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Related papers: Strangeness -2 hypertriton

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Recently, many efforts are being put in studying three-hadron systems made of mesons and baryons and interesting results are being found. In this talk, I summarize the main features of the formalism used to study such three hadron systems…

Nuclear Theory · Physics 2013-09-27 A. Martínez Torres , K. P. Khemchandani , D. Jido , Y. Kanada-En'yo , E. Oset

The hypernuclear systems $NN\Xi $ and $\Xi\Xi N$ are considered as an analogue of $nnp$ ($^3$H) nuclear system (with the notation as $AAB$ system). We use the recently proposed modification for the $s$-wave Malfliet-Tjon potential. The…

Nuclear Theory · Physics 2017-05-10 Igor Filikhin , Vladimir M. Suslov , Branislav Vlahovic

We study exotic baryon systems composed of anticharmed mesons and strange baryons using the extended local hidden gauge approach. By solving the coupled-channel Bethe-Salpeter equation with interaction kernels from vector meson exchange, we…

High Energy Physics - Phenomenology · Physics 2025-07-03 Jing Song , Eulogio Oset

The properties of strange hadronic matter are studied in the context of the modified quark-meson coupling model using two substantially different sets of hyperon-hyperon ($YY$) interactions. The first set is based on the Nijmegen hard core…

Nuclear Theory · Physics 2016-09-08 I. Zakout , H. R. Jaqaman , H. Steocker , W. Greiner

JLab has recently found indications of the possible existence of a $\Sigma NN$ resonance at $(3.14 \pm 0.84) - i (2.28 \pm 1.2)$ MeV. In the past, using models that exploit symmetries between the two-baryon sector with and without…

Nuclear Theory · Physics 2022-11-28 H. Garcilazo , A. Valcarce

In the framework of $RGM$, the binding energy of the six quark system with strangeness s=-5 is systematically investigated under the SU(3) chiral constituent quark model. The single $\Xi^*\Omega$ channel calculation with spins S=0 and 3 and…

Nuclear Theory · Physics 2009-10-31 Q. B. Li , P. N. Shen

The strangeness $S=-3$ and $-4$ baryon-baryon interactions are investigated in the relativistic chiral effective field theory at leading order. First, the potentials are derived from the $S=-1$ sector assuming that the corresponding…

Nuclear Theory · Physics 2021-02-10 Zhi-Wei Liu , Jing Song , Kai-Wen Li , Li-Sheng Geng

The in-medium properties of a baryon-baryon interaction for the strangeness $S=-2$ sector derived within chiral effective field theory up to next-to-leading order are investigated. The considered $\Xi N$ interaction is in line with…

Nuclear Theory · Physics 2019-03-27 J. Haidenbauer , U. -G. Meißner

Since the incident nuclei in heavy-ion collisions do not carry strangeness, the global net strangeness of the detected hadrons has to vanish. We show that there is an intimate relation between strangeness neutrality and baryon-strangeness…

High Energy Physics - Phenomenology · Physics 2019-07-19 Fabian Rennecke , Wei-jie Fu , Jan M. Pawlowski

The strangeness-changing ($\Delta S = 1$) weak baryon-baryon interaction is studied through the nonmesonic weak decay of double-$\Lambda$ hypernuclei. Besides the usual nucleon-induced decay $\Lambda N \to N N$ we discuss novel…

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

We investigate molecular states formed by bottom mesons and multistrange baryons from both octet and decuplet flavor representations, using the local hidden gauge approach combined with coupled-channel Bethe-Salpeter equations. Focusing on…

High Energy Physics - Phenomenology · Physics 2025-07-03 Jing Song , Yi-Yao Li , Eulogio Oset

We describe {\it ab initio} calculations of doubly strange, $S=-2$, $s$-shell hypernuclei ($^4_{\Lambda\Lambda}$H, $^5_{\Lambda\Lambda}$H, $^5_{\Lambda\Lambda}$He and $^6_{\Lambda\Lambda}$He) as a first attempt to explore the few-body…

Nuclear Theory · Physics 2008-11-26 H. Nemura , S. Shinmura , Y. Akaishi , Khin Swe Myint

In view of the renewing experimental interest for searching strangeness $+1$ baryons at J-PARC, we study the existence of light baryon resonances with strangeness +1 generated in the $K$-$(N^*/\Delta^*)$ system, where $N^*$ represents…

High Energy Physics - Phenomenology · Physics 2025-01-15 Brenda B. Malabarba , K. P. Khemchandani , A. Martinez Torres , Seung-il Nam

We derive a simple relation between strangeness neutrality and baryon-strangeness correlations. In heavy-ion collisions, the former is a consequence of quark number conservation of the strong interactions while the latter are sensitive…

High Energy Physics - Phenomenology · Physics 2020-01-22 Wei-jie Fu , Jan M. Pawlowski , Fabian Rennecke

We have used realistic local interactions based on the recent update of the strangeness $-2$ Nijmegen ESC08c potential to calculate the bound state problem of the $\Xi NN$ system in the $(I)J^P=(\frac{1}{2})\frac{3}{2}^+$ state. We found…

High Energy Physics - Phenomenology · Physics 2016-05-16 H. Garcilazo , A. Valcarce

Nuclear experiments near and below the threshold of hyperon production have shown that the production of Kaons is a sensitive probe for the dense QCD equation of state. At beam energies up to 1.5AGeV, strangeness production can probe the…

Nuclear Theory · Physics 2026-02-09 Jan Steinheimer , Tom Reichert , Marcus Bleicher

We use two-body potentials derived from a constituent quark cluster model to analyze the bound-state problem of the $\Sigma NN$ system. The observables of the two-body subsystems, $NN$ and $\Sigma N$, are well reproduced. We do not find…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Fernandez-Carames , A. Valcarce , H. Garcilazo , P. Gonzalez

We calculate the hypertriton binding energy and the $\Lambda d$ and $\Sigma d$ scattering lengths using baryon-baryon interactions obtained from a chiral constituent quark model. We study consistently the $\Lambda NN$ and $\Sigma NN$…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Garcilazo , T. Fernandez-Carames , A. Valcarce

The Faddeev equations for the $\Xi NN$ bound-state problem are solved where the three $S$=$-2$ baryon-baryon interactions of J\"ulich-Bonn-M\"unchen chiral EFT, HAL QCD and Nijmegen ESC08c are used. The $T$-matrix $T_{\Xi N, \Xi N}$…

Nuclear Theory · Physics 2021-08-18 K. Miyagawa , M. Kohno

We determine baryon-baryon bound states in 3+1 dimensional ${\rm SU}(3)$ lattice QCD with two flavors, $4\times 4$ spin matrices, and in an imaginary time formulation. For small hopping parameter, $\kappa>0$, and large glueball mass (strong…

High Energy Physics - Lattice · Physics 2007-05-23 Paulo A. Faria da Veiga , Michael O'Carroll