Difference between revisions of "GlueX Physics Strong Decay Models"
From GlueXWiki
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==[[GlueX_Physics_Strong_Decay_Models | Strong Decay Models]]== | ==[[GlueX_Physics_Strong_Decay_Models | Strong Decay Models]]== | ||
| − | + | ===SU(3) Decay Calculations=== | |
| + | ===The <sup>3</sup>P<sub>0</sub> Model=== | ||
Attempts at modeling strong decays date from 1969, | Attempts at modeling strong decays date from 1969, | ||
when Micu suggested | when Micu suggested | ||
| Line 36: | Line 37: | ||
disagree with experiment. | disagree with experiment. | ||
| − | + | ===References=== | |
| − | + | ====Meson Decay References==== | |
| − | + | * <i>Higher quarkonia</i>, T.Barnes, F.E. Close, P.R. Page and E.S. Swanson, Phys. Rev. D<b>55</b> (1997), 4157-4188 [http://dx.doi.org/10.1103/PhysRevD.55.4157 PRD]. | |
| − | + | * <i>On the mechanism of open flavor strong decays</i>, E.S. Ackleh, T. Barnes and E.S. Swanson, Phys. Rev. D<b>54</b> (1996), 6811-6829, [http://dx.doi.org/10.1103/PhysRevD.54.6811 PRD]. | |
| − | + | * <i> Hybrid and conventional mesons in the flux tube model: Numerical studies and their phenomenological implications</i>, T. Barnes, F.E. Close and E.S. Swanson, Phys. Rev. D<b>52</b> (1995), 5242-5256, [http://dx.doi.org/10.1103/PhysRevD.52.5242 PRD]. | |
| − | + | * <i> The Quenched Approximation In The Quark Model</i>, P. Geiger and N. Isgur, Phys. Rev. D<b>41</b> (1990), 1595, [http://dx.doi.org/10.1103/PhysRevD.41.1595 PRD]. | |
| − | + | * <i>Meson Decays by Flux Tube Breaking</i>, R. Kokoski and N. Isgur, Phys. Rev. D<b>35</b> (1987), 907, [http://dx.doi.org/10.1103/PhysRevD.35.907 PRD]. | |
| − | + | * <i>A Flux Tube Model for Hadrons in QCD</i>, N. Isgur, J. E. Paton, Phys. Rev. D<b>31</b> (1985), 2910, [http://dx.doi.org/10.1103/PhysRevD.31.2910 PRD]. | |
| − | + | * <i>A Flux Tube Model for Hadrons</i> N. Isgur and J. E. Paton, Phys. Lett. B<b>124</b>, (1983), 247, [http://dx.doi.org/10.1016/0370-2693(83)91445-4 Science Direct]. | |
| − | + | ====Hybrid Meson Decay References==== | |
| + | * <i>The "forbidden" decays of hybrid mesons to π ρ can be large</i>, F.E. Close and J.J. Dudek, Phys. Rev. D<b>70</b> (2004), 094015, [http://arxiv.org/abs/hep-ph/0308099v2 arXiv]. | ||
** <i>Hybrid Meson Decay Phenomenology</i>, P.R. Page, E.S. Swanson and A.P. Szczepaniak, Phys. Rev. D<b>59</b> (1999), 034016, [http://arxiv.org/abs/hep-ph/9808346v1 arXiv]. | ** <i>Hybrid Meson Decay Phenomenology</i>, P.R. Page, E.S. Swanson and A.P. Szczepaniak, Phys. Rev. D<b>59</b> (1999), 034016, [http://arxiv.org/abs/hep-ph/9808346v1 arXiv]. | ||
| − | + | * <i>Why Hybrid Meson Coupling to Two S-wave Mesons is Suppressed</i>, P.R. Page, Phys. Lett. B<b>402</b> (1996), 183-188, [http://arxiv.org/abs/hep-ph/9611375v2 arXiv]. | |
| − | + | * <i>Q anti-Q G Hermaphrodite Mesons in the MIT Bag Model</i>, T. Barnes, F.E. Close, F. de Viron and J. Weyers, Nucl. Phys. B<b>224</b> (1983), 241, [http://dx.doi.org/10.1016/0550-3213(83)90004-4 Science Direct]. | |
