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Related papers: Constituent quark models and pentaquark baryons

200 papers

We make predictions for the production and decays of $X(2900)$ states, and their possible charged partners, in $B^+$ and $B^0$ decays, considering a number of competing models for the states, including triangle diagrams mediated by quark…

High Energy Physics - Phenomenology · Physics 2021-01-13 T. J. Burns , E. S. Swanson

Octet and Decuplet baryons are described within the hadronized NJL model as diquark--quark states, which are bound by quark exchange. Including scalar and axial--vector diquark correlations, we project the previously obtained relativistic…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. Buck , H. Reinhardt

We consider the implications of the most general two-body quark-quark interaction Hamiltonian for the spin-flavor structure of the negative parity L=1 excited baryons. Assuming the most general two-body quark interaction Hamiltonian, we…

High Energy Physics - Phenomenology · Physics 2009-06-16 Dan Pirjol , Carlos Schat

A discussion is presented of the estimates of the energy and width of resonances in constituent models, with focus on the tetraquark states containing heavy quarks.

High Energy Physics - Phenomenology · Physics 2024-06-21 Jean-Marc Richard , Alfredo Valcarce , Javier Vijande

We review the application of non-relativistic constituent quark models to study one, two and three non-strange baryon systems. We present results for the baryon spectra, potentials and observables of the NN, N$\Delta$, $\Delta\Delta$ and…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Valcarce , H. Garcilazo , F. Fernandez , P. Gonzalez

A potential quark model is used to search for a $P_{c\bar{c}s}^0=(c\bar{c}uds)^0$, $J^P=1/2^-$ pentaquark state that has recently been observed experimentally by the LHCb collaboration at 4338.2 MeV, with a width of 7.0 MeV and high…

High Energy Physics - Phenomenology · Physics 2026-03-10 Emiko Hiyama , Atsushi Hosaka , Makoto Oka , Georg Wolschin

Using the SU(3) flavor symmetry, we construct the chiral Lagrangians for the light and heavy pentaquarks. The correction from the nonzero quark is taken into account perturbatively. We derive the Gell-Mann$-$Okubo type relations for various…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. -R. Liu , A. Zhang , P. -Z. Huang , W. -Z. Deng , X. -L. Chen , Shi-Lin Zhu

We calculate the properties of the pentaquarks $\Theta^+$ and $\Xi^{--,0}$ in symmetric nuclear matter using the quark meson coupling model (QMC). The stability of the $\Theta^+$ in the medium with respect to the channel $\Theta^+\to NK^+$…

Nuclear Theory · Physics 2009-11-11 P. K. Panda , C. Providência , D. P. Menezes

We construct the spin-flavor wave functions of the possible heavy pentaquarks containing an anti-charm or anti-bottom quark using various clustered quark models. Then we estimate the masses and magnetic moments of the $J^P={1\over 2}^+$ or…

High Energy Physics - Phenomenology · Physics 2011-01-27 P. -Z. Huang , Y. -R. Liu , W. -Z. Deng , X. -L. Chen , Shi-Lin Zhu

Exotic multi-quark states are examined in the quark model and in QCD. Current status of theoretical studies of the pentaquark Theta^+ is reported. We show recent analyses of multi-quark components of baryons. A novel method to extract a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Makoto Oka

In previous papers we developed the light front formulation for Hamiltonians and wave functions (WFs) for mesons and baryons, with both confinement and chiral symmetry breaking. For baryons limited to the lowest Fock component with three…

High Energy Physics - Phenomenology · Physics 2025-11-04 Nicholas Miesch , Edward Shuryak , Ismail Zahed

We study the octet to decuplet baryon electromagnetic transitions using the covariant spectator quark model, and predict the transition magnetic dipole form factors for those involving the strange baryons. Utilizing SU(3) symmetry, the…

High Energy Physics - Phenomenology · Physics 2013-06-06 G. Ramalho , K. Tsushima

We incorporate fine-structure corrections into the dynamical diquark model of multiquark exotic hadrons. These improvements include effects due to finite diquark size, spin-spin couplings within the diquarks, and most significantly,…

High Energy Physics - Phenomenology · Physics 2020-01-28 Jesse F. Giron , Richard F. Lebed , Curtis T. Peterson

We review and discuss the experimental evidence on predicted baryonic states made by 4 quarks and one antiquark, called pentaquarks. Theoretical and experimental advances in the last few years led to the observation of pentaquark candidates…

High Energy Physics - Experiment · Physics 2009-11-11 Sonia Kabana

We review the experimental and theoretical status of baryons containing one heavy quark. The charm and bottom baryon states are classified and their mass spectra are listed. The appropriate theoretical framework for the description of heavy…

High Energy Physics - Phenomenology · Physics 2011-01-25 J. G. Koerner , D. Pirjol , M. Kraemer

A quark model is applied to the spectrum of baryons containing heavy quarks. The model gives masses for the known heavy baryons that are in agreement with experiment, but for the doubly-charmed baryon Cascade_{cc}, the model prediction is…

Nuclear Theory · Physics 2008-11-26 W. Roberts , Muslema Pervin

We explore further the idea that the lattice QCD data for hadron properties in the region m_\pi^2 > 0.2 GeV^2 can be described by the constituent quark model. This leads to a natural explanation of the fact that nucleon excited states are…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. W. Thomas , R. D. Young

We evaluate two-meson couplings of Theta+, using experimental information of nucleon resonances decaying into pi pi N channels, in which the two pions are in scalar- and vector-type correlations. We examine two assignments of spin and…

High Energy Physics - Phenomenology · Physics 2014-11-18 Tetsuo Hyodo , Atsushi Hosaka

We study the decay of Theta+ in a non-relativistic quark model. The wave function of Theta+ is constructed for the two cases JP = 1/2+- as products of color, spin, flavor and orbital parts respecting total antisymmetrization among the four…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Hosaka , M. Oka , T. Shinozaki

I discuss the structure of current-induced bottom baryon to charm baryon transitions, and the structure of pion and photon transitions between heavy charm or bottom baryons in the Heavy Quark Symmetry (HQS) limit as $m_Q\rightarrow\infty$.…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. G. Körner