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Related papers: Pseudoscalar glueball mass: a window on three-gluo…

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We discuss our results on scalar glueball decay in the top-down holographic Witten-Sakai-Sugimoto model for low-energy QCD and compare with available experimental data, which appear to disfavor the glueball candidate $f_0(1500)$ but seem to…

High Energy Physics - Phenomenology · Physics 2015-11-05 Frederic Brünner , Denis Parganlija , Anton Rebhan

We consider a simple supersymmetric hidden sector: pure SU(N) gauge theory. Dark matter is made up of hidden glueballinos with mass $m_X$ and hidden glueballs with mass near the confinement scale $\Lambda$. For $m_X \sim 1\,\text{TeV}$ and…

High Energy Physics - Phenomenology · Physics 2015-07-13 Kimberly K. Boddy , Jonathan L. Feng , Manoj Kaplinghat , Yael Shadmi , Timothy M. P. Tait

We measure glueball masses and the string tension in twelve-flavour QCD, aiming at comparing the emerging gluonic spectrum to the mesonic one. When approaching the critical surface at zero quark mass, the hierarchy of masses in the…

A QCD-Pomeron composed by two non-perturbative gluons with a dynamically generated mass, is constructed in a gauge invariant way. The gluon propagator is infrared-finite. The model properly describes data on elastic scattering, exclusive…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. B. Gay Ducati

Lattice QCD and other theoretical models predict that the 0(-+), 2(++) and 2(-+) glueballs have masses in the range of 2.0 to 2.4 GeV. For resonances in such an energy range, three-body decay modes are expected to be large. The strategy for…

High Energy Physics - Experiment · Physics 2009-10-31 Bing-Song Zou

We calculate the branching ratios of the lightest pseudoscalar glueball with a mass of 2.6 GeV predicted by lattice QCD by using a chiral Lagrangian. This study is relevant in view of the planned PANDA experiment at the upcoming FAIR…

High Energy Physics - Phenomenology · Physics 2015-06-12 Walaa I. Eshraim , Stanislaus Janowski

Based on a semiclassical expansion for quantum chromodynamics in the instanton liquid background, the correlation function of the $0^{++}$ scalar glueball current is given, and the properties of the $0^{++}$ scalar glueball are studied in…

High Energy Physics - Phenomenology · Physics 2010-11-12 Shuiguo Wen , Zhenyu Zhang , Jueping Liu

This paper is a continuation of ArXiv:0707.1324 where improved holographic theories for QCD were set up and explored. Here, the IR confining geometries are classified and analyzed. They all end in a "good" (repulsive) singularity in the IR.…

High Energy Physics - Theory · Physics 2009-01-06 U. Gursoy , E. Kiritsis , F. Nitti

The mixing angles between scalar isoscalar resonances and a scalar glueball are determined from their decays into two pseudoscalar mesons. For $f_0(1370)$ and $f_0(1500)$, at most a small glueball component is admitted by the data. The…

High Energy Physics - Phenomenology · Physics 2022-03-14 Eberhard Klempt , Andrey V. Sarantsev

The lowest-lying glueball masses are computed in SU($N$) gauge theory on a spacetime lattice for constant value of the lattice spacing $a$ and for $N$ ranging from 3 to 8. The lattice spacing is fixed using the deconfinement temperature at…

High Energy Physics - Lattice · Physics 2011-01-19 Biagio Lucini , Antonio Rago , Enrico Rinaldi

Although marginally more complicated than the traditional Laplace sum-rules, Gaussian sum-rules have the advantage of being able to probe excited and ground states with similar sensitivity. Gaussian sum-rule analysis techniques are applied…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Harnett , T. G. Steele

We study the vacuum properties of the pseudoscalar glueball and charmed mesons by using the so-called extended Linear Sigma Model (eLSM). This model includes scalar and pseudoscalar mesons, as well as vector and axial-vector mesons. We…

High Energy Physics - Phenomenology · Physics 2019-01-14 Walaa I. Eshraim

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 prove a theorem in QCD stating that in the limit of strong coupling, $g\to\infty$, the observed spectrum of glueballs in QCD is the same of a pure Yang-Mills theory, being mixing effects due to the next-to-leading order. A full effective…

High Energy Physics - Phenomenology · Physics 2009-05-18 Marco Frasca

Continuum and lattice analyses have revealed the existence of a mass-scale in the gluon two-point Schwinger function. It has long been conjectured that this expresses the action of a Schwinger mechanism for gauge boson mass generation in…

High Energy Physics - Phenomenology · Physics 2023-05-03 A. C. Aguilar , F. De Soto , M. N. Ferreira , J. Papavassiliou , F. Pinto-Gómez , C. D. Roberts , J. Rodríguez-Quintero

Because glueballs are SU(3)_{Flavor} singlets, they are expected to couple equally to u,d, and s quarks, so that equal coupling strengths to \pi^+\pi^- and K^+K^- are predicted. However, we show that chiral symmetry implies the scalar…

High Energy Physics - Phenomenology · Physics 2008-11-26 Michael Chanowitz

According to lattice simulations and other theoretical approaches, the scalar glueball is the lightest state in the Yang-Mills sector of QCD. Since within this sector the scalar glueball is stable, the scattering between two glueballs is a…

High Energy Physics - Phenomenology · Physics 2022-01-03 Enrico Trotti , Francesco Giacosa

We study the spectra of two-gluon glueballs and three-gluon oddballs and corresponding equation of state in $5$-dimensional deformed holographic QCD models in the graviton-dilaton system, where the metric, the dilaton field and dilaton…

High Energy Physics - Phenomenology · Physics 2022-02-02 Lin Zhang , Chutian Chen , Yidian Chen , Mei Huang

The spectrum of glueballs with quantum numbers $J^\mathsf{PC}=0^{\pm+},2^{\pm+},3^{\pm+},4^{\pm+}$ is calculated in quenched quantum chromodynamics from bound state equations. The input is taken from a parameter-free calculation of two- and…

High Energy Physics - Phenomenology · Physics 2022-01-17 Markus Q. Huber , Christian S. Fischer , Hèlios Sanchis-Alepuz

The decay of 2-gluon colour singlets in quarks: 2g --> q-qbar +2q-2qbar has been simulated with the Monte-Carlo method, taking into account an effective 1-gluon exchange interaction between the emitted quarks, which was folded with a…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. P. Morsch , P. Zupranski
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