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Related papers: The Charm and Bottom Hyperons in a Chiral Quark Mo…

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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

Beyond the spontaneous chiral symmetry breaking scale light and strange baryons should be considered as systems of three constituent quarks with an effective confining interaction and a flavor-spin chiral interaction that is mediated by the…

High Energy Physics - Phenomenology · Physics 2007-05-23 L. Ya. Glozman

Beyond the spontaneous chiral symmetry breaking scale light and strange baryons should be considered as systems of three constituent quarks with an effective confining interaction and a chiral interaction that is mediated by the octet of…

High Energy Physics - Phenomenology · Physics 2009-10-28 L. Ya. Glozman

New results on baryon structure and spectrum developed in collaboration with Dan Riska [1-4] are reported. The main idea is that beyond the chiral symmetry spontaneous breaking scale light and strange baryons should be considered as systems…

High Energy Physics - Phenomenology · Physics 2008-02-03 L. Ya. Glozman

The spectra of the nucleons and the strange hyperons are well described by a harmonic confinement potential for the constituent quarks and an SU(3) flavor-symmetric interaction mediated by the pseudoscalar octet that is associated with the…

High Energy Physics - Phenomenology · Physics 2008-02-03 L. Ya. Glozman , D. O. Riska

Beyond the scale of spontaneous breaking of chiral symmetry light and strange baryons should be considered as systems of three constituent quarks with confining interaction and a chiral interaction that is mediated by Goldstone bosons…

High Energy Physics - Phenomenology · Physics 2009-10-30 L. Ya. Glozman

An implication of the spontaneous chiral symmetry breaking in QCD is that at low energy and resolution there appear quasiparticles - constituent quarks and Goldstone bosons. Thus, light and strange baryons should be considered as systems of…

High Energy Physics - Phenomenology · Physics 2009-10-30 L. Ya. Glozman

The fine structure of the low energy part of the nucleon and strange hyperon spectra, which are formed of single states without parity doublets, may be understood in terms of an $SU(3)$ flavor-symmetric quark-quark interaction that…

High Energy Physics - Phenomenology · Physics 2011-04-20 L. Ya. Glozman , D. O. Riska

We present a chiral constituent quark model for light and strange baryons providing a unified description of their ground states and excitation spectra. The model relies on constituent quarks and Goldstone bosons arising as effective…

High Energy Physics - Phenomenology · Physics 2009-10-30 L. Ya. Glozman , W. Plessas , K. Varga , R. F. Wagenbrunn

New results on baryon structure and spectrum developed in collaboration with Dan Riska [1-4] are reported. The main idea is that beyond the chiral symmetry spontaneous breaking scale light and strange baryons should be considered as systems…

High Energy Physics - Phenomenology · Physics 2014-11-17 L. Ya. Glozman

In the low-energy regime light and strange baryons should be considered as systems of constituent quarks with confining interaction and a chiral interaction that is mediated by Goldstone bosons as well as by vector and scalar mesons. The…

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

We present ground state spectra of mesons containing a charm and a bottom quark. For the charm quark we use overlap valence quarks while a non-relativistic formulation is utilized for the bottom quark on a background of 2+1+1 flavors HISQ…

High Energy Physics - Lattice · Physics 2016-11-15 Nilmani Mathur , M. Padmanath , Randy Lewis

We present preliminary results on the light, charmed and bottom baryon spectra using overlap valence quarks on the background of 2+1+1 flavours HISQ gauge configurations of the MILC collaboration. These calculations are performed on three…

High Energy Physics - Lattice · Physics 2018-04-18 Sourav Mondal , M. Padmanath , Nilmani Mathur

We discuss the SU(3) and heavy quark spin-symmetry breaking mixing between the Xi_c and Xi'_c charmed baryons. Chromomagnetic hyperfine interactions are the leading source of spin-symmetry breaking and together with the SU(3) breaking mass…

High Energy Physics - Phenomenology · Physics 2014-11-17 C. Glenn Boyd , Ming Lu , Martin J. Savage

The chiral quark model with a nonet of Goldstone bosons can yield an adequate description of the observed proton flavor and spin structure. In a previous publication we have compared the results of a SU(3) symmetric calculation with the…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. P. Cheng , Ling-Fong Li

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

The $B_c ^+$ family of $(c\bar{b})$ mesons with beauty and charm is of special interest among heavy quarkonium systems. The $B_c ^+$ mesons are intermediate between $(c\bar{c})$ and $(b\bar{b})$ states both in mass and size, so many…

High Energy Physics - Phenomenology · Physics 2019-06-18 Estia J. Eichten , Chris Quigg

On the basis of the Bethe-Salpeter Equation we developed a covariant constituent quark model, with confinement implemented by a linear potential and an instanton induced interaction explaining mass splittings and mixing of pseudoscalar…

High Energy Physics - Phenomenology · Physics 2009-10-30 Bernard Metsch

We report results from a study of heavy-baryon spectroscopy within a relativistic constituent- quark model, whose hyperfine interaction is based on Goldstone-boson-exchange dynamics. While for light-flavor constituent quarks it is now…

High Energy Physics - Phenomenology · Physics 2011-08-18 Joseph P. Day , Ki-Seok Choi , Willibald Plessas

We study heavy-light baryon resonances with quantum numbers J^P=1/2^- in terms of the non-linear chiral SU(3) Lagrangian. Within the chi-BS(3) approach a parameter-free leading order prediction is obtained for the scattering of Goldstone…

High Energy Physics - Phenomenology · Physics 2010-12-16 M. F. M. Lutz , E. E. Kolomeitsev
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