By Maria-Novella Kienzle-Focacci, Maneesh Wadhwa
This quantity reviews on all points of high-energy photon interactions utilizing either photon and proton ambitions. major effects from the LEP and HERA experiments in addition to from CLEO II and BELLE are provided. those info are faced with diversified theoretical versions. particularly, predictions of QCD in either the perturbative and the non-perturbative quarter are generally mentioned. The customers for gamma-gamma physics at destiny high-energy colliders also are reviewed.
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Additional info for Photon 2001: International Conference on the Structure and Interactions of the Photon Including the 14th International Workshop on Photon-Photon Collisions Ascona,
M. Ciafaloni, Nucl. Phys. B 296, 49 (1988); S. Catani, F. Fiorani and G. Marchesini, Nucl. Phys. B 336, 18 (1990). S U M M A R Y OF T H E S T R U C T U R E F U N C T I O N SESSION AT P H O T O N 2001 RICHARD NISIUS CERN, Switzerland, E-mail: Richard. ch The status of and ongoing developments in the measurements and theoretical studies of the structure of the photon have been presented at the PHOTON 2001 conference in Ascona. The results presented in the structure function session are briefly summarised.
References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. R. Nisius, Phys. Rep. 332, 165 (2000). I. Tiapkin, these proceedings. R. Taylor, these proceedings, hep-ex/0110024. V. Blobel, Regularized Unfolding for High-Energy Physics Experiments, RUN program manual, unpublished (1996). A. Csilling, these proceedings. , G. , Eur. Phys. J. C16, 579 (2000). E. , Phys. Rev. D49, 5753 (1994); E. Laenen and S. Riemersma, Phys. Lett. B376, 169 (1996). A. Valkarova, these proceedings. K. Sedlak, these proceedings.
The total cross-section for cc production in deep-inelastic electron-photon scattering, shown in Figure 4a), is the result of an extrapolation to the whole kinematic region using the HERWIG scaled model. The value of the charm structure function of the photon, - F ^ x , (Q2))/aem, averaged over the corresponding bin in x, shown in Figure 4b), is obtained using the ratio F%c(x, (Q2))/aem/cr(e+e~ —* e + e _ c c X ) given by the NLO 2 calculation. 1, where the purely perturbative point-like process is dominant and both the experimental and the theoretical uncertainties are moderate.
Photon 2001: International Conference on the Structure and Interactions of the Photon Including the 14th International Workshop on Photon-Photon Collisions Ascona, by Maria-Novella Kienzle-Focacci, Maneesh Wadhwa