2008
DOI: 10.1140/epja/i2008-10675-5
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Constituent gluon interpretation of glueballs and gluelumps

Abstract: Arguments are given that support the interpretation of the lattice QCD glueball and gluelump spectra in terms of bound states of massless constituent gluons with helicity-1. In this scheme, the mass hierarchy of the currently known gluelumps and glueballs is mainly due to the number of constituent gluons and can be understood within a simple flux tube model. It is also argued that the lattice QCD 0 +− glueball should be seen as a four-gluon bound state.

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Cited by 29 publications
(50 citation statements)
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“…The spin-space part could also depend on the gauge algebra through a change in the numerical values of the parameters appearing in a specific Hamiltonian, but this would only affect quantitatively the mass spectrum, not the basic properties studied in this work like the allowed quantum numbers and the mass hierarchy. As stressed in [11], those global properties are mostly consequences of the colour structure of a given state -responsible for C according to (2) -and of the peculiar dynamics induced by the transversality of the quasigluons and the Pauli principle -responsible for J P .…”
Section: The Quasigluon Picturementioning
confidence: 99%
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“…The spin-space part could also depend on the gauge algebra through a change in the numerical values of the parameters appearing in a specific Hamiltonian, but this would only affect quantitatively the mass spectrum, not the basic properties studied in this work like the allowed quantum numbers and the mass hierarchy. As stressed in [11], those global properties are mostly consequences of the colour structure of a given state -responsible for C according to (2) -and of the peculiar dynamics induced by the transversality of the quasigluons and the Pauli principle -responsible for J P .…”
Section: The Quasigluon Picturementioning
confidence: 99%
“…Although the explicit form of (anti)symmetrized threequasigluon states within Wick's three-body helicity formalism [38] will not be given here for the sake of clarity, some observations can be made concerning the quantum numbers of the lightest three-quasigluon states. Group-theoretical arguments developed in [11] show that the lowest-lying three-quasigluon glueballs will have the quantum numbers 0 −+ and (1, 3) +− . The absence of low-lying 0 P − state is in agreement with [39], that is actually an extension of Yang's theorem to three-photon states, showing that no (pseudo)scalar three-photon state may exist.…”
Section: Three-quasigluon Glueballsmentioning
confidence: 99%
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“…This work is in progress. However, we have some indications that the lowest-lying odd-C glueballs with transverse gluons are spin 1 and 3 [13]. Symmetry arguments are also in favour of a four-gluon interpretation for 0 +− .…”
Section: Pos(confinement8)084mentioning
confidence: 65%
“…Table 2: Possible number of constituent gluons corresponding to the number of hybrid mesons upto multiplicityThe predictions discussed above do not give any information about the relationship between the number of constituent gluons and the masses of the observed hybrids since in exact SU (3) C symmetry, gluons are massless. However, there are specific models in literature, where the constituent gluons have effective mass of the order of 0.7 GeV [16,17] resulting in the following degenerate mass relation:…”
Section: Number Of Constituent Gluonsmentioning
confidence: 99%