The Soft Gluon Emission Process in the Color-Octet Model for Heavy Quarkonium Production
arXiv:hep-ph/9906291 · doi:10.1103/PhysRevD.60.114025
Abstract
The Color-Octet Model has been used successfully to analyze many problems in heavy quarkonium production. We examine some of the conceptual and practical problems of the soft gluon emission process in the Color-Octet Model. We use a potential model to describe the initial and final states in the soft gluon emission process, as the emission occurs at a late stage after the production of the heavy quark pair. It is found in this model that the soft gluon M1 transition, 1S0(8)->3S1(1), dominates over the E1 transition, 3PJ(8)->3S1(1), for J/psi and psi' production. Such a dominance may help resolve the questions of isotropic polarization and color-octet matrix element universality in the Color-Octet Model.
26 pages, in LaTex
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Cited by in corpus (12)
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- Relativistic Modification of the Gamow Factor
- Bottomonium suppression at TeV using model based on color screening and gluonic dissociation with collisional damping
- Anomalous J/psi suppression and charmonium dissociation cross sections
- Nuclear annihilation by antinucleons
- Temperature dependent formation-time approach for suppression at energies available at the CERN Large Hadraon Collider
- Total Hadron-Hadron Cross Sections at High Energies
- Colour-octet bound states, induced by Higgs mechanism