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Related papers: Nucleon Resonances with Hidden Charm in Coupled-Ch…

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In the extended chiral constituent quark model, the intrinsic $c \bar{c}$ content of the nucleon is investigated. The probabilities of the quark-antiquark components in the nucleon wave functions are calculated by taking the nucleon to be…

High Energy Physics - Phenomenology · Physics 2016-06-22 Shaorong Duan , C. S. An , B. Saghai

The constituent quark model can explain the strong selectivity of the $N\eta$ decay branching ratios of the nucleon resonances if the fine structure interaction between the constituent quarks is described in terms of Goldstone boson…

High Energy Physics - Phenomenology · Physics 2009-10-28 L. Ya. Glozman , D. O. Riska

In this talk I summarize recent findings around the description of axial vector mesons as dynamically generated states from the interaction of pseudoscalar mesons and vector mesons, dedicating some attention to the two $K_1(1270)$ states.…

In the present paper we address the interaction of pairs of charmed mesons with hidden charm in a finite box. We use the interaction from a recent model based on heavy quark spin symmetry that predicts molecules of hidden charm in the…

High Energy Physics - Lattice · Physics 2013-08-09 Miguel Albaladejo , Carlos Hidalgo-Duque , Juan Nieves , Eulogio Oset

We study two- and three-baryon systems with two units of charm looking for possible bound states or resonances. All two-baryon interactions are consistently derived from a constituent quark model tuned in the light-flavor hadron…

High Energy Physics - Phenomenology · Physics 2020-08-12 H. Garcilazo , A. Valcarce

We have studied the meson-baryon interaction in coupled channels with the same quantum numbers of $\Xi_{bc}$. The interaction is attractive in some channels and of sufficient intensity to lead to bound states or resonances. We use a model…

High Energy Physics - Phenomenology · Physics 2019-12-02 Qi-Xin Yu , J. M. Dias , Wei-Hong Liang , E. Oset

We study the nucleon-nucleon interaction in a chiral constituent quark model by using the resonating group method, convenient for treating the interaction between composite particles. The calculated phase shifts for the 3S1 and 1S0 channels…

Nuclear Theory · Physics 2009-11-06 D. Bartz , Fl. Stancu

We discuss the non-relativistic multichannel quark model and describe the techniques developed to solve the resulting equations. We then investigate some simple solutions to demonstrate how the model unifies meson-meson scattering with…

Nuclear Theory · Physics 2007-05-23 John Weinstein

We discuss the behavior of dynamically-generated charmed baryonic resonances in matter within a unitarized coupled-channel model consistent with heavy-quark spin symmetry. We analyze the implications for the formation of $D$-meson bound…

Nuclear Theory · Physics 2017-04-05 Laura Tolos

A symmetry-preserving treatment of a vector-vector contact interaction is used to study charmed heavy-light mesons. The contact interaction is a representation of nonperturbative kernels used in Dyson-Schwinger and Bethe-Salpeter equations…

High Energy Physics - Phenomenology · Physics 2017-07-26 Fernando E. Serna , Bruno El-Bennich , Gastão Krein

Using a $\overline D$ meson cloud model we calculate the squared charm radius of the nucleon . The ratio between this squared radius and the ordinary baryon squared radius is identified with the probability of ``seeing'' the intrinsic charm…

High Energy Physics - Phenomenology · Physics 2009-10-28 F. S. NAVARRA , M. NIELSEN , C. A. A. NUNES , M. TEIXEIRA

The interactions of $\bar{D}\Sigma_{c}$-$\bar D\Lambda_c$, $\bar{D}^{*}\Sigma_{c}$-$\bar D^*\Lambda_c$, and related strangeness channels, are studied within the framework of the coupled channel unitary approach with the local hidden gauge…

Nuclear Theory · Physics 2015-03-17 Jia-Jun Wu , R. Molina , E. Oset , B. S. Zou

We generalized our approach to the hypernuclei with $A=B=3$ containing one charm or one bottom quark. We derive the relativistic nine-quark equations using the dispersion relation technique. The hypernuclei as the system of interacting…

Nuclear Theory · Physics 2015-10-08 S. M. Gerasyuta , E. E. Matskevich

We discuss some puzzling aspects of the narrow hidden charm resonance that was recently discovered by the Belle Collaboration at mass 3872 MeV. In order to determine its quantum numbers, a crucial piece of information is the spin of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sandip Pakvasa , Mahiko Suzuki

We develop an extension of the usual three flavor quark model to four flavors (u, d, s and c), and discuss the classification of pentaquark states with hidden charm. We fit our model to the known baryon spectrum and we predict the double…

Nuclear Theory · Physics 2019-04-29 Emmanuel Ortiz-Pacheco , Roelof Bijker , César Fernández-Ramírez

In this work we present our model that dynamically generates resonances from charmed and light pseudoscalar and vector mesons. The model generates a rich spectrum of charmed and hidden charm scalar and axial resonances, most of them which…

High Energy Physics - Phenomenology · Physics 2009-05-12 D. Gamermann , E. Oset , B. S. Zou

Resonances with strong couplings to strangeness channels are investigated in a coupled-channels framework of kaon production with pions and photons. We find evidence for an additional D13 resonance around 1900 MeV that has a significant…

Nuclear Theory · Physics 2007-05-23 C. Bennhold , A. Waluyo , H. Haberzettl , T. Mart , G. Penner , U. Mosel

The classical quenched quark models with three constituent quarks provide a good description for the baryon spatial ground states, but fail to reproduce the spectrum of baryon excited states. More and more evidences suggest that unquenched…

Nuclear Theory · Physics 2016-06-22 Jia-Jun Wu , B. S. Zou

Compound states manifest themselves as bound states, resonances, or primitives, and their character is determined by their interaction with the continuum. If the interaction experiences a perturbation, a compound state can change its…

Nuclear Theory · Physics 2011-08-08 M. I. Krivoruchenko

We have developed a physical model for the non-perturbative x-shape of parton density functions in the proton, based on Gaussian fluctuations in momenta, and quantum fluctuations of the proton into meson-baryon pairs. The model describes…

High Energy Physics - Phenomenology · Physics 2007-05-23 Johan Alwall