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Related papers: Heavy $K^*(4307)$ meson with hidden charm

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Several observed states close to the $D\bar{D}^*$ and $D^*_{(s)}\bar{D}^*_{(s)}$ thresholds, as the X(3872) and some XYZ particles can be described in terms of a two-meson molecule. Furthermore, doubly charmed states are also predicted.…

High Energy Physics - Phenomenology · Physics 2013-11-08 R. Molina , H. Nagahiro , A. Hosaka

Nowadays, it is generally accepted that the $DK$ interaction in isospin zero is strongly attractive and the $D_{s0}^*(2317)$ can be described as a $DK$ molecular state. Recent studies show that the three-body $DDK$ system binds as well with…

High Energy Physics - Phenomenology · Physics 2020-02-05 Yin Huang , Ming-Zhu Liu , Ya-Wen Pan , Li-Sheng Geng , A. Martínez Torres , K. P. Khemchandani

We present selected results on the properties of strange and heavy-flavoured mesons in a hot and dense nuclear medium, with emphasis in selfconsistent coupled-channel approaches based on the chiral Lagrangian. In the strangeness sector, we…

I present results of a heavy hadron chiral perturbation theory analysis of the decays and masses of the recently discovered excited charm mesons. The present data on the electromagnetic branching ratios are consistent with heavy quark…

High Energy Physics - Phenomenology · Physics 2014-11-18 Thomas Mehen

The charm fragmentation function has been measured in photoproduction of jets containing D^*+- mesons. The measured function has been used to extract free parameters of different fragmentation models. Measurements of excited charm,…

High Energy Physics - Experiment · Physics 2019-08-13 Leonid Gladilin

We calculate the masses of baryons containing one, two, or three heavy quarks using lattice QCD. We consider all possible combinations of charm and bottom quarks, and compute a total of 36 different states with $J^P = \frac12^+$ and $J^P =…

High Energy Physics - Lattice · Physics 2014-11-26 Zachary S. Brown , William Detmold , Stefan Meinel , Kostas Orginos

The recent observation at CDF and D0 of $\Sigma_b$, $\Sigma^*_b$ and $\Xi_b$ baryons opens the door to the advent of new states in the bottom baryon sector. The states measured provide sufficient constraints to fix the parameters of…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Valcarce , H. Garcilazo , 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

Using the Fixed Center Approximation to Faddeev equations we have investigated the $DKK$ and $DK\bar{K}$ three-body systems, considering that the $D^*_{s0}(2317)$ acts as the heavy cluster in both cases, generated from the $DK$ interaction…

High Energy Physics - Phenomenology · Physics 2018-12-04 V. R. Debastiani , J. M. Dias , E. Oset

We investigate on exotic tetraquark hadrons of the kind [cs][cbar sbar] by computing their spectrum and decay modes within a constituent diquark-antidiquark model. We also compare these predictions with the present experimental knowledge.

High Energy Physics - Phenomenology · Physics 2013-05-29 NV Drenska , R Faccini , AD Polosa

Stimulated by the recent observation of the $D_2^\ast(3000)$, we study the decay behaviors of the $3P$ and $2F$ charmed mesons in the present work. By comparing the masses and decay properties of the $3^3P_2$ and $2^3F_2$ charmed mesons…

High Energy Physics - Phenomenology · Physics 2016-12-07 Jun-Zhang Wang , Dian-Yong Chen , Qin-Tao Song , Xiang Liu , Takayuki Matsuki

We give heavy quark-diquark symmetry predictions for doubly heavy baryons and tetraquarks in light of the recent discovery of the $\Xi_{cc}^{++}$ by LHCb. For five excited doubly charm baryons that are predicted to lie below the $\Lambda_c…

High Energy Physics - Phenomenology · Physics 2017-12-06 Thomas Mehen

In 2012, we investigated the possible molecular states composed of two charmed mesons [Phys.Rev. D 88, 114008 (2013), arXiv:1211.5007 [hep-ph](2012)]. The $D^*D$ system with the quantum numbers of $I(J^P)=0(1^+)$ was found to be a good…

High Energy Physics - Phenomenology · Physics 2021-09-07 Ning Li , Zhi-Feng Sun , Xiang Liu , Shi-Lin Zhu

We study the spectral distributions of charmed meson with $J^P=0^-$ quantum numbers in cold nuclear matter applying a self-consistent and covariant many-body approach established previously for the nuclear dynamics of kaons. At leading…

Nuclear Theory · Physics 2010-12-16 M. F. M. Lutz , C. L. Korpa

The spectrum of the charmed meson-(anti)meson system is a fundamental tool for disentangling the nature of a few exotic hadrons, including the recently discovered $T_{cc}^+(3875)$ tetraquark, the $X(3960)$, or the $X(3872)$, the nature of…

High Energy Physics - Phenomenology · Physics 2024-10-22 Fang-Zheng Peng , Mao-Jun Yan , Manuel Pavon Valderrama

The molecular assignments to the three $P_c$ states and the similar production mechanism between the $\Lambda_b\to P_c+K$ and $B\to XYZ+K$ convince us the $B$ decaying to a charmonium state plus light mesons could be the appropriate…

High Energy Physics - Phenomenology · Physics 2021-11-11 Fu-Lai Wang , Xin-Dian Yang , Rui Chen , Xiang Liu

We explore the possibility of experimentally detecting a predicted $h_1 ~[I^G(J^{PC})=0^-(1^{+-})]$ state of hidden charm made out from the $D^* \bar D^*$ interaction. The method consists in measuring the decay of X(4660) into $\eta D^*…

High Energy Physics - Phenomenology · Physics 2015-06-16 Weihong Liang , M. Albaladejo , E. Oset

Possible $2S$ and $1D$ excited $D$ and $D_s$ states are studied, the charmed states $D(2550)^0$, $D^\ast(2600)$, $D(2750)^0$ and $D^\ast(2760)$ newly observed by the BaBar Collaboration are analyzed. The masses of these states are explored…

High Energy Physics - Phenomenology · Physics 2011-06-30 Bing Chen , Ling Yuan , Ailin Zhang

In this work, $T_{cc}$ double charm tetraquark and $1^{+}$ and $0^{+}$ hidden charm tetraquarks are studied within the QCD sum rules framework. In the heavy-quark limit, the $1^+$ and $0^+$ tetraquarks are degenerate and the difference in…

High Energy Physics - Phenomenology · Physics 2025-02-11 Semra Sari Ferah , Altug Ozpineci

Discovery of the X(3872) meson in 2003 ignited intense interest in exotic (neither $q\bar{q}$ nor $qqq$) hadrons, but a $c\bar{c}$ interpretation of this state was difficult to exclude. An unequivocal exotic was discovered in the…

High Energy Physics - Phenomenology · Physics 2024-10-16 Feng Zhu , Gerry Bauer , Kai Yi