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Related papers: One or two poles for the $\Xi(1820)$?

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We recall that the chiral unitary approach for the interaction of pseudoscalar mesons with the baryons of the decuplet predicts two states for the $\Xi(1820)$ resonance, one with a narrow width and the other one with a large width. We…

High Energy Physics - Phenomenology · Physics 2023-09-08 R. Molina , Wei-Hong Liang , Chu-Wen Xiao , Zhi-Feng Sun , E. Oset

We propose the reaction $\psi(3686) \to \bar{\Xi}^+ \bar{K}^0 \Sigma^{*-}$, with the $\Sigma^{*-}$ decaying to $\pi^- \Lambda$ in order to show evidence for the existence of two $\Xi(1820)$ states, one around $1824$ MeV and narrow, and…

High Energy Physics - Phenomenology · Physics 2024-05-07 Man-Yu Duan , Jing Song , Wei-Hong Liang , E. Oset

The s-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons is studied in a unitarized coupled channel approach. We obtain a fair agreement for mass and width of several 3/2- resonances. In particular, the Xi(1820),…

Nuclear Theory · Physics 2007-05-23 M. J. Vicente Vacas , E. Oset , Sourav Sarkar

We study $S$-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons using the lowest order chiral Lagrangian. We find two bound states in the SU(3) limit corresponding to the octet and decuplet representations. These…

Nuclear Theory · Physics 2011-02-09 E. Oset , S. Sarkar , M. J. Vicente Vacas

The strong decays of $\Xi$ baryons up to N=2 shell were studied in a chiral quark model. The strong decay properties of these well-established ground decuplet baryons were reasonably described. We found that (i) $\Xi(1690)$ and $\Xi(1820)$…

High Energy Physics - Phenomenology · Physics 2013-05-07 Li-Ye Xiao , Xian-Hui Zhong

We have investigated the $qss\bar{q}q$ ($q = u$ or $d$) system to find possible pentaquark explanations for the $\Xi$ resonances. The bound state calculation is carried out within the framework of the quark delocalization color screening…

High Energy Physics - Phenomenology · Physics 2024-04-24 Ye Yan , Qi Huang , Xinmei Zhu , Hongxia Huang , Jialun Ping

Nonleptonic weak decays of Xi_c into pi^+ and a meson (M)-baryon (B) final state, MB, are analyzed from the viewpoint of probing S=-2 baryon resonances, i.e. Xi(1620) and Xi(1690), of which spin-parity and other properties are not well…

Nuclear Theory · Physics 2017-04-05 Kenta Miyahara , Tetsuo Hyodo , Makoto Oka , Juan Nieves , Eulogio Oset

Using a unitary extension of chiral perturbation theory with a lowest-order s-wave SU(3) chiral Lagrangian we study low-energy meson-baryon scattering in the strangeness $S=-2$ sector. A scattering-matrix pole is found around 1606 MeV which…

Nuclear Theory · Physics 2009-11-07 A. Ramos , E. Oset , C. Bennhold

We study $S$-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons using the lowest order chiral Lagrangian. In the S=1 sector, we find an attractive interaction in the $\Delta K$ channel with I=1 while it is…

Nuclear Theory · Physics 2008-11-26 Sourav Sarkar , E. Oset , M. J. Vicente Vacas

We study the Belle reaction $\Xi_c^+ \to \Xi^- \pi^+ \pi^+$ looking at the mass distribution of $\pi^+ \Xi$, where clear signals for the $\Xi(1620)$ and $\Xi(1690)$ resonances are seen. These two resonances are generated dynamically from…

High Energy Physics - Phenomenology · Physics 2023-10-20 Hai-Peng Li , Gong-Jie Zhang , Wei-Hong Liang , E. Oset

The $\Xi$ baryons are expected to be naturally narrower as compared to their nonstrange and strange counterparts since they have only one light quark and, thus, their decay involves producing either a light meson and doubly strange baryon…

Nuclear Theory · Physics 2018-02-14 K. P. Khemchandani , A. Martínez Torres , A. Hosaka , H. Nagahiro , F. S. Navarra , M. Nielsen

In this manuscript we discuss the results of our recent study on $\Xi$ resonances. We have studied meson-baryon interaction with strangeness $-2$ by solving scattering equations in a coupled channel approach and found that the dynamics…

High Energy Physics - Phenomenology · Physics 2017-12-29 K. P. Khemchandani , A. Martínez Torres , A. Hosaka , H. Nagahiro , F. S. Navarra , M. Nielsen

Motivated by the recent BESIII measurements of the $J/\psi \to \Xi^0 \bar{\Lambda}K_S^0 + c.c.$ process, we investigate this reaction by considering the contributions from the $\Xi(1690)$ and $\Lambda(1890)$ resonances. The $\Xi(1690)$…

