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Related papers: Line Shapes of the X(3872)

200 papers

We evaluate the contribution to the $X(3872)$ width from a triangle mechanism in which the $X$ decays into $D^{*0}\bar{D}^0 -cc$, then the $D^{*0} (\bar{D}^{*0})$ decays into $D^0 \pi^0$ ($\bar{D}^0 \pi^0$) and the $D^0 \bar{D}^0$ fuse to…

High Energy Physics - Phenomenology · Physics 2020-06-24 Raquel Molina , Eulogio Oset

Through the scattering of light-pseudoscalar mesons ($\pi,K,\eta,\eta'$) off charmed mesons ($D, D_s$), we study the $D^{*}_{s0}(2317)$ state and other relevant charm scalar mesons in a unitarized chiral effective field theory approach. We…

High Energy Physics - Phenomenology · Physics 2015-11-11 Zhi-Hui Guo , Ulf-G. Meißner , De-Liang Yao

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

A recent quark-model description of X(3872) as an unquenched $2\,{}^{3\!}P_1$ $c\bar{c}$ state is generalised by now including all relevant meson-meson configurations, in order to calculate the widths of the experimentally observed…

High Energy Physics - Phenomenology · Physics 2015-01-28 Marco Cardoso , George Rupp , Eef van Beveren

In this work the production of the state $X(3872)$ is estimated via the reaction $B^0 \to K^{\ast 0} X(3872)$ through triangle mechanisms described by the sequence $B^0 \to D_s^{(*)+} (\to K^{\ast 0} D^{(*)+} ) \ D^{(*)-} \to K^{\ast 0} \ (…

High Energy Physics - Phenomenology · Physics 2025-11-06 Luciano M. Abreu

We study $D\bar{D}^*$ ($D^*\bar{D}$) scattering in the framework of unitarized heavy meson chiral perturbation theory with pion exchange and a contact interaction. $^3S_1-$$^3D_1$ mixing effects are taken into account. A loosely bound state…

High Energy Physics - Phenomenology · Physics 2013-04-04 P. Wang , X. G. Wang

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

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 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

We discuss some puzzling aspects of the narrow hidden charm resonance that was recently discovered by the Belle Collaboration at mass 3872 MeV. In order to determine its quantum numbers, a crucial piece of information is the spin of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sandip Pakvasa , Mahiko Suzuki

We study the properties of the scalar charm resonances $D_{s0}(2317)$ and $D_0(2400)$, and the theoretical hidden charm state X(3700) in nuclear matter. We find that for the $D_{s0}(2317)$ and X(3700) resonances, with negligible and small…

Nuclear Theory · Physics 2010-02-25 Laura Tolos , Raquel Molina , Daniel Gamermann , Eulogio Oset

We measure the dipion mass spectrum in X(3872)--> J/Psi Pi+ Pi- decays using 360 pb-1 of pbar-p collisions at 1.96 TeV collected with the CDF II detector. The spectrum is fit with predictions for odd C-parity (3S1, 1P1, and 3DJ) charmonia…

High Energy Physics - Experiment · Physics 2010-05-12 A. Abulencia , D. Acosta , J. Adelman

We present results on the X(3872), produced in $B^+ \to X(3872) K^+$ and $B^0 \to X(3872) K^0_S$ decays where $X(3872) \to J/\psi \pi^+ \pi^-$. We report the first statistically significant observation of $B^0 \to X(3872) K^0_S$ and measure…

High Energy Physics - Experiment · Physics 2012-08-27 Belle collaboration

We calculate the properties of excited charm and charm-strange mesons. We use the relativized quark model to calculate their masses and wavefunctions that are used to calculate radiative transition partial widths and the $^3P_0$…

High Energy Physics - Phenomenology · Physics 2016-03-02 Stephen Godfrey , Kenneth Moats

In this article, we assign the newly reported state $X(3842)$ to be a D-wave $\overline{c}c$ meson, and study its mass and decay constant with the QCD sum rules by considering the contributions of the vacuum condensates up to dimension-6 in…

High Energy Physics - Phenomenology · Physics 2021-11-16 Guo Liang Yu , Zhi Gang Wang

In this work we present our model that dynamically generates resonances from charmed and light pseudoscalar and vector mesons. The model generates a rich spectrum of charmed and hidden charm scalar and axial resonances, most of them which…

High Energy Physics - Phenomenology · Physics 2009-05-12 D. Gamermann , E. Oset , B. S. Zou

Belle data for the pi-pi mass spectrum in X(3872) -> pi-pi + JPsi are well fitted by rho + J/Psi with JPC = 1++, but are poorly fitted by the pi-pi S-wave. Formulae for partial wave amplitudes are given for all likely JPC and decay modes of…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. V. Bugg

The recently BaBar results raise the possibility that X(3872) has negative parity. This makes people reconsider assigning X(3872) to the $1{^1D_2}(c\bar c)$ state. In this paper we give a general form of the wave function of $2^{-+}$…

High Energy Physics - Phenomenology · Physics 2016-01-05 Tianhong Wang , Guo-Li Wang , Yue Jiang , Wan-Li Ju

We fit the invariant mass distribution of ${X(3872)}\rightarrow{J}/{\psi}\pi^+\pi^-$ from LHCb using the propagator for S-wave near-threshold states in effective field theory. In this way, we can directly determine the $Z$ which measures…

High Energy Physics - Phenomenology · Physics 2025-04-10 Hongge Xu , Ning Yu , Zuman Zhang

The properties of the $X(3872)$ and its spin partner, the $X(4014)$, are studied both in vacuum and at finite temperature. Using an effective hadron theory based on the hidden-gauge Lagrangian, the $X(3872)$ is dynamically generated from…

High Energy Physics - Phenomenology · Physics 2023-03-14 Gloria Montaña , Angels Ramos , Laura Tolos , Juan M. Torres-Rincon