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The binding energy of nuclear matter including exchange and pionic effects is calculated in a quark-meson coupling model with massive constituent quarks. As in the case with elementary nucleons in QHD, exchange effects are repulsive.…

Nuclear Theory · Physics 2009-10-31 M. E. Bracco , G. Krein , M. Nielsen

The $X(3872)$ resonance has been conjectured to be a $J^{PC} = 1^{++}$ charm meson-antimeson two-body molecule. Meanwhile, there is no experimental evidence for larger, few-body compounds of multiple charm meson-antimeson pairs which would…

High Energy Physics - Phenomenology · Physics 2021-03-05 Lorenzo Contessi , Johannes Kirscher , Manuel Pavon Valderrama

We study $D\bar{D}^*$ ($D^*\bar{D}$) scattering in the framework of unitarized heavy meson chiral perturbation theory with pion exchange and a contact interaction. $^3S_1-$$^3D_1$ mixing effects are taken into account. A loosely bound state…

High Energy Physics - Phenomenology · Physics 2013-04-04 P. Wang , X. G. Wang

We study the heavy-light mesons in a relativistic model, which is derived from the instantaneous Bethe-Salpeter equation by applying the Foldy-Wouthuysen transformation on the heavy quark. The kernel we choose is based on scalar confining…

High Energy Physics - Phenomenology · Physics 2016-05-10 Jing-Bin Liu , Mao-Zhi Yang

It is argued that the charged $Z^+_c(3885)$ resonance, treated as a `molecular' state of charmed $D$ and $D^*$ mesons, is likely to consist of two peaks unequally coupled to the $D^{*+} \bar D^0$ and $D^+ \bar D^{*0}$ channels. The peaks…

High Energy Physics - Phenomenology · Physics 2016-10-12 M. B. Voloshin

We discuss the possibility and the description of bound states between $B$ and $\bar{B}^*$ mesons. We argue that the existence of such a bound state can be deduced from (i) the weakly bound X(3872) state, (ii) certain assumptions about the…

High Energy Physics - Phenomenology · Physics 2015-05-28 J. Nieves , M. Pavon Valderrama

Employing the relativized quark model and the quark-interchange model, we investigate the decay of the charged heavy quarkonium-like states $Z_c(3900)$, $Z_c(4020)$, $Z_c(4430)$, $Z_b(10610)$ and $Z_b(10650)$ into the ground and radially…

High Energy Physics - Phenomenology · Physics 2019-08-07 Guang-Juan Wang , Xiao-Hai Liu , Li Ma , Xiang Liu , Xiao-Lin Chen , Wei-Zhen Deng , Shi-Lin Zhu

We present a quark model calculation of the charmonium spectrum with self energy corrections due to the coupling to the meson-meson continuum. The bare masses used in the calculation are computed within the relativized quark model by…

High Energy Physics - Phenomenology · Physics 2015-10-05 J. Ferretti , G. Galatà , E. Santopinto

We investigate the low-energy elastic DbarN interaction using a quark model that confines color and realizes dynamical chiral symmetry breaking. The model is defined by a microscopic Hamiltonian inspired in the QCD Hamiltonian in Coulomb…

Nuclear Theory · Physics 2015-06-11 C. E. Fontoura , G. Krein , V. E. Vizcarra

We explore the role of a scalar meson exchange interaction between quarks in a semirelativistic constituent quark model where the quarks are also subject to a linear confinement. We search for a variational solution and study how the…

Nuclear Theory · Physics 2008-11-26 P. Stassart , Fl. Stancu , J. -M. Richard

Whether molecular states indeed exist in nature has been disputed for a long time. Several new resonances have been observed in the recent experiments and they seem to be of exotic structures and some of them have been proposed to be…

High Energy Physics - Phenomenology · Physics 2012-04-23 Hong-Wei Ke , Xue-Qian Li , Yan-Liang Shi , Guo-Li Wang , Xu-Hao Yuan

We describe the effective heavy meson lagrangian for S- and P-wave heavy-light mesons in terms of a model based on meson-quark interactions, where mesonic transition amplitudes are represented by diagrams with heavy mesons attached to loops…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. Deandrea , N. Di Bartolomeo , R. Gatto , G. Nardulli , A. D. Polosa

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

To illustrate the campaign to understand heavy quarkonium systems, I focus on a puzzling new state, $X(3872) \to \pi^+\pi^- J/\psi$. Studying the influence of open-charm channels on charmonium properties leads us to propose a new charmonium…

High Energy Physics - Phenomenology · Physics 2007-05-23 Chris Quigg

We present a model of charmonium as two heavy quarks propagating classically in a weakly coupled quark-gluon plasma. The quarks interact via a static, color-dependent potential and also suffer collisions with the plasma particles. We…

High Energy Physics - Phenomenology · Physics 2009-10-28 Daphne Levin-Plotnik , Benjamin Svetitsky

The difference between Z(4430) as a $D^{*}D_1$ molecule and a tetraquark state and how to distinguish between them are discussed. We construct an effective Lagrangian with $D^{*}D_1$ contact interactions constrained by the heavy quark…

High Energy Physics - Phenomenology · Physics 2007-11-26 Gui-Jun Ding

We investigate the variation with light quark mass of the mass of the nucleon as well as the masses of the mesons commonly used in a one-boson-exchange model of the nucleon-nucleon force. Care is taken to evaluate the meson mass shifts at…

Nuclear Theory · Physics 2013-05-30 M. E. Carrillo-Serrano , I. C. Clöet , K. Tsushima , A. W. Thomas , I. R. Afnan

Applying knowledge of the interaction between heavy quarks derived from the study of $c\overline{c}$ and $b\overline{b}$ bound states, we calculate the spectrum of $c\overline{b}$ mesons. We compute transition rates for the electromagnetic…

High Energy Physics - Phenomenology · Physics 2009-09-25 Estia J. Eichten , Chris Quigg

We report on some ideas concerning the nature of the X(3872) resonance and the need for approximately equal charged and neutral components of $D \bar{D}^* +cc$. Then we discuss how some hidden charm states are obtained from the interaction…

High Energy Physics - Phenomenology · Physics 2015-05-27 E. Oset , D. Gamermann , R. Molina , J. M. Nieves , E. Ruiz Arriola , T. Branz , Wei Hong Liang

Recently, several exotic bosons have been confirmed as multi-quark states, but there are violent disputes about their inner structures, namely if they are molecular states or tetraquarks, or even mixtures of the two structures. It would be…

High Energy Physics - Phenomenology · Physics 2017-09-08 Hong-Wei Ke , Lei Gao , Xue-Qian Li
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