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Related papers: Does the $J^{PC}=1^{+-}$ counterpart of the $X(387…

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Very recently the BaBar collaboration has put forward a claim that the X(3872) is not a 1^++ resonance, as most of the phenomenological work on the subject was relying on, but rather a 2^-+ one. We examine the consequences of this quantum…

High Energy Physics - Phenomenology · Physics 2014-11-21 T. J. Burns , F. Piccinini , A. D. Polosa , C. Sabelli

Since the discovery of X(3872), its structure has been in ceaseless dispute. The data of $X(3872)\rightarrow \pi^+\pi^-\pi^0 J/\psi$ suggest that X(3872) may be a high-spin charmonium-like of $2^{-+}$. In terms of the light front quark…

High Energy Physics - Phenomenology · Physics 2012-01-04 Hong-Wei Ke , Xue-Qian Li

Very recently, the Belle and BESIII experiments observed a new charmonium-like state $X(3823)$, which is a good candidate for the $D$-wave charmonium $\psi(1^3D_2)$. Because the $X(3823)$ is just near the $D\bar{D}^*$ threshold, the decay…

High Energy Physics - Phenomenology · Physics 2016-03-01 Bo Wang , Hao Xu , Xiang Liu , Dian-Yong Chen , Susana Coito , Estia Eichten

The $D^{(\ast)}\Xi_{cc}^{(\ast)}$ system and $\bar{\Xi}_{cc}^{(\ast)}\Xi_{cc}^{(\ast)}$ system can be related to the $D^{(\ast)}\bar{D}^{(\ast)}$ system via heavy anti-quark di-quark symmetry (HADS). In this work, we employ a contact-range…

High Energy Physics - Phenomenology · Physics 2021-03-17 Ming-Zhu Liu , Li-Sheng Geng

We have used the dynamically constrained phase space coalescence model to study the production of the exotic state $X(3872)$ based on the hadronic final states generated by the parton and hadron cascade model (PACIAE) with $|y|<1$ and $p_T…

High Energy Physics - Phenomenology · Physics 2021-10-29 Hong-ge Xu , Zhi-Lei She , Dai-Mei Zhou , Liang Zheng , Xiao-Lin Kang , Gang Chen , Ben-Hao Sa

Heavy-light diquarks can be the building blocks of a rich spectrum of states which can accommodate some of the newly observed charmonium-like resonances not fitting a pure c-cbar assignment. We examine this possibility for hidden and open…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Maiani , F. Piccinini , A. D. Polosa , V. Riquer

The nature of the $X(3872)$ and other exotic hadrons has been a subject of extensive investigation since the first observation of the $X(3872)$ in 2003. While various theoretical models have been proposed, including hadronic molecular and…

High Energy Physics - Phenomenology · Physics 2025-08-12 Kotaro Miyake , Yasuhiro Yamaguchi

By using a combined amplitude analysis of the $\gamma\gamma\rightarrow D\bar{D}$ and $\gamma\gamma\rightarrow J/\psi\omega$ data, we demonstrate that the $X(3915)$, which is quoted as a $J^{PC}=0^{++}$ state in the Particle Data Group…

High Energy Physics - Phenomenology · Physics 2015-07-15 Zhi-Yong Zhou , Zhiguang Xiao , Hai-Qing Zhou

The $X$(3872) formation and decay processes in the $B$-decay are investigated by a $c\bar c$-two-meson hybrid model. The two-meson state consists of the $D^0{\bar D}^*{}^0$, $D^+D^{*-}$, $J/\psi\rho$, and $J/\psi\omega$ channels. The…

High Energy Physics - Phenomenology · Physics 2015-05-13 Sachiko Takeuchi , Kiyotaka Shimizu , Makoto Takizawa

The possible neutral $D^{(*)}\bar{D}^{(*)}$ and $B^{(*)}\bar{B}^{(*)}$ molecular states are studied in the framework of the constituent quark models, which is extended by including the $s$-channel one gluon exchange. Using different types…

