1999
DOI: 10.1103/physrevd.61.014015
|View full text |Cite
|
Sign up to set email alerts
|

Scalar quarkonium masses and mixing with the lightest scalar glueball

Abstract: We evaluate the continuum limit of the valence ͑quenched͒ approximation to the mass of the lightest scalar quarkonium state, for a range of different quark masses, and to the mixing energy between these states and the lightest scalar glueball. Our results support the interpretation of f 0 (1710) as composed mainly of the lightest scalar glueball.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

6
110
1

Year Published

2000
2000
2015
2015

Publication Types

Select...
4
4

Relationship

0
8

Authors

Journals

citations
Cited by 218 publications
(117 citation statements)
references
References 20 publications
(62 reference statements)
6
110
1
Order By: Relevance
“…Based on their lattice calculations of the quenched scalar glueball mass at 1625(94) MeV at the infinite volume and continuum limits [13] and the ss meson mass in the connected insertion (no annihilation) at ∼ 1500 MeV, Lee and Weingarten [14,15] considered a mixing scheme where f 0 (1500) is an almost pure ss meson and f 0 (1710) and f 0 (1370) are primarily the glueball and uū + dd meson respectively, but with substantial mixing between the two (∼ 25% for the small component). With the effective chiral Lagrangian approach, Giacosa et al [16] performed a fit to the experimental masses and decay widths of f 0 (1710), f 0 (1500) and f 0 (1370) and found four possible solutions, depending on whether the direct decay of the glueball component is considered.…”
Section: Introductionmentioning
confidence: 99%
“…Based on their lattice calculations of the quenched scalar glueball mass at 1625(94) MeV at the infinite volume and continuum limits [13] and the ss meson mass in the connected insertion (no annihilation) at ∼ 1500 MeV, Lee and Weingarten [14,15] considered a mixing scheme where f 0 (1500) is an almost pure ss meson and f 0 (1710) and f 0 (1370) are primarily the glueball and uū + dd meson respectively, but with substantial mixing between the two (∼ 25% for the small component). With the effective chiral Lagrangian approach, Giacosa et al [16] performed a fit to the experimental masses and decay widths of f 0 (1710), f 0 (1500) and f 0 (1370) and found four possible solutions, depending on whether the direct decay of the glueball component is considered.…”
Section: Introductionmentioning
confidence: 99%
“…2 Table 2 ground state contributions so that the systematic error on E from this assumption is hard to estimate. The mixing estimated by ref [4] is similar in magnitude at these lattice parameters (E ≈ 0.3 GeV) but they claim that on extrapolation to the continuum limit a much smaller value is obtained. Here we are using clover improvement so order a effects are suppressed.…”
Section: Scalar Mesonsmentioning
confidence: 69%
“…Using the glueball mass of 0.97(4) from ref. [4] and scalar qq mass of 1.48(15) from fitting the connected correlations, we are able to fit the disconnected correlation and the hairpin-Wilson loop correlation from t-values of 1 to 3 with a mixing given by Ea = 0.4 assuming N f = 2. This fit (see fig.…”
Section: Scalar Mesonsmentioning
confidence: 99%
See 1 more Smart Citation
“…In quenched QCD, DeTar and Kogut first measured the σ meson screening mass in a lattice simulation [5], Alford and Jaffe discussed the possible light scalar mesons asq 2 q 2 states [6], and masses and mixing of qq states and a glueball have been investigated by Lee and Weingarten [7]. However, as we have already reported in the previous proceedings [8], the connected and disconnected diagrams give almost the same amount of the contributions, indicating that the dynamical quark effect seems to be essential in the calculation.…”
Section: Introductionmentioning
confidence: 99%