudd\sbar pentaquarks by employing quark models with the meson exchange and the effective gluon exchange as qq and q\qbar interactions. The system for five quarks is dynamically solved; two quarks are allowed to have a…

High Energy Physics - Phenomenology · Physics 2017-08-23 Sachiko Takeuchi , Kiyotaka Shimizu

The splittings between positive parity pentaquarks containing a single heavy (c,b) antiquark and four light (u,d) quarks are investigated in models having spin-dependent interactions generated by either effective Goldstone boson exchange or…

High Energy Physics - Phenomenology · Physics 2009-11-10 K. Maltman
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