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Related papers: Hidden-charm scalar tetra-quark mesons

200 papers

With the heavy quark symmetry and spin rearrangement scheme, we study the strong decay behavior of the hidden-charm pentaquark states with $J^P={\frac{3}{2}}^{\pm}, {\frac{5}{2}}^{\pm}$ assuming they are molecular candidates composed of…

High Energy Physics - Phenomenology · Physics 2016-03-02 Guang-Juan Wang , Li Ma , Xiang Liu , Shi-Lin Zhu

Results on light scalar mesons in charmed particle decays studied by the CLEO Collaboration at the Cornell Electron Storage Ring are reviewed.

High Energy Physics - Experiment · Physics 2008-11-26 Jonathan L. Rosner

If a narrow Theta^+ pentaquark exists, it is likely that a ud\bar s-ud triquark-diquark configuration is a significant component of its wave function. If so, the mechanism responsible for the binding of a triquark and a diquark is also…

High Energy Physics - Phenomenology · Physics 2010-04-05 Marek Karliner , Harry J. Lipkin

Combining heavy quark effective theory and the chiral Lagrangian approach we investigate D meson radiative decays. First, we reanalyse $D^{*} \rightarrow D \gamma$ decays using heavy quark spin symmetry, chiral symmetry Lagrangian, but…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Bajc , S. Fajfer , R. J. Oakes

We discuss prospects for detecting the two charm-related phenomena of $D^0$-${\bar D}^0$ mixing and weak radiative decays of $D$ mesons ({\it e.g.} $D\to K^* + \gamma$). A general update of particle-antiparticle mixing for the pseudoscalar…

High Energy Physics - Phenomenology · Physics 2007-05-23 Eugene Golowich

With the spin rearrangement, we have performed a comprehensive investigation of the decay patterns of the S-wave tetraquarks and P-wave tetraquarks where the P-wave excitation exists either between the diquark and anti-diquark pair or…

High Energy Physics - Phenomenology · Physics 2015-12-15 Li Ma , Wei-Zhen Deng , Xiao-Lin Chen , Shi-Lin Zhu

We probe the inner structure of the meson $D^*_{s0}(2317)$ through the decays of $B_{(s)}$ to two charmed mesons within pQCD approach. Assuming $D^*_{s0}(2317)$ as a scalar meson with $\bar cs$ structure, we find that the predictions for…

High Energy Physics - Phenomenology · Physics 2021-07-07 Zhi-Qing Zhang , Meng-Ge Wang , Yan-Chao Zhao , Zhi-Lin Guan , Na Wang

We develop a moment QCD sum rule method augmented by fundamental inequalities to study the existence of exotic doubly hidden-charm/bottom tetraquark states made of four heavy quarks. Using the compact diquark-antidiquark configuration, we…

High Energy Physics - Phenomenology · Physics 2017-09-08 Wei Chen , Hua-Xing Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

We study the quark structure of the sigma meson through the decay of $D_1(2430)$ meson by constructing an effective Lagrangian for charmed mesons interacting with light mesons based on the chiral symmetry and heavy quark symmetry. Within…

High Energy Physics - Phenomenology · Physics 2017-08-23 H. Hoshino , M. Harada , Y. L. Ma

The newly observed hidden-charm meson Zc(3900) with quantum numbers J(P) = 1(+) is considered as a hadronic molecule composed of DD*. We give detailed predictions for the decay modes Zc(+) -> J/psi + pi(+) + gamma and Zc(+) -> J/psi + pi(+)…

High Energy Physics - Phenomenology · Physics 2014-11-19 Thomas Gutsche , Matthias Kesenheimer , Valery E. Lyubovitskij

We study the mass spectra for the $cc\bar c\bar c$ and $bb\bar b\bar b$ tetraquark states by developing a moment sum rule method. Our results show that the $bb\bar b\bar b$ tetraquarks lie below the threshold of $\eta_b(1S)\eta_b(1S)$. They…

High Energy Physics - Phenomenology · Physics 2018-08-29 Wei Chen , Hua-Xing Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

We present a theoretical framework that accounts for the new $D_J$ and $D_{sJ}$ mesons measured in the open-charm sector. These resonances are properly described if considered as a mixture of conventional $P-$wave quark-antiquark states and…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Vijande , F. Fernandez , A. Valcarce

In this work, we take the $X(3872)$ as the hidden-charm tetraquark state with both isospin $I=0$ and $1$ components, then investigate the strong decays $X(3872)\to J/\psi \pi^+\pi^-$, $J/\psi\omega$, $\chi_{c1}\pi^0$, $D^{*0}\bar{D}^0$ and…

High Energy Physics - Phenomenology · Physics 2024-03-12 Zhi-Gang Wang

I briefly review the experimental observations concerning the charmed mesons $D_{sJ}^*(2317)$, $D_{sJ}(2460)$ and survey on some of the interpretations proposed in order to understand their nature. I present an analysis of their decay modes…

High Energy Physics - Phenomenology · Physics 2017-08-23 F. De Fazio

An extended $U(3)_L\bigotimes U(3)_R$ chiral theory which includes pseudoscalar and vector meson nonets as dynamic degrees of freedom is presented. We combine a hidden symmetry approach with a general procedure of including the $\eta'$…

Nuclear Theory · Physics 2007-05-23 E. Gedalin , A. Moalem , L. Razdolskaya

We discuss how the latest data on X(3872) in B and B_s decays speak about its tetraquark nature. The established decay pattern, including the up to date observations by CMS, are explained by the mixing of two quasi-degenerate, unresolvable,…

High Energy Physics - Phenomenology · Physics 2020-08-19 Luciano Maiani , Antonio D. Polosa , Veronica Riquer

We propose a model explaining the strong isospin violations observed in X(3872) decays. The X is assumed to be a compact isosinglet tetraquark and its charged partners to form an isotriplet, together with an additional neutral state mixing…

High Energy Physics - Phenomenology · Physics 2026-03-26 A. Carducci , B. Grinstein , D. Germani , A. D. Polosa

In the framework of one-pion-exchange (OPE) model, we study the hidden-charm and charm-strange molecular pentaquark systems composed of a heavy baryon $(\Sigma_c, \Sigma_c^*)$ and a vector meson $(\bar{K}^*, \bar{D}^*)$, where the S-D…

High Energy Physics - Phenomenology · Physics 2016-08-09 Rui Chen , Xiang Liu , Shi-Lin Zhu

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

We enlarge the so-called extended linear Sigma model (eLSM) by including the charm quark according to the global $U(4)_r\times U(4)_l$ chiral symmetry. In the eLSM, besides scalar and pseudoscalar mesons, also vector and axial-vector mesons…

High Energy Physics - Phenomenology · Physics 2015-06-22 Walaa I. Eshraim , Francesco Giacosa