Glueballs and other resonances with large gluonic components are predicted as
bound states by Quantum Chromodynamics (QCD). The lightest (scalar) glueball is
estimated to have a mass in the range from 1 to 2 GeV/c**2; a pseudoscalar and
tensor glueball are expected at higher masses. Many different experiments
exploiting a large variety of production mechanisms have presented results in
recent years on light mesons with J(PC) = 0(++), 0(-+), and 2(++) quantum
numbers. This review looks at the experimental status of glueballs. Good
evidence exists for a scalar glueball which is mixed with nearby mesons, but a
full understanding is still missing. Evidence for tensor and pseudoscalar
glueballs are weak at best. Theoretical expectations of phenomenological models
and QCD on the lattice are briefly discussed.
%0 Journal Article
%1 Crede2008Experimental
%A Crede, V.
%A Meyer, C. A.
%D 2008
%K glueball, nuclear
%T The Experimental Status of Glueballs
%U http://arxiv.org/abs/0812.0600
%X Glueballs and other resonances with large gluonic components are predicted as
bound states by Quantum Chromodynamics (QCD). The lightest (scalar) glueball is
estimated to have a mass in the range from 1 to 2 GeV/c**2; a pseudoscalar and
tensor glueball are expected at higher masses. Many different experiments
exploiting a large variety of production mechanisms have presented results in
recent years on light mesons with J(PC) = 0(++), 0(-+), and 2(++) quantum
numbers. This review looks at the experimental status of glueballs. Good
evidence exists for a scalar glueball which is mixed with nearby mesons, but a
full understanding is still missing. Evidence for tensor and pseudoscalar
glueballs are weak at best. Theoretical expectations of phenomenological models
and QCD on the lattice are briefly discussed.
@article{Crede2008Experimental,
abstract = {{Glueballs and other resonances with large gluonic components are predicted as
bound states by Quantum Chromodynamics (QCD). The lightest (scalar) glueball is
estimated to have a mass in the range from 1 to 2 GeV/c**2; a pseudoscalar and
tensor glueball are expected at higher masses. Many different experiments
exploiting a large variety of production mechanisms have presented results in
recent years on light mesons with J(PC) = 0(++), 0(-+), and 2(++) quantum
numbers. This review looks at the experimental status of glueballs. Good
evidence exists for a scalar glueball which is mixed with nearby mesons, but a
full understanding is still missing. Evidence for tensor and pseudoscalar
glueballs are weak at best. Theoretical expectations of phenomenological models
and QCD on the lattice are briefly discussed.}},
added-at = {2019-02-23T22:09:48.000+0100},
archiveprefix = {arXiv},
author = {Crede, V. and Meyer, C. A.},
biburl = {https://www.bibsonomy.org/bibtex/2a44128ff1a0801d5f07a64805b0c95ca/cmcneile},
citeulike-article-id = {3744420},
citeulike-linkout-0 = {http://arxiv.org/abs/0812.0600},
citeulike-linkout-1 = {http://arxiv.org/pdf/0812.0600},
day = 3,
eprint = {0812.0600},
interhash = {00ec349da170fa7870919f76ecf68594},
intrahash = {a44128ff1a0801d5f07a64805b0c95ca},
keywords = {glueball, nuclear},
month = dec,
posted-at = {2009-05-21 13:54:41},
priority = {2},
timestamp = {2019-02-23T22:15:27.000+0100},
title = {{The Experimental Status of Glueballs}},
url = {http://arxiv.org/abs/0812.0600},
year = 2008
}