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Related papers: The Isgur-Karl model revisited

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A spin-flavor symmetry emerges for baryons in the large-N_c limit. Large-N_c baryons form irreducible representations of the spin-flavor algebra, and their static properties can be computed in a systematic expansion in 1/N_c. Symmetry…

High Energy Physics - Phenomenology · Physics 2008-11-26 Elizabeth Jenkins

We review results for the mass spectrum of orbitally excited baryons obtained in the $1/N_c$ expansion. We show the dependence of various contributions to the mass operator as a function of the excitation energy.

High Energy Physics - Phenomenology · Physics 2017-08-23 N. Matagne , Fl. Stancu

Spin-flavor symmetry breaking in the levels of excited Baryons are studied to leading order in the 1/$N_c$ expansion. This breaking occurs at zeroth order. For non-strange Baryons with a single quark excited, it is shown that to first order…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. L. Goity

In order to better understand the fundamental issue regarding the compatibility between the quark-shell picture and that of resonances in meson-nucleon scattering in large $N_c$ QCD we extend the work of Cohen and Lebed on mixed symmetric…

High Energy Physics - Phenomenology · Physics 2011-09-22 N. Matagne , Fl. Stancu

The 1/N_c expansion of the heavy baryon Isgur-Wise functions is discussed. Because of the contracted SU(2N_f) light quark spin-flavor symmetry, the universality relations among the Isgur-Wise functions of \Lambda_b to \Lambda_c and…

High Energy Physics - Phenomenology · Physics 2009-10-30 Chun Liu

In the large Nc limit, the mass spectrum of the L=1 orbitally excited baryons N* has a very simple structure, with states degenerate in pairs of spins J=(1/2,3/2), (3/2,5/2), corresponding to irreducible representations (towers) of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dan Pirjol , Carlos Schat

A simple procedure within the $1/N_c$ expansion method where all the $N_c$ quarks are treated on the same footing has been found successful in describing mixed symmetric negative parity baryon states belonging to the $[{\bf 70},\ell^-]$…

High Energy Physics - Phenomenology · Physics 2014-06-13 N. Matagne , Fl. Stancu

The masses of highly excited negative parity baryons belonging to the $N$ = 3 band are calculated in the $1/N_c$ expansion method of QCD. We use a procedure which allows to write the mass formula by using a small number of linearly…

High Energy Physics - Phenomenology · Physics 2012-11-30 N. Matagne , Fl. Stancu

The space-like elastic form factors of baryons containing a heavy quark are investigated within a light-front constituent quark model in the limit of infinite heavy-quark mass, adopting a gaussian-like ansatz for the three-quark wave…

High Energy Physics - Phenomenology · Physics 2009-10-30 F. Cardarelli , S. Simula

The physics of the orbitally excited baryons simplifies drastically in the large Nc limit. The states are arranged into irreducible representations of the contracted SU(4)_c symmetry, with mixing angles determined exactly. The ratios of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dan Pirjol , Carlos Schat

We present a comparative study of the charmed baryon$-$nucleon interaction based on different theoretical approaches. For this purpose, we make use of i) a constituent quark model tuned in the light-flavor baryon$-$baryon interaction and…

High Energy Physics - Phenomenology · Physics 2019-07-17 H. Garcilazo , A. Valcarce , T. F. Carames

A variational analysis is performed within the framework of lattice QCD to extract the masses of the spin-3/2 positive parity $ \Delta^+ $ baryons, including radial excitations. $2+1$ flavour dynamical gauge-field configurations provided by…

High Energy Physics - Lattice · Physics 2023-07-05 Liam Hockley , Waseem Kamleh , Derek Leinweber , Anthony Thomas

Light-baryon resonances (with u,d, and s quarks in the SU(3) classification) fall on Regge trajectories. When their squared masses are plotted against the intrinsic orbital angular momenta {\rm L}, $\Delta^*$'s with even and odd parity can…

Nuclear Experiment · Physics 2017-08-23 E. Klempt

Excited state spectra are calculated using lattice QCD for baryons that can be formed from $u$, $d$ and $s$ quarks, namely the $N$, $\Delta$, $\Lambda$, $\Sigma$, $\Xi$ and $\Omega$ families of baryons. Baryonic operators are constructed…

High Energy Physics - Phenomenology · Physics 2013-04-12 Robert G. Edwards , Nilmani Mathur , David G. Richards , Stephen J. Wallace

A good agreement between a flux tube-based quark model of light baryons (strange and nonstrange) and the $1/N_c$ expansion mass formula has been found in previous studies. In the present work a larger connection is established between the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Semay , F. Buisseret , F. Stancu

The design and implementation of large sets of spatially-extended, gauge-invariant operators for use in determining the spectrum of baryons in lattice QCD computations are described. Group-theoretical projections onto the irreducible…

High Energy Physics - Lattice · Physics 2014-11-17 S. Basak , R. G. Edwards , G. T. Fleming , U. M. Heller , C. Morningstar , D. Richards , I. Sato , S. Wallace

The construction of the first baryon operators for staggered lattice QCD exploited the taste symmetry to emulate physical quark flavor; contemporary 2+1 flavor simulations explicitly include three physical quark flavors and necessitate…

High Energy Physics - Lattice · Physics 2008-11-26 Jon A. Bailey

An $SU(3)$ flavor projection operator technique is implemented to construct the baryon-meson scattering amplitude in the framework of the $1/N_c$ expansion of QCD, where $N_c$ is the number of color charges. The operator technique is…

High Energy Physics - Phenomenology · Physics 2025-09-10 Victor Miguel Banda Guzmán , Ruben Flores-Mendieta , Johann Hernandez

Using the $1/N_c$ expansion of QCD we analyze the spectrum of positive parity resonances with strangeness $S = 0, -1, -2$ and -3 in the 2-3 GeV mass region, supposed to belong to the $[\textbf{56},4^+]$ multiplet. The mass operator is…

High Energy Physics - Phenomenology · Physics 2009-11-10 N. Matagne , Fl. Stancu

This paper which is part of a series, is devoted to several technical issues. In the first part of the paper, we discuss the usual wavefunctions in the CM frame for baryons, by clarifying the representations of the three-quark permutation…

High Energy Physics - Phenomenology · Physics 2023-08-29 Nicholas Miesch , Edward Shuryak , Ismail Zahed