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Related papers: Is two-poles' $\Lambda(1405)$ one state or two?

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The pole structure of the $\Lambda(1405)$ is examined by fitting the couplings of an underlying Hamiltonian effective field theory to cross sections of $K^- p$ scattering in the infinite-volume limit. Finite-volume spectra are then obtained…

Nuclear Theory · Physics 2017-02-01 Zhan-Wei Liu , Jonathan M. M. Hall , Derek B. Leinweber , Anthony W. Thomas , Jia-Jun Wu

We investigate the photoproduction of $K^*$ vector meson for the study of the $\Lambda(1405)$ resonance. The invariant mass distribution of $\pi\Sigma$ shows a different shape from the nominal one, peaking at 1420 MeV. This is considered as…

Nuclear Theory · Physics 2007-05-23 T. Hyodo , A. Hosaka , M. J. Vicente Vacas , E. Oset

We discuss the spacial structure of the resonance state, Lambda(1405), solving the Schrodinger equation with the KbarN local potential. The potential is constructed by paying attention to the two points, the constraint from the recent…

Nuclear Theory · Physics 2015-12-10 Kenta Miyahara , Tetsuo Hyodo

We investigated the dependence of the $K^- d$ scattering length on models of $\bar{K}N$ interaction with one or two poles for $\Lambda(1405)$ resonance. The $\bar{K}NN - \pi \Sigma N$ system is described by coupled-channel Faddeev equations…

Nuclear Theory · Physics 2012-10-10 N. V. Shevchenko

The radiative decay of $\Lambda (1405)$ is investigated from the viewpoint of compositeness, which corresponds to the amount of two-body states composing resonances as well as bound states. For a $\bar{K}N (I=0)$ bound state without…

Nuclear Theory · Physics 2014-02-26 T. Sekihara , S. Kumano

The $K^- p \to \pi^0 \pi^0 \Sigma^0$ reaction is studied within a chiral unitary model. The distribution of $\pi^0 \Sigma^0$ states forming the $\Lambda(1405)$ shows, in agreement with a recent experiment, a peak at 1420 MeV and a…

Nuclear Theory · Physics 2009-11-11 E. Oset , V. K. Magas , A. Ramos

We study the $K\Lambda(1405)$ configuration of the $K\bar{K}N$ system by considering $K\pi\Sigma$ as a coupled channel. We solve the Faddeev equations for these systems and find confirmation of the existence of a new $N^{*}$ resonance…

Nuclear Theory · Physics 2011-11-10 A. Martínez Torres , D. Jido

The $\Lambda(1405)$ has been one of the most controversial exotic baryons. If the $\Lambda(1405)$ possesses a two-pole molecular structure, these poles are expected to evolve differently towards the SU(3) limit. From an analysis of a recent…

High Energy Physics - Phenomenology · Physics 2025-06-04 Zejian Zhuang , Raquel Molina , Jun-Xu Lu , Li-Sheng Geng

In this work we investigate different possible explanations for the observed low mass {\Lambda}(1405) signal associated to the production of the {\Lambda}(1405) in p+p reactions at 3.5 GeV beam kinetic energy measured by the HADES…

Nuclear Experiment · Physics 2015-06-16 Johannes Siebenson , Laura Fabbietti

This work aims at determining the composition of certain $N^*$ and $\Delta$ resonances, i.e. whether they are compact states formed directly by quarks and gluons, or hadronic molecules generated from the meson-baryon interaction. The…

Nuclear Theory · Physics 2024-01-03 Yu-Fei Wang , Ulf-G. Meißner , Deborah Rönchen , Chao-Wei Shen

In this paper, we study the polarization of the $\Lambda(1405)$ in the $\gamma p \rightarrow K^+ \pi \Sigma$ reaction within an effective Lagrangian approach and isobar model. In our model, the $\Lambda(1405)$ is excited through the…

Nuclear Theory · Physics 2021-02-03 Ke Wang , Bo-Chao Liu

We show that a $\Xi ^{\ast}$ pole can be dynamically generated near the $\bar{K} \Sigma$ threshold as an $s$-wave $\bar{K} \Sigma$ molecular state in a coupled-channels unitary approach with the leading-order chiral interaction. This $\Xi…

High Energy Physics - Phenomenology · Physics 2015-09-30 Takayasu Sekihara

Using a chiral unitary approach for the meson--baryon interactions, we show that two octets of J^{\pi}=1/2^- baryon states, which are degenerate in the limit of exact SU(3) symmetry, and a singlet are generated dynamically. The SU(3)…

Nuclear Theory · Physics 2009-11-10 D. Jido , J. A. Oller , E. Oset , A. Ramos , U. -G. Meißner

This talk focuses on a recent work aiming at determining the composition of certain $N^*$ and $\Delta$ resonances, i.e. whether they are compact states formed directly by quarks and gluons, or composite generated from the meson-baryon…

Nuclear Theory · Physics 2024-01-03 Yu-Fei Wang

A coupled channel model is used to study the nature of the f0(980) resonance. It is shown that the existence of two poles close to KKbar threshold, as found in many data fits and confirmed here, can be reconciled with the KKbar molecular…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. P. Locher , V. E. Markushin , H. Q. Zheng

We study the feasibility of having the $\Sigma^*(1430)$ state, predicted within the chiral unitary approach and recently reported by the Belle Collaboration, as corresponding to a state of non-molecular nature. Starting from this…

High Energy Physics - Phenomenology · Physics 2025-05-22 Jia-Xin Lin , Jing Song , Miguel Albaladejo , Albert Feijoo , Eulogio Oset

We have studied the strangeness changing antineutrino induced reactions $\bar{\nu}_{l} p \rightarrow l^+ \phi B $, with $\phi B = K^-p$, $\bar{K}^0n$, $\pi^0\Lambda$, $\pi^0\Sigma^0$, $\eta\Lambda$, $\eta\Sigma^0$, $\pi^+\Sigma^-$,…

High Energy Physics - Phenomenology · Physics 2015-04-16 Xiulei Ren , E. Oset , L. Alvarez-Ruso , M. J. Vicente Vacas

We demonstrate how an effective density of states can be derived from the S-matrix describing a coupled-channel system. Besides the locations of poles, the phase of the determinant of the S-matrix encodes essential details in characterizing…

High Energy Physics - Phenomenology · Physics 2020-09-09 Pok Man Lo

Low-energy data on the three charge states in $\gamma p \to K^+(\Sigma\pi)$ from CLAS at JLab, on $K^-p\to \pi^0\pi^0\Lambda$ and $\pi^0\pi^0\Sigma$ from the Crystal Ball at BNL, bubble chamber data on…

Nuclear Experiment · Physics 2019-05-15 A. V. Anisovich , A. V. Sarantsev , V. A. Nikonov , V. Burkert , R. A. Schumacher , U. Thoma , E. Klempt