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Related papers: Charm spectroscopy beyond the constituent quark mo…

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We review how quark models are able to describe the phenomenology of the charm meson sector. The spectroscopy and decays of charmonium and open charm mesons are described in a particular quark model and compared with the data and the…

High Energy Physics - Phenomenology · Physics 2015-06-17 J. Segovia , D. R. Entem , F. Fernandez , E. Hernandez

The past four years has witnessed the renaissance of the hadron spectroscopy. Many interesting new hadron states were discovered experimentally, some of which do not fit into the quark model easily. I will give a concise overview of these…

High Energy Physics - Phenomenology · Physics 2008-11-26 Shi-Lin Zhu

Many new results on open and hidden charm spectroscopy have been obtained recently. We present a short review of the experimental findings in the meson sector, of the theoretical interpretations and of the open problems, with a discussion…

High Energy Physics - Phenomenology · Physics 2017-08-23 P. Colangelo , F. De Fazio , R. Ferrandes , S. Nicotri

The physics of charm has become one of the best laboratories exposing the limitations of the naive constituent quark model and also giving hints into a more mature description of meson spectroscopy, beyond the simple quark--antiquark…

High Energy Physics - Phenomenology · Physics 2015-05-18 J. Vijande , A. Valcarce

Using a constituent quark model we study the mass and decay channels of meson meson and meson baryon structures in the charm sector. We show that the $X(3872)$ and $X(3940)$ resonances can be described as mixed charmonium-molecular states…

High Energy Physics - Phenomenology · Physics 2013-12-03 F. Fernandez , D. R. Entem , P. G. Ortega

The physics of charm has become one of the best laboratories exposing the limitations of the naive constituent quark model and also giving hints into a more mature description of hadron spectroscopy. Recent discoveries are a challenge that…

High Energy Physics - Phenomenology · Physics 2008-07-30 A. Valcarce , J. Vijande , N. Barnea

The masses of the excited heavy tetraquarks with hidden charm are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely relativistically. The diquark…

High Energy Physics - Phenomenology · Physics 2008-12-18 D. Ebert , R. N. Faustov , V. O. Galkin

Exotic charmonium and bottonomium resonances recently discovered are discussed and interpreted as diquark-antidiquark states containing a pair of charm quarks and a pair of light, up and down, quarks. Successes, shortcomings and predictions…

High Energy Physics - Phenomenology · Physics 2014-04-29 Luciano Maiani

Over the past few years, there has been a lot of progress in the areas of charm and charmonium spectroscopy, in large part due to the very large data samples being accumulated at the e+e- B-Factories. In this presentation I will focus on…

High Energy Physics - Experiment · Physics 2007-05-23 Helmut Marsiske

The physics of charm has become one of the best laboratories exposing the limitations of the naive constituent quark model and also giving hints into a more mature description of meson spectroscopy, beyond the simple quark--antiquark…

High Energy Physics - Phenomenology · Physics 2009-05-04 J. Vijande , A. Valcarce , J. -M. Richard , N. Barnea

The masses of the ground state and excited heavy tetraquarks with hidden charm and bottom are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely…

High Energy Physics - Phenomenology · Physics 2009-11-13 D. Ebert , R. N. Faustov , V. O. Galkin

Four exotic charmonium-like states, i.e. $X(4140)$, $X(4274)$, $X(4500)$, and $X(4700)$, have been observed very recently by LHCb Collaboration in the decay process $B^+\to J/\psi \phi K^+$ using the 3${\rm fb}^{-1}$ data of $p\bar p$…

High Energy Physics - Phenomenology · Physics 2016-09-21 Ruilin Zhu

The observation of the D_{sJ}^*(2317), D_{sJ}(2460), and SELEX D^*_{sJ}(2632) states with properties differing considerably from what was expected has led to a renewed interest in hadron spectroscopy. In addition to these states,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Stephen Godfrey

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

Since 2003 many charmonium-like states were observed experimentally. Especially those charged charmonium-like $Z_c$ states and bottomonium-like $Z_b$ states cannot be accommodated within the naive quark model, which are good candidates of…

High Energy Physics - Phenomenology · Physics 2017-01-10 Hua-Xing Chen , Wei Chen , Jun He , Xiang Liu , Shi-Lin Zhu

This contribution to the SQM2024 conference covers the molecular hypothesis for the internal structure of some open and hidden charm states. The use of effective theories that incorporate heavy-quark spin symmetry, combined with…

High Energy Physics - Phenomenology · Physics 2024-10-02 Juan M. Torres-Rincon

Inspired by the newly reported $Z_{cs}(3985)^{-}$ by the BESIII Collaboration, we systematically investigate the strange hidden-charm tetraquark systems $cs\bar{c}\bar{u}$ with two structures: meson-meson and diquark-antidiquark. Two quark…

High Energy Physics - Phenomenology · Physics 2022-01-05 Xin Jin , Xuejie Liu , Yaoyao Xue , Hongxia Huang , Jialun Ping

In the past decade many charmonium-like states were observed experimentally. Especially those charged charmonium-like $Z_c$ states and bottomonium-like $Z_b$ states can not be accommodated within the naive quark model. These charged $Z_c$…

High Energy Physics - Phenomenology · Physics 2016-06-20 Hua-Xing Chen , Wei Chen , Xiang Liu , Shi-Lin Zhu

In recent years the B-factories and other machines have found evidence for a large number of new states with hidden charm: candidate h_c(1P), eta_c(2S), and chi_{c2}(2P) states; the well-established X(3872); enhancements called X(3940),…

High Energy Physics - Experiment · Physics 2008-11-26 B. D. Yabsley

We calculate the spectrum of $q\bar q c \bar c$ and $s\bar s c \bar c$ tetraquarks, where $q$, $s$ and $c$ stand for light ($u,d$), strange and charm quarks, respectively, in a relativized diquark model, characterized by one-gluon-exchange…

High Energy Physics - Phenomenology · Physics 2018-11-28 Muhammad Naeem Anwar , Jacopo Ferretti , Elena Santopinto
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