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Heavy meson spectroscopy above open flavor thresholds has become a challenge both from the experimental and theoretical points of view. Experimentally, several signals have been interpreted as meson resonances with unusual properties;…

High Energy Physics - Phenomenology · Physics 2013-09-06 A. Valcarce , T. F. Caramés , J. Vijande

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

Quark models taking into account the dynamical effects of hadronic decay often produce very different predictions for mass shifts in the hadron spectrum. The consequences for meson spectroscopy can be dramatic and completely obscure the…

High Energy Physics - Phenomenology · Physics 2016-05-16 George Rupp , Susana Coito , Eef van Beveren

We present a plausible mechanism for the origin of the $XYZ$ mesons in the heavy meson spectra within a standard quark-model picture. We discuss the conditions required for the existence of four--quark bound states or resonances…

High Energy Physics - Phenomenology · Physics 2015-07-30 J. Vijande , A. Valcarce

Results obtained by various experiments show that the $D_{s0}^{\ast}(2317)$ and $D_{s1}(2460)$ mesons are very narrow states located below the $DK$ and $D^{\ast}K$ thresholds, respectively. This is markedly in contrast with the expectations…

High Energy Physics - Phenomenology · Physics 2016-11-02 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernandez

The last two decades are marked by a renaissance in hadronic spectroscopy caused by the arrival of vast experimental information on exotic states in the spectrum of charmonium and bottomonium. Most of such states have properties at odds…

High Energy Physics - Phenomenology · Physics 2022-12-02 Christoph Hanhart , Alexey Nefediev

Heavy hadron spectroscopy was well understood within the naive quark model until the end of the past century. However, in 2003, the $X(3872)$ was discovered, with puzzling properties difficult to understand in the simple naive quark model…

High Energy Physics - Phenomenology · Physics 2020-12-21 Pablo G. Ortega , David R. Entem

Many efforts have been made to reveal the nature of the overabundant resonant structures observed by the worldwide experiments in the last two decades. Hadronic molecules attract special attention because many of these seemingly…

High Energy Physics - Phenomenology · Physics 2021-08-10 Xiang-Kun Dong , Feng-Kun Guo , Bing-Song Zou

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

We study heavy hadron spectroscopy near heavy meson thresholds. We employ heavy pseudoscalar meson P and heavy vector meson P* as effective degrees of freedom and consider meson exchange potentials between them. All possible composite…

High Energy Physics - Phenomenology · Physics 2015-06-11 Shunsuke Ohkoda , Y. Yamaguchi , S. Yasui , K. Sudoh , A. Hosaka

Prompted by the recent surprising results in QCD spectroscopy, we extend to heavy flavors the hadron mass relations showing that the constituent quark mass differences and ratios have the same values when obtained from mesons and baryons.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marek Karliner , Harry J. Lipkin

Motivated by the recent surprising discovery of two new meson states with c s-bar quark content but unexpectedly low masses and narrow total decay widths, we work out, in a nonrelativistic potential-model approach developed already some two…

High Energy Physics - Phenomenology · Physics 2009-11-10 Wolfgang Lucha , F. F. Schoberl

Mesonic resonances are generally observed in data as narrow, moderately broad, or wide peaks in scattering or production processes. In the eyes of nearly all experimentalists, any suchlike bump is a true resonance as soon as its statistical…

High Energy Physics - Phenomenology · Physics 2015-06-03 George Rupp , Susana Coito , Eef van Beveren

We show that under a number of rather plausible assumptions QCD spectrum may contain a number of mesons which have not been predicted or observed. Such states will have the quantum numbers of two existing mesons and masses very close to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas D. Cohen , Boris A. Gelman , Shmuel Nussinov

The $\Upsilon(10753)$ state has been recently observed by the Belle and Belle~II collaborations with enough global significance to motivate an assessment of the high-energy spectrum usually predicted by any reasonable \emph{na\"ive} quark…

High Energy Physics - Phenomenology · Physics 2024-03-07 P. G. Ortega , D. R. Entem , F. Fernández , J. Segovia

The bottom-charmed ($B_c$) mesons are more stable than their charmonium ($c\bar c$) and bottomium ($b\bar b$) partners because they cannot annihilate into gluons. However, the low production cross-sections and signal-to-background ratios…

High Energy Physics - Phenomenology · Physics 2020-04-22 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernandez

Recent developments in hadron spectroscopy triggers the discussion on various exotic configurations beyond the simple three-quark state for baryons and quark-anti-quark pair for mesons. In particular, the states observed near a two-hadron…

High Energy Physics - Phenomenology · Physics 2020-01-08 Tetsuo Hyodo

Since the discovery of the $J/\psi$, the quark model was very successful in describing the spectrum and properties of heavy mesons including only $q\bar q$ components. However since 2003, with the discovery of the $X(3872)$, many states…

High Energy Physics - Phenomenology · Physics 2019-02-20 D. R. Entem , P. G. Ortega , J. Segovia , F. Fernández

The implementation of the heavy quark spin symmetry in possible molecular states at the mixed bottom-charm threshold is somewhat different from that at the open charm or bottom thresholds. In particular it depends on two parameters…

High Energy Physics - Phenomenology · Physics 2018-10-10 M. B. Voloshin

A semi-relativistic potential model is adopted to calculate the mass spectra of charmed and charmed-strange meson states up to the $2D$ excitations.The strong decay properties are further analyzed with a chiral quark model by using the…

High Energy Physics - Phenomenology · Physics 2022-03-23 Ru-Hui Ni , Qi Li , Xian-Hui Zhong
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