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Related papers: Is the X(3872) Production Cross Section at Tevatro…

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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

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 a recent paper we have proposed a method to estimate the prompt production cross section of X(3872) at the Tevatron assuming that this particle is a loosely bound molecule of a D and a D*bar meson. Under this hypothesis we find that it…

High Energy Physics - Phenomenology · Physics 2010-04-23 C Bignamini , B Grinstein , F Piccinini , AD Polosa , V Riquer , C Sabelli

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

In these proceedings we summarise the recent studies of exotic hadrons performed at the LHC and Tevatron. The X(3872) production cross section and mass measurements are reported, along with the determination of its quantum numbers, the…

High Energy Physics - Experiment · Physics 2019-08-15 Vincenzo Chiochia

We predict the differential cross sections for production of the X(3872) at the Tevatron and the Large Hadron Collider from both prompt QCD mechanisms and from decays of b hadrons. The prompt cross section is calculated using the NRQCD…

High Energy Physics - Phenomenology · Physics 2014-11-20 Pierre Artoisenet , Eric Braaten

We show the results obtained for the cross sections of the processes $\bar D D$, $\bar D^* D$, $\bar D^* D^*\to\pi X(3872)$, information which is necessary to determine the $X(3872)$ abundance in heavy ion collisions. Our formalism is based…

High Energy Physics - Phenomenology · Physics 2015-07-21 A. Martinez Torres , K. P. Khemchandani , F. S. Navarra , M. Nielsen , Luciano M. Abreu

The $X(3872)$, whose mass coincides with the $D^0\bar D^{*0}$ threshold, is the most extended hadron object. Since its discovery in 2003, debates have never stopped regarding its internal structure. We propose a new object, the $X$ atom,…

High Energy Physics - Phenomenology · Physics 2021-07-01 Zhen-Hua Zhang , Feng-Kun Guo

The claim that the $X(3872)$ meson cannot be a charm-meson molecule because its prompt production cross section at hadron colliders is too large is based on an upper bound in terms of a cross section for producing charm-meson pairs.…

High Energy Physics - Phenomenology · Physics 2019-11-28 Eric Braaten , Li-Ping He , Kevin Ingles

In this proceeding we show the results found for the cross sections of the processes $\bar D D\to\pi X(3872)$, $\bar D^* D\to \pi X(3872)$ and $\bar D^* D^*\to\pi X(3872)$, information needed for calculations of the $X(3872)$ abundance in…

High Energy Physics - Phenomenology · Physics 2014-12-18 A. Martinez Torres , K. P. Khemchandani , F. S. Navarra , M. Nielsen , Luciano M. Abreu

We evaluate the production cross sections of $X(3872)$ at the LHC and Tevatron at NLO in $\alpha_s$ in NRQCD by assuming that the short-distance production proceeds dominantly through its $\chi_{c1}'$ component in our…

High Energy Physics - Phenomenology · Physics 2017-10-25 Ce Meng , Hao Han , Kuang-Ta Chao

We have determined the production cross sections of the $X(3872)$ state in the reactions $\bar D D\to\pi X$, $\bar D^* D\to \pi X$ and $\bar D^* D^*\to\pi X$, information which is useful for studies of the $X(3872)$ meson abundance in heavy…

High Energy Physics - Phenomenology · Physics 2014-12-24 A. Martinez Torres , K. P. Khemchandani , F. S. Navarra , M. Nielsen , Luciano M. Abreu

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

Exploring the nature of exotic multiquark candidates such as the $X(3872)$ plays a pivotal role in understanding quantum chromodynamics (QCD). Despite significant efforts, consensus on their internal structures is still lacking. As a prime…

High Energy Physics - Phenomenology · Physics 2021-02-09 Hui Zhang , Jinfeng Liao , Enke Wang , Qian Wang , Hongxi Xing

Inclusive production cross sections of the possible exotic state X(3872) in proton-proton, pionp-roton and proton-antiproton collisions are calculated using a statistical based model, which is previously used to describe inclusive charmed…

High Energy Physics - Phenomenology · Physics 2021-11-11 Gábor Balassa , György Wolf

In order to understand the structure of the X(3872), the $c \bar c$ charmonium core state coupling to the $D^0 \bar D^{\ast 0}$ and $D^+ D^{\ast -}$ molecular states are studied. The strengths of the couplings between the charmonium state…

High Energy Physics - Phenomenology · Physics 2014-05-07 Makoto Takizawa , Sachiko Takeuchi

If the $X(3872)$ is a weakly bound charm-meson molecule, it can be produced by the creation of $D^{*0} \bar{D}^0$ or $D^{0} \bar{D}^{*0}$ at short distances followed by the formation of the bound state from the charm-meson pair. The $X$ can…

High Energy Physics - Phenomenology · Physics 2019-11-20 Eric Braaten , Li-Ping He , Kevin Ingles

Latest measurements suggest that the X(3872) mass lies less than 200 keV away from the D0-Dbar0* threshold, reenforcing its interpretation as a loosely-bound mesonic molecule. This observation implies that in processes like D0-Dbar0-pi0…

High Energy Physics - Phenomenology · Physics 2018-07-27 M. Schmidt , M. Jansen , H. -W. Hammer

All existing experimental evidence of the bound state nature of the $X(3872)$ relies on considering its decay products with a finite experimental spectral mass resolution which is typically $\Delta m \ge 2 $MeV and much larger than its…

High Energy Physics - Phenomenology · Physics 2020-01-08 Pablo G. Ortega , Enrique Ruiz Arriola

Because of the controversial X(3872) meson's very close proximity to the $D^0\bar{D}^{*0}$ threshold, this charmonium-like resonance is often considered a meson-meson molecule. However, a molecular wave function must be essentially of a…

High Energy Physics - Phenomenology · Physics 2012-11-06 S. Coito , G. Rupp , E. van Beveren
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