High Energy Physics - Phenomenology · Physics 2017-09-13 You-Chang Yang , Zhi-Yun Tan , Jialun Ping , Hong-Shi Zong

QCD sum-rules are employed to determine whether the X(3872) can be described as a mixed state that couples to $J^{PC}=1^{++}$ charmonium hybrid and $\bar D D^*$ molecular currents. After calculating the mixed correlator of hybrid and…

High Energy Physics - Phenomenology · Physics 2013-09-24 Wei Chen , Hong-ying Jin , R. T. Kleiv , T. G. Steele , Meng Wang , Qing Xu

We explore the quark-mass dependence of the pole position of the X(3872) state within the molecular picture. The calculations are performed within the framework of a nonrelativistic Faddeev-type three-body equation for the $D\bar{D}\pi$…

High Energy Physics - Phenomenology · Physics 2013-10-01 V. Baru , E. Epelbaum , A. A. Filin , C. Hanhart , U. -G. Meißner , A. V. Nefediev

We revisit the consequences of the heavy-quark spin symmetry for the possible spin partners of the $X(3872)$. We confirm that, if the $X(3872)$ were a $D\bar{D}^*$ molecular state with the quantum numbers $J^{PC}=1^{++}$, then in the strict…

High Energy Physics - Phenomenology · Physics 2016-11-04 V. Baru , E. Epelbaum , A. A. Filin , C. Hanhart , Ulf-G. Meißner , A. V. Nefediev

The nature of the $X(3872)$ and other exotic hadrons has been a subject of extensive investigation. While various theoretical models have been proposed, experimental evidence suggests that the $X(3872)$ may be a mixture state of a hadronic…

High Energy Physics - Phenomenology · Physics 2026-05-12 Kotaro Miyake , Yasuhiro Yamaguchi

We re-examine the re-scattering mechanism for the X(3872), as a candidate for the 2P charmonium state $\chi_{c1}(2P)$, decaying to $J/\psi\rho(\omega)$ through exchanging $D^{(*)}$ mesons between intermediate states $D(\bar{D})$ and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ce Meng , Kuang-Ta Chao

The bound state problem of $D^0\bar{D}^{\ast0}$ ($\bar{D}^0{D}^{\ast0}$) is relevant to the molecular interpretation of the X(3872). We investigated this problem in a chiral quark model by solving the resonating group method equation. We…

High Energy Physics - Phenomenology · Physics 2009-05-07 Yan-Rui Liu , Zong-Ye Zhang

A solvable coordinate-space model is employed to study the $c\bar{c}$ component of the X(3872) wave function, by coupling a confined $^3P_1$ $c\bar{c}$ state to the almost unbound $S$-wave $D^0\bar{D}^{*0}$ channel via the $^3P_0$…

High Energy Physics - Phenomenology · Physics 2015-06-12 Susana Coito , George Rupp , Eef van Beveren

The BaBar analysis which favours $2^{-+}$ quantum numbers for the X(3872) implies that it may be none other than the 1D2 charmonia state. In that case the isospin breaking in closed flavour modes may be the result of re-scattering from open…

High Energy Physics - Phenomenology · Physics 2015-05-27 T. J. Burns

The four--quark system $c\bar c n\bar n$ is studied in the framework of the constituent quark model. Using different types of quark-quark potentials, we solve the four--body Schr\"odinger equation by means of the hyperspherical harmonic…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Vijande , E. Weissman , N. Barnea , A. Valcarce

The LHCb collaboration has recently announced the discovery of two hidden-charm pentaquark states with also strange quark content, $P_{cs}(4338)$ and $P_{cs}(4459)$; its analysis points towards having both hadrons isospin equal to zero and…

High Energy Physics - Phenomenology · Physics 2023-11-03 Gang Yang , Jialun Ping , Jorge Segovia