| − | + | * <i> Gluonic Excitations of Mesons: Why They Are Missing and Where to Find Them</i>, N. Isgur, R. Kokoski and J. E. Paton, Phys. Rev. Lett. <b>54</b> (1985), 869, [http://dx.doi.org/10.1103/PhysRevLett.54.869 PRL]. | |
Revision as of 10:16, 19 April 2010
Contents
GlueX Physics
Review Papers
Mesons in the Quark Model
Exotic Quantum Number Mesons
Lattice QCD Calculations
Photoproduction
Strong Decay Models
SU(3) Decay Calculations
The 3P0 Model
Attempts at modeling strong decays date from 1969,
when Micu suggested
that hadron decay proceeds through $q\bar q$ pair production with vacuum
quantum numbers, 
. Since this corresponds to a 3P0
state, it is now generally referred to as the 3p0
decay model. This suggestion was developed and applied extensively by
Le Yaouanc et al. in the 1970s.
Studies of hadron decays using the 3p0 model
have been
concerned almost exclusively with numerical predictions, and have not led to
any fundamental modifications to the original model.
Recent studies have considered changes in the spatial
dependence of the pair production amplitude as a function of
quark coordinates
but the fundamental decay mechanism is usually not
addressed; this is widely believed to be a nonperturbative process,
involving ``flux tube breaking".
There have been some studies of the decay
mechanism which consider an alternative phenomenological
model in which the pair is produced with 3S1
quantum numbers; this possibility however appears to
disagree with experiment.
References
Meson Decay References
- Higher quarkonia, T.Barnes, F.E. Close, P.R. Page and E.S. Swanson, Phys. Rev. D55 (1997), 4157-4188 PRD.
- On the mechanism of open flavor strong decays, E.S. Ackleh, T. Barnes and E.S. Swanson, Phys. Rev. D54 (1996), 6811-6829, PRD.
- Hybrid and conventional mesons in the flux tube model: Numerical studies and their phenomenological implications, T. Barnes, F.E. Close and E.S. Swanson, Phys. Rev. D52 (1995), 5242-5256, PRD.
- The Quenched Approximation In The Quark Model, P. Geiger and N. Isgur, Phys. Rev. D41 (1990), 1595, PRD.
- Meson Decays by Flux Tube Breaking, R. Kokoski and N. Isgur, Phys. Rev. D35 (1987), 907, PRD.
- A Flux Tube Model for Hadrons in QCD, N. Isgur, J. E. Paton, Phys. Rev. D31 (1985), 2910, PRD.
- A Flux Tube Model for Hadrons N. Isgur and J. E. Paton, Phys. Lett. B124, (1983), 247, Science Direct.
Hybrid Meson Decay References
- The "forbidden" decays of hybrid mesons to π ρ can be large, F.E. Close and J.J. Dudek, Phys. Rev. D70 (2004), 094015, arXiv.
- Hybrid Meson Decay Phenomenology, P.R. Page, E.S. Swanson and A.P. Szczepaniak, Phys. Rev. D59 (1999), 034016, arXiv.
- Why Hybrid Meson Coupling to Two S-wave Mesons is Suppressed, P.R. Page, Phys. Lett. B402 (1996), 183-188, arXiv.
- Q anti-Q G Hermaphrodite Mesons in the MIT Bag Model, T. Barnes, F.E. Close, F. de Viron and J. Weyers, Nucl. Phys. B224 (1983), 241, Science Direct.
- Gluonic Excitations of Mesons: Why They Are Missing and Where to Find Them, N. Isgur, R. Kokoski and J. E. Paton, Phys. Rev. Lett. 54 (1985), 869, PRL.
