scholarly journals Scalar glueball and meson spectroscopy in unquenched lattice QCD with improved staggered quarks

Author(s):  
Alan C. Irving ◽  
Eric B. Gregory ◽  
Craig McNeile ◽  
Steven Miller ◽  
Zbyszek Sroczynski
2017 ◽  
Vol 58 (3) ◽  
Author(s):  
Christopher E. Thomas

2013 ◽  
Author(s):  
Christopher E. Thomas ◽  
Hadron Spectrum Collaboration

2011 ◽  
Author(s):  
Christopher E. Thomas ◽  
David Armstrong ◽  
Volker Burkert ◽  
Jian-Ping Chen ◽  
Will Detmold ◽  
...  

2009 ◽  
Vol 24 (18n19) ◽  
pp. 3392-3402 ◽  
Author(s):  
HAI-YANG CHENG

We employ two simple and robust results to constrain the mixing matrix of the isosinglet scalar mesons f0(1710), f0(1500), f0(1370): one is the approximate SU (3) symmetry empirically observed in the scalar sector above 1 GeV and confirmed by lattice QCD, and the other is the scalar glueball mass at 1710 MeV in the quenched approximation. In the SU (3) symmetry limit, f0(1500) becomes a pure SU (3) octet and is degenerate with a0(1450), while f0(1370) is mainly an SU (3) singlet with a slight mixing with the scalar glueball which is the primary component of f0(1710). These features remain essentially unchanged even when SU (3) breaking is taken into account. The observed enhancement of ωf0(1710) production over ɸf0(1710) in hadronic J/ψ decays and the copious f0(1710) production in radiative J/ψ decays lend further support to the prominent glueball nature of f0(1710). We deduce the mass of the pseudoscalar glueball G from an η-η′-G mixing formalism based on the anomalous Ward identity for transition matrix elements. With the inputs from the recent KLOE experiment, we find a solution for the pseudoscalar glueball mass around (1.4±0.1) GeV, which is fairly insensitive to a range of inputs with or without Okubo-Zweig-Iizuka-rule violating effects. This affirms that η(1405), having a large production rate in the radiative J/ψ decay and not seen in γγ reactions, is indeed a leading candidate for the pseudoscalar glueball. It is much lower than the results from quenched lattice QCD (> 2.0 GeV) due to the dynamic fermion effect. It is thus urgent to have a full QCD lattice calculation of pseudoscalar glueball masses.


2017 ◽  
Author(s):  
David Tims ◽  
Gavin Cheung ◽  
Cian O'Hara ◽  
Graham Moir ◽  
M. J. Peardon ◽  
...  

2012 ◽  
Author(s):  
Christopher E. Thomas ◽  
Hadron Spectrum Collaboration

2003 ◽  
Vol 18 (03) ◽  
pp. 515-523
Author(s):  
D. Urner

The CLEO collaboration will explore the charm sector starting 2003. It is foreseen to collect on the order of 6 million [Formula: see text] pairs, 300000 [Formula: see text] pair at threshold and one billion J/ψ decays. High precision charm data will enable us to validate upcoming lattice QCD calculations that are expected to produce 1-3% errors for some non-perturbative QCD quantities. Virtually background free, they will provide interesting decay mechanisms to explore light meson spectroscopy. The radiative J/ψ decays will be the first high statistics data set well suited for meson spectroscopy between 1600 and 3000 MeV. Together with the already existing data from the ϒ resonances, data sets for a large number of decay mechanisms will be available, which, combined, can be used to extract the nature of many resonances.


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