High Energy Physics - Phenomenology · Physics 2026-04-17 Wen-Tao Lyu , Lian-Rong Dai , Eulogio Oset

The newly observed $\Xi(1620)^0$ by the Belle Collaboration inspires our interest in performing a systematic study on the interaction of an anti-strange meson $(\bar{K}^{(*)})$ with a strange or doubly strange ground octet baryon…

High Energy Physics - Phenomenology · Physics 2019-10-14 Kan Chen , Rui Chen , Zhi-Feng Sun , Xiang Liu

Using the lowest order chiral Lagrangian we study s-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons. We find two bound states in the flavour SU(3) limit corresponding to the octet and decuplet representations.…

Nuclear Theory · Physics 2011-02-09 Sourav Sarkar , E. Oset , M. J. Vicente Vacas

We calculated the decay widths of the $1^3F_2$ and $1^3F_4$ $s\bar{s}$ mesons and compared them to the measured properties of the $\xi(2220)$ (now known as the $f_4(2220)$). Including previously neglected decay modes we found that the width…

High Energy Physics - Phenomenology · Physics 2009-10-28 Harry G. Blundell , Stephen Godfrey

We report the first observation of the doubly-strange baryon $\Xi(1620)^0$ in its decay to $\Xi^-\pi^+$ via $\Xi_c^+ \rightarrow \Xi^- \pi^+ \pi^+$ decays based on a $980\,{\rm fb}^{-1}$ data sample collected with the Belle detector at the…

High Energy Physics - Experiment · Physics 2019-02-27 Belle collaboration , M. Sumihama , I. Adachi , J. K. Ahn , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , I. Badhrees , S. Bahinipati , A. M. Bakich , V. Bansal , C. Beleno , M. Berger , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , G. Bonvicini , A. Bozek , M. Bracko , T. E. Browder , D. Cervenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe Czank , N. Dash , S. Di Carlo , Z. Dolezal , T. V. Dong , Z. Drasal , S. Eidelman , D. Epifanov , J. E. Fast , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , M. Gelb , A. Giri , P. Goldenzweig , E. Guido , J. Haba , K. Hayasaka , H. Hayashii , S. Hirose , W. -S. Hou , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , H. B. Jeon , S. Jia , Y. Jin , K. K. Joo , T. Julius , A. B. Kaliyar , K. H. Kang , G. Karyan , Y. Kato , C. Kiesling , D. Y. Kim , J. B. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodys , S. Korpar , D. Kotchetkov , P. Krizan , R. Kroeger , P. Krokovny , R. Kumar , A. Kuzmin , Y. -J. Kwon , J. S. Lange , I. S. Lee , S. C. Lee , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , M. Lubej , T. Luo , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , H. K. Moon , T. Mori , R. Mussa , E. Nakano , T. Nakano , M. Nakao , T. Nanut , K. J. Nath , Z. Natkaniec , M. Niiyama , N. K. Nisar , S. Nishida , H. Ono , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , V. Popov , M. Ritter , G. Russo , D. Sahoo , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , A. Sokolov , E. Solovieva , M. Staric , J. F. Strube , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , N. Taniguchi , F. Tenchini , M. Uchida , T. Uglov , S. Uno , P. Urquijo , S. E. Vahsen , C. Van Hulse , G. Varner , V. Vorobyev , A. Vossen , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , S. Watanuki , E. Widmann , E. Won , H. Ye , J. Yelton , C. Z. Yuan , Y. Yusa , S. Zakharov , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

Since its discovery in 1977, the spin-parity of $\Xi(2030)$ has not been fully determined experimentally. The latest Particle Data Group (PDG) listing suggests it may be a baryon with $J=5/2$. Therefore, studying the mass spectrum and decay…

High Energy Physics - Phenomenology · Physics 2024-09-20 Jing-wen Feng , Cai Cheng , Yin Huang

We study the $\Xi(1620)$ resonance near the $\bar{K}\Lambda$ threshold in the light of the recent experimental constraints. The Belle collaboration have found a resonance peak of $\Xi(1620)$ slightly below the $\bar{K}^{0}\Lambda$ threshold…

High Energy Physics - Phenomenology · Physics 2023-05-19 Takuma Nishibuchi , Tetsuo Hyodo

In this work, we study the strong decays of the newly observed $\Xi(1620)^0$ assuming that it is a meson-baryon molecular state of $\Lambda\bar{K}$ and $\Sigma\bar{K}$. We consider four possible spin-parity assignments $J^P=1/2^{\pm}$ and…

High Energy Physics - Phenomenology · Physics 2020-06-12 Yin Huang , Lisheng Geng
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