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Related papers: On Lowest Lying $\frac{1}{2}^-$ Octet Baryons

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We present a comprehensive analysis of the SU(3) octet and decuplet baryon masses and $\sigma$-terms using high-precision lattice QCD data and chiral SU(3) effective theory with finite range regularization. The effects of various systematic…

Nuclear Theory · Physics 2023-06-01 P. M. Copeland , Chueng-Ryong Ji , W. Melnitchouk

This study focuses on the interaction of the pseudoscalar meson octet and the baryon decuplet. In the continuum, it is observed that several $J^{P}=\frac32^-$ baryon resonances can be produced by the Weinberg-Tomozawa interaction in…

High Energy Physics - Phenomenology · Physics 2024-04-24 Teng Ji , Xiang-Kun Dong , Ulf-G. Meißner

The splittings between the spin 1/2 and spin 3/2 iso-singlet baryons Lambda_s(1405) and Lambda_s(1520), and their charmed counterparts Lambda_c(2593) and Lambda_c(2625), have been a theoretical conundrum. Here we investigate the possibility…

High Energy Physics - Phenomenology · Physics 2007-05-23 Olaf Kittel , Glennys R. Farrar

We investigate baryon-baryon (BB) interactions in the 3-flavor full QCD simulations with degenerate quark masses for all flavors. The BB potentials in the orbital S-wave are extracted from the Nambu-Bethe-Salpeter wave functions measured on…

High Energy Physics - Lattice · Physics 2011-01-05 Takashi Inoue , Noriyoshi Ishii , Sinya Aoki , Takumi Doi , Tetsuo Hatsuda , Yoichi Ikeda , Keiko Murano , Hidekatsu Nemura , Kenji Sasaki

The flavor SU(3) group structure of pentaquark baryons which form $\bm{1}$, $\bm{8}$, $\bm{10}$, $\bar{\bm{10}}$, $\bm{27}$, and $\bm{35}$ multiplets is investigated in quark model. The flavor wave functions of all the pentaquark baryons…

High Energy Physics - Phenomenology · Physics 2017-08-23 Yongseok Oh , Hungchong Kim

The semileptonic decays and two-body nonleptonic decays of light baryon octet ($T_8$) and decuplet ($T_{10}$) consisting of light $u,d,s$ quarks are studied with the SU(3) flavor symmetry in this work. We obtain the amplitude relations…

High Energy Physics - Phenomenology · Physics 2019-10-23 Ru-Min Wang , Mao-Zhi Yang , Hai-Bo Li , Xiao-Dong Cheng

A combined expansion in the number of QCD colors 1/N_c and SU(3) flavor breaking parameter epsilon has long been known to provide an excellent accounting for the mass spectrum of the lightest spin-1/2, 3/2 baryons when the quarks are taken…

High Energy Physics - Phenomenology · Physics 2013-05-30 Aleksey Cherman , Thomas D. Cohen , Richard F. Lebed

We investigate baryon-baryon (BB) interactions in the flavor SU(3) symmetric world, by using the 3-flavor full QCD simulations. In the SU(3) limit, six independent two-baryon states exist for a given orbital angular momentum. We forcus on…

High Energy Physics - Lattice · Physics 2019-08-13 Takashi Inoue

Low-lying $\Lambda$ baryons with spin 1/2 are analyzed in two-flavor unquenched lattice QCD. We construct $2 \times 2$ cross correlators from flavor SU(3) ``octet'' and ``singlet'' baryon operators, and diagonalize them so that we can…

High Energy Physics - Lattice · Physics 2010-11-05 Toru T. Takahashi , Makoto Oka

Progress in the calculation of the electromagnetic properties of baryon excitations in lattice QCD is presenting new challenges in the determination of sea-quark loop contributions to matrix elements. A reliable estimation of the sea-quark…

High Energy Physics - Lattice · Physics 2016-11-11 J. M. M. Hall , D. B. Leinweber

1/N_c baryon mass relations are compared with lattice simulations of baryon masses using different values of the light-quark masses, and hence different values of SU(3) flavor-symmetry breaking. The lattice data clearly display both the…

High Energy Physics - Lattice · Physics 2010-04-30 Elizabeth Ellen Jenkins , Aneesh V. Manohar , John W. Negele , Andre Walker-Loud

We obtain from the quark-gluon dynamics, the Gell'Mann-Ne'eman eightfold way baryons in an imaginary-time functional integral formulation of 3+1 lattice QCD in the strong coupling regime (small hopping parameter $\kappa>0$). The model has…

High Energy Physics - Lattice · Physics 2007-07-13 Paulo A. Faria da Veiga , Michael O'Carroll

We present an effective model, which is an extension of the usual linear sigma model, that contains a low energy multiplet for every hadronic particle type. These multiplets are a scalar nonet, a pseudoscalar nonet, a vector nonet, an…

High Energy Physics - Phenomenology · Physics 2014-04-29 Peter Kovacs , Arpad Lukacs , Janos Varoczy , Gyorgy Wolf , Miklos Zetenyi

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

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

The self-energies of the full set of flavor SU(3) octet and decuplet baryons are computed within a relativistic chiral effective theory framework. The leading nonanalytic chiral behavior is derived for the octet and decuplet masses, and a…

High Energy Physics - Phenomenology · Physics 2021-05-26 P. M. Copeland , Chueng-Ryong Ji , W. Melnitchouk

The masses of heavy quark baryons are studied in an expansion in 1/N_c, SU(3) flavor symmetry breaking, and heavy-quark symmetry breaking. Very accurate model-independent mass relations are obtained for charm and bottom baryons.

High Energy Physics - Phenomenology · Physics 2009-11-07 E. Jenkins

The baryon mass operator is studied within a combined expansion in $1/N_c$ and perturbative $SU(3)$ flavor symmetry breaking, where $N_c$ denotes the number of quark charges. Flavor projection operators are used to classify the baryon…

Distinctive patterns are predicted by quenched quark models and unquenched quark models for the lowest SU(3) baryon nonet with spin parity $J^P=1/2^-$. While the quenched quark models predict the lowest $1/2^-$ $\Sigma^*$ resonance to be…

High Energy Physics - Phenomenology · Physics 2009-08-13 Jia-Jun Wu , S. Dulat , B. S. Zou

We calculate baryon decuplet to octet electromagnetic transition form factors in quenched and partially quenched chiral perturbation theory. We work in the isospin limit of SU(3) flavor, up to next-to-leading order in the chiral expansion,…

High Energy Physics - Lattice · Physics 2009-11-10 Daniel Arndt , Brian C. Tiburzi
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