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Related papers: The Case for a Vector Glueball

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The properties of the $0^{++}$ and $0^{-+}$ meson multiplets are discussed. Quoted are the $0^{++}$ and $0^{-+}$ glueball masses determined from data fit.

High Energy Physics - Phenomenology · Physics 2007-10-11 Michal Majewski

Building on recent work by Brodsky {\it et al.}, we advocate searching for glueball degrees of freedom in $e^+e^- \to J/\psi\to \phi f_0$ at CLEO-c and BES.

High Energy Physics - Phenomenology · Physics 2009-11-10 Frank E. Close , Qiang Zhao

The mass of the lowest scalar glueball is discussed by using QCD sum rules. We find that the glueball mass is sensitive to the choice of moments and slightly depends on the radiative corrections. With the help of suitable moments and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tao Huang , Ai-lin Zhang

This is a contribution to the review "50 Years of Quantum Chromdynamics" edited by F. Gross and E. Klempt [arXiv:2212.11107], to be published in EPJC. The contribution remembers the early searches and explains how to find a glueball, based…

High Energy Physics - Phenomenology · Physics 2022-12-27 Eberhard Klempt

Glueballs remain an experimentally undiscovered expectation of QCD. Lattice QCD (As well as other theoretical approaches) predicts a spectrum of glueballs, with the tensor ($J^{PC}=2^{++}$) glueball being the second lightest, behind the…

High Energy Physics - Phenomenology · Physics 2023-08-02 Arthur Vereijken , Shahriyar Jafarzade , Milena Piotrowska , Francesco Giacosa

We present a two-flavour linear sigma model with global chiral symmetry and (axial-)vector mesons as well as an additional glueball degree of freedom. We study the structure of the well-established scalar resonances f0(1370) and f0(1500):…

High Energy Physics - Phenomenology · Physics 2012-06-14 Stanislaus Janowski , Denis Parganlija , Francesco Giacosa , Dirk H. Rischke

Lattice QCD predictions have motivated several recent studies of the mixing between the predicted JPC = 0++ glueball and a qqbar nonet in the 1.3 to 1.7 GeV region. We show that results from apparently different approaches have some common…

High Energy Physics - Phenomenology · Physics 2016-09-06 F. E. Close , A. Kirk

The scalar glueball $G$ is the lightest particle of the Yang-Mills sector of QCD, with a lattice predicted mass of about $m_{G}\simeq1.7$ GeV. It is natural to investigate glueball-glueball scattering and the possible emergence of a bound…

High Energy Physics - Phenomenology · Physics 2022-06-15 Francesco Giacosa , Alessandro Pilloni , Enrico Trotti

Double vector meson photoproduction, p(gamma, G -> VV)p, mediated by a scalar glueball G is investigated. Using vector meson dominance (VMD) and Regge/pomeron phenomenology, a measureable glueball enhancement is predicted in the invariant…

Nuclear Theory · Physics 2014-11-18 Stephen R. Cotanch , Robert A. Williams

A coupled-channel analysis of BESIII data on radiative $J/\psi$ decays into $\pi\pi$, $K\bar K$, $\eta\eta$ and $\omega\phi$ has been performed. The partial-wave amplitude is constrained by a large number of further data. The analysis finds…

High Energy Physics - Phenomenology · Physics 2021-04-14 Andrey V. Sarantsev , Igor Denisenko , Ulrike Thoma , Eberhard Klempt

We scrutinize the determination of glueball masses in pure Yang-Mills theory from functional equations, i.e. Dyson-Schwinger and Bethe-Salpeter equations. We survey the state-of-the-art input (dressed propagators and vertices) with an…

High Energy Physics - Phenomenology · Physics 2025-03-07 Markus Q. Huber , Christian S. Fischer , Hèlios Sanchis-Alepuz

We discuss recent results on the calculation of glueball decay rates in the Witten-Sakai-Sugimoto model, which favor the $f_0(1710)$ meson as a glueball candidate. The flavor asymmetric decay of $f_0(1710)$ is frequently attributed to a…

High Energy Physics - Phenomenology · Physics 2015-10-30 Frederic Brünner , Anton Rebhan

The omega-phi threshold peak observed by BES in J/Psi -> gamma(omega-phi) may be interpreted quantitatively in terms of a glueball component in fo(1790).

High Energy Physics - Phenomenology · Physics 2007-05-23 D. V. Bugg

Using the ``glueball dominance'' picture of the mixing between q\bar{q} mesons of different hidden flavors, we establish new glueball-meson mass relations which serve as a basis for glueball spectral systematics. For the tensor glueball…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. M. Brisudova , L. Burakovsky , T. Goldman

The $f_0(1500)$ is identified in three glueball favoured production mechanisms: $p\bar{p}$ annihilation, $\psi \to \gamma f_0$ and Central Production. The production rate for glueballs in $\psi \to \gamma G$ has been quantified and the…

High Energy Physics - Phenomenology · Physics 2009-10-30 Frank Close

We study the glueballs in a four-dimensional ${\cal N}=2$ super Yang-Mills theory with fundamental matters in terms of the supergravity dual. The supergravity background is constructed by $N$ D3 brane with a probe D7 brane. We numerically…

High Energy Physics - Theory · Physics 2007-05-23 Kenji Suzuki

The scalar mesons are established for a long time, but their nature is still an open question. In this paper, we investigate the potential of categorizing their $SU(3)_f$ representations via $J/\psi\to SV$ and $\gamma S$, offering a…

High Energy Physics - Phenomenology · Physics 2024-09-30 Chao-Qiang Geng , Chia-Wei Liu , Xiao Yu , Ao-Wen Zhou

We compute the matrix elements of the energy-momentum tensor between glueball states and the vacuum in SU(3) lattice gauge theory and extrapolate them to the continuum. These matrix elements may play an important phenomenological role in…

High Energy Physics - Lattice · Physics 2009-02-02 Harvey B. Meyer

This paper is devoted to proving that, in QCD, the lightest glueball state must be the scalar with $J^{PC} = 0^{++}$. The proof relies upon the positivity of the path integral measure in Euclidean space and the fact that interpolating…

High Energy Physics - Phenomenology · Physics 2009-10-28 Geoffrey B. West

The pseudoscalar mesons with the masses higher than 1 GeV are assumed to belong to the meson decuplet including the glueball as the basis state supplementing the standard $SU(3)_F$ nonet of light $q\bar{q}$ states $(u,d,s)$. The decuplet is…

High Energy Physics - Phenomenology · Physics 2011-02-18 M. Majewski , V. A. Meshcheryakov
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