glueball state
Recently Published Documents


TOTAL DOCUMENTS

8
(FIVE YEARS 0)

H-INDEX

3
(FIVE YEARS 0)

2019 ◽  
Vol 99 (4) ◽  
Author(s):  
Phillip Lakaschus ◽  
Justin L. P. Mauldin ◽  
Francesco Giacosa ◽  
Dirk H. Rischke




2018 ◽  
Vol 175 ◽  
pp. 05016
Author(s):  
Wei Sun ◽  
Long-Cheng Gui ◽  
Ying Chen ◽  
Ming Gong ◽  
Zhaofeng Liu

Abstract.We perform a glueball-relevant study on isoscalars based on anisotropic Nf = 2 lattice QCD gauge configurations. In the scalar channel, we identify the ground state obtained through gluonic operators to be a single-particle state through its dispersion relation. When qq operator is included, we find the mass of this state does not change, and the qq operator couples very weakly to this state. So this state is most likely a glueball state. For pseudoscalars, along with the exiting lattice results, our study implies that both the conventional qq state η2 (or η' in flavor SU(3)) and a heavier glueball-like state with a mass of roughly 2.6 GeV exist in the spectrum of lattice QCD with dynamical quarks.



2003 ◽  
Vol 18 (19) ◽  
pp. 3335-3346 ◽  
Author(s):  
De-Min Li ◽  
Bing Ma ◽  
Hong Yu

Considering corrections due to SU(3) flavor symmetry breaking, non-ideal ω - ϕ mixing, double OZI and electromagnetic amplitudes of J/ψ decays into a vector and a pseudo-scalar meson, and three-gluon-annihilation amplitudes of radiative decays of J/ψ into a pseudoscalar meson, we investigate two-photon decays of pseudoscalar mesons, radiative decays between pseudoscalar and vector mesons, decays of J/ψ into a vector and a pseudoscalar meson, and radiative decays of J/ψ into a pseudoscalar meson. The quarkonia-glueball structure of η, η′ and η(1440) is phenomenologically deduced from the fit to the updated world average data concerning the above mentioned decays. We find that η (η′) contains about 48.7%, 47.6%, 3.7% (32.9%, 48.8%, 18.3%) non-strange quarkonium, strange quarkonium and glueball components, respectively, and that η(1410) is mainly a glueball state (about 78% glueball component), mixed with 18.5% non-strange quarkonium and 3.5% strange quarkonium. We predict that Br (J/ψ→γη) : Br (J/ψ→γη′) : Br (J/ψ→γη(1410)) = 1.0:5.2:8.0, which can be tested at BEPC/BES with 50 million J/ψ events.



2002 ◽  
Vol 17 (22) ◽  
pp. 1419-1429 ◽  
Author(s):  
DA QING LIU ◽  
JI MIN WU

Under the quenched approximation, we perform a lattice calculation for the mass of the ground 4++ glueball state in E++ channel on a D =3 + 1 lattice. Our calculation shows that the mass of this state is MG (4++) = 3.65(6)(18) GeV , which rules out the 4++ or mainly 4++ glueball state interpretation for ξ(2230).



1996 ◽  
Vol 77 (13) ◽  
pp. 2622-2625 ◽  
Author(s):  
Geoffrey B. West
Keyword(s):  


1986 ◽  
Vol 33 (2) ◽  
pp. 596-597 ◽  
Author(s):  
Helmut Kamenzki ◽  
Bernd Berg
Keyword(s):  


1985 ◽  
Vol 31 (7) ◽  
pp. 1743-1745 ◽  
Author(s):  
A. C. B. Antunes ◽  
F. Caruso
Keyword(s):  


Sign in / Sign up

Export Citation Format

Share Document