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− | ==[[GlueX_Physics_Review_Papers | Review Papers]]== | + | ==[[GlueX Physics]]== |
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− | ==[[GlueX_Physics_Exotc_Quantum_Number_Mesons | Exotic Quantum Number Mesons]]== | + | ==[[GlueX_Physics_Review_Papers | Review Papers]]== |
| + | <font color=green>(Papers with abstracts)</font> |
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− | ==Lattice QCD Calculations== | + | ==[[GlueX_Physics_Quark_Model | Mesons in the Quark Model]]== |
| + | <font color=blue>(Long text description)</font> |
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− | * <b>Hybrid Meson Calculations</b>
| + | ==[[GlueX_Physics_Exotic_Quantum_Number_Mesons | Exotic Quantum Number Mesons]]== |
− | ** <i>Highly excited and exotic meson spectrum from dynamical lattice QCD</i>, Jozef J Dudek, Robert G Edwards, David G Richards, Christopher E Thomas, (2009), [http://arxiv.org/abs/0909.0200v1 arXiv].
| + | <font color=blue>(Some text and List of Papers)</font> |
− | ** <i>Decay width of light quark hybrid meson from the lattice</i>, C. McNeile and C. Michael, Phys. Rev. D<b>73</b>, (2006), 074506, [http://arxiv.org/abs/hep-lat/0603007v3 arXiv].
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− | ** <i>Lattice calculation of 1<sup>-+</sup> hybrid mesons with improved Kogut-Susskind fermions</i>, C. Bernard <i>et al.</i>, Phys. Rev. D<b>68</b>, (2003), 074505, [http://arxiv.org/abs/hep-lat/0301024v2 arXiv].
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− | ** <i>The heavy-quark hybrid meson spectrum in lattice QCD</i>, J. Juge, J. Kuti and C. Morningstar, AIP Conf.Proc.<b>688</b> (2004),193-207, [http://arxiv.org/abs/nucl-th/0307116v1 arXiv].
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− | ** <i>Hybrid meson decay from the lattice</i>, C. McNeile, C. Michael and P. Pennanen, Phys. Rev. D<b>65</b>, (2002), 094505, [http://arxiv.org/abs/hep-lat/0201006v1 arXiv].
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− | ** <i>Ab initio study of hybrid anti-b g b mesons</i>, K.J. Juge, J. Kuti and C.J. Morningstar, Phys. Rev. Lett.<b>82</b> (1999), 4400-4403, [http://dx.doi.org/10.1103/PhysRevLett.82.4400 PRL].
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− | ** <i>Exotic mesons in quenched lattice QCD</i>, C. Bernard <i>et al.</i> (MILC Collaboration), Phys. Rev. D<b>56</b> (1997), 7039, [http://dx.doi.org/10.1103/PhysRevD.56.7039 PRD].
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− | ** <i>Hybrid mesons from quenched QCD</i>, P. Lacock, C. Michael, P. Boyle and P. Rowland, Phys. Lett. B<b>401</b> (1996), 308-312, [http://arxiv.org/abs/hep-lat/9611011v1 arXiv].
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− | * <b>Glueball Calculations</b>
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− | ** <i>Glueball spectrum and matrix elements on anisotropic lattices</i>, Y. Chen <i>et al.</i>, Phys. Rev. D<b>73</b> (2006), 014516, [http://dx.doi.org/10.1103/PhysRevD.73.014516 PRD].
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− | ** <i> The Glueball spectrum from an anisotropic lattice study</i>, C. Morningstar <i>et al.</i>, Phys. Rev. D<b>60</b> (1999), 034509, [http://dx.doi.org/10.1103/PhysRevD.60.034509 PRD].
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− | ==Photoproduction== | + | ==[[GlueX_Physics_Lattice_QCD_Calculations | Lattice QCD Calculations]]== |
| + | <font color=green>(List of Papers)</font> |
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− | *<b>Experimental Papers</b>
| + | ==[[GlueX_Physics_Photoproduction | Photoproduction]]== |
− | ** <i>Differential cross sections and spin density matrix elements for γp → ω p</i>, M. Williams, <i>et al.</i>, (CLAS Collaboration), submitted to Phys. Rev. C (2009), [http://xxx.lanl.gov/abs/0908.2910 arXiv].
| + | <font color=green>(List of Papers)</font> |
− | ** <i>Partial wave analysis of γ p → ω p and the search for nucleon resonances</i>, M. Williams, <i>et al.</i>, (CLAS Collaboration), submitted to Phys. Rev. C (2009), [http://xxx.lanl.gov/abs/0908.2911 arXiv].
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− | ** <i>Differential cross sections for the reactions γ p → η p and γ p → η' p</i>, M. Williams, <i>et al.</i>, (CLAS Collaboration), submitted to Phys. Rev. C (2009), [http://xxx.lanl.gov/abs/0909.0616 arXiv].
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− | ** <i>On the Analysis of Vector-Meson Production by Polarized Photons</i>,K. Schilling, P. Seyboth and G. Wolf, Nucl. Phys. B<b>15</b> (1970), 397-412, [http://www.curtismeyer.com/articles/photoproduction/Schilling.pdf pdf]
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− | ** <i>Bubble-Chamber Study of Photoproduction by 2.8 and 4.7 GeV Polarized Photons. I. Cross-Section Determination and Production of ρ<sup>0</sup> and Δ<sup>++</sup> in the Reaction γp → pπ+π-</i> J. Ballam <i> et al.</i>, Phys. Rev. D<b>5</b> (1972), 545-589, [http://www.curtismeyer.com/articles/photoproduction/ballam_prd5.pdf pdf].
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− | ** <i>Vector-Meson Production by Polarized Photons at 2.8, 4.7 and 9.3 GeV</i>, J. Ballam <i>et al.</i>, Phys. Rev. D<b>7</b> (1973), 3150-3177, [http://www.curtismeyer.com/articles/photoproduction/ballam_prd7.pdf pdf].
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− | ** <i>Spin-Parity Analysis of ρ' in the reaction γ p → π+ π+ π- π-p at 9 to 18 GeV</i>, Joseph C.H. Park, Nucl. Phys. B<b>58</b>, (1973), 45-54, [http://www.curtismeyer.com/articles/photoproduction/Park_1973.pdf pdf].
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− | ** <i>High-Energy Production and Decay of vector and Tensor Mesons</i>, A.C. Irving and C. Michel, Nucl. Phys. B<b>82</b>, (1974), 282-325, [http://www.curtismeyer.com/articles/photoproduction/Irving_1974.pdf pdf].
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− | ** <i>The Reaction γ p → π+ π- π+ π- p at High-energy and dissociation into 4π</i>, M. Davier, <i>et al.</i>, Nucl. Phys. B<b>58</b> (1973), 31-44, [http://www.curtismeyer.com/articles/photoproduction/Davier_1973.pdf pdf].
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− | ==Strong Decay Models== | + | ==[[GlueX_Physics_Strong_Decay_Models | Strong Decay Models]]== |
| + | <font color=blue>(Some text and List of Papers)</font> |
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− | | + | ==[[Journal_Club | Journal Club]]== |
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− | Attempts at modeling strong decays date from 1969,
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− | when Micu suggested
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− | that hadron decay proceeds through $q\bar q$ pair production with vacuum
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− | quantum numbers, <math>J^{PC} = 0^{++}</math>. Since this corresponds to a <sup>3</sup>P<sub>0</sub>
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− | <math>q\bar q</math> state, it is now generally referred to as the 3p0
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− | decay model. This suggestion was developed and applied extensively by
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− | Le Yaouanc <i>et al.</i> in the 1970s.
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− | Studies of hadron decays using the 3p0 model
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− | have been
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− | concerned almost exclusively with numerical predictions, and have not led to
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− | any fundamental modifications to the original model.
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− | Recent studies have considered changes in the spatial
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− | dependence of the pair production amplitude as a function of
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− | quark coordinates
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− | but the fundamental decay mechanism is usually not
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− | addressed; this is widely believed to be a nonperturbative process,
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− | involving ``flux tube breaking".
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− | There have been some studies of the decay
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− | mechanism which consider an alternative phenomenological
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− | model in which the <math>q\bar q</math> pair is produced with <sup>3</sup>S<sub>1</sub>
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− | quantum numbers; this possibility however appears to
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− | disagree with experiment.
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− | *<b>mesons</b>
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | *<b>hybrids</b>
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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− | ** <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].
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