Difference between revisions of "GlueX Physics"

From GlueXWiki
Jump to: navigation, search
(Photoproduction)
Line 9: Line 9:
 
==[[GlueX_Physics_Photoproduction | Photoproduction]]==
 
==[[GlueX_Physics_Photoproduction | Photoproduction]]==
  
*<b>Experimental Papers</b>
 
** <i>Differential cross sections and spin density matrix elements for &gamma;p &rarr; &omega; p</i>, M. Williams, <i>et al.</i>, (CLAS Collaboration), submitted to Phys. Rev. C (2009), [http://xxx.lanl.gov/abs/0908.2910 arXiv].
 
** <i>Partial wave analysis of &gamma; p &rarr; &omega; 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].
 
** <i>Differential cross sections for the reactions &gamma; p &rarr; &eta; p and &gamma; p &rarr; &eta;' p</i>, M. Williams, <i>et al.</i>, (CLAS Collaboration), submitted to Phys. Rev. C (2009), [http://xxx.lanl.gov/abs/0909.0616 arXiv].
 
** <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]
 
** <i>Bubble-Chamber Study of Photoproduction by 2.8 and 4.7 GeV Polarized Photons. I. Cross-Section Determination and Production of &rho;<sup>0</sup> and &Delta;<sup>++</sup> in the Reaction &gamma;p &rarr; p&pi;+&pi;-</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].
 
** <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].
 
** <i>Spin-Parity Analysis of &rho;' in the reaction &gamma; p &rarr; &pi;+ &pi;+ &pi;- &pi;-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].
 
** <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].
 
** <i>The Reaction &gamma; p &rarr; &pi;+ &pi;- &pi;+ &pi;- p at High-energy and  dissociation into 4&pi;</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].
 
  
==Strong Decay Models==
+
==[[GlueX_Physics_Strong_Decay_Models | Strong Decay Models]]==
  
  

Revision as of 17:24, 2 April 2010

GlueX Physics

Review Papers

Exotic Quantum Number Mesons

Lattice QCD Calculations

Photoproduction

Strong Decay Models

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, J^{{PC}}=0^{{++}}. Since this corresponds to a 3P0 q{\bar  q} 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 q{\bar  q} pair is produced with 3S1 quantum numbers; this possibility however appears to disagree with experiment.

  • mesons
    • 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.
  • hybrids
    • 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.