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Related papers: Is the X(3872) a bound state ?

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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

We study the molecular probability of the $X(3872)$ in the $D^0 \bar D^{*0}$ and $D^+ D^{*-}$ channels in several scenarios. One of them assumes that the state is purely due to a genuine nonmolecular component. However, it gets unavoidably…

High Energy Physics - Phenomenology · Physics 2023-07-13 Jing Song , L. R. Dai , E. Oset

It has been proposed that the recently discovered archetypical "exotic" meson, X(3872), with M(X(3872))=3871.68+-0.17 MeV/c^2, and an extremely narrow width, Gamma(X(3872))<1.2 MeV, is a hadronic molecule of bound D^0 and D^*0 mesons. If…

High Energy Physics - Experiment · Physics 2012-12-19 A. Tomaradze , S. Dobbs , T. Xiao , Kamal K. Seth , G. Bonvicini

We use QCD spectral sum rules to test the nature of the meson X(3872), assumed to be an exotic four-quark (c\bar{c}q\bar{q}) state with J^{PC}=1^{++}. For definiteness, we work with the current proposed recently by Maiani et al [1], at…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. D. Matheus , S. Narison , M. Nielsen , J. M. Richard

We analyze the recent data from the BESIII collaboration on the $X(3872)$ state in the $J/\psi\pi^+\pi^-$ and $D^0\bar{D}^0\pi^0$ decay channels. The quantum number and mass of the $X(3872)$ state allow us to exploit the universal feature…

High Energy Physics - Phenomenology · Physics 2025-04-10 Xian-Wei Kang , Jin-Zhe Zhang , Xin-Heng Guo

The present day experimental data on the $X(3872)$ decays do not allow to make clear conclusions on the dominating structure of this state. We discuss here an alternative way to study its structure by means of the two-step $\bar D^*$ (or…

Nuclear Theory · Physics 2016-06-22 Alexei Larionov , Mark Strikman , Marcus Bleicher

Using a general parameterization of two-body scattering amplitude, we systematically analyze the corresponding data on $X(3872)$, more explicitly, the CDF data on inclusive $p\bar{p}$ scattering to $J/\psi \pi^+\pi^-$, and the Belle and…

High Energy Physics - Phenomenology · Physics 2019-12-03 Xian-Wei Kang , J. A. Oller

It is pointed out that in the decays $X(3872) \to D {\bar D} \gamma$ the possible `molecular' component of the X(3872) should give rise essentially only to a $D^0 {\bar D}^0 \gamma$ final state with a predictable spectrum, and should yield…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. B. Voloshin

We show that the literature on pion exchange between charm and bottom mesons is inconsistent. We derive the formalism explicitly, expose differences between papers in the literature and clarify the implications. We show that the X(3872) can…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. E. Thomas , F. E. Close

We present recent studies of charmonium multiquark states. We use different interacting models and numerical methods to study deeply bound four-quark states and meson-meson molecules. No deeply bound four-quark states are found in our…

High Energy Physics - Phenomenology · Physics 2015-05-20 A. Valcarce , J. Vijande

Contrary to almost standard opinion that the X(3872) resonance is the D^{*0}\bar D^0+c.c. molecule or the qc\bar q\bar c four-quark state, we discuss the scenario where the X(3872)resonance is the c\bar c = \chi_{c1}(2P) charmonium which…

High Energy Physics - Phenomenology · Physics 2015-10-16 N. N. Achasov , E. V. Rogozina

The $X(3872)$ is the first and the most interesting one amongst the abundant $XYZ$ states. Its mass coincides exactly with the $D^0\bar D^{*0}$ threshold with an uncertainty of 180 keV. Precise knowledge of its mass is crucial to understand…

High Energy Physics - Phenomenology · Physics 2019-05-28 Feng-Kun Guo

The observation of many unexpected states decaying into heavy quarkonia has challenged the usual QQbar interpretation. One of the most studied exotic states, the X(3872), happens to be copiously produced in high-energy hadron collisions. We…

High Energy Physics - Phenomenology · Physics 2016-06-22 A. Pilloni

The properties of the resonance X(3872) are discussed under the assumption that this resonance is dominantly a `molecular' $J^{PC}=1^{++}$ state of neutral $D$ and $D^*$ mesons. It is argued that in these properties should dominate the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. B. Voloshin

We use QCD sum rules to test the nature of the meson X(3872), assumed to be a mixture between charmonium and exotic molecular [c\bar{q}][q\bar{c}] states with J^{PC}=1^{++}. We find that there is only a small range for the values of the…

High Energy Physics - Phenomenology · Physics 2009-09-24 R. D. Matheus , F. S. Navarra , M. Nielsen , C. M. Zanetti

The Bethe-Salpeter equation for the T-Matrix of D-D* scattering is solved with a meson-meson potential that results from 2nd order Born approximation of quark exchange processes. This potential turns out to be complex and energy dependent…

High Energy Physics - Phenomenology · Physics 2012-09-20 Carlos Pena , David Blaschke

We explore the consequences of treating the X(3872) meson as a tetraquark bound state. As dynamical framework we employ a relativistic constituent quark model which includes infrared confinement in an effective way. We calculate the decay…

High Energy Physics - Phenomenology · Physics 2014-11-20 Stanislav Dubnicka , Anna Z. Dubnickova , Mikhail A. Ivanov , Juergen G. Korner

The production of the X(3872) as a hadronic molecule in hadron colliders is clarified. We show that the conclusion of Bignamini et al., Phys. Rev. Lett. 103 (2009) 162001, that the production of the X(3872) at high $p_T$ implies a…

High Energy Physics - Phenomenology · Physics 2017-11-20 Miguel Albaladejo , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner , Juan Nieves , Andreas Nogga , Zhi Yang

In this talk, we review our recent work about the dynamical studies of $Z^+(4430)$ and X(3872). $Z^+(4430)$ can not be explained as a $D_1'D^*$ or $D_1D^*$ molecular state only considering one pion exchange potential without the cutoff,…

High Energy Physics - Phenomenology · Physics 2009-11-13 Xiang Liu , Yan-Rui Liu , Wei-Zhen Deng

Both the mass (just below the D^{*0}Dbar^0 threshold) and the likely quantum numbers (J^{PC}=1^{++}) of the X(3872) suggest that it is either a weakly-bound hadronic ``molecule'' or a virtual state of charmed mesons. Assuming the X(3872) is…

High Energy Physics - Phenomenology · Physics 2009-09-02 David L. Canham , H. -W. Hammer , Roxanne P. Springer