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Related papers: Ground State Baryons in Covariant Level-Classifica…

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A family of simply solvable covariant quark models for the baryons is presented. With optimal parameter choices the models reproduce the empirical spectra of the baryons in all flavor sectors to an accuracy of a few percent. Complete…

High Energy Physics - Phenomenology · Physics 2011-01-27 F. Coester , K. Dannbom , D. O. Riska

We continue our attempts to systematize baryons, which are composed of light quarks ($q=u,d$), as quark--diquark systems. The notion of two diquarks is used: (i) $D^{1}_{1}$, with the spin $S_D=1$ and isospin $I_D=1$ and (ii) $D^{0}_{0}$,…

High Energy Physics - Phenomenology · Physics 2010-02-09 A. V. Anisovich , V. V. Anisovich , M. A. Matveev , V. A. Nikonov , A. V. Sarantsev , T. O. Vulfs

We present an analysis of the octet baryon masses and the $\pi N$ and $KN$ $\sigma$--terms in the framework of heavy baryon chiral perturbation theory. At next-to-leading order, ${\cal O}(q^3)$, knowledge of the baryon masses and…

High Energy Physics - Phenomenology · Physics 2016-08-14 Véronique Bernard , Norbert Kaiser , Ulf-G. Meißner

The properties of four quark cn - nbar cbar states are investigated as cn di-quark and nbar cbar di-antiquark system in U(12)-classification scheme of hadrons, recently proposed by us. We consider the negative-parity di-quark and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Muneyuki Ishida , Shin Ishida , Tomohito Maeda

We study the conjectured "Insensitivity to Chiral Symmetry Breaking" in the highly excited light baryon spectrum. While the experimental spectrum is being measured at JLab and CBELSA/TAPS, this insensitivity remains to be computed…

High Energy Physics - Phenomenology · Physics 2016-09-14 Pedro Bicudo , Marco Cardoso , Felipe J. Llanes-Estrada , Tim Van Cauteren

Physics of the low-lying and high-lying hadrons in the light flavors sector is reviewed. While the low-lying hadrons are strongly affected by both $U(1)_A$ and spontaneous $SU(2)_L \times SU(2)_R$ breakings, in the high-lying hadrons these…

High Energy Physics - Phenomenology · Physics 2015-06-25 L. Ya. Glozman

The spectra of the nucleons, $\Delta$ resonances and the strange hyperons are well described by the constituent quark model if in addition to the harmonic confinement potential the quarks are assumed to interact by exchange of the $SU(3)_F$…

High Energy Physics - Phenomenology · Physics 2011-07-19 L. Ya. Glozman , D. O. Riska

We have calculated the mass spectra of nucleon and delta hybrid baryons with both positive-parity and negative-parity by using the method of QCD sum rules. We predicte that the lowest-lying hybrid baryons are the negative-parity $N_{1/2^-}$…

High Energy Physics - Phenomenology · Physics 2025-07-25 Wei Chen , Qi-Nan Wang , Ding-Kun Lian , Hui-Min Yang , Hua-Xing Chen , J. H , T. G. Steele

We describe a calculation of the spectrum of strange and nonstrange hadrons that simultaneously correlates the dressed-quark-core masses of meson and baryon ground- and excited-states within a single framework. The foundation for this…

Nuclear Theory · Physics 2015-06-04 Chen Chen , Lei Chang , Craig D. Roberts , Shaolong Wan , David J. Wilson

In the heavy quark limit, there are three independent strong axial coupling constants in chiral Lagrangians for ground-state heavy hadrons: g in the meson sector, and g_1, g_2 in the baryon sector. The coupling g_2 is extracted from recent…

High Energy Physics - Phenomenology · Physics 2009-10-30 Hai-Yang Cheng

We revisit the mass splittings of SU(3) baryons, taking into account the second-order effects of isospin and SU(3) flavor symmetry breakings within the framework of a chiral soliton model. The masses of the baryon decuplet turn out to be…

High Energy Physics - Phenomenology · Physics 2015-05-27 Ghil-Seok Yang , Hyun-Chul Kim

The level classification of quark-antiquark systems is generally made by the LS-coupling scheme, resorting to the non-relativistic quark model. However, it has been well known that the pi-meson with the (L,S)=(0,0) shows also the properties…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shin Ishida , Muneyuki Ishida

We extend the $D4$-$D8$ holographic construction to include three chiral and one heavy flavor, to describe heavy-light baryons with strangeness and their exotics. At strong coupling, the heavy meson always binds to the bulk instanton in the…

High Energy Physics - Phenomenology · Physics 2017-10-04 Yizhuang Liu , Ismail Zahed

We study the possibility that four iso-singlet baryons $\Lambda_s(1405)$ $J^P=1/2^{-}$, $\Lambda_s(1520)$ $J^P=3/2^{-}$, $\Lambda_c(2593)$ $J^P=1/2^{-}$ and $\Lambda_c(2625)$ $J^P=3/2^{-}$ are hybrids: three quark one gluon states (udsg).…

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

Starting from the bi-local Klein-Gordon Equation with spin-independent squared-mass operator, we give a covariant quark representation of general composite meson systems with definite Lorentz transformation properties. For benefit of this…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shin Ishida , Muneyuki Ishida , Tomohito Maeda

The discovery of $\Xi_{cc}^{++}$ by the LHCb Collaboration triggers predictions of more doubly charmed baryons. By taking into account both the $P$-wave excitations between the two charm quarks and the scattering of light pseudoscalar…

High Energy Physics - Phenomenology · Physics 2018-11-28 Mao-Jun Yan , Xiao-Hai Liu , Sergi Gonzàlez-Solís , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner , Bing-Song Zou

We report a calculation of the low-lying baryon magnetic moments using covariant chiral perturbation theory within the extended-on-mass-shell renormalization scheme including intermediate octet and decuplet contributions. For the case of…

High Energy Physics - Phenomenology · Physics 2014-11-20 J. Martin Camalich , L. Alvarez-Ruso , L. S. Geng , M. J. Vicente Vacas

We perform a preliminary study of the 1/2+ and 3/2+ ground-state baryons containing a heavy quark in the framework of the chiral SU(3) quark model. By using the calculus of variations, masses of Lambda_Q, Sigma_Q, Xi_Q, Omega_Q, Sigma_Q^*,…

Nuclear Theory · Physics 2011-06-27 Qiao-Yan Zhao , Dan Zhang , Qiu-Yang Zhang

We show that the average multiplet masses in the baryon octet and decuplet can be fitted with an average error of only $0.5\pm 0.3$ MeV in a meson loop expansion with chiral SU(6) couplings, with the hadrons treated as composite particles…

High Energy Physics - Phenomenology · Physics 2009-10-31 Phuoc Ha , Loyal Durand

We report on a systematic study of the ground-state octet baryon masses in the covariant baryon chiral perturbation theory with the extended-on-mass-shell renormalization scheme up to next-to-next-to-next-to-leading order, taking into…

Nuclear Theory · Physics 2015-06-17 Xiu-Lei Ren , Lisheng Geng , Jie Meng , Hiroshi